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1

availability in two different treatment implementations: (1) from seedlings exposed to 360, 550, and 700 mu mol mol(-1) CO2 in a  

E-Print Network [OSTI]

(A(max)), carboxylation efficiency (CE), and Rubisco catalytic sites, whereas droughted Larrea showed a differing response depending on treatment technique. A(max) and CE were lower in droughted Larrea compared LEAVES, RESPONSES, RIBULOSE-1;5-BISPHOSPHATE CARBOXYLASE, TEMPERATURE 988 Hymus, G.J., D.S. Ellsworth, N.R

2

Search for the rare decays Bs -> mu+ mu- and B0 -> mu+ mu-  

E-Print Network [OSTI]

A search for the decays Bs -> mu+ mu- and B0 -> mu+ mu- is performed with 0.37 fb^-1 of pp collisions at sqrt{s} = 7 TeV collected by the LHCb experiment in 2011. The upper limits on the branching fractions are BR (Bs -> mu+ mu-) mu+ mu-) mu+ mu-) mu+ mu-) < 3.2 x 10^-9 at 95% confidence level.

LHCb Collaboration; R. Aaij; C. Abellan Beteta; B. Adeva; M. Adinolfi; C. Adrover; A. Affolder; Z. Ajaltouni; J. Albrecht; F. Alessio; M. Alexander; G. Alkhazov; P. Alvarez Cartelle; A. A. Alves Jr; S. Amato; Y. Amhis; J. Anderson; R. B. Appleby; O. Aquines Gutierrez; F. Archilli; L. Arrabito; A. Artamonov; M. Artuso; E. Aslanides; G. Auriemma; S. Bachmann; J. J. Back; D. S. Bailey; V. Balagura; W. Baldini; R. J. Barlow; C. Barschel; S. Barsuk; W. Barter; A. Bates; C. Bauer; Th. Bauer; A. Bay; I. Bediaga; S. Belogurov; K. Belous; I. Belyaev; E. Ben-Haim; M. Benayoun; G. Bencivenni; S. Benson; J. Benton; R. Bernet; M. -O. Bettler; M. van Beuzekom; A. Bien; S. Bifani; T. Bird; A. Bizzeti; P. M. Bjørnstad; T. Blake; F. Blanc; C. Blanks; J. Blouw; S. Blusk; A. Bobrov; V. Bocci; A. Bondar; N. Bondar; W. Bonivento; S. Borghi; A. Borgia; T. J. V. Bowcock; C. Bozzi; T. Brambach; J. van den Brand; J. Bressieux; D. Brett; M. Britsch; T. Britton; N. H. Brook; H. Brown; A. Büchler-Germann; I. Burducea; A. Bursche; J. Buytaert; S. Cadeddu; O. Callot; M. Calvi; M. Calvo Gomez; A. Camboni; P. Campana; A. Carbone; G. Carboni; R. Cardinale; A. Cardini; L. Carson; K. Carvalho Akiba; G. Casse; M. Cattaneo; Ch. Cauet; M. Charles; Ph. Charpentier; N. Chiapolini; K. Ciba; X. Cid Vidal; G. Ciezarek; P. E. L. Clarke; M. Clemencic; H. V. Cliff; J. Closier; C. Coca; V. Coco; J. Cogan; P. Collins; A. Comerma-Montells; F. Constantin; G. Conti; A. Contu; A. Cook; M. Coombes; G. Corti; G. A. Cowan; R. Currie; B. D'Almagne; C. D'Ambrosio; P. David; P. N. Y. David; I. De Bonis; S. De Capua; M. De Cian; F. De Lorenzi; J. M. De Miranda; L. De Paula; P. De Simone; D. Decamp; M. Deckenhoff; H. Degaudenzi; M. Deissenroth; L. Del Buono; C. Deplano; D. Derkach; O. Deschamps; F. Dettori; J. Dickens; H. Dijkstra; P. Diniz Batista; F. Domingo Bonal; S. Donleavy; F. Dordei; P. Dornan; A. Dosil Suárez; D. Dossett; A. Dovbnya; F. Dupertuis; R. Dzhelyadin; A. Dziurda; S. Easo; U. Egede; V. Egorychev; S. Eidelman; D. van Eijk; F. Eisele; S. Eisenhardt; R. Ekelhof; L. Eklund; Ch. Elsasser; D. Elsby; D. Esperante Pereira; L. Estéve; A. Falabella; E. Fanchini; C. Färber; G. Fardell; C. Farinelli; S. Farry; V. Fave; V. Fernandez Albor; M. Ferro-Luzzi; S. Filippov; C. Fitzpatrick; M. Fontana; F. Fontanelli; R. Forty; M. Frank; C. Frei; M. Frosini; S. Furcas; A. Gallas Torreira; D. Galli; M. Gandelman; P. Gandini; Y. Gao; J-C. Garnier; J. Garofoli; J. Garra Tico; L. Garrido; D. Gascon; C. Gaspar; N. Gauvin; M. Gersabeck; T. Gershon; Ph. Ghez; V. Gibson; V. V. Gligorov; C. Göbel; D. Golubkov; A. Golutvin; A. Gomes; H. Gordon; M. Grabalosa Gándara; R. Graciani Diaz; L. A. Granado Cardoso; E. Graugés; G. Graziani; A. Grecu; E. Greening; S. Gregson; B. Gui; E. Gushchin; Yu. Guz; T. Gys; G. Haefeli; C. Haen; S. C. Haines; T. Hampson; S. Hansmann-Menzemer; R. Harji; N. Harnew; J. Harrison; P. F. Harrison; J. He; V. Heijne; K. Hennessy; P. Henrard; J. A. Hernando Morata; E. van Herwijnen; E. Hicks; K. Holubyev; P. Hopchev; W. Hulsbergen; P. Hunt; T. Huse; R. S. Huston; D. Hutchcroft; D. Hynds; V. Iakovenko; P. Ilten; J. Imong; R. Jacobsson; A. Jaeger; M. Jahjah Hussein; E. Jans; F. Jansen; P. Jaton; B. Jean-Marie; F. Jing; M. John; D. Johnson; C. R. Jones; B. Jost; M. Kaballo; S. Kandybei; M. Karacson; T. M. Karbach; J. Keaveney; I. R. Kenyon; U. Kerzel; T. Ketel; A. Keune; B. Khanji; Y. M. Kim; M. Knecht; P. Koppenburg; A. Kozlinskiy; L. Kravchuk; K. Kreplin; M. Kreps; G. Krocker; P. Krokovny; F. Kruse; K. Kruzelecki; M. Kucharczyk; T. Kvaratskheliya; V. N. La Thi; D. Lacarrere; G. Lafferty; A. Lai; D. Lambert; R. W. Lambert; E. Lanciotti; G. Lanfranchi; C. Langenbruch; T. Latham; C. Lazzeroni; R. Le Gac; J. van Leerdam; J. -P. Lees; R. Lefévre; A. Leflat; J. Lefrançois; O. Leroy; T. Lesiak; L. Li; L. Li Gioi; M. Lieng; M. Liles; R. Lindner; C. Linn; B. Liu; G. Liu; J. H. Lopes; E. Lopez Asamar; N. Lopez-March; H. Lu; J. Luisier; A. Mac Raighne; F. Machefert; I. V. Machikhiliyan; F. Maciuc; O. Maev; J. Magnin; S. Malde; R. M. D. Mamunur; G. Manca; G. Mancinelli; N. Mangiafave; U. Marconi; R. Märki; J. Marks; G. Martellotti; A. Martens; L. Martin; A. Martín Sánchez; D. Martinez Santos; A. Massafferri; Z. Mathe; C. Matteuzzi; M. Matveev; E. Maurice; B. Maynard; A. Mazurov; G. McGregor; R. McNulty; C. Mclean; M. Meissner; M. Merk; J. Merkel; R. Messi; S. Miglioranzi; D. A. Milanes; M. -N. Minard; J. Molina Rodriguez; S. Monteil; D. Moran; P. Morawski; R. Mountain; I. Mous; F. Muheim; K. Müller; R. Muresan; B. Muryn; B. Muster; M. Musy; J. Mylroie-Smith; P. Naik; T. Nakada; R. Nandakumar; I. Nasteva; M. Nedos; M. Needham; N. Neufeld; C. Nguyen-Mau; M. Nicol; V. Niess; N. Nikitin; A. Nomerotski; A. Novoselov; A. Oblakowska-Mucha; V. Obraztsov; S. Oggero; S. Ogilvy; O. Okhrimenko; R. Oldeman; M. Orlandea

2012-01-15T23:59:59.000Z

3

MU Eneg  

Annual Energy Outlook 2013 [U.S. Energy Information Administration (EIA)]

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecember 2005 (Thousand9,0, 1997EnvironmentElectricityrgy81 §98 3.241MTBE,MU Eneg

4

Strong constraints on the rare decays Bs -> mu+ mu- and B0 -> mu+ mu-  

E-Print Network [OSTI]

A search for Bs -> mu+ mu- and B0 -> mu+ mu- decays is performed using 1.0 fb^-1 of pp collision data collected at \\sqrt{s}=7 TeV with the LHCb experiment at the Large Hadron Collider. For both decays the number of observed events is consistent with expectation from background and Standard Model signal predictions. Upper limits on the branching fractions are determined to be BR(Bs -> mu+ mu-) mu+ mu-) < 1.0 (0.81) x 10^-9 at 95% (90%) confidence level.

LHCb collaboration; R. Aaij; C. Abellan Beteta; A. Adametz; B. Adeva; M. Adinolfi; C. Adrover; A. Affolder; Z. Ajaltouni; J. Albrecht; F. Alessio; M. Alexander; S. Ali; G. Alkhazov; P. Alvarez Cartelle; A. A. Alves Jr; S. Amato; Y. Amhis; J. Anderson; R. B. Appleby; O. Aquines Gutierrez; F. Archilli; A. Artamonov; M. Artuso; E. Aslanides; G. Auriemma; S. Bachmann; J. J. Back; V. Balagura; W. Baldini; R. J. Barlow; C. Barschel; S. Barsuk; W. Barter; A. Bates; C. Bauer; Th. Bauer; A. Bay; J. Beddow; I. Bediaga; S. Belogurov; K. Belous; I. Belyaev; E. Ben-Haim; M. Benayoun; G. Bencivenni; S. Benson; J. Benton; R. Bernet; M. -O. Bettler; M. van Beuzekom; A. Bien; S. Bifani; T. Bird; A. Bizzeti; P. M. Bjørnstad; T. Blake; F. Blanc; C. Blanks; J. Blouw; S. Blusk; A. Bobrov; V. Bocci; A. Bondar; N. Bondar; W. Bonivento; S. Borghi; A. Borgia; T. J. V. Bowcock; C. Bozzi; T. Brambach; J. van den Brand; J. Bressieux; D. Brett; M. Britsch; T. Britton; N. H. Brook; H. Brown; A. Büchler-Germann; I. Burducea; A. Bursche; J. Buytaert; S. Cadeddu; O. Callot; M. Calvi; M. Calvo Gomez; A. Camboni; P. Campana; A. Carbone; G. Carboni; R. Cardinale; A. Cardini; L. Carson; K. Carvalho Akiba; G. Casse; M. Cattaneo; Ch. Cauet; M. Charles; Ph. Charpentier; N. Chiapolini; M. Chrzaszcz; K. Ciba; X. Cid Vidal; G. Ciezarek; P. E. L. Clarke; M. Clemencic; H. V. Cliff; J. Closier; C. Coca; V. Coco; J. Cogan; E. Cogneras; P. Collins; A. Comerma-Montells; A. Contu; A. Cook; M. Coombes; G. Corti; B. Couturier; G. A. Cowan; R. Currie; C. D'Ambrosio; P. David; P. N. Y. David; I. De Bonis; K. De Bruyn; S. De Capua; M. De Cian; J. M. De Miranda; L. De Paula; P. De Simone; D. Decamp; M. Deckenhoff; H. Degaudenzi; L. Del Buono; C. Deplano; D. Derkach; O. Deschamps; F. Dettori; J. Dickens; H. Dijkstra; P. Diniz Batista; F. Domingo Bonal; S. Donleavy; F. Dordei; P. Dornan; A. Dosil Suárez; D. Dossett; A. Dovbnya; F. Dupertuis; R. Dzhelyadin; A. Dziurda; A. Dzyuba; S. Easo; U. Egede; V. Egorychev; S. Eidelman; D. van Eijk; F. Eisele; S. Eisenhardt; R. Ekelhof; L. Eklund; Ch. Elsasser; D. Elsby; D. Esperante Pereira; A. Falabella; C. Färber; G. Fardell; C. Farinelli; S. Farry; V. Fave; V. Fernandez Albor; M. Ferro-Luzzi; S. Filippov; C. Fitzpatrick; M. Fontana; F. Fontanelli; R. Forty; O. Francisco; M. Frank; C. Frei; M. Frosini; S. Furcas; A. Gallas Torreira; D. Galli; M. Gandelman; P. Gandini; Y. Gao; J-C. Garnier; J. Garofoli; J. Garra Tico; L. Garrido; D. Gascon; C. Gaspar; R. Gauld; N. Gauvin; M. Gersabeck; T. Gershon; Ph. Ghez; V. Gibson; V. V. Gligorov; C. Göbel; D. Golubkov; A. Golutvin; A. Gomes; H. Gordon; M. Grabalosa Gándara; R. Graciani Diaz; L. A. Granado Cardoso; E. Graugés; G. Graziani; A. Grecu; E. Greening; S. Gregson; O. Grünberg; B. Gui; E. Gushchin; Yu. Guz; T. Gys; C. Hadjivasiliou; G. Haefeli; C. Haen; S. C. Haines; T. Hampson; S. Hansmann-Menzemer; N. Harnew; J. Harrison; P. F. Harrison; T. Hartmann; J. He; V. Heijne; K. Hennessy; P. Henrard; J. A. Hernando Morata; E. van Herwijnen; E. Hicks; K. Holubyev; P. Hopchev; W. Hulsbergen; P. Hunt; T. Huse; R. S. Huston; D. Hutchcroft; D. Hynds; V. Iakovenko; P. Ilten; J. Imong; R. Jacobsson; A. Jaeger; M. Jahjah Hussein; E. Jans; F. Jansen; P. Jaton; B. Jean-Marie; F. Jing; M. John; D. Johnson; C. R. Jones; B. Jost; M. Kaballo; S. Kandybei; M. Karacson; T. M. Karbach; J. Keaveney; I. R. Kenyon; U. Kerzel; T. Ketel; A. Keune; B. Khanji; Y. M. Kim; M. Knecht; I. Komarov; R. F. Koopman; P. Koppenburg; M. Korolev; A. Kozlinskiy; L. Kravchuk; K. Kreplin; M. Kreps; G. Krocker; P. Krokovny; F. Kruse; K. Kruzelecki; M. Kucharczyk; V. Kudryavtsev; T. Kvaratskheliya; V. N. La Thi; D. Lacarrere; G. Lafferty; A. Lai; D. Lambert; R. W. Lambert; E. Lanciotti; G. Lanfranchi; C. Langenbruch; T. Latham; C. Lazzeroni; R. Le Gac; J. van Leerdam; J. -P. Lees; R. Lefévre; A. Leflat; J. Lefrançois; O. Leroy; T. Lesiak; L. Li; Y. Li; L. Li Gioi; M. Lieng; M. Liles; R. Lindner; C. Linn; B. Liu; G. Liu; J. von Loeben; J. H. Lopes; E. Lopez Asamar; N. Lopez-March; H. Lu; J. Luisier; A. Mac Raighne; F. Machefert; I. V. Machikhiliyan; F. Maciuc; O. Maev; J. Magnin; S. Malde; R. M. D. Mamunur; G. Manca; G. Mancinelli; N. Mangiafave; U. Marconi; R. Märki; J. Marks; G. Martellotti; A. Martens; L. Martin; A. Martín Sánchez; M. Martinelli; D. Martinez Santos; A. Massafferri; Z. Mathe; C. Matteuzzi; M. Matveev; E. Maurice; B. Maynard; A. Mazurov; G. McGregor; R. McNulty; M. Meissner; M. Merk; J. Merkel; S. Miglioranzi; D. A. Milanes; M. -N. Minard; J. Molina Rodriguez; S. Monteil; D. Moran; P. Morawski; R. Mountain; I. Mous; F. Muheim; K. Müller; R. Muresan; B. Muryn; B. Muster; J. Mylroie-Smith; P. Naik; T. Nakada; R. Nandakumar; I. Nasteva; M. Needham; N. Neufeld; A. D. Nguyen; C. Nguyen-Mau; M. Nicol; V. Niess; N. Nikitin; T. Nikodem; A. Nomerotski

2012-04-26T23:59:59.000Z

5

SUMMON@MU---Intro Video MU Libraries 1  

E-Print Network [OSTI]

SUMMON@MU---Intro Video MU Libraries 1 This is a brief introduction to Summon@MU, the newest way options are also available. #12;SUMMON@MU---Intro Video MU Libraries 2 After running a search... you can... #12;SUMMON@MU---Intro Video MU Libraries 3 And you can also limit your items to those with full text

Taylor, Jerry

6

Mixed-mu superconducting bearings  

DOE Patents [OSTI]

A mixed-mu superconducting bearing including a ferrite structure disposed for rotation adjacent a stationary superconductor material structure and a stationary permanent magnet structure. The ferrite structure is levitated by said stationary permanent magnet structure.

Hull, John R. (Hinsdale, IL); Mulcahy, Thomas M. (Western Springs, IL)

1998-01-01T23:59:59.000Z

7

Mixed-mu superconducting bearings  

DOE Patents [OSTI]

A mixed-mu superconducting bearing is disclosed including a ferrite structure disposed for rotation adjacent a stationary superconductor material structure and a stationary permanent magnet structure. The ferrite structure is levitated by said stationary permanent magnet structure. 9 figs.

Hull, J.R.; Mulcahy, T.M.

1998-03-03T23:59:59.000Z

8

Producing [mu][sup [minus  

SciTech Connect (OSTI)

After the feasibility of vacuum isolated [mu][sup -]d production was demonstrated at TRIUMF in 1989, development was begun on a target system that would take advantage of the process to aid in the understanding of the muon catalyzed fusion cycle. Minimal neutron backgrounds, the ability to use silicon detectors, and compatibility with tritium were considered important for a very versatile target system. the advantages which the target gives isolating [mu]CF process will be outlined.

Knowles, P.E.; Beer, G.A.; Mason, G.R.; Olin, A. (Victoria Univ., BC (Canada)); Bailey, J.M. (Liverpool Univ. (United Kingdom)); Beveridge, J.L.; Marshall, G.M.; Brewer, J.H.; Forster, B.M. (British Columbia Univ., Vancouver, BC (Canada)); Huber, T.M. (Gustavus Adolphus Coll., St. Peter, MN (United States)); Jacot-Guillarmod, R.; Schellenberg, L. (Fribourg Univ. (Switzerland). Inst. de Physique); Kammel,

1992-01-01T23:59:59.000Z

9

4.5 A Carnot cycle uses 1.00 mol of a monatomic perfect gas as the working substance from an initial state of 10.0 atm and 600 K. It expands isothermally to a pressure of 1.00 atm (step 1),  

E-Print Network [OSTI]

, write +, -, or ? as appropriate. 4.15 Suppose that an internal combustion engine runs on octane, for which the enthalpy of combustion is -5512 kJ mol-1 , and take the mass of 1 gallon of fuel as 3 kg. What.00 gallon of fuel given that the engine cylinder temperature is 2000°C and the exit temperature is 800°C? 4

Findley, Gary L.

10

Search for $B_s \\to \\mu^+\\mu^-$ and $B_d \\to \\mu^+\\mu^-$ Decays with CDF II  

SciTech Connect (OSTI)

A search has been performed for B{sub s}{sup 0} {yields} {mu}{sup +}{mu}{sup -} and B{sup 0} {yields} {mu}{sup +}{mu}{sup -} decays using 7 fb{sup -1} of integrated luminosity collected by the CDF II detector at the Fermilab Tevatron collider. The observed number of B{sup 0} candidates is consistent with background-only expectations and yields an upper limit on the branching fraction of {Beta}(B{sup 0} {yields} {mu}{sup +}{mu}{sup -}) < 6.0 x 10{sup -9} at 95% confidence level. We observe an excess of B{sub s}{sup 0} candidates. The probability that the background processes alone could produce such an excess or larger is 0.27%. The probability that the combination of background and the expected standard model rate of B{sub s}{sup 0} {yields} {mu}{sup +}{mu}{sup -} could produce such an excess or larger is 1.9%. These data are used to determine {Beta}(B{sub s}{sup 0} {yields} {mu}{sup +}{mu}{sup -}) = (1.8{sub -0.9}{sup +1.1}) x 10{sup -8} and provide an upper limit of {Beta}(B{sub s}{sup 0} {yields} {mu}{sup +}{mu}{sup -}) < 4.0 x 10{sup -8} at 95% confidence level.

Aaltonen, T.; /Helsinki Inst. of Phys.; Alvarez Gonzalez, B.; /Oviedo U. /Cantabria Inst. of Phys.; Amerio, S.; /INFN, Padua; Amidei, D.; /Michigan U.; Anastassov, A.; /Northwestern U.; Annovi, A.; /Frascati; Antos, J.; /Comenius U.; Apollinari, G.; /Fermilab; Appel, J.A.; /Fermilab; Apresyan, A.; /Purdue U.; Arisawa, T.; /Waseda U. /Dubna, JINR

2011-07-01T23:59:59.000Z

11

Noether theorem for mu-symmetries  

E-Print Network [OSTI]

We give a version of Noether theorem adapted to the framework of mu-symmetries; this extends to such case recent work by Muriel, Romero and Olver in the framework of lambda-symmetries, and connects mu-symmetries of a Lagrangian to a suitably modified conservation law. In some cases this "mu-conservation law'' actually reduces to a standard one; we also note a relation between mu-symmetries and conditional invariants. We also consider the case where the variational principle is itself formulated as requiring vanishing variation under mu-prolonged variation fields, leading to modified Euler-Lagrange equations. In this setting mu-symmetries of the Lagrangian correspond to standard conservation laws as in the standard Noether theorem. We finally propose some applications and examples.

G. Cicogna; G. Gaeta

2007-08-23T23:59:59.000Z

12

Updated Search for $B_s \\to \\mu^+$ mu- at CDF  

SciTech Connect (OSTI)

The decay B{sub s}{sup 0} {yields} {mu}{sup +}{mu}{sup -} is very sensitive to contributions from new physics processes. Thus the Tevatron and LHC experiments are hunting for an observation of a B{sub s}{sup 0} {yields} {mu}{sup +}{mu}{sup -} signal. In this article the updated search for B{sub s}{sup 0} {yields} {mu}{sup +}{mu}{sup -} and B{sup 0} {yields} {mu}{sup +}{mu}{sup -} by the CDF experiment is presented. The CDF result was received with great interest because an excess over the background expectation is seen, although of modest statistical significance and still consistent with the prediction of a standard model signal and other experimental results.

Kuhr, Thomas; /Karlsruhe, Inst. Technol. /Karlsruhe U., EKP

2011-11-01T23:59:59.000Z

13

Behavioural Ecology Field Course Mols Laboratories, Denmark 2007  

E-Print Network [OSTI]

1 REPORTS Behavioural Ecology Field Course Mols Laboratories, Denmark 2007 Teachers: Dr. Trine ................................................................................................................................... 64 Receptor based feeding preferences; An investigation of the taste perception of three classes ............................................................................................................................ 79 Taste perception in the wood ant, Formica rufa Jeppe Jensen

Hamburg,.Universität

14

Search for NMSSM Higgs bosons in the h ---> aa ---> mu mu mu mu, mu mu tau tau channels using p anti-p collisions at s**(1/2) = 1.96-TeV  

SciTech Connect (OSTI)

We report on a first search for production of the lightest neutral CP-even Higgs boson (h) in the next-to-minimal supersymmetric standard model, where h decays to a pair of neutral pseudoscalar Higgs bosons (a), using 4.2 fb{sup -1} of data recorded with the D0 detector at Fermilab. The a bosons are required to either both decay to {mu}{sup +}{mu}{sup -} or one to {mu}{sup +}{mu}{sup -} and the other to {tau}{sup +}{tau}{sup -}. No significant signal is observed, and we set limits on its production as functions of M{sub a} and M{sub h}.

Abazov, V.M.; /Dubna, JINR; Abbott, B.; /Oklahoma U.; Abolins, M.; /Michigan State U.; Acharya, B.S.; /Tata Inst.; Adams, M.; /Illinois U., Chicago; Adams, T.; /Florida State U.; Aguilo, E.; /Alberta U. /Simon Fraser U. /York U., Canada /McGill U.; Ahsan, M.; /Kansas State U.; Alexeev, G.D.; /Dubna, JINR; Alkhazov, Georgiy D.; /St. Petersburg, INP; Alton, Andrew K.; /Michigan U. /Northeastern U.

2009-05-01T23:59:59.000Z

15

Mu2e Technical Design Report  

E-Print Network [OSTI]

The Mu2e experiment at Fermilab will search for charged lepton flavor violation via the coherent conversion process mu- N --> e- N with a sensitivity approximately four orders of magnitude better than the current world's best limits for this process. The experiment's sensitivity offers discovery potential over a wide array of new physics models and probes mass scales well beyond the reach of the LHC. We describe herein the preliminary design of the proposed Mu2e experiment. This document was created in partial fulfillment of the requirements necessary to obtain DOE CD-2 approval.

Bartoszek, L; Miller, J P; Mott, J; Palladino, A; Quirk, J; Roberts, B L; Crnkovic, J; Polychronakos, V; Tishchenko, V; Yamin, P; Cheng, C -h; Echenard, B; Flood, K; Hitlin, D G; Kim, J H; Miyashita, T S; Porter, F C; Röhrken, M; Trevor, J; Zhu, R -Y; Heckmaier, E; Kang, T I; Lim, G; Molzon, W; You, Z; Artikov, A M; Budagov, J A; Davydov, Yu I; Glagolev, V V; Simonenko, A V; Usubov, Z U; Oh, S H; Wang, C; Ambrosio, G; Andreev, N; Arnold, D; Ball, M; Bernstein, R H; Bianchi, A; Biery, K; Bossert, R; Bowden, M; Brandt, J; Brown, G; Brown, H; Buehler, M; Campbell, M; Cheban, S; Chen, M; Coghill, J; Coleman, R; Crowley, C; Deshpande, A; Deuerling, G; Dey, J; Dhanaraj, N; Dinnon, M; Dixon, S; Drendel, B; Eddy, N; Evans, R; Evbota, D; Fagan, J; Feher, S; Fellenz, B; Friedsam, H; Gallo, G; Gaponenko, A; Gardner, M; Gaugel, S; Genser, K; Ginther, G; Glass, H; Glenzinski, D; Hahn, D; Hansen, S; Hartsell, B; Hays, S; Hocker, J A; Huedem, E; Huffman, D; Ibrahim, A; Johnstone, C; Kashikhin, V; Kashikhin, V V; Kasper, P; Kiper, T; Knapp, D; Knoepfel, K; Kokoska, L; Kozlovsky, M; Krafczyk, G; Kramp, M; Krave, S; Krempetz, K; Kutschke, R K; Kwarciany, R; Lackowski, T; Lamm, M J; Larwill, M; Leavell, F; Leeb, D; Leveling, A; Lincoln, D; Logashenko, V; Lombardo, V; Lopes, M L; Makulski, A; Martinez, A; McArthur, D; McConologue, F; Michelotti, L; Mokhov, N; Morgan, J; Mukherjee, A; Murat, P; Nagaslaev, V; Neuffer, D V; Nicol, T; Niehoff, J; Nogiec, J; Olson, M; Orris, D; Ostojic, R; Page, T; Park, C; Peterson, T; Pilipenko, R; Pla-Dalmau, A; Poloubotko, V; Popovic, M; Prebys, E; Prieto, P; Pronskikh, V; Pushka, D; Rabehl, R; Ray, R E; Rechenmacher, R; Rivera, R; Robotham, W; Rubinov, P; Rusu, V L; Scarpine, V; Schappert, W; Schoo, D; Stefanik, A; Still, D; Tang, Z; Tanovic, N; Tartaglia, M; Tassotto, G; Tinsley, D; Tschirhart, R S; Vogel, G; Wagner, R; Wands, R; Wang, M; Werkema, S; White, H B; Whitmore, J; Wielgos, R; Woods, R; Worel, C; Zifko, R; Ciambrone, P; Colao, F; Cordelli, M; Corradi, G; Dane, E; Giovannella, S; Happacher, F; Luca, A; Miscetti, S; Ponzio, B; Pileggi, G; Saputi, A; Sarra, I; Soleti, R S; Stomaci, V; Martini, M; Fabbricatore, P; Farinon, S; Musenich, R; Alexander, D; Daniel, A; Empl, A; Hungerford, E V; Lau, K; Gollin, G D; Huang, C; Roderick, D; Trundy, B; Brown, D Na; Ding, D; Kolomensky, Yu G; Lee, M J; Cascella, M; Grancagnolo, F; Ignatov, F; Innocente, A; L'Erario, A; Miccoli, A; Maffezzoli, A; Mazzotta, P; Onorato, G; Piacentino, G M; Rella, S; Rossetti, F; Spedicato, M; Tassielli, G; Taurino, A; Zavarise, G; Hooper, R; Brown, D No; Djilkibaev, R; Matushko, V; Ankenbrandt, C; Boi, S; Dychkant, A; Hedin, D; Hodge, Z; Khalatian, V; Majewski, R; Martin, L; Okafor, U; Pohlman, N; Riddel, R S; Shellito, A; de Gouvea, A L; Cervelli, F; Carosi, R; Di Falco, S; Donati, S; Lomtadze, T; Pezzullo, G; Ristori, L; Spinella, F; Jones, M; Corcoran, M D; Orduna, J; Rivera, D; Bennett, R; Caretta, O; Davenne, T; Densham, C; Loveridge, P; Odell, J; Bomgardner, R; Dukes, E C; Ehrlich, R; Frank, M; Goadhouse, S; Ho, E; Ma, H; Oksuzian, Y; Purvis, J; Wu, Y; Hertzog, D W; Kammel, P; Lynch, K R; Popp, J L

2015-01-01T23:59:59.000Z

16

Mu2e Technical Design Report  

E-Print Network [OSTI]

The Mu2e experiment at Fermilab will search for charged lepton flavor violation via the coherent conversion process mu- N --> e- N with a sensitivity approximately four orders of magnitude better than the current world's best limits for this process. The experiment's sensitivity offers discovery potential over a wide array of new physics models and probes mass scales well beyond the reach of the LHC. We describe herein the preliminary design of the proposed Mu2e experiment. This document was created in partial fulfillment of the requirements necessary to obtain DOE CD-2 approval.

L. Bartoszek; E. Barnes; J. P. Miller; J. Mott; A. Palladino; J. Quirk; B. L. Roberts; J. Crnkovic; V. Polychronakos; V. Tishchenko; P. Yamin; C. -h. Cheng; B. Echenard; K. Flood; D. G. Hitlin; J. H. Kim; T. S. Miyashita; F. C. Porter; M. Röhrken; J. Trevor; R. -Y. Zhu; E. Heckmaier; T. I. Kang; G. Lim; W. Molzon; Z. You; A. M. Artikov; J. A. Budagov; Yu. I. Davydov; V. V. Glagolev; A. V. Simonenko; Z. U. Usubov; S. H. Oh; C. Wang; G. Ambrosio; N. Andreev; D. Arnold; M. Ball; R. H. Bernstein; A. Bianchi; K. Biery; R. Bossert; M. Bowden; J. Brandt; G. Brown; H. Brown; M. Buehler; M. Campbell; S. Cheban; M. Chen; J. Coghill; R. Coleman; C. Crowley; A. Deshpande; G. Deuerling; J. Dey; N. Dhanaraj; M. Dinnon; S. Dixon; B. Drendel; N. Eddy; R. Evans; D. Evbota; J. Fagan; S. Feher; B. Fellenz; H. Friedsam; G. Gallo; A. Gaponenko; M. Gardner; S. Gaugel; K. Genser; G. Ginther; H. Glass; D. Glenzinski; D. Hahn; S. Hansen; B. Hartsell; S. Hays; J. A. Hocker; E. Huedem; D. Huffman; A. Ibrahim; C. Johnstone; V. Kashikhin; V. V. Kashikhin; P. Kasper; T. Kiper; D. Knapp; K. Knoepfel; L. Kokoska; M. Kozlovsky; G. Krafczyk; M. Kramp; S. Krave; K. Krempetz; R. K. Kutschke; R. Kwarciany; T. Lackowski; M. J. Lamm; M. Larwill; F. Leavell; D. Leeb; A. Leveling; D. Lincoln; V. Logashenko; V. Lombardo; M. L. Lopes; A. Makulski; A. Martinez; D. McArthur; F. McConologue; L. Michelotti; N. Mokhov; J. Morgan; A. Mukherjee; P. Murat; V. Nagaslaev; D. V. Neuffer; T. Nicol; J. Niehoff; J. Nogiec; M. Olson; D. Orris; R. Ostojic; T. Page; C. Park; T. Peterson; R. Pilipenko; A. Pla-Dalmau; V. Poloubotko; M. Popovic; E. Prebys; P. Prieto; V. Pronskikh; D. Pushka; R. Rabehl; R. E. Ray; R. Rechenmacher; R. Rivera; W. Robotham; P. Rubinov; V. L. Rusu; V. Scarpine; W. Schappert; D. Schoo; A. Stefanik; D. Still; Z. Tang; N. Tanovic; M. Tartaglia; G. Tassotto; D. Tinsley; R. S. Tschirhart; G. Vogel; R. Wagner; R. Wands; M. Wang; S. Werkema; H. B. White Jr.; J. Whitmore; R. Wielgos; R. Woods; C. Worel; R. Zifko; P. Ciambrone; F. Colao; M. Cordelli; G. Corradi; E. Dane; S. Giovannella; F. Happacher; A. Luca; S. Miscetti; B. Ponzio; G. Pileggi; A. Saputi; I. Sarra; R. S. Soleti; V. Stomaci; M. Martini; P. Fabbricatore; S. Farinon; R. Musenich; D. Alexander; A. Daniel; A. Empl; E. V. Hungerford; K. Lau; G. D. Gollin; C. Huang; D. Roderick; B. Trundy; D. Na. Brown; D. Ding; Yu. G. Kolomensky; M. J. Lee; M. Cascella; F. Grancagnolo; F. Ignatov; A. Innocente; A. L'Erario; A. Miccoli; A. Maffezzoli; P. Mazzotta; G. Onorato; G. M. Piacentino; S. Rella; F. Rossetti; M. Spedicato; G. Tassielli; A. Taurino; G. Zavarise; R. Hooper; D. No. Brown; R. Djilkibaev; V. Matushko; C. Ankenbrandt; S. Boi; A. Dychkant; D. Hedin; Z. Hodge; V. Khalatian; R. Majewski; L. Martin; U. Okafor; N. Pohlman; R. S. Riddel; A. Shellito; A. L. de Gouvea; F. Cervelli; R. Carosi; S. Di Falco; S. Donati; T. Lomtadze; G. Pezzullo; L. Ristori; F. Spinella; M. Jones; M. D. Corcoran; J. Orduna; D. Rivera; R. Bennett; O. Caretta; T. Davenne; C. Densham; P. Loveridge; J. Odell; R. Bomgardner; E. C. Dukes; R. Ehrlich; M. Frank; S. Goadhouse; R. Group; E. Ho; H. Ma; Y. Oksuzian; J. Purvis; Y. Wu; D. W. Hertzog; P. Kammel; K. R. Lynch; J. L. Popp

2015-01-21T23:59:59.000Z

17

CLIMATE STUDY Phase II: MU Student Services Providers Survey  

E-Print Network [OSTI]

MU CAMPUS CLIMATE STUDY VOLUME 2 Phase II: MU Student Services Providers Survey Phase III: MU CAMPUS CLIMATE STUDY: PHASES II ­ IV Over the past three years, members of the University of Missouri-Columbia (MU) have participated in the MU Campus Climate Study for Underrepresented Groups conducted by a team

Taylor, Jerry

18

MU PURCHASING CARD CARDHOLDER ENROLLMENT / CHANGE FORM  

E-Print Network [OSTI]

MU PURCHASING CARD CARDHOLDER ENROLLMENT / CHANGE FORM Action: ( ) Initial Enrollment ( ) Change/WBS/Internal Order # _________________________________________ Office Phone transaction limit Any increase in limits and type of charge (MCC Code) must be approved by the Purchasing

Hardy, Christopher R.

19

Search for Doubly-charged Higgs Boson Production in the Decay H++ H-- ---> mu+ mu+ mu- mu- with 1.1 fb**(-1) at D0 Detector  

SciTech Connect (OSTI)

This work presents a search for the pair production of doubly-charged Higgs bosons in the process p{bar p} {yields} H{sup ++}H{sup --} {yields} {mu}{sup +}{mu}{sup +}{mu}{sup -}{mu}{sup -} using the data corresponding to an integrated luminosity of about 1.1 fb{sup -1}. This is the complete dataset of RunIIa taken from April 19, 2002 to February 22, 2006 by the D0 experiment at the Fermilab Tevatron Collider. In the absence of significant excess above standard model background, 95% confidence level mass limits of M(H{sub L}{sup {+-}{+-}}) > 150 GeV and M(H{sub R}{sup {+-}{+-}}) > 126.5 GeV are set for left-handed and right-handed doubly-charged Higgs bosons respectively assuming a 100% branching ratio into muons.

Kim, Tae Jeong; /Korea U.

2007-06-01T23:59:59.000Z

20

FAPRI-MU Biofuel Baseline FAPRI-MU Report #02-13  

E-Print Network [OSTI]

FAPRI-MU Biofuel Baseline March 2013 FAPRI-MU Report #02-13 Providing objective analysis for more of Education, Office of Civil Rights. #12;1 Executive Summary This report takes a closer look at the biofuels portion of the U.S. Agricultural and Biofuels Baseline released by the Food and Agricultural Policy

Noble, James S.

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


21

The next generation of $\\mu\\ -> e \\gamma$ and $\\mu\\ -> 3e$ CLFV search experiments  

E-Print Network [OSTI]

We explore the possibilities for extending the sensitivity of current searches for the charged lepton flavor violating decays $\\mu\\ -> e \\gamma$ and $\\mu\\ -> eee$. A future facility such as Project X at Fermilab could provide a much more intense stopping $\\mu^+$ beam, facilitating more sensitive searches, but improved detectors will be required as well. Current searches are limited by accidental and physics backgrounds, as well as by the total number of stopped muons. One of the limiting factors in current detectors for $\\mu\\ -> e \\gamma$ searches is the photon energy resolution of the calorimeter. We present a new fast Monte Carlo simulation of a conceptual design of a new experimental concept that detects converted $e^+e^-$ pairs from signal photons, taking advantage of the improved energy resolution of a pair spectrometer based on a silicon charged particle tracker. We also study a related detector design for a next generation $\\mu\\to eee$ search experiment.

Cheng, Chih-hsiang; Hitlin, David G

2013-01-01T23:59:59.000Z

22

Higgs boson decay to mu mubar gamma  

E-Print Network [OSTI]

The Higgs boson decay, H -> mu mubar gamma, is studied in the Standard Model at the tree and one-loop levels. It is shown that for Higgs boson masses above 110 GeV, the contribution to the radiative width from the one-loop level exceeds the contribution from the tree level, and for Higgs boson masses above 140 GeV, it even exceeds the contribution from the tree level decay H -> mu mubar. We also show that the contributions to the radiative decay width from the interference terms between the tree and one-loop diagrams are negligible.

Ali Abbasabadi; Wayne W. Repko

2000-04-17T23:59:59.000Z

23

Producing {mu}{sup {minus}}d and {mu}{sup {minus}}t in vacuum  

SciTech Connect (OSTI)

After the feasibility of vacuum isolated {mu}{sup -}d production was demonstrated at TRIUMF in 1989, development was begun on a target system that would take advantage of the process to aid in the understanding of the muon catalyzed fusion cycle. Minimal neutron backgrounds, the ability to use silicon detectors, and compatibility with tritium were considered important for a very versatile target system. the advantages which the target gives isolating {mu}CF process will be outlined.

Knowles, P.E.; Beer, G.A.; Mason, G.R.; Olin, A. [Victoria Univ., BC (Canada); Bailey, J.M. [Liverpool Univ. (United Kingdom); Beveridge, J.L.; Marshall, G.M.; Brewer, J.H.; Forster, B.M. [British Columbia Univ., Vancouver, BC (Canada); Huber, T.M. [Gustavus Adolphus Coll., St. Peter, MN (United States); Jacot-Guillarmod, R.; Schellenberg, L. [Fribourg Univ. (Switzerland). Inst. de Physique; Kammel, P.; Zmeskal, J. [Oesterreichische Akademie der Wissenschaften, Vienna (Austria). Inst. fuer Mittelenergiephysik; Kunselman, A.R. [Wyoming Univ., Laramie, WY (United States); Martoff, C.J. [Temple Univ., Philadelphia, PA (United States); Petitjean, C. [Paul Scherrer Inst. (PSI), Villigen (Switzerland)

1992-12-31T23:59:59.000Z

24

Diffractive Z/gamma* --> mu+mu- boson production in proton - antiproton collisions  

SciTech Connect (OSTI)

Measurements of the inclusive diffractive Z {yields} {mu}{sup +}{mu}{sup -} cross section with gap requirement for M{sub {mu}}{sub {mu}} > 40 GeV at {radical} s = 1.96 TeV and fraction of Z bosons produced diffractively with gap requirement from Z inclusive production are presented. The measurements are performed using a data sample corresponding to an integrated luminosity of 820 pb{sup -1}, collected with the D0 detector at the Tevatron, between 2002 to 2005. A total of 39945 di-muons events are selected and final results of: {sigma}{sub Diff}{sup gap} x Br(Z/{gamma}* {yields} {mu}{sup +}{mu}{sup -}) = 4.09 {+-} 0.64(stat.) {+-} 0.88(syst.) {+-} 0.27(lumi.) pb and, R{sub Diff}{sup gap} = 1.92 {+-} 0.30(stat.) {+-} 0.41(syst.) {+-} 0.12(lumi) % are obtained. In addition, d{sigma}/d{zeta} and d{sigma}/dy distributions are presented and they are compared with diffractive montecarlo (POMWIG). A reasonable agreement is obtained in this comparation. Finally, comparison of fraction of Z bosons produced diffractively with gap requirement (gap fraction) as measured with D0 during Run I of the Tevatron is compared. A good agreement is found for gap fraction results.

Mendoza Navas, Luis Miguel; /Andes U., Bogota

2007-07-01T23:59:59.000Z

25

Optimal MU-MIMO precoder with MISO decomposition approach  

E-Print Network [OSTI]

Optimal MU-MIMO precoder with MISO decomposition approach Mustapha Amara, Yi Yuan-Wu Orange Labs considered the best existing precoder design algorithm for a MISO multiuser sys- tem proposed in [1 procedure transforming the MU-MIMO channel for each iteration into a MU-MISO channel trough virtual channel

Gesbert, David

26

FAINT SUBMILLIMETER GALAXY COUNTS AT 450 {mu}m  

SciTech Connect (OSTI)

We present the results of SCUBA-2 observations at 450 {mu}m and 850 {mu}m of the field lensed by the massive cluster A370. With a total survey area >100 arcmin{sup 2} and 1{sigma} sensitivities of 3.92 and 0.82 mJy beam{sup -1} at 450 and 850 {mu}m, respectively, we find a secure sample of 20 sources at 450 {mu}m and 26 sources at 850 {mu}m with a signal-to-noise ratio (S/N) > 4. Using the latest lensing model of A370 and Monte Carlo simulations, we derive the number counts at both wavelengths. The 450 {mu}m number counts probe a factor of four deeper than the counts recently obtained from the Herschel Space Telescope at similar wavelengths, and we estimate that {approx}47%-61% of the 450 {mu}m extragalactic background light resolved into individual sources with 450 {mu}m fluxes greater than 4.5 mJy. The faint 450 {mu}m sources in the 4{sigma} sample have positional accuracies of 3 arcsec, while brighter sources (S/N >6{sigma}) are good to 1.4 arcsec. Using a deep radio map (1{sigma} {approx} 6 {mu}Jy) we find that the percentage of submillimeter sources having secure radio counterparts is 85% for 450 {mu}m sources with intrinsic fluxes >6 mJy and 67% for 850 {mu}m sources with intrinsic fluxes >4 mJy. We also find that 67% of the >4{sigma} 450 {mu}m sources are detected at 850 {mu}m, while the recovery rate at 450 {mu}m of >4{sigma} 850 {mu}m sources is 54%. Combined with the source redshifts estimated using millimetric flux ratios, the recovered rate is consistent with the scenario where both 450 {mu}m and 20 cm emission preferentially select lower redshift dusty sources, while 850 {mu}m emission traces a higher fraction of dusty sources at higher redshifts. We identify potential counterparts in various wavelengths from X-ray to mid-infrared and measure the multiwavelength photometry, which we then use to analyze the characteristics of the sources. We find three X-ray counterparts to our robust submillimeter sample (S/N > 5), giving an active galactic nucleus fraction for our 450 (850) {mu}m sample of 3/8 (3/9) or 38% (33%). We also find a correlation between the K{sub s} band and the 850 {mu}m/20 cm flux ratio.

Chen, Chian-Chou; Cowie, Lennox L.; Barger, Amy J.; Casey, Caitlin M.; Lee, Nicholas; Sanders, David B.; Williams, Jonathan P. [Institute for Astronomy, University of Hawaii, 2680 Woodlawn Drive, Honolulu, HI 96822 (United States)] [Institute for Astronomy, University of Hawaii, 2680 Woodlawn Drive, Honolulu, HI 96822 (United States); Wang, Wei-Hao [Academia Sinica Institute of Astronomy and Astrophysics, P.O. Box 23-141, Taipei 10617, Taiwan (China)] [Academia Sinica Institute of Astronomy and Astrophysics, P.O. Box 23-141, Taipei 10617, Taiwan (China)

2013-01-10T23:59:59.000Z

27

Search for the Decay Modes D0 to e+ e-, D0 to mu+ mu-, and D0 to e+/- mu+/-  

SciTech Connect (OSTI)

We present searches for the rare decay modes D{sup 0} {yields} e{sup +}e{sup -}, D{sup 0} {yields} {mu}{sup +}{mu}{sup -}, and D{sup 0} {yields} e{sup {+-}}{mu}{sup {-+}} in continuum e{sup +}e{sup -} {yields} c{bar c} events recorded by the BABAR detector in a data sample that corresponds to an integrated luminosity of 468 fb{sup -1}. These decays are highly GIM suppressed but may be enhanced in several extensions of the Standard Model. Our observed event yields are consistent with the expected backgrounds. An excess is seen in the D{sup 0} {yields} {mu}{sup +}{mu}{sup -} channel, although the observed yield is consistent with an upward background fluctuation at the 5% level. Using the Feldman-Cousins method, we set the following 90% confidence level intervals on the branching fractions: {Beta}(D{sup 0} {yields} e{sup +}e{sup -}) < 1.7 x 10{sup -7}, {Beta}(D{sup 0} {yields} {mu}{sup +}{mu}{sup -}) within [0.6, 8.1] x 10{sup -7}, and {Beta}(D{sup 0} {yields} e{sup {+-}}{mu}{sup {-+}}) < 3.3 x 10{sup -7}.

Lees, J. P.

2012-08-03T23:59:59.000Z

28

Search for the rare decays B{sup +}{yields}{mu}{sup +}{mu}{sup -}K{sup +}, B{sup 0}{yields}{mu}{sup +}{mu}{sup -}K*(892){sup 0}, and B{sub s}{sup 0}{yields}{mu}{sup +}{mu}{sup -}{phi} at CDF  

SciTech Connect (OSTI)

We search for b{yields}s{mu}{sup +}{mu}{sup -} transitions in B meson (B{sup +}, B{sup 0}, or B{sub s}{sup 0}) decays with 924 pb{sup -1} of pp collisions at {radical}(s)=1.96 TeV collected with the CDF II detector at the Fermilab Tevatron. We find excesses with significances of 4.5, 2.9, and 2.4 standard deviations in the B{sup +}{yields}{mu}{sup +}{mu}{sup -}K{sup +}, B{sup 0}{yields}{mu}{sup +}{mu}{sup -}K*(892){sup 0}, and B{sub s}{sup 0}{yields}{mu}{sup +}{mu}{sup -}{phi} decay modes, respectively. Using B{yields}J/{psi}h (h=K{sup +}, K*(892){sup 0}, {phi}) decays as normalization channels, we report branching fractions for the previously observed B{sup +} and B{sup 0} decays, B(B{sup +}{yields}{mu}{sup +}{mu}{sup -}K{sup +})=(0.59{+-}0.15{+-}0.04)x10{sup -6}, and B(B{sup 0}{yields}{mu}{sup +}{mu}{sup -}K*(892){sup 0})=(0.81{+-}0.30{+-}0.10)x10{sup -6}, where the first uncertainty is statistical, and the second is systematic. We set an upper limit on the relative branching fraction B(B{sub s}{sup 0}{yields}{mu}{sup +}{mu}{sup -}{phi})/B(B{sub s}{sup 0}{yields}J/{psi}{phi})<2.6(2.3)x10{sup -3} at the 95(90)% confidence level, which is the most stringent to date.

Aaltonen, T.; Maki, T.; Mehtala, P.; Orava, R.; Osterberg, K.; Saarikko, H.; Remortel, N. van [Division of High Energy Physics, Department of Physics, University of Helsinki and Helsinki Institute of Physics, FIN-00014, Helsinki (Finland); Adelman, J.; Brubaker, E.; Fedorko, W. T.; Grosso-Pilcher, C.; Kim, Y. K.; Kwang, S.; Levy, S.; Paramonov, A. A.; Schmidt, M. A.; Shiraishi, S.; Shochet, M.; Wolfe, C.; Yang, U. K. [Enrico Fermi Institute, University of Chicago, Chicago, Illinois 60637 (United States)] (and others)

2009-01-01T23:59:59.000Z

29

Observation of the decay Xi0 ---> Sigma+ mu- anti-nu(mu)  

SciTech Connect (OSTI)

The {Xi}{sup 0} muon semi-leptonic decay has been observed for the first time with nine identified events using the KTeV beam line and detector at Fermilab. The decay is normalized to the {Xi}{sup 0} beta decay mode and yields a value for the ratio of decay rates {Lambda}({Xi}{sup 0} {yields} {Sigma}{sup +}{mu}{sup -}{bar {nu}}{sub {mu}})/{Lambda}({Xi}{sup 0} {yields} {Sigma}{sup +}e{sup -} {bar {nu}}{sub e}) of (1.8{sub -0.5}{sup +0.7}(stat.) {+-} 0.2(syst.)) x 10{sup -2} at the 68% confidence level. This is in agreement with the SU(3) flavor symmetric quark model.

Alavi-Harati, A.; Alexopoulos, T.; Arenton, M.; Barbosa, R.F.; Barker, A.R.; Barrio, M.; Bellantoni, L.; Bellavance, A.; Blucher, E.; Bock, G.J.; Bown, C.; Bright, S.; Cheu, E.; Coleman, R.; Corcoran, M.D.; Cox, B.; Erwin, A.R.; Escobar, C.O.; Ford, R.; Glazov, A.; Golossanov, A.; /Arizona U. /UCLA /UC, San Diego /Campinas State U. /Chicago U.,

2005-04-01T23:59:59.000Z

30

Broadband laser diode emitting at 1. 28. mu. m wavelength  

SciTech Connect (OSTI)

This letter presents a broadband laser diode (LD) emitting at the 1.28 ..mu..m wavelength fabricated by introducing an absorption region (300 ..mu..m long) into a conventional 600-..mu..m-long InGaAsP laser diode. The LD operates by the pulsed modulation of a high peak current whose repetition rate and duty cycle are respectively 200 kHz and 5%. The typical output power and the spectral width of the LD are 3.8 mW and 58 A, and the measured coherence length is 210 ..mu..m.

Takada, K.; Noda, J.

1985-10-15T23:59:59.000Z

31

A new expected upper limit on the rare decay B(s) ---> mu+ mu- with the D0 experiment  

SciTech Connect (OSTI)

We present a new expected upper limit of the rare decay branching ratio B{sub s} {yields} {mu}{sup +}{mu}{sup -} using about 5 fb{sup -1} of Run II data collected with the D0 detector at the Tevatron. When setting limits on the branching ratio, selected events are normalized to reconstructed B{sup {+-}} {yields} J/{Psi}K{sup {+-}} events in order to decrease the systematic uncertainty. The resulting expected upper limit is {Beta}(B{sub s} {yields} {mu}{sup +}{mu}{sup -}) = 4.3(5.3) x 10{sup -8} at the 90% (95%) C.L.

Ripp-Baudot, Isabelle; /Strasbourg, IPHC

2009-01-01T23:59:59.000Z

32

September 2010 FAPRI-MU US Biofuels, Corn Processing,  

E-Print Network [OSTI]

September 2010 FAPRI-MU US Biofuels, Corn Processing, Distillers Grains, Fats, Switchgrass-882-4256 or the US Department of Education, Office of Civil Rights. #12;1 Overview of FAPRI-MU Biofuels, Corn listed here represent US biofuel, corn processing, distillers grains, fats, switchgrass, and corn stover

Noble, James S.

33

Effect of multiple step excitation on the reactivation and x-ray intensities following the fusion d. mu. d, d. mu. t and p. mu. t  

SciTech Connect (OSTI)

Menshikov and Ponomarev recently studied analytically the effect of multistep excitation on the muon reactivation for d..mu..t fusion and got a rather large activation factor of 35%. As expected, this shows a large density effect on the reactivation factor. The numerical cascade calculation with the cross section for multistep excitation, used by them, indicates that the reactivation factor is 25%. Due to the large Auger transition rates in the high excited states, the density effect on the reactivation factor is not large. Muonic x-ray spectra of ..mu../sup 3/He from ..mu..-catalyzed pd and dd fissions, measured by H. bossy et al., are analyzed by the cascade model used for the muon reactivation calculation. The model calculation is in good agreement with the intensity ratios ..mu../sup 3/He(3-1)/..mu../sup 3/He(2-1) of 0.13 +- 0.02 and 0.03 +- 0.007 measured for dd and pd fusions, and the multistep excitation increases 5% of the x-ray ratio for dd fusion. 10 refs., 3 figs., 2 tabs.

Takahashi, H.

1986-01-01T23:59:59.000Z

34

Lepton flavor violating processes \\tau ->\\mu\\gamma$, $\\tau-> 3\\mu$ and $Z-> \\mu\\tau$ in the Supersymmetric economical 3-3-1 model  

E-Print Network [OSTI]

In this work, we study the charged lepton flavor violating (cLFV) decays $\\tau-> \\mu\\gamma$, $\\tau-> 3\\mu$ and $Z->\\mu\\tau$ in the framework of the Supersymmetric economical 3-3-1 model. Analytic formulas for branching ratios (BR) of these decays are presented. We assume that there exist lepton flavor violation (LFV) sources in both right- and left-handed slepton sectors. This leads to the strong enhancement of cLFV decay rates. We also show that the effects of the LFV source to the cLFV decay rates in the left-handed slepton sector are greater than those in the right- handed slepton sector. By numerical investigation, we show that the model under consideration contains the relative light mass spectrum of sleptons which satisfies the current experimental bounds on LFV processes in the limit of small $\\tan \\gamma$. The interplay between monopole and dipole operators also was studied.

Hue, L T; Long, H N

2013-01-01T23:59:59.000Z

35

446 | Mol. BioSyst., 2014, 10, 446--453 This journal is The Royal Society of Chemistry 2014 Cite this: Mol. BioSyst., 2014,  

E-Print Network [OSTI]

and serve as a powerful tool for genome engineering. Site-specific DNA cleavage can be made this: Mol. BioSyst., 2014, 10, 446 A single-chain TALEN architecture for genome engineering Ning Suna) nucleases (TALENs) have been widely used for genome editing or engineering in various organisms during

Zhao, Huimin

36

744 Mol. BioSyst., 2012, 8, 744752 This journal is c The Royal Society of Chemistry 2012 Cite this: Mol. BioSyst., 2012, 8, 744752  

E-Print Network [OSTI]

: Mol. BioSyst., 2012, 8, 744­752 Dissecting ensemble networks in ES cell populations reveals micro in pluripotency in eighty-three ES cells to create Gene Regulatory Networks (GRNs) at the single cell level. We is associated with a collection of active sub-networks, with differing degrees of connectivity between

Babu, M. Madan

37

The Mu2e Experiment at Fermilab: a Search for Charged Lepton Flavor Violation  

E-Print Network [OSTI]

The Mu2e Experiment at Fermilab: a Search for Charged Lepton Flavor of the Mu2e Collaboration. A new experiment, Mu2e, is being developed at Fermilab

38

Observation of the rare $B^0_s\\to\\mu^+\\mu^-$ decay from the combined analysis of CMS and LHCb data  

E-Print Network [OSTI]

A joint measurement is presented of the branching fractions $B^0_s\\to\\mu^+\\mu^-$ and $B^0\\to\\mu^+\\mu^-$ in proton-proton collisions at the LHC by the CMS and LHCb experiments. The data samples were collected in 2011 at a centre-of-mass energy of 7 TeV, and in 2012 at 8 TeV. The combined analysis produces the first observation of the $B^0_s\\to\\mu^+\\mu^-$ decay, with a statistical significance exceeding six standard deviations, and the best measurement of its branching fraction so far, and three standard deviation evidence for the $B^0\\to\\mu^+\\mu^-$ decay. The measurements are statistically compatible with SM predictions and impose stringent constraints on several theories beyond the SM.

Khachatryan, Vardan; Tumasyan, Armen; Adam, Wolfgang; Bergauer, Thomas; Dragicevic, Marko; Erö, Janos; Friedl, Markus; Fruehwirth, Rudolf; Ghete, Vasile Mihai; Hartl, Christian; Hörmann, Natascha; Hrubec, Josef; Jeitler, Manfred; Kiesenhofer, Wolfgang; Knünz, Valentin; Krammer, Manfred; Krätschmer, Ilse; Liko, Dietrich; Mikulec, Ivan; Rabady, Dinyar; Rahbaran, Babak; Rohringer, Herbert; Schöfbeck, Robert; Strauss, Josef; Treberer-Treberspurg, Wolfgang; Waltenberger, Wolfgang; Wulz, Claudia-Elisabeth; Mossolov, Vladimir; Shumeiko, Nikolai; Suarez Gonzalez, Juan; Alderweireldt, Sara; Bansal, Sunil; Cornelis, Tom; De Wolf, Eddi A; Janssen, Xavier; Knutsson, Albert; Lauwers, Jasper; Luyckx, Sten; Ochesanu, Silvia; Rougny, Romain; Van De Klundert, Merijn; Van Haevermaet, Hans; Van Mechelen, Pierre; Van Remortel, Nick; Van Spilbeeck, Alex; Blekman, Freya; Blyweert, Stijn; D'Hondt, Jorgen; Daci, Nadir; Heracleous, Natalie; Keaveney, James; Lowette, Steven; Maes, Michael; Olbrechts, Annik; Python, Quentin; Strom, Derek; Tavernier, Stefaan; Van Doninck, Walter; Van Mulders, Petra; Van Onsem, Gerrit Patrick; Villella, Ilaria; Caillol, Cécile; Clerbaux, Barbara; De Lentdecker, Gilles; Dobur, Didar; Favart, Laurent; Gay, Arnaud; Grebenyuk, Anastasia; Léonard, Alexandre; Mohammadi, Abdollah; Perniè, Luca; Randle-conde, Aidan; Reis, Thomas; Seva, Tomislav; Thomas, Laurent; Vander Velde, Catherine; Vanlaer, Pascal; Wang, Jian; Zenoni, Florian; Adler, Volker; Beernaert, Kelly; Benucci, Leonardo; Cimmino, Anna; Costantini, Silvia; Crucy, Shannon; Dildick, Sven; Fagot, Alexis; Garcia, Guillaume; Mccartin, Joseph; Ocampo Rios, Alberto Andres; Ryckbosch, Dirk; Salva Diblen, Sinem; Sigamani, Michael; Strobbe, Nadja; Thyssen, Filip; Tytgat, Michael; Yazgan, Efe; Zaganidis, Nicolas; Basegmez, Suzan; Beluffi, Camille; Bruno, Giacomo; Castello, Roberto; Caudron, Adrien; Ceard, Ludivine; Da Silveira, Gustavo Gil; Delaere, Christophe; Du Pree, Tristan; Favart, Denis; Forthomme, Laurent; Giammanco, Andrea; Hollar, Jonathan; Jafari, Abideh; Jez, Pavel; Komm, Matthias; Lemaitre, Vincent; Nuttens, Claude; Pagano, Davide; Perrini, Lucia; Pin, Arnaud; Piotrzkowski, Krzysztof; Popov, Andrey; Quertenmont, Loic; Selvaggi, Michele; Vidal Marono, Miguel; Vizan Garcia, Jesus Manuel; Beliy, Nikita; Caebergs, Thierry; Daubie, Evelyne; Hammad, Gregory Habib; Aldá Júnior, Walter Luiz; Alves, Gilvan; Brito, Lucas; Correa Martins Junior, Marcos; Dos Reis Martins, Thiago; Mora Herrera, Clemencia; Pol, Maria Elena; Rebello Teles, Patricia; Carvalho, Wagner; Chinellato, Jose; Custódio, Analu; Da Costa, Eliza Melo; De Jesus Damiao, Dilson; De Oliveira Martins, Carley; Fonseca De Souza, Sandro; Malbouisson, Helena; Matos Figueiredo, Diego; Mundim, Luiz; Nogima, Helio; Prado Da Silva, Wanda Lucia; Santaolalla, Javier; Santoro, Alberto; Sznajder, Andre; Tonelli Manganote, Edmilson José; Vilela Pereira, Antonio; Bernardes, Cesar Augusto; Dogra, Sunil; Tomei, Thiago; De Moraes Gregores, Eduardo; Mercadante, Pedro G; Novaes, Sergio F; Padula, Sandra; Aleksandrov, Aleksandar; Genchev, Vladimir; Hadjiiska, Roumyana; Iaydjiev, Plamen; Marinov, Andrey; Piperov, Stefan; Rodozov, Mircho; Sultanov, Georgi; Vutova, Mariana; Dimitrov, Anton; Glushkov, Ivan; Litov, Leander; Pavlov, Borislav; Petkov, Peicho; Bian, Jian-Guo; Chen, Guo-Ming; Chen, He-Sheng; Chen, Mingshui; Cheng, Tongguang; Du, Ran; Jiang, Chun-Hua; Plestina, Roko; Romeo, Francesco; Tao, Junquan; Wang, Zheng; Asawatangtrakuldee, Chayanit; Ban, Yong; Li, Qiang; Liu, Shuai; Mao, Yajun; Qian, Si-Jin; Wang, Dayong; Xu, Zijun; Zou, Wei; Avila, Carlos; Cabrera, Andrés; Chaparro Sierra, Luisa Fernanda; Florez, Carlos; Gomez, Juan Pablo; Gomez Moreno, Bernardo; Sanabria, Juan Carlos; Godinovic, Nikola; Lelas, Damir; Polic, Dunja; Puljak, Ivica; Antunovic, Zeljko; Kovac, Marko; Brigljevic, Vuko; Kadija, Kreso; Luetic, Jelena; Mekterovic, Darko; Sudic, Lucija; Attikis, Alexandros; Mavromanolakis, Georgios; Mousa, Jehad; Nicolaou, Charalambos; Ptochos, Fotios; Razis, Panos A; Bodlak, Martin; Finger, Miroslav; Finger Jr, Michael; Assran, Yasser; Ellithi Kamel, Ali; Mahmoud, Mohammed; Radi, Amr; Kadastik, Mario; Murumaa, Marion; Raidal, Martti; Tiko, Andres; Eerola, Paula; Fedi, Giacomo; Voutilainen, Mikko; Härkönen, Jaakko; Karimäki, Veikko; Kinnunen, Ritva; Kortelainen, Matti J; Lampén, Tapio; Lassila-Perini, Kati; Lehti, Sami; Lindén, Tomas; Luukka, Panja-Riina; Mäenpää, Teppo; Peltola, Timo; Tuominen, Eija; Tuominiemi, Jorma; Tuovinen, Esa; Wendland, Lauri; Talvitie, Joonas; Tuuva, Tuure

2014-01-01T23:59:59.000Z

39

Methods Mol Biol . Author manuscript 3D structural models of transmembrane proteins  

E-Print Network [OSTI]

proteins is a major research area. Due to the lack of available 3D structures, automatic homology modelingMethods Mol Biol . Author manuscript Page /1 9 3D structural models of transmembrane proteins: Alexandre De Brevern Abstract Summary Transmembrane proteins

Paris-Sud XI, Université de

40

Accepted in Methods Mol Biol. 2010 3D-structural models of transmembrane proteins.  

E-Print Network [OSTI]

of transmembrane proteins is a major research area. Due to the lack of available 3D structures, automatic homology1 Accepted in Methods Mol Biol. 2010 3D-structural models of transmembrane proteins. Alexandre G proteins are macromolecules implicated in major biological process and diseases. Due to their specific

Paris-Sud XI, Université de

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


41

J. Mol. Biol. (1976) 108, 139-150 Head to Tail Polymerization of Actin  

E-Print Network [OSTI]

J. Mol. Biol. (1976) 108, 139-150 Head to Tail Polymerization of Actin ALBRECHTWEGNER Department actin monomers to solutions of polymeric actin. The incoqooration and release of subunits can be explained by a polymerization mechanism in which the filaments grow at one end and shorten simultaneously

Scholey, Jonathan

42

J. Mol. Riol. (1991) 222, 1085-1108 Complementary Recognition in Condensed DNA: Accelerated  

E-Print Network [OSTI]

J. Mol. Riol. (1991) 222, 1085-1108 Complementary Recognition in Condensed DNA: Accelerated DNA) Condensation of denatured DNA greatly accelerates the kinetics of DNA renaturation. We propose a unifying explanation for the effects of several accelerating solvents studied here including polymers, di

Church, George M.

43

J. Mol. Model. 2000, 6, 1 8 Springer-Verlag 2000FULL PAPER  

E-Print Network [OSTI]

candidates in the conformational space of a protein loop. This high efficiency is due to our grid mapping with a simplified energy function and a grid-map- ping method. As a comparison of single simulation, it takes only, Cluster analysis, Simplified energy function, Grid-mapping method Correspondence to: L. Lai #12;2 J. Mol

Luhua, Lai

44

J. Mol. Biol. (1996) 264, 11641179 How to Derive a Protein Folding Potential? A New  

E-Print Network [OSTI]

J. Mol. Biol. (1996) 264, 1164­1179 How to Derive a Protein Folding Potential? A New Approach of deriving a pairwise potentialHarvard University Department of Chemistry for protein folding. The potential of accuracy. 7 1996 Academic Press Limited *Corresponding author Keywords: protein folding; protein folding

Mirny, Leonid

45

J. Mol. Biol. (1988) 201, 751-754 Aromatic Rings Act as Hydrogen  

E-Print Network [OSTI]

J. Mol. Biol. (1988) 201, 751-754 Aromatic Rings Act as Hydrogen Bond Acceptors Michael Levitt that there is a significant interaction between a hydrogen bond donor (like the > NH group) and the centre of a benzene ring, which acts as a hydrogen bond acceptor. This interaction, hvdrogen bond, which is about half as strong

Levitt, Michael

46

c : solute concentration in solution, mol or g solutes/ cm3  

E-Print Network [OSTI]

by a finite difference, a finite element or a boundary element technique. Then a discretization scheme) algebraic equations that can be solved by different methods. The operation by means of such a mathematical : soil bulk density, g/cm3 : source/sink term, µ mol/cm3 /h or µg/cm3 /h INTRODUCTION In many arid

Kumar, C.P.

47

SUBMILLIMETER POLARIZATION OF GALACTIC CLOUDS: A COMPARISON OF 350 {mu}m AND 850 {mu}m DATA  

SciTech Connect (OSTI)

The Hertz and SCUBA polarimeters, working at 350 {mu}m and 850 {mu}m, respectively, have measured the polarized emission in scores of Galactic clouds. Of the clouds in each data set, 17 were mapped by both instruments with good polarization signal-to-noise ratios. We present maps of each of these 17 clouds comparing the dual-wavelength polarization amplitudes and position angles at the same spatial locations. In total number of clouds compared, this is a four-fold increase over previous work. Across the entire data set real position angle differences are seen between wavelengths. While the distribution of {phi}(850)-{phi}(350) is centered near zero (near-equal angles), 64% of data points with high polarization signal-to-noise (P {>=} 3{sigma}{sub p}) have |{phi}(850)-{phi}(350)| > 10 Degree-Sign . Of those data with small changes in position angle ({<=}10 Degree-Sign ) the median ratio of the polarization amplitudes is P(850)/P(350) = 1.7 {+-} 0.6. This value is consistent with previous work performed on smaller samples and models that require mixtures of different grain properties and polarization efficiencies. Along with the polarization data we have also compiled the intensity data at both wavelengths; we find a trend of decreasing polarization with increasing 850-to-350 {mu}m intensity ratio. All the polarization and intensity data presented here (1699 points in total) are available in electronic format.

Vaillancourt, John E. [SOFIA Science Center, Universities Space Research Association, NASA Ames Research Center, Moffett Field, CA 94035 (United States); Matthews, Brenda C., E-mail: jvaillancourt@sofia.usra.edu, E-mail: brenda.matthews@nrc-cnrc.gc.ca [Herzberg Institute, National Research Council of Canada, 5071 W. Saanich Road, Victoria, BC V9E 2E7 (Canada)

2012-08-01T23:59:59.000Z

48

Farzana Rahman (http://www.mscs.mu.edu/~frahman/) Curriculum Vitae  

E-Print Network [OSTI]

RFID Systems Advisor: Dr. Sheikh Iqbal Ahamed (http://www.mscs.mu.edu/~iq/) Marquette University. Sheikh Iqbal Ahamed (http://www.mscs.mu.edu/~iq/) Bangladesh University of Engineering and Technology

Brylow, Dennis

49

Improvements to a MODIS global terrestrial evapotranspiration algorithm Qiaozhen Mu , Maosheng Zhao, Steven W. Running  

E-Print Network [OSTI]

towers. The global annual total ET over the vegetated land surface is 62.8Ã?103 km3 , agrees very wellImprovements to a MODIS global terrestrial evapotranspiration algorithm Qiaozhen Mu , Maosheng Zhao Vegetation cover fraction MODIS MODIS global evapotranspiration (ET) products by Mu et al. [Mu, Q., Heinsch

Montana, University of

50

The MuCool Test Area and RF Program  

SciTech Connect (OSTI)

The MuCool RF Program focuses on the study of normal conducting RF structures operating in high magnetic field for applications in muon ionization cooling for Neutrino Factories and Muon Colliders. This paper will give an overview of the program, which will include a description of the test facility and its capabilities, the current test program, and the status of a cavity that can be rotated in the magnetic field which allows for a more detailed study of the maximum stable operating gradient vs. magnetic field strength and angle.

Bross, A D; Jansson, A; Moretti, A; Yonehara, K; Huang, D; Torun, Y; Li, D; Norem, J; Palmer, R B; Stratakis, D

2010-05-01T23:59:59.000Z

51

NuSTORM {\\mu} Ring -- Design and Injection Optimization  

E-Print Network [OSTI]

The design of the NuSTORM muon production beam line and storage ring is discussed. The facility includes a pion production target station with a pion collection horn and transport into a straight section of a storage ring. {\\pi} decay within that straight section provides {\\mu}'s that are stored within the ring for subsequent decay providing precision electron and muon neutrino beams. The ring and transport designs are described and optimized. Genetic Algorithm optimization of the horn and transport into the ring has been performed, providing a significant increase in intensity

Neuffer, David; Bross, A

2015-01-01T23:59:59.000Z

52

Fermilab Today | Experiment Profiles Archive | Mu2e  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr MayAtmospheric Optical Depth7-1D: Vegetation ProposedUsing ZirconiaPolicyFeasibility ofSmall Works: 2008SubmitMu2e photo FACT SHEET: Click

53

Solenoid magnet system for the Fermilab Mu2e experiment  

DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

The Fermilab Mu2e experiment seeks to measure the rare process of direct muon to electron conversion in the field of a nucleus. Key to the design of the experiment is a system of three superconducting solenoids; a muon production solenoid (PS) which is a 1.8 m aperture axially graded solenoid with a peak field of 5 T used to focus secondary pions and muons from a production target located in the solenoid aperture; an 'S shaped' transport solenoid (TS) which selects and transports the subsequent muons towards a stopping target; a detector solenoid (DS) which is an axially graded solenoid at the upstream end to focus transported muons to a stopping target, and a spectrometer solenoid at the downstream end to accurately measure the momentum of the outgoing conversion elections. The magnetic field requirements, the significant magnetic coupling between the solenoids, the curved muon transport geometry and the large beam induced energy deposition into the superconducting coils pose significant challenges to the magnetic, mechanical, and thermal design of this system. In this paper a conceptual design for the magnetic system which meets the Mu2e experiment requirements is presented.

Lamm, M J [Fermilab; Andreev, N [Fermilab /Boston U.; Ambrosio, G [Fermilab; Brandt, J [Fermilab; Coleman, R [CERN; Evbota, D [Fermilab; Kashikhin, V V [City Coll., N.Y.; Lopes, M [Fermilab; Miller, J [Fermilab; Nicol, T [KEK; Ostojic, R [Tsukuba

2012-06-08T23:59:59.000Z

54

Atmos. Chem. Phys., 14, 59215941, 2014 www.atmos-chem-phys.net/14/5921/2014/  

E-Print Network [OSTI]

, acetonitrile and isoprene were measured for the first time in the IGP. A new atmo- spheric chemistry facility mol-1 for acetonitrile, 1.9 nmol mol-1 for isoprene, 567 nmol mol-1 for carbon monoxide, 57.8 nmol mol parameters and applying chemical tracers (e.g., acetonitrile for biomass burning) and inter-VOC cor

Pierce, Jeffrey

55

Mu2e production solenoid cryostat conceptual design  

SciTech Connect (OSTI)

Mu2e is a muon-to-electron conversion experiment being designed by an international collaboration of more than 65 scientists and engineers from more than 20 research institutions for installation at Fermilab. The experiment is comprised of three large superconducting solenoid magnet systems, production solenoid (PS), transport solenoid (TS) and detector solenoid (DS). A 25 kW, 8 GeV proton beam strikes a target located in the PS creating muons from the decay of secondary particles. These muons are then focused in the PS and the resultant muon beam is transported through the TS towards the DS. The production solenoid presents a unique set of design challenges as the result of high radiation doses, stringent magnetic field requirements, and large structural forces. This paper describes the conceptual design of the PS cryostat and will include discussions of the vacuum vessel, thermal shield, multi-layer insulation, cooling system, cryogenic piping, and suspension system.

Nicol, T.H.; Kashikhin, V.V.; Page, T.M.; Peterson, T.J.; /Fermilab

2011-06-01T23:59:59.000Z

56

Entropy Production at High Energy and mu_B  

E-Print Network [OSTI]

The systematics of bulk entropy production in experimental data on A+A, p+p and e+e- interactions at high energies and large mu_B is discussed. It is proposed that scenarios with very early thermalization, such as Landau's hydrodynamical model, capture several essential features of the experimental results. It is also pointed out that the dynamics of systems which reach the hydrodynamic regime give similar multiplicities and angular distributions as those calculated in weak-coupling approximations (e.g. pQCD) over a wide range of beam energies. Finally, it is shown that the dynamics of baryon stopping are relevant to the physics of total entropy production, explaining why A+A and e+e- multiplicities are different at low beam energies.

Peter Steinberg

2007-02-08T23:59:59.000Z

57

Laboratory Hydro-mechanical Characterisation of Boom Clay at Essen and Mol Y. F. Deng1, 2  

E-Print Network [OSTI]

of 220 - 260 m and from HADES that is the underground rock laboratory at Mol in Belgium, at 223-m depth facility called HADES (High-Activity Disposal Experimental Site) excavated at 223-m depth close to the city

Paris-Sud XI, Université de

58

Search for heavy Majorana neutrinos in $\\mu^\\pm \\mu^\\pm$+jets events in proton-proton collisions at $\\sqrt{s}$ = 8 TeV  

E-Print Network [OSTI]

A search is performed for heavy Majorana neutrinos (N) using an event signature defined by two muons of the same charge and two jets ($\\mu^\\pm \\mu^\\pm \\mathrm{j j}$). The data correspond to an integrated luminosity of 19.7 fb$^{-1}$ of proton-proton collisions at a center-of-mass energy of 8 TeV, collected with the CMS detector at the CERN LHC. No excess of events is observed beyond the expected standard model background and upper limits are set on $|V_{\\mu\\mathrm{N}}|^2$ as a function of Majorana neutrino mass $\\mathrm{m}_{\\mathrm{N}}$ for masses in the range of 40-500 GeV, where $|V_{\\mu\\mathrm{N}}|$ is the mixing element of the heavy neutrino with the standard model muon neutrino. The limits obtained are $|V_{\\mu\\mathrm{N}}|^2 \\le 0.00470$ for $\\mathrm{m}_{\\mathrm{N}} = 90$ GeV, $|V_{\\mu\\mathrm{N}}|^2 \\le 0.0123$ for $\\mathrm{m}_{\\mathrm{N}} = 200$ GeV, and $|V_{\\mu\\mathrm{N}}|^2 \\le 0.583$ for $\\mathrm{m}_{\\mathrm{N}} = 500$ GeV. These results extend considerably the regions excluded by previous direct s...

CMS Collaboration

2015-01-01T23:59:59.000Z

59

A Measurement of the Inclusive Z / gamma* --> mu+ mu- Cross-Section and Study of W and Z Events in proton - anti-proton Collisions at D0  

SciTech Connect (OSTI)

A measurement of the inclusive Z/{gamma}* {yields} {mu}{sup +}{mu}{sup -} cross section for M{sub {mu}{mu}} > 40 GeV at {radical}s = 1.96 TeV is presented. The measurement is performed using a data sample corresponding to an integrated luminosity of 147.7 pb{sup -1}, collected with the D0 detector at the Tevatron, Fermilab, between September 2002 and October 2003. A total of 14352 di-muon events are selected and a final result of {sigma}(Z/{gamma}*) = 327.8 {+-} 3.4(stat.) {+-} 8.4(syst.) {+-} 21.3(lumi.) pb is obtained. Correcting the number of di-muon events by a factor of 0.885 {+-} 0.015 for the contribution from pure {gamma}* exchange and Z/{gamma}* interference, the inclusive Z {yields} {mu}{sup +}{mu}{sup -} cross section is found to be: {sigma}(Z) = 290.1 {+-} 3.0(stat.) {+-} 7.4(syst.) {+-} 18.9(lumi.) pb. Finally, comparisons of W and Z boson p{sub T} distributions as measured with D0 during Run I of the Tevatron are compared to HERWIG and MC{at}NLO predictions. Relevant parameters in the simulations are tuned to obtain the best possible fit to the data. An excellent agreement is found for both HERWIG and MC{at}NLO.

Nurse, Emily L

2005-02-01T23:59:59.000Z

60

The changing accretion states of the intermediate polar MU Camelopardalis  

E-Print Network [OSTI]

We study the timing and spectral properties of the intermediate polar MU Camelopardalis (1RXS J062518.2+733433) to determine the accretion modes and the accretion geometry from multi-wavelength, multi-epoch observational data. Light curves in different observed energy ranges (optical, UV, X-ray) are extracted. The timescales of variability in these light curves are determined using Analysis of Variance. Phase-resolved X-ray spectra are created with respect to the most prominent detected periodicities and each fitted with an identical model, to quantify the differences in the fitted components. The published tentative value for the spin period is unambiguously identified with the rotation period of the white dwarf. We detect a distinct soft X-ray component that can be reproduced well by a black body. The analysis of data obtained at different epochs demonstrates that the system is changing its accretion geometry from disk-dominated to a combination of disk- plus stream-dominated, accompanied with a significant change in brightness at optical wavelengths.

A. Staude; A. D. Schwope; R. Schwarz; J. Vogel; M. Krumpe; A. Nebot Gomez-Moran

2008-06-04T23:59:59.000Z

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


61

The changing accretion states of the intermediate polar MU Camelopardalis  

E-Print Network [OSTI]

We study the timing and spectral properties of the intermediate polar MU Camelopardalis (1RXS J062518.2+733433) to determine the accretion modes and the accretion geometry from multi-wavelength, multi-epoch observational data. Light curves in different observed energy ranges (optical, UV, X-ray) are extracted. The timescales of variability in these light curves are determined using Analysis of Variance. Phase-resolved X-ray spectra are created with respect to the most prominent detected periodicities and each fitted with an identical model, to quantify the differences in the fitted components. The published tentative value for the spin period is unambiguously identified with the rotation period of the white dwarf. We detect a distinct soft X-ray component that can be reproduced well by a black body. The analysis of data obtained at different epochs demonstrates that the system is changing its accretion geometry from disk-dominated to a combination of disk- plus stream-dominated, accompanied with a significant...

Staude, A; Schwarz, R; Vogel, J; Krumpe, M; Gomez-Moran, A Nebot

2008-01-01T23:59:59.000Z

62

Thermal Design of the Mu2e Detector Solenoid  

SciTech Connect (OSTI)

The reference design for a superconducting Detector Solenoid (DS) for the Mu2e experiment has been completed. The main functions of the DS are to provide a graded field in the region of the stopping target which ranges from 2 T to 1 T and a uniform precision magnetic field of 1 T in a volume large enough to house a tracker downstream of the stopping target. The inner diameter of the magnet cryostat is 1.9 m and the length is 10.9 m. The gradient section of the magnet is about 4 m long and the spectrometer section with a uniform magnetic field is about 6 m long. The inner cryostat wall supports the stopping target, tracker, calorimeter and other equipment installed in the DS. This warm bore volume is under vacuum during operation. It is sealed on one end by the muon beam stop, while it is open on the other end where it interfaces with the Transport Solenoid. The operating temperature of the magnetic coil is 4.7 K and is indirectly cooled with helium flowing in a thermosiphon cooling scheme. This paper describes the thermal design of the solenoid, including the design aspects of the thermosiphon for the coil cooling, forced flow cooling of the thermal shields with 2 phase LN2 (Liquid Nitrogen) and the transient studies of the cool down of the cold mass as well.

Dhanaraj, Nandhini; Wands, Bob; Buehler, Marc; Feher, Sandor; Page, Thomas M; Peterson, Thomas; Schmitt, Richard L

2014-12-18T23:59:59.000Z

63

Confocal {mu}-XRF, {mu}-XAFS, and {mu}-XRD Studies of Sediment from a Nuclear Waste Disposal Natural Analogue Site and Fractured Granite Following a Radiotracer Migration Experiment  

SciTech Connect (OSTI)

Combined {mu}-XRF, {mu}-XAFS, and {mu}-XRD investigations of a uranium-rich tertiary sediment, from a nuclear repository natural analogue site, and a fractured granite bore core section after a column tracer experiment using a Np(V) containing cocktail have been performed. Most {mu}-XRF/{mu}-XAFS measurements are recorded in a confocal geometry to provide added depth information. The U-rich sediment results show uranium to be present as a tetravalent phosphate and that U(IV) is associated with As(V). Arsenic present is either As(V) or As(0). The As(0) forms thin coatings on the surface of pyrite nodules. A hypothesis for the mechanism of uranium immobilization is proposed, where arsenopyrite acted as reductant of ground water dissolved U(VI) leading to precipitation of less soluble U(IV) and thereby forming As(V). Results for the granite sample show the immobilized Np to be tetravalent and associated with facture material.

Denecke, Melissa A.; Brendebach, Boris; Rothe, Joerg; Simon, Rolf [Forschungszentrum Karlsruhe, P.O. Box 3640, D-76021 Karlsruhe (Germany); Janssens, Koen; Nolf, Wout de; Vekemans, Bart [Department of Chemistry, University of Antwerp, Universiteitsplein 1, B-2610 Antwerp (Belgium); Falkenberg, Gerald [Hamburger Synchrotronstrahlungslabor (HASYLAB) at DESY, Notkestr. 85, D-22603 Hamburg (Germany); Somogyi, Andrea [Synchrotron Soleil, F-91192 Gif-sur-Yvette Cedex (France); Noseck, Ulrich [Gesellschaft fuer Anlagen- und Reaktorsicherheit (GRS) mbH, Theodor-Heuss-Strasse 4, D-38122 Braunschweig (Germany)

2007-02-02T23:59:59.000Z

64

mu-term: A Tool for Proving Termination of Context-Sensitive Rewriting ?  

E-Print Network [OSTI]

mu-term: A Tool for Proving Termination of Context-Sensitive Rewriting ? Salvador Lucas DSIC@dsic.upv.es Abstract. Restrictions of rewriting can eventually achieve termination by pruning all in#12;nite rewrite. This paper describes mu-term, a tool which can be used to automatically prove termination of CSR. The tool

Lucas, Salvador

65

mu-term: A Tool for Proving Termination of Context-Sensitive Rewriting  

E-Print Network [OSTI]

mu-term: A Tool for Proving Termination of Context-Sensitive Rewriting Salvador Lucas DSIC@dsic.upv.es Abstract. Restrictions of rewriting can eventually achieve termination by pruning all infinite rewrite. This paper describes mu-term, a tool which can be used to automatically prove termination of CSR. The tool

Lucas, Salvador

66

Summer 2012Protecting MU's Health, Safety, and the Environment Laboratory Safety Incidents  

E-Print Network [OSTI]

to be safety conscious in the work they do, especially in a laboratory setting. In fiscal year 2011, MU and Safety is working to raise awareness of the need to work safely in laboratories. It is important to have Laboratory Safety plays an important role at MU. As Environmental Health and Safety works to promote lab

Taylor, Jerry

67

Feasibility Studies on a Downstream Injection System for Mu2e Calorimeter Calibration Guangyong Koha  

E-Print Network [OSTI]

Feasibility Studies on a Downstream Injection System for Mu2e Calorimeter Calibration Electrons A calibration-electron injection system sited downstream of the calorimeters within the Mu2e detector solenoid directed along the beam axis), progressing downstream over the extent of the stopping target array.1

Gollin, George

68

Recent results of. mu. CF experiments at SIN (Swiss Institute For Nuclear Research)  

SciTech Connect (OSTI)

Important topics concerning Muon Catalyzed Fusion were investigated in experiments at the Swiss Institute for Nuclear Research (SIN), including transient and steady state rates for the main d..mu..t cycle as well as detailed information about the competing d..mu..d and t..mu..t fusion branches. The basic kinetic parameters were determined and striking features of the resonant d..mu..t formation process were revealed (density effect, epithermal behavior). DT sticking was measured with independent techniques, i.e., detection of fusion neutrons as well as ..mu..He x-rays after fusion. Fusion yields per muon of 113 +- 10 were observed at liquid conditions, yields exceeding 200 are anticipated for optimal conditions from our results. 43 refs., 8 figs., 3 tabs.

Breunlich, W.H.; Cargnelli, M.; Bistirlich, J.; Crowe, K.M.; Justice, M.; Kurck, J.; Petitjean, C.; Sherman, R.H.; Bossy, H.; Daniel, H.

1986-09-01T23:59:59.000Z

69

J. Mol. Biol. (1975) 91, 101-120 A Neutron Scattering Study of the Distribution of Protein  

E-Print Network [OSTI]

J. Mol. Biol. (1975) 91, 101-120 A Neutron Scattering Study of the Distribution of Protein and RNA coli have been measured by neutron scattering experiments on the intact subunit. In addition the radius, 1972; Lutter et al., 1972), and neutron scattering (Engelman & Moore, 1972; Moore et al., 1974

70

Eur J Nucl Med Mol Imaging . Author manuscript The age of reason for FDG PET image-derived indices  

E-Print Network [OSTI]

Eur J Nucl Med Mol Imaging . Author manuscript Page /1 3 The age of reason for FDG PET image Author Keywords image derived parameters ; 18F-FDG-PET ; prediction ; prognosis ; therapy response The clinical use of Positron Emission Tomography (PET) imaging using the 2-deoxy-2-(18F

Paris-Sud XI, Université de

71

ISOLATION OF NUCLEAR DNA FROM PLANTS Based on Peterson et al. (1997), Plant Mol. Biol. Reptr. 15: 148-153.  

E-Print Network [OSTI]

ISOLATION OF NUCLEAR DNA FROM PLANTS Based on Peterson et al. (1997), Plant Mol. Biol. Reptr. 15 quantities of nuclear DNA from a wide variety of plants including pine, tomato, juniper, cypress, sorghum for plants in which polyphenols are a problem, although it has provided good results for every plant species

Ray, David

1997-01-01T23:59:59.000Z

72

Measurement of \\Gamma_{ee}(J/\\psi)*Br(J/\\psi->e^+e^-) and \\Gamma_{ee}(J/\\psi)*Br(J/\\psi->\\mu^+\\mu^-)  

E-Print Network [OSTI]

The products of the electron width of the J/\\psi meson and the branching fraction of its decays to the lepton pairs were measured using data from the KEDR experiment at the VEPP-4M electron-positron collider. The results are \\Gamma_{ee}(J/\\psi)*Br(J/\\psi->e^+e^-)=0.3323\\pm0.0064\\pm0.0048 keV, \\Gamma_{ee}(J/\\psi)*Br(J/\\psi->\\mu^+\\mu^-)=0.3318\\pm0.0052\\pm0.0063 keV. Assuming e\\mu universality and using the world average value of the lepton branching fraction, we also determine the leptonic \\Gamma_{ll}=5.59\\pm0.12 keV and total \\Gamma=94.1\\pm2.7 keV widths of the J/\\psi meson.

Anashin, V V; Baldin, E M; Barladyan, A K; Barnyakov, A Yu; Barnyakov, M Yu; Baru, S E; Bedny, I V; Beloborodova, O L; Blinov, A E; Blinov, V E; Bobrov, A V; Bobrovnikov, V S; Bogomyagkov, A V; Bondar, A E; Bondarev, D V; Buzykaev, A R; Eidelman, S I; Glukhovchenko, Yu M; Gulevich, V V; Gusev, D V; Karnaev, S E; Karpov, G V; Karpov, S V; Kharlamova, T A; Kiselev, V A; Kononov, S A; Kotov, K Yu; Kravchenko, E A; Kulikov, V F; Kurkin, G Ya; Kuper, E A; Levichev, E B; Maksimov, D A; Malyshev, V M; Maslennikov, A L; Medvedko, A S; Meshkov, O I; Mishnev, S I; Morozov, I I; Muchnoi, N Yu; Neufeld, V V; Nikitin, S A; Nikolaev, I B; Okunev, I N; Onuchin, A P; Oreshkin, S B; Orlov, I O; Osipov, A A; Peleganchuk, S V; Pivovarov, S G; Piminov, P A; Petrov, V V; Poluektov, A O; Popkov, I N; Prisekin, V G; Ruban, A A; Sandyrev, V K; Savinov, G A; Shamov, A G; Shatilov, D N; Shwartz, B A; Simonov, E A; Sinyatkin, S V; Skovpen, Yu I; Skrinsky, A N; Smaluk, V V; Sokolov, A V; Sukharev, A M; Starostina, E V; Talyshev, A A; Tayursky, V A; Telnov, V I; Tikhonov, Yu A; Todyshev, K Yu; Tumaikin, G M; Usov, Yu V; Vorobiov, A I; Yushkov, A N; Zhilich, V N; Zhulanov, V V; Zhuravlev, A N

2009-01-01T23:59:59.000Z

73

DISCOVERY AND ANALYSIS OF 21 {mu}m FEATURE SOURCES IN THE MAGELLANIC CLOUDS  

SciTech Connect (OSTI)

Spitzer Space Telescope mid-infrared spectroscopy has been obtained for 15 carbon-rich protoplanetary nebulae (PPNe) in the Large Magellanic Cloud (LMC) and for two other such stars in the Small Magellanic Cloud (SMC). Of these 17 PPNe, the unidentified 21 {mu}m feature is strong in 7 spectra, weak in 2 spectra, and very weak or questionable in 4 spectra. Two of the four spectra without the 21 {mu}m feature have a very strong feature near 11 {mu}m, similar to a feature observed in some carbon-rich planetary nebulae (PNe) in the LMC. We attribute this feature to unusual SiC dust, although the feature-to-continuum ratio is much larger than for SiC features in Galactic or Magellanic Cloud carbon star spectra. The remaining two objects show typical carbon-rich PPNe spectra with no 21 {mu}m features. One of the LMC objects that lacks the 21 {mu}m feature and one SMC object with a questionable 21 {mu}m detection may have mixed dust chemistries based upon their spectral similarity to Galactic [WC] PNe. The 13 objects that either definitely or may show the 21 {mu}m feature have distinct dust shell properties compared to the Galactic 21 {mu}m objects-the 21 {mu}m features are weaker, the estimated dust temperatures are significantly higher, the unidentified infrared (UIR) bands are stronger, and the UIRs show more structure. Four of the 21 {mu}m objects appear to show normal SiC emission features in their spectra. Many of the PPNe show strong 30 {mu}m features, although this feature carries less of the total mid-infrared emission than is normally the case for the Galactic 21 {mu}m PPNe. The LMC objects are in the LMC halo rather than in the LMC bar. The estimated luminosities of these PPNe vary from 4700 to 12,500 L{sub sun}.

Volk, Kevin; Meixner, Margaret; Gordon, Karl D. [Space Telescope Science Institute, 3700 San Martin Drive, Baltimore, MD 21218 (United States); Hrivnak, Bruce J. [Department of Physics and Astronomy, Valparaiso University, Valparaiso, IN 46383 (United States); Matsuura, Mikako [Department of Physics and Astronomy, UCL-Institute of Origins, University College London, Gower Street, London WC1E 6BT (United Kingdom); Bernard-Salas, Jeronimo [Institut d Astrophysique Spatiale, CNRS/Universite Paris-Sud 11, 91405, Orsay (France); Szczerba, Ryszard [N. Copernicus Astronomical Center, Rabianska 8, 87-100 Torun (Poland); Sloan, G. C. [Department of Astronomy, Cornell University, Ithaca, NY 14853 (United States); Kraemer, Kathleen E. [Air Force Research Laboratory, AFRL/RVBYB, 29 Randolph Road, Hanscom AFB, MA 01731 (United States); Van Loon, Jacco Th. [Astrophysics Group, Lennard-Jones Laboratories, Keele University, Staffordshire ST5 5BG (United Kingdom); Kemper, F.; Woods, Paul M.; Zijlstra, Albert A. [Jodrell Bank Centre for Astrophysics, Alan Turing Building, School of Physics and Astronomy, University of Manchester, Oxford Road, Manchester M13 9PL (United Kingdom); Sahai, Raghvendra [Jet Propulsion Laboratory, MS 183-900, California Institute of Technology, Pasadena, CA 91109 (United States); Gruendl, Robert A. [Astronomy Department, University of Illinois, 1002 West Green Street, Urbana, IL 61801 (United States); Tielens, Alexander G. G. M. [Leiden Observatory, P.O. Box 9513, NL-2300 RA Leiden (Netherlands); Indebetouw, Remy [Department of Astronomy, University of Virginia, P.O. Box 400325, Charlottesville, VA 22903 (United States); Marengo, Massimo, E-mail: volk@stsci.edu [Department of Physics and Astronomy, Iowa State University, A313E Zaffarano, Ames, IA 50011 (United States)

2011-07-10T23:59:59.000Z

74

The AAA+ ClpX machine unfolds a keystone subunit to remodel the Mu transpososome  

E-Print Network [OSTI]

A hyperstable complex of the tetrameric MuA transposase with recombined DNA must be remodeled to allow subsequent DNA replication. ClpX, a AAA+ enzyme, fulfills this function by unfolding one transpososome subunit. Which ...

Baker, Tania

75

Design, Synthesis and Evaluation of Peptide-Based Affinity Labels for Mu Opioid Receptors  

E-Print Network [OSTI]

Narcotic analgesics produce pain relief generally through activation of &mu opioid receptors (MOR), but the use of these analgesics is limited by their side effects, namely respiratory depression, tolerance, physical ...

Sinha, Bhaswati

2009-07-17T23:59:59.000Z

76

A 205 {mu}m [N II] MAP OF THE CARINA NEBULA  

SciTech Connect (OSTI)

We present the results of a {approx}250 arcmin{sup 2} mapping of the 205 {mu}m [N II] fine-structure emission over the northern Carina Nebula, including the Car I and Car II H II regions. Spectra were obtained using the South Pole Imaging Fabry-Perot Interferometer (SPIFI) at the Antarctic Submillimeter Telescope and Remote Observatory (AST/RO) at the South Pole. We supplement the 205 {mu}m data with new reductions of far-IR fine-structure spectra from the Infrared Space Observatory (ISO) Long Wavelength Spectrometer (LWS) in 63 {mu}m [O I], 122 {mu}m [N II], 146 {mu}m [O I], and 158 {mu}m [C II]; the 146 {mu}m [O I] data include 90 raster positions which have not been previously published. Morphological comparisons are made with optical, radio continuum, and CO maps. The 122/205 line ratio is used to probe the density of the low-ionization gas, and the 158/205 line ratio is used to probe the fraction of C{sup +} arising from photodissociation regions (PDRs). The [O I] and [C II] lines are used to construct a PDR model of Carina. When the PDR properties are compared with other sources, Carina is found to be more akin to 30 Doradus than galactic star-forming regions such as Orion, M17, or W49; this is consistent with the view of Carina as a more evolved region, where much of the parent molecular cloud has been ionized or swept away. These data constitute the first ground-based detection of the 205 {mu}m [N II] line, and the third detection overall since those of COBE FIRAS and the Kuiper Airborne Observatory in the early 1990s.

Oberst, T. E.; Parshley, S. C.; Nikola, T.; Stacey, G. J. [Department of Astronomy, Cornell University, Ithaca, NY 14853 (United States); Loehr, A.; Lane, A. P.; Stark, A. A. [Harvard-Smithsonian Center for Astrophysics, Cambridge, MA 02138 (United States); Kamenetzky, J., E-mail: oberstte@westminster.edu [Center for Astrophysics and Space Astronomy, University of Colorado, Boulder, CO 80303 (United States)

2011-10-01T23:59:59.000Z

77

On the model discriminating power of mu to e conversion in nuclei  

SciTech Connect (OSTI)

Lepton Flavor Violating (LFV) charged lepton decays provide a highly sensitive probe of physics beyond the Standard Model (SM), due to the un-observably small branching fractions ({approx}10{sup -50}) predicted for these modes in the SM (minimally extended to include massive neutrinos). Searches for SM forbidden muon processes, such as {mu} {yields} e{gamma}, {mu} {yields} e{bar e}e, and {mu} {yields} e conversion in nuclei, have provided so far the strongest constraints on LFV new physics. This statement can be characterized in a model-independent way as a lower bound on the scale associated to a set of dimension six effective operators parameterizing new physics beyond the SM. It is a well known fact that while the decay {mu} {yields} e{gamma} is only sensitive to a transition magnetic dipole operator, both {mu} {yields} e{bar e}e and {mu} {yields} e conversion in nuclei are sensitive to transition charge radii operators as well as purely contact four-fermion interactions induced by physics beyond the SM. In other words, different LFV decays have different sensitivities to underlying LFV mechanisms (effective operators). This leads naturally to ask the question whether one could infer the relative strength of these different operators in a completely phenomenological and model-independent way. This would allow one to discriminate among different underlying models of LFV and thus would provide valuable input for model building. In Ref. [1] it was pointed out that in principle, by combining the rates of {mu} {yields} e{gamma} and {mu} {yields} e conversion on different target nuclei, one could discriminate underlying models. In this work we go back to this issue with the aim to: quantify the theoretical uncertainty induced by the hadronization process; and quantify the experimental precision required to realistically infer useful information on the underlying LFV mechanisms. We organize our discussion as follows: in Section 2 we review the derivation of the {mu} {yields} e conversion rate starting from a general effective theory description of the LFV physics. In Section 3 we explore the phenomenological consequence of the simplest possible models, in which only one effective LFV operator dominates. We extend this analysis in Section 4 to the class of models in which two operators dominate. In Section 5 we specialize our discussion to the SUSY see-saw model and summarize the conclusions of our analysis in Section 6.

Cirigliano, Vincenzo [Los Alamos National Laboratory; Kitano, Ryuichiro [JAPAN; Okada, Yashuiro [JAPAN; Tuzon, Paulo [ITALY

2009-01-01T23:59:59.000Z

78

Search for B?s ? ?+ ?- and B?d ? mu+mu- decays in p anti-p collisions with CDF. II.  

SciTech Connect (OSTI)

We report on a search for B?s ? ?+ ?- and B?d ? mu+mu- decays in p anti-p collisions at ?s = 1.96 TeV using 364.4 pb -1 of data collected by the CDF II dectector at Fermilab Tevatron Collider. After applying all selection requirements, we observe no candidates inside the B?s or B?d mass windows. The resulting upper limits on the branching fractions are ?(B?s ? ?+?-) < 1.5 x 10-7 and ?(B?d ? ?+?-) < 3.9 x 10-8 at 90 % confidence level. (auth)

Abulencia, A.; Acosta, D.; Adelman, J.; Affolder, T.; Akimoto, T.; Albrow, M. G.; Ambrose, D.; Amerio, S.; Amidei, D.; Anastassov, A.; Anikeev, K.; Annovi, A.; Antos, J.; Aoki, M.; Apollinari, G.; Arguin, J. -F.; Arisawa, T.; Artikov, A.; Ashmanskas, W.; Attal, A.; Azfar, F.

2005-08-01T23:59:59.000Z

79

Routine {sup 18}F{sup -} production with 180 {mu}A to 200 {mu}A target beam current on a GE PETtrace 800 cyclotron  

SciTech Connect (OSTI)

Through upgrades and enhancements, which are now standard on current PETtrace 800 cyclotrons, a GE PETtrace cyclotron installed in 2002 has demonstrated reliable routine [{sup 18}F]FDG production at total target beam currents of 180 {mu}A without detriment to saturation and [{sup 18}F]FDG yields. Routine production at 200 {mu}A has been achieved and its evaluation is continuing. Self-shielded target using W/Cu alloy for the target body afforded a reduction in dose rate from the Havar foils by a factor of {approx} 8-10, reducing dose from the targets and need for removing targets during maintenance. The main activation product in the shield is {sup 187}W (T1/2 24 h). The {sup 60}Co ((T1/2 5.3 y) activation is about 250 times less at 24 h post EOB and is not considered a major issue despite its long half-life.

Eberl, S.; Eriksson, T.; Svedberg, O.; Norling, J.; Henderson, D.; Lam, P.; Bourdier, T.; Fulham, M. [Department of PET and Nuclear Medicine, Royal Prince Alfred Hospital, Sydney, NSW (Australia); GEMS PET Systems AB, Uppsala (Sweden); Department of PET and Nuclear Medicine, Royal Prince Alfred Hospital, Sydney, NSW (Australia)

2012-12-19T23:59:59.000Z

80

An upper limit on the decay D/sup 0/. -->. mu. e  

SciTech Connect (OSTI)

A search for the lepton family number violating decay D/sup 0/ ..-->.. ..mu..e is reported. No signal is observed in a data sample of 9.3 pb/sup -1/ collected at the psi(3770) resonance with the Mark III detector, where 0.18 +- 0.06 +- 0.05 background events are expected. A 90% confidence level upper limit on the branching fraction B(D/sup 0/ ..-->.. ..mu..e) of 1.5 x 10/sup -4/ is obtained.

Stockhausen, W.

1987-04-01T23:59:59.000Z

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


81

A new determination of $\\mathcal{S} \\mathcal{T} \\langle N| \\overline{q} D_{\\mu} D_{\  

E-Print Network [OSTI]

The symmetric and traceless part of the matrix element $\\mathcal{S} \\mathcal{T} \\langle N| \\overline{q} D_{\\mu} D_{\

Gubler, Philipp; Lee, Su Houng

2015-01-01T23:59:59.000Z

82

MU FAPRI reports economic impact of extending ethanol tax credit, tariff Contact:Duane Dailey  

E-Print Network [OSTI]

. ­ Extending the current ethanol tax credit and tariff would boost corn-based fuel production -- and corn for corn as an ethanol fuel source would expand corn acreage by 1.7 million acres, said Seth Meyer, MU for blended fuel at the pump. "At the same time, blenders can pay more to ethanol plants that in turn pay

Noble, James S.

83

Improving MU-MIMO Performance in LTE-(Advanced) by Efficiently Exploiting Feedback  

E-Print Network [OSTI]

(CDI/PMI). The standard supports finer granularity feedback i.e. sub-band feedback method, but it-band feedback for providing more frequent update of PMI. However, in order to support this feedback method, we), Downlink Control Information (DCI), Multi-user MIMO (MU-MIMO), Precoding Matrix Indi- cator (PMI

Gesbert, David

84

Mu2e collaboration meeting, August 7, 2009 1 Matthew McHugh  

E-Print Network [OSTI]

Inside L-Tracker #12;Mu2e collaboration meeting, August 7, 2009 2 The Point · Differentiate between-Kutta ­ Accurate, coinciding paths ­ 1 picosecond intervals · Coordinate transformation ­ Particle within tracker, August 7, 2009 5 Stopping Power, dE/dx · Approximate material as homogenous · Bethe-Bloch for heavy

Gollin, George

85

Dynamic Software Update Emili Miedes and Francesc D. Mu~noz-Escoi  

E-Print Network [OSTI]

the software. Furthermore, it complicates the design and development of the software service. For instanceDynamic Software Update Emili Miedes and Francesc D. Mu~noz-Esco´i Instituto Universitario Mixto Tecnol´ogico de Inform´atica Universitat Polit`ecnica de Val`encia Campus de Vera s/n, 46022 Valencia

Muñoz, Francesc

86

Dynamic Software Update Emili Miedes and Francesc D. Mu~noz-Escoi  

E-Print Network [OSTI]

, it complicates the design and development of the software service. For instance, the software must be ableDynamic Software Update Emili Miedes and Francesc D. Mu~noz-Esco´i Instituto Universitario Mixto Tecnol´ogico de Inform´atica Universitat Polit`ecnica de Val`encia Campus de Vera s/n, 46022 Valencia

Muñoz, Francesc

87

Propagation of Intercellular Calcium Waves in Retinal Astrocytes and Mu ller Cells  

E-Print Network [OSTI]

Propagation of Intercellular Calcium Waves in Retinal Astrocytes and Mu¨ ller Cells Eric A. Newman. Experiments were conducted to determine the mechanism of Ca2 wave propagation between glial cells in an intact fluo-4. Mechanical stimulation of astrocyte somata evoked Ca2 waves that propagated through both

Newman, Eric A.

88

Optimizing microalgal production in raceway systems Rafael Mu~noz-Tamayoa  

E-Print Network [OSTI]

have been10 identified as a renewable source for biodiesel production [5, 18]. However, despite these11Optimizing microalgal production in raceway systems Rafael Mu~noz-Tamayoa , Francis Maireta is characterized by the production of high value compounds. Optimization of the performance of microalgae culture

Boyer, Edmond

89

Small scale turbulence and instabilities observed simultaneously by radiosondes and the MU radar.  

E-Print Network [OSTI]

Small scale turbulence and instabilities observed simultaneously by radiosondes and the MU radar. R-French field campaign devoted to study small-scale turbulence and instabilities in the lower atmosphere for retrieving small-scale turbulence parameters from ST radars. However, the dominant sources

90

HYDROGEN DISTILLATION AT THE DEUTERIUM REMOVAL UNIT OF MuCap EXPERIMENT  

E-Print Network [OSTI]

321 HYDROGEN DISTILLATION AT THE DEUTERIUM REMOVAL UNIT OF MuCap EXPERIMENT I.A. Alekseev, E hydrogen gas (so- called protium) must be used. It is necessary to avoid transfers of - to impurities imposes strict and critical requirements on the hydrogen gas system supporting the detector. Desirable

Titov, Anatoly

91

Leaf gas exchange and carbohydrate concentrations in Pinus pinaster plants subjected to elevated CO2  

E-Print Network [OSTI]

to elevated CO2 and a soil drying cycle Catherine Picon-Cochard Jean-Marc Guehl Unité de recherches en.) were acclimated for 2 years under ambient (350 ?mol mol-1)and elevated (700 ?mol mol-1) CO2 concentrations ([CO2]). In the summer of the second growing season, the plants were subjected to a soil drying

Paris-Sud XI, Université de

92

Measurement of the CP-violation parameter of B0 mixing and decay with p anti-p ---> mu mu X data  

SciTech Connect (OSTI)

The authors measure the dimuon charge asymmetry A in p{bar p} collisions at a center of mass energy {radical}s 1960 GeV. The data was recorded with the D0 detector and corresponds to an integrated luminosity of approximately 1.0 fb{sup -1}. Assuming that the asymmetry A is due to asymmetric B{sup 0} {leftrightarrow} {bar B}{sup 0} mixing and decay, they extract the CP-violation parameter of B{sup 0} mixing and decay: R({epsilon}{sub B{sup 0}}/1) + |{epsilon}{sub B{sup 0}}|{sup 2} = A{sub B{sup 0}}/4 = -0.0023 {+-} 0.0011(stat) {+-} 0.0008(syst). A{sub B{sup 0}} is the dimuon charge asymmetry from decays of B{sup 0}{bar B}{sup 0} pairs. The general case, with CP violation in both B{sup 0} and B{sub s}{sup 0} systems, is also considered. Finally they obtain the forward-backward asymmetry that quantifies the tendency of {mu}{sup +} to go in the proton direction and {mu}{sup -} to go in the anti-proton direction. The results are consistent with the standard model and constrain new physics.

Abazov, V.M.; Abbott, B.; Abolins, M.; Acharya, B.S.; Adams, M.; Adams, T.; Agelou, M.; Aguilo, E.; Ahn, S.H.; Ahsan, M.; Alexeev, G.D.; /Buenos Aires U. /Rio de Janeiro,

2006-09-01T23:59:59.000Z

93

Proving Termination Properties with mu-term Beatriz Alarcon, Raul Gutierrez, Salvador Lucas, and Rafael Navarro-Marset  

E-Print Network [OSTI]

Proving Termination Properties with mu-term Beatriz Alarc´on, Ra´ul Guti´errez, Salvador Lucas Valencia, Spain Abstract. mu-term is a tool which can be used to verify a number of termination properties of (variants of) Term Rewriting Systems (TRSs): termination of rewriting, termination of innermost rewriting

Lucas, Salvador

94

The Case for UHF-Band MU-MIMO Narendra Anand, Ryan E. Guerra, and Edward W. Knightly  

E-Print Network [OSTI]

-user MIMO (MU- MIMO). In this paper we design and implement the first open MU- MIMO Software-Defined Radio-MIMO performance in both outdoor, indoor, line-of-sight (LOS), and non-line-of-sight (NLOS) environ- ments in UHF bands for high spectral efficiency and low-overhead wireless access. Categories and Subject

95

A classification theorem on Fano bundles Roberto Mu~noz, Gianluca Occhetta, and Luis E. Sola Conde  

E-Print Network [OSTI]

A classification theorem on Fano bundles Roberto Mu~noz, Gianluca Occhetta, and Luis E. Sol´a Conde;2 ROBERTO MU~NOZ, GIANLUCA OCCHETTA, AND LUIS E. SOL´A CONDE (P2) Q3 = LG(1, 3) G(1, 3), (P3) P3 = G(1, 4)Q

Occhetta, Gianluca

96

1. R Aaij ,...,G.Alkhazov et al. First evidence for the decay Bs -> mu+ mu-. CERN-PH-EP-2012-335, LHCB-PAPER-2012-043  

E-Print Network [OSTI]

1 2 3 4 1. R Aaij ,...,G.Alkhazov et al. First evidence for the decay Bs -> mu+ mu-. CERN-PH-EP - + - LHCB-PAPER-2012-033, and B ¯ 0 s D s1 (2536) + -. CERN-PH-EP-2012-327 e-Print: arXiv:1211.1541 [hep-ex]. 4. R Aaij ,...,G.Alkhazov et al. Observation of D0-D0bar oscillations. CERN-PH-EP-2012-333, LHCB

Titov, Anatoly

97

Searches for Lepton Flavor Violation in the Decays tau+- ---> e+- gamma and tau+- ---> mu+- gamma  

SciTech Connect (OSTI)

Searches for lepton-flavor-violating decays of a {tau} lepton to a lighter mass lepton and a photon have been performed with the entire dataset of (963 {+-} 7) x 10{sup 6} {tau} decays collected by the BABAR detector near the {Upsilon}(4S), {Upsilon}(3S) and {Upsilon}(2S) resonances. The searches yield no evidence of signals and they set upper limits on the branching fractions of {Beta}({tau}{sup {+-}} {yields} e{sup {+-}}{gamma}) < 3.3 x 10{sup -8} and {Beta}({tau}{sup {+-}} {yields} {mu}{sup {+-}}{gamma}) < 4.4 x 10{sup -8} at 90% confidence level.

Aubert, Bernard; Karyotakis, Y.; Lees, J.P.; Poireau, V.; Prencipe, E.; Prudent, X.; Tisserand, V.; /Annecy, LAPP; Garra Tico, J.; Grauges, E.; /Barcelona U., ECM; Martinelli, M.; Palano, A.; Pappagallo, M.; /INFN, Bari /Bari U.; Eigen, G.; Stugu, B.; Sun, L.; /Bergen U.; Battaglia, M.; Brown, David Nathan; Hooberman, B.; Kerth, L.T.; Kolomensky, Yu.G.; Lynch, G.; /LBL, Berkeley /UC, Berkeley /Birmingham U. /Ruhr U., Bochum /British Columbia U. /Brunel U. /Novosibirsk, IYF /UC, Irvine /UC, Riverside /UC, San Diego /UC, Santa Barbara /UC, Santa Cruz /Caltech /Cincinnati U. /Colorado U. /Colorado State U. /Dortmund U. /Dresden, Tech. U. /Ecole Polytechnique /Edinburgh U. /INFN, Ferrara /Ferrara U. /INFN, Ferrara /INFN, Ferrara /Ferrara U. /INFN, Ferrara /INFN, Ferrara /Ferrara U. /Frascati /INFN, Genoa /Genoa U. /INFN, Genoa /INFN, Genoa /Genoa U. /INFN, Genoa /INFN, Genoa /Genoa U. /Harvard U. /Heidelberg U. /Humboldt U., Berlin /Imperial Coll., London /Iowa U. /Iowa State U. /Johns Hopkins U. /Orsay, LAL /LLNL, Livermore /Liverpool U. /Queen Mary, U. of London /Royal Holloway, U. of London /Louisville U. /Mainz U., Inst. Kernphys. /Manchester U. /Maryland U. /Massachusetts U., Amherst /MIT, LNS; /more authors.; ,

2010-06-11T23:59:59.000Z

98

Conceptual design of the Mu2e production solenoid cold mass  

SciTech Connect (OSTI)

The Muon-to-Electron conversion experiment (Mu2e), under development at Fermilab, seeks to detect direct muon to electron conversion to provide evidence for a process violating muon and electron lepton number conservation that cannot be explained by the Standard Model of particle physics. The required magnetic field is produced by a series of superconducting solenoids of various apertures and lengths. This paper describes the conceptual design of the 5 T, 4 m long solenoid cold mass with 1.67 m bore with the emphasis on the magnetic, radiation and thermal analyses.

Kashikhin, V.V.; Ambrosio, G.; Andreev, N.; Lamm, M.; Mokhov, N.V.; Nicol, T.H.; Page, T.M.; Pronskikh, V.; /Fermilab

2011-06-01T23:59:59.000Z

99

Optimization of a Mu2e production solenoid heat and radiation shield using MARS15  

SciTech Connect (OSTI)

A Monte-Carlo study of several Mu2e Production Solenoid (PS) absorber (heat shield) versions using the MARS15 code has been performed. Optimizations for material as well as cost (amount of tungsten) have been carried out. Studied are such quantities as the number of displacements per atom (DPA) in the helium-cooled solenoid superconducting coils, power density and dynamic heat load in various parts of the PS and its surrounding structures. Prompt dose, residual dose, secondary particle flux are also simulated in the PS structures and the experimental hall. A preliminary choice of the PS absorber design is made on the ground of these studies.

Pronskikh, V.S.; Mokhov, N.V.; /Fermilab

2011-02-01T23:59:59.000Z

100

J. Phys. B: At. Mol. Phys. 16 (1983) 1595-1603. Printed in Great Britain Atomic orbital expansion study of electron capture in  

E-Print Network [OSTI]

J. Phys. B: At. Mol. Phys. 16 (1983) 1595-1603. Printed in Great Britain Atomic orbital expansion of H+ and Hez+ ions with Li atoms. The calculated total and partial transfer cross sections constitute.1-2.0keVamu-' for HeZ++Li collisions. Total capture cross sections are found to agree well

Lin, Chii-Dong

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


101

Tanikawa C et al. Mol Cancer Res 8: 855-863, 2010. Tanikawa C et al. Cancer Res 69: 8761-9, 2009.  

E-Print Network [OSTI]

p53 p53 30000 p53 Tanikawa C et al. Mol Cancer Res 8: 855-863, 2010. Tanikawa C et al. Cancer Res 69: 8761-9, 2009. Tanikawa C et al.Oncogene 28: 3081-92, 2009. Morioka K et al. Cancer Science 100: 1227-1233, 2009. Kidokoro T et al. Oncogene 27: 1562-1571, 2008

Katsumoto, Shingo

102

{mu}-{tau} symmetry, sterile right-handed neutrinos, and leptogenesis  

SciTech Connect (OSTI)

Leptogenesis is studied in a seesaw model with {mu}-{tau} symmetry for SU{sub L}(2)-singlet right-handed neutrinos. It is shown that lepton asymmetry is not zero and is given by the square of the solar neutrino mass difference and can be of the right order of magnitude. Further it involves the same Majorana phase which appears in the neutrinoless double {beta}-decay. In this framework one of the right-handed seesaw partners of light neutrinos can be made massless. This can be identified with a sterile neutrino, once it acquires a tiny mass ({approx_equal}1 eV) when {mu}-{tau} symmetry is broken in the right-handed neutrino sector. The above mentioned sterile neutrino together with another one can be identified to explain the MiniBooNE and LSND results. The light 5x5 neutrino mass matrix is completely fixed if CP is conserved and so is the effective mass for neutrinoless double {beta}-decay.

Riazuddin [National Centre for Physics, Quaid-i-Azam University, Islamabad (Pakistan)

2008-01-01T23:59:59.000Z

103

Airbreathing Laser Propulsion Experiments with 1 {mu}m Terawatt Pharos IIILaser: Part 2  

SciTech Connect (OSTI)

This basic research study examines the physics of airbreathing laser propulsion at the extreme flux range of 1-2x10{sup 11} W/cm{sup 2}--within the air breakdown threshold for l {mu}m radiation--using the terawatt Pharos III neodymium-glass pulsed laser. Six different experimental setups were employed using a 34 mm line focus with 66 {mu}m focal waist, positioned near the flat impulse surface. The 2nd Campaign investigated impulse generation with the laser beam focused at grazing incidence across near horizontal target surfaces, with pulse energies ranging from 55 to 186 J, and pulse-widths of 2 to 30 ns FWHM. Laser generated impulse was measured with a horizontal Plexiglas registered ballistic pendulum equipped with either a steel target insert or 0.5 Tesla permanent magnet (NEIT-40), to quantify changes in the momentum coupling coefficient (C{sub M}). Part 2 of this 2-part paper covers Campaign no. 2 results including C{sub M} performance data, and long exposure color photos of LP plasma phenomena.

Myrabo, L. N.; Lyons, P. W.; Jones, R. A.; Liu, S. [Department of Mechanical, Aerospace and Nuclear Engineering, Rensselaer Polytechnic Institute, Troy, New York 12180 (United States); Manka, C. [Space Plasma Branch, Plasma Physics Division, Naval Research Laboratory, Washington, D.C. (United States)

2011-11-10T23:59:59.000Z

104

A Circulating Hydrogen Ultra-High Purification System for the MuCap Experiment  

E-Print Network [OSTI]

The MuCap experiment is a high-precision measurement of the rate for the basic electroweak process of muon capture, mu- + p -> n + nu . The experimental approach is based on an active target consisting of a time projection chamber (TPC) operating with pure hydrogen gas. The hydrogen has to be kept extremely pure and at a stable pressure. A Circulating Hydrogen Ultrahigh Purification System was designed at the Petersburg Nuclear Physics Institute (PNPI) to continuously clean the hydrogen from impurities. The system is based on an adsorption cryopump to stimulate the hydrogen flow and on a cold adsorbent for the hydrogen cleaning. It was installed at the Paul Scherrer Institute (PSI) in 2004 and performed reliably during three experiment runs. During several months long operating periods the system maintained the hydrogen purity in the detector on the level of 20 ppb for moisture, which is the main contaminant, and of better than 7 ppb and 5 ppb for nitrogen and oxygen, respectively. The pressure inside the TPC was stabilized to within 0.024% of 10 bar at a hydrogen flow rate of 3 standard liters per minute.

V. A. Ganzha; P. A. Kravtsov; O. E. Maev; G. N. Schapkin; G. G. Semenchuk; V. Trofimov; A. A. Vasilyev; M. E. Vznuzdaev; S. M. Clayton; P. Kammel; B. Kiburg; M. Hildebrandt; C. Petitjean; T. I. Banks; B. Lauss

2007-05-10T23:59:59.000Z

105

Assessment of neutron skyshine near unmodified Accumulator Debuncher storage rings under Mu2e operational conditions  

SciTech Connect (OSTI)

Preliminary plans for providing the proton beam needed by the proposed Mu2e experiment at Fermilab will require the transport of 8 GeV protons to the Accumulator/Debuncher where they be processed into an intensity and time structure useful for the experiment. The intensities involved are far greater that those encountered with antiprotons of the same kinetic energy in the same beam enclosures under Tevatron Collider operational conditions, the operating parameters for which the physical facilities of the Antiproton Source were designed. This note explores some important ramifications of the proposed operation for radiation safety and demonstrates the need for extensive modifications of significant portions of the shielding of the Accumulator Debuncher storage rings; notably that underneath the AP Service Buildings AP10, AP30, and AP50. While existing shielding is adequate for the current operating mode of the Accumulator/Debuncher as part of the Antiproton Source used in the Tevatron Collider program, without significant modifications of the shielding configuration in the Accumulator/Debuncher region and/or beam loss control systems far more effective than seen in most applications at Fermilab, the proposed operational mode for Mu2e is not viable for the following reasons: 1. Due to skyshine alone, under normal operational conditions large areas of the Fermilab site would be exposed to unacceptable levels of radiation where most of the Laboratory workforce and some members of the general public who regularly visit Fermilab would receive measurable doses annually, contrary to workforce, public, and DOE expectations concerning the As Low as Reasonably Achievable (ALARA) principle. 2. Under normal operational conditions, a sizeable region of the Fermilab site would also require fencing due to skyshine. The size of the areas involved would likely invite public inquiry about the significant and visible enlargement of Fermilab's posted radiological areas. 3. There would be aesthetics questions about the employment of so much new fencing on the Fermilab site. 4. The assumption of only 1.0% 'normal condition' beam losses over the three locations is regarded as being extremely optimistic. Thus, it is evident that it is necessary to pursue shielding improvements to support viable operation of the Mu2e experiment.

Cossairt, J.Donald; /Fermilab

2010-12-01T23:59:59.000Z

106

Energy transfer and 1.54 {mu}m emission in amorphous silicon nitride films  

SciTech Connect (OSTI)

Er-doped amorphous silicon nitride films with various Si concentrations (Er:SiN{sub x}) were fabricated by reactive magnetron cosputtering followed by thermal annealing. The effects of Si concentrations and annealing temperatures were investigated in relation to Er emission and excitation processes. Efficient excitation of Er ions was demonstrated within a broad energy spectrum and attributed to disorder-induced localized transitions in amorphous Er:SiN{sub x}. A systematic optimization of the 1.54 {mu}m emission was performed and a fundamental trade-off was discovered between Er excitation and emission efficiency due to excess Si incorporation. These results provide an alternative approach for the engineering of sensitized Si-based light sources and lasers.

Yerci, S.; Li, R. [Department of Electrical and Computer Engineering, Boston University, 8 Saint Mary's Street, Boston, Massachusetts 02215-2421 (United States); Kucheyev, S. O.; Buuren, T. van [Lawrence Livermore National Laboratory, Livermore, California 94551 (United States); Basu, S. N. [Division of Materials Science and Engineering, Boston University, 15 Saint Mary's Street, Brookline, Massachusetts 02446 (United States); Department of Mechanical Engineering, Boston University, 110 Cummington Street, Boston, Massachusetts 02215 (United States); Dal Negro, L. [Department of Electrical and Computer Engineering, Boston University, 8 Saint Mary's Street, Boston, Massachusetts 02215-2421 (United States); Division of Materials Science and Engineering, Boston University, 15 Saint Mary's Street, Brookline, Massachusetts 02446 (United States)

2009-07-20T23:59:59.000Z

107

Studies of Nu-mu to Nu-e Oscillation Appearance in the MINOS Experiment  

SciTech Connect (OSTI)

The MINOS experiment uses a long baseline neutrino beam, measured 1 km downstream from its origin in the Near Detector at Fermilab, and 734 km later in the large underground Far Detector in the Soudan mine. By comparing these two measurements, MINOS can probe the atmospheric domain of the neutrino oscillation phenomenology with unprecedented precision. Besides the ability to perform a world leading determination of the {Delta}m{sub 23}{sup 2} and {theta}{sub 23} parameters, via {nu}{sub {mu}} flux disappearance, MINOS has the potential to make a leading measurement of {nu}{sub {mu}} {yields} {nu}{sub e} oscillations in the atmospheric sector by looking for {nu}{sub e} appearance at the Far Detector. The observation of {nu}{sub e} appearance, tantamount to establishing a non-zero value of the {theta}{sub 13} mixing angle, opens the way to studies of CP violation in the leptonic sector, the neutrino spectral mass pattern ordering and neutrino oscillations in matter, the driving motivations of the next generation of neutrino experiments. In this thesis, we study the MINOS potential for measuring {theta}{sub 13} in the context of the MINOS Mock Data Challenge using a multivariate discriminant analysis method. We show the method's validity in the application to {nu}{sub e} event classification and background identification, as well as in its ability to identify a {nu}{sub e} signal in a Mock Data sample generated with undisclosed parameters. An independent shower reconstruction method based on three-dimensional hit matching and clustering was developed, providing several useful discriminator variables used in the multivariate analysis method. We also demonstrate that within 2 years of running, MINOS has the potential to improve the current best limit on {theta}{sub 13}, from the CHOOZ experiment, by a factor of 2.

Pereira e Sousa, Alexandre Bruno; /Tufts U.

2005-12-01T23:59:59.000Z

108

Water vapor on supergiants. The 12 micron TEXES spectra of mu Cephei  

E-Print Network [OSTI]

Several recent papers have argued for warm, semi-detached, molecular layers surrounding red giant and supergiant stars, a concept known as a MOLsphere. Spectroscopic and interferometric analyses have often corroborated this general picture. Here, we present high-resolution spectroscopic data of pure rotational lines of water vapor at 12 microns for the supergiant mu Cephei. This star has often been used to test the concept of molecular layers around supergiants. Given the prediction of an isothermal, optically thick water-vapor layer in Local Thermodynamic Equilibrium around the star (MOLsphere), we expected the 12 micron lines to be in emission or at least in absorption but filled in by emission from the molecular layer around the star. Our data, however, show the contrary; we find definite absorption. Thus, our data do not easily fit into the suggested isothermal MOLsphere scenario. The 12 micron lines, therefore, put new, strong constraints on the MOLsphere concept and on the nature of water seen in signatures across the spectra of early M supergiants. We also find that the absorption is even stronger than that calculated from a standard, spherically symmetric model photosphere without any surrounding layers. A cool model photosphere, representing cool outer layers is, however, able to reproduce the lines, but this model does not account for water vapor emission at 6 microns. Thus, a unified model for water vapor on mu Cephei appears to be lacking. It does seem necessary to model the underlying photospheres of these supergiants in their whole complexity. The strong water vapor lines clearly reveal inadequacies of classical model atmospheres.

N. Ryde; M. J. Richter; G. M. Harper; K. Eriksson; D. L. Lambert

2006-03-15T23:59:59.000Z

109

A precision measurement of the branching ratio K{sup +} {r_arrow} {pi}{sup +}{pi}{sup 0}/K{sup +} {r_arrow} {mu}{sup +}{nu}{sub {mu}}  

SciTech Connect (OSTI)

A measurement of the branching ratio K{sup +} {r_arrow} {pi}{sup +}{pi}{sup 0}/K{sup +} {r_arrow} {mu}{sup +}{nu}{sub {mu}} was made using stopped kaons from p{anti p} annihilations at rest and a magnetic spectrometer to measure the momenta of the charged decay product to the 1% to 1.5% level. The determination is based on 45,500 events passing final data cuts. The resulting ratio is .3329 {+-} .0047 (statistical) {+-} .0010 (systematic).

Usher, T.; Fero, M.; Gee, M.; Graf, N.A.; Mandelkern, M.; Shultz, D.; Schultz, J.

1991-08-01T23:59:59.000Z

110

Optical losses of Al-free lasers for {lambda}=0.808 and 0.98 {mu}m  

SciTech Connect (OSTI)

In this work, we study the origin of the optical losses in Al-free InGaAsP/GaAs ({lambda}=0.808 {mu}m) and InGaAs/GaAs/InGaP ({lambda}=0.980 {mu}m) lasers. Theoretical modeling and the experimental results indicate that the scattering of the laser beam by refractive index fluctuation in the alloys is the dominant loss in our lasers, and the loss due to the free-carrier absorption and scattering by interface roughness are negligible. {copyright} {ital 1996 American Institute of Physics.}

Yi, H.; Diaz, J.; Lane, B.; Razeghi, M. [Center for Quantum Devices, Northwestern University, Evanston, Illinois 60208 (United States)] [Center for Quantum Devices, Northwestern University, Evanston, Illinois 60208 (United States)

1996-11-01T23:59:59.000Z

111

New building blocks for the ALICE SDD readout and Detector Control System in a commercial 0.25 $\\mu$ m CMOS technology  

E-Print Network [OSTI]

New building blocks for the ALICE SDD readout and Detector Control System in a commercial 0.25 $\\mu$ m CMOS technology

Rivetti, A; Idzik, M; Rotondo, F

2001-01-01T23:59:59.000Z

112

Revisiting the relationship between 6 {\\mu}m and 2-10 keV continuum luminosities of AGN  

E-Print Network [OSTI]

We have determined the relation between the AGN luminosities at rest-frame 6 {\\mu}m associated to the dusty torus emission and at 2-10 keV energies using a complete, X-ray flux limited sample of 232 AGN drawn from the Bright Ultra-hard XMM-Newton Survey. The objects have X-ray luminosities corrected for intrinsic absorption between 10^42 and 10^46 erg/s and redshifts from 0.05 to 2.8. The rest-frame 6 {\\mu}m luminosities were computed using data from the Wide-Field Infrared Survey Explorer and are based on a spectral energy distribution decomposition into AGN and galaxy emission. The best-fit relationship for the full sample is consistent with being linear, L_6 {\\mu}m $\\propto$ L_2-10 keV^0.99$\\pm$0.032, but has significant intrinsic scatter, ~0.35 dex in log L_6 {\\mu}m. Assuming a constant X-ray bolometric correction, the fraction of AGN bolometric luminosity reprocessed in the mid-IR decreases weakly, if at all, with the AGN luminosity, a finding at odds with simple receding torus models. Type 2 AGN have re...

Mateos, S; Alonso-Herrero, A; Rovilos, E; Hernán-Caballero, A; Barcons, X; Blain, A; Caccianiga, A; Della Ceca, R; Severgnini, P

2015-01-01T23:59:59.000Z

113

On rank 2 vector bundles on Fano manifolds Roberto Mu~noz, Gianluca Occhetta, and Luis E. Sola Conde  

E-Print Network [OSTI]

On rank 2 vector bundles on Fano manifolds Roberto Mu~noz, Gianluca Occhetta, and Luis E. Sol´a~NOZ, GIANLUCA OCCHETTA, AND LUIS E. SOL´A CONDE setting of rank two vector bundles on Fano manifolds of Picard

Occhetta, Gianluca

114

SPITZER 24 {mu}m EXCESSES FOR BRIGHT GALACTIC STARS IN BOOeTES AND FIRST LOOK SURVEY FIELDS  

SciTech Connect (OSTI)

Optically bright Galactic stars (V {approx}< 13 mag) having f {sub {nu}}(24 {mu}m) > 1 mJy are identified in Spitzer mid-infrared surveys within 8.2 deg{sup 2} for the Booetes field of the NOAO Deep Wide-Field Survey and within 5.5 deg{sup 2} for the First Look Survey (FLS). One hundred and twenty-eight stars are identified in Booetes and 140 in the FLS, and their photometry is given. (K - [24]) colors are determined using K magnitudes from the Two Micron All Sky Survey for all stars in order to search for excess 24 {mu}m luminosity compared to that arising from the stellar photosphere. Of the combined sample of 268 stars, 141 are of spectral types F, G, or K, and 17 of these 141 stars have 24 {mu}m excesses with (K - [24]) > 0.2 mag. Using limits on absolute magnitude derived from proper motions, at least eight of the FGK stars with excesses are main-sequence stars, and estimates derived from the distribution of apparent magnitudes indicate that all 17 are main-sequence stars. These estimates lead to the conclusion that between 9% and 17% of the main-sequence FGK field stars in these samples have 24 {mu}m infrared excesses. This result is statistically similar to the fraction of stars with debris disks found among previous Spitzer targeted observations of much brighter, main-sequence field stars.

Hovhannisyan, L. R.; Mickaelian, A. M. [Byurakan Astrophysical Observatory and Isaac Newton Institute of Chile Armenian Branch, 378433, Byurakan, Aragatzotn Province (Armenia); Weedman, D. W.; Houck, J. R. [Astronomy Department, Cornell University, Ithaca, NY 14853 (United States); Le Floc'h, E. [Steward Observatory, University of Arizona, Tucson, AZ, 85721 (United States); Soifer, B. T. [Spitzer Science Center, California Institute of Technology, 220-6, Pasadena, CA 91125 (United States); Brand, K. [Space Telescope Science Institute, 3700 San Martin Dr., Baltimore, MD 21218 (United States); Dey, A.; Jannuzi, B. T. [National Optical Astronomy Observatory, 950 N. Cherry Ave., Tucson, AZ 85719 (United States)], E-mail: lilithov11@yahoo.com, E-mail: dweedman@isc.astro.cornell.edu

2009-07-15T23:59:59.000Z

115

The source of widespread 3-$\\mu$m absorption in Jupiter's clouds: Constraints from 2000 Cassini VIMS observations  

E-Print Network [OSTI]

The Cassini flyby of Jupiter in 2000 provided spatially resolved spectra of Jupiter's atmosphere using the Visual and Infrared Mapping Spectrometer (VIMS). These spectra contain a strong absorption at wavelengths from about 2.9 $\\mu$m to 3.1 $\\mu$m, previously noticed in a 3-$\\mu$m spectrum obtained by the Infrared Space Observatory (ISO) in 1996. While Brooke et al. (1998, Icarus 136, 1-13) were able to fit the ISO spectrum very well using ammonia ice as the sole source of particulate absorption, Sromovsky and Fry (2010, Icarus 210, 211-229), using significantly revised NH$_3$ gas absorption models, showed that ammonium hydrosulfide (NH$_4$SH) provided a better fit to the ISO spectrum than NH$_3$ , but that the best fit was obtained when both NH$_3$ and NH$_4$SH were present. Although the large FOV of the ISO instrument precluded identification of the spatial distribution of these two components, the VIMS spectra at low and intermediate phase angles show that 3-$\\mu$m absorption is present in zones and belts...

Sromovsky, Lawrence

2015-01-01T23:59:59.000Z

116

Thermonuclear yield of targets under the action of high-power short-wavelength (lambda< or =1. mu. ) lasers  

SciTech Connect (OSTI)

A unified optimization scheme is used in a numerical calculation of the dependences of the thermonuclear yield of two-layer shell targets on the absorbed laser energy in the range 0.3--10 mJ for lasers emitting radiation of wavelengths shorter than 1 ..mu...

Basov, N.G.; Gus'kov, S.Y.; Danilova, G.V.; Demchenko, N.N.; Zmitrenko, N.V.; Karpov, V.Y.; Mishchenko, T.V.; Rozanov, V.B.; Samarskii, A.A.

1985-06-01T23:59:59.000Z

117

INFRARED LUMINOSITIES AND AROMATIC FEATURES IN THE 24 {mu}m FLUX-LIMITED SAMPLE OF 5MUSES  

SciTech Connect (OSTI)

We study a 24 {mu}m selected sample of 330 galaxies observed with the infrared spectrograph for the 5 mJy Unbiased Spitzer Extragalactic Survey. We estimate accurate total infrared luminosities by combining mid-IR spectroscopy and mid-to-far infrared photometry, and by utilizing new empirical spectral templates from Spitzer data. The infrared luminosities of this sample range mostly from 10{sup 9} L{sub sun} to 10{sup 13.5} L{sub sun}, with 83% in the range 10{sup 10} L{sub sun} < L{sub IR} < 10{sup 12} L{sub sun}. The redshifts range from 0.008 to 4.27, with a median of 0.144. The equivalent widths of the 6.2 {mu}m aromatic feature have a bimodal distribution, probably related to selection effects. We use the 6.2 {mu}m polycyclic aromatic hydrocarbon equivalent width (PAH EW) to classify our objects as starburst (SB)-dominated (44%), SB-AGN composite (22%), and active galactic nucleus (AGN)-dominated (34%). The high EW objects (SB-dominated) tend to have steeper mid-IR to far-IR spectral slopes and lower L{sub IR} and redshifts. The low EW objects (AGN-dominated) tend to have less steep spectral slopes and higher L{sub IR} and redshifts. This dichotomy leads to a gross correlation between EW and slope, which does not hold within either group. AGN-dominated sources tend to have lower log(L{sub PAH7.7{sub {mu}m}}/L{sub PAH11.3{sub {mu}m}}) ratios than star-forming galaxies, possibly due to preferential destruction of the smaller aromatics by the AGN. The log(L{sub PAH7.7{sub {mu}m}}/L{sub PAH11.3{sub {mu}m}}) ratios for star-forming galaxies are lower in our sample than the ratios measured from the nuclear spectra of nearby normal galaxies, most probably indicating a difference in the ionization state or grain size distribution between the nuclear regions and the entire galaxy. Finally, we provide a calibration relating the monochromatic continuum or aromatic feature luminosity to L{sub IR} for different types of objects.

Wu Yanling; Helou, George; Shi Yong, E-mail: yanling@ipac.caltech.ed, E-mail: gxh@ipac.caltech.ed, E-mail: yong@ipac.caltech.ed [Infrared Processing and Analysis Center, California Institute of Technology, 1200 East California Boulevard, Pasadena, CA 91125 (United States)

2010-11-01T23:59:59.000Z

118

CONSTRAINING EXPLOSION TYPE OF YOUNG SUPERNOVA REMNANTS USING 24 {mu}m EMISSION MORPHOLOGY  

SciTech Connect (OSTI)

Determination of the explosion type of supernova remnants (SNRs) can be challenging, as SNRs are hundreds to thousands of years old and supernovae are classified based on spectral properties days after explosion. Previous studies of thermal X-ray emission from Milky Way and Large Magellanic Cloud SNRs have shown that Type Ia and core-collapse (CC) SNRs have statistically different symmetries, and thus these sources can be typed based on their X-ray morphologies. In this Letter, we extend the same technique, a multipole expansion technique using power ratios, to infrared (IR) images of SNRs to test whether they can be typed using the symmetry of their warm dust emission as well. We analyzed archival Spitzer Space Telescope Multiband Imaging Photometer 24 {mu}m observations of the previously used X-ray sample, and we find that the two classes of SNRs separate according to their IR morphologies. The Type Ia SNRs are statistically more circular and mirror symmetric than the CC SNRs, likely due to the different circumstellar environments and explosion geometries of the progenitors. Broadly, our work indicates that the IR emission retains information of the explosive origins of the SNR and offers a new method to type SNRs based on IR morphology.

Peters, Charee L.; Stassun, Keivan G. [Department of Physics, Fisk University, 1000 17th Ave N Nashville, TN 37208 (United States); Lopez, Laura A.; Figueroa-Feliciano, Enectali [MIT-Kavli Institute for Astrophysics and Space Research, 77 Massachusetts Avenue, 37-664H, Cambridge, MA 02139 (United States); Ramirez-Ruiz, Enrico, E-mail: charee.l.peters@vanderbilt.edu [Department of Astronomy and Astrophysics, University of California Santa Cruz, 1156 High Street, Santa Cruz, CA 95060 (United States)

2013-07-10T23:59:59.000Z

119

THE LEGACY OF SCUPOL: 850 {mu}m IMAGING POLARIMETRY FROM 1997 TO 2005  

SciTech Connect (OSTI)

SCUPOL, the polarimeter for SCUBA on the James Clerk Maxwell Telescope, was the most prolific thermal imaging polarimeter built to date. Between 1997 and 2005, observations of 104 regions were made at 850 {mu}m in the mapping mode. The instrument has produced {approx}50 refereed journal publications, and that number is still growing. We have systematically re-reduced all imaging polarimetry made in the standard 'jiggle-map' mode from the SCUBA archive (2800+ individual observations) to produce a catalog of SCUPOL images and tables. We present the results of our analysis with figures and data tables produced for all 83 regions where significant polarization was detected. In addition, the reduced data cubes and data tables can be accessed online. In many cases, the data included in this paper have been previously published elsewhere. However, this publication includes unpublished data sets, in whole or in part, toward 39 regions, including cores in {rho} Ophiuchus, Orion's OMC-2 region, several young stellar objects, and the galaxy M87.

Matthews, Brenda C.; McPhee, Christie A.; Fissel, Laura M. [Herzberg Institute of Astrophysics, National Research Council of Canada, 5071 W. Saanich Road, Victoria, BC V9E 2E7 (Canada); Curran, Rachel L. [Dublin Institute for Advanced Studies, 31 Fitzwilliam Place, Dublin 2 (Ireland)], E-mail: brenda.matthews@nrc-cnrc.gc.ca

2009-05-15T23:59:59.000Z

120

An Estimate of Out of Time Beam Upon Extraction for Mu2e  

SciTech Connect (OSTI)

For future experiments at the intensity frontier precise and accurate knowledge of beam time structure will be critical to understanding backgrounds. The proposed Mu2e experiment calls for {approx} 200ns (FW, 40 ns rms) bunches of 3 x 10{sup 7} 8 GeV protons and a bunch spacing of 1695 ns. The interbunch beam must be suppressed from the main pulse by a factor of 10{sup -10}, this is known as the beam extinction requirement. Beam from Fermilab's Booster will be formed into 2.5 MHz buckets in the Fermilab Recycler then transferred to the Delivery Ring (formerly the Debuncher) and slow spilled from a single filled bucket in an h = 4 RF system. Because the final extinction level is not expected from the Delivery Ring an AC dipole and collimation system will be used to achieve final extinction. Here I present calculations leading to a first estimate of the extinction level expected upon extraction from the Delivery Ring of {le} 3.36 x 10{sup -4}. Intrabunch, residual gas scattering and scattering off the extraction septum are included. Contributions from bunch formation are not considered.

Prebys, E.; /Fermilab; Evans, N.J.; Kopp, S.E.; /Texas U.

2012-05-01T23:59:59.000Z

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
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We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


121

Commissioning report of the MuCool 5 Tesla solenoid coupled with helium refrigerator  

SciTech Connect (OSTI)

MuCool 5T solenoid was successfully cooled down and operated coupled with MTA 'Brown' refrigerator. The system performed as designed with substantial performance margin. All process alarms and interlocks, as well as ODH and fire alarms, were active and performed as designed. The cooldown of the refrigerator started from warm conditions and took 44 hours to accumulate liquid helium level and solenoid temperature below 5K. Average liquid nitrogen consumption for the refrigerator precool and solenoid shield was measured as 20 gal/hr (including boil-off). Helium losses were small (below 30 scfh). The system was stable and with sufficient margin of performance and ran stably without wet expansion engine. Quench response demonstrated proper operation of the relieving devices and pointed to necessity of improving tightness of the relieving manifolds. Boil-off test demonstrated average heat load of 3 Watts for the unpowered solenoid. The solenoid can stay up to 48 hours cold and minimally filled if the nitrogen shield is maintained. A list of improvements includes commencing into operations the second helium compressor and completion of improvements and tune-ups for system efficiency.

Geynisman, Michael; /Fermilab

2010-05-01T23:59:59.000Z

122

Radiation and thermal analysis of production solenoid for Mu2e experimental setup  

SciTech Connect (OSTI)

The Muon-to-Electron (Mu2e) experiment at Fermilab, will seek the evidence of direct muon to electron conversion at the sensitivity level where it cannot be explained by the Standard Model. An 8-GeV 25-kW proton beam will be directed onto a tilted gold target inside a large-bore superconducting Production Solenoid (PS) with the peak field on the axis of {approx}5T. The negative muons resulting from the pion decay will be captured in the PS aperture and directed by an S-shaped Transport Solenoid towards the stopping target inside the Detector Solenoid. In order for the superconducting magnets to operate reliably and with a sufficient safety margin, the peak neutron flux entering the coils must be reduced by 3 orders of magnitude that is achieved by means of a sophisticated absorber placed in the magnet aperture. The proposed absorber, consisting of W- and Cu-based alloy parts, is optimized for the performance and cost. Results of MARS15 simulations of energy deposition and radiation are reported. The results of the PS magnet thermal analysis, coordinated with the coil cooling scheme, are reported as well for the selected absorber design.

Pronskikh, V.S.; Kashikhin, V.V.; Mokhov, N.V.; /Fermilab

2011-03-01T23:59:59.000Z

123

Optimization of Extinction Efficiency in the 8-GeV Mu2e Beam Line  

SciTech Connect (OSTI)

A muon-to-electron conversion experiment at Fermilab, Mu2e, is being designed to probe for new physics beyond the standard model at mass scales up to 10{sup 4} TeV. For this experiment, the advance in experimental sensitivity will be four orders of magnitude when compared to existing data on charged lepton flavor violation. The muon beam will be produced by delivering a proton beam contained in short 100-ns bunches onto a muon production target, with an inter-bunch separation of about 1700 ns. A critical requirement of the experiment is to ensure a low level of background at the muon detector consistent with the required sensitivity. To meet the sensitivity requirement, protons that reach the target between bunches must be suppressed by an enormous factor, so that an extinction factor, defined as a number of background protons between main bunches per proton in such a bunch, should not exceed 10{sup -9}. This paper describes the advanced beam optics and results of numerical modeling with STRUCT and MARS codes for a beam line with a collimation system that allows us to achieve the experimental extinction factor of one per billion.

Rakhno, I.L.; Drozhdin, A.I.; Johnstone, C.; Mokhov, N.V.; Prebys, E.; /Fermilab

2012-05-11T23:59:59.000Z

124

Copyright 2002 by the Genetics Society of America Maize Mu Transposons Are Targeted to the 5 Untranslated Region of the gl8  

E-Print Network [OSTI]

Untranslated Region of the gl8 Gene and Sequences Flanking Mu Target-Site Duplications Exhibit Nonrandom. Analysis of 79 independently isolated Mu-induced alleles at the gl8 locus established that at least 75 are located in the 5 untranslated region (UTR) of the gl8 gene. Ten positions within the 5 UTR experienced

Schnable, Patrick S.

125

Effect of active layer thickness on differential quantum efficiency of 1. 3 and 1. 55. mu. m InGaAsP injection lasers  

SciTech Connect (OSTI)

The dependence of differential quantum efficiency (eta/sub d/) on active layer thickness (d) for 1.3 and 1.55 ..mu..m InGaAsP buried crescent (BC) injection lasers has been measured. A comparison of the results shows that eta/sub d/ for 1.55 ..mu..m lasers increases more rapidly with decreasing d than eta/sub d/ for 1.3 ..mu..m lasers. The significantly different dependence of eta/sub d/ on d in BC lasers suggests that the optical absorption in the active region of InGaAsP lasers is strongly wavelength dependent. This gives the important practical conclusion that the eta/sub d/ for 1.55 ..mu..m lasers can be significantly improved by reducing d, whereas the eta/sub d/ for 1.3 ..mu..m lasers can only be slightly improved by reducing d. As a result of eta/sub d/ vs d investigation, we have obtained high performance 1.3 and 1.55 ..mu..m BC lasers which exhibit threshold currents as low as 9 mA at 25 /sup 0/C, high-temperature operation (up to 100 /sup 0/C), and eta/sub d/ over 65% (1.3 ..mu..m) and 45% (1.55 ..mu..m).

Cheng, W.H.; Su, C.B.; Renner, D.

1987-07-06T23:59:59.000Z

126

Water in Emission in the ISO Spectrum of the Early M Supergiant Star mu Cephei  

E-Print Network [OSTI]

We report a detection of water in emission in the spectrum of the M2 supergiant atar mu Cep (M2Ia) observed by the Short Wavelength Spectrometer (SWS) aboard Infrared Space Observatory (ISO) and now released as the ISO Archives. The emission first appears in the 6 micron region (nu2 fundamental) and then in the 40 micron region (pure rotation lines) despite the rather strong dust emission. The intensity ratios of the emission features are far from those of the optically thin gaseous emission. Instead, we could reproduce the major observed emission features by an optically thick water sphere of the inner radius about two stellar radii (1300Rsun), Tex = 1500K, and Ncol (H2O) = 3.0E+20/cm2. This model also accounts for the H2O absorption bands in the near infrared (1.4, 1.9, and 2.7 micron) as well. The detection of water in emission provides strong constraints on the nature of water in the early M supergiant stars, and especially its origin in the outer atmosphere is confirmed against other models such as the large convective cell model. We finally confirm that the early M supergiant star is surrounded by a huge optically thick sphere of the warm water vapor, which may be referred to as MOLsphere for simplicity. Thus, the outer atmosphere of M supergiant stars should have a complicated hierarchical and/or hybrid structure with at least three major constituents including the warm MOLsphere (T about 1.0E+3K) together with the previously known hot chromosphere (T about 1.0E+4K) and cool expanding gas-dust envelope (T about 1.0E+2K).

T. Tsuji

2000-08-03T23:59:59.000Z

127

The 10 $\\mu$m infrared band of silicate dust: A laboratory study comparing the aerosol and KBr pellet techniques  

E-Print Network [OSTI]

The profile of the silicate 10 $\\mu$m IR band contains important information about the evolutional stage of dust in circumstellar environments and the possible ongoing process of planetesimal formation. In order to extract this information, the observed band profiles are compared with calculated or laboratory-measured absorption cross sections of amorphous and crystalline grains with different sizes and compositions. We present in this study the first laboratory measurements of the 10 $\\mu$m band profiles of nonembedded, i.e. free-flying, particles of amorphous and crystalline Mg$_2$SiO$_4$ (with two different particle shapes), amorphous and crystalline MgSiO$_3$, and crystalline olivine. We compare the spectra with those measured on embedded grains and discuss the potential of the new experimental method for comparison with observed spectra, as well as for future studies of agglomeration and surface manipulation of the grains.

Tamanai, A; Blum, J; Meeus, G

2006-01-01T23:59:59.000Z

128

Results of the LSND search for {ovr {nu}}{sub {mu}} {yields} {ovr {nu}}{sub e} oscillations  

SciTech Connect (OSTI)

A search for {ovr {nu}}{sub {mu}}{yields}{ovr {nu}}{sub e} oscillations has been conducted at the Los Alamos Meson Physics Facility by using {ovr {nu}}{sub {mu}} from {mu}{sup +} decay at rest. The {ovr {nu}}{sub e} are detected via the reaction {ovr {nu}}{sub e}p {yields} e{sup +} n , correlated with a {gamma} from np {yields} d{gamma} (2.2 MeV). The use of tight cuts to identify e{sup +} events with correlated {gamma} rays yields 22 events with e{sup +} energy between 36 and 60 MeV and only 4.6 {plus_minus} 0.6 background events. The probability that this observation can be explained by statistical fluctuation is less than 10{sup -7}. Assuming these events are due to oscillations, a likelihood fit to all the e{sup +} events between 20 and 60 MeV has been performed to extract the oscillation parameters sin{sup 2} 2{theta} and {Delta}m{sup 2}. The favored region resulting from this fit is shown.

Federspiel, F.J.

1996-07-01T23:59:59.000Z

129

Experiment to investigate anti. nu. /sub. mu. /. -->. anti. nu. /sub e/ oscillations at Los Alamos Meson Physics Facility  

SciTech Connect (OSTI)

An experiment, being planned at LAMPF, aims to investigate a possible neutrino oscillation channel, anti ..nu../sub ..mu../ ..-->.. anti ..nu../sub e/. If anti ..nu../sub ..mu../, produced in the LAMPF beam stop, oscillate to anti ..nu../sub e/, then interactions anti ..nu../sub e/ + p ..-->.. e/sup +/ + n, may be detected. A large volume liquid scintillator (4470 liter) emplaced at 33 m from the beam stop, detects e/sup +/ and n, after moderation in the hydrogenous liquid and capture in Gd, loaded into the scintillator. Our anticipated signal rate is currently estimated at 1.67 (sigma m/sup 2/)/sup 2//day assuming full amplitude oscillation. The corresponding counting rate, assuming all anti ..nu../sub ..mu../ have oscillated to anti ..nu../sub e/ at the detector is 1.5/day. Cosmic rates are estimated at 0.033/day. Correlated backgrounds from the beam stop are calculated to be small in comparison to cosmic events, except for reactions of ..nu../sub e/ in Pb. These reactions may be reduced with an Fe shield within the detector. With the above rate, a limit on the sensitivity of our experiment for the value of sigma m/sup 2/ is estimated at 0.12 eV/sup 2/ with 70 days of counting. Detector features, estimated background rates, and sensitivity values are discussed.

Kruse, H.W.; Toevs, J.W.

1981-01-01T23:59:59.000Z

130

Search for excited and exotic muons in the mu gamma decay channel in p anti-p collisions at s**(1/2) = 1.96-TeV  

SciTech Connect (OSTI)

The authors present a search for excited and exotic muon states {mu}*, conducted using an integrated luminosity of 371 pb{sup -1} of data collected in p{bar p} collisions at {radical}s = 1.96 TeV at the Tevatron with the CDF II detector. They search for associated production of {mu}{mu}* followed by the decay {mu}* {yields} {mu}{gamma}, resulting in the {mu}{mu}{gamma} final state. They compare the data to model predictions as a function of the mass of the excited muon M{sub {mu}*}, the compositeness energy scale {Lambda}, and the gauge coupling factor f. No signal above the standard model expectation is observed in the {mu}{gamma} mass spectrum. In the contact interaction model, they exclude 107 < M{sub {mu}*} < 853 GeV/c{sup 2} for {Lambda} = M{sub {mu}*}; in the gauge-mediated model, they exclude 100 < M{sub {mu}*} < 410 GeV/c{sup 2} for f/{Lambda} = 10{sup -2} GeV{sup -1}. These 95% confidence level exclusions extend previous limits and are the first hadron collider results on {mu}* production in the gauge-mediated model.

Abulencia, A.; Acosta, D.; Adelman, Jahred A.; Affolder, T.; Akimoto, T.; Albrow, M.G.; Ambrose, D.; Amerio, S.; Amidei, D.; Anastassov, A.; Anikeev, K.; /Taiwan, Inst.

2006-06-01T23:59:59.000Z

131

1. R Aaij ,...,G.Alkhazov et al. First evidence for the decay Bs -> mu+ mu-. CERN-PH-EP-2012-335, LHCB-PAPER-2012-043  

E-Print Network [OSTI]

+ mu-. CERN-PH-EP-2012-335, LHCB-PAPER- 2012-043 e-Print: arXiv:1211.2674 [hep-ex]. 2. V.M. Abazov B ¯ 0 (s) D + s K - + - LHCB-PAPER-2012-033, and B ¯ 0 s D s1 (2536) + -. CERN-PH-EP-2012-327 e-Print: arXiv:1211.1541 [hep-ex]. 4. R Aaij ,...,G.Alkhazov et al. Observation of D0-D0bar oscillations. CERN-PH-EP

Titov, Anatoly

132

12/19/07 3:38 PMGlaser Baseball Article -MU College of Arts and Science Research Communication Project Page 1 of 1http://rcp.missouri.edu/articles/glaser-baseball.html  

E-Print Network [OSTI]

12/19/07 3:38 PMGlaser Baseball Article - MU College of Arts and Science Research Communication Project Page 1 of 1http://rcp.missouri.edu/articles/glaser-baseball.html skip navigation home the archives faculty services arts & science departments college of arts & science mu campus MU professor available

Glaser, Rainer

133

Wavelength dependence of characteristics of 1. 2-1. 55. mu. m InGaAsP/InP P-substrate buried crescent laser diodes  

SciTech Connect (OSTI)

Various wavelength laser diodes with p-substrate buried crescent (PBC) structure have been fabricated at 1.2-1.55 ..mu..m. The dependences of laser characteristics on wavelength have been measured. Up to 70/sup 0/C, the increasing rates of the threshold current with temperature of these lasers are similar, while, above 70/sup 0/C, a shorter wavelength laser shows a larger increasing rate. At the same full width at half maximum of the far-field pattern perpendicular to the junction plane, the external differential quantum efficiency of 1.55 ..mu..m laser diode is found to be only 10 percent smaller than that of the 1.3 ..mu..m laser. The absorption loss coefficients in the active layer of 1.2, 1.3, and 1.55 ..mu..m laser are estimated to be 26, 34, and 73 cm/sup -1/, respectively.

Kakimoto, S.; Takemoto, A.; Sakakibara, Y.; Nakajima, Y.; Fujiwara, M.; Namizaki, H.; Higuchi, H.; Yamamoto, Y.

1988-01-01T23:59:59.000Z

134

Absorption, emission, and gain spectra of 1. 3. mu. m InGaAsP quaternary lasers  

SciTech Connect (OSTI)

The spontaneous emission spectrum of mesa lasers was analyzed to determine the absorption and gain spectra at threshold. The radiative current density at threshold was found to be 4.4 kA cm/sup -2/ ..mu..m/sup -1/, which is 60 percent of the total current density for the lowest threshold mesa laser. The increase in radiative lifetime due to reabsorption of emitted radiation was calculated to be 1.5, using the measured absorption and emission spectra. Contrary to other studies, this investigation of an LED and 3 lasers of different types yielded no evidence of carrier heating.

Henry, C.H.; Logan, R.A.; Merritt, F.R.; Temkin, H.

1983-06-01T23:59:59.000Z

135

Selective enhancement of the 251-. mu. m line in an optically pumped CH/sub 3/OH laser  

SciTech Connect (OSTI)

To obtain a high output power on the 251-..mu..m line of a CH/sub 3/OH laser, four types of far-infrared output mirror are examined. It is found that the capacitive aluminium-mesh mirror of the Danielewicz type, which is fabricated by conventional vacuum deposition techniques in the present work, selectively extracts an output power of 18 mW from a 25-W pump. Also, exact assignment of the line is achieved by tuning the far-infrared cavity using the mirror.

Sakurai, T.

1983-02-15T23:59:59.000Z

136

FOUR DECADES OF IRC +10216: EVOLUTION OF A CARBON-RICH DUST SHELL RESOLVED AT 10 {mu}m WITH MMT ADAPTIVE OPTICS AND MIRAC4  

SciTech Connect (OSTI)

The evolved carbon-rich asymptotic giant branch star IRC +10216 (CW Leo) is the brightest mid-infrared source outside the solar system, as well as one of the closest examples of an evolved star losing mass. It has a complex and variable circumstellar structure on small scales in the near-infrared, and mid-infrared interferometry has revealed a dynamic dust formation zone. We have obtained diffraction-limited imaging and grism spectroscopy of IRC +10216 at the 6.5 m MMT in the N band ({approx}8-13 {mu}m). These new observations show that a change has occurred in the dust shell surrounding IRC +10216 over the last two decades, which is illustrated by a change in the apparent shape of the well-known SiC spectral feature at {approx}11 {mu}m and a reduction in the continuum at 13 {mu}m. As expected, our diffraction-limited spatial information shows an extended circumstellar envelope. We also demonstrate that the dusty envelope appears to be {approx}30% larger at the wavelengths of the SiC feature, likely due to the increased opacity of SiC. The deconvolved full width at half-maximum of the object increases from 0.''43 ({approx} 56 AU) for {lambda} < 10 {mu}m to 0.''58 ({approx}75 AU) at 11.8 {mu}m, then decreases to 0.''5 ({approx}65 AU) at 12.7 {mu}m. Our estimates of IRC +10216's size allow us to plausibly tie the change in the spectrum over the last 12.5 years to the evolution of the dusty circumstellar envelope at speeds of 12-17 km s{sup -1}.

Males, Jared R.; Close, Laird M.; Skemer, Andrew J.; Hinz, Philip M.; Hoffmann, William F. [Steward Observatory, Department of Astronomy, University of Arizona, Tucson, AZ 85721 (United States); Marengo, Massimo, E-mail: jrmales@email.arizona.edu [Department of Physics and Astronomy, Iowa State University, Ames, IA 50011 (United States)

2012-01-10T23:59:59.000Z

137

Comment Policy The MU Counseling Center Facebook page is not intended as a crisis service and does not provide any clinical service or support.  

E-Print Network [OSTI]

Comment Policy The MU Counseling Center Facebook page is not intended as a crisis service and does relationship with any staff member or the Counseling Center. Our Facebook page is not continuously monitored and about relevant events on our campus. We encourage your comments on MUCC Facebook page, and hope you

Taylor, Jerry

138

Simple qualitative description of EMC ratios {mu}{sup A} for 0.2 < or approx. x < or approx. 1.5 and some sample calculations  

SciTech Connect (OSTI)

We study EMC ratios on the basis of a relation between structure functions (SF) for a nucleus and for a nucleon, which is governed by a SF f{sup PN,A}(x,Q{sup 2}) of an unphysical nucleus, composed of point nucleons (PN). We demonstrate that the characteristic features of EMC ratios {mu}{sup A} are determined by the above f{sup PN,A} and the SF of free nucleons. We account for the positions of the points x{sub 1,2} in the interval 0.2 < or approx. x < or approx. 0.9, where {mu}{sup A}(x,Q{sup 2})=1 and also for the minimum x{sub m} in that interval. We similarly describe the oscillations in {mu}{sup A} for Q{sup 2} < or approx. 3.5-4.0 GeV{sup 2} in the quasielastic peak region 0.95 < or approx. x < or approx. 1.05 and for its subsequent continuous increase up to x{approx_equal}1.4. Finally we compute {mu}{sup A} over the entire range above for A= {sup 4}He, C, Fe, and Au and several Q{sup 2} values. The results are in reasonable agreement with both directly measured and indirectly extracted data.

Rinat, A.S.; Taragin, M.F.; Viviani, M. [Weizmann Institute of Science, Department of Particle Physics, Rehovot 76100 (Israel); INFN, Sezione Pisa and Phys. Dept., University of Pisa, I-56100 (Italy)

2005-07-01T23:59:59.000Z

139

Modeling of plasma-controlled evaporation and surface condensation of Al induced by 1.06 and 0.248 {mu}m laser radiations  

SciTech Connect (OSTI)

Phase transition on the surface of an aluminum target and vapor plasma induced by laser irradiation in the nanosecond regime at the wavelengths of 1.06 {mu}m in the infrared range and 0.248 {mu}m in the ultraviolet range with an intensity of 10{sup 8}-10{sup 9} W/cm{sup 2} in vacuum are analyzed. Special attention is paid to the wavelength dependence of the observed phenomena and the non-one-dimensional effects caused by the nonuniform (Gaussian) laser intensity distribution and the lateral expansion of the plasma plume. A transient two-dimensional model is used which includes conductive heat transfer in the condensed phase, radiative gas dynamics, and laser radiation transfer in the plasma as well as surface evaporation and back condensation at the phase interface. It was shown that distinctions in phase transition dynamics for the 1.06 and 0.248 {mu}m radiations result from essentially different characteristics of the laser-induced plasmas. For the 1.06 {mu}m radiation, evaporation stops after the formation of hot optically thick plasma, can occasionally resume at a later stage of the pulse, and proceeds nonuniformly in the spot area, and the major contribution to the mass removal occurs in the outer part of the irradiated region. Plasma induced by the 0.248 {mu}m laser is colder and partially transparent since it transmits 30%-70% of the incident radiation; therefore evaporation does not stop but continues in the subsonic regime with the Mach number of about 0.1. The amount of evaporated matter that condenses back to the surface is as high as 15%-20% and less than 10% for the 1.06 and 0.248 {mu}m radiations, respectively. For a beam radius smaller than {approx}100 {mu}m, the screening and retarding effect of the plasma weakens because of the lateral expansion, thickness of the removed layer increases, and condensation after the end of the pulse is not observed. Comparison of the numerical and experimental results on the removed layer thickness has shown, in particular, the importance of accounting for the plasma effect to predict the correct trends for radiation intensity and beam radius.

Mazhukin, V. I.; Nossov, V. V.; Smurov, I. [Institute of Mathematical Modeling of RAS, 4a Miusskaya Square, 125047 Moscow (Russian Federation); Ecole Nationale d'Ingenieurs de Saint-Etienne, 58 rue Jean Parot, 42023 Saint-Etienne Cedex 2 (France)

2007-01-15T23:59:59.000Z

140

Diversity in extinction laws of Type Ia supernovae measured between $0.2$ and $2\\,\\mu\\mathrm{m}$  

E-Print Network [OSTI]

We present ultraviolet (UV) observations of six nearby Type~Ia supernovae (SNe~Ia) obtained with the Hubble Space Telescope, three of which were also observed in the near-IR (NIR) with Wide-Field Camera~3. UV observations with the Swift satellite, as well as ground-based optical and near-infrared data provide complementary information. The combined data-set covers the wavelength range $0.2$--$2~\\mu$m. By also including archival data of SN 2014J, we analyse a sample spanning observed colour excesses up to $E(B-V)=1.4~$mag. We study the wavelength dependent extinction of each individual SN and find a diversity of reddening laws when characterised by the total-to-selective extinction $R_V$. In particular, we note that for the two SNe with $E(B-V)\\gtrsim1~$mag, for which the colour excess is dominated by dust extinction, we find $R_V=1.4\\pm0.1$ and $R_V=2.8\\pm0.1$. Adding UV photometry reduces the uncertainty of fitted $R_V$ by $\\sim50\\,$% allowing us to also measure $R_V$ of individual low-extinction objects whi...

Amanullah, R; Goobar, A; Ferretti, R; Papadogiannakis, S; Petrushevska, T; Brown, P J; Cao, Y; Contreras, C; Dahle, H; Elias-Rosa, N; Fynbo, J P U; Gorosabel, J; Guaita, L; Hangard, L; Howell, D A; Hsiao, E Y; Kankare, E; Kasliwal, M; Leloudas, G; Lundqvist, P; Mattila, S; Nugent, P; Phillips, M M; Sandberg, A; Stanishev, V; Sullivan, M; Taddia, F; Östlin, G; Asadi, S; Herrero-Illana, R; Jensen, J J; Karhunen, K; Lazarevi, S; Varenius, E; Santos, P; Sridhar, S Seethapuram; Wallström, S H J; Wiegert, J

2015-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


141

First Search for the Standard Model Higgs Boson Using the Semileptonic Decay Channel: H --> WW --> mu bar nu jj  

SciTech Connect (OSTI)

This dissertation presents the first search for the standard model Higgs boson (H) in decay topologies containing a muon, an imbalance in transverse momentum (E{sub T}) and jets, using p{bar p} collisions at {radical}s = 1.96 TeV with an integrated luminosity of 4.3 fb{sup -1} recorded with the D0 detector at the Fermilab Tevatron Collider. This analysis is sensitive primary to contributions from Higgs bosons produced through gluon fusion, with subsequent decay H {yields} WW {yields} {mu}{nu}jj where W represents a real or virtual W boson. In the absence of signal, limits are set at 95% confidence on the production and decay of the standard model Higgs boson for M{sub H} in the range of 115-200 GeV. For M{sub H} = 165 GeV, the observed and expected limits are factors of 11.2 larger than the standard model value. Combining this channel with e{nu}jj final states and including earlier data to increase the integrated luminosity to 5.4 fb{sup -1} produces observed(expected) limits of 5.5(3.8) times the standard model value.

Zelitch, Shannon Maura; /Virginia U.

2010-09-01T23:59:59.000Z

142

CoMuEx  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May JunDatastreamsmmcrcalgovInstrumentsruc DocumentationP-Series to User Group and Userof aChristinaCliff joinsClimate,

143

MU-CAT  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr MayAtmospheric Optical Depth7-1D: VegetationEquipment Surfaces and InterfacesAdministration -Lowell L.FallU . S . D e p aMSTandTruman

144

Frequency stabilization of 1. 5-. mu. m InGaAsP distributed feedback laser to NH/sub 3/ absorption lines  

SciTech Connect (OSTI)

NH/sub 3/ absorption lines due to vibration-rotation transitions are observed at 1.50--1.54 ..mu..m by using an InGaAsP superluminescent diode. A 1.5-..mu..m InGaAsP distributed feedback (DFB) laser is frequency stabilized to an NH/sub 3/ linear absorption line at 15196 A. Frequency stability of sigma(2,tau) = 8 x 10/sup -11/tau/sup -1/ is achieved for an averaging time range of 10 ms< or =tau< or =1 s. Such an absolute frequency-stabilized DFB laser is useful for coherent optical system applications, since it is free from the longitudinal mode jumping which results from a wide range of temperature changes and long-term device degradation.

Yanagawa, T.; Saito, S.; Yamamoto, Y.

1984-10-15T23:59:59.000Z

145

Structural, magnetic, and mechanical properties of 5 {mu}m thick SmCo films suitable for use in microelectromechanical systems  

SciTech Connect (OSTI)

5 {mu}m thick SmCo films were deposited onto Si substrates using triode sputtering. A study of the influence of deposition temperature (T{sub dep}{<=}600 deg. C) on the structural, magnetic, and mechanical properties has shown that optimum properties [highest degree of in-plane texture, maximum in-plane coercivity and remanence (1.3 and 0.8 T, respectively), and no film peel-off] are achieved for films deposited at the relatively low temperature of 350 deg. C. This temperature is compatible with film integration into microelectromechanical systems. The deposition rate was increased from 3.6 to 18 {mu}m/h by increasing the surface area of the target from 7 to 81 cm{sup 2} while keeping the target potential fixed. Mechanically intact films could be prepared by deposition onto prepatterned films or deposition through a mask.

Walther, A. [Institut Neel, CNRS-UJF, 25 rue des Martyrs, 38042 Grenoble (France); CEA Leti-MINATEC, 17 rue des Martyrs, 38054 Grenoble (France); Givord, D.; Dempsey, N. M. [Institut Neel, CNRS-UJF, 25 rue des Martyrs, 38042 Grenoble (France); Khlopkov, K.; Gutfleisch, O. [IFW Dresden, Institute of Metallic Materials, Helmholtzstr. 20, 01069 Dresden (Germany)

2008-02-15T23:59:59.000Z

146

THE CARNEGIE HUBBLE PROGRAM: THE LEAVITT LAW AT 3.6 AND 4.5 {mu}m IN THE MILKY WAY  

SciTech Connect (OSTI)

The Carnegie Hubble Program (CHP) is designed to calibrate the extragalactic distance scale using data from the post-cryogenic era of the Spitzer Space Telescope. The ultimate goal of the CHP is a systematic improvement in the distance scale leading to a determination of the Hubble constant to within an accuracy of 2%. This paper focuses on the measurement and calibration of the Galactic Cepheid period-luminosity (PL, Leavitt) relation using the warm Spitzer/IRAC 1 and 2 bands at 3.6 and 4.5 {mu}m. We present photometric measurements covering the period range 4-70 days for 37 Galactic Cepheids. Data at 24 phase points were collected for each star. Three PL relations of the form M = a(log (P) - 1) + b are derived. The method adopted here takes the slope a to be -3.31, as determined from the Spitzer Large Magellanic Cloud (LMC) data of Scowcroft et al. Using the geometric Hubble Space Telescope guide-star distances to 10 Galactic Cepheids, we find a calibrated 3.6 {mu}m PL zero point of -5.80 {+-} 0.03. Together with our value for the LMC zero point, we determine a reddening-corrected distance modulus of 18.48 {+-} 0.04 mag to the LMC. The mid-IR period-color diagram and the [3.6]-[4.5] color variation with phase are interpreted in terms of CO absorption at 4.5 {mu}m. This situation compromises the use of the 4.5 {mu}m data for distance determinations.

Monson, Andrew J.; Freedman, Wendy L.; Madore, Barry F.; Persson, S. E.; Scowcroft, Victoria; Seibert, Mark [Observatories of the Carnegie Institution of Washington, 813 Santa Barbara Street, Pasadena, CA 91101 (United States); Rigby, Jane R., E-mail: amonson@obs.carnegiescience.edu, E-mail: wendy@obs.carnegiescience.edu, E-mail: barry@obs.carnegiescience.edu, E-mail: persson@obs.carnegiescience.edu, E-mail: vs@obs.carnegiescience.edu, E-mail: mseibert@obs.carnegiescience.edu, E-mail: Jane.R.Rigby@nasa.gov [Observational Cosmology Lab, NASA Goddard Space Flight Center, Greenbelt, MD 20771 (United States)

2012-11-10T23:59:59.000Z

147

Adaptive Gain and Order Scheduling of Optimal Fractional Order PI{\\lambda}D{\\mu} Controllers with Radial Basis Function Neural-Network  

E-Print Network [OSTI]

Gain and order scheduling of fractional order (FO) PI{\\lambda}D{\\mu} controllers are studied in this paper considering four different classes of higher order processes. The mapping between the optimum PID/FOPID controller parameters and the reduced order process models are done using Radial Basis Function (RBF) type Artificial Neural Network (ANN). Simulation studies have been done to show the effectiveness of the RBFNN for online scheduling of such controllers with random change in set-point and process parameters.

Das, Saptarshi; Mukherjee, Ayan; Pan, Indranil; Gupta, Amitava; 10.1109/PACC.2011.5979047

2012-01-01T23:59:59.000Z

148

Ternary mutual diffusion coefficients of NaCl-SrCl/sub 2/-H/sub 2/O at 25/degrees/C. 2. Total concentrations of 2. 0 and 3. 0 mol/times/dm/sup /minus/3/  

SciTech Connect (OSTI)

Mutual diffusion coefficients were measured for aqueous NaCl-SrCl/sub 2/ mixtures at 25/degrees/C by using free-diffusion Rayleigh interferometry. These mixtures were total molarities of 2.0 and 3.0 mol/times/dm/sup /minus/3/ with molarity fractions of 2/3, 1/2, and 1/3, the results complement the authors earlier data at 0.5 and 1.0 mol/times/dm/sup /minus/3/. At a constant molarity ratio, the NaCl main-term coefficient decreases regularly by 19-36% with increasing concentration, in contrast, the SrCl/sub 2/ main-term coefficient is relatively constant, with 18% or less variation with concentration. The SrCl/sub 2/ cross-term coefficient is 7-23% of its corresponding main-term coefficient, whereas the NaCl cross-term coefficient varies from 8% to 73% of its corresponding main-term coefficient. Clearly, coupled diffusion is very important for these systems. Various estimation procedures were considered, including variations using the Nernst-Hartley equations and estimates from the corresponding binary solutions. None of these methods, for which sufficient auxiliary data are available, gave reliable estimates of diffusion coefficients for mixtures. At a total molarity of 3.0 mol/times/dm/sup /minus/3/ and molarity fractions of 1/2 and 1/3 NaCl, experiments with the SrCl/sub 2/ ..delta..c approx. 0 are convectively unstable with regard to fingering at the center of the boundary. Density data were also measured for the above systems.

Rard, J.A.; Miller, D.G.

1988-10-20T23:59:59.000Z

149

Oxygen Isotope Effects on Electron Transfer to O2 Probed Using Chemically Modified Flavins Bound to Glucose Oxidase  

E-Print Network [OSTI]

-reaching consequences, possibly leading to improved biosensors1 and fuel cells2 and to the development of "green2 of ) 28 kcal mol-1 at optimal pH, which is similar to the value obtained earlier from temperature

Roth, Justine P.

150

Thermochemistry of onion-like carbons  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

Furthermore, OLC are approximately 5-9 kJ mol 1 less stable than single-wall carbon nanotubes (SWCNTs). The samples prepared at 1800 C are energetically less stable...

151

Barium in Twilight Zone suspended matter as a potential proxy for particulate organic carbon remineralization: Results for the North Pacific  

E-Print Network [OSTI]

considering TdR conversion factors 1 and 2 x 10 18 cellsrates using TdR conversion factors of 1 - 2 x 10 18mol -1 and a carbon conversion factor of 15 fg C cell -1 ;

Dehairs, F.

2008-01-01T23:59:59.000Z

152

Thermodynamics, Interfacial Structure, and pH Hysteresis of Rb+ Adsorption at the Muscovite (001)-Solution Interface  

E-Print Network [OSTI]

, Illinois 60439, and Department of Earth and EnVironmental Sciences, UniVersity of Illinois at Chicago (MC-186), 845 West Taylor Street, Chicago, Illinois 60607 ReceiVed July 30, 2008. ReVised Manuscript Recei.0 kJ·mol-1 and a correlation energy, Sr ) -7.2 ( 3.7 kJ·mol-1. The average height of each adsorbed

Illinois at Chicago, University of

153

EXPLAINING THE [C II]157.7 {mu}m DEFICIT IN LUMINOUS INFRARED GALAXIES-FIRST RESULTS FROM A HERSCHEL/PACS STUDY OF THE GOALS SAMPLE  

SciTech Connect (OSTI)

We present the first results of a survey of the [C II]157.7 {mu}m emission line in 241 luminous infrared galaxies (LIRGs) comprising the Great Observatories All-sky LIRG Survey (GOALS) sample, obtained with the PACS instrument on board the Herschel Space Observatory. The [C II] luminosities, L{sub [C{sub II]}}, of the LIRGs in GOALS range from {approx}10{sup 7} to 2 Multiplication-Sign 10{sup 9} L{sub Sun }. We find that LIRGs show a tight correlation of [C II]/FIR with far-IR (FIR) flux density ratios, with a strong negative trend spanning from {approx}10{sup -2} to 10{sup -4}, as the average temperature of dust increases. We find correlations between the [C II]/FIR ratio and the strength of the 9.7 {mu}m silicate absorption feature as well as with the luminosity surface density of the mid-IR emitting region ({Sigma}{sub MIR}), suggesting that warmer, more compact starbursts have substantially smaller [C II]/FIR ratios. Pure star-forming LIRGs have a mean [C II]/FIR {approx} 4 Multiplication-Sign 10{sup -3}, while galaxies with low polycyclic aromatic hydrocarbon (PAH) equivalent widths (EWs), indicative of the presence of active galactic nuclei (AGNs), span the full range in [C II]/FIR. However, we show that even when only pure star-forming galaxies are considered, the [C II]/FIR ratio still drops by an order of magnitude, from 10{sup -2} to 10{sup -3}, with {Sigma}{sub MIR} and {Sigma}{sub IR}, implying that the [C II]157.7 {mu}m luminosity is not a good indicator of the star formation rate (SFR) for most local LIRGs, for it does not scale linearly with the warm dust emission most likely associated to the youngest stars. Moreover, even in LIRGs in which we detect an AGN in the mid-IR, the majority (2/3) of galaxies show [C II]/FIR {>=} 10{sup -3} typical of high 6.2 {mu}m PAH EW sources, suggesting that most AGNs do not contribute significantly to the FIR emission. We provide an empirical relation between the [C II]/FIR and the specific SFR for star-forming LIRGs. Finally, we present predictions for the starburst size based on the observed [C II] and FIR luminosities which should be useful for comparing with results from future surveys of high-redshift galaxies with ALMA and CCAT.

Diaz-Santos, T.; Armus, L.; Howell, J. H.; Surace, J. A. [Spitzer Science Center, California Institute of Technology, MS 220-6, Pasadena, CA 91125 (United States); Charmandaris, V. [IESL/Foundation for Research and Technology-Hellas, GR-71110, Heraklion (Greece); Stierwalt, S.; Evans, A. S.; Mazzarella, J. M. [Department of Astronomy, University of Virginia, P.O. Box 400325, Charlottesville, VA 22904 (United States); Murphy, E. J. [Observatories of the Carnegie Institution for Science, 813 Santa Barbara Street, Pasadena, CA 91101 (United States); Haan, S. [CSIRO Astronomy and Space Science, Marsfield NSW 2122 (Australia); Inami, H. [National Optical Astronomy Observatory, 950 North Cherry Avenue, Tucson, AZ 85719 (United States); Malhotra, S. [School of Earth and Space Exploration, Arizona State University, Tempe, AZ 85287 (United States); Meijerink, R. [Kapteyn Astronomical Institute, University of Groningen, P.O. Box 800, NL-9700 AV Groningen (Netherlands); Stacey, G. [Department of Astronomy, Cornell University, Ithaca, NY 14853 (United States); Petric, A. O.; Lu, N. [Astronomy Department, California Institute of Technology, Pasadena, CA 91125 (United States); Veilleux, S. [Joint Space-Science Institute, University of Maryland, College Park, MD 20742 (United States); Van der Werf, P. P. [Leiden Observatory, Leiden University, P.O. Box 9513, NL-2300 RA Leiden (Netherlands); Lord, S.; Appleton, P., E-mail: tanio@ipac.caltech.edu [NASA Herschel Science Center, IPAC, California Institute of Technology, MS 100-22, Cech, Pasadena, CA 91125 (United States); and others

2013-09-01T23:59:59.000Z

154

A SEARCH FOR C II 158 {mu}m LINE EMISSION IN HCM 6A, A Ly{alpha} EMITTER AT z = 6.56  

SciTech Connect (OSTI)

We report a Plateau de Bure Interferometer search for C II 158 {mu}m emission from HCM 6A, a lensed Ly{alpha} emitter (LAE) at z = 6.56. Our non-detections of C II 158 {mu}m line emission and 1.2 mm radio continuum emission yield 3{sigma} limits of L{sub CII} < 6.4 x 10{sup 7} x ({Delta}V/100 km s{sup -1}){sup 1/2} L{sub Sun} for the C II 158 {mu}m line luminosity and S{sub 1.2mm} < 0.68 mJy for the 1.2 mm flux density. The local conversion factor between L{sub CII} and the star formation rate (SFR) yields an SFR < 4.7 M{sub Sun} yr{sup -1}, Almost-Equal-To 2 times lower than that inferred from the ultraviolet (UV) continuum, suggesting that the local factor may not be applicable in high-z LAEs. The non-detection of 1.2 mm continuum emission yields a total SFR < 28 M{sub Sun} yr{sup -1}; any obscured star formation is thus within a factor of two of the visible star formation. Our best-fit model to the rest-frame UV/optical spectral energy distribution of HCM 6A yields a stellar mass of 1.3 Multiplication-Sign 10{sup 9} M{sub Sun} and an SFR of Almost-Equal-To 10 M{sub Sun} yr{sup -1}, with negligible dust obscuration. We fortuitously detect CO J = 3-2 emission from a z = 0.375 galaxy in the foreground cluster A370, and obtain a CO line luminosity of L'(CO) > (8.95 {+-} 0.79) Multiplication-Sign 10{sup 8} K km s{sup -1} pc{sup 2} and a molecular gas mass of M(H{sub 2}) > (4.12 {+-} 0.36) Multiplication-Sign 10{sup 9} M{sub Sun }, for a CO-to-H{sub 2} conversion factor of 4.6 M{sub Sun} (K km s{sup -1} pc{sup 2}){sup -1}.

Kanekar, Nissim [National Centre for Radio Astrophysics, Tata Institute of Fundamental Research, Pune 411 007 (India); Wagg, Jeff [European Southern Observatory, Alonso de Cordova 3107, Vitacura, Casilla 19001, Santiago 19 (Chile); Chary, Ranga Ram [U.S. Planck Data Center, MS220-6 Caltech, Pasadena, CA 91125 (United States); Carilli, Christopher L., E-mail: nkanekar@ncra.tifr.res.in [National Radio Astronomy Observatory, P.O. Box O, Socorro, NM 87801 (United States)

2013-07-10T23:59:59.000Z

155

Search for the rare decays B+-->mu+mu-K+, B-->mu+mu-K*(892), and Bs-->mu+mu- phi at CDF  

E-Print Network [OSTI]

We search for b?s?[superscript +]?[superscript -] transitions in B meson (B[superscript +], B[superscript 0], or B[subscript s][superscript 0]) decays with 924??pb[superscript -1] of pp[over -bar] collisions at sqrt ...

Makhoul, K.

156

Mind the gap on Icecube: Cosmic neutrino spectrum and muon anomalous magnetic moment in the gauged L_{\\mu} - L_{\\tau} model  

E-Print Network [OSTI]

The energy spectrum of cosmic neutrinos, which was recently reported by the IceCube collaboration, shows a gap between 400 TeV and 1 PeV. An unknown neutrino interaction mediated by a field with a mass of the MeV scale is one of the possible solutions to this gap. We examine if the leptonic gauge interaction L_{\\mu} - L_{\\tau} can simultaneously explain the two phenomena in the lepton sector: the gap in the cosmic neutrino spectrum and the unsettled disagreement in muon anomalous magnetic moment. We illustrate that there remains the regions in the model parameter space, which account for both the problems. Our results also provide a hint for the distance to the source of the high-energy cosmic neutrinos.

Araki, Takeshi; Konishi, Yasufumi; Ota, Toshihiko; Sato, Joe; Shimomura, Takashi

2014-01-01T23:59:59.000Z

157

Diode laser measurements of H[sub 2]O line intensities and self-broadening coefficients in the 1. 4-[mu]m region  

SciTech Connect (OSTI)

Precise knowledge of water vapor radiative properties in the infrared spectrum is needed for many applications. Such applications include atmospheric sounding experiments, radiative sensing of combustion processes, and optical diagnostics for gas-dynamic and aerodynamic studies. Spectrally resolved measurements of pure water vapor absorption spectra have been performed with a tunable diode laser. The laser, a distributed feedback InGaAsP diode, emits in the 1.4-[mu]m region. A total of 12 lines were studied corresponding to rovibrational transitions within the [nu][sub 1] + [nu][sub 3] and 2[nu][sub 1] vibrational bands. A Voigt profile analysis of lineshape is used to infer both intensities and self-collision-broadening coefficients of the water vapor. Good agreements is found between the observed line intensities and those recently measured by Toth. These results are apparently the first published measurements of the broadening coefficient within this spectral range.

Langlois, S.; Birbeck, T.P.; Hanson, R.K. (Stanford Univ., CA (United States). Dept. of Mechanical Engineering)

1994-01-01T23:59:59.000Z

158

Compositional dependence of the 1.8 {mu}m emission properties of Tm{sup 3+} ions in silicate glass  

SciTech Connect (OSTI)

The compositional dependence of the 1.8 {mu}m emission properties of Tm{sup 3+} ion-doped lead silicate glasses is investigated. Judd-Ofelt parameters are calculated and their variation with different glass modifier ions is obtained. The Judd-Ofelt parameters increase with decreased modifier ionic radius. A large spontaneous emission probability and a large emission cross-section are found to be related with the strength of the modifier ion. Fluorescence spectra are analyzed using rate equations and compared with recorded data. The results are very close, indicating the reliability of this method. Non-radiative probability is deduced by fitting the fluorescence decay curve; it becomes smaller with increased ionic field strength. Energy transfer processes are studied using the extended overlap integral method.

Wang Xin; Fan Sijun; Li Kefeng; Zhang Lei; Wang Shikai; Hu Lili [Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Jia Ding, Shanghai 201800 (China)

2012-11-15T23:59:59.000Z

159

Pulseshape characteristics of a 300 $\\mu$m PR03 R-measuring VELO sensor read out with a Beetle1.3 chip  

E-Print Network [OSTI]

The signal-to-noise, overspill and undershoot characteristics of a VELO module equipped with Beetle1.3 read-out chips have been measured using 120 GeV pions from the SPS test beam facility at CERN. The module consists of a PR03 n-on-n 300 $\\mu$m R measuring prototype sensor and a fully populated K03 hybrid. Results are presented for a single Beetle1.3 chip with a variety of chip parameter settings controlling the pre-amplifier and shaper currents and feedback voltages, with the objective of establishing the performance of the module and understanding its dependence on the read-out chip settings.

Palacios, A; Buytaert, J; Borel, J; Collins, P; Eckstein, D; Eklund, L; Ferro-Luzzi, M; Jans, E; Ketel, T; Petrie, D; Pivk, M; Tobin, M

2005-01-01T23:59:59.000Z

160

FIRST DETECTIONS OF THE [N II] 122 {mu}m LINE AT HIGH REDSHIFT: DEMONSTRATING THE UTILITY OF THE LINE FOR STUDYING GALAXIES IN THE EARLY UNIVERSE  

SciTech Connect (OSTI)

We report the first detections of the [N II] 122 {mu}m line from a high-redshift galaxy. The line was strongly (>6{sigma}) detected from SMMJ02399-0136, and H1413+117 (the Cloverleaf QSO) using the Redshift (z) and Early Universe Spectrometer on the Caltech Submillimeter Observatory. The lines from both sources are quite bright with line to far-infrared (FIR) continuum luminosity ratios that are {approx}7.0 x 10{sup -4} (Cloverleaf) and 2.1 x 10{sup -3} (SMMJ02399). With ratios 2-10 times larger than the average value for nearby galaxies, neither source exhibits the line-to-continuum deficits seen in nearby sources. The line strengths also indicate large ionized gas fractions, {approx}8%-17% of the molecular gas mass. The [O III]/[N II] line ratio is very sensitive to the effective temperature of ionizing stars and the ionization parameter for emission arising in the narrow-line region (NLR) of an active galactic nucleus (AGN). Using our previous detection of the [O III] 88 {mu}m line, the [O III]/[N II] line ratio for SMMJ02399-0136 indicates that the dominant source of the line emission is either stellar H II regions ionized by O9.5 stars, or the NLR of the AGN with ionization parameter log(U) = -3.3 to -4.0. A composite system, where 30%-50% of the FIR lines arise in the NLR also matches the data. The Cloverleaf is best modeled by a superposition of {approx}200 M82-like starbursts accounting for all of the FIR emission and 43% of the [N II] line. The remainder may come from the NLR. This work demonstrates the utility of the [N II] and [O III] lines in constraining properties of the ionized medium.

Ferkinhoff, Carl; Brisbin, Drew; Nikola, Thomas; Parshley, Stephen C.; Stacey, Gordon J. [Department of Astronomy, Cornell University, Ithaca, NY 14853 (United States); Phillips, Thomas G. [California Institute of Technology, Pasadena, CA 91125 (United States); Falgarone, Edith [LERMA, CNRS, Observatoire de Paris and ENS (France); Benford, Dominic J.; Staguhn, Johannes G. [Observational Cosmology Laboratory (Code 665), NASA Goddard Space Flight Center, Greenbelt, MD 20771 (United States); Tucker, Carol E., E-mail: cferkinh@astro.cornell.edu [Department of Physics and Astronomy, Cardiff University, Cardiff CF24 3AA (United Kingdom)

2011-10-10T23:59:59.000Z

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


161

FIRST DETECTION OF THE [O III] 88 {mu}m LINE AT HIGH REDSHIFTS: CHARACTERIZING THE STARBURST AND NARROW-LINE REGIONS IN EXTREME LUMINOSITY SYSTEMS  

SciTech Connect (OSTI)

We have made the first detections of the 88 {mu}m [O III] line from galaxies in the early universe, detecting the line from the lensed active galactic nucleus (AGN)/starburst composite systems APM 08279+5255 at z = 3.911 and SMM J02399-0136 at z = 2.8076. The line is exceptionally bright from both systems, with apparent (lensed) luminosities {approx}10{sup 11} L {sub sun}. For APM 08279, the [O III] line flux can be modeled in a star formation paradigm, with the stellar radiation field dominated by stars with effective temperatures, T {sub eff} > 36,000 K, similar to the starburst found in M82. The model implies {approx}35% of the total far-IR luminosity of the system is generated by the starburst, with the remainder arising from dust heated by the AGN. The 88 {mu}m line can also be generated in the narrow-line region of the AGN if gas densities are around a few 1000 cm{sup -3}. For SMM J02399, the [O III] line likely arises from H II regions formed by hot (T {sub eff} > 40,000 K) young stars in a massive starburst that dominates the far-IR luminosity of the system. The present work demonstrates the utility of the [O III] line for characterizing starbursts and AGN within galaxies in the early universe. These are the first detections of this astrophysically important line from galaxies beyond a redshift of 0.05.

Ferkinhoff, C.; Hailey-Dunsheath, S.; Nikola, T.; Parshley, S. C.; Stacey, G. J. [Department of Astronomy, Cornell University, Ithaca, NY 14853 (United States); Benford, D. J.; Staguhn, J. G., E-mail: cferkinh@astro.cornell.ed, E-mail: steve@mpe.mpg.d [Observational Cosmology Laboratory (Code 665), NASA Goddard Space Flight Center, Greenbelt, MD 20771 (United States)

2010-05-01T23:59:59.000Z

162

WISE TF: A MID-INFRARED, 3.4 {mu}m EXTENSION OF THE TULLY-FISHER RELATION USING WISE PHOTOMETRY  

SciTech Connect (OSTI)

We present a mid-infrared Tully-Fisher (TF) relation using photometry from the 3.4 {mu}m W1 band of the Wide-field Infrared Survey Explorer (WISE) satellite. The WISE TF relation is formed from 568 galaxies taken from the all-sky 2MASS Tully-Fisher (2MTF) galaxy catalog, spanning a range of environments including field, group, and cluster galaxies. This constitutes the largest mid-infrared TF relation constructed to date. After applying a number of corrections to galaxy magnitudes and line widths, we measure a master TF relation given by M{sub corr} = -22.24 - 10.05[log (W{sub corr}) - 2.5], with an average dispersion of {sigma}{sub WISE} = 0.686 mag. There is some tension between WISE TF and a preliminary 3.6 {mu}m relation, which has a shallower slope and almost no intrinsic dispersion. However, our results agree well with a more recent relation constructed from a large sample of cluster galaxies. We additionally compare WISE TF to the near-infrared 2MTF template relations, finding a good agreement between the TF parameters and total dispersions of WISE TF and the 2MTF K-band template. This fact, coupled with typical galaxy colors of (K - W1) {approx} 0, suggests that these two bands are tracing similar stellar populations, including the older, centrally-located stars in the galactic bulge which can (for galaxies with a prominent bulge) dominate the light profile.

Lagattuta, David J.; Mould, Jeremy R. [Centre for Astrophysics and Supercomputing, Swinburne University of Technology, P.O. Box 218, Hawthorn, VIC 3122 (Australia); Staveley-Smith, Lister; Hong Tao; Springob, Christopher M. [ARC Centre of Excellence for All-sky Astrophysics (CAASTRO), Redfern, NSW (Australia); Masters, Karen L. [Institute for Cosmology and Gravitation, University of Portsmouth, Dennis Sciama Building, Burnaby Road, Portsmouth, PO1 3FX (United Kingdom); Koribalski, Baerbel S. [CSIRO Astronomy and Space Science, Australia Telescope National Facility (ATNF) P.O. Box 76, Epping, NSW 1710 (Australia); Jones, D. Heath, E-mail: dlagattu@astro.swin.edu.au [School of Physics, Monash University, Clayton, VIC 3800 (Australia)

2013-07-10T23:59:59.000Z

163

Search for sneutrino production in $e\\mu$ final states in 5.3 fb$^{-1}$ of $p\\bar{p}$ collisions at $\\sqrt(s) =1.96$ TeV  

SciTech Connect (OSTI)

We report the results of a search for R parity violating (RPV) interactions leading to the production of supersymmetric sneutrinos decaying into e{mu} final states using 5.3 fb{sup -1} of integrated luminosity collected by the D0 experiment at the Fermilab Tevatron Collider. Having observed no evidence for production of e{mu} resonances, we set direct bounds on the RPV couplings {lambda}{prime}{sub 311} and {lambda}{sub 312} as a function of sneutrino mass.

Abazov, Victor Mukhamedovich; /Dubna, JINR; Abbott, Braden Keim; /Oklahoma U.; Abolins, Maris A.; /Michigan State U.; Acharya, Bannanje Sripath; /Tata Inst.; Adams, Mark Raymond; /Illinois U., Chicago; Adams, Todd; /Florida State U.; Alexeev, Guennadi D.; /Dubna, JINR; Alkhazov, Georgiy D.; /St. Petersburg, INP; Alton, Andrew K.; /Michigan U. /Augustana Coll., Sioux Falls; Alverson, George O.; /Northeastern U.; Alves, Gilvan Augusto; /Rio de Janeiro, CBPF /Nijmegen U.

2010-07-01T23:59:59.000Z

164

Ternary mutual diffusion coefficients of NaCl-SrCl/sub 2/-H/sub 2/O at 25/sup 0/C. 1. Total concentrations of 0. 5 and 1. 0 mol. dm/sup -3/  

SciTech Connect (OSTI)

Mutual diffusion coefficients have been measured for aqueous NaCl-SrCl/sub 2/ mixtures at 25/sup 0/C by using free-diffusion Rayleigh interferometry. These diffusion experiments were done at total molarities of 0.5 and 1.0 mol x dm/sup -3/ and with molarity fractions of 1/3, 1/2, and 2/3. Main-term diffusion coefficients for NaCl and SrCl/sub 2/ show a 10-15% variation with concentration and composition. Coupled diffusion is important for these systems, with cross-term diffusion coefficients being 6.5-36% as large as their corresponding main terms. At a constant molarity ratio, doubling the concentration causes cross-term diffusion coefficients to increase. Attempts to estimate the ternary solution diffusion coefficients from those of their corresponding binary solutions or from the ternary solution analogues of the Nernst-Hartley equation do not yield particularly accurate results.

Rard, J.A.; Miller, D.G.

1987-08-13T23:59:59.000Z

165

03/04/2006 07:26 PMGlaser CIITN Article -MU College of Arts and Science Research Communication Project Page 1 of 2http://rcp.missouri.edu/articles/glaser-CIITN.html  

E-Print Network [OSTI]

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Glaser, Rainer

166

Two-chord interferometry using 3.39 {mu}m He-Ne laser on a flux-coil-generated FRC  

SciTech Connect (OSTI)

A two-chord {lambda}{sub IR}{approx}3.39 {mu}m He-Ne laser interferometer system was developed for a flux-coil-generated field-reversed configuration to estimate the electron density and the total temperature of the field-reversed configuration (FRC) plasma. This two-chord heterodyne interferometer system consists of a single {approx}2 mW infrared He-Ne laser, a visible ({lambda}{sub vis}{approx}632.8 nm) He-Ne laser for the alignment, a 40 MHz acousto-optic modulator, photodetectors, and quadrature phase detectors. Initial measurement was performed and the measured average electron densities were 2-10x10{sup 19} m{sup -3} at two different radial positions in the midplane. A time shift in density was observed as the FRC expands radially. The time evolution of the line-averaged density agrees with the density estimated from the in situ internal magnetic probes, based on a rigid-rotor profile model.

Gota, H.; Deng, B. H.; Gupta, D.; Kiyashko, V.; Knapp, K.; Mendoza, R.; Morehouse, M. [Tri Alpha Energy, Inc., Rancho Santa Margarita, California 92688 (United States); Bolte, N.; Roche, T.; Wessel, F. [Tri Alpha Energy, Inc., Rancho Santa Margarita, California 92688 (United States); Department of Physics and Astronomy, University of California, Irvine, California 92697 (United States)

2010-10-15T23:59:59.000Z

167

Selection Tests of MnZn and NiZn Ferrites for Mu2e 300 kHz and 5.1 MHz AC Dipoles  

SciTech Connect (OSTI)

Mu2e, a charged lepton flavor violation (CLFV) experiment is planned to start at Fermilab late in this decade. The proposed experiment will search for neutrinoless muon to electron conversions with unprecedented sensitivity, better than 6 x 10{sup -17 }at 90% CL. To achieve this sensitivity the incoming proton beam must be highly suppressed during the window for detecting the muon decays. The current proposal for beam extinction is based on a collimator design with two dipoles running at {approx}300 kHz and 5.1 MHz and synchronized to the proton bunch spacing. The appropriate choice of ferrite material for the magnet yoke is a critical step in the overall design of the dipoles and their reliable operation at such high frequencies over the life of the experiment. This choice, based on a series of the thermal and magnetic measurements of the ferrite samples, is discussed in the paper. Additionally, the first results from the testing at 300 kHz of a prototype AC dipole are presented.

Bourkland, K.; Elementi, L.; Feher, S.; Harding, D.J.; Kashikhin, V.S.; Makarov, A.; Pfeffer, H.; Velev, G.V.; /Fermilab; Mulushev, E.; /Institute of Automatics and Electrometry; Iedmeska, I.; /Moscow, MIPT; Venturini, M.; /Pisa U.

2011-09-09T23:59:59.000Z

168

Temperature-dependent collision-broadening parameters of H[sub 2]O lines in the 1. 4-[mu]m region using diode laser absorption spectroscopy  

SciTech Connect (OSTI)

Radiative properties of water vapor in the infrared spectrum are important in a variety of applications, including atmospheric sounding experiments, radiative sensing of combustion processes, and optical diagnostics for gasdynamic and aerodynamic studies. Here, spectrally resolved measurements of water vapor absorption spectra near 1.4 [mu]m have been performed with a tunable, distributed-feedback InGaAsP diode laser. A lineshape analysis was used to infer the collision-broadening coefficient of 11 rovibrational transitions in the [nu] + [nu][sub 3] and 2[nu][sub 1] vibration bands perturbed separately by N[sub 2], O[sub 2], CO[sub 2], and H[sub 2]. The temperature dependence of the broadening coefficients was determined using a temperature-controlled static cell and a pressure-driven shock tube over the range 300--1,200 K. The measured coefficients are in good agreement with the previous calculations of Delaye. Also, agreement is found between prior experimental data, obtained for the same rotational transitions but different vibration bands, and the results.

Langlois, S.; Birbeck, T.P.; Hanson, R.K. (Stanford Univ., CA (United States). Dept. of Mechanical Engineering)

1994-10-01T23:59:59.000Z

169

Measurements of line strengths in the HO sub 2. nu. sub 1 overtone band at 1. 5. mu. m using an InGaAsP laser  

SciTech Connect (OSTI)

The hydroperoxyl radical, HO{sub 2}, is a pivotal atmospheric species, being closely coupled to OH, the most important oxidant in both tropospheric and stratospheric chemistry. The authors report the first observation of resolved rotational-vibrational overtone (2{nu}{sub 1}) absorptions of the hydroperoxyl radical (HO{sub 2}) in the 1.5-{mu}m region, using two-tone frequency modulation spectroscopy (TTFMS) with an InGaAsP laser diode and White-cell optics. Photolysis of Cl{sub 2}/H{sub 2}O{sub 2} mixtures was used to produce the HO{sub 2}, and the concentration was determined by modulated-photolysis UV absorption spectroscopy. The line center adsorption cross sections for the strongest lines ranged between 1.3 {times} 10{sup {minus}20} and 10 {times} 10{sup {minus}20} cm{sup 2} molecule{sup {minus}1} under Doppler-limited conditions. For the strongest line this corresponds to an integrated line strength S of 1.6 {times} 10{sup {minus}21} cm{sup 2} molecule{sup {minus}1} cm{sup {minus}1}, a line strength of the same order of magnitude as lines previously observed in the relatively weak {nu}{sub 1} fundamental.

Johnson, T.J.; Wienhold, F.G.; Burrows, J.P.; Harris, G.W. (Max Planck Inst. for Chemistry, Mainz (Germany)); Burkhard, H. (DBP Telekom Research Inst., Darmstadt (Germany))

1991-08-22T23:59:59.000Z

170

MU INTERNATIONAL DIRECTORY International Directory  

E-Print Network [OSTI]

of Ag., Food & Natural Resources International Programs http://students.missouri.edu/~asa Association of Malaysian Students http://www.missouri.edu/~ctl2m5/index.html Bangladesh Student Association

Taylor, Jerry

171

Experiment Profile: Mu2e  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr MayAtmospheric Optical Depth7-1D: Vegetation ProposedUsing ZirconiaPolicy and Assistance100 tonusingdeposition.EnergyExpedited6

172

Proton form factor ratio, {mu}{sub p}G{sub E}{sup P}/G{sub M}{sup P} from double spin asymmetry  

SciTech Connect (OSTI)

The form factors are fundamental properties of the nucleon representing the effect of its structure on its response to electromagnetic probes such as electrons. They are functions of the four-momentum transfer squared Q{sup 2} between the electron and the proton. This thesis reports the results of a new measurement of the ratio of the electric and magnetic form factors of the proton up to Q{sup 2} = 5.66 (GeV/c){sup 2} using the double spin asymmetry with a polarized beam and target. Experiment E07-003 (SANE, Spin Asymmetries of the Nucleon Experiment) was carried out in Hall C at Jefferson Lab in 2009 to study the proton spin structure functions with a dynamically polarized ammonia target and longitudinally polarized electron beam. By detecting elastically scattered protons in the High-Momentum Spectrometer (HMS) in coincidence with the electrons in the Big Electron Telescope Array (BETA), elastic measurements were carried out in parallel. The elastic double spin asymmetry allows one to extract the proton electric to magnetic form factor ratio G{sup p}{sub E}/G{sup p}{sub M} at high-momentum transfer, Q{sup 2} = 5.66 (GeV/c){sup 2}. In addition to the coincidence data, inclusively scattered electrons from the polarized ammonia target were detected by HMS, which allows to measure the beam-target asymmetry in the elastic region with the target spin nearly perpendicular to the momentum transfer, and to extract G{sup p}{sub E}/G{sup p}{sub M} at low Q{sup 2} = 2.06 (GeV/c){sup 2}. This alternative measurement of G{sup p}{sub E}/G{sup p}{sub M} has verified and confirmed the dramatic discrepancy at high Q{sup 2} between the Rosenbluth and the recoil-polarization-transfer iv method with a different measurement technique and systematic uncertainties uncorrelated to those of the recoil-polarization measurements. The measurement of the form factor ratio at Q{sup 2} = 2.06 (GeV/c){sup 2} has been determined as {mu}{sub p}G{sup p}{sub E}/G{sup p}{sub M} = 0.605{+-}0.178{sub stat}{+-}0.033{sub sys} which is in agreement with an earlier measurement with the polarized target technique at similar kinematics. The measurement of the form factor ratio at Q{sup 2} = 5.66 (GeV/c){sup 2} has been determined as {mu}{sub p}G{sup p}{sub E}/G{sup p}{sub M} = 0.672 {+-} 0.362{sub stat} which represents the highest Q{sup 2} reach with the double spin asymmetry to date.

Habarakada Liyanage, Anusha Pushpakumari [Hampton U., JLAB] [Hampton U., JLAB

2013-08-01T23:59:59.000Z

173

Measurement of transmission efficiency for 400 MeV proton beam through collimator at Fermilab MuCool Test Area using Chromox-6 scintillation screen  

SciTech Connect (OSTI)

The MuCool Test Area (MTA) at Fermilab is a facility to develop the technology required for ionization cooling for a future Muon Collider and/or Neutrino Factory. As part of this research program, feasibility studies of various types of RF cavities in a high magnetic field environment are in progress. As a unique approach, we have tested a RF cavity filled with a high pressure hydrogen gas with a 400 MeV proton beam in an external magnetic field (B = 3 T). Quantitative information about the number of protons passing through this cavity is an essential requirement of the beam test. The MTA is a flammable gas (hydrogen) hazard zone. Due to safety reasons, no active (energized) beam diagnostic instrument can be used. Moreover, when the magnetic field is on, current transformers (toroids) used for beam intensity measurements do not work due to the saturation of the ferrite material of the transformer. Based on these requirements, we have developed a passive beam diagnostic instrumentation using a combination of a Chromox-6 scintillation screen and CCD camera. This paper describes details of the beam profile and position obtained from the CCD image with B = 0 T and B = 3 T, and for high and low intensity proton beams. A comparison is made with beam size obtained from multi-wires detector. Beam transmission efficiency through a collimator with a 4 mm diameter hole is measured by the toroids and CCD image of the scintillation screen. Results show that the transmission efficiency estimated from the CCD image is consistent with the toroid measurement, which enables us to monitor the beam transmission efficiency even in a high magnetic field environment.

Jana, M. R.; Chung, M.; Leonova, M.; Moretti, A.; Palmer, M.; Schwarz, T.; Tollestrup, A.; Yonehara, K. [Fermi National Accelerator Laboratory, Batavia, Illinois 60510 (United States); Freemire, B.; Hanlet, P.; Torun, Y. [Illinois Institute of Technology, Chicago, Illinois 60616 (United States)

2013-06-15T23:59:59.000Z

174

THE 0.5-2.22 {mu}m SCATTERED LIGHT SPECTRUM OF THE DISK AROUND TW Hya: DETECTION OF A PARTIALLY FILLED DISK GAP AT 80 AU  

SciTech Connect (OSTI)

We present a 0.5-2.2 {mu}m scattered light spectrum of the circumstellar disk around TW Hya from a combination of spatially resolved Hubble Space Telescope STIS spectroscopy and NICMOS coronagraphic images of the disk. We investigate the morphology of the disk at distances >40 AU over this wide range of wavelengths, and identify the presence of a depression in surface brightness at {approx}80 AU that could be caused by a gap in the disk. Additionally, we quantify the surface brightness, azimuthal symmetry, and spectral character of the disk as a function of radius. Our analysis shows that the scattering efficiency of the dust is largely neutral to blue over the observed wavelengths. We model the disk as a steady {alpha}-disk with an ad hoc gap structure. The thermal properties of the disk are self-consistently calculated using a three-dimensional radiative transfer code that uses ray tracing to model the heating of the disk interior and scattered light images. We find a good fit to the data over a wide range of distances from the star if we use a model disk with a partially filled gap of 30% depth at 80 AU and with a self-similar truncation knee at 100 AU. The origin of the gap is unclear, but it could arise from a transition in the nature of the disk's dust composition or the presence of a planetary companion. Based on scalings to previous hydrodynamic simulations of gap-opening criteria for embedded proto-planets, we estimate that a planetary companion forming the gap could have a mass between 6 and 28 M{sub Circled-Plus }.

Debes, John H. [Space Telescope Science Institute, Baltimore, MD 21218 (United States); Jang-Condell, Hannah [University of Wyoming, Laramie, WY 82071 (United States); Weinberger, Alycia J. [Department of Terrestrial Magnetism, Carnegie Institution of Washington, Washington, DC 20015 (United States); Roberge, Aki [Goddard Space Flight Center, Greenbelt, MD 20771 (United States); Schneider, Glenn [Steward Observatory, University of Arizona, Tuscon, AZ 85721 (United States)

2013-07-01T23:59:59.000Z

175

Genetic Algorithm Based Improved Sub-Optimal Model Reduction in Nyquist Plane for Optimal Tuning Rule Extraction of PID and PI{\\lambda}D{\\mu} Controllers via Genetic Programming  

E-Print Network [OSTI]

Genetic Algorithm (GA) has been used in this paper for a new Nyquist based sub-optimal model reduction and optimal time domain tuning of PID and fractional order (FO) PI{\\lambda}D{\\mu} controllers. Comparative studies show that the new model reduction technique outperforms the conventional H2-norm based reduced order modeling techniques. Optimum tuning rule has been developed next with a test-bench of higher order processes via Genetic Programming (GP) with minimum value of weighted integral error index and control signal. From the Pareto optimal front which is a trade-off between the complexity of the formulae and control performance, an efficient set of tuning rules has been generated for time domain optimal PID and PI{\\lambda}D{\\mu} controllers.

Das, Saptarshi; Das, Shantanu; Gupta, Amitava; 10.1109/PACC.2011.5978962

2012-01-01T23:59:59.000Z

176

A wide-bandwidth low-noise InGaAsP-InAlAs superlattice avalanche photodiode with a flip-chip structure for wavelengths of 1. 3 and 1. 55 [mu]m  

SciTech Connect (OSTI)

This paper reports the fabrication of a flip-chip InGaAsP-InAlAs superlattice avalanche photodiode using gas source molecular beam epitaxy. The incident light reaches the InGaAs photoabsorption layer through the InP substrate and an InGaAsP-InAlAs superlattice multiplication region which are transparent for wavelengths of 1.55 and 1.3 [mu]m. The light reflection by the electrode enables the absorption layer to be as thin as 0.8 [mu]m without significantly reducing the quantum efficiency. A maximum bandwidth of 17 GHz was obtained at a low multiplication factor because of the transit time through the absorption layer is reduced.

Kagawa, Toshiaki; Kawamura, Yuichi; Iwamura, Hidetoshi (NTT Opto-electronics Labs., Atsugi-shi, Kanagawa (Japan))

1993-05-01T23:59:59.000Z

177

Event-triggered nonlinear control for attitude stabilization of a J.F. Guerrero-Castellanos, J.J. Tellez-Guzman, S. Durand, N. Marchand, J.U. Alvarez-Mu~noz  

E-Print Network [OSTI]

-Castellanos, J.J. T´ellez-Guzm´an, S. Durand, N. Marchand, J.U. Alvarez-Mu~noz Abstract-- Event-triggered control, sylvain@durandchamontin.fr N. Marchand is with GIPSA-lab laboratory, Control Systems Dept., SySCo team, CNRS-Univ. of Grenoble, ENSE3 BP 46, 38402 St Martin d'H`eres Cedex, France, nicolas.marchand

Paris-Sud XI, Université de

178

Supporting Information Wiley-VCH 2011  

E-Print Network [OSTI]

dissolved in anhydrous THF (1000 ml), then allyl acetate (50.0 ml, 0.46 mol), 1,3-cyclopentadione (12, 45OH. #12; 2 Compound 13 was synthesized based on reported procedure with modification[1-3] : Allyl.0 g, 0.46 mol), N,O-bis (trimethylsilyl)acetamide (114 ml, 0.46 mol) and sodium acetate (1.10 g, 13

Theodorakis, Emmanuel

179

Probing the Electronic Structures of [Cmu(Mu-XR(2)]**N+ Diamond Cores As a Function of the Bridging X Atom (X = N Or P) And Charge (N=0, 1, 2)  

SciTech Connect (OSTI)

A series of dicopper diamond core complexes that can be isolated in three different oxidation states ([Cu{sub 2}({mu}-XR{sub 2})]{sup n+}, where n = 0, 1, 2 and X = N or P) is described. Of particular interest is the relative degree of oxidation of the respective copper centers and the bridging XR{sub 2} units, upon successive oxidations. These dicopper complexes feature terminal phosphine and either bridging amido or phosphido donors, and as such their metal-ligand bonds are highly covalent. Cu K-edge, Cu L-edge, and P K-edge spectroscopies, in combination with solid-state X-ray structures and DFT calculations, provides a complementary electronic structure picture for the entire set of complexes that tracks the involvement of a majority of ligand-based redox chemistry. The electronic structure picture that emerges for these inorganic dicopper diamond cores shares similarities with the Cu{sub 2}({mu}-SR){sub 2} Cu{sub A} sites of cytochrome c oxidases and nitrous oxide reductases.

Harkins, S.B.; Mankad, N.P.; Miller, A.J.M.; Szilagyi, R.K.; Peters, J.C.

2009-05-18T23:59:59.000Z

180

Spectroscopic investigation of 2.02 {mu}m emission in Ho{sup 3+}/Tm{sup 3+} codoped transparent glass ceramic containing CaF{sub 2} nanocrystals  

SciTech Connect (OSTI)

Tm{sup 3+} and Ho{sup 3+} codoped transparent glass ceramic (GC) containing CaF{sub 2} nanocrystals were fabricated by melt-quenching and subsequent thermal treatment. X-ray diffraction and transmission electron microscopy analysis confirmed the precipitation of CaF{sub 2} nanocrystals among the glass matrix. Energy-dispersive x-ray spectroscopy results evidenced the incorporation of Tm{sup 3+} and Ho{sup 3+} into the CaF{sub 2} nanocrystals. Judd-Ofelt parameters were calculated based on the absorption spectra, the smaller {Omega}{sub 2} and larger {Omega}{sub 6} imply that Tm{sup 3+} and Ho{sup 3+} ions has entered into a symmetrical ionic crystal field. 2.02 {mu}m emission spectral of the GC samples were recorded at room temperature with an excitation of 808 nm laser diode. The enhancement of the emission at 2.02 {mu}m in the GC samples could be attributed to more efficient cross relaxation process of Tm{sup 3+}:{sup 3}H{sub 4+}Tm{sup 3+}:{sup 3}H{sub 6}{yields}{sup 2}Tm{sup 3+}:{sup 3}H{sub 4}, and energy transfer from Tm{sup 3+} to Ho{sup 3+} benefited from the incorporation of rare earth ions into CaF{sub 2} nanocrystals.

Chen, Q. J.; Zhang, W. J.; Qian, Q.; Yang, Z. M.; Zhang, Q. Y. [MOE Key Lab of Specially Functional Materials and Institute of Optical Communication Materials, South China University of Technology, Guangzhou 510641 (China)

2010-05-15T23:59:59.000Z

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
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181

E-Print Network 3.0 - alpha class glutathione Sample Search Results  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

the Detoxification of 2-Phenylpropenal, a Reactive Summary: of the genotoxic aldehyde acrolein by human glutathione transferases of classes alpha, pi, and mu. Mol. Pharmacol......

182

Measurement of the W Gamma --> mu nu gamma Cross-Section, Limits on Anomalous Trilinear Vector Boson Couplings, and the Radiation Amplitude Zero in p anti-p Collisions at s**(1/2) = 1.96 TeV  

SciTech Connect (OSTI)

This thesis details the measurement of the p{bar p} {yields} W{gamma} + X {yields} {mu}{nu}{gamma} + X cross section at {radical}s = 1.96 TeV using the D0 detector at Fermilab, in 134.5 pb{sup -1} of integrated luminosity. From the photon E{sub T} spectrum limits on anomalous couplings of the photon to the W are obtained. At 95% confidence level, limits of -1.05 < {Delta}{kappa} < 1.04 for {lambda} = 0 and -0.28 < {lambda} < 0.27 for {Delta}{kappa} = 0 are obtained on the anomalous coupling parameters. The charge signed rapidity difference from the data is displayed, and its significance discussed.

Askew, Andrew Warren

2004-11-01T23:59:59.000Z

183

Optical remote monitoring of CH/sub 4/ gas using low-loss optical fiber link and InGaAsP light-emitting diode in 1. 33-. mu. m region  

SciTech Connect (OSTI)

Purely optical remote monitoring of low-level CH/sub 4/ gas is realized for the first time by the method employing a 2-km long-distance, low-loss silica optical fiber link and a compact absorption cell in conjunction with a high radiant InGaAsP light-emitting diode (LED) at 1.33 ..mu..m. Based on the present experiment, the detection limit of CH/sub 4/ in air was confirmed to be approximately 2000 ppm, i.e., 4% of the lower explosion limit of CH/sub 4/. This result supports the conclusion that the fully optical remote sensing system incorporating ultralow loss optical fiber networks and near infrared LEDs or laser diodes can be extensively used for the detection and surveillance of various inflammable and/or explosive gases in industrial and mining complexes as well as in residential areas.

Chan, K.; Ito, H.; Inaba, H.

1983-10-01T23:59:59.000Z

184

Some conclusive considerations on the comparison of the ICARUS nu_mu to nu_e oscillation search with the MiniBooNE low-energy event excess  

E-Print Network [OSTI]

A sensitive search for anomalous LSND-like nu_mu to nu_e oscillations has been performed by the ICARUS Collaboration exposing the T600 LAr-TPC to the CERN to Gran Sasso (CNGS) neutrino beam. The result is compatible with the absence of additional anomalous contributions giving a limit to oscillation probability of 3.4E-3 and 7.6E-3 at 90% and 99% confidence levels respectively showing a tension between these new limits and the low-energy event excess (200 energy excess has been performed, including the energy resolution as obtained from the official MiniBooNE data release. As a result the previously reported tension is confirmed at 90% C.L., suggesting an unexplained nature or an otherwise instrumental effect for the MiniBooNE low energy event excess

Antonello, M; Benetti, P; Boffelli, F; Bubak, A; Calligarich, E; Centro, S; Cesana, A; Cieslik, K; Cline, D B; Cocco, A G; Dabrowska, A; Dermenev, A; Falcone, A; Farnese, C; Fava, A; Ferrari, A; Gibin, D; Gninenko, S; Guglielmi, A; Haranczyk, M; Holeczek, J; Kirsanov, M; Kisiel, J; Kochanek, I; Lagoda, J; Mania, S; Menegolli, A; Meng, G; Montanari, C; Otwinowski, S; Picchi, P; Pietropaolo, F; Plonski, P; Rappoldi, A; Raselli, G L; Rossella, M; Rubbia, C; Sala, P; Scaramelli, A; Sergiampietri, F; Stefan, D; Sulej, R; Szarska, M; Terrani, M; Torti, M; Varanini, F; Ventura, S; Vignoli, C; Wang, H; Yang, X; Zalewska, A; Zani, A; Zaremba, K

2015-01-01T23:59:59.000Z

185

Supporting Information Copyright Wiley-VCH Verlag GmbH & Co. KGaA, 69451 Weinheim, 2013  

E-Print Network [OSTI]

CHCl3 or anhydrous MeOH. #12;2 11: Allyl palladium chloride dimer (1.69 g, 4.6 mmol) and 1,2-bis(diphenylphosphino)ethane (9.20 g, 23 mmol) were dissolved in anhydrous THF (1000 ml), then allyl acetate (50.0 ml, 0.46 mol), 1,3-cyclopentadione (10, 45.0 g, 0.46 mol), N

Theodorakis, Emmanuel

186

Properties of Diazocarbene [CNN] and the Diazomethyl Radical [HCNN] via Ion Chemistry and Spectroscopy  

E-Print Network [OSTI]

endothermic, rxnH0 ) 1.6 ( 0.7 kcal mol-1 . I. Introduction In an internal combustion engine, air known1 for some time that "thermal" NO is generated in the post- combustion region by the Zeldovich mechanism involving O atoms and N2. In most combustion processes, hydrocarbons are degraded to produce

Ellison, Barney

187

Agricultural and Forest Meteorology 119 (2003) 5368 Partitioning overstory and understory evapotranspiration  

E-Print Network [OSTI]

relative humidity [H2O] water vapor concentration (mmol mol-1) R molar ratio of heavy to light isotopes to light isotopes of water from soil evaporation Rs molar ratio of heavy to light isotopes of soil water evapotranspiration in a semiarid savanna woodland from the isotopic composition of water vapor Enrico A. Yepeza

188

Crossed Molecular Beams Study on the Formation of Vinylacetylene in Titan's Atmosphere Fangtong Zhang, Yong Seol Kim, and Ralf I. Kaiser*  

E-Print Network [OSTI]

), was investigated at a collision energy of 20.6 ( 0.4 kJ mol-1 utilizing the crossed-beams technique. Combined such as Titan's atmosphere via the neutral-neutral reaction of ethynyl radicals with ubiquitous ethylene and their role in the build-

Kaiser, Ralf I.

189

ORIGINAL PAPER Aragonite Kinetics in Dilute Solutions  

E-Print Network [OSTI]

), geothermal energy production (Arnorsson 1979; Amjad 1987), and waste treatment (Reddy 1978). More recently. From these data, an Arrhenius activation energy of 71.2 kJ mol-1 is cal- culated for the heterogeneous Department of Oceanography, Texas A&M University, College Station, TX 77843, USA E. L. Grossman Department

Grossman, Ethan L.

190

Quantum Chemical Calculations of Sulfate Adsorption at the Al-and  

E-Print Network [OSTI]

Quantum Chemical Calculations of Sulfate Adsorption at the Al- and Fe-(Hydr)oxide-H2O Interfaces to estimate relative Gibbs free energies of sulfate adsorption on variably charged Al- and Fe on positively charged Al- and Fe- (hydr)oxides (ranging from -19 to -124 kJ mol-1). However, inner-sphere and H

Sparks, Donald L.

191

Study of Interfacial Charge-Transfer Complex on TiO2 Particles in Aqueous Suspension by Second-Harmonic Generation  

E-Print Network [OSTI]

/mol. 1. Introduction Titanium dioxide (TiO2) is a wide band-gap semiconductor having two common crystal, the adsorption isotherm of catechol on the colloidal TiO2 suspension was obtained and gave an excellent fit to the Langmuir adsorption model. From this, we infer the free energy of the adsorption to be G° ) -6.8 kcal

Eisenthal, Kenneth B.

192

Calcite Reaction Kinetics in Saline Waters  

E-Print Network [OSTI]

with the calcite surface than K^ or that water is less available in NaCl solutions. Rates increased with increasing pCO2 and temperature, and their influence diminished at high I. Arrhenius plots yielded a relatively high activation energy (Ea ? 20 ± 2 kJ mol-1...

Finneran, David

2012-02-14T23:59:59.000Z

193

Insight into Proton Transfer in Phosphotungstic Acid Functionalized Mesoporous Silica-Based Proton Exchange Membrane Fuel Cells  

E-Print Network [OSTI]

University, Perth, Western Australia 6102, Australia Materials and Process Simulation Center, California 138632, Singapore § Fuels and Energy Technology Institute & Department of Chemical Engineering, Curtin humidity (RH) with a low activation energy of 14 kJ mol-1 . In order to determine the energetics associated

Goddard III, William A.

194

Physical Models of Noncovalent Interactions Involving Aromatic Rings  

E-Print Network [OSTI]

-aromatic rings are often quite favourable. For example, the above computed interaction energies for model ethene-benzene and butadiene-benzene complexes are substantial (–0.85 and –1.50 kcal mol–1 for ethene and butadiene, respectively). In the latter case...

Bloom, Jacob Walter Goldstein

2014-04-17T23:59:59.000Z

195

Cubane, Cuneane, and Their Carboxylates: A Calorimetric, Crystallographic, Calculational, and Conceptual Coinvestigation  

E-Print Network [OSTI]

Henares, Spain, Department of Chemistry & Biochemistry, University of Missouri St. Louis, 8001 Natural Bridge Road, St Louis, Missouri 63121-4499, Department of Chemistry & Biochemistry, University, fH°m(cr)/kJ,mol-1 ) -232.62 ( 5.84 and -413.02 ( 5.16, respectively. The enthalpies of sublimation

Chickos, James S.

196

Kinetics of Thermal Decomposition of Cubic Ammonium Perchlorate  

E-Print Network [OSTI]

. Wight* Center for Thermal Analysis, Department of Chemistry, University of Utah, 315 S., 1400 E., Salt to dissociative sublimation of AP. A new computational technique (advanced isoconversional method) has been used respectively rises to 110 and 130 kJ mol-1, which are assigned to the activation energy of sublimation

Utah, University of

197

Methane Activation with Rhenium Catalysts. 1. Bidentate Oxygenated Ligands  

E-Print Network [OSTI]

Methane Activation with Rhenium Catalysts. 1. Bidentate Oxygenated Ligands Jason M. Gonzales, Jonas, California 90089 ReceiVed July 31, 2006 Trends in methane activation have been explored for rhenium complexes proceeds with methane activation through a barrier of less than 35 kcal mol-1 . Study

Goddard III, William A.

198

Crystal ball 2011mbt_245 109..137 In this feature, leading researchers in the field of microbial  

E-Print Network [OSTI]

, lowering the pH from ~7 to ~5.8, acetate (-26.9 kJ e-mol-1 ) accumulates because hydrogenotrophic metha methanogens as well, and will shift the fermentation end-product spectrum to a mixture of carboxylates (e cell residence times, n-butyrate is often found at high relative ratios within the fermentation product

Angenent, Lars T.

199

J. Mol. Biol. (1995) 245, 151179 Structural and Mechanistic Analysis  

E-Print Network [OSTI]

phenol-lyase; PPL-Cys-Hg, N-(5'-phosphopyridoxyl)-S-methylmercuri-L-cysteine; MIR, multiple isomorphous

Toney, Michael

200

Unstructured Adaptive Mesh MOL Solvers for Atmospheric Reacting  

E-Print Network [OSTI]

. Achieving high resolution in air pollution models is a difficult challenge because of the large number for the next generation of air pollution models in order to "capture important smaller scale atmospheric in understanding the complex processes which lead to the formation of pollutants such as greenhouse gases, acid

Utah, University of

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


201

CafeMol (www.cafemol.org) Features are;  

E-Print Network [OSTI]

$ pjqstat display job status(-A:all user) $ pjdel [JOBID] cancel job $ pjsub --interact interactive job e directory of native info files >>>> job_cntl i_run_mode = 2 2:constat T, 6:REMD i_simulate_type = 1 1(essential block 2) energy_function LOCAL(1) L_GO local energy L_GO, L_AICG2_PLUS, L_BDNA NLOCAL(1/1) GO EXV

Fukai, Tomoki

202

12/17/07 10:32 AMMU Researcher Develops Origin-Of-Life Theory for Young Earth -freshare.net Page 1 of 2http://www.freshare.net/exp/article/mu_researcher_develops_origin_of_life_theory_for_young_earth/list/  

E-Print Network [OSTI]

.niagarafrontierbible.com Creation Books &Creation Books & DVDsDVDs One of the largest selections of Creation books and DVDs of adenine, an essential organic molecule. Without it, the basic building blocks of life would not come is not outrageous," said Glaser, professor of chemistry in MU's College of Arts and Science. "You can find large

Glaser, Rainer

203

Page 1 of 2 Pi Gamma Mu  

E-Print Network [OSTI]

Fielding Lewis, Leon Walls, Denise Dunbar, Mediha Jusufagi, Harri Williams and, Robert Skiff. 1. Call selections c) Harri Williams will be in charge of refreshments d) Yolanda Flores will read the history e.6 Pictures for our website: A note of gratitude to our members Jeff Bukowski for the design of the society

Hayden, Nancy J.

204

RESEARCH PAPER Florin Iancu Norbert Mu ller  

E-Print Network [OSTI]

in 1995, with the MIT ``Micro Gas Turbine'' project, the engineering research world has explored F. Iancu in the 10­100 kW range), the concept of ultra-micro gas turbines (UlGT) has been introduced to define

Müller, Norbert

205

Charter Members History of Pi Mu Epsilon  

E-Print Network [OSTI]

Daniel Frey Jacob P. Gagnon Brittany Marie Grenzig James M Grippe Risa Gul Matthew Joseph Hems Nicholas S Guzman Matthew E. Hassell Kevin A. Kass Adam A. Sasson Prof. Dmytro Savchuk Jessica M. Tchorowski Prof Joining in 2014 Daniel Irmihaev Taylor Rose Juran Garreth Joshua Kaplan Navdep Kaur Colleen Kearney

Feingold, Alex

206

MU TRAVEL CARD CARDHOLDER ENROLLMENT / CHANGE FORM  

E-Print Network [OSTI]

: _______________________ Office Phone #: _____________________________ Cell Phone #: _______________________________ Email address: ______________ Approval Purchasing Director __________________________ Date : ____________ JP MorganChase Data User ID: ______________ Password: _____________ User Role: _________________ Control Group ________ Purchasing Department Revised

Hardy, Christopher R.

207

MU(& Ge-+v,  

Office of Legacy Management (LM)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) "ofEarlyEnergyDepartment ofDepartment ofof EnergyYou$ EGcG ENERGYELIkNATIONHEALXH:LTS-S,:?' _.JMOUNDI'

208

Thenature of marbled Terra Sigillata slips: a combined mu XRF and mu XRD investigation  

SciTech Connect (OSTI)

In addition to the red terra sigillata production, the largest Gallic workshop (La Graufesenque) made a special type of terra sigillata, called 'marbled' by the archaeologists. Produced exclusively on this site, this pottery is characterized by a surface finish made of a mixture of yellow and red slips. Because the two slips are intimately mixed, it is difficult to obtain the precise composition of one of the two constituents without contamination by the other. In order to obtain very precise correlation at the appropriate scale between the color aspect and the element and mineralogical phase distributions in the slip, combined electron microprobe, x-ray micro spectroscopies and micro diffraction on cross sectional samples were performed. The aim is to discover how potters were able to produce this unique type of terra sigillata and especially this slip showing an intense yellow color. Results show that the yellow component of marbled sigillata was made from a titanium-rich clay preparation. The color is related to the formation of a pseudobrookite (TiFe2O5) phase in the yellow part of the slip, the main characteristics of that structure being considered nowadays as essential for the fabrication of stable yellow ceramic pigments. Its physical properties such as high refractive indices and a melting point higher than that of most silicates widely used as ceramic colorants are indeed determinant for this kind of applications. Finally, the red parts have a similar composition (elementary and mineralogical) to the one of standard red slip.

Leon, Yoanna; Sciau, Philippe; Goudeau, Philippe; Tamura, Nobumichi; Webb, Sam; Mehta, Apurva

2009-01-31T23:59:59.000Z

209

The nature of marbled Terra Sigillata slips: a combined mu XRF and mu XRD investigation  

E-Print Network [OSTI]

Sigillata slips: a combined µXRF and µXRD investigation Y.and micro x-ray fluorescence (µXRF), as it makes correlationthe highest quality µXRD and µXRF measurements we decided to

Leon, Yoanna

2009-01-01T23:59:59.000Z

210

NEWS & VIEWS nature materials | VOL 4 | DECEMBER 2005 | www.nature.com/naturematerials 883  

E-Print Network [OSTI]

the sphalerite form. There is a free-energy difference of ~13 kJ mol­1 between the sphalerite and wurtzite forms. This is essential knowledge for preparing ZnS products of the desired structure, and suggests a strategy and defects, and can be up to several millimetres long. The local structure of both forms of ZnS is the same6

Downs, Robert T.

211

The archaeomalacology of four middle to late preceramic (5000-1800 BC) sites on the central coast of Peru  

E-Print Network [OSTI]

). Other sources in the literature classify molluscan use by geographical region. Molluscs as food resources are described in Australia (Bailey 1975), New Zealand (Shawcross 1967; Snow 1972), Europe (Clark 1966), the Near East (Flannery 1969) amd... of molluscan species as well as other marine and terrestrial resources to meet nutritional requirements, The mol 1 us- can faunal assembly indicates the mixed rocky/sandy littoral envir- onments of the middle preceramic shifted to more rocky littoral en...

Capps, Keith William

1987-01-01T23:59:59.000Z

212

Formation of the diphenyl molecule in the crossed beam reaction of phenyl radicals with benzene  

E-Print Network [OSTI]

February 2008 The chemical dynamics to form the D5-diphenyl molecule, C6H5C6D5, via the neutral-neutral experiment at a collision energy of 185 kJ mol-1 . The laboratory angular distribution and time, diphenyl C6H5C6H5 , which is considered as a building block to form anthracene and more complex PAHs

Kaiser, Ralf I.

213

GS-2013 (Chemistry) TATA INSTITUTE OF FUNDAMENTAL RESEARCH  

E-Print Network [OSTI]

-1 Boltzmann constant k = 1.38Ã?10-23 J K-1 R = 8.314 J K-1 mol-1 En = 2 2 2n Z - a.u. for hydrogen a plane of symmetry and B has a 2-fold rotation axis; B is chiral #12;Page 2 of 12 4. The methodH becomes less than optimal C) Substrate concentration increases D) All of the above 6. Predict the products

Bhalla, Upinder S.

214

Formulas/Constants: Physics/Oceanography 4500/5500 A Atmospheric Physics In addition to these formulas, there are many thermodynamic concepts and interrelationships between  

E-Print Network [OSTI]

at the lifting condensation level: TLCL = 9.8Tdo - 1.8To 8 Entropy S = S0 + CV ln( TV -1 T0V -1 0 ) where T0 weight of each consituent. R = 8.314 J mol-1 K-1 is the universal gas constant. p = RdTv (for moist air where Tv is the virtual temperature) Rv = 461.5 J/(kg K) (ideal gas constant for water vapor) = Mv

Folkins, Ian

215

Description of coordinatively unsaturated sites regeneration over MoS2-based HDS catalysts using 35  

E-Print Network [OSTI]

envisaged. Moreover, on the sulfur edge the H2S release activation energy is too high (~ 13.5 kcal.mol-1 likely to occur on the MoS2 metallic edge through the departure of an H2S molecule. In the present paper, we aimed at examining the H2S departure from MoS2 catalysts promoted with Co and Ni. The [35 S

Boyer, Edmond

216

1 Copyright 2014 by ASME A SOFT COMBUSTION-DRIVEN PUMP FOR SOFT ROBOTS  

E-Print Network [OSTI]

reach output flows up to 40 ml/min. Methane (CH4) combustion is used as the actuation source. The pump + 2H2O + 3.76N2 ­ 891kJ/mol (1) where the energy is released as heat. Air was used instead of pure1 Copyright © 2014 by ASME A SOFT COMBUSTION-DRIVEN PUMP FOR SOFT ROBOTS Constantinos Stergiopulos

Wood, Robert

217

Water and Carbon Dioxide Adsorption at Olivine Surfaces  

SciTech Connect (OSTI)

Plane-wave density functional theory (DFT) calculations were performed to simulate water and carbon dioxide adsorption at the (010) surface of five olivine minerals, namely, forsterite (Mg2SiO4), calcio-olivine (Ca2SiO4), tephroite (Mn2SiO4), fayalite (Fe2SiO4), and Co-olivine (Co2SiO4). Adsorption energies per water molecule obtained from energy minimizations varied from -78 kJ mol-1 for fayalite to -128 kJ mol-1 for calcio-olivine at sub-monolayer coverage and became less exothermic as coverage increased. In contrast, carbon dioxide adsorption energies at sub-monolayer coverage ranged from -20 kJ mol-1 for fayalite to -59 kJ mol-1 for calcio-olivine. Therefore, the DFT calculations show a strong driving force for carbon dioxide displacement by water at the surface of all olivine minerals in a competitive adsorption scenario. Additionally, adsorption energies for both water and carbon dioxide were found to be more exothermic for the alkaline-earth (AE) olivines than for the transition-metal (TM) olivines and to not correlate with the solvation enthalpies of the corresponding divalent cations. However, a correlation was obtained with the charge of the surface divalent cation indicating that the more ionic character of the AE cations in the olivine structure relative to the TM cations leads to greater interactions with adsorbed water and carbon dioxide molecules at the surface and thus more exothermic adsorption energies for the AE olivines. For calcio-olivine, which exhibits the highest divalent cation charge of the five olivines, ab initio molecular dynamics simulations showed that this effect leads both water and carbon dioxide to react with the surface and form hydroxyl groups and a carbonate-like species, respectively.

Kerisit, Sebastien N.; Bylaska, Eric J.; Felmy, Andrew R.

2013-11-14T23:59:59.000Z

218

Struct Chem DOI 10.1007/s11224-006-9111-4  

E-Print Network [OSTI]

,6-14 dien-2-one (2, fHm = - 79.7 ± 22.9 and 20.1 ± 23.115 kJ mol-1 ) are reported. Sublimation enthalpies of General Chemistry, Polytechnic University of Bucharest, 1 Polizu str., Bucharest 78126, Romania e-mail: s perisanu@chim.upb.ro I. Contineanu Institute of Physical Chemistry of the Romanian Academy, spl

Chickos, James S.

219

A SPRAY REACTOR CONCEPT FOR CATALYTIC OXIDATION OF P-XYLENE TO PRODUCE HIGH-PURITY TEREPHTHALIC ACID  

E-Print Network [OSTI]

analyzing and solving problems, about perseverance and staying positive when research hits a snag. Prof. Subramaniam has been and will always be a great mentor and an invaluable asset to me. Special thanks are also due to Prof. Daryle Busch, Prof. Raghunath...: T = 200 °C, P = 15 bar; Initial pX = 25 mM, Co = 12.5 mM, Mn = 12.5 mM, Br = 32.5 mM; O2:CO2 (mol:mol) = 1:1) ....................................42 Figure 2.9 Figure 2.9: Color changes of the reaction solution due to the formation of various cobalt...

LI, MENG

2013-08-31T23:59:59.000Z

220

1224 Mol. BioSyst., 2011, 7, 12241231 This journal is c The Royal Society of Chemistry 2011 Cite this: Mol. BioSyst., 2011, 7, 12241231  

E-Print Network [OSTI]

vancomycin against MRSA as they carry an extra aliphatic acyl side chain on glucosamine (Glm) at residue 4 (r the drugs of the last resort to treat methicillin-resistant Staphylococcus aureus (MRSA) infections. Lipoglycopeptides, Tei and A40926 (3, Fig. 1) were reported to be more effective than vancomycin against MRSA

Tsai, Ming-Daw

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


221

1316 Mol. BioSyst., 2013, 9, 1316--1325 This journal is c The Royal Society of Chemistry 2013 Cite this: Mol. BioSyst., 2013,  

E-Print Network [OSTI]

in human health exposure and environmental hazard assessment, because chemical­gene­disease networks could, industrial chemicals, pesticides, and other environmental agents provide an invaluable opportunity to extend integrate three networks of chemical­gene interactions (CGIs), chemical­disease associations (CDAs) and gene­disease

Timmer, Jens

222

PSI activity, MuCap, MuSun 1. P. Winter and MuCap collaboration. Muon Capture on the Proton. International  

E-Print Network [OSTI]

on 22 Apr 2011 arXiv:1104.4421. 15. R. Engels, R. Emmerich, K. Grigoryev, P. Kravtsov, L. Kochenda, M.Phys.Conf.Ser. 295 (2011) 012161 16. H. Seyfarth, V. Baryshevsky, C. Duweke, R. Emmerich, R. Engels, K. Grigoryev, A

Titov, Anatoly

223

Gas-Phase Oxidation of Cm+ and Cm2+ -- Thermodynamics of neutral and ionized CmO  

SciTech Connect (OSTI)

Fourier transform ion cyclotron resonance mass spectrometry was employed to study the products and kinetics of gas-phase reactions of Cm+ and Cm2+; parallel studies were carried out with La+/2+, Gd+/2+ and Lu+/2+. Reactions with oxygen-donor molecules provided estimates for the bond dissociation energies, D[M+-O](M = Cm, Gd, Lu). The first ionization energy, IE[CmO], was obtained from the reactivity of CmO+ with dienes, and the second ionization energies, IE[MO+](M = Cm, La, Gd, Lu), from the rates of electron-transfer reactions from neutrals to the MO2+ ions. The following thermodynamic quantities for curium oxide molecules were obtained: IE[CmO]= 6.4+-0.2 eV; IE[CmO+]= 15.8+-0.4 eV; D[Cm-O]= 710+-45 kJ mol-1; D[Cm+-O]= 670+-40 kJ mol-1; and D[Cm2+-O]= 342+-55 kJ mol-1. Estimates for the M2+-O bond energies for M = Cm, La, Gd and Lu are all intermediate between D[N2-O]and D[OC-O]--i.e., 167 kJ mol-1< D[M2+-O]< 532 kJ mol-1 -- such that the four MO2+ ions fulfill the thermodynamic requirement for catalytic O-atom transport from N2O to CO. It was demonstrated that the kinetics are also favorable and that the CmO2+, LaO2+, GdO2+ and LuO2+ dipositive ions each catalyze the gas-phase oxidation of CO to CO2 by N2O. The CmO2+ ion appeared during the reaction of Cm+ with O2 when the intermediate, CmO+, was not collisionally cooled -- although its formation is kinetically and/or thermodynamically unfavorable, CmO2+ is a stable species.

Gibson, John K; Haire, Richard G.; Santos, Marta; Pires de Matos, Antonio; Marcalo, Joaquim

2008-12-08T23:59:59.000Z

224

A Translator for ISIS and TRIUMF MuSR Data  

E-Print Network [OSTI]

ISIS data, fit byvii ISIS List of Tables Grouping rules for a transverse-The Hardware . . 3.3 The ISIS NeXus Data Format 3.4 The

Mackie, John Morgan

2011-01-01T23:59:59.000Z

225

NSF, MU chemistry program combines science with current news  

E-Print Network [OSTI]

science centers & arts science departments & arts science people & arts science projects & arts science site last updated August 2004 copyright Project Home . . . College of Arts and Science . . . University of Arts and Science Research Communication Project story Page 2 of 2http

Glaser, Rainer

226

anti mu events: Topics by E-print Network  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

in a secluded sector, leading to a final state with a dark photon U and a dark Higgs boson h', with the KLOE detector at DAFNE. We investigated the case of h' lighter than U,...

227

The design and implementation of the [mu]Modelica compiler.  

E-Print Network [OSTI]

??Modelica is a recently developed object-oriented language for physical systems modeling. It is a modern language built on non-causal modeling with mathematical equations and object-oriented… (more)

Xu, Weigao, 1974-

2005-01-01T23:59:59.000Z

228

Interplay between Domain Mu-Calculus and Formal Languages  

E-Print Network [OSTI]

of type , and inl , inr are formulas of type . If is a formula of type [rec t, ) or (, b) is a member of ([[

Zhang, Guo-Qiang

229

Reconciling leptogenesis with observable mu --> e gamma rates  

E-Print Network [OSTI]

We perform a detailed analysis of thermal leptogenesis in the framework of seesaw models which approximately conserve lepton number. These models are known to allow for large Yukawa couplings and a low seesaw scale in agreement with neutrino mass constraints, and hence to lead to large lepton flavour violating rates that can be probed experimentally. Although large Yukawa couplings lead to (inverse) decay rates much larger than the Hubble expansion rate, we show that the leptogenesis washout induced is generically small if the mass splitting between the right-handed neutrinos is small enough. As a result, large lepton flavour violating rates are compatible with successful leptogenesis. We emphasize that this scenario does not require any particular flavour structure. A small splitting is natural and radiatively stable in this context because it is protected by the lepton number symmetry.

Steve Blanchet; Thomas Hambye; Francois-Xavier Josse-Michaux

2010-02-15T23:59:59.000Z

230

The {mu}Mural : a six-projector tiled display.  

SciTech Connect (OSTI)

Tiled displays have become a recent technical solution to aggregating commodity displays in order to provide higher resolution displays. This document describes the background, design, and implementation of the micromural, a six projector tiled display developed at Argonne National Laboratory.

Judson, I. R.

2002-06-27T23:59:59.000Z

231

A MEASUREMENT OF THE POSITIVE pi- Mu DECAY LIFETIME  

E-Print Network [OSTI]

Idaho Operations Office Iowa State College Kansas City Operations Branch Kellex Corporation Knolls Atomic Power Laboratory Los Alamos Scientific

Chamberlain, O.; Mozely, R.F.; Steinberger, J.; Wiegand, C.

2008-01-01T23:59:59.000Z

232

TB Testing Information MU HEALTH SERVICES, WITMER BUILDING  

E-Print Network [OSTI]

, if needed, will be permitted for paper-based requests of ACT 34. ACT 114 (FBI FEDERAL CRIMINAL HISTORY)* Request paper copy of the FBI Fingerprinting results and obtain Registration Identification Number (starts IDENTIFICATION NUMBER FOR YOUR ACT 114 (FBI FINGERPRINTING) clearance. You may present them in person, via fax

Hardy, Christopher R.

233

Games and Modal Mu-Calculus Colin Stirling  

E-Print Network [OSTI]

of authors has noted that it is essentially game theoretic 3, 18, 16] (and 15] extends this description, Edinburgh EH9 3JZ, UK, email: cps@dcs.ed.ac.uk #12;112 Colin Stirling checking algorithms: furthermore

Stirling, Colin

234

Helio Micro Utility Helio mU | Open Energy Information  

Open Energy Info (EERE)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home5b9fcbce19 No revision hasInformation Earth's Heat Jump to:Photon Place:NetHealth Division

235

.I. Mol. Biol. (1984) 179, 55-81 Microsecond Rotational Motions of Eosin-labeled Myosin  

E-Print Network [OSTI]

of Biochemistry l!niversity of Minnesota Medical 8chool Minneapolis, MN 554.5.5. lT.S..A. ROBERT H. AUSTIN

Thomas, David D.

236

J. Mol. Biol. (1995) 252, 672708 Acid and Thermal Denaturation of Barnase  

E-Print Network [OSTI]

.g. on tyrosine and tryptophan sidechains. The hydrogen-bonding propensity of the water molecules tends structural elements, where water molecules compete with the interstrand and intrahelical hydrogen bonds state to a partially unfoldedDepartment of Chemistry conformation has been studied by molecular dynamics

Caflisch, Amedeo

237

RasMol v2.5 A Molecular Visualisation Program  

E-Print Network [OSTI]

Incorporated. Alchemy and Sybyl are trademarks of Tripos Associates Inc. VAX is a trademark of Digital&S workstations, DEC Alpha (OSF/1, OpenVMS and Windows NT), IBM RS/6000, Cray, Sequent, VAX VMS (under DEC windows

Meagher, Mary

238

J. Mol. Model. 2000, 6, 65 66 Springer-Verlag 2000PREFACE  

E-Print Network [OSTI]

about structure and bonding. John Pople described his interaction with Paul at this stage, electronic properties, energies and a host of other information was the start of a new direc- tion and remark- able in the history of chemistry. I remember well the heady days of "STO-3G-lithium

Glaser, Rainer

239

Mol Biosyst . Author manuscript Strong and oriented immobilization of single domain antibodies from  

E-Print Network [OSTI]

-Throughput Screening Assays ; economics ; methods ; Humans ; Immobilized Proteins ; metabolism ; Immunoassay ; Protein to monitor mRNA abundance from small amount of materials. However, this approach is biased by the lack of relation between mRNA and proteins abundance, and is not sufficient to understand complex cellular networks

Paris-Sud XI, Université de

240

J. Mol. Biol. (1991) 220, 133-149 Analysis of Protein Loop Closure  

E-Print Network [OSTI]

). Next, there are hinge movements of domains, e.g. in the immunoglobulins (Bennet & Huber, 1984; Lesk

Gerstein, Mark

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


241

J. Mol. Biol. (1985) 181, 423447 Protein Normal-mode Dynamics: Trypsin Inhibitor,  

E-Print Network [OSTI]

, especiallv collective motion, is important for protein function (see review by Huber & Bennet!t, 1983). Bv

Levitt, Michael

242

Int. J. Mol. Sci. 2008, 9, 679-697 International Journal of  

E-Print Network [OSTI]

used by different organisms, even within the same organism the nuclear and mitochondrial genes may on genes subject to mutations, and have estimated how these genes "survive" over generations. We have used ­ Crick [1] had postulated the coevolution and frozen accident hypotheses, where similar amino acids would

Kurnaz, Levent

243

J Mol Model (2006) 12: 611619 DOI 10.1007/s00894-005-0068-9  

E-Print Network [OSTI]

­Cr­Mn and of Ni­Co­Mo­Mn (10% spacing) have been measured for the oxidation of propene to acroleine. The data have Selective oxidation . Acroleine materials modeling . Kriging . Heterogeneous catalysts . Composition

Hamprecht, Fred A.

244

Curr Mol Med . Author manuscript ACE inhibition prevents diastolic Ca2+ overload and loss of myofilament  

E-Print Network [OSTI]

-volume loops revealed that MI induced hypertrophy and dilatation, and altered both contraction and relaxation ; pharmacology ; therapeutic use ; Animals ; Calcium ; metabolism ; Diastole ; Disease Models, Animal Calcium Release Channel ; metabolism ; Sarcoplasmic Reticulum ; metabolism ; Ventricular Remodeling ; drug

Boyer, Edmond

245

=5*10^19 Pa*s R=8.31 J/mol*K  

E-Print Network [OSTI]

the role of viscoelastoplasticity, we numerically model subduction initiation at an extinct ridge-transform dependent Newtonian viscosity[4] and a temperature dependent power-law rheology[1] . Some models include the experimentalists. Inside the Subduction Factory, Eiler, J., ed., vol. 138 of Geophysical Monograph. 5. Schubert, G

Meng, Ellis

246

Cell. Mol. Life Sci. 62 (2005) 31063116 1420-682X/05/243106-11  

E-Print Network [OSTI]

towards sper- mine. Despite the reduced uptake, the resistant strains ac- cumulated significant levels of polyamines and displayed increased ornithine decarboxylase activity, suggesting re- duced polyamine sensing stimulate proliferation and metastasis of cancer cells they have become a target for therapeutic efforts [3

Kahana, Chaim

247

J. Mol. Biol. (1984) 177, 201-206 Some X-ray Diffraction Patterns from  

E-Print Network [OSTI]

awaits a molecular model. In vivo and in vitro produced two-dimensional sheets and helices have been methanol (type M) or a mixture of methanol and ethylene glycol (type ME). Sharp, resolvable patterns% (v v methanol at pH 8.7, using a modified version of' the/ ) crystallization method described

Yonath, Ada E.

248

J Mol Cell Cardiol 29, 3175-3188 (1997) Feature Article  

E-Print Network [OSTI]

d a ' ,Steven L. Roberds2,Emma ~older', Teresa ~ohlmeyer',James B. Young3and Kevin P. Campbell2,M. MAEDA,S. L. ROBERDS,E. HOLDER,T. BOHLMEYER,J. B. YOUNGAND K. P. CAMPBELL.A 5' Dystrophin Duplication associated amples where a mutation in the gene encoding the with a high mortality (Goldstein and Brown, 1988

Campbell, Kevin P.

249

J. Mol. Biol. (1996) 259, 970987 Solution Structure of the Granular Starch Binding  

E-Print Network [OSTI]

, 1991; PDB, accession code, 1cgt); 1D, one-dimensional; 2D, two-dimensional; 3D, three-dimensional; bCD (Lawson et al. 1994; PDB accession code, 1cdg); 1CGT, crystal structure of free CGTase (Klein & Schulz

Williamson, Mike P.

250

Mol Gen Genet (1985) 201:409-414 Springer-Verlag1985  

E-Print Network [OSTI]

by the deficiency sDf2 (Moerman and Baillie 1981). Previous genetic studies of the unc-22 region of linkage group IV of the region defined by sDf2. We expand and refine the existing unc-22 fine-structure map and position University: s7, s8, s12, s18 and s32 (Moerman and Baillie 1979), s35, s36, sDf2, sDf7, sDfS, sDf9, s

Baillie, David

251

Mol Gen Genet (1993)236:289-298 MGG Springer-Verlag 1993  

E-Print Network [OSTI]

-hand breakpoints of the deficiencies sDf9, sDfl9 and sDf65. This small interval at present contains a single breakpoint of sDfl9 and the left breakpoint of sDf65, between the essential genes let-653 and let-56. Key content of a specific region, the 2 map unit unc-22(IV) region, defined by the deficiency sDf2

Baillie, David

252

J. Mol. Model. 2000, 6, 498 516 Springer-Verlag 2000FULL PAPER  

E-Print Network [OSTI]

constraints of the target protein, LigBuilder builds up ligands step by step using a library of organicBuilder is able to generate chemical structures similar to the known ligands. Keywords Structure-based drug design as de novo design. In this case, ligand molecules are built up within the constraints of the binding

Luhua, Lai

253

Plant Mol Biol DOI 10.1007/s11103-014-0247-0  

E-Print Network [OSTI]

. Microarray data gen- erated from wild-type and dhu1 under low doses of UV-B revealed that 209 or 124 genes under low doses of UV-B. Other light did not alter hypocotyl growth patterns in dhu1, indicating to bind to DDB1, an adaptor of CRL4; accordingly, DHU1 is thought to act as a substrate receptor of CRL4

Deng, Xing-Wang

254

MOL.19980331.0174 PARTICULATE MATTEX AMBIENT A I R QUALITY  

National Nuclear Security Administration (NNSA)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) "ofEarlyEnergyDepartmentNationalRestart of the Review of theOFFICEACMEFUTURE MOBILITYMarchUnitedrLead9/%2A

255

J. Mol. Biol. (1996) 259, 988994 Local Interactions Dominate Folding in a Simple  

E-Print Network [OSTI]

Unger1,2 * and John Moult2 Recent computational studies of simple models of protein folding have1 Press Limited Keywords: protein folding; lattice models; local interactions*Corresponding author Introduction What are the dominant contributions guiding the process of protein folding? The short life

Unger, Ron

256

Fixation of atmospheric CO[sub 2] by a series of hydroxo complexes of divalent metal ions and the implication for the catalytic role of metal ion in carbonic anhydrase. Synthesis, characterization, and molecular structure of [LM(OH)][sub n] (n = 1 or 2) and LM([mu]-CO[sub 3])ML (M(II) = Mn, Fe, Co, Ni, Cu, Zn; L = HB(3,5-iPr[sub 2]pz)[sub 3])  

SciTech Connect (OSTI)

By using the hindered tris(pyrazoly)borate ligand HB(3,5-iPr[sub 2]pz)[sub 3], (hydrotris(3,5-diisopropyl-1-pyrazolyl)-borate), a series of hydroxo complexes of first-row divalent metal ions (Mn (1), Fe (2), Co (3), Ni (4), Cu (5), Zn (6)) was synthesized. X-ray crystallography was applied to 1-5, establishing that all these hydroxo complexes have a dinuclear structure solely bridged with a bis(hydroxo) unit. The structure of 6 was characterized by spectroscopy, which indicates that 6 is monomeric. All these hydroxo complexes were found to react with CO[sub 2], even atmospheric CO[sub 2], to afford [mu]-carbonato dinuclear complexes of Mn (7), Fe (8), Co (9), Ni (10), Cu (11), and Zn (12). The molecular structures of the complexes 8-12 were determined. A variety of coordination modes of the carbonate group was seen. In 10 and 11, the carbonate group is bound to both metal centers bidentately in a symmetric fashion, while in 8 and 9, the carbonate coordination modes are described as an unsymmetric bidentate. The carbonate group in 12 is coordinated to one zinc ion bidentately, but it is bound to the other zinc ion unidentately. From IR data, the coordination mode of the carbonate group in 7 was suggested to be similar to those found in 8 and 9. Thus, the order of the coordination distortions of the carbonate groups in this series of [mu]-carbonato dinuclear complexes is determined. 40 refs., 8 figs., 4 tabs.

Kitajima, Nobumasa; Hikichi, Shiro; Tanaka, Masako; Moro-oka, Yoshihiko (Tokyo Inst. of Technology, Yokohama (Japan))

1993-06-30T23:59:59.000Z

257

Theoretical Investigation of the Enzymatic Phosphoryl Transfer of ?-phosphoglucomutase: Revisiting Both Steps of the Catalytic Cycle  

SciTech Connect (OSTI)

Enzyme catalyzed phosphate transfer is a part of almost all metabolic processes. Such reactions are of central importance for the energy balance in all organisms and play important roles in cellular control at all levels. Mutases transfer a phosphoryl group while nucleases cleave the phosphodiester linkages between two nucleotides. The subject of our present study is the Lactococcus lactis ?-phosphoglucomutase (?-PGM), which effectively catalyzes the interconversion of ?-D-glucose-1-phosphate (?-G1P) to ?- D-glucose-6-phosphate (?-G6P) and vice versa via stabile intermediate ?-D-glucose-1,6-(bis)phosphate (?-G1,6diP) in the presence of Mg2+. In this paper we revisited the reaction mechanism of the phosphoryl transfer starting from the bisphosphate ?-G1,6diP in both directions (toward ?-G1P and ?-G6P) combining docking techniques and QM/MM theoretical method at the DFT/PBE0 level of theory. In addition we performed NEB (nudged elastic band) and free energy calculations to optimize the path and to identify the transition states and the energies involved in the catalytic cycle. Our calculations reveal that both steps proceed via dissociative pentacoordinated phosphorane, which is not a stabile intermediate but rather a transition state. In addition to the Mg2+ ion, Ser114 and Lys145 also play important roles in stabilizing the large negative charge on the phosphate through strong coordination with the phosphate oxygens and guiding the phosphate group throughout the catalytic process. The calculated energy barrier of the reaction for the ?-G1P to ?-G1,6diP step is only slightly higher than for the ?-G1,6diP to ?-G6P step (16.10 kcal mol-1 versus 15.10 kcal mol-1) and is in excellent agreement with experimental findings (14.65 kcal mol-1).

Elsasser, Brigitta M.; Dohmeier-Fischer, Silvia; Fels, Gregor

2012-07-12T23:59:59.000Z

258

Routine production of copper-64 using 11.7MeV protons  

SciTech Connect (OSTI)

Reliable production of copper-64 ({sup 64}Cu) was achieved by irradiating enriched nickel-64 ({sup 64}Ni, >94.8%) in an IBA 18/9 cyclotron. Nickel-64 (19.1 {+-} 3.0 mg) was electroplated onto an Au disc (125{mu}m Multiplication-Sign 15mm). Targets were irradiated with 11.7 MeV protons for 2 hours at 40{mu}A. Copper isotopes ({sup 60,61,62,64}Cu) were separated from target nickel and cobalt isotopes ({sup 55,57,61}Co) using a single ion exchange column, eluted with varying concentration of low HCl alcohol solutions. The {sup 64}Ni target material was recovered and reused. The {sup 64}Cu production rate was 1.46{+-}0.3MBq/{mu}A.hr/mg{sup 64}Ni(n = 10) (with a maximum of 2.6GBq of {sup 64}Cu isolated after 2hr irradiation at 40uA. Radionuclidic purity of the {sup 64}Cu was 98.7 {+-} 1.6 % at end of separation. Cu content was < 6mg/L (n = 21). The specific activity of {sup 64}Cu was determined by ICP-MS and by titration with Diamsar to be 28.9{+-}13.0GBq/{mu}mol[0.70{+-}0.35Ci/{mu}mol]/({mu}A.hr/mg{sup 64}Ni)(n = 10) and 13.1{+-}12.0GBq/{mu}mol[0.35{+-}0.32Ci/{mu}mol]/({mu}A.hr/mg{sup 64}Ni)(n 9), respectively; which are in agreement, however, further work is required.

Jeffery, C. M.; Smith, S. V.; Asad, A. H.; Chan, S.; Price, R. I. [Medical Technology and Physics, Sir Charles Gairdner Hospital, Nedlands, Western Australia, 6009 (Australia); Centre for Forensic Science, University of Western Australia, Nedlands, Western Australia, 6009 (Australia) and ARC Centre of Excellence in A (Australia); ARC Centre of Excellence in Antimatter-Matter Studies, Australian National University, Canberra, ACT 0200 (Australia) and Collider-Accelerator Department, Brookhaven National Laboratory, Upton, NY 11973 (United States); Medical Technology and Physics, Sir Charles Gairdner Hospital, Nedlands, Western Australia, 6009 (Australia); ARC Centre of Excellence in Antimatter-Matter Studies, Australian National University, Canberra, ACT 0200 (Australia) and Imaging and Applied (Australia); Medical Technology and Physics, Sir Charles Gairdner Hospital, Nedlands, Western Australia, 6009 (Australia); Medical Technology and Physics, Sir Charles Gairdner Hospital, Nedlands, Western Australia, 6009 (Australia) and School of Physics, University of Western Australia, Nedlands, Western Australia, 6009 (Australia)

2012-12-19T23:59:59.000Z

259

Thermochemical Insight into the Reduction of CO to CH3OH with [Re(CO)]+ and [Mn(CO)]+ Complexes  

SciTech Connect (OSTI)

To gain insight into thermodynamic barriers for reduction of CO into CH3OH, free energies for reduction of [CpRe(PPh3)(NO)(CO)]+ into CpRe(PPh3)(NO)(CH2OH) have been determined from experimental measurements. Using model complexes, the free energies for the transfer of H+, H–, and e– have been determined. A pKa of 10.6 was estimated for [CpRe(PPh3)(NO)(CHOH)]+ by measuring the pKa for the analogous [CpRe(PPh3)(NO)(CMeOH)]+. The hydride donor ability (?G°H–) of CpRe(PPh3)(NO)(CH2OH) was estimated to be 58.0 kcal mol–1, based on calorimetry measurements of the hydride transfer reaction between CpRe(PPh3)(NO)(CHO) and [CpRe(PPh3)(NO)(CHOMe)]+ to generate the methylated analog, CpRe(PPh3)(NO)(CH2OMe). Cyclic voltammograms recorded on CpRe(PPh3)(NO)(CMeO), CpRe(PPh3)(NO)(CH2OMe), and [CpRe(PPh3)(NO)(CHOMe)]+ displayed either a quasireversible oxidation (neutral species) or reduction (cationic species). These potentials were used as estimates for the oxidation of CpRe(PPh3)(NO)(CHO) or CpRe(PPh3)(NO)(CH2OH), or the reduction of [CpRe(PPh3)(NO)(CHOH)]+. Combination of the thermodynamic data permits construction of three-dimensional free energy landscapes under varying conditions of pH and PH2. The free energy for H2 addition (?G°H2) to [CpRe(PPh3)(NO)(CO)]+ (+15 kcal mol–1) was identified as the most significant thermodynamic impediment for the reduction of CO. DFT computations indicate that ?G°H2 varies by only 4.3 kcal mol–1 across a series of [CpXRe(L)(NO)(CO)]+, while the experimental ?G°H– values for the analogous series of CpRe(PPh3)(NO)(CHO) varies by 12.9 kcal mol–1. The small range of ?G°H2 values is attributed to a minimal change in the C–O bond polarization upon modification of the ancillary ligands, as determined from the computed atomic charges. This work was supported by the US Department of Energy, Office of Basic Energy Sciences, Division of Chemical Sciences, Geosciences & Biosciences. Pacific Northwest National Laboratory (PNNL) is a multiprogram national laboratory operated for DOE by Battelle.

Wiedner, Eric S.; Appel, Aaron M.

2014-05-22T23:59:59.000Z

260

Influence of dietary energy source on in vitro substrate utilization and insulin sensitivity of muscle and adipose tissue of beef cattle  

E-Print Network [OSTI]

to CO2, lactate, total lipid, glyceride-fatty acids, and glyceride-glycerol (nmol#1;100 mg-1#1;h-1) in muscle (LM), subcutaneous (s.c) and intramuscular (i.m.) adipose tissues from steers fed hay- or corn-based diets incubated with 0 or 500 ng... at endpoints A and B ................... 114 20 Least squares means for glycolytic intermediate concentrations (?mol#1;g) in muscle (LM), and subcutaneous (s.c.) and intramuscular (i.m.) adipose tissue from steers fed Hay- or Corn-based diets at A...

Rhoades, Ryan D.

2009-05-15T23:59:59.000Z

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


261

1. Physical constants 101 1. PHYSICAL CONSTANTS  

E-Print Network [OSTI]

with the Fermi coupling constant) comes from the Particle Data Group. The figures in parentheses after the values of 1 eV/c particle hc/(1 eV) 1.239 841 875(31)Ã?10-6 m 25 Rydberg energy hcR = mee4/2(4 0)2 2 = mec22 accel. gN 9.806 65 m s-2 exact Avogadro constant NA 6.022 141 79(30)Ã?1023 mol-1 50 Boltzmann constant k

262

1. Physical constants 1 1. PHYSICAL CONSTANTS  

E-Print Network [OSTI]

of constants (beginning with the Fermi coupling constant) comes from the Particle Data Group. The figures of 1 eV/c particle hc/(1 eV) 1.239 841 930(27)Ã?10-6 m 22 Rydberg energy hcR = mee4/2(40)2 2 = mec22 gravitational accel. gN 9.806 65 m s-2 exact Avogadro constant NA 6.022 141 29(27)Ã?1023 mol-1 44 Boltzmann

263

MODULATION OF COX I AND COX II-MEDIATED FORMATION OF VARIOUS ARACHIDONIC ACID METABOLITES IN VITRO AND IN VIVO BY DIETARY POLYPHENOLS  

E-Print Network [OSTI]

for formation of compound I (~ 2 X 10 7 mol -1 s -1 ) versus soluble peroxides such as ethylhydroperoxide and have lower apparent K M values (~ 10 µM versus 300 µM for H 2 O 2 ) for the peroxidase reaction as measured by rates of oxidation of reducing... of compound I to compound 7 II/intermediate II is considerably more rapid for COX II (Lu et al., 1999). This partly accounts for the fact that for COX II, intermediate II is formed more rapidly and at lower peroxide concentrations. There is no obvious...

Bai, Hyoungwoo

2009-12-03T23:59:59.000Z

264

Effect of mono-(2-ethylhexyl) phthalate on steroid production of human granulosa cells  

SciTech Connect (OSTI)

The phthalate ester mono-(2-ethylhexyl) phthalate (MEHP) is the active metabolite of di-(2-ethylhexyl) phthalate, a high-production-volume chemical used as a plasticizer and solvent in numerous consumer products. MEHP has been demonstrated to be a reproductive toxicant in rodents decreasing estradiol and progesterone production in preovulatory granulosa cells. In the present study, we examined the effect of MEHP on steroid production of human granulosa-lutein (GL) cells. Human GL cells collected from women undergoing in vitro fertilization were cultured in medium containing FSH, hCG and 8-Br-cAMP, respectively, together with various concentrations of MEHP (0-500 {mu}mol L{sup -1}). After incubation for 48 h estradiol and progesterone were assayed in the spent culture medium. Furthermore, aromatase activity and mRNA levels of GL cells were determined. Basal as well as FSH-, hCG- and 8-Br-cAMP-stimulated estradiol production of GL cells was suppressed by MEHP in a dose-dependent manner (IC{sub 50} = 105 {mu}mol L{sup -1}, 138 {mu}mol L{sup -1}, 49 {mu}mol L{sup -1} and 78 {mu}mol L{sup -1}). Furthermore aromatase activity and mRNA levels were reduced in GL cells cultured with MEHP. In contrast, MEHP did not alter the production of progesterone up to a concentration of 167 {mu}mol L{sup -1}. The present data indicate that MEHP is a specific inhibitor of estradiol production in human GL cells with a post-cAMP site of action. The inhibition of estradiol production obviously results from a reduction of aromatase activity on the transcript level. As the in vitro effective doses of MEHP are within the range of real environmental exposure levels an inhibitory effect on estrogen production in vivo seems to be possi0009b.

Reinsberg, Jochen [Department of Gynecological Endocrinology and Reproductive Medicine, University of Bonn, Sigmund-Freud-Strasse 25, D-53127 Bonn (Germany)], E-mail: jochen.reinsberg@ukb.uni-bonn.de; Wegener-Toper, Petra [Department of Clinical Chemistry and Clinical Pharmacology, University of Bonn, Sigmund-Freud-Strasse 25, D-53127 Bonn (Germany); Ven, Katrin van der; Ven, Hans van der [Department of Gynecological Endocrinology and Reproductive Medicine, University of Bonn, Sigmund-Freud-Strasse 25, D-53127 Bonn (Germany); Klingmueller, Dietrich [Department of Clinical Chemistry and Clinical Pharmacology, University of Bonn, Sigmund-Freud-Strasse 25, D-53127 Bonn (Germany)

2009-08-15T23:59:59.000Z

265

Computational Study of Bond Dissociation Enthalpies for Substituted $\\beta$-O-4 Lignin Model Compounds  

SciTech Connect (OSTI)

The biopolymer lignin is a potential source of valuable chemicals. Phenethyl phenyl ether (PPE) is representative of the dominant $\\beta$-O-4 ether linkage. Density functional theory (DFT) is used to calculate the Boltzmann-weighted carbon-oxygen and carbon-carbon bond dissociation enthalpies (BDEs) of substituted PPE. These values are important in order to understand lignin decomposition. Exclusion of all conformers that have distributions of less than 5\\% at 298 K impacts the BDE by less than 1 kcal mol$^{-1}$. We find that aliphatic hydroxyl/methylhydroxyl substituents introduce only small changes to the BDEs (0-3 kcal mol$^{-1}$). Substitution on the phenyl ring at the $ortho$ position substantially lowers the C-O BDE, except in combination with the hydroxyl/methylhydroxyl substituents, where the effect of methoxy substitution is reduced by hydrogen bonding. Hydrogen bonding between the aliphatic substituents and the ether oxygen in the PPE derivatives has a significant influence on the BDE. CCSD(T)-calculated BDEs and hydrogen bond strengths of $ortho$-substituted anisoles when compared with M06-2X values confirm that the latter method is sufficient to describe the molecules studied and provide an important benchmark for lignin model compounds.

Younker, Jarod M [ORNL; Beste, Ariana [ORNL; Buchanan III, A C [ORNL

2011-01-01T23:59:59.000Z

266

Molecular Dynamics Simulations of Uranyl and Uranyl Carbonate Adsorption at Alumino-silicate Surfaces  

SciTech Connect (OSTI)

Adsorption at mineral surfaces is a critical factor controlling the mobility of uranium(VI) in aqueous environments. Therefore, molecular dynamics (MD) simulations were performed to investigate uranyl(VI) adsorption onto two neutral alumino-silicate surfaces, namely the orthoclase (001) surface and the octahedral aluminum sheet of the kaolinite (001) surface. Although uranyl preferentially adsorbed as a bi-dentate innersphere complex on both surfaces, the free energy of adsorption at the orthoclase surface (-15 kcal mol-1) was significantly more favorable than that at the kaolinite surface (-3 kcal mol-1), which was attributed to differences in surface functional groups and to the ability of the orthoclase surface to dissolve a surface potassium ion upon uranyl adsorption. The structures of the adsorbed complexes compared favorably with X-ray absorption spectroscopy results. Simulations of the adsorption of uranyl complexes with up to three carbonate ligands revealed that uranyl complexes coordinated to up to 2 carbonate ions are stable on the orthoclase surface whereas uranyl carbonate surface complexes are unfavored at the kaolinite surface. Combining the MD-derived equilibrium adsorption constants for orthoclase with aqueous equilibrium constants for uranyl carbonate species indicates the presence of adsorbed uranium complexes with one or two carbonates in alkaline conditions, in support of current uranium(VI) surface complexation models.

Kerisit, Sebastien N.; Liu, Chongxuan

2014-03-03T23:59:59.000Z

267

1521-0111/85/5/671681$25.00 http://dx.doi.org/10.1124/mol.113.091199 MOLECULAR PHARMACOLOGY Mol Pharmacol 85:671681, May 2014  

E-Print Network [OSTI]

-yl)-[2-(1H-tetrazol-5-yl)-phenyl]- amine] enhance the activity of TREK1 currents, and we show that BL

Tucker, Stephen J.

268

J. Phys. B: At. Mol. Phys. 19 (1986) L519-L525. Printed in Great Britain LETTER TO THE EDITOR  

E-Print Network [OSTI]

Rydberg states of lithium in a uniform magnetic field have been excited from the ground state by v field, numerous theoretical studies have been devoted to the analysis of the properties the diamagnetic interaction El;;"' between states belonging to different manifolds. The existence

Cacciani, Patrice

1986-01-01T23:59:59.000Z

269

Int. J. Mol. Sci. 2013, 14, 4372-4374; doi:10.3390/ijms14024372 International Journal of  

E-Print Network [OSTI]

Bhatnagar and Keshav C. Das Biomass Production Potential of a Wastewater Alga Chlorella vulgaris ARC 1 under

Millar, Andrew J.

270

Mol. Crysr. Liq.Cryst. 1990, Vol. 192, pp. 75-78 Reprints available directly from the publisher  

E-Print Network [OSTI]

States of America TBSTING METHODS OB MEASUREMENTS OF LIQUID CRYSTAL- '20-SOLID SURFACE ANCHORING ENERGY O determined by the equality of the elastic and surface energy contrib&ions t o the energy balance. As- suming Photocopying permittedby license only O 1990 Gordon and Breach Science Publishers S.A. Rinted in the United

Lavrentovich, Oleg D.

271

Yeast Polysome Profiles Adapted from Baim et al., 1985, Mol. Cell. Biol. 5(8):1839-46.  

E-Print Network [OSTI]

of yeast, swirl, and pour into precooled 50 ml tube in ice water. Rapid cooling is essential. Hold in ice vigorously eight times for 15 sec each with 30 sec cooling on ice between each burst. It is essential to get yeast, make sure all solutions are at 4°C. Have stock of 5 mg/ml cyclohexamide thawed and on ice. Have

Aris, John P.

272

Threshold Photoelectron Photoion Coincidence (TPEPICO) Studies: The Road to ? 0.1 kJ/mol Thermochemistry  

SciTech Connect (OSTI)

The threshold photoelectron photoion coincidence (TPEPICO) technique is utilized to investigate the dissociation dynamics and thermochemistry of energy selected medium to large organic molecular ions. The reactions include parallel and consecutive steps that are modeled with the statistical theory in order to extract dissociation onsets for multiple dissociation paths. These studies are carried out with the aid of molecular orbital calculations of both ions and the transition states connecting the ion structure to their products. The results of these investigations yield accurate heats of formation of ions, free radicals, and stable molecules. In addition, they provide information about the potential energy surface that governs the dissociation process. Isomerization reactions prior to dissociation are readily inferred from the TPEPICO data.

Baer, Tomas [University of North Carolina

2013-10-14T23:59:59.000Z

273

JMB--MS 422 Cust. Ref. No. CAM 502/94 [SGML] J. Mol. Biol. (1995) 247, 536540  

E-Print Network [OSTI]

(Chothia, 1984; Finkelstein & Ptitsyn, 1987) and provide the basis for the classification of protein folds (1993). An extensive bibliography of papers on the classification and the determinants of protein folds

274

Int. J. Mol. Sci. 2009, 10, 3478-3487; doi:10.3390/ijms10083478 International Journal of  

E-Print Network [OSTI]

.M.E.) # Current address: Department of Radiation Oncology, Rhode Island Hospital, 593 Eddy Street, Providence, RI that are invisible to the surgeon. Near infrared (NIR) fluorescence imaging might improve surgical outcomes-guided surgery has been introduced to maximize tumor excision and minimize collateral damage. Surgeons usually

Rhode Island, University of

275

Int. J. Mol. Sci. 2012, 13, 8740-8751; doi:10.3390/ijms13078740 International Journal of  

E-Print Network [OSTI]

.: +86-871-5223505 (L.-M.G.); +86-871-5223503 (D.-Z.L.); Fax: +86-871-5217791 (D.-Z.L.). Received: 8

Provan, Jim

276

Int. J. Mol. Sci. 2011, 12, 1908-1920; doi:10.3390/ijms12031908 International Journal of  

E-Print Network [OSTI]

and are based on the synergic effect between synthetic and biopolymeric constituents. Naturally occurring

North Texas, University of

277

Int. J. Mol. Sci. 2012, 13, 5138-5162; doi:10.3390/ijms13045138 International Journal of  

E-Print Network [OSTI]

-dong, Jinju, 660-701, Korea; E-Mails: suguna@bio.gnu.ac.kr (S.S.); megac@bio.gnu.ac.kr (C.M.); ysohn@bio obesity. Cortisol is an important regulator of fuel metabolism during the starvation and stress which

Lee, Keun Woo

278

Int. J. Mol. Sci. 2014, 15, 850-877; doi:10.3390/ijms15010850 International Journal of  

E-Print Network [OSTI]

community composition between Type-1 and Type-2 mats. Fluorescence in-situ hybridization (FISH) coupled; FISH, fluorescence in-situ hybridization; GIS, geographical information systems; CSLM, confocal in microspatial proximity. The surface mats of open-water marine stromatolites (Highborne Cay, Bahamas) contain

Decho, Alan

279

Mol Genet Genomics (2008) 280:249261 DOI 10.1007/s00438-008-0360-3  

E-Print Network [OSTI]

activity is essential for the process of self-incompatibility in several plant families (reviewed in Mc are not involved in self-incompatibility, but seem to have impor- tant functions throughout the plant kingdomCubbin and Kao 2000). Enzymes related to, but dis- tinct from, S-RNases are also present in self

Green, Pamela

280

Mol Gen Genet (1996) 250:180-488 Springer-Verlag 1996 Joaquin Royo Norbert Nass Daniel P. Matron  

E-Print Network [OSTI]

clone for the N. alata S6-ribonuclease (S6-RNase), a gene required for self- incompatibility. alata styles (self-incompatibility genotype S6S6)hybridized to Tnal and accumulated in the style a population of N. alata plants segregating for alleles of the self-incom- patibility locus and is closely

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


281

Search for the Standard Model Higgs Boson in p-pbar Interactions with the decay mode H -> W+ W- -> mu+ nu mu- nu at the D0 Experiment.  

E-Print Network [OSTI]

??A search for the standard model Higgs boson in p-pbar collisions resulting in two muons and large missing transverse energy is presented. The analysis uses… (more)

Johnston, Dale M

2010-01-01T23:59:59.000Z

282

Observation of Exclusive Charmonium Production and gamma gamma -->mu+mu- in pp-bar Collisions at sqrt[s]=1.96 TeV  

E-Print Network [OSTI]

In CDF we have observed the reactions p+p? ?p+X+p? , with X being a centrally produced J/?, ?(2S), or ?[subscript c0], and ????[superscript +]?[superscript -] in pp? collisions at ?s=1.96??TeV. The event signature requires ...

Xie, Si

283

Cold Dark Matter, Radiative Neutrino Mass, mu to e gamma, and Neutrinoless Double Beta Decay  

E-Print Network [OSTI]

Two of the most important and pressing questions in cosmology and particle physics are: (1) What is the nature of cold dark matter? and (2) Will near-future experiments on neutrinoless double beta decay be able to ascertain that the neutrino is a Majorana particle, i.e. its own antiparticle? We show that these two seemingly unrelated issues are intimately connected if neutrinos acquire mass only because of their interactions with dark matter.

Jisuke Kubo; Ernest Ma; Daijiro Suematsu

2006-08-24T23:59:59.000Z

284

Bibliography [1] Global solutions. http://www.mscs.mu.edu/ globsol/.  

E-Print Network [OSTI]

, J. Dongarra, J. Du Croz, A. Green- baum, S. Hammarling, A. McKenney, and D. Sorensen. LAPACK Users, W. Kahan, and O. Marques. On computing givens rotations reliably and eÃ?ciently. LAPACK Working Note(1):61{70, 1993. [14] D. Chiriaev and G. W. Walster. Interval arithmetic speci#12;cation. http

Tennessee, University of

285

The Story of the Therac-25 in LOTOS Mu y Thomas  

E-Print Network [OSTI]

of Canada Ltd. (AECL) during the 1980s and was used at hospitals and clinics in the U.S.A. and Canada

Calder, Muffy

286

Scheduling Freight Trains Traveling on Complex etworks SHI MU and MAGED DESSOUKY*  

E-Print Network [OSTI]

, namely a simple look-ahead greedy heuristic and a global neighborhood search algorithm, in terms goods from other countries usually enter the United States through ports and then transported inland

Dessouky, Maged

287

Fixing Two-Nucleon Weak-Axial Coupling L_{1,A} From mu-d Capture  

E-Print Network [OSTI]

We calculate the muon capture rate on the deuteron to next-to-next-to-leading order in the pionless effective field theory. The result can be used to constrain the two-nucleon isovector axial coupling L_{1,A} to +/- 2 fm^3 if the muon capture rate is measured to 2% level. From this, one can determine the neutrino-deuteron break up reactions and the pp-fusion cross section in the sun to a same level of accuracy.

Jiunn-Wei Chen; Takashi Inoue; Xiangdong Ji; Yingchuan Li

2006-01-11T23:59:59.000Z

288

Thermomechanical properties and performance of microfabricated solid oxide fuel cell ([mu]SOFC) structures  

E-Print Network [OSTI]

The mechanical properties of a ceramic electrolyte, sputtered yttria-stabilized zirconia (YSZ), in thin film (<1Clm) form were studied in order to design and fabricate thermomechanically stable microfabricated SOFCs (SOFCs) ...

Yamamoto, Namiko

2006-01-01T23:59:59.000Z

289

Nanostructured ceria based thin films ({<=}1 {mu}m) As cathode/electrolyte interfaces  

SciTech Connect (OSTI)

Gadolinium doped cerium oxide (CGO: Ce{sub 0,9}Gd{sub 0,1}O{sub 2-{delta}}) films were used as an oxygen anion diffusion layer at the cathode/electrolyte interface of Solid Oxide Fuel Cells (SOFCs), between LSCF (lanthanum strontium cobalt ferrite) and YSZ (yttria-stabilized zirconia). Thin ({approx}100 nm) and thick ({approx}700 nm) mesoporous CGO layers were synthesized through a sol-gel process including organic template coupled with the dip-coating method. Structural and microstructural characterizations were performed, highlighting a well-bonded crystalline CGO nanoparticles network which delineates a 3-D inter-connected mesoporous network. Their electrical behaviors were investigated by impedance spectroscopy analysis of YSZ/mesoporous-CGO/LSCF half-cell. Anode-supported SOFCs, operating at 800 Degree-Sign C, with either dense or mesoporous CGO dip-coated interlayers were also fabricated [NiO-YSZ anode/YSZ/CGO/LSCF cathode]. The impact of the mesoporous CGO interlayers on SOFCs performances was investigated by galvanostatic analysis and compared to the behavior of a dense CGO interlayer. The polarization curves revealed an enhancement in the electrical performance of the cell, which is assigned to a decrease of the polarization resistance at the cathode/electrolyte interface. The integrity and connectivity of the CGO nanoparticles bonded network facilitates O{sup 2-} transport across the interface. - Graphical abstract: Thin and thick CGO films have been prepared through a sol-gel process and their potential application as SOFC cathode/electrolyte interlayer in SOFC has been investigated. Highlights: Black-Right-Pointing-Pointer Mesoporous ceria based thin films exhibit interesting performances for Solid Oxide Fuel Cell. Black-Right-Pointing-Pointer Mesoporous films were synthesized through the sol-gel process combined with the dip-coating. Black-Right-Pointing-Pointer Integrity and connectivity of the nanoparticles facilitates O{sup 2-} transport across the interface.

Hierso, J. [Laboratoire de Chimie de la Matiere Condensee de Paris, Universite Paris 6-UMR 7574-College de France, 11 Place Marcelin Berthelot, 75005 Paris (France); Boy, P.; Valle, K. [CEA-Le Ripault, LSCG, BP 15, 37000 Monts (France); Vulliet, J.; Blein, F. [CEA-Le Ripault, LCCA, BP 15, 37000 Monts (France); Laberty-Robert, Ch., E-mail: christel.laberty@upmc.fr [Laboratoire de Chimie de la Matiere Condensee de Paris, Universite Paris 6-UMR 7574-College de France, 11 Place Marcelin Berthelot, 75005 Paris (France); Sanchez, C. [Laboratoire de Chimie de la Matiere Condensee de Paris, Universite Paris 6-UMR 7574-College de France, 11 Place Marcelin Berthelot, 75005 Paris (France)

2013-01-15T23:59:59.000Z

290

The Univer siTy ClUb of MU A Tradition of Excellence  

E-Print Network [OSTI]

Display with Ranch Dip ... $4.95 per guest International & Domestic Cheese Display with Assorted Gourmet & cheeses, marinated and grilled vegetables, artichoke hearts in mustard dressing, croustades and crackers

Taylor, Jerry

291

PROLOG-LINDA : AN EMBEDDING OF LINDA IN muPROLOG  

E-Print Network [OSTI]

,The University of Western Australia, Nedlands, 6009, Western Australia and JAMES PINAKIS Department of Computer Science,The University of Western Australia, Nedlands, 6009, Western Australia ABSTRACT This paper

Sutcliffe, Geoff

292

Mantid - Data Analysis and Visualization Package for Neutron Scattering and $\\mu SR$ Experiments  

SciTech Connect (OSTI)

The Mantid framework is a software solution developed for the analysis and visualization of neutron scattering and muon spin measurements. The framework is jointly developed by a large team of software engineers and scientists at the ISIS Neutron and Muon Facility and the Oak Ridge National Laboratory. The objective of the development is to improve software quality, both in terms of performance and ease of use, for the the user community of large scale facilities. The functionality and novel design aspects of the framework are described.

Arnold, Owen [ISIS Facility, Rutherford Appleton Laboratory (ISIS); Bilheux, Jean-Christophe [ORNL; Borreguero Calvo, Jose M [ORNL; Buts, Alex [ISIS Facility, Rutherford Appleton Laboratory (ISIS); Campbell, Stuart I [ORNL; Doucet, Mathieu [ORNL; Draper, Nicholas J [ORNL; Ferraz Leal, Ricardo F [ORNL; Gigg, Martyn [ISIS Facility, Rutherford Appleton Laboratory (ISIS); Lynch, Vickie E [ORNL; Mikkelson, Dennis J [ORNL; Mikkelson, Ruth L [ORNL; Miller, Ross G [ORNL; Perring, Toby G [ORNL; Peterson, Peter F [ORNL; Ren, Shelly [ORNL; Reuter, Michael A [ORNL; Savici, Andrei T [ORNL; Taylor, Jonathan W [ORNL; Taylor, Russell J [ORNL; Zhou, Wenduo [ORNL; Zikovsky, Janik L [ORNL

2014-01-01T23:59:59.000Z

293

Self-referenced 1.5 [mu]m fiber frequency combs at GHz repetition rates  

E-Print Network [OSTI]

Tremendous advances in recent years to the optical frequency comb, particularly frequency combs deriving from solid-state and fiber architectures, have enabled a host of important new applications to emerge - applications ...

Chao, David, Ph. D. Massachusetts Institute of Technology

2012-01-01T23:59:59.000Z

294

Erbium-ytterbium-yttrium compounds for light emission at 1.54[mu]m  

E-Print Network [OSTI]

Silicon microphotonics has emerged as the leading technology to overcome the interconnect bottleneck that limits a further increase of computation power following Moore's law. Optical interconnects between different ...

Vanhoutte, Michiel

2013-01-01T23:59:59.000Z

295

Integrated high-repetition-rate femtosecond lasers at 1.55 [mu]m  

E-Print Network [OSTI]

Performance of state-of-the-art, electronic analog-to-digital converters is currently limited by the 100-fs aperture jitter. However, optical sampling can overcome the jitter limit by using femtosecond lasers that have ...

Byun, Hyunil

2010-01-01T23:59:59.000Z

296

Characteristics of atmospheric gravity waves observed using the MU (Middle and Upper atmosphere) radar  

E-Print Network [OSTI]

in 1970s.6) In order to explain this weakening *1 Research Institute for Sustainable Humanosphere (RISH for Sustainable Humanosphere (RISH), Kyoto Univer- sity, Uji, Kyoto 611-0011, Japan (e-mail: tsuda processes of atmospheric gravity waves was proposed.7),8) In the 1980s a notable advance was made

Takada, Shoji

297

SciTech Connect: Crystal structure of the[mu]-opioid receptor bound to a  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr MayAtmosphericNuclear Security Administrationcontroller systems controllerAdditiveBetatron RadiationDirectmorphinan antagonist

298

A 2 Gb/s Directly Driven Wireless Link Qianli Mu, Luke Sankey and Zoya Popovic  

E-Print Network [OSTI]

antenna arrays that can perform radar, electronic warfare, information warfare and communication functions requirements on the electronic hardware in terms of digital clock rates [6]-[9]. This paper presents sim

Popovic, Zoya

299

Novel broadband light sources and pulse generation techniques at 1.5 [mu]m  

E-Print Network [OSTI]

A wide diversity of applications, in both fundamental science and practical technology, has come to rely on broadband optical light sources as key enabling tools. In this thesis, we investigate three devices that contribute ...

Shen, Hanfei M, 1979-

2009-01-01T23:59:59.000Z

300

Enfmt Plaza. S. W.. Washingron, DC 200262174. Tekphonr: (202) 488~MU0  

Office of Legacy Management (LM)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) "ofEarlyEnergyDepartment ofDepartment ofof EnergyYou$ EGcG ENERGY MEASUREMENTS;/:4,4 (; .369s . I Suite

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


301

Search for tau -> gamma mu: A test of lepton number conservation  

E-Print Network [OSTI]

A search for the lepton number violating decay of the tau lepton to the gammamu final state has been performed with the CLEO II detector at the Cornell e+e- storage ring CESR. In a data sample that corresponds to an ...

Ammar, Raymond G.; Ball, S.; Baringer, Philip S.; Coppage, Don; Copty, N.; Davis, Robin E. P.; Hancock, N.; Kelly, M.; Kwak, Nowhan; Lam, H.

1993-01-01T23:59:59.000Z

302

MuSIC: Mobility-Aware Optimal Service Allocation in Mobile Cloud Computing  

E-Print Network [OSTI]

interpretation) - despite advances in device technology, resources (energy, storage, processing) at the mobileS goals such application delay, device power consumption and user cost/price. In this paper, we propose consumption and cost at the user side. In contrast, Wi-Fi deployments, e.g. 802.11 hotspots, exhibit low

Venkatasubramanian, Nalini

303

The Role of N-Acetylcysteine in the Prevention of Contrast-Induced Nephrotoxicity  

SciTech Connect (OSTI)

Purpose. To determine the role of prophylactic N-acetylcysteine in the prevention of contrast-induced nephrotoxicity. Methods. One hundred and sixteen patients undergoing noncoronary angiography, with or without pre-existing renal impairment, were randomly assigned to receive prophylactic oral N-acetylcysteine or no treatment. Serum creatinine (sCr) was measured prior to angiography and 48 hr after the procedure. Urine samples were collected before and after the examination for measurement of malondialdehyde (MDA) concentration. Contrast-induced nephrotoxicity (CIN) was defined as a rise in serum creatinine of 0.5 mg/dl (44 mmol/l) at 48 hr. Results. Complete data were available on 106 patients, 53 of whom had received N-acetylcysteine. There were no significant differences between the two groups in baseline characteristics, type of angiogram, or volume and concentration of contrast used. Three patients (2.8%), all of whom had received N-acetylcysteine, developed CIN. In the N-acetylcysteine group, the mean serum creatinine in patients with renal impairment was 151.0 {+-} 44.2 {mu}mol/l prior to the procedure and 155.6 {+-} 48.6 {mu}mol/l (p = 0.49) after the procedure. Respective values for those without renal impairment were 79.6 {+-} 15.1 {mu}mol/l and 81.2 {+-} 20.0 {mu}mol/l (p = 0.65). In the group that had not received N-acetylcysteine, the mean serum creatinine levels before and after the procedure were 150.0 {+-} 58.1 and 141.4 {+-} 48.0 {mu}mol/l (p = 0.17) in patients with renal impairment and 79.7 {+-} 14.2 and 81.4 {+-} 15.4 {mu}mol/l (p = 0.34) in those without renal impairment. In both groups, no significant change in urinary MDA concentration was observed. Conclusion. There is no benefit to the prophylactic administration of N-acetylcysteine in patients undergoing peripheral angiography using current contrast media.

Sandhu, Caron [Guy's and St. Thomas's Hospital, Department of Radiology (United Kingdom)], E-mail: caron.sandhu@gstt.sthames.nhs.uk; Belli, Anna-Maria [St. George's Hospital, Department of Radiology (United Kingdom); Oliveira, David B. [St. George's Hospital, Department of Renal Medicine (United Kingdom)

2006-06-15T23:59:59.000Z

304

mol10x6.0mV10x1.0mC10x2.6 1-231-930 EU rotationdipole  

E-Print Network [OSTI]

. Results I - Pore Formation and Ion Transport A potential over the membrane is generated by placing different numbers of Na (black spheres) and Cl (pink spheres) ions on each side of the membrane (lipid tails the hydrophilic pore. When the potential from the ion imbalance dissipates, the pore subsides and the membrane

Southern California, University of

305

glacial-scale enrichment would result in an air-to-sea flux of about 4.6 mol C m 2  

E-Print Network [OSTI]

an area of 225 km2 . Iron infusions in the north patch of 631 kg and 450 kg were repeated on 16 January, with repeated infusions on 29 January, 1 February, and 5 Feb- ruary. Each infusion involved 315 kg spread over a 225 km2 area. For both patches, initial iron infusions were supple- mented with infusions of SF6 and 3

306

J. Phys. B: At. Mol. Opt. Phys. 21 (1988) 3499-3521. Printed in the UK Rydberg atoms in parallel magnetic and electric fields: 11.  

E-Print Network [OSTI]

the energy of the states to be calculated. The main properties of the spectra and their evolution when one of lithium (Cacciani er a1 1986a, I). The present paper aims to analyse the structure of an n manifold fields are supposed to be weak enough for the corresponding interactions to be considered as t Present

Cacciani, Patrice

1988-01-01T23:59:59.000Z

307

COMPETENT CELLS (based on Hanahan 1983 J Mol Biol 166, 557580) STREAK a fresh plate the day before inoculation from parent stock (NOT previous  

E-Print Network [OSTI]

mM KCl 10 mM CaCl2 15% w/v glycerol Mix well, pH to 5.8 with 0.2 M acetic acid Tfb2: filterM KCl 75 mM CaCl2 15% w/v glycerol #12;

Cross, George

308

J. Phys. B AL Mol. Opt Phys. 26 (1993) 1569-1578. Printed in the UK Pure and mixed state calculationsof the laser-induced  

E-Print Network [OSTI]

, altemative methods for separating the elements of uranium are being studied, notably the use of lasers of the isotopes of uranium has major commercial importance in the nuclear fuel industry. As is well known to induce preferential ionization of 23sU(see Greenland 1991 for a review). Laser isotope separation relies

Ford, Ian

309

J Mol Cell Cardiol 33, 947956 (2001) doi:10.1006/jmcc.2001.1357, available online at http://www.idealibrary.com on  

E-Print Network [OSTI]

dam- light/dark cycle schedule and were given standard laboratory chow and tap water ad libitum the mitochondrial ATP-sensitive K+ channel. The consequence is preservation of energy transfer processes from

Garlid, Keith

310

Mol. Biol. Evol. 18(4):627638. 2001 2001 by the Society for Molecular Biology and Evolution. ISSN: 0737-4038  

E-Print Network [OSTI]

to morphological evolution. For ex- ample, naturally occurring alleles of the MADS box transcription factor within the Andropogoneae. The phylogeny suggests that the tribe underwent a rapid radiation during its

Doebley, John

311

41. K. J. Keeler and G. B. Gloor, Mol. Cell. Biol. 17, 627 42. Y. Bellaiche, V. Mogila, N. Perrimon, Genetics 152,  

E-Print Network [OSTI]

. Jasin for plasmid pCMV/SCE1XNLS, P. Geyer for plasmid pS/G, E. Raff for the 5-kb genomic fragment of 2t

California at San Diego, University of

312

Eur J Nucl Med Mol Imaging. Author manuscript Non-invasive estimation of hepatic blood perfusion from H2 15O PET  

E-Print Network [OSTI]

perfusion from H2 15O PET images using tissue-derived arterial and portal input functions Kudomi Nobuyuki 1 Timo 2 , Knuuti Juhani 1 , Iida Hirokazu 3 , Nuutila Pirjo 1 4 , Iozzo Patricia 1 5 Turku PET Centre1 artery. When its perfusion is assessed using PET and O-labeled water15 (H O), calculations require a dual

Paris-Sud XI, Université de

313

Mol. Biol. Evol. 16(10):13911399. 1999 1999 by the Society for Molecular Biology and Evolution. ISSN: 0737-4038  

E-Print Network [OSTI]

and Evolution. ISSN: 0737-4038 Genomic Signature: Characterization and Classification of Species Assessed´ INSERM 494, Paris, France We explored DNA structures of genomes by means of a new tool derived from that subsequences of a genome exhibit the main characteristics of the whole genome, attesting to the validity

Wehenkel, Louis

314

Recovery of propylene glycol from dilute aqueous solutions by reversible chemical complexation with organoboronates  

SciTech Connect (OSTI)

Extractants consisting of an ion-pair of Aliquat 336 with phenylboronate or 3-nitrophenylboronate were prepared in various diluents (2-ethylhexanol, toluene, o-xylene or diisobutylketone). In batch experiments propyleneglycol (1,2-PD) was effectively extracted even at low concentrations. Heterogeneous complexation constants {beta}{sub 11} calculated at 25 C were 45-120 (mol/1){sup {minus}1} in 2-ethylhexanol, 34.8 (mol/l){sup {minus}1} in toluene, 37.6 (mol/l){sup {minus}1} in o-xylene and 14.4 (mol/l){sup {minus}1} in diisobutylketone. In 2-ethythexanol, there was no significant effect of extractant concentration on the complexation constant. Equilibrium water concentration in the extractants was 8-12 wt %, decreasing with 1,2-PD uptake. Nearly all extractant/diluent systems exhibited overloading (more than stoichiometric uptake of 1,2-PD). Evidence for aggregation of the ion-pair extractant in organic phase was found from water solubilization studies (molar solubilization ratios up to 10) and {sup 1}H NMR spectroscopy studies. Solubilization of 1,2-PD within hydrophilic aggregate interiors may explain the observed overloading. The complexation constant decreased with increasing temperature, but not enough to make back extraction after a temperature change attractive. Back extraction may be achieved after acidification with carbon dioxide to convert the organoboronate anion to the corresponding organoboronic acid. Up to 80% of the extracted 1,2-PD was backextracted in a batch extraction using C0{sub 2}. The extractant could then be regenerated by stripping carbon dioxide from solution at temperatures exceeding 110 C. However, at these temperatures the extractant appears to undergo a transformation in which color changes and extraction capacity is reduced to about 60% of original value.

Broekhuis, R.R.; Lynn, S.; King, C.J.

1995-05-01T23:59:59.000Z

315

Urinary 1-hydroxypyrene concentrations in Chinese coke oven workers relative to job category, respirator usage, and cigarette smoking  

SciTech Connect (OSTI)

1-Hydroxypyrene (1-OHP) is a biomarker of recent exposure to polycyclic aromatic hydrocarbons (PAHs). We investigated whether urinary 1-OHP concentrations in Chinese coke oven workers (COWs) are modulated by job category, respirator usage, and cigarette smoking. The present cross-sectional study measured urinary 1-OHP concentrations in 197 COWs from Coking plant I and 250 COWs from Coking plant II, as well as 220 unexposed referents from Control plant I and 56 referents from Control plant II. Urinary 1-OHP concentrations (geometric mean, {mu}mol/mol creatinine) were 5.18 and 4.21 in workers from Coking plants I and II, respectively. The highest 1-OHP levels in urine were found among topside workers including lidmen, tar chasers, and whistlers. Benchmen had higher 1-OHP levels than other workers at the sideoven. Above 75% of the COWs exceeded the recommended occupational exposure limit of 2.3 {mu}mol/mol creatinine. Respirator usage and increased body mass index (BMI) slightly reduced 1-OHP levels in COWs. Cigarette smoking significantly increased urinary 1-OHP levels in unexposed referents but had no effect in COWs. Chinese COWs, especially topside workers and benchmen, are exposed to high levels of PAHs. Urinary 1-OHP concentrations appear to be modulated by respirator usage and BMI in COWs, as well as by smoking in unexposed referents.

Bo Chen; Yunping Hu; Lixing Zheng; Qiangyi Wang; Yuanfen Zhou; Taiyi Jin [Fudan University, Shanghai (China). School of Public Health

2007-09-15T23:59:59.000Z

316

Search for the Standard Model Higgs Boson in p anti-p Interactions with the Decay Mode H --> W+W- --> mu+nu mu-anti-nu at the D0 Experiment  

SciTech Connect (OSTI)

A search for the standard model Higgs boson in p{bar p} collisions resulting in two muons and large missing transverse energy is presented. The analysis uses 4.2 fb{sup -1} of integrated luminosity at a center-of-mass energy of {radical}s = 1.96 TeV collected between April 2002 and December 2008 with the D0 detector at the Fermilab Tevatron collider. No significant excess above the background estimation is observed and limits are derived on Higgs boson production.

Johnston, Dale Morgan; /Nebraska U.

2010-04-01T23:59:59.000Z

317

[(eta5-PentamethylcyclopentadienylYb(III)(5,5'-dimethyl-2,2-bipyridyl)mu-OH)2(mu 2-trifluoromethylsulfanato-O,O')][tetraphenylborate](5,5'-dimethyl-2,2-bipyridyl)  

SciTech Connect (OSTI)

The title compound C{sub 81}H{sub 88}BF{sub 3}N{sub 6}O{sub 5}SYb{sub 2}, crystallizes as a half-sandwich complex with a bridging inner-sphere trifluoro-methane sulfonate as well as two bridging hydroxide groups. there is uncoordinated 5,5{prime}-dimethyl-2,2{prime}-bipyridine in the crystal structure. The bound bipyridine ligands have N-C-C{prime}-n{prime} torsion angles of 12-13{sup o}. The triply bridged Yb centers are 3.5990(4) Angstroms apart. The Yb-N bonds range from 2.389(6)-2.424(5) Angstroms.

Kazhdan, Daniel

2008-01-23T23:59:59.000Z

318

An engineering-economic analysis of combined heat and power technologies in a (mu)grid application  

E-Print Network [OSTI]

draft, 2001. Danish Energy Agency (1998). Combined Heat andpolicies and measures, Danish Energy Agency. Hirschenhofer,demand in 1996 (Danish Energy Agency 1998). Reliance on CHP

Bailey, Owen; Ouaglal, Boubekeur; Bartholomew, Emily; Marnay, Chris; Bourassa, Norman

2002-01-01T23:59:59.000Z

319

PRIDE IN ACADEMIC ACHIEVEMENTS TAM is one of the Top 20 academic programs at MU in terms of undergraduate enrollment.  

E-Print Network [OSTI]

Printing technology for creative textile design done using sustainable strategies. · The Kellwood Company Lab featuring the latest in software and technology, including 3D body scanner, Optitex, and others of ten sites across the country to participate in the national sizing survey, Size USA, which used a 3-D

Taylor, Jerry

320

MuSiC: a Multibunch and multiparticle Simulation Code with an alternative approach to wakefield effects  

E-Print Network [OSTI]

The simulation of beam dynamics in presence of collective effects requires a strong computational effort to take into account, in a self consistent way, the wakefield acting on a given charge and produced by all the others. Generally this is done by means of a convolution integral or sum. Moreover, if the electromagnetic fields consist of resonant modes with high quality factors, responsible, for example, of coupled bunch instabilities, a charge is also affected by itself in previous turns, and a very long record of wakefield must be properly taken into account. In this paper we present a new simulation code for the longitudinal beam dynamics in a circular accelerator, which exploits an alternative approach to the currently used convolution sum, reducing the computing time and avoiding the issues related to the length of wakefield for coupled bunch instabilities. With this approach it is possible to simulate, without the need of a large computing power, simultaneously, the single and multi-bunch beam dynamics...

Migliorati, M

2015-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


321

An engineering-economic analysis of combined heat and power technologies in a (mu)grid application  

SciTech Connect (OSTI)

This report describes an investigation at Ernesto Orlando Lawrence Berkeley National Laboratory (Berkeley Lab) of the potential for coupling combined heat and power (CHP) with on-site electricity generation to provide power and heating, and cooling services to customers. This research into distributed energy resources (DER) builds on the concept of the microgrid (mGrid), a semiautonomous grouping of power-generating sources that are placed and operated by and for the benefit of its members. For this investigation, a hypothetical small shopping mall (''Microgrid Oaks'') was developed and analyzed for the cost effectiveness of installing CHP to provide the mGrid's energy needs. A mGrid consists of groups of customers pooling energy loads and installing a combination of generation resources that meets the particular mGrid's goals. This study assumes the mGrid is seeking to minimize energy costs. mGrids could operate independently of the macrogrid (the wider power network), but they are usually assumed to be connected, through power electronics, to the macrogrid. The mGrid in this study is assumed to be interconnected to the macrogrid, and can purchase some energy and ancillary services from utility providers.

Bailey, Owen; Ouaglal, Boubekeur; Bartholomew, Emily; Marnay, Chris; Bourassa, Norman

2002-03-01T23:59:59.000Z

322

VERY LONG BASELINE NEUTRINO OSCILLATION EXPERIMENTS FOR PRECISE MEASURMENTS OF OSCILLATION PARAMETERS AND SEARCH FOR N MU YIELDS N EPSILON.  

SciTech Connect (OSTI)

Brookhaven National Laboratory and collaborators started a neutrino working group to identify new opportunities in the field of neutrino oscillations and explore how our laboratory facilities can be used to explore this field of research. The memo to the working group and the charge are included in Appendix I. This report is the result of the deliberations of the working group. Previously, we wrote a letter of intent to build a new high intensity neutrino beam at BNL. A new intense proton beam will be used to produce a conventional horn focused neutrino beam directed at a detector located in either the Homestake mine in Lead, South Dakota at 2540 km or the Waste Isolation Pilot Plant (WIPP) in Carlsbad, NM at 2880 km. As a continuation of the study that produced the letter of intent, this report examines several items in more detail. We mainly concentrate on the use of water Cherenltov detectors because of their size, resolution, and background rejection capability, and cost. We examine the prospects of building such a detector in the Homestake mine. The accelerator upgrade will be carried out in phases. We expect the first phase to yield a 0.4 MW proton beam and the second phase to result in a 1.0 MW beam. The details of this upgrade will be reported in a companion report. In this report we assume accelerator intensity of 1 MW for calculating event rates and spectra. We also assume a total experimental duration of 5 years with running time of 10{sup 7} seconds per year. We examine the target station and the horn produced neutrino beam with focus on two topics: target and horn design for a 1 MW beam and the broad band spectrum of neutrinos from a 28 GeV proton beam.

DIWAN,M.; MARCIANO,W.; WENG,W.; BEAVIS,D.; BRENNAN,M.; CHEN,M.C.; FERNOW,R.; ET AL

2002-10-18T23:59:59.000Z

323

An engineering-economic analysis of combined heat and power technologies in a (mu)grid application  

E-Print Network [OSTI]

reduction in the use of compressor cooling (kWe) Market Datawas used to displace compressor cooling. However, theincludes the load for compressor cooling and was input into

Bailey, Owen; Ouaglal, Boubekeur; Bartholomew, Emily; Marnay, Chris; Bourassa, Norman

2002-01-01T23:59:59.000Z

324

High-power, hybrid Er:fiber/Tm:fiber frequency comb source in the 2 {\\mu}m wavelength region  

E-Print Network [OSTI]

We present a 2-\\mum frequency comb based on a reliable mode-locked Er:fiber laser with 100 MHz repetition rate. After shifting the spectrum of the amplified Er:fiber comb to longer wavelengths, a single-clad Tm/Ho:fiber is used as a self-pumped pre-amplifier to generate a coherent and broadband spectrum centered at 1.93 \\mum. Subsequently, a cladding-pumped Tm:fiber amplifier boosts the system to a maximum output power of 4.8 W at 1.96 \\mum. After compression in a compact grating compressor, our amplified Er:fiber/Tm:fiber hybrid system delivers as much as 2.9 W with a pulse duration of 141 fs. The system's comb properties are examined via heterodyne measurement.

Adler, Florian

2012-01-01T23:59:59.000Z

325

Standard Model Higgs Boson Discovery Potential in the Decay Channel H - > ZZ(*) - > 4 mu with the CMS Detector.  

E-Print Network [OSTI]

??The Compact Muon Solenoid (CMS) is a general purpose detector at the Large Hadron Collider (LHC) currently under construction at CERN with start-up date in… (more)

Drozdetski, Alexei Alexandrovic

2007-01-01T23:59:59.000Z

326

1.22 {mu}m GaInNAs Saturable Absorber Mirrors with Tailored Recovery Time  

SciTech Connect (OSTI)

The effect of in-situ N-ion irradiation on the recombination dynamics of GaInNAs/GaAs semiconductor saturable absorber mirrors has been studied. The samples were fabricated by molecular beam epitaxy using a radio frequency plasma source for nitrogen incorporation in the absorber layers as well as for the irradiation. The recombination dynamics of irradiated samples were studied by pump-probe measurements. The recombination time of the absorbers could be reduced by increasing the irradiation time. The effect of the reduced recombination time on the pulse dynamics of a mode-locked laser setup was studied with a Bi-doped fibre laser. The pulse quality was found to improve with increased irradiation time and reduced recombination time, demonstrating the potential of the in-situ irradiation method for device applications.

Puustinen, Janne; Guina, Mircea; Korpijaervi, Ville-Markus; Tukiainen, Antti; Kivistoe, Samuli; Pessa, Markus [Optoelectronics Research Centre, Tampere University of Technology, P.O. Box 692, FIN-33101 Tampere (Finland); Marcinkevicius, Saulius [Royal Institute of Technology, Electrum 229, 16440, Kista (Sweden)

2010-11-10T23:59:59.000Z

327

An engineering-economic analysis of combined heat and power technologies in a (mu)grid application  

E-Print Network [OSTI]

Economic Analysis of Combined Heat and Power Technologies inEconomic Analysis of Combined Heat and Power Technologies inAgency (1998). Combined Heat and Power in Denmark. Version

Bailey, Owen; Ouaglal, Boubekeur; Bartholomew, Emily; Marnay, Chris; Bourassa, Norman

2002-01-01T23:59:59.000Z

328

Search for the Decays B(s)-->e+mu- and B(s)-->e+e- in CDF Run II  

E-Print Network [OSTI]

We report results from a search for the lepton flavor violating decays B[subscript s][superscript 0]?e[superscript +]?[superscript -] and B[superscript 0]?e[superscript +]?[superscript -], and the flavor-changing neutral-current ...

Xie, Si

329

An engineering-economic analysis of combined heat and power technologies in a (mu)grid application  

E-Print Network [OSTI]

Technologies in a µGrid Application heat, usually in thethe µGrid. In this µGrid the heat loads are not that great,Combined Heat and Power Technologies in a µGrid Application

Bailey, Owen; Ouaglal, Boubekeur; Bartholomew, Emily; Marnay, Chris; Bourassa, Norman

2002-01-01T23:59:59.000Z

330

RF optimization and analysis of the 805-MHz cavity for the MuCool program using ACE3P  

SciTech Connect (OSTI)

An 805 MHz pillbox cavity tested at Fermilab's MTA facility showed significant degradation in gradient when operated in a several Tesla solenoidal magnetic field. We have used the advanced ACE3P simulation codes developed at SLAC to study the cavity dark current and multipacting characteristics to gain more insight into the gradient limitations. We also checked whether there is an optimal cavity length that minimizes the dark current impact energy. Finally, we have improved on the cavity design, significantly lowering the fields outside the beam area. These and other results are presented in this paper.

Li Zenghai; Ge Lixin; Adolphsen, Chris; Li Derun; Bowring, Daniel [SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025 (United States); Lawrence Berkeley National Laboratory, 1 Cyclotron Road, Berkeley, CA 94720 (United States)

2012-12-21T23:59:59.000Z

331

Lab-on-a-chip flow cytometer and microfluidic fluorescence activated cell sorter ([Mu]FACS) for biomedical applications  

E-Print Network [OSTI]

with highly integrated microfluidics, optics, acoustics, andactuation,” submitted to Microfluidics and Nanofluidics (S. Tsai, Yu- Hwa Lo, “Microfluidics and photonics for Bio-

Cho, Sung Hwan

2010-01-01T23:59:59.000Z

332

THE EVOLUTION OF SOLAR FLUX FROM 0.1 nm TO 160 {mu}m: QUANTITATIVE ESTIMATES FOR PLANETARY STUDIES  

SciTech Connect (OSTI)

Understanding changes in the solar flux over geologic time is vital for understanding the evolution of planetary atmospheres because it affects atmospheric escape and chemistry, as well as climate. We describe a numerical parameterization for wavelength-dependent changes to the non-attenuated solar flux appropriate for most times and places in the solar system. We combine data from the Sun and solar analogs to estimate enhanced UV and X-ray fluxes for the young Sun and use standard solar models to estimate changing visible and infrared fluxes. The parameterization, a series of multipliers relative to the modern top of the atmosphere flux at Earth, is valid from 0.1 nm through the infrared, and from 0.6 Gyr through 6.7 Gyr, and is extended from the solar zero-age main sequence to 8.0 Gyr subject to additional uncertainties. The parameterization is applied to a representative modern day flux, providing quantitative estimates of the wavelength dependence of solar flux for paleodates relevant to the evolution of atmospheres in the solar system (or around other G-type stars). We validate the code by Monte Carlo analysis of uncertainties in stellar age and flux, and with comparisons to the solar proxies {kappa}{sup 1} Cet and EK Dra. The model is applied to the computation of photolysis rates on the Archean Earth.

Claire, Mark W. [School of Environmental Sciences, University of East Anglia, Norwich, UK NR4 7TJ (United Kingdom); Sheets, John; Meadows, Victoria S. [Virtual Planetary Laboratory and Department of Astronomy, University of Washington, Box 351580, Seattle, WA 98195 (United States); Cohen, Martin [Radio Astronomy Laboratory, University of California, Berkeley, CA 94720-3411 (United States); Ribas, Ignasi [Institut de Ciencies de l'Espai (CSIC-IEEC), Facultat de Ciencies, Torre C5 parell, 2a pl, Campus UAB, E-08193 Bellaterra (Spain); Catling, David C., E-mail: M.Claire@uea.ac.uk [Virtual Planetary Laboratory and Department of Earth and Space Sciences, University of Washington, Box 351310, Seattle, WA 98195 (United States)

2012-09-20T23:59:59.000Z

333

Poly[bis(N,N-dimethylformamide-[kappa]O)([mu]4-naphthalene-1,5-disulfonato)magnesium(II)  

SciTech Connect (OSTI)

The structure of the title compound, [Mg(C{sub 10}H{sub 6}O{sub 6}S{sub 2})(C{sub 3}H{sub 7}NO){sub 2}]{sub n}, consists of MgO{sub 6} octahedra ({bar 1} symmetry) connected to naphthalene-1,5-disulfonate ligands ({bar 1} symmetry) in the equatoral plane, forming a two-dimensional network propagating parallel to (010). The coordination sphere of the Mg atom is completed by the O atoms of two N,N-dimethylformamide (DMF) molecules in the axial positions. The title compound represents the first time the naphthalene-1,5-disulfonate anion is bound directly to a Mg{sup 2+} atom. Disorder over two positions was found in the DMF molecule in a 0.518 (8):0.482 (8) ratio.

Borkowski, Lauren A.; Banerjee, Debasis; Parise, John B. (SBU)

2011-08-16T23:59:59.000Z

334

YAG laser-induced structural modification in transition metal ion containing 40K{sub 2}O-40Nb{sub 2}O{sub 5}-20SiO{sub 2} glasses  

SciTech Connect (OSTI)

Glasses with the compositions of 40K{sub 2}O-40Nb{sub 2}O{sub 5}-20SiO{sub 2} (in mol%) containing different concentrations (0.01, 1 and 2 mol%) of NiO were prepared by a melt quenching technique. The glasses were irradiated with a continuous wave Nd:YAG laser with a wavelength of 1064 nm, and a metastable crystalline phase of KNbO{sub 3} was obtained. In 2 mol% NiO-doped glass, lines with a width of {approx}10 {mu}m are successfully patterned by laser irradiations with a power of 0.9 W and a scanning speed of 15 {mu}m/s. It is found from micro-Raman scattering spectra that the lines are composed of the metastable crystalline phase of KNbO{sub 3}. The crystallization mechanism in Nd:YAG laser-induced crystallization in the glasses is discussed in comparison with the usual crystallization in an electric furnace.

Venkataraman, B. Harihara [Department of Materials Science and Technology, Nagaoka University of Technology, 1603-1 Kamitomioka-cho, Nagaoka 940-2188 (Japan); Komatsu, Takayuki [Department of Materials Science and Technology, Nagaoka University of Technology, 1603-1 Kamitomioka-cho, Nagaoka 940-2188 (Japan)], E-mail: komatsu@mst.nagaokaut.ac.jp

2008-10-02T23:59:59.000Z

335

Structural and Spectroscopic Characterization of 17- and 18-Electron Piano-Stool Complexes of Chromium. Thermochemical Analyses of Weak Cr-H Bonds  

SciTech Connect (OSTI)

The 17-electron radical CpCr(CO)2(IMe)• (IMe = 1,3-dimethylimidazol-2-ylidene) was synthesized by the reaction of IMe with [CpCr(CO)3]2, and characterized by single crystal X-ray diffraction and by EPR, IR and variable temperature 1H NMR spectroscopy. The metal-centered radical is monomeric under all conditions and exhibits Curie paramagnetic behavior in solution. An electrochemically reversible reduction to 18-electron CpCr(CO)2(IMe)? takes place at E½ = ?1.89(1) V vs Cp2Fe+•/0 in MeCN, and was accomplished chemically with KC8 in THF. The salts K+(18-crown-6)[CpCr(CO)2(IMe)]? • ½THF and K+[CpCr(CO)2(IMe)]? • ¾THF were crystallographically characterized. Monomeric ion pairs are found in the former, whereas the latter has a polymeric structure due to a network of K???O(CO) interactions. Protonation of K+(18-crown-6)[CpCr(CO)2(IMe)]? • ½THF gives the hydride CpCr(CO)2(IMe)H, which could not be isolated, but was characterized in solution; a pKa of 27.2(4) was determined in MeCN. A thermochemical analysis provides the Cr-H bond dissociation free energy (BDFE) for CpCr(CO)2(IMe)H in MeCN solution as 47.3(6) kcal mol?1. This value is exceptionally low for a transition metal hydride, and implies that the reaction 2 [Cr-H] ? 2 [Cr•] + H2 is exergonic (?G = ?9.0(8) kcal mol?1). This analysis explains the experimental observation that generated solutions of the hydride produce CpCr(CO)2(IMe)• (typically on the timescale of days). By contrast, CpCr(CO)2(PCy3)H has a higher Cr-H BDFE (52.9(4) kcal mol?1), is more stable with respect to H2 loss, and is isolable. We thank the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences, Division of Chemical Sciences, Geosciences and Biosciences for support. M.L.H. carried out the crystallographic studies and was supported as part of the Center for Molecular Electrocatalysis, an Energy Frontier Research Center funded by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences. The EPR studies were performed at the William R. Wiley Environmental Molecular Sciences Laboratory (EMSL), a national scientific user facility sponsored by the Department of Energy’s Office of Biological and Environmental Research located at PNNL. Pacific Northwest National Laboratory is a multiprogram national laboratory operated by Battelle for the U.S. Department of Energy.

van der Eide, Edwin F.; Helm, Monte L.; Walter, Eric D.; Bullock, R. Morris

2013-02-04T23:59:59.000Z

336

Measurement of genotoxic air pollutant exposures in street vendors and school children in and near Bangkok  

SciTech Connect (OSTI)

The effects of air pollution on human health are a great concern, particularly in big cities with severe traffic problems such as Bangkok, Thailand. In this study, exposure to genotoxic compounds in ambient air was studied by analysis of particle-associated polycyclic aromatic hydrocarbons (PAHs) and benzene through direct measurement of concentrations in air as well as through the use of different biomarkers of exposure: urinary 1-hydroxypyrene (1-OHP) for PAHs and urinary t,t-muconic acid (t,t-MA) for benzene. The study was conducted in various susceptible groups of the population with different occupations in 5 traffic-congested areas of Bangkok, as well as in primary school children. The level of total PAHs on the main roads at various sites ranged from 7.10 to 83.04 ng/m{sup 3}, while benzene levels ranged from 16.35 to 49.25 ppb. In contrast, ambient levels in nearby temples, the control sites, ranged from 1.67 to 3.04 ng/m{sup 3} total PAHs and 10.16 to 16.25 ppb benzene. Street vendors selling clothes were exposed to 16.07 {+-} 1.64 ng/m{sup 3} total PAHs and 21.97 {+-} 1.50 ppb benzene, levels higher than in monks and nuns residing in nearby temples (5.34 {+-} 0.65 ng/m{sup 3} total PAHs and 13.69 {+-} 0.77 ppb benzene). Grilled-meat vendors in the same area were exposed to both total PAHs and benzene at even higher levels, possibly due to additional formation of PAHs during the grilling of meat (34.27 {+-} 7.02 ng/m{sup 3} total PAHs; 27.49 {+-} 2.72 ppb benzene). At the end of the workday, urinary 1-OHP levels in street vendors (0.12 and 0.15 {mu}mol/mol creatinine in clothes and grilled-meat vendors, respectively) were significantly higher than in controls (0.04 {mu}mol/mol creatinine; P < 0.01). Afternoon urinary t,t-MA levels in both groups of street vendors (0.12 mg/g creatinine) were also significantly higher than in controls (0.08 mg/g creatinine; P < 0.05). School children from two schools in Bangkok were exposed to total PAHs and benzene at levels of 6.70 {+-} 0.47 ng/m{sup 3} and 4.71 {+-} 0.25 ppb, respectively, higher than those to which children living outside the city were exposed (1.25 {+-} 0.24 ng/m{sup 3} total PAHs; 2.10 {+-} 0.16 ppb benzene). At the end of the school day, levels of urinary 1-OHP and t,t-MA were significantly higher (P < 0.001 and P < 0.01, respectively) in Bangkok school children (0.23 {mu}mol/mol creatinine and 0.27 mg/g creatinine, respectively) than in school children from outside Bangkok (0.10 {mu}mol/mol creatinine and 0.08 mg/g creatinine, respectively)

Ruchirawat, Mathuros [Laboratory of Environmental Toxicology, Chulabhorn Research Institute, Bangkok 10210 (Thailand) and Department of Pharmacology, Faculty of Science, Mahidol University, Bangkok 10400 (Thailand)]. E-mail: mathuros@tubtim.cri.or.th; Navasumrit, Panida [Laboratory of Environmental Toxicology, Chulabhorn Research Institute, Bangkok 10210 (Thailand); Settachan, Daam [Laboratory of Environmental Toxicology, Chulabhorn Research Institute, Bangkok 10210 (Thailand); Tuntaviroon, Jantamas [Laboratory of Environmental Toxicology, Chulabhorn Research Institute, Bangkok 10210 (Thailand); Buthbumrung, Nantaporn [Laboratory of Environmental Toxicology, Chulabhorn Research Institute, Bangkok 10210 (Thailand); Sharma, Suman [Laboratory of Environmental Toxicology, Chulabhorn Research Institute, Bangkok 10210 (Thailand)

2005-08-07T23:59:59.000Z

337

Enthalpy of formation and magnetic susceptibility of curium sesquioxide, Cm/sub 2/O/sub 3/  

SciTech Connect (OSTI)

Monoclinic Cm/sub 2/O/sub 3/ has been prepared from the long-lived isotope /sup 248/Cm (t/sub 1///sub 2/ = 3.4 x 10/sup 5/ y), and its enthalpy of formation has been determined at 298 K to be -1682 +/- 12 kJ mol/sup -1/ from solution calorimetry measurements on four different samples. The magnetic susceptibility of three of these samples has been measured on a Faraday balance between 2 and 298 K. Cm/sub 2/O/sub 3/ exhibits Curie-Weiss behavior from 100 to 300 K with ..mu../sub eff/ = 7.89 +/- 0.04 ..mu../sub B/ and THETA = -130 +/- 2 K. The compound appears to order magnetically as the temperature decreases and has an antiferromagnetic transition at 13 +/- 2 K. The results are interpreted by comparison with similar properties of related lanthanide and actinide compounds.

Morss, L.R. (Argonne National Lab., IL); Fuger, J.; Goffart, J.; Haire, G.

1983-07-06T23:59:59.000Z

338

Water stress, temperature, and light effects on isoprene emission and photosynthesis of Kudzu leaves  

SciTech Connect (OSTI)

Kudzu (Pueraia lobata (Willd) Ohwi.) emits isoprene, a hydrocarbon which can significantly affect atmospheric chemistry. Isoprene emission under standard conditions of 1000 [mu]mol photons[center dot]M[sup [minus]2][center dot]S[sup [minus]1] and 30[degrees]C developed only after the leaf bad reached full expansion and was not maximal until up to two weeks past the point of full expansion of the leaf. Isoprene emission from kudzu was stimulated by increases in temperature and photon flux density (up to 3000 [mu]mol photons[center dot]m[sup [minus]2][center dot]s[sup [minus]1]). For unstressed plants, 20 % of the carbon fixed in photosynthesis was reemitted as isoprene at 1000 [mu]mol photons[center dot]m[sup [minus]2][center dot]S[sup [minus]1]. Following the relief of water stress, photosynthesis recovered to the prestress rate but isoprene emission increased up to five times the prestress rate. At 1000 [mu]mol photons[center dot]M[sup [minus]2][center dot]S[sup [minus]1] and 35[degrees]C, 67% of the carbon fixed in photosynthesis was reemitted as isoprene eight days after water stress. For some leaves the rate of isoprene emission exceeded 500 nmol[center dot]M[sup [minus]2][center dot]S[sup [minus]1], substantially higher than ever reported before. Leaves of plants grown at less than 20[degrees]C did not make isoprene until an inductive treatment was given. Withholding water from plants or keeping leaves at 30[degrees]C induced isoprene emission. The observation of rapid and dramatic changes in the rate of isoprene emission from leaves in response to water stress and temperature may indicate that isoprene emission improves the ability of plants to cope with these conditions. With the new information on temperature and water stress effects on isoprene emission we speculate on possible reasons for isoprene emission from plants.

Sharkey, T.D.; Loreto, F. (Univ. of Wisconsin, Madison (United States))

1993-05-01T23:59:59.000Z

339

PdZnAl Catalysts for the Reactions of Water-Gas-Shift, Methanol Steam Reforming, and Reverse-Water-Gas-Shift  

SciTech Connect (OSTI)

Pd/ZnO/Al2O3 catalysts were studied for water-gas-shift (WGS), methanol steam reforming, and reverse-water-gas-shift (RWGS) reactions. WGS activity was found to be dependent on the Pd:Zn ratio with a maximum activity obtained at approximately 0.50, which was comparable to that of a commercial Pt-based catalyst. The catalyst stability was demonstrated for 100 hours time-on-stream at a temperature of 3600C without evidence of metal sintering. WGS reaction rates were approximately 1st order with respect to CO concentration, and kinetic parameters were determined to be Ea = 58.3 kJ mol-1 and k0 = 6.1x107 min-1. During methanol steam reforming, the CO selectivities were observed to be lower than the calculated equilibrium values over a range of temperatures and steam/carbon ratios studied while the reaction rate constants were approximately of the same magnitude for both WGS and methanol steam reforming. These results indicate that although Pd/ZnO/Al2O3 are active WGS catalysts, WGS is not involved in methanol steam reforming. RWGS rate constants are on the order of about 20 times lower than that of methanol steam reforming, suggesting that RWGS reaction could be one of the sources for small amount of CO formation in methanol steam reforming.

Dagle, Robert A.; Platon, Alexandru; Datye, Abhaya K.; Vohs, John M.; Wang, Yong; Palo, Daniel R.

2008-03-07T23:59:59.000Z

340

[sup 7]Li-NMR determination of stability constants as a function of temperature for lithium-crown ether complexes in a molten salt mixtures  

SciTech Connect (OSTI)

The stability constants of several crown ethers with lithium ion were determined by [sup 7]Li-NMR measurements. A room temperature, basic molten salt of the composition of 55/45 mol % 1-methyl-3-ethyl-imidazolium chloride to aluminum (III) chloride was used as solvent. On the basis of a 1:1 complex formation the following order was found for the stability constants of the investigated crown ethers: 18-crown-6 < 12-crown-4 < benzo-15-crown-5 < 15-crown-5. A temperature dependence study for 12-crown-4, benzo-15-crown-5, and 15-crown-5 was undertaken for the range 5-84[degree]C. Values of [Delta]H and [Delta]S were calculated. At 5.5[degree]C the splitting of the single, fast exchange peak into two separate signals was observed for benzo-15-crown-5, providing further evidence for the formation of the 1:1 complex. 34 refs., 4 figs., 5 tabs.

Gerhard, A. (Univ. of Utah, Salt Lake City, UT (United States) Univ. of Witten/Herdecke (Germany)); Cobranchi, D.P.; Garland, B.A.; Highley, A.M.; Huang, Y.H.; Konya, G.; Eyring, E.M. (Univ. of Utah, Salt Lake City, UT (United States)); Zahl, A.; Eldik, R. van (Univ. of Witten/Herdecke (Germany)); Petrucci, S. (Polytechnic Univ., Farmingdale, NY (United States))

1994-08-11T23:59:59.000Z

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


341

Berthon P, Katoh M, Dusanter-Fourt 1, Kelly PA, Djiane J, 1986b. Purification of prolactin receptor from sow mam-mary gland and polyclonal antibodies production. Mol Cell Endocrinol, soumis publication  

E-Print Network [OSTI]

Berthon P, Katoh M, Dusanter-Fourt 1, Kelly PA, Djiane J, 1986b. Purification of prolactin receptor publication Djiane J, Durand P, Kelly PA, 1977. Evolution of prolactin receptors in rabbit mammary gland during pregnancy and lactation. Endocrinology, 100:1348-1356 Djiane J, Dusanter-Fourt 1, Katoh M, Kelly

Paris-Sud XI, Université de

342

INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS B: ATOMIC, MOLECULAR AND OPTICAL PHYSICS J. Phys. B: At. Mol. Opt. Phys. 37 (2004) 25852592 PII: S0953-4075(04)75545-5  

E-Print Network [OSTI]

June 2004 Online at stacks.iop.org/JPhysB/37/2585 doi:10.1088/0953-4075/37/12/013 Abstract We Opacity Project data. We find significant differences in photoionization rates for O II metastable states and Planck bound-free opacities is relatively small, but may be potentially significant. 1. Introduction

Nahar, Sultana Nurun

343

IOP PUBLISHING JOURNAL OF PHYSICS B: ATOMIC, MOLECULAR AND OPTICAL PHYSICS J. Phys. B: At. Mol. Opt. Phys. 42 (2009) 105201 (5pp) doi:10.1088/0953-4075/42/10/105201  

E-Print Network [OSTI]

of core and valence electron excitation in molecules and the dissociation dynamics under such excitations- coincidence technique may permit reconstruction of the geometry of the excited molecular ion. As an example in excitation into a discrete molecular orbital as a function of the molecular alignment has been studied

Bapat, Bhas

344

INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS B: ATOMIC, MOLECULAR AND OPTICAL PHYSICS J. Phys. B: At. Mol. Opt. Phys. 36 (2003) 41274143 PII: S0953-4075(03)64763-2  

E-Print Network [OSTI]

in molecular gases, focusing on collisional excitation of molecularrotationaland ro conservation and the vector dynamics associated with rotational excitation. It is pointed out. In particular, for swarms of electrons or ions in molecular gases, it is clear that excitation of rotational

Morrison, Michael A.

345

INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS B: ATOMIC, MOLECULAR AND OPTICAL PHYSICS J. Phys. B: At. Mol. Opt. Phys. 37 (2004) R57R88 PII: S0953-4075(04)63251-2  

E-Print Network [OSTI]

of the high-energy storage rings used in high-energy particle physics, in particular LEAR [8], and use mainly, they are usually smaller and require neither high-energy (MeV) accelerators for injecting the beam, nor and nuclear physics, nonlinear dynamics, single component plasmas, mass spectrometry, biophysics, quantum

Zajfman, Daniel

346

INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS B: ATOMIC, MOLECULAR AND OPTICAL PHYSICS J. Phys. B: At. Mol. Opt. Phys. 34 (2001) 36693678 PII: S0953-4075(01)23490-7  

E-Print Network [OSTI]

Rolles2 , F J Garc´ia de Abajo2 , C S Fadley2 , M A Van Hove2 , A Cassimi6 , H Schmidt-B¨ocking1 and R D the kinetic energ

Muiño, Ricardo Díez

347

Mol. Cryst. Lip. Crpr ,1997,Vol. 2W.pp. 301-306 0 lPY7 OPA ( O v m PublishersAssociati~n) Reprinuavailabledirmrly from the publisher Amnrerdam B.V.PubLshcd inTbe Nethdanda  

E-Print Network [OSTI]

can be Uustrated by differentid geometry theoremsg. If n ia normal to a family of surfaces S energ in Eq.(2). The appearance of a loop would mean that G in the region endored by the loop is reduced

Lavrentovich, Oleg D.

348

IOP PUBLISHING JOURNAL OF PHYSICS B: ATOMIC, MOLECULAR AND OPTICAL PHYSICS J. Phys. B: At. Mol. Opt. Phys. 42 (2009) 055506 (7pp) doi:10.1088/0953-4075/42/5/055506  

E-Print Network [OSTI]

interferometry Stefano Olivares1,2 and Matteo G A Paris1,2,3 1 CNISM, UdR Milano Universit`a, I-20133 Milano by means of Monte Carlo simulated experiments with a small number of homodyne data, thus giving

Paris, Matteo G. A.

349

IOP PUBLISHING JOURNAL OF PHYSICS B: ATOMIC, MOLECULAR AND OPTICAL PHYSICS J. Phys. B: At. Mol. Opt. Phys. 42 (2009) 035502 (6pp) doi:10.1088/0953-4075/42/3/035502  

E-Print Network [OSTI]

-parameter qubit gates Berihu Teklu1, Stefano Olivares1,2 and Matteo G A Paris1,2,3 1 Dipartimento di Fisica and a comparison with the results of Monte Carlo simulated experiments, we show that asymptotic optimality

Paris, Matteo G. A.

350

Journal of Physics B: Atomic, Molecular and Optical Physics J. Phys. B: At. Mol. Opt. Phys. 47 (2014) 075301 (12pp) doi:10.1088/0953-4075/47/7/075301  

E-Print Network [OSTI]

for the analysis of such condensates [4]. The long-range and anisotropic character of the DDI leads to new physical (2014) 075301 (12pp) doi:10.1088/0953-4075/47/7/075301 Bright solitons in Bose­Einstein condensates-dimensional model of a bosonic gas of particles carrying collinear dipole moments which are induced by an external

Gammal, Arnaldo

351

INSTITUTE OF PHYSICS PUBLISHING JOURNAL OF PHYSICS B: ATOMIC, MOLECULAR AND OPTICAL PHYSICS J. Phys. B: At. Mol. Opt. Phys. 37 (2004) 35513562 PII: S0953-4075(04)81883-2  

E-Print Network [OSTI]

in an accelerating potential Timothy M Roach Physics Department, The College of the Holy Cross, Worcester, MA 01610 #12;3552 T M Roach y gUBU U atoms grating(a) (b) y Figure 1. (a) Cloud of atoms accelerated towards

Roach, Timothy

352

Er{sup 3+}-doped strontium lithium bismuth borate glasses for broadband 1.5 {mu}m emission - optical properties  

SciTech Connect (OSTI)

Strontium lithium bismuth borate glasses (SLBiB) doped with various concentrations of Er{sup 3+} were prepared using conventional melt quench technique and investigated their optical properties. The amorphous nature of the prepared glass samples was confirmed by X-ray diffraction and SEM analysis. Optical properties were studied by measuring the optical absorption and near infrared luminescence spectra at room temperature. Judd-Ofelt (J-O) theory has been applied for the f.f transitions of Er{sup 3+} ions to evaluate J-O intensity parameters, {Omega}{lambda} ({lambda} = 2, 4 and 6). Using the J-O intensity parameters, radiative properties such as transition probabilities (A{sub R}), branching ratios ({beta}) and radiative lifetimes ({tau}) are estimated for certain transitions. From the emission spectra, peak emission-cross sections ({sigma}{sub p}) and products of stimulated emission cross-section and full width at half maximum ({sigma}{sub p} Multiplication-Sign FWHM) were calculated for the observed emission transition, {sup 4}I{sub 13/2}{yields}{sup 4}I{sub 15/2}.

Rajesh, D.; Balakrishna, A.; Ratnakaram, Y. C. [Department of Physics, Sri Venkateswara University, Tirupati-517502 (India)

2013-02-05T23:59:59.000Z

353

REcuRsiVE TRust-REGion MEthoDs FoR MuLtiLEVEL NonLinEAR ...  

E-Print Network [OSTI]

Aug 11, 2004 ... reasonable performance, more elaborate strategies exist for choosing it in ...... ould like to thank Arnaud FrPseville and the Nord-Pas-de-Calais.

2004-08-11T23:59:59.000Z

354

Systematic examination of the impact of pre-stimulus alpha- mu and gamma band oscillations on perception : correlative and causal manipulation in mouse and human  

E-Print Network [OSTI]

The over-arching hypothesis that drives my work is that neural dynamics, fluctuating on millisecond to second time scales, powerfully impact perception. In this thesis, I employ correlative electrophysiological recording ...

Pritchett, Dominique L. (Dominique Leon)

2012-01-01T23:59:59.000Z

355

Star Formation and AGN activity in Galaxies classified using the 1.6 {\\mu}m Bump and PAH features at $z = 0.4-2$  

E-Print Network [OSTI]

We have studied the star-formation and AGN activity of massive galaxies in the redshift range $z=0.4-2$, which are detected in a deep survey field using the AKARI InfraRed (IR) astronomical satellite and {\\em Subaru} telescope toward the North Ecliptic Pole (NEP). The AKARI/IRC Mid-InfraRed (MIR) multiband photometry is used to trace their star-forming activities with the Polycyclic-Aromatic Hydrocarbon (PAH) emissions, which is also used to distinguish star-forming populations from AGN dominated ones and to estimate the Star Formation Rate (SFR) derived from their total emitting IR (TIR) luminosities. In combination with analyses of their stellar components, we have studied the MIR SED features of star-forming and AGN-harboring galaxies.

Hanami, Hitoshi; Fujishiro, Naofumi; Nakanishi, Kouichiro; Miyaji, Takamitsu; Krumpe, Mirko; Umetsu, Keiichi; Ohyama, Youichi; Shim, Hyun Jin; Im, Myungshin; Lee, Hyoung Mok; Lee, Myung Gyoon; Serjeant, Stephen; White, Glenn J; Willmer, Christopher N; Goto, Tomotsugu; Oyabu, Shinki; Takagi, Toshinobu; Wada, Takehiko; Matsuhara, Hideo

2011-01-01T23:59:59.000Z

356

The effect of the earth's atmosphere on the zenith-angle variation of the intensity of mu-mesons at sea level  

E-Print Network [OSTI]

+ and g +~~a i The oonstant X is adJusted to give the observed intensity when E ia expressed in oleO tron voltsc and the exponent has been ohosen to fit ths energy dependsnoe of tihe speotrun at high essrgieso Gonsidsr the inoidenoe of a p~ oosnio ray... with velocity $ t-' with respect tc the laboratory fram of reference is It It / Vi- p it the high energ1es oousidered here the pal'ticle velocities ere vezy close to C ~ When h- is neasured in actual distance unitsl 1 4 g osn tineters rather than grano per...

Gondran, Albert Donald

1954-01-01T23:59:59.000Z

357

CLOUD SCREENING METHODOLOGY FOR MERIS/AATSR SYNERGY PRODUCTS Luis Gomez-Chova, Gustavo Camps-Valls, Jordi Mu~noz-Mari, Javier Calpe, and Jose Moreno  

E-Print Network [OSTI]

CLOUD SCREENING METHODOLOGY FOR MERIS/AATSR SYNERGY PRODUCTS Luis G´omez-Chova, Gustavo Camps (Valencia), Spain. ABSTRACT This paper describes the current development status of a cloud-screening method to improve current cloud mask- ing products for both sensors. Preliminary results based on simulated TOA

Camps-Valls, Gustavo

358

Mu suM national d'Histoire naturelle 57 rue Cuvier -75005 Paris -+33 (0)1 40 79 56 01 / 54 79 -www.mnhn.fr  

E-Print Network [OSTI]

- www.mnhn.fr 26 Hectares of galleries, greenHouses, laboratories, learning facilities and a zoo GrandeColoGy, sustainable develoPment and enerGy Cover Photos: Cypraea sp Or «COWZry», raDIOGrapHy © asT-rX/MNHN VIGNeNCHOT/MNHN. LarGe INsIDe pHOTOs LeFT TO rIGHT: Lys © MNHN ; BuTTerFLy arGeMa MIMOsae, MOZaMBIQue © XaVIer Des

359

1424 VOLUME 18 NUMBER 12 DECEMBER 2011 NATURE STRUCTURAL & MOLECULAR BIOLOGY B R I E F COM MU N I CAT I ON S  

E-Print Network [OSTI]

CAT I ON S A shared structural solution for neutralizing ebolaviruses João M Dias1,7, Ana I Kuehne2

Chandran, Kartik

360

AUTOMATIC CODE GENERATION FOR MULTI-MICROBLAZE SYSTEM WITH Pengcheng Mu, Mickal Raulet, Jean-Franois Nezan, Jean-Gabriel Cousin  

E-Print Network [OSTI]

20, avenue des Buttes de Coësmes, 35043 RENNES Cedex, France pmu@ens.insa-rennes.fr {mraulet, jnezan distribution: manual data

Paris-Sud XI, Université de

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


361

Visible Light-Induced Electron Transfer from Di-mu-oxo Bridged Dinuclear Mn Complexes to Cr Centers in Silica Nanopores  

E-Print Network [OSTI]

mg) was placed in 10 mL of acetonitrile buffered with 0.01 Mform a brown solid in pure acetonitrile. 32 Depending on thewashed with 5 x 20 mL acetonitrile, and dried in vacuo for 2

Weare, Walter

2008-01-01T23:59:59.000Z

362

Photomagnetic Switching of the Complex [Nd(dmf)[subscript 4](H[subscript 2]O)[subscript 3]([mu]-CN)Fe(CN)[subscript 5  

SciTech Connect (OSTI)

Single-crystal XRD experiments (see picture) reveal the excited-state structure of the photomagnetic heterobimetallic title complex. The system shows a decrease in all the iron-ligand bond lengths, suggesting that photoexcitation involves a ligand-to-metal charge transfer or a change in the superexchange coupling between the metal centers.

Svendsen, Helle; Overgaard, Jacob; Chevallier, Marie; Collet, Eric; Iversen, Bo B.; (Aarhus); (Universite de Rennes)

2009-10-21T23:59:59.000Z

363

Academic Exploration and Advising Services M110 Student Success Center 884-9700 http://aeas.missouri.edu October 2008 MU UNDERGRADUATE MAJORS, EMPHASIS AREAS,  

E-Print Network [OSTI]

and Biotechnology; Plant Protection; Precision Agriculture; Turfgrass Management College of Arts and Science Engineering BS IE Information Technology BS Mechanical Engineering BS ME College of Human Environmental

Taylor, Jerry

364

Design and construction of equipment for determining the zenith-angle dependence of the high-energy mu-meson intensity at sea level  

E-Print Network [OSTI]

field of a nucleus j ~? if they are energetio enough? znsezesons 4 can intezmct electromagnetically with nuclei to produce enezgetic pho toner ClasaioaLly the total energy radiated by a charged particle which is accelerated is proportional... to the souare of the aoceleration of the particle, This essential feature is zm flected in ohe quantum-eleotrodynsmic result that the probability for the emission of a photon of a given ener;y is proportional to the square of the accelezation suffered...

Anderson, Floyd Chris

1954-01-01T23:59:59.000Z

365

COLUP: The Cautious Optimistic Lazy Update Luis Irun-Briz, Francesc D. Mu~noz-Escoi, Josep M. Bernabeu-Auban  

E-Print Network [OSTI]

conflicts. In this paper, we present the problem of the abortion rate in such protocols from the statistical to have an undesirable behavior in respect to the abortion rate in scenarios with high degree of access of this expres- sion, allowing the system to reduce the abortion rate, and maintaining stable, or even improve

Muñoz, Francesc

366

Two Pathways for Electrocatalytic Oxidation of Hydrogen by a Nickel Bis(diphosphine) Complex with Pendant Amines in the Second Coordination Sphere  

SciTech Connect (OSTI)

A nickel bis(diphosphine) complex containing pendant amines in the second coordination sphere, [Ni(PCy2Nt-Bu2)2](BF4)2 (PCy2Nt-Bu2 = 1,5-di(tert-butyl)-3,7-dicyclohexyl-1,5-diaza-3,7-diphosphacyclooctane), is an electrocatalyst for hydrogen oxidation. Under 1.0 atm H2 using NEt3 as a base and with added water, a turnover frequency of 45 s-1 is observed at 23 °C; this is the fastest observed for a molecular catalyst. The addition of hydrogen to the NiII complex gives thee isomers of the doubly protonated Ni0 complex [Ni(PCy2HNt-Bu2)2](BF4)2; these complexes have been studied by 1H and 31P NMR spectroscopy, and for one isomer, an X-ray diffraction study. Using the pKa values and NiII/I and NiI/0 redox potentials in a thermochemical cycle, the free energy of hydrogen addition to [Ni(PCy2Nt-Bu2)2]2+ was determined to be -7.9 kcal mol-1. The catalytic rate observed in dry acetonitrile for the oxidation of H2 at the NiII/I couple depends on base size, with larger bases (NEt3, tert-BuNH2) resulting in slower catalysis than n-BuNH2. Addition of water accelerates the rate of catalysis, especially for the larger bases. The results of these studies provide important insights into the design of catalysts for hydrogen oxidation that facilitate proton movement and operate at moderate potentials. This research was supported as part of the Center for Molecular Electrocatalysis, an Energy Frontier Research Center funded by the U.S. Department of Energy, Office of Science. Pacific Northwest National Laboratory is operated by Battelle for the U.S. Department of Energy.

Yang, Jenny Y.; Smith, Stuart E.; Liu, Tianbiao L.; Dougherty, William G.; Hoffert, Wesley A.; Kassel, W. S.; Rakowski DuBois, Mary; DuBois, Daniel L.; Bullock, R. Morris

2013-07-03T23:59:59.000Z

367

1-Dodecane-sulfonic-acid-sodium-salt(LAS) assisted hydrothermal synthesis of Cd{sub x}Zn{sub 1-x}S solid solution as efficient photocatalysts under visible light irradiation  

SciTech Connect (OSTI)

With anionic surfactant LAS assisted, series of zinc cadmium sulfide semiconductor photocatalysts were synthesized by hydrothermal method. These products were characterized by X-ray diffraction (XRD), UV-Vis absorption spectra (UV-Vis) and scanning electron microscopy (FESEM). The photocatalytic activities of as-prepared samples were evaluated by photocatalytic hydrogen production from water under visible-light irradiation. The best synthesis parameters are: Composition 0.9:0.1 (Cd:Zn molar ratio), Temperature 160 deg. C, Hydrothermal Time 48 Hour, LAS Concentration 1.7 mmol/L, the maximum visible-light-catalytic hydrogen production rate is 161.25 {mu}mol/h (lambda>430 nm) which is higher than those of by coprecipitation method. The experiment results indicate that surfactant assisted hydrothermal method is an effective way to get highly active CdZnS solid solution photocatalyst.

Jia, B.; Guo, L. J. [State Key Laboratory of Multiphase Flow in power Engineering, Xi'an Jiaotong University (China)

2010-03-01T23:59:59.000Z

368

Arsenic remediation of drinking water using iron-oxide coated coal bottom ash  

SciTech Connect (OSTI)

We describe laboratory and field results of a novel arsenic removal adsorbent called 'Arsenic Removal Using Bottom Ash' (ARUBA). ARUBA is prepared by coating particles of coal bottom ash, a waste material from coal fired power plants, with iron (hydr)oxide. The coating process is simple and conducted at room temperature and atmospheric pressure. Material costs for ARUBA are estimated to be low (~;;$0.08 per kg) and arsenic remediation with ARUBA has the potential to be affordable to resource-constrained communities. ARUBA is used for removing arsenic via a dispersal-and-removal process, and we envision that ARUBA would be used in community-scale water treatment centers. We show that ARUBA is able to reduce arsenic concentrations in contaminated Bangladesh groundwater to below the Bangladesh standard of 50 ppb. Using the Langmuir isotherm (R2 = 0.77) ARUBA's adsorption capacity in treating real groundwater is 2.6x10-6 mol/g (0.20 mg/g). Time-to-90percent (defined as the time interval for ARUBA to remove 90percent of the total amount of arsenic that is removed at equilibrium) is less than one hour. Reaction rates (pseudo-second-order kinetic model, R2>_ 0.99) increase from 2.4x105 to 7.2x105 g mol-1 min-1 as the groundwater arsenic concentration decreases from 560 to 170 ppb. We show that ARUBA's arsenic adsorption density (AAD), defined as the milligrams of arsenic removed at equilibrium per gram of ARUBA added, is linearly dependent on the initial arsenic concentration of the groundwater sample, for initial arsenic concentrations of up to 1600 ppb and an ARUBA dose of 4.0 g/L. This makes it easy to determine the amount of ARUBA required to treat a groundwater source when its arsenic concentration is known and less than 1600 ppb. Storing contaminated groundwater for two to three days before treatment is seen to significantly increase ARUBA's AAD. ARUBA can be separated from treated water by coagulation and clarification, which is expected to be less expensive than filtration of micron-scale particles, further contributing to the affordability of a community-scale water treatment center.

MATHIEU, JOHANNA L.; GADGIL, ASHOK J.; ADDY, SUSAN E.A.; KOWOLIK, KRISTIN

2010-06-01T23:59:59.000Z

369

Complete oxidation of CO, ethanol, and ethyl acetate over copper oxide supported on titania and ceria modified titania  

SciTech Connect (OSTI)

Titania and titania modified with 3 and 12 {mu}mol Ce/m{sup 2} surface area of the titania were prepared and were used as supports for copper oxide. Preparations with 3 and 12 {mu}mol CuO{sub x}/m{sup 2} surface area of the support were tested for the combustion of CO, ethyl acetate, and ethanol. The results show that the Ce-doped titania surface is good as support for CuO{sub x} and that the cerium not only enhances the activity of the copper species, but also stabilizes the surface area of the TiO{sub 2} support in the presence of copper oxide. Additions of Al, K, and La are also found to stabilize the TiO{sub 2} support but, compared with Ce, these elements do not to the same extent enhance the activity of the copper species. Acetaldehyde is observed to ban an intermediate in the combustion of both ethanol and ethyl acetate over Cu-Ce-Ti-O catalysts. Since acetaldehyde is more harmful than any of the reactants and also is photochemically active, it is in applications important to assure that the combustion is complete. Cu-Ce-Ti-O catalysts show good performance not only for feeds without water vapor, but also for humid feeds. Although the concentrations of intermediates are affected by the addition of water, there is little effect on the temperature required for obtaining complete conversion to carbon dioxide and water. Characterization with XRD, FT-Raman, TPR, and XPS indicates that the dispersed copper species are in the form of patches or a bidimensional layer which interacts with the surface of the support. When the content of cerium and copper is low, other types of dispersed copper species are present, which possibly are monomers or dimers. The copper species are predominantly Cu{sup 2+} species.

Larsson, P.O. [Perstorp AB (Sweden)] [Perstorp AB (Sweden); Andersson, A. [Univ. of Lund (Sweden). Dept. of Chemical Engineering II] [Univ. of Lund (Sweden). Dept. of Chemical Engineering II

1998-10-01T23:59:59.000Z

370

Synthesis, structure and magnetic properties of La{sub 3}Co{sub 2}SbO{sub 9}: A double perovskite with competing antiferromagnetic and ferromagnetic interactions  

SciTech Connect (OSTI)

The synthesis, structural characterization, and magnetic properties of La{sub 3}Co{sub 2}SbO{sub 9} double perovskite are reported. The crystal structure has been refined by X-ray and neutron powder diffraction data in the monoclinic space group P2{sub 1}/n. Co{sup 2+} and Sb{sup 5+} have the maximum order allowed for the La{sub 3}Co{sub 2}SbO{sub 9} stoichiometry. Rietveld refinements of powder neutron diffraction data show that at room temperature the cell parameters are a=5.6274(2) A, b=5.6842(2) A, c=7.9748(2) A and {beta}=89.999(3) Degree-Sign . Magnetization measurements indicate the presence of ferromagnetic correlations with T{sub C}=55 K attributed to the exchange interactions for non-linear Co{sup 2+}-O-Sb{sup 5+}-O-Co{sup 2+} paths. The effective magnetic moment obtained experimentally is {mu}{sub exp}=4.38 {mu}{sub B} (per mol Co{sup 2+}), between the theoretical one for spin only (3.87 {mu}{sub B}) and spin-orbit value (6.63 {mu}{sub B}), indicating partially unquenched contribution. The low magnetization value at high magnetic field and low temperature (1 {mu}{sub B}/f.u., 5 T and 5 K) and the difference between ZFC and FC magnetization curves (at 5 kOe) indicate that the ferromagnetism do not reach a long range order and that the material has an important magnetic frustration. - Graphical abstract: Co-O-Co (Yellow octahedra only) rich zones (antiferromagnetic) are in contact with Co-O-Sb-O-Co (Red and yellow octahedra) rich zones (Ferromagnetic) to give the peculiar magnetic properties, as a consequence, a complex hysteresis loop can be observed composed by a main and irreversible curve in all the measured range, superimposed with a ferromagnetic component at low fields. Highlights: Black-Right-Pointing-Pointer La{sub 3}Co{sub 2}SbO{sub 9} has small Goldschmidt Tolerance Factor (t) due to the small size of La{sup 3+}. Black-Right-Pointing-Pointer Small t determines an angle for the path Co{sup 2+}-O-Sb{sup 5+}-O-Co{sup 2+} of 153 Degree-Sign . Black-Right-Pointing-Pointer Ferromagnetism is attributed to exchange interactions for Co{sup 2+}-O-Sb{sup 5+}-O-Co{sup 2+} paths. Black-Right-Pointing-Pointer Ferromagnetic nanoclusters are embedded in an antiferromagnetic matrix.

Franco, D.G.; Fuertes, V.C.; Blanco, M.C. [INFIQC (CONICET), Departamento de Fisicoquimica, Facultad de Ciencias Quimicas, Universidad Nacional de Cordoba, Ciudad Universitaria, X5000HUA Cordoba (Argentina)] [INFIQC (CONICET), Departamento de Fisicoquimica, Facultad de Ciencias Quimicas, Universidad Nacional de Cordoba, Ciudad Universitaria, X5000HUA Cordoba (Argentina); Fernandez-Diaz, M.T. [Institute Laue-Langevin (ILL) 156X, F-38042 Grenoble Cedex 9 (France)] [Institute Laue-Langevin (ILL) 156X, F-38042 Grenoble Cedex 9 (France); Sanchez, R.D., E-mail: rodo@cab.cnea.gov.ar [Centro Atomico Bariloche, CNEA and Instituto Balseiro, Universidad Nacional de Cuyo, Av. Bustillo 9500, 8400 Rio Negro (Argentina); Carbonio, R.E., E-mail: carbonio@fcq.unc.edu.ar [INFIQC (CONICET), Departamento de Fisicoquimica, Facultad de Ciencias Quimicas, Universidad Nacional de Cordoba, Ciudad Universitaria, X5000HUA Cordoba (Argentina)

2012-10-15T23:59:59.000Z

371

Light and CO sub 2 effects on photosynthesis and growth in Kudzu  

SciTech Connect (OSTI)

Kudzu (Pueraria lobata Willd.) was grown for 28 days under four permutations of light (1,500 or 450 {mu}mol quanta m{sup {minus}2} s{sup {minus}1}) and CO{sub 2} (700 or 350 {mu}L L{sup {minus}1} CO{sub 2}). Total biomass and leaf area were up to 55% and 52% respectively greater in the high CO{sub 2} treatments. When measured at the growth CO{sub 2} concentration, photosynthetic rates showed little reduction over the 28 day period, and remained up to 29% higher in the high CO{sub 2} treatments. Under high light, soluble protein was 27% greater in the plants grown at high CO{sub 2}. Neither light nor CO{sub 2} had a significant effect on the initial or total rubisco activities. However, phosphoribulokinase activity was decreased under the high CO{sub 2} treatments. These data indicate that photosynthesis in kudzu shows little acclimation when grown at elevated CO{sub 2}.

Schweder, M.; Bowes, G. (Univ. of Florida, Gainesville (USA)); Cure, J. (Duke Univ., Durham, NC (USA))

1990-05-01T23:59:59.000Z

372

Gas temperature profiles at different flow rates and heating rates suffice to estimate kinetic parameters for fluidised bed combustion  

SciTech Connect (OSTI)

Experimental work on estimation kinetic parameters for combustion was conducted in a bench-scale fluidised bed (FB: 105x200mm). Combustion medium was obtained by using an electrical heater immersed into the bed. The ratio of heating rate (kJ/s) to molar flow rate of air (mol/s) regulated by a rheostat so that the heat of combustion (kJ/mol) can be synthetically obtained by an electrical power supply for relevant O{sub 2}-feedstock concentration (C{sub 0}). O{sub 2}-restriction ratio ({beta}) was defined by the ratio of O{sub 2}-feedstock concentration to O{sub 2}-air concentration (C{sub O{sub 2}-AIR}) at prevailing heating rates. Compressed air at further atmospheric pressure ({approx_equal}102.7kPa) entered the bed that was alumina particles (250{mu}m). Experiments were carried out at different gas flow rates and heating rates. FB was operated with a single charge of (1300g) particles for obtaining the T/T{sub 0} curves, and than C/C{sub 0} curves. The mathematical relationships between temperature (T) and conversion ratio (X) were expressed by combining total energy balance and mass balance in FB. Observed surface reaction rate constants (k{sub S}) was obtained from the combined balances and proposed model was also tested for these kinetic parameters (frequency factor: k{sub 0}, activation energy: E{sub A}, and reaction order: n) obtained from air temperature measurements. It was found that the model curves allow a good description of the experimental data. Thus, reaction rate for combustion was sufficiently expressed. (author)

Suyadal, Y. [Faculty of Engineering, Department of Chemical Engineering, Ankara University, 06100-Tandogan, Ankara (Turkey)

2006-07-15T23:59:59.000Z

373

Search for resonant second generation slepton production at the Fermilab Tevatron  

E-Print Network [OSTI]

We present a search for supersymmetry in the R-parity violating resonant production and decay of smuons and muon sneutrinos in the channels mu ->chi(0)(1)mu, mu ->chi(0)(2,3,4)mu, and nu(mu)->chi(+/-)(1,2)mu. We analyzed ...

Bandurin, V.; Baringer, Philip S.; Bean, Alice; Christofek, L.; Coppage, Don; Gardner, J.; Hensel, Carsten; Moulik, Tania; Wilson, Graham Wallace

2006-09-01T23:59:59.000Z

374

Writing of nonlinear optical Sm{sub 2}(MoO{sub 4}){sub 3} crystal lines at the surface of glass by samarium atom heat processing  

SciTech Connect (OSTI)

Some glasses such as 21.25Sm{sub 2}O{sub 3}.63.75MoO{sub 3}.15B{sub 2}O{sub 3} (mol %) giving the formation of nonlinear optical Sm{sub 2}(MoO{sub 4}){sub 3} crystals through conventional crystallization in an electric furnace and through continuous-wave Nd: yttrium aluminum garnet (YAG) laser (wavelength: 1064 nm) irradiation (samarium atom heat processing) have been developed. It is proposed from x-ray diffraction analyses, micro-Raman-scattering spectra, and second-harmonic generation measurements that the crystal structure of Sm{sub 2}(MoO{sub 4}){sub 3} formed by the crystallization is the {beta}{sup '}-phase structure with an orthorhombic (noncentrosymmetric) symmetry. The lines consisting of nonlinear optical {beta}{sup '}-Sm{sub 2}(MoO{sub 4}){sub 3} crystals are written at the surface of glasses by YAG laser irradiation (laser power: P=0.4 W, laser scanning speed: S=1-10 {mu}m/s), and, in particular, homogeneous crystal lines are formed at the laser scanning speed of 1 {mu}m/s. Refractive index changes (not crystallization) are also induced by YAG laser irradiation of P=0.4 W and a high laser scanning speed of S=25 {mu}m/s. The crystallization mechanism in the laser-irradiated region has been proposed. The present study demonstrates that the samarium atom heat processing is a technique for the writing of rare earth containing optical nonlinear/ferroelectric crystal lines in glass.

Abe, M.; Benino, Y.; Fujiwara, T.; Komatsu, T.; Sato, R. [Department of Chemistry, Nagaoka University of Technology, 1603-1 Kamitomioka-cho, Nagaoka 940-2188 (Japan); Department of Materials Engineering, Tsuruoka National College of Technology, Tsuruoka 997-8511 (Japan)

2005-06-15T23:59:59.000Z

375

Synthesis of Sm{sup 3+}-doped strontium barium niobate crystals in glass by samarium atom heat processing  

SciTech Connect (OSTI)

New glasses giving the crystallization of Sm{sup 3+}-doped Sr {sub x} Ba{sub 1-} {sub x} Nb{sub 2}O{sub 6} (SBN) ferroelectrics have been developed in the Sm{sub 2}O{sub 3}-SrO-BaO-Nb{sub 2}O{sub 5}-B{sub 2}O{sub 3} system, and the formation of SBN crystal dots and lines by continuous wave Nd:YAG laser (wavelength:1064 nm, power: 1 W) irradiations, i.e., samarium atom heat processing, has been examined. The formation of Sm{sup 3+}-doped SBN non-linear optical crystals is confirmed from X-ray diffraction analyses, micro-Raman scattering spectra, second harmonic generations, and photoluminescence spectra. Sm{sup 3+}-doped SBN crystal dots with the diameters of 20-70 {mu}m and lines with the widths of 20-40 {mu}m are written at the surface of some glasses such as 10Sm{sub 2}O{sub 3}.10SrO.10BaO.20Nb{sub 2}O{sub 5}.50B{sub 2}O{sub 3} (mol%) by Nd:YAG laser irradiations with the irradiation times of 20-70 s for the dots and with the scanning speeds of 1-5 {mu}m/s for the lines. The present study suggests that the samarium atom heat processing has a potential for the patterning of optical waveguides consisting of ferroelectric SBN crystals in glass substrates.

Chayapiwut, Nakorn [Department of Chemistry, Nagaoka University of Technology, 1603-1 Kamitomioka-cho, Nagaoka 940-2188 (Japan); Honma, Tsuyoshi [Department of Chemistry, Nagaoka University of Technology, 1603-1 Kamitomioka-cho, Nagaoka 940-2188 (Japan); Benino, Yasuhiko [Department of Chemistry, Nagaoka University of Technology, 1603-1 Kamitomioka-cho, Nagaoka 940-2188 (Japan); Fujiwara, Takumi [Department of Chemistry, Nagaoka University of Technology, 1603-1 Kamitomioka-cho, Nagaoka 940-2188 (Japan); Komatsu, Takayuki [Department of Chemistry, Nagaoka University of Technology, 1603-1 Kamitomioka-cho, Nagaoka 940-2188 (Japan)]. E-mail: komatsu@chem.nagaokaut.ac.jp

2005-11-15T23:59:59.000Z

376

Microstructure, strengthening mechanisms and hot deformation behavior of an oxide-dispersion strengthened UFG Al6063 alloy  

SciTech Connect (OSTI)

An ultrafine-grained Al6063/Al{sub 2}O{sub 3} (0.8 vol.%, 25 nm) nanocomposite was prepared via powder metallurgy route through reactive mechanical alloying and hot powder extrusion. Scanning electron microcopy, transmission electron microscopy, and back scattered electron diffraction analysis showed that the grain structure of the nanocomposite is trimodal and composed of nano-size grains (< 0.1 {mu}m), ultrafine grains (0.1-1 {mu}m), and micron-size grains (> 1 {mu}m) with random orientations. Evaluation of the mechanical properties of the nanocomposite based on the strengthening-mechanism models revealed that the yield strength of the ultrafine-grained nanocomposite is mainly controlled by the high-angle grain boundaries rather than nanometric alumina particles. Hot deformation behavior of the material at different temperatures and strain rates was studied by compression test and compared to coarse-grained Al6063 alloy. The activation energy of the hot deformation process for the nanocomposite was determined to be 291 kJ mol{sup -1}, which is about 64% higher than that of the coarse-grained alloy. Detailed microstructural analysis revealed that dynamic recrystallization is responsible for the observed deformation softening in the ultrafine-grained nanocomposite. - Highlights: Black-Right-Pointing-Pointer The strengthening mechanisms of Al6063/Al{sub 2}O{sub 3} nanocomposite were evaluated. Black-Right-Pointing-Pointer Hot deformation behavior of the nanocomposite was studied. Black-Right-Pointing-Pointer The hot deformation activation energy was determined using consecutive models. Black-Right-Pointing-Pointer The restoration mechanisms and microstructural changes are presented.

Asgharzadeh, H. [Department of Mechanical Engineering, University of Tabriz, P.O. Box 51666-16471, Tabriz (Iran, Islamic Republic of)] [Department of Mechanical Engineering, University of Tabriz, P.O. Box 51666-16471, Tabriz (Iran, Islamic Republic of); Kim, H.S. [Department of Materials Science and Engineering, Pohang University of Science and Technology, P.O. Box 790-784, Pohang (Korea, Republic of)] [Department of Materials Science and Engineering, Pohang University of Science and Technology, P.O. Box 790-784, Pohang (Korea, Republic of); Simchi, A., E-mail: simchi@sharif.edu [Department of Materials Science and Engineering and Institute for Nanoscience and Nanotechnology, Sharif University of Technology, P.O. Box 11365-9466, Tehran (Iran, Islamic Republic of)

2013-01-15T23:59:59.000Z

377

First measurement of the ratio of branching fractions BR(Lambda(b) to Lambda(c) mu nu)/BR(Lambda(b) to Lambda(c) pi) at CDF II  

SciTech Connect (OSTI)

In this dissertation, we measure the properties of the lowest-mass beauty baryon, {Lambda}{sub b}. Baryons are the bound states of three quarks. Protons and neutrons, constituents of atomic nuclei, are the most common baryons. Other types of baryons can be produced and studied in the high-energy collider environment. Three-body dynamics makes baryons composed of low mass quarks difficult to study. On the other hand, baryons with one heavy quark simplify the theoretical treatment of baryon structure, since the heavy quark can be treated the same way as the nucleus in the atom. The {Lambda}{sub b} is composed of u, d, and b quarks, where the b quark is much heavier than the other two. Although, it is accessible, little is known about {Lambda}{sub b}. In 1991, UA1 [1] reconstructed 9 {+-} 1 {Lambda}{sub b} {yields} J/{Psi}{Lambda} candidates. In 1996, ALEPH and DELPHI reconstructed the decay {Lambda}{sub b} {yields} {Lambda}{sub c}{sup +}{pi}{sup -} and found only 3-4 candidates [2, 3]. ALEPH measured a {Lambda}{sub b} mass of 5614 {+-} 21 MeV/c{sup 2}, while DELPHI measured 5668 {+-} 18 MeV/c{sup 2}, about 2 {sigma} higher. Subsequently, CDF-I observed 20 {Lambda}{sub b} {yields} J/{Psi}{Lambda} events [4], confirmed the existence of {Lambda}{sub b} unambiguously and made a more precise measurement of {Lambda}{sub b} mass, 5621 {+-} 5 MeV/c{sup 2}. A recent CDF-II measurement by Korn [5] yields 5619.7 {+-} 1.7 MeV/c{sup 2}, which will significantly improve the current world average, 5624 {+-} 9 MeV/c{sup 2}, and resolve the discrepancy of ALEPH and DELPHI.

Yu, Shin-shan; /Pennsylvania U.

2005-01-01T23:59:59.000Z

378

Classifying Three-way Seismic Volcanic Data by Dissimilarity Representation Diana Porro-Mu~noz , Isneri Talavera, Robert P.W. Duin, Mauricio Orozco-Alzate and John Makario Londo~no-Bonilla  

E-Print Network [OSTI]

Classifying Three-way Seismic Volcanic Data by Dissimilarity Representation Diana Porro in a natural way. As an example, the classification of seismic volcanic events is used. It is shown features. Keywords-volcanic seismic data, three-way representation, dissimilarity representation

Duin, Robert P.W.

379

OC$78@MU%3!<%Q%9$N7ABVAG2r@O Fb85 @65. y LnH* <~ y ;3ED FF y 4X:, Ao z 0f:486 6Q y  

E-Print Network [OSTI]

$rkJ}K! (Nc$($P (3) $J$I) $G$"$j!"$b$&0l$D$O L$CN8l$G$b2r@O$G$­$k$h$&$J%b%G%k$r:n@.$9$kJ}K! (Nc$( $P (4, 5) $J$I) $G$"$k!#$3$3$G!"A0

Sekine, Satoshi

380

PubMed contains all of MEDLINE (1966-present), OLDMEDLINE (1946-1965), PubMed in-process records (new citations not yet fully indexed) and some additional non-MEDLINE citations. It is the primary database for researchers in the fields of biochemistry, mol  

E-Print Network [OSTI]

BASIC SEARCH TECHNIQUES PubMed searching is easy. Just enter your search terms in the search box to additional searching options. Keyword Searching Enter one or more keywords (e.g., molecular motors) in the search box and click Search. PubMed automatically combines (ANDs) significant terms together using

California at Berkeley, University of

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


381

The highly attenuated oncolytic recombinant vaccinia virus GLV-1h68: comparative genomic features and the contribution of F14.5L inactivation  

E-Print Network [OSTI]

Mol Genet Genomics (2009) 282:417–435 DOI 10.1007/s00438-DQ121394) Mol Genet Genomics (2009) 282:417–435 VacciniaU ml ¡1 , Mol Genet Genomics (2009) 282:417–435 amphotericin

Zhang, Qian; Liang, Chunguang; Yu, Yong A.; Chen, Nanhai; Dandekar, Thomas; Szalay, Aladar A.

2009-01-01T23:59:59.000Z

382

Genetic interactions between a phospholipase A2 and the Rim101 pathway components in S. cerevisiae reveal a role for this pathway in response to changes in membrane composition and shape  

E-Print Network [OSTI]

Mol Genet Genomics (2010) 283:519–530 DOI 10.1007/s00438-products that Mol Genet Genomics (2010) 283:519–530 remainRim13p. Mol Genet Genomics (2010) 283:519–530 Materials and

Mattiazzi, M.; Jambhekar, A.; Kaferle, P.; DeRisi, J. L.; Križaj, I.; Petrovi?, U.

2010-01-01T23:59:59.000Z

383

The YEATS domain of Taf14 in Saccharomyces cerevisiae has a negative impact on cell growth  

E-Print Network [OSTI]

and osmolarity, Mol Genet Genomics (2010) 283:365–380 Fig. 7Mol Genet Genomics (2010) 283:365–380 DOI 10.1007/s00438-thought to play a Mol Genet Genomics (2010) 283:365–380 role

Schulze, Julia M.; Kane, Caroline M.; Ruiz-Manzano, Ana

2010-01-01T23:59:59.000Z

384

Ty1 integrase overexpression leads to integration of non-Ty1 DNA fragments into the genome of Saccharomyces cerevisiae  

E-Print Network [OSTI]

Mol Genet Genomics (2010) 284:231–242 DOI 10.1007/s00438-by ordered Mol Genet Genomics (2010) 284:231–242 proteolyticexperiments. Mol Genet Genomics (2010) 284:231–242 In RSY12

Friedl, Anna A.; Kiechle, Markus; Maxeiner, Horst G.; Schiestl, Robert H.; Eckardt-Schupp, Friederike

2010-01-01T23:59:59.000Z

385

A Fluid-Inclusion Investigation Of The Tongonan Geothermal Field...  

Open Energy Info (EERE)

observations indicate that early trapped fluids contained up to (approximate)2 mol% CO2 (now measured at <0.4 mol%). reservoir temperatures have decreased by...

386

Purification of soluble and active RaxH, a transmembrane histidine protein kinase from Xanthomonas oryzae pv. oryzae required for AvrXa21 activity.  

E-Print Network [OSTI]

of the plant pathogenic bacterium Xanthomonas campestris pv.oryzae pv. oryzae isolates in transgenic plants. Mol. Plant–Xanthomonas oryzae pv. oryzae. Mol. Plant–Microbe Interact.

Stolov, Avital; Valverde, Angel; Ronald, Pamela; Burdman, Saul

2007-01-01T23:59:59.000Z

387

E-Print Network 3.0 - abschlubericht fr das Sample Search Results  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

Sp Ges IIIB Mu IVA IIID IVC... IA En Bio IIIC IVD 10 - 12 Sp Soz EvR, Phi Geo Ges De, Phy Bi, Mu Soz Mu IVD Fr* IVA De, Phy IIIA Spo Source: Kurtz, Stefan - Center for...

388

Carbon dioxide, hydrographic, and chemical data obtained in the Central South Pacific Ocean (WOCE sections P17S and P16S) during the tunes-2-expedition of the R/V Thomas Washington, July--August 1991  

SciTech Connect (OSTI)

This data documentation discusses the procedures and methods used to measure total carbon dioxide (TCO{sub 2}), discrete partial pressure of TCO{sub 2} (pCO{sub 2}), and total alkalinity (TALK), during the Research Vessel (R/V) Thomas Washington TUNES Leg 2 Expedition in the central South Pacific Ocean. Conducted as part of the World Ocean Circulation Experiment (WOCE), the cruise began in Papeete, Tahiti, French Polynesia, on July 16, 1991, and returned to Papeete on August 25, 1991. WOCE Meridional Sections P17S along 135{degrees} W and P16S along 150{degrees} W were completed during the 40-day expedition. A total of 97 hydrographic stations were occupied. Hydrographic and chemical measurements made along WOCE Sections P17S and P16S included pressure, temperature, salinity, and oxygen measured by conductivity, temperature and depth sensor; bottle salinity; oxygen; phosphate; nitrate; nitrite; silicate; CFC-12; CFC- 11; TCO{sub 2}; TALK; and pCO{sub 2} measured at 20{degrees}C. The TCO{sub 2} concentration in 1000 seawater samples was determined with a coulometric analysis system, the pCO{sub 2} in 940 water samples was determined with an equilibrator/gas chromatograph system, while the TALK concentration in 139 samples was determined on shore at the laboratory of C. Goyet of Woods Hole Oceanographic Institution with an alkalinity titration system. In addition, 156 coulometric measurements for the Certified Reference Material (Batch {number_sign}6) were made and yielded a mean value of 2303.2 {plus_minus} 1.5 {mu}mol/kg. This mean value agrees within a standard deviation of the 2304.6 {plus_minus} 1.6 {mu}mol/kg (N=9) value determined with the manometer of C. D. Keeling at Scripps Institution of Oceanography (SIO). Replicate samples from 11 Niskin bottles at 4 stations were also collected for later shore-based reference analyses of TCO{sub 2} and TALK by vacuum extraction and manometry in the laboratory of C. D. Keeling of SIO.

NONE

1991-12-31T23:59:59.000Z

389

Thermodynamic and transport properties of single-crystal Yb{sub 14}MnSb{sub 11}  

SciTech Connect (OSTI)

Relatively large (up to 250 mg) single crystals of the intermetallic compound Yb{sub 14}MnSb{sub 11} have been prepared by a flux-growth technique. The results of thermodynamic and transport measurements of these samples are presented. The compound orders ferromagnetically at approximately T{sub C}=53{plus_minus}1K, with a magnetization consistent with the assignment Mn{sup 3+} (3d{sup 4}) and Yb{sup 2+} (4f{sup 14}). The Mn moments are local in nature, with the full effective and saturated moment of the Hund{close_quote}s rule spin-only ground state. The electrical resistivity has a metallic temperature dependence, with only a modest anisotropy. Room-temperature values of the resistivity are relatively high for an intermetallic compound: 1630{plus_minus}160 {mu}{Omega}cm and 1250{plus_minus}130 {mu}{Omega}cm for currents flowing approximately parallel and perpendicular to the {ital c} axis, respectively. There is a distinct loss of spin-disorder scattering in the resistivity at T{sub C}. From the heat capacity, a rough estimation of the magnetic entropy gives {Delta}S{sub M}{approx}12.1 J/mol K, the value in reasonable agreement with the expected {Delta}S{sub M}{approx}R ln 5 from the assignment of these moments. All of these data are consistent with a picture of Mn{sup 3+} local moments being coupled via conduction electrons. To this end, Yb{sub 14}MnSb{sub 11} appears to be analogous to local-moment rare-earth intermetallic compounds, and may point the way toward a class of 3d Kondo lattice compounds. {copyright} {ital 1999} {ital The American Physical Society}

Fisher, I.R.; Wiener, T.A.; Budko, S.L.; Canfield, P.C. [Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011 (United States)] [Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011 (United States); Chan, J.Y.; Kauzlarich, S.M. [Department of Chemistry, One Shields Avenue, University of California, Davis, California 95616 (United States)] [Department of Chemistry, One Shields Avenue, University of California, Davis, California 95616 (United States)

1999-06-01T23:59:59.000Z

390

Cell wide responses to low oxygen exposure in Desulfovibrio vulgaris Hildenborough  

E-Print Network [OSTI]

antioxidant systems of Helicobacter pylori. Mol Microbiolincluding Helicobacter pylori (56) and Bacteroides

2007-01-01T23:59:59.000Z

391

Heavy-electron behavior in single-crystal YbNi{sub 2}B{sub 2}C  

SciTech Connect (OSTI)

We have measured the magnetic susceptibility, specific heat, and electrical resistivity on single crystals of the intermetallic borocarbide YbNi{sub 2}B{sub 2}C. An enhanced linear contribution is observed in the specific heat with a Sommerfeld coefficient of 530 mJ/molK{sup 2}, indicative of a heavy-electron system with a Kondo temperature {approximately}10 K. The magnetic susceptibility, which is anisotropic and Curie-Weiss-like at high temperatures, is also consistent with our interpretation of a strongly correlated ground state at low temperatures and crystal-electric- field excitations at higher temperatures. At {ital T}=1.8 K, the Wilson ratio is determined to be 0.85 using the high-temperature effective moment. The resistivity shows a quadratic temperature dependence below 1.5 K with a {ital T}{sup 2} coefficient of 1.2 {mu}{Omega}cmK{sup {minus}2}. Unlike the other members of the series {ital R}Ni{sub 2}B{sub 2}C ({ital R}=Y, Gd{endash}Lu), YbNi{sub 2}B{sub 2}C does not order above our lowest measurement temperature of 0.34 K. The suppression of superconductivity in YbNi{sub 2}B{sub 2}C is consistent with a significantly enhanced hybridization between the conduction electrons and the 4{ital f} states. {copyright} {ital 1996 The American Physical Society.}

Yatskar, A.; Budraa, N.K.; Beyermann, W.P. [University of California, Riverside, California 92521 (United States)] [University of California, Riverside, California 92521 (United States); Canfield, P.C.; Budko, S.L. [Ames Laboratory and Iowa State University, Ames, Iowa 50011 (United States)] [Ames Laboratory and Iowa State University, Ames, Iowa 50011 (United States)

1996-08-01T23:59:59.000Z

392

Functional Representation for the Born-Oppenheimer Diagonal Correction and Born-Huang Adiabatic Potential Energy Surfaces for Isotopomers of H3  

SciTech Connect (OSTI)

Multireference configuration interaction (MRCI) calculations of the Born-Oppenheimer diagonal correction (BODC) for H3 were performed at 1397 symmetry-unique configurations using the Born-Handy approach; isotopic substitution leads to 4041 symmetry-unique configurations for the DH2 mass combination. These results were then fit to a functional form that permits calculation of the BODC for any combination of isotopes. Mean unsigned fitting errors on a test grid of configurations not included in the fitting process were 0.14, 0.12, and 0.65 cm?1 for the H3, DH2, and MuH2 isotopomers, respectively. This representation can be combined with any Born-Oppenheimer potential energy surface (PES) to yield Born-Huang (BH) PESs; herein we choose the CCI potential energy surface, the uncertainties of which (~0.01 kcal/mol) are much smaller than the magnitude of the BODC. FORTRAN routines to evaluate these BH surfaces are provided. Variational transition state theory calculations are presented comparing thermal rate constants for reactions on the BO and BH surfaces to provide an initial estimate of the significance of the diagonal correction for the dynamics.

Mielke, Steven L.; Schwenke, David; Schatz, George C.; Garrett, Bruce C.; Peterson, Kirk A.

2009-04-23T23:59:59.000Z

393

Spillover sites on a 19% Ni/Al sub 2 O sub 3 catalyst  

SciTech Connect (OSTI)

Two distinct methanation sites are clearly identified on a 19% Ni/Al{sub 2}O{sub 3} catalyst by temperature-programmed reaction (TPR) employing isotope labeling. The two sites, which are present after reduction at 975 K, are due to CO adsorption on Ni crystallites and CO and H spillover onto the Al{sub 2}O{sub 3} support. The concentration of sites on the support is 250 {mu}mol/G Al{sub 2}O{sub 3} (5 {times} 10{sup 13} molecules/cm{sup 2}), which is the same value measured for a 5.1% Ni/Al{sub 2}O{sub 3} catalyst and for a 1.0% Ru/Al{sub 2}O{sub 3} catalyst. Temperature-programmed desorption suggest that the CO and H on the Al{sub 2}O{sub 3} are in the form of a H-CO complex. The formation of this complex is an activated process, which is related to the activated adsorption of H{sub 2}. The H{sub 2} that adsorbs between 300 and 385 K is responsible for this spillover process onto the Al{sub 2}O{sub 3}. Isotope labeling and TPR were used to verify that a H-CO complex does not form on Ni/SiO{sub 2} catalysts. Carbon monoxide adsorption on Ni/SiO{sub 2} was not activated and only one methanation site was seen.

Sen, B.; Falconer, J.L. (Univ. of Colorado, Boulder (USA))

1989-06-01T23:59:59.000Z

394

New oxyfluoride glass with high fluorine content and laser patterning of nonlinear optical BaAlBO{sub 3}F{sub 2} single crystal line  

SciTech Connect (OSTI)

A new oxyfluoride glass of 50BaF{sub 2}-25Al{sub 2}O{sub 3}-25B{sub 2}O{sub 3} (mol. %) with a large fraction of fluorine, i.e., F/(F + O) = 0.4, was prepared using a conventional melt-quenching method in order to synthesize new glass-ceramics containing nonlinear optical oxyfluoride crystals. The refractive index at 632.8 nm and ultra-violet cutoff wavelength of the glass were 1.564 and {approx}200 nm, respectively. Eu{sup 3+} ions in the glass showed a high quantum yield of 88% in the photoluminescence spectrum in the visible region. BaAlBO{sub 3}F{sub 2} crystals (size: 50-100 nm) showing second harmonic generations were formed through the crystallization of the glass. Lines consisting of BaAlBO{sub 3}F{sub 2} crystals were patterned successfully on the glass surface by laser irradiations (Yb:YVO{sub 4} laser with a wavelength of 1080 nm, laser power of 1.1 W, scanning speed of 8 {mu}m/s). High resolution transmission electron microscope observations combined with a focused ion beam technique indicate that BaAlBO{sub 3}F{sub 2} crystals are highly oriented just like a single crystal. The present study proposes that the new oxyfluoride glass and glass-ceramics prepared have a high potential for optical device applications.

Shionozaki, K.; Honma, T.; Komatsu, T. [Department of Materials Science and Technology, Nagaoka University of Technology, 1603-1 Kamitomioka-cho, Nagaoka 940-2188 (Japan)

2012-11-01T23:59:59.000Z

395

Elevated sulfate reduction in metal-contaminated freshwater lake sediments  

SciTech Connect (OSTI)

Although sulfate-reducing prokaryotes have long been studied as agents of metals bioremediation, impacts of long-term metals exposure on biologically mediated sulfur cycling in natural systems remains poorly understood. The effects of long-term exposure to metal stress on the freshwater sulfur cycle were studied, with a focus on biologic sulfate reduction using a combination of microbial and chemical methods. To examine the effects after decades of adaptation time, a field-based experiment was conducted using multiple study sites in a natural system historically impacted by a nearby zinc smelter (Lake DePue, Illinois). Rates were highest at the most metals-contaminated sites (-35 {mu}mol/cm{sup 3}/day) and decreased with decreased pore water zinc and arsenic contamination levels, while other environmental characteristics (i.e., pH, nutrient concentrations and physical properties) showed little between-site variation. Correlations were established using an artificial neural network to evaluate potentially non-linear relationships between sulfate reduction rates (SRR) and measured environmental variables. SRR in Lake DePue were up to 50 times higher than rates previously reported for lake sediments and the chemical speciation of Zn was dominated by the presence of ZnS as shown by X-ray Absorption Spectroscopy (XAS). These results suggest that long-term metal stress of natural systems might alter the biogeochemical cycling of sulfur by contributing to higher rates of sulfate reduction.

Gough, H.L.; Dahl, A.L.; Tribou, E.; Noble, P.A.; Gaillard, J.-F.; Stahl, D.A. (UWASH); (NWU)

2009-01-06T23:59:59.000Z

396

A comparison of the alpha and gamma radiolysis of CMPO  

SciTech Connect (OSTI)

The radiation chemistry of CMPO has been investigated using a combination of irradiation and analytical techniques. The {alpha}-, and {gamma}-irradiation of CMPO resulted in identical degradation rates (G-value, in {mu}mol Gy{sup -1}) for both radiation types, despite the difference in their linear energy transfer (LET). Similarly, variations in {gamma}-ray dose rates did not affect the degradation rate of CMPO. The solvent extraction behavior was different for the two radiation types, however. Gamma-irradiation resulted in steadily increasing distribution ratios for both forward and stripping extractions, with respect to increasing absorbed radiation dose. This was true for samples irradiated as a neat organic solution, or irradiated in contact with the acidic aqueous phase. In contrast, {alpha}-irradiated samples showed a rapid drop in distribution ratios for forward and stripping extractions, followed by essentially constant distribution ratios at higher absorbed doses. These differences in extraction behavior are reconciled by mass spectrometric examination of CMPO decomposition products under the different irradiation sources. Irradiation by {gamma}-rays resulted in the rupture of phosphoryl-methylene bonds with the production of phosphinic acid products. These species are expected to be complexing agents for americium that would result in higher distribution ratios. Irradiation by {alpha}-sources appeared to favor rupture of carbamoyl-methylene bonds with the production of less deleterious acetamide products.

Bruce J. Mincher; Stephen P. Mezyk; Gary Groenewold; Gracy Elias

2011-06-01T23:59:59.000Z

397

Low-melting point heat transfer fluid  

DOE Patents [OSTI]

A low-melting point, heat transfer fluid made of a mixture of five inorganic salts including about 29.1-33.5 mol % LiNO.sub.3, 0-3.9 mol % NaNO.sub.3, 2.4-8.2 mol % KNO.sub.3, 18.6-19.9 mol % NaNO.sub.2, and 40-45.6 mol % KNO.sub.2. These compositions can have liquidus temperatures below 80.degree. C. for some compositions.

Cordaro, Joseph Gabriel (Oakland, CA); Bradshaw, Robert W. (Livermore, CA)

2010-11-09T23:59:59.000Z

398

PET 424304 2013 Exercises 1+2 of 4 12 Feb + 14 Feb 2013 1. ideal gas: s = s2-s1 = cpln(T2/T1) -R ln(p2/p1) (T << Tcrit; p << pcrit)  

E-Print Network [OSTI]

/mol = 31,25 mol/s s = - R· ln(1/20) = 24,9 J/(molK) x = ·T°· s = 31,25·293·24,9 = 228,1 kW 2. 1 kg Al/kmol with ni = 16,86 mol) Exergy decrease as a result of mixing: n·R·T°·xi·lnxi = -0,56 kJ/mol (can) - R· ln(p2/p1) (T

Zevenhoven, Ron

399

Study of collisons of supersymmetric top Quark in the channel stop anti-stop -> e+- mu-+ sneutrino anti-sneutrino b anti-b with the experience of D0 at the Tevatron. Callibration of the electromagnetic calorimeter at D0.  

SciTech Connect (OSTI)

Supersymmetry is one of the most natural extensions of the Standard Model. At low energy it may consist in the Minimal Supersymmetric Standard Model which is the framework chosen to perform the search of the stop with 350 pb{sup -1} of data collected by D0 during the RunIIa period of the TeVatron. They selected the events with an electron, a muon, missing transverse energy and non-isolated tracks, signature for the stop decay in 3-body ({bar t} {yields} bl{bar {nu}}). Since no significant excess of signal is seen, the results are interpreted in terms of limit on the stop production cross-sections, in such a way that they extend the existing exclusion region in the parameter space (m{sub {bar t}},m{sub {bar {nu}}}) up to stop masses of 168 (140) GeV for sneutrino masses of 50 (94) GeV. Finally because of the crucial role of the electromagnetic calorimeter, a fine calibration was performed using Z {yields} e{sup +}e{sup -} events, which improved significantly the energy resolution.

Mendes, Aurelien; /Marseille U., Luminy

2006-10-01T23:59:59.000Z

400

Acetylation and glycation of fibrinogen in vitro occur at specific lysine residues in a concentration dependent manner: A mass spectrometric and isotope labeling study  

SciTech Connect (OSTI)

Highlights: Black-Right-Pointing-Pointer Fibrinogen was incubated in vitro with glucose or aspirin. Black-Right-Pointing-Pointer Acetylations and glycations were found at twelve lysine sites by mass spectrometry. Black-Right-Pointing-Pointer The labeling by aspirin and glucose occurred dose-dependently. Black-Right-Pointing-Pointer No competition between glucose and aspirin for binding to fibrinogen was found. -- Abstract: Aspirin may exert part of its antithrombotic effects through platelet-independent mechanisms. Diabetes is a condition in which the beneficial effects of aspirin are less prominent or absent - a phenomenon called 'aspirin resistance'. We investigated whether acetylation and glycation occur at specific sites in fibrinogen and if competition between glucose and aspirin in binding to fibrinogen occurs. Our hypothesis was that such competition might be one explanation to 'aspirin resistance' in diabetes. After incubation of fibrinogen in vitro with aspirin (0.8 mM, 24 h) or glucose (100 mM, 5-10 days), we found 12 modified sites with mass spectrometric techniques. Acetylations in the {alpha}-chain: {alpha}K191, {alpha}K208, {alpha}K224, {alpha}K429, {alpha}K457, {alpha}K539, {alpha}K562, in the {beta}-chain: {beta}K233, and in the {gamma}-chain: {gamma}K170 and {gamma}K273. Glycations were found at {beta}K133 and {gamma}K75, alternatively {gamma}K85. Notably, the lysine 539 is a site involved in FXIII-mediated cross-linking of fibrin. With isotope labeling in vitro, using [{sup 14}C-acetyl]salicylic acid and [{sup 14}C]glucose, a labeling of 0.013-0.084 and 0.12-0.5 mol of acetylated and glycated adduct/mol fibrinogen, respectively, was found for clinically (12.9-100 {mu}M aspirin) and physiologically (2-8 mM glucose) relevant plasma concentrations. No competition between acetylation and glycation could be demonstrated. Thus, fibrinogen is acetylated at several lysine residues, some of which are involved in the cross-linking of fibrinogen. This may mechanistically explain why aspirin facilitates fibrin degradation. We find no support for the idea that glycation of fibrin(ogen) interferes with acetylation of fibrinogen.

Svensson, Jan, E-mail: jan.svensson@ki.se [Department of Molecular Medicine and Surgery, Karolinska Institutet, Karolinska University Hospital (Solna), SE-171 76 Stockholm (Sweden) [Department of Molecular Medicine and Surgery, Karolinska Institutet, Karolinska University Hospital (Solna), SE-171 76 Stockholm (Sweden); Karolinska Institutet, Department of Clinical Sciences, Danderyd Hospital, SE-182 88 Stockholm (Sweden); Bergman, Ann-Charlotte [Department of Molecular Medicine and Surgery, Karolinska Institutet, Karolinska University Hospital (Solna), SE-171 76 Stockholm (Sweden)] [Department of Molecular Medicine and Surgery, Karolinska Institutet, Karolinska University Hospital (Solna), SE-171 76 Stockholm (Sweden); Adamson, Ulf [Karolinska Institutet, Department of Clinical Sciences, Danderyd Hospital, SE-182 88 Stockholm (Sweden)] [Karolinska Institutet, Department of Clinical Sciences, Danderyd Hospital, SE-182 88 Stockholm (Sweden); Blombaeck, Margareta [Department of Molecular Medicine and Surgery, Karolinska Institutet, Karolinska University Hospital (Solna), SE-171 76 Stockholm (Sweden)] [Department of Molecular Medicine and Surgery, Karolinska Institutet, Karolinska University Hospital (Solna), SE-171 76 Stockholm (Sweden); Wallen, Hakan; Joerneskog, Gun [Karolinska Institutet, Department of Clinical Sciences, Danderyd Hospital, SE-182 88 Stockholm (Sweden)] [Karolinska Institutet, Department of Clinical Sciences, Danderyd Hospital, SE-182 88 Stockholm (Sweden)

2012-05-04T23:59:59.000Z

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


401

E-Print Network 3.0 - acute metabolic decompensation Sample Search...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

a nonreactive acute hepatitis panel, and an ammonia level of 71 molL (9-35 molL). His white... withdrawal and decompensated cirrhosis. He was treated with benzodiazepines,...

402

Fixation of CO2 by chrysotile in low-pressure dry and moist carbonation: Ex-situ and in-situ characterizations  

E-Print Network [OSTI]

. Emitted in large proportions, especially from (stationary) fossil-fuel based power plants, carbon dioxide­1200 °C), humidity (0­10 mol %) and CO2 partial pressure (20­67 mol %), thermal preconditioning

Long, Bernard

403

Nickel-Catalyzed Cross-Coupling of Phenol Derivatives and Total Synthesis of Welwitindolinone Natural Products  

E-Print Network [OSTI]

heterocyclic carbene ligand IPr in toluene at 120 °C (Scheme1.52 Ni(COD) 2 (20 mol%) IPr•HCl (40 mol%) OCH 3 HNR 2 NR 2heterocyclic carbene ligand IPr, allows for the coupling of

Quasdorf, Kyle

2012-01-01T23:59:59.000Z

404

Ex 9.8(a) The equilibrium constant for the reaction 2 C3H6(g) W C2H4(g) + C4H8(g) is found to fit the expression  

E-Print Network [OSTI]

coefficient for CaCl2 in a solution that is 0.020 mol kg-1 CaCl2(aq) and 0.030 mol kg-1 NaF(aq). #12;

Findley, Gary L.

405

E-Print Network 3.0 - acetyltransferase positive cells Sample...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

Hbo1. Mol. Cell. Biol. 26, 1098-1108. Iizuka, M... ). Nucleosomes positioned by ORC facilitate the initiation of DNA replication. Mol. Cell 7, 21-30. Lucas, I... Molecular...

406

Elucidation of XA21-mediated innate immunity.  

E-Print Network [OSTI]

oryzae pv. oryzae AvrXa21 and implications for plant innateoryzae pv. oryzae isolates in trans- genic plants. Mol Plantnas oryzae pv. oryzae in rice. Mol Plant 1: 446–458. Peng,

Park, Chang-Jin; Han, Sang-Wook; Chen, Xuewei; Ronald, Pamela C

2010-01-01T23:59:59.000Z

407

Engineering design of a hypobaric plant growth chamber  

E-Print Network [OSTI]

plants with the chamber in place and removed. With the chamber removed, PAR levels were recorded as 461 []mol m?² s?¹; inside the complete chamber the level decreased to 408 []mol m?² s?¹, a difference of 11.5%....

Purswell, Joseph Lawrence

2002-01-01T23:59:59.000Z

408

Bound state spectra of three-body muonic molecular ions  

E-Print Network [OSTI]

The results of highly accurate calculations are presented for all twenty-two known bound $S(L = 0)-, P(L = 1)-, D(L = 2)-$ and $F(L = 3)-$states in the six three-body muonic molecular ions $pp\\mu, pd\\mu, pt\\mu, dd\\mu, dt\\mu$ and $tt\\mu$. A number of bound state properties of these muonic molecular ions have been determined numerically to high accuracy. The dependence of the total energies of these muonic molecules upon particle masses is considered. We also discuss the current status of muon-catalysis of nuclear fusion reactions.

Alexei M. Frolov; David M. Wardlaw

2010-08-18T23:59:59.000Z

409

Bound state spectra of three-body muonic molecular ions  

E-Print Network [OSTI]

The results of highly accurate calculations are presented for all twenty-two known bound $S(L = 0)-, P(L = 1)-, D(L = 2)-$ and $F(L = 3)-$states in the six three-body muonic molecular ions $pp\\mu, pd\\mu, pt\\mu, dd\\mu, dt\\mu$ and $tt\\mu$. A number of bound state properties of these muonic molecular ions have been determined numerically to high accuracy. The dependence of the total energies of these muonic molecules upon particle masses is considered. We also discuss the current status of muon-catalysis of nuclear fusion reactions.

Frolov, Alexei M

2010-01-01T23:59:59.000Z

410

Harmonic oscillator in twisted Moyal plane: eigenvalue problem and relevant properties  

E-Print Network [OSTI]

The paper reports on a study of a harmonic oscillator (ho) in the twisted Moyal space, in a well defined matrix basis, generated by the vector fields $X_{a}=e_{a}^{\\mu}(x)\\partial_{\\mu}=(\\delta_{a}^{\\mu}+\\omega_{ab}^{\\mu}x^{b})\\partial_{\\mu}$, which induce a dynamical star product. The usual multiplication law can be hence reproduced in the $\\omega_{ab}^{\\mu}$ null limit. The star actions of creation and annihilation functions are explicitly computed. The ho states are infinitely degenerate with energies depending on the coordinate functions.

Mahouton Norbert Hounkonnou; Dine Ousmane Samary

2010-08-07T23:59:59.000Z

411

Carbon Nanotubes: Bearing Stress Like Never Before  

E-Print Network [OSTI]

energy effects that cause aggregation in the first place to attaching mol- ecules to the outside of carbon nanotubes

Limaye, Aditya

2013-01-01T23:59:59.000Z

412

Use of a promiscuous, constitutively-active bacterial enhancer-binding protein to define the Ï?54 (RpoN) regulon of Salmonella Typhimurium LT2  

E-Print Network [OSTI]

flagellar system of Helicobacter pylori. Mol Microbiol 2004,JW, Hoover TR: Helicobacter pylori FlgR is an enhancer-

2013-01-01T23:59:59.000Z

413

Use of a promiscuous, constitutively-active bacterial enhancer-binding protein to define the ?54 (RpoN) regulon of Salmonella Typhimurium LT2  

E-Print Network [OSTI]

flagellar system of Helicobacter pylori. Mol Microbiol 2004,JW, Hoover TR: Helicobacter pylori FlgR is an enhancer-

2013-01-01T23:59:59.000Z

414

On the Disposition of Graphite Containing TRISO Particles and the Aqueous Transport of Radionuclides via Heterogeneous Geological Formations  

E-Print Network [OSTI]

Nwptunium, Plutonium, Americium, and Technetium, Amsterdam,Database. Table 4.5 Americium Solubility (mol/kg) Calculated42 Americium

van den Akker, Bret Patrick

2012-01-01T23:59:59.000Z

415

Modeling of LNG Pool Spreading and Vaporization  

E-Print Network [OSTI]

..................................................................................... 15 Figure 5: 90 mol% Methane 10mol% Ethane mixture VLE phase envelope .................. 18 Figure 6: Boiling temperature and vapor composition of 90 mol% methane 10mol% ethane mixture... process of natural gas allows a 600 fold reduction in the volume of the gas being transported at ambient pressure. The resulting liquid which is mainly composed of methane presents some hazardous properties linked to its flammable nature and its...

Basha, Omar 1988-

2012-11-20T23:59:59.000Z

416

Biotransformation of 2,3,3,3-tetrafluoropropene (HFO-1234yf)  

SciTech Connect (OSTI)

2,3,3,3-Tetrafluoropropene (HFO-1234yf) is a non-ozone-depleting fluorocarbon replacement with a low global warming potential which has been developed as refrigerant. The biotransformation of HFO-1234yf was investigated after inhalation exposure. Male Sprague-Dawley rats were exposed to air containing 2000, 10,000, or 50,000 ppm HFO-1234yf for 6 h and male B6C3F1 mice were exposed to 50,000 ppm HFO-1234yf for 3.5 h in a dynamic exposure chamber (n = 5/concentration). After the end of the exposure, animals were individually housed in metabolic cages and urines were collected at 6 or 12-hour intervals for 48 h. For metabolite identification, urine samples were analyzed by {sup 1}H-coupled and decoupled {sup 19}F-NMR and by LC/MS-MS or GC/MS. Metabolites were identified by {sup 19}F-NMR chemical shifts, signal multiplicity, {sup 1}H-{sup 19}F coupling constants and by comparison with synthetic reference compounds. In all urine samples, the predominant metabolites were two diastereomers of N-acetyl-S-(3,3,3-trifluoro-2-hydroxy-propyl)-L-cysteine. In {sup 19}F-NMR, the signal intensity of these metabolites represented more than 85% (50,000 ppm) of total {sup 19}F related signals in the urine samples. Trifluoroacetic acid, 3,3,3-trifluorolactic acid, 3,3,3-trifluoro-1-hydroxyacetone, 3,3,3-trifluoroacetone and 3,3,3-trifluoro-1,2-dihydroxypropane were present as minor metabolites. Quantification of N-acetyl-S-(3,3,3-trifluoro-2-hydroxy-propyl)-L-cysteine by LC/MS-MS showed that most of this metabolite (90%) was excreted within 18 h after the end of exposure (t{sub 1/2} app. 6 h). In rats, the recovery of N-acetyl-S-(3,3,3-trifluoro-2-hydroxy-propyl)-L-cysteine excreted within 48 h in urine was determined as 0.30 {+-} 0.03, 0.63 {+-} 0.16, and 2.43 {+-} 0.86 {mu}mol at 2000, 10,000 and 50,000 ppm, respectively suggesting only a low extent (<< 1% of dose received) of biotransformation of HFO-1234yf. In mice, the recovery of this metabolite was 1.774 {+-} 0.4 {mu}mol. Metabolites identified after in vitro incubations of HFO-1234yf in liver microsomes from rat, rabbit, and human support the metabolic pathways of HFO-1234yf revealed in vivo. The obtained results suggest that HFO-1234yf is subjected to a typical biotransformation reaction for haloolefins, likely by a cytochrome P450 2E1-catalyzed formation of 2,3,3,3-tetrafluoroepoxypropane at low rates, followed by glutathione conjugation or hydrolytic ring opening.

Schuster, Paul; Bertermann, Ruediger [Institut fuer Toxikologie, Universitaet Wuerzburg, Versbacher Str. 9, 97078 Wuerzburg (Germany); Snow, Timothy A.; Han Xing [DuPont Haskell Global Centers for Health and Environmental Sciences, Newark, DE 19714 (United States); Rusch, George M. [Honeywell, P.O. Box 1057, Morristown, NJ 07962-1057 (United States); Jepson, Gary W. [DuPont Haskell Global Centers for Health and Environmental Sciences, Newark, DE 19714 (United States); Dekant, Wolfgang [Institut fuer Toxikologie, Universitaet Wuerzburg, Versbacher Str. 9, 97078 Wuerzburg (Germany)], E-mail: dekant@toxi.uni-wuerzburg.de

2008-12-01T23:59:59.000Z

417

QCD phase diagram at finite baryon and isospin chemical potentials  

SciTech Connect (OSTI)

The phase structure of two-flavor QCD is explored for thermal systems with finite baryon- and isospin-chemical potentials, {mu}{sub B} and {mu}{sub iso}, by using the Polyakov-loop extended Nambu-Jona-Lasinio (PNJL) model. The PNJL model with the scalar-type eight-quark interaction can reproduce lattice QCD data at not only {mu}{sub iso}={mu}{sub B}=0, but also {mu}{sub iso}>0 and {mu}{sub B}=0. In the {mu}{sub iso}-{mu}{sub B}-T space, where T is temperature, the critical endpoint of the chiral phase transition in the {mu}{sub B}-T plane at {mu}{sub iso}=0 moves to the tricritical point of the pion-superfluidity phase transition in the {mu}{sub iso}-T plane at {mu}{sub B}=0 as {mu}{sub iso} increases. The thermodynamics at small T is controlled by {radical}({sigma}{sup 2}+{pi}{sup 2}) defined by the chiral and pion condensates, {sigma} and {pi}.

Sasaki, Takahiro; Sakai, Yuji; Yahiro, Masanobu [Department of Physics, Graduate School of Sciences, Kyushu University, Fukuoka 812-8581 (Japan); Kouno, Hiroaki [Department of Physics, Saga University, Saga 840-8502 (Japan)

2010-12-01T23:59:59.000Z

418

S1_Thu_C57 6 International Conference on Multiphase Flow,  

E-Print Network [OSTI]

Langmuir constant (mol m-3 ) c concentration (mol m-3 ) D diffusion coefficient (m2 s-1 ) Di interfacial diffusion coefficient (m2 s-1 ) g gravitational constant (ms-1 ) j molecular flux (mol m-2 s-1 ) ji ­ 13, 2007 1 VOF-SIMULATION OF FLUID PARTICLES INFLUENCED BY SOLUBLE SURFACTANT Andreas Alke*, Dieter

Bothe, Dieter

419

Name:_____________________________ (Web Exercise)  

E-Print Network [OSTI]

Name:_____________________________ (Web Exercise) Model quality, validation exercise. You will need a web link to MolProbity (with Java), and the file 1JIRon1S83_Arg66_supr.kin download- ed from the kinemage.biochem.duke.edu BCH681 web site, or from Sakai. Part 1: MolProbity Go to the MolProbity web

Richardson, David

420

Plant lectins: the ties that bind in root symbiosis and plant defense  

E-Print Network [OSTI]

CA 92037, USA Mol Genet Genomics (2009) 282:1–15 Lis 2004;Mol Genet Genomics (2009) 282:1–15 DOI 10.1007/s00438-009-Etzler 1995). Mol Genet Genomics (2009) 282:1–15 ? Fig. 1

De Hoff, Peter L.; Brill, Laurence M.; Hirsch, Ann M.

2009-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


421

Characterization of the maintained vegetative phase deletions from diploid wheat and their effect on VRN2 and FT transcript levels  

E-Print Network [OSTI]

100:6263–6268 Mol Genet Genomics (2010) 283:223–232 Yan L,Mol Genet Genomics (2010) 283:223–232 DOI 10.1007/s00438-jdubcovsky@ucdavis.edu Mol Genet Genomics (2010) 283:223–232

Distelfeld, Assaf; Dubcovsky, Jorge

2010-01-01T23:59:59.000Z

422

Intestinal metabolism of lineoleic acid during its intestinal absorption in the  

E-Print Network [OSTI]

was de- tected at the peak of absorption of !4C linoleic acid infused intraduodenally in the rat (Bernard, we investigated to what extent the intra- duodenally infused 14C linoleate taken up from the portal/30/30 mol/ mol/ mol) emulsified with 1 ml bile and 0.5 ml Ringer's solution were infused intraduodenally

Boyer, Edmond

423

BioElectrochemically Assisted Microbial Reactor  

E-Print Network [OSTI]

microbial fuel cell-based technologies. Bruce Logan and John M. Regan Hydrogen Energy Center. Technol. (2005) Hydrogen recovery: Acetate: > 95% (3.8 mol/mol) achieved Glucose: > 90% (11 mol/m3 ) Above results: Cheng and Logan (unpublished) · · View Our Presentation From NHA Hydrogen

Lee, Dongwon

424

Self-powdering and nonlinear optical domain structures in ferroelastic beta'-Gd{sub 2}(MoO{sub 4}){sub 3} crystals formed in glass  

SciTech Connect (OSTI)

Ferroelastic beta'-Gd{sub 2}(MoO{sub 4}){sub 3}, (GMO), crystals are formed through the crystallization of 21.25Gd{sub 2}O{sub 3}-63.75MoO{sub 3}-15B{sub 2}O{sub 3} glass (mol%), and two scientific curious phenomena are observed. (1) GMO crystals formed in the crystallization break into small pieces with a triangular prism or pyramid shape having a length of 50-500 {mu}m spontaneously during the crystallizations in the inside of an electric furnace, not during the cooling in air after the crystallization. This phenomenon is called 'self-powdering phenomenon during crystallization' in this paper. (2) Each self-powdered GMO crystal grain shows a periodic domain structure with different refractive indices, and a spatially periodic second harmonic generation (SHG) depending on the domain structure is observed. It is proposed from polarized micro-Raman scattering spectra and the azimuthal dependence of second harmonic intensities that GMO crystals are oriented in each crystal grain and the orientation of (MoO{sub 4}){sup 2-} tetrahedra in GMO crystals changes periodically due to spontaneous strains in ferroelastic GMO crystals. - Graphical abstract: This figure shows the polarized optical photograph at room temperature for a particle (piece) obtained by a heat treatment of the glass at 590 deg. C for 2 h in an electric furnace in air. This particle was obtained through the self-powdering behavior in the crystallization of glass. The periodic domain structure is observed. Ferroelastic beta'-Gd{sub 2}(MoO{sub 4}){sub 3} crystals are formed in the particle, and second harmonic generations are detected, depending on the domain structure.

Tsukada, Y.; Honma, T. [Department of Materials Science and Technology, Nagaoka University of Technology, 1603-1 Kamitomioka-cho, Nagaoka 940-2188 (Japan); Komatsu, T., E-mail: komatsu@mst.nagaokaut.ac.j [Department of Materials Science and Technology, Nagaoka University of Technology, 1603-1 Kamitomioka-cho, Nagaoka 940-2188 (Japan)

2009-08-15T23:59:59.000Z

425

Deinhibition of cardiac Na/sup +/-K/sup +/-ATPase after exposure to exogenous phospholipase A/sub 2/  

SciTech Connect (OSTI)

After 2 h of exogenous phospholipase A/sub 2/ (PLA/sub 2/) exposure, membrane phospholipid decreased from 3.22 +/- 0.31 to 1.06 +/- 0.13 ..mu..mol/mg (33% of control). All classes of phospholipid, except sphingomyelin, were hydrolyzed, whereas total cholesterol content was unaffected. Increases in nonesterified fatty acids (NEFA) were reflected primarily in oleic (18:1), linoleic (18:2), and arachidonic (20:4). Na/sup +/-K/sup +/-adenosinetriphosphatase (ATPase) activity was inhibited to 29% of control by 2 h of PLA/sub 2/ treatment, and this inhibition was reversed (albeit, not completely after 5 min of PLA/sub 2/ treatment) by removal of the hydrolysis products with 0.1% bovine serum albumin (BSA). In contrast, the apparent binding capacity for (/sup 3/H)ouabain was not affected by PLA/sub 2/ treatment. Unmasking of latent (/sup 3/H)ouabain binding by alamethicin was utilized to estimate changes in the proportion of sealed vesicles present before and after PLA/sub 2/ treatment. PLA/sub 2/ treatment resulted in a time-dependent loss of sealed vesicles that paralleled the time course of phospholipid hydrolysis and was not reversed by washing with BSA. These studies demonstrate that cardiac Na/sup +/-K/sup +/-ATPase activity is inhibited by accumulation of endogenously produced lysophospholipids and NEFA. In contrast, loss of vesicle integrity may result from both accumulation of endogenously produced hydrolysis products and membrane phospholipid depletion.

Colvin, R.A.

1987-01-01T23:59:59.000Z

426

Expression of kidney injury molecule-1 (Kim-1) in relation to necrosis and apoptosis during the early stages of Cd-induced proximal tubule injury  

SciTech Connect (OSTI)

Cadmium (Cd) is a nephrotoxic industrial and environmental pollutant that causes a generalized dysfunction of the proximal tubule. Kim-1 is a transmembrane glycoprotein that is normally not detectable in non-injured kidney, but is up-regulated and shed into the urine during the early stages of Cd-induced proximal tubule injury. The objective of the present study was to examine the relationship between the Cd-induced increase in Kim-1 expression and the onset of necrotic and apoptotic cell death in the proximal tubule. Adult male Sprague-Dawley rats were treated with 0.6 mg (5.36 {mu}mol) Cd/kg, subcutaneously, 5 days per week for up to 12 weeks. Urine samples were analyzed for levels of Kim-1 and the enzymatic markers of cell death, lactate dehydrogenase (LDH) and alpha-glutathione-S-transferase ({alpha}-GST). In addition, necrotic cells were specifically labeled by perfusing the kidneys in situ with ethidium homodimer using a procedure that has been recently developed and validated in the Prozialeck laboratory. Cryosections of the kidneys were also processed for the immunofluorescent visualization of Kim-1 and the identification of apoptotic cells by TUNEL labeling. Results showed that significant levels of Kim-1 began to appear in the urine after 6 weeks of Cd treatment, whereas the levels of total protein, {alpha}-GST and LDH were not increased until 8-12 weeks. Results of immunofluorescence labeling studies showed that after 6 weeks and 12 weeks, Kim-1 was expressed in the epithelial cells of the proximal tubule, but that there was no increase in the number of necrotic cells, and only a modest increase in the number of apoptotic cells at 12 weeks. These results indicate that the Cd-induced increase in Kim-1 expression occurs before the onset of necrosis and at a point where there is only a modest level of apoptosis in the proximal tubule.

Prozialeck, Walter C. [Department of Pharmacology, Midwestern University, 555 31st Street, Downers Grove, IL 60515 (United States)], E-mail: wprozi@midwestern.edu; Edwards, Joshua R.; Lamar, Peter C. [Department of Pharmacology, Midwestern University, 555 31st Street, Downers Grove, IL 60515 (United States); Liu, Jie [Inorganic Carcinogenesis Section, Laboratory of Comparative Carcinogenesis, NCI at NIEHS, Research Triangle Park, NC 27709 (United States); Vaidya, Vishal S. [Renal Division, Department of Medicine, Brigham and Women's Hospital, Harvard Medical School, Boston, MA 02115 (United States); Bonventre, Joseph V. [Renal Division, Department of Medicine, Brigham and Women's Hospital, Harvard Medical School, Boston, MA 02115 (United States); Harvard-MIT Division of Health Sciences and Technology (United States)

2009-08-01T23:59:59.000Z

427

Enhanced durability of desulfurization sorbents for fluidized-bed applications  

SciTech Connect (OSTI)

To extend the operating temperature range and further improve the durability of fluidizable sorbents, zinc titanate, another leading regenerable sorbent, was selected for development in the later part of this project. A number of zinc titanate formulations were prepared in the 50 to 300 {mu}m range using granulation and spray drying methods. Important sorbent preparation variables investigated included zinc to titanium ratio, binder type, binder amount, and various chemical additives such as cobalt and molybdenum. A number of sorbents selected on the basis of screening tests were subjected to bench-scale testing for 10 cycles at high temperature, high pressure (HTHP) conditions using the reactor system designed and constructed during the base program. This reactor system is capable of operation either as a 2.0 in. or 3.0 in. I.D. bubbling bed and is rated up to 20 atm operation at 871{degrees}C. Bench-scale testing variables included sorbent type, temperature (550 to 750{degrees}C), gas type (KRW or Texaco gasifier gas), steam content of coal gas, and fluidizing gas velocity (6 to 15 cm/s). The sorbents prepared by spray drying showed poor performance in terms of attrition resistance and chemical reactivity. On the other hand, the granulation method proved to be very successful. For example, a highly attrition-resistant zinc titanate formulation, ZT-4, prepared by granulation exhibited virtually no zinc loss and demonstrated a constant high reactivity and sulfur capacity over 10 cycles, i.e., approximately a 60 percent capacity utilization, with Texaco gas at 750{degrees}C, 15 cm/s fluidizing velocity and 15 atm pressure. The commercial potential of the granulation method for zinc titanate manufacture was demonstrated by preparing two 80 lb batches of sorbent with zinc to titanium mol ratios of 0.8 and 1.5.

Gupta, R.P.; Gangwal, S.K.

1992-11-01T23:59:59.000Z

428

Enhanced durability of desulfurization sorbents for fluidized-bed applications  

SciTech Connect (OSTI)

To extend the operating temperature range and further improve the durability of fluidizable sorbents, zinc titanate, another leading regenerable sorbent, was selected for development in the later part of this project. A number of zinc titanate formulations were prepared in the 50 to 300 [mu]m range using granulation and spray drying methods. Important sorbent preparation variables investigated included zinc to titanium ratio, binder type, binder amount, and various chemical additives such as cobalt and molybdenum. A number of sorbents selected on the basis of screening tests were subjected to bench-scale testing for 10 cycles at high temperature, high pressure (HTHP) conditions using the reactor system designed and constructed during the base program. This reactor system is capable of operation either as a 2.0 in. or 3.0 in. I.D. bubbling bed and is rated up to 20 atm operation at 871[degrees]C. Bench-scale testing variables included sorbent type, temperature (550 to 750[degrees]C), gas type (KRW or Texaco gasifier gas), steam content of coal gas, and fluidizing gas velocity (6 to 15 cm/s). The sorbents prepared by spray drying showed poor performance in terms of attrition resistance and chemical reactivity. On the other hand, the granulation method proved to be very successful. For example, a highly attrition-resistant zinc titanate formulation, ZT-4, prepared by granulation exhibited virtually no zinc loss and demonstrated a constant high reactivity and sulfur capacity over 10 cycles, i.e., approximately a 60 percent capacity utilization, with Texaco gas at 750[degrees]C, 15 cm/s fluidizing velocity and 15 atm pressure. The commercial potential of the granulation method for zinc titanate manufacture was demonstrated by preparing two 80 lb batches of sorbent with zinc to titanium mol ratios of 0.8 and 1.5.

Gupta, R.P.; Gangwal, S.K.

1992-11-01T23:59:59.000Z

429

Thermoterrabacterium ferrireducens gen. nov., sp. nov., a thermophilic anaerobic dissimilatory Fe(III)-reducing bacterium from a continental hot spring  

SciTech Connect (OSTI)

A strain of a thermophilic, anaerobic, dissimilatory, Fe(III)-reducing bacterium, Thermoterrabacterium ferrireducens gen. nov., sp. nov. (type strain JW/AS-Y7{sup T}; DSM 11255), was isolated from hot springs in Yellowstone National Park and New Zealand. The gram-positive-staining cells occurred singly or in pairs as straight to slightly curved rods, 0.3 to 0.4 by 1.6 to 2.7 {mu}m, with rounded ends and exhibited a tumbling motility. Spores were not observed. The temperature range for growth was 50 to 74{degrees}C with an optimum at 65{degrees}C. The pH range for growth at 65{degrees}C was from 5.5 to 7.6, with an optimum at 6.0 to 6.2. The organism coupled the oxidation of glycerol to reduction of amorphous Fe(III) oxide or Fe(III) citrate as an electron acceptor. In the presence as well as in the absence of Fe(III) and in the presence of CO{sub 2}, glycerol was metabolized by incomplete oxidation to acetate as the only organic metabolic product; no H{sub 2} was produced during growth. The organism utilized glycerol, lactate, 1,2-propanediol, glycerate, pyruvate, glucose, fructose, mannose, and yeast extract as substrates. In the presence of Fe(III) the bacterium utilized molecular hydrogen. The organism reduced 9,10-anthraquinone-2,6-disulfonic acid, fumarate (to succinate), and thiosulfate (to elemental sulfur) but did not reduce MnO{sub 2}, nitrate, sulfate, sulfite, or elemental sulfur. The G+C content of the DNA was 41 mol% (as determined by high-performance liquid chromatography). The 16S ribosomal DNA sequence analysis placed the isolated strain as a member of a new genus within the gram-type positive Bacillus-Clostridium subphylum.

Slobodkin, A.; Wiegel, J. [Univ. of Georgia, Athens, GA (United States); Reysenbach, A.L. [Rutgers Univ., New Brunswick, NJ (United States)] [and others

1997-04-01T23:59:59.000Z

430

Design and development of a high-altitude, in-flight-deployable micro-UAV  

E-Print Network [OSTI]

A micro-UAV ([mu] UAV) system was developed to provide maximum endurance for a small atmospheric sensing payload. The system, composed of a ([mu] UAV) and protective case, folds and fits into a MJU-10/B flare cartridge ...

Tao, Tony S

2012-01-01T23:59:59.000Z

431

anomalous retroesophageal left: Topics by E-print Network  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

mu+mu-gamma, through a t-channel exchange of an additional charged triplet Higgs boson. The DM is leptophilic which is useful for explaining the non-observation of any...

432

analysis babar experiment: Topics by E-print Network  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

- Experiment (arXiv) Summary: We search for a new light non-Standard Model CP-odd Higgs boson, A0, decaying to tau+tau-, mu+mu-, and invisible in radiative...

433

Ceramic Mugs & Dishes Incandescent Light Bulbs  

E-Print Network [OSTI]

, MU East Rock Hall/19-B CELL PHONES - EYEGLASSES 654 Minnesota Street Room 208, copy room CVRI Helen. Zion Cancer Research Building N423 Parnassus Campus: eyeglasses "I" level, Optometry Store, MU West

Yamamoto, Keith

434

Managing internode data communications for an uninitialized process in a parallel computer  

DOE Patents [OSTI]

A parallel computer includes nodes, each having main memory and a messaging unit (MU). Each MU includes computer memory, which in turn includes, MU message buffers. Each MU message buffer is associated with an uninitialized process on the compute node. In the parallel computer, managing internode data communications for an uninitialized process includes: receiving, by an MU of a compute node, one or more data communications messages in an MU message buffer associated with an uninitialized process on the compute node; determining, by an application agent, that the MU message buffer associated with the uninitialized process is full prior to initialization of the uninitialized process; establishing, by the application agent, a temporary message buffer for the uninitialized process in main computer memory; and moving, by the application agent, data communications messages from the MU message buffer associated with the uninitialized process to the temporary message buffer in main computer memory.

Archer, Charles J; Blocksome, Michael A; Miller, Douglas R; Parker, Jeffrey J; Ratterman, Joseph D; Smith, Brian E

2014-05-20T23:59:59.000Z

435

Univerzita Karlova v Praze Matematickofyzik#ln# fakulta  

E-Print Network [OSTI]

#kladn#ch funkc#ch : : : : : : : : : : : : : : : : : : : 83 7 Implementace automatick#ho derivov#n# v syst#mu UFO 84 7.1 Stru#n# popis syst#mu UFO : : : : : : : : : : : : : : : : : : : : : 84 7.2 N#vrh implementace

Savicky, Petr

436

Lepton flavor violation decays with the fourth generation neutrino  

E-Print Network [OSTI]

We investigate the lepton flavor violation decays, $\\tau \\to \\mu\\gamma$, $\\tau \\to e\\gamma$ and $\\mu \\to e\\gamma$, in the framwork of a squential fourth generation model with a heavy fourth neutrino, $\

Wu-Jun Huo; Tai-Fu Feng

2002-03-22T23:59:59.000Z

437

Observation of the rare $B^0_s\\to?^+?^-$ decay from the combined analysis of CMS and LHCb data  

E-Print Network [OSTI]

A joint measurement is presented of the branching fractions $B^0_s\\to\\mu^+\\mu^-$ and $B^0\\to\\mu^+\\mu^-$ in proton-proton collisions at the LHC by the CMS and LHCb experiments. The data samples were collected in 2011 at a centre-of-mass energy of 7 TeV, and in 2012 at 8 TeV. The combined analysis produces the first observation of the $B^0_s\\to\\mu^+\\mu^-$ decay, with a statistical significance exceeding six standard deviations, and the best measurement of its branching fraction so far, and three standard deviation evidence for the $B^0\\to\\mu^+\\mu^-$ decay. The measurements are statistically compatible with SM predictions and impose stringent constraints on several theories beyond the SM.

The CMS; LHCb Collaborations; :; V. Khachatryan; A. M. Sirunyan; A. Tumasyan; W. Adam; T. Bergauer; M. Dragicevic; J. Erö; M. Friedl; R. Frühwirth; V. M. Ghete; C. Hartl; N. Hörmann; J. Hrubec; M. Jeitler; W. Kiesenhofer; V. Knünz; M. Krammer; I. Krätschmer; D. Liko; I. Mikulec; D. Rabady; B. Rahbaran; H. Rohringer; R. Schöfbeck; J. Strauss; W. Treberer-Treberspurg; W. Waltenberger; C. -E. Wulz; V. Mossolov; N. Shumeiko; J. Suarez Gonzalez; S. Alderweireldt; S. Bansal; T. Cornelis; E. A. De Wolf; X. Janssen; A. Knutsson; J. Lauwers; S. Luyckx; S. Ochesanu; R. Rougny; M. Van De Klundert; H. Van Haevermaet; P. Van Mechelen; N. Van Remortel; A. Van Spilbeeck; F. Blekman; S. Blyweert; J. D'Hondt; N. Daci; N. Heracleous; J. Keaveney; S. Lowette; M. Maes; A. Olbrechts; Q. Python; D. Strom; S. Tavernier; W. Van Doninck; P. Van Mulders; G. P. Van Onsem; I. Villella; C. Caillol; B. Clerbaux; G. De Lentdecker; D. Dobur; L. Favart; A. P. R. Gay; A. Grebenyuk; A. Léonard; A. Mohammadi; L. Perniè; A. Randle-conde; T. Reis; T. Seva; L. Thomas; C. Vander Velde; P. Vanlaer; J. Wang; F. Zenoni; V. Adler; K. Beernaert; L. Benucci; A. Cimmino; S. Costantini; S. Crucy; S. Dildick; A. Fagot; G. Garcia; J. Mccartin; A. A. Ocampo Rios; D. Ryckbosch; S. Salva Diblen; M. Sigamani; N. Strobbe; F. Thyssen; M. Tytgat; E. Yazgan; N. Zaganidis; S. Basegmez; C. Beluffi; G. Bruno; R. Castello; A. Caudron; L. Ceard; G. G. Da Silveira; C. Delaere; T. du Pree; D. Favart; L. Forthomme; A. Giammanco; J. Hollar; A. Jafari; P. Jez; M. Komm; V. Lemaitre; C. Nuttens; D. Pagano; L. Perrini; A. Pin; K. Piotrzkowski; A. Popov; L. Quertenmont; M. Selvaggi; M. Vidal Marono; J. M. Vizan Garcia; N. Beliy; T. Caebergs; E. Daubie; G. H. Hammad; W. L. Aldá Júnior; G. A. Alves; L. Brito; M. Correa Martins Junior; T. Dos Reis Martins; C. Mora Herrera; M. E. Pol; P. Rebello Teles; W. Carvalho; J. Chinellato; A. Custódio; E. M. Da Costa; D. De Jesus Damiao; C. De Oliveira Martins; S. Fonseca De Souza; H. Malbouisson; D. Matos Figueiredo; L. Mundim; H. Nogima; W. L. Prado Da Silva; J. Santaolalla; A. Santoro; A. Sznajder; E. J. Tonelli Manganote; A. Vilela Pereira; C. A. Bernardes; S. Dogra; T. R. Fernandez Perez Tomei; E. M. Gregores; P. G. Mercadante; S. F. Novaes; Sandra S. Padula; A. Aleksandrov; V. Genchev; R. Hadjiiska; P. Iaydjiev; A. Marinov; S. Piperov; M. Rodozov; G. Sultanov; M. Vutova; A. Dimitrov; I. Glushkov; L. Litov; B. Pavlov; P. Petkov; J. G. Bian; G. M. Chen; H. S. Chen; M. Chen; T. Cheng; R. Du; C. H. Jiang; R. Plestina; F. Romeo; J. Tao; Z. Wang; C. Asawatangtrakuldee; Y. Ban; Q. Li; S. Liu; Y. Mao; S. J. Qian; D. Wang; Z. Xu; W. Zou; C. Avila; A. Cabrera; L. F. Chaparro Sierra; C. Florez; J. P. Gomez; B. Gomez Moreno; J. C. Sanabria; N. Godinovic; D. Lelas; D. Polic; I. Puljak; Z. Antunovic; M. Kovac; V. Brigljevic; K. Kadija; J. Luetic; D. Mekterovic; L. Sudic; A. Attikis; G. Mavromanolakis; J. Mousa; C. Nicolaou; F. Ptochos; P. A. Razis; M. Bodlak; M. Finger; M. Finger Jr.; Y. Assran; A. Ellithi Kamel; M. A. Mahmoud; A. Radi; M. Kadastik; M. Murumaa; M. Raidal; A. Tiko; P. Eerola; G. Fedi; M. Voutilainen; J. Härkönen; V. Karimäki; R. Kinnunen; M. J. Kortelainen; T. Lampén; K. Lassila-Perini; S. Lehti; T. Lindén; P. Luukka; T. Mäenpää; T. Peltola; E. Tuominen; J. Tuominiemi; E. Tuovinen; L. Wendland; J. Talvitie; T. Tuuva; M. Besancon; F. Couderc; M. Dejardin; D. Denegri; B. Fabbro; J. L. Faure; C. Favaro; F. Ferri; S. Ganjour; A. Givernaud; P. Gras; G. Hamel de Monchenault; P. Jarry; E. Locci; J. Malcles; J. Rander; A. Rosowsky; M. Titov; S. Baffioni; F. Beaudette; P. Busson; C. Charlot; T. Dahms; M. Dalchenko; L. Dobrzynski; N. Filipovic; A. Florent; R. Granier de Cassagnac; L. Mastrolorenzo; P. Miné; C. Mironov; I. N. Naranjo; M. Nguyen; C. Ochando; G. Ortona; P. Paganini; S. Regnard; R. Salerno; J. B. Sauvan; Y. Sirois; C. Veelken; Y. Yilmaz; A. Zabi; J. -L. Agram; J. Andrea; A. Aubin; D. Bloch; J. -M. Brom; E. C. Chabert; C. Collard; E. Conte; J. -C. Fontaine; D. Gelé; U. Goerlach; C. Goetzmann; A. -C. Le Bihan; K. Skovpen; P. Van Hove; S. Gadrat; S. Beauceron; N. Beaupere; G. Boudoul; E. Bouvier; S. Brochet; C. A. Carrillo Montoya; J. Chasserat; R. Chierici; D. Contardo; P. Depasse; H. El Mamouni; J. Fan; J. Fay; S. Gascon; M. Gouzevitch; B. Ille; T. Kurca; M. Lethuillier; L. Mirabito; S. Perries; J. D. Ruiz Alvarez; D. Sabes; L. Sgandurra; V. Sordini; M. Vander Donckt; P. Verdier; S. Viret; H. Xiao; Z. Tsamalaidze; C. Autermann; S. Beranek; M. Bontenackels; M. Edelhoff; L. Feld; A. Heister; O. Hindrichs; K. Klein; A. Ostapchuk; F. Raupach; J. Sammet; S. Schael; J. F. Schulte; H. Weber; B. Wittmer; V. Zhukov; M. Ata; M. Brodski; E. Dietz-Laursonn; D. Duchardt; M. Erdmann; R. Fischer; A. Güth; T. Hebbeker; C. Heidemann; K. Hoepfner; D. Klingebiel

2014-11-17T23:59:59.000Z

438

Reconstruction of $5D$ Cosmological Models From Equation of State of Dark Energy  

E-Print Network [OSTI]

We consider a class of five-dimensional cosmological solutions which contains two arbitrary function $\\mu(t)$ and $\

Lixin Xu; Hongya Liu; Chengwu Zhang

2005-10-24T23:59:59.000Z

439

A FIRST ACCOUNT OF FRESHWATER POTAMOLEPID SPONGES (DEMOSPONGIAE, SPONGILLINA, POTAMOLEPIDAE) FROM THE MIDDLE  

E-Print Network [OSTI]

documented from European sites including the famous Messel oil shales (Mu¨ller et al., 1982; Richter

Wolfe, Alexander P.

440

A Survey of Residuated Lattices P. Jipsen and C. Tsinakis  

E-Print Network [OSTI]

for example [AF88], [Mu86], [Ha98] and [NPM99]. We conclude the introduction by summarizing the contents

Jipsen, Peter

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


441

vol. 174, no. 2 the american naturalist august 2009 Difference in Plumage Color Used in Species Recognition  

E-Print Network [OSTI]

this mu- tation in causing melanism. Birds from a second satellite island (Ugi) do not show the same

Uy, J. Albert C.

442

Homo-dimerization and ligand binding by the leucine-rich repeat domain at RHG1/RFS2 underlying resistance to two soybean pathogens  

E-Print Network [OSTI]

change in free energy between the wild type protein (Pekingfree energy differences between the 3 mu- tants and the wild

2013-01-01T23:59:59.000Z

443

The Transmembrane Domain of Vam3 Affects the Composition of cis-and trans-SNARE Complexes to  

E-Print Network [OSTI]

der Biopolymere, Technische Universita¨t Mu¨nchen, Weihenstephaner Berg 3, 85345 Freising, Germany

Dietrich, Lars

444

ORIGINAL PAPER Secondary structure and distribution of fusogenic LV-peptides  

E-Print Network [OSTI]

. Poschner Á M. W. Hofmann Á D. Langosch (&) Lehrstuhl Chemie der Biopolymere, Technische Universita¨t Mu

Gerwert, Klaus

445

Role of Collaborative Academic Partnerships in Surgical Training, Education, and Provision  

E-Print Network [OSTI]

members visited MU for didactics and collaborative research,are expected to give didactics for students and residents,

Riviello, Robert; Ozgediz, Doruk; Hsia, Renee Y.; Azzie, Georges; Newton, Mark; Tarpley, John

2010-01-01T23:59:59.000Z

446

$B_s \\to ?^+ ?^-$ and the upward-going muon flux from the WIMP annihilation in the sun or the earth  

E-Print Network [OSTI]

We consider the upward-going muon flux due to the WIMP annihilations in the cores of the sun and the earth, including the upper bound on the branching ratio for $B_s \\to \\mu^+ \\mu^-$ decay. We find that the constraint from $B_s \\to \\mu^+ \\mu^-$ is very strong in most parameter space, and exclude the supergravity parameter space regions where the expected upward-going muon fluxes are within the expected reach of AMANDA II.

Seungwon Baek; Yeong Gyun Kim; P. Ko

2005-06-13T23:59:59.000Z

447

Missouri's Future University of Missouri Extension 2011 ANNUAL REPORT  

E-Print Network [OSTI]

and natural resource managers by conducting research and offering demonstrations on best practices. MU ..................................................................................................5 Human Environmental

Taylor, Jerry

448

Cinfony - combining Open Source cheminformatics toolkits behind a common interface  

E-Print Network [OSTI]

on molecules Atom Wraps an atom instance of the underlying toolkit MoleculeData Provides dictionary-like access to the information contained in the tag fields in SDF and MOL2 files Outputfile Handles multimolecule output file formats Smarts Wraps the SMARTS... .calcfp() output = cdk.Outputfile("sdf", "similar mols.sdf") for mol in cdk.readfile("sdf", "input file.sdf"): fp = mol.calcfp() if fp | targetfp >= 0.7: output.write(mol) output.close() Alternatively, we could just have made a single change to the original script...

O'Boyle, Noel M; Hutchison, Geoffrey R

2008-12-03T23:59:59.000Z

449

Statistics of the Coulomb-blockade peak spacings of a silicon quantum dot Center for NanoScience and Sektion Physik, LMU Munchen, Geschwister-Scholl-Platz 1, D-80539 Munchen, Germany  

E-Print Network [OSTI]

Statistics of the Coulomb-blockade peak spacings of a silicon quantum dot F. Simmel Center for NanoScience-Magder* Center for NanoScience and Sektion Physik, LMU Mu¨nchen, Geschwister-Scholl-Platz 1, D-80539 Mu, Cambridge, Massachusetts 02139 J. P. Kotthaus Center for NanoScience and Sektion Physik, LMU Mu

Ludwig-Maximilians-Universität, München

450

Free Form of the Foldy-Wouthuysen Transformation in External Electromagnetic Fields  

E-Print Network [OSTI]

We derive the exact Foldy-Wouthuysen transformation for Dirac fermions in a time independent external electromagnetic field in the basis of the Ritus eigenfunctions, namely the eigenfunctions of the operator $(\\gamma \\cdot \\Pi)^2$, with $\\Pi^\\mu = p^\\mu - e A^\\mu$. In this basis, the transformation acquires a free form involving the dynamical quantum numbers induced by the field.

Gabriela Murguia; Alfredo Raya

2010-08-29T23:59:59.000Z

451

Search for the Higgs boson in H -> WW(*) decays in p(p)over-bar collisions at root(s)=1.96 TeV  

E-Print Network [OSTI]

We present a search for the standard model Higgs boson in H -> WW(*) decays with e(+)e(-), e(+/-)mu(-/+), and mu(+)mu(-) final states in p (p) over bar collisions at a center-of-mass-energy of root s = 1.96 TeV. The data, collected from April 2002...

Baringer, Philip S.; Bean, Alice; Christofek, L.; Coppage, Don; Gardner, J.; Hensel, Carsten; Jabeen, S.; Moulik, Tania; Wilson, Graham Wallace

2006-01-01T23:59:59.000Z

452

Mass spectrum of diquarks and mesons in the color--flavor locked phase of dense quark matter  

E-Print Network [OSTI]

The spectrum of meson and diquark excitations of dense quark matter is considered in the framework of the Nambu -- Jona-Lasinio model with three types of massless quarks in the presense of a quark number chemical potential $\\mu$. We investigate the effective action of meson- and diquark fields both at sufficiently large values of $\\mu>\\mu_c\\approx 330$ MeV, where the color--flavor locked (CFL) phase is realized, and in the chirally broken phase of quark matter ($\\mu\\mu_c$.

Ebert, D; Yudichev, V L

2007-01-01T23:59:59.000Z

453

Critical edition of the eleventh volume of 'Iqd al-jum?n f? t?r?kh ahl al-zam?n, with particular reference to the historical fragments from the lost book of Mu?ammad b. 'Abd al-Malik al-Hamadh?n? called: 'Unw?n al-siyar f? ma??sin ahl al-Bad? wa'l ?a?ar or Al-Ma'?rif al-muta'khkhira   

E-Print Network [OSTI]

This thesis is divided into four sections. The first chapter deals with Maml?k historiography and its major characteristics, alongside an examination of the life al' Ayn?'s, who was one of the most prominent historians of the period. Special...

Al-Hajeri, Shayea Abdulhadi Saif

2007-11-28T23:59:59.000Z

454

Blood lead levels and remediation of an abandoned smelter site  

SciTech Connect (OSTI)

Elevated soil lead levels were documented in a New Mexico community, with levels up to 24,800 ppm in a smelter slag pile, 20 or more feet from residences. The New Mexico Department of Health offered blood lead screening to residents of three geographic areas before and after an emergency cleanup by the US Environmental Protection Agency. Blood lead levels prior to the cleanup ranged from undetectable (< 5 {mu}g/dl) to 29 {mu}g/dl; after the cleanup, they ranged from undetectable to 10 {mu}g/dl. Significant reductions in mean blood lead levels after the cleanup were found for all three geographic areas: from 6.67 {mu}g/dl to 4 {mu}dl (smelter area), from 4.12 {mu}g/dl to 2.5 {mu}g/dl (town area), and from 5.5 {mu}g/dl to 2.5 {mu}g/dl (northeast area). In both years, the mean blood lead levels of individuals who lived near the smelter area were significantly higher than the levels for those living in town for those participating in both years of the study. Mean blood lead levels were significantly higher for smelter area participants who had a household member working at a lead battery plant (19.4 {mu}g/dl) compared to those residents who did not (5.83 {mu}g/dl).

Eidson, M. [New Mexico Dept. of Health, Santa Fe, NM (United States). Div. of Epidemiology, Evaluation, and Planning; Tollestrup, K. [Univ. of New Mexico School of Medicine, Albuquerque, NM (United States). Family and Community Medicine Dept.

1995-05-01T23:59:59.000Z

455

Thermostatistics of ?-deformed analog of Bose gas model  

E-Print Network [OSTI]

For the recently introduced \\mu-deformed analog of Bose gas model (\\mu-Bose gas model) we study some thermodynamical aspects. Namely, we calculate total number of particles and, from it, the deformed partition function, both involving dependence on the deformation parameter \\mu. Such dependence of thermodynamic functions on the \\mu-parameter is at the core of modification of Bose gas model and arises through the use of new techniques given by us, the \\mu-calculus, an alternative to the well-known q-calculus (Jackson derivative and integral). Necessary elements of \\mu-calculus are first presented. Then, for high temperatures we obtain virial expansion of the equation of state and find five first virial coefficients, as functions of \\mu. At the other end, for low temperatures the critical temperature of condensation T_c^(\\mu) depending on \\mu is found and compared with the usual T_c, and with the T_c^(p,q) of earlier studied p,q-Bose gas model. The internal energy, specific heat and the entropy of \\mu-Bose gas are also given, both for high and low temperatures. Features peculiar for the \\mu-Bose gas model are emphasized.

A. M. Gavrilik; I. I. Kachurik; A. P. Rebesh

2013-09-05T23:59:59.000Z

456

Measurement of the Formation Rate of Muonic Hydrogen Molecules  

E-Print Network [OSTI]

Background: The rate \\lambda_pp\\mu\\ characterizes the formation of pp\\mu\\ molecules in collisions of muonic p\\mu\\ atoms with hydrogen. In measurements of the basic weak muon capture reaction on the proton to determine the pseudoscalar coupling g_P, capture occurs from both atomic and molecular states. Thus knowledge of \\lambda_pp\\mu\\ is required for a correct interpretation of these experiments. Purpose: Recently the MuCap experiment has measured the capture rate \\Lambda_S from the singlet p\\mu\\ atom, employing a low density active target to suppress pp\\mu\\ formation (PRL 110, 12504 (2013)). Nevertheless, given the unprecedented precision of this experiment, the existing experimental knowledge in \\lambda_pp\\mu\\ had to be improved. Method: The MuCap experiment derived the weak capture rate from the muon disappearance rate in ultra-pure hydrogen. By doping the hydrogen with 20 ppm of argon, a competing process to pp\\mu\\ formation was introduced, which allowed the extraction of \\lambda_pp\\mu\\ from the observed t...

Andreev, V A; Carey, R M; Case, T A; Clayton, S M; Crowe, K M; Deutsch, J; Egger, J; Freedman, S J; Ganzha, V A; Gorringe, T; Gray, F E; Hertzog, D W; Hildebrandt, M; Kammel, P; Kiburg, B; Knaack, S; Kravtsov, P A; Krivshich, A G; Lauss, B; Lynch, K R; Maev, E M; Maev, O E; Mulhauser, F; Petitjean, C; Petrov, G E; Prieels, R; Schapkin, G N; Semenchuk, G G; Soroka, M A; Tishchenko, V; Vasilyev, A A; Vorobyov, A A; Vznuzdaev, M E; Winter, P

2015-01-01T23:59:59.000Z

457

Non-Equilibrium Beta Processes in Neutron Stars: A Relationship between the Net Reaction Rate and the Total Emissivity of Neutrinos  

E-Print Network [OSTI]

Several different processes could be changing the density in the core of a neutron star, leading to a departure from $\\beta$ equilibrium, quantified by the chemical potential difference $\\delta\\mu\\equiv\\mu_n-\\mu_p-\\mu_e$. The evolution of this quantity is coupled to that of the star's interior temperature $T$ by two functions that quantify the rate at which neutrino-emitting reactions proceed: the net reaction rate (difference between $\\beta$ decay and capture rates), $\\Gamma_{\\rm net}(T,\\delta\\mu)$, and the total emissivity (total energy emission rate in the form of neutrinos and antineutrinos), $\\epsilon_{\\rm tot}(T,\\delta\\mu)$. Here, we present a simple and general relationship between these variables, ${\\partial\\epsilon_{\\rm tot}/\\partial\\delta\\mu=3\\Gamma_{\\rm net}}$, and show that it holds even in the case of superfluid nucleons. This relation may simplify the numerical calculation of these quantities, including superfluid reduction factors.

Sergio Flores-Tulian; Andreas Reisenegger

2006-07-25T23:59:59.000Z

458

Unexpected formation of a trinuclear complex containing a Ta(IV)-Ta(IV) bond in the reactions of ButN=Ta(NMe2)3 with silanes  

SciTech Connect (OSTI)

A new trinuclear species containing a Ta(IV)-Ta(IV) bond, Ta{sub 3}({mu}-H)({mu}-NMe{sub 2})({mu}NBu{sup t}){sub 2}(NBu{sup t})(NMe{sub 2}){sub 5}, has been formed by reductive elimination of H{sub 2}. Ta{sub 2}H{sub 2}({mu}-NMe{sub 2}){sub 2}(NMe{sub 2}){sub 2}(NBu{sup t}){sub 2} has also been isolated. O{sub 2} oxidizes the Ta(IV)-Ta(IV) bond to yield Ta{sub 3}({mu}{sub 3}-O)(H)({mu}NBu{sup t})({mu}-NMe{sub 2}){sub 2}(NMe{sub 2}){sub 4}(NBu{sup t}){sub 2} under ligand exchange. Delocalization of d electrons is discussed.

Cheng, Shu-Jian [University of Tennessee, Knoxville (UTK); Dougan, Brenda A. [University of Tennessee, Knoxville (UTK); Steren, Carlos A. [University of Tennessee, Knoxville (UTK); Wang, Xiaoping [ORNL; Chen, Xue-Tai [University of Tennessee, Knoxville (UTK); Lin, Zhenyang [University of Tennessee, Knoxville (UTK); Xue, Zi-Ling [University of Tennessee, Knoxville (UTK)

2011-01-01T23:59:59.000Z

459

Problem Set 5: Chemistry 223 DUE: Friday, November 22, 2013  

E-Print Network [OSTI]

point is 327.4 C and the heat of fusion is 4770J/ mol. The heat capacity of liquid lead is CP(l)[J/K mol. The heat capacity of solid lead is: CP(s)[J/K mol] = 22. 13 + 0. 01172T + 0. 96 Ã? 105 T-2 . The melt- ing] = 32. 51 - 0. 00301T. a) Calculate the standard entropy of liquid lead at 500 C. b) Calculate the H

Ronis, David M.

460

E-Print Network 3.0 - alternaria alternata fungo Sample Search...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

phus... oxysporum and Alternaria alternata. Mol Plant-Microbe Interact 13:130-139 Armstrong CL, Chongo G, Gossen BD... in MAT loci of several loculoascomycete fungi,...

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


461

IN SITU CHEMICAL AND BIOLOGICAL TREATMENT OF TCE IN GROUNDWATER AT A LEGACY RAILROAD SITE  

E-Print Network [OSTI]

.0 1.5 2.0 2.5 3.0 -50 0 50 100 150 200 250 300 350 400 Ethene(mol/L) PCE,TCE,DCE,VC(mol/L) Days (Day 0 = July 18, 2013) MW-19 Molar Concentration PCE TCE Total DCE VC Total ethene #12;Results 0.00 0.20 0.40 0 300 350 400 Ethene(mol/L) PCE,TCE,DCE,VC(mol/L) Days (Day 0 = July 15, 2013) MW-26 Molar Concentration

Illinois at Urbana-Champaign, University of

462

The Ascomycete Verticillium longisporum Is a Hybrid and a Plant Pathogen with an Expanded Host Range  

E-Print Network [OSTI]

of three new Neotyphodium endophyte species from grassesal. (2007) New Neotyphodium endophyte species from the grassamongst asexual fungal endophytes of grasses. Mol Ecol 13:

Subbarao, Krishna V

2011-01-01T23:59:59.000Z

463

E-Print Network 3.0 - alver jaan alver Sample Search Results  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

to mitochondria in chronologically old... cells (A.Y.S., Ashley Alvers, Jennifer Westcott, Michael Wood, Roy Ferraiuolo, Michelle Marraffini et al... to induce apoptosis. Mol....

464

E-Print Network 3.0 - alver lehte alver Sample Search Results  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

to mitochondria in chronologically old... cells (A.Y.S., Ashley Alvers, Jennifer Westcott, Michael Wood, Roy Ferraiuolo, Michelle Marraffini et al... to induce apoptosis. Mol....

465

Comparative genomics of citric-acid producing Aspergillus niger ATCC 1015 versus enzyme-producing CBS 513.88  

E-Print Network [OSTI]

expression  profiles.   Mol.   Genet.   Genomics  279: Comparative genomics of citric-acid producing Aspergillus2006.  Aspergillus niger genomics: past, present and into 

Grigoriev, Igor V.

2011-01-01T23:59:59.000Z

466

E-Print Network 3.0 - active urea transport Sample Search Results  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

Reconstitution of the UreaNaCl-Washed PSII Membranes... with Various MSPs oxygen evolving activity sample bound MSP (%) mol of O2 (mg of ... Source: Tian, Weidong -...

467

http://bio.c.u-tokyo.ac.jp 15316 Tel: 03-5454-6641 Fax: 03-5454-4337 E-mail: mikeuchi@bio.c.u-tokyo.ac.jp  

E-Print Network [OSTI]

. Struct. Mol. Biol 16, 353-8 (2009); J. Am. Chem. Soc. 130, 7232-4 (2008); Nature 454, 358-61 (2008); Nat

Kawato, Suguru

468

Molecular Ecology of Pyrethroid Knockdown Resistance in Culex pipiens pallens Mosquitoes  

E-Print Network [OSTI]

with resistance to DDT and pyrethroid insecticides. Mol Genassociated with resistance to DDT and pyrethroids. InsectShort report: permethrin and DDT resistance in the malaria

2010-01-01T23:59:59.000Z

469

Structural Dynamics of the ActinMyosin Interface by Site-directed Spectroscopy  

E-Print Network [OSTI]

-mail address of the corresponding author: ddt@ddt.biochem.umn.edu doi:10.1016/j.jmb.2005.10.024 J. Mol. Biol

Thomas, David D.

470

E-Print Network 3.0 - atp induces ventricular Sample Search Results  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

Search Powered by Explorit Topic List Advanced Search Sample search results for: atp induces ventricular Page: << < 1 2 3 4 5 > >> 1 J Mol Cell Cardiol. Author manuscript...

471

Computational biology and high performance computing  

E-Print Network [OSTI]

Paper in Computational Biology The First Step Beyond theM . Glaeser, Mol. & Cell Biology, UCB and Life SciencesLBNL-44460 Computational Biology and High Performance

Shoichet, Brian

2011-01-01T23:59:59.000Z

472

PEGylated Nanoceria as Radical Scavenger with Tunable Redox Chemistry...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

non-PEGylated enzymes. Herein, we report our efforts to synthesize CNPs directly in polyethylene glycol (mol wt 600) solution and determine the effect of increasing concentration...

473

E-Print Network 3.0 - archaeon aeropyrum pernix Sample Search...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

James M Berger Summary: DB: Conformational changes induced by nucleotide binding in Cdc6ORC from Aeropyrum pernix. J Mol... origins in other archaeons, although not all origins...

474

Simultaneous cell growth and ethanol production from cellulose by an engineered yeast consortium displaying a functional mini-cellulosome  

E-Print Network [OSTI]

Cellulase, clostridia, and ethanol. Microbiol Mol Biol RevNext- generation cellulosic ethanol technologies and theirProduction of cellulosic ethanol in Saccharomyces cerevisiae

Goyal, Garima; Tsai, Shen-Long; Madan, Bhawna; DaSilva, Nancy A; Chen, Wilfred

2011-01-01T23:59:59.000Z

475

Analysis of Two Widespread Versions of a Bacterial Replicative DNA Polymerase  

E-Print Network [OSTI]

of studying multi-domain protein folding. Cell. Mol. Lifeenergy landscape of protein folding: a synthesis. Proteins,barrier mechanism in protein folding. Journal of Molecular

Guenther, Joel Michael

2010-01-01T23:59:59.000Z

476

PROPRITS DILECTRIQUES DE QUELQUES HALOGNURES D'HYDROGNE ET DE DEUTRIUM A L'TAT SOLIDE  

E-Print Network [OSTI]

structure mol6culaire est la plus simple, sont les halog6nures d'hydro- gene et de deuterium. On connait les

Paris-Sud XI, Université de

477

ELEVATED TEMPERATURE CORROSION BEHAVIOR OF IRON-BASE TERNARY ALLOYS THAT DEVELOP Cr2O3 AND/OR Al2O3 BARRIER SCALES  

E-Print Network [OSTI]

Resistant Alloy for Coal Gasification Service, LockheedI.M. , Table H Coal gasification atmosphere (mol fraction).development of "coal gasification" processes. large number

Nagarajan, V.

2011-01-01T23:59:59.000Z

478

E-Print Network 3.0 - antibiotic molecules bypassing Sample Search...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

Engineering, State University of New York at Buffalo Collection: Engineering 63 J. Mol. Biol. (1996) 262, 421436 RNA Sequence Determinants for Aminoglycoside Summary: - molecules...

479

E-Print Network 3.0 - anaerobic exercise performance Sample Search...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

words: anaerobic metabolism, critical swimming speed, sub- maximal swimming, exercise, energy... of lactate 1mol of glycosyl unit; Arthur et al. 1992; Moyes et al. 1993). During...

480

Copper Transporter 2 (CTR2) as a regulator of cisplatin accumulation and sensitivity  

E-Print Network [OSTI]

for the activation of tyrosinase." Hum Mol Genet 9(19):Cu incorporation into tyrosinase (Petris, Strausak et al.2000). Activation of tyrosinase can be measured by the

Blair, Brian G.

2009-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "mu mol mol-1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


481

Expression of sialic acids and other nonulosonic acids in Leptospira  

E-Print Network [OSTI]

PR, Brinkmann V, et al: Helicobacter pylori HP0518 affectsglycosylation process in Helicobacter pylori. Mol Microbiolacid pathway in Helicobacter pylori: synthesis from UDP-N-

Ricaldi N, Jessica; Matthias, Michael A; Vinetz, Joseph M; Lewis, Amanda L

2012-01-01T23:59:59.000Z

482

Analysis of a Ferric Uptake Regulator (Fur) Mutant of Desulfovibrio vulgaris Hildenborough  

E-Print Network [OSTI]

profiling of Helicobacter pylori Fur- and iron-regulateddissection of the Helicobacter pylori Fur regulatory circuitrepressed genes in Helicobacter pylori. Mol. Microbiol. 42:

Bender, Kelly S.

2010-01-01T23:59:59.000Z

483

Zita Martins Astrobiloga portuguesa do Imperial College de Londres "Estamos mais perto  

E-Print Network [OSTI]

-- que nós defendemos -- afirma que a vida tem origem nas moléculas orgânicas extra- terrestres. O que

Instituto de Sistemas e Robotica

484

E-Print Network 3.0 - atomic conformational transition Sample...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

; Biology and Medicine ; Engineering 17 J. Mol. Hiol. (1983) 170, 723-764 Protein Folding by Restrained Energy Minimization Summary: , and the native conformation is found...

485

Complejidad: Mecanica Estadistica y Ciencia No Lineal Angel Sanchez  

E-Print Network [OSTI]

, las mol´eculas, formadas por ´atomos, el tiempo atmosf´erico, formado por flujos de aire y agua, son

Sánchez, Angel "Anxo"

486

164 | VOL.2 NO.3 | MARCH 2005 | NATURE METHODS NEWS AND VIEWS  

E-Print Network [OSTI]

­820 (2002). 7. Kohout, T.A. & Lefkowitz, R.J. Mol. Pharmacol. 63, 9­18 (2003). 8. Sneddon, W.B. et al. J

Cai, Long

487

Li corrosion resistant glasses for headers in ambient temperature Li batteries  

DOE Patents [OSTI]

Glass compositions containing 10 to 50 mol% CaO, 10 to 50 mol% Al/sub 2/O/sub 3/, 30 to 60 mol% B/sub 2/O/sub 3/, and 0 to 30 mol% MgO are provided. These compositions are capable of forming a stable glass-to-metal seal possessing electrical insulating properties for use in a lithium battery. Also provided are lithium cells containing a stainless steel body and molybdenum center pin electrically insulated by means of a seal produced according to the invention.

Hellstrom, E.E.; Watkins, R.D.

1985-10-11T23:59:59.000Z

488

Fragment-Based QM/MM Method for Modeling Molecular Crystals and Clusters  

E-Print Network [OSTI]

Sublimation Enthalpies in kJ/mol for “2c” and “9a1” structures 115 xiii Chapter 1 Introduction Broad Overview of Computational Chemistry

Nanda, Kaushik

2013-01-01T23:59:59.000Z

489

Vrme-och strmningsteknik / Thermal and flow engineering Massverfring & separationsteknik /  

E-Print Network [OSTI]

av vatten och ammoniak (NH3) som innehåller xNH3 = 0.6·a·(c+d+e) mol-% och xH2O = (100-xNH3) mol-%, i jämvikt med en gas med sammansättningen yNH3 = 0.6·a·(c+d+e) mol-% och yH2O = (100-yNH3) mol-% vid vatten. 0°C 10°C 20°C 30°C 40°C 50°C p°H2O (kPa) 0.611 1.228 2.339 4.246 7.384 12.35 p°NH3 (kPa) 435

Zevenhoven, Ron

490

Genome sequence and rapid evolution of the rice pathogen Xanthomonas oryzae pv. oryzae PXO99A.  

E-Print Network [OSTI]

pathovar; pv. ), which demonstrate distinct host plantcampestris pv. malvacearum avr genes. Mol Plant Microbepv. vesicatoria, which is responsible for bacterial spot in tomato and pepper plants.

2008-01-01T23:59:59.000Z

491

An efficient method for visualization and growth of fluorescent Xanthomonas oryzae pv. oryzae in planta.  

E-Print Network [OSTI]

strains, plants and growth conditions Xanthomonas oryzae pv.Xanthomonas oryzae pv. oryzae. Mol Plant Microbe InteractOryzae sativa L. ) plants. X. oryzae pv. oryzae infection

Han, Sang-Wook; Park, Chang-Jin; Lee, Sang-Won; Ronald, Pamela C

2008-01-01T23:59:59.000Z

492

Biochemical and Functional Characterization of the GH3 Amino Acid-Conjugase PBS3 of Arabidopsis thaliana  

E-Print Network [OSTI]

with the plant pathogen Pseudomonas syringae pv. tomatosyringae pv. Phaseolicola. Mol Plant Microbe Interact 8,plants were treated with elicitors such as Pseudomonas syringae pv.

Okrent, Rachel Allegra

2010-01-01T23:59:59.000Z

493

Combining frequency and time domain approaches to systems with multiple spike train input and output  

E-Print Network [OSTI]

between neuronal spike trains. Prog Biophys Mol Biol Vapnikto systems with multiple spike train input and output D. R.Keywords Multiple spike trains · Neural coding · Maximum

Brillinger, D. R.; Lindsay, K. A.; Rosenberg, J. R.

2009-01-01T23:59:59.000Z

494

apical membrane vesicles: Topics by E-print Network  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

were incorporated at low levels (up to 5 mol %) in vesicles composed of 1 Smith, Bradley D. 2 TRPM7 facilitates cholinergic vesicle fusion with the plasma membrane...

495

E-Print Network 3.0 - austromenidia teleostei atherinidae Sample...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

and identity of Gobius lagocephalus (Teleostei: Gobiidae). Mol. Phylogenet. Evol. Pallas, P Source: Sparks, John S. - Department of Ichthyology, American Museum of Natural...

496

E-Print Network 3.0 - alepocephaliformes teleostei otocephala...  

Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

and identity of Gobius lagocephalus (Teleostei: Gobiidae). Mol. Phylogenet. Evol. Pallas, P Source: Sparks, John S. - Department of Ichthyology, American Museum of Natural...

497

Origin of periodic domain structure in Er{sup 3+}-doped beta'-(Sm,Gd){sub 2}(MoO{sub 4}){sub 3} crystal lines patterned by laser irradiations in glasses  

SciTech Connect (OSTI)

Er{sup 3+}-doped beta'-(Sm,Gd){sub 2}(MoO{sub 4}){sub 3} crystal lines are patterned on the surface of Er{sub 2}O{sub 3}-Gd{sub 2}O{sub 3}-Sm{sub 2}O{sub 3}-MoO{sub 3}-B{sub 2}O{sub 3} glasses by continuous-wave Yb:YVO{sub 4} laser irradiations (wavelength: 1080 nm, power: 1.3 W, scanning speeds: 5 {mu}m/s), and the origin of the periodicity of self-organized domain structures with high and low refractive index regions in crystal lines is examined from polarized optical microscope (POM) observations, micro-Raman scattering spectrum, and photoluminescence spectrum measurements. It is found that the periodicity of domain structures changes largely depending on Er{sub 2}O{sub 3} content, i.e., the length of high (bright color in POM observations) and low (dark color) refractive index regions increases with increasing Er{sub 2}O{sub 3} content and homogeneous crystal lines with no periodic domain structures are patterned in Er{sub 2}O{sub 3}-Sm{sub 2}O{sub 3}-MoO{sub 3}-B{sub 2}O{sub 3} glass with no Gd{sub 2}O{sub 3}. Considering that the degree of ferroelasticities in beta'-(Sm,Gd){sub 2}(MoO{sub 4}){sub 3} crystals decreases due to the incorporation of Er{sup 3+} ions, it is demonstrated that the origin of periodic domain structures in laser-patterned lines is due to spontaneous strains in ferroelastic beta'-(Sm,Gd){sub 2}(MoO{sub 4}){sub 3} crystals. - Graphical abstract: This figure shows the polarized optical photographs (top view) for the lines patterned by laser irradiations with the power of P=1.3 W and the scanning speed of S=5 {mu}m/s in xEr{sub 2}O{sub 3}-(18.25-x)Gd{sub 2}O{sub 3}-3Sm{sub 2}O{sub 3}-63.75MoO{sub 3}-15B{sub 2}O{sub 3} (mol%) glasses. This figure indicates that the periodicity of domain structures in beta'-(Sm,Gd){sub 2}(MoO{sub 4}){sub 3} crystal lines, i.e., the lengths of bright (high refractive index) and dark (low refractive index) color regions, changes depending on the amount of Er{sub 2}O{sub 3} addition. It is demonstrated that the origin of the periodicity of domain structures is due to spontaneous strains in ferroelastic beta'-(Sm,Gd){sub 2}(MoO{sub 4}){sub 3} crystals.

Suzuki, Futoshi; Honma, Tsuyoshi [Department of Materials Science and Technology, Nagaoka University of Technology, 1603-1 Kamitomioka-cho, Nagaoka 940-2188 (Japan); Komatsu, Takayuki, E-mail: komatsu@mst.nagaokaut.ac.j [Department of Materials Science and Technology, Nagaoka University of Technology, 1603-1 Kamitomioka-cho, Nagaoka 940-2188 (Japan)

2010-04-15T23:59:59.000Z

498

Enhanced Sensitivities for the Searches of Neutrino Magnetic Moments through Atomic Ionization  

SciTech Connect (OSTI)

A new detection channel on atomic ionization for possible neutrino electromagnetic interactions is identified and studied. Significant sensitivity enhancement is demonstrated when the energy transfer to the target is of the atomic-transition scale. The interaction cross section induced by neutrino magnetic moments ({mu}{sub {nu}}) is evaluated with the equivalent photon method. A new limit of {mu}{sub {nu}}({nu}e)<1.3x10{sup -11}{mu}{sub B} at 90% confidence level is derived by using current reactor neutrino data. Potential reaches for future experiments are explored. Experiments with sub-keV sensitivities can probe {mu}{sub {nu}} to 10{sup -13}{mu}{sub B}. Positive observations of {mu}{sub {nu}} in this range would imply that neutrinos are Majorana particles.

Wong, Henry T.; Li, Hau-Bin; Lin, Shin-Ted [Institute of Physics, Academia Sinica, Taipei 11529, Taiwan (China)

2010-08-06T23:59:59.000Z

499

Method for fabrication of crack-free ceramic dielectric films  

DOE Patents [OSTI]

The invention provides a process for forming crack-free dielectric films on a substrate. The process comprise the application of a dielectric precursor layer of a thickness from about 0.3 .mu.m to about 1.0 .mu.m to a substrate. The deposition is followed by low temperature heat pretreatment, prepyrolysis, pyrolysis and crystallization step for each layer. The deposition, heat pretreatment, prepyrolysis, pyrolysis and crystallization are repeated until the dielectric film forms an overall thickness of from about 1.5 .mu.m to about 20.0 .mu.m and providing a final crystallization treatment to form a thick dielectric film. Also provided was a thick crack-free dielectric film on a substrate, the dielectric forming a dense thick crack-free dielectric having an overall dielectric thickness of from about 1.5 .mu.m to about 20.0 .mu.m.

Ma, Beihai; Balachandran, Uthamalingam; Chao, Sheng; Liu, Shanshan; Narayanan, Manoj

2014-02-11T23:59:59.000Z

500

Magnetic moments of the ground-state $\\mathbf{J^P=(3/2)}^{+}$ baryon decuplet  

E-Print Network [OSTI]

The magnetic moment - a function of the electric charge form factor $F_{1}(q^{2})$ and the magnetic dipole form factor $F_{2}(q^{2})$ at zero four-momentum transfer $q^{2}$-of the ground-state $J^{P}=(3/2)^{+}$ baryon decuplet magnetic moments have been studied for many years with limited success. At present, only the magnetic moment of the $\\Omega^{-}$ has been accurately determined. We calculate nonperturbatively the magnetic moments of the \\emph{physical baryon decuplet $J^{P}=(3/2)^{+}$} members and in particular, we obtain $\\mu_{\\Delta^{++}}= (+3.67 \\pm 0.07) \\mu_{N}$, $\\mu_{\\Delta^{+}}= (+1.83 \\pm 0.04) \\mu_{N}$, $\\mu_{\\Delta^{0}}= (0) \\mu_{N}$, and the magnetic moments of their $U$-Spin partners in terms of $\\Omega^{-}$ magnetic moment data.

Milton Dean Slaughter

2011-07-18T23:59:59.000Z