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1

NREL: Energy Sciences - Kara Podkaminer  

NLE Websites -- All DOE Office Websites (Extended Search)

Kara Podkaminer Kara Podkaminer Postdoctoral Researcher Photo of Kara Podkaminer Phone: (303) 384-7970 Email: Kara.Podkaminer@nrel.gov At NREL Since: 2011 Kara Podkaminer received her Ph.D. in Engineering Sciences from the Thayer School of Engineering at Dartmouth College in 2011. For her dissertation work, she studied the thermophilic, anaerobic bacterium Thermoanaerobacterium saccharolyticum ALK2 and its application in a thermophliic SSF process. At NREL, Dr. Podkaminer is working on heterologous protein expression in T. reesei, looking to better understand the bottlenecks and increase protein production. This work will serve as the foundation for future expression of NREL's chimera proteins. Printable Version NREL is a national laboratory of the U.S. Department of Energy, Office of Energy Efficiency and Renewable Energy, operated by the Alliance for Sustainable Energy, LLC.

2

Deconstructing KK Monopoles  

E-Print Network (OSTI)

We describe a procedure for finding Kaluza-Klein monopole solutions in deconstructed four and five dimensional supersymmetric gauge theories. In the deconstruction of a four dimensional theory, the KK monopoles are finite-action solutions of the Euclidean equations of motion of the finite lattice spacing theory. The "lattice" KK monopoles can be viewed as constituents of continuum-limit four dimensional instantons. In the five dimensional case, the KK monopoles are static finite-energy stringlike configurations, wrapped and twisted around the compact direction, and can similarly be interpreted as constituents of five dimensional finite-energy gauge solitons. We discuss the quantum numbers and zero modes of the towers of deconstructed KK monopoles and their significance for understanding anomalies and nonperturbative effects in deconstruction.

Erich Poppitz

2003-06-20T23:59:59.000Z

3

Kk electronic A S | Open Energy Information  

Open Energy Info (EERE)

Kk electronic A S Jump to: navigation, search Name kk-electronic AS Place Herning, Denmark Zip DK-7400 Sector Wind energy Product Provides electronic wind turbine controllers....

4

Toyo Aluminium KK | Open Energy Information  

Open Energy Info (EERE)

Toyo Aluminium KK Toyo Aluminium KK Jump to: navigation, search Name Toyo Aluminium KK Place Japan Sector Solar Product Japan-based aluminium powder maker for solar cell electrodes. References Toyo Aluminium KK[1] LinkedIn Connections CrunchBase Profile No CrunchBase profile. Create one now! This article is a stub. You can help OpenEI by expanding it. Toyo Aluminium KK is a company located in Japan . References ↑ "Toyo Aluminium KK" Retrieved from "http://en.openei.org/w/index.php?title=Toyo_Aluminium_KK&oldid=352355" Categories: Clean Energy Organizations Companies Organizations Stubs What links here Related changes Special pages Printable version Permanent link Browse properties 429 Throttled (bot load) Error 429 Throttled (bot load) Throttled (bot load) Guru Meditation:

5

PPaAJ~f~-"'  

Office of Legacy Management (LM)

- PgOPO6bt OF MURD . COls'iRACT AT(lI&1)-140~ FIlli ml3 (31EXIUL CON6'E'JCTICB - PgOPO6bt OF MURD . COls'iRACT AT(lI&1)-140~ FIlli ml3 (31EXIUL CON6'E'JCTICB :i:, cbp, ., ,,. ._. SBMOL: "' PPaAJ~f~-"' :: "' ~ .' ., .~ : c !. .: ..:.. ..~ : ,. r. :;: A?TiL.C?@!, " ' If. D&do& . . . . . .' .' :: ,,,, A&g.?% Tigs mwonodum raquosts mat a cmtnot with (ho chwloal Cmetructlm Cerp.. bo jinqmrod la aw~danao with inforwtla hemlaaf4.r se4 fstb. Ski? mebere&dw proadsa a empfste reaord oizthe aego4Aa4lws leadia~ $e'the'prop~d OcDtrrrot and alro cPnstltutor the rvpotr or the stuf ma01 emrllaing~of Eomrs. I!. Lbdvh, P. Tobin, 5. K. B?-own and A. J. Beysr uhiah not m svvcrol oooasions dw& the ooureo of negotfatluim for the propoDd ec4erMt'~ ,., ,.. Rand8 are available under Budget Aotivity 2601. . .

6

Internet Engineering Task Force KK Ramakrishnan ...  

Science Conference Proceedings (OSTI)

... Engineering Task Force KK Ramakrishnan INTERNET DRAFT AT&T Labs Research draft-kksjf-ecn-00.txt Sally Floyd LBNL November 1997 ...

2009-08-19T23:59:59.000Z

7

AOCS Official Method Aj 4-89  

Science Conference Proceedings (OSTI)

Oil in Corn Germ AOCS Official Method Aj 4-89 Methods Methods and Analyses Analytical Chemistry Methods Downloads DEFINITION This method determines the amount of hexane soluble substances in corn germ that are e

8

AOCS Official Method Aj 5a-97  

Science Conference Proceedings (OSTI)

Determination of Fumonisins B1, B2, and B3 in Corn by Liquid Chromatography AOCS Official Method Aj 5a-97 Methods Methods and Analyses Analytical Chemistry Methods Downloads DEFINITION This method determines fum

9

AOCS Official Method Aj 5-93  

Science Conference Proceedings (OSTI)

Chromatography AOCS Official Method Aj 5-93 Methods Methods and Analyses Analytical Chemistry Methods Downloads DEFINITION This method determines fumonisin B 1 and fumonisin B 2 metabolites o

10

AOCS Official Method Aj 2-86  

Science Conference Proceedings (OSTI)

Zearalenone and a-Zearalenol in Corn AOCS Official Method Aj 2-86 Methods Methods and Analyses Analytical Chemistry Methods Downloads DEFINITION This method determines zearalenone and ?-zearalenol under the

11

AOCS Official Method Aj 1-86  

Science Conference Proceedings (OSTI)

Aflatoxins in Corn AOCS Official Method Aj 1-86 Methods Methods and Analyses Analytical Chemistry Methods Downloads DEFINITION This method detects total aflatoxins (B 1 + B 2 + G 1

12

AOCS Official Method Aj 3-87  

Science Conference Proceedings (OSTI)

Aflatoxins in Corn AOCS Official Method Aj 3-87 Methods Methods and Analyses Analytical Chemistry Methods Downloads DEFINITION This thin-layer chromatographic method determines aflatoxins B 1 , B 2...

13

AOCS Official Method Aj 6a-97  

Science Conference Proceedings (OSTI)

Determination of Aflatoxins B1, B2, and G1 in Corn by ELISA AOCS Official Method Aj 6a-97 Methods Methods and Analyses Analytical Chemistry Methods Downloads DEFINITION This method specifies a screening procedur

14

AOCS Official Method Aj 6-95  

Science Conference Proceedings (OSTI)

Total Aflatoxins (B1, B2, and G1) in Corn, Cottonseed, Peanuts, and Peanut Butter AOCS Official Method Aj 6-95 Methods Methods and Analyses Analytical Chemistry Methods Downloads DEFINITION This method specifies

15

Canadian Solar Japan KK | Open Energy Information  

Open Energy Info (EERE)

Japan KK Japan KK Jump to: navigation, search Name Canadian Solar Japan KK Place Shinjuku-ku, Tokyo, Japan Zip 160-0022 Sector Solar Product Tokyo-based subsidiary of Canadian Solar, producing solar equipment. Coordinates 35.7015°, 139.709244° Loading map... {"minzoom":false,"mappingservice":"googlemaps3","type":"ROADMAP","zoom":14,"types":["ROADMAP","SATELLITE","HYBRID","TERRAIN"],"geoservice":"google","maxzoom":false,"width":"600px","height":"350px","centre":false,"title":"","label":"","icon":"","visitedicon":"","lines":[],"polygons":[],"circles":[],"rectangles":[],"copycoords":false,"static":false,"wmsoverlay":"","layers":[],"controls":["pan","zoom","type","scale","streetview"],"zoomstyle":"DEFAULT","typestyle":"DEFAULT","autoinfowindows":false,"kml":[],"gkml":[],"fusiontables":[],"resizable":false,"tilt":0,"kmlrezoom":false,"poi":true,"imageoverlays":[],"markercluster":false,"searchmarkers":"","locations":[{"text":"","title":"","link":null,"lat":35.7015,"lon":139.709244,"alt":0,"address":"","icon":"","group":"","inlineLabel":"","visitedicon":""}]}

16

A.J. Rose Manufacturing Company | Open Energy Information  

Open Energy Info (EERE)

A.J. Rose Manufacturing Company A.J. Rose Manufacturing Company Jump to: navigation, search Name A.J. Rose Manufacturing Company Address 38000 Chester Road Place Avon, OH Zip 44011 Sector Renewable Energy Product Manufacturing Phone number 440-934-2859 Website http://www.ajrose.com Coordinates 41.468414°, -82.046652° Loading map... {"minzoom":false,"mappingservice":"googlemaps3","type":"ROADMAP","zoom":14,"types":["ROADMAP","SATELLITE","HYBRID","TERRAIN"],"geoservice":"google","maxzoom":false,"width":"600px","height":"350px","centre":false,"title":"","label":"","icon":"","visitedicon":"","lines":[],"polygons":[],"circles":[],"rectangles":[],"copycoords":false,"static":false,"wmsoverlay":"","layers":[],"controls":["pan","zoom","type","scale","streetview"],"zoomstyle":"DEFAULT","typestyle":"DEFAULT","autoinfowindows":false,"kml":[],"gkml":[],"fusiontables":[],"resizable":false,"tilt":0,"kmlrezoom":false,"poi":true,"imageoverlays":[],"markercluster":false,"searchmarkers":"","locations":[{"text":"","title":"","link":null,"lat":41.468414,"lon":-82.046652,"alt":0,"address":"","icon":"","group":"","inlineLabel":"","visitedicon":""}]}

17

Nippon Yusen KK NYK Link | Open Energy Information  

Open Energy Info (EERE)

Yusen KK NYK Link Yusen KK NYK Link Jump to: navigation, search Name Nippon Yusen KK (NYK Link) Place Tokyo, Tokyo, Japan Zip 100-0005 Sector Solar Product Logistics and shipping company moving to use solar power on its ships to reduce fuel useage. Coordinates 35.670479°, 139.740921° Loading map... {"minzoom":false,"mappingservice":"googlemaps3","type":"ROADMAP","zoom":14,"types":["ROADMAP","SATELLITE","HYBRID","TERRAIN"],"geoservice":"google","maxzoom":false,"width":"600px","height":"350px","centre":false,"title":"","label":"","icon":"","visitedicon":"","lines":[],"polygons":[],"circles":[],"rectangles":[],"copycoords":false,"static":false,"wmsoverlay":"","layers":[],"controls":["pan","zoom","type","scale","streetview"],"zoomstyle":"DEFAULT","typestyle":"DEFAULT","autoinfowindows":false,"kml":[],"gkml":[],"fusiontables":[],"resizable":false,"tilt":0,"kmlrezoom":false,"poi":true,"imageoverlays":[],"markercluster":false,"searchmarkers":"","locations":[{"text":"","title":"","link":null,"lat":35.670479,"lon":139.740921,"alt":0,"address":"","icon":"","group":"","inlineLabel":"","visitedicon":""}]}

18

Anaysis of high energy K+K- photoproduction on hydrogen  

E-Print Network (OSTI)

We have analyzed the K+K- photoproduction on hydrogen in the effective mass region around the mass of the phi(1020) meson. The interference of the S-wave contribution with the P-wave has been studied. Both scalar resonances f0(980) and a0(980) have been taken into account. We have obtained a good description of the available experimental data, in particular the mass distributions and the moments of the kaon angular distribution. Our calculations give values of the integrated S-wave total photoproduction cross section between 4 and 7 nb for the K+K- effective mass range around the phi(1020) mass and at the laboratory photon energy near 5 GeV. These numbers favor lower experimental estimates obtained at DESY.

L. Bibrzycki; L. Lesniak; A. P. Szczepaniak

2004-07-21T23:59:59.000Z

19

MENORANDUN TO: FILE CUI-IM. M. AJ  

Office of Legacy Management (LM)

-- -- MENORANDUN .~ \ TO: FILE CUI-IM. M. AJ w!EEG1 past: ~~~~_-------~----------- Current: ~~--------___--------~~~~~ Owner contacted a yez, ano; if yea, date contacted TYPE OF OPERATION -------__~------_ 5 Research & Development a Production scali testing a Pilot s~di.9 a sench Scale Process i Theoretical Studies Sample SC Plnalysis 0 Production a Di 5p0sal /storage LvPE-oE-cwIEncI @ Prime m Subcontractbr to lul,ll~' ,,krodt a Purchase Order a Facility Type 0 Manufacturing q University q Research Organization a Gavernment Sponsored Facility a ather -----------_--_______ a dther information (i.e., cost + fixed fee, unit price. time 84 matkial, etc) m(~O-ltlt70 - rod + Cmd Fe4 --_------------------------- OWNERSHIP: clEC/MED INVOLVEYEXT CIT SITE

20

S-P wave interference in the K+K- photoproduction on hydrogen  

E-Print Network (OSTI)

We have studied the partial wave interference effects to obtain a new information about the contribution of the S-wave to the cross section of the K+K- photoproduction on hydrogen. The K+K- photoproduction channel for the effective masses around 1 GeV is dominated by the phi(1020) resonance with only a small fraction of events coming from decays of scalar resonances f0(980) and a0(980). However, a careful analysis of angular distributions of the outgoing kaons shows that the S-wave adds an asymmetry to the angular distribution of kaons. A fairly precise estimation of the K+K- photoproduction cross section in the S-wave has been obtained.

L. Bibrzycki; L. Lesniak; A. P. Szczepaniak

2005-09-23T23:59:59.000Z

Note: This page contains sample records for the topic "aj podkaminer kk" 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

Measurement of the effective $B^0_s \\rightarrow K^+K^-$ lifetime  

E-Print Network (OSTI)

A measurement of the effective $B^0_s \\rightarrow K^+K^-$ lifetime is presented using approximately $37 pb^{-1}$ of data collected by LHCb during 2010. This quantity can be used to put constraints on contributions from processes beyond the Standard Model in the $B_s$ meson system and is determined by two complementary approaches as $\\tau_{B_s\\to K^+K^-} = 1.440 \\pm 0.096 (stat) \\pm 0.008 (syst) \\pm 0.003 (model) ps$.

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

2012-01-01T23:59:59.000Z

22

Measurement of D-D-bar mixing using the ratio of lifetimes for the decays D-->K- pi + and K+K-  

E-Print Network (OSTI)

We measure the rate of D0-D[over-bar] 0 mixing with the observable yCP=(?Kpi/?KK)-1, where ?KK and ?Kpi are, respectively, the mean lifetimes of CP-even D0-->K+K- and CP-mixed D0-->K-pi+ decays, using a data sample of ...

Fisher, Peter H.

23

The A.J. Goddard: Reconstruction and Material Culture of a Klondike Gold Rush Sternwheeler  

E-Print Network (OSTI)

The A.J. Goddard, a steamboat built for the Klondike Gold Rush of 1897-1898, wrecked in 1901 on Lake Laberge, Yukon Territory, where it lay undisturbed until its rediscovery in 2008 by the Yukon River Survey Project, directed by John Pollack. The complete and undisturbed nature of the wreck site, which is the only known site from this period to show such remarkable preservation, provides an unparalleled opportunity for studying the construction features of one of the Klondike steamboats and its associated material culture. The wreck of the A.J. Goddard is the only known surviving example of a small, prefabricated sternwheeler from the Yukon River's sternwheeler days. Due to the nature of its construction and building material, the A.J. Goddard represents a period of vast change in shipbuilding techniques, and is part of the fascinating juxtaposition between traditional wooden boats and a new, prefabricated industrial solution to boatbuilding. Work thus far has revealed that the A.J. Goddard possessed a simple design and construction, likely not one developed specifically for the Yukon River. It appears that the need to carry it over a mountain influenced its design more than the qualities of the Yukon River. Modifications were made over the course of its short career to make it more suitable, but its tragic end indicates that it was not a good choice for open-water navigation, though it admirably and successfully fulfilled its mission of serving throughout the gold rush. Though it was not ideally suited for the river and lakes environment where it was built, the quickness and ingenuity with which the vessel was constructed made it one of the few vessels, out of the thousands that set out for the Yukon in the summer of 1898, to actually make it to Dawson in time for the gold rush without being delayed by ice in the north, as so many were. Field seasons were conducted in 2009 and 2010 that focused on recording the boat's construction features and artifacts. Select artifacts were recovered for study and display in Whitehorse, Yukon Territory with the intention of creating an exhibit for the Yukon public.

Thomas, Lindsey Hall

2011-08-01T23:59:59.000Z

24

Advanced Security Infrastructures for Grid Education Prof R.O. Sinnott, A.J. Stell, Dr J.P. Watt, Prof D.W. Chadwick,  

E-Print Network (OSTI)

, Prof D.W. Chadwick, National e-Science Centre, Information Systems Security Group, University://www.edina.ac.uk/projects/ties/ties_23-9.pdf [9] R.O. Sinnott, A.J. Stell, D.W. Chadwick, O.Otenko, Experiences of Applying Advanced Grid

Kent, University of

25

Using NMR to study full intact wine bottles A.J. Weekley, P. Bruins, M. Sisto, and M.P. Augustine*  

E-Print Network (OSTI)

Using NMR to study full intact wine bottles A.J. Weekley, P. Bruins, M. Sisto, and M.P. Augustine 2002; revised 19 November 2002 Abstract A nuclear magnetic resonance (NMR) probe and spectrometer Sauvignons with high resolution 1 H NMR spectroscopy. Selected examples of full bottle 13 C NMR spectra

Augustine, Mathew P.

26

Measurements of indirect CP asymmetries in $D^0\\to K^-K^+$ and $D^0\\to\\pi^-\\pi^+$ decays  

E-Print Network (OSTI)

A study of indirect CP violation in $D^0$ mesons through the determination of the parameter $A_\\Gamma$ is presented using a data sample of $pp$ collisions, corresponding to an integrated luminosity of 1.0 fb$^{-1}$, collected with the LHCb detector and recorded at the centre-of-mass energy of 7 TeV at the LHC. The parameter $A_\\Gamma$ is the asymmetry of the effective lifetimes measured in decays of $D^0$ and $\\bar{D}^0$ mesons to the CP eigenstates $K^-K^+$ and $\\pi^-\\pi^+$. Fits to the data sample yield $A_\\Gamma(KK)=(-0.35\\pm0.62\\pm0.12)\\times 10^{-3}$ and $A_\\Gamma(\\pi\\pi)=(0.33\\pm1.06\\pm0.14)\\times 10^{-3}$, where the first uncertainties are statistical and the second systematic. The results represent the world's best measurements of these quantities. They show no difference in $A_\\Gamma$ between the two final states and no indication of CP violation.

Aaij, R; Adinolfi, M; Adrover, C; Affolder, A; Ajaltouni, Z; Albrecht, J; Alessio, F; Alexander, M; Ali, S; Alkhazov, G; Alvarez Cartelle, P; Alves Jr, A A; Amato, S; Amerio, S; Amhis, Y; Anderlini, L; Anderson, J; Andreassen, R; Andrews, J E; Appleby, R B; Aquines Gutierrez, O; Archilli, F; Artamonov, A; Artuso, M; Aslanides, E; Auriemma, G; Baalouch, M; Bachmann, S; Back, J J; Badalov, A; Baesso, C; Balagura, V; Baldini, W; Barlow, R J; Barschel, C; Barsuk, S; Barter, W; Bauer, Th; Bay, A; Beddow, J; Bedeschi, F; Bediaga, I; Belogurov, S; Belous, K; Belyaev, I; Ben-Haim, E; Bencivenni, G; Benson, S; Benton, J; Berezhnoy, A; Bernet, R; Bettler, M -O; van Beuzekom, M; Bien, A; Bifani, S; Bird, T; Bizzeti, A; Bjrnstad, P M; Blake, T; Blanc, F; Blouw, J; Blusk, S; Bocci, V; Bondar, A; Bondar, N; Bonivento, W; Borghi, S; Borgia, A; Bowcock, T J V; Bowen, E; Bozzi, C; Brambach, T; van den Brand, J; Bressieux, J; Brett, D; Britsch, M; Britton, T; Brook, N H; Brown, H; Bursche, A; Busetto, G; Buytaert, J; Cadeddu, S; Callot, O; Calvi, M; Calvo Gomez, M; Camboni, A; Campana, P; Campora Perez, D; Carbone, A; Carboni, G; Cardinale, R; Cardini, A; Carranza-Mejia, H; Carson, L; Carvalho Akiba, K; Casse, G; Castillo Garcia, L; Cattaneo, M; Cauet, Ch; Cenci, R; Charles, M; Charpentier, Ph; Cheung, S -F; Chiapolini, N; Chrzaszcz, M; Ciba, K; Cid Vidal, X; Ciezarek, G; Clarke, P E L; Clemencic, M; Cliff, H V; Closier, J; Coca, C; Coco, V; Cogan, J; Cogneras, E; Collins, P; Comerma-Montells, A; Contu, A; Cook, A; Coombes, M; Coquereau, S; Corti, G; Couturier, B; Cowan, G A; Craik, D C; Cruz Torres, M; Cunliffe, S; Currie, R; D'Ambrosio, C; David, P; David, P N Y; Davis, A; De Bonis, I; De Bruyn, K; De Capua, S; De Cian, M; De Miranda, J M; De Paula, L; De Silva, W; De Simone, P; Decamp, D; Deckenhoff, M; Del Buono, L; Dlage, N; Derkach, D; Deschamps, O; Dettori, F; Di Canto, A; Dijkstra, H; Dogaru, M; Donleavy, S; Dordei, F; Dosil Surez, A; Dossett, D; Dovbnya, A; Dupertuis, F; Durante, P; Dzhelyadin, R; Dziurda, A; Dzyuba, A; Easo, S; Egede, U; Egorychev, V; Eidelman, S; van Eijk, D; Eisenhardt, S; Eitschberger, U; Ekelhof, R; Eklund, L; El Rifai, I; Elsasser, Ch; Falabella, A; Frber, C; Farinelli, C; Farry, S; Ferguson, D; Fernandez Albor, V; Ferreira Rodrigues, F; Ferro-Luzzi, M; Filippov, S; Fiore, M; Fitzpatrick, C; Fontana, M; Fontanelli, F; Forty, R; Francisco, O; Frank, M; Frei, C; Frosini, M; Furfaro, E; Gallas Torreira, A; Galli, D; Gandelman, M; Gandini, P; Gao, Y; Garofoli, J; Garosi, P; Garra Tico, J; Garrido, L; Gaspar, C; Gauld, R; Gersabeck, E; Gersabeck, M; Gershon, T; Ghez, Ph; Gibson, V; Giubega, L; Gligorov, V V; Gbel, C; Golubkov, D; Golutvin, A; Gomes, A; Gorbounov, P; Gordon, H; Grabalosa Gndara, M; Graciani Diaz, R; Granado Cardoso, L A; Graugs, E; Graziani, G; Grecu, A; Greening, E; Gregson, S; Griffith, P; Grillo, L; Grnberg, O; Gui, B; Gushchin, E; Guz, Yu; Gys, T; Hadjivasiliou, C; Haefeli, G; Haen, C; Haines, S C; Hall, S; Hamilton, B; Hampson, T; Hansmann-Menzemer, S; Harnew, N; Harnew, S T; Harrison, J; Hartmann, T; He, J; Head, T; Heijne, V; Hennessy, K; Henrard, P; Hernando Morata, J A; van Herwijnen, E; He, M; Hicheur, A; Hicks, E; Hill, D; Hoballah, M; Hombach, C; Hulsbergen, W; Hunt, P; Huse, T; Hussain, N; Hutchcroft, D; Hynds, D; Iakovenko, V; Idzik, M; Ilten, P; Jacobsson, R; Jaeger, A; Jans, E; Jaton, P; Jawahery, A; Jing, F; John, M; Johnson, D; Jones, C R; Joram, C; Jost, B; Kaballo, M; Kandybei, S; Kanso, W; Karacson, M; Karbach, T M; Kenyon, I R; Ketel, T; Khanji, B; Kochebina, O; Komarov, I; Koopman, R F; Koppenburg, P; Korolev, M; Kozlinskiy, A; Kravchuk, L; Kreplin, K; Kreps, M; Krocker, G; Krokovny, P; Kruse, F; Kucharczyk, M; Kudryavtsev, V; Kurek, K; Kvaratskheliya, T; La Thi, V N; Lacarrere, D; Lafferty, G; Lai, A; Lambert, D; Lambert, R W; Lanciotti, E; Lanfranchi, G; Langenbruch, C; Latham, T; Lazzeroni, C; Le Gac, R; van Leerdam, J; Lees, J -P; Lefvre, R; Leflat, A; Lefranois, J; Leo, S; Leroy, O; Lesiak, T; Leverington, B; Li, Y; Li Gioi, L; Liles, M; Lindner, R; Linn, C; Liu, B; Liu, G; Lohn, S; Longstaff, I; Lopes, J H; Lopez-March, N; Lu, H; Lucchesi, D; Luisier, J; Luo, H; Lupton, O; Machefert, F; Machikhiliyan, I V; Maciuc, F; Maev, O; Malde, S; Manca, G; Mancinelli, G; Maratas, J; Marconi, U; Marino, P; Mrki, R; Marks, J; Martellotti, G; Martens, A; Martn Snchez, A; Martinelli, M; Martinez Santos, D; Martins Tostes, D; Martynov, A; Massafferri, A; Matev, R; Mathe, Z; Matteuzzi, C; Maurice, E; Mazurov, A; McCarthy, J; McNab, A; McNulty, R; McSkelly, B; Meadows, B; Meier, F; Meissner, M; Merk, M; Milanes, D A; Minard, M -N; Molina Rodriguez, J; Monteil, S; Moran, D; Morawski, P; Mord, A; Morello, M J; Mountain, R; Mous, I; Muheim, F; Mller, K; Muresan, R; Muryn, B; Muster, B; Naik, P; Nakada, T

2013-01-01T23:59:59.000Z

27

Detection of optical linear polarization in the SN2006aj/GRB060218 non-spherical expansion  

E-Print Network (OSTI)

We have performed optical polarimetric observations of the SN2006aj associated to the gamma-ray burst (GRB) of February 18, 2006, GRB060218 that provide information on its expansion geometry. The data were acquired in the R-band with the 0.7m telescope of Crimea, 2.5m Nordic Optical Telescope and the 2.2m of Calar Alto. We report the detection of linear polarization between 3 and 39 days after the gamma-ray event (t-t_0). This represents the first polarization detection of a Ic supernova (SN) associated to an X-ray flash. Our data exhibit a degree of linear polarization (P) around P~4% at t-t_0 ~ 3-5 days, followed by a constant polarization phase with P~1.4% at 13.7 < t-t_0 < 39 days. Our data suggest a decay in P, and more interestingly, show a position angle (\\theta) rotation of ~100 degrees comparing data taken before and after the R-band lightcurve peak. The reported polarization measurements can be explained by the evolution of an asymmetric SN expansion. We discuss on several ingredients that cou...

Gorosabel, J; Castro-Tirado, A J; Guziy, S; Larionova, L; Olmo, A D; Martnez, M A; Cepa, J; Cedres, B; De Postigo, A U; Jelinek, M; Bogdanov, O; Llorente, A

2006-01-01T23:59:59.000Z

28

Detection of optical linear polarization in the SN2006aj/XRF060218 non-spherical expansion  

E-Print Network (OSTI)

We have performed optical polarimetric observations of the SN2006aj associated to the X-ray flash (XRF) of February 18, 2006, XRF060218 that provide information on its expansion geometry. The data were acquired in the R-band with the 0.7m telescope of Crimea, 2.5m Nordic Optical Telescope and the 2.2m of Calar Alto. We report the detection of linear polarization between 3 and 39 days after the gamma-ray event (t-t_0). This represents the first polarization detection of a Ic supernova (SN) associated to an XRF. Our data exhibit a degree of linear polarization (P) around P~4% at t-t_0 ~ 3-5 days, followed by a constant polarization phase with P~1.4% at 13.7 < t-t_0 < 39 days. Our data suggest a decay in P, and more interestingly, show a position angle (\\theta) rotation of ~100 degrees comparing data taken before and after the R-band lightcurve peak. The reported polarization measurements can be explained by the evolution of an asymmetric SN expansion. We discuss on several ingredients that could account for the observed \\theta rotation.

J. Gorosabel; V. Larionov; A. J. Castro-Tirado; S. Guziy; L. Larionova; A. Del Olmo; M. A. Martinez; J. Cepa; B. Cedres; A. de Ugarte Postigo; M. Jelinek; O. Bogdanov; A. LLorente

2006-09-27T23:59:59.000Z

29

Photometric study of new southern SU UMa-type dwarf novae and candidates: V877 Ara, KK Tel and PU CMa  

E-Print Network (OSTI)

We photometrically observed three dwarf novae V877 Ara, KK Tel and PU CMa. We discovered undisputed presence of superhumps in V877 Ara and KK Tel, with mean periods of 0.08411(2) d and 0.08808(3) d, respectively. Both V877 Ara and KK Tel are confirmed to belong to long-period SU UMa-type dwarf novae. In V877 Ara, we found a large decrease of the superhump period (dot(P)/P = -14.5 +/- 2.1 x 10^(-5)). There is evidence that the period of KK Tel decreased at a similar or a more exceptional rate. Coupled with the past studies of superhump period changes, these findings suggest that a previously neglected diversity of phenomena is present in long-period SU UMa-type dwarf novae. The present discovery of a diversity in long-period SU UMa-type systems would become an additional step toward a full understanding the dwarf nova phenomenon. PU CMa is shown to be an excellent candidate for an SU UMa-type dwarf nova. We examined the outburst properties of these dwarf novae, and derived characteristic outburst recurrence times. Combined with the recently published measurement of the orbital period of PU CMa, we propose that PU CMa is the first object filling the gap between the extreme WZ Sge-type and ER UMa-type stars.

T. Kato; R. Santallo; G. Bolt; T. Richards; P. Nelson; B. Monard; M. Uemura; S. Kiyota; R. Stubbings; A. Pearce; T. Watanabe; P. Schmeer; H. Yamaoka

2002-10-31T23:59:59.000Z

30

Effect of low-dose, low-LET γ-radiation and BaP injection on pulmonary immunity in A/J mice  

NLE Websites -- All DOE Office Websites (Extended Search)

low-dose, low-LET γ-radiation and BaP injection on pulmonary immunity in A/J mice low-dose, low-LET γ-radiation and BaP injection on pulmonary immunity in A/J mice K. Gott, V. Gonzales, M. Makvandi, N. Kikendall, A. Monier, E. Maloy, C. Rietz, B. Scott and J. Wilder. Lovelace Respiratory Research Institute, Albuquerque, NM Introduction: Low-dose, low-linear-energy-transfer (LET) radiation (LDR; < 100 mGy) activates the immune response (Nowosielska et al., 2006), presumably via epigenetic pathways (Scott et al., 2009) and has been implicated as suppressing both alpha-radiation-induced and smoking-related lung cancer (Scott et al. 2009). One of the hypothesized adaptive-response mechanisms by which LDR does so is by activating immune cell function in the lung, which would then increase their anti-cancer surveillance

31

Omega-3 Oils: Applications in Functional FoodsChapter 12 Effect of Dietary Fish Protein and Fish Oil on Azoxymethane-induced Aberrant Crypt Foci in A/J Mice  

Science Conference Proceedings (OSTI)

Omega-3 Oils: Applications in Functional Foods Chapter 12 Effect of Dietary Fish Protein and Fish Oil on Azoxymethane-induced Aberrant Crypt Foci in A/J Mice Health Nutrition Biochemistry eChapters Health - Nutrition - Biochemistry AOCS

32

Professor KK Chawla  

Science Conference Proceedings (OSTI)

Sep 20, 2011 ... Shortly after receiving his Ph.D., Chawla traveled to Brazil to join the faculty of the Instituto Militar de Engenharia where he led the development...

33

Low-dose, low-LET γ-radiation alters carcinogen-induced splenic cytokine production and immune cell phenotype of A/J mice  

NLE Websites -- All DOE Office Websites (Extended Search)

dose, low-LET γ-radiation alters carcinogen-induced splenic cytokine production and immune cell dose, low-LET γ-radiation alters carcinogen-induced splenic cytokine production and immune cell phenotype of A/J mice. V. Gonzales, K. Gott, M. Makvandi, N. Kikendall, A. Monier, E. Maloy, C. Rietz, B. Scott and J. Wilder. Lovelace Respiratory Research Institute, Albuquerque, NM. Introduction: Low-dose, low-linear-energy-transfer (LET) radiation (LDR; < 100 mGy) activates the immune response, presumably via epigenetic pathways (Scott et al. 2009) and may lead to cancer suppression (Nowosielska et al. 2006). One of the mechanisms by which it might do so is by altering the cytokines produced after carcinogen and/or radiation exposure. Alternatively, LDR may activate

34

Measurement of D0-D0bar Mixing using the Ratio of D0->K-pi and K-K Lifetimes  

SciTech Connect

We measure the rate of D{sup 0}-{bar D}{sup 0} mixing with the observable y{sub CP} = ({tau}{sub K{pi}}/{tau}{sub KK}) - 1, where {tau}{sub KK} and {tau}{sub K{pi}} are respectively the mean lifetimes of CP-even D{sup 0} {yields} K{sup +}K{sup -} and CP-mixed D{sup 0} {yields} K{sup -}{pi}{sup +} decays, using a data sample of 384 fb{sup -1} collected by the BABAR detector at the SLAC PEP-II asymmetric-energy B Factory. From a sample of D{sup 0} and {bar D}{sup 0} decays where the initial flavor of the decaying meson is not determined, we obtain y{sub CP} = [1.12 {+-} 0.26(stat) {+-} 0.22(syst)]%, which excludes the no-mixing hypothesis at 3.3{sigma}, including both statistical and systematic uncertainties. This result is in good agreement with a previous BABAR measurement of y{sub CP} obtained from a sample of D*{sup +} {yields} D{sup 0}{pi}{sup +} events, where the D{sup 0} decays to K{sup -}{pi}{sup +}, K{sup +}K{sup -}, and {pi}{sup +}{pi}{sup -}, which is disjoint with the untagged D{sup 0} events used here. Combining the two results taking into account statistical and systematic uncertainties, where the systematic uncertainties are assumed to be 100% correlated, we find y{sub CP} = [1.16 {+-} 0.22(stat) {+-} 0.18(syst)]%, which excludes the no-mixing hypothesis at 4.1{sigma}.

Aubert, B.; Karyotakis, Y.; Lees, J.P.; Poireau, V.; Prencipe, E.; Prudent, X.; Tisserand, V.; /Annecy, LAPP; Tico, J.Garra; Grauges, E.; /Barcelona U.; Martinelli, M.; Palano, A.; Pappagallo, M.; /INFN, Bari /Bari U.; Eigen, G.; Stugu, B.; Sun, L.; /Bergen U.; Battaglia, M.; Brown, D.N.; Hooberman, B.; Kerth, L.T.; Kolomensky, Yu.G.; Lynch, G.; /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. /INFN, Genoa /INFN, Genoa /Genoa U. /Harvard U. /Heidelberg U. /Humboldt State U. /Imperial Coll., London /Iowa State U. /Iowa State U. /Johns Hopkins U. /Orsay, LAL /LLNL, Livermore /Liverpool U. /Queen Mary, U. of London /Royal Holloway, U. of London /Royal Holloway, U. of London /Louisville U. /Mainz U., Inst. Kernphys. /Manchester U. /Maryland U. /Massachusetts U., Amherst /MIT /McGill U. /INFN, Milan /Milan U. /INFN, Milan /INFN, Milan /Milan U. /Mississippi U. /Montreal U. /Mt. Holyoke Coll. /INFN, Naples /Naples U. /INFN, Naples /INFN, Naples /Naples U. /NIKHEF, Amsterdam /NIKHEF, Amsterdam /Notre Dame U. /Ohio State U. /Oregon U. /INFN, Padua /Padua U. /INFN, Padua /INFN, Padua /Padua U. /Paris U., VI-VII /Pennsylvania U. /INFN, Perugia /Perugia U. /INFN, Pisa /Pisa U. /INFN, Pisa /Pisa, Scuola Normale Superiore /INFN, Pisa /Pisa U. /INFN, Pisa /Princeton U. /INFN, Rome /INFN, Rome /Rome U. /INFN, Rome /INFN, Rome /Rome U. /INFN, Rome /INFN, Rome /Rome U. /INFN, Rome /INFN, Rome /Rome U. /INFN, Rome /Rostock U. /Rutherford /DAPNIA, Saclay /SLAC /South Carolina U. /Stanford U., Phys. Dept. /SUNY, Albany /Tel Aviv U. /Tennessee U. /Texas U. /Texas U., Dallas /INFN, Turin /Turin U. /INFN, Trieste /Trieste U. /Valencia U. /Victoria U. /Warwick U. /Wisconsin U., Madison

2009-10-17T23:59:59.000Z

35

S U B G A P A B S O R P T I O N IN CONJUGATED POLYMERS M. Sinclair*, C. H. Seager*, D. McBranch**, A.J. Heeger** f^fij^-^; Baker***  

NLE Websites -- All DOE Office Websites (Extended Search)

U U B G A P A B S O R P T I O N IN CONJUGATED POLYMERS M. Sinclair*, C. H. Seager*, D. McBranch**, A.J. Heeger** f^fij^-^; Baker*** *Sandia National Laboratories, Albuquerque, NM **University of California, Santa Barbara, CA SAND-90-3023C ***Bell Communications Research, Red Bank, NJ ^ , ^ , « , ^ ^ ' DE91 012655 A B S T R A C T ^ Along with x^^\ the magnitude of the optical absorption in the transparent window be- low the principal absorption edge is an important parameter which will ultimately determine the utihty of conjugated polymers in active integrated optical devices. With an aibsorptance sensitivity of < 10~^, Photothermal Deflection Spectroscopy (PDS) is ideal for determin- ing the absorption coefficients of thin films of "transpjo-ent" materials. We have used PDS

36

This Provisional PDF  

NLE Websites -- All DOE Office Websites (Extended Search)

thermophilic simultaneous saccharification and fermentation (tSSF) Biotechnology for Biofuels 2012, 5:43 doi:10.11861754-6834-5-43 Kara K Podkaminer (kara.podkaminer@nrel.gov)...

37

Session KK: Indium Nitride - Programmaster.org  

Science Conference Proceedings (OSTI)

Jun 25, 2010 ... PL spectra clearly demonstrate two peaks: at 0.678eV due to InN ... Kamimura1; Katsumi Kishino1; Akihiko Kikuchi1; 1Sophia University

38

Mouse Strain-Dependent Variations in Sensitivity to Induction of Gamma-H2AX Foci after Continuous Low Dose-Rate Irradiation: The Atm-/- vs Atm +/+ genotypes on Balb/c, 129S6, C57BL/6J, and A/J inbred strains  

NLE Websites -- All DOE Office Websites (Extended Search)

Mouse Strain-Dependent Variations in Sensitivity to Induction of Gamma-H2AX Foci Mouse Strain-Dependent Variations in Sensitivity to Induction of Gamma-H2AX Foci after Continuous Low Dose-Rate Irradiation: The Atm-/- vs Atm +/+ genotypes on Balb/c, 129S6, C57BL/6J, and A/J inbred strains. J.R.Brogan 1 , H. Nagasawa 1 , T.A Kato 1 , C.Fallgren 1 , T.Wade 1 . P.Genik 1 , J.B.Little 2 , J.S.Bedford 1 , and M.M.Weil 1 1 Department of Environmental and Radiological Health Sciences, Colorado State University, Fort Collins, CO 80523; 2 Department of Genetics and Complex Diseases, Harvard School of Public Health, Boston MA 02115 We have recently developed a 'low dose rate' gamma-H2AX assay that is sufficiently sensitive to distinguish differences in response for cells from normal Atm +/+ (mouse) or ATM+/+ (human) and the phenotypes associated with the corresponding

39

Diesel Engine idling test appendiz a-j  

NLE Websites -- All DOE Office Websites (Extended Search)

73432 Miles on Filter Months on Filter Bus 73433 Miles on Filter Months on Filter Start Test Date 2112003 1242002 Start Test Mileage 47612 0 0 198671 0 0 1 Filter Change Date...

40

KK4, Optical and Electrical Transport Properties of Nearly Intrinsic ...  

Science Conference Proceedings (OSTI)

We have also measured the electrical transport properties of single InN:Si .... F1, Applications of SiC Power Devices A Materials and Device Perspective.

Note: This page contains sample records for the topic "aj podkaminer kk" from the National Library of EnergyBeta (NLEBeta).
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they are not comprehensive nor are they the most current set.
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41

KK8, Aligned Assembly of Nanowire Arrays with Intrinsic Control  

Science Conference Proceedings (OSTI)

Selective conjugation of 1-D nanostructures only onto the lines within the array. 3 . ... CC1, In Situ High-Temperature Scanning Tunneling Microscopy Studies of Graphene ... Electroluminescent Devices with a Low Turn-on Voltage and High...

42

PPaauull KK.. BBaarrtteenn,, PPhh..DD.. PPrrooffeessssoorr ooff FFoorreesstt RReessoouurrcceess  

E-Print Network (OSTI)

, Petersham, Massachusetts 2001... Co-Director, Forest-to-Faucet Partnership (UMass-Amherst and U.S. Forest in the Northeastern U.S., National Association of State Foresters- Northeast Section, Harvard Forest, Petersham, MA Series, Petersham, MA, January 20, 2004 #12;

Schweik, Charles M.

43

The $\\epem\\to?^+?^-?^+?^-$, $K^+K^-?^+?^-$, and $K^+K^- K^+K^- $ Cross Sections at Center-of-Mass Energies 0.5--4.5 \\gev Measured with Initial-State Radiation  

E-Print Network (OSTI)

We study the process $e^+e^-\\to\\pi^+\\pi^-\\pi^+\\pi^-\\gamma$, with a hard photon radiated from the initial state. About 60,000 fully reconstructed events have been selected from 89 $fb^{-1}$ of BaBar data. The invariant mass of the hadronic final state defines the effective \\epem center-of-mass energy, so that these data can be compared with the corresponding direct $e^+e^-$ measurements. From the $4\\pi$-mass spectrum, the cross section for the process $e^+e^-\\to\\pi^+\\pi^-\\pi^+\\pi^-$ is measured for center-of-mass energies from 0.6 to 4.5 $GeV/c^2$. The uncertainty in the cross section measurement is typically 5%. We also measure the cross sections for the final states $K^+ K^- \\pi^+\\pi^-$ and $K^+ K^- K^+ K^-$. We observe the $J/\\psi$ in all three final states and measure the corresponding branching fractions. We search for X(3872) in $J/\\psi (\\to\\mu^+\\mu^-) \\pi^+\\pi^-$ and obtain an upper limit on the product of the $e^+e^-$ width of the X(3872) and the branching fraction for $X(3872) \\to J/\\psi\\pi^+\\pi^-$.

B. Aubert; BABAR Collaboration

2005-02-12T23:59:59.000Z

44

Wind energy mission analysis. Final report, appendices A--J. [USA  

DOE Green Energy (OSTI)

Information is presented concerning meteorological data and supporting analyses, gross energy consumption patterns and end-use analysis, analysis for industrial applications of wind energy conversion systems (WECS), analysis for residential applications of WECS, analysis for application of WECS to communities remote from utility grids, analysis for agricultural applications of WECS, regional evaluation of the economics of wind turbine generation to the U. S. electric utility district, impact of storage on WECS, financial analysis techniques, and system spacing.

Not Available

1977-02-18T23:59:59.000Z

45

Fluid Dynamics Dr. A.J. Hogg Example Sheet 2 October 2001  

E-Print Network (OSTI)

in a tank of still water of density w(> p). Calculate the depth of the lowest part of the solid object below/3 . Hydrostatics 6. Calculate the force (per unit width) and torque (per unit width) about the bottom of a lock gas has temperature, T, given by the ideal gas law T = P R , where R is a constant. It is adiabatic so

Hogg, Andrew

46

Article #11, May 23, 2006 AJ's Technical Tips: Technologies for Lighting in Rural Africa  

E-Print Network (OSTI)

- enriched light (PAM 101 light emitting diode, 650 nm) for 5 min, during which time fluorescence emission measurements, PS I-enriched light (PAM 102 FR light emitting diode, 730 nm) was added to the PS II light

Jacobson, Arne

47

Coloring kk-free intersection graphs of geometric objects in the plane  

Science Conference Proceedings (OSTI)

The intersection graph of a collection C of sets is a graph on the vertex set C, in which C1,C2 ? C are joined by an edge if and only if C1 ? C2 ... Keywords: chromatic number, intersection graph, quasi-planar, string graph, topological graph

Jacob Fox; Jnos Pach

2008-06-01T23:59:59.000Z

48

KK3, Growth Orientation Control of InN by Pulsed Excitation ...  

Science Conference Proceedings (OSTI)

DD3, A New Approach to Make ZnO-Cu2O Heterojunctions for Solar Cells ... E2, AlGaAs/GaAs/GaN Wafer Fused HBTs with Ar Implanted Extrinsic Collectors.

49

KK2, OMVPE Growth and Characterization of III-Nitride Nanorod LEDs  

Science Conference Proceedings (OSTI)

2A. Kikuchi, et. el., Proc. SPIE 6129, 612905(2006). 3P . Deb, et. el., Nano Lett. 5, 1847(2005). Proceedings Inclusion? Undecided...

50

Prof. K.K. Chawla Honorary Symposium on Fibers, Foams, and ...  

Science Conference Proceedings (OSTI)

Advances in the Development of Composite Porous Structures for Bone ... In-Situ X-Ray Studies of Ceramic Matrix Composites and Their Protective Coatings.

51

KK9, Nanostructure Decorated AlGaN/GaN HEMTs for Chemical ...  

Science Conference Proceedings (OSTI)

The high sensitivity of ZnO, towards the exposure to NH3, H2, O3, CO, NO2, and ethanol etc., makes it viable for gas sensing applications. Similarly, the same...

52

LATE NEWS: KK3, Non-Catalytic Synthesis of GaN Nanostructures ...  

Science Conference Proceedings (OSTI)

We have observed the synthesis of gallium nitride (GaN) nanopowders on boron ... as 400C. The synthesis process is based on the reaction between gallium atoms from the decomposition of gallium acetylacetonate and ammonia gas molecules. ... the crystal structure and growth mechanism of the grown nanostructures.

53

High Temperature Corrosion Research in Progress: 1997: Volume 1 (A-J), Volume 2 (K-U)  

Science Conference Proceedings (OSTI)

High-temperature oxidation and corrosion are important life-limiting factors for several critical components in thermal power systems. Research into many aspects of the problem is taking place in laboratories worldwide. This report, a survey of work in progress, updates and extends EPRI's 1994 report TR-104124, Volumes 1 and 2.

1998-08-11T23:59:59.000Z

54

On Programming Atomic Actions in Ada 95 A. Romanovsky, S.E. Mitchell and A.J. Wellings  

E-Print Network (OSTI)

as possible of control structure within a support package with a well-defined interface, · To make "client for the protected object is encapsulated within an Atomic_Support package: 1 with Ada.Exceptions; use Ada for Ada 95. We then present two implementa- tions of actions; first using Ada 95 packages to create

Newcastle upon Tyne, University of

55

Search for CP Violation using T-odd Correlations in D+ to K+K0spi+pi- and DS+ to K+K0spi+pi- Decays  

SciTech Connect

We search for CP violation in a sample of 20,000 Cabibbo-suppressed decays, D{sup +} {yields} K{sup +}K{sub S}{sup 0}{pi}{sup +}{pi}{sup -}, and 30,000 Cabibbo-favored decays, D{sub s}{sup +} {yields} K{sup +}K{sub S}{sup 0}{pi}{sup +}{pi}{sup -}. We use 520 fb{sup -1} of data recorded by the BABAR detector at the PEP-II asymmetric-energy e{sup +}e{sup -} collider operating at center of mass energies near 10.6 GeV. We search for CP violation in the difference between the T-odd asymmetries obtained using triple product correlations of the D+ (D{sub s}{sup +}) and D{sup -} (D{sub s}{sup -}) decays, respectively. The T violation parameter values obtained are {Alpha}{sub T} (D{sup +}) = (-12.0 {+-} 10.0{sub stat} {+-} 4.6{sub syst}) x 10{sup -3} and {Alpha}{sub T}(D{sub s}{sup +}) = (-13.6 {+-} 7.7{sub stat} {+-} 3.4{sub syst}) x 10{sup -3}, which are consistent with the Standard Model expectations.

Lees, J.P.; Poireau, V.; Tisserand, V.; /Annecy, LAPP; Garra Tico, J.; Grauges, E.; /Barcelona U., ECM; Martinelli, M.; /INFN, Bari /Bari U.; Milanes, D.A.; /INFN, Bari; Palano, A.; Pappagallo, M.; /INFN, Bari /Bari U.; Eigen, G.; Stugu, B.; Sun, L.; /Bergen U.; Brown, D.N.; Kerth, L.T.; Kolomensky, Yu.G.; Lynch, G.; /UC, Berkeley; Koch, H.; Schroeder, T.; /Ruhr U., Bochum; Asgeirsson, D.J.; Hearty, C.; Mattison, T.S.; /British Columbia U. /Brunel U. /Novosibirsk, IYF /UC, Irvine /UC, Riverside /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 /INFN, Ferrara /Ferrara U. /INFN, Ferrara /Frascati /INFN, Genoa /Genoa U. /INFN, Genoa /INFN, Genoa /Genoa U. /INFN, Genoa /Indian Inst. Tech., Guwahati /Harvard U. /Harvey Mudd Coll. /Heidelberg U. /Humboldt U., Berlin /Imperial Coll., London /Iowa State U. /Iowa State U. /Johns Hopkins U. /Paris U., VI-VII /LLNL, Livermore /Liverpool U. /Queen Mary, U. of London /Royal Holloway, U. of London /Royal Holloway, U. of London /Louisville U. /Mainz U., Inst. Kernphys. /Manchester U. /Maryland U. /Massachusetts U., Amherst /MIT /McGill U. /INFN, Milan /Milan U. /INFN, Milan /INFN, Milan /Milan U. /Mississippi U. /Montreal U. /INFN, Naples /Naples U. /NIKHEF, Amsterdam /NIKHEF, Amsterdam /Notre Dame U. /Ohio State U. /Oregon U. /INFN, Padua /Padua U. /INFN, Padua /INFN, Padua /Padua U. /Paris U., VI-VII /INFN, Perugia /Perugia U. /INFN, Pisa /Pisa U. /INFN, Pisa /Pisa, Scuola Normale Superiore /INFN, Pisa /Pisa U. /INFN, Pisa /INFN, Pisa /Pisa U. /INFN, Pisa /Princeton U. /INFN, Rome /INFN, Rome /Rome U. /INFN, Rome /INFN, Rome /Rome U. /INFN, Rome /Rostock U. /Rutherford /DAPNIA, Saclay /SLAC /South Carolina U. /Southern Methodist U. /Stanford U., Phys. Dept. /SUNY, Albany /Tel Aviv U. /Tennessee U. /Texas Nuclear Corp., Austin /Texas U. /INFN, Turin /Turin U. /INFN, Trieste /Trieste U. /Valencia U. /Victoria U. /Warwick U. /Wisconsin U., Madison

2011-08-22T23:59:59.000Z

56

Research and Engineering Division semiannual report. KK process development and technology, November 1, 1974--April 30, 1975  

SciTech Connect

Research and engineering activities with the goal of improving the performance of the plutonium processing and waste management programs being operated by the Atlantic Richfield Hanford Company are reported. (auth)

Fox, R.D. (ed.)

1975-08-01T23:59:59.000Z

57

RECOGNITION OF NOISY SPEECH USING CUMULANT-BASED LINEAR PREDICTION ANALYSIS K.K. Paliwal and M.M. Sondhi  

E-Print Network (OSTI)

]. The cumulant-based LF analysis method can suppress the effects of ad&he Gaussiannoise whether white or colored to deal with thus problem [2,3,4, 5,6,7]. In this paper, we propose to use LF parameters derived through-order cumulants in thuspaper. However, the results reported in this paper can be extended to higher

58

Yank: Enabling Green Data Centers to Pull the Plug Rahul Singh, David Irwin, Prashant Shenoy, and K.K. Ramakrishnan  

E-Print Network (OSTI)

.7-2.2% of electricity usage in the United States [16]. The rise in power usage has led data cen- ters to experiment connections to multiple electric grids, high-capacity UPSs, and backup genera- tors, others may connect to only a single grid and use cheaper lower-capacity UPSs, and still others may rely solely on renewables

Shenoy, Prashant

59

Image Enhancement and Understanding for Remote Visual Inspection of Aircraft Surface. Priyan Gunatilake * , M.W. Siegel ** , A.J. Jordan *,** , G. Podnar **  

E-Print Network (OSTI)

Security Services 1 Safecomputing.umich.edu How to Remove Hidden Data from Office 2007 Documents ESTIMATED to use the Document Inspector to identify both hidden and non-hidden data. You can choose to delete data. This page is derived from information on the Microsoft Office online Web site. Please see http://office

Siegel, Mel

60

Measurement of the difference of CP--violating asymmetries in $D^0 \\to K^+K^-$ and $D^0 \\to \\pi^+\\pi^-$ decays at CDF  

Science Conference Proceedings (OSTI)

We report a measurement of the difference (D/Acp) between time-integrated-violating asymmetries in D{sup 0} K{sup +}K{sup -} and D{sup 0} {pi}{sup +}{pi}{sup -} decays reconstructed in the full data set of proton-antiproton collisions collected by the Collider Detector at Fermilab, corresponding to 9.7 fb{sup -1} of integrated luminosity. The strong decay D*{sup +} D{sup 0}{pi}{sup +} is used to identify the charm meson at production as D{sup 0} or ['D]{sup 0}. We measure D/Acp = (-0.62 0.21 /stat 0.10 /syst)%, which differs from zero by 2.7 Gaussian standard deviations. This result supports similar evidence for violation in charm-quark obtained in proton-proton collisions.

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. /Fermilab; Annovi, A.; /Frascati; Antos, J.; /Comenius U.; Apollinari, G.; /Fermilab; Appel, J.A.; /Fermilab; Arisawa, T.; /Waseda U.; Artikov, A.; /Dubna, JINR /Texas A-M

2012-07-01T23:59:59.000Z

Note: This page contains sample records for the topic "aj podkaminer kk" 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

Measurement of CP--violating asymmetries in $D^0\\to\\pi^+\\pi^-$ and $D^0\\to K^+K^-$ decays at CDF  

SciTech Connect

We report on a measurement of CP-violating asymmetries (A{sub CP}) in the Cabibbo-suppressed D{sup 0} {yields} {pi}{sup +}{pi}{sup -} and D{sup 0} {yields} K{sup +}K{sup -} decays reconstructed in a data sample corresponding to 5.9 fb{sup -1} of integrated luminosity collected by the upgraded Collider Detector at Fermilab. We use the strong decay D*{sup +} {yields} D{sup 0}{pi}{sup +} to identify the flavor of the charmed meson at production and exploit CP-conserving strong c{bar c} pair-production in p{bar p} collisions. High-statistics samples of Cabibbo-favored D{sup 0} {yields} K{sup -}{pi}{sup +} decays with and without a D*{sup {+-}} tag are used to correct for instrumental effects and significantly reduce systematic uncertainties. We measure A{sub CP}(D{sup 0} {yields} {pi}{sup +}{pi}{sup -}) = (+0.22 {+-} 0.24(stat) {+-} 0.11 (syst))% and A{sub CP}(D{sup 0} {yields} K{sup +}K{sup -}) = (-0.24 {+-} 0.22 (stat) {+-} 0.09 (syst))%, in agreement with CP conservation. These are the most precise determinations from a single experiment to date. Under the assumption of negligible direct CP violation in D{sup 0} {yields} {pi}{sup +}{pi}{sup -} and D{sup 0} {yields} K{sup +}K{sup -} decays, the results provide an upper limit to the CP-violating asymmetry in D{sup 0} mixing, |A{sub CP}{sup ind}(D{sup 0})| < 0.13% at the 90% 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. /Fermilab; Annovi, A.; /Frascati; Antos, J.; /Comenius U.; Apollinari, G.; /Fermilab; Appel, J.A.; /Fermilab; Arisawa, T.; /Waseda U.; Artikov, A.; /Dubna, JINR /Texas A-M

2011-11-01T23:59:59.000Z

62

Physics potential of T2KK: An extension of the T2K neutrino oscillation experiment with a far detector in Korea  

E-Print Network (OSTI)

We study physics potential of placing a far detector in the east coast of Korea, where the off-axis beam from J-PARC at Tokai village for the T2K project has significant intensity at a few GeV range. In particular we examine the capability of determining the mass hierarchy pattern and the CP phase of the lepton-flavor-mixing matrix when a 100 kt water Cerenkov detector is placed at various locations in Korea for the off-axis beam (OAB) of 2.5 deg. and 3 deg. at the Super-Kamiokande site. The best results are found for a combination of 3 deg. OAB at SK (L = 295 km) and 0.5 deg. OAB at L = 1000km, where the mass hierarchy pattern can be determined at 3-\\sigma level for sin^2 2\\theta_{RCT} \\simgt 0.05 (0.06) when the hierarchy is normal (inverted), after 5 years of running (5 \\times 10^{21}POT). We also find that the leptonic CP phase, \\delta_{MNS}, can be constrained uniquely, without invoking anti-neutrino beams, as long as the mass hierarchy pattern is determined. Those results are obtained by assuming that the charged current quasi-elastic events can be separated from the other backgrounds with high efficiency, the neutrino energy can be reconstructed with a hundred MeV uncertainty, and the earth matter density along the baseline can be determined with 3% accuracy.

Kaoru Hagiwara; Naotoshi Okamura; Ken-ichi Senda

2006-07-23T23:59:59.000Z

63

Reconstruction of microbial and environmental conditions in an Australian hypersaline ecosystem from the mid-Pleistocene through the present  

E-Print Network (OSTI)

JE, in Lacustrine Petroleum Source Rocks, Fleet AJ, Kelts K,JK, in Lacustrine Petroleum Source Rocks, Fleet AJ, Kelts K,P, in Lacustrine Petroleum Source Rocks, Fleet AJ, Kelts K,

Jones, Claudia Meredith

2011-01-01T23:59:59.000Z

64

Reconstruction of microbial and environmental conditions in an Australian hypersaline ecosystem from the mid-Pleistocene through the present  

E-Print Network (OSTI)

of petroleum source rocks The American Association ofLacustrine Petroleum Source Rocks, Fleet AJ, Kelts K, TalbotLacustrine Petroleum Source Rocks, Fleet AJ, Kelts K, Talbot

Jones, Claudia Meredith

2011-01-01T23:59:59.000Z

65

Column basis reduction and decomposable knapsack problems  

E-Print Network (OSTI)

A:,j. ? cn(r +1)?k. (6.14). To get a contradiction, suppose pj = 0. Then, since pj is integral,. . A:,j. ? |aj|. = |pjM + rj|. ? M ? |rj|. (6.15). Hence. M ?. . A:,j. +|rj|.

66

8441.full.pdf  

NLE Websites -- All DOE Office Websites (Extended Search)

28 September 2012. 28 September 2012. 10.1128/AEM.02130-12. 2012, 78(23):8441. DOI: Appl. Environ. Microbiol. David A. Hogsett and Lee R. Lynd Kara K. Podkaminer, Adam M. Guss, Heather L. Trajano, through Targeted Gene Deletions Thermoanaerobacterium saccharolyticum Discovery of a New Endoxylanase in Characterization of Xylan Utilization and http://aem.asm.org/content/78/23/8441 Updated information and services can be found at: These include: SUPPLEMENTAL MATERIAL Supplemental material REFERENCES http://aem.asm.org/content/78/23/8441#ref-list-1 at: This article cites 29 articles, 13 of which can be accessed free CONTENT ALERTS more» articles cite this article), Receive: RSS Feeds, eTOCs, free email alerts (when new http://journals.asm.org/site/misc/reprints.xhtml Information about commercial reprint orders:

67

Enzyme inactivation by ethanol and development of a kinetic model for thermophilic simultaneous saccharification and fermentation at 50C with Thermoanaerobacterium saccharolyticum ALK2  

NLE Websites -- All DOE Office Websites (Extended Search)

Enzyme Enzyme Inactivation by Ethanol and Development of a Kinetic Model for Thermophilic Simultaneous Saccharification and Fermentation at 50 -C with Thermoanaerobacterium saccharolyticum ALK2 Kara K. Podkaminer, 1 Xiongjun Shao, 1 David A. Hogsett, 2 Lee R. Lynd 1 1 Thayer School of Engineering, Dartmouth College, Hanover, New Hampshire 03755; telephone: 603-646-2231; fax: 603-646-2277; e-mail: lee.lynd@dartmouth.edu 2 Mascoma Corporation, Lebanon, New Hampshire Received 6 August 2010; revision received 16 November 2010; accepted 14 December 2010 Published online 29 December 2010 in Wiley Online Library (wileyonlinelibrary.com). DOI 10.1002/bit.23050 ABSTRACT: Studies were undertaken to understand phe- nomena operative during simultaneous saccharification and fermentation (SSF) of a model cellulosic substrate (Avicel) at 508C with enzymatic hydrolysis mediated

68

Overview of the Quality and Completeness of Resource Assessment...  

NLE Websites -- All DOE Office Websites (Extended Search)

K K K KK KK x fs AES APEC BOB CRIB PI CWEEDS PERC HDR IRR ITCZ JMA LNG LPG MSW NBS NREL NSRDB PV RDF SOLMET SOLRAD WMO WRDC WTG Ac ronyms Atmospheric...

69

Research Highlight  

NLE Websites -- All DOE Office Websites (Extended Search)

McFarquhar, G. Zhang, M.R. Poellot, P.J. DeMott, A.J. Prenni and A.J. Heymsfield, 2007: Ice properties of single-layer stratocumulus during the Mixed-Phase Arctic Cloud...

70

Privacy Act Exemptions | National Nuclear Security Administration  

National Nuclear Security Administration (NNSA)

exemptions: Section 552a(j)(1) which covers records maintained by the Central Intelligence Agency, Section 552a(j)(2) which covers records relating to law enforcement...

71

Correlations Between Gene Expression and Mercury Levels in Blood of Boys With and Without Autism  

E-Print Network (OSTI)

AJ (2005) Inorganic mercury dissociates preassembledmetabolize toxicants, such as mercury, differently. RNA wasexpression microarrays. Mercury levels were measured using

2011-01-01T23:59:59.000Z

72

Dependenceof the ultrasonicpropertiesof biologicaltissue on constituent proteins  

E-Print Network (OSTI)

Olmob, A.J. Solera, G. Espesoc, M. Gomendiob, E.R.S. Roldanb, a Reproductive Biology Group, Instituto de

Illinois at Urbana-Champaign, University of

73

Undergraduate Catalog P.O. Box 1002  

E-Print Network (OSTI)

Olmob, A.J. Solera, G. Espesoc, M. Gomendiob, E.R.S. Roldanb, a Reproductive Biology Group, Instituto de

Hardy, Christopher R.

74

Haddad, T., Wright, D., Dailey, M., Klarin, P., Dana, R., Marra, J., and Revell, D., in press. The tools of the Oregon Coastal Atlas, in Wright, D.J. and Scholz, A.J. (eds.), Place Matters--Geospatial Tools for Marine Science, Conservation, and Management  

E-Print Network (OSTI)

easily be used together. Individually documented datasets were entered into a database and a web search using COMCI as a bibliographic search tool. Similarly, the glossary of scientific and technical terms to coastal zone management. Therefore as a portal, the Oregon Coastal Atlas enables users to search and find

Wright, Dawn Jeannine

75

Implication of a large ?_13 for the Tokai to Kamioka and Korea setup  

E-Print Network (OSTI)

In this paper, I present the implications of the large value of \\theta_13 on the Tokai to Kamioka and Korea setup (T2KK). I study the sensitivity of T2KK when using a 750 kW beam (the design luminosity of T2K planned to be achieved by 2017) and a potential 1.66 MW upgraded beam. In addition I compare the capability of the T2KK setup with the T2HK letter of intent.

Fanny Dufour

2012-11-16T23:59:59.000Z

76

Physics with large extra dimensions  

Science Conference Proceedings (OSTI)

scale, the KK excitations of gauge bosons and other standard model (sM) parti- ..... symmetry is broken by the vacuum expectation values of two Higgs doublets,

77

Benzo(a)pyrene and 7,12-dimethylbenz(a)anthrecene differentially affect bone marrow cells of the lymphoid and myeloid lineages  

E-Print Network (OSTI)

lineages. Nature 404, 193­197. Allan, L.L., Mann, K.K., Matulka, R.A., Ryu, H.Y., Schlezinger, J.J., Sherr

Jefcoate, Colin R.

78

You are now leaving Energy.gov | Department of Energy  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

MyWellhome?utmsourcesearch-results&utmmediumsearch&utmcampaignsem-energy-brand&gclidCMSqrNrozKkCFcjAKgod9w3uOA...

79

View PDF  

Science Conference Proceedings (OSTI)

Organizers: N. Chawla (Arizona State University, United States), R.D. Toledo Filho (Universidade Federal do Rio de Janeiro, Brazil), K.K. Chawla (University of

80

Detection of thin lines in low quality video Joshua Candamo, Rangachar Kasturi, Dmitry Goldgof, Sudeep Sarkar  

E-Print Network (OSTI)

] Fontana, R.J. Richley, E.A. Marzullo, A.J. Beard, L.C. Mulloy, R.W.T. Knight, E.J., "An ultra wideband

Sarkar, Sudeep

Note: This page contains sample records for the topic "aj podkaminer kk" 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

Fluctuations and Nanoscale Control  

Science Conference Proceedings (OSTI)

... Selected Publications: Simultaneous positioning and orientation of a single nano-object by flow control: theory and simulations, PP Mathai, AJ ...

2012-03-29T23:59:59.000Z

82

Temporal Variation in Fish Communities off Santa Cruz Island, California  

E-Print Network (OSTI)

blacksmith, Chromis punctipinnis, a planktivorous reef fish.U.S. Fish Bull Brooks AJ, Schmitt RJ, Holbrook SJ.2002. Declines in regional fish populations: have species

Graves, Michelle R.; Larson, Ralph J.; Alevizon, William S.

2006-01-01T23:59:59.000Z

83

Reservoir Management in Mediterranean Climates through the European Water Framework Directive  

E-Print Network (OSTI)

the EuropeanWater Framework Directive? Elsevier Cabecinha,Under the Water Framework Directive. Conacher, A.J. , Sala,The EU Water Framework Directive: measures and implications.

O'Reilly, Clare; Silberblatt, Rafael

2009-01-01T23:59:59.000Z

84

The Symposium on Computational Methods in Materials Education  

Science Conference Proceedings (OSTI)

... Materials Processing and Diffusion, by S.E. Mohney, A.J. Miller, and G.L. Gray; Our Experience in Teaching Thermodynamics at the University of Wisconsin,...

85

Assuming Responsibility for Packaging and Packaging Waste  

E-Print Network (OSTI)

> Natural Resources Institute, University of ManitobaWinnipeg, Manitoba, Canada R3T 2N2.and A.J. Sinclair. (1997). "Manitobas Product Stewardship

Sinclair, A. John

2000-01-01T23:59:59.000Z

86

NIST CNR SANS NG3 30 Meter SANS Instrument  

Science Conference Proceedings (OSTI)

... 3, Characterization of Fly Ash Reactivity in Hydrating Cement by Neutron Scattering, W. Bumrongjaroen, RA Livingston, DA Neumann, AJ Allen, J ...

87

Volume 131, Number 41 tech.mit.edu Friday, September 30, 2011 Oldest and Largest  

E-Print Network (OSTI)

of abuse. Mazei-Robison MS, Koo JW, Friedman AK, Lansink CS, Robison AJ, Vinish M, Krishnan V, Kim S, Siuta

88

A N N U A L R E P O R T 2 0 1 0 -2 0 1 1 NATIONAL INSTITUTE OF ADVANCED STUDIES  

E-Print Network (OSTI)

of abuse. Mazei-Robison MS, Koo JW, Friedman AK, Lansink CS, Robison AJ, Vinish M, Krishnan V, Kim S, Siuta

Udgaonkar, Jayant B.

89

Fabrication and Characterization of Organic Solar Cells  

E-Print Network (OSTI)

processablepolymerphotovoltaiccellsbyself?organizationPhotodiodes, and Photovoltaic Cells. AppliedPhysicsF, Heeger AJ. Polymer Photovoltaic Cells ? Enhanced

Yengel, Emre

2010-01-01T23:59:59.000Z

90

SE33 References  

Science Conference Proceedings (OSTI)

... In: DNA Fingerprinting: State of the Science, edited by Pena, SDJ, Chakraborty, R., Epplen, JT, and Jeffreys, AJ Basel, Switzerland:Birkauser Verlag ...

2007-07-10T23:59:59.000Z

91

Bayesian random local clocks, or one rate to rule them all  

E-Print Network (OSTI)

AJ, Rambaut A: BEAST: Bayesian evolutionary analysis bypractical implementation of Bayesian model selection. ModelWeiss RE, Sinsheimer JS: Bayesian selection of continuous-

Drummond, Alexei J; Suchard, Marc A

2010-01-01T23:59:59.000Z

92

Selected References  

Science Conference Proceedings (OSTI)

...A.J. Pesce, C-G Rosen, T.L. Pasby, Ed., Fluorescence Spectroscopy: An Introduction for Biology and Medicine, Marcel Dekker, 1971...

93

Magnetic Order in Superconductors  

Science Conference Proceedings (OSTI)

... Intrinsic Properties of Stoichiometric LaOFeP, TM McQueen, M. Regulacio, AJ Williams, Q. Huang, JW Lynn, YS Hor, DV West, and RJ Cava, Phys. ...

94

Iron-based Superconductors  

Science Conference Proceedings (OSTI)

... Intrinsic Properties of Stoichiometric LaOFeP, TM McQueen, M. Regulacio, AJ Williams, Q. Huang, JW Lynn, YS Hor, DV West, and RJ Cava, Phys. ...

95

Synthesis, Characterization, and Integration of Silicon Nanowires for Nanosystems Technology  

E-Print Network (OSTI)

J.A. Sioss, K.K. Lew, J.M. Redwing, C.D. Keating, and T.S.Dilts, E.C. Dickey, J.M. Redwing, Y.F. Wang, M. Cabassi,134] L. Pan, K.K. Lew, J.M. Redwing, and E.C. Dickey. Effect

Doerk, Gregory Stephen

2010-01-01T23:59:59.000Z

96

A new semidefinite programming relaxation for the quadratic ...  

E-Print Network (OSTI)

vP@BAjvP@BAs. @j;jA kk. . @s;sA kk. @by Theorem 1.1(iv)A a @XvP@BAA. P k ; as required. Finally, one may verify in a similar way that the constraints.

97

World Catalog of the Beach-Fly Family Canacidae (Diptera)  

E-Print Network (OSTI)

lessoni Australia NA EU556308 EU556266 Autropeplea ollula Philippines NA NA U82067 Autropeplea tomentosa, Quifangondo AF503573 AM921961 AY029550 Bullastra cumingiana Philippines, Luzon NA EU556314 U82068 Fossaria HQ283241 Lymnaea fuscus Germany, Westfallen AJ626855 AJ319622 NA Lymnaea gen. sp. Hawaii, Kauai NA NA

Mathis, Wayne N.

98

2012 COMMENCEMENT CEREMONY COMMENCEMENT SCORE  

E-Print Network (OSTI)

of Students #12;SINGING OF "AMERICA THE BEAUTIFUL" Song Leaders: Craig Boddy, Christian Cain, Patricia Chico, Amish Desai, Denise Lopez Domowicz, A.J. Mariano, Damaris Ortiz, Albert Sohn, Steven Wisel, MD Associate Dean Kashima MD CLASS REMARKS A.J. Mariano, MD, President, Class of 2012 THE PHYSICIAN'S OATH Dean

Illinois at Chicago, University of

99

Editors: Prof. Stephen Nortcliff Department of Soil Science  

E-Print Network (OSTI)

Editors: Prof. Stephen Nortcliff Department of Soil Science The University of Reading PO Box 233@reading.ac.uk Dr. Alfred E. Hartemink ISRIC ­ World Soil Information P.O. Box 353 6700 AJ Wageningen: Drs. J. Hans V. van Baren ISRIC ­ World Soil Information P.O. Box 353 6700 AJ Wageningen

Sparks, Donald L.

100

Analysis of Casimir forces with window functions: Kramers-Kronig general approach for real measured dielectric data  

Science Conference Proceedings (OSTI)

In this work we describe how the window method, which has been used with ideal Kramers-Kroning (K-K) consistent dielectric functions, is affected by real optical data where some degree of K-K inconsistency is always present. Analysis using measured data of the frequency-dependent dielectric function for gold and phase-change materials shows that the window method can in some cases amplify the errors introduced in the calculation of the Casimir force due to K-K inconsistency instead of minimizing them. The latter indicates that caution is required for the proper choice of the window function for dielectric data analysis and Casmir force calculations.

Shpak, O. [Physics of Fluids Group, Department of Science and Technology, University of Twente, P.O. Box 217, NL-7500 AE Enschede (Netherlands); Palasantzas, G. [Materials Innovation Institute (M2i) and Zernike Institute for Advanced Materials, University of Groningen, NL-9747 AG Groningen (Netherlands)

2011-10-15T23:59:59.000Z

Note: This page contains sample records for the topic "aj podkaminer kk" 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

HH5, Antiferromagnetic Interlayer Exchange Couplings in Ga  

Science Conference Proceedings (OSTI)

Author(s), Sun Jae Chung, Sanghoon Lee, Brian J. Kirby, Julie A. Borchers, ... LATE NEWS: KK3, Non-Catalytic Synthesis of GaN Nanostructures at Low...

102

The Dalhousie University Community Committee Meeting Lord Dalhousie Room  

E-Print Network (OSTI)

& 3 is permanently shut down and decommissioned. F. Nuclear Safety Culture SCE is committed. Evaluation of Lessons Learned from KK Nuclear Plant............................12 5. Seismic Reliability of Extended Operations .....................................................30 c) Decommissioning Period

Beaumont, Christopher

103

Collective phenomena in non-central nuclear collisions  

E-Print Network (OSTI)

Low density and ideal hydro limits, v 2 /? plot . Viscousexpression v 2 /? = (v 2 /?) hydro (1 + K/K 0 ) ?1 , wherebe up to 30% below the ideal hydro limit even for the most

Voloshin, Sergei A.

2008-01-01T23:59:59.000Z

104

How to Protect DES Against Exhaustive Key Search (an Analysis of ...  

Science Conference Proceedings (OSTI)

Jan 1, 2001 ... The block cipher \\DESX is defined by \\DESX k.k1.k2 (x) = k2\\xor \\DES k (k1\\xor x) , where \\xor denotes bitwise exclusive-or. This construction...

105

C H A P T E R S E V E N MacIntyre and the Emotivists  

E-Print Network (OSTI)

forecast ewf k = wf k ;bf k: (6) Similarly, ewo k = wo k ;bo k (7) would be a set of unbiased observations which properly accounts for bias is then ewa k = ewf k + Kk h ewo k ;Hk ewf k i (8) where ewa k wo k wf k in place of ewo k ewf k the analysis equation is wa k = wf k + Kk h wo k ;Hkwf k i : (11

Marsh, David

106

High temperature elemental losses and mineralogical  

E-Print Network (OSTI)

5] Baxter LL. Biomass Bioenergy 1993;4:85102. [6] Miles RR,BM, Oden LL. Biomass Bioenergy 1996;10:12538. [7] HastieKW, Baker AJ. Biomass Bioenergy 1993;4:10316. [16] Jensen

Thy, P.; Jenkins, B. M.; Grundvig, S.; Shiraki, R.; Lesher, C. E.

2006-01-01T23:59:59.000Z

107

Sustainable Energy Through Recycling Used Nuclear Fuel  

NLE Websites -- All DOE Office Websites (Extended Search)

Energy Through Recycling Used Nuclear Fuel M.A. Williamson, A.V. Guelis, J.L. Willit, C. Pereira and A.J. Bakel Argonne National Laboratory Recycle of used nuclear fuel is central...

108

Cold Fusion Production and Decay of Neutron-Deficient Isotopes of Dubnium and Development of Extraction Systems for Group V Elements  

E-Print Network (OSTI)

separator for the study of fusion reaction products."by heavy-ion induced fusion?" Zeitschrift Fur Physik a-J. Wilczy?ski (2003). "Fusion by Diffusion." Acta Physica

Gates, Jacklyn M.

2008-01-01T23:59:59.000Z

109

table of contents  

Science Conference Proceedings (OSTI)

P. Hanniala, L. Helle and I.V. Kojo. Developments in Direct-to-Blister Smelting at Olympic Dam [pp. 239-253] ... A.J. Rigby and M.D. Lanyi. Redesigning the Flash ...

110

FAST ALGORITHMS FOR THE GENERALIZED FOLEY-SAMMON ...  

E-Print Network (OSTI)

results on several real world data sets indicate the efficiency of the algorithm and ... Suppose A = [A1, ,Ac] ? RNn, where each Aj ? RNnj for j = 1, ,c, c ?.

111

Microsoft Word - El_Dorado_Final_EA 2011.2.10  

NLE Websites -- All DOE Office Websites (Extended Search)

following sites were not mapped: Site Name Database(s) BRUCE OIL CO-EL DORADO REFINERY TIER 2 REGIONAL ENERGY GROUP-EL DORADO TIER 2 AJ'S TANK TRUCK...

112

Animal calcium release-activated calcium (CRAC) channels are homologous and derived from the ubiquitous Cation Diffusion Facilitators  

E-Print Network (OSTI)

A.J. (1996) A DEAD-box RNA helicase in the Escherichia colito the RhlB predicted ATP-dependent RNA helicase of theDEAD box helicase family (Py et al. , 1996). Cai (2007a) has

Matias, Madeleine Gundayao

2008-01-01T23:59:59.000Z

113

William J. Behrens | BNL  

NLE Websites -- All DOE Office Websites (Extended Search)

Society, Washington, DC. October, 1995. Ashjian, C.J., Smith, S.L., Flagg, C.N., Mariano, A.J., Behrens, W.J., and Lane, P. The influence of a Gulf Stream meander on the...

114

Peter Nugent  

NLE Websites -- All DOE Office Websites (Extended Search)

and GRB 060218SN 2006aj, but smaller than the other SNe firmly associated with gamma-ray bursts (GRBs). We conducted a multi-wavelength follow-up campaign with Palomar 48 inch,...

115

Nurture over nature: Summer germinating Lupinus nanus are a result of anthropogenic germination cues and are not an independently evolving population  

E-Print Network (OSTI)

395, Goodman KR, Morris VRF, Welter SC, Roderick GK (2008)Moore AJ, Moore WL, Morris VRF, Baldwin BG (2009) Molecular90, 378-387. Morris VRF and Dodd RS (2006) Characterization

Morris, Veronica Ruth Franco

2009-01-01T23:59:59.000Z

116

Diagnosing Mesoscale Vertical Motion from Horizontal Velocity and Density Data  

Science Conference Proceedings (OSTI)

The mesoscale vertical velocity is obtained by solving a generalized omega equation (? equation) using density and horizontal velocity data from three consecutive quasi-synoptic high-resolution surveys in the Alboran Sea. The Atlantic Jet (AJ) ...

Enric Palls Sanz; lvaro Videz

2005-10-01T23:59:59.000Z

117

Low Dose Radiation Research Program: David Nelson  

NLE Websites -- All DOE Office Websites (Extended Search)

L.E., Nelson, D., Sorensen, K., Tucker, J.D., and Wyrobek, A.J. (2005). Low-dose irradiation alters the transcript profiles of human lymphoblasoid cells, including genes...

118

Contextualizing the Nabataeans: A Critical Reassessment of their History and Material Culture  

E-Print Network (OSTI)

of modern Arabic, see esp. Cantineau (1934/5), 77-97;weak and ineffectual. See esp. Josephus AJ 16.220; 280; 288Spijkerman (1978), passim, but esp. the coins from Gadara

Pearson, Jeffrey Eli

2011-01-01T23:59:59.000Z

119

NIST CNR SANS NG7 30 Meter SANS Instrument  

Science Conference Proceedings (OSTI)

... B. Tang, T. Koga, MH Rafailovich, JC Sokolov, DG Peiffer, Z. Li, AJ Dias, KO McElrath, MY Lin, SK Satija, SG Urquhart, H. Ade, D. Nguyen, Macromol ...

120

SANS Publications - 2001  

Science Conference Proceedings (OSTI)

... B. Tang, T. Koga, MH Rafailovich, JC Sokolov, DG Peiffer, Z. Li, AJ Dias, KO McElrath, MY Lin, SK Satija, SG Urquhart, H. Ade, D. Nguyen, Macromol ...

Note: This page contains sample records for the topic "aj podkaminer kk" 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.


121

A Promising Alternative to Traditional Photovoltaic Materials...  

Office of Science (SC) Website

Publications Morfa AJ, TH Reilly, JC Johnson, and J van de Lagemaat. 2009. "Plasmons in Solar Energy Conversion." SPIE Newsroom. Reilly TH, RC Tenent, TM Barnes, KL Rowlen, and J...

122

THE USE OF CALORIMETRY IN SUPERFLUID HE II TO MEASURE LOSSES IN SUPERCONDUCTING MAGNETS  

E-Print Network (OSTI)

chamber where the He II heat exchanger is located. Duringthrough a counterflow heat exchanger and expanded through aJ T) valve. Leaving the heat exchanger at low pressure the

Caspi, S.

2010-01-01T23:59:59.000Z

123

Stalled on the Road to the Market: Analysis of Field Experience with a Project to Promote Lighting Efficiency in India  

E-Print Network (OSTI)

1991. "Energy-Efficient Lighting in Brazil and India:on Energy-Efficient Lighting. Stockholm, Sweden. Katzev,with a Project to Promote Lighting Efficiency in India AJ.

Gadgil, A.J.

2008-01-01T23:59:59.000Z

124

ARM - Publications: Science Team Meeting Documents  

NLE Websites -- All DOE Office Websites (Extended Search)

Retrieval of Ice Water Path Using Thermal Channels Mitchell, D.L. (a), d'Entremont, R.P. (b), Stackhouse, P.W., Jr. (c), and Heymsfield, A.J. (d), Desert Research Institute (a),...

125

Applied Science  

NLE Websites -- All DOE Office Websites (Extended Search)

Nuclear Science EXAFS and XANES of plutonium and uranium edges from titanate ceramics for fissile materials disposition J.A. Fortner, A.J. Kropf, R.J. Finch, M.C. Hash, S.B. Aase,...

126

Sphingosine 1-phosphate signaling in the heart and its role in cardioprotection  

E-Print Network (OSTI)

309: 155-160, 2003. 18. Fukushima N, Kimura Y and Chun J. AJ Biol Chem 276: 37. Ishii I, Fukushima N, Ye X and Chun J.G, Contos JJ, Weiner JA, Fukushima N and Chun J. Comparative

Means, Christopher Kable

2007-01-01T23:59:59.000Z

127

Page 1 of 20 A Five Year Diversity Plan Draft  

E-Print Network (OSTI)

Martin Kimi Mojica Steve Morozumi Karen Munro Erin O'Brien A.J. Peper Steve Pickett Leslie Sanchez John Laura Blake-Jones Doug Blandy Heather Bottorff Chris Browning James Chang Diane Del Guercio Kassia

Kleshchev, Alexander

128

Solid-state photonic interfaces using semiconductor quantum dots  

E-Print Network (OSTI)

. Boyer de la Giroday, N. Skold, I. Farrer, C.A. Nicoll, D.A. Ritchie, and A.J. Shields Nature Physics, 6, 947 (2010) 3. All-electrical coherent control of the exciton states in a single quantum dot A. Boyer de la Giroday, A.J. Bennett, M.A. Pooley, R... O. Thomas, C.L. Salter, A.J. Bennett, R.M. Stevenson, M.A. Pooley, M.B. Ward, R.B. Patel, A. Boyer de la Giroday, N. Skold, I. Far- rer, C.A. Nicoll, D.A. Ritchie, and A.J. Shields Proc. QCMC 2010 2. Observation of anticrossings in the exciton state...

Boyer de la Giroday, Antoine

2012-02-07T23:59:59.000Z

129

At the Biological Modeling and Simulation Frontier  

E-Print Network (OSTI)

Odell GM, Foe VE. An agent-based model contrasts oppositeAJ, Peirce SM. Agent-based model of therapeutic adipose-An unvalidated agent-based model can implement detailed

2009-01-01T23:59:59.000Z

130

Partial Convexification of General MIPs by Dantzig-Wolfe ...  

E-Print Network (OSTI)

and n railcars, the jth having weight aj and to be transported from station sj to station fj, gaining ..... A freight service design problem for a railway corridor. Tran.

131

table of contents  

Science Conference Proceedings (OSTI)

Thermochemical Modeling of Smelting Operations [pp. 309-321] A.L. Davies, J.F. Castle, P.J. Gabb, M.A.S. Siraa, J.A. Gisby and A.J. Weddick. Software for the...

132

Seismic soil-structure interaction in buildings. I: Analytical aspects  

E-Print Network (OSTI)

J. Struct. Engrg. , ASCE, 101(1), 109 129. Veletsos, A.J. Geotech. Engrg. , ASCE, 112(2), 109 135. Duke, C. M. ,medium. J. Engrg. Mech. , ASCE, 108(6), 1103 1120.

Stewart, Jonathan P; Fenves, Gregory L; Seed, Raymond B

1999-01-01T23:59:59.000Z

133

NUMERICAL ANALYSIS OF FLOW FIELDS GENERATED BY ACCELERATING FLAMES  

E-Print Network (OSTI)

A.J. and Oppenheim, A.K. , "Initial Flame Acceleration in anGeneration of a Shock Wave by a Flame in an Explosive Gas",of Pressure Waves by Accelerating Flames", Tenth Symposium (

Kurylo, J.

2011-01-01T23:59:59.000Z

134

Studies in History and Philosophy of Modern Physics 37 (2006) 661691  

E-Print Network (OSTI)

] is a Bernoulli automorphism if there exists a partition a ¼ fa1; :::; ang such that all T i a, ?1oio1 such that T i a, ?1oio1, are independent; that is if mðTn ai \\ Tm aj? ¼ mðTn ai?mðTm aj? for any ?1om; no1

Skyrms, Brian

135

Kaluza-Klein gluon searches using the three-b-jet decay channel at the Large Hadron Collider  

E-Print Network (OSTI)

We study observability of a Kaluza-Klein (KK) excitation of a gluon in a five-dimensional model with a warped geometry at the Large Hadron Collider. In this model, the Standard Model fields reside in the bulk and the third generation quarks couple to the KK gluon strongly. We focus on the processes including three b-quarks as a final state where the first KK gluon propagates as an intermediate state. We evaluate a significance of those processes by taking account of kinematical cuts and a detector efficiency at the Large Hadron Collider and find that the significance is lager than 5-sigma with the integrated luminosity of 10 (100) fb^{-1} for a certain range of parameters of the model.

Masato Arai; Gi-Chol Cho; Karel Smolek

2013-07-24T23:59:59.000Z

136

Plasma graviton production in TeV-scale gravity  

E-Print Network (OSTI)

We develop the theory of interaction of classical plasma with Kaluza-Klein (KK) gravitons in the ADD model of TeV-scale gravity. Plasma is described within the kinetic approach as the system of charged particles and Maxwell field both confined on the brane. Interaction with multidimensional gravity living in the bulk with $n$ compact extra dimensions is introduced within the linearized theory. The KK gravitons emission rates are computed taking into account plasma collective effects through the two-point correlation functions of the fluctuations of the plasma energy-momentum tensor. Apart from known mechanisms (such as bremsstrahlung and gravi-Primakoff effect) we find essentially collective channels such as the coalescence of plasma waves into gravitons which may be manifest in turbulent plasmas. Our results indicate that commonly used rates of the KK gravitons production in stars and supernovae may be underestimated.

E. Yu. Melkumova

2010-12-14T23:59:59.000Z

137

EPRI Independent Peer Review of the TEPCO Seismic Walkdown and Evaluation of the Kashiwazaki-Kariwa Nuclear Power Plants  

Science Conference Proceedings (OSTI)

The Tokyo Electric Power Company's (TEPCO's) Kashiwazaki-Kariwa (KK) plant is the largest nuclear power plant in the world with a total output of 8212 MW. The KK plant is 16 kilometers away from the epicenter of the Niigataken-Chuetsu-Oki (NCO) offshore earthquake, which took place at 10:13 a.m. on July 16, 2007, and had a Richter magnitude of 6.6. Ground motion recordings at the basemat of the seven boiling water reactors at the site revealed that the S2 seismic design level had been exceeded during the...

2008-01-14T23:59:59.000Z

138

Search for universal extra dimensions in ppbar collisions  

Science Conference Proceedings (OSTI)

We present a search for Kaluza-Klein (KK) particles predicted by models with universal extra dimensions (UED) using a data set corresponding to an integrated luminosity of 7.3 fb{sup -1}, collected by the D0 detector at a p{bar p} center of mass energy of 1.96 TeV. The decay chain of KK particles can lead to a final state with two muons of the same charge. This signature is used to set a lower limit on the compactification scale of R{sup -1} > 260 GeV in a minimal UED model.

Abazov, Victor Mukhamedovich; /Dubna, JINR; Abbott, Braden Keim; /Oklahoma 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.; Aoki, Masato; /Fermilab; Askew, Andrew Warren; /Florida State U. /Stockholm U.

2011-12-01T23:59:59.000Z

139

Search for Universal Extra Dimensions in p(p)over-bar Collisions  

Science Conference Proceedings (OSTI)

We present a search for Kaluza-Klein (KK) particles predicted by models with universal extra dimensions (UED) using a data set corresponding to an integrated luminosity of 7.3 fb{sup -1}, collected by the D0 detector at a p{bar p} center-of-mass energy of 1.96 TeV. The decay chain of KK particles can lead to a final state with two muons of the same charge. This signature is used to set a lower limit on the compactification scale of R{sup -1} > 260 GeV in a minimal UED model.

Abazov V. M.; Abbott B.; Acharya B. S.; Adams M.; Adams T.; Alexeev G. D.; Alkhazov G.; Alton A.; Alverson G.; Aoki M.; Askew A.; Asman B.; Atkins S.; Atramentov O.; Augsten K.; Avila C.; BackusMayes J.; Badaud F.; Bagby L.; Baldin B.; Bandurin D. V.; Banerjee S.; Barberis E.; Baringer P.; Barreto J.; Bartlett J. F.; Bassler U.; Bazterra V.; Bean A.; Begalli M.; Belanger-Champagne C.; Bellantoni L.; Beri S. B.; Bernardi G.; Bernhard R.; Bertram I.; Besancon M.; Beuselinck R.; Bezzubov V. A.; Bhat P. C.; Bhatia S.; Bhatnagar V.; Blazey G.; Blessing S.; Bloom K.; Boehnlein A.; Boline D.; Boos E. E.; Borissov G.; Bose T.; Brandt A.; Brandt O.; Brock R.; Brooijmans G.; Bross A.; Brown D.; Brown J.; Bu X. B.; Buehler M.; Buescher V.; Bunichev V.; Burdin S.; Burnett T. H.; Buszello C. P.; Calpas B.; Camacho-Perez E.; Carrasco-Lizarraga M. A.; Casey B. C. K.; Castilla-Valdez H.; Chakrabarti S.; Chakraborty D.; Chan K. M.; Chandra A.; Chapon E.; Chen G.; Chevalier-Thery S.; Cho D. K.; Cho S. W.; Choi S.; Choudhary B.; Cihangir S.; Claes D.; Clutter J.; Cooke M.; Cooper W. E.; Corcoran M.; Couderc F.; Cousinou M-C; Croc A.; Cutts D.; Das A.; Davies G.; de Jong S. J.; De La Cruz-Burelo E.; Deliot F.; Demina R.; Denisov D.; Denisov S. P.; Desai S.; Deterre C.; DeVaughan K.; Diehl H. T.; Diesburg M.; Ding P. F.; Dominguez A.; Dorland T.; Dubey A.; Dudko L. V.; Duggan D.; Duperrin A.; Dutt S.; Dyshkant A.; Eads M.; Edmunds D.; Ellison J.; Elvira V. D.; Enari Y.; Evans H.; Evdokimov A.; Evdokimov V. N.; Facini G.; Ferbel T.; Fiedler F.; Filthaut F.; Fisher W.; Fisk H. E.; Fortner M.; Fox H.; Fuess S.; Garcia-Bellido A.; Garcia-Guerra G. A.; Gavrilov V.; Gay P.; Geng W.; Gerbaudo D.; Gerber C. E.; Gershtein Y.; Ginther G.; Golovanov G.; Goryachev V. N.; Goussiou A.; Grannis P. D.; Greder S.; Greenlee H.; Greenwood Z. D.; Gregores E. M.; Grenier G.; Gris Ph; Grivaz J-F; Grohsjean A.; Gruenendahl S.; Gruenewald M. W.; Guillemin T.; Gutierrez G.; Gutierrez P.; Haas A.; Hagopian S.; Haley J.; Han L.; Harder K.; Harel A.; Hauptman J. M.; Hays J.; Head T.; Hebbeker T.; Hedin D.; Hegab H.; Heinson A. P.; Heintz U.; Hensel C.; Heredia-De La Cruz I.; Herner K.; Hesketh G.; Hildreth M. D.; Hirosky R.; Hoang T.; Hobbs J. D.; Hoeneisen B.; Hohlfeld M.; Hubacek Z.; Hynek V.; Iashvili I.; Ilchenko Y.; Illingworth R.; Ito A. S.; Jabeen S.; Jaffre M.; Jamin D.; Jayasinghe A.; Jesik R.; Johns K.; Johnson M.; Jonckheere A.; Jonsson P.; Joshi J.; Jung A. W.; Juste A.; Kaadze K.; Kajfasz E.; Karmanov D.; Kasper P. A.; Katsanos I.; Kehoe R.; Kermiche S.; Khalatyan N.; Khanov A.; Kharchilava A.; Kharzheev Y. N.; Kohli J. M.; Kozelov A. V.; Kraus J.; Kulikov S.; Kumar A.; Kupco A.; Kurca T.; Kuzmin V. A.; Lammers S.; Landsberg G.; Lebrun P.; Lee H. S.; Lee S. W.; Lee W. M.; Lellouch J.; Li H.; Li L.; Li Q. Z.; Lietti S. M.; Lim J. K.; Lincoln D.; Linnemann J.; Lipaev V. V.; Lipton R.; Liu Y.; Lobodenko A.; Lokajicek M.; de Sa R. Lopes; Lubatti H. J.; Luna-Garcia R.; Lyon A. L.; Maciel A. K. A.; Mackin D.; Madar R.; Magana-Villalba R.; Malik S.; Malyshev V. L.; Mansour J.; Maravin Y.; Martinez-Ortega J.; McCarthy R.; McGivern C. L.; Meijer M. M.; Melnitchouk A.; Menezes D.; Mercadante P. G.; Merkin M.; Meyer A.; Meyer J.; et al.

2012-03-30T23:59:59.000Z

140

Arokiasamy J. Francis | BNL  

NLE Websites -- All DOE Office Websites (Extended Search)

Arokiasamy J. (AJ) Francis Arokiasamy J. (AJ) Francis Emeritus Microbiologist Arokiasamy J. (A.J.) Francis, retired from the Environmental Sciences Department in 2011 and was named Scientist Emeritus in 2012. During his nearly 37 years at Brookhaven National Laboratory, he has concentrated on the realm of microbial interactions with organic and inorganic contaminants - and their remediation. Francis' investigations have ranged from nitrogen cycling and the control of nitrate pollution to the transformation of radioactive contaminants in the environment. The latter became his primary research focus, taking shape in many different projects, including his groundbreaking work with the use of citric acid to sequester uranium from contaminated soils, wastes and materials. Francis first came to Brookhaven in 1975 as a microbiologist on a project

Note: This page contains sample records for the topic "aj podkaminer kk" 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

Phase Transformations in Heterogeneous Steels  

E-Print Network (OSTI)

Vidmanstatten ferrite is an undesirable constituent because of its inferior toughness properties[lB,17]. If a plate or lath ij idealijed aj a rectangular parallelepiped with jidej of lengths aJ bJ and CJ then a=bc for a plate and abc for a lath. 4 Fig. 1... : Welding and Performance of Pipelines, p. 17-1, editor P. H. M. Hart, The 'Welding Institute, Abington, 1986. 49. K. C. Russell: Acta Metall., 1969, vol. 17, p. 1123. 50. J. W. Christian: Theory of Tran.sjormations in Metals and Alloys, p. 375, Perga- mon...

Khan, Shahid Amin

1990-05-08T23:59:59.000Z

142

Numerical study of reaction in porous catalysts under composition modulation  

E-Print Network (OSTI)

be solved numerically ALLOCATE(CIM(ngz,ntc),CIV(2,nciv)) !k=k+1; ! index of CIV CIM(j,i)=k; ! store column index ofstore column index of C ELSE CIM(j,i)=0; END IF ELSEIF (i>=

Hsiao, Hsu-Wen

2010-01-01T23:59:59.000Z

143

Generating random graphs with large girth  

Science Conference Proceedings (OSTI)

We present a simple and efficient algorithm for randomly generating simple graphs without small cycles. These graphs can be used to design high performance Low-Density Parity-Check (LDPC) codes. For any constant k, ? ? 1/2k(k ...

Mohsen Bayati; Andrea Montanari; Amin Saberi

2009-01-01T23:59:59.000Z

144

Engineering Design Example CompressedCompressed--Air System for a Manufacturing PlantAir System for a Manufacturing Plant  

E-Print Network (OSTI)

to operate C/A tools: Compressor and piping layoutCompressor and piping layout Air supply circumferentially: · Estimate the load [cfm] based on current and future demand. · Size the compressor(s). · Size the pipes so*1.35=1900 cfm. · Centrifugal or reciprocating compressor may be chosen (later). From handbooks: P kk /)1

Kostic, Milivoje M.

145

Physics Letters A 337 (2005) 397407 www.elsevier.com/locate/pla  

E-Print Network (OSTI)

: 52.27.Gr; 52.57.Kk; 52.25.Mq Keywords: Aneutronic; Fusion; Degeneracy; Stopping; Cold; Pycnonuclear; Helium; Deuterium; Chain; Reaction 1. Introduction In cold ultra-dense matter, fusion reactions are quite the fusion reaction rate in this regime, quite different methods must be used. While the so-called cold

146

SHA-3 Conference, February 2009, AURORA  

Science Conference Proceedings (OSTI)

... DD LL DD L DL DD BLL pp r B h BB loo cc kk ccciphh ee r BB ll ockcipp herr vv svv svv ss DD MMM vv ss . DD M DD M vv ss . DD MM vss vs.. vss . ...

2012-06-05T23:59:59.000Z

147

Ultrafast tracking electronics for the ATLAS trigger at the CERN Large Hadron Collider  

E-Print Network (OSTI)

FTK Ultrafast tracking electronics for the ATLAS trigger at the CERN Large Hadron Collider Italy challenge at a hadron collider is determining what a new phenomenon is. Higgs, SUSY, KK excitations, Z of decay products multiple decay modes couplings to other particles · For each of these, large samples

148

Light Vector Mesons from dAu in PHENIX  

E-Print Network (OSTI)

A first measurement of the e+e-decay rate of phi mesons in dAu collisions from the PHENIX detector at RHIC and its comparison to the K+K- decay channel is described. The comparison of the two decay channels can be sensitive to chiral symmetry restoration.

Richard Seto

2004-04-01T23:59:59.000Z

149

Graphical Method for Effective Interaction with a New Vertex Function  

E-Print Network (OSTI)

Introducing a new vertex function, Z(E), of an energy variable E, we derive a new equation for the effective interaction. The equation is obtained by replacing the Q-box in the Krenciglowa-Kuo (KK) method by Z(E). This new approach can be viewed as an extension of the KK method. We show that this equation can be solved both in iterative and non-iterative ways. We observe that the iteration procedure with Z(E) brings about fast convergence compared to the usual KK method. It is shown that, as in the KK approach, the procedure of calculating the effective interaction can be reduced to determining the true eigenvalues of the original Hamiltonian H and they can be obtained as the positions of intersections of graphs generated from Z(E). We find that this graphical method yields always precise results and reproduces any of the true eigenvalues of H. The calculation in the present approach can be made regardless of overlaps with the model space and energy differences between unperturbed energies and the eigenvalues of H. We find also that Z(E) is a well-behaved function of E and has no singularity. These characteristics of the present approach ensure stability in actual calculations and would be helpful to resolve some difficulties due to the presence of poles in the Q-box. Performing test calculations we verify numerically theoretical predictions made in the present approach.

K. Suzuki; R. Okamoto; H. Kumagai; S. Fujii

2010-12-28T23:59:59.000Z

150

Static four-dimensional abelian black holes in Kaluza-Klein theory  

E-Print Network (OSTI)

Static, four-dimensional (4-d) black holes (BH's) in (4+n)-d Kaluza-Klein (KK) theory with Abelian isometry and diagonal internal metric have at most one electric (Q) and one magnetic (P) charges, which can either come from the same U(1)-gauge field (corresponding to BH's in effective 5-d KK theory) or from different ones (corresponding to BH's with U(1)_M\\times U(1)_E isometry of an effective 6-d KK theory). In the latter case, explicit non-extreme solutions have the global space-time of Schwarzschild BH's, finite temperature, and non-zero entropy. In the extreme (supersymmetric) limit the singularity becomes null, the temperature saturates the upper bound T_H=1/4\\pi\\sqrt{|QP|}, and entropy is zero. A class of KK BH's with constrained charge configurations, exhibiting a continuous electric-magnetic duality, are generated by global SO(n) transformations on the above classes of the solutions.

Cvetic, M; Cvetic, Mirjam; Youm, Donam

1995-01-01T23:59:59.000Z

151

Walker, E., Rummel, N., McLaren, B. M. & Koedinger, K. R. (2007). The Student Becomes the Master: Integrating Peer Tutoring with Cognitive Tutoring. In the Proceedings of the Conference on Computer-Supported Collaborative Learning (CSCL 2007).  

E-Print Network (OSTI)

is not massive or critical. Let = sds1 , dwG 2 e. There are at least 2 +2 s1-chains in 3-blkG. Let M be the set of s1-chain leaves. By adding 2k;k , edges to connect 2k + 1 vertices of M, we reduce both sds1

McLaren, Bruce Martin

152

Copyright owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike Licence. http://pos.sissa.it Study of the radiation-hardness of VCSEL and PIN  

E-Print Network (OSTI)

. This provides a simple mechanism to recover from the radiation damage. 9th International Conference on Large the radiation exposure and simplify the detector construction. In fact, the electric signals from the front-NonCommercial-ShareAlike Licence. http://pos.sissa.it Study of the radiation-hardness of VCSEL and PIN K.K. Gan1 , W. Fernando, H

Gan, K. K.

153

Non-Standard Neutrino Physics Probed by Tokai-to-Kamioka-Korea Two-Detector Complex  

E-Print Network (OSTI)

The discovery potentials of non-standard physics (NSP) which might be possessed by neutrinos are examined by taking a concrete setting of Tokai-to-Kamioka-Korea (T2KK) two detector complex which receives neutrino superbeam from J-PARC. We restrict ourselves into \

Nei Cipriano Ribeiro; Takaaki Kajita; Pyungwon Ko; Hisakazu Minakata; Shoei Nakayama; Hiroshi Nunokawa

2008-01-16T23:59:59.000Z

154

50 2sBe?t3X%7%s%]%8%&%`!&FAEgBg3X!$2005 G/8 7n2 F--GLn N g I/j Langlands BP1~  

E-Print Network (OSTI)

(K/Q) $NCf$G6&Lr$G$"$k$+$i!$$H$/$KK/Q Abel 3H Bg$J$i$PFrP HGP p N GDj j rGp, Frp GI/ Frp Gp N G j p OK G [K

Yoshino, Yuji

155

Flavor Physics in the Randall-Sundrum Model: I. Theoretical Setup and Electroweak Precision Tests  

E-Print Network (OSTI)

A complete discussion of tree-level flavor-changing effects in the Randall-Sundrum (RS) model with brane-localized Higgs sector and bulk gauge and matter fields is presented. The bulk equations of motion for the gauge and fermion fields, supplemented by boundary conditions taking into account the couplings to the Higgs sector, are solved exactly. For gauge fields the Kaluza-Klein (KK) decomposition is performed in a covariant R_xi gauge. For fermions the mixing between different generations is included in a completely general way. The hierarchies observed in the fermion spectrum and the quark mixing matrix are explained naturally in terms of anarchic five-dimensional Yukawa matrices and wave-function overlap integrals. Detailed studies of the flavor-changing couplings of the Higgs boson and of gauge bosons and their KK excitations are performed, including in particular the couplings of the standard W and Z bosons. A careful analysis of electroweak precision observables including the S and T parameters and the Zbb couplings shows that the simplest RS model containing only Standard Model particles and their KK excitations is consistent with all experimental bounds for a KK scale as low as a few TeV, if one allows for a heavy Higgs boson and/or for an ultra-violet cutoff below the Planck scale. The study of flavor-changing effects includes analyses of the non-unitarity of the quark mixing matrix, anomalous right-handed couplings of the W bosons, tree-level flavor-changing neutral current couplings of the Z and Higgs bosons, the rare decays t-->c(u)+Z and t-->c(u)+h, and the flavor mixing among KK fermions. The results obtained in this work form the basis for general calculations of flavor-changing processes in the RS model and its extensions.

S. Casagrande; F. Goertz; U. Haisch; M. Neubert; T. Pfoh

2008-07-31T23:59:59.000Z

156

UNITED STATES ENVIRONMENTAL PROTECTION AGENCY WASHINGTON, D.C. 20460  

E-Print Network (OSTI)

bg p(wj|0) P; p=1 ; wiPp p(wi|Y, hp, p) = ; wj bg p(xr j |X 0 )p(aj|A 0 ) P; p=1 ; wiPp p(xr i |Y, hp

157

Structure and growth morphology of an archetypal system for organic epitaxy: PTCDA on Ag,,111... B. Krause,1  

E-Print Network (OSTI)

.10.Aj, 61.66.Hq I. INTRODUCTION Over the last few years, organic semiconductors have ex- periencedStructure and growth morphology of an archetypal system for organic epitaxy: PTCDA on Ag,,111... B; revised manuscript received 24 July 2002; published 10 December 2002 The planar organic molecule 3

Schreiber, Frank

158

Bias Temperature Instability Analysis, Monitoring and Mitigation for  

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Prof.dr. G.Q. Zhang Technische Universiteit Delft, The Netherlands Dr.ir. M. Meijer NXP Semiconductor, Eindhoven, The Netherlands Prof.dr. A.J. van der Veen Technische Universiteit Delft, reservelid This thesis. Published and distributed by: Seyab Email: m.seyab.khan@gmail.com ISBN: 978-94-6186-209-9 Subject headings

159

Spectroscopy on Metal-Halide Lamps under Varying Gravity Conditions  

E-Print Network (OSTI)

orange street lighting), which has a slightly lower discharge conversion efficiency, but the 589 nm line. They are mainly used for applications where a high light output is desired; examples are shop lighting, street. Haverlag Copromotor: dr.ir. W.W. Stoffels Copyright c 2008 by A.J. Flikweert This research was financially

Eindhoven, Technische Universiteit

160

Duality in spaces of finite linear combinations of atoms  

E-Print Network (OSTI)

in Hp . In other words, Hp and Fp are both quotients of the space of "formal series" of (p, )-atoms understand the space Fp we prove now the following. Proposition. Given any sequence of (p, ) atoms aj and anyDuality in spaces of finite linear combinations of atoms Fulvio Ricci and Joan Verdera Abstract

Verdera, Joan

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161

Duality in spaces of finite linear combinations of atoms  

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are both quotients of the space of "formal series" of (p, )-atoms with p coefficients, but the equivalence understand the space Fp we prove now the following. Proposition. Given any sequence of (p, ) atoms aj and anyDuality in spaces of finite linear combinations of atoms Fulvio Ricci and Joan Verdera Abstract

Autònoma de Barcelona, Universitat

162

WhyFord Escort's success was easy to forecast.  

E-Print Network (OSTI)

were heated to 57.5°C for 10 min in a PTC200 thermocycler (MJ Re- search), rapidly cooled to 4°C and conformational studies of [Orn-10, Nle-13]-S-peptide. J Am Chem Soc 91:492­496. Ruettinger RT, Wen LP, Fulco AJ

Queitsch, Christine

163

Contents  

Science Conference Proceedings (OSTI)

... rela- tionship AkFk;j = AjFj;k, to convert the above ... A1a 1aT4 1a + energy from upper wall z }| { ... to use for the solution of linear systems (even for 2 2 ...

2000-02-25T23:59:59.000Z

164

and Early Jurassic sediments, and  

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, H.V., Marsh, J.S. & Cox, K.G., 1984. The Karoo igneous province: An introduction, in Petrogenesis of the Volcanic Rocks of the Karoo Province, pp. 1­26, ed. Erlank, A.J., Geological Society of South Africa­1866. Hargraves, R.B., Rehacek, J. & Hooper, P.R., 1997. Palaeomagnetism of the Karoo igneous rocks in Southern

Olsen, Paul E.

165

Proceedings of ICRC 2001: 1 c Copernicus Gesellschaft 2001 A Search for Bursts of TeV Gamma Rays with Milagro  

E-Print Network (OSTI)

Abstract. The Very High Energy (VHE, E > 100 GeV) component of Gamma-Ray Bursts (GRBs) remains unmea- suredV Gamma Rays with Milagro A.J. Smith for the Milagro Collaboration University of Maryland, College Park close enough to observe at TeV energies remains unknown. The Milagro Gamma Ray Obser- vatory began

California at Santa Cruz, University of

166

Coherent control of pump-probe signals of helical structures by adaptive pulse polarizations  

E-Print Network (OSTI)

excitons in multidimensional spectroscopy.11­14 Shaping the polarization state of the electric field-Stokes Raman spectroscopy CARS .18 Multipolar- ization optimal control two-dimensional 2D and three with a sequence of laser pulses Fig. 1 , whose electric field is given by E r, = j=1 4 Aj -¯j exp ikjr - i¯ j -¯j

Mukamel, Shaul

167

J U N E 2 0 1 2 Storms make the oak grow deeper roots.  

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in Concrete AJ Weller Corp 5346 Mary Murimi Youth4Health Outreach Project HRSA 150,000 Niel Crews CAREER Allouche Optimization of Geopolymer Formulation in View of Workability & Strength Development Hansen Pipe 5,000 12-235 Allouche, Erez Patil/Mainardi Testing of Geopolymer Binder in Rocket Plume Environments

Selmic, Sandra

168

D E C E M B E R 2 0 1 1 Chance favors only the prepared mind.  

E-Print Network (OSTI)

in Concrete AJ Weller Corp 5346 Mary Murimi Youth4Health Outreach Project HRSA 150,000 Niel Crews CAREER Allouche Optimization of Geopolymer Formulation in View of Workability & Strength Development Hansen Pipe 5,000 12-235 Allouche, Erez Patil/Mainardi Testing of Geopolymer Binder in Rocket Plume Environments

Selmic, Sandra

169

At Home With The Homeless By Ian Jamison  

E-Print Network (OSTI)

line, where I met volunteering veterans Tony and A.J. They easily accepted me into their group after stopping to thank us for our work. They'll be back--the diners and the volunteers both. As one on the street. For others, it's a place to get the resources they need to get their lives back on track

Wisconsin at Madison, University of

170

David W. Dewhirst A Bibliography  

E-Print Network (OSTI)

.F.OD. & Newberry, A.J. Impressions of the Pic du Midi Observatory Research vol. 2, 492- (1949) G.C. Smith: D.W. Dewhirst Metallography and mechanical properties of internally oxidized alloys The Journal of the Iron and Steel Institute vol. 169, 221-227 (1951) D...

Hurn, Mark David

171

Unbinned  

Science Conference Proceedings (OSTI)

Unbinned. A, B, C, D, E, F, G, H, I, J, K, L, M, N, O, P, Q, R, S, T, U, V, W, X, Y, Z, AA, AB, AC, AD, AE, AF, AG, AH, AI, AJ, AK, AL, AM, AN, AO, AP, AQ. ...

2008-07-03T23:59:59.000Z

172

Molecular mechanisms of traumatic brain injury; the missing link in management  

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JAR: The association between APOE ?4, age and outcome after head injury: a prospective cohort study. Brain 2005, 128:2556-2561. 46. Fine EM, Delis DC, Wetter SR, Jacobson MW, Jak AJ, McDonald CR, Braga JC, Thal LJ, Salmon DP, Bondi MW: Cognitive...

Veenith, Tonny; Goon, Serena H; Burnstein, Rowan M

2009-02-02T23:59:59.000Z

173

Residential Care Facilities  

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All material appearing in this report is in the public domain and may be reproduced or copied without permission; citation as to source, however, is appreciated. Suggested citation Moss AJ, Harris-Kojetin LD, Sengupta M, et al. Design and operation of the

unknown authors

2011-01-01T23:59:59.000Z

174

Geothermal Energy Utilization via Effective Design of Ground-Coupled  

E-Print Network (OSTI)

Geothermal Energy Utilization via Effective Design of Ground-Coupled Heat Exchange System Charlie of Tennessee Knoxville, TN 37996 05/18/2010 #12;Geothermal energy is the most recent research subject AJ and I ­ Reactive Flow Film Cooling in Turbine · Renewable Energy ­ Geothermal Energy Heat Exchange System ­ Bio

Tennessee, University of

175

Interactive Arrangement of Botanical L-System Joanna L. Power1  

E-Print Network (OSTI)

models of plants, capableof simulating their growth and interaction with theenvironment[4, 10Interactive Arrangement of Botanical L-System Models Joanna L. Power1 , A.J. Bernheim Brush1 Abstract In this paper, we explore the problem of interactively mauipulating plant models without

Prusinkiewicz, Przemyslaw

176

A finite-element approximation of a quasi-magnetostatic 3D eddy current model by fractional-step A-? scheme  

Science Conference Proceedings (OSTI)

We propose in this paper a fractional-step A-@j scheme for a quasi-magnetostatic 3D eddy current model by means of finite-element approximations. Bounds for continuous and discrete error in finite time are given, and it is verified that provided the ... Keywords: Eddy current problem, Error estimates, Finite-element approximation, Fractional-step A-? scheme

Changfeng Ma

2004-02-01T23:59:59.000Z

177

Spring 2011 College of ArChiteCture  

E-Print Network (OSTI)

as a postdoctoral researcher. In addition, thanks to Detlev Majewski from the German Weather Service DWD and countless dinner meetings. Thank you, Dave, Laurie, A.J. and Heather for your friendship, companionship and fun evenings. Dave, I hope I was a good housemate. And of course special thanks to you, Rainer

Heller, Barbara

178

THE UNIVERSITY OF CHICAGO HIGHLY-SENSITIVE AND EFFICIENT INFRARED SPECTROSCOPY OF  

E-Print Network (OSTI)

as a postdoctoral researcher. In addition, thanks to Detlev Majewski from the German Weather Service DWD and countless dinner meetings. Thank you, Dave, Laurie, A.J. and Heather for your friendship, companionship and fun evenings. Dave, I hope I was a good housemate. And of course special thanks to you, Rainer

Lindsay, C. Michael

179

THE NEWSLETTER OF THE UNIVERSITY OF WISCONSIN -MADISON  

E-Print Network (OSTI)

as a postdoctoral researcher. In addition, thanks to Detlev Majewski from the German Weather Service DWD and countless dinner meetings. Thank you, Dave, Laurie, A.J. and Heather for your friendship, companionship and fun evenings. Dave, I hope I was a good housemate. And of course special thanks to you, Rainer

Sheridan, Jennifer

180

The Illustrated University of Arizona  

E-Print Network (OSTI)

as a postdoctoral researcher. In addition, thanks to Detlev Majewski from the German Weather Service DWD and countless dinner meetings. Thank you, Dave, Laurie, A.J. and Heather for your friendship, companionship and fun evenings. Dave, I hope I was a good housemate. And of course special thanks to you, Rainer

Watkins, Joseph C.

Note: This page contains sample records for the topic "aj podkaminer kk" from the National Library of EnergyBeta (NLEBeta).
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181

BBeesstt PPrraaccttiicceess ffoorr tthhee CCoolllleeccttiioonn ooff LLoonngglliinnee DDaattaa ttoo FFaacciilliittaattee RReesseeaarrcchh aanndd  

E-Print Network (OSTI)

as a postdoctoral researcher. In addition, thanks to Detlev Majewski from the German Weather Service DWD and countless dinner meetings. Thank you, Dave, Laurie, A.J. and Heather for your friendship, companionship and fun evenings. Dave, I hope I was a good housemate. And of course special thanks to you, Rainer

182

Page I N S I D E U V A May 18, 007 Carol Wood, assistant vice president  

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as a postdoctoral researcher. In addition, thanks to Detlev Majewski from the German Weather Service DWD and countless dinner meetings. Thank you, Dave, Laurie, A.J. and Heather for your friendship, companionship and fun evenings. Dave, I hope I was a good housemate. And of course special thanks to you, Rainer

Whittle, Mark

183

Environmental Toxicology and Chemistry, Vol. 21, No. 12, pp. 26312639, 2002 Printed in the USA  

E-Print Network (OSTI)

bodies with large stagnation regions and internal flow, turbines, pumps, etc. Hence, we shall introduce sin(`) +B sin(OE)) \\Gamma jAj(1 \\Gamma cos(`)) \\Gamma jBj(1 \\Gamma cos(OE)) and so G(?; ?) = \\Gamma2j (three) dimen­ sions. This dramatically increases both the computing time and storage of the code

Alvarez, Pedro J.

184

Ortho n+1 - Optimization Online  

E-Print Network (OSTI)

Oct 12, 2012 ... [22] K.R. Fowler, J.P. Reese, C.E. Kees, J.E. Dennis Jr., C.T. Kelley, C.T. Miller, C. Audet, A.J.. Booker, G. Couture, R.W. Darwin, M.W. Farthing,...

185

Talanta 69 (2006) 232238 Simultaneous detection of Escherichia coli O157:H7, Salmonella spp. and  

E-Print Network (OSTI)

-liposomal nanovesicles Chien-Sheng Chen, Richard A. Durst Department of Food Science and Technology, Cornell University assay for the detection of Escherichia coli O157:H7 [C.-S. Chen, A.J. Baeumner, R.A. Durst, Talanta 67: +1 315 787 2397. E-mail address: rad2@cornell.edu (R.A. Durst). Salmonella is estimated

Chen, Chien-Sheng

186

Sheet1  

Science Conference Proceedings (OSTI)

Sheet1. A, B, C, D, E, F, G, H, I, J, K, L, M, N, O, P, Q, R, S, T, U, V, W, X, Y, Z, AA, AB, AC, AD, AE, AF, AG, AH, AI, AJ, AK, AL, AM, AN, AO, AP, AQ, AR ...

2010-06-01T23:59:59.000Z

187

Proceedings of the 17th Biennial Waste Processing Conference WASTE SEPARATION-  

E-Print Network (OSTI)

Proceedings of the 17th Biennial Waste Processing Conference ASME 1996 WASTE SEPARATION- DOES IT INFLUENCE MUNICIPAL WASTE COMBUSTOR EMISSIONS? A. John Chandler A.J. Chandler & Associates Ltd. Willowdale that MSW incinerator emissions show significant variations because of the heterogeneous nature of the waste

Columbia University

188

J. Mol. Biol. (1996) 259, 819827 Selection of Chymotrypsin Inhibitors from a  

E-Print Network (OSTI)

were heated to 57.5°C for 10 min in a PTC200 thermocycler (MJ Re- search), rapidly cooled to 4°C and conformational studies of [Orn-10, Nle-13]-S-peptide. J Am Chem Soc 91:492­496. Ruettinger RT, Wen LP, Fulco AJ

Leatherbarrow, Robin J.

189

SOLID WASTE PREPROCESSING: THE RETURN OF AN ALTERNATIVE TO MASS BURN  

E-Print Network (OSTI)

(al OPF = Dedicated prepared Fuel, RDFz Refuse Derived Fuel (b) Designed for co-firing with wood chips (c) Designed for co-firing with coal (d) Existing coal-fired boilers extensively modified Power There are several reasons why many project sponsors are selecting preprocessing: (aJ Co-firing with other fuels. (b

Columbia University

190

LLNL-JRNL-402318 Hyperfine quenching of the 2s2p 3  

E-Print Network (OSTI)

LLNL-JRNL-402318 Hyperfine quenching of the 2s2p 3 P0 state of berylliumlike ions K. T. Cheng, the measured value. PACS numbers: 31.30.Gs, 32.10.Fn, 31.15.aj, 31.15.am ktcheng@llnl.gov chen7@llnl

Johnson, Walter R.

191

Post-prandial reactive hypoglycaemia and diarrhea caused by idiopathic accelerated gastric emptying: a case report  

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beta- cell function. Obes Surg 2010, 20(8):1110-1116. 9. Playford RJ, Domin J, Beacham J, Parmar KB, Tatemoto K, Bloom SR, Calam J: Preliminary report: role of peptide YY in defence against diarrhoea. Lancet 1990, 335(8705):1555-1557. 10. Scheen AJ...

Middleton, Stephen J; Balan, Kottekkattu

2011-05-13T23:59:59.000Z

192

Jill Ann Marshall The University of Texas, Austin  

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, R., Weaver, E.C. & Gans, D.M. (2010). Women and men of the Manhattan Project. The Physics Teacher, A.J. & Martin, H.T. (2010). Pre-service teachers' conceptions and enactments of Project Based Journal, 19(1), 45-76. Marshall, J.A., Pine, B. & Taylor, W.W.L (2007). INSPIRE: A VLF radio project

Lightsey, Glenn

193

Observation of ?_{cJ} decaying into the p\\bar{p}K^{+}K^{-} final state  

E-Print Network (OSTI)

First measurements of the decays of the three $\\chi_{cJ}$ states to $p\\bar{p}K^{+}K^{-}$ final states are presented. Intermediate $\\phi\\to K^{+}K^{-}$ and $\\Lambda(1520)\\to pK^{-}$ resonance states are observed, and branching fractions for $\\chi_{cJ}\\to \\bar{p}K^{+}\\Lambda(1520)$, $\\Lambda(1520) \\bar{\\Lambda}(1520)$, and $\\phi p\\bar{p}$ are reported. We also measure branching fractions for direct $\\chi_{cJ}\\to p\\bar{p} K^{+}K^{-}$ decays. These are first observations of $\\chi_{cJ}$ decays to unstable baryon resonances and provide useful information about the $\\chi_{cJ}$ states. The experiment uses samples of $\\chi_{cJ}$ mesons produced via radiative transitions from 106 million $\\psi^{\\prime}$ mesons collected in the BESIII detector at the BEPCII $e^+e^-$ collider.

BESIII Collaboration

2011-03-14T23:59:59.000Z

194

Measurement of Interference between Electromagnetic and Strong Amplitudes in psi(2S) Decays to Two Pseudoscalar Mesons  

E-Print Network (OSTI)

Using a sample of 3.08 million psi(2S) decays collected at sqrt{s} = 3.686 GeV with the CLEO detector at the Cornell Electron Storage Ring, we have measured the branching fractions for psi(2S) decays to pseudoscalar pairs pi+pi-, K+K-, and KsKl. We obtain B(psi(2S) -> pi+pi-) K+K-) = (6.3 +- 0.6(stat) +- 0.3(syst)) x 10^{-5}, and B(psi(2S) -> KsKl) = (5.8 +- 0.8(stat) +- 0.4(syst)) x 10^{-5}. The branching fractions allow extraction of the relative phase Delta = (95 +- 15) degrees and strength ratio R = (2.5 +- 0.4) of the three-gluon and one-photon amplitudes for these modes.

S. Dobbs; CLEO Collaboration

2006-03-09T23:59:59.000Z

195

Supersymmetric dyonic black holes in Kaluza-Klein theory  

E-Print Network (OSTI)

We study supersymmetric, four-dimensional (4-d), Abelian charged black holes (BH's) arising in (4+n)-d (1 \\le n \\le 7) Kaluza-Klein (KK) theories. Such solutions, which satisfy supersymmetric Killing spinor equations (formally satisfied for any n) and saturate the corresponding Bogomol'nyi bounds, can be obtained if and only if the isometry group of the internal space is broken down to the U(1)_E \\times U(1)_M gauge group; they correspond to dyonic BH's with electric Q and magnetic P charges associated with {\\it different} U(1) factors. The internal metric of such configurations is diagonal with (n-2) internal radii constant, while the remaining two radii (associated with the respective electric and magnetic U(1) gauge fields) and the 4-d part of the metric turn out to be independent of n, i.e., solutions are effectively those of supersymmetric 4-d BH's of 6-d KK theory. For Q \

Cvetic, M; Cveti, Mirjam; Youm, Donam

1994-01-01T23:59:59.000Z

196

All the four dimensional static, spherically symmetric solutions of abelian Kaluza-Klein theory  

E-Print Network (OSTI)

The explicit form for all the four dimensional, static, spherically symmetric solutions in (4+n)-d Abelian Kaluza-Klein (KK) theory is presented by performing two SO(1,1) boosts on the non-extreme U(1)_M \\times U(1)_E KK black hole (BH) and supplementing it by SO(n)/SO(n-2) transformations. The solutions are parameterized by the mass M, Taub-Nut charge a, n electric \\vec{\\cal Q} and n magnetic \\vec{\\cal P} charges. Non-extreme BH's (with zero Taub-NUT charge) have either the Reissner-Nordstr\\" om or Schwarzschild global space-time, nonzero entropy and temperature. Extreme (supersymmetric) BH's satisfy \\vec{\\cal P} \\cdot \\vec{\\cal Q} = 0 and have a null or naked singularity, with S [T_H] reaching the zero lower [finite or infinite upper] bound.

Cvetic, M; Cveti, Mirjam; Youm, Donam

1995-01-01T23:59:59.000Z

197

National Environmental Policy Act (NEPA) Compliance Guide Volume 1 - General NEPA References  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

54 Federa 54 Federa l Register / Vol. 49, No. 247 / Friday, December 21, 1984 / Rules and Regulations Commission . Room TMNOK=45 Fifth St., kK= Was>-. DC. OQVJM N K= xOMOF=OTOJTSUK= Small Business Administration Direc1or . Office of Busines1 Loans, Small Business Administration . Room UI= 1441 i= St .. NW . Wash . . D .C. OMNSM l K=EOMOF=S S= Susquehanna River Basin Com1nission Executive Director, Susquehanna River

198

PROPRIETARY MATERIAL. 2011 The McGraw-Hill Companies, Inc. Limited distribution permitted only to teachers and educators for course preparation. If you are a student using this Manual, you are using it without permission.  

E-Print Network (OSTI)

PROPRIETARY MATERIAL. © 2011 The McGraw-Hill Companies, Inc. Limited distribution permitted only it without permission. 8-49 50 kPa 100C 140 m/s STEAM 80 m/s 6 MPa 600C 5 MW 8-61 Steam expands in a turbine of the surroundings is given to be 25C. Properties From the steam tables (Tables A-4 through A-6) KkJ/kg1693.7 kJ/kg8

Bahrami, Majid

199

PROPRIETARY MATERIAL. 2011 The McGraw-Hill Companies, Inc. Limited distribution permitted only to teachers and educators for course preparation. If you are a student using this Manual, you are using it without permission.  

E-Print Network (OSTI)

PROPRIETARY MATERIAL. © 2011 The McGraw-Hill Companies, Inc. Limited distribution permitted only it without permission. 8-65 8-77 Steam is accelerated in an adiabatic nozzle. The exit velocity of the steam of steam at the inlet and the exit of the nozzle are (Tables A-4 through A-6) KkJ/kg8000.6 kJ/kg4.3411 C500

Bahrami, Majid

200

The earth matter effects in neutrino oscillation experiments from Tokai to Kamioka and Korea  

E-Print Network (OSTI)

We study the earth matter effects in the Tokai-to-Kamioka-and-Korea experiment (T2KK), which is a proposed extension of the T2K (Tokai-to-Kamioka) neutrino oscillation experiment between J-PARC at Tokai and Super-Kamiokande (SK) in Kamioka, where an additional detector is placed in Korea along the same neutrino beam line.By using recent geophysical measurements, we examine the earth matter effects on the oscillation probabilities at Kamioka and Korea. The average matter density along the Tokai-to-Kamioka baseline is found to be 2.6 g/cm^3, and that for the Tokai-to-Korea baseline is 2.85, 2.98, and 3.05 g/cm^3 for the baseline length of L = 1000, 1100, and 1200 km, respectively. The uncertainty of the average density is about 6%, which is determined by the uncertainty in the correlation between the accurately measured sound velocity and the matter density. The effect of the matter density distribution along the baseline is studied by using the step function approximation and the Fourier analysis. We find that the nu_mu -> nu_e oscillation probability is dictated mainly by the average matter density, with small but non-negligible contribution from the real part of the first Fourier mode. We also find that the sensitivity of the T2KK experiment on the neutrino mass hierarchy does not improve significantly by reducing the matter density error from 6% to 3%, since the measurement is limited by statistics for the minimum scenario of T2KK with SK at Kamioka anda 100 kt detector in Korea considered in this report. The sensitivity of the T2KK experiment on the neutrino mass hierarchy improves significantly by splitting the total beam time into neutrino and anti-neutrino runs, because the matter effect term contributes to the oscillation amplitudes with the opposite sign.

Kaoru Hagiwara; Naotoshi Okamura; Ken-ichi Senda

2011-07-29T23:59:59.000Z

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201

$WW?/Z$ production in the Randall-Sundrum model at LHC and CLIC  

E-Print Network (OSTI)

We study the $W^+W^-\\gamma(Z)$ productions at both the CERN Large Hadron Collider (LHC) and the Compact Linear Collider (CLIC) in the framework of the Randall-Sundrum (RS) model. The impacts of the virtual RS Kaluza-Klein (KK) graviton on these processes are studied and compared with the standard model (SM) background. We present the integrated and differential cross sections in both the RS model and the SM. The results show that the relative RS discrepancies at the CLIC differ from those at the LHC, particularly in the transverse momentum and rapidity distributions. We also find that the RS signature performance, as a result of the resonance character of the RS KK-graviton spectrum, is distinctively unlike that in the large extra dimensions model. We conclude that the CLIC with unprecedented precision and high center-of-mass energy has a potential advantage over the LHC in exploring the effects of the RS KK graviton on the $W^+W^-\\gamma(Z)$ production processes.

Li Xiao-Zhou; Ma Wen-Gan; Zhang Ren-You; Guo Lei

2013-03-10T23:59:59.000Z

202

Observation of Tau Decays with Two Neutral Kaons  

E-Print Network (OSTI)

We report on the observation of the decay \\Gamma ! K 0 K 0 \\Gamma in 3.11 fb \\Gamma1 of data taken with the CLEO II detector at the Cornell Electron Storage Ring. Both K 0 mesons are detected through their decays via K S ! + \\Gamma . Preliminary results on the branching fraction and on the resonant substructure are presented. In particular, we find B( \\Gamma ! K 0 K 0 \\Gamma ) = 0:083 \\Sigma 0:017 \\Sigma 0:017 %. We also comment on the sensitivity of the KK invariant mass spectrum to a non-zero tau-neutrino mass. Permanent address: University of Hawaii at Manoa y Permanent address: INP, Novosibirsk, Russia 2 I. INTRODUCTION Tau lepton decays of the type \\Gamma ! [KK] \\Gamma have been known to exist [1] for nearly a decade. However, due to the small decay width and difficulties associated with identifying kaons, little information is presently available for these decays. In this paper, we report on the observation of KK decays where both...

Balest Cho Ford; Ichep Ref; Gsl Cleo Conf; K. Cho; K. Lingel; M. Lohner; P. Rankin

1994-01-01T23:59:59.000Z

203

Higgs Boson Mass and Electroweak-Gravity Hierarchy from Dynamical Gauge-Higgs Unification in the Warped Spacetime  

E-Print Network (OSTI)

Dynamical electroweak symmetry breaking by the Hosotani mechanism in the Randall-Sundrum warped spacetime is examined, relations among the W-boson mass (m_W), the Kaluza-Klein mass scale (M_{KK}), and the Higgs boson mass (m_H) being derived. It is shown that M_{KK}/m_W = (2 pi kR)^{1/2} (pi/theta_W) and m_H /m_W = 0.058 kR (pi/theta_W), where k^2, R, and theta_W are the curvature and size of the extra-dimensional space and the Wilson line phase determined dynamically. For typical values kR = 12 and theta_W = (0.2 to 0.4) pi, one finds that M_{KK} = (1.7 to 3.5) TeV, k = (1.3 to 2.6) x 10^{19} GeV, and m_H = (140 to 280) GeV.

Yutaka Hosotani; Mitsuru Mabe

2005-03-02T23:59:59.000Z

204

Probing Brane-World Scenarios with Vacuum Refraction of Light Using Gamma-Ray Bursts  

E-Print Network (OSTI)

We argue that in fat brane-world scenarios the light propagating in vacuum will, because of massive ``Kaluza-Klein'' (KK) excitations, experience a refraction. The motion of a photon inside a fat brane can be decomposed in the longitudinal and transverse directions with respect to the surface of the brane. Since the light observable propagation is related only with the longitudinal motion, the observed speed of light depends on the value of the momentum transverse fraction contributing as the massive KK excitations. This is directly connected with the energy of the particles emitting the light, and hence with the frequency of the light itself. Using recent results on the arrival times of radiation of different energies from the measurements of gamma-ray bursters with known redshifts, we establish the limit M>620 TeV on the inverse thickness of the brane, and thus on the masses of the KK excitations. This limit exceeds by at least one order of magnitude the typical energy scale currently in use to characterize brane phenomena in the realm of future colliders.

Merab Gogberashvili; Alexander S. Sakharov; Edward K. G. Sarkisyan

2006-05-30T23:59:59.000Z

205

Final Technical Report  

SciTech Connect

Final Technical Report for U.S. Department of Energy Grant No. DE-FG02-09ER55005 Nonlinear FLR Effects in Reduced Fluid Models Alain J. Brizard, Saint Michael??s College The above-mentioned DoE grant was used to support research activities by the PI during a sabbatical leave from Saint Michael??s College in 2009. The major focus of the work was the role played by guiding-center and gyrocenter (linear and nonlinear) polarization and magnetization effects in understanding transport processes in turbulent magnetized plasmas. The theoretical tools used for this work include Lie-transform perturbation methods and Lagrangian (variational) methods developed by the PI in previous work. The present final technical report lists (I) the peer-reviewed publications that were written based on work funded by the Grant; (II) invited and contributed conference presentations during the period funded by the Grant; and (III) seminars presented during the period funded by the Grant. I. Peer-reviewed Publications A.J. Brizard and N. Tronko, 2011, Exact momentum conservation for the gyrokinetic Vlasov- Poisson equations, Physics of Plasmas 18 , 082307:1-14 [http://dx.doi.org/10.1063/1.3625554 ]. J. Decker, Y. Peysson, A.J. Brizard, and F.-X. Duthoit, 2010, Orbit-averaged guiding-center Fokker-Planck operator for numerical applications, Physics of Plasmas 17, 112513:1-12 [http://dx.doi.org/10.1063/1.3519514]. A.J. Brizard, 2010, Noether derivation of exact conservation laws for dissipationless reduced fluid models, Physics of Plasmas 17, 112503:1-8 [http://dx.doi.org/10.1063/1.3515303]. F.-X. Duthoit, A.J. Brizard, Y. Peysson, and J. Decker, 2010, Perturbation analysis of trapped particle dynamics in axisymmetric dipole geometry, Physics of Plasmas 17, 102903:1-9 [http://dx.doi.org/10.1063/1.3486554]. A.J. Brizard, 2010, Exact energy conservation laws for full and truncated nonlinear gyrokinetic equations, Physics of Plasmas 17, 042303:1-11 [http://dx.doi.org/10.1063/1.3374428]. A.J. Brizard, J. Decker, Y. Peysson, and F.-X. Duthoit, 2009, Orbit-averaged guiding-center Fokker-Planck operator, Physics of Plasmas 16, 102304:1-9[http://dx.doi.org/10.1063/1.3249627]. A.J. Brizard, 2009, Variational Principles for Reduced Plasma Physics, Journal of Physics: Conference Series 169, 012003 [http://dx.doi.org/10.1088/1742-6596/169/1/012003]. II. Invited and Contributed Conference Presentations A.J. Brizard and N. Tronko, Momentum conservation law for the gyrokinetic Vlasov-Poisson equations, 53rd Annual Meeting of the APS Division of Plasma Physics, Salt Lake City (Utah), November 14-18, 2011. A.J. Brizard, P.J. Morrison, C. Chandre, and E. Tassi, On the road to the Hamiltonian formulation of gyrokinetic theory, 52nd Annual Meeting of the APS Division of Plasma Physics, Chicago (Illinois), November 8-12, 2010. F.-X. Duthoit, A.J. Brizard, Y. Peysson, and J. Decker, Lie-transform perturbation analysis of trapped-particle dynamics in axisymmetric dipole geometry, 2010 International Sherwood Fusion Theory Conference, Seattle (Washington), April 19-21, 2010. N. Tronko and A.J. Brizard, Gyrokinetic momentum conservation law, 2010 International Sherwood Fusion Theory Conference, Seattle (Washington), April 19-21, 2010. C. Chandre and A.J. Brizard, Hamiltonian formulation of reduced Vlasov-Maxwell equations, 50th Annual Meeting of the APS Division of Plasma Physics, Dallas (Texas), November 17-21, 2008. A.J. Brizard, Nonlinear FLR effects in reduced fluid models, Invited Presentation at 11th Easter Plasma Meeting, Torino (Italy), April 15-17, 2009. III. Seminars Reduced Fokker-Planck operators for advanced plasma simulations, seminar given at CEA Cadarache (France), May 25, 2009. Ray phase-space methods in linear mode conversion, seminar given at CPT Luminy (France), April 1, 2009. Old and new methods in gyrokinetic theory, seminar given at CEA Cadarache (France), March 20, 2009. Hamiltonian theory of adiabatic motion of relativistic charged particles, seminar given at CPT Luminy (France), March 11, 2009. Noether method for fluids a

Alain J. Brizard

2009-12-31T23:59:59.000Z

206

Mechanisms for Enhanced Supercurrent Across Meandered Grain Boundaries in High-Temperature Superconductors  

Science Conference Proceedings (OSTI)

It has been well established that the critical current density J{sub c} across grain boundaries (GBs) in high-temperature superconductors decreases exponentially with misorientation angle {theta} beyond {approx}2-3 degrees. This rapid decrease is due to a suppression of the superconducting order parameter at the grain boundary, giving rise to weakly pinned Abrikosov-Josephson (AJ) vortices. Here we show that if the GB plane meanders, this exponential dependence no longer holds, permitting greatly enhanced J{sub c} values: up to six times at 0 T and four times at 1 T at {theta}{approx}4-6 degrees. This enhancement is due to an increase in the current-carrying cross section of the GBs and the appearance of short AJ vortex segments in the GB plane, confined by the interaction with strongly pinned Abrikosov (A) vortices in the grains.

Feldmann, D. M. [University of Wisconsin, Madison; Holesinger, T. G. [Los Alamos National Laboratory (LANL); Feenstra, Roeland [ORNL; Cantoni, Claudia [ORNL; Zhang, W. [American Superconductor Corporation, Westborough, MA; Rupich, Marty [American Superconductor Corporation, Westborough, MA; Li, Xiaoping [American Superconductor Corporation, Westborough, MA; Durrell, J. H. [University of Cambridge; Gurevich, A. [Florida State University; Larbalestier, D. C. [University of Wisconsin, Madison

2007-01-01T23:59:59.000Z

207

An adaptive grid refinement strategy for the simulation of negative streamers  

Science Conference Proceedings (OSTI)

The evolution of negative streamers during electric breakdown of a non-attaching gas can be described by a two-fluid model for electrons and positive ions. It consists of continuity equations for the charged particles including drift, diffusion and reaction ... Keywords: 52.25.Aj, 52.35.Mw, 52.65.Kj, 52.80.Mj, Adaptive grid refinements, Elliptic-parabolic system, Finite volumes, Negative streamers, Pulled front

C. Montijn; W. Hundsdorfer; U. Ebert

2006-12-01T23:59:59.000Z

208

John Reif and Urmi Majumder Department of Computer Science  

E-Print Network (OSTI)

: Likelihood and rate of a state transition Rate of Polymerization Rate formulation [Rose et al, 2001] -29 Current state of Rule i-1 Next state of Rule i-1 n rules transition table Reference: M Hagiya, M Arita, D Whiplash PCR Machine(Contd) aj * = bi * State S5 ai bi ai+1bi+1ai-1bi-1 anbn a1b1 ajbj Transition from

Reif, John H.

209

Unfurling of the band 4.1, ezrin, radixin, moesin (FERM) domain of the merlin tumor suppressor  

Science Conference Proceedings (OSTI)

The merlin-1 tumor suppressor is encoded by the Neurofibromatosis-2 (Nf2) gene and loss-of-function Nf2 mutations lead to nervous system tumors in man and to several tumor types in mice. Merlin is an ERM (ezrin, radixin, moesin) family cytoskeletal protein that interacts with other ERM proteins and with components of cell-cell adherens junctions (AJs). Merlin stabilizes the links of AJs to the actin cytoskeleton. Thus, its loss destabilizes AJs, promoting cell migration and invasion, which in Nf2{sup +/-} mice leads to highly metastatic tumors. Paradoxically, the 'closed' conformation of merlin-1, where its N-terminal four-point-one, ezrin, radixin, moesin (FERM) domain binds to its C-terminal tail domain, directs its tumor suppressor functions. Here we report the crystal structure of the human merlin-1 head domain when crystallized in the presence of its tail domain. Remarkably, unlike other ERM head-tail interactions, this structure suggests that binding of the tail provokes dimerization and dynamic movement and unfurling of the F2 motif of the FERM domain. We conclude the 'closed' tumor suppressor conformer of merlin-1 is in fact an 'open' dimer whose functions are disabled by Nf2 mutations that disrupt this architecture.

Yogesha, S.D.; Sharff, Andrew J.; Giovannini, Marco; Bricogne, Gerard; Izard, Tina (House Ear); (Globel Phasing); (Scripps)

2012-03-26T23:59:59.000Z

210

THE SPECTROSCOPIC CLASSIFICATION AND EXPLOSION PROPERTIES OF SN 2009nz ASSOCIATED WITH GRB 091127 AT z = 0.490  

SciTech Connect

We present spectroscopic observations of GRB 091127 (z = 0.490) at the peak of the putative associated supernova SN 2009nz. Subtracting a late-time spectrum of the host galaxy, we isolate the contribution of SN 2009nz and uncover broad features typical of nearby gamma-ray-burst-supernovae (GRB-SNe). This establishes unambiguously that GRB 091127 was accompanied by a broad-lined Type Ic SN, and links a cosmological long burst with a standard energy release (E{sub {gamma},iso} Almost-Equal-To 1.1 Multiplication-Sign 10{sup 52} erg) to a massive star progenitor. The spectrum of SN 2009nz closely resembles that of SN 2006aj, with SN 2003dh also providing an acceptable match, but has significantly narrower features than SNe 1998bw and 2010bh, indicative of a lower expansion velocity. The photospheric velocity inferred from the Si II {lambda}6355 absorption feature, v{sub ph} Almost-Equal-To 17, 000 km s{sup -1}, is indeed closer to that of SNe 2006aj and 2003dh than to the other GRB-SNe. Combining the measured velocity with the light curve peak brightness and width, we estimate the following nominal (maximal) explosion parameters: M{sub Ni} Almost-Equal-To 0.35 (0.6) M{sub Sun }, E{sub K} Almost-Equal-To 2.3 Multiplication-Sign 10{sup 51} (8.4 Multiplication-Sign 10{sup 51}) erg, and M{sub ej} Almost-Equal-To 1.4 (3.5) M{sub Sun }, similar to those of SN 2006aj. These properties indicate that SN 2009nz follows a trend of lower M{sub Ni} for GRB-SNe with lower E{sub K} and M{sub ej}. Equally important, since GRB 091127 is a typical cosmological burst, the similarity of SN 2009nz to SN 2006aj either casts doubt on the claim that XRF 060218/SN 2006aj was powered by a neutron star or indicates that the nature of the central engine is encoded in the SN properties but not in the prompt emission. Future spectra of GRB-SNe at z {approx}> 0.3 will shed light on the full dispersion of SN properties for standard long GRBs, on the relation between SNe associated with sub-energetic and standard GRBs, and on a potential dispersion in the associated SN types.

Berger, E.; Chornock, R.; Holmes, T. R.; Foley, R. J. [Harvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA 02138 (United States); Cucchiara, A. [Lawrence Berkeley National Laboratory, M.S. 50-F, 1 Cyclotron Road, Berkeley, CA 94720 (United States); Wolf, C.; Podsiadlowski, Ph. [Department of Astrophysics, Denys Wilkinson Building, University of Oxford, Keble Road, Oxford OX1 3RH (United Kingdom); Fox, D. B. [Department of Astronomy and Astrophysics, Pennsylvania State University, 525 Davey Laboratory, University Park, PA 16802 (United States); Roth, K. C. [Gemini Observatory, 670 N. Aohoku Place Hilo, HI 96720 (United States)

2011-12-20T23:59:59.000Z

211

Searching for an Attractive Force in Holographic Nuclear Physics  

E-Print Network (OSTI)

We are looking for a holographic explanation of nuclear forces, especially the attractive forces. Recently, the repulsive hard core of a nucleon-nucleon potential was obtained in the Sakai-Sugimoto model, and we show that a generalized version of that model -- with an asymmetric configuration of the flavor D8 branes -- also has an attractive potential. While the repulsive potential stems from the Chern-Simons interactions of the U(2) flavor gauge fields in 5D, the attractive potential is due to a coupling of the gauge fields to a scalar field describing fluctuations of the flavor branes' geometry. At intermediate distances r between baryons -- smaller than R_KK=O(1)/M_{omega meson} but larger than the radius rho=R_KK/sqrt('t Hooft coupling) of the instanton at the core of a baryon -- both the attractive and the repulsive potentials behave as 1/r^2, but the attractive potential is weaker: Depending on the geometry of the flavor D8 branes, the ratio C=-V_attr/V_rep ranges from 0 to 1/9. The 5D scalar fields also affect the isovector tensor and spin-spin forces, and the overall effect is similar to the isoscalar central forces: V(r)->(1-C)*V(r). At longer ranges $r\\gtrsim R_{\\rm KK}$, we find that the attractive potential decays faster than the repulsive potential, so the net potential is always repulsive. This unrealistic behavior may be peculiar to the Sakai-Sugimoto-like models, or it could be a general problem of the large N_c limit inherent in holography.

Vadim S. Kaplunovsky; Jacob Sonnenschein

2010-03-12T23:59:59.000Z

212

Limits on Large Extra Dimensions Based on Observations of Neutron Stars with the Fermi-LAT  

Science Conference Proceedings (OSTI)

We present limits for the compactification scale in the theory of Large Extra Dimensions (LED) proposed by Arkani-Hamed, Dimopoulos, and Dvali. We use 11 months of data from the Fermi Large Area Telescope (Fermi-LAT) to set gamma ray flux limits for 6 gamma-ray faint neutron stars (NS). To set limits on LED we use the model of Hannestad and Raffelt (HR) that calculates the Kaluza-Klein (KK) graviton production in supernova cores and the large fraction subsequently gravitationally bound around the resulting NS. The predicted decay of the bound KK gravitons to {gamma}{gamma} should contribute to the flux from NSs. Considering 2 to 7 extra dimensions of the same size in the context of the HR model, we use Monte Carlo techniques to calculate the expected differential flux of gamma-rays arising from these KK gravitons, including the effects of the age of the NS, graviton orbit, and absorption of gamma-rays in the magnetosphere of the NS. We compare our Monte Carlo-based differential flux to the experimental differential flux using maximum likelihood techniques to obtain our limits on LED. Our limits are more restrictive than past EGRET-based optimistic limits that do not include these important corrections. Additionally, our limits are more stringent than LHC based limits for 3 or fewer LED, and comparable for 4 LED. We conclude that if the effective Planck scale is around a TeV, then for 2 or 3 LED the compactification topology must be more complicated than a torus.

Ajello, M.; /SLAC /KIPAC, Menlo Park; Baldini, L.; /INFN, Pisa; Barbiellini, G.; /INFN, Trieste /Trieste U.; Bastieri, D.; /INFN, Padua /Padua U.; Bechtol, K.; /SLAC /KIPAC, Menlo Park; Bellazzini, R.; /INFN, Pisa; Berenji, B.; /SLAC /KIPAC, Menlo Park; Bloom, E.D.; /SLAC /KIPAC, Menlo Park; Bonamente, E.; /INFN, Perugia /Perugia U.; Borgland, A.W.; /SLAC /KIPAC, Menlo Park; Bregeon, J.; /INFN, Pisa; Brigida, M.; /Bari Polytechnic /INFN, Bari; Bruel, P.; /Ecole Polytechnique; Buehler, R.; /SLAC /KIPAC, Menlo Park; Buson, S.; /INFN, Padua /Padua U.; Caliandro, G.A.; /CSIC, Catalunya; Cameron, R.A.; /SLAC /KIPAC, Menlo Park; Caraveo, P.A.; /Brera Observ.; Casandjian, J.M.; /AIM, Saclay; Cecchi, C.; /INFN, Perugia /Perugia U.; Charles, E.; /SLAC /KIPAC, Menlo Park /Naval Research Lab, Wash., D.C. /SLAC /KIPAC, Menlo Park /ASDC, Frascati /Perugia U. /SLAC /KIPAC, Menlo Park /Montpellier U. /Stockholm U. /Stockholm U., OKC /Royal Swedish Acad. Sci. /ASDC, Frascati /Udine U. /INFN, Trieste /Bari Polytechnic /INFN, Bari /Naval Research Lab, Wash., D.C. /SLAC /KIPAC, Menlo Park /SLAC /KIPAC, Menlo Park /SLAC /KIPAC, Menlo Park /SLAC /KIPAC, Menlo Park /Bari Polytechnic /INFN, Bari /Ecole Polytechnique /NASA, Goddard /Hiroshima U. /Bari Polytechnic /INFN, Bari /INFN, Bari /ASDC, Frascati /INFN, Perugia /Perugia U. /Bari Polytechnic /INFN, Bari /Bari Polytechnic /INFN, Bari /Bologna Observ. /SLAC /KIPAC, Menlo Park /SLAC /KIPAC, Menlo Park /SLAC /KIPAC, Menlo Park /AIM, Saclay /Alabama U., Huntsville /INFN, Padua; /more authors..

2012-08-17T23:59:59.000Z

213

MEMORANDUM TO: FILE SUBJECT:  

Office of Legacy Management (LM)

SUBJECT: SUBJECT: -Li&$diM ---------- -2' ~~EI: ---- --------:------- CITY: %-k&&k/ -------------------------- ST&T& oi+ OWN_EM_SL Past : ---------------------A-- Current:___--~---____------_______ Owner contacted q yes anno; if yes, date contacted ------------- TYPE OF OPERATION ~_------_~~-----_ tJ Research & Development 0 Production scale tssting Cl Pilot Scale 0 Bench Scale Process 0 Theoretical Studies 0 Sample & Analysis 0 Production 0 Disposal/Storage @ ' Facility Type 0 Manufacturing a University 0 Research Organization -------- 0 Prime' 0 Subcontractor 0 Purchase Order q Other information (i.e., cost + fixed fee, unit price, time 81 material, etc) ------- ~_-----_------~-------~~~~~~ Contract/Purchase Order # ----------------------------

214

CITY, Aa.  

Office of Legacy Management (LM)

c I..:.. : - I) c I..:.. : - I) ",A;' ,: /iL;L#d -___-___-_--~~~--~-- CITY, Aa. ;:.--w-e- ____ )kk- ________ STAT%d$ ___ Current: -----------------------__- if Yee, date contacted __ TYPE OF OPERATION ~~---~~--~---__-- IJ Research & Development I n Facility Type I 0 Production scale testing a Pilat scale 0 Bench Scale Process i Theoretical Studies Sample SC Analysis * ~~oy~~~"4 Io.*l--t r-J Manufacturing 0 University 0 Research Organization 0 Government Sponsored Facility 0 Other ---------r----l------ U Disposal/Storage q Prime 0 0 Subcontract& Other information (i.e., cost + fixed fee, unit price, 0 Purchase Order time & material, qtc) -------------__-____________ Contract/Purchase Order # ~~-~~~~-~~--~~---_-______________ OWNERSHiP: !

215

Can the beta decay of neutral kaons be observed?  

E-Print Network (OSTI)

The rate of the beta decay of neutral kaons is calculated within the meson dominance approach taking into account the relation between the KK\\rho and \\pi\\pi\\rho coupling constants which follows from the vector meson dominance in electromagnetic interactions and isospin symmetry. The decay rate transforms into the following branching fraction summed over the charge states indicated: B(K0L -> K+- e-+ nu)=(2.53+-0.10)x10^{-9}. The error is dominated by our estimate of isospin violating effects. Experimental aspects of such a measurement are discussed.

Peter Lichard; Julia Thompson

2000-04-25T23:59:59.000Z

216

Qualification Tests of 474 Photomultiplier Tubes for the Inner Detector of the Double Chooz Experiment  

E-Print Network (OSTI)

The hemispherical 10" photomultiplier tube (PMT) R7081 from Hamamatsu Photonics K.K. (HPK) is used in various experiments in particle and astroparticle physics. We describe the test and calibration of 474 PMTs for the reactor antineutrino experiment Double Chooz. The unique test setup at Max-Planck-Institut f\\"ur Kernphysik Heidelberg (MPIK) allows one to calibrate 30 PMTs simultaneously and to characterize the single photo electron response, transit time spread, linear behaviour and saturation effects, photon detection efficiency and high voltage calibration.

C. Bauer; E. Borger; R. Hofacker; K. Jnner; F. Kaether; C. Langbrandtner; M. Lindner; S. Lucht; M. Reissfelder; S. Schnert; A. Stken; C. Wiebusch

2011-04-05T23:59:59.000Z

217

Plasmon-graviton conversion in a magnetic field in TeV-scale gravity  

E-Print Network (OSTI)

Kaluza-Klein (KK) gravitons emission rates due to plasmon-graviton conversion in magnetic field are computed within the ADD model of TeV-scale gravity. Plasma is described in the kinetic approach as the system of charged particles and Maxwell field both confined on the brane. Interaction with multidimensional gravity living in the bulk with $n$ compact extra dimensions is introduced within the linearized theory. Plasma collective effects enter through the two-point correlation function of the fluctuations of the energy-momentum tensor. The estimate for magnetic stars is presented leading to the lower limit of the D-dimensional Plank mass.

Melkumova, E Yu

2011-01-01T23:59:59.000Z

218

Chiral approach to Phi Radiative Decays  

E-Print Network (OSTI)

(980) and f0(980) according to ? ? f0, a0 + ? and hence are generally considered to provide valuable information about the puzzling light scalar mesons[2] of low energy QCD. The theoretical analysis of this type of decay was initiated by Achasov and Ivanchenko... [3] and followed up by many others [4]. The starting point was the observation that the ? meson decays about 50 per cent of the time into K+K?. Since this final state can easily annihilate to produce either an f0 or a0 together with an emitted photon...

Black, Deirdre; Harada, Masayasu; Shechter, Joseph

2006-01-01T23:59:59.000Z

219

Insulator-to-Conducting Transition in Dense Fluid Helium  

Science Conference Proceedings (OSTI)

By combining diamond-anvil-cell and laser-driven shock wave techniques, we produced dense He samples up to 1.5 g/cm{sup 3} at temperatures reaching 60 kK. Optical measurements of reflectivity and temperature show that electronic conduction in He at these conditions is temperature-activated (semiconducting). A fit to the data suggests that the mobility gap closes with increasing density, and that hot dense He becomes metallic above {approx}1.9 g/cm{sup 3}. These data provide a benchmark to test models that describe He ionization at conditions found in astrophysical objects, such as cold white dwarf atmospheres.

Celliers, P. M.; Eggert, J. H.; Hicks, D. G.; Collins, G. W. [Lawrence Livermore National Laboratory, Post Office Box 808, Livermore, California 94551 (United States); Loubeyre, P.; Brygoo, S. [CEA/DAM/DIF, 91297 Arpajon. France (France); McWilliams, R. S. [Institute for Shock Physics, Washington State University, Pullman, Washington 99164 (United States); University of California, Berkeley, California 94720 (United States); Boehly, T. R. [Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623 (United States); Jeanloz, R. [University of California, Berkeley, California 94720 (United States)

2010-05-07T23:59:59.000Z

220

En vue de l'obtention du DOCTORAT DE L'UNIVERSIT DE TOULOUSEDOCTORAT DE L'UNIVERSIT DE TOULOUSE  

E-Print Network (OSTI)

entièrement définie par sa densité de transition a(k, l) = p (X2 = l |X1 = k) et sa loi a priori (k) = p (X1 K , k . Induction (1 n a(k, l) fl(yn+1) n+1(l), k . (2.10) pour les A = {a(k, l)}k,l et les paramètres = {k}k des K lois paramétriques d'attache aux données {f(y; k

Paris-Sud XI, Université de

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221

p-barp-Annihilation processes in the tree approximation of SU(3) chiral effective theory  

Science Conference Proceedings (OSTI)

The p-barp-annihilation reactions p-barp {yields} {eta}{eta} {eta} and p-barp {yields} {eta}KK-bar at rest are considered in the tree approximation in the framework of SU(3) chiral effective theory at leading order. The calculated branchings are compared with the data. The results for neutral ({eta}{eta}{eta}, K{sup 0}K-bar{sup 0}{sub {eta}}) and charged (K{sup +}K{sup -}{sub {eta}}) channels are essentially different.

Tarasov, V. E.; Kudryavtsev, A. E., E-mail: kudryavt@itep.ru; Romanov, A. I.; Weinberg, V. M. [Institute of Theoretical and Experimental Physics (Russian Federation)

2012-12-15T23:59:59.000Z

222

Dictionary of LHC Signatures  

E-Print Network (OSTI)

We report on a plan to establish a "Dictionary of LHC Signatures", an initiative that started at the WHEPPX workshop in January 2008. This study aims towards the strategy on distinguishing of 3 classes of dark matter motivated scenarios such as R-parity conserved supersymmetry, Little Higgs models with T-parity conservation and Universal Extra Dimensions with KK-parity for generic cases of their realization in wide range of the model space. Discriminating signatures are tabulated and will need a further detailed analysis.

A. Belyaev; I. A. Christidi; A. De Roeck; R. M. Godbole; B. Mellado; A. Nyffeler; C. Petridou; D. P. Roy

2008-06-17T23:59:59.000Z

223

Holographic Gauge Mediation  

SciTech Connect

We discuss gravitational backgrounds where supersymmetry is broken at the end of a warped throat, and the SUSY-breaking is transmitted to the Standard Model via gauginos which live in (part of) the bulk of the throat geometry. We find that the leading effect arises from splittings of certain 'messenger mesons,' which are adjoint KK-modes of the D-branes supporting the Standard Model gauge group. This picture is a gravity dual of a strongly coupled field theory where SUSY is broken in a hidden sector and transmitted to the Standard Model via a relative of semi-direct gauge mediation.

Benini, Francesco; /Princeton U.; Dymarsky, Anatoly; /Stanford U., ITP; Franco, Sebastian; /Santa Barbara, KITP; Kachru, Shamit; Simic, Dusan; /Stanford U., ITP /SLAC; Verlinde, Herman; /Princeton, Inst. Advanced Study

2009-06-19T23:59:59.000Z

224

Characterisation of microRNA expression in post-natal mouse mammary gland development  

E-Print Network (OSTI)

, Inmaculada Spiteri1, Konstantina Karagavriilidou1, Christine J Watson6, Simon Tavar2,5, Eric A Miska*4 and Carlos Caldas*1 Address: 1Breast Cancer Functional Genomics Laboratory, Cancer Research UK Cambridge Research Institute and Department of Oncology... .spiteri@cancer.org.uk; Konstantina Karagavriilidou - kk406@cam.ac.uk; Christine J Watson - cjw53@mole.bio.cam.ac.uk; Simon Tavar - simon.tavare@cancer.org.uk; Eric A Miska* - e.miska@gurdon.cam.ac.uk; Carlos Caldas* - carlos.caldas@cancer.org.uk * Corresponding authors Equal...

Avril-Sassen, Stefanie; Goldstein, Leonard D; Stingl, John; Blenkiron, Cherie; Le Quesne, John; Spiteri, Inmaculada; Karagavriilidou, Konstantina; Watson, Christine J; Tavare, Simon; Miska, Eric A; Caldas, Carlos

2009-11-20T23:59:59.000Z

225

Black Rings, Boosted Strings and Gregory-Laflamme  

E-Print Network (OSTI)

We investigate the Gregory-Laflamme instability for black strings carrying KK-momentum along the internal direction. We demonstrate a simple kinematical relation between the thresholds of the classical instability for the boosted and static black strings. We also find that Sorkin's critical dimension depends on the internal velocity and in fact disappears for sufficiently large boosts. Our analysis implies the existence of an analogous instability for the five-dimensional black ring of Emparan and Reall. We also use our results for boosted black strings to construct a simple model of the black ring and argue that such rings exist in any number of space-time dimensions.

J. L. Hovdebo; R. C. Myers

2006-01-12T23:59:59.000Z

226

Transient radiation-induced absorption in the materials for a GSGG laser  

Science Conference Proceedings (OSTI)

Materials used in the optical elements of a 1,061 m GSGG (gadolinium scandium gallium garnet) laser have been tested for transient radiation-induced absorption. The transient radiation-induced absorption in KK1, Schott S7005 and S7010, and M382 glasses have been determined for discrete wavelengths in the range 440--750 nm. Also, the transient radiation-induced absorption in {open_quotes}pure{close_quotes} and MgO doped LiNbO{sub 3} has been measured at 1,061 nm. Mathematical expressions composed of exponentials are fitted to the data.

Brannon, P.J.

1993-11-01T23:59:59.000Z

227

Ultra-large distance modification of gravity from Lorentz symmetry breaking at the Planck scale  

E-Print Network (OSTI)

We present an extension of the Randall--Sundrum model in which, due to spontaneous Lorentz symmetry breaking, graviton mixes with bulk vector fields and becomes quasilocalized. The masses of KK modes comprising the four-dimensional graviton are naturally exponentially small. This allows to push the Lorentz breaking scale to as high as a few tenth of the Planck mass. The model does not contain ghosts or tachyons and does not exhibit the van Dam--Veltman--Zakharov discontinuity. The gravitational attraction between static point masses becomes gradually weaker with increasing of separation and gets replaced by repulsion (antigravity) at exponentially large distances.

D. S. Gorbunov; S. M. Sibiryakov

2005-06-08T23:59:59.000Z

228

Wrapping up the bad news - HIV assembly and release  

E-Print Network (OSTI)

form a filamentous structure in vitro [104,127,128] and in vivo [126,129], it was proposed that the progression of this filament would lead to thinning of the plasma membrane and to a cer- tain degree the energy accumulated would favor fission [145... mediates the functional link between human immunodeficiency virus type 1 RNA nuclear export elements and the assembly competency of Gag in murine cells. J Virol 2009, 83:85258535. 40. Mouland AJ, Mercier J, Luo M, Bernier L, DesGroseillers L, Cohen EA...

Meng, Bo; Lever, Andrew ML

2013-01-10T23:59:59.000Z

229

Breaking the energy-bandwidth limit of electro-optic modulators: theory and a device proposal  

E-Print Network (OSTI)

In this paper, we quantitatively analyzed the trade-off between energy per bit for switching and modulation bandwidth of classical electro-optic modulators. A formally simple energy-bandwidth limit (Eq. 10) is derived for electro-optic modulators based on intra-cavity index modulation. To overcome this limit, we propose a dual cavity modulator device which uses a coupling modulation scheme operating at high bandwidth (> 200 GHz) not limited by cavity photon lifetime and simultaneously features an ultra-low switching energy of 0.26 aJ, representing over three orders of magnitude energy consumption reduction compared to state-of-the-art electro-optic modulators.

Lin, Hongtao; Liu, Jifeng; Zhang, Lin; Michel, Jurgen; Hu, Juejun

2013-01-01T23:59:59.000Z

230

Performing statistical analyses on quantitative data in Taverna workflows: an example using R and maxdBrowse to identify differentially-expressed genes from microarray data  

E-Print Network (OSTI)

and hypothesis-driven science in the post-genomic era. Bioessays 2004, 26:99-105. 4. Hayes A, Castrillo JI, Oliver SG, Brass A, Zeef LAH: Transcript Analysis: A Microarray Approach. In Methods in Microbiology. Yeast Gene Analysis Volume 36. Edited by... , Senger M, Wilkinson MD: BioMoby extensions to the Taverna workflow management and enactment software. BMC Bioinformatics 2006, 7:523. 17. Hancock D, Wilson M, Velarde G, Morrison N, Hayes A, Hulme H, Wood AJ, Nashar K, Kell DB, Brass A: maxdLoad2 and maxd...

Li, Peter; Castrillo, Juan I; Velarde, Giles; Wassink, Ingo; Soiland-Reyes, Stian; Owen, Stuart; Withers, David; Oinn, Tom; Pocock, Matthew R; Goble, Carole A; Oliver, Stephen G; Kell, Douglas B

2008-08-07T23:59:59.000Z

231

Fibrillar beta-amyloid peptide Abeta1-40activates microglial proliferation via stimulating TNF-alpha release and H2O2derived from NADPH oxidase: a cell culture study  

E-Print Network (OSTI)

, Palwinder K Mander1, Anna Tickler2, Martyn Sharpe3 and Guy C Brown*1 Address: 1Department of Biochemistry, University of Cambridge, Tennis Court Road, Cambridge CB2 1QW, UK, 2Cavendish laboratory, University of Cambridge, Cambridge CB3 0HE, UK and 3... Biochemistry and Molecular Biology Department, Biochemistry Building, Michigan State University, East Lansing, MI 48824-1319, USA Email: Aiste Jekabsone - aj293@mole.bio.cam.ac.uk; Palwinder K Mander - palwinder.k.mander@gsk.com; Anna Tickler - annatickler...

Jekabsone, Aiste; Mander, Palwinder K; Tickler, Anna; Sharpe, Martyn; Brown, Guy C

2006-09-07T23:59:59.000Z

232

Origins of chromosomal rearrangement hotspots in the human genome: evidence from the AZFadeletion hotspots  

E-Print Network (OSTI)

-Bromage, P. Tempst , T. Honjo, and L.D. Vales. 1994. The recombination signal sequence-binding protein RBP-2N functions as a transcriptional repressor. Mol. Cell. Biol. 14: 3310-3319. Frisse, L., R.R. Hudson, A. Batoszewicz, J.D. Wall, J. Donfack, and A... Tree: analyzing and visualizing evolutionary data. Bioinformatics 14: 68-73. Jeffreys, A.J. and C.A. May. 2004. Intense and highly localized gene conversion activity in human meiotic crossover hot spots. Nature Genet. 36: 152-256. Jobling, M.A. and C. Tyler...

Hurles, Matthew E; Willey, David; Matthews, Lucy; Hussain, Syed Sufyan

2004-07-14T23:59:59.000Z

233

Analysis of polymorphisms in 16 genes in type 1 diabetes that have been associated with other immune-mediated diseases  

E-Print Network (OSTI)

, Whittaker J, Meeks J, Powell RJ, Isenberg DA, Walport MJ, Vyse TJ: Polymorphism at the C-reactive protein locus influences gene expression and predisposes to systemic lupus ery- thematosus. Hum Mol Genet 2004, 13:137-147. 15. Szalai AJ, McCrory MA, Cooper... , Chow C, Cohen A, Lan- gelier D, Lapointe G, Gaudet D, Faith J, Branco N, Bull SB, McLeod RS, Griffiths AM, Bitton A, Greenberg GR, Lander ES, Siminovitch KA, Hudson TJ: Genetic variation in the 5q31 cytokine gene clus- ter confers susceptibility...

Smyth, Deborah J; Howson, Joanna M M; Payne, Felicity; Maier, Lisa M; Bailey, Rebecca; Holland, Kieran; Lowe, Christopher E; Cooper, Jason D; Hulme, John S; Vella, Adrian; Dalhman, Ingrid; Lam, Alex C; Nutland, Sarah; Walker, Neil M; Twells, Rebecca C J; Todd, John A

2006-03-06T23:59:59.000Z

234

Relationship between the tissue-specificity of mouse gene expression and the evolutionary origin and function of the proteins  

E-Print Network (OSTI)

to few tissues [9]. In germ cells, where lactate is a preferred energy source [10], we observe specific expression of Ldhc (testis-specific expression). The expression of Ldhc is an example of a function occurring in the ancestral unicellular cell... , Schaffer AA, Zhang J, Zhang Z, Miller W, Lip- man DJ: Gapped BLAST and PSI-BLAST: a new generation of protein database search programs. Nucleic Acids Res 1997, 25:3389-3402. 25. Janssen P, Enright AJ, Audit B, Cases I, Goldovsky L, Harte N, Kunin V...

Freilich, Shiri; Massingham, Tim; Bhattacharyya, Sumit; Ponstingl, Hannes; Lyons, Paul A; Freeman, Tom C; Thornton, Janet M

2005-06-29T23:59:59.000Z

235

Vista and Pemex in LAB deal  

SciTech Connect

Vista Chemical (Houston) and Petroleos Mexicanos (Pemex; Mexico City) have firmed up their long-negotiated plans for Pemex to supply feedstock for a linear alkylbenzene (LAB) plant that Vista will build in Mexico (CW, Sept. 16, 1992 p. 8). Specifically, the two companies have signed an agreement of understanding to pursue negotiations and finalize agreements. The plant would cost $250 million, produce 260 million-330 million lbs/year of LAB, and create about 200 permanent jobs. Final agreements, including a site selection, are expected to be completed by midyear. Vista expects startup in 1996, and is considering forming aj oint venture with a Mexican partner.

Morris, G.D.L.

1993-01-20T23:59:59.000Z

236

Newsfront 7-13 April 2008, Issue 61  

E-Print Network (OSTI)

Kathmandu l 7-13 Apr, 2008 l # 61 l Price Rs. 25 www.newsfront.com.np Ph:- Shop 5011685, Factory: 5555459 New outlet in Lainchour also Nir aj Sa pko ta nf correspondent Amidst hopes and doubts, an estimated 17.6 million voters are set to go... to the poll this week on April 10 as world watches with vigilant eyes. At least 1000 international observers led by former US President Jimmy Carter will be observing the poll as fears rise that they may not be free from violence, intimidation and rigging...

Ghimire, Yubaraj

237

Nonlinear effects in kinetic resolutions  

E-Print Network (OSTI)

The impact of nonlinear effects in the asymmetric catalysis of kinetic resolutions is analyzed. It is found with minimal assumptions that the kinetics of homocompetitive reactions should apply generally to kinetic resolutions involving partially resolved catalysts, and this is supported by experimental observations with the Jacobsen hydrolytic kinetic resolution (HKR) of epoxides. The criterion for a nonlinear effect in asymmetric catalysis--a nonlinear correlation between the enantiomeric excess in a choral ligand and the product enantiomeric excess obtained from a reaction--is examined. The nonlinear effect idea is found to be generalizable to kinetic resolutions and other reactions by replacing consideration of the product enantiomeric excess with the quantity (k[]/k[]-1)/(k[]/k[]+1), a differential kinetic enantiomeric enhancement (DKEE). A nonlinear effect may then be defined by a nonlinear correlation between the DKEE and the chiral ligand enantiomeric excess. The application of these ideas to previously reported kinetic resolutions of sulfoxides and to nonlinear effects in the Jacobsen HKR is described. Relatively small nonlinear effects in kinetic resolutions are sufficient to obtain large asymmetric amplifications. A catalyst modification in the Jacobsen HKR also allows for the development of a novel recyclable system for the iterative enhancement of optical activity.

Johnson, Derrell W.

1999-01-01T23:59:59.000Z

238

Diphoton and Z photon Decays of Higgs Boson in Gauge-Higgs Unification: A Snowmass white paper  

E-Print Network (OSTI)

In the context of gauge-Higgs unification scenario in a 5-dimensional flat spacetime, we investigate Higgs boson production via gluon fusion and its diphoton and Z gamma decay modes at the LHC. We show that the signal strength of the Higgs diphoton decay mode observed at ATLAS (and CMS), which is considerably larger than the Standard Model expectation, can be explained by a simple gauge-Higgs unification model with color-singlet bulk fermions to which a half-periodic boundary condition is assigned. The bulk fermions with mass at the TeV scale also play a crucial role in reproducing the observed Higgs boson mass of around 125 GeV. One naturally expects that the KK modes also contribute to the effective H-Z-gamma coupling. However, we show a very specific and general prediction of the gauge-Higgs unification scenario that KK-mode contributions to the H-Z-gamma coupling do not exist at the 1-loop level. If the excess of the Higgs to diphoton decay mode persists, its correlation with the Higgs to Z photon decay mode can be a clue to distinguish scenarios beyond the SM, providing a significant improvement of the sensitivity for the Higgs boson signals in the future.

Nobuhito Maru; Nobuchika Okada

2013-07-31T23:59:59.000Z

239

KO-Homology and Type I String Theory.  

E-Print Network (OSTI)

We study the classification of D-branes and Ramond-Ramond fields in Type I string theory by developing a geometric description of KO-homology. We define an analytic version of KO-homology using KK-theory of real C*-algebras, and construct explicitly the isomorphism between geometric and analytic KO-homology. The construction involves recasting the Cl(n)-index theorem and a certain geometric invariant into a homological framework which is used, along with a definition of the real Chern character in KO-homology, to derive cohomological index formulas. We show that this invariant also naturally assigns torsion charges to non-BPS states in Type I string theory, in the construction of classes of D-branes in terms of topological KO-cycles. The formalism naturally captures the coupling of Ramond-Ramond fields to background D-branes which cancel global anomalies in the string theory path integral. We show that this is related to a physical interpretation of bivariant KK-theory in terms of decay processes on spacetime-filling branes. We also provide a construction of the holonomies of Ramond-Ramond fields in Type II string theory in terms of topological K-chains.

240

Inclusive hadron production and two particle correlations in e/sup +/e/sup -/ annihilation at 29 GeV center-of-mass energy  

SciTech Connect

We have studied hadron production in e/sup +/e/sup -/ annihilation at 29 GeV center-of-mass energy using the PEP-4 Time Projection Chamber Detector. The inclusive cross sections and mean multiplicities for ..pi../sup + -/, K/sup + -/ and (p + anti p) production have been measured using ionization energy loss to separate particle species. We find on average 10.7 +- 0.6 ..pi../sup + -/, 1.35 +- .13 K/sup + -/ and 0.60 +- 0.08 (p + anti p) per multihadron event. The differential cross section is well described by a number of Monte Carlo hadronization models. In addition, we have observed correlations in rapidity space for identified pions and kaons. Short-range KK correlations provide evidence for local flavor compensation during hadronization. Long-range ..pi pi.. and KK correlations indicate that the initial partons carry flavor. We also observe significant long-range ..pi..K correlations as a result of heavy quark decays. 85 references, 67 figures, 11 tables.

Shapiro, M.

1984-12-01T23:59:59.000Z

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241

Higgs phenomenology in warped extra dimensions with a fourth generation  

Science Conference Proceedings (OSTI)

We study a warped extra-dimension scenario where the standard model fields lie in the bulk, with the addition of a fourth family of fermions. We concentrate on the flavor structure of the Higgs couplings with fermions in the flavor anarchy ansatz. Even without a fourth family, these couplings will be generically misaligned with respect to the standard model fermion mass matrices. The presence of the fourth family typically enhances the misalignment effects and we show that one should expect them to be highly nonsymmetrical in the (34) intergenerational mixing. The radiative corrections from the new fermions and their flavor-violating couplings to the Higgs affect negligibly known experimental precision measurements such as the oblique parameters and Z{yields}bb or Z{yields}{mu}{sup +}{mu}{sup -}. On the other hand, {Delta}F=1, 2 processes, mediated by tree-level Higgs exchange, as well as radiative corrections to b{yields}s{gamma} and {mu}{yields}e{gamma} put some generic pressure on the allowed size of the flavor-violating couplings. But more importantly, these couplings will alter the Higgs decay patterns as well as those of the new fermions, and produce very interesting new signals associated to Higgs phenomenology in high energy colliders. These signals might become very important indirect signals for these type of models as they would be present even when the KK mass scale is high and no heavy KK particle is discovered.

Frank, Mariana; Korutlu, Beste; Toharia, Manuel [Department of Physics, Concordia University, 7141 Sherbrooke St. West, Montreal Quebec, H4B 1R6 (Canada)

2011-10-01T23:59:59.000Z

242

Search for Large Extra Dimensions Based on Observations of Neutron Stars with the Fermi-LAT  

SciTech Connect

Large extra dimensions (LED) have been proposed to account for the apparent weakness of gravitation. These theories also indicate that the postulated massive Kaluza-Klein (KK) gravitons may be produced by nucleon-nucleon bremsstrahlung in the course of core collapse of supernovae. Hannestad and Raffelt have predicted energy spectra of gamma ray emission from the decay of KK gravitons trapped by the gravity of the remnant neutron stars (NS). These and other authors have used EGRET data on NS to obtain stringent limits on LED. Fermi-LAT is observing radio pulsar positions obtained from radio and x-ray catalogs. NS with certain characteristics are unlikely emitter of gamma rays, and emit in radio and perhaps x-rays. This talk will focus on the blind analysis we plan to perform, which has been developed using the 1st 2 months of all sky data and Monte Carlo simulations, to obtain limits on LED based on about 1 year of Fermi-LAT data. Preliminary limits from this analysis using these first 2 months of data will be also be discussed.

Berenji, Bijan; /Stanford U., Appl. Phys. Dept. /SLAC

2012-09-19T23:59:59.000Z

243

rwj10d4.tmp  

NLE Websites -- All DOE Office Websites (Extended Search)

o/2AL\AJ[-&2 o/2AL\AJ[-&2 DOE/ER-0713 (Part 1) Part 1, Overview and Progress \ UNITED STATES DEPARTMENT OF ENERU OFFICEOF ENERGY RESEARCH C!!!iiF OFFICE OF BIOLOWALAND ENVIRONMENTAL RESEARCH DOE/ER-0713 (Part1) HUMAN CENOME PROWAM REPORT Part 1, Overview and Progress Date Published: November 1997 Prepared for the U.S. Department of Energy Office of Energy Research Office of Biological and Environmental Research Germantown, MD 20874-1290 Prepared by the Human Genome Management Information System Oak Ridge National Laboratory Oak Ridge, TN 37830-6480 managed by Lockheed Martin Energy ResearchCorporation for the U.S. Department of Energy Under Contract DE-AC05-960R22464 I 1 I I I I MASTER I q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q q .,. ,> '. ,. ,- ., ,,. . ....~,,. -.7 r.. - ,. 1983 LANL and LLNL begin production of

244

Effect of Surface Charges on the Rates of Intermolecular Electron-Transfer  

NLE Websites -- All DOE Office Websites (Extended Search)

Surface Charges on the Rates of Intermolecular Electron-Transfer Surface Charges on the Rates of Intermolecular Electron-Transfer between de Novo Designed Metalloproteins A. Y. Kornilova, J. F. Wishart, and M. Y. Ogawa Biochem. 40, 12186-12192 (2001) [Find paper at ACS Publications] Abstract: A de novo designed coiled-coil metalloprotein was prepared that uses electrostatic interactions to control both its conformational and bimolecular electron-transfer properties. The title protein exists as a coiled-coil heterodimer of the [Ru(trpy)(bpy)-KK(37-mer)] and [Ru(NH3)5-EE(37-mer)] polypeptides which is formed by interhelix electrostatic attractions. Circular dichroism studies show that the electrostatic heterodimer has Kd = 0.19 ± 0.03 µM and is 96% helical at high concentrations. Intercomplex electron-transfer reactions were studied

245

A Partial-Wave Analysis of Centrally Produced Two-Pseudoscalar Final States in pp Reactions at COMPASS  

E-Print Network (OSTI)

COMPASS is a fixed-target experiment at CERN SPS which focused on light-quark hadron spectroscopy during the data taking in 2008 and 2009. A world-leading data set was collected with a 190GeV/c hadron beam impinging on a liquid hydrogen target in order to study the central production of glueball candidates. In this report, we motivate double-Pomeron exchange as a relevant production process for mesons without valence quark content. We select a centrally produced sample from the COMPASS data set recorded with a proton beam and introduce a decomposition into partial waves. Particular attention is paid to inherent mathematical ambiguities in the amplitude analysis of two-pseudoscalar final states. Furthermore, we show a simple parametrisation for the centrally produced K+K- system which can describe the mass dependence of the fit results with sensible Breit-Wigner parameters.

A. Austregesilo for the COMPASS Collaboration

2013-06-28T23:59:59.000Z

246

Unstable Hadrons in Hot Hadron Gas in Laboratory and in the Early Universe  

E-Print Network (OSTI)

We study kinetic master equations for chemical reactions involving the formation and the natural decay of unstable particles in a thermal bath. We consider the decay channel of one into two particles, and the inverse process, fusion of two thermal particles into one. We present the master equations the evolution of the density of the unstable particles in the early Universe. We obtain the thermal invariant reaction rate using as an input the free space (vacuum) decay time and show the medium quantum effects on $\\pi+\\pi \\leftrightarrow \\rho$ reaction relaxation time. As another laboratory example we describe the $K+K \\leftrightarrow \\phi$ process in thermal hadronic gas in heavy ions collisions. A particularly interesting application of our formalism is the $\\pi^{0}\\leftrightarrow \\gamma +\\gamma$ process in the early Universe. We also explore the physics of $\\pi^{\\pm}$ and $\\mu^{\\pm}$ freeze-out in the Universe.

Kuznetsova, Inga

2010-01-01T23:59:59.000Z

247

Unstable Hadrons in Hot Hadron Gas in Laboratory and in the Early Universe  

E-Print Network (OSTI)

We study kinetic master equations for chemical reactions involving the formation and the natural decay of unstable particles in a thermal bath. We consider the decay channel of one into two particles, and the inverse process, fusion of two thermal particles into one. We present the master equations the evolution of the density of the unstable particles in the early Universe. We obtain the thermal invariant reaction rate using as an input the free space (vacuum) decay time and show the medium quantum effects on $\\pi+\\pi \\leftrightarrow \\rho$ reaction relaxation time. As another laboratory example we describe the $K+K \\leftrightarrow \\phi$ process in thermal hadronic gas in heavy-ion collisions. A particularly interesting application of our formalism is the $\\pi^{0}\\leftrightarrow \\gamma +\\gamma$ process in the early Universe. We also explore the physics of $\\pi^{\\pm}$ and $\\mu^{\\pm}$ freeze-out in the Universe.

Inga Kuznetsova; Johann Rafelski

2010-02-02T23:59:59.000Z

248

CX-004717: Categorical Exclusion Determination | Department of Energy  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

717: Categorical Exclusion Determination 717: Categorical Exclusion Determination CX-004717: Categorical Exclusion Determination Earl Fisher Biofuels CX(s) Applied: B5.1 Date: 12/14/2010 Location(s): Chester, Montana Office(s): Energy Efficiency and Renewable Energy, Golden Field Office The Montana Department of Environmental Quality is proposing to provide $25,000 of State Energy Program American Recovery and Reinvestment Act funds to Earl Fisher Biofuels, LLC (EFB) for the purchase and installation of two Kern Kraft KK40 oil seed crushers at their existing biodiesel production facility located in Chester's industrial park west of Chester, Montana. The purpose of the proposed project is to increase oil seed crushing capacity and biodiesel production by 40% and support a self sustaining industry by creating a market for oilseed crops that can be

249

EVG USAIX, Svergreen chalk River Liaison Office Ontario, Canada  

Office of Legacy Management (LM)

and Special Nuc.lear and Special Nuc.lear ?kk?rials kcc+ntabilitg EVG USAIX, Svergreen chalk River Liaison Office Ontario, Canada iulff USAEC, Washington Office See Div. of Rak Materials c~!:KRGO O?ER.i~TIONS ---.-- :ri:i!k USAZC, Ctricago Opnrations Office AGT General Electric Company AN? Project A.J,I Argonne Nat'1 Lab. AYL Al-tonne Nat'1 Lab. B XI Battelle Xfemorial Inst. CKX Vi.l;ro Carp, of America Em USAEC, East Hartford Area a TSC Ioxa State College ITS General Electric Company ANP Jk!pt, -%IAO IJSAK;, Lo&land Area Office . George L. ldercer P. 0. Box 59 Lemont, .Illinois P. 0. Box 132 Cincinnati 15, Ohio P. 0. Box 1096 Idaho Falls, Idaho P. 0. Box 299 -Lemont, Illinois 505 King Ave, Columbus, Ohio J. J. Uawning Lemont 800 bxt. 20~3 . . . . B. J. Sevold

250

Ram Shenoy | Department of Energy  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

Ram Shenoy Ram Shenoy About Us Ram Shenoy - Chief Technology Officer, ConocoPhillips Ram Shenoy Ram Shenoy is the chief technology officer for ConocoPhillips. An electrical engineer by training, he has twenty years of oil and gas industry experience. Before taking on his current role at ConocoPhillips, Shenoy was vice president of research for Schlumberger Limited, responsible for all Schlumberger's corporate scientific research laboratories. In prior years, he held a series of marketing and technology management positions with increasing responsibility, including managing director of Schlumberger-Doll Research Boston, and director and technology center manager of Schlumberger K.K. overseeing all the Engineering, Manufacturing and Sustaining activities of Schlumberger's R&D center in Tokyo, Japan.

251

Property:Foaf/Page | Open Energy Information  

Open Energy Info (EERE)

Page Page Jump to: navigation, search Property Name Foaf/Page Property Type URL Description Link to an external page discussing the same topic. (URL) It is equivalent to the well-known foaf:page property. Pages using the property "Foaf/Page" Showing 25 pages using this property. (previous 25) (next 25) 1 10 CFR § 1021 + http://en.openei.org/wiki/File:10CFRPart1021.pdf + 2 2-D Magnetotellurics At The Geothermal Site At Soultz-Sous-Forets- Resistivity Distribution To About 3000 M Depth + http://www.sciencedirect.com/science/article/pii/S1631071310001070 + 2.8-Ma Ash-Flow Caldera At Chegem River In The Northern Caucasus Mountains (Russia), Contemporaneous Granites, And Associated Ore Deposits + http://www.sciencedirect.com/science/article/B6VCS-48B5BV5-KK/2/a841cce0d247b754e5163bb62f72dc05 +

252

First observation of Bs -> J/psi f0(980) decays  

E-Print Network (OSTI)

Using data collected with the LHCb detector in proton-proton collisions at a centre-of-mass energy of 7 TeV, the hadronic decay Bs -> J/psi f0(980) is observed. This CP eigenstate mode could be used to measure mixing-induced CP violation in the B_s system. Using a fit to the pi+ pi- mass spectrum with interfering resonances gives R_{f0/phi} = [Gamma(Bs -> J/psi f0, f0 -> pi+ pi-)]/[Gamma(Bs -> J/psi phi, phi -> K+K-)] = 0.252^{+0.046+0.027}_{-0.032-0.033}, where the uncertainties are statistical and systematic, respectively.

The LHCb Collaboration; R. Aaij; B. Adeva; M. Adinolfi; C. Adrover; A. Affolder; Z. Ajaltouni; J. Albrecht; F. Alessio; M. Alexander; P. Alvarez Cartelle; A. A. Alves Jr; S. Amato; Y. Amhis; J. Amoraal; J. Anderson; R. B. Appleby; O. Aquines Gutierrez; L. Arrabito; M. Artuso; E. Aslanides; G. Auriemma; S. Bachmann; D. S. Bailey; V. Balagura; W. Baldini; R. J. Barlow; C. Barschel; S. Barsuk; A. Bates; C. Bauer; Th. Bauer; A. Bay; I. Bediaga; K. Belous; I. Belyaev; E. Ben-Haim; M. Benayoun; G. Bencivenni; R. Bernet; M. -O. Bettler; M. van Beuzekom; S. Bifani; A. Bizzeti; P. M. Bj\\ornstad; T. Blake; F. Blanc; C. Blanks; J. Blouw; S. Blusk; A. Bobrov; V. Bocci; A. Bondar; N. Bondar; W. Bonivento; S. Borghi; A. Borgia; E. Bos; T. J. V. Bowcock; C. Bozzi; T. Brambach; J. van den Brand; J. Bressieux; S. Brisbane; M. Britsch; T. Britton; N. H. Brook; H. Brown; A. Bchler-Germann; A. Bursche; J. Buytaert; S. Cadeddu; J. M. Caicedo Carvajal; O. Callot; M. Calvi; M. Calvo Gomez; A. Camboni; L. Camilleri; P. Campana; G. Capon; A. Carbone; G. Carboni; R. Cardinale; A. Cardini; L. Carson; K. Carvalho Akiba; G. Casse; M. Cattaneo; M. Charles; Ph. Charpentier; N. Chiapolini; X. Cid Vidal; P. J. Clark; P. E. L. Clarke; M. Clemencic; H. V. Cliff; J. Closier; C. Coca; V. Coco; J. Cogan; P. Collins; F. Constantin; G. Conti; A. Contu; M. Coombes; G. Corti; G. A. Cowan; R. Currie; B. D'Almagne; C. D'Ambrosio; W. Da Silva; P. 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; H. Degaudenzi; M. Deissenroth; L. Del Buono; C. Deplano; O. Deschamps; F. Dettori; J. Dickens; H. Dijkstra; M. Dima; P. Diniz Batista; S. Donleavy; D. Dossett; A. Dovbnya; F. Dupertuis; R. Dzhelyadin; C. Eames; S. Easo; U. Egede; V. Egorychev; S. Eidelman; D. van Eijk; F. Eisele; S. Eisenhardt; L. Eklund; D. G. d'Enterria; D. Esperante Pereira; L. Estve; E. Fanchini; C. Frber; G. Fardell; C. Farinelli; S. Farry; V. Fave; V. Fernandez Albor; M. Ferro-Luzzi; S. Filippov; C. Fitzpatrick; F. Fontanelli; R. Forty; M. Frank; C. Frei; M. Frosini; J. L. Fungueirino Pazos; S. Furcas; A. Gallas Torreira; D. Galli; M. Gandelman; P. Gandini; Y. Gao; J-C. Garnier; J. Garofoli; L. Garrido; C. Gaspar; N. Gauvin; M. Gersabeck; T. Gershon; Ph. Ghez; V. Gibson; V. V. Gligorov; C. Gbel; D. Golubkov; A. Golutvin; A. Gomes; H. Gordon; M. Grabalosa Gndara; R. Graciani Diaz; L. A. Granado Cardoso; E. Graugs; G. Graziani; A. Grecu; S. Gregson; B. Gui; E. Gushchin; Yu. Guz; T. Gys; G. Haefeli; S. C. Haines; T. Hampson; S. Hansmann-Menzemer; R. Harji; N. Harnew; P. F. Harrison; J. He; K. Hennessy; P. Henrard; J. A. Hernando Morata; E. van Herwijnen; A. Hicheur; E. Hicks; W. Hofmann; K. Holubyev; P. Hopchev; W. Hulsbergen; P. Hunt; T. Huse; R. S. Huston; D. Hutchcroft; V. Iakovenko; C. Iglesias Escudero; P. Ilten; J. Imong; R. Jacobsson; M. Jahjah Hussein; E. Jans; F. Jansen; P. Jaton; B. Jean-Marie; F. Jing; M. John; D. Johnson; C. R. Jones; B. Jost; F. Kapusta; T. M. Karbach; J. Keaveney; U. Kerzel; T. Ketel; A. Keune; B. Khanji; Y. M. Kim; M. Knecht; S. Koblitz; A. Konoplyannikov; P. Koppenburg; A. Kozlinskiy; L. Kravchuk; G. Krocker; P. Krokovny; F. Kruse; K. Kruzelecki; M. Kucharczyk; S. Kukulak; R. Kumar; T. Kvaratskheliya; V. N. La Thi; D. Lacarrere; G. Lafferty; A. Lai; R. W. Lambert; G. Lanfranchi; C. Langenbruch; T. Latham; R. Le Gac; J. van Leerdam; J. -P. Lees; R. Lefvre; A. Leflat; J. Lefran\\ccois; O. Leroy; T. Lesiak; L. Li; Y. Y. 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; J. Luisier; B. M'charek; F. Machefert; I. V. Machikhiliyan; F. Maciuc; O. Maev; J. Magnin; A. Maier; S. Malde; R. M. D. Mamunur; G. Manca; G. Mancinelli; N. Mangiafave; U. Marconi; R. Mrki; J. Marks; G. Martellotti; A. Martens; L. Martin; A. Martin Sanchez; D. Martinez Santos; A. Massafferri; Z. Mathe; C. Matteuzzi; M. Matveev; V. Matveev; E. Maurice; B. Maynard; A. Mazurov; G. McGregor; R. McNulty; C. Mclean; M. Meissner; M. Merk; J. Merkel; M. Merkin; R. Messi; S. Miglioranzi; D. A. Milanes; M. -N. Minard; S. Monteil; D. Moran; P. Morawski; J. V. Morris; R. Mountain; I. Mous; F. Muheim; K. Mller; R. Muresan; F. Murtas; B. Muryn; M. Musy; J. Mylroie-Smith; P. Naik; T. Nakada; R. Nandakumar; J. Nardulli; M. Nedos; M. Needham; N. Neufeld; M. Nicol; S. Nies; V. Niess; N. Nikitin; A. Oblakowska-Mucha; V. Obraztsov; S. Oggero; O. Okhrimenko; R. Oldeman; M. Orlandea; A. Ostankov; B. Pal; J. Palacios; M. Palutan; J. Panman; A. Papanestis; M. Pappagallo; C. Parkes; C. J. Parkinson; G. Passaleva; G. D. Patel; M. Patel; S. K. Paterson; G. N. Patrick; C. Patrignani; C. Pavel -Nicorescu; A. Pazos Alvarez; A. Pellegrino; G. Penso; M. Pepe Altarelli; S. Perazzini; D. L. Perego; E. Perez Trigo

2011-02-01T23:59:59.000Z

253

Flavor mixing in gauge-Higgs unification  

SciTech Connect

Gauge-Higgs unification is the fascinating scenario solving the hierarchy problem without supersymmetry. In this scenario, the Standard Model (SM) Higgs doublet is identified with extra component of the gauge field in higher dimensions and its mass becomes finite and stable under quantum corrections due to the higher dimensional gauge symmetry. On the other hand, Yukawa coupling is provided by the gauge coupling, which seems to mean that the flavor mixing and CP violation do not arise at it stands. In this talk, we discuss that the flavor mixing is originated from simultaneously non-diagonalizable bulk and brane mass matrices. Then, this mechanism is applied to various flavor changing neutral current (FCNC) processes via Kaluza-Klein (KK) gauge boson exchange at tree level and constraints for compactification scale are obtained.

Adachi, Y.; Kurahashi, N.; Lim, C. S.; Maru, N.; Tanabe, K. [Department of Sciences, Matsue College of Technology, Matsue 690-8518 (Japan); Department of Physics, Kobe University, Kobe 657-8501 (Japan); Department of Physics, and Research and Education Center for Natural Sciences, Keio University, Yokohama 223-8521 (Japan); Department of Physics, Kobe University, Kobe 657-8501 (Japan)

2012-07-27T23:59:59.000Z

254

Indirect signatures for axion(-like) particles  

E-Print Network (OSTI)

Magnetic field dependent transient solar observations are suggestive for axion-photon oscillations with light axion(-like) particle involvement. Novel dark-moon measurements with the SMART X-ray detectors can be conclusive for radiatively decaying massive exotica like the generic solar Kaluza-Klein (KK) axions. Furthermore, the predicted intrinsic strong solar magnetic fields could be the reason of enhanced low energy axion production. Such an axion component could be the as yet unknown origin of the strong quiet Sun X-ray luminosity at energies below ? 1 keV. Solar axion telescopes should lower their threshold, aiming to copy processes that might occur near the solar surface, be it due to spontaneous or magnetically induced radiative decay of axion(-like) particles. This is motivated also by the recent claim of an axion-like particle detection by the laser experiment PVLAS. 2 1

K. Zioutas; K. Dennerl; M. Gr; D. H. H. Hoffmann; J. Huovelin; B. Laki?; S. Orl; A. Ortiz; Th. Papaevangelou; Y. Semertzidis

2006-01-01T23:59:59.000Z

255

Kaon production in heavy ion reactions at intermediate energies  

E-Print Network (OSTI)

The article reviews the physics related to kaon and antikaon production in heavy ion reactions at intermediate energies. Chiral dynamics predicts substantial modifications of the kaon properties in a dense nuclear environment. The status of the theoretical predictions as well as experimental evidences for medium effects such as repulsive/attractive mass shifts for $K^+/K^-$ are reviewed. In the vicinity of the thresholds, and even more pronounced below threshold, the production of strangeness is a highly collective process. Starting from elementary reaction channels the phenomenology of $K^+$ and $K^-$ production, i.e. freeze-out densities, time scales etc. as derived from experiment and theoretical transport calculations is presented. Below threshold kaon production shows a high sensitivity on the nuclear compression reached in heavy ion reactions. This allows to put constraints on the nuclear equation-of-state which are finally discussed.

Christian Fuchs

2005-07-07T23:59:59.000Z

256

Mass gap for gravity localized on thick branes  

Science Conference Proceedings (OSTI)

We present a scalar thick brane configuration arising in a theory of 5D gravity coupled to a selfinteracting scalar field. We start from a classical solution of the field equations and study the physics of linear fluctuations around this background which obey a Schrdingerlike equation. We further focus our attention on a special case in which it is possible to solve this equation analytically for any massive mode. This fact allows us to make a closed analysis of the massive spectrum of KaluzaKlein (KK) excitations and to compute the corrections to Newtons law in the thin brane limit. There exist two bound states: the massless 4D graviton

N. BarbosaCendejas; A. HerreraAguilar; U. Nucamendi; I. Quiros; M. A. Reyes Santos; C. Schubert

2008-01-01T23:59:59.000Z

257

Evaluation of electrical conductivity and equations of state of non-ideal plasma through microsecond timescale underwater electrical wire explosion  

Science Conference Proceedings (OSTI)

Experimental and simulation results of underwater electrical Cu, Al, and W wire explosions in the microsecond timescale are presented. It was shown that the electrical conductivity results for Cu and Al agree well with modified Lee-More and quantum molecular dynamic models for temperatures above 10 kK. The equation of state (EOS) values based on SESAME tables for Cu and Al were slightly modified for intermediate temperatures in order to obtain fitting between experimental and simulated exploding wire radial expansion. Also, it was shown that the electrical conductivity results and the EOS evaluation differ significantly from the results obtained in nanosecond timescale experiments. Finally, it was found that underwater electrical W wire explosion is characterized by the appearance of non-uniformities along the z-axis of the wire. This phenomena adds uncertainty to the possibility of applying this type of experiments for evaluation of the electrical conductivity and EOS of W.

Sheftman, D.; Krasik, Ya. E. [Physics Department, Technion, Haifa 32000 (Israel)

2011-09-15T23:59:59.000Z

258

Microsoft Word - SAFARI 2000_special_ed_refs_20040804.doc  

NLE Websites -- All DOE Office Websites (Extended Search)

Global Change Biology Global Change Biology March 2004 - Volume 10 Issue 3 The SAFARI 2000 - Kalahari Transect Wet Season Campaign of year 2000 HH. Shugart, SA. Macko, P. Lesolle, TA. Szuba, MM. Mukelabai, P. Dowty, RJ. Swap Global Change Biology 2004 10:3 p. 273 Vegetation structure characteristics and relationships of Kalahari woodlands and savannas JL. Privette, Y. Tian, G. Roberts, RJ. Scholes, Y. Wang, KK. Caylor, P. Frost, M. Mukelabai Global Change Biology 2004 10:3 p. 281 Canopy structure in savannas along a moisture gradient on Kalahari sands Robert J. Scholes, Peter GH. Frost, Yuhong Tian Global Change Biology 2004 10:3 p. 292 Effects of precipitation and soil water potential on drought deciduous phenology in the Kalahari William M. Jolly, Steven W. Running

259

A RARE EARLY-TYPE STAR REVEALED IN THE WING OF THE SMALL MAGELLANIC CLOUD  

SciTech Connect

Sk 183 is the visually brightest star in the N90 nebula, a young star-forming region in the Wing of the Small Magellanic Cloud (SMC). We present new optical spectroscopy from the Very Large Telescope which reveals Sk 183 to be one of the most massive O-type stars in the SMC. Classified as an O3-type dwarf on the basis of its nitrogen spectrum, the star also displays broadened He I absorption, which suggests a later type. We propose that Sk 183 has a composite spectrum and that it is similar to another star in the SMC, MPG 324. This brings the number of rare O2- and O3-type stars known in the whole of the SMC to a mere four. We estimate physical parameters for Sk 183 from analysis of its spectrum. For a single-star model, we estimate an effective temperature of 46 {+-} 2 kK, a low mass-loss rate of {approx}10{sup -7} M{sub Sun} yr{sup -1}, and a spectroscopic mass of 46{sup +9}{sub -8} M{sub Sun} (for an adopted distance modulus of 18.7 mag to the young population in the SMC Wing). An illustrative binary model requires a slightly hotter temperature ({approx}47.5 kK) for the primary component. In either scenario, Sk 183 is the earliest-type star known in N90 and will therefore be the dominant source of hydrogen-ionizing photons. This suggests Sk 183 is the primary influence on the star formation along the inner edge of the nebula.

Evans, C. J. [UK Astronomy Technology Centre, Royal Observatory Edinburgh, Blackford Hill, Edinburgh EH9 3HJ (United Kingdom); Hainich, R.; Oskinova, L. M.; Hamann, W.-R.; Todt, H. [Institute for Physics and Astronomy, University of Potsdam, 14476 Potsdam (Germany); Gallagher III, J. S. [Department of Astronomy, University of Wisconsin-Madison, 5534 Sterling, 475 North Charter St., Madison, WI 53706 (United States); Chu, Y.-H.; Gruendl, R. A. [Astronomy Department, University of Illinois, 1002 W. Green Street, Urbana, IL 61801 (United States); Henault-Brunet, V. [Scottish Universities Physics Alliance (SUPA), Institute for Astronomy, University of Edinburgh, Royal Observatory Edinburgh, Blackford Hill, Edinburgh EH9 3HJ (United Kingdom)

2012-07-10T23:59:59.000Z

260

Optimization of the signal selection of exclusively reconstructed decays of B0 and B/s mesons at CDF-II  

SciTech Connect

The work presented in this thesis is mainly focused on the application in a {Delta}m{sub s} measurement. Chapter 1 starts with a general theoretical introduction on the unitarity triangle with a focus on the impact of a {Delta}m{sub s} measurement. Chapter 2 then describes the experimental setup, consisting of the Tevatron collider and the CDF II detector, that was used to collect the data. In chapter 3 the concept of parameter estimation using binned and unbinned maximum likelihood fits is laid out. In addition an introduction to the NeuroBayes{reg_sign} neural network package is given. Chapter 4 outlines the analysis steps walking the path from the trigger level selection to fully reconstructed B mesons candidates. In chapter 5 the concepts and formulas that form the ingredients to an unbinned maximum likelihood fit of {Delta}m{sub s} ({Delta}m{sub d}) from a sample of reconstructed B mesons are discussed. Chapter 6 then introduces the novel method of using neural networks to achieve an improved signal selection. First the method is developed, tested and validated using the decay B{sup 0} {yields} D{pi}, D {yields} K{pi}{pi} and then applied to the kinematically very similar decay B{sub s} {yields} D{sub s}{pi}, D{sub s} {yields} {phi}{pi}, {phi} {yields} KK. Chapter 7 uses events selected by the neural network selection as input to an unbinned maximum likelihood fit and extracts the B{sup 0} lifetime and {Delta}m{sub d}. In addition, an amplitude scan and an unbinned maximum likelihood fit of {Delta}m{sub s} is performed, applying the neural network selection developed for the decay channel B{sub s} {yields} D{sub s}{pi}, D{sub s} {yields} {phi}{pi}, {phi} {yields} KK. Finally chapter 8 summarizes and gives an outlook.

Doerr, Christian; /Karlsruhe U., EKP

2006-06-01T23:59:59.000Z

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261

JOHN B. KERR  

NLE Websites -- All DOE Office Websites (Extended Search)

B. KERR B. KERR Lawrence Berkeley National Laboratory MS 62R0203, 1 Cyclotron Road, Berkeley, CA 94720 (510)-486-6279 FAX: (510)-486-4995 e-mail: jbkerr@lbl.gov Web Page: http://energy.lbl.gov/aet/kerr/ EDUCATION. * Ph.D. University of Edinburgh , Scotland, 1978. Thesis Title, "Electrochemical Reduction of some Unsaturated Organic Chemicals." Advisor A.J. Bellamy. * Recipient of a NATO Studentship at the University of Aarhus, Denmark with P.E. Iversen and H. Lund, 1975-76 and at the Universite de Dijon, France with C. Degrand and E. Laviron,, 1976. * B.Sc.,Honours, 1st Class in Chemistry , University of Edinburgh , Scotland, 1974. * January 1978 - July 1979. Research Associate at the Department of Chemistry, University of Minnesota, Minneapolis with L.L. Miller. i) polymer coated electrodes

262

Monday,  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

February 23, 2004 February 23, 2004 0 Part m Department of Defense General Services Administration National Aeronautics and Space Administration r1 ~ ~ I I ~ 48 CPR Parts 2, 10, et al. Federal Acquisition Regulation; Special Emergency Procurement Authorit}'; Small Entity Compliance Guide; Interim Rules 8312 Federal Register/Vol. 69, No. 35/Monday, Febrnary 23, 2004/Rules and Regulations . DEPARTMENT OF DEFENSE GENERAL SERVICES ADMINISTRATION NATIONAL AERONAUTICS AND SPACE ADMINISTRATION 48 CFR Parts 2,10, 12, 13, 15, 19, and 25 [FAC 2001-20; FAR Case 2003--O22J RIN 900o-AJ88 Federal Acquisition Regulation; Special Emergency Procurltment Authority AGENCIES: Department of Defense (000), General Services Adminisuation (GSA). and National Aeronautics arId Space Administration (NASA). ACTION: Interim rule with request for

263

svte073.tmp  

Office of Scientific and Technical Information (OSTI)

FLUID FLUID DYNAMICS IN SUCKER ROD PUMPS by Robert P, Cutler and A.J. (Chip) Mansure Sandia National Laboratories Albuquerque, New Mexico Abstract Sucker rod pumps are installed in approximately 90% of all oil wells in the U.S. Although they have been widely used for decades, there are many issues regarding the fluid dynamics of the pump that have not been fully investigated. A project was conducted at Sandia National Laboratories to develop unimproved understanding of the fluid dynamics inside a sucker rod pump. A mathematical flow model was developed to predict pressures in any pump component or an entire pump under single-phase fluid and pumping conditions. Laboratory flow tests were conducted on instrumented individual pump components and on a complete pump to verify and refine the model. The mathematical model was then converted to a Visual Basic program to allow easy input of fluid,

264

INFORMAL REPORT PROPERTIES AND PERFORMANCE OF CEMENT- BASED GROUTS FOR GEOTHERMAL HEAT  

Office of Scientific and Technical Information (OSTI)

67006 67006 INFORMAL REPORT PROPERTIES AND PERFORMANCE OF CEMENT- BASED GROUTS FOR GEOTHERMAL HEAT PUMP APPLICATIONS FINAL REPORT FY 1999 M.L. Allan and A.J. Philippacopoulos November 1999 Prepared for: Office of Geothermal Technologies United States Department of Energy Washington, DC 20585 Materials and Chemical Sciences Division DISCLAIMER This document was prepared as an account of work sponsored by an agenc:y of the United States Government. Neither the United States Government nor any agency thereof, nor any of their employees, nor any of their contractors, subcontractors, or their employees makers any warranty, express or implied, or assumes any legal liability or responsibility of the accuracy, completeness, or usefulness of any information, apparatus, product or process disclosed, or represents that its use

265

Research Highlight  

NLE Websites -- All DOE Office Websites (Extended Search)

Testing and Comparing the Modified Anomalous Diffraction Approximation Testing and Comparing the Modified Anomalous Diffraction Approximation Submitter: Mitchell, D. L., Desert Research Institute Area of Research: Cloud Distributions/Characterizations Working Group(s): Radiative Processes Journal Reference: Mitchell, D.L., A.J. Baran, W.P. Arnott, C. Schmitt, 2006: Testing and comparing the anomalous diffraction approximation. J. Atmos. Sci., 63, 2948-2962. Comparison of MADA and T-matrix with measured Qext. Regions without data were contaminated by water vapor or CO2 absorption. MADA and T-matrix calculations are based on the measured PSD of hexagonal columns having an effective diameter of 14 microns. Comparison of the PSD weighted Qabs predicted by FDTD and MADA for a tunneling efficiency corresponding to aggregates. Cirrus clouds play a large role in the Earth's radiation budget and the way

266

LCC-0103 text.PDF  

NLE Websites -- All DOE Office Websites (Extended Search)

3 3 UCRL-JC- 149787 September 2002 Characterization of W-26% Re Target Material A.J. Sunwoo, D.C. Freeman, W. Stein, Lawrence Livermore National Laboratory Livermore, CA V. K. Bharadwaj , D. C. Schultz, J. C. Sheppard Stanford Linear Accelerator Center Stanford, CA 94309, USA Abstract: The power deposition of an incident electron beam in a tungsten-rhenium target and the resultant thermal shock stresses in the material have been modeled with a transient, dynamic, structural response finite element code. The Next Linear Collider electron beam is assumed split into three parts, with each part impinging on a 4 radiation lengths thick target. Three targets are required to avoid excessive thermal stresses in the targets. Energy deposition from each beam pulse occurs over 265

267

Microsoft PowerPoint - Dose Ranges 24Jan 05.ppt  

NLE Websites -- All DOE Office Websites (Extended Search)

20 40 60 20 40 60 80 100 rem NRC Dose Limit for Public 100 mrem/yr = 1 mSv/yr (DOE, ICRP, NCRP) ANSI standard N43.17 Personnel scanner, max = 25 mrem/yr Cleanup criteria for site decommissioning/ license termination 25 mrem/yr NCRP "Negligible Dose" Medical Diagnostics (A-J) A C D E G B Temporary "Special Case" annual Public Limit (NRC, DOE) NRC Dose Limit for Workers = 5 rem/yr = 50 mSv/yr Cancer Epidemiology Life Span Study (A-bomb survivors) ( Chart compiled by NF Metting, Office of Science DOE/BER; 24Jan2005,"Orders of Magnitude") Absorbed dose: 100 rad = 1 Gray Dose equivalent: 100 rem = 1 Sievert 100 mrem = 1 mSv (1 rem = 1 rad for x- and gamma- rays) Estimated dose for

268

Engineered Geothermal Systems Energy Return On Energy Investment  

NLE Websites -- All DOE Office Websites (Extended Search)

EGS EROI - 1 EGS EROI - 1 Engineered Geothermal Systems Energy Return On Energy Investment A.J. Mansure, Geothermal Consultant, ajm@q.com Albuquerque, NM 12/10/2012 Key Words: energy, EROI, EGS, efficiency, energy investment, energy return, input energy, energy payback, and net energy. Abstract Energy Return On Investment (EROI) is an important figure of merit for assessing the viability of energy alternatives. Too often comparisons of energy systems use "efficiency" when EROI would be more appropriate. For geothermal electric power generation, EROI is determined by the electricity delivered to the consumer compared to the energy consumed to construct, operate, and decommission the facility. Critical factors in determining the EROI of Engineered Geothermal Systems (EGS

269

 

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

097 097 On this page you'll find information about the DesignBuilder version 3.0.0.097 qualified computer software (www.buildings.energy.gov/qualified_software.html), which calculates energy and power cost savings that meet federal tax incentive requirements for commercial buildings. Date Documentation Received by DOE: 12 January 2012 Statements in quotes are from the software developer. Internal Revenue Code §179D (c)(1) and (d) Regulations Notice 2006-52, Section 6 requirements as amplified by Notice 2008-40, Section 4 requirements. (1) The name, address, and (if applicable) web site of the software developer; Design Builder Software Ltd. Place Chambers 41 London Rd. Stroud, Glos, GL5 2AJ, UK http://www.designbuilder.gov (2) The name, email address, and

270

1  

NLE Websites -- All DOE Office Websites (Extended Search)

Continuous Flow Ice Thermal Diffusion Chamber Continuous Flow Ice Thermal Diffusion Chamber Measurements of Ice Nuclei in the Arctic A.J. Prenni, P.J. DeMott, and S.M. Kreidenweis Department of Atmospheric Science, Colorado State University Fort Collins, Colorado D.C. Rogers National Center for Atmospheric Research EOL/RAF Broomfield, Colorado Introduction Mixed-phase stratus clouds are ubiquitous in the Arctic and play an important role in climate in this region. However, climate and regional models have generally proven unsuccessful at simulating arctic cloudiness, particularly during the colder months. Specifically, models tend to under-predict the amount of liquid water in mixed-phase clouds. This is problematic because cloud phase can greatly impact the radiative budget. The Mixed-Phase Arctic Cloud Experiment (M-PACE), conducted from late

271

Ohio's 13th congressional district: Energy Resources | Open Energy  

Open Energy Info (EERE)

3th congressional district: Energy Resources 3th congressional district: Energy Resources Jump to: navigation, search Equivalent URI DBpedia This article is a stub. You can help OpenEI by expanding it. This page represents a congressional district in Ohio. US Recovery Act Smart Grid Projects in Ohio's 13th congressional district FirstEnergy Service Company Smart Grid Project Registered Energy Companies in Ohio's 13th congressional district A.J. Rose Manufacturing Company Advanced Hydro Solutions Akrong Machine Services Castle Energy Services Echogen Power Systems, Inc. FirstEnergy Free Energy Alliance Green Energy Technologies Green Energy Technologies LLC GreenField Solar Corp. Jennings The Energy Factory Pier Associates, Inc. Randa Energy Solutions LLC R A Energy Solutions Raymond Plumbing & Heating

272

Research Highlight  

NLE Websites -- All DOE Office Websites (Extended Search)

Study Aerosol Humidity Effects Using the ARM Measurements Study Aerosol Humidity Effects Using the ARM Measurements Submitter: Li, Z., University of Maryland Area of Research: Radiation Processes Working Group(s): Aerosol Journal Reference: Jeong, M.-J., Z. Li, E. Andrews, and S.-C. Tsay (2007). Effect of aerosol humidification on the column aerosol optical thickness over the Atmospheric Radiation Measurement Southern Great Plains site, J. Geophys. Res., 112, D10202, doi:10.1029/2006JD007176. (a)-(j) Column-mean aerosol humidification factor as functions of the weighted column mean RH, . The ambient RH at one of the ten level-legs of the In-situ Aerosol Profile (IAP) measurements is replaced with RH equals 99%. Comparison of estimated column R(RH) following six different methods (M1~M6). Gray solid lines and black dashed lines are linear fit and

273

Final Environmental Assessment of Ground Water Compliance at the Slick Rock, Colorado, UMTRA Project Site  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

Impact Impact Ground Water Compliance at the Slick Rock, Colorado, UMTRA Project Sites AGENCY: U.S. DEP.4RTMENT OF ENERGY ACTIOK: FL&-DING OF NO SIGNIFICANT IMP-ACT (FONSI) SU$IM$RY: The U.S. Department of Energy (DOE) plans to implement ground lvater compliance strategies for two Uranium Mill Tailings Remedial Action (UMTR.4) Project sites near Slick Rock. Colorado. The purpose of the strategies is to comply with U.S. En\.ironmental Protection .Qency (EP.Aj ground n'ater standards defined in Title 40 Codr ~fF~d~w/ iieplutio?r.s (CFR) Part 192. and in so doing. protect human health and the en\.ironment. Ground water at the Slick Rock sites is contaminated with residual radioactive materials from hisTorica acti\,ities, associated with the processin of uranium ore, The planned action (~formeri>,.

274

Final Letter to DOE Regulatory Burden 9_7_2012.pdf  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

EXECUTIVE COMMITTEE EXECUTIVE COMMITTEE STEVE NARDELLA President (Winchester Homes Inc.) RICK BAILEY Vice President/Calvert Co. (Marrick Properties) DOUG MEEKER Vice President/Charles Co. (Elm Street Development) ROBERT J. SPALDING Vice President/Mont. Co. (Miller & Smith Homes) HILLARY P.COLT Vice President/Prince George's Co. (Konterra) MIKE MUMMAUGH Vice President/St. Mary's Co. (Paragon Properties Inc.) BRIAN "A.J." JACKSON Vice President/Washington DC (EYA, LLC) FRANK BOSSONG, IV, P.E Associate Vice President (Rodgers Consulting Inc.) CLARK WAGNER Treasurer (Bozzuto Homes) DAVE LUNDEN Vice President, State Legis./Secretary (Timberlake Homes, Inc.) ROBERT R. HARRIS Life Director (Lerch, Early & Brewer Chtd.) MARTY MITCHELL Immediate Past President

275

Property:Address | Open Energy Information  

Open Energy Info (EERE)

Address Address Jump to: navigation, search This is a property of type String. Pages using the property "Address" Showing 25 pages using this property. (previous 25) (next 25) 1 1366 Technologies + 45 Hartwell Avenue + 1st Light Energy, Inc. + 3224 McHennry Ave Suite F + 2 21-Century Silicon, Inc. + 1681 Firman Drive, Suite 103 + 3 3Degrees + 2 Embarcadero Center Suite 2950 + 3M + 3M Center + 3TIER + 2001 Sixth Avenue + 4 4th Day Energy + 38886 River Belle + 5 5 boro biofuel + 100 maiden lane + 8 8minutenergy Renewables, LLC + 111 Woodmere Road, Suite 190 + @ @Ventures (California) + 800 Menlo Avenue, Suite 120 + @Ventures (Massachusetts) + 187 Ballardvale Street, Suite A260 + A A.J. Rose Manufacturing Company + 38000 Chester Road + A1 Sun, Inc. + 1435 4th St. +

276

Il.-'",.'  

Office of Legacy Management (LM)

,,.. .r' ,,.. .r' +p,o~ ,!,*' A;>$, :.::> ,' ; ,.;I:- : ~ ", ,r .,,. ' , ' i.,l<, ~ ,1* .iT ,.~~~~~~~I~ _,L :,~.:/: .,,.,,,.,' ,, ;, ,, ,, I .. ,(: _ : ; . , y.,+ lar&f&r!rj&~+ ,id) L"'w#~~~~* I. ,& f ;";.y,m; ,I @ & **t&,y%:iis ;*a k' q&t ,:.: ;,I,' ,,, ,_ *, . ,. ,,&S_ ;, , (, t+ I . 1. -. ' ,' ~' i"'i,!..l + *I .(, h," ,rz ,. ,' :' ,' . :,' . ,.' _-#I_ ,. ,I. :, ,.' , ..I>. Xi,,? ,I. , ,r c/i' ,"" >.:1.. .>,. w/.&q:r*x Il.-'",.' !,.~~,,,~~iyY;~~~aj' ,~,,~~~~~~~~~ri~ *~i..iz~~ri~~~J~illi~;' ~(l~.~~i:)i9:ll~,-' i ?, ".' a? ,,?J,?" ~~~~I~~.~,~~~~~~~~.~~~~~~~~~~~~~-~ +q86?,r$w4t .r:~:@o:, " .", ' 1 j/ +$+. : WJl @+&?+&&w ' . 2 _ ._ b )., .;,a. :,. I .b.i.:.,*. A'

277

Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

the U.S. Department of Energy's NNSA the U.S. Department of Energy's NNSA U N C L A S S I F I E D Nanoscale Stable Precipitation- Strengthened Steels for Nuclear Applications Nuclear Energy Enabling Technologies (NEET) Reactor Materials LANL - K.D. Clarke (PI), A.J. Clarke, R.D. Field, S.A. Maloy, Y. Wang, R.E. Hackenberg NETL - O.N. Dogan, P.D. Jablonski CSM - K.O. Findley, J.G. Speer, K. Tippey NU - S. Vaynman, M.E. Fine DOE-NE Materials Crosscut Coordination Meeting, August 20, 2013 LA-UR-13-26637 Operated by Los Alamos National Security, LLC for the U.S. Department of Energy's NNSA U N C L A S S I F I E D Overview Slide 2 n Background n Investigative Team n Materials Processing Strategies * Colorado School of Mines (CSM) * Northwestern University (NU) n Material production

278

 

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

105 105 On this page you'll find information about the DesignBuilder version 3.0.0.105 qualified computer software (www.buildings.energy.gov/qualified_software.html), which calculates energy and power cost savings that meet federal tax incentive requirements for commercial buildings. Date Documentation Received by DOE: 16 March 2012 Statements in quotes are from the software developer. Internal Revenue Code §179D (c)(1) and (d) Regulations Notice 2006-52, Section 6 requirements as amplified by Notice 2008-40, Section 4 requirements. (1) The name, address, and (if applicable) web site of the software developer; Design Builder Software Ltd. Place Chambers 41 London Rd. Stroud, Glos, GL5 2AJ, UK http://www.designbuilder.gov (2) The name, email address, and

279

December 3, 2003, Board Public Meeting - Board Opening Remarks  

NLE Websites -- All DOE Office Websites (Extended Search)

PUBLIC MEETING ON OVERSIGHT PUBLIC MEETING ON OVERSIGHT + + + + + WEDNESDAY DECEMBER 3 , 2003 + + + + + The Board met in the Defense Nuclear Facilities Safety Board Hearing Room at 625 Indiana Avenue, N.W. , Suite 300, Washington, D.C., at 9 : 0 0 a.m., John T. Conway, Chairman, presiding. PRESENT JOHN T. CONWAY A.J. EGGENBERGER JOHN E. MANSFIELD R. BRUCE MATTHEWS STAFF PRESENT RICHARD A. AZZARO JAMES J. McCONNELL KENNETH M. PUSATERI ALSO PRESENT DANIEL E. GLENN MICHAEL B. MALLORY WILLIAM J. BRUMLY DENNIS R. RUDDY Chairman Vice Chairman Board Member Board Member General Counsel Deputy Technical Director General Manager Manager, Pantex Site Office General Manager, BWXT Pantex, LLC Manager, Y-12 Site Office General Manager, BWXT Y-12, LLC NEAL R. GROSS COURT REPORTERS AND TRANSCRIBERS

280

Atmospheric Carbon Dioxide Record from In Situ Measurements at Baring Head  

NLE Websites -- All DOE Office Websites (Extended Search)

Baring Head Baring Head Atmospheric Carbon Dioxide Record from In Situ Measurements at Baring Head graphics Graphics data Data Investigators M.R. Manning, A.J. Gomez, K.P. Pohl National Institute of Water and Atmospheric Research, Ltd., Climate Division, Gracefield Road, Gracefield, P.O. Box 31-311, Lower Hutt, New Zealand Period of Record 1970-93 Methods Determinations of atmospheric CO2 mixing ratios are made using a Siemens Ultramat-3 nondispersive infrared (NDIR) gas analyzer. The NDIR CO2 analyzer is connected via a gas manifold consisting of stainless steel tubing and computer-controlled solenoid switches to 12 gas cylinders and 2 sample air lines. The NDIR analyzer compares ambient air CO2 mixing ratios relative to known CO2 mixing ratios in tanks of compressed reference gases.

Note: This page contains sample records for the topic "aj podkaminer kk" 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

Mouse Strain-Dependent Variations in Sensitivity to Induction of Gamma-H2AX  

NLE Websites -- All DOE Office Websites (Extended Search)

Mouse Strain-Dependent Variations in Sensitivity to Induction of Gamma-H2AX Mouse Strain-Dependent Variations in Sensitivity to Induction of Gamma-H2AX Foci after Continuous Low Dose-Rate Irradiation: The Atm-/- vs Atm +/+ genotypes on Balb/c, 129S6, C57BL/6J, and A/J inbred strains J.R. Brogan Colorado State University Abstract We have recently developed a ‘low dose rate’ gamma-H2AX assay that is sufficiently sensitive to distinguish differences in response for cells from normal Atm +/+ (mouse) or ATM+/+ (human) and the phenotypes associated with the corresponding heterozygous genotypes(1, 2). The assay is also capable of distinguishing mild hypersensitivities for cells from an appreciable proportion of apparently normal individuals(3). We used this assay to determine whether the genetic background of four commonly used

282

Document  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

44 Federal Register 44 Federal Register / Vol. 76, No. 62 / Thursday, March 31, 2011 / Notices not anticipate recurrence of violations that gave rise to this PDL. As a result, under the authority in 20 U.S.C. 1234a(j), the Department has determined that compromise of this claim to $675,000 is appropriate. The public is invited to comment on the Department's intent to compromise this claim. Additional information may be obtained by contacting the person listed under FOR FURTHER INFORMATION CONTACT. Electronic Access to This Document: You can view this document, as well as all other documents of this Department published in the Federal Register, in text or Adobe Portable Document Format (PDF) on the Internet at the following site: http://www.ed.gov/news/ fedregister. To use PDF you must have

283

September 2013 Most Viewed Documents for Fossil Fuels | OSTI, US Dept of  

Office of Scientific and Technical Information (OSTI)

Fossil Fuels Fossil Fuels EXPERIMENTAL AND THEORETICAL DETERMINATION OF HEAVY OIL VISCOSITY UNDER RESERVOIR CONDITIONS Dr. Jorge Gabitto; Maria Barrufet (2003) 42 Molecular catalytic hydrogenation of aromatic hydrocarbons and hydrotreating of coal liquids. Yang, Shiyong; Stock, L.M. (1996) 36 Fluid Dynamics in Sucker Rod Pumps Cutler, R.P.; Mansure, A.J. (1999) 35 Controlled low strength materials (CLSM), reported by ACI Committee 229 Rajendran, N. (1997) 35 Fundamental Research on Percussion Drilling: Improved rock mechanics analysis, advanced simulation technology, and full-scale laboratory investigations Michael S. Bruno (2005) 35 Autothermal Reforming of Natural Gas to Synthesis Gas Steven F. Rice; David P. Mann (2007) 34 Evaluation of Wax Deposition and Its Control During Production of

284

Withdrawal of Notice of Intent To Prepare an Environmental Impact Statement for the High Flux Beam Reactor at the Brookhaven National Laboratory (11/30/99)  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

904 904 Federal Register / Vol. 64, No. 229 / Tuesday, November 30, 1999 / Notices Anyone who wishes to comment, provide technical information or data may do so in writing, either in lieu of, or in addition to, making an oral presentation. Documents will be accepted at the meeting or may be sent to the Defense Nuclear Facilities Safety Board's Washington, DC, office. The Board reserves its right to further schedule and otherwise regulate the course of the meeting, to recess, reconvene, postpone or adjourn the meeting, conduct further reviews, and otherwise exercise its power under the Atomic Energy Act of 1954, as amended. Dated: November 26, 1999. A.J. Eggenberger, Vice-Chairman. [FR Doc. 99-31182 Filed 11-26-99; 11:20 am] BILLING CODE 3670-01-P DEPARTMENT OF EDUCATION Submission for OMB Review;

285

EIA-802  

U.S. Energy Information Administration (EIA) Indexed Site

20","='Parts3-4'!$E$11:$K$11" 20","='Parts3-4'!$E$11:$K$11" "_020AJ","='Parts3-4'!$F$40" "_020AL","='Parts3-4'!$B$40" "_020AO","='Parts3-4'!$C$40" "_020AR","='Parts3-4'!$D$40" "_020AS","='Parts3-4'!$E$40" "_020BR","='Parts3-4'!$G$40" "_020CA","='Parts3-4'!$H$40" "_020CD","='Parts3-4'!$J$40" "_020CF","='Parts3-4'!$B$42" "_020CH","='Parts3-4'!$K$40" "_020CM","='Parts3-4'!$I$40" "_020CO","='Parts3-4'!$L$40" "_020EC","='Parts3-4'!$C$42" "_020EK","='Parts3-4'!$D$42" "_020GB","='Parts3-4'!$E$42"

286

Scotia Wind Ltd | Open Energy Information  

Open Energy Info (EERE)

Scotia Wind Ltd Scotia Wind Ltd Jump to: navigation, search Name Scotia Wind Ltd Place Stirling, Scotland, United Kingdom Zip FK9 7AJ Sector Wind energy Product Scotia Wind is an independent developer and operator of small to medium scale wind energy projects in the United Kingdom. Coordinates 40.67068°, -74.494569° Loading map... {"minzoom":false,"mappingservice":"googlemaps3","type":"ROADMAP","zoom":14,"types":["ROADMAP","SATELLITE","HYBRID","TERRAIN"],"geoservice":"google","maxzoom":false,"width":"600px","height":"350px","centre":false,"title":"","label":"","icon":"","visitedicon":"","lines":[],"polygons":[],"circles":[],"rectangles":[],"copycoords":false,"static":false,"wmsoverlay":"","layers":[],"controls":["pan","zoom","type","scale","streetview"],"zoomstyle":"DEFAULT","typestyle":"DEFAULT","autoinfowindows":false,"kml":[],"gkml":[],"fusiontables":[],"resizable":false,"tilt":0,"kmlrezoom":false,"poi":true,"imageoverlays":[],"markercluster":false,"searchmarkers":"","locations":[{"text":"","title":"","link":null,"lat":40.67068,"lon":-74.494569,"alt":0,"address":"","icon":"","group":"","inlineLabel":"","visitedicon":""}]}

287

DOE/SC-ARM-13-014 Biomass Burning Observation Project Science  

NLE Websites -- All DOE Office Websites (Extended Search)

4 4 Biomass Burning Observation Project Science Plan LI Kleinman AJ Sedlacek September 2013 DISCLAIMER This report was prepared as an account of work sponsored by the U.S. Government. Neither the United States nor any agency thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise, does not necessarily constitute or imply its endorsement, recommendation, or favoring by the U.S. Government or any agency thereof. The views and

288

1  

NLE Websites -- All DOE Office Websites (Extended Search)

Ice Nuclei Variability and Ice Formation in Ice Nuclei Variability and Ice Formation in Mixed-Phase Clouds PJ DeMott, AJ Prenni, and SM Kreidenweis Colorado State University Department of Atmospheric Science Fort Collins, Colorado CH Twohy Oregon State University Department of Atmospheric and Oceanic Sciences Corvallis, Oregon DC Rogers EOL-RAF National Center for Atmospheric Research Broomfield, Colorado Introduction First ice formation in mixed-phase clouds is thought to result from special particles known as ice nuclei (IN). IN from natural and possibly manmade sources thereby impact issues ranging from precipitation prediction to cloud radiative forcing (ice indirect effects). After considering our capabilities for detecting IN, we review evidence supporting the fact that IN measurements predict first ice formation in

289

Microsoft Word - Shehabi_etal_2009_Manuscript_Final.doc  

NLE Websites -- All DOE Office Websites (Extended Search)

939E 939E Can combining economizers with improved filtration save energy and protect equipment in data centers? A. Shehabi 1,2 , S. Ganguly 1 , L.A. Gundel 1 , A. Horvath 2 , T.W. Kirchstetter 1 , M.M. Lunden 1 , W. Tschudi 1 , A.J. Gadgil 1,2 , W.W. Nazaroff 1,2 1 Lawrence Berkeley National Laboratory 2 University of California, Berkeley August 2009 Building and Environment, v. 45, Issue 3, pp.718-726 DISCLAIMER This document was prepared as an account of work sponsored by the United States Government. While this document is believed to contain correct information, neither the United States Government nor any agency thereof, nor The Regents of the University of California, nor any of their employees, makes any warranty, express or implied, or assumes any legal responsibility for the accuracy, completeness, or usefulness of any information,

290

F=Q  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

;' ;' F=Q ~ Thursday, April 3, 2003 Part m ~ ~ ~ Department of Defense General Services Administration National Aeronautics and Space Administration ~ 48 CPR Part 2, et at. Federal Acquisition Regulation; Central Contractor Registration; ProJK}Sed Rule 16366 Federal R.e8i8ter/Vol. 68, No. 64/Thunday, April 3, 2003/Proposed Rules DEPARTMENT OF DEFENSE GENERAL SERVICES ADMINISTRATION NATIONAL AERONAUTICS AND SPACE ADMINISTRATION 48 CFR Part 2, et al. [FAR Ca.e 2002-G18] RIN 900O-AJ61 Federal Acqul81t1on Regul8tlon; Centrel Contractor Regl8tr8tlon AGENCIES: Department of Defense (DoD), General Services Administration (GSA). and National Aeronautics and Space Administration (NASA). ~- - -~ supplies at FAR 13.102 to reflect statutory chaQ8es in 15 V.S.C. 644(g). DATES: Interested parties should submit

291

December 4, 2003, Board Public Meeting - Board Opening Remarks  

NLE Websites -- All DOE Office Websites (Extended Search)

r r ' PUBLIC MEETING + + + + + THURSDAY DECEMBER 4, 2003 + + + + + The Board met in the DNFSB Hearing Room at 625 Indiana Avenue, N.W., Suite 300, Washington, D.C., at 9:00 a.m., John T. Conway, Chairman, presiding. PRESENT JOHN T. CONWAY A.J. EGGENBERGER JOHN E. MANSFIELD R. BRUCE MATTHEWS STAFF PRESENT RICHARD A. AZZARO J. KENT FORTENBERRY JAMES J . McCONNELL KENNETH M. PUSATERI ALSO PRESENT JESSIE ROBERSON JEFFERY M. ALLISON KEITH A. KLEIN FRAZER R. LOCKHART Chairman Vice Chairman Board Member Board Member General Counsel Technical Director Deputy Technical Director General Manager Asst. Secretary, Environmental Management, DOE Manager, DOE, Savannah River Operations Office Manager, DOE, Richland Operations Office Manager, DOE, Rocky Flats Field Off ice

292

EL-  

Office of Legacy Management (LM)

EL- EL- 019 MDP-02 r r = = = = = = = = = = = Attachment C Page 1 of 1 " .... ---- PLEASE FILM BOTH - SIDES BOTHSIDE.FRM COMPL. DATE , , CLOSING REF ~ READING FILE PROCUREMENT BPO ~ ~ DOE/CONTRACTS: SMITH DCO PROJECT ADMINISTRATION 81'1. ! ~ ~ DOEiHEAooUARTERS DHQ TECHNICAL REPORTS BTR ~ ~ PROJECT CONTROLS BPe ~ ~ ANL' A.J [Norak ANL ENGINEERING & TECHNOLOGY BET "'""' ~. . ~ ~ : : : : : ::~ ~II~~: :~:~::::::ANCE : : : ~ ~ M.A. Zurek ANL 11. 1 TO DOE ~ ~ 137/138 WAYNE/MAYWOOD POCC READING FILE FROM DOE ~ ~ 139 COLONIE (CISS) ADMIN RCD _ H. L ~~ Y"'.:L ~ ~ '""" CAm """,

293

IE  

Office of Legacy Management (LM)

/ / / / / ORAU 89/J-178 IE Prepared by Oak Ridge Associated VERIFICATION Universities OF Prepared for the Division of 1983 AND 1984 REMEDIAL ACTIONS Facility and Site Decommissioning NIAGARA FALLS STORAGE SITE I P rojets VICINITY PROPERTIES U.S. Department of Energy LEWISTON, NEW YORK I~~~| ~S. A. WICAL, M. R. LANDIS, and A. J. BOERNER I I I I I Environmental Survey and Site Assessment Program l3*~~~~~~~ ~~~Energy/Environment Systems Division FINAL REPORT DECEMBER 1989 I VERIFICATION OF 1983 AND 1984 REMEDIAL ACTIONS NIAGARA FALLS STORAGE SITE VICINITY PROPERTIES LEWISTON, NEW YORK 3~~ ~~~~~~1 ~Prepared by S.A. Wical, M.R. Landis, and A.J. Boerner Environmental Survey and Site Assessment Program Energy/Environment Systems Division Oak Ridge Associated Universities Oak Ridge, TN 37831-0117

294

DOE Hydrogen and Fuel Cells Program: 2009 Annual Progress Report - Systems  

NLE Websites -- All DOE Office Websites (Extended Search)

Systems Analysis Systems Analysis Printable Version 2009 Annual Progress Report VII. Systems Analysis This section of the 2009 Progress Report for the DOE Hydrogen Program focuses on systems analysis. Each technical report is available as an individual Adobe Acrobat PDF. Download Adobe Reader. Systems Analysis Program Element Introduction, Fred Joseck, U.S. Department of Energy (PDF 411 KB) HyDRA: Hydrogen Demand and Resource Analysis Tool (PDF 243 KB), Johanna Levene, National Renewable Energy Laboratory Water Needs and Constraints for Hydrogen Pathways (PDF 99 KB), A.J. Simon, Lawrence Livermore National Laboratory Cost Implications of Hydrogen Quality Requirements (PDF 817 KB), Shabbir Ahmed, Argonne National Laboratory Macro-System Model (PDF 384 KB), Mark Ruth, National Renewable

295

Biological Systems for Hydrogen Photoproduction (Presentation)  

DOE Green Energy (OSTI)

This presentation summarizes NREL biological systems for hydrogen photoproduction work for the DOE Hydrogen and Fuel Cells Program Annual Merit Review and Peer Evaluation Meeting, May 14-18, 2012. General goal is develop photobiological systems for large-scale, low cost and efficient H{sub 2} production from water (barriers AH, AI and AJ). Specific tasks are: (1) Address the O{sub 2} sensitivity of hydrogenases that prevent continuity of H{sub 2} photoproduction under aerobic, high solar-to-hydrogen (STH) light conversion efficiency conditions; and (2) Utilize a limited STH H{sub 2}-producing method (sulfur deprivation) as a platform to address or test other factors limiting commercial algal H{sub 2} photoproduction, including low rates due to biochemical and engineering mechanisms.

Ghirardi, M. L.

2012-05-01T23:59:59.000Z

296

Hartree-Fock-Roothaan energies and expectation values for the neutral atoms He to Uuo: The B-spline expansion method  

SciTech Connect

The ground state energies and expectation values of atoms are given by Hartree-Fock-Roothaan calculations with one B-spline set. For the neutral atoms He to Uuo, the total energies, kinetic energies, potential energies, and virial ratios are tabulated. Our total energies are in excellent agreement with the highly accurate 10-digit numerical Hartree-Fock energies given by Koga and Thakkar [T. Koga, A.J. Thakkar, J. Phys. B 29 (1996) 2973]. The virial ratios are in complete agreement to within 12-digits of the exact value -2. Orbital energies, electron densities at the nucleus, electron-nucleus cusp ratios, and radial expectation values (n = 2, 1, -1, -2, -3) are also given.

Saito, Shiro L. [School of International Liberal Studies, Chukyo University, Toyota 470-0393 (Japan)], E-mail: luna@trinity.lets.chukyo-u.ac.jp

2009-11-15T23:59:59.000Z

297

Document  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

March 26, 2004 Part IV Department of Defense General Services Adminstration National Aeronautics and Space Administration 48 CFR Chapter 1 Federal Acquisition Regulations; Purchases from Federal Prison Industries- Requirement for Market Research and Small Entity Compliance Guide; Interim Rules VerDate jul2003 20:45 Mar 25, 2004 Jkt 203001 PO 00000 Frm 00001 Fmt 4737 Sfmt 4737 E:\FR\FM\26MRR4.SGM 26MRR4 16148 Federal Register / Vol. 69, No. 59 / Friday, March 26, 2004 / Rules and Regulations DEPARTMENT OF DEFENSE GENERAL SERVICES ADMINISTRATION NATIONAL AERONAUTICS AND SPACE ADMINISTRATION 48 CFR Parts 8, 19, 42, and 52 [FAC 2001-21; FAR Case 2003-023] RIN 9000-AJ91 Federal Acquisition Regulation; Purchases From Federal Prison Industries-Requirement for Market

298

March 10, 2005, Board letter forwarding Recommendation 2005-1, Nuclear Material Packaging  

NLE Websites -- All DOE Office Websites (Extended Search)

FACLLTIlEs FACLLTIlEs SAFETYBOARD John T. Conway, Chairman A.J. Eggenberger, Vice Chairman Joseph F. Bader John E. Mansfield R. Bruce Matthews 625 Indiana Avenue, NW, Suite 700, Wa5hington. D.C. 20004-2901 (202) 694-7000 March 10, 2005 The Honorable Samuel W. Bodman Secretary of Energy 1000 Independence Avenue, SW Washington, DC 20585-1000 Dear Secretary Bodman: On March 10,2005, the Defense Nuclear Facilities Safety Board (Board), in accordance with 42 U.S.C. 9 2286a(a)(5), unanimously approved Recommendation 2005- 1, Nuclear Material Packaging, which is enclosed for your consideration. This recommendation addresses issuance of a requirement that nuclear material packaging meet technically justified criteria for safe storage and handling outside of engineered contamination barriers.

299

Effect of low-dose, low-LET γ-radiation and BaP injection on pulmonary  

NLE Websites -- All DOE Office Websites (Extended Search)

low-dose, low-LET γ-radiation and BaP injection on pulmonary low-dose, low-LET γ-radiation and BaP injection on pulmonary immunity in A/J mice K. Gott Lovelace Respiratory Research Institute Abstract Introduction: Low-dose, low-linear-energy-transfer (LET) radiation (LDR; < 100 mGy) activates the immune response (Nowosielska et al., 2006), presumably via epigenetic pathways (Scott et al., 2009) and has been implicated as suppressing both alpha-radiation-induced and smoking-related lung cancer (Scott et al. 2009). One of the hypothesized adaptive-response mechanisms by which LDR does so is by activating immune cell function in the lung, which would then increase their anti-cancer surveillance function (Liu, 2007; Bogdandi et al., 2010). One measure of activated immune cell function is their expression of markers on their cell surface that are

300

Department Members | Environmental Sciences | BNL  

NLE Websites -- All DOE Office Websites (Extended Search)

Department Members Department Members Administration and Support Staff Scientific and Technical Staff Mary Jane Bartholomew William J. Behrens Alexei Belochitski Alice T. Cialella Peter H. Daum Satoshi Endo Arokiasamy J. (AJ) Francis Michele Galletti Scott Giangrande Laurie Gregory John H. Heiser Dong Huang Michael P. Jensen Karen Lee Johnson Paul D. Kalb Lawrence I. Kleinman Chongai Kuang Stefanie Lasota Kathy Lazar Yin-Nan Lee Keith Lewin Ernie R. Lewis Min Liang Wuyin Lin Yangang Liu Edward Luke L. Lynn Ma Robert L. McGraw Andrew McMahon Laurence W. Milian Alistair Rogers Martin Schoonen - Chair Stephen E. Schwartz Arthur J. Sedlacek Gunnar I. Senum Scott Smith Hua Song Stephen R. Springston Terrence Sullivan Ryan Thalman Alison Tilp Tami Toto David Troyan Gabriel J. Vignato Andrew M. Vogelmann Richard Wagener

Note: This page contains sample records for the topic "aj podkaminer kk" 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

Calibration and Validation of a Spar-Type Floating Offshore Wind Turbine Model using the FAST Dynamic Simulation Tool: Preprint  

NLE Websites -- All DOE Office Websites (Extended Search)

Calibration and Validation of a Calibration and Validation of a Spar-Type Floating Offshore Wind Turbine Model using the FAST Dynamic Simulation Tool Preprint J.R. Browning University of Colorado-Boulder J. Jonkman and A. Robertson National Renewable Energy Laboratory A.J. Goupee University of Maine Presented at the Science of Making Torque from Wind Oldenburg, Germany October 9-11, 2012 Conference Paper NREL/CP-5000-56138 November 2012 NOTICE The submitted manuscript has been offered by an employee of the Alliance for Sustainable Energy, LLC (Alliance), a contractor of the US Government under Contract No. DE-AC36-08GO28308. Accordingly, the US Government and Alliance retain a nonexclusive royalty-free license to publish or reproduce the published form of this contribution, or allow others to do so, for US Government purposes.

302

Supernova Cosmology Project  

NLE Websites -- All DOE Office Websites (Extended Search)

The Hubble Space Telescope Cluster Supernova Survey: The Hubble Space Telescope Cluster Supernova Survey: An Intensive HST Survey for z>1 Type Ia Supernovae by Targeting Galaxy Clusters Survey Paper: Dawson et al. (The Supernova Cosmology Project) 2009, AJ, 138, 1271 [ADS] [arXiv] We present a new survey strategy to discover and study high redshift Type Ia supernovae (SNe Ia) using the Hubble Space Telescope (HST). By targeting massive galaxy clusters at 0.9 0.95, nine of which were in galaxy clusters. This strategy provides a SN sample that can be used to decouple the effects of host galaxy extinction and intrinsic color in high redshift SNe, thereby reducing one of the largest systematic uncertainties in SN cosmology.

303

Induction of murine CYP1A2 gene expression by acenaphthylene  

E-Print Network (OSTI)

Acenaphthylene and related polynuclear aromatic hydrocarbons (PAH) are industrial combustion by-products which are also found in cooked foods. Recent studies in this laboratory have shown that acenaphthylene induces Cypla2 gene expression in mice and this study further investigates this induction response. Studies with six genetically-inbred strains of mice have shown that the activity of acenaphthylene (300 mg/kg) as an inducer of CYPlA2-dependent methoxyresorufin 0-demethylase (MROD) was age-and strain-dependent. The results showed that DBA mice, compared to the C57BL/6, C3H, CBA, A/j and SJL strains were most responsive to induction after a single dose of acenaphthylene (300 mg/kg). Hepatic MROD activity in acenaphthylene-treated DBA mice was induced 22-and 4-fold in males and females respectively. In contrast, a <2 to 4-fold induction of ethoxyresorufin 0-deethylase (EROD) activity was observed in both sexes. The other inbred strains had higher basal rates of hepatic MROD activity than the DBA strain, (i.e. C3H, C57BL/6, CBA, A/j and SJL). Differences in induction of MROD activity by acenaphthylene among the strains was primarily due to allelic variation (responsive or non responsive) at the aryl hydrocarbon (Ah) locus. Current studies are focused on further characterizing the strain-specific effects of acenaphthylene and related compounds and the molecular regulation of hepatic CYPlA2 gene expression in male and female DBA mice and other rodent species.

Miggins, John Wesley

1996-01-01T23:59:59.000Z

304

Experimental and Numerical Examination of the Thermal Transmittance of High  

NLE Websites -- All DOE Office Websites (Extended Search)

Experimental and Numerical Examination of the Thermal Transmittance of High Experimental and Numerical Examination of the Thermal Transmittance of High Performance Window Frames Title Experimental and Numerical Examination of the Thermal Transmittance of High Performance Window Frames Publication Type Conference Paper LBNL Report Number LBNL-3886E Year of Publication 2010 Authors Gustavsen, Arlid, Goce Talev, Dariush K. Arasteh, Howdy Goudey, Christian Kohler, Sivert Uvsløkk, and Bjørn Petter Jelle Conference Name Thermal Performance of the Exterior Envelopes of Whole Buildings XI International Conference Date Published Dec 5-9, 2010 Conference Location Clearwater Beach, FL Call Number LBNL-3886E Abstract While window frames typically represent 20-30% of the overall window area, their impact on the total window heat transfer rates may be much larger. This effect is even greater in low-conductance (highly insulating) windows which incorporate very low conductance glazings. Developing low-conductance window frames requires accurate simulation tools for product research and development.

305

Property:Link | Open Energy Information  

Open Energy Info (EERE)

Link Link Jump to: navigation, search This is a property of type URL. Pages using the property "Link" Showing 25 pages using this property. (previous 25) (next 25) 1 10 CFR § 1021 + http://en.openei.org/wiki/File:10CFRPart1021.pdf + 2 2-D Magnetotellurics At The Geothermal Site At Soultz-Sous-Forets- Resistivity Distribution To About 3000 M Depth + http://www.sciencedirect.com/science/article/pii/S1631071310001070 + 2.8-Ma Ash-Flow Caldera At Chegem River In The Northern Caucasus Mountains (Russia), Contemporaneous Granites, And Associated Ore Deposits + http://www.sciencedirect.com/science/article/B6VCS-48B5BV5-KK/2/a841cce0d247b754e5163bb62f72dc05 + 2007 Annual Report + https://www.enel.com/en-GB/investors/financial_reports/annual/ + 238U Decay Series Systematics Of Young Lavas From Batur Volcano, Sunda Arc + http://www.sciencedirect.com/science/article/B6VCS-48B0DW7-F/2/8e2bc55d34022c3d13f71c2dd57cd45b +

306

Second moment method for a family of boolean CSP  

E-Print Network (OSTI)

The estimation of phase transitions in random boolean Constraint Satisfaction Problems (CSP) is based on two fundamental tools: the first and second moment methods. While the first moment method on the number of solutions permits to compute upper bounds on any boolean CSP, the second moment method used for computing lower bounds proves to be more tricky and in most cases gives only the trivial lower bound 0. In this paper, we define a subclass of boolean CSP covering the monotone versions of many known NP-Complete boolean CSPs. We give a method for computing non trivial lower bounds for any member of this subclass. This is achieved thanks to an application of the second moment method to some selected solutions called characteristic solutions that depend on the boolean CSP considered. We apply, as an example, this method to establish that the threshold r_{k} of monotone 1-in-k-SAT is \\log k/k\\leq r_{k}\\leq\\log^{2}k/k

Boufkhad, Yacine

2011-01-01T23:59:59.000Z

307

ds_branching_s034dsb-web.dvi  

NLE Websites -- All DOE Office Websites (Extended Search)

More More than a dozen papers on the D + s , most of them from the CLEO experiment, have been published since the 2008 Review. We now know enough to attempt an overview of the branching fractions. Figure 1 shows a partial breakdown of the fractions. The rest of this note is about how the figure was constructed. The values shown make heavy use of CLEO measurements of inclusive branching fractions [1] For other data and references cited in the following, see the Listings. Modes with leptons: The bottom (20.0 ± 0.9)% of Fig. 1 shows the fractions for the exclusive modes that include lep- tons. Measured e + ν e fractions have been doubled to get the semileptonic ℓ + ν fractions. The sum of the exclusive e + ν e frac- tions is (6.9 ± 0.4)%, consistent with an inclusive semileptonic e + ν e measurement of (6.5 ± 0.4)%. There seems to be little missing here. Inclusive hadronic KK fractions: The Cabibbo-favored

308

Citation: D.E. Groom  

NLE Websites -- All DOE Office Websites (Extended Search)

f f J (2220) I G (J PC ) = 0 + (2 + + or 4 + + ) OMITTED FROM SUMMARY TABLE THE f J (2220) Updated April 2000 by M. Doser (CERN). This state has been observed in J/ψ(1S) radiative decay into KK (K + K - and K 0 S K 0 S modes seen (BALTRUSAITIS 86D, BAI 96B)). An upper limit from DM2 for these modes (AUGUSTIN 88) is at the level at which observation is claimed. There are also indications for further decay modes (π + π - and pp (BAI 96B) and π 0 π 0 (BAI 98H)) in the same production process, although again at the level at which previous upper limits had been obtained (BALTRUSAITIS 86D). This was also seen in ηη (ALDE 86B), K 0 S K 0 S (ASTON 88D), and K + K - (ALDE 88 F), albeit with very low statistics. Its J P C is determined from the angular distributions of these observations. It is not seen in Υ radiative decays (BARU 89), B inclusive decays (BEHRENDS 84), nor in γγ (GODANG 97, ALAM 98C), which is not surprising, since

309

On the infimum of the energy-momentum spectrum of a homogeneous Bose gas  

E-Print Network (OSTI)

We consider second quantized homogeneous Bose gas in a large cubic box with periodic boundary conditions, at zero temperature. We discuss the energy-momentum spectrum of the Bose gas and its physical significance. We review various rigorous and heuristic results as well as open conjectures about its properties. Our main aim is to convince the readers, including those with mainly mathematical background, that this subject has many interesting problems for rigorous research. In particular, we investigate the upper bound on the infimum of the energy for a fixed total momentum $\\kk$ given by the expectation value of one-particle excitations over a squeezed states. This bound can be viewed as a rigorous version of the famous Bogoliubov method. We show that this approach seems to lead to a (non-physical) energy gap. The variational problem involving squeezed states can serve as the preparatory step in a perturbative approach that should be useful in computing excitation spectrum. This version of a perturbative approach to the Bose gas seems (at least in principle) superior to the commonly used approach based on the $c$-number substitution.

H. D. Cornean; J. Derezi?ski; P. Zi?

2005-11-02T23:59:59.000Z

310

Higgs Bosons in Extra Dimensions  

E-Print Network (OSTI)

In this paper, motivated by the recent discovery of a Higgs-like boson at the LHC with a mass m_H\\simeq 126 GeV, we review different models where the hierarchy problem is solved by means of a warped extra dimension. In the Randall-Sundrum model electroweak observables provide very strong bounds on the mass of KK modes which motivates extensions to overcome this problem. Two extensions are briefly discussed. One particular extension is based on the deformation of the metric such that it strongly departs from the AdS_5 structure in the IR region while it goes asymptotically to AdS_5 in the UV brane. This model has the IR brane close to a naked metric singularity (which is outside the physical interval) characteristic of soft-walls constructions. The proximity of the singularity provides a strong wave-function renormalization for the Higgs field which suppresses the T and S parameters. The second class of considered extensions are based on the introduction of an extra gauge group in the bulk such that the custodial SU(2)_R symmetry is gauged and protects the T parameter. By further enlarging the bulk gauge symmetry one can find models where the Higgs is identified with the fifth component of gauge fields and for which the Higgs potential, along with the Higgs mass, can be dynamically determined by the Coleman-Weinberg mechanism.

Mariano Quiros

2013-11-12T23:59:59.000Z

311

On X-Channels with Feedback and Delayed CSI  

E-Print Network (OSTI)

The sum degrees of freedom (DoF) of the two-user MIMO X-channel is characterized in the presence of output feedback and delayed channel state information (CSI). The number of antennas at each transmitters is assumed to be M and the number of antennas at each of the receivers is assumed to be N. It is shown that the sum DoF of the two-user MIMO X-channel is the same as the sum DoF of a two-user MIMO broadcast channel with 2M transmit antennas, and N antennas at each receiver. Hence, for this symmetric antenna configuration, there is no performance loss in the sum degrees of freedom due to the distributed nature of the transmitters. This result highlights the usefulness of feedback and delayed CSI for the MIMO X-channel. The K-user X-channel with single antenna at each transmitter and each receiver is also studied. In this network, each transmitter has a message intended for each receiver. For this network, it is shown that the sum DoF with partial output feedback alone is at least 2K/(K+1). This lower bound is...

Tandon, Ravi; Poor, H Vincent; Shamai, Shlomo

2012-01-01T23:59:59.000Z

312

Measurements of the equations of state and spectrum of nonideal xenon plasma under shock compression  

Science Conference Proceedings (OSTI)

Experimental equations of state on generation of nonideal xenon plasma by intense shock wave compression was presented in the ranges of pressure of 2-16 GPa and temperature of 31-50 kK, and the xenon plasma with the nonideal coupling parameter {Gamma} range from 0.6-2.1 was generated. The shock wave was produced using the flyer plate impact and accelerated up to {approx}6 km/s with a two-stage light gas gun. Gaseous specimens were shocked from two initial pressures of 0.80 and 4.72 MPa at room temperature. Time-resolved spectral radiation histories were recorded by using a multiwavelength channel pyrometer. The transient spectra with the wavelength range of 460-700 nm were recorded by using a spectrometer to evaluate the shock temperature. Shock velocity was measured and particle velocity was determined by the impedance matching methods. The equations of state of xenon plasma and ionization degree have been discussed in terms of the self-consistent fluid variational theory.

Zheng, J.; Gu, Y. J.; Chen, Z. Y.; Chen, Q. F. [National Key Laboratory of Shock Wave and Detonation Physics, Institute of Fluid Physics, P.O. Box 919-102, Mianyang, Sichuan (China)

2010-08-15T23:59:59.000Z

313

Enhancement of Loop induced 125GeV Higgs pair production through Large-Extra-Dimensions model at the LHC  

E-Print Network (OSTI)

Based on the analysis of 5 fb^-1 of data at the LHC, the ATLAS and CMS collaborations have presented evidence for a Higgs boson with a mass in the 125 GeV range. We consider the 125 GeV neutral Higgs pair production process in the context of large-extra-dimensions(LED) model including the Kaluza-Klein(KK) excited gravitons at the LHC. We take into account the LED effects coming from gluon-gluon fusion and quark-antiquark collision channels as well as their corresponding next-to-leading order(NLO) QCD loop induced corrections. We analyse their impacts on both the total cross section and some key distributions. Indeed,pp -> HH has the clear advantage of a lower standard model(SM) background compare to process like pp -> jj, though its SM prediction is very small, it is shown that the LED model raises the cross section of Higgs pair production compare to its SM prediction and enhance the transverse momentum(pHT) and invariant mass(MHH) Distributions especially at high scales of pH T and MHH. By including the NLO QCD loop corrections, the scale dependence of total cross section can be reduced obviously. Choose suitable decay modes like HH -> bbrr or HH -> bbmumu and some simple cuts, we can strongly reduce the SM background but keep most of the LED effects, leading Higgs pair production a promising channel to search LED effects.

Hao Sun; Ya-Jin Zhou

2012-11-27T23:59:59.000Z

314

Constraints on large-extra-dimensions model through 125 GeV Higgs pair production at the LHC  

E-Print Network (OSTI)

Based on the analysis of 5 fb^-1 of data at the LHC, the ATLAS and CMS collaborations have presented evidence for a Higgs boson with a mass in the 125 GeV range. We consider the 125 GeV neutral Higgs pair production process in the context of large-extra-dimensions (LED) model including the Kaluza-Klein (KK)excited gravitons at the LHC. We consider the standard model(SM) Higgs pair production in gluon-gluon fusion channel and pure LED effects through graviton exchange as well as their interferences. It is shown that such interferences should be included; the LED model raises the transverse momentum (Pt)and invariant mass (M_HH) distributions at high scales of Pt and M_HH of the Higgs pair production. By using the Higgs pair production we could set the discovery limit on the cutoff scale M_S up to 6 TeV for delta = 2 and 4.5 TeV for delta = 6.

Hao Sun; Ya-Jin Zhou; He Chen

2012-11-22T23:59:59.000Z

315

Triple $Z^0$-boson production in large extra dimensions model at ILC  

E-Print Network (OSTI)

We investigate the effects induced by the interactions of the Kaluza-Klein (KK) graviton with the standard model (SM) particles on the triple $Z^0$-boson production process at the ILC in the framework of the large extra dimension (LED) model. We present the dependence of the integrated cross sections on the electron-positron colliding energy $\\sqrt{s}$, and various kinematic distributions of final $Z^0$ bosons and their subsequential decay products in both the SM and the LED model. We also provide the relationship between the integrated cross section and the fundamental scale $M_S$ by taking the number of the extra dimensions ($d$) as 3, 4, 5, and 6, respectively. The numerical results show that the LED effect can induce a observable relative discrepancy for the integrated cross section ($\\delta_{LED}$), which can reach the value of $13.11% (9.27%)$ when $M_S = 3.5 (3.8) TeV$ and the colliding energy $\\sqrt{s} = 1 TeV$. We find the relative discrepancy of LED effect can even reach few dozen percent in the high transverse momentum area or the central rapidity region of the final $Z^0$-bosons and muons.

Jiang Ruo-Cheng; Li Xiao-Zhou; Ma Wen-Gan; Guo Lei; Zhang Ren-You

2012-11-29T23:59:59.000Z

316

Nuclear modification factors of phi mesons in d+Au, Cu+Cu and Au+Au collisions at sqrt(S_NN)=200 GeV  

E-Print Network (OSTI)

The PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC) has performed systematic measurements of phi meson production in the K+K- decay channel at midrapidity in p+p, d+Au, Cu+Cu and Au+Au collisions at sqrt(S_NN)=200 GeV. Results are presented on the phi invariant yield and the nuclear modification factor R_AA for Au+Au and Cu+Cu, and R_dA for d+Au collisions, studied as a function of transverse momentum (1phi exhibits a suppression relative to expectations from binary scaled p+p results. The amount of suppression is smaller than that of the neutral pion and the eta meson in the intermediate p_T range (2--5 GeV/c); whereas at higher p_T the phi, pi^0, and eta show similar suppression. The baryon (protons and anti-protons) excess observed in central Au+Au collisions at intermediate p_T is not observed for the phi meson despite the similar mass of the proton and the phi. This suggests that the excess is lin...

Adare, A; Aidala, C; Ajitanand, N N; Akiba, Y; Al-Bataineh, H; Alexander, J; Al-Jamel, A; Angerami, A; Aoki, K; Aphecetche, L; Aramaki, Y; Armendariz, R; Aronson, S H; Asai, J; Atomssa, E T; Averbeck, R; Awes, T C; Azmoun, B; Babintsev, V; Bai, M; Baksay, G; Baksay, L; Baldisseri, A; Barish, K N; Barnes, P D; Bassalleck, B; Basye, A T; Bathe, S; Batsouli, S; Baublis, V; Bauer, F; Baumann, C; Bazilevsky, A; Belikov, S; Belmont, R; Bennett, R; Berdnikov, A; Berdnikov, Y; Bhom, J H; Bickley, A A; Bjorndal, M T; Blau, D S; Boissevain, J G; Bok, J S; Borel, H; Borggren, N; Boyle, K; Brooks, M L; Brown, D S; Bucher, D; Buesching, H; Bumazhnov, V; Bunce, G; Burward-Hoy, J M; Butsyk, S; Campbell, S; Caringi, A; Cassano, N; Chai, J -S; Chang, B S; Charvet, J -L; Chen, C -H; Chernichenko, S; Chiba, J; Chi, C Y; Chiu, M; Choi, I J; Choi, J B; Choudhury, R K; Christiansen, P; Chujo, T; Chung, P; Churyn, A; Chvala, O; Cianciolo, V; Citron, Z; Cleven, C R; Cobigo, Y; Cole, B A; Comets, M P; del Valle, Z Conesa; Connors, M; Constantin, P; Csanad, M; Csorgo, T; Dahms, T; Dairaku, S; Danchev, I; Das, K; Datta, A; David, G; Dayananda, M K; Deaton, M B; Dehmelt, K; Delagrange, H; Denisov, A; d'Enterria, D; Deshpande, A; Desmond, E J; Dharmawardane, K V; Dietzsch, O; Dion, A; Donadelli, M; Orazio, L D; Drachenberg, J L; Drapier, O; Drees, A; Drees, K A; Dubey, A K; Durham, J M; Durum, A; Dutta, D; Dzhordzhadze, V; Edwards, S; Efremenko, Y V; Egdemir, J; Ellinghaus, F; Emam, W S; Engelmore, T; Enokizono, A; En'yo, H; Espagnon, B; Esumi, S; Eyser, K O; Fadem, B; Fields, D E; Finger, M; Finger, M; Fleuret, F; Fokin, S L; Forestier, B; Fraenkel, Z; Frantz, J E; Franz, A; Frawley, A D; Fujiwara, K; Fukao, Y; Fung, S -Y; Fusayasu, T; Gadrat, S; Garishvili, I; Gastineau, F; Germain, M; Glenn, A; Gong, H; Gonin, M; Gosset, J; Goto, Y; de Cassagnac, R Granier; Grau, N; Greene, S V; Grim, G; Perdekamp, M Grosse; Gunji, T; Gustafsson, H -A; Hachiya, T; Henni, A Hadj; Haegemann, C; Haggerty, J S; Hagiwara, M N; Hahn, K I; Hamagaki, H; Hamblen, J; Hanks, J; Han, R; Harada, H; Hartouni, E P; Haruna, K; Harvey, M; Haslum, E; Hasuko, K; Hayano, R; Heffner, M; Hemmick, T K; Hester, T; Heuser, J M; He, X; Hiejima, H; Hill, J C; Hobbs, R; Hohlmann, M; Holmes, M; Holzmann, W; Homma, K; Hong, B; Horaguchi, T; Hornback, D; Huang, S; Hur, M G; Ichihara, T; Ichimiya, R; Iinuma, H; Ikeda, Y; Imai, K; Inaba, M; Inoue, Y; Isenhower, D; Isenhower, L; Ishihara, M; Isobe, T; Issah, M; Isupov, A; Ivanischev, D; Iwanaga, Y; Jacak, B V; Jia, J; Jiang, X; Jin, J; Jinnouchi, O; Johnson, B M; Jones, T; Joo, K S; Jouan, D; Jumper, D S; Kajihara, F; Kametani, S; Kamihara, N; Kamin, J; Kaneta, M; Kang, J H; Kanou, H; Kapustinsky, J; Karatsu, K; Kasai, M; Kawagishi, T; Kawall, D; Kawashima, M; Kazantsev, A V; Kelly, S; Kempel, T; Khanzadeev, A; Kijima, K M; Kikuchi, J; Kim, A; Kim, B I; Kim, D H; Kim, D J; Kim, E J; Kim, E; Kim, Y -J; Kim, Y -S; Kinney, E; Kiss, A; Kistenev, E; Kiyomichi, A; Klay, J; Klein-Boesing, C; Kochenda, L; Kochetkov, V; Komkov, B; Konno, M; Koster, J; Kotchetkov, D; Kotov, D; Kozlov, A; Kral, A; Kravitz, A; Kroon, P J; Kubart, J; Kunde, G J; Kurihara, N; Kurita, K; Kurosawa, M; Kweon, M J; Kwon, Y; Kyle, G S; Lacey, R; Lai, Y S; Lajoie, J G; Lebedev, A; Le Bornec, Y; Leckey, S; Lee, D M; Lee, J; Lee, K B; Lee, K S; Lee, M K; Lee, T; Leitch, M J; Leite, M A L; Lenzi, B; Lichtenwalner, P; Liebing, P; Lim, H; Levy, L A Linden; Liska, T; Litvinenko, A; Liu, H; Liu, M X; Li, X; Li, X H; Love, B; Lynch, D; Maguire, C F; Makdisi, Y I; Malakhov, A; Malik, M D; Manko, V I; Mannel, E; Mao, Y; Masek, L; Masui, H; Matathias, F; McCain, M C; McCumber, M; McGaughey, P L; Means, N; Meredith, B; Miake, Y; Mibe, T; Mignerey, A C; Mikes, P; Miki, K; Miller, T E; Milov, A; Mioduszewski, S; Mishra, G C; Mishra, M; Mitchell, J T; Mitrovski, M; Mohanty, A K; Moon, H J; Morino, Y; Morreale, A; Morrison, D P; Moss, J M; Moukhanova, T V; Mukhopadhyay, D; Murakami, T; Murata, J; Nagamiya, S; Nagata, Y; Nagle, J L; Naglis, M; Nagy, M I; Nakagawa, I; Nakamiya, Y; Nakamura, K R; Nakamura, T; Nakano, K; Nam, S; Newby, J; Nguyen, M; Nihashi, M; Norman, B E; Nouicer, R; Nyanin, A S; Nystrand, J; Oakley, C; O'Brien, E; Oda, S X; Ogilvie, C A; Ohnishi, H; Ojha, I D; Okada, K; Oka, M; Omiwade, O O; Onuki, Y; Oskarsson, A; Otterlund, I; Ouchida, M; Ozawa, K; Pak, R; Pal, D; Palounek, A P T; Pantuev, V; Papavassiliou, V; Park, I H; Park, J; Park, S K; Park, W J; Pate, S F; Pei, H; Peng, J -C; Pereira, H; Peresedov, V; Peressounko, D Yu; Petti, R; Pinkenburg, C; Pisani, R P; Proissl, M; Purschke, M L; Purwar, A K; Qu, H; Rak, J; Rakotozafindrabe, A; Ravinovich, I; Read, K F; Rembeczki, S; Reuter, M; Reygers, K; Riabov, V; Riabov, Y; Richardson, E; Roach, D; Roche, G; Rolnick, S D; Romana, A; Rosati, M; Rosen, C A; Rosendahl, S S E; Rosnet, P; Rukoyatkin, P; Ruzicka, P; Rykov, V L

2010-01-01T23:59:59.000Z

317

D$_s^+$ meson production at central rapidity in proton-proton collisions at $\\sqrt{s}$ = 7 TeV  

E-Print Network (OSTI)

The pt-differential inclusive production cross section of the prompt charm-strange meson D$_s^+$ in the rapidity range |y|<0.5 was measured in proton--proton collisions at $\\sqrt{s}$=7 TeV at the LHC using the ALICE detector. The analysis was performed on a data sample of 2.98 10$^8$ events collected with a minimum-bias trigger. The corresponding integrated luminosity is $L_{int}=4.8 nb^{-1}$. Reconstructing the decay $D_s^+ \\to \\phi\\pi^+$, with $\\phi \\to K^-K^+$, and its charge conjugate, about 480 D$_s^{\\pm}$ mesons were counted, after selection cuts, in the transverse momentum range 2

Abelev, Betty; Adamova, Dagmar; Adare, Andrew Marshall; Aggarwal, Madan; Aglieri Rinella, Gianluca; Agocs, Andras Gabor; Agostinelli, Andrea; Aguilar Salazar, Saul; Ahammed, Zubayer; Ahmad, Nazeer; Ahmad, Arshad; Ahn, Sul-Ah; Ahn, Sang Un; Akindinov, Alexander; Aleksandrov, Dmitry; Alessandro, Bruno; Alfaro Molina, Jose Ruben; Alici, Andrea; Alkin, Anton; Almaraz Avina, Erick Jonathan; Alme, Johan; Alt, Torsten; Altini, Valerio; Altinpinar, Sedat; Altsybeev, Igor; Andrei, Cristian; Andronic, Anton; Anguelov, Venelin; Anielski, Jonas; Anson, Christopher Daniel; Anticic, Tome; Antinori, Federico; Antonioli, Pietro; Aphecetche, Laurent Bernard; Appelshauser, Harald; Arbor, Nicolas; Arcelli, Silvia; Arend, Andreas; Armesto, Nestor; Arnaldi, Roberta; Aronsson, Tomas Robert; Arsene, Ionut Cristian; Arslandok, Mesut; Asryan, Andzhey; Augustinus, Andre; Averbeck, Ralf Peter; Awes, Terry; Aysto, Juha Heikki; Azmi, Mohd Danish; Bach, Matthias Jakob; Badala, Angela; Baek, Yong Wook; Bailhache, Raphaelle Marie; Bala, Renu; Baldini Ferroli, Rinaldo; Baldisseri, Alberto; Baldit, Alain; Baltasar Dos Santos Pedrosa, Fernando; Ban, Jaroslav; Baral, Rama Chandra; Barbera, Roberto; Barile, Francesco; Barnafoldi, Gergely Gabor; Barnby, Lee Stuart; Barret, Valerie; Bartke, Jerzy Gustaw; Basile, Maurizio; Bastid, Nicole; Basu, Sumit; Bathen, Bastian; Batigne, Guillaume; Batyunya, Boris; Baumann, Christoph Heinrich; Bearden, Ian Gardner; Beck, Hans; Behera, Nirbhay Kumar; Belikov, Iouri; Bellini, Francesca; Bellwied, Rene; Belmont-Moreno, Ernesto; Bencedi, Gyula; Beole, Stefania; Berceanu, Ionela; Bercuci, Alexandru; Berdnikov, Yaroslav; Berenyi, Daniel; Bergognon, Anais Annick Erica; Berzano, Dario; Betev, Latchezar; Bhasin, Anju; Bhati, Ashok Kumar; Bhom, Jihyun; Bianchi, Livio; Bianchi, Nicola; Bianchin, Chiara; Bielcik, Jaroslav; Bielcikova, Jana; Bilandzic, Ante; Bjelogrlic, Sandro; Blanco, F; Blanco, Francesco; Blau, Dmitry; Blume, Christoph; Boccioli, Marco; Bock, Nicolas; Boettger, Stefan; Bogdanov, Alexey; Boggild, Hans; Bogolyubsky, Mikhail; Boldizsar, Laszlo; Bombara, Marek; Book, Julian; Borel, Herve; Borissov, Alexander; Bose, Suvendu Nath; Bossu, Francesco; Botje, Michiel; Botta, Elena; Boyer, Bruno Alexandre; Braidot, Ermes; Braun-Munzinger, Peter; Bregant, Marco; Breitner, Timo Gunther; Browning, Tyler Allen; Broz, Michal; Brun, Rene; Bruna, Elena; Bruno, Giuseppe Eugenio; Budnikov, Dmitry; Buesching, Henner; Bufalino, Stefania; Busch, Oliver; Buthelezi, Edith Zinhle; Caballero Orduna, Diego; Caffarri, Davide; Cai, Xu; Caines, Helen Louise; Calvo Villar, Ernesto; Camerini, Paolo; Canoa Roman, Veronica; Cara Romeo, Giovanni; Carena, Francesco; Carena, Wisla; Carlin Filho, Nelson; Carminati, Federico; Casanova Diaz, Amaya Ofelia; Castillo Castellanos, Javier Ernesto; Castillo Hernandez, Juan Francisco; Casula, Ester Anna Rita; Catanescu, Vasile; Cavicchioli, Costanza; Ceballos Sanchez, Cesar; Cepila, Jan; Cerello, Piergiorgio; Chang, Beomsu; Chapeland, Sylvain; Charvet, Jean-Luc Fernand; Chattopadhyay, Subhasis; Chattopadhyay, Sukalyan; Chawla, Isha; Cherney, Michael Gerard; Cheshkov, Cvetan; Cheynis, Brigitte; Chibante Barroso, Vasco Miguel; Chinellato, David; Chochula, Peter; Chojnacki, Marek; Choudhury, Subikash; Christakoglou, Panagiotis; Christensen, Christian Holm; Christiansen, Peter; Chujo, Tatsuya; Chung, Suh-Urk; Cicalo, Corrado; Cifarelli, Luisa; Cindolo, Federico; Cleymans, Jean Willy Andre; Coccetti, Fabrizio; Colamaria, Fabio; Colella, Domenico; Conesa Balbastre, Gustavo; Conesa del Valle, Zaida; Constantin, Paul; Contin, Giacomo; Contreras, Jesus Guillermo; Cormier, Thomas Michael; Corrales Morales, Yasser; Cortese, Pietro; Cortes Maldonado, Ismael; Cosentino, Mauro Rogerio; Costa, Filippo; Cotallo, Manuel Enrique; Crescio, Elisabetta; Crochet, Philippe; Cruz Alaniz, Emilia; Cuautle, Eleazar; Cunqueiro, Leticia; Dainese, Andrea; Dalsgaard, Hans Hjersing; Danu, Andrea; Das, Indranil; Das, Debasish; Das, Kushal; Dash, Sadhana; Dash, Ajay Kumar; De, Sudipan; de Barros, Gabriel; De Caro, Annalisa; de Cataldo, Giacinto; de Cuveland, Jan; De Falco, Alessandro; De Gruttola, Daniele; Delagrange, Hugues; Deloff, Andrzej; Demanov, Vyacheslav; De Marco, Nora; Denes, Ervin; De Pasquale, Salvatore; Deppman, Airton; D'Erasmo, Ginevra; de Rooij, Raoul Stefan; Diaz Corchero, Miguel Angel; Di Bari, Domenico; Dietel, Thomas; Di Giglio, Carmelo; Di Liberto, Sergio; Di Mauro, Antonio; Di Nezza, Pasquale; Divia, Roberto; Djuvsland, Oeystein; Dobrin, Alexandru Florin

2012-01-01T23:59:59.000Z

318

What's New in the Computational Biology Section  

NLE Websites -- All DOE Office Websites (Extended Search)

What's New? What's New? Kane, SR, Chakicherla, AY, Chain, PSG, Schmidt, R, Shin, MW, Legler, TC, Scow, KM, Larimer, FW, Lucas, SM, Richardson, PM, and Hristova, KR. (2007). Whole-Genome Analysis of the Methyl tert-Butyl Ether-Degrading Beta-Proteobacterium Methylibium petroleiphilum PM1. J. Bacteriol. 189(5): 1931-1945. PubMed Scott KM, Sievert SM, Abril FN, Ball LA, Barrett CJ, Blake RA, Boller AJ, Chain PS, Clark JA, Davis CR, Detter C, Do KF, Dobrinski KP, Faza BI, Fitzpatrick KA, Freyermuth SK, Harmer TL, Hauser LJ, Hugler M, Kerfeld CA, Klotz MG, Kong WW, Land M, Lapidus A, Larimer FW, Longo DL, Lucas S, Malfatti SA, Massey SE, Martin DD, McCuddin Z, Meyer F, Moore JL, Ocampo LH, Paul JH, Paulsen IT, Reep DK, Ren Q, Ross RL, Sato PY, Thomas P, Tinkham LE, Zeruth GT. (2006). The Genome of Deep-Sea Vent Chemolithoautotroph Thiomicrospira crunogena XCL-2. PLoS Biol. 4(12): e383. PubMed

319

NOI1VU1SININQV NOLLVINUOdNI A9H3N3 AO^HNH  

Gasoline and Diesel Fuel Update (EIA)

-661 J9QUJ9AON -661 J9QUJ9AON NOI1VU1SININQV NOLLVINUOdNI A9H3N3 AO^HNH 1661 '98902 00 'uoi6mi|SEM 'MS 'anuaAV aouapuadspui QOOl 'IG2-I3 'UOJIBJISIUILUPV UOIJBIUJOJUI 'yoo/jno Xfi/eu3 uuaj_-no^s o; sa6ueiJO ssejppe puas :yaiSVlNlSOd 'saojjjo BUIUBUI iBuomppe pus '8666-99002 OO 'uoiBingsEM JB p|Bd sBeisod ssep-puooag -(soiiou aouBApe >noni!/« a6uBi|o oj joafqns soud) jseA jed 00>L$ J J snas pus 'gggos 00 'uoj6u!MSBM 'MS 'enuoAV eouepuedepui oOOI-'uoiJBJisiuiijupv UOUBUUOJUI ABjaug agj Aq A|jaiJBnb pagsnqnd S] (t?090-Ct'/0 NSSl)^ooWO A6JSU3 UUB±-)JOLJS aqj. 1-661 '9 JOqiiieAON :6u!iuud JQJ p8SB9|9u -j-|AJ '8UIII UJ8JSB8 "LU'd S - 'WE 9 18U-989 (202) ^ '8lUI}UJaiSE8 "Urd g- 'WE 8 3MJ J 0) 2LS-202-LXVd 0088-989(202) 8E2E-E8/ (202) 98902 DO 'uo}6u|L|SBM

320

MESSAGE: WIA W/O CLOSING REF CLOSING REF  

Office of Legacy Management (LM)

MESSAGE: MESSAGE: WIA W/O CLOSING REF CLOSING REF _ CONSTRUCTION COMPL DATE J. King SAIC J. Waddell SAIC R. Wright SAIC T. Gangwer SAIC M. Khan SAIC T. Patterson SAIC R. Tucker SAIC C.Helie SAIC K. Renfro SAIC S. Heptinstall SAIC PLEASE RETURN TO PDCC FOR CORRECTIONS MGMT. SYSTEMS: PROGRAM ADMIN.: DEPUTY PROGRAM MGR: PROJECT MANAGER: () I PROGRAM MANAGER: I I ANL: AJ. Dvorak ANL A Geisler ANL G. Maraman ANL D. Dunning ANL J. Wing BNI DIRECTOR. FSRD: L Price FSRD DEP. DIRECTOR. FSRD: W.Seay FSRD SITE MANAGER: D.Adler FSRD " S. Cange FSRD R. Kirk FSRD J. Kopotic FSRD M. Nee FSRD PROJECT SUPPORT GRP: J.Hart FSRD S. Oldham FSRD 4- G. Hartman FSRD L Marz FSRD PRGM ANALYST: B. Hughlett FSRD SECRETARY: M. Seiber"''' Dyke FSRD FSRD CHRON FILE FSRD NOTEBOOKS READING FILE DOEIP&CD: French/Sistrunk DCO DOEIHO: J. Wagoner DHO RESeDNSE TRACKING INFORMATION SECONDARY: / : SECONDARY: ~ OWED TO: / lOWED

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321

Active Hydrogenation Catalyst with a Structured, Peptide-Based Outer-Coordination Sphere  

Science Conference Proceedings (OSTI)

The synthesis, catalytic activity, and structural features of a rhodium-based hydrogenation catalyst containing a phosphine ligand coupled to a 14-residue peptide are reported. Both CD and NMR spectroscopy show that the peptide adopts a helical structure in 1:1:1 TFE/MeCN/H2O that is maintained when the peptide is attached to the ligand and when the ligand is attached to the metal complex. The metal complex hydrogenates aqueous solutions of 3-butenol to 1-butanol at 360 50 turnovers/Rh/h at 294 K. This peptide- based catalyst represents a starting point for developing and characterizing a peptide-based outer-coordination sphere that can be used to introduce enzyme-like features into molecular catalysts. This work was funded by the US DOE Basic Energy Sciences, Chemical Sciences, Geoscience and Biosciences Division (AJ, JCL and WJS), the Office of Science Early Career Research Program through the Office of Basic Energy Sciences (GWB, MLR and WJS). Part of the research was conducted at the W.R. Wiley Environmental Molecular Sciences Laboratory, a national scientific user facility sponsored by U.S. Department of Energys Office of Biolog-ical and Environmental Research (BER) program located at Pacific Northwest National Laboratory (PNNL). PNNL is operated by Battelle for the U.S. Department of Energy.

Jain, Avijita; Buchko, Garry W.; Reback, Matthew L.; O'Hagan, Molly J.; Ginovska-Pangovska, Bojana; Linehan, John C.; Shaw, Wendy J.

2012-10-05T23:59:59.000Z

322

MR-CAT  

NLE Websites -- All DOE Office Websites (Extended Search)

MR-CAT, Materials Research Collaborative Access Team MR-CAT, Materials Research Collaborative Access Team 10-ID A bent Laue analyzer detection system for dilute fluorescence XAFS C. Karanfil, Z. Zhong, L.D. Chapman, R. Fischetti, C.U. Segre, B.A. Bunker, and G.B. Bunker Binding of Cd ions to the cell wall of B. Subtilis - an EXAFS study M. Boyanov, D. Fowle, K. Kemner, B. Bunker, and J. Fein Crystal structure of a new polymorph of sulfabenzamide J. Kaduk, S. Maginn, J. Cole, and K. Shankland Crystal structures of BaSrRTaO6 (R = Tm, Lu) J. Kaduk and W. Wong-Ng EXAFS and XANES of plutonium and uranium edges from titanate ceramics for fissile materials disposition J.A. Fortner, A.J. Kropf, R.J. Finch, M.C. Hash, S.B. Aase, and D.B. Chamberlain Formation of cyanide bridged networks at the air/water interface J. Culp, G. Weerasekera, D.R. Talham, and R. Duran

323

Residential Energy Consumption Survey: Housing Characteristics,  

Gasoline and Diesel Fuel Update (EIA)

tni tni Residential Energy Consumption Survey: Housing Characteristics, 1981 Energy Information Administration Washington. D.C August 1983 T86T -UJ9AO9 aiji uuojj pasenojnd uaaq (OdO) i|oii)/v\ suoijdijosqns o; Ajdde jou saop aoiiou :e|ON asBa|d 'pjBo^sod at|j noA j| 3Sj| Suiije'Lu vi3 3M1 uo ;u!Buuaj o^sn o} }i ujnja> isnoi nox 'pJBOisod iuB»jodoi! UB aABL) pjnons hoA '}s\\ BujUBUJ VI3 9L|} uo ajB noA|| 'MaiAaj jsij SUJMBUJ suouBOjiqnd |BnuuBS}j BUJ -jonpuoo Sj (vi3) uoijej^siujuupv UOIJBLUJOIUI Afijau^ agj 'uoiieinBaj iuaoiujaAOQ Aq pajmbaj sv 30HON 02-13 maoj aapao ay 05. pa^oajjp aq pus siuamnooa jo 0088-353 (303) S8SOZ "D'Q 'uoiSu-pqsBtt T rao°H 50 UOT^BOLIOJUI

324

LS-132  

NLE Websites -- All DOE Office Websites (Extended Search)

2 2 Kei th Symon November 1988 ANALYSIS OF THE WALKINSHAW DIFFERENCE RESONANCE In preparation for the Aladdin experiments, I will give an analytic treatment of the Walkinshaw difference resonance. The treatment nearly parallels that in LS-l3l for the third-integral resonance. I. Analysis of the Resonance The Hami 1 tonian in the neighborhood of the Wa lkinshaw resonance Vx - 2 vy = m (1.1) can be written in terms of angle-action variables in the form h V J +v J +S(2J )1/2(2J )sin(y -2y -m&+ç) xx yy x y x y +aJ 2+2bJ J +cJ 2 x x Y Y (1. 2) We first transform to resonant coordinates via the generating function F(Ji,J2,yx,yy,8) Ji(y -2y -m8+ç)+J2Y x y y (1.3 ) which gives Yl = Y - 2y - m8 + ç x Y Y2 yy (1.4 ) J x J 1 Jy = J 2 - 2J 1 (i.5 ) J 1 = J x J 2 J + 2J Y x (1. 6) 2 The resonant hamiltonian is

325

Property:PhoneNumber | Open Energy Information  

Open Energy Info (EERE)

PhoneNumber PhoneNumber Jump to: navigation, search This is a property of type String. Pages using the property "PhoneNumber" Showing 25 pages using this property. (previous 25) (next 25) 1 1st Light Energy, Inc. + 209-824-5500 + 2 21-Century Silicon, Inc. + 972-591-0713 + 3 3Degrees + 415.449.0500 + 3M + 1-888-364-3577 + 4 4C Offshore Limited + +44 (0)1502 509260 + 4th Day Energy + 877-484-3291 + @ @Ventures (California) + (650) 322-3246 + @Ventures (Massachusetts) + (978) 658-8980 + A A.J. Rose Manufacturing Company + 440-934-2859 + A.O. Smith + 414-359-4000 + A1 Sun, Inc. + (510) 526-5715 + A10 Power + 415-729-4A10 or 415-729-4210 + ABC Solar, Inc. + 1-866-40-SOLAR + ABS Alaskan Inc + (800) 235-0689 + ACME solar works + 877-226-3004 + ACORE + 202-393-0001 +

326

NEPA Review Routing Form  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

Concrete Storage Yard Concrete Storage Yard Document Number: 301 Date of Routing: 12/01/2010 (after MJT review 11/30/2010) Name Reviewed Signature Forwarded To Forwarded Date Date Anne Theriault 12/01/2010 ~ ..... --1 .L - Steve Ames 12/01/2010 Steve Ames 12/01/2010 :"#-~- /2--........, Email MJT 12/01/2010 Steve Ames 12/01/2010 s.£~ ~~ Jeff Christiansen 12/01/2010 ~ / / Jeff Christiansen 12/01/2010 /7~ A"' A'"~ Mike Taylor 12/01/2010 ~~"'' 1-4'1''-..t:P~ JZ-/2.//C> AJ El'l>S t..Ji!) ~K tf7TIJ c ,t/rtf f ~ !:z..Lz_L/.o , r S·rP:IIE At11Ef' .~ { L/lt:- ~.a A\ lt"L"' 1A'l1Al I 1-- I 'f../ /0 _.., _, ---r79 '(_L47 /2--. 12-/.L I IP ~L"/Y~A sn:vc 19"1r5 12-/2//P

327

I  

Office of Legacy Management (LM)

-,qy4 I _ -,qy4 I _ . I .__. ..-.- -....k ~&cTIAL USE UNL-T 0 L; : A I ,; ,' MN- I?%-(83 aj 0.3 ' f4lttaIIurgicaI lafioratorph k+ A- - p 111~ uu-mnt consists of _____. 5 ___-- .^_. F%es and.--m_m - No...---:- ---.- -.---_ Q- -15 ____ of b ,,;-+~----c------ __-_ figures - --------=-.LupieS, &je3me-&vw-y wu Readers File. - UT, h 5 lDcnLats* P&r W% l290 ma - , (1k.h kas tl61t6d xb&eeTTiul~onf aQ At the pmumat * guwxwlm on Pun* PM thracr htiheu 'ba% &+#8' end one en tiho flnl6hlBaiq 0 hb &um8 &6k4:4 t?Lo aKr0 ar eseallOZVb* ua lfo na@ifibUs A v6atiZatici~1, aycptu ha Q63&u#eoat~e~ln~ilLiua8~d#~~m~i0 pwtt;:3.tQtorr, ltio8aspLw~~~OQa-~lllCI)brrL# tmhIp sum wh6 I)&, mrdraTl6g frw droar vm6 84 cflaplpl+ktaa6xt~moma*~(~}ww

328

STATEJVU:NT OF CONSIJ mnATIONS RFQllEST B'{ CREE, JNC. (CREE) FOR AN ADV!' NCE \V ;\JVER OF DOrv1ESTIC AND  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

STATEJVU:NT OF CONSIJ mnATIONS STATEJVU:NT OF CONSIJ mnATIONS RFQllEST B'{ CREE, JNC. (CREE) FOR AN ADV!' NCE \V ;\JVER OF DOrv1ESTIC AND FOREIGN PATENT RICI HTS l DER NRFL Si IBCONTRACT NFT-2-224'.26-0l: \V(AJ-2012-0(f The Petitioner, Cree, hns requested a waiver of d imestic and f(m::ign patent rights for all subject inventions arising from its participation under th' above referenced subcontract entitled .. Gearbox Design for U.S.-SourcccL Next ()cneration Dr Vclrain f'or Land-Based and Offshore Wind Turbines;' Cree is a subcumrnctor to the National 1~1.·newnbk Fnergy L<1boratory (NRFL). l Jndcr its subcontract\\ ith NREL. Cree is perfrirming wcrk ll.tnlkd under DF-FOA-0000439. U.S. Wind Power: Next Generation Drivetrain Den:lopmcnt. Under this award. NREL is leading the

329

Toxicity of ionic liquids to Clostridium sp. and effects on uranium biosorption  

NLE Websites -- All DOE Office Websites (Extended Search)

of Hazardous Materials 264 (2014) 246- 253 of Hazardous Materials 264 (2014) 246- 253 Contents lists available at ScienceDirect Journal of Hazardous Materials j o u r n a l h o m e p a g e : w w w . e l s e v i e r . c o m / l o c a t e / j h a z m a t Toxicity of ionic liquids to Clostridium sp. and effects on uranium biosorption C. Zhang a,b,∗ , S.V. Malhotra b,1 , A.J. Francis c,d a College of Environmental Science and Engineering, Nankai University, Tianjin, China 300071 b Department of Chemistry and Environmental Science, New Jersey Institute of Technology, Newark, NJ 07104 USA c Environmental Sciences Department, Brookhaven National Laboratory, Upton, NY 11973 USA d Division of Advanced Nuclear Engineering, Pohang University of Science and Technology, Pohang, 790-784 South Korea h i g h l i g h t s * Three ILs showed varying degrees of toxicity to Clostridium sp.

330

Seven Data Sets Released from LBA Carbon Dynamics and Trace Gas Teams  

NLE Websites -- All DOE Office Websites (Extended Search)

Data Sets Released from LBA Carbon Dynamics and Trace Gas Teams Data Sets Released from LBA Carbon Dynamics and Trace Gas Teams The ORNL DAAC and the LBA DIS announce the release of four data sets from the Carbon Dynamics teams and three data sets from the Trace Gas and Aerosol Fluxes science teams, components of the LBA-ECO Large Scale Biosphere-Atmosphere Experiment in Amazonia (LBA). LBA-ECO CD-02 C and N Isotopes in Leaves and Atmospheric CO2, Amazonas, Brazil . Data set prepared by A.C. de Araujo, J.P.H.B. Ometto, A.J. Dolman, B. Kruijt, M.J. Waterloo and J.R. Ehleringer. This data set reports delta 13C/12C results for leaf tissues and atmospheric carbon dioxide (CO2), delta 15N/14N ratios for leaf tissue, and leaf carbon and nitrogen concentrations along a topographical gradient in old-growth forests near Manaus, Amazonas, Brazil. Also included are coincident

331

Proceedings of the 34th International Conference in High Energy Physics (ICHEP08), Philadelphia, PA, 2008, eConf C080730, [hep-ph/0809.xxx  

SciTech Connect

In 2004 a team from the University of Pennsylvania, Princeton University, and the Institute for Advanced Study proposed to host the 2008 International Conference on High Energy Physics (ICHEP) on the campus of the University of Pennsylvania in Philadelphia. The proposal was approved later that year by the C-11 committee of the International Union of Pure and Applied Physics. The Co-Chairs were Nigel S. Lockyer (U. Penn/TRIUMF) and A.J. Stewart Smith (Princeton); Joe Kroll of U. Penn served as Deputy Chair from 2007 on. Highlights of the proposal included 1. greatly increased participation of young scientists, women scientists, and graduate students 2. new emphasis on formal theory 3. increased focus on astrophysics and cosmology 4. large informal poster session (170 posters) in prime time 5. convenient, contiguous venues for all sessions and lodging 6. landmark locations for the reception and banquet. The conference program consisted of three days of parallel sessions and three days of plenary talks.

Lockyer, Nigel S.; Smith, AJ Stewart,; et. al.

2008-09-01T23:59:59.000Z

332

A Framework for Automating Cost Estimates in Assembly Processes  

SciTech Connect

When a product concept emerges, the manufacturing engineer is asked to sketch out a production strategy and estimate its cost. The engineer is given an initial product design, along with a schedule of expected production volumes. The engineer then determines the best approach to manufacturing the product, comparing a variey of alternative production strategies. The engineer must consider capital cost, operating cost, lead-time, and other issues in an attempt to maximize pro$ts. After making these basic choices and sketching the design of overall production, the engineer produces estimates of the required capital, operating costs, and production capacity. 177is process may iterate as the product design is refined in order to improve its pe~ormance or manufacturability. The focus of this paper is on the development of computer tools to aid manufacturing engineers in their decision-making processes. This computer sof~are tool provides aj?amework in which accurate cost estimates can be seamlessly derivedfiom design requirements at the start of any engineering project. Z+e result is faster cycle times through first-pass success; lower ll~e cycie cost due to requirements-driven design and accurate cost estimates derived early in the process.

Calton, T.L.; Peters, R.R.

1998-12-09T23:59:59.000Z

333

The role of GRB 031203 in clarifying the astrophysical GRB scenario  

E-Print Network (OSTI)

The luminosity and the spectral distribution of the afterglow of GRB 031203 have been presented within our theoretical framework, which envisages the GRB structure as composed by a proper-GRB, emitted at the transparency of an electron-positron plasma with suitable baryon loading, and an afterglow comprising the "prompt emission" as due to external shocks. In addition to the GRB emission, there appears to be a prolonged soft X-Ray emission lasting for 10^6-10^7 seconds followed by an exponential decay. This additional source has been called by us URCA-3. It is urgent to establish if this component is related to the GRB or to the Supernova (SN). In this second case, there are two possibilities: either the interaction of the SN ejecta with the interstellar medium or, possibly, the cooling of a young neutron star formed in the SN 2003lw process. The analogies and the differences between this triptych GRB 031203 / SN 2003lw / URCA-3 and the corresponding ones GRB 980425 / SN 1998bw / URCA-1 and GRB 030329 / SN 2003dh / URCA-2, as well as GRB 060218 / SN 2006aj are discussed.

Remo Ruffini; Maria Grazia Bernardini; Carlo Luciano Bianco; Letizia Caito; Pascal Chardonnet; Maria Giovanna Dainotti; Federico Fraschetti; Roberto Guida; Gregory Vereshchagin; She-Sheng Xue

2007-05-16T23:59:59.000Z

334

Retrofit of waste-to-energy facilities equipped with electrostatic precipitators. Volume III: Test protocol  

DOE Green Energy (OSTI)

The American Society of Mechanical Engineers' [ASME] Center for Research and Technology Development [CRTD] has been awarded a subcontract by the National Renewable Energy Laboratory [NREL] to demonstrate the technical performance and viability of flue gas temperature control in combination with dry acid gas reagent and activated carbon injection at an existing electrostatic precipitator [ESP] equipped municipal waste combustor [MWC]. The objective of this proof-of-concept demonstration test is to economically and reliably meet 40 CFR 60 Subpart Cb Emissions Guidelines for MWC's at existing ESP equipped facilities. The effort is being directed by a Subcommittee of tile ASME Research Committee on Industrial and Municipal Wastes [RCIMW] chaired by Dave Hoecke. Mr. Greg Barthold of ASME/CRTD is the Project Manager. ASME/CRTD contracted with Rigo & Rigo Associates, Inc. in cooperation with A.J. Chandler & Associates, Ltd. to be the Principal Investigator for the project and manage the day-t o-day aspects of the program, conduct the testing reduce and interpret the data and prepare the report. Testing will be conducted at the 2 by 210 TPD, ESP equipped MWC at the Davis County Resource Recovery Facility in Layton, Utah. The test plan calls for duplicate metals (Cd, Pb and Hg), dioxin and acid gas runs.

Rigo, H.G. [Rigo & Rigo Associates, Inc., Berea, OH (US); Chandler, A.J. [A.J. Chandler & Associates, Inc., Toronto, Ontario (Canada)

1996-04-01T23:59:59.000Z

335

Modelling of Carbide and Laves Phase Precipitation in 9-12 wt% Chromium Steels  

E-Print Network (OSTI)

;707`j_*-9;R-.#7;9;?",EKF,EDE78.01FDE137[OkU'4@2#7;4;L-LJ.09%l#19;1F=#17;4;70,/K3Om*J4@K3?a70*J4@7#7;.0,/h#19;R-13.8,EH 13:nc@d;o@emp qr4@D *#19;70,/.a4;:-Hnst:-:J1328utc@d;d@o;v3Wrw-13:JDE,x70*J,y,E4;.0KFOMc@d@z;e@2Q13:JDE.8,E4;28,EHnDE9@:JDE,/.0:n9... ,E4@78,E.?70*J4@:#7;78*-4;7'1F:x:#19;RJDEKF,E4@. LJK34@:#19;7#17;p qr,/1328=I4@:{4;:-H{stD i%4@.870u#3;c;d@z;o@v3W6)+*-,a*J13<;*{2870.8,E:-<;70*{d;c;?@U+70??}G.?2878,E,EKF2/?4;.0,a78*-,E.8,E?#18;9;.0,aAC,/13:J< V[:n70*J132QU'9;.8iM70*J,x70...

Robson, Joseph Douglas

1997-01-28T23:59:59.000Z

336

ORIGINAL PAPER Initial characterization of Pf62, a novel protein of Plasmodium falciparum identified by immunoscreening  

E-Print Network (OSTI)

# The Author(s) 2009. This article is published with open access at Springerlink.com Abstract In order to find new antigens from Plasmodium falciparum, a complementary DNA (cDNA) library was constructed and screened. The study of expression library of P. falciparum was performed in an attempt to identify new antigens that could have potential relevance for the falciparum-malaria diagnosis and/or protection. Between the positive clones detected (ring erythrocyte surface antigen, merozoite erythrocyte surface antigen, RHOP H3, CSP, LSA), a new gene that correspond to a new protein (Pf62) was isolated and characterized. This antigen was useful for the diagnosis of malaria in enzyme-linked immunosorbent assay tests. The cDNA corresponding to this antigen and structure of the gene were characterized. Pf62 is a single copy gene that contains one exon. The Pf62 cDNA has an open reading frame of 1,599 nucleotides that code for a putative protein of 532 amino acids with a predicted molecular mass of 62 kDa. The polypeptide contains in the central section two regions of repeats of 21 and 19 amino Nucleotide sequence data reported in this paper are available in the Genbank database under the accession number AJ 493426.

Eva M. Moyano; Luis Miguel Gonzlez; Estrella Montero; Laureano Cuevas; Esperanza Perez-pastrana; Ysmael Santa-maria; Agustn Benito; E. Montero

2008-01-01T23:59:59.000Z

337

Diversity of the Supernova - Gamma-Ray Burst Connection  

E-Print Network (OSTI)

The connection between the long Gamma Ray Bursts (GRBs) and Type Ic Supernovae (SNe) has revealed interesting diversity. We review the following types of the GRB-SN connection. (1) GRB-SNe: The three SNe all explode with energies much larger than those of typical SNe, thus being called Hypernovae (HNe). They are massive enough for forming black holes. (2) Non-GRB HNe/SNe: Some HNe are not associated with GRBs. (3) XRF-SN: SN 2006aj associated with X-Ray Flash 060218 is dimmer than GRB-SNe and has very weak oxygen lines. Its progenitor mass is estimated to be small enough to form a neutron star rather than a black hole. (4) Non-SN GRB: Two nearby long GRBs were not associated SNe. Such ``dark HNe'' have been predicted in this talk (i.e., just before the discoveries) in order to explain the origin of C-rich (hyper) metal-poor stars. This would be an important confirmation of the Hypernova-First Star connection. We will show our attempt to explain the diversity in a unified manner with the jet-induced explosion model.

K. Nomoto; N. Tominaga; M. Tanaka; K. Maeda; T. Suzuki; J. S. Deng; P. A. Mazzali

2007-02-19T23:59:59.000Z

338

NF45/ILF2 tissue expression, promoter analysis, and interleukin-2 transactivating function  

SciTech Connect

NF45/ILF2 associates with NF90/ILF3 in the nucleus and regulates IL-2 gene transcription at the antigen receptor response element (ARRE)/NF-AT DNA target sequence (P.N. Kao, L. Chen, G. Brock, J. Ng, A.J. Smith, B. Corthesy, J. Biol. Chem. 269 (1994) 20691-20699). NF45 is widely expressed in normal tissues, especially testis, brain, and kidney, with a predominantly nuclear distribution. NF45 mRNA expression is increased in lymphoma and leukemia cell lines. The human and murine NF45 proteins differ only by substitution of valine by isoleucine at amino acid 142. Fluorescence in situ hybridization localized the human NF45 gene to chromosome 1q21.3, and mouse NF45 gene to chromosome 3F1. Promoter analysis of 2.5 kB of the murine NF45 gene reveals that significant activation is conferred by factors, possible including NF-Y, that bind to the CCAAT-box sequence. The function of human NF45 in regulating IL-2 gene expression was characterized in Jurkat T-cells stably transfected with plasmids directing expression of NF45 cDNA in sense or antisense orientations. NF45 sense expression increased IL-2 luciferase reporter gene activity 120-fold, and IL-2 protein expression 2-fold compared to control cells. NF45 is a highly conserved, regulated transcriptional activator, and one target gene is IL-2.

Zhao Guohua [Division of Pulmonary and Critical Care Medicine, Stanford University Medical Center, 300 Pasteur Drive, Stanford, CA 94305-5236 (United States); Shi Lingfang [Division of Pulmonary and Critical Care Medicine, Stanford University Medical Center, 300 Pasteur Drive, Stanford, CA 94305-5236 (United States); Qiu Daoming [Division of Pulmonary and Critical Care Medicine, Stanford University Medical Center, 300 Pasteur Drive, Stanford, CA 94305-5236 (United States); Hu Hong [Division of Pulmonary and Critical Care Medicine, Stanford University Medical Center, 300 Pasteur Drive, Stanford, CA 94305-5236 (United States); Kao, Peter N. [Division of Pulmonary and Critical Care Medicine, Stanford University Medical Center, 300 Pasteur Drive, Stanford, CA 94305-5236 (United States)]. E-mail: peterkao@stanford.edu

2005-05-01T23:59:59.000Z

339

Pure state quantum statistical mechanics and black holes  

E-Print Network (OSTI)

Chapter 3 of S. Lloyd's 1988 Ph.D. thesis, `Black Holes, Demons, and the Loss of Coherence: How complex systems get information and what they do with it,' supervisor Heinz Pagels. Reformulates statistical mechanics in terms of pure states and shows that (a) quantum statistics of typical pure states are very close to the mechanics of statistical mechanical ensembles; (b) if a system is in a typical state with energy E, then the reduced density matrix of a subsystem is very close to a thermal state. (A similar result was derived using Levy's lemma some years later by S. Popescu, A.J. Short, A.Winter, Nature Physics 2, 754-758 (2006).) Pure state quantum statistical mechanics is applied to black holesto show that for typical states of matter insideand outside a black hole, the external state is likely to be thermal. Proposes novel interpretation of probabilities in quantum statistical mechanics. Full thesis available at http://meche.mit.edu/documents/slloyd_thesis.pdf. This chapter was submitted for publication to Physical Review in 1988 but rejected by one sentence referee report: `There is no physics in this paper.' You be the judge.

Seth Lloyd

2013-07-01T23:59:59.000Z

340

Large scale total synthesis of apoptolidinone and progress towards the total synthesis of ammocidin  

E-Print Network (OSTI)

Apoptolidin 1.1 was isolated in 1997 by Hayakawa and co-workers from a soil bacterium Nocardiopsis sp. during screening for specific apoptosis inducers. The primary biological test revealed that this polyketide macrolide induced apoptosis in cells transformed with the adenovirus type E1A oncognene, but not normal cells. This dissertation describes the latest studies in understanding of apoptolidins biological activity mechanism and previous contributions towards its total synthesis. Synthesizing apoptolidinone 1.26 by an intra-molecular Horner-Wadsworth-Emmons approach featuring a Suzuki coupling, cross metathesis and two diastereoselective aldol reactions is discussed. 15 mg apoptolidinone is prepared via our previously developed intramolecular Suzuking coupling approach. Ammocidin 3.1, which was found to induce apoptosis in Ba/F3-v12 cells in an IL- 3 free medium, is a specific apoptosis inducer discovered by Hayakawa and co-workers in 2001 from Saccharothrix sp. AJ9571. A strategy featuring Suzuki coupling, cross metathesis, Yamaguchi macrolactonization and three asymmetric aldol reactions was applied to the total synthesis of ammocidinone 3.6, the aglycone of ammocidin. The preparation of the key building blocks was discussed in the following chapter: aldehyde 3.8 (C14-C19) was synthesized via Sharpless asymmetric epoxidation; ethyl ketone 3.9 (C20-C28) was prepared via Kobayashi and Crimminss asymmetric aldol methodologies; aldehyde 3.14 (C7-C13) was generated by Brown crotylation and cross metathesis.

Liu, Qingsong

2006-12-01T23:59:59.000Z

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341

Ultra Wideband (UWB) communication vulnerability for security applications.  

Science Conference Proceedings (OSTI)

RF toxicity and Information Warfare (IW) are becoming omnipresent posing threats to the protection of nuclear assets, and within theatres of hostility or combat where tactical operation of wireless communication without detection and interception is important and sometimes critical for survival. As a result, a requirement for deployment of many security systems is a highly secure wireless technology manifesting stealth or covert operation suitable for either permanent or tactical deployment where operation without detection or interruption is important The possible use of ultra wideband (UWB) spectrum technology as an alternative physical medium for wireless network communication offers many advantages over conventional narrowband and spread spectrum wireless communication. UWB also known as fast-frequency chirp is nonsinusoidal and sends information directly by transmitting sub-nanosecond pulses without the use of mixing baseband information upon a sinusoidal carrier. Thus UWB sends information using radar-like impulses by spreading its energy thinly over a vast spectrum and can operate at extremely low-power transmission within the noise floor where other forms of RF find it difficult or impossible to operate. As a result UWB offers low probability of detection (LPD), low probability of interception (LPI) as well as anti-jamming (AJ) properties in signal space. This paper analyzes and compares the vulnerability of UWB to narrowband and spread spectrum wireless network communication.

Cooley, H. Timothy

2010-07-01T23:59:59.000Z

342

Gluon Fusion Processes at One-loop within the Standard Model and Beyond  

E-Print Network (OSTI)

In this thesis, we have studied certain gluon fusion processes which proceed via quark loop diagrams at the leading order. The fact that these gluon-gluon channel processes are independent processes, their contributions towards the total/differential hadronic cross sections can be calculated separately. We have considered the production of a pair of electroweak vector bosons in association with a jet via gluon fusion within the standard model. These processes were not accessible at earlier hadron colliders such as the Tevatron. Therefore, observation of these rare processes at the LHC will be a test of the standard model itself. Like the di-vector boson production via gluon fusion processes, these processes are also important backgrounds for many new physics signals, and the standard model Higgs boson signal at the LHC. These leading order gluon fusion processes contribute to the corresponding hadronic processes at the next-to-next-to-leading order in {\\alpha}_s. We have taken a model of extra-dimensions, the ADD (Arkani-Hamed, Dimopoulos and Dvali) model, as the possible candidate of new physics at the LHC. This model tries to solve the hierarchy problem of the standard model by proposing large extra space dimensions which may be accessible at TeV scale. We have considered the direct production of KK-gravitons (GKK) in association with an electroweak boson (H/{\\gamma}/Z) via gluon fusion. These processes contribute to the corresponding hadronic processes at the next-to-leading order in {\\alpha}_s. Many interesting issues related to the fermion loop amplitudes have also been discussed.

Ambresh Shivaji

2013-05-21T23:59:59.000Z

343

Photoproduction of the K+ K0-(1750)  

SciTech Connect

While photoproduction has often been advertised as an important environment in which to study light meson spectroscopy, solid experimental results are sparse. In fact, beyond the relatively straightforward photoproduction of the {rho}, {omega}, and {phi} mesons, the few results of exclusive photoproduction that do exist are poorly understood, and several, perhaps, have even been misinterpreted. After extensively reviewing the sometimes tenuous history of the exclusive photoproduction of the ''{rho}{sup 1}(1600)'', the ''{omega}{pi}{sup 0}(1250)'', the ''{omega}(1650)'', and the ''K{sup +}K{sup -}(1750)'', new results from the E831/FOCUS photoproduction experiment at Fermilab are presented which address the interpretation of the K{sup +}K{sup -}(1750). This enhancement in low-p{sub T} K{sup +}K{sup -} pairs at a mass near 1750 MeV/c{sup 2} has been observed by several previous photoproduction experiments, but, despite several apparent inconsistencies, it has always been interpreted as the J{sup PC} = 1{sup --} {phi}(1680) meson. With nearly two orders of magnitude more events than any previous observation of the K{sup +}K{sup -}(1750), and based on precise measurements of its mass and width, and its absence from the K*K final state, the FOCUS data can finally render this interpretation implausible. In addition, several steps have been taken towards establishing a new interpretation. Based on limited angular analyses of its decay and the beam energy dependence of its production, they argue that, in the absence of any wild interference scenarios, the K{sup +}K{sup -}(1750) has J{sup PC} {ne} 1{sup --}, and, in fact, the most likely assignment appears to be 2{sup ++}. It is hoped that this work can help set the stage for future reevaluations and new insights in photoproduction.

Mitchell, Ryan Edward; /Tennessee U.

2003-01-01T23:59:59.000Z

344

Photocatalytic degradation of oil industry hydrocarbons models at laboratory and at pilot-plant scale  

Science Conference Proceedings (OSTI)

Photodegradation/mineralization (TiO{sub 2}/UV Light) of the hydrocarbons: p-nitrophenol (PNP), naphthalene (NP) and dibenzothiophene (DBT) at three different reactors: batch bench reactor (BBR), tubular bench reactor (TBR) and tubular pilot-plant (TPP) were kinetically monitored at pH = 3, 6 and 10, and the results compared using normalized UV light exposition times. The results fit the Langmuir-Hinshelwood (LH) model; therefore, LH adsorption equilibrium constants (K) and apparent rate constants (k) are reported as well as the apparent pseudo-first-order rate constants, k{sub obs}{sup '} = kK/(1 + Kc{sub r}). The batch bench reactor is the most selective reactor toward compound and pH changes in which the reactivity order is: NP > DBT > PNP, however, the catalyst adsorption (K) order is: DBT > NP > PNP at the three pH used but NP has the highest k values. The tubular pilot-plant (TPP) is the most efficient of the three reactors tested. Compound and pH photodegradation/mineralization selectivity is partially lost at the pilot plant where DBT and NP reaches ca. 90% mineralization at the pH used, meanwhile, PNP reaches only 40%. The real time, in which these mineralization occur are: 180 min for PNP and 60 min for NP and DBT. The mineralization results at the TPP indicate that for the three compounds, the rate limiting step is the same as the degradation one. So that, there is not any stable intermediate that may accumulate during the photocatalytic treatment. (author)

Vargas, Ronald; Nunez, Oswaldo [Laboratorio de Fisicoquimica Organica y Quimica Ambiental, Departamento de Procesos y Sistemas, Universidad Simon Bolivar, Apartado Postal 89000, Caracas (Venezuela)

2010-02-15T23:59:59.000Z

345

Vortex Lattice Structures of a Bose-Einstein Condensate in a Rotating Lattice Potential  

E-Print Network (OSTI)

We study vortex lattice structures of a trapped Bose-Einstein condensate in a rotating lattice potential by numerically solving the time-dependent Gross-Pitaevskii equation. By rotating the lattice potential, we observe the transition from the Abrikosov vortex lattice to the pinned lattice. We investigate the transition of the vortex lattice structure by changing conditions such as angular velocity, intensity, and lattice constant of the rotating lattice potential. PACS numbers: 03.75.Lm, 03.75.Kk Quantized vortices are one of the most characteristic manifestations of superfluidity associated with a Bose-Einstein condensate (BEC) in atomic gases. By rotating anisotropic trap potentials, several experimental groups observed formation of triangular Abrikosov lattices of vortices in rotating BECs 1,2,3. Microscopic mechanism of the vortex lattice formation has been extensively studied both analytically and numerically using the Gross-Pitaevskii (GP) equation for the condensate wavefunction 4,5,6,7,8,9,10,11. More recently, the vortex phase diagrams of a BEC in rotating lattice potentials have attracted theoretical attention, since one expects vortex pinning and structural phase transition of vortex lattice structures 12,13,14. Recently, a rotating lattice has been experimentally realized at JILA, makinig use of a laser beam passing through a rotating mask 12. Stimulated by the recent JILA experiment, in this paper, we study vortex lattice structures of a BEC in a rotating triangular lattice potential created by blue-detuned laser beams. We numerically solve the two-dimensional Gross-Pitaevskii (GP) equa-T. Sato, T. Ishiyama and T. Nikuni Fig. 1. Density profile (a) and Structure factor profile (b) of BEC in the lattice potential. The lattice potential geometry is triangular lattice at a/aho = 2.2 and ?/aho = 0.65. tion in a frame rotationg with anguler velocity ?: (i ? ?)h ??(r,t)

Toshihiro Sato; Tomohiko Ishiyama; Tetsuro Nikuni

2006-01-01T23:59:59.000Z

346

Cloning of the canine glucose-6-phosphatase gene  

SciTech Connect

Two Maltese puppies with massive hepatomegaly and failure to thrive were found to have a markedly reduced Glucose-6-phosphatase (G-6-Pase) activity in the liver and kidney. Deficiency of G-6-Pase activity causes type 1a glycogen storage disease in humans. To further study the mutation responsible for the disease in dog, we cloned G-6-Pase canine cDNA from normal mixed breed dog liver RNA using reverse transcriptase and PCR amplification using primers derived from the published murine G-6-Pase gene sequence. Sequencing revealed an open reading frame of 1071 nucleotides that encodes a predicted 357 amino acid polypeptide in the canine G-6-Pase gene, same as mouse and human. We found more than 90% sequence homology between dog and human G-6-Pase sequence. Hydropathy analysis of the deduced canine G-6-Pase polypeptide shows six transmembrane-spanning segments similar to those seen in human and mouse. Endoplasmic reticulum (ER) localization is similarly predicted by the presence of the ER protein retention signal KK positioned 3 and 4 amino acids from the carboxy terminal. Potential asparagine-linked glycosylation sites are identified at positions 96, 203, and 276. Northern blot analysis revealed increased G-6-Pase mRNA in the deficient dog liver compared to control. This could possibly reflect upregulation of transcription due to the persistent hypoglycemic state. Further studies are directed at the identification of the mutation involved in this deficient dog strain. Characterization of the G-6-Pase gene and protein in the deficient dog model can pave the way for new understanding in the pathophysiology of this disease and for the trials of novel therapeutic approaches including gene therapy.

Kishnani, P.; Bao, Y. [Duke University Medical Center, Durham, NC (United States); Brix, A.E. [and others

1994-09-01T23:59:59.000Z

347

Nuclear modification factors of phi mesons in d+Au, Cu+Cu and Au+Au collisions at sqrt(S_NN)=200 GeV  

E-Print Network (OSTI)

The PHENIX experiment at the Relativistic Heavy Ion Collider (RHIC) has performed systematic measurements of phi meson production in the K+K- decay channel at midrapidity in p+p, d+Au, Cu+Cu and Au+Au collisions at sqrt(S_NN)=200 GeV. Results are presented on the phi invariant yield and the nuclear modification factor R_AA for Au+Au and Cu+Cu, and R_dA for d+Au collisions, studied as a function of transverse momentum (1phi exhibits a suppression relative to expectations from binary scaled p+p results. The amount of suppression is smaller than that of the neutral pion and the eta meson in the intermediate p_T range (2--5 GeV/c); whereas at higher p_T the phi, pi^0, and eta show similar suppression. The baryon (protons and anti-protons) excess observed in central Au+Au collisions at intermediate p_T is not observed for the phi meson despite the similar mass of the proton and the phi. This suggests that the excess is linked to the number of constituent quarks rather than the hadron mass. The difference gradually disappears with decreasing centrality and for peripheral collisions the R_AA values for both particles are consistent with binary scaling. Cu+Cu collisions show the same yield and suppression as Au+Au collisions for the same number of N_part. The R_dA of phi shows no evidence for cold nuclear effects within uncertainties.

PHENIX Collaboration; A. Adare; S. Afanasiev; C. Aidala; N. N. Ajitanand; Y. Akiba; H. Al-Bataineh; J. Alexander; A. Al-Jamel; A. Angerami; K. Aoki; L. Aphecetche; Y. Aramaki; R. Armendariz; S. H. Aronson; J. Asai; E. T. Atomssa; R. Averbeck; T. C. Awes; B. Azmoun; V. Babintsev; M. Bai; G. Baksay; L. Baksay; A. Baldisseri; K. N. Barish; P. D. Barnes; B. Bassalleck; A. T. Basye; S. Bathe; S. Batsouli; V. Baublis; F. Bauer; C. Baumann; A. Bazilevsky; S. Belikov; R. Belmont; R. Bennett; A. Berdnikov; Y. Berdnikov; J. H. Bhom; A. A. Bickley; M. T. Bjorndal; D. S. Blau; J. G. Boissevain; J. S. Bok; H. Borel; N. Borggren; K. Boyle; M. L. Brooks; D. S. Brown; D. Bucher; H. Buesching; V. Bumazhnov; G. Bunce; J. M. Burward-Hoy; S. Butsyk; S. Campbell; A. Caringi; N. Cassano; J. -S. Chai; B. S. Chang; J. -L. Charvet; C. -H. Chen; S. Chernichenko; J. Chiba; C. Y. Chi; M. Chiu; I. J. Choi; J. B. Choi; R. K. Choudhury; P. Christiansen; T. Chujo; P. Chung; A. Churyn; O. Chvala; V. Cianciolo; Z. Citron; C. R. Cleven; Y. Cobigo; B. A. Cole; M. P. Comets; Z. Conesa del Valle; M. Connors; P. Constantin; M. Csanad; T. Csorgo; T. Dahms; S. Dairaku; I. Danchev; K. Das; A. Datta; G. David; M. K. Dayananda; M. B. Deaton; K. Dehmelt; H. Delagrange; A. Denisov; D. d'Enterria; A. Deshpande; E. J. Desmond; K. V. Dharmawardane; O. Dietzsch; A. Dion; M. Donadelli; L. D Orazio; J. L. Drachenberg; O. Drapier; A. Drees; K. A. Drees; A. K. Dubey; J. M. Durham; A. Durum; D. Dutta; V. Dzhordzhadze; S. Edwards; Y. V. Efremenko; J. Egdemir; F. Ellinghaus; W. S. Emam; T. Engelmore; A. Enokizono; H. En'yo; B. Espagnon; S. Esumi; K. O. Eyser; B. Fadem; D. E. Fields; M. Finger Jr.; M. Finger; F. Fleuret; S. L. Fokin; B. Forestier; Z. Fraenkel; J. E. Frantz; A. Franz; A. D. Frawley; K. Fujiwara; Y. Fukao; S. -Y. Fung; T. Fusayasu; S. Gadrat; I. Garishvili; F. Gastineau; M. Germain; A. Glenn; H. Gong; M. Gonin; J. Gosset; Y. Goto; R. Granier de Cassagnac; N. Grau; S. V. Greene; G. Grim; M. Grosse Perdekamp; T. Gunji; H. -A. Gustafsson; T. Hachiya; A. Hadj Henni; C. Haegemann; J. S. Haggerty; M. N. Hagiwara; K. I. Hahn; H. Hamagaki; J. Hamblen; J. Hanks; R. Han; H. Harada; E. P. Hartouni; K. Haruna; M. Harvey; E. Haslum; K. Hasuko; R. Hayano; M. Heffner; T. K. Hemmick; T. Hester; J. M. Heuser; X. He; H. Hiejima; J. C. Hill; R. Hobbs; M. Hohlmann; M. Holmes; W. Holzmann; K. Homma; B. Hong; T. Horaguchi; D. Hornback; S. Huang; M. G. Hur; T. Ichihara; R. Ichimiya; H. Iinuma; Y. Ikeda; K. Imai; M. Inaba; Y. Inoue; D. Isenhower; L. Isenhower; M. Ishihara; T. Isobe; M. Issah; A. Isupov; D. Ivanischev; Y. Iwanaga; B. V. Jacak; J. Jia; X. Jiang; J. Jin; O. Jinnouchi; B. M. Johnson; T. Jones; K. S. Joo; D. Jouan; D. S. Jumper; F. Kajihara; S. Kametani; N. Kamihara; J. Kamin; M. Kaneta; J. H. Kang; H. Kanou; J. Kapustinsky; K. Karatsu; M. Kasai; T. Kawagishi; D. Kawall; M. Kawashima; A. V. Kazantsev; S. Kelly; T. Kempel; A. Khanzadeev; K. M. Kijima; J. Kikuchi; A. Kim; B. I. Kim; D. H. Kim; D. J. Kim; E. J. Kim; E. Kim; Y. -J. Kim; Y. -S. Kim; E. Kinney; A. Kiss; E. Kistenev; A. Kiyomichi; J. Klay; C. Klein-Boesing; L. Kochenda; V. Kochetkov; B. Komkov; M. Konno; J. Koster; D. Kotchetkov; D. Kotov; A. Kozlov; A. Kral; A. Kravitz; P. J. Kroon; J. Kubart; G. J. Kunde; N. Kurihara; K. Kurita; M. Kurosawa; M. J. Kweon; Y. Kwon; G. S. Kyle; R. Lacey; Y. S. Lai; J. G. Lajoie; A. Lebedev; Y. Le Bornec; S. Leckey; D. M. Lee; J. Lee; K. B. Lee; K. S. Lee; M. K. Lee; T. Lee; M. J. Leitch; M. A. L. Leite; B. Lenzi; P. Lichtenwalner; P. Liebing; H. Lim; L. A. Linden Levy; T. Liska; A. Litvinenko; H. Liu; M. X. Liu; X. Li; X. H. Li; B. Love; D. Lynch; C. F. Maguire; Y. I. Makdisi; A. Malakhov; M. D. Malik; V. I. Manko; E. Mannel; Y. Mao; L. Masek; H. Masui; F. Matathias; M. C. McCain; M. McCumber; P. L. McGaughey; N. Means; B. Meredith; Y. Miake; T. Mibe; A. C. Mignerey; P. Mikes; K. Miki; T. E. Miller; A. Milov; S. Mioduszewski; G. C. Mishra; M. Mishra; J. T. Mitchell; M. Mitrovski; A. K. Mohanty; H. J. Moon; Y. Morino; A. Morreale; D. P. Morrison; J. M. Moss; T. V. Moukhanova; D. Mukhopadhyay; T. Murakami; J. Murata; S. Nagamiya; Y. Nagata; J. L. Nagle; M. Naglis; M. I. Nagy; I. Nakagawa; Y. Nakamiya; K. R. Nakamura; T. Nakamura; K. Nakano; S. Nam; J. Newby; M. Nguyen; M. Nihashi; B. E. Norman; R. Nouicer; A. S. Nyanin; J. Nystrand; C. Oakley; E. O'Brien; S. X. Oda; C. A. Ogilvie; H. Ohnishi; I. D. Ojha; K. Okada; M. Oka; O. O. Omiwade; Y. Onuki; A. Oskarsson; I. Otterlund; M. Ouchida; K. Ozawa; R. Pak; D. Pal; A. P. T. Palounek; V. Pantuev; V. Papavassiliou; I. H. Park; J. Park; S. K. Park; W. J. Park; S. F. Pate; H. Pei; J. -C. Peng; H. Pereira; V. Peresedov; D. Yu. Peressounko; R. Petti; C. Pinkenburg; R. P. Pisani; M. Proissl; M. L. Purschke; A. K. Purwar; H. Qu; J. Rak; A. Rakotozafindrabe; I. Ravinovich; K. F. Read; S. Rembeczki; M. Reuter

2010-04-20T23:59:59.000Z

348

Evaluation of an in vitro toxicogenetic mouse model for hepatotoxicity  

Science Conference Proceedings (OSTI)

Numerous studies support the fact that a genetically diverse mouse population may be useful as an animal model to understand and predict toxicity in humans. We hypothesized that cultures of hepatocytes obtained from a large panel of inbred mouse strains can produce data indicative of inter-individual differences in in vivo responses to hepato-toxicants. In order to test this hypothesis and establish whether in vitro studies using cultured hepatocytes from genetically distinct mouse strains are feasible, we aimed to determine whether viable cells may be isolated from different mouse inbred strains, evaluate the reproducibility of cell yield, viability and functionality over subsequent isolations, and assess the utility of the model for toxicity screening. Hepatocytes were isolated from 15 strains of mice (A/J, B6C3F1, BALB/cJ, C3H/HeJ, C57BL/6J, CAST/EiJ, DBA/2J, FVB/NJ, BALB/cByJ, AKR/J, MRL/MpJ, NOD/LtJ, NZW/LacJ, PWD/PhJ and WSB/EiJ males) and cultured for up to 7 days in traditional 2-dimensional culture. Cells from B6C3F1, C57BL/6J, and NOD/LtJ strains were treated with acetaminophen, WY-14,643 or rifampin and concentration-response effects on viability and function were established. Our data suggest that high yield and viability can be achieved across a panel of strains. Cell function and expression of key liver-specific genes of hepatocytes isolated from different strains and cultured under standardized conditions are comparable. Strain-specific responses to toxicant exposure have been observed in cultured hepatocytes and these experiments open new opportunities for further developments of in vitro models of hepatotoxicity in a genetically diverse population.

Martinez, Stephanie M.; Bradford, Blair U. [Department of Environmental Sciences and Engineering, University of North Carolina at Chapel Hill, NC 27599 (United States); Soldatow, Valerie Y. [Department of Environmental Sciences and Engineering, University of North Carolina at Chapel Hill, NC 27599 (United States); CellzDirect/Invitrogen (a part of Life Technologies), Durham, NC 27703 (United States); Kosyk, Oksana; Sandot, Amelia [Department of Environmental Sciences and Engineering, University of North Carolina at Chapel Hill, NC 27599 (United States); Witek, Rafal; Kaiser, Robert; Stewart, Todd; Amaral, Kirsten; Freeman, Kimberly; Black, Chris; LeCluyse, Edward L.; Ferguson, Stephen S. [CellzDirect/Invitrogen (a part of Life Technologies), Durham, NC 27703 (United States); Rusyn, Ivan, E-mail: iir@unc.edu [Department of Environmental Sciences and Engineering, University of North Carolina at Chapel Hill, NC 27599 (United States)

2010-12-15T23:59:59.000Z

349

Flux  

NLE Websites -- All DOE Office Websites (Extended Search)

5000 5000 6000 7000 8000 Wavelength (Angstroms) Flux (in arbitrary units) SN 1990N SN 1989B SN 1993O SN 1981B SN 1994D SN 1997ap Iron Peak Blends Ca II Si II & Co II Fe II & III Day -7 Day -5 Day -4 Day -2 ± 2 Day 0 Day +2 * -50 0 50 100 150 Observed days from peak Observed I magnitude 27 26 25 24 23 Observed R magnitude 27 26 25 24 Observed I magnitude 27 26 25 24 23 R band Ground-based I band HST I band (b) (c) (a) Pre-SN observation 3.5 4.0 4.5 5.0 5.5 log(cz) 14 16 18 20 22 24 26 effective m B 0.02 0.05 0.1 0.2 0.5 1.0 redshift z Hamuy et al (A.J. 1996) Supernova Cosmology Project 6 8 % 9 0 % 0.5 1.0 1.5 2.0 2.5 3.0 ! M Age < 9.6 Gyr (H = 50 km s -1 Mpc -1 ) No Big Bang 0.0 0.5 1.0 1.5 2.0 2.5 3.0 -3 -2 -1 0 1 2 3 -3 -2 -1 0 1 2 3 ! " z ~ 0 . 4 z = 0 . 8 3 6 8 % 9 0 % 0.5 1.0 1.5 2.0 2.5 3.0 ! M Age < 9.6 Gyr (H=50 km/s/Mpc)

350

PTF 10bzf (SN 2010ah): A BROAD-LINE Ic SUPERNOVA DISCOVERED BY THE PALOMAR TRANSIENT FACTORY  

Science Conference Proceedings (OSTI)

We present the discovery and follow-up observations of a broad-line Type Ic supernova (SN), PTF 10bzf (SN 2010ah), detected by the Palomar Transient Factory (PTF) on 2010 February 23. The SN distance is {approx_equal}218 Mpc, greater than GRB 980425/SN 1998bw and GRB 060218/SN 2006aj, but smaller than the other SNe firmly associated with gamma-ray bursts (GRBs). We conducted a multi-wavelength follow-up campaign with Palomar 48 inch, Palomar 60 inch, Gemini-N, Keck, Wise, Swift, the Allen Telescope Array, Combined Array for Research in Millimeter-wave Astronomy, Westerbork Synthesis Radio Telescope, and Expanded Very Large Array. Here we compare the properties of PTF 10bzf with those of SN 1998bw and other broad-line SNe. The optical luminosity and spectral properties of PTF 10bzf suggest that this SN is intermediate, in kinetic energy and amount of {sup 56}Ni, between non-GRB-associated SNe like 2002ap or 1997ef, and GRB-associated SNe like 1998bw. No X-ray or radio counterpart to PTF 10bzf was detected. X-ray upper limits allow us to exclude the presence of an underlying X-ray afterglow as luminous as that of other SN-associated GRBs such as GRB 030329 or GRB 031203. Early-time radio upper limits do not show evidence for mildly relativistic ejecta. Late-time radio upper limits rule out the presence of an underlying off-axis GRB, with energy and wind density similar to the SN-associated GRB 030329 and GRB 031203. Finally, by performing a search for a GRB in the time window and at the position of PTF 10bzf, we find that no GRB in the interplanetary network catalog could be associated with this SN.

Corsi, A. [LIGO Laboratory, California Institute of Technology, MS 100-36, Pasadena, CA 91125 (United States); Ofek, E. O.; Kulkarni, S. R.; Kasliwal, M. M. [Cahill Center for Astrophysics, California Institute of Technology, Pasadena, CA 91125 (United States); Frail, D. A. [National Radio Astronomy Observatory, P.O. Box 0, Socorro, NM 87801 (United States); Poznanski, D.; Nugent, P. [Computational Cosmology Center, Lawrence Berkeley National Laboratory, 1 Cyclotron Road, Berkeley, CA 94720 (United States); Arcavi, I.; Gal-Yam, A.; Green, Y.; Xu, D.; Ben-ami, S. [Department of Particle Physics and Astrophysics, The Weizmann Institute of Science, Rehovot 76100 (Israel); Hurley, K. [Space Sciences Laboratory, University of California Berkeley, 7 Gauss Way, Berkeley, CA 94720 (United States); Mazzali, P. A. [INAF-Osservatorio Astronomico, vicolo dell'Osservatorio 5, I-35122 Padova (Italy); Howell, D. A.; Murray, D. [Las Cumbres Observatory Global Telescope Network, Inc., Santa Barbara, CA 93117 (United States); Sullivan, M. [Department of Physics (Astrophysics), University of Oxford, DWB, Keble Road, Oxford OX1 3RH (United Kingdom); Bloom, J. S.; Cenko, S. B. [Department of Astronomy, 601 Campbell Hall, University of California, Berkeley, CA 94720-3411 (United States); Law, N. M., E-mail: corsi@caltech.edu [Dunlap Institute for Astronomy and Astrophysics, University of Toronto, 50 St. George Street, Toronto M5S 3H4, Ontario (Canada)

2011-11-10T23:59:59.000Z

351

Mercury and autoimmunity: implications for occupational and environmental health  

SciTech Connect

Mercury (Hg) has long been recognized as a neurotoxicant; however, recent work in animal models has implicated Hg as an immunotoxicant. In particular, Hg has been shown to induce autoimmune disease in susceptible animals with effects including overproduction of specific autoantibodies and pathophysiologic signs of lupus-like disease. However, these effects are only observed at high doses of Hg that are above the levels to which humans would be exposed through contaminated fish consumption. While there is presently no evidence to suggest that Hg induces frank autoimmune disease in humans, a recent epidemiological study has demonstrated a link between occupational Hg exposure and lupus. In our studies, we have tested the hypothesis that Hg does not cause autoimmune disease directly, but rather that it may interact with triggering events, such as genetic predisposition, exposure to antigens, or infection, to exacerbate disease. Treatment of mice that are not susceptible to Hg-induced autoimmune disease with very low doses and short term exposures of inorganic Hg (20-200 {mu}g/kg) exacerbates disease and accelerates mortality in the graft versus host disease model of chronic lupus in C57Bl/6 x DBA/2 mice. Furthermore, low dose Hg exposure increases the severity and prevalence of experimental autoimmune myocarditis (induced by immunization with cardiac myosin peptide in adjuvant) in A/J mice. To test our hypothesis further, we examined sera from Amazonian populations exposed to Hg through small-scale gold mining, with and without current or past malaria infection. We found significantly increased prevalence of antinuclear and antinucleolar antibodies and a positive interaction between Hg and malaria. These results suggest a new model for Hg immunotoxicity, as a co-factor in autoimmune disease, increasing the risks and severity of clinical disease in the presence of other triggering events, either genetic or acquired.

Silbergeld, Ellen K. [Department of Environmental Health Sciences, Johns Hopkins University Bloomberg School of Public Health, Baltimore, MD 21205 (United States)]. E-mail: esilberg@jhsph.edu; Silva, Ines A. [Department of Environmental Health Sciences, Johns Hopkins University Bloomberg School of Public Health, Baltimore, MD 21205 (United States); Nyland, Jennifer F. [Department of Environmental Health Sciences, Johns Hopkins University Bloomberg School of Public Health, Baltimore, MD 21205 (United States)

2005-09-01T23:59:59.000Z

352

Scaling of cell size in cellular instabilities of nonpremixed jet flames  

SciTech Connect

Systematic experiments have been undertaken to study the parameter dependence of cellular instability and in particular the scaling of the resulting cell size in CO{sub 2}-diluted H{sub 2}-O{sub 2} jet diffusion flames. Cellular flames are known to arise near the extinction limit when reactant Lewis numbers are relatively low. The Lewis numbers of the investigated near-extinction mixtures, based on the initial mixture strength {phi}{sub m} and ambient conditions, varied in the ranges [1.1-1.3] for oxygen and [0.25-0.29] for hydrogen ({phi}{sub m} is defined here as the fuel-to-oxygen mass ratio, normalized by the stoichiometric ratio). The experiments were carried out both in an axisymmetric jet (AJ) burner and in a two-dimensional slot burner known as a Wolfhard-Parker (WP) burner with an oxidizer co-flow (mostly 100% O{sub 2}) of fixed low velocity. First, the region of cellular flames adjacent to the extinction limit was characterized in terms of initial H{sub 2} concentration and fuel jet velocity, with all other parameters fixed. Then, the wavelength of the cellular instability, i.e., the cell size, was determined as a function of the fuel jet velocity and the initial mixture strength {phi}{sub m}. For conditions not too close to extinction, this wavelength is found to increase with the square root of the vorticity thickness of the jet shear layer and roughly the 1/5 power of {phi}{sub m}. Very close to extinction, this scaling breaks down and will likely switch to a scaling with the flame thickness, i.e., involving the Damkoehler number. (author)

Lo Jacono, D.; Monkewitz, P.A. [Ecole Polytechnique Federale de Lausanne, Laboratory of Fluid Mechanics, CH-1015 Lausanne (Switzerland)

2007-10-15T23:59:59.000Z

353

Contribution of liver mitochondrial membrane-bound glutathione transferase to mitochondrial permeability transition pores  

Science Conference Proceedings (OSTI)

We recently reported that the glutathione transferase in rat liver mitochondrial membranes (mtMGST1) is activated by S-glutathionylation and the activated mtMGST1 contributes to the mitochondrial permeability transition (MPT) pore and cytochrome c release from mitochondria [Lee, K.K., Shimoji, M., Quazi, S.H., Sunakawa, H., Aniya, Y., 2008. Novel function of glutathione transferase in rat liver mitochondrial membrane: role for cytochrome c release from mitochondria. Toxcol. Appl. Pharmacol. 232, 109-118]. In the present study we investigated the effect of reactive oxygen species (ROS), generator gallic acid (GA) and GST inhibitors on mtMGST1 and the MPT. When rat liver mitochondria were incubated with GA, mtMGST1 activity was increased to about 3 fold and the increase was inhibited with antioxidant enzymes and singlet oxygen quenchers including 1,4-diazabicyclo [2,2,2] octane (DABCO). GA-mediated mtMGST1 activation was prevented by GST inhibitors such as tannic acid, hematin, and cibacron blue and also by cyclosporin A (CsA). In addition, GA induced the mitochondrial swelling which was also inhibited by GST inhibitors, but not by MPT inhibitors CsA, ADP, and bongkrekic acid. GA also released cytochrome c from the mitochondria which was inhibited completely by DABCO, moderately by GST inhibitors, and somewhat by CsA. Ca{sup 2+}-mediated mitochondrial swelling and cytochrome c release were inhibited by MPT inhibitors but not by GST inhibitors. When the outer mitochondrial membrane was isolated after treatment of mitochondria with GA, mtMGST1 activity was markedly increased and oligomer/aggregate of mtMGST1 was observed. These results indicate that mtMGST1 in the outer mitochondrial membrane is activated by GA through thiol oxidation leading to protein oligomerization/aggregation, which may contribute to the formation of ROS-mediated, CsA-insensitive MPT pore, suggesting a novel mechanism for regulation of the MPT by mtMGST1.

Hossain, Quazi Sohel [Laboratory of Molecular Genetics and Pharmacology, School of Health Sciences, Faculty of Medicine, University of the Ryukyus, 207 Uehara, Nishihara, Okinawa 903-0215 (Japan); Department of Biochemistry, School of Medicine, Faculty of Medicine, University of the Ryukyus, 207 Uehara, Nishihara, Okinawa 903-0215 (Japan); Ulziikhishig, Enkhbaatar; Lee, Kang Kwang [Laboratory of Molecular Genetics and Pharmacology, School of Health Sciences, Faculty of Medicine, University of the Ryukyus, 207 Uehara, Nishihara, Okinawa 903-0215 (Japan); Yamamoto, Hideyuki [Department of Biochemistry, School of Medicine, Faculty of Medicine, University of the Ryukyus, 207 Uehara, Nishihara, Okinawa 903-0215 (Japan); Aniya, Yoko [Laboratory of Molecular Genetics and Pharmacology, School of Health Sciences, Faculty of Medicine, University of the Ryukyus, 207 Uehara, Nishihara, Okinawa 903-0215 (Japan)], E-mail: yaniya@med.u-ryukyu.ac.jp

2009-02-15T23:59:59.000Z

354

THE CHANDRA X-RAY SURVEY OF PLANETARY NEBULAE (CHANPLANS): PROBING BINARITY, MAGNETIC FIELDS, AND WIND COLLISIONS  

Science Conference Proceedings (OSTI)

We present an overview of the initial results from the Chandra Planetary Nebula Survey (CHANPLANS), the first systematic (volume-limited) Chandra X-Ray Observatory survey of planetary nebulae (PNe) in the solar neighborhood. The first phase of CHANPLANS targeted 21 mostly high-excitation PNe within {approx}1.5 kpc of Earth, yielding four detections of diffuse X-ray emission and nine detections of X-ray-luminous point sources at the central stars (CSPNe) of these objects. Combining these results with those obtained from Chandra archival data for all (14) other PNe within {approx}1.5 kpc that have been observed to date, we find an overall X-ray detection rate of {approx}70% for the 35 sample objects. Roughly 50% of the PNe observed by Chandra harbor X-ray-luminous CSPNe, while soft, diffuse X-ray emission tracing shocks-in most cases, 'hot bubbles'-formed by energetic wind collisions is detected in {approx}30%; five objects display both diffuse and point-like emission components. The presence (or absence) of X-ray sources appears correlated with PN density structure, in that molecule-poor, elliptical nebulae are more likely to display X-ray emission (either point-like or diffuse) than molecule-rich, bipolar, or Ring-like nebulae. All but one of the point-like CSPNe X-ray sources display X-ray spectra that are harder than expected from hot ({approx}100 kK) central stars emitting as simple blackbodies; the lone apparent exception is the central star of the Dumbbell nebula, NGC 6853. These hard X-ray excesses may suggest a high frequency of binary companions to CSPNe. Other potential explanations include self-shocking winds or PN mass fallback. Most PNe detected as diffuse X-ray sources are elliptical nebulae that display a nested shell/halo structure and bright ansae; the diffuse X-ray emission regions are confined within inner, sharp-rimmed shells. All sample PNe that display diffuse X-ray emission have inner shell dynamical ages {approx}< 5 Multiplication-Sign 10{sup 3} yr, placing firm constraints on the timescale for strong shocks due to wind interactions in PNe. The high-energy emission arising in such wind shocks may contribute to the high excitation states of certain archetypical 'hot bubble' nebulae (e.g., NGC 2392, 3242, 6826, and 7009).

Kastner, J. H.; Montez, R. Jr.; Rapson, V. [Center for Imaging Science and Laboratory for Multiwavelength Astrophysics, Rochester Institute of Technology, 54 Lomb Memorial Drive, Rochester, NY 14623 (United States); Balick, B. [Department of Astronomy, University of Washington, Seattle, WA (United States); Frew, D. J.; De Marco, O.; Parker, Q. A. [Department of Physics and Astronomy and Macquarie Research Centre for Astronomy, Astrophysics and Astrophotonics, Macquarie University, Sydney, NSW 2109 (Australia); Miszalski, B. [South African Astronomical Observatory, P.O. Box 9, Observatory, 7935 (South Africa); Sahai, R. [Jet Propulsion Laboratory, California Institute of Technology, MS 183-900, Pasadena, CA 91109 (United States); Blackman, E.; Frank, A. [Department of Physics and Astronomy, University of Rochester, Rochester, NY (United States); Chu, Y.-H. [Department of Astronomy, University of Illinois, Champagne-Urbana, IL (United States); Guerrero, M. A. [Instituto de Astrofisica de Astronomia, Glorieta de la Astronomia s/n, Granada 18008 (Spain); Lopez, J. A. [Instituto de Astronomia, Universidad Nacional Autonoma de Mexico, Campus Ensenada, Apdo. Postal 22860, Ensenada, B. C. (Mexico); Zijlstra, A. [School of Physics and Astronomy, University of Manchester, Manchester M13 9PL (United Kingdom); Behar, E. [Department of Physics, Technion (Israel); Bujarrabal, V. [Observatorio Astronomico Nacional, Apartado 112, E-28803, Alcala de Henares (Spain); Corradi, R. L. M. [Instituto de Astrofisica de Canarias, E-38200 La Laguna, Tenerife (Spain); Nordhaus, J. [Center for Computational Relativity and Gravitation, Rochester Institute of Technology, Rochester, NY 14623 (United States); Sandin, C., E-mail: jhk@cis.rit.edu, E-mail: soker@physics.technion.ac.il, E-mail: eva.villaver@uam.es [Leibniz Institute for Astrophysics Potsdam (AIP), An der Sternwarte 16, D-14482 Potsdam (Germany); and others

2012-08-15T23:59:59.000Z

355

Improved analysis of J/{psi} decays into a vector meson and two pseudoscalars  

SciTech Connect

Recently, the BES collaboration has published an extensive partial-wave analysis of experimental data on J/{psi}{yields}{phi}{pi}{sup +}{pi}{sup -}, J/{psi}{yields}{omega}{pi}{sup +}{pi}{sup -}, J/{psi}{yields}{phi}K{sup +}K{sup -} and J/{psi}{yields}{omega}K{sup +}K{sup -}. These new results are analyzed here, with full account of detection efficiencies, in the framework of a chiral unitary description with coupled-channel final state interactions between {pi}{pi} and KK pairs. The emission of a dimeson pair is described in terms of the strange and nonstrange scalar form factors of the pion and the kaon, which include the final state interaction and are constrained by unitarity and by matching to the next-to-leading-order chiral expressions. This procedure allows for a calculation of the S-wave component of the dimeson spectrum including the f{sub 0}(980) resonance, and for an estimation of the low-energy constants of Chiral Perturbation Theory, in particular, the large N{sub c} suppressed constants L{sub 4}{sup r} and L{sub 6}{sup r}. The decays in question are also sensitive to physics associated with OZI violation in the 0{sup ++} channel. It is found that the S-wave contributions to {phi}{pi}{sup +}{pi}{sup -}, {phi}K{sup +}K{sup -} and {omega}{pi}{sup +}{pi}{sup -} given by the BES partial-wave analysis may be very well fitted up to a dimeson center-of-mass energy of {approx}1.2 GeV, for a large and positive value of L{sub 4}{sup r} and a value of L{sub 6}{sup r} compatible with zero. An accurate determination of the amount of OZI violation in the J/{psi}{yields}{phi}{pi}{sup +}{pi}{sup -} decay is achieved, and the S-wave contribution to {omega}K{sup +}K{sup -} near threshold is predicted.

Laehde, Timo A. [Helmholtz-Institut fuer Strahlen- und Kernphysik (HISKP), Bonn University, Nussallee 14-16, D-53115 Bonn (Germany); Meissner, Ulf-G. [Helmholtz-Institut fuer Strahlen- und Kernphysik (HISKP), Bonn University, Nussallee 14-16, D-53115 Bonn (Germany); Forschungszentrum Juelich, Institut fuer Kernphysik (Thailand), D-52425 Juelich (Germany)

2006-08-01T23:59:59.000Z

356

Measurement of the Decays $B^0_s\\to J/?\\,?(1020)$, $B^0_{s}\\to J/?\\,f'_2(1525)$ and $B^0_s\\to J/?\\,K^+K^-$ at Belle  

E-Print Network (OSTI)

We report a measurement of the branching fraction of the decay $B^0_s\\to J/\\psi\\,\\phi(1020)$, evidence and a branching fraction measurement for $B^0_s\\to J/\\psi\\,f'_2(1525)$, and the determination of the total $B^0_s\\to J/\\psi\\,K^+K^-$ branching fraction, including the resonant and non-resonant contributions to the $K^+K^-$ channel. We also determine the $S$-wave contribution within the $\\phi(1020)$ mass region. The absolute branching fractions are $\\mathcal{B}[B^0_s\\to J/\\psi\\,\\phi(1020)]=(1.25 \\pm 0.07\\left(\\mathrm{stat}\\right)\\pm 0.08\\left(\\mathrm{syst}\\right)\\pm 0.22\\left(f_s\\right))\\times 10^{-3}$, $\\mathcal{B}[B^0_s\\to J/\\psi\\,f'_2(1525)]=(0.26\\pm 0.06\\left(\\mathrm{stat}\\right)\\pm 0.02\\left(\\mathrm{syst}\\right) \\pm 0.05\\left(f_s\\right))\\times 10^{-3}$ and $\\mathcal{B}[B^0_s\\to J/\\psi\\,K^+K^-] = (1.01\\pm 0.09\\left(\\mathrm{stat}\\right) \\pm 0.10\\left(\\mathrm{syst}\\right)\\pm 0.18\\left(f_s\\right))\\times 10^{-3}$, where the last systematic error is due to the branching fraction of $b\\bar{b}\\to B^{(*)}_s B^{(*)}_s$. The branching fraction ratio is found to be $\\mathcal{B}[B^0_s\\to J/\\psi\\,f'_2(1525)]/\\mathcal{B}[B^0_s\\to J/\\psi\\,\\phi(1020)]=(21.5\\pm 4.9\\left(\\mathrm{stat}\\right) \\pm2.6\\left(\\mathrm{syst}\\right))%$. All results are based on a 121.4 fb$^{-1}$ data sample collected at the $\\Upsilon(5S)$ resonance by the Belle experiment at the KEKB asymmetric-energy $e^+e^-$ collider.

Belle Collaboration; F. Thorne; C. Schwanda; I. Adachi; H. Aihara; D. M. Asner; V. Aulchenko; T. Aushev; A. M. Bakich; A. Bala; B. Bhuyan; G. Bonvicini; M. Bra?ko; M. -C. Chang; V. Chekelian; A. Chen; B. G. Cheon; K. Chilikin; R. Chistov; K. Cho; V. Chobanova; S. -K. Choi; Y. Choi; D. Cinabro; J. Dalseno; Z. Doleal; Z. Drsal; D. Dutta; S. Eidelman; S. Esen; H. Farhat; J. E. Fast; M. Feindt; T. Ferber; V. Gaur; N. Gabyshev; R. Gillard; Y. M. Goh; B. Golob; J. Haba; T. Hara; K. Hayasaka; H. Hayashii; Y. Hoshi; W. -S. Hou; H. J. Hyun; T. Iijima; A. Ishikawa; R. Itoh; Y. Iwasaki; T. Iwashita; I. Jaegle; T. Julius; D. H. Kah; J. H. Kang; E. Kato; C. Kiesling; D. Y. Kim; H. O. Kim; J. B. Kim; J. H. Kim; M. J. Kim; Y. J. Kim; J. Klucar; B. R. Ko; P. Kody; P. Krian; P. Krokovny; T. Kuhr; J. S. Lange; S. -H. Lee; J. Libby; C. Liu; Y. Liu; P. Lukin; D. Matvienko; H. Miyata; R. Mizuk; G. B. Mohanty; A. Moll; T. Mori; Y. Nagasaka; E. Nakano; M. Nakao; Z. Natkaniec; M. Nayak; C. Ng; S. Nishida; O. Nitoh; S. Okuno; C. Oswald; G. Pakhlova; H. Park; H. K. Park; R. Pestotnik; M. Petri?; L. E. Piilonen; M. Prim; M. Ritter; A. Rostomyan; S. Ryu; H. Sahoo; T. Saito; Y. Sakai; S. Sandilya; L. Santelj; T. Sanuki; V. Savinov; O. Schneider; G. Schnell; D. Semmler; K. Senyo; M. E. Sevior; M. Shapkin; C. P. Shen; T. -A. Shibata; J. -G. Shiu; B. Shwartz; A. Sibidanov; F. Simon; Y. -S. Sohn; A. Sokolov; E. Solovieva; S. Stani?; M. Stari?; U. Tamponi; K. Tanida; G. Tatishvili; Y. Teramoto; M. Uchida; Y. Unno; S. Uno; P. Urquijo; G. Varner; K. E. Varvell; V. Vorobyev; M. N. Wagner; C. H. Wang; M. -Z. Wang; P. Wang; X. L. Wang; Y. Watanabe; K. M. Williams; E. Won; J. Yamaoka; Y. Yamashita; S. Yashchenko; C. Z. Yuan; Z. P. Zhang; V. Zhilich; A. Zupanc

2013-09-03T23:59:59.000Z

357

Adsorption of Potassium on the MoS2(100) Surface: A First-Principles Investigation  

DOE Green Energy (OSTI)

Periodic density functional theory calculations were performed to investigate the interaction that potassium with the Mo and S edges of the MoS2(100) surface. Both neutral and cationic (+1) charged potassium-promoted systems at different sulfur coverages were considered. Our calculations indicate that the potassium atom readily donates its single 4s valence electron to the MoS2 structure for the neutral potassium-promoted system, and the neutral and cationic potassium-promoted systems demonstrate a similar adsorption behavior. Moreover, potassium changes the magnetic properties known to occur at the metallic edge surface, which have implications for electron spin dependent surface characterization methods (i.e., electron spin/paramagnetic spectroscopy). Potassium in both the neutral and cationic systems tends to maximize its interactions with the available sulfur atoms at the edge surface, preferring sites over four-fold S hollows on fully sulfided Mo and S edges and over the interstitial gap where two to four edge surface S atoms are available for coordination. As the potassium coverage increases, the adsorption energy per potassium atom, surface work function, and transfer of the K 4s electron to the MoS2(100) surface decreases, which is in line with an increased metallization of the potassium adlayer. The potassium adlayer tends to form chains along the interstitial with K-K distances ~1 , which is notably less than those of bulk bcc K metal (4.61 ). Density of states for the potassium-saturated surface suggests enhanced involvement of broad K 3d states beginning just above the Fermi level. Potassium-promotion of MoS2(100) has implications for alcohol catalysis: increasing the surface basicity by increasing the electron charge of the surface, providing hydrogenation-promoting CO site, blocking edge surface that dissociate CO and lead to methanation, and limiting H2 dissociative adsorption to the edge surface and possibly inhibiting the H2 dissociative adsorption via s character electron repulsion. This research was performed in part using the Molecular Science Computing Facility in the William R. Wiley Environmental Molecular Sciences Laboratory, a U.S. Department of Energy (DOE) national scientific user facility located at the Pacific Northwest National Laboratory (PNNL). PNNL is operated by Battelle for DOE.

Andersen, Amity; Kathmann, Shawn M.; Lilga, Michael A.; Albrecht, Karl O.; Hallen, Richard T.; Mei, Donghai

2011-04-15T23:59:59.000Z

358

Incorporating Amino Acid Esters into Catalysts for Hydrogen Oxidation: Steric and Electronic Effects and the Role of Water as a Base  

Science Conference Proceedings (OSTI)

Four derivatives of a hydrogen oxidation catalyst, [Ni(PCy2NBn-R2)]2+ (Cy=cyclohexyl, Bn=benzyl, R= OMe, COOMe, CO-Alanine-methyl ester or CO-Phenylalanine-methyl ester), have been prepared to investigate steric and electronic effects on catalysis. Each complex was characterized spectroscopically and electrochemically, and thermodynamic data were determined. Crystal structures are also reported for the -OMe and -COOMe derivatives. All four catalysts were found to be active for H2 oxidation. The methyl ester (R = COOMe) and amino acid ester containing complexes (R = CO-Alanine-methyl ester or CO-Phenylalanine-methyl ester) had slower rates (4 s-1) than that of the parent complex (10 s-1), in which R = H, consistent with the lower amine pKas and less favorable ?GH2s found for these electron-withdrawing substituents. Dynamic processes for the amino acid ester containing complexes were also investigated and found not to hinder catalysis. The electron-donating methoxy ether derivative (R = OMe) was prepared to compare electronic effects and has a similar catalytic rate as the parent complex. In the course of these studies, it was found that water could act as a weak base for H2 oxidation, although catalytic turnover requires a significantly higher potential and utilizes a different sequence of catalytic steps than when using a base with a higher pKa. Importantly, these catalysts provide a foundation upon which larger peptides can be attached to [Ni(PCy2NBn2)2]2+ hydrogen oxidation catalysts in order to more fully investigate and implement the effects of the outer-coordination sphere. This work was funded by the DOE Office of Science Early Career Research Program through the Office of Basic Energy Sciences (SL and WJS), by the Center for Molecular Electrocatalysis, an Energy Frontier Research Center funded by the US Department of Energy, Office of Science, Office of Basic Energy Sciences (JR), and by the US DOE Basic Energy Sciences, Chemical Sciences, Geoscience and Biosciences Division (AMA, AJ). Pacific Northwest National Laboratory is operated by Battelle for the U.S. Department of Energy.

Lense, Sheri; Ho, Ming-Hsun; Chen, Shentan; Jain, Avijita; Raugei, Simone; Linehan, John C.; Roberts, John A.; Appel, Aaron M.; Shaw, Wendy J.

2012-10-08T23:59:59.000Z

359

Failure of catalase to protect against aflatoxin B{sub 1}-induced mouse lung tumorigenicity  

SciTech Connect

The carcinogenic mycotoxin aflatoxin B{sub 1} (AFB{sub 1}) induces 8-hydroxy-2'-deoxyguanosine (8-OHdG) formation in mouse lung, an effect that can be prevented by treatment with polyethylene glycol-conjugated catalase (PEG-CAT). G {yields} T transversion mutation in K-ras, an early event in AFB{sub 1}-induced mouse lung carcinogenesis, is thought to result from AFB{sub 1}-8,9-exo-epoxide binding to DNA to form AFB{sub 1}-N{sup 7}-guanine, but may also result from formation of 8-OHdG. Therefore, oxidative DNA damage may be important in AFB{sub 1} carcinogenicity. The objective of this study was to determine whether PEG-CAT would prevent AFB{sub 1} tumorigenicity. Mouse lung tumorigenesis was assessed following treatment of female A/J mice with 300 kU/kg PEG-CAT ip and/or 50 mg/kg AFB{sub 1}. Mice were killed 7 months post-treatment and tumors greater than 1 mm in diameter were excised. Unexpectedly, the mean number of tumors per mouse in the PEG-CAT + AFB{sub 1} group (8.81 {+-} 3.64, n = 47) was greater than that of the group treated with AFB{sub 1} alone (7.05 {+-} 3.45, n = 42) (P < 0.05). The tumors obtained from mice treated with PEG-CAT + AFB{sub 1} were larger than those from mice treated with AFB{sub 1} alone (P < 0.05). There was no difference in K-ras exon 1 mutation spectrum or in the histological diagnosis of tumors between AFB{sub 1} and PEG-CAT + AFB{sub 1} groups (P > 0.05). In vitro incubation with mouse liver catalase (CAT) resulted in conversion of [{sup 3}H]AFB{sub 1} into a DNA-binding species, a possible explanation for the results observed in vivo. These results demonstrate that PEG-CAT is not protective against AFB{sub 1} carcinogenicity in mouse lung despite preventing DNA oxidation.

Guindon, Katherine A. [Department of Pharmacology and Toxicology, Queen' s University, Kingston, Ontario, K7L 3N6 (Canada); Foley, Julie F.; Maronpot, Robert R. [National Institute of Environmental Health Sciences, Research Triangle Park, NC 27709 (United States); Massey, Thomas E. [Department of Pharmacology and Toxicology, Queen' s University, Kingston, Ontario, K7L 3N6 (Canada)], E-mail: masseyt@queensu.ca

2008-03-01T23:59:59.000Z

360

Unit physics testing of a mix model in an eulerian fluid computation  

Science Conference Proceedings (OSTI)

A K-L turbulence mix model driven with a drag-buoyancy source term is tested in an Eulerian code in a series of basic unit-physics tests, as part of a mix validation milestone. The model and the closure coefficient values are derived in the work of Dimonte-Tipton [D-T] in Phys.Flu.18, 085101 (2006), and many of the test problems were reported there, where the mix model operated in Lagrange computations. The drag-buoyancy K-L mix model was implemented within the Eulerian code framework by A.J. Scannapieco. Mix model performance is evaluated in terms of mix width growth rates compared to experiments in select regimes. Results in our Eulerian code are presented for several unit-physics I-D test problems including the decay of homogeneous isotropic turbulence (HIT), Rayleigh-Taylor (RT) unstable mixing, shock amplification of initial turbulence, Richtmyer-Meshkov (RM) mixing in several single shock test cases and in comparison to two RM experiments including re-shock (Vetter-Sturtevant and Poggi, et.al.). Sensitivity to model parameters, to Atwood number, and to initial conditions are examined. Results here are in good agreement in some tests (HIT, RT) with the previous results reported for the mix model in the Lagrange calculations. The HIT turbulent decay agrees closely with analytic expectations, and the RT growth rate matches experimental values for the default values of the model coefficients proposed in [D-T]. Results for RM characterized with a power law growth rate differ from the previous mix model work but are still within the range for reasonable agreement with experiments. Sensitivity to IC values in the RM studies are examined; results are sensitive to initial values of L[t=O], which largely determines the RM mix layer growth rate, and generally differs from the IC values used in the RT studies. Result sensitivity to initial turbulence, K[t=O], is seen to be small but significant above a threshold value. Initial conditions can be adjusted so that single shock RM mix width results match experiments but we have not been able to obtain a good match for first shock and re-shock growth rates in the same experiment with a single set of parameters and Ie. Problematic issues with KH test problems are described. Resolution studies for an RM test problem show the K-L mix growth rate decreases as it converges at a supra-linear rate, and, convergence requires a fine grid (on the order of 10 microns). For comparison, a resolution study of a second mix model [Scannapieco and Cheng, Phys.Lett.A, 299(1),49, (2002)] acting on a two fluid interface problem was examined. The mix in this case was found to increase with grid resolution at low to moderate resolutions, but converged at comparably fine resolutions. In conclusion, these tests indicate that the Eulerian code K-L model, using the Dimonte Tipton default model closure coefficients, achieve reasonable results across many of the unit-physics experimental conditions. However, we were unable to obtain good matches simultaneously for shock and re-shock mix in a single experiment. Results are sensitive to initial conditions in the regimes under study, with different IC best suited to RT or RM mix. It is reasonable to expect IC sensitivity in extrapolating to high energy density regimes, or to experiments with deceleration due to arbitrary combinations of RT and RM. As a final comparison, the atomically generated mix fraction and the mix width were each compared for the K-L mix model and the Scannapieco model on an identical RM test problem. The Scannapieco mix fraction and width grow linearly. The K-L mix fraction and width grow with the same power law exponent, in contrast to expectations from analysis. In future work it is proposed to do more head-to-head comparisons between these two models and other mix model options on a full suite of physics test problems, such as interfacial deceleration due to pressure build-up during an idealized ICF implosion.

Vold, Erik [Los Alamos National Laboratory; Douglass, Rod [Los Alamos National Laboratory

2010-01-01T23:59:59.000Z

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361

[Utilizing the ultraintense JanUSP laser at LLNL]. 99-ERD-049 Final LDRD Report  

Science Conference Proceedings (OSTI)

Recent advances in laser and optical technologies have now enabled the current generation of high intensity, ultrashort-pulse lasers to achieve focal intensities of 10{sup 20}-10{sup 21} W/cm{sup 2} in pulse durations of 100-500fs. These ultraintense laser pulses are capable of producing highly relativistic plasma states with densities, temperatures, and pressures rivaling those found in the interiors of stars and nuclear weapons. Utilizing the ultraintense 100TW JanUSP laser at LLNL we have explored the possibility of ion shock heating small micron-sized plasmas to extremely high energy densities approaching 1GJ/g on timescales of a few hundred femtoseconds. The JanUSP laser delivers 10 Joules of energy in a 100fs pulse in a near diffraction-limited beam, producing intensities on target of up to 10{sup 21}W/cm{sup 2}. The electric field of the laser at this intensity ionizes and accelerates electrons to relativistic MeV energies. The sudden ejection of electrons from the focal region produces tremendous electrostatic forces which in turn accelerate heavier ions to MeV energies. The predicted ion flux of 1 MJ/cm{sup 2} is sufficient to achieve thermal equilibrium conditions at high temperature in solid density targets. Our initial experiments were carried out at the available laser contrast of 10{sup -7} (i.e. the contrast of the amplified spontaneous emission (ASE), and of the pre-pules produced in the regenerative amplifier). We used the nuclear photoactivation of Au-197 samples to measure the gamma production above 12MeV-corresponding to the threshold for the Au-197(y,n) reaction. Since the predominant mechanism for gamma production is through the bremsstrahlung emission of energetic electrons as they pass through the solid target we were able to infer a conversion yield of several percent of the incident laser energy into electrons with energies >12MeV. This result is consistent with the interaction of the main pulse with a large pre-formed plasma. The contrast of the laser was improved to the 10{sup -10} level by the insertion of two additional pockel cells to reduce the pre-pulse intensities, and by the implementation of a pulse clean up technique based on adding an additional pre-amplifier and saturable absorber which resulted in a reduction in the ASE level by a factor of approximately 1000. In FY00/01 we performed a series of experiments to investigate the mechanisms for ion generation and acceleration in thin foil targets irradiated at incident laser intensities above 10{sup 20} W/cm{sup 2}, and with the laser contrast at 10{sup -10}. Full details of this work can be found in the two accompanying papers: Energy spectrum and angular distribution of multi-MeV protons produced from ultraintense laser interactions, UCRL-JC-143112, P.K. Pate1 et al., and Enhancement of proton acceleration by hot electron re-circulation in thin foils irradiated by ultra-intense laser pulses, A.J. Mackinnon et al. UCRL-JC-145540. To obtain a more complete picture of the ion emission a range of detectors were developed and fielded including radiachromic films (measuring ion, electron, and x-ray dose), nuclear activation detectors (high energy protons), and single particle nuclear track detectors (protons and heavy ions). Significantly we found that a large fraction of the incident laser energy (greater than 1%) is coupled to highly energetic protons forming a well-collimated beam. The proton spectrum can be fit by an exponential distribution containing 10{sup 11} particles with a mean energy of 3 MeV and a high energy cutoff of 25 MeV. However, these particles appear to originate not from the interaction region at the front of the target but rather from a thin adsorption layer on the rear surface.

Patel, P K; Price, D F; Mackinnon, A J; Springer, P T

2002-04-17T23:59:59.000Z