Connection between GRW "spontaneous collapse" and Mensky's "restricted path integral" models
Roman Sverdlov
2015-02-09T23:59:59.000Z
In this paper we will show how Mensky's model of "restricted path integrals" can be derived from GRW "spontaneous collapse" model.
Last resorts : a tour guide to territorial protection for the Republic of the Maldives
Sleeper, Buck (Thomas Buck)
2011-01-01T23:59:59.000Z
A two meter rise in sea levels projected by the end of this century threatens the sovereignty of the Maldivian nation state. While flight from the Maldives to establish a new homeland elsewhere has been proposed, the culture ...
Alford, Simon
M1 Year - Regular Curriculum ^ Satisfactorily complete all requirements Pass at least 67% of weighted curriculum Take make-up exam(s) or approved summer course Satisfactorily complete all requirements ¹ Fail any requirement ² If No Previous Repeat Year Pass 40% to 66% of weighted curriculum * Students who
Infinitely many N=1 dualities from $m+1-m=1$
Prarit Agarwal; Kenneth Intriligator; Jaewon Song
2015-05-01T23:59:59.000Z
We discuss two infinite classes of 4d supersymmetric theories, ${T}_N^{(m)}$ and ${\\cal U}_N^{(m)}$, labelled by an arbitrary non-negative integer, $m$. The ${T}_N^{(m)}$ theory arises from the 6d, $A_{N-1}$ type ${\\cal N}=(2,0)$ theory reduced on a 3-punctured sphere, with normal bundle given by line bundles of degree $(m+1, -m)$; the $m=0$ case is the ${\\cal N}=2$ supersymmetric $T_N$ theory. The novelty is the negative-degree line bundle. The ${\\cal U}_N^{(m)}$ theories likewise arise from the 6d ${\\cal N}=(2,0)$ theory on a 4-punctured sphere, and can be regarded as gluing together two (partially Higgsed) ${T}_N^{(m)}$ theories. The ${T}_N^{(m)}$ and ${\\cal U}_N^{(m)}$ theories can be represented, in various duality frames, as quiver gauge theories, built from $T_N$ components via gauging and nilpotent Higgsing. We analyze the RG flow of the ${\\cal U}_N^{(m)}$ theories, and find that, for all integer $m>0$, they end up at the same IR SCFT as $SU(N)$ SQCD with $2N$ flavors and quartic superpotential. The ${\\cal U}_N^{(m)}$ theories can thus be regarded as an infinite set of UV completions, dual to SQCD with $N_f=2N_c$. The ${\\cal U}_N^{(m)}$ duals have different duality frame quiver representations, with $2m+1$ gauge nodes.
Antelope Creek Lakes · Babes · Babbitt Pbitt Peakeak Backbone Creek · Bald Mountain · Bell MeadoBackbone Creek · Bald Mountain · Bell Meadow · Big Grw · Big Grizzlizzly Mountain · Big Piney Mountain · Big Pine Mountain · Bishop Creek PMountain · Bishop Creek Ponderosa Pine · Black Butte · BlacksMountain
G. T. Gussie
1994-09-15T23:59:59.000Z
The published properties of M1-78 are discussed with the purpose to resolve the object's classification as either a planetary nebula or an ultracompact HII region. A classification as a planetary nebula is rejected primarily because of the high luminosity of the object, but because of the chemical composition and expansion velocity of the nebula, a novel classification is proposed instead: that of an ultracompact HII region with a post-main sequence central star (possibly a WN star). It must therefore follow that observable ultracompact HII regions persist beyond the main sequence lifetimes of at least some massive stars, and so cannot be transient phenomena that are seen only during pre-main sequence or early main sequence evolution.
ARM - VAP Product - visstpx08m1rv4minnis
Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)
AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level:5 TablesExports(Journal Article)41cloth Documentation Data Management FacilityProductssondecalcsondewndcalcg15v4minnis Documentation visst8m1rv4minnis
Maldives: Energy Resources | Open Energy Information
AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on DeliciousPlasmaP a gHigh Plains Wind Farm JumpKahului,Coos BayTHEInformation
Maldives-NREL Cooperation | Open Energy Information
AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on DeliciousPlasmaPLawrence County, Pennsylvania:1975 | Open EnergySeaGenMagpie Jump
Babu, M. Madan
M-1 SUPPLEMENTARY METHODS M1: ALGORITHM TO RECONSTRUCT TRANSCRIPTIONAL NETWORKS ..................................................M-2 Figure 1: Procedure to reconstruct transcriptional regulatory networks ....................................M-2 M2: PROCEDURE TO IDENTIFY ORTHOLOGOUS PROTEINS...................................................................M
Part I -Mechanics M05M.1 -Vibration Damping With a Piston M05M.1 -Vibration Damping With a Piston
Petta, Jason
Part I - Mechanics M05M.1 - Vibration Damping With a Piston M05M.1 - Vibration Damping With a Piston Problem Sometimes it is required to reduce the influence of vertical floor vibration larger than atmospheric pressure. The pistons are typically equipped with a mechanism to dampen
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Compass-M1 Broadcast Codes and Their Application to Acquisition and Tracking
Stanford University
Compass-M1 Broadcast Codes and Their Application to Acquisition and Tracking Grace Xingxin Gao his Ph.D. from the University of Illinois in 1983. ABSTRACT With the launch of the Compass-M1 systems (GNSS). The satellite, sometimes referred to as Compass-2 or Beidou-2, is the first of the Compass
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Involvement of the transcription factor FoxM1 in contact inhibition
Faust, Dagmar; Al-Butmeh, Firas; Linz, Berenike [Institute of Toxicology, Medical Center of the Johannes Gutenberg-University, Obere Zahlbacherstr. 67, 55131 Mainz (Germany)] [Institute of Toxicology, Medical Center of the Johannes Gutenberg-University, Obere Zahlbacherstr. 67, 55131 Mainz (Germany); Dietrich, Cornelia, E-mail: cdietric@uni-mainz.de [Institute of Toxicology, Medical Center of the Johannes Gutenberg-University, Obere Zahlbacherstr. 67, 55131 Mainz (Germany)] [Institute of Toxicology, Medical Center of the Johannes Gutenberg-University, Obere Zahlbacherstr. 67, 55131 Mainz (Germany)
2012-10-05T23:59:59.000Z
Highlights: Black-Right-Pointing-Pointer The transcription factor FoxM1 is downregulated upon contact inhibition. Black-Right-Pointing-Pointer The decrease in FoxM1 levels occurs very likely due to inhibition of ERK activity. Black-Right-Pointing-Pointer The decrease in FoxM1 is not sufficient, but required for contact inhibition. Black-Right-Pointing-Pointer We propose a new model of contact inhibition involving pRB/E2F and FoxM1. -- Abstract: Contact inhibition is a crucial mechanism regulating proliferation in vitro and in vivo. Although it is generally accepted that contact inhibition plays a pivotal role in maintaining tissue homeostasis, the molecular mechanisms of contact inhibition are still not fully understood. FoxM1 is known as a proliferation-associated transcription factor and is upregulated in many cancer types. Vice versa, anti-proliferative signals, such as TGF-{beta} and differentiation signals decrease FoxM1 expression. Here we investigated the role of FoxM1 in contact inhibition in fibroblasts. We show that protein expression of FoxM1 is severely and rapidly downregulated upon contact inhibition, probably by inhibition of ERK activity, which then leads to decreased expression of cyclin A and polo-like kinase 1. Vice versa, ectopic expression of FoxM1 prevents the decrease in cyclin A and polo-like kinase 1 and causes a two-fold increase in saturation density indicating loss of contact inhibition. Hence, we show that downregulation of FoxM1 is required for contact inhibition by regulating expression of cyclin A and polo-like kinase 1.
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M1 Master Mathematiques de Metz Mod`eles probabilistes en finance
Thalmaier, Anton
M1 Master Math´ematiques de Metz Mod`eles probabilistes en finance 2007/2008 R. Lamberton, B. Lapeyre: Introduction au calcul stochastique appliqu´e `a la finance. Ellipses, 1997 (b) S. E. Shreve: Stochastic calculus for finance. I: The binomial asset pricing model. Springer Finance, 2004 (c
New probe of M1 and E1 strengths in GDR regions
Hayakawa, T. [Japan Atomic Energy Agency and National Astronomical Observatory in Japan (Japan); Ogata, K. [RCNP, Osaka University (Japan); Miyamoto, S.; Mochizuki, T.; Horikawa, K.; Amano, S. [University of Hyogo (Japan); Imazaki, K.; Li, D.; Izawa, Y. [Institute for Laser Technology (Japan); Chiba, S. [Tokyo Institute of Technology (Japan)
2014-05-02T23:59:59.000Z
The M1 strengths (or level density of 1{sup +} states) are of importance for estimation of interaction strengths between neutrinos and nuclei for the study of the supernova neutrino-process. In 1957, Agodi predicted theoretically angular distribution of neutrons emitted from states excited via dipole transitions with linearly polarized gamma-ray beam at the polar angle of ?=90° should be followed by a simple function, a + b cos(2?), where ?, is azimuthal angel. However, this theoretical prediction has not been verified over the wide mass region except for light nuclei as deuteron. We have measured neutron angular distributions with (polarized gamma, n) reactions on Au, Nal, and Cu. We have verified the Agodi's prediction for the first time over the wide mass region. This suggests that (polarized gamma, n) reactions may be useful tools to study M1 strengths in giant resonance regions.
IUP SID M1, 2005 T.P. SAS numero 01
Lagnoux, Agnès
IUP SID M1, 2005 T.P. SAS num´ero 01 Apr`es quelques g´en´eralit´es sur le logiciel SAS, l'objet de place l'environnement UNIX n´ecessaire `a l'utilisation de SAS dans des conditions commodes. G´en´eralit´es sur le logiciel SAS Le logiciel SAS est de conception am´ericaine : il est developp´e et commercialis
Maldives-Supporting the Zero Emissions Strategy | Open Energy Information
AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on DeliciousPlasmaPLawrence County, Pennsylvania:1975 | Open EnergySeaGenMagpie Jump(SREP) | Open Energy
15.01.01.M1 Treatment of Costs for Sponsored Agreements Page 1 of 2 UNIVERSITY RULE
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Search for 14.4 keV solar axions from M1 transition of Fe-57...
Office of Scientific and Technical Information (OSTI)
Search for 14.4 keV solar axions from M1 transition of Fe-57 with CUORE crystals Citation Details In-Document Search Title: Search for 14.4 keV solar axions from M1 transition of...
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Bermúdez, José Luis
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Cathey, Carol Grmela
1993-01-01T23:59:59.000Z
The aflatoxins comprise a subgroup of mycotoxins usually produced by Aspergillus parasiticus or Aspergillus flavus. Dairy cattle which ingest aflatoxin-contaminated feed will excrete aflatoxin M1 into the milk. The presence of this metabolite...
Global m=1 modes and migration of protoplanetary cores in eccentric protoplanetary discs
J. C. B. Papaloizou
2002-04-11T23:59:59.000Z
We calculate global $m=1$ modes with low pattern speed corresponding to introducing a finite eccentricity into a protoplanetary disc. We consider disc models which are either isolated or contain one or two protoplanets orbiting in an inner cavity. Global modes that are strongly coupled to inner protoplanets are found to have disc orbits which tend to have apsidal lines antialigned with respect to those of the inner protoplanets. Other modes corresponding to free disc modes may be global over a large range of length scales and accordingly be long lived. We consider the motion of a protoplanet in the earth mass range embedded in an eccentric disc and determine the equilibrium orbits which maintain fixed apsidal alignment with respect to the disc gas orbits. Equilibrium eccentricities are found to be comparable or possibly exceed the disc eccentricity. We then approximately calculate the tidal interaction with the disc in order to estimate the orbital migration rate. Results are found to deviate from the case of axisymmetric disc with near circular protoplanet orbit once eccentricities of protoplanet and disc orbits become comparable to the disc aspect ratio in magnitude. Aligned protoplanet orbits with very similar eccentricity to that of the gas disc are found to undergo litle eccentricity change while undergoing inward migration in general. However, for significantly larger orbital eccentricities, migration may be significantly reduced or even reverse from inwards to outwards. Thus the existence of global non circular motions in discs with radial excursions comparable to the semi-thickness may have important consequences for the migration and survival of protoplanetary cores in the earth mass range.
The M 31 double nucleus probed with OASIS and HST. A natural m=1 mode?
R. Bacon; E. Emsellem; F. Combes; Y. Copin; G. Monnet; P. Martin
2001-02-23T23:59:59.000Z
We present observations with the adaptive optics assisted integral field spectrograph OASIS of the M 31 double nucleus at a spatial resolution better than 0.5 arcsec FWHM. These data are used to derive the two-dimensional stellar kinematics within the central 2 arcsec. Archival WFPC2/HST images are revisited to perform a photometric decomposition of the nuclear region. We also present STIS/HST kinematics obtained from the archive. The luminosity distribution of the central region is well separated into the respective contributions of the bulge, the nucleus including P1 and P2, and the so-called UV peak. We then show that the axis joining P1 and P2, the two local surface brightness maxima, does not coincide with the kinematic major-axis, which is also the major-axis of the nuclear isophotes (excluding P1). We also confirm that the velocity dispersion peak is offset by ~ 0.2 arcsec from the UV peak, assumed to mark the location of the supermassive black hole. The newly reduced STIS/HST velocity and dispersion profiles are then compared to OASIS and other published kinematics. We find significant offsets with previously published data. Simple parametric models are then built to successfully reconcile all the available kinematics. We finally interpret the observations using new N-body simulations. The nearly keplerian nuclear disk of M31 is subject to a natural m=1 mode, with a very slow pattern speed (3 km/s/pc for M_BH = 7 10^7~\\Msun), that can be maintained during more than a thousand dynamical times. The resulting morphology and kinematics of the mode can reproduce the M~31 nuclear-disk photometry and mean stellar velocity, including the observed asymmetries. It requires a central mass concentration and a cold disk system representing between 20 and 40% of its mass. Abridged..
UNIVERSITYOF HAWAI'I lIl3RARY INTERNAL TIDE SCATTERING AT M1DOCEAN TOPOGRAPHY
Luther, Douglas S.
of the topography and along a tidal beam up to the first surface bounce. A transition from a beam structure nearUNIVERSITYOF HAWAI'I lIl3RARY INTERNAL TIDE SCATTERING AT M1DOCEAN TOPOGRAPHY A DISSERTATION The scattering ofmode-oneM, internal tides from I) idealized Gaussian topography and 2) the Line Islands Ridge
29.01.03.M1.12 Information Resources Network Access Page 1 of 3 STANDARD ADMINISTRATIVE PROCEDURE
by University Information Technology services, and which backhaul data from a location to a central site thus Technology Risk Management #12;29.01.03.M1.12 Information Resources Network Access Page 3 of 3 OFFICE OF RESPONSIBILITY: Associate Vice President for Information Technology & Chief Information Officer #12;
The $E1$ & $M1$ Spontaneous Decay Rates for an Emitter Inside a Cavity Within a Medium
Singh, Jaideep
2015-01-01T23:59:59.000Z
We discuss the $E1$ and $M1$ spontaneous decay rates of the an emitter residing inside of a real cavity carved out of a vast, uniform, homogenous, isotropic, linear, lossless, dispersionless, and continuous medium. The ratio of the medium rate to vacuum rate is given by $\\Gamma_m/\\Gamma_0 = [G(u)]^2 n^3 / u$, where $G(u) = 3u/(2u+1)$ is the local field correction factor, $n = \\sqrt{\\epsilon\\mu/(\\epsilon_0\\mu_0)}$ is the index of refraction of the medium, $\\epsilon(\\epsilon_0)$ is the electric permitivity of the medium (vacuum), $\\mu(\\mu_0)$ is the magnetic permeability of the medium (vacuum), and $u = \\epsilon/\\epsilon_0$ for $E1$ transitions or $u = \\mu_0/\\mu$ for $M1$ transitions.
Evidence for binarity in the bipolar planetary nebulae A79, He2-428 and M1-91
M. Rodriguez; R. L. M. Corradi; A. Mampaso
2001-09-25T23:59:59.000Z
We present low and high resolution long-slit spectra of three bipolar planetary nebulae (PNe) with bright central cores: A79, He2-428 and M1-91. He2-428 and M1-91 have high density (from 10^3.3 to 10^6.5 cm^-3) unresolved nebular cores that indicate that strong mass loss/exchange phenomena are occurring close to their central stars. An F0 star is found at the centre of symmetry of A79; its reddening and distance are consistent with the association of the star with the nebula. The spectrum of the core of He2-428 shows indications of the presence of a hot star with red excess emission, probably arising in a late-type companion. A79 is one of the richest PNe in N and He, the abundances of M1-91 are at the lower end of the range spanned by bipolar PNe, and He2-428 shows very low abundances, similar to those measured for halo PNe. The extended nebulae of A79 and He2-428 have inclined equatorial rings expanding at a velocity of approx. 15 km/s, with kinematical ages 10^4 yr. The association of these aged, extended nebulae with a dense nebular core (He2-428) or a relatively late type star (A79) is interpreted as evidence for the binarity of their nuclei.
Evidence for binarity in the bipolar planetary nebulae A79, He2-428 and M1-91
Rodríguez, M; Mampaso, A
2001-01-01T23:59:59.000Z
We present low and high resolution long-slit spectra of three bipolar planetary nebulae (PNe) with bright central cores: A79, He2-428 and M1-91. He2-428 and M1-91 have high density (from 10^3.3 to 10^6.5 cm^-3) unresolved nebular cores that indicate that strong mass loss/exchange phenomena are occurring close to their central stars. An F0 star is found at the centre of symmetry of A79; its reddening and distance are consistent with the association of the star with the nebula. The spectrum of the core of He2-428 shows indications of the presence of a hot star with red excess emission, probably arising in a late-type companion. A79 is one of the richest PNe in N and He, the abundances of M1-91 are at the lower end of the range spanned by bipolar PNe, and He2-428 shows very low abundances, similar to those measured for halo PNe. The extended nebulae of A79 and He2-428 have inclined equatorial rings expanding at a velocity of approx. 15 km/s, with kinematical ages 10^4 yr. The association of these aged, extended ...
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Behmer, Spencer T.
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MSU Recycling recycle.msu.edu 517-355-1723 MARCH 15, 2014 9:00A.M.1:00P.M.
Liu, Taosheng
MSU Recycling · recycle.msu.edu · 517-355-1723 MARCH 15, 2014 · 9:00A.M.1:00P.M. RECYCLINGLn Green Way Public Recycling Drop-o Center E-Waste Drop-o MSU Surplus Store & Recycling Center Service Rd Service Rd RecyclingDr NORTH Public Electronics Recycling March 15, 2014 · 9:00A.M.1:00P.M. MSU Surplus
He, Qian [ORNL; Woo, Jungwon [University of Cincinnati; Belianinov, Alex [ORNL; Guliants, Vadim V. [University of Cincinnati; Borisevich, Albina Y [ORNL
2015-01-01T23:59:59.000Z
In recent decades, catalysis research has transformed from the predominantly empirical field to one where it is possible to control the catalytic properties via characterization and modification of the atomic-scale active centers. Many phenomena in catalysis, such as synergistic effect, however, transcend the atomic scale and also require the knowledge and control of the mesoscale structure of the specimen to harness. In this paper, we use our discovery of atomic-scale epitaxial interfaces in molybdenum vanadium based complex oxide catalysts systems (i.e., MoVMO, M = Ta, Te, Sb, Nb, etc.) to achieve control of the mesoscale structure of this complex mixture of very different active phases. We can now achieve true epitaxial intergrowth between the catalytically critical M1 and M2 phases in the system that are hypothesized to have synergistic interactions, and demonstrate that the resulting catalyst has improved selectivity in the initial studies. Finally, we highlight the crucial role atomic scale characterization and mesoscale structure control play in uncovering the complex underpinnings of the synergistic effect in catalysis.
Gonzalez-Horta, Francisco A; Ramirez-Cortes, Juan M; Martinez-Carballido, Jorge; Buenfil-Alpuche, Eldamira
2011-01-01T23:59:59.000Z
Performance curves of queueing systems can be analyzed by separating them into three regions: the flat region, the knee region, and the exponential region. Practical considerations, usually locate the knee region between 70-90% of the theoretical maximum utilization. However, there is not a clear agreement about where the boundaries between regions are, and where exactly the utilization knee is located. An open debate about knees in performance curves was undertaken at least 20 years ago. This historical debate is mainly divided between those who claim that a knee in the curve is not a well defined term in mathematics, or it is a subjective and not really meaningful concept, and those who define knees mathematically and consider their relevance and application. In this paper, we present a mathematical model and analysis for identifying the three mentioned regions on performance curves for M/M/1 systems; specifically, we found the knees, or optimal utilization percentiles, at the vertices of the hyperbolas tha...
Behmer, Spencer T.
08.01.01.M1.02 Investigation and Resolution of Complaints Against Faculty Members for Illegal 08.01.01.M1.02 Investigation and Resolution of Complaints Against Faculty Members for Illegal;08.01.01.M1.02 Investigation and Resolution of Complaints Against Faculty Members for Illegal Discrimination
., utilized to verify the accuracy of FAMIS records. This system is not used to provide management reports statement, used to verify the accuracy of FAMIS records. This system is not used to provide management21.01.01.M1.01 Accounting Procedures for Departmental Fiscal Record Keeping Page 1 of 4 STANDARD
Maldives-Program for Scaling Up Renewable Energy in Low Income...
the activities of other existing energy initiatives. It operates in a small number of low-income countries to maximize its impact and demonstrative effect." References "Program...
Maldives-Program for Scaling Up Renewable Energy in Low Income Countries
AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on DeliciousPlasmaPLawrence County, Pennsylvania:1975 | Open EnergySeaGenMagpie Jump(SREP) | Open Energy Information
Zevenhoven, Ron
Svar 1303: a. Långsamt & adiabatiskt reversibel, dvs en isentropisk process V1 = n·R·T1 / p1 = (m/M) ·R·T1/p1 , massa m = 1 kg H2 : M = 0.002 kg/mol; CO : M = 0.028 kg/mol; CO2 : M = 0.044 kg/mol p1 = z bar V1 = (R/M) · (300 + 50·a) / z m3 . t.ex. 30066 : p = 3 bar, gas = CO, T1 = 450 K V1 = 0.445 m3
Song, Young-Ho; Lazauskas, Rimantas; Park, Tae-Sun [Department of Physics, Duke University, Durham, North Carolina 27708 (United States); IPHC, IN2P3-CNRS/Universite Louis Pasteur BP 28, F-67037 Strasbourg Cedex 2 (France); Department of Physics and BAERI, Sungkyunkwan University, Suwon 440-746 (Korea, Republic of)
2009-06-15T23:59:59.000Z
M1 properties, comprising magnetic moments and radiative capture of thermal neutron observables, are studied in two- and three-nucleon systems. We use meson exchange current derived up to N{sup 3}LO using heavy baryon chiral perturbation theory a la Weinberg. Calculations have been performed for several qualitatively different realistic nuclear Hamiltonians, which permits us to analyze model dependence of our results. Our results are found to be strongly correlated with the effective range parameters such as binding energies and the scattering lengths. Taking into account such correlations, the results are in good agreement with the experimental data with small model dependence.
Muthukumar, Kaliappan [University of Cincinnati; Yu, Junjun [University of Cincinnati; Xu, Ye [ORNL; Guliants, Vadim V. [University of Cincinnati
2011-01-01T23:59:59.000Z
Density functional theory calculations (GGA-PBE) have been performed to investigate the adsorption of C3 (propane, isopropyl, propene, and allyl) and H species on the proposed active center present in the surface ab planes of the bulk Mo-V-Te-Nb-O M1 phase in order to better understand the roles of the different surface cations in propane ammoxidation. Modified cluster models were employed to isolate the closely spaced V=O and Te=O from each other and to vary the oxidation state of the V cation. While propane and propene adsorb with nearly zero adsorption energy, the isopropyl and allyl radicals bind strongly to V=O and Te=O with adsorption energies, {Delta}E, being {le} -1.75 eV, but appreciably more weakly on other sites, such as Mo=O, bridging oxygen (Mo-O-V and Mo-O-Mo), and empty metal apical sites ({Delta}E > -1 eV). Atomic H binds more strongly to Te = O ({Delta}E {le} -3 eV) than to all the other sites, including V = O ({Delta}E = -2.59 eV). The reduction of surface oxo groups by dissociated H and their removal as water are thermodynamically favorable except when both H atoms are bonded to the same Te=O. Consistent with the strong binding of H, Te=O is markedly more active at abstracting the methylene H from propane (E{sub a} {le} 1.01 eV) than V = O (E{sub a} = 1.70 eV on V{sup 5+} = O and 2.13 eV on V{sup 4+} = O). The higher-than-observed activity and the loose binding of Te = O moieties to the mixed metal oxide lattice of M1 raise the question of whether active Te = O groups are in fact present in the surface ab planes of the M1 phase under propane ammoxidation conditions.
New limit on the mass of 14.4-keV solar axions emitted in an M1 transition in {sup 57}Fe nuclei
Derbin, A. V., E-mail: derbin@pnpi.spb.ru; Muratova, V. N.; Semenov, D. A.; Unzhakov, E. V. [Russian Academy of Sciences, Petersburg Nuclear Physics Institute (Russian Federation)
2011-04-15T23:59:59.000Z
Axions of energy 14.4 keV that originated from the M1 transition in {sup 57}Fe nuclei in the Sun were sought by using the resonance-absorption reaction A+{sup 57}Fe {yields} {sup 57}Fe* {yields} {sup 57}Fe+{gamma} (14.4 keV). Asectioned Si(Li) detector arranged in a low-background facility was used to record photons from this reaction. This resulted in setting a new limit on the axion couplings to nucleons, vertical bar -1.19g{sub AN}{sup 0} + g{sub AN}{sup 3} vertical bar {<=} 3.0 Multiplication-Sign 10{sup -6}. Within the hadronic-axion model, the respective constraint on the axion mass is m{sub A} {<=} 145 eV (at a 95% C.L.).
Search for 14.4-KeV Solar Axions Emitted in the M1-Transition of Fe-57 Nuclei with CAST
Andriamonje, S.; Aune, S.; /DAPNIA, Saclay; Autiero, D.; /CERN /Lyon, IPN; Barth, K.; /CERN; Belov, A.; /Moscow, INR; Beltran, B.; /Zaragoza U. /Queen's U., Kingston; Brauninger, H.; /Garching, Max Planck Inst., MPE; Carmona, J.M.; Cebrian, S.; /Zaragoza U.; Collar, J.I.; /Chicago U., EFI /Chicago U., KICP; Dafni, T.; /DAPNIA, Saclay /Darmstadt, Tech. Hochsch. /Zaragoza U.; Davenport, M.; /CERN; Di Lella, L.; /CERN /Pisa, Scuola Normale Superiore; Eleftheriadis, C.; /Aristotle U., Thessaloniki; Englhauser, J.; /Garching, Max Planck Inst., MPE; Fanourakis, G.; /Democritos Nucl. Res. Ctr.; Ferrer-Ribas, E.; /DAPNIA, Saclay; Fischer, H.; Franz, J.; /Freiburg U.; Friedrich, P.; /Garching, Max Planck Inst., MPE; Geralis, T.; /Democritos Nucl. Res. Ctr. /DAPNIA, Saclay /Moscow, INR /Zaragoza U. /British Columbia U. /Freiburg U. /Darmstadt, Tech. Hochsch. /DAPNIA, Saclay /Zaragoza U. /Frankfurt U. /Boskovic Inst., Zagreb /Freiburg U. /Munich, Max Planck Inst. /Boskovic Inst., Zagreb /Democritos Nucl. Res. Ctr. /Darmstadt, Tech. Hochsch. /Garching, Max Planck Inst., MPE /Boskovic Inst., Zagreb /CERN /Aristotle U., Thessaloniki /Boskovic Inst., Zagreb /Munich, Max Planck Inst. /Zaragoza U. /Chicago U., EFI /Chicago U., KICP /Stanford U., Phys. Dept. /SLAC /Zaragoza U. /CERN /DAPNIA, Saclay /CERN /Munich, Max Planck Inst. /Darmstadt, Tech. Hochsch. /Zaragoza U. /Aristotle U., Thessaloniki /Patras U. /Brookhaven /CERN /Munich, Max Planck Inst. /CERN /Chicago U., EFI /Chicago U., KICP /Zaragoza U. /Freiburg U. /CERN /CERN /Patras U.
2011-12-02T23:59:59.000Z
We have searched for 14.4 keV solar axions or more general axion-like particles (ALPs), that may be emitted in the M1 nuclear transition of 57Fe, by using the axion-to-photon conversion in the CERN Axion Solar Telescope (CAST) with evacuated magnet bores (Phase I). From the absence of excess of the monoenergetic X-rays when the magnet was pointing to the Sun, we set model-independent constraints on the coupling constants of pseudoscalar particles that couple to two photons and to a nucleon g{sub ay}|-1.19g{sub aN}{sup 0}+g{sub aN}{sup 3}| < 1.36 x 10{sup -16} GeV{sup -1} for ma < 0.03 eV at the 95% confidence level.
D Blom; X Li; S Mitra; T Vogt; D Buttrey
2011-12-31T23:59:59.000Z
A full frozen phonon multislice simulation of high angle annular dark field scanning transmission electron microscopy (HAADF STEM) images from the M1 phase of the Mo-V-Nb-Te-O propane oxidation catalyst has been performed by using the latest structural model obtained using the Rietveld method. Simulated contrast results are compared with experimental HAADF images. Good agreement is observed at ring sites, however significant thickness dependence is noticed at the linking sites. The remaining discrepancies between the model based on Rietveld refinement and image simulations indicate that the sampling of a small volume element in HAADF STEM and averaging elemental contributions of a disordered site in a crystal slab by using the virtual crystal approximation might be problematic, especially if there is preferential Mo/V ordering near the (001) surface.
Govindasamy, Agalya [University of Cincinnati; Muthukumar, Kaliappan [University of Cincinnati; Yu, Junjun [University of Cincinnati; Xu, Ye [ORNL; Guliants, Vadim V. [University of Cincinnati
2010-01-01T23:59:59.000Z
The Mo-V-Te-Nb-O mixed metal oxide catalyst possessing the M1 phase structure is uniquely capable of directly converting propane into acrylonitrile. However, the mechanism of this complex eight-electron transformation, which includes a series of oxidative H-abstraction and N-insertion steps, remains poorly understood. We have conducted a density functional theory study of cluster models of the proposed active and selective site for propane ammoxidation, including the adsorption of propane, isopropyl (CH{sub 3}CHCH{sub 3}), and H which are involved in the first step of this transformation, that is, the methylene C-H bond scission in propane, on these active site models. Among the surface oxygen species, the telluryl oxo (Te=O) is found to be the most nucleophilic. Whereas the adsorption of propane is weak regardless of the MO{sub x} species involved, isopropyl and H adsorption exhibits strong preference in the order of Te=O > V=O > bridging oxygens > empty Mo apical site, suggesting the importance of TeO{sub x} species for H abstraction. The adsorption energies of isopropyl and H and consequently the reaction energy of the initial dehydrogenation of propane are strongly dependent on the number of ab planes included in the cluster, which points to the need to employ multilayer cluster models to correctly capture the energetics of surface chemistry on this mixed metal oxide catalyst.
Search for 14.4 keV solar axions from M1 transition of {sup 57}Fe with CUORE crystals
NONE
2013-05-01T23:59:59.000Z
We report the results of a search for axions from the 14.4 keV M1 transition from {sup 57}Fe in the core of the sun using the axio-electric effect in TeO{sub 2} bolometers. The detectors are 5 × 5 × 5 cm{sup 3} crystals operated at about 10 mK in a facility used to test bolometers for the CUORE experiment at the Laboratori Nazionali del Gran Sasso in Italy. An analysis of 43.65 kg?d of data was made using a newly developed low energy trigger which was optimized to reduce the energy threshold of the detector. An upper limit of 0.58 c?kg{sup ?1}?d{sup ?1} is established at 95% C.L., which translates into lower bounds f{sub A} ? 3.12 × 10{sup 5} GeV 95% C.L. (DFSZ model) and f{sub A} ? 2.41 × 10{sup 4} GeV 95% C.L. (KSVZ model) on the Peccei-Quinn symmetry-breaking scale, for a value of S = 0.5 of the flavor-singlet axial vector matrix element. These bounds can be expressed in terms of axion masses as m{sub A} ? 19.2 eV and m{sub A} ? 250 eV at 95% C.L. in the DFSZ and KSVZ models respectively. Bounds are given also for the interval 0.35 ? S ? 0.55.
International reserves management and the current account
Aizenman, Joshua
2007-01-01T23:59:59.000Z
Italy Japan Kuwait Luxembourg Malta Netherlands NetherlandsMalaysia Maldives Mali Malta Mauritania Mauritius MexicoMalaysia Maldives Mali Malta Mauritius Mexico Mongolia
International reserves management and the current account
Aizenman, Joshua
2007-01-01T23:59:59.000Z
Iran, I.R. of Lesotho Macedonia, FYR Maldives Mali MexicoJamaica Jordan Kazakhstan Macedonia, FYR Maldives MoroccoLibya Lithuania Luxembourg Macedonia, FYR Madagascar Malawi
3 = 10:0S=m 2 = 0:01S=m 1 = 0:1S=m 0 = 10 7 S=m 5 = 1:0S=m 6 ...
3 = 10:0S=m. 2 = 0:01S=m. 1 = 0:1S=m. 0 = 10 7. S=m. 5 = 1:0S=m. 6 = 0:01S=m. z [km]. x [km]. -20.0. 20.0. -70.0. 70.0. 2.5. 12.5. 32.5. 60.0.
Cai, Wei
= subs(diff(t1,x,2),x,0)/factorial(2) s3 = subs(diff(t1,x,1),x,0)/factorial(1) s4 = subs(t1,x,0) s5 s = solve(s1, s2, s3, s4+p, s5, s6, s7, s8, ... s9, s10,s11,s12, s13,s14,s15,s16, ... b1, b2, b3, Fx1,M1, Fy
M 1 Partners | Open Energy Information
AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on DeliciousPlasmaP a g eWorks -09-0018-CX JumpShun DaSilicon CoCalifornia)EnergyLowJinman RiverLyntegarLincoln1 Partners
M1 Energy | Open Energy Information
AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on DeliciousPlasmaPLawrence County, Pennsylvania: EnergyInformationLoyola,Lyndeborough,Lyonsdale Biomass LLCM AMM1
Departement Informatique M1 Informatique, UE 1
Richer, Jean-Michel
(string& s) qui Â´elimine les espaces, tabulations et re- tour `a la ligne en partie gauche de la cha`ere de la cha^ine qui n'est pas un espace, puis la fonction erase pour supprimer les caract`eres indÂ´esirables. Exercice 2 - Ecrire une fonction trim right(string& s) qui Â´elimine les espaces, tabulations et retour `a
STUDENT HEALTH SERVICES University of Massachusetts Lowell
Massachusetts at Lowell, University of
-Bissau Maldives Papua New Guinea Swaziland Anguilla Colombia Guyana Mali Paraguay Tajikistan Argentina Comoros
Zevenhoven, Ron
M = 1x 50 kPa = x100 kPa+ (1x)10 kPa 50 = 100x + 10(1x) x = 0,444 = xB xM = 0,556 pB = yBp = xBpB° yB = xBpB° / p = 0,888 yM = 1 yB = 0,112 424. a. van Laar coefficients: B = ln (B ) = 1,97, A = ln (A ) = 2,40 x = 0.5: ln B = B / (1 + B/A)2 = 0,594 B = 1,81 ln
Etrejeun?/9-m 1-I tre jeune en Palestine
Boyer, Edmond
, bloquÃ©s par une jeep de soldats israÃ©liens.Leurs cartesd'identitÃ© sont saisies,ils attendent sous le soldats: Â«Tu veux tirer, tire, mais moi je vais passer mes examensÂ» et il leur tourne le dos pour entrer
ARM - VAP Product - visstpx04m1rv1minnis
Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)
AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level:5 TablesExports(Journal Article)41cloth Documentation Data Management FacilityProductssondecalcsondewndcalcg15v4minnis Documentation visst : XDCrv1minnis
ARM - VAP Product - visstpx04m1rv3minnis
Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)
AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level:5 TablesExports(Journal Article)41cloth Documentation Data Management FacilityProductssondecalcsondewndcalcg15v4minnis Documentation visst :
ARM - VAP Product - visstpx04m1rv4minnis
Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)
AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level:5 TablesExports(Journal Article)41cloth Documentation Data Management FacilityProductssondecalcsondewndcalcg15v4minnis Documentation visst :rv4minnis
Hard two photon processes ??--> M_2 M_1 in QCD
Victor L. Chernyak
2012-12-06T23:59:59.000Z
A short review of leading term QCD predictions vs those of the handbag model for large angle cross sections \\gamma\\gamma --> P_2 P_1 (P is the pseudoscalar meson \\pi^{\\pm,o}, K^{\\pm,o}, \\eta), and for \\gamma\\gamma --> V_2 V_1 (V is the neutral vector meson \\rho^o, \\omega, \\phi), in comparison with Belle Collaboration measuments
Part I--Mechanics J01M.1--Particle on a Torus J01M.1--Particle on a Torus
Petta, Jason
frame acceleration is 2 times that in the lab frame. #12;Part II--E & M J01E.3--Electromagnetic Wave on a Slab of Dielectric J01E.3--Electromagnetic Wave on a Slab of Dielectric Problem A plane electromagnetic pulse E(z, t) = f(z/c - t) is incident from vacuum at z
Rynkun, P., E-mail: pavel.rynkun@gmail.com [Department of Physics and Information Technologies, Lithuanian University of Educational Science, Studentu 39, LT-08106 Vilnius (Lithuania); Jönsson, P. [Group for Materials Science and Applied Mathematics, Malmö University, 20506 Malmö (Sweden)] [Group for Materials Science and Applied Mathematics, Malmö University, 20506 Malmö (Sweden); Gaigalas, G. [Department of Physics and Information Technologies, Lithuanian University of Educational Science, Studentu 39, LT-08106 Vilnius (Lithuania) [Department of Physics and Information Technologies, Lithuanian University of Educational Science, Studentu 39, LT-08106 Vilnius (Lithuania); Vilnius University, Institute of Theoretical Physics and Astronomy, A. Goštauto 12, LT-01108 Vilnius (Lithuania); Froese Fischer, C. [National Institute of Standards and Technology, Gaithersburg, MD 20899-8420 (United States)] [National Institute of Standards and Technology, Gaithersburg, MD 20899-8420 (United States)
2014-03-15T23:59:59.000Z
Based on relativistic wavefunctions from multiconfiguration Dirac–Hartree–Fock and configuration interaction calculations, E1, M1, E2, and M2 transition rates, weighted oscillator strengths, and lifetimes are evaluated for the states of the (1s{sup 2})2s{sup 2}2p{sup 3},2s2p{sup 4}, and 2p{sup 5} configurations in all nitrogen-like ions between F III and Kr XXX. The wavefunction expansions include valence, core–valence, and core–core correlation effects through single–double multireference expansions to increasing sets of active orbitals. The computed energies agree very well with experimental values, with differences of only 300–600 cm{sup ?1} for the majority of the levels and ions in the sequence. Computed transitions rates are in close agreement with available data from MCHF-BP calculations by Tachiev and Froese Fischer [G.I. Tachiev, C. Froese Fischer, A and A 385 (2002) 716].
, Frida Gorani, Gülden Þorvaldsson, Jón Þórir lpv 6 ingen uppsamling Ingelström, Mattias Jönsson, Hedda
Explaining the causes and consequences of internationally monitored elections
Hyde, Susan Dayton
2006-01-01T23:59:59.000Z
Maldives San Marino Bahamas Malta Sao Tome & PrincipePapua New Guinea, Bahamas*, Malta* Bolivia, Cyprus, Jamaica,Slovenia, Cape Verde*, Malta* Poland, Slovenia, Mongolia,
The Right to Life with Dignity: Economic and Social Rights Respect in the World
Kolp, Felicity Ann
2010-01-01T23:59:59.000Z
Malaysia Maldives Mali Malta Mauritania Mauritius MexicoItaly Ukraine Trinidad and Tobago Malta New Zealand IcelandCyprus Germany Greece Malta Freq. Country Sweden Finland
National Nuclear Security Administration (NNSA)
AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level:5 TablesExports to3,1,50022,3,,0,,6,1,Separation 23Tribal EnergyCatalytic Coby Mods 002, 006, 020,holidayCFRThe Summary S-5 *C C l lRevision* S H
National Nuclear Security Administration (NNSA)
AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level:5 TablesExports to3,1,50022,3,,0,,6,1,Separation 23Tribal EnergyCatalytic Coby Mods 002, 006, 020,holidayCFRThe Summary S-5 *C C l lRevision* S HM
Water/Wastewater Engineering Report (Storm Sewer/Infiltration Sanitary Sewage Separation-M1 Model)
Liu, Z.; Brumbelow, K.; Haberl, J. S.
2006-10-30T23:59:59.000Z
In some cities, the municipal sewer system collects both storm water and sanitary sewage in the same pipes. During dry weather these sewers carry all the sanitary sewage to the wastewater treatment plant for treatment. However, when rainstorms...
Water/Wastewater Engineering Report (Storm Sewer/Infiltration Sanitary Sewage Separation-M1 Model)
Liu, Z.; Brumbelow, K.; Haberl, J. S.
2006-10-30T23:59:59.000Z
The Energy Systems Laboratory greatly appreciates the assistance and guidance provided by the staff at the Texas Commission on Environmental Quality on this report, especially the assistance of Mr. Steve Anderson. Assistance from Ms. Sherrie Hughes (ESL...
The M 31 double nucleus probed with OASIS and HST. A natural m=1 mode?
Bacon, R; Combes, F; Copin, Y; Monnet, G; Martin, P
2001-01-01T23:59:59.000Z
We present observations with the adaptive optics assisted integral field spectrograph OASIS of the M 31 double nucleus at a spatial resolution better than 0.5 arcsec FWHM. These data are used to derive the two-dimensional stellar kinematics within the central 2 arcsec. Archival WFPC2/HST images are revisited to perform a photometric decomposition of the nuclear region. We also present STIS/HST kinematics obtained from the archive. The luminosity distribution of the central region is well separated into the respective contributions of the bulge, the nucleus including P1 and P2, and the so-called UV peak. We then show that the axis joining P1 and P2, the two local surface brightness maxima, does not coincide with the kinematic major-axis, which is also the major-axis of the nuclear isophotes (excluding P1). We also confirm that the velocity dispersion peak is offset by ~ 0.2 arcsec from the UV peak, assumed to mark the location of the supermassive black hole. The newly reduced STIS/HST velocity and dispersion p...
34.03.01.M1 Alcoholic Beverages Page 1 of 6 UNIVERSITY RULE
under the control of Texas A&M University will not be permitted except at locations designated below license required Presidential Conference Center Requires review and concurrence by the Executive Associate Vice President for each event Bush Presidential Apartment None George Bush Foundation Suite None
Universite Paris 7-Denis Diderot Alg`ebre Annee 2007-08 M1 mathematiques
Merel, Loïc - Institut de Mathématiques de Jussieu, Université Paris 7
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C:\MYDOCS\FBSS-M~1\HATTIE\LAYOUT94.TXT
U.S. Energy Information Administration (EIA) Indexed Site
AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level: National and Regional Data; Row: NAICS Codes; Column:3,2,19,30,"BANGOR HYDRO ELECTRICTables and Spreadsheets 1991A 6Feet) Year7 0 2 4 64221993
Microsoft Word - Sandia-VT M-1 Summary Report_FINAL.docx
Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)
AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level:5 TablesExports(Journal Article) |govInstrumentsmfrirtA Journey Inside the Complex andFOUR Los Phase 1 Radiological TO: SAVINGS PROGRAM FORA Model for
21.99.09.M1 Access to University Property for Sales and Solicitation Purposes
Behmer, Spencer T.
as all University-owned property located in Brazos County, Texas, including Main Campus, West Campus Regulation 21.99.09 1. GENERAL The President of Texas A&M University has delegated the authority to approve organization, Texas A&M University organization, nonprofit, non- student organizations authorized to use Texas
Compass-M1 Broadcast Codes and Their Application to Acquisition and Tracking
Gao, Grace Xingxin
. David has worked previously for Lockheed Martin and for the Intel Corporation. Todd Walter is a Senior MIT in 2001. His current research interests involves UXOs, sensor fusion, autonomous helicopters
Hard two photon processes \\gamma\\gamma --> M_2 M_1 in QCD
Chernyak, Victor L
2012-01-01T23:59:59.000Z
A short review of leading term QCD predictions vs those of the handbag model for large angle cross sections \\gamma\\gamma --> P_2 P_1 (P is the pseudoscalar meson \\pi^{\\pm,o}, K^{\\pm,o}, \\eta), and for \\gamma\\gamma --> V_2 V_1 (V is the neutral vector meson \\rho^o, \\omega, \\phi), in comparison with Belle Collaboration measuments
SI}M!1ARY REPORT ON SITE nnTESTIGATION AND REMOVAL ACTIVITIES
/QC ·..·.······················.·.···..··········.·.. 12 6.0 CONCLUSIONS AND RECO~~OATIONS .·······....·..········ 12 7. () llE.!'.LTH & SAFETY PLAN ···································· 13 9.01 General Site Activities 13 9 .. 02 Health &- Safety " ~ · ~ .. '" '" '" '" . " ~ ~ 1.4 9 ~ 03 activities at the Colorado School of Mines Research Institute (CSMRI) creekside site in Golden~ Colorado
M1G / M2G Rotation Summaries Thursday, August 15th
Engelhardt, John F.
and ATF4 Mediate Distinct and Additive Pathways to Disuse Skeletal Muscle Atrophy" Krishna Iyer, M5G "Dual Energy CT method to assess heterogeneity of perfused blood volume in smokers susceptible to emphysema" 3
A. E. K. Ris Ris-M-[ 1U07 Title and author(s)
-+- 7 illustrations Date Department or group Reactor Physics Department Group's own registration numbers) Abstract A method for treating heterogeneities in diffusion calculations for a reactor is de- scribed.2. Principles of the Monte Carlo Calculation ... 5 2.3. The Monte Carlo Program MOVAX 8 2.3.1. Data Input 8 2
Proposition de stage (M1) de Segret Boris Nom : Segret Boris
Aulanier, Guillaume
pour BIRDY, un CubeSat interplanétaire de survol de Mars et retour. Ces outils sont sous OCTAVE/MATLAB
Crust formation and its role during bread baking1 Vanin, F.M.1,2
Paris-Sud XI, Université de
according to a distinct local heat-moisture treatment. As soon as the dough is placed in the oven, water in the literature are discussed. Keywords crust, bread, baking, water loss, temperature, heating rate, heat and mass 48 21 15. 1 E-mail address: tiphaine.lucas@cemagref.fr Author-produced version of the article
A Realizability-Preserving Discontinuous Galerkin Method for the $M_1$ Model of Radiative Transfer
Frank, Martin [RWTH Aachen University; Olbrant, Edgar [RWTH Aachen University; Hauck, Cory D [ORNL
2012-01-01T23:59:59.000Z
The M{sub 1} model for radiative transfer coupled to a material energy equation in planar geometry is studied in this paper. For this model to be well-posed, its moment variables must fulfill certain realizability conditions. Our main focus is the design and implementation of an explicit Runge-Kutta discontinuous Galerkin method which, under a more restrictive CFL condition, guarantees the realizability of the moment variables and the positivity of the material temperature. An analytical proof for our realizability-preserving scheme, which also includes a slope-limiting technique, is provided and confirmed by various numerical examples. Among other things, we present accuracy tests showing convergence up to fourth-order, compare our results with an analytical solution in a Riemann problem, and consider a Marshak wave problem.
A.E. K.Ris Ris -M -1 i34b Title and author(s)
The programme fits a sum of Lorentzian lines to a given MSssbauer spectrum by means of the Gauss non- linear regression procedure with a facility for con- straining any set of parameters or linear combinations
Landers, Robert G.
step with zero initial conditions. Calculate the unforced response when the initial displacement is 0 force with zero initial conditions. Calculate the forced response to a unit step in the applied force response to a step #12;State Equation 3 with magnitude M. The initial conditions of the states are x1
to the University network system at any time. Definitions CISO Chief Information Security Officer Network Scanning developed by the CISO and at other times as needed by current threats. 2.3 The NIS security team
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/ Responsibilities/ Process 1. REPORTING 1.1 The Office of the Associate Vice President for Information Technology for Information Technology & Chief Information Officer office through email message to complaint@tamu.edu. Reports for Information Technology & Chief Information Officer is responsible for a determination as to whether
Search for 14.4 keV solar axions from M1 transition of Fe-57 with CUORE
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Search for 14.4 keV solar axions from M1 transition of Fe-57 with CUORE
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AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level:5 TablesExports to3,1,50022,3,,0,,6,1,SeparationConnect JournalPentoxide.Conference: to be submittedArticle)SciTechProjectSeaborg Institute
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-competitivenesswith fossil fuel systems,while substantiallyreducingemissionsof Co,. to theatmosphere[Hall, et aI., 1991. This paperexaminesthe effectsof scaleon theprospectivecostsof producingelectricity and alcohol fuels from plantationUion/yearto keeperodiblelandsout of productionundertheConservationReserveProgram (CRP). In addition,price
Chung, Chi-Jung [Department of Health Risk Management, College of Public Health, China Medical University, Taichung, Taiwan (China) [Department of Health Risk Management, College of Public Health, China Medical University, Taichung, Taiwan (China); Department of Medical Research, China Medical University Hospital, Taichung, Taiwan (China); Huang, Chao-Yuan; Pu, Yeong-Shiau [Department of Urology, National Taiwan University Hospital, Taipei, Taiwan (China)] [Department of Urology, National Taiwan University Hospital, Taipei, Taiwan (China); Shiue, Horng-Sheng [Department of Chinese Medicine, Chang Gung Memorial Hospital, Taipei, Taiwan (China)] [Department of Chinese Medicine, Chang Gung Memorial Hospital, Taipei, Taiwan (China); Su, Chien-Tien [Department of Family Medicine, Taipei Medical University Hospital, Taipei, Taiwan (China)] [Department of Family Medicine, Taipei Medical University Hospital, Taipei, Taiwan (China); Hsueh, Yu-Mei, E-mail: ymhsueh@tmu.edu.tw [Department of Public Health, School of Medicine, College of Medicine, Taipei Medical University, Taipei, Taiwan (China) [Department of Public Health, School of Medicine, College of Medicine, Taipei Medical University, Taipei, Taiwan (China); School of Public Health, College of Public Health and Nutrition, Taipei Medical University, Taipei, Taiwan (China)
2013-01-15T23:59:59.000Z
Inter-individual variation in the metabolism of xenobiotics, caused by factors such as cigarette smoking or inorganic arsenic exposure, is hypothesized to be a susceptibility factor for urothelial carcinoma (UC). Therefore, our study aimed to evaluate the role of gene–environment interaction in the carcinogenesis of UC. A hospital-based case–control study was conducted. Urinary arsenic profiles were measured using high-performance liquid chromatography–hydride generator-atomic absorption spectrometry. Genotyping was performed using a polymerase chain reaction-restriction fragment length polymorphism technique. Information about cigarette smoking exposure was acquired from a lifestyle questionnaire. Multivariate logistic regression was applied to estimate the UC risk associated with certain risk factors. We found that UC patients had higher urinary levels of total arsenic, higher percentages of inorganic arsenic (InAs%) and monomethylarsonic acid (MMA%) and lower percentages of dimethylarsinic acid (DMA%) compared to controls. Subjects carrying the GSTM1 null genotype had significantly increased UC risk. However, no association was observed between gene polymorphisms of CYP1A1, EPHX1, SULT1A1 and GSTT1 and UC risk after adjustment for age and sex. Significant gene–environment interactions among urinary arsenic profile, cigarette smoking, and GSTM1 wild/null polymorphism and UC risk were observed after adjustment for potential risk factors. Overall, gene–environment interactions simultaneously played an important role in UC carcinogenesis. In the future, large-scale studies should be conducted using tag-SNPs of xenobiotic-metabolism-related enzymes for gene determination. -- Highlights: ? Subjects with GSTM1 null genotype had significantly increased UC risk. ? UC patients had poor arsenic metabolic ability compared to controls. ? GSTM1 null genotype may modify arsenic related UC risk.
BENDIX SYSTEMS DIVISION ANN A R8 oR, M1CH NO. REV.NO. Solar Wind Programming for
Rathbun, Julie A.
~====~----~--------------~~~~~==~~~ ,f:flow chart is intended only to provide interested parties with an outline of program flow. As program debugging progresses, detailed flow charts just above the coding level format. The mean, variance, and sample size by energy level, arranged in columnar format. The mean
Packer, Alissa A.
ECOLOGY LECTURE (BI 40601) & LABORATORY (BI40711) FALL 2005 Lecture Fischer 316, TTH 10 EMAILpacker@susqu.edu OFFICE HOURS MW 9:0010:00, W 1:302:30 WHAT IS ECOLOGY? Ecology is the study of interrelationships between organisms and their biotic and abiotic environments. As a basic science, ecology informs
, regulation and economic activity should be in the near future? M3 p133. "Cheap energy .. made us the first of civilization, the world in which North America, Europe, and much of the rest of the planet are warm enough
Shyy, Wei
. He is an affiliate of the National PovertyCenterandthe, cities with high rates of poverty, and low-income neighborhoods. University of Michigan Alumni #12;SAVE THE DATE! Please join us for the following 2010 University of Michi
and Unrelated Third Parties for Illegal Discrimination, Sexual Harassment, or Related Retaliation Charges Page 1 Against Non- Faculty Employees and Unrelated Third Parties for Illegal Discrimination, Sexual Harassment-faculty Employees and Unrelated Third Parties for Illegal Discrimination, Sexual Harassment, or Related Retaliation
Administrative Procedure Statement All owners and custodians of information technology resources are expected of a requested exclusion to an information technology rules or SAP. Definitions Information Resource Owner or department, or by the Associate Vice President for Information Technology & Chief Information Officer
Nizet, Victor
University, Cairo, Egypt, 3 The VA Hospital, Memphis, Tennessee, United States of America, 4 The Department Epidemiological studies of group A streptococcus (GAS) have noted an inverse relationship between SpeB expression show that an intact RopB and efficient SpeB production are necessary for systemic infection with GAS
Kalirai, Jason S; Dotter, Aaron; Richer, Harvey B; Fahlman, Gregory G; Hansen, Brad M S; Hurley, Jarrod; Reid, I Neill; Rich, R Michael; Shara, Michael M
2012-01-01T23:59:59.000Z
We present a new measurement of the stellar initial mass function (IMF) based on ultra-deep, high-resolution photometry of >5,000 stars in the outskirts of the Small Magellanic Cloud (SMC) galaxy. The Hubble Space Telescope (HST) Advanced Camera for Surveys (ACS) observations reveal this rich, co-spatial population behind the foreground globular cluster 47 Tuc, which we targeted for 121 HST orbits. The stellar main sequence of the SMC is measured in the F606W, F814W color-magnitude diagram (CMD) down to ~30th magnitude, and is cleanly separated from the foreground star cluster population using proper motions. We simulate the SMC population by extracting stellar masses (single and unresolved binaries) from specific IMFs, and converting those masses to luminosities in our bandpasses. The corresponding photometry for these simulated stars is drawn directly from a rich cloud of 4 million artificial stars, thereby accounting for the real photometric scatter and completeness of the data. Over a continuous and well ...
COLING 2014 The 25th International Conference
, Maldives, Nepal, Pakistan and Sri Lanka. Southeast Asia, on the other hand, consists of Brunei, Burma Abdul Rauf, Fatima Jinnah Women University, Pakistan WSSANLP Invited Speaker Vincent Berment, INa, France (Director) Program Committee Sadaf Abdul Rauf, Fatima Jinnah Women University, Pakistan Nave
SPRING BOOKS 2011 Cover design by Mary Shanahan
Mateo, Jill M.
, 144145, 174, 214, 243 Archaeology 214215 Architecture 3233, 125, 127, 159, 161, 170, 175176, 208 or Africa IND NE Not for sale in India, Nepal, Bhutan, Maldive Islands, Bangladesh, and Sri Lanka IND SA
Selective, annotated bibliography on the nations of south Asia (part 1). Final report
LePoer, B.
1984-01-01T23:59:59.000Z
Monthly (previously annual, semiannual, and quarterly) bibliography series contains citations of monographs and serial articles relating to the countries of the Indian subcontinent: Afghanistan, Bangladesh, Bhutan, India, Maldives, Nepal, Pakistan, and Sri Lanka. The compilation is selective and is intended principally as a reference work for research on the foreign relations, governments, and politics of the nations concerned.
Selective, annotated bibliography on the nations of south Asia. Final report
Curtiss, E.R.
1984-03-01T23:59:59.000Z
Monthly (previously annual, semiannual, and quarterly) bibliography series contains citations of monographs and serial articles relating to the countries of the Indian subcontinent: Afghanistan, Bangladesh, Bhutan, India, Maldives, Nepal, Pakistan, and Sri Lanka. The compilation is selective and is intended principally as a reference work for research on the foreign relations, governments, and politics of the nations concerned.
Selective, annotated bibliography on the nations of south Asia (part 2). Final report
Curtiss, E.
1984-01-01T23:59:59.000Z
Monthly (previously annual, semiannual, and quarterly) bibliography series contains citations of monographs and serial articles relating to the countries of the Indian subcontinent: Afghanistan, Bangladesh, Bhutan, India, Maldives, Nepal, Pakistan, and Sri Lanka. The compilation is selective and is intended principally as a reference work for research on the foreign relations, governments, and politics of the nations concerned.
Selective, annotated bibliography on the nations of south Asia (part 3). Final report
Curtiss, E.
1984-01-01T23:59:59.000Z
Monthly (previously annual, semiannual, and quarterly) bibliography series contains citations of monographs and serial articles relating to the countries of the Indian subcontinent: Afghanistan, Bangladesh, Bhutan, India, Maldives, Nepal, Pakistan, and Sri Lanka. The compilation is selective and is intended principally as a reference work for research on the foreign relations, governments, and politics of the nations concerned.
Selective, annotated bibliography on the nations of south Asia (part 1). Final report
Curtiss, E.
1984-05-01T23:59:59.000Z
Monthly (previously annual, semiannual, and quarterly) bibliography series contains citations of monographs and serial articles relating to the countries of the Indian subcontinent: Afghanistan, Bangladesh, Bhutan, India, Maldives, Nepal, Pakistan, and Sri Lanka. The compilation is selective and is intended principally as a reference work for research on the foreign relations, governments, and politics of the nations concerned.
Selective, annotated bibliography on the nations of south Asia (part 2). Final report
Curtiss, E.
1984-05-01T23:59:59.000Z
Monthly (previously annual, semiannual, and quarterly) bibliography series contains citations of monographs and serial articles relating to the countries of the Indian subcontinent; Afghanistan, Bangladesh, Bhutan, India, Maldives, Nepal, Pakistan, and Sri Lanka. The compilation is selective and is intended principally as a reference work for research on the foreign relations, governments, and politics of the nations concerned.
Selective, annotated bibliography on the nations of south Asia (part 4). Final report
Curtiss, E.
1984-01-01T23:59:59.000Z
Monthly (previously annual, semiannual, and quarterly) bibliography series contains citations of monographs and serial articles relating to the countries of the Indian subcontinent: Afghanistan, Bangladesh, Bhutan, India, Maldives, Nepal, Pakistan, and Sri Lanka. The compilation is selective and is intended principally as a reference work for research on the foreign relations, governments, and politics of the nations concerned.
Real-time forecasting of the April 11, 2012 Sumatra tsunami Dailin Wang,1
Duputel, Zacharie
Real-time forecasting of the April 11, 2012 Sumatra tsunami Dailin Wang,1 Nathan C. Becker,1 David generated a tsunami that was recorded at sea-level stations as far as 4800 km from the epi- center, Sri Lanka, Thailand, and Maldives issued tsunami warnings for their coastlines. The United States
Quality Control and Census of SMART-R Observations from the DYNAMO/CINDY2011 Field Campaign
Fliegel, Jonathan 1988-
2012-09-24T23:59:59.000Z
variability in the year 2011 (CINDY2011) campaign on Addu Atoll, Maldives. One of SMART-R’s objectives was to provide continuous volume scans of precipitating clouds during all phases of the Madden-Julian Oscillation (MJO) for the full duration of the campaign...
Measurements of aerosol vertical profiles and optical properties during INDOEX
, and the Kaashidhoo Climate Observatory (KCO) in the Maldives. Sun photometers were used to provide aerosol optical depths (AOD) needed to calibrate the MPL. This study focuses on the height distribution and optical trajectories, radiosonde profiles of temperature and humidity, and aerosol concentration and optical
Zhou, Tao [Nanjing University of Aeronautics and Astronautics, Nanjing 210016, China; Gao, Yi [Nanjing Normal University, Nanjing 210023, China; Zhu, Jian-Xin [Los Alamos National Laboratory, Los Alamos, NM 87545, USA
2015-01-01T23:59:59.000Z
Recently it was revealed that the whole Fermi surface is fully gapped for several families of underdoped cuprates. The existence of the finite energy gap along the$d$-wave nodal lines (nodal gap) contrasts the common understanding of the$d$-wave pairing symmetry, which challenges the present theories for the high-${T}_{c}$superconductors. Here we propose that the incommensurate diagonal spin-density-wave order can account for the above experimental observation. The Fermi surface and the local density of states are also studied. Our results are in good agreement with many important experiments in high-${T}_{c}$superconductors.
J.Org. Chem. 1981,46,3721-3727 3721 cm-'; 'H NMR 6 7.20(m,1 H17),6.18(d,1H,J = 2Hz, Hl& 3.66
Reich, Hans J.
in the metabolism of aromatic compounds. In fact, many of the adverse bio- logical effects of aromatic compounds and biphenyl 2,3-0xide,~~have been prepared. 2,5,2',5'-Tetrachlorobiphenyl (1)has been extensively c Y & c l c ~ ~ l\\ \\ 8\\ / I 1 2 3 'CI / CI studied as a model for the biological effects of Arachlor mixtures,6
Nigussie, Yared
@kam.mff.cuni.cz (J. Nesetril), nigussie@etsu.edu (Y. Nigussie). 1 Supported by a Grant 1M002160808 of Czech Ministry
A1 = (b1 + m1y1)y1 = (2 + 2 1)(1) = 4 m2 A2 = (b2 + m2y2)y2 = (2.5 + 2 1)(1) = 4.5 m2
Bowen, James D.
.79)(8.4)(0.147) = 12.1 kW where w = 9.79 kN/m3 at 20C. 3.24. The Darcy-Weisbach equation can be written as hf = ¯fL D ¯V 2 2g Defining S = hf L and ¯R = D 4 and substituting into the Darcy-Weisbach equation gives S = ¯f = Q A1 = 8.4 4 = 2.10 m/s V2 = Q A2 = 8.4 4.5 = 1.87 m/s Substituting into the energy equation gives 1
Random walk computations of diffusive fields
Lindstrom, Gregory Scot
1993-01-01T23:59:59.000Z
the operation of the Vax computer system at Texas AgtM University. An invaluable debt is owed to Harding University, in particular to: Dean Priest, Don England, James Mackey and Lainbert Murray, and Linda 'I'hompson, who have shown infinite patience with me... variables . Rw header 50 53 54 57 58 60 61 62 65 66 67 68 69 71 72 74 75 77 78 79 VITA LIST OF FIGURES Figure 1 Heat equation on semi-infinite domain. . . 2 GRW vs. Fourier solution with 1000 globs and At = 0. 01. Page 12 13 3...
Non-thermal quantum channels as a thermodynamical resource
Miguel Navascués; Luis Pedro García-Pintos
2015-03-31T23:59:59.000Z
Quantum thermodynamics can be understood as a resource theory, whereby thermal states are free and the only allowed operations are unitary transformations commuting with the total Hamiltonian of the system. Previous literature on the subject has just focused on transformations between different state resources, overlooking the fact that quantum operations which do not commute with the total energy also constitute a potentially valuable resource. In this Letter, given a number of non-thermal quantum channels, we study the problem of how to integrate them in a thermal engine so as to distill a maximum amount of work. We find that, in the limit of asymptotically many uses of each channel, the distillable work is an additive function of the considered channels, computable for both finite dimensional quantum operations and bosonic channels. We apply our results to bound the amount of distillable work due to the natural non-thermal processes postulated in the Ghirardi-Rimini-Weber (GRW) collapse model. We find that, although GRW theory predicts the possibility to extract work from the vacuum at no cost, the power which a \\emph{collapse engine} could in principle generate is extremely low.
Non-thermal quantum channels as a thermodynamical resource
Miguel Navascués; Luis Pedro García-Pintos
2015-06-15T23:59:59.000Z
Quantum thermodynamics can be understood as a resource theory, whereby thermal states are free and the only allowed operations are unitary transformations commuting with the total Hamiltonian of the system. Previous literature on the subject has just focused on transformations between different state resources, overlooking the fact that quantum operations which do not commute with the total energy also constitute a potentially valuable resource. In this Letter, given a number of non-thermal quantum channels, we study the problem of how to integrate them in a thermal engine so as to distill a maximum amount of work. We find that, in the limit of asymptotically many uses of each channel, the distillable work is an additive function of the considered channels, computable for both finite dimensional quantum operations and bosonic channels. We apply our results to bound the amount of distillable work due to the natural non-thermal processes postulated in the Ghirardi-Rimini-Weber (GRW) collapse model. We find that, although GRW theory predicts the possibility to extract work from the vacuum at no cost, the power which a \\emph{collapse engine} could in principle generate is extremely low.
Selective, annotated bibliography on the nations of south Asia. Final report
Makeig, D.; Ross, R.
1981-12-01T23:59:59.000Z
This bibliography contains citations of monographs and serial articles relating to countries of the Indian Subcontinent: Afghanistan, Bangladesh, Bhutan, India, Maldives, Nepal, Pakistan, and Sri Lanka. The compilation is selective and is intended principally as a reference work for research in the foreign relations, governments, and politics of the nations concerned. The bibliography is divided into country sections preceded initially by a general interest and reference section. This first issue covers material published or copyrighted in 1981. Wherever the hard copy of the material being cited could be obtained, a brief abstract, review or summary is presented with the citation. Where existence of a work was reported or verified (e.g., through publishers` notices, review articles, etc.) but a hard copy could not be obtained, the article/book is merely cited without further description. All listings are by author, last name first, except where the author is unknown. In such cases, the work is listed by title.
Essays on International Finance and Trade
Zeng, Li
2009-01-01T23:59:59.000Z
1973M 1-20 09M7 Real oil prices TOT 1973M 1-20 09M7 1973M 1-1973M 1-20 09M7 REER Real oil prices 1973M 1-20 09M7 1973M1975M 1-20 09M7 Real oil prices TOT 1975M 1-20 09M7 1975M 1-
ON THE m-ENUMERATION OF MAXIMUM AND LEFT-TO-RIGHT MAXIMA IN GEOMETRICALLY DISTRIBUTED WORDS
Wagner, Stephan
by a prime. Then F (mz, 1) = m F(z, 1) m-1 F (z, 1) = mez(m-1) F (z, 1) and F (mz, 1) = mez(m-1) F (z, 1) + m
Travis Norsen; Damiano Marian; Xavier Oriols
2014-10-14T23:59:59.000Z
The ontology of Bohmian mechanics includes both the universal wave function (living in 3N-dimensional configuration space) and particles (living in ordinary 3-dimensional physical space). Proposals for understanding the physical significance of the wave function in this theory have included the idea of regarding it as a physically-real field in its 3N-dimensional space, as well as the idea of regarding it as a law of nature. Here we introduce and explore a third possibility in which the configuration space wave function is simply eliminated -- replaced by a set of single-particle pilot-wave fields living in ordinary physical space. Such a re-formulation of the Bohmian pilot-wave theory can exactly reproduce the statistical predictions of ordinary quantum theory. But this comes at the rather high ontological price of introducing an infinite network of interacting potential fields (living in 3-dimensional space) which influence the particles' motion through the pilot-wave fields. We thus introduce an alternative approach which aims at achieving empirical adequacy (like that enjoyed by GRW type theories) with a more modest ontological complexity, and provide some preliminary evidence for optimism regarding the (once popular but prematurely-abandoned) program of trying to replace the (philosophically puzzling) configuration space wave function with a (totally unproblematic) set of fields in ordinary physical space.
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Shawn M. (1) Rosa, Guilherme J.M. (1) Spalding, Edgar P (1) Save Results Excel (limit 2000) CSV (limit 5000) XML (limit 5000) Have feedback or suggestions for a way to improve...
ASE 2004 Sep 22, 2004 A Differencing Algorithm for
Orso, Alessandro "Alex"
CFG Entry call a.m1() catch Exception:E1, Exception:E1:E2 catch Exception... exit ... A void m1() BG: Extend CFG Entry call a.m1() catch Exception:E1, Exception:E1:E2 catch Exception... exit ... EX EX A voidG: Simplify the extended CFG Entry call a.m1() try catch Exception:E1, Exception:E1:E2 catch Exception... exit
Rinehart, Amanda J.
2009-05-15T23:59:59.000Z
. ................................................................................................. 31 3 Relationship of Yukon discharge to DOC (mg L -1 ), spectral slope (?m -1 ), and SUVA (L (mg OC) -1 m -1 )..................................................... 37 4 Fluorescence EEM?s measured in Yukon samples from low flow... .................................................................................................. 46 8 Relationship of Mackenzie discharge to DOC (mg L -1 ), spectral slope (?m -1 ), and SUVA (L (mg OC) -1 m -1 )...................................................... 47 x FIGURE Page 9 Fluorescence EEM?s measured...
Directions to King's Meadow Campus FROM THE SOUTH
Aickelin, Uwe
junction 26 off the M1 following signs marked A610 Nottingham. After passing the petrol station on your
Promoting system-level learning from project-level lessons
Jong, Amos A. de, E-mail: amosdejong@gmail.com [Innovation Management, Utrecht (Netherlands); Runhaar, Hens A.C., E-mail: h.a.c.runhaar@uu.nl [Section of Environmental Governance, Utrecht University, Utrecht (Netherlands); Runhaar, Piety R., E-mail: piety.runhaar@wur.nl [Organisational Psychology and Human Resource Development, University of Twente, Enschede (Netherlands); Kolhoff, Arend J., E-mail: Akolhoff@eia.nl [The Netherlands Commission for Environmental Assessment, Utrecht (Netherlands); Driessen, Peter P.J., E-mail: p.driessen@geo.uu.nl [Department of Innovation and Environment Sciences, Utrecht University, Utrecht (Netherlands)
2012-02-15T23:59:59.000Z
A growing number of low and middle income nations (LMCs) have adopted some sort of system for environmental impact assessment (EIA). However, generally many of these EIA systems are characterised by a low performance in terms of timely information dissemination, monitoring and enforcement after licencing. Donor actors (such as the World Bank) have attempted to contribute to a higher performance of EIA systems in LMCs by intervening at two levels: the project level (e.g. by providing scoping advice or EIS quality review) and the system level (e.g. by advising on EIA legislation or by capacity building). The aims of these interventions are environmental protection in concrete cases and enforcing the institutionalisation of environmental protection, respectively. Learning by actors involved is an important condition for realising these aims. A relatively underexplored form of learning concerns learning at EIA system-level via project level donor interventions. This 'indirect' learning potentially results in system changes that better fit the specific context(s) and hence contribute to higher performances. Our exploratory research in Ghana and the Maldives shows that thus far, 'indirect' learning only occurs incidentally and that donors play a modest role in promoting it. Barriers to indirect learning are related to the institutional context rather than to individual characteristics. Moreover, 'indirect' learning seems to flourish best in large projects where donors achieved a position of influence that they can use to evoke reflection upon system malfunctions. In order to enhance learning at all levels donors should thereby present the outcomes of the intervention elaborately (i.e. discuss the outcomes with a large audience), include practical suggestions about post-EIS activities such as monitoring procedures and enforcement options and stimulate the use of their advisory reports to generate organisational memory and ensure a better information dissemination.
Rajen, Gauray
1999-06-01T23:59:59.000Z
The cessation of hostilities between India and Pakistan is an immediate need and of global concern, as these countries have tested nuclear devices, and have the capability to deploy nuclear weapons and long-range ballistic missiles. Cooperative monitoring projects among neighboring countries in South Asia could build regional confidence, and, through gradual improvements in relations, reduce the threat of war and the proliferation of weapons of mass destruction. This paper discusses monitoring the trans-border movement of flow and sediment in the Indian and Pakistani coastal areas. Through such a project, India and Pakistan could initiate greater cooperation, and engender movement towards the resolution of the Sir Creek territorial dispute in their coastal region. The Joint Working Groups dialogue being conducted by India and Pakistan provides a mechanism for promoting such a project. The proposed project also falls within a regional framework of cooperation agreed to by several South Asian countries. This framework has been codified in the South Asian Seas Action Plan, developed by Bangladesh, India, Maldives, Pakistan and Sri Lanka. This framework provides a useful starting point for Indian and Pakistani cooperative monitoring in their trans-border coastal area. The project discussed in this paper involves computer modeling, the placement of in situ sensors for remote data acquisition, and the development of joint reports. Preliminary computer modeling studies are presented in the paper. These results illustrate the cross-flow connections between Indian and Pakistani coastal regions and strengthen the argument for cooperation. Technologies and actions similar to those suggested for the coastal project are likely to be applied in future arms control and treaty verification agreements. The project, therefore, serves as a demonstration of cooperative monitoring technologies. The project will also increase people-to-people contacts among Indian and Pakistani policy makers and scientists. In the perceptions of the general public, the project will crystallize the idea that the two countries share ecosystems and natural resources, and have a vested interest in increased collaboration.
Paragios, Nikos
of Environment, Energy & Transport · M1EconomicsofEnvironment, andEnergy · M2EconomicsofEnergy Coordinator hichem.dammak@ecp.fr Nuclear Energy · M1NuclearEnergy · M2Operation · M2Decommissioning&Waste Management.modaressi@ecp.fr Energy · M1Energy:Materials, Transfers,ElectricalSystems · M2ThermalScience · M2Processes&Environment · M
Empirical modeling and simulation of edgewater cusping and coning
Ayeni, Kolawole Babajide
2008-10-10T23:59:59.000Z
considered 45, 51. Fig. 3.1 represents a stable displacement when the gravity number is greater than the end point mobility ratio i.e. G>M-1, the end point Fig. 3.1-Stable: G>M-1; M>1, #2; < #3;. #1; dx Oil Water y x #2; -dy 22 mobility ratio...
Learning Unbiased Features Yujia Li, Kevin Swersky, Richard Zemel
Toronto, University of
that are invariant to certain task irrelevant biases in the data. Multi-Distribution MMD 1 N NX n=1 (Xn) 1 M MX m=1 (Ym) 2 = 1 N2 NX n=1 NX n0=1 (Xn)> (Xn0 ) + 1 M2 MX m=1 MX m0=1 (Ym)> (Ym0 ) 2 NM NX n=1 MX m=1 (Xn)> (Ym) = 1 N2 NX n=1 NX n0=1 k(Xn, Xn0 ) + 1 M2 MX m=1 MX m0=1 k(Ym, Ym0 ) 2 MN NX n=1 NX m=1 k(Xn, Ym
On the rate of approximation in finite-alphabet longest increasing subsequence problems
Houdre, Christian; Talata, Zsolt
2012-09-05T23:59:59.000Z
=1 ?rB˜r (jr n ) ,(4.4) APPROXIMATION RATE IN LIS PROBLEMS 11 we have for any ? > 0 P(|Ln/ ?pmax ? Jk|> 2?) (4.5) ? P(|Ln ? H˜n,k|> ? ?pmax) + P(|H˜n,k ? ?pmaxJk|> ? ?pmax). Using Lemmas 4.4 and 4.5 below, (4.5) can be upper bounded by 1 + (m? 1)2?2...max 2 ? ?pmax + exp ( ??? ?npmax 16(m? 1) )m?1? r=1 ( 1 + ?r ?n 1? |µr| ) (4.6) + 4(m? 1)n exp ( ??2npmax 8?2max(m? 1)2 ) . Now, from Proposition 3.1, |P(Ln/ ?pmax ? x)? P(Jk ? x)| ? P(|Ln/ ?pmax ? Jk| ? 2?) + P(x? 2?? Jk ? x+2?) ? 1 + (m? 1) 2?2max 2...
Kuligowski, Bob
approach a 30 year time span is required to produce climate norms. Major requirements: 1km - AVHRR, 250m Min accuracy Surface Albedo 250m 1day 5% 10% Surface radiation budget (SW and LW) 25km 3h-1day 5Wm-2 10Wm-2 Land cover (incl. vegetation type) 10m-1km 1yr 5% 10% Leaf Area Index (LAI) 250m 1day 5% 10
Figueira, Santiago
Â´atica de sistemas MetodologÂ´ia para su implementaciÂ´on computacional Trabajo PrÂ´actico 3 Enunciado: En este trabajo vamos a simular el movimiento bidimensional en el plano XY de un cuerpo mÂ´ovil de masa m1 que se forma vectorial - F = G m2m1 r3 -r siendo G una constante y r la distancia entre el cuerpo de masa m1 y
COMPARISON OF QUENCHED AND ANNEALED INVARIANCE PRINCIPLES FOR RANDOM CONDUCTANCE MODEL
Barlow, Martin T.
of percolation see [BeB, MP, SS], and for the Random Conductance Model with Âµe i.i.d see [BP, M1, BD, ABDH
Winkelmann, F.C.
2010-01-01T23:59:59.000Z
ECONOMICS LITCHG = = ELECTRICTY = M2 MONTH—CHGS ENERGY—CHGElectric rate (not lights) ELECTRICTY M1 $ Default meter E N
A variant of Wiener's attack on RSA Andrej Dujella
International Association for Cryptologic Research (IACR)
the form p q = rpm+1 ± spm rqm+1 ± sqm (3) for some m -1 and nonnegative integers r and s such that rs
Succeeding in politics : dynasties in democracies
Smith, Daniel Markham; Smith, Daniel Markham
2012-01-01T23:59:59.000Z
advantage (normalized using the Droop quota to account forof the vote divided by the Droop quota (1/(M+1)), which iscomparison, success rates and Droop margins for incumbents
Oberwolfach Mathematisches Forschungsinstitut Oberwolfach gGmbH
if there is a contac- tomorphism (M1, 1) (M2, 2) carrying L1 to L2. Here the contact structures are understood
Khalifa, Hesham Ezzat
2009-01-01T23:59:59.000Z
fracture toughness because preferential nucleation of the ductilefracture toughness values of less than 2 MPa*m 1/2 . Outlook for ductile
Si?-implanted Si-wire waveguide photodetectors for the mid...
Office of Scientific and Technical Information (OSTI)
Driscoll, Jeffrey B. 1 ; Stein, Aaron 2 ; Bakhru, Hassaram 3 ; Bergman, Keren 1 ; Green, William M. J. 4 ; Osgood, Jr., Richard M. 1 + Show Author Affiliations Columbia...
Shifting Power in Sacramento: The Effects of Term Limits on Legislative Staff
Robinson, Katerina L
2011-01-01T23:59:59.000Z
and Implications. Sacramento: California Senate Office ofRobinson: Shifting Power in Sacramento Price, Charles M.1 Shifting Power in Sacramento: The Effects of Term Limits
Poster Presentations -188 Poster III-43
O'Leary, Dianne P.
, Daniel M. *1 , Conroy, John M. 2 , O'Leary, Timothy J. 3 , O'Leary, Dianne P. 1 1 University of Maryland
Schlegel, Jacob Peter
2012-01-01T23:59:59.000Z
see Section 2.1.4), and periscope before arriving at theeffective FL=10.16 cm Periscope assembly with M1 C-axis cut
Gomez, Gustavo Adolfo
2013-01-01T23:59:59.000Z
Tables SM1 and SM2). Bowtie (version 0.12.8) (Langmead etraw reads before mapping. Bowtie( --sam --best –n 2 –m 1) (
: Problem Set 1 Useful Information
Ronis, David M.
Avogadro´s Number = 6. 022169 × 1023 1atm = 1. 01325 × 105 J/m3 Geometric Series: M i=0 xi = (1 - xM+1
Chemistry 365: Quiz I Useful Information
Ronis, David M.
Avogadro´s Number = 6. 022169 × 1023 1atm = 1. 01325 × 105 J/m3 Geometric Series: M i=0 xi = (1 - xM+1
Dynamic analysis in productivity, oil shock, and recession
Katayama, Munechika
2008-01-01T23:59:59.000Z
SALES HOUSE CSA EMP VENDOR CSAA HOUSE EXP CSAAA VENDORM0 HOURS EMP CEMP M0 HOURS HOUSE DJ30 M0 VENDOR CEMP CEMP M1
Building Noetherian and non-Noetherian integral domains using ...
... the National Science Foundation and the National Security Agency for sup- .... the definition and information on excellent rings see [M1, Chapter 13], [M2, ...
Mina de Malfois and the Charitable Impulse
2006-08-16T23:59:59.000Z
for the function of the neurotransmitter-binding ECD in nAChRs. The features of M1 that are essential for ECD function, however, are not fully known. M1 sequences from ionotropic serotonin (5HT3A) and from ?4, ?2, and ?7 nAChR subunits are similar but behave...
Deriving Atmospheric Density Estimates Using Satellite Precision Orbit Ephemerides
Hiatt, Andrew Timothy
2009-01-01T23:59:59.000Z
due to atmospheric drag m/s2 ap geomagnetic 3-hourly planetary equivalent amplitude index gamma, Telsa, or kg s m-1 A satellite cross-sectional area m2 Ap geomagnetic daily planetary amplitude index gamma, Telsa, or kg s m-1 B B? estimated...
Can we do without the Majorana term in the effective nuclear interaction?
Barrett, B.R.; Diallo, A.F. [Univ. of Arizona, Tucson, AZ (United States); Davis, E.D. [Universiteit van Stellenbosch, Stellenbosch (South Africa)]|[Univ. of Washington, Seattle, WA (United States)
1994-08-01T23:59:59.000Z
Probably not, but the authors present phenomenological evidence that the strength of this term necessary to reproduce collective M1-transition strength data could be significantly smaller than is conventionally assumed and therefore more in line with naive microscopic considerations. They also find that g-boson effects are important to the reproduction of the summed M1 strength.
Nielsen, Steven O.
Name: Chem 3322 test #3 formula sheet I want complete, detailed answers to the questions. Show all is the reduced mass. reduced mass formula: µ = m1m2/(m1 + m2) energy levels of the harmonic oscillator: En = (n
Dallos, P., Zheng, J., and Cheatham, M.A. (2006). J. Physiol. 576, 3742.
Movshon, Joseph Anthony
2006-01-01T23:59:59.000Z
.S., and Holt, J.R. (2003). Trends Neuro- sci. 26, 115117. Gold, T. (1948). Proc. R. Soc. Lond. B. Biol. Sci motor cortex (M1) during isometric movements in different postures. By modeling the output of M1 neurons of muscle actions. Controlling complex movements is a profoundly challenging problem for the nervous system
Princeton Plasma Physics Laboratory NSTX Experimental Proposal
Princeton Plasma Physics Laboratory
to observe the heating/CD effectiveness in sustaining the plasma current. Starting with 250 kA at tflattop = 40 ms. A k|| = 14 m-1 heating phasing will be used first, and then k|| = 10 m-1 co-CD, heating, and cntr-CD. Advantage will be taken of the RF voltage-power control to reduce the injected power
Homo-and Cross-[2+2]-Cycloaddition of 1,1-Diphenylsilene and 1,1-Diphenylgermene. Absolute
Leigh, William J.
, McMaster University, 1280 Main Street West, Hamilton, Ontario, L8S 4M1 Canada Received June 10, 1999 always rela- tively facile and occurs at rates in excess of ca. 107 M-1 s-1 in derivatives bearing simple.1,2 The head-to-head regiochemistry is common with derivatives bearing sterically bulky substituents
EINSTEIN METRICS ON SPHERES CHARLES P. BOYER, KRZYSZTOF GALICKI AND J ANOS KOLLAR
EINSTEIN METRICS ON SPHERES CHARLES P. BOYER, KRZYSZTOF GALICKI AND J Â´ANOS KOLLÂ´AR 1. Introduction and Einstein, that is the Ricci curvature is a constant multiple of the metric. The spheres S4m+3 , m > 1 are known to have another Sp(m + 1)-homogeneous Einstein metric discovered by Jensen [Jen73]. In addi- tion
EINSTEIN METRICS ON SPHERES CHARLES P. BOYER, KRZYSZTOF GALICKI AND J
EINSTEIN METRICS ON SPHERES CHARLES P. BOYER, KRZYSZTOF GALICKI AND J â?? ANOS KOLL â?? AR 1 are homogeneous and Einstein, that is the Ricci curvature is a constant multiple of the metric. The spheres S 4m+3 , m > 1 are known to have another Sp(m + 1)Âhomogeneous Einstein metric discovered by Jensen [Jen73
Heidelberg University Institute of Environmental Physics
Roth, Kurt
geothermal gradient (red line) is 0.014 K m-1 . The deviation from the mean temperature (green sym- bols active zones. This flux leads to an average geothermal gradient of 0.025. . . 0.03 K m-1 . It is higher, the fluctuations become negligible and the tem- perature profile is dominated by the geothermal heat flux which
MT3522 Knot Theory Solutions 4 1. (i) The closure of 2
Walker, Grant
molecule. O 1 :unknot O 2 :split unlink or opposite matched M 1 :pos trefoil M 2 :pos Hopf link or 3 #12; or opposite O 1 O 2 :pos trefoil :pos Hopf link :unknot or matched M 2 :split unlink M 1 opposite 2 or O 1 O
JOURNAL DE PHYSIQUE 1V ColloqueC2, suppl6mentau Journal de Physique 111,Volume 5, f6vrier 1995
Paris-Sud XI, UniversitÃ© de
Mexico * Centro Atdmico de Bariloche, 8400 S.C. de Bariloche, Argentina **Labovatoire GEMPPM-INSA de Lyon stability of the beta Cu-AI-Be phase with an eutectoid composition was studied by thermoelectric power; another etching solution was 95 m1 of ethanol + 2gr of FeCl, + 2 m1 of HCl. 3. RESULTS. 3.1 Thermoelectric
Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)
as FEv1.2u except the 1 st Fixed Mask is M1-20 instead of M1-30 11 Elliptical multipole wiggler (16 cm) K y,max 14.3, N18 3 2.2. Source Parameters For undulator power...
The FASEB Journal Research Communication Tracing the evolutionary history of the pandemic group
Nizet, Victor
, USA; ¶ Department of Microbiology and Immunology, Faculty of Pharmacy, Cairo University, Cairo, Egypt A Streptococcus (GAS) M1T1 clone, first detected in the mid-1980s in the United States, has since dissem- inated Organization strain collection of serotype M1 GAS and reconstructed its phylogeny based on the analysis of core
About the extensional collapse of Rel Thomas Ehrhard
Ehrhard, Thomas - Laboratoire Preuves, Programmes et SystÃ¨mes, UniversitÃ© Paris 7
of coherence in the qualitative setting as well and to replace finite cliques by finite sets) pE = {(m1 + Â· Â· Â· + mn, [m1, . . . , mn]) | n N and i mi Mfin(E)} (digging) wE = {([], )} Rel
One-Parameter Continuous Fields of Kirchberg Algebras. II
2011-04-13T23:59:59.000Z
Y = [t0,t1] ? [t2,t3] ?···? [t2m,t2m+1], and. Z = [t1,t2] ? [t3,t4] ?···? [t2m?1,t2m]; thus, Y ? Z = {t1,t2,...,t2m}. For the sake of brevity let us refer to the above cover.
Review article Induced seismicity and hydraulic fracturing for the recovery of
Foulger, G. R.
Review article Induced seismicity and hydraulic fracturing for the recovery of hydrocarbons Richard Davies a,*, Gillian Foulger a , Annette Bindleya,1 , Peter Styles b a Durham Energy Institute, Department mining (M 1.0e5.2); (h) geothermal operations (M 1.0e4.6) and (i) hydraulic fracturing for recovery
Magnetic dipole transition rates from measured lifetimes of levels of Be-like and B-like argon ions
Moehs, D. P.; Church, David A.
1998-01-01T23:59:59.000Z
calculations of the 2s2p P-3(1)-P-3(2) M1 transition rate of Ar XV, but are in reasonable agreement with calculations for the 2p P-2(1/2)-P-2(3/2) M1 rate of Ar XIV. [S1050-2947(98)07108-X]...
Fan, Xiaohua
2009-05-15T23:59:59.000Z
due to their potential closed loop stability problems. Different frequency compensation schemes have been proposed in the literatures. ________________ *?[2007] IEEE. Reprinted, with permission, from ?Single Miller Capacitor Frequency...L2m oL2o1o mL2m1m mL2m 2m1m2 mL 2m oL2o1o mL2m1m v gg CCs gg )g(gCs1 ggg ggCs1 gg CCs g Cs1 ggg ggg (s)A (2.1a) 2 CC gg4 C g C g Z 2m1m mL2m 2 ml 2 2m 1m 2m 2,1 +?? = (2.1b...
An iterative technique for the factorization of polynomials
Gray, Jerry Edwin
1964-01-01T23:59:59.000Z
= Z pb, 0&) &m-1 i n-)-1' Then, (2. 4) f(z) = g(z) h (z) m-1 + i=o i rz For the procf construct the right l. and side of (2. 4), m-1 g(z) h(z) + i=o rz = S pz p bz m-1 + k=o k rkz E k=o E i+j =k i&m ]& n-m n-k pb z m-1 + E r z...-1 + g, '=o Thus we may write for the right hand side of (2. 4) (2. 5) n-m min [k, m] 7 k=o i=o 0& k-i~ n-m n-k Pik i' n + km-m+1 min [k, n-m] E ]=0 0&k-] & m n-k p b z k-] E k =n-m+1 n-k I Z n-k n-m for the part involving E...
COMPUTATION OF COVARIANCE MATRICES FOR CONSTRAINED PARAMETER ESTIMATION PROBLEMS
Stanford University
f1(x) 2 2 s.t. f2(x) = 0, (1.1) where f1(x) is a vector of weighted residuals for a model of the form i = M(xtrue, ti) + i, i = 1, . . . , m1. (1.2) Thus, f1(x) = (1 - M(x, t1))/ ... (m1 - M(x, tm1 ))/ , f1(x) 2 2 := m1 i=1 (i - M(x, ti))2 2 . (1.3) The model M(x, t) R that describes the parameter
The Fukaya category, exotic forms and exotic autoequivalences
Harris, Richard
2012-04-10T23:59:59.000Z
. . . . . . . . . . . . . . . . . . . . . . . . . . . . . 14 1.5.3 Fragility of symplectomorphisms . . . . . . . . . . . . . . . 14 I Projective twists in A?-catgeories 19 2 A?-categories 21 2.1 Categories . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 21 2.2 Functors... consider the moduli 4 1.1. Fukaya categories space of discs with one boundary puncture M1(L; ?), there is an evaluation map ev : M¯1(L; ?)? L and we can define µ0(L) = ? ??pi2(M,L) q?(?)ev?([M¯1(L; ?)]). Now, when we examine whether µ1 is a differential, we...
Carcinogen induced inflammation and pancreatic cancer INTRODUCT ION
Korhonen, Anna
Da Figure 5. Calcineurin was activated by Trichloropropane(TCP), Chlorendic acid (CA) and Benzyl acetate (BA acetate 500 M + KN62 100 nM ATP 200 M 1.0 2.0 3.0 4.0 5.0 0.0 Benzyl acetate 200 M ATP 200 M 1.0 2.0 3.0 4.0 ATP 500 M Trichloropropane 250 M 1.0 2.0 3.0 4.0 5.0 0.0 Chlorendic acid 100 M ATP 200 M 0.0 1.0 2.0 3
Warland, Arild
1986-01-01T23:59:59.000Z
15 22 30 31 32 33 34 12 13 14 Simulated and Calculated Non-isothermal Skin Factors for Case 1 (M 1. 9) Simulated Falloff Tests for Case 1 (M- 1. 9) Simulated Falloff Tests with Formation Damage for Case 1 (M= 1. 9... From the fractional flow curve, Fig. 6, S(r3) 0. 50 f (0. 50) 0. 93 f'(0. 50) ' . ' 2. 33 0. 9 - 0. 0 I ~Zg. 2 (2. 33)'60 + (0 25) ) 111. 77 tt 2. Calculate S2 and T2 a) Volumetric average of S2. .10 r2 2 I2 2 S - { S(r ) - S(r ) ~ ( ? J - (f...
A Generalization of Euler's Theorem on Congruencies
Florentin Smarandache
2006-10-20T23:59:59.000Z
We present a theorem which generalizes the classical Euler's theorem on congruencies: if $(a,m)=1$ then $a^ \\phi(m) \\equiv 1 (mod m)$ for the case when $a$ and $m$ are not relatively primes.
Phylogeny and adaptive evolution of the brain-development gene microcephalin (MCPH1) in cetaceans
McGowen, Michael R; Montgomery, Stephen H; Clark, Clay; Gatesy, John
2011-01-01T23:59:59.000Z
positive selection (p > 0.95, BEB) M1a v. M2a: df = 2, -A Bayes Empirical Bayes (BEB) analysis was implemented tohigh probabilities (?0.95 in BEB analysis) of belonging to
Characterizing, Verifying and Improving Software Resilience with Exception Contracts and Test Suites
Boyer, Edmond
At the Fukushima nuclear power plant, the anticipated maximum height of waves in a tsunami was 5.6m[1]. How- ever, and those that happen in production mode yet never anticipated, as Fukushima's tsunami. In this presentation
Retooling Michigan: Tanks to Turbines
Broader source: Energy.gov [DOE]
A company that has manufactured geared systems for the M1 Abrams tank for more than 20 years is now part of the forces working toward energy security and independence.
Media Advisory: Poster Session Highlights Projects, Research...
Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)
Media Advisory: Poster Session Highlights Projects, Research Carried Out by Summer Interns at Jefferson Lab Date: Friday, July 31, 2015 Time: 11:45 a.m. - 1:15 p.m. Place: The...
Cryptographie et algorithmique pour la Clement PERNET
Pernet, Clément
;Modes de chiffrement CFB: Cipher Feedback m1 IV=c0 c 1 K E K E K E c 2 c r mr m2 ... ... ci = mi EK (ci
Remote monitoring of a model levee constructed on soft peaty organic soil
Reinert, Edward T; Lemke, John; Stewart, Jonathan P; Brandenberg, Scott J
2013-01-01T23:59:59.000Z
of the model levee. MEMS sensor readings were recorded at 10is not measured by the MEMS sensors, but could conceivablySystems (MEMS) accelerometer sensors spaced 0.30m (1 ft)
Discretization and Algorithms for Strong Coupling in Computational Aeroelasticity
8 4.1 Flow discretization . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 8 4.2 Structural discretization . . . . . . . . . . . . . . . . . . . . . . . . . . . . 9 4.3 Mimicing the energy.4 A bifurcation at M1 = 0:95 . . . . . . . . . . . . . . . . . . . . . . . . . . 22 6.5 Stability chart
Analysis of microelectronic power distribution networks and exploration of 3D ICs
Hu, Xiang
2012-01-01T23:59:59.000Z
II.5: Figure III.1: Step response of a second-order all-passvoltage noise: Theorem of Step Response Derivation. Assumingby the super- position of step responses. Let V M 1 , V M
Art, Spirituality, and the Ethic of Care: Alternative Masculinities in Chinese American Literature
Cheung, KK
2015-01-01T23:59:59.000Z
AOo::3\\v. 535$ 243 95? W33 web. 3% DE? rmsaos msmuo Fun».man». Qmwva on Sam; RE. Oba om WEB W. m ..m1mr.na:5m_< 5%
Goldreich, Oded
by a n-by-m probability matrix Pn;m = fpi;v : i 2 f1;:::;ng;v 2 f0;:::;m 1gg, which is a matrix of non
Goldreich, Oded
by a n-by-m probability matrix Pn;m = fpi;v : i 2 f1;:::;ng;v 2 f0;:::;m 1gg, which is a matrix of non
, 2004, 30, . 21 12 E-mail: http://www.pnpi.spb.ru/
Titov, Anatoly
, 2004, 30, . 21 12 02 Â© .. , .. , .. , .. , .. .- . .. E-mail: http://www.pnpi.spb.ru/ 22 2004 . P- . , P- - . , P- , , 1% 1-. (400 Ã· 4000) Gs , P- . , M1-1 . 1 . . , 2004, 30, . 21 #12
Master Program `Software Engineering for Embedded Systems'
Berns, Karsten
Modules Master Program `Software Engineering for Embedded Systems' November 2014 #12;1 Table............................................................................................................................ 4 B-M.1 SOFTWARE ENGINEERING INTRODUCTION ............................................................................................................. 15 E-M.3 - SOFTWARE PRODUCT LINE ENGINEERING
RIS-M-2235 LIMIT CYCLE BEHAVIOUR OF THE BUMP-ON-TAIL AND
.E.M. Janssenx Department of Electrical Engineering, Eindhoven University of Technology, Eindhoven and final steady state, e.g. a) the m - 1 kink modes in a sharp boundary plasma pinch , and b) the g * B
Cedex 05 4 University of Virginia, Charlottesville, Virginia Abstract We study an adaptive variantâ??epeau and Robert [BCR87] is deceptively simple: there is a sender S with messages M 1 , . . . , MN and a receiver R
: ... ... .... .... «» , 28 2007 : « » #12; · ·· #12; 2 #12; (GAS HYDRATES) #12;Y · µ 2 µ () µ · µ µ · µ µ µ ·µ: - - µ CO2 - - #12; - 3S·2M·1L·34H3S
Transcriptional Profiling of Polarized Macrophages using RNA-Sequencing
Kanameni, Srikanth
2015-04-17T23:59:59.000Z
-inflammatory M1 state in adipose tissues of obese individuals. Modulatory networks governing ATMs polarized activation have been investigated but the full picture remains vague. To understand the genome wide signaling networks in controlling ATM polarization, we...
CX-012096: Categorical Exclusion Determination
Broader source: Energy.gov [DOE]
M1 a and b Habitat Enhancement Project, Site 300 CX(s) Applied: B1.20 Date: 06/19/2013 Location(s): California Offices(s): Lawrence Livermore Site Office
R-groups and Elliptic Representations for SL David Goldberg To ...
1910-30-31T23:59:59.000Z
We use this explicit description of the elements of R, and a theorem of Arthur [1], ..... Theorem 3.4. Suppose m1 = m2 = ... = mr. Let ? ? E2(M), and choose ?? ?.
Yaghoobian, Neda; Kleissl, Jan
2012-01-01T23:59:59.000Z
and Applications of Radiation Heat Transfer, HTD?Vol. 72, heat transfer due to convection, longwave and shortwave radiationheat transfer coefficient effective thermal conductivity (W m -1 K -1 ) L longwave radiation (
Raw Cotton Requirements of Textile Mills: Implications for Southwestern Cotton.
Graves, James W. (James Wilson)
1967-01-01T23:59:59.000Z
,Ar,NTO,WT,ST WTO ETO WT Ar, WT WT,Ga Ar,SE ETO ETO WT WT CS,R,CN CN CN CN W&F CS CS CS P CS. CN CB~ETO WT CS-CN Any WTO E,WT SLM-s SGO EM+ SGO+ SLM+ M-s SLM M-1s M-IS BG SLM-IS M-1s M-1s M-1s SLM SLM-IS SLM-1s SLM+ SLM...,300 32 Knitting yarn SLM+ 9,000 3 0 Knitting and weaving yarn LM M SLM 1,500 34 33 : I 1 Tufting yarn SLM SMls MIS 90,000 29 30 Weaving yam LM M LM+ 6,000 29 31 30 6.0 ' Rope and cordage M SMs 5,250 3 0 >.? 1 Denim and ticking LM+ 83,200 3 2 8...
THE 2D BOUSSINESQ-NAVIER-STOKES EQUATIONS WITH LOGARITHMICALLY SUPERCRITICAL DISSIPATION
Wu, Jiahong
such that r m(r) is non-increasing. This type of dissipation operator was introduced by Dabkowski, Kiselev. REGMI, L. TAO AND J. WU for P(||) = m( 1 || ) when P() satisfies the following conditions: (1) P
AO18: Satellite tracking of volcanic eruption plumes using ash and Candidate number: 782932
Oxford, University of
reactions [7]: SO2 + OH + M HSO3 + M (1) HSO3 + O2 HO2 + SO3 (2) SO3 + H2O + M H2SO4 + M (3) Page 1 #12
Mechanical Properties of Nanocrystal Supercrystals
Tam, Enrico
2010-01-01T23:59:59.000Z
A. ; Weller, H. , Colloidal Crystals of Monodisperse FePtThe nucleation of 3D colloidal crystals occurred mostly at~ 39±3 KPa/m 1/2 gives colloidal crystal clay-like behavior.
BoseEinstein Condensation in the Large Deviations Regime with Applications to Information
Merhav, Neri
BoseEinstein Condensation in the Large Deviations Regime with Applications to Information System(U) = lim M " - 1 M log Pr ( X i ni MU )# may exhibit phase transitions BoseEinstein condensation (BEC
Atomic-Scale Observations Aid Mesoscale Catalyst Design | ornl...
Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)
Materials Characterization Atomic-Scale Observations Aid Mesoscale Catalyst Design April 08, 2015 Fig.1. Z-contrast STEM image shows the Mo-V-Te-Ta oxide catalyst. (a) "M1-like"...
Jul Aug Sep Nov Dec Apr May Jun Begin Residency Training as M.D.
Cui, Yan
Jul Aug Sep Nov Dec Apr May Jun First Year Second Year Third Year Fourth Year Begin Residency Longitudinal Scholars Program - Longitudinal(M1-M4 year, beginning with the Class of 2016) Senior Clerkship JI
Vapor deposited samarium zirconate thermal barrier coatings Hengbei Zhao a,
Wadley, Haydn
technology for the gas turbine engines used for propulsion and power generation [1]. Through their ability conductivity (~2.1 W m- 1 K- 1 at 1000 T1200 °C [9]), its thermochemical compatibility with the underlying TGO
Cui, Yan
.andit Mco.n.tl J.$000- 0tvld co.m111 MOrftl M1tW1C. Ml,lffff ----_,,... .....--·-"'*-"L m.cl"..... Dr
A SHARP STABILITY ESTIMATE IN TENSOR TOMOGRAPHY 1 ...
2008-03-26T23:59:59.000Z
Mar 26, 2008 ... ?p(N)ijkl(x, ?)=2?. ?. SxM1 ?i?j?k?l?(? · ?)d?x(?), where ? · ? = ?i?i. This formula generalizes in an obvious way to tensors of any order. It.
Software for Numerical Methods for Partial Differential Equations
(multigrid-data) smoother-maker smoother-name r m1 m2 p) .... a; abbr; acronym; address; applet; area; b; base; basefont; bdo; big; blockquote; body; br; button ...
Sandia Energy - EC Publications
Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)
SAND2015-0545 M (1)Tara Camacho-Lopez2015-04-06T22:15:34+00:00 Order by: Title Date added Download count The First Cost-Effective Solution for CO2 Capture (47...
Block-wise Alternating Direction Method of Multipliers for Multiple ...
2014-08-24T23:59:59.000Z
Aug 12, 2014 ... We present the convergence analysis, including both the global ..... failure of convergence of (1.13) for a generic case where both m1 ? 2 and ...
Hypertrapezoidal fuzzy membership functions
Painter, John H.; Kelly, W. E. III
1996-09-08T23:59:59.000Z
version of fuzzy logic which requires that set membership sum to one. The fuzzy partitioning which stems from the presented method is parameterized by M+1 values, yielding an efficient mechanism for designing complex fuzzy systems....
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Office of Scientific and Technical Information (OSTI)
Shawn M (1) Spalding, Edgar P (1) de Leon, Natalia (1) Save Results Excel (limit 2000) CSV (limit 5000) XML (limit 5000) Have feedback or suggestions for a way to improve...
Applying a global optimisation algorithm to Fund of Hedge Funds ...
rthapar
2009-09-01T23:59:59.000Z
Aug 1, 2009 ... The search space is sampled using a probability distribution ... temperature to decrease defects, thus minimising the system energy [M1]. By ..... [MSRY] L Mitra, X Sun, D Roman, G Mitra & K Yu, Mixture distribution scenarios.
Transcription Factor-Based Small-Molecule Screens and Selections
Dietrich, Jeffrey Allen
2011-01-01T23:59:59.000Z
for the production of 3-methyl-1- butanol. Appl. Environ.for the production of 3-Methyl-1-Butanol. Appl. Environ.butanol; 3M-1-C4OH, 3-methyl-1- butanol; C4=O, butaldehyde;
Greg Hammett Imperial College, London & Princeton Plasma Physics Lab
Hammett, Greg
Corona & Wind Gyrokinetic Simulations Needed & In Progress #12;MHD Turbulence in Astrophysical Plasmas Medium Power Spectrum Of Electron Density Fluctuations Wavenumber (m-1) Power law over ~ 12 orders more & more nonlinear Hypothesize "critical balance": linear time ~ nonlinear time Anisotropic
Gas Flux Sampling At Long Valley Caldera Geothermal Area (Bergfeld...
thermal gradient in the center of the areas is around 320C m- 1. We estimate total heat loss from the two areas to be about 6.1 and 2.3 MW. Given current thinking on the...
Compound and Elemental Analysis At Long Valley Caldera Geothermal...
thermal gradient in the center of the areas is around 320C m- 1. We estimate total heat loss from the two areas to be about 6.1 and 2.3 MW. Given current thinking on the...
The N-body Problem I. Vectors and Basic Operations
Wang, Quidong
of these two particles. -- Three major elements: (i) (The Law of Gravitation) The force from m1 acting on m2 major elements: (i) (The Law of Gravitation) The force from mj acting on mi is Fij = Gmimj(rj - ri + 0 = 2 u1 Ã? u2 = (6, -3, 6). II. The Two-body Problem Let m1, m2 be two gravitational particles lo
Graphene quantum dots formed by a spatial modulation of the Dirac gap G. Giavaras1,a
Nori, Franco
/2 f1 r exp i m -1 ,if2 r exp im , where m=0, 1,... is the angular momentum quantum number. The radial functions f1 and f2 satisfy V - E + f1 + U + d dr f2 = 0, 2 U - d dr f1 + V - E - f2 = 0, 3 with U= 2m-1 /2r to con- fined states.4,5 It is experimentally possible to engineer an energy gap in graphene's band
Acta Mathematica Sinica, English Series Jan., 2009, Vol. 25, No. 1, pp. 120
Hida, Haruzo
Series The Editorial Office of AMS & Springer-Verlag 2009 Irreducibility of The Igusa Tower Haruzo HIDA of the stabilizer. Here is a general axiomatic approach to prove the irreducibility of an Â´etale covering : Ig = M1 Ã? G1 acts on Ig and S compatibly so that M1 Aut(Ig/S), G1 Aut(S) and G1 acts trivially on 0(Ig
CATEGORICAL GROTHENDIECK RINGS AND PICARD 1. The ring K(R) and the group Pic(R) 1
May, J. Peter
Pic(R) 1 2. Symmetric monoidal categories, K(C ), and Pic(C ) 2 3. The unit endomorphism ring R(C ) 5 4. Some examples of Grothendieck rings 6 1. The ring K(R) and the group Pic(R) We assume familiarity to be invertible if there is an R-module M-1 such that M R M-1 is isomorphic to R. Define the Picard group Pic
High order difference methods for parabolic equations
Matuska, Daniel Alan
1971-01-01T23:59:59.000Z
? d 6)k/24 x t x 't x 10 and (2. 6) n 2 n 3 j =Y 6 [V] j =1, M ? 1 J=l, M ? 1 (h 6 ? 2 6 )[Vb] dB ' = y 6 [V ] j = 2, M ? 2 j 3 x b dB ' = Y (h 6 ? 2h 6 + 5 6 )[V ] ' 1, M ? 1 2, M ? 2 dB. ' = Y 6 [V ] j = 3, M ? 3 n, 4 2 n j 4 x b dB ' = 0...) X. = ? 4 sin j9/2, j c l(O, M), 9 = v/M 2 along with the eigenvalues W = X. . = 0. 0 From this definition of the norm ~ ~ ~ ~ ~ and above, it is clear that the requirement ~[B]( & 1 of theorem 1. 1 is equivalent to max Iu 0~&&M 15 Thus...
Interaction of influenza virus proteins with nucleosomes
Garcia-Robles, Inmaculada [EMBL Grenoble Outstation, BP 181, 38042 Grenoble Cedex 9 (France); Akarsu, Hatice [EMBL Grenoble Outstation, BP 181, 38042 Grenoble Cedex 9 (France); Laboratoire de Virologie Moleculaire et Structurale, EA 2939, Universite Joseph Fourier, Grenoble (France); Mueller, Christoph W. [EMBL Grenoble Outstation, BP 181, 38042 Grenoble Cedex 9 (France); Ruigrok, Rob W.H. [EMBL Grenoble Outstation, BP 181, 38042 Grenoble Cedex 9 (France); Laboratoire de Virologie Moleculaire et Structurale, EA 2939, Universite Joseph Fourier, Grenoble (France); Baudin, Florence [EMBL Grenoble Outstation, BP 181, 38042 Grenoble Cedex 9 (France) and Laboratoire de Virologie Moleculaire et Structurale, EA 2939, Universite Joseph Fourier, Grenoble (France) and Institut de Biologie Structurale, UMR 5075 CEA-CNRS-UJF, 41 rue Jules Horowitz, 38027 Grenoble Cedex 1 (France)]. E-mail: baudin@embl-grenoble.fr
2005-02-05T23:59:59.000Z
During influenza virus infection, transcription and replication of the viral RNA take place in the cell nucleus. Directly after entry in the nucleus the viral ribonucleoproteins (RNPs, the viral subunits containing vRNA, nucleoprotein and the viral polymerase) are tightly associated with the nuclear matrix. Here, we have analysed the binding of RNPs, M1 and NS2/NEP proteins to purified nucleosomes, reconstituted histone octamers and purified single histones. RNPs and M1 both bind to the chromatin components but at two different sites, RNP to the histone tails and M1 to the globular domain of the histone octamer. NS2/NEP did not bind to nucleosomes at all. The possible consequences of these findings for nuclear release of newly made RNPs and for other processes during the infection cycle are discussed.
Ruiz, Hildebrando Argeo
1986-01-01T23:59:59.000Z
I section 1ndicat1ng locat1on of control points. Using the sketch in Figure 6(b) and Equation (8) and assum1ng small angles, the following relations are derived, w = U s1nQ, = U Q?. . Q, = w/U cl /9, = c. /(w/Ug = 47F(h/c) From this 1t..., hence, (m-1) /2 CL [ /FAR/(m+1)](6 + 2 ~ 6 szn 0 ) n=l For the zero net lift case this equation is equated to zero, and with substitution of Equation (16) in Equation ( 13), a set of 1+(m+1) /2 simultaneous equat i ons is formed which involves...
A methodology of mathematical models with an application
Wood, Richard Brian
1972-01-01T23:59:59.000Z
of one more occurrence of state S . Therefore SP33 qlP33 (3. 13) Now I m E q a q m ~ 0 + E q m~l 21 bgl + E q m 1 qi ~P33 ' 19 since Z q is a geometric series by (3. 13). From (3. i4) we have m 1 ql = ( - P33) ( - 21) Hence, m-1 33 24...~O From (2. 1) we see that ? n P R' (2. 2) A basic result of finite absorbing Markov chain theory is; THEOREN 2. 4. Suppose P is any transitional probability matrix for an absorbing Narkov chain. Then lim Q ~ 0. n n~~ PROOF. Case l. Q irreducible...
DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)
Wang, Qiang [Univ. of Massachusetts at Boston, Boston, MA (United States); Yang, Xiao -Qing [Brookhaven National Laboratory (BNL), Upton, NY (United States); Zheng, Doug [Univ. of Massachusetts at Boston, Boston, MA (United States); McKinnon, Meaghan E. [Univ. of Massachusetts at Boston, Boston, MA (United States); Qu, Deyang [Univ. of Massachusetts at Boston, Boston, MA (United States)
2015-01-01T23:59:59.000Z
Superoxide reacts with carbonate solvents in Li–air batteries. Tris(pentafluorophenyl)borane is found to catalyze a more rapid superoxide (O2-) disproportionation reaction than the reaction between superoxide and propylene carbonate (PC). With this catalysis, the negative impact of the reaction between the electrolyte and O2-produced by the O2 reduction can be minimized. A simple kinetic study using ESR spectroscopy was reported to determine reaction orders and rate constants for the reaction between PC and superoxide, and the disproportionation of superoxide catalyzed by Tris(pentafluorophenyl)borane and Li ions. The reactions are found to be first order and the rate constants are 0.033 s-1 M-1, 0.020 s-1 M-1and 0.67 s-1M-1 for reactions with PC, Li ion and Tris(pentafluorophenyl)borane, respectively.
Magnetic-field dependent trap loss of ultracold metastable helium
J. S. Borbely; R. van Rooij; S. Knoop; W. Vassen
2011-11-24T23:59:59.000Z
We have experimentally studied the magnetic-field dependence of the decay of a Bose-Einstein condensate of metastable 4He atoms confined in an optical dipole trap, for atoms in the m=+1 and m=-1 magnetic substates, and up to 450 G. Our measurements confirm long-standing calculations of the two-body loss rate coefficient that show an increase above 50 G. We demonstrate that for m=-1 atoms, decay is due to three-body recombination only, with a three-body loss rate coefficient of 6.5(0.4)(0.6)10^(-27)cm^6s^(-1), which is interesting in the context of universal few-body theory. We have also searched for a recently-predicted d-wave Feshbach resonance, but did not observe it.
DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)
Wang, Qiang; Yang, Xiao -Qing; Zheng, Doug; McKinnon, Meaghan E.; Qu, Deyang
2014-10-28T23:59:59.000Z
Superoxide reacts with carbonate solvents in Li–air batteries. Tris(pentafluorophenyl)borane is found to catalyze a more rapid superoxide (O2-) disproportionation reaction than the reaction between superoxide and propylene carbonate (PC). With this catalysis, the negative impact of the reaction between the electrolyte and O2-produced by the O2 reduction can be minimized. A simple kinetic study using ESR spectroscopy was reported to determine reaction orders and rate constants for the reaction between PC and superoxide, and the disproportionation of superoxide catalyzed by Tris(pentafluorophenyl)borane and Li ions. The reactions are found to be first order and the rate constants are 0.033 s-1 M-1,more »0.020 s-1 M-1and 0.67 s-1M-1 for reactions with PC, Li ion and Tris(pentafluorophenyl)borane, respectively.« less
Scales in the fine structure of the magnetic dipole resonance: A wavelet approach to the shell model
Petermann, I.; Langanke, K. [Institut fuer Kernphysik, Technische Universitaet Darmstadt, D-64289 Darmstadt (Germany); GSI Helmholtzzentrum fuer Schwerionenforschung, D-64291 Darmstadt (Germany); Martinez-Pinedo, G. [GSI Helmholtzzentrum fuer Schwerionenforschung, D-64291 Darmstadt (Germany); Neumann-Cosel, P. von [Institut fuer Kernphysik, Technische Universitaet Darmstadt, D-64289 Darmstadt (Germany); Nowacki, F. [Institute Pluridisciplinaire Hubert Curien, F-67037 Strasbourg (France); Richter, A. [Institut fuer Kernphysik, Technische Universitaet Darmstadt, D-64289 Darmstadt (Germany); ECT, Villa Tambosi, I-38050 Villazano, Trento (Italy)
2010-01-15T23:59:59.000Z
Wavelet analysis is applied as a tool for the examination of magnetic dipole (M1) strength distributions in pf-shell nuclei by the extraction of wavelet scales. Results from the analysis of theoretical M1 strength distributions calculated with the KB3G interaction are compared to experimental data from (e,e{sup '}) experiments and good agreement of the deduced wavelet scales is observed. This provides further insight into the nature of the scales from the model results. The influence of the number of Lanczos iterations on the development and stability of scales and the role of the model space in terms of the truncation level are studied. Moreover, differences in the scales of spin and orbital parts of the M1 strength are investigated, as is the use of different effective interactions (KB3G, GXPF1, and FPD6).
Paramagnetic resonance at low fields
Becker, Stewart
1954-01-01T23:59:59.000Z
$ 15?$ 62Mo1iM1t 1J"o 5M1$kwi15Mk 1J$ o5kMiW 2K$w ?2w$ 6L6W$o) rM6w$io5Mk 1J$ 15?$ 62Mo1iM1 h$L2MS .)A o$62MSo S5S M21 i''w$65ihWL 5?m 'w2K$ 1J5o '$w-2w?iM6$ iMS ?iS$ 1J$ i?'W5-5$w S5--56"W1 12 T2w^ T51J) 0J$ ?2W$M25S $?? -???????? ??h...
V. R. Gavrilov; V. N. Melnikov
1998-01-13T23:59:59.000Z
The D-dimensional cosmological model on the manifold $M = R \\times M_{1} \\times M_{2}$ describing the evolution of 2 Einsteinian factor spaces, $M_1$ and $M_2$, in the presence of multicomponent perfect fluid source is considered. The barotropic equation of state for mass-energy densities and the pressures of the components is assumed in each space. When the number of the non Ricci-flat factor spaces and the number of the perfect fluid components are both equal to 2, the Einstein equations for the model are reduced to the generalized Emden-Fowler (second-order ordinary differential) equation, which has been recently investigated by Zaitsev and Polyanin within discrete-group analysis. Using the integrable classes of this equation one generates the integrable cosmological models. The corresponding metrics are presented. The method is demonstrated for the special model with Ricci-flat spaces $M_1,M_2$ and the 2-component perfect fluid source.
Moffitt, John Russell
1972-01-01T23:59:59.000Z
thickness. Both Rayleigh and isotropic scattering are considered and examples are included for r = 1, m = 1, n = -1, m ' o ' 1 and A = 0. The method is also extended to include non-zero ground albedos and an example is included. A method... scattering for = 1 m = 1 n = -1 and A = 0. The continuous m o 1 10 curve is Matrix Operator Theory result 27 INTROBNCTION 1. Current and Past Methods for Calculating Reflected and Trans- mitted Radiance Early work in calculating the reflected...
Comparison of Precision Orbit Derived Density Estimates for CHAMP and GRACE Satellites
Fattig, Eric
2011-04-21T23:59:59.000Z
NOMENCLATURE Symbol Definition Units draga acceleration vector due to atmospheric drag m/s 2 ap geomagnetic 3-hourly planetary equivalent amplitude index gamma, Telsa, or kg s m-1 A satellite cross-sectional area m2 Ap geomagnetic daily planetary... amplitude index gamma, Telsa, or kg s m-1 BB estimated ballistic coefficient correction ~ BC ballistic coefficient m2/kg Dc satellite drag coefficient ~ d cross correlation delay F10.7 daily solar radio flux measured at 10.7 cm wavelength SFU 10.7F...
Initial characerization of human spermine oxidase
Juarez, Paul Ramon
2009-05-15T23:59:59.000Z
-Rojas for their relentless encouragement and friendly advice. vii NOMENCLATURE SPM Spermine DDAD 4,9-Dioxo-1,12-diaminododecane DDD 1,12-Diaminododecane DAO 1,8-Diaminooctane FAD Flavin adenine dinucleotide SET Single electron...-3; the resulting kinetic parameters are shown in Table 6. Table 6: Steady state kinetic parameters for spermine oxidase at pH 8.5, 25 ?C. Equation k cat (s -1 ) K O2 (mM) k cat /K O2 (s -1 mM -1 ) K Spm (?M) k cat /K Spm (s -1 ?M -1...
Empirical Essays on the Efficiency of Heterogeneous Good Auction
Martin, Thomas A., IV
2010-01-14T23:59:59.000Z
follow Nautz [29], Horta?csu [22] and Kang and Puller [24] in developing the discrete model. The prices for good m are restricted to lie on a discrete grid. Let p m,0 ? p m,1 ? ??? ? p m,J m ? p m,J m +1 be the price grid for good m. There are J m + 2... of all strictly decreasing, differentiable functions y : R M + ? [0,1] M . 2 Hence the bidders? pure strategies are ? i : S i ? Y. For a bidder of type s i , the bid function is y i (p|s i ), which specifies for each vector of prices, p, what share...
Interpretation of data from a pulse reactor
Desai, Nayneshkumar Shantilal
1988-01-01T23:59:59.000Z
? Overall conversion in the reactor CP(M, J, K) ? Pore concentration CS(M, J, K) ? Surface concentration CT ? Total site concentration DEFF ? Effective diffusivity of the catalyst EB ? Catalyst bed porosity EC ? Voidage within the catalyst pellet GL... = GLeKA/VI CKR = GLeKR/VI Initialize bulk, pore, and surface concentrations DQ 1 M = 1, 10i CB(M, 1) = O. OD+00 DO 1 J = 1, 11 CP(M, J, 1) = O. OD+00 CS(M, J, 1) = O. OD+00 CONTINUE Initialize the time counter and input thr initial time L=11 K...
DEGAS 2 Neutral Transport Modeling of High Density, Low Temperature Plasmas
, the resulting fluid neutral momentum balance in a slab geometry is d dx ³ mnv 2 + nT ´ = # T n dT dx - m# cx nv.24, and the charge exchange frequency, # cx = 2.93# cx n(T/m) 1/2 . With a neutral source on one end of the slab (x density # # n(x)/n(L), d# dx = - 2 4 (1-# T ) T (L) dT (x) dx # + ##cx [T (L)/m] 1/2 T (x) T (L) - # 2 # 2
A Fully-Integrated 5GHz CMOS Wireless-LAN Receiver
Lee, Thomas H.
( ) ------------------ fmin fmax #12;Parasitic capacitance Cx degrades the noise performance. Noise Rejection In M3 M1 X Cx Lx;Equivalent Noise Circuit for the LNA M1 X Cx Zin Ls Lg M3 Iout + - + - V s 2 V g1 2 I g1 2 I d3 2 Rs Rin1 Cx drain noise modeled) #12;Filter Noise Model I d5 2 I L5 2 C3 C1Cx L5 1 gm5 ----------Â I d5 2 I L5 2
HOPM1 mediated disease resistance to Pseudomonas syringae in Arabidopsis
He, Sheng Yang (Okemos, MI); Nomura, Kinya (East Lansing, MI)
2011-11-15T23:59:59.000Z
The present invention relates to compositions and methods for enhancing plant defenses against pathogens. More particularly, the invention relates to enhancing plant immunity against bacterial pathogens, wherein HopM1.sub.1-300 mediated protection is enhanced, such as increased protection to Pseudomonas syringae pv. tomato DC3000 HopM1 and/or there is an increase in activity of an ATMIN associated plant protection protein, such as ATMIN7. Reagents of the present invention further provide a means of studying cellular trafficking while formulations of the present inventions provide increased pathogen resistance in plants.
California at Santa Cruz, University of
fractional transformations: M = m(z) = az + b cz + d , ad - bc = 1 , where a, b, c, d and z are complex transformations. If we define m1(z) = a1z + b1 c1z + d1 , then the composition of two successive linear fractional transformations is given by: m2(m1(z)) = a2 a1z + b1 c1z + d1 + b2 c2 a1z + b1 c1z + d1 + d2 = a2(a1z + b1) + b2(c
Shaping Coil Currents: 0 kA Vedge/Vcore: 43.8
Base Shaping Coil Currents: 0 kA 0 kA Vedge/Vcore: 43.8 Pcore/Pedge: 544 0 1 2 R (m) -1 -0.5 0 0.5 1 1.5 Z(m) Psi and |B| Contours High Shaping Coil Currents: 1 kA 12 kA Vedge/Vcore: 187 Pcore/Pedge: 6120 0 1 2 R (m) -1 -0.5 0 0.5 1 1.5 Z(m) Psi and |B| Contours Shaping Coil Currents: 50 kA 50 kA Vedge
Sigma-models having supermanifolds as target spaces
Albert Schwarz
1995-06-10T23:59:59.000Z
We study a topological sigma-model ($A$-model) in the case when the target space is an ($m_0|m_1$)-dimensional supermanifold. We prove under certain conditions that such a model is equivalent to an $A$-model having an ($m_0-m_1$)-dimensional manifold as a target space. We use this result to prove that in the case when the target space of $A$-model is a complete intersection in a toric manifold, this $A$-model is equivalent to an $A$-model having a toric supermanifold as a target space.
Algoritmos y Estructuras de Datos II Ejercicios Tema 1. Anlisis de algoritmos
GimÃ©nez, Domingo
Algoritmos y Estructuras de Datos II Ejercicios Tema 1. AnÃ¡lisis de algoritmos 1 1.1. Obtener el tiempo de ejecuciÃ³n t(n), O(t(n)), (t(n)) y o(t(n)) para el siguiente algoritmo de multiplicaciÃ³n de algoritmo de bÃºsqueda binaria. i= 1 j= n repeat m= (i+j) div 2 if a[m] > x j= m-1 else i= m+1 endif until i
Regions of influence for several methods of factoring polynomials
Schulze, Tommy Joe
1965-01-01T23:59:59.000Z
, or if preferred, over the field of complex numbers be denoted n n-1 f(x) = x + a x + + a x + a n-1 n' Let a factor of the above be (2) III m-1 g(x) x + p x +'''+ p x + p m-1 Ill If an iterative technique is used to find the factor (2) then iteration must... factors of any degree, it is [Sj presented in this section for quadratic factors only, to permit easy comparison with Bairstow's Method. 2 Let f(x) be as in (1), and let g(x) = x + plx + p be any 2 quadratic expression. Then the process of long...
A critical bibliography of Dr. Henry Sacheverell
Madan, F. F. (Francis Falconer); Speck, W. A. (William Arthur)
1978-01-01T23:59:59.000Z
. Sacheverel's intitul'd The Political Union, &c. lately printed at Oxford. In a letter to a new-elected Member of Parliament. London. Printed in the year 1702." 4°: A-F2; [1-2] 3-22 [23-24]. M 1. REPRINTED WITH THE TITLE "PRIESTCRAFT DANGEROUS TO RELIGION... of a church-man: shewing the false pretences to that name. Humbly offer'd to all the electors of the ensuing Parliament and Convocation. . . . printed in the year, 1702. 4°: 7r\\ [=C4] A-C* [-C4]; [i-ii] 3-22. M 1. Daily Courant, 29 July 1702. 9...
Ting Gao; Feng-Li Yan; Zhi-Xi Wang; You-Cheng Li
2006-04-18T23:59:59.000Z
We analyze the capacity of a simultaneous quantum secure direct communication scheme between the central party and other $M$ parties via $M+1$-particle GHZ states and swapping quantum entanglement. It is shown that the encoding scheme should be secret if other $M$ parties wants to transmit $M+1$ bit classical messages to the center party secretly. However when the encoding scheme is announced publicly, we prove that the capacity of the scheme in transmitting the secret messages is 2 bits, no matter how big $M$ is.
STATE RESEARCH CENTER OF RUSSIA INSTITUTE FOR HIGH ENERGY PHYSICS
, JINR) SPIN OKA (IHEP, INR, JINR) SVD (IHEP, MSU) FODS E=70 GeV, I=1.7·1013 ppp Beams of , K, p, e) · Primary beam - 50÷70 GeV protons, I=1013 ppp · Target - 50 cm Be · Energy of secondary K± - 12.5 - 18 GeV · Intensity of K+ (K-) beam - ~106 ppp Test area of RF separators #12;13 RF1 RF2Optics BS L m1 m2 m1 m2 m2
Linear Algebra Meets Lie Algebra The Kostant-Wallach Theory
Higham, Nicholas J.
Dual Coordinates B M(n) M(n). (G1m) Bm = Gmm(Gm)-1, Gm GL(m). Gm unique if last row is ones, by (G2m). Definition bm and cm Cm, given by Bm+1 = Gm 0 0T 1 m cm bm T m+1 Gm -1 0 0T 1 = Bm Gmcm bm T Gm -1 m+1 . #12;The Dual Coordinates B M(n) M(n). (G1m) Bm = Gmm(Gm)-1, Gm GL(m). Gm unique if last
Lechtenberg, Travis Francis
2015-05-31T23:59:59.000Z
............................................................................................... 78 vi NOMENCLATURE Symbol Definition Units av acceleration vector due to atmospheric drag m/s2 ap geomagnetic 3-hourly planetary equivalent amplitude index gamma, Tesla, or kg s m- 1 A satellite cross-sectional area m2 Ap geomagnetic... daily planetary amplitude index gamma, Tesla, or kg s m- 1 B B? estimated ballistic coefficient correction ~ BC ballistic coefficient m2/kg Dc satellite drag coefficient ~ d cross correlation delay F10.7 daily solar radio flux measured at 10...
Doctor of Nursing Practice Program DNP INTENSIVE
Bordenstein, Seth
Donaldson, DNP, ACNP-BC DNP Program Co-Director 10:00 a.m.-12noon 1st Year: 140FH 2nd Year: 144FH N442 early for your appointment** 3:00-5:00 p.m. 1st Year: 140FH 2nd Year: 144FH N422: Evidence/Session Event/Session 8:00-10:00 a.m. 1st Year: 140FH 2nd Year: 144FH N422: Evidence-Based Practice II
Loewe, Robert S.; Tomizaki, Kin-ya; Lindsey, Jonathan S.
2005-07-12T23:59:59.000Z
The present invention provides methods, compounds, and compositions for the synthesis of light harvesting arrays, such arrays comprising: (a) a first substrate comprising a first electrode; and (b) a layer of light harvesting rods electrically coupled to said first electrode, each of said light harvesting rods comprising a polymer of Formula I: wherein m is at least 1; X.sup.1 is a charge separation group, and X.sup.2 through X.sup.m+1 are chromophores. At least one of X.sup.2 through X.sup.m+1 has at least one perylene group coupled thereto.
PHC Dining Room Closes at 2 p.m.
Simons, Jack
PHC Dining Room August 2- Closes at 2 p.m. August 4 Â August 20 Breakfast 7 a.m.- 8:30 a.m. Lunch 11 a.m.- 1:30 p.m. Dinner 5 p.m. - 6:30 p.m. Saturday & Sunday Brunch 11 a.m. - 1 p.m. Dinner 5:30 p.m. - 6:30 p.m. Crimson Corner August 2- Closes at 2 p.m. August 4 Â August 20 8 a.m.- 3 p.m. Saturday
Limit Domains in Several Complex Variables
Console, Alexander
2013-12-31T23:59:59.000Z
sequence of automor- phisms" in [Fornæss & Stensønes, 2004], both the approaches to constructing Fatou-Bieberbach domains discussed above can be seen as constructing basins of attraction. We will not pursue this viewpoint. 3.2 Push-Out Constructions... n ? N and z ??n and k > m? n. Then writing w = Gm(z) ? Dm, a) and b) 17 imply |Gk(z)?Gm(z)|= |Hk ?Hk?1 ? · · · ?Hm+1(w)?w| ? |w?Hm+1(w)|+ |Hm+1(w)?Hm+2(Hm+1(w))| + · · ·+ |Hk?1 ? · · · ?Hm+1(w)?Hk(Hk?1 ? · · · ?Hm+1(w))| < ?m 2m + ?m+1 2m+1...
Korshunov, Dmitry
> 0 F EeM 1 1 - F (6) , , P(M > x) = o(e-x ) x . . , eM n=0 eSn , , Ee a > 0 , lim inf x P(M > x) F(x) lim inf x 1 F(x) P M > x, n1 Aa,x-a n (1 - ) EeM 1 - F . . (1) F a a 0 P(M dt)et = EeM , (14). P(M > x), - F S. 3. , F S > 0 F
Poles of Intertwining Operators via Endoscopy; the Connection with ...
Freydoon Shahidi
1910-00-20T23:59:59.000Z
In this paper, we determine the residues at poles of standard intertwining operators for parabolically ...... Here {m1} is as earlier just the M ? ?-conjugacy class and does not denote the projection .... 116 (1994), 1101–1151. 11. Goldberg, D. and ...
Ghosh, Joydeep
/A Collection station on first floor of the Student Services Building. Facilities Services Styrofoam Hard-mold Styrofoam used in packing packing peanuts food packaging First Mondays of each month from 10 a.m. 1 p.m. at the Robert A. Welch Hall loading dock. Office of Sustainability Bag the Styrofoam in clear/white bags before
Dynamic Master selection in wireless networks Maurits de Graaf
Boucherie, Richard J.
the condition that the remaining battery capacity of each node is positive duri' algorithm. 1 Introduction Mobile wireless networks are often battery powered which makes it im- portant = m, maxvV c(v, m) for v = m. (1) Each vertex is equipped with battery supply bv, which is reduced
How Generic is Burning Plasma Physics? S.C. Prager
How Generic is Burning Plasma Physics? S.C. Prager University of Wisconsin December, 2000 #12;Are axisymmetric: RFP, spheromak · q= 0 axisymmetric: FRC, dipole · Nonaxisymmetric: stellarator family #12 (except FRC with B = 0) r (m, n) (m +1,n) gap { #12;elliptical gap toroidal gap r { r { With elliptic
Governing equations -Ohm's Law
Washington at Seattle, University of
conserving boundaries to drive current in an FRC, full penetration is not observed. Instead, the RMF only could be explained with a radially inward plasma flow (which must also be accompanied long RMF Antenna TCS Vacuum Chamber TCS Internal Magnetic Probe 0.8 m 1.5 m 2.6 m FRC Magnetic probes
Interpreting Neural Activity Through Linear and Nonlinear
Slatton, Clint
(~100-900 msec) Muscle strength is limited Learn about neurophysiology! #12;6/4/2003 3 Modeling) Preparation and guidance (visual inputs) Primary Motor (M1) Initiates muscle contraction We invoke Movement Segmentation 0 10 20 30 40 50 60 70 -30 -20 -10 0 10 20 30 40 50 60 70 X Y Z Food to Mouth Mouth
JET SCHEMES OF TORIC SURFACES ESPACES DE JETS DES SURFACES TORIQUES
Favre, Charles - Institut de Mathématiques de Jussieu, Université Paris 7
JET SCHEMES OF TORIC SURFACES ESPACES DE JETS DES SURFACES TORIQUES HUSSEIN MOURTADA Abstract. For m N, m 1, we determine the irreducible components of the m - th jet scheme of a toric surface S irr´eductibles des m-espaces des jets d'une surface torique S. Pour m assez grand, on relie le nombre
Faraway, Julian
, University of Michigan, Ann Arbor, Michigan, Xudong Zhang, University of Illinois, Urbana-Champaign, Illinois, and Charles Woolley, University of Michigan, Ann Arbor, Michigan The rapid adoption of software to simulate of Michigan, Ann Arbor. M1 48019-2117; dchaffin@umich.edu. HUMAN FACTORS, Vol. 42, No. 3, Fall 2000. pp. 408
Developpement Web -Servlet Developpement Web -Servlet
Hao, Jin-Kao
D´eveloppement Web - Servlet D´eveloppement Web - Servlet Jean-Michel Richer jean-michel.richer@univ-angers.fr http://www.info.univ-angers.fr/pub/richer M1/M2 Informatique - 2010-2011 1 / 34 #12;D´eveloppement Web / 34 #12;D´eveloppement Web - Servlet Introduction Programmation Web avec Java Objectifs · initiation
Developpement Web -Servlet Developpement Web -Servlet
Richer, Jean-Michel
D´eveloppement Web - Servlet D´eveloppement Web - Servlet Jean-Michel Richer jean-michel.richer@univ-angers.fr http://www.info.univ-angers.fr/pub/richer M1 Informatique - 2010-2011 1 / 33 #12;D´eveloppement Web´eveloppement Web - Servlet Introduction Programmation Web avec Java Objectifs · initiation `a la programmation Web
Developpement Web -Servlet Developpement Web -Servlet
Hao, Jin-Kao
D´eveloppement Web - Servlet D´eveloppement Web - Servlet Jean-Michel Richer jean-michel.richer@univ-angers.fr http://www.info.univ-angers.fr/pub/richer M1/M2 Informatique - 2010-2011 1 / 30 #12;D´eveloppement Web Bibliographie 2 / 30 #12;D´eveloppement Web - Servlet Introduction Introduction Introduction 3 / 30 #12;D
Developpement Web -Servlet Developpement Web -Servlet
Richer, Jean-Michel
D´eveloppement Web - Servlet D´eveloppement Web - Servlet Jean-Michel Richer jean-michel.richer@univ-angers.fr http://www.info.univ-angers.fr/pub/richer M1 Informatique - 2010-2011 1 / 29 #12;D´eveloppement Web´eveloppement Web - Servlet Introduction Introduction Introduction 3 / 29 #12;D´eveloppement Web - Servlet
ISOPERlMETRIC INEQUALITIES FOR RIEMANNIAN PRODUCTS A. A. Crigor ' yan
Grigor'yan, Alexander
or the dire c t product .lI, x M,Â£ of t he mani f o l ds M1 and "'10 if i s operbetric inequalit ies on "'I c inequalit y holds . Where 38 , No.4. 0001-4346/&5 /3845- 0849$09 . 50 0 1986 Plenum Publishinl
'Texas A & M University-Central Texas CPSY 554 Group Procedures for Counselors
Diestel, Geoff
'Texas A & M University- Central Texas CPSY 554 Group Procedures for Counselors 10:30 a.m. -1:20 p.m. Summer 2012 Instructor: Dr. Pauline Moseley Office: Phone: Texas A & M University North Campus 519: Texas A & M University- Central Texas North Campus 107N Unilert Emergency Warning System for Texas A & M
Power variation of some integral fractional processes
Corcuera, José Manuel; Nualart, David; Woerner, Jeannette H.C.
2006-08-01T23:59:59.000Z
(i) jB Hj=m #1; B H( j#1;1)=mj p ! þ m#1;1þ pH X[nt] i¼1 ju(i#1;1)=nj p X j2 I n(i) jB Hj=m #1; B H( j#1;1)=mj p #1; c p n#1;1 X[nt] i¼1 ju(i#1;1)=nj p þ c p n#1;1 X[nt] i¼1 ju(i#1;1)=nj p #1; ð t 0 jusj p ds ! ¼ A(m)t þ B(n,m)t þ C(n,m)t þ D...(n)t , where I n(i) ¼ j : j m 2 i #1; 1 n , i n #5; #6;#7; #8; , 1 < i < [nt]: For any fixed n, C(n,m)t converges in probability to zero, uniformly in t, as m tends to infinity. In fact, kC(n,m)k1 < X[nT ] i¼1 ju(i#1;1)=nj p #3;#3;#3;#3;m#1;1þ pH X j2 I n(i) jB...
Chapter 26: Earth's Interior Did you read chapter 26
Hart, Gus
Drilling Program Deepest hole penetrated · 2,111 m (1.31 mi) · E Pacific Ocean Shallowest water depth. No The Interior of the Earth The main features of the earth's surface are continents and ocean basins. What is the world's deepest mine, 3585m (2.2 miles) below surface 1933, ½ mile 2005, ~2 miles Drilling a Hole Ocean
US National Technical Meeting of the Combustion Institute
Raman, Venkat
density function (PDF) of species mass fraction and enthalpy. Computing the PDF using traditional density function (PDF) methodol- ogy, where the joint-PDF of the gas phase thermochemical composition and sensible enthalpy can thus be written as F,h(, ) = Ne n=1 wn( - n) Ns m=1 (m - mn) (1) Here, Ne
Thermochemistry of (H2 A DFT Study
Yu, Fangqun
enthalpies, entropies, and Gibbs free energies of (H2 SO4 )m (H2 O)n (NH3 )k (n = 1,2; m = 15; k = 0 appropriate, presumably larger, basis set is necessary. In this paper, the structure, thermochemical
A Proposal to Reform the Kyoto Protocol: the Role of Escape Clauses and Foresight
Karp, Larry; Zhao, Jinhua
2007-01-01T23:59:59.000Z
size of its associated IEA, rather than by the identities ofM j+1 are the same type of IEA, and were they are differentM 1 ). Consequently, at any IEA M j , j < k, a group of M k
RECURSIVELY RENEWABLE WORDS AND CODING OF IRRATIONAL ROTATIONS
Akiyama, Shigeki
RECURSIVELY RENEWABLE WORDS AND CODING OF IRRATIONAL ROTATIONS SHIGEKI AKIYAMA AND MASAYUKI us come back to a general A = {0, 1, . . . , m - 1}. An element z = z0z1 · · · AN is k-renewable is called recursively k-renewable. To be more precise, z = z0z1 . . . is recursively k- renewable when
Single mode terahertz quantum cascade amplifier
Ren, Y; Wallis, R.; Shah, Y. D.; Jessop, D. S.; Degl'Innocenti, R.; Klimont, A.; Kamboj, V.; Beere, H. E.; Ritchie, D. A.
2014-10-06T23:59:59.000Z
from the device were analysed. According to the Fresnel expression, an antireflective layer is obtained when its refractive index nAR, and thickness d, satisfy the conditions nAR = nanb and d=(2m+1)??/4nAR, such that the reflection at the interface...
Introduction to Queuing Networks MATH 35800/M5800 Problem Sheet 6 Autumn 2014
Collins, Sean
and the transition rates q (n, m) for the reversed process. (c) Guess the invariant distribution for this network satisfies the requirements for a closed Jackson network. Find the distribution of the remaining M - 1 that this distribution is the same as the invariant distribution of customers for a model with the same network
media preparation protocols Revised on 5/23/08 Trypanosome Media Preparation Protocols
Cross, George
concentration is 1.5 mM) 1,100 mg Pyruvic acid 390 mg Thymidine 140 µl 2-mercaptoethanol Filter disulfonic acid (final concentration is 50 µm) 1,820 mg Cysteine (add after Bathocuproine) (final acid composition differs significantly from MEM. DTM calls for adding BME vitamins solution, which
Dynamic Load Balancing for I/O-and Memory-Intensive Workload in Clusters Using a
Zhu, Yifeng
Load-Balancing Scheme We consider the issue of a feedback control method in a cluster, M = {M1, ..., Mn/O, respectively, without any resource sharing. For a newly arrived job j at a node i, load balancing schemesDynamic Load Balancing for I/O- and Memory-Intensive Workload in Clusters Using a Feedback Control
Multiple Exciton Generation and Charge Extraction in All-Inorganic Nanostructured Solar Cells (DMR a comparative analysis of the results in relation to PbS NP solar cells (E3) Optimize the charge transport-equilibrium rate equations will be developed to determine the full rate of MEG Mathematical framework (M1) Lanczos
Minimizing Actuator-Induced Residual Error in Active Space Telescope Primary Mirrors
de Weck, Olivier L.
/m2 Diameter: 6.5 m (1.3 m segments) Shape control: active (7 DOF) Actuators: cryogenic stepper motors SSL3 26 January 2010 Background · Trend toward large aperture space telescopes Higher resolving: 2.4 m Shape control: passive Actuators: none Previous generation: Hubble Space Telescope (HST) [1
Peirce Algebras and Relation Algebras are equipollent* Renate A. Schmidt
Schmidt, Renate A.
the axioms M1-M6 of Bool* *ean modules and the axioms P1 and P2 of Peirce algebras. see Brink et al. (1994 Peirce Algebras and Relation Algebras are equipollent@mpi-sb.mpg.de September 1993/August 1994 Extended Abstract I assume relation algebras
Wang, Wei Hua
(2000) J. Ihlemann et al. Appl. Phy. A54, 363 (1992) Fused Silica Quartz Laser Drilling - Straight holes #12;Laser Drilling - L shaped hole Sample: fused silica thickness ~ 1.5mm Laser: YAG, 1.06m, 1ms Drilling from rear surface in contact with absorption solution L-shaped hole formed by changing the laser
Rcifs, trottoirs et autres biolithosores du bassin de San Miguel de Salinas
Paris-Sud XI, Université de
" and others "biolithosores" of the San Miguel de Salinas Basin GARCIN M.1, VACHARD D.2 1 BRGM SGN/UPE/RNG Av courante Vermets-stromatolithes est discutée. Abstract The San Miguel de Salinas basin, located in SE Spain1 Récifs, trottoirs et autres biolithosores du bassin de San Miguel de Salinas Reefs, "trottoirs
High-Speed, Low-Power Analog-to-Digital Converters
Chiang, Shiuh-hua
2013-01-01T23:59:59.000Z
CS op amp and (b) its step response. 4.17 Conventional one-4.20 Op amp step responseCS op amp and (b) its step response. ?C in g m1,2 g m3,4 V
HIGH-TEMPERATURE FRACTURE AND FATIGUE RESISTANCE OF A DUCTILE b-TiNb REINFORCED g-TiAl
Ritchie, Robert
are in part aimed at improving their low room-temperature ten- sile ductility and fracture toughness, bothHIGH-TEMPERATURE FRACTURE AND FATIGUE RESISTANCE OF A DUCTILE b-TiNb REINFORCED g the fracture toughness of g-TiAl, even at high temperatures, from about 12 to H40 MPa m1/2 , although
Kent, John T.
and Robert G. Aykroyd Department of Statistics, University of Leeds, Leeds LS2 9JT, UK Abstract Growth models = 1;::: ;N labels different individuals, k = 1;::: ;K labels different landmarks, m = 1;::: ;M labels different coordinates, h = 1;::: ;H labels different times t1;::: ;tH. It is convenient to represent
FOURIER AND BIOT NUMBERS AND THE ACCURACY OF CONDUCTION MODELLING Jan L M Hensen, Abdullatif E Nakhi
Mukasyan, Alexander
FOURIER AND BIOT NUMBERS AND THE ACCURACY OF CONDUCTION MODELLING Jan L M Hensen, Abdullatif E of the associated theory the paper concentrates on the effects of Fourier and Biot numbers on the accuracy, °C Fo Fourier number ( t x-2 ), - thermal conductivity, W m-1 K-1 h convective heat transfer
Construction of the noncommutative complex ball
Wang, Zhituo, E-mail: zhituo@mat.uniroma3.it [Dipartimento di Matematica, Università di Roma Tre Largo S. L. Murialdo 1, 00146 Roma (Italy)
2014-09-15T23:59:59.000Z
We describe the construction of the noncommutative complex ball whose commutative analog is the Hermitian symmetric space D = SU(m, 1)/U(m), with the method of coherent state quantization. In the commutative limit, we obtain the standard manifold. We also consider a quantum field theory model on the noncommutative manifold.
District of Columbia, University of the
Hamburg, Germany's second largest city, is home to two of the most important urban development for ecological sustainability and mixed use development along the Elbe River in Hamburg, Germany e m b e r 1 5 , 9 a m 1 2 : 30 p m The City of Hamburg, Germany is a city-state. Like Washington
Laser Worker Registration Form (LWRF) Surname: Forenames
Martin, Ralph R.
ABCDEFGHI Laser Worker Registration Form (LWRF) Surname: Forenames: School of: Ext No.: Email YY Class of Laser to be Used 1 1M 1E 2 2M 3R 3B 4 Work Location(s) Lab No. Laser Work Currently Undertaken Elsewhere Are you currently engaged in work elsewhere involving laser radiation? YES
Internal conversion coefficients in (134)Cs, (137)Ba, and (139)La: A precise test of theory
Nica, N.; Hardy, John C.; Iacob, V. E.; Balonek, C.; Trzhaskovskaya, M. B.
2008-01-01T23:59:59.000Z
Recently we measured the ratio of K-shell internal conversion coefficients, alpha(K), for the 127.5-keV E3 transition in (134)Cs and the 661.7-keV M4 transition in (137)Ba. We here report a measurement of the 165.9-keV M1 transition in (139)La...
Willsky, Alan S.
, This resulted in a rolling supersonic dive( M =1.03).The altitude transition during the run was from 20 OOO.pp. U2-240, May-June 1969. C. R. Chalk and R. K. Wilson, `Airplane flying qualitm specificatton
Stresa, Italy, 25-27 April 2007 0-LEVEL VACUUM PACKAGING RT PROCESS FOR MEMS RESONATORS
Paris-Sud XI, Université de
and hole clogging. It discusses mass production compatibility in terms of packaging stress during back]. The device is based on a suspended-gate resonating over a MOSFET channel which modulates the drain current. Suspended- Gate Drain Source Bulk contact a) 10 m Drain Source Suspended- Gate 6 m 1 m b) SiO2 c) 1 m Hole
JUSTIFICATION OF THE SHALLOW WATER LIMIT FOR A RIGID LID FLOW WITH BOTTOM TOPOGRAPHY
Oliver, Marcel
JUSTIFICATION OF THE SHALLOW WATER LIMIT FOR A RIGID LID FLOW WITH BOTTOM TOPOGRAPHY MARCEL OLIVER with bottom topography. We prove an a priori estimate in the Sobolev space H m for m #21; 3 which shows and the magnitude of the initial data in H m , the gradient of the bottom topography in H m+1 , and the aspect ratio
Exploration of a Submerged Sinkhole Ecosystem in Lake Huron
Exploration of a Submerged Sinkhole Ecosystem in Lake Huron Bopaiah A. Biddanda,1 * Dwight F in the bedrock (sinkholes), through which groundwater emerges onto the lake floor. During September 2003, we explored a recently discovered submerged sinkhole ecosystem (55 m · 40 m · 1 m) located at a depth of 93 m
JOURNAL DE PHYSIQUE IV C3-277 Colloque C3, suppl. au Journal de Physique III, Vol. 1, octobre 1991
Paris-Sud XI, Université de
. By using homogeneous and both bonded and unbonded laminated targets of several aluminium alloys and bond content was selected to be equivalent to approximately 6 mm of aluminium alloy, with all target areal. Laminates M1 and M3, whilst made of the different parent alloys 2024-T351 and the aluminium-lithium alloy
Andrew J. Long; Cecilia Lunardini; Eray Sabancilar
2014-11-12T23:59:59.000Z
We study the physics potential of the detection of the Cosmic Neutrino Background via neutrino capture on tritium, taking the proposed PTOLEMY experiment as a case study. With the projected energy resolution of $\\Delta \\sim$ 0.15 eV, the experiment will be sensitive to neutrino masses with degenerate spectrum, $m_1 \\simeq m_2 \\simeq m_3 = m_\
Prediction of Asphalt Mixture Compactability from Mixture, Asphalt, and Aggregate Properties
Muras, Andrew J.
2010-07-14T23:59:59.000Z
. Predicted Plot of CV Neural Net of Entire Data Set for a ............................ 50 Figure 32. Predicted Plot of CV Neural Net of Entire Data Set for AV Nini ................... 51 Figure 33. a versus Predicted a... ................................................... 24 Table 5 HMA Mixing and Compaction Temperatures ............................................. 27 Table 6 Compaction Parameters a, c, and AV Nini ................................................... 38 Table 7 Compaction Parameters m1, m2...
Crane Scheduling for ABB: Progress Latife Gen
Grossmann, Ignacio E.
-1 Job n Job 5 Job 6 OK OK ILLEGAL ILLEGAL ILLEGAL ILLEGAL OK Examples of sequencing moves (on equipment (4) Job 3 Job 4 Job m-1 Job m Job 5 Job 6 OK OK OK OK ILLEGAL ILLEGAL X X X X Examples
H O W T O M O R R O W M O V E S HOW TOMORROW MOVES
Illinois at Urbana-Champaign, University of
is a van-Genuchten parameter, and it is defined as: m=1-1/n. 3) Swr: residual water saturation 4) Srn Thickness Scaled to Water Pressure · 20 Select Well Locations Used · Elevations Grid Generated with Surfer: residual LNAPL saturation 5) KLNAPL: LNAPL hydraulic conductivity Notes: #12;API EQUATIONS APPLIED
INTERIM VALIDATION REPORT MIDDLE DISTILLATE PRICE MONITORING SYSTEM
Hopelain, D.G.
2011-01-01T23:59:59.000Z
~fv . : :l'! ~m.fol? m EIA-9. . · i . . .. ·. . ~F -· lJl:J. ~ ll\\lv->1;1\\'t from ionn EIA-9. _ .. •,:,,··,..,.,_,d i 1vicl'~ 1 OF Ei\\ll:ii~Y EIA 9 Supersedes F EA·P112-M-1
Hernandez Garduno, David
2009-05-15T23:59:59.000Z
transfer function given by the ratio of two polynomials as follows: H(z) = Y (z)X(z) = M 1X k=0 bkz k N 1X k=0 akz k (1.6) Coe cients ak and bk determine the location of the poles and zeros respectively. One of the main advantages of IIR lters...
RAPID COMMUNICATIONS PHYSICAL REVIEW B 85, 020101(R) (2012)
Wu, Junqiao
2012-01-01T23:59:59.000Z
of the insulating phases of VO2 near the metal-insulator transition Joanna M. Atkin, Samuel Berweger, Emily K distorted variant of the M1 monoclinic phase, while a discontinuous transition into the M2 phase occurs from T insulating phases and their transitions induced by temperature or strain. The triclinic phase is found
Comparison of QM-Only and QM/MM Models for the Mechanism of Tungsten-Dependent Acetylene Hydratase
Liao, Rongzhen
Comparison of QM-Only and QM/MM Models for the Mechanism of Tungsten-Dependent Acetylene Hydratase-only and QM/MM approaches for the modeling of enzymatic reactions. For this purpose, we present a QM/MM case of the previously suggested one-water attack mechanism. The QM/MM calculations with the minimal QM region M1 (32
Spatial and Temporal Distribution of Desiccation Cracks in Shrink-Swell Soils
Neely, Haly Lury
2014-04-17T23:59:59.000Z
shrinkage by using a single borehole for all vertical soil movement and water content measurements. Then measurements of soil layer thickness and water content were made for seven soils with varying COLE values, from 0.01 to 0.17 m m^(-1). Soil crack volume...
Einstein manifolds with convex boundaries JeanMarc Schlenker \\Lambda
Schlenker, Jean-Marc
Einstein manifolds with convex boundaries JeanÂMarc Schlenker \\Lambda February 2, 1999 Abstract Let (M; @M) be a compact m+1Âmanifold with boundary with an Einstein metric g 0 , with ric g0 = \\Gammamg metric on @M . Then any metric close enough to h 0 is induced on @M by an Einstein metric g with ric g
Einstein manifolds with convex boundaries Jean-Marc Schlenker*
Schlenker, Jean-Marc
Einstein manifolds with convex boundaries Jean Let (M, @M) be a compact m+1-manifold with boundary with an Einstein me* *tric g0, with ricg0 be the induced metric on @M. Then any metric close e* *nough to h0 is induced on @M by an Einstein metric g
On the closedness of the linear image of a closed convex cone. Part I
A n al. O pt i m. ,1R :30) 3 - 3 1 3 ,1 141 6 . [3 ] G.P . ( A R K R . The lattice of faces of a finite dimensional cone. L ine ar Alg e bra a n d i ts Appl. , : 1 -5S 2,1 1 3.
applications of manure (M1, M2), sewage biosolids (B1, B2), or fertilizer only con- trol (F1, F2), although, B2, and F1. Percolate sodium was elevat- ed on all M and B fields and sulfur was greatest at M2, B1, and Professor, Department of Biological and Envi- ronmental Engineering, Cornell University, Riley-Robb Hall
People's Physics Book 3e A-1 Appendix A: Answers to Selected Problems
California at Santa Cruz, University of
. f1= µkm1gcos; f2 = µkm2gcos 36c. Ma 36d TA= (m1 + m2) (a + µcos) and TB = m2a + µm2cos 36e. Solve. 5700 N 32d. Friction between the tires and the ground 32e. Fuel, engine, or equal and opposite reaction
On the Riemann Problem for a Hyperbolic TwoPhase D. Zeidan a,# , E. Toro b and A. Slaouti c
. Slaouti c a Department of Computing and Mathematics Manchester Metropolitan University, Manchester M1 5GD is hyperbolic, Godunovtype numerical methods for the model can be employed using locally approximate analytical accuracy as achieved using MUSCLHancock and WAF [3, 4] schemes. The numerical results for twophase shock
On the Riemann Problem for a Hyperbolic Two-Phase D. Zeidana,
a Department of Computing and Mathematics Manchester Metropolitan University, Manchester M1 5GD, UK b is hyperbolic, Godunov-type numerical methods for the model can be employed using locally approximate analytical accuracy as achieved using MUSCL-Hancock and WAF [3, 4] schemes. The numerical results for two-phase shock
SUB-RIEMANNIAN CALCULUS ON HYPERSURFACES IN ...
2006-08-23T23:59:59.000Z
Aug 23, 2006 ... 27. 10. Sub-Riemannian calculus on hypersurfaces. 36. 11. Tangential ..... For simplicity, we set m = m1, k = m2, and let. (2.11). {e1, ... , em} ..... Let G be a Carnot group and denote by Hs the s-dimensional Hausdorff measure.
Kastner, J. H.
We explore the possibility that GSC 07396-00759 (spectral type M1e) is a widely separated (~2[' over .]82, or projected separation ~12,350 AU) companion to the "old" (age ~12 Myr) classical T Tauri binary system V4046 Sgr ...
APS-DPP 11/07 Alfvn Instabilities Driven by Energetic
Field in the LAPD Periodic variation in B Periodic variation in vA Periodic variation in index of refraction N Frequency gap that is proportional to N #12;APS-DPP 11/07 Periodic index of refraction in an actual stellarator Spong, Phys. Plasmas 10 (2003) 3217 BAE "beta" compression TAE "toroidicity" m & m+1
Short, Daniel
Pollution in the Groundwater of Anar Plain Dehghani, M.1* , Abbasnejad, A.2 1- M.Sc. Of Environmental in the groundwater of Anar Plain. Anar plain is located in southeast part of Iran (west of Rafsanjan plain) between create the groundwater aquifer of the Anar plain. The huge recharging alluvial fans are located
Electric field and ionization-gradient effects on inertial-confinement-fusion implosions.1088/0741-3335/51/12/124048 Electric field and ionization-gradient effects on inertial-confinement-fusion implosions P A Amendt1 , J L-generated electric fields (108 109 V m-1 ) in direct-drive, inertial-confinement-fusion capsules has been reported
Generalised RudinShapiro Constructions Matthew G. Parker 1
Parker, Matthew Geoffrey
toAveragePowerRatio (PAPR) # 2.0 for its onedimensional continuous Discrete Fourier Transform (DFT) spec trum. Davis have PAPR # 2.0 under all unitary transforms whose rows are unimodular linear (Linear Unimodular , 1 # n # #, F1m = {(0, #) # (0, 2#) # (0, 4#) # . . . # (0, 2 m-1 #), mod n 1 # n # #, 0 # #
Generalised Rudin-Shapiro Constructions Matthew G. Parker 1
Parker, Matthew Geoffrey
-to-Average-Power-Ratio (PAPR) 2.0 for its one-dimensional continuous Discrete Fourier Transform (DFT) spec- trum. Davis have PAPR 2.0 under all unitary transforms whose rows are unimodular linear (Linear Unimodular Unitary all alphabets, Zn, 1 n , F1m = {(0, ) (0, 2) (0, 4) . . . (0, 2m-1), mod n 1 n , 0
Jackson, Robert B.
South American grasslands Altesor, A.1*; Piñeiro, G.2,4; Lezama, F.1,5; Jackson, R.B.3,6; Sarasola, M.1-mail jackson@duke.edu; 7E-mail sarasola@fcien.edu.uy; 8E-mail paruelo@agro.uba.ar; *Corresponding author; Fax
Nutrient Management in North Deanna L. Osmond, NCSU, Dept. Soil Science
Nutrient Management in North Carolina Deanna L. Osmond, NCSU, Dept. Soil Science Carroll Pierce, NC Carolina 43 M Turkeys $ 452 M #1 US 712 M Broilers $ 1.7 B #4 US 9.6 M Swine $ 1.7 B #2 US #12;Crop Agriculture in North Carolina Tobacco $ 719 M Cotton $ 254 M Soybeans $185 M Corn $184 M #12;Crop Production
Low Power and Low Leakage Implementation of RNS FIR Filters
Nannarelli, Alberto
, Italy Dept. of Informatics & Math. Modelling, Technical University of Denmark, Kongens Lyngby, Denmark of the energy consumed a few years ago. With the technology scaling, and the increased transistor's leakage due integers {m1, m2, . . . , mP } . The dynamic range of the system is given by the product of all the moduli
Popovych, Roman
-MannÂOkubo (GMO) one, that is, mN +m = 3 2 m + 1 2m. On the contrary, the spectrum generating (or dynamical between isomultilplets (breaking of SU(3) to SU(2)), instead of the standard GMO mass relation
Kobilka, David William
1999-01-01T23:59:59.000Z
0 Og ~ 040 ~ 065 ' 063 ppm 200m, 500m 1 Oppm ru ~ 073 Oo, ~ 060 ~ 098 BPPO m 2' 2' Fig. 9. Core locations in relation to Damuth's (1994) structural provinces. 2' 8 o 3 55pp c 83 3 + + + Niger Delta porn 200m sppm Scale...
Radar Chart: Scanning for Satisfactory QoE in QoS Dimensions
Chen, Sheng-Wei
, MOS can be estimated from objective, automated methods like PESQ [3] to avoid the personnel cost, ..., n} as in QoE = f(M1, M2, M3, ..., Mn) if everything including the production level of equipments of line charts, box plots, histograms, scatter graphs, etc. to establish their arguments. It is therefore
On the Fundamental Feedback-vs-Performance Tradeoff over the MISO-BC with Imperfect and
Gesbert, David
On the Fundamental Feedback-vs-Performance Tradeoff over the MISO-BC with Imperfect and Delayed--This work considers the multiuser multiple-input single-output (MISO) broadcast channel (BC), where. Specifically, this work provides a novel DoF region outer bound for the general K- user M ×1 MISO BC
Zwier, Timothy S.
Resonant ion-dip infrared spectroscopy of benzene(methanol)m clusters with m 16 R. Nathaniel bonding between benzene and methanol. The m 2 spectrum features two strong transitions at 3506 and 3605 cm in the absence of benzene, is redshifted by 76 cm 1 due to a strengthened hydrogen bond. In benzene CH3OH 3
A PERFORMER'S ANALYSIS OF SELECTED JAZZ WORKS FOR SAXOPHONE QUARTET
Spaeth, Carl Thomas
2014-05-31T23:59:59.000Z
– Mintzer, Three Pieces for Saxophone Quartet, “Swingin’,” soprano part, mm. 57-64 ........... 7 Example 3 - Piano reduction of Mintzer Movement 1, m. 1 ......................................................................... 9 Example 4 - Mintzer, Three... Pieces for Saxophone Quartet, “Swingin’,” soprano part, mm. 13-14 ............ 9 Example 5 - Mintzer, Three Pieces for Saxophone Quartet, “Softly,” alto part, m. 36 .............................. 11 Example 6 - Mintzer, Three Pieces for Saxophone...
ACUTE LEUKEMIAS ACUTE MYELOGENOUS
9/16/2013 1 ACUTE LEUKEMIAS ACUTE MYELOGENOUS LEUKEMIA Malignant neoplastic proliferation granules #12;9/16/2013 3 AML-MO Acute Myeloblastic Leukemia Myeloblasts without granules Negative reactions with Cytochemical Stains CD13, CD33, CD 34 AML-M1 Acute Myeloblastic Leukemia with Minimal
A Hand-held, PDA Based System for Seabird Data Collection During Cetacean Surveys and C. Saylan1
A Hand-held, PDA Based System for Seabird Data Collection During Cetacean Surveys Bearzi M.1 and C involving direct entry of data by seabird observers using a hand-held, pen-based com- puter or PDA (Personal allow to record an ever- increasing number of complex and accurate field data at sea but information
Geosci. Model Dev., 6, 687720, 2013 www.geosci-model-dev.net/6/687/2013/
Drange, Helge
Access The Cryosphere OpenAccess The Norwegian Earth System Model, NorESM1-M Part 1: Description and basic evaluation- ter's Earth System Model, named NorESM1-M, is presented. The NorESM family of models are based with NorESM1-M. 1 Introduction In the following, the Norwegian Earth System Model (NorESM) is presented
Model for J/psi absorption in hadronic matter
Lin, ZW; Ko, Che Ming.
2000-01-01T23:59:59.000Z
M 1inlD e2ne3l , ~14! with 034903- M 1anl52gpDD*gcDD~22p11p3!l 3S 1 t2mD 2 D ~p12p31p4!n, M 1bnl5gpDD*gcD*D*~2p12p4!aS 1 u2mD* 2 D 3F gab2 ~p12p4!a~p12p4!b mD* 2 G 3@~2p22p3!bgnl1~2p11p21p4!lgbn 1~p11p32p4!ngbl# , M 1cnl52gpc...- tions for J/c absorption by p and r mesons are then evalu- ated. The amplitudes for the coherent sum of individual dia- grams are checked to ensure that the hadronic currentis conserved in the limit of zero vector meson masses. We then show in Sec...
NOMENCLATURE (Journal of Heat Transfer, Vol. 121, No. 4. pp 770-773, November 1999)
NOMENCLATURE (Journal of Heat Transfer, Vol. 121, No. 4. pp 770-773, November 1999) QUANTITY SYMBOL (constant v or p) molar (constant v or p) ratio cp/cv C pcvc , pcvc , J/K J/kg K J/kmol K Heat Transfer COHERENT SI UNIT Absorptivity (radiation) Absorption Coefficient (radiation) m-1 Activation Energy
In SIAM J. Numer. Anal., 35 : 1998, 376-392. FINITE ELEMENT ANALYSIS OF MICROSTRUCTURE FOR THE
Luskin, Mitchell
-convex and is minimized on a set of deformation gradients SO3U1 ::: SO3UM for M 1; where SO3 is the set of proper rotations, that is, SO3 = Q 2 R33 : QT = Q,1 and detQ = 1 ; where R33 is the set of all 3 3 real matrices
Epstein, Irving R.
with rate constant k = 0.025 M-1 s-1 . With HOS2O3 - , HSO3 - /SO3 2- , S3O6 2- , S4O6 2- , and S5O6 2 in the H2O2-S2O3 2- -SO3 2- reaction.9 This system displays oscillatory dynamics ranging from simple
METRISCHE RUIMTEN EN CONTINUE AFBEELDINGEN aanvullend materiaal voor het college Analyse 1
Hulshof, Joost
onderscheiden twee gevallen. (i) M elk natuurlijk getal n een xn A, zodat f(xn) > M - 1 n . (ii) M = +. Dan bestaat er voor elk natuurlijk getal n een xn A, zodat f(xn) > n. In beide, of "Principles of Mathematical Analysis" van W. Rudin (McGraw Hill 1964). Voor meer algemene metrische (en
Hitchcock, Adam P.
of Chemistry & BIMR, McMaster University, Hamilton, Ontario L8S 4M1, Canada Received September 20, 2000 display matrices containing dis- persed phases that respond to applied electric fields,1 structural epoxy (STXM)24-27 at the Advanced Light Source (ALS) used in this work provides images with better than 100 nm
A Joint Model for Quotation Attribution and Coreference Resolution Mariana S. C. Almeida
Murphy, Robert F.
. Almeida Andr´e F. T. Martins Priberam Labs, Alameda D. Afonso Henriques, 41, 2o , 1000-123 Lisboa- spective, it will be of little use without a corefer- ence system that correctly resolves the anaphora with subscripts some of the mentions: (a) Rivals carp at "the principle of [Pilson]M1 ," as [NBC's Arthur Watson
. Almeida AndrÂ´e F. T. Martins Priberam Labs, Alameda D. Afonso Henriques, 41, 2o , 1000-123 Lisboa- spective, it will be of little use without a corefer- ence system that correctly resolves the anaphora with subscripts some of the mentions: (a) Rivals carp at "the principle of [Pilson]M1 ," as [NBC's Arthur Watson
Kenmerk: EWI05/DWMP/t13/dh Tentamen Deterministische Modellen in de OR
Al Hanbali, Ahmad
) Carco produceert auto's en trucks. Iedere auto geeft 300 ¤winst en iedere truck 400 ¤. De resources die.000000 0.000000 X2 27.599998 0.000000 M1 98.000000 0.000000 Row Slack or surplus Dual prices 2) 0
UW-Milwaukee Strategic Planning Core Team
Saldin, Dilano
UW-Milwaukee Strategic Planning Core Team MINUTES Wednesday, February 13, 2013 Lubar Hall, N440, 9 a.m. 1. Welcome 2. Finalized Thematic Team memberships Thematic Team members were identified with the student association to identify potential students to serve on the Thematic teams. 3. Updates
UW-Milwaukee Strategic Planning Core Team
Saldin, Dilano
UW-Milwaukee Strategic Planning Core Team Minutes Tuesday, December 18, 2012 Regents Room, Chapman Hall, 8-10 a.m. 1. Welcome and meeting objectives 2. Core Team Suggested Guidelines ("Ground Rules") a. Communication (within team and with across campus and others) Input is always welcomed Open communication
recommendations. Up-to-date information about many topics can be obtained from your local Extension office. Grape of Defects for Michig~ u.s. G,Ft) --------------------------~~~~~~tM~I;C~H~IG~A~N~N~01.11~A~NNnD----,M~1C
Journal of Elasticity 75: 187192, 2004. 2004 Kluwer Academic Publishers. Printed in the Netherlands.
Barber, James R.
. The Gravitational Potential The basic law of Newtonian gravitation states that two particles of mass m1, m2 in the Netherlands. 187 Stresses in a Half Space Due to Newtonian Gravitation J.R. BARBER Department of Mechanical z > 0 with a traction-free surface experiencing gravitational attraction to an arbitrarily shaped
Mitchell, Nicole Jean
2013-08-30T23:59:59.000Z
........................................................................................................77 2.2.2 Participant recruitment, questionnaire, and data collection ...........................77 2.2.3 Determination of AFM1 in urine....................................................................78 2... 2.3.1 Aflatoxin M1 concentration in urine ..............................................................79 2.3.2 Sociodemographic characteristics .................................................................80 2.3.3 Health...
Lyapunov functions for time varying systems satisfying generalized conditions of Matrosov
Nesic, Dragan
Lyapunov functions for time varying systems satisfying generalized conditions of Matrosov theorem F a weak Lyapunov function (positive definite, decrescent, with negative semi- definite derivative along of the Lyapunov function is zero [M1]. Recently, sev- eral generalizations of the classical Matrosov theorem
Elaborazione dei segnali nei sistemi di controllo Identificazione dei Modelli e Analisi dei dati
Chisci, Luigi
) determinare l'intervallo di confidenza al 95% della variabile Y ; (c) determinare la regione di confidenza al , 13 4 -3 4 3 -3 4 3 7 4 (a) determinare l'intervallo di confidenza al 95% della variabile X; (b) indipendenti fra loro e dai coefficienti 0, 1, . . . , m, 1, . . . , n che si vogliono determinare. (a) Posto x
Stansifer, Ryan
of motion Newton's law of universal gravitation Newton DelaunayLagrangeKepler EulerBernoulli Poincaré #12;11 Force Between Two Bodies Newton's law of universal gravitation. F = G m1 m2 / r 2. Direction of forceDraw.point(r.cartesian(0), r.cartesian(1)); } } #12;13 Force Between Two Bodies Newton's law of universal gravitation. F
Fournier, John J.F.
the definition shortly. These notes are intended to provide a lightning fast introduction to integration . Definition M.1 Let n 1 be an integer. (a) Let a IRn and > 0. The open ball of radius centred on a is B is open if and only if it is a union of open balls. (c) Fix any W IRn . A subset V W is said
Ho, David
Comparison of SF6 and Fluorescein as Tracers for Measuring Transport Processes in a Large Tidal SF6 as tracers of advection and longitudinal dispersion from a dual tracer release experiment of SF6 were injected into the Hudson River at an averaged depth of 9.5 m, 1 m above the bottom, near
Microsoft Word - Report Cover.doc
Broader source: Energy.gov (indexed) [DOE]
Defense Related High Risk Property OAS-M-08-06 April 2008 Departtment sf Energy VVashlnyon, u i 5 6 5 A p r i l 2 4 , 2008 M1:MOIIANDUM FOR l f 1 E 4SSOCIA'PE ADMIlVlSTRATOR...
Erratum (astro-ph/0510172): Robust Limits on Lorentz Violation from Gamma-Ray Bursts
John Ellis; N. E. Mavromatos; D. V. Nanopoulos; A. S. Sakharov; E. K. G. Sarkisyan
2007-12-17T23:59:59.000Z
We correct the fitting formula used in refs. [1,2] to obtain a robust limit on a violation of Lorentz invariance that depends linearly on the photon energy. The correction leads to a slight increase of the limit on the scale of the violation, to M > 1.4 x 10^{16} GeV.
Stress relief cracking in creep resisting low alloy ferritic steels.
Tait, Robert Andrew
1976-10-26T23:59:59.000Z
in the direct immobilisation of s lip dislocations or by the provision of a high equilibrium solute content. During the 1970's further measurements of carbide morphology and mechanisms of nucleation and growth have been made . 27 28 using Field Ion M1...
Bahrami, Majid
it without permission. 6-35 6-52 Steam expands in a turbine. The change in kinetic energy, the power output, and the turbine inlet area are to be determined. Assumptions 1 This is a steady-flow process since m m m1 2 . We take the turbine as the system, which is a control volume since mass crosses
Complete Electric Dipole Response and the Neutron Skin in 208 I. Poltoratska,2
Ponomarev, Vladimir
of the Witwatersrand, Johannesburg 2050, South Africa 7 Department of Physics, Kyushu University, Fukuoka 812Themba LABS, Somerset West 7129, South Africa 14 ECT*, Villa Tambosi, I-38123, Villazzano (Trento), Italy 15) and spin magnetic dipole (M1) modes in nuclei over a broad excitation energy range to test up
US Army Corps of Engineers
Uranium-238, Thorium-230, and Radium-226 are the predominant radioactive contaminents on Formerly of time. Uranium-238 decays by alpha emission into thorium-234, which itself decays by beta emission-life* thorium-234 24.1 days protactinium-234m 1.17 minutes uranium-234 244,000 years radon-222 3.82 days
Schuck, Götz
-stretching region of synthetic staurolites MONIKA KOCH-MÜLLER1 , KLAUS LANGER1 , HARALD BEHRENS2 , GOTZ SCHUCK1 3_05 [M4] bauer spectroscopy. Dutrow (1991) experimen- Al2 D2 [M3] Al,6 [M1 'M2] Si8 [T,] O48H2
Migration and Final Location of Hot Super Earths in the Presence of Gas Giants
Ji-Lin Zhou; Douglas N. C. Lin
2008-02-01T23:59:59.000Z
Based on the conventional sequential-accretion paradigm, we have proposed that, during the migration of first-born gas giants outside the orbits of planetary embryos, super Earth planets will form inside the 2:1 resonance location by sweeping of mean motion resonances (Zhou et al. 2005). In this paper, we study the subsequent evolution of a super Earth (m_1) under the effects of tidal dissipation and perturbation from a first-born gas giant (m_2) in an outside orbit. Secular perturbation and mean motion resonances (especially 2:1 and 5:2 resonances) between m_1 and m_2 excite the eccentricity of m_1, which causes the migration of m_1 and results in a hot super Earth. The calculated final location of the hot super Earth is independent of the tidal energy dissipation factor Q'. The study of migration history of a Hot Super Earth is useful to reveal its Q' value and to predict its final location in the presence of one or more hot gas giants. When this investigation is applied to the GJ876 system, it correctly reproduces the observed location of GJ876d around 0.02AU.
Liu UCD Phy9B 07 9 35-4. Interference in Thin Films
Yoo, S. J. Ben
change at the interface: (if reflects off an optically denser material) Normal incidence 2t =m, no phase shift 2t = m, m=0, 1, 2, 3... Destructive reflection 2t = (m+1/2), m=0, 1, 2, 3... : Light wavelength in the film : Light wavelength in air = /n #12;Liu UCD Phy9B 07 10 Phase Shift at Interface When
Reaching towards higher masses of supersymmetric particles
Olsen, Agnethe Seim
This thesis presents an optimisation of the search for SUSY in final states with one tau lepton, jets and large missing transverse energy. The search is performed in proton-proton collisions at sqrt(s) = 8TeV corresponding to an integrated luminosity of 20.3 fb^(?1). The SUSY model considered is mSUGRA with parameter values: m0 and m1/2 are treated as grid parameters, A0 = ?2m0, tan beta = 30 and mu>0. The event selection is optimised for maximal sensitivity to mSUGRA in the low m0, high m1/2 region of the mass plane. The result of the optimised analysis is interpreted in the mSUGRA model and a limit in the (m0, m1/2) plane is obtained. Values of m1/2 up to 640 GeV are excluded for low m0 and 300 GeV for high m0 ( 2000 GeV < m0 < 5400 GeV).
Boundary control laws and observer design for convective, turbulent and magnetohydrodynamic flows
Vazquez Valenzuela, Rafael
2006-01-01T23:59:59.000Z
? 3 , . . . , ? n ) = ? k nx (x, x, ? 2 , ? 3 , . . . , ?=1 T n?m+1 (x,?) ˆ n ˆ n k nx (x, ? 1 )d ? 1 n ? m m(n ? m ?u(x) n=1 n=1 T n (1,?) ˆ n k nx (x, ? 1 ) T n (x,?) ˆ n k n+
Kevin Kiesler 1/7/2014 http://www.cstl.nist.gov/biotech/strbase/pub_pres/Vallone-NGS-SWGDAM-Jan2014://www.cstl.nist.gov/biotech/strbase/pub_pres/Vallone-NGS-SWGDAM-Jan2014.pdf 2 Applied Genetics Platform 316 6 M 1 Gb 318 11 M 2 Gb #12;Kevin Kiesler 1/7/2014 http://www.cstl.nist.gov/biotech
Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)
START UP 2532 -Terry 2532 -Terry 2532 -Terry 2532 -Terry 2532 -Terry START UP START UP Biotech 2514A-DeWitt 2514A-DeWitt 2514A-DeWitt 6-2 Wig-Exxon START UP START UP X-S12M1...
Takano, Yoshihide
optics and wave theory Yoshihide Takano and Masayuki Tanaka The phase matrix and several quantities of ray optics, which includes geometrical reflection and refraction plus Fraunhofer diffraction optics approximations for m = 1.31-O.Oi and 1.31-0.li. Results by these methods approach oneanother
Fax +41 61 306 12 34 E-Mail karger@karger.ch
Nizet, Victor
, Faculty of Pharmacy, Cairo University, Cairo, Egypt; e VA Medical Center and f Molecular Resource Center M types is proposed. The vast majority of GAS infection is benign. Nonetheless, many divergent M types possess limited capacity to cause invasive infection. M1T1 GAS readily switch to a covRS mutant
(kf k 0 + hjf j 1) Cjfj 4h4: (1.7.21). It is a simple consequence of compactness that the conclusion of the theorem re-. mains valid if. max. 1 i N 1. hi. hi+1. 1. M < 1:.
Yao, Jianping
-Coded Microwave Waveform With Ultrawide Frequency Tunable Range Liang Gao, Student Member, IEEE, Xiangfei Chen-coded microwave waveform with ultrawide frequency tunable range using two polarization modulators (Pol signal with a switching voltage of V to PolM1, a phase-coded microwave waveform is generated. The key
GeV electron beams from a centimetre-scale accelerator
to synchrotron radiation facilities and free-electron lasers, and as modules for high-energy particle physics. Radiofrequency-based accelerators are limited to relatively low accelerating fields (10-50 MV m-1 ), requiring tens to hundreds of metres to reach the multi-GeV beam energies needed to drive radiation sources
PROPAGATION OF ELF WAVES GENERATED BY AN HF IONOSPHERIC HEATER IN THE EARTH'S PLASMA
(HAARP) transmitter array is used to generate ELF waves. The HAARP array generates ELF waves by heating generated by HAARP were detected by the DEMETER satellite at an altitude of 670 km. In additionV·m-1 at 2 kHz. In Region 2, which can extend up to 300 km laterally from HAARP, it is believed
a .nlD. P X m. anI. _ O m r. e m mam 3_83_51_24_7.5_8 .w hm EN __ __ __. ) w. 5 Sm . _ E E f . 6 7 w 0 A C D E. 1T6 <__$ m @m. \\1/ Wm. /0\\ __ m y w .. m f w e ...
Nica, N.; Hardy, John C.; Iacob, VE; Montague, JR; Trzhaskovskaya, MB.
2005-01-01T23:59:59.000Z
We have measured the total intensity of K x rays relative to 129.4-keV gamma rays from decay of the second excited state in Ir-191. This (M1+E2) transition was observed following the beta decay of 15.4-d Os-191. Our measured ...
Tailoring the Thermoelectric Behavior of Electrically Conductive Polymer Composites
Moriarty, Gregory P.
2013-05-21T23:59:59.000Z
the promise of fully organic composites as thermoelectric materials. This combination of CNT and stabilizer produced metallic electrical conductivity (200,000 S m-1) and power factors (S2?) within an order of magnitude of commonly used semiconductors (~400 ?W...
Harmon, Julie P.
, single-walled carbon nanotube (SWNT)±polymer composites have received much attention due to their im is at least 10±6 S m±1 . Composites of SWNTs have been proposed as a possible way to increase the conductivity of the SWNT±PMMA composite. Structural changes of both SWNTs and polymers resulting from their interactions
FROM REPRESENTATION THEORY TO HOMOTOPY GROUPS ...
Then v-11ss2m(X; p) = (coker(OEm ))# and v-11ss2m-1(X; p) = (ker(OEm ))#; where .... 24 D. DAVIS Now let P = 24k, and write w4 as a unit times 54 times the
Leucobacter salsicius sp. nov., from a salt-fermented food
Bae, Jin-Woo
Leucobacter salsicius sp. nov., from a salt- fermented food Ji-Hyun Yun,1 Seong Woon Roh,1,2 Min, Daejeon 305-806, Republic of Korea Strain M1-8T was isolated from jeotgal, a Korean salt-fermented food contained 2,4-diaminobutyric acid, glutamic acid, alanine, glycine and c-aminobutyric acid. The major
:194:698 Research Practicum 26:620:556 Organization Theory M 1:00-3:50 26:620:677 Culture & Organizations M 12 Behavior 5. 26:620:556 Organization Theory Area Requirements: Minor (2 courses) 1. 16:194:633 Mediated Comm Behavior 3. 26:620:556 Organization Theory 4. 26:620:677 Culture & Organizations 5. 16
OF A DOUBLE-DECKER FILAMENT. I. OBSERVATIONS AND INTERPRETATION Rui Liu1,2 , Bernhard Kliem3,4 , Tibor T, as inferred from three-dimensional reconstruction by combining SDO and STEREO-B observations. This "double- decker" configuration sustained for days before the upper branch erupted with a GOES-class M1.0 flare
The Party of Lincoln: How Black Republicans Have Adjusted their Campaign Appeals from 1972-2010
Postal, Andrew
2012-01-01T23:59:59.000Z
Twilley Face Tough Race Tulsa GOP Field is Impressive Goingfor Largent, Price Page D1 B1 M1 D1 C1 B1 C4 Tulsa WorldN1 Tulsa World N6 Tulsa World N1 Postal 64 Steven Largent
QUANTUM MECHANICS II Physics 342
Rosner, Jonathan L.
QUANTUM MECHANICS II Physics 342 KPTC 103 9:00 10:20 a.m. 1 Tues., Thurs. Winter Quarter 2011 quantum mechanics at the graduate level. The text for Quantum Mechanics II will be J. J. Sakurai and Jim Napolitano, Modern Quantum Mechanics, Second Edition (Addison-Wesley, San Francisco, 2011). For supplemental
Ismagilov, et al. S1 Supplementary Information for
Ismagilov, Rustem F.
. & Lakshman, S. Laminar-Flow in Rectangular Ducts - Prediction of Velocity Profiles and Friction Factor. Ind], U is flow velocity [m/s], is density of fluid [kg m-3 ], and µ is viscosity of fluid [kg m-1 s-1 ]. At a flow velocity of 5 cm/s, the calculated Re was 13. Laminar flow is present at Re
The infinite interface limit of multiple-region relaxed magnetohydrodynamics
Hudson, Stuart
with mobile dust grains Phys. Plasmas 20, 032102 (2013) On the formation of m=1, n=1 density snakes Phys. Plasmas 20, 032504 (2013) The effect of emissive biased limiter on the magnetohydrodynamic modes in the IR subject to AIP license or copyright; see http://pop.aip.org/about/rights_and_permissions #12;The infinite
Ohta, Shigemi
(ENSDF) database at Brookhaven) to each of the energy levels. Band Intensity The quoted value, when of Technology, Roorkee 247667, India The table presents experimental data (extracted from recent publications contains gamma-ray energies, associated level energies with spins and parities, level lifetimes, B(M1
proteinsSTRUCTURE O FUNCTION O BIOINFORMATICS On the accuracy of inferring energetic
Thirumalai, Devarajan
and Technology, University of Maryland, College Park, Maryland 20742 2 Department of Chemistry and Biochemistry,11 Comparison of the free energy changes in the protein with simultaneous mutations at two sites m1 and m2-based methods because a larger database of evolved protein with related function can be simultane- ously
A. M. Sukhovoj; V. A. Khitrov
2009-06-16T23:59:59.000Z
The re-analysis of the published experimental data on the primary gamma-transition intensities following neutron capture in different groups of neutron resonances in $^{156,158}$Gd has been performed. There are determined the most probable values of sum of E1 and M1 primary transitions, numbers of excited by them levels of both parities, ratios of radiative strength functions k(M1)/k(E1), dispersions of deviations of random values of intensities from the average and ratios of mean intensities of primary transitions to levels J=5/2 with respect to analogous data for J=1/2 and 3/2 (capture of the 24 keV neutrons) in narrow excitation energy intervals. All the data on level density and sums of radiative strength functions confirm the presence of clearly expressed step-like structure in level density below 3 MeV and general trend in change in strength functions as changing primary gamma-transition energy. Variations of distribution dispersions and, especially, ratio k(M1)/k(E1) (or $k(E1)/k(M1)$) at changing excitation energy point to strong change in structure of these nuclei above 1.0-1.5 MeV.
Water Infiltration and Permeability of Selected Urban Soils as Affected by Salinity and Sodicity
Miyamoto, S.
2012-10-05T23:59:59.000Z
water (EC of 1.4 and 2.2 dS m-1 and SAR of 6 and 11) were applied twice a week at 1.7 cm per application for a total of 27 irrigation events using 46 cm of water. No significant effect of water quality was detected in Delnorte gravelly loam (Paleorthid...
APPLIED THERMAL ENGINEERING Manuscript Draft
Paris-Sud XI, Université de
with PCM integrated in a air ventilation system · Laboratory experiment to analyze the heat exchanger of a PCM to air heat exchanger storage system for building ventilation application Labat M.1,3 , Virgone J deviation difference Subscripts A air HVAC Heating Ventilation Air Conditioning Meas measured PCM phase
High frequency and high dynamic range continuous time filters
Lewinski Komincz, Artur Juliusz
2007-09-17T23:59:59.000Z
T TSGdssat =??= (2.9) For a simplified distortion analysis, the above expression can be expanded in taylor series around v in =0, such that: ? = + + ?= 0 12 )12( n n innMo vGi (2.10) where, 18 1)1(2 2 ?? = j dssat j m Mj V g G (2.11) G M1...
Brown, Michael R.
2015-01-01T23:59:59.000Z
drift region. This provides unique laboratory conditions approaching that in the solar wind speed is on the order of the local sound speed (M 1), so flow energy density is comparable to thermal energy density; and the ratio of thermal to magnetic pressure is of order unity (plasma 1) so thermal
INTERACTIONS OF POINT DEFECTS WITH BORON AND ARSENIC PRECIPITATES
Dunham, Scott
]. The price for this re duction in the number of variables is that two nonlinear equations have to be solved tables are computed for the quantities which depend on the distribution, in terms of m 1 =m 0 and m 2 =m 0 , and the tables used for interpolation during a simulation. The model was successfully applied
An Analysis of Deflection-Based Wormhole Routing with Virtual Channels 1
Varvarigo, Emmanouel "Manos"
their destination, because M1 resources are occupied by worms waiting for resources to become available. Virtual messages, as opposed to buffering them un- til the resources become available. As network congestion],[KoS94]), and wormhole routing ([LBB94], [LNG96]). The wormhole deflection scheme with virtual
Module Catalogue Bachelor of Science Chemistry
Schubart, Christoph
Module Catalogue Bachelor of Science Chemistry University of Regensburg 13.1.2014 The Bachelor of Science Chemistry at the University of Regensburg comprises the following modules: 1. Compulsory Courses: CHE-BSc-M 1 General Chemistry CHE-BSc-M 2 Mathematics CHE-BSc-M 3 Physics CHE-BSc-M 4 Chemistry
On Advection by Hermite Methods Daniel Appelo
Appelö, Daniel
flows [2, 4, 3]. Our goal here is to examine the properties of Hermite methods for piece- wise smooth-of-freedom are the coefficients of a tensor-product Taylor polynomial of degree m in each coordinate has order 2m + 1 convergence The numerical simulation of waves presents numerous challenges. On the one hand, it may be necessary
Transition between Spherical RFP and Spherical Torus during the Helicity Injection Process
Washington at Seattle, University of
(major radius R = 0.30 m, minor radius a = 0.24 m, aspect ratio #12;22 Gas Puff Valves (4) Insulator, must pass through the m=1/n=1 rational barrier, i.e. the Kruskal-Shafranov limit. It is thus
2011 GSA Annual Meeting in Minneapolis (912 October 2011) Paper No. 243-18
COMPOSITIONS OF CR-SPINEL FROM SERPENTINIZED FOREARC MANTLE PERIDOTITES: INSIGHTS ON GEOCHEMICAL PROCESSES DURING MELT EXTRACTION AND METAMORPHISM SAUMUR, B.-M.1 , HATTORI, Kéiko H.1 , STERN, Fabio1 , and JACKSON8, Canada Cr-spinel is a useful petrological indicator mineral as it is resistant to alteration
Computer-aided modeling of the binding sites of anti-fluorescein antibodies
Harris, Jonathan S
1996-01-01T23:59:59.000Z
quenching studies determined that four of the antibodies (FL43.1, FL43.4, FL43.6 and FL55.3) had Kd values (dissociation constants) in the nanomolar range and that the fifth antibody (FL43.11) had a significantly lower Kd in the 10-7M-1 range. Fluorescence...
Molecular Gas in NUclei of GAlaxies (NUGA) I.The counter-rotating LINER NGC4826
S. Garcia-Burillo; F. Combes; L. K. Hunt; F. Boone; A. J. Baker; L. J. Tacconi; A. Eckart; R. Neri; S. Leon; E. Schinnerer; P. Englmaier
2003-06-06T23:59:59.000Z
We present new high-resolution observations of the nucleus of the counter-rotating LINER NGC4826, made in the J=1-0 and J=2-1 lines of 12CO with the IRAM Plateau de Bure mm-interferometer(PdBI).The CO maps, which achieve 0.8''(16pc) resolution in the 2-1 line, fully resolve an inner molecular gas disk which is truncated at an outer radius of 700pc. The total molecular gas mass is distributed in a lopsided nuclear disk of 40pc radius and two one-arm spirals, which develop at different radii in the disk. The distribution and kinematics of molecular gas in the inner 1kpc of NGC4826 show the prevalence of different types of m=1 perturbations in the gas. Although dominated by rotation, the gas kinematics are perturbed by streaming motions related to the m=1 instabilities. The non-circular motions associated with the inner m=1 perturbations agree qualitatively with the pattern expected for a trailing wave developed outside corotation ('fast' wave). In contrast, the streaming motions in the outer m=1 spiral are better explained by a 'slow' wave. A paradoxical consequence is that the inner m=1 perturbations would not favour AGN feeding. An independent confirmation that the AGN is not being generously fueled at present is found in the low values of the gravitational torques exerted by the stellar potential for R<530pc. The distribution of star formation in the disk of NGC4826 is also strongly asymmetrical. Massive star formation is still vigorous, fed by the significant molecular gas reservoir at R<700pc. There is supporting evidence for a recent large mass inflow episode in NGC4826. These observations have been made in the context of the NUclei of GAlaxies (NUGA) project, aimed at the study of the different mechanisms for gas fueling of AGN.
Hsu, Feng-Ming [Department of Oncology, National Taiwan University Hospital, National Taiwan University College of Medicine, Taipei, Taiwan (China); Cancer Research Center, National Taiwan University College of Medicine, Taipei, Taiwan (China); Graduate Institute of Biomedical Electronics and Bioinformatics, National Taiwan University, Taipei, Taiwan (China); Lee, Jang-Ming; Huang, Pei-Ming [Department of Surgery, National Taiwan University Hospital, National Taiwan University College of Medicine, Taipei, Taiwan (China); Lin, Chia-Chi; Hsu, Chih-Hung; Tsai, Yu-Chieh [Department of Oncology, National Taiwan University Hospital, National Taiwan University College of Medicine, Taipei, Taiwan (China); Cancer Research Center, National Taiwan University College of Medicine, Taipei, Taiwan (China); Lee, Yung-Chie [Department of Surgery, National Taiwan University Hospital, National Taiwan University College of Medicine, Taipei, Taiwan (China); Chia-Hsien Cheng, Jason, E-mail: jasoncheng@ntu.edu.tw [Department of Oncology, National Taiwan University Hospital, National Taiwan University College of Medicine, Taipei, Taiwan (China); Cancer Research Center, National Taiwan University College of Medicine, Taipei, Taiwan (China); Graduate Institute of Oncology, National Taiwan University College of Medicine, Taipei, Taiwan (China); Graduate Institute of Biomedical Electronics and Bioinformatics, National Taiwan University, Taipei, Taiwan (China)
2011-11-15T23:59:59.000Z
Purpose: To evaluate the efficacy and patterns of failure of elective nodal irradiation (ENI) in patients with esophageal squamous cell carcinoma (SCC) undergoing preoperative concurrent chemoradiation (CCRT) followed by radical surgery. Methods and Materials: We retrospectively studied 118 patients with AJCC Stage II to III esophageal SCC undergoing preoperative CCRT (median, 36 Gy), followed by radical esophagectomy. Of them, 73 patients (62%) had ENI and 45 patients (38%) had no ENI. Patients with ENI received radiotherapy to either supraclavicular (n = 54) or celiac (n = 19) lymphatics. Fifty-six patients (57%) received chemotherapy with paclitaxel plus cisplatin. The 3-year progression-free survival, overall survival, and patterns of failure were analyzed. Distant nodal recurrence was classified into M1a and M1b regions. A separate analysis using matched cases was conducted. Results: The median follow-up was 38 months. There were no differences in pathological complete response rate (p = 0.12), perioperative mortality rate (p = 0.48), or delayed Grade 3 or greater cardiopulmonary toxicities (p = 0.44), between the groups. More patients in the non-ENI group had M1a failure than in the ENI group, with 3-year rates of 11% and 3%, respectively (p = 0.05). However, the 3-year isolated distant nodal (M1a + M1b) failure rates were not different (ENI, 10%; non-ENI, 14%; p = 0.29). In multivariate analysis, pathological nodal status was the only independent prognostic factor associated with overall survival (hazard ratio = 1.78, p = 0.045). The 3-year overall survival and progression-free survival were 45% and 45%, respectively, in the ENI group, and 52% and 43%, respectively, in the non-ENI group (p = 0.31 and 0.89, respectively). Matched cases analysis did not show a statistical difference in outcomes between the groups. Conclusions: ENI reduced the M1a failure rate but was not associated with improved outcomes in patients undergoing preoperative CCRT for esophageal SCC. Pathological nodal metastasis predicted poor outcome.
2010-2035 Metropolitan Transportation Plan
Hidalgo County Metropolitan Planning Organization
2009-12-10T23:59:59.000Z
!"#"$%$!"&'$()*+,-,./*01$2+013-,+*0*/,1$4.01$ !"#$$%&'( #)( *+&,$( ! ! ! ! ! ! ! ! "##$%&'(!"! )*+,! C O U N T Y L I N E R D E UBA NKS R D W A L L A C E R D F M 2 2 2 1 S E M I N A R Y R D... F M 5 0 6 I O W A F M 4 9 0 S T A T E H W Y 1 0 7 F M 1 4 2 2 B I G 5 F M 4 9 1 D O O L I T T L E F M 6 8 1 J A R A C H I N A S R D F M 4 9 3 B R U S H L I N E F M 1 4 2 5 M I L E MI L I T A R Y H W Y F M 8 8 I N T E R N A T I...
Absolute Values of Neutrino Masses implied by the Seesaw Mechanism
Tsujimoto, H
2005-01-01T23:59:59.000Z
It is found that the seesaw mechanism not only explain the smallness of neutrino masses but also account for the large mixing angles simultaneously, once the unification of the neutrino Dirac mass matrix with that of up-quark sector is realized. We show that provided the Majorana masses have hierarchical structure as is seen in the up-quark sector, we can reduce the information about the absolute values of neutrino masses through the data set of neutrino experiments. The results for the light neutrino masses are $m_1:m_2:m_3\\approx 1:3:17$ $(m_1\\simeq m_2:m_3\\approx 1.2:1)$ in the case of normal mass spectrum (inverted mass spectrum), and the heaviest Majorana mass turns out to be $m_3^R=1\\times 10^{15}$ GeV which just corresponds to the GUT scale.
Solar cells incorporating light harvesting arrays
Lindsey, Jonathan S. (Raleigh, NC); Meyer, Gerald J. (Baltimore, MD)
2002-01-01T23:59:59.000Z
A solar cell incorporates a light harvesting array that comprises: (a) a first substrate comprising a first electrode; and (b) a layer of light harvesting rods electrically coupled to the first electrode, each of the light harvesting rods comprising a polymer of Formula I: X.sup.1.paren open-st.X.sup.m+1).sub.m (I) wherein m is at least 1, and may be from two, three or four to 20 or more; X.sup.1 is a charge separation group (and preferably a porphyrinic macrocycle, which may be one ligand of a double-decker sandwich compound) having an excited-state of energy equal to or lower than that of X.sup.2 ; and X.sup.2 through X.sup.m+1 are chromophores (and again are preferably porphyrinic macrocycles).
Nonparametric estimation of varying coefficient dynamic panel models
Cai, Zongwu; Li, Qi
2008-10-01T23:59:59.000Z
#2; m2 because the number of parameters in ~6! is m2+ However, when m1 #7; m2, the model is overidentified, and there may not exist a unique a to satisfy ~6!+ To obtain a unique a satisfy- ing ~6!, we premultiply ~6! by an m2 #3; m1 matrix Sn' , where... with Qit #1; Q~Vit ! and n #1; NT, Sn #1; 1 n #6; i#1;1 N #6; t#1;1 T QitUit' Kh~Zit #5; z!+ Then solving for a we obtain [a #1; ~Sn' Sn !#5;1Sn' Tn , (7) where Tn #1; 1 n #6; i#1;1 N #6; t#1;1 T Qit Kh~Zit #5; z!Yit + The estimator [a defined in ~7...
An application of Laplace transforms to a machine maintenance problem
Boone, James Robert
1962-01-01T23:59:59.000Z
solutions, P (t), P 1(t), and P 2 (t), it is possible to make the following statement; Theorem: For each integer k satisfying o & k & m, and k a. ) p k(s) = (k) Z (-1)' ( ) p k&, (s) j=o m-k m m-k b. ) P (t) = ( k ) ( ? ) ( ) (1-?p L t(M+X)j) ( ' k...) -u p (s) 0 1 -mk p (s) + [s+ (m-1) k + u] p (s) - 2g p (s) 0 1 2 m 0 -[(m-n+l)k]p (s)+[s+(m-n)k+nii] p (s)-[(n+1)u]p (s) = 0 n-l n n+1 -2& p 2(s)+[s+'h+(m-1)~] p 1(s) - mu p (s) -kp (s) + (s+mii)p (s) = 0 ? 0 As this system of algebraic...
On some proofs of Muntz-Szasz theorems
Smith, Lyle Ross
1970-01-01T23:59:59.000Z
) = x, k 1& n, gives pn pn G(x, . . . , x ) TT (p - p ) ~(m- p. ) 2 2 j n n 2 (p. +p. 1)~ (p. +m+1) (2~1) ~ (p. +p. +1) i '=1 2 j=l (m+p. +1) j A s imp 1 i f ica t ion shows 2 2m+ 1 j=l (m+p. +1) 2 j As a further consequence, a well... f, g ~?01) In particular, when g(x) =- 1, x, {0, 1, ' l(f, l) I & llfll which can be written 19 1 1 1 (2. 20) J ( f(x) I dx - (I I f(x) I ?) z 0 0 We now prove (2. 21) IIuntz ' s Second Theorem, Consider the system of functions { l, x 1 & p...
On the Error in the Product QR Decomposition
Van Vleck, Erik
2010-03-17T23:59:59.000Z
for sequences of matrices by ?{Vk}?k=1? = supk ?Vk?F , we have ?? ?1G(x 0 )? ? ? for G defined in (3.1) and (3.2), ? defined in (4.9), (4.10), and (4.11), x 0 = {I}?k=1, and ? given in (4.2). Proof. To determine this bound, we consider the linear system ?V = G(x... ?Vn+1?F = sup n ? 2 ? ? m?1 ? j=1 m ? i=j+1 (Vn+1) 2 ji ? ? 1/2 (4.16) ? ? 2 ? ? m?1 ? j=1 m ? i=j+1 ( ?ij |Eij | Rjj ) 2 ? ? 1/2 . 4.3. Bounds on ???1G?(x 0 ) ? I?. We next prove the following lemma to obtain the bound ? on ???1G?(x 0 )? I? given...
Cook, C. Wayne
1950-01-01T23:59:59.000Z
EM ,M?~R,M2M15J ?L, 5EM VM?,MM L? ?'CH'N '? ?O?F'A'?O! ?*?L, A~8?M35? N*1?M *1V ?L,MJ5,Y ???? M HTIFG '? C'PHGPHA ?*?M ?PHN'??CH?'P ------------------------------------------------------------------------------------------? NG??GZ '? F...---------------------------------------------------------------------- ?? ?5R7R?*5RL1 M1V IL5*1R3*7 CL2BLJR5RL1 L? 5EM ?RM5 - - ? ?? CEM2R3*7 T1*7YJRJ L? ?7*15J *1V P~5,R5RUM CL15M15 L? 5EM ? R M 5 ------------------------------------------------------ ?? P~5,R5RUM ?*7~M L? N*1?M ?L,*?M *J T??M35MV 8Y ?M?M5*5RL1 HYBM...
Partially twisted superconformal M5 brane in R-symmetry gauge field backgrounds
Bak, Dongsu
2015-01-01T23:59:59.000Z
We obtain the action for a curved superconformal abelian M5 brane with the background R-symmetry gauge field turned on. We then restrict ourselves to superconformal M5 brane on a sphere times flat Minkowski space. We choose R-symmetry SO(1,4) instead of SO(5), which enables us to partially twist on Minkowski space and replace it by some curved Lorentzian manifold. We obtain M5 brane actions on $M_{1,1} \\times S^4$ and $M_{1,2} \\times S^3$ where actions and all fields, including the background gauge field, are real. Dimensional reduction along time gives real 5d SYM actions with nonabelian generalizations.
Integrated Approach to Revamping Heat Exchangers Networks
Glass, K. E.; Dhole, V.; Wang, Y.
2002-01-01T23:59:59.000Z
Figure 4: The "new" exchanger is added to the Aspen Plus preheat train model >t, I~s..", ,r-.uFI L . ,. ---" , f2iI EI3? . (lD >?Am> -?tlD M1XERDI " i2II M1XER02 J:! f1ll fo,EW ~ "tup ~ Optlons ?6 Hel.ran Options ~ Hetren Browser 6 Geometry... Plus both model the existing preheat train using Aspen Detran models. 96 ESL-IE-02-04-12 Proceedings from the Twenty-fourth National Industrial Energy Technology Conference, Houston, TX, April 16-19, 2002 ..mlEI!lmIIl!BI_..... ~~======_-....JCf?.J9...
A variant of Marstrand's theorem for projections of cartesian products
Velázquez, Jorge Erick López
2011-01-01T23:59:59.000Z
We prove the following variant of Marstrand's theorem about projections of cartesian products of sets: Consider the space $\\Lambda_m=\\set{(t,O), t\\in\\R, O\\in SO(m)}$ with the natural measure and set $\\Lambda=\\Lambda_{m_1}\\times\\ppp\\times\\Lambda_{m_n}$. For every $\\la=(t_1,O_1,\\ppp,t_n,O_n)\\in\\Lambda$ and every $x=(x^1,\\ppp,x^n)\\in\\R^{m_1}\\times\\ppp\\times\\R^{m_n}$ we define $\\pi_\\la(x)=\\pi(t_1O_1x^1,\\ppp,t_nO_nx^n)$. Suppose that $\\pi$ is surjective and set $$\\mathfrak{m}:=\\min\\set{\\sum_{i\\in I}\\dim_H(K_i) + \\dim\\pi(\\bigoplus_{i\\in I^c}\\R^{m_i}), I\\subset\\set{1,\\ppp,n}, I\
Joint synchronization and calibration of multi-channel transform-domain charge sampling receivers
Kotte Prakasam, Pradeep
2010-07-14T23:59:59.000Z
, the expansion coe?cients become the Fourier series coe?cients, hence, the receiver is referred to as the Frequency domain (FD) receiver. In each channel, the input signal is mixed with the basis signal and integrated in a window of duration Tc seconds... that cover the entire signal block provide a total of MN coe?cients R(m;n)jM?1m=0jN?1n=0 given by, Rm;n = Z mTs+Tc mTs x(t)'?n(t)dt; (1.1) where Ts = Tc ? Tov, x(t) is the received signal, m = 0 to M ? 1 indicates the mth segment in each channel and n = 0...
Stokesian dynamic simulations and analyses of interfacial and bulk colloidal fluids
Anekal, Samartha Guha
2006-10-30T23:59:59.000Z
.................................................... 59 4.3. Potential energy profiles for the interaction of two 652 nm polystyrene (PS) colloids (? p=1055 kg/m3, ? p=-178 mV) below a glass microscope slide (? w=-71 mV) in a 0.0012 mM (? -1=275 nm) 1:1 aqueous electrolyte... for h=2.5 ? m. (b) Particle-particle potential energy profile for the interaction of two 652 nm polystyrene (PS) colloids (? p=1055 kg/m3, ? p=-178 mV) below an uncharged wall (? w=0 mV) in a 0.0012 mM (? -1=275 nm) 1:1 H2...
Low-energy magnetic radiation: Deviations from GOE
Frauendorf, S. [University Notre Dame, IN 46557 (United States); Schwengner, R. [IRP, HZDR, 01328 Dresden (Germany); Wimmer, K. [Central Michigan University, Mt. Pleasant, MI 48859 (United States)
2014-10-15T23:59:59.000Z
A pronounced spike at low energy in the strength function for magnetic radiation (LEMAR) is found by means of Shell Model calculations, which explains the experimentally observed enhancement of the dipole strength. LEMAR originates from statistical low-energy M1-transitions between many excited complex states. Re-coupling of the proton and neutron high-j orbitals generates the strong magnetic radiation. LEMAR is closely related to Magnetic Rotation. LEMAR is predicted for nuclides participating in the r-process of element synthesis and is expected to change the reaction rates. An exponential decrease of the strength function and a power law for the size distribution of the B(M1) values are found, which strongly deviate from the ones of the GOE of random matrices, which is commonly used to represent complex compound states.
Saraswat, Jyoti
2009-06-11T23:59:59.000Z
) is the spectral radius of AT A: 0.2 Definitions 0.2.1 Vandermonde Matrix. A classical (n+1) (n+1) Vandermonde matrix is defined as follows ?V = 2 66 66 66 64 1 x1 ::: xn1 1 x2 ::: xn2 ... ... ... ... 1 xn+1 ::: xnn+1 3 77 77 77 75 : Vandermonde matrices generally... m+1;1 i n+1 = 2 66 66 66 64 p0(x1) p1(x1) ::: pm(x1) p0(x2) p1(x2) ::: pm(x2) ... ... ::: ... p0(xn+1) p1(xn+1) ::: pm(xn+1) 3 77 77 77 75 = vk j 1 k n+1;1 j m+1 6 where p j is a polynomial of degree j. 0.2.3 Krylov Matrices. For a given matrix A2Rn...
A magnetically shielded room with ultra low residual field and gradient
Altarev, I.; Chesnevskaya, S.; Gutsmiedl, E.; Kuchler, F.; Lins, T.; Marino, M.; McAndrew, J.; Niessen, B.; Paul, S.; Petzoldt, G.; Singh, J.; Stoepler, R.; Stuiber, S.; Sturm, M.; Taubenheim, B. [Physikdepartment, Technische Universität München, D-85748 Garching (Germany); Babcock, E. [Jülich Center for Neutron Science, Lichtenbergstrasse 1, D-85748 Garching (Germany); Beck, D.; Sharma, S. [Physics Department, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801 (United States); Burghoff, M.; Fan, I. [Physikalisch-Technische Bundesanstalt Berlin, D-10587 Berlin (Germany); and others
2014-07-15T23:59:59.000Z
A versatile and portable magnetically shielded room with a field of (700 ± 200) pT within a central volume of 1 m × 1 m × 1 m and a field gradient less than 300 pT/m, achieved without any external field stabilization or compensation, is described. This performance represents more than a hundredfold improvement of the state of the art for a two-layer magnetic shield and provides an environment suitable for a next generation of precision experiments in fundamental physics at low energies; in particular, searches for electric dipole moments of fundamental systems and tests of Lorentz-invariance based on spin-precession experiments. Studies of the residual fields and their sources enable improved design of future ultra-low gradient environments and experimental apparatus. This has implications for developments of magnetometry beyond the femto-Tesla scale in, for example, biomagnetism, geosciences, and security applications and in general low-field nuclear magnetic resonance (NMR) measurements.
Identification and Adaptive Control Methods for Some Stochastic Systems
Zachariou, Ioannis
2011-02-21T23:59:59.000Z
n = 1n nX k=1 a 1k (Xk ^mnak)2 (3.5) and the choice of the contrl for Un is U)n = 8> >>: 1 Xn if P( ^m 1n xn+1) = 0 P( ^m 1n xn+1 Xn otherwise (3.6) where (xn) is a sequence of non-negative integer valued random variables and P the projection... the sequence futg1t=1, where ut = (^ t; ) converge almost surely? 4. Does the sequence futg1t=1, where ut = (^ t; ) converge to u0 = ( 0; ) almost surely? 5. Does the average cost Ct = 1t Pt 1k=0C(xk:uk) converge almost surely? 6. Does the average cost Ct...
Convergent synthesis of multiporphyrin light-harvesting rods
Lindsey, Jonathan S.; Loewe, Robert S.
2003-08-05T23:59:59.000Z
The present invention provides a convergent method for the synthesis of light harvesting rods. The rods are oligomers of the formula A.sup.1 (A.sup.b+1).sub.b, wherein b is at least 1, A.sup.1 through A.sup.b+1 are covalently coupled rod segments, and each rod segment A.sup.1 through A.sup.1+b comprises a compound of the formula X.sup.1 (X.sup.m+1).sub.m wherein m is at least 1 and X.sup.1 through X.sup.m+1 are covalently coupled porphyrinic macrocycles. Light harvesting arrays and solar cells containing such light harvesting rods are also described, along with intermediates useful in such methods and rods produced by such methods.
Lindsey, Jonathan S. (Raleigh, NC)
2002-01-01T23:59:59.000Z
A light harvesting array useful for the manufacture of devices such as solar cells comprises: (a) a first substrate comprising a first electrode; and (b) a layer of light harvesting rods electrically coupled to the first electrode, each of the light harvesting rods comprising a polymer of Formula I: X.sup.1.paren open-st.X.sup.m+1).sub.m (I) wherein m is at least 1, and may be from two, three or four to 20 or more; X.sup.1 is a charge separation group (and preferably a porphyrinic macrocycle, which may be one ligand of a double-decker sandwich compound) having an excited-state of energy equal to or lower than that of X.sup.2, and X.sup.2 through X.sup.m+1 are chromophores (and again are preferably porphyrinic macrocycles).
Drake, Paschal Otho
1951-01-01T23:59:59.000Z
SaN VXX? S'il ~VX~ 4$' ~S PRXQRS %9 L@AR MAL ~ k5 ~ SX ~ CCS~E(S YXD GURVM JCT9 C(M-KUBX~J?8 rtcte Chs~s sn &weifieN ~ fsr Cbsies ~ad (~ l~ies sf Cnw;. ases, ~. t Chic", ~-m, 1P~:-P ~ries ~ss on S~oifked ~w for Cnad snab, Anise 6reses ef...~s at Chisoso o~! l o&I Yore;, ss Boo(& PPC Chris& 1 irs g s4&, ps At Fort . Grthg lg"+p 3 . ". -'ig? stash Df Cl':, iso h . ziti C":vc'"'-'aao '-+~ oG +&xigla~8 St CM. csgo use Fe~~ Yol4 ?, m1 Coo@ m6 Choice hive . "~e st Fort "&orth, 19? RsLtg -riess sf...
Video transmission over wireless networks
Zhao, Shengjie
2005-08-29T23:59:59.000Z
, and operating with a coher- 22 ent BPSK modulation format. The continuous-time waveform received by a given user in such a system can be modeled as follows r(t) = GX k=1 p Pk M?1X i=0 bk[i]sk(t ? iT) + n(t); (2.3) where M is the number of data symbols per user... in the data frame of interest; T is the symbol interval; Pk, fbk[i]gM?1i=0 and sk(t) denote respectively the power level, the transmitted symbol stream, and the normalized signaling waveform of the k-th user; and n(t) is the baseband white Gaussian ambient...
Heavy-baryon chiral perturbation theory approach to thermal neutron capture on {sup 3}He
Lazauskas, Rimantas [IPHC, IN2P3-CNRS/Universite Louis Pasteur, B.P. 28, F-67037 Strasbourg Cedex 2 (France); Song, Young-Ho [Department of Physics, Duke University, Durham, North Carolina 27708 (United States); Department of Physics and Astronomy, University of South Carolina, Columbia, South Carolina 29208 (United States); Park, Tae-Sun [Department of Physics and Astronomy, University of South Carolina, Columbia, South Carolina 29208 (United States); Department of Physics and BAERI, Sungkyunkwan University, Suwon 440-746 (Korea, Republic of)
2011-03-15T23:59:59.000Z
The cross section for radiative thermal neutron capture on {sup 3}He ({sup 3}He+n{yields}{sup 4}He+{gamma}; known as the hen reaction) is calculated based on heavy-baryon chiral perturbation theory. The relevant M1 operators are derived up to next-to-next-to-next-to-leading order (N{sup 3}LO). The initial and final nuclear wave functions are obtained from the rigorous Faddeev-Yakubovski equations for five sets of realistic nuclear interactions. Up to N{sup 3}LO, the M1 operators contain two low-energy constants, which appear as the coefficients of nonderivative two-nucleon contact terms. After determining these two constants using the experimental values of the magnetic moments of the triton and {sup 3}He, we carry out a parameter-free calculation of the hen cross section. The results are in good agreement with the data.
The Search for the CP-violating emission of an E1 photon from the K(L) ---> pi+ pi- gamma decay
Shields, John Michael
2005-01-01T23:59:59.000Z
A search for the CP-violating electric dipole (E1) direct emission contribution to the K{sub L} {yields} {pi}{sup +}{pi}{sup -}{gamma} decay is performed using data from the 1997 KTeV/E832 experiment. Because the K{sub L} {yields} {pi}{sup +}{pi}{sup -}{gamma} decay mode is massively dominated by the CP-violating inner bremsstrahlung (IB) and the CP-conserving magnetic dipole (M1) direct emission processes, previous analyses have neglected the E1 contribution. Therefore, this measurement is the first attempt to directly quantify the size of the E1 decay process. This E1 transition is one of the very few CP-violating processes that is accessible to experiment and, in principle, will produce new insights into the structure of the neutral kaon. The result of this analysis is that the E1 contribution is below the threshold of sensitivity, and therefore an upper bound of |g{sub E1}| < 0.14 (90% CL) is reported. In the process of obtaining this upper limit, high resolution measurements of fit parameters ({tilde g}{sub M1} and a{sub 1}/a{sub 2}) associated with the size and shape of the M1 direct emission peak are also extracted. The fit results for these parameters: {tilde g}{sub M1} = 1.229 {+-} 0.035 (stat) {+-} 0.087 (syst); a{sub 1}/a{sub 2} = -0.733 {+-} 0.007 (stat) {+-} 0.014 (syst) are in strong agreement with previous measurements.
First Year Physics: Prelims CP1 Classical Mechanics: Prof. P. L. Read
Read, Peter L.
for viscous drag is applicable: drag force F1 = 6av [N], where a is the radius of the sphere [m], = 1.7 × 10 speed of fall, assuming a linear drag law [i.e. assume the balloon is a sphere, and that Stokes' formula would your result for (a) change if an additional drag force due to turbulent eddies of the form F2 = 0
Developpement Web -JDBC Developpement Web -JDBC
Hao, Jin-Kao
D´eveloppement Web - JDBC D´eveloppement Web - JDBC Jean-Michel Richer jean-michel.richer@univ-angers.fr http://www.info.univ-angers.fr/pub/richer M1/M2 Informatique 2010-2011 1 / 32 #12;D´eveloppement Web - JDBC Plan Plan 1 Pr´eambule 2 Utilisation de JDBC 3 Outils 2 / 32 #12;D´eveloppement Web - JDBC Pr
Optical fiber based ultrashort pulse multispectral nonlinear optical microscopy
Larson, Adam Michael
2009-05-15T23:59:59.000Z
be exploited. In our laser, modelocking through the optical Kerr effect and self-phase modulation (SPM, Sec 2.2.1) is used to generate sub-10-fs pulses. The Kerr... will induce modelocking. Green: Pump beam. Red: CW beam. Blue: Pulsed beam. M1: End mirror. M2 & M5: Intracavity mirrors. M3 & M4: Curved mirrors. OC: Output coupler. The second consequence of the optical Kerr effect is SPM. SPM results...
Systematic Variability of Soil Hydraulic Conductivity Across Three Vertisol Catenas
Rivera, Leonardo Daniel
2011-10-21T23:59:59.000Z
................................................................................................ 54 20 Boxplots of ROSETTA Estimates of Log-transformed Ks, Based on Particle Size Distribution with Bulk Density and Water Content at -33 kPa Water Potential, Compared with the Measured Estimates of Ks Separated by Landscape Position... is the water potential gradient (m m -1). The geometry and size distribution of the soil pores have a strong influence on the magnitude of K. The hydraulic conductivity can be related to the saturated hydraulic conductivity (Ks) and the degree...
EART265 Order of Magnitude Phys & Chem Lecture Outline 2
Nimmo, Francis
is fundamental to processes involving stretching or breaking of bonds, such as chemical reactions, thermal on their temperature: v 3kT m 1/2 2 #12;where gases have a thermal energy = 3 2 kT. For gases, the thermal velocity. Atom size, spacing and energy All atoms have (roughly) the same radius: 1 °A(=0.1 nm). The number
Proceedings of the Joint International Workshop on Professional Learning, Competence
Olmedilla, Daniel
and Challenges of the Social Dimension 19 Simone Braun, Andreas Schmidt The User as Prisoner: How the Dilemma Braun, S. 19 Burgos, D. 1 Johnson, M. 67 Jones, S.V. 42 Kohlhase, A. 26 Koulouris, P. 32 Kump, B. 42 Ley, T. 42 Liber, O. 67 Lindstaedt, S.N. 42 Maiden, N.A.M. 42 Markkanen, H. 8 Memmel, M. 1 Milligan, C
TkF Vrmeteknik Massverfring & separationsteknik 2006 Tentamen 170506
Zevenhoven, Ron
tar det för handduken i situation B att bli torr? AA B L=1 m 1 m 2 m x=0 x x=0 x wind vx = 3 m/s wind vx = 3 m/s AA B1 m L=2m 2 m x=0 xx=0 x x=0 xx=0 x wind vx = 3 m/swind vx = 3 m/s wind vx = 3 m
An application of Laplace transforms to a machine maintenance problem
Boone, James Robert
1962-01-01T23:59:59.000Z
of Department August I962 ACKNOWLEDGMENT Professor S. A. Sims' valuable guidance and generous time allot- ment have made this work possible. The author's gratitude and respect shall remain a guiding memory. TABLE OF CONTENTS Page INTRODUCTION... (o)=0 n n40 By the means of Laplace transforms, it is possible to transform th(s system of m + 1 ordinary, linear, first order differential equations into a system of m + I linear algebraic equations. The Laplace transform of the above system...
On the electric and magnetic properties of conductors
Arbab I. Arbab
2010-07-18T23:59:59.000Z
Application of the generalized continuity equation reveals that the drift current in conductors is equivalent to a negative diffusion current. A phenomenological model of conductivity is developed using the generalized continuity equations. Consequently, a limiting conductivity is obtained that amounts to $1.09\\times \\,10^9\\,\\Omega^{-1}m^{-1}$. A magnetomotive force (current) is hypothesized to exist, which is exhibited when a voltage changes with time. Magnetic charges and currents are found to be related to displacement current.
Resonance Conversion as a Catalyser of Nuclear Reactions
Feodor Karpeshin; Jingbo Zhang; Weining Zhang
2014-08-18T23:59:59.000Z
It is shown that resonance interal conversion offers a feasible tool for mastering nuclear processes with laser or synchrotron radiation. Physics of the process is discussed in detail in historical aspect. Possible way of experimental applicaytion is shown in the case of the $M1$ 70.6-keV transition in nuclei of $^{169}$Yb. Nuclear transition rate in hydrogenlike ions of this nuclide can be enhanced by up to four orders of magnitude.
Bhashyam, Srikrishna
EC305 Problem Set 1 1. Let x(t) = m(t) cos 2fct, where m(t) is a real lowpass signal with bandwidth a bandpass signal x(t) = m1(t) cos 2fct - m2(t) sin 2fct. (a) Determine the in-phase and quadrature components of this signal when the local os- cillators used have a phase offset of , i.e., they are cos (2fct
Dantzig, G.B.
1992-10-01T23:59:59.000Z
Analogous to gunners firing trial shots to bracket a target in order to adjust direction and distance, we demonstate that it is sometimes faster not to apply an algorithm directly, but to roughly approximately solve several perturbations of the problem and then combine these rough approximations to get an exact solution. To find a feasible solution to an m-equation linear program with a convexity constraint, the von Neumann Algorithm generates a sequence of approximate solutions which converge very slowly to the right hand side b{sup 0}. However, it can be redirected so that in the first few iterations it is guaranteed to move rapidly towards the neighborhood of one of m + 1 perturbed right hand sides {cflx b}{sup i}, then redirected in turn to the next {cflx b}{sup i}. Once within the neighborhood of each {cflx b}{sup i}, a weighted sum of the approximate solutions. {bar x}{sup i} yields the exact solution of the unperturbed problem where the weights are found by solving a system of m + 1 equations in m + 1 unknowns. It is assumed an r > 0 is given for which the problem is feasible for all right hand sides b whose distance {parallel}b - b{sup 0}{parallel}{sub 2} {le} r. The feasible solution is found in less than 4(m+ 1){sup 3}/r{sup 2} iterations. The work per iteration is {delta}mn + 2m + n + 9 multiplications plus {delta}mn + m + n + 9 additions or comparisons where {delta} is the density of nonzero coeffients in the matrix.
Dantzig, G.B.
1992-10-01T23:59:59.000Z
Analogous to gunners firing trial shots to bracket a target in order to adjust direction and distance, we demonstate that it is sometimes faster not to apply an algorithm directly, but to roughly approximately solve several perturbations of the problem and then combine these rough approximations to get an exact solution. To find a feasible solution to an m-equation linear program with a convexity constraint, the von Neumann Algorithm generates a sequence of approximate solutions which converge very slowly to the right hand side b[sup 0]. However, it can be redirected so that in the first few iterations it is guaranteed to move rapidly towards the neighborhood of one of m + 1 perturbed right hand sides [cflx b][sup i], then redirected in turn to the next [cflx b][sup i]. Once within the neighborhood of each [cflx b][sup i], a weighted sum of the approximate solutions. [bar x][sup i] yields the exact solution of the unperturbed problem where the weights are found by solving a system of m + 1 equations in m + 1 unknowns. It is assumed an r > 0 is given for which the problem is feasible for all right hand sides b whose distance [parallel]b - b[sup 0][parallel][sub 2] [le] r. The feasible solution is found in less than 4(m+ 1)[sup 3]/r[sup 2] iterations. The work per iteration is [delta]mn + 2m + n + 9 multiplications plus [delta]mn + m + n + 9 additions or comparisons where [delta] is the density of nonzero coeffients in the matrix.
Design-Space Exploration for CMOS Photonic Processor Vladimir Stojanovi!a
Batten, Christopher
can achieve up to 4x better energy-efficiency and throughput than electrical interconnects in core interconnectsM IEK0.K300L Ohotonic integrated circuitsM 1. Introduction Phis paper presents a revie4 of recent, the interconnect, and band4idth density Q3,4R. Due to pin-density, 4ire-band4idth and po4er dissipation limits
Electromagnetic effects on geodesic acoustic modes
Bashir, M. F., E-mail: frazbashir@yahoo.com [Salam Chair in Physics, G. C. University Lahore, Katchery Road, Lahore 54000 (Pakistan); Department of Physics, G. C. University Lahore, Katchery Road, Lahore 54000 (Pakistan); Smolyakov, A. I. [University of Saskatchewan, 116 Science Place, Saskatoon S7N 5E2 (Canada); Institute of Tokamak Physics, NRC “Kurchatov Institute,” 123182 Moscow (Russian Federation); Elfimov, A. G. [Institute of Physics, University of São Paulo, São Paulo 05508-090 (Brazil); Melnikov, A. V. [Institute of Tokamak Physics, NRC “Kurchatov Institute,” 123182 Moscow (Russian Federation); National Research Nuclear University MEPhI, 115409, Moscow (Russian Federation); Murtaza, G. [Visiting Professor, Department of Physics, Quaid-e-Azam University, Islamabad (Pakistan)
2014-08-15T23:59:59.000Z
By using the full electromagnetic drift kinetic equations for electrons and ions, the general dispersion relation for geodesic acoustic modes (GAMs) is derived incorporating the electromagnetic effects. It is shown that m?=?1 harmonic of the GAM mode has a finite electromagnetic component. The electromagnetic corrections appear for finite values of the radial wave numbers and modify the GAM frequency. The effects of plasma pressure ?{sub e}, the safety factor q, and the temperature ratio ? on GAM dispersion are analyzed.
DIffusion of Plasma in Magnetic Fields APAM Research Conference
Mauel, Michael E.
of Geomagnetic Cavity (Easily Measured!) . A Axisymmetric L 4 Re Rm 3 - 4 30 L2 Re Re Rm 4 cos m=±1: Measurements of Fluctuating N(!,,t) and " (!,,t) Net Current (AU) -0.00 0.01 0.03 0.05 0.07 0.09 0.11 0.13 Vf Vf Vf Vf, Isat, Triple Terrella L ! Rotation Density 60 40 20 0 20 40 60 60 40 20 0 20 40 60 Measured
Brugnano, Luigi
;Numerical comparisons between Gauss-Legendre methods and Hamiltonian BVMs defined over Gauss points Luigi. In particular, in the way they are described in this note, they are related to Gauss collocation methods with a canonical Hamiltonian system y = J H(y), y(t0) = y0 R2m , J = 0 I -I 0 R2mÃ?2m , (1) Work developed within
Fracture and Creep in an All-Tungsten Divertor for ARIES
Fracture and Creep in an All- Tungsten Divertor for ARIES Jake Blanchard University of Wisconsin by these designs Fracture Thermal creep #12;The Design #12;Major Input Parameters Parameter Value Units Surface c/a=10 Fracture Results 0 1 2 3 4 5 6 7 8 0 0.2 0.4 0.6 StressIntensity(MPa-m1/2) Crack Depth (mm) c
Lecture Notes 2. 1 Positive Dimensional Varieties
's Nullstellensatz, we have that g = 0 strictly follows from h1, . . . , hn if and only if m 1 such that gm h1 such that gm h1, . . . , ht if and only if 1 h1, . . . , ht, 1 - yg k[x1, . . . , xn, y]. Proof. To prove the equivalence, on one hand, if gm h1, . . . , hn then 1 = ym gm + (1 - ym gm ) = ym gm + (1 - yg)(1 + yg
Noncollinear double quasi phase matching in one-dimensional poled crystals
Arie, Ady
lattice vector Gm1 =2 m1/ , and the sum frequency of the fundamental and the SH is phase matched by Gm2 that the equivalent system of equa- tions is k2 2 -4k1 2 =Gm1 2 -4k1Gm1 cos and k3 2 -9k1 2 = Gm1+Gm2 2 -6k1 Gm1+Gm2
Popovych, Roman
-MannÂOkubo (GMO) mass relation for the SU(3) octet baryons 1 2 + derived in a particular version [5] of `diquark. The alternative improved version of GMO for octet baryons is the extremely precise mass sum rule (MSR) obtained-analog (1) yields the familiar [7] Gell-MannÂOkubo (GMO) mass relation MN +M = 3 2M + 1 2M in the `classical
SEVIS FEE (I-901) for J and F visa applicants Please see US Government Website at www.fmjfee.com
their entry to, stay in, and exit from the United States, will be used to record and track the I-901 fee.1a) wishing to apply for F-1, F-3, M-1, M-3, or J-1 status at a Port of Entry into the United States must pay and process the SEVIS fee before appearing at the Port of Entry. Nonimmigrants currently
Lega, Joceline
of map distance. How big will the map be? 2) If you are to build a model house out of the 1 cm blocks at a ratio of 1 m:1 cm. If the base of the house is 20 meters by 30 meters, how many blocks do you need a 220 lb person weigh on the moon? 4) Homework: Choose an object (animal, plane, ship, landmark
NO reduction using sublimation of cyanuric acid
Perry, R.A.
1996-05-21T23:59:59.000Z
A method of reducing the NO content of a gas stream comprises contacting the gas stream with an amount of HNCO at a temperature effective for heat-induced decomposition of cyanuric acid, said amount and temperature being effective for the resultant lowering of the NO content of the gas stream, said cyanuric acid being particulate and having a particle size of less than 90 {micro}m. 1 fig.
Physics 112 Mathematical Notes Winter 2000 1. Power Series Expansion of the FermiDirac Integral
California at Santa Cruz, University of
Physics 112 Mathematical Notes Winter 2000 1. Power Series Expansion of the FermiDirac Integral The FermiDirac integral is defined as: f n (z) # 1 #(n) # # 0 x n-1 dx z -1 e x + 1 , where x # #/kT and z e -(m+1)x x n-1 dx . Using the well known integral: # # 0 e -Ax x n-1 dx = #(n) A n , and changing
No evidence for association between SLC11A1 and visceral leishmaniasis in India
Mehrotra, Sanjana; Oommen, Joyce; Mishra, Anshuman; Sudharshan, Medhavi; Tiwary, Puja; Jamieson, Sarra E.; Fakiola, Michaela; Rani, Deepa Selvi; Thangaraj, Kumarasamy; Rai, Madhukar; Sundar, Shyam; Blackwell, Jenefer M.
2011-05-20T23:59:59.000Z
performed to take account of multiple trios within a pedigree. Association tests for the replication case- control sample were undertaken using logistic regression analysis performed in PLINK [29] or LOGIT (Stata) using an additive model and a genotypic test... spectrophotometer (Thermo Fischer Scientific) and agarose (Sigma Aldrich) gel elec- trophoresis. 500 ng of RNA was reverse transcribed using the High Capacity cDNA synthesis kit (Applied Biosys- tems). Taqman predesigned gene expression assay (Hs00184453_m1...
Storage-ring measurements of hyperfine induced transition rates in berylliumlike ions
Schippers, Stefan [Institute for Atomic and Molecular Physics, Justus-Liebig-University Giessen, Leihgesterner Weg 217, 35392 Giessen (Germany)
2013-07-11T23:59:59.000Z
The status of experimental measurements and theoretical calculations of the hyperfine induced 2s2p{sup 3}P{sub 0}{yields}2s{sup 21}S{sub 0} transition rate in Be-like ions is reviewed. Possible reasons, such as external electromagnetic fields and competing E1M1 two-photon transitions, for presently existing significant discrepancies between experiment and theory are discussed. Finally, directions for future research are outlined.
3.3. Radon's and Helly's Theorems 67 with > 0. Thus, we have
Gallier, Jean
3.3. Radon's and Helly's Theorems 67 with Âµ > 0. Thus, we have iI Âµi Âµ Oxi = jJ - Âµj Âµ Oxj, with i is nonempty. Proof . The proof is by induction on n m+1 and uses Radon's theorem in the induction step. For n, we can pick a set X = {a1, . . . , an+1} such that ai Ci, for every i L. By Radon's Theorem
PHYSICS 201 --FORMULA SUMMARY --MODULE 2 Uniform Circular Motion
Allen, Roland E.
T or vtangential = 2R T r aradial = r v 2 r r or aradial = v2 R Newton's Law of Universal Gravitation r Fgravity = G m1m2 r2 Universal Gravitation and Weight G mEm RE 2 = mg Kepler /Newton Law of Periods = r F r r cos WorkEnergy Theorem Wtotal = K = 1 2 mvfinal 2 - 1 2 mvinitial 2 #12;Gravitational
Method Development of Characterization of N-linked Glycoproteins in Mass Spectrometry
Zhang, Ying
2008-02-25T23:59:59.000Z
of the electric field. When the ions pass through the extraction grid, their velocities (v) are inversely proportional to the square root of their m/q (or m/z) values: v = (2qV/m) 1/2 (1.3... Table of Contents I. Introduction 1.1 Mass spectrometry……………………………………………………………………1 1.2 Matrix-assisted laser desorption/ionization (MALDI)…………………………...2 1.3 Electrospray ionization (ESI)………………………………………………………17 1.4 Principle of quadrupole ion...
c 1997 by Jay H. Lee, Jin Hoon Choi, and Kwang Soon Lee HEICON Adersa
Hong, Deog Ki
-point control in a distillation column input con- straints, interaction 0.5 - 0.5 - 0.5 0.5 strong interaction-switching logic is di cult to design debug can you do it? and causes "bumps", etc. 12 #12;c 1997 by Jay H. Lee Vmin 3 7 5 2 6 4 Lk+ijk Vk+ijk 3 7 5 2 6 4 Lmax Vmax 3 7 5 for i = 0;;m ,1 easy to design debug recon
Bier, Martin
Comparison of proton and helium induced M subshell X-ray production cross sections with the ECUSAR-ray production cross sections have been measured for Ma12, Mb1, Mc, M2N4 and M1O23 transitions representing all and helium ion energy range from 0.5 to 3 MeV on thin W, Au, Pb, Th and U targets. Ó 2013 Elsevier B.V. All
Akhmetshin, R R; Anisenkov, A V; Aulchenko, V M; Banzarov, V Sh; Bashtovoy, N S; Berkaev, D E; Bondar, A E; Bragin, A V; Eidelman, S I; Epifanov, D A; Epshteyn, L B; Erofeev, A L; Fedotovich, G V; Gayazov, S E; Grebenuk, A A; Gribanov, S S; Grigoriev, D N; Gromov, E M; Ignatov, F V; Ivanov, V L; Karpov, S V; Kasaev, A S; Kazanin, V F; Khazin, B I; Kirpotin, A N; Koop, I A; Kovalenko, O A; Kozyrev, A N; Kozyrev, E A; Krokovny, P P; Kuzmenko, A E; Kuzmin, A S; Logashenko, I B; Lukin, P A; Mikhailov, K Yu; Okhapkin, V S; Otboev, A V; Pestov, Yu N; Pivovarov, S G; Popov, A S; Razuvaev, G P; Romanov, A L; Ruban, A A; Ryskulov, N M; Ryzhenenkov, A E; Shebalin, V E; Shemyakin, D N; Shwartz, B A; Shwartz, D B; Sibidanov, A L; Shatunov, P Yu; Shatunov, Yu M; Solodov, E P; Titov, V M; Talyshev, A A; Vorobiov, A I; Yudin, Yu V; Zharinov, Yu M
2015-01-01T23:59:59.000Z
Using a data sample of 6.8 pb$^{-1}$ collected with the CMD-3 detector at the VEPP-2000 $e^+e^-$ collider we select about 2700 events of the $e^+e^- \\to p\\bar{p}$ process and measure its cross section at 12 energy ponts with about 6\\% systematic uncertainty. From the angular distribution of produced nucleons we obtain the ratio $|G_{E}/G_{M}| = 1.49 \\pm 0.23 \\pm 0.30$.
Shape Matching Michael Kazhdan
Kazhdan, Michael
· Minimum SSD Descriptor #12;Goal Given a database of 3D models, and given a query shape, find the database it is to M3 #12;Database Retrieval · Compute the distance from the query to each database model 3D Query Database Models Q M1 M2 Mn D(Q,Mi) #12;Database Retrieval · Sort the database models by proximity 3D Query
Callaway, Cody Douglas
1993-01-01T23:59:59.000Z
readership by the agricultural producer D. Examining the potential effectiveness of promotional flyers. The remaining objective, to identify seasonality patterns associated with purchases of construction, fencing, farm, and ranch products for inventory... to carry fencing, farm and ranch products? Please checkM1bstgttulx. Weedsen's Furrow's Producer's hicCey's Farm fe Braces Coup Ranch Valley Lumber Still another multiple category question, question thirteen was presented as follows. Radic Flyers...
Jayaraman, Sivaguru
) of CB8 was prepared in a 1000 mL volumetric flask. Stock solution (1 x 10-3 M) of 1 was prepared in a separate 500 mL volumetric flask. Solutions for MS and LC-MS studies were prepared by using 100 µM 1@CB8 by infusing the aqueous solution samples into the source with a syringe pump (KdScientific, model 781100, USA
TOKYO INSTITUTE OF TECHNOLOGY STAFF/STUDENTNUMBERS
Students GrandTotal 1st year 2nd year M FM F M F M F M F 3rd year Enrollment 4th year Total Note: 1.Figures of Bioscience and Biotechnology M 1st year School of Engineering Group 2 Group 3 Group 4 Group 5 Group 7Group 6 marked with * represent the number of transfer students moving into the 3rd year. 2.Figures given
of these bubbles A) in kilograms? B) in solar mass units if 1 SMU = 2.0 x 10 30 kg? Problem 3 - Suppose of these bubbles A) in kilograms? B) in solar mass units if 1 SMU = 2.0 x 10 30 kg? Answer: A) Mass in one cubic) In solar mass units M= 1.4 x 10 27 kg x (1 SMU/2.0x 10 30 kg) = 1.1 x 10 10 solar masses. Problem 3
Structure Effects on Coulomb Dissociation of $^8$B
F. M. Nunes; R. Shyam; I. J. Thompson
1998-05-23T23:59:59.000Z
Coulomb Dissociation provides an alternative method for determining the radiative capture cross sections at astrophysically relevant low relative energies. For the breakup of $^8$B on $^{58}$Ni, we calculate the total Coulomb Dissociation cross section and the angular distribution for E1, E2 and M1. Our calculations are performed first within the standard first order semiclassical theory of Coulomb Excitation, including the correct three body kinematics, and later including the projectile-target nuclear interactions.
Effects of Salinity and Specific Ions on Seedling Emergence and Growth of Onions
Miyamoto, S.; Martinez, I.; Niu, G.
2008-01-01T23:59:59.000Z
of salinity: 1.0, 1.8, 3.7 and 5.2 dS m-1 (or 630, 1200, 2500 and 3700 ppm) at a constant ionic ratio of 1:1 for Na: Ca + Mg, and Cl: SO4, and other solutions had three levels of ionic concentration ratios; 3:1, 1:1, and 1:3 at fixed levels of salinity, either...
Double major in Psychology and Organization Management Year 1 (2009-2010)
:620:556 Organization Theory M 1:00-3:50 26:620:677 Culture & Organizations M 12:30-3:20 26:620:687 Second early:620:556 Organization Theory 5. 26:620:677 Culture & Organizations Research (36 credits) 1. 26:620:686 First Early:620:558 Strategy 2. 26:620:555 Organization Behavior 3. 26:620:556 Organization Theory 4. 26:620:677 Culture
A STUDY OF MISSA ARIRANG BY COOL-JAE HUH: ELEMENTS OF KOREAN TRADITIONAL FOLK MUSIC
Son, Dong-Hyun
2013-05-31T23:59:59.000Z
-mo-ri ---------------------------------------------------------- 26 15. “Credo,” mm. 11-25 --------------------------------------------------------------------- 28 16. Use of Hemiola in “Sanctus,” mm. 9-12 ---------------------------------------------- 29 17. Use of Hemiola in “Sanctus,” mm. 92...-56 -------------------------------------------------------- 33 21. Toe-sung in “Agnus Dei,” mm. 1-4 ---------------------------------------------------- 34 vii 22. Toe-sung and Choo-sung in “Credo,” m. 1-11 --------------------------------------- 35 23. Choo-sung in “Gloria,” mm. 11...
Entangling characterization of (SWAP)1/m and Controlled unitary gates
Balakrishnan, S
2008-01-01T23:59:59.000Z
We study the entangling power and perfect entangler nature of (SWAP)1/m, for m>=1, and controlled unitary (CU) gates. It is shown that (SWAP)1/2 is the only perfect entangler in the family. On the other hand, a subset of CU which is locally equivalent to CNOT is identified. It is shown that the subset, which is a perfect entangler, must necessarily possess the maximum entangling power.
Entangling characterization of (SWAP)1/m and Controlled unitary gates
S. Balakrishnan; R. Sankaranarayanan
2009-01-05T23:59:59.000Z
We study the entangling power and perfect entangler nature of (SWAP)1/m, for m>=1, and controlled unitary (CU) gates. It is shown that (SWAP)1/2 is the only perfect entangler in the family. On the other hand, a subset of CU which is locally equivalent to CNOT is identified. It is shown that the subset, which is a perfect entangler, must necessarily possess the maximum entangling power.
Tausk, Daniel Victor
- eraliza,c"oes para espa,cos de se,c"oes de um fibrado geral, mas o objetivo des* *ta se,c"ao 'e jus N agora passa a ser chamad* *a de M. Teremos sempre um tipo M de espa,co de se,c"oes que fibrado misto sobre I (cu* *jo fibrado das bases 'e I x M). Teremos ent"ao dois tipos M1, M2 de espa
Public Parking Lots > Agriculture Building Parkade
Saskatchewan, University of
P P P P P P P P P P P M M M 1 C 3 2 B A R O O 9 L 5 Y Q T U U 16 15 4 P 18 17 7 Public Parking Lots > Agriculture Building Parkade > Pay Parking Lots > Stadium Parkade > Diefenbaker Lot > Health Sciences Parkade Disabled Persons' Parking* Motorcyle Parking* Faculty & Sta Parking Lots* Student Parking Lots* Royal
GeV electron beams from a centimetre-scale accelerator
Geddes, Cameron Guy Robinson
GeV electron beams from a centimetre-scale accelerator W. P. LEEMANS1 * , B. NAGLER1 , A. J-quality electron beam with 1 GeV energy by channelling a 40 TW peak-power laser pulse in a 3.3-cm-long gas-100 GV m-1 in laser-wakefield accelerators1,2 , until recently the electron beams (e-beams) from
A p-cell approach to integer gate sizing
Doddannagari, Uday
2009-05-15T23:59:59.000Z
was chosen to be the minimum size possible in 0.18 m technology : : : : : : : : : : : 35 III The source and drain parameters for the ve transistors in g. 22. M1,M2,M3 and M4 are identical to each other but M5 is not : : : : : 35 IV Table illustrating... time and load capacitance : : : : : : : : : : : 5 3 A typical delay table : : : : : : : : : : : : : : : : : : : : : : : : : : : 5 4 Figure illustrating the use of delay tables for timing analysis : : : : : 6 5 A parallel cell realization example...
Computing the lowest eigenvalues of the Fermion matrix by subspace iterations
B. Bunk
1996-08-21T23:59:59.000Z
Subspace iterations are used to minimise a generalised Ritz functional of a large, sparse Hermitean matrix. In this way, the lowest $m$ eigenvalues are determined. Tests with $1 \\leq m \\leq 32$ demonstrate that the computational cost (no. of matrix multiplies) does not increase substantially with $m$. This implies that, as compared to the case of a $m=1$, the additional eigenvalues are obtained for free.
TO CONSTRUCTION AS OF 10/4/2011 Current/Approved Projects Project: Solar Energy Research Center Bldg. #:TBD. #: TBD Affected Area: R1 Road & V Road (58) Dates: 8/2011 - 9/2013 6 Small Projects: A. B50 Electrical/1/2014 N3 (58) 42 11/1/2011 2/1/2014 M-1 (35) 12 10/1/2010 11/1/2011 B81 (21) 18 10/1/2010 11/1/2011 V Road
Analysis of Nanopore Data using Hidden Markov Models
Schreiber, J.; Karplus, K.
2015-01-01T23:59:59.000Z
S1 E1 E2 S2 E2 S3 E3 S3 E3 S4 E4 S4 I M1 S2 SS SE M2 S5 M3E4 E5 S5 E5 E6 S6 E6 E7 S7 E7 M4 S6 S7 U B b c 40 ms 250 ms
Microcomputers in Process Control
Vinson, D. R.; Chatterjee, N.
M1CROCOMPUTERS IN PROCESS CONTROL ", D. R. Vinson and N. Chatterjee (?)Air Products and Chemicals, Inc. Allentown, Pennsylvania Computers have been extensively used for process control and optimization since the 1970's. Many articles have... the process industries continued utilization of microcomputers throughout the plant, even with the current decrease in the price of oil. Full utilization of the process control computer can only be achieved when it performs the function of the best...
Doing data regression in the TI-85 Entering the data
Torres, Rodolfo
Doing data regression in the TI-85 Entering the data Press to get the statistics menu. Press (key F2). Select and and press .xStat yStat Enter the x-data and y-data. Doing the regression Press in the menu (key M1= 2nd F1).STAT Select and .xStat yStat Select the type of regression. For example, and get
A Gentle Introduction to Dynamical Systems Theory
Beer, Randall D.
A Gentle Introduction to Dynamical Systems Theory Reading: Chapter 1 #12;IU/COGS-Q580/Beer Isaac = -F2 = G m1m2 r2 #12;IU/COGS-Q580/Beer Henri Poincaré and His 3 Bodies Diacu, F. and Holmes, P. (1996 to almost all differential equations cannot be expressed as an explicit formula #12;IU/COGS-Q580/Beer
S. Pascoli; S. T. Petcov
2007-11-30T23:59:59.000Z
If future neutrino oscillation experiments show that the neutrino mass spectrum is with normal ordering, m1 | > 0.01 eV give negative results, the next frontier in the quest for neutrinoless double beta-decay will correspond to || ~ 0.001 eV. Assuming that massive neutrinos are Majorana particles and their exchange is the dominant mechanism generating neutrinoless double beta-decay, we analise the conditions under which ||, in the case of three neutrino mixing and neutrino mass spectrum with normal ordering, would satisfy || > 0.001 eV. We consider the specific cases of i) normal hierarchical neutrino mass spectrum, ii) of relatively small value of the CHOOZ angle theta13 as well as iii) the general case of spectrum with normal ordering, partial hierarchy and a value of theta13 close to the existing upper limit. We study the ranges of the lightest neutrino mass m1 and/or of sin^2 theta13, for which ||> 0.001 eV and discuss the phenomenological implications of such scenarios. We provide also an estimate of || when the three neutrino masses and the neutrino mixing originate from neutrino mass term of Majorana type for the (left-handed) flavour neutrinos and m1 Ue1^2 + m2 U_e2^2 + m3 Ue3^2 =0, but there does not exist a symmetry which forbids the neutrinoless double beta-decay.
Cavallo, A.; Hsuan, H.; Boyd, D.; Grek, B.; Johnson, D.; Kritz, A.; Mikkelsen, D.; LeBlanc, B.; Takahashi, H.
1984-10-01T23:59:59.000Z
During first harmonic electron cyclotron heating (ECH) on the Princeton Divertor Experiment (PDX) (R/sub 0/ = 137 cm, a = 40 cm), electron temperature was monitored using a grating polychromator which measured second harmonic electron cyclotron emission from the low field side of the tokamak. Interference from the high power heating pulse on the broadband detectors in the grating instrument was eliminated by using a waveguide filter in the transmission line which brought the emission signal to the grating instrument. Off-axis (approx. 4 cm) location of the resonance zone resulted in heating without sawtooth or m = 1 activity. However, heating with the resonance zone at the plasma center caused very large amplitude sawteeth accompanied by strong m = 1 activity: ..delta..T/T/sub MAX/ approx. = 0.41, sawtooth period approx. = 4 msec, m = 1 period approx. = 90 ..mu.. sec, (11 kHz). This is the first time such intense MHD activity driven by ECH has been observed. (For both cases there was no sawtooth activity in the ohmic phase of the discharge before ECH.) At very low densities there is a clear indication that a superthermal electron population is created during ECH.