Crude Depletion Conditions for XKCM1 Arshad Desai
Mitchison, Tim
Crude Depletion Conditions for XKCM1 Arshad Desai 3/17/95 Problems: The main problem with immunodepletion of crude CSF extracts is that they activate during or soon after immunodepletion. Empirically well in crude). However, we have never been able to cycle a depleted crude - all assays were performed
Scalable Hierarchical Locking for Distributed Systems Nirmit Desai and Frank Mueller
Mueller, Frank
Scalable Hierarchical Locking for Distributed Systems Nirmit Desai and Frank Mueller Dept share computational resources in distributed environments, such as high-end clusters with ever larger requests in distributed systems. But concurrency protocols currently lack scalability. Adding
Asymptotic Unitary Equivalence in KK-Theory
2001-09-17T23:59:59.000Z
Key words: KK-theory, Cuntz pairs, classification of nuclear C?-algebras. 1. ... realizations of KK(A,B) for purely infinite simple nuclear C. ?. -algebras, [Kir94],.
On the representation of $A_{\\kk}(2)$ algebra and $A_{\\kk}(d)$ algebra
Won Sang Chung
2012-12-27T23:59:59.000Z
In this paper the representation of $A_{\\kk}(2)$ algebra given by Daoud and Kibler [M.Daoud and M.Kibler, J.Phys.A 43 115303 (2010), 45 244036 (2012)] is investigated. It is shown that the new generators are necessary for consistency of the algebra. The multi-mode extension of $A_{\\kk}(2)$ algebra, which is called $A_{\\kk}(d)$ algebra, is also obtained. The positivity condition of the energy spectrum is also investigated for $A_{\\kk}(2)$ algebra and $A_{\\kk}(d)$ algebra.
Perturbations of supertube in KK monopole background
Yogesh K. Srivastava
2006-11-29T23:59:59.000Z
We study perturbations of supertube in KK monopole background, at both DBI and supergravity levels. We analyse both NS1-P as well as D0-F1 duality frames and study different profiles. This illuminates certain aspects of bound states of KK monopoles with supertubes.
Study of Bc->KK decay with perturbative QCD approach
Yue-Ling Yang; Jun-Feng Sun; Na Wang
2010-04-16T23:59:59.000Z
In the framework of the perturbative QCD approach, we study the charmless pure weak annihilation Bc->KK decay and find that the branching ratio BR(Bc->KK) O(10^-7). This prediction is so tiny that the Bc->KK decay might be unmeasurable at the Large Hadron Collider.
Kk electronic A S | 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 onYou are now leaving Energy.gov You are now leaving Energy.gov You are being directedAnnual Siteof Energy 2,AUDIT REPORTEnergyFarmsPower Co LtdTN LLCKirmart Corporation Jump to:Kk
Carpick, Robert W.
Hydraulic Drivetrain and Regenerative Braking Team 13: Andrew Brown, Karan Desai, Andrew Mc Pressure Reservior Filter Variable Vane Pump Motor/Pump Hydraulic Accumulators Solenoid Valve Relief Valve Suction Line Since their development in 2006, hydraulic drivetrain systems have gained considerable
Dangerous Angular KK/Glueball Relics in String Theory Cosmology
J. F. Dufaux; L. Kofman; M. Peloso
2008-07-07T23:59:59.000Z
The presence of Kaluza-Klein particles in the universe is a potential manifestation of string theory cosmology. In general, they can be present in the high temperature bath of the early universe. In particular examples, string theory inflation often ends with brane-antibrane annihilation followed by the energy cascading through massive closed string loops to KK modes which then decay into lighter standard model particles. However, massive KK modes in the early universe may become dangerous cosmological relics if the inner manifold contains warped throat(s) with approximate isometries. In the complimentary picture, in the AdS/CFT dual gauge theory with extra symmetries, massive glueballs of various spins become the dangerous cosmological relics. The decay of these angular KK modes/glueballs, located around the tip of the throat, is caused by isometry breaking which results from gluing the throat to the compact CY manifold. We address the problem of these angular KK particles/glueballs, studying their interactions and decay channels, from the theory side, and the resulting cosmological constraints on the warped compactification parameters, from the phenomenology side. The abundance and decay time of the long-lived non-relativistic angular KK modes depend strongly on the parameters of the warped geometry, so that observational constraints rule out a significant fraction of the parameter space. In particular, the coupling of the angular KK particles can be weaker than gravitational.
SG Biofuels | 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 onYou are now leaving Energy.gov You are now leaving Energy.gov You are beingZealand Jump to:Ezfeedflag JumpID-f < RAPIDâ€Ž |Rippey Jump to:WY) JumpLand FocusSCSENDECO2 JumpSolarSG
On the KK system as two-kaons system
Jaroslav Hruby
2005-04-01T23:59:59.000Z
The time evolution of the KK system as a two-qubit system is given. The effect which is interpreted as CP violation in neutral kaon decays is explained via violation of quantum correlations during time evolution of the KK system as two-kaons system and description is via Yang-Baxterization and unitary time dependent R-matrices to con- struct Hamiltonian, determining the time evolution of two-kaons sys- tem. The nonseparability ideas and criterion can be extended on all mixing state-antistate system and all CP violation cases in particle physics.
Significant effects of second KK particles on LKP dark matter physics
Mitsuru Kakizaki; Shigeki Matsumoto; Yoshio Sato; Masato Senami
2005-06-17T23:59:59.000Z
We point out that Kaluza-Klein (KK) dark matter physics is drastically affected by second KK particles. In this work various interesting phenomena caused by the second KK modes are discussed. In particular, we reevaluate the annihilation cross section and thermal relic density of the KK dark matter quantitatively in universal extra dimensions, in which all the standard model particles propagate. In these models, the first KK mode of $B$ boson is a viable dark matter candidate by virtue of KK-parity. We demonstrate that the KK dark matter annihilation cross section can be enhanced, compared with the tree level cross section mediated only by first KK particles. The dark matter mass consistent with the WMAP observation is increased.
Anaysis of high energy K+K- photoproduction on hydrogen
L. Bibrzycki; L. Lesniak; A. P. Szczepaniak
2004-07-21T23:59:59.000Z
We have analyzed the K+K- photoproduction on hydrogen in the effective mass region around the mass of the phi(1020) meson. The interference of the S-wave contribution with the P-wave has been studied. Both scalar resonances f0(980) and a0(980) have been taken into account. We have obtained a good description of the available experimental data, in particular the mass distributions and the moments of the kaon angular distribution. Our calculations give values of the integrated S-wave total photoproduction cross section between 4 and 7 nb for the K+K- effective mass range around the phi(1020) mass and at the laboratory photon energy near 5 GeV. These numbers favor lower experimental estimates obtained at DESY.
Nippon Yusen KK NYK Link | 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 onYou are now leaving Energy.gov You are now leaving Energy.gov YouKizildere I Geothermal Pwer PlantMunhall,Missouri: Energy Resources Jump to:Nigeria: EnergyNinilchik,Yusen KK NYK Link
THESIS FOR THE DEGREE OF LICENTIATE OF PHILOSOPHY Equivariant KK-theory and twists
Patriksson, Michael
THESIS FOR THE DEGREE OF LICENTIATE OF PHILOSOPHY Equivariant KK-theory and twists Magnus Goffeng;#12;Preface This text constitutes my thesis for a Licentiate degree at the department of Mathematical Sciences
Coloring Kk-free intersection graphs of geometric objects in the plane
Fox, Jacob
Coloring Kk-free intersection graphs of geometric objects in the plane Jacob Fox Department that copies are not made or distributed for profit or commercial advantage and that copies bear this notice
SG BioFuels | 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 onYou are now leaving Energy.gov You are now leaving Energy.gov YouKizildere IRaghuraji Agro Industries Pvt Ltd Jump to:RoscommonSBY Solutions Jump to: navigation,SEMASSSES CoSF-299SG
Advanced Security Acceleration Project for Smart Grid (ASAP-SG...
Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)
Security Acceleration Project for Smart Grid (ASAP-SG) June 12, 2013 Problem Statement: The goal of this project is to develop a set of computer and network security requirements...
S-P wave interference in the K+K- photoproduction on hydrogen
L. Bibrzycki; L. Lesniak; A. P. Szczepaniak
2005-09-23T23:59:59.000Z
We have studied the partial wave interference effects to obtain a new information about the contribution of the S-wave to the cross section of the K+K- photoproduction on hydrogen. The K+K- photoproduction channel for the effective masses around 1 GeV is dominated by the phi(1020) resonance with only a small fraction of events coming from decays of scalar resonances f0(980) and a0(980). However, a careful analysis of angular distributions of the outgoing kaons shows that the S-wave adds an asymmetry to the angular distribution of kaons. A fairly precise estimation of the K+K- photoproduction cross section in the S-wave has been obtained.
T-651: Blue Coat ProxySG Discloses Potentially Sensitive Information in Core Files
Broader source: Energy.gov [DOE]
A vulnerability was reported in Blue Coat ProxySG. A local user can obtain potentially sensitive information
A LOGICAL INVERTED TAXONOMY OF SORTING ALGORITHMS S.M. Merritt K.K. Lau
Lau, Kung-Kiu
A LOGICAL INVERTED TAXONOMY OF SORTING ALGORITHMS S.M. Merritt K.K. Lau School of Computer Science taxonomy of sorting algorithms, a highÂlevel, topÂdown, conceptually simple and symmetric categorization taxonomy of sorting algorithms. This provides a logical basis for the inverted taxonomy and expands
K.K. Gan Siena02 1 The Ohio State University
Gan, K. K.
.K. Gan Siena02 6 l Decode Bi-Phase Mark encoded (BPM) clock and command signals from PIN diode l Input Error Rate (BER): BPM #12;K.K. Gan Siena02 7 l Training period: ~25 ms of 20 MHz clock (BPM with no data) DORIC Logic ] Ready
KK-monopoles and G-structures in M-theory/type IIA reductions
Ulf Danielsson; Giuseppe Dibitetto; Adolfo Guarino
2015-02-17T23:59:59.000Z
We argue that M-theory/massive IIA backgrounds including KK-monopoles are suitably described in the language of G-structures and their intrinsic torsion. To this end, we study classes of minimal supergravity models that admit an interpretation as twisted reductions in which the twist parameters are not restricted to satisfy the Jacobi constraints $\\omega\\, \\omega=0$ required by an ordinary Scherk-Schwarz reduction. We first derive the correspondence between four-dimensional data and torsion classes of the internal space and, then, check the one-to-one correspondence between higher-dimensional and four-dimensional equations of motion. Remarkably, the whole construction holds regardless of the Jacobi constraints, thus shedding light upon the string/M-theory interpretation of (smeared) KK-monopoles.
gamma+gamma --> pi+pi, K+K : leading term QCD vs handbag model
Victor L. Chernyak
2006-06-15T23:59:59.000Z
The "handbag" model was proposed as an alternative, at the present day energies, to the leading term QCD predictions for some hard exclusive processes. The recent precise data from the Belle Collaboration on the large angle cross sections $\\gamma\\gamma --> \\pi\\pi, KK $ allow a check of these two approaches to be performed. It is shown that the handbag model fails to describe the data from Belle, while the leading term QCD predictions are in reasonable agreement with these data
K.K. Gan ATLAS Pixel Week 1 New Results on Opto-Electronics
Gan, K. K.
with lower thresholds with BPM/DRX ] opto-board design is compatible with BPM/DRX PIN Current Thresholds with BPM/DRX 0 5 10 15 20 25 30 35 link#1 link#2 link#3 link#4 link#5 link#6 link#7 Ipin(mA) Opto-Board on Test Board Opto-Board on Test Board with BPM/DRX #12;K.K. Gan ATLAS Pixel Week 8 l one irradiated VCSEL
Merging Flavour Symmetries with QCD Factorisation for B-->KK Decays
Joaquim Matias
2007-01-15T23:59:59.000Z
The interplay between flavour symmetries connecting Bs-->KK decays with the recently measured Bd--> K0 anti-K0 decay and QCD Factorisation opens new strategies to describe the decays Bs--> K0 anti-K0 and Bs--> K+ K- in the SM and in supersymmetry. A new relation, emerging from the sum-rule for the Bs--> K0 anti-K0 decay mode, is presented offering a new way to determine the weak mixing angle phi_s of the Bs system.
Measurements of {psi}(2S) decays into {gamma}KK{pi} and {gamma}{eta}{pi}{sup +}{pi}{sup -}
Ablikim, M.; Bai, J. Z.; Bian, J. G.; Cai, X.; Chen, H. S.; Chen, H. X.; Chen, J. C.; Chen, Jin; Chen, Y. B.; Chu, Y. P.; Cui, X. Z.; Deng, Z. Y.; Du, S. X.; Fang, J.; Fu, C. D.; Gao, C. S.; Gu, S. D.; Guo, Y. N.; Guo, Y. Q.; He, K. L. [Institute of High Energy Physics, Beijing 100049 (China)] (and others)
2006-10-01T23:59:59.000Z
Radiative decays of the {psi}(2S) into {gamma}KK{pi} and {gamma}{eta}{pi}{sup +}{pi}{sup -} final states are studied using 14x10{sup 6} {psi}(2S) events collected with the BESII detector. Branching fractions or upper limits on the branching fractions of {psi}(2S) and {chi}{sub cJ} decays are reported. No significant signal for {eta}(1405)/{eta}(1475) is observed in the KK{pi} or {eta}{pi}{sup +}{pi}{sup -} mass spectra, and upper limits on the branching fractions of {psi}(2S){yields}{gamma}{eta}(1405)/{eta}(1475), {eta}(1405)/{eta}(1475){yields}KK{pi}, and {eta}{pi}{sup +}{pi}{sup -} are determined.
Production of K?K? pairs in proton-proton collisions below the ? meson threshold
Ye, Q. J.; Hartmann, M.; Chiladze, D.; Dymov, S.; Dzyuba, A.; Gao, H.; Gebel, R.; Hejny, V.; Kacharava, A.; Lorentz, B.; Mchedlishvili, D.; Merzliakov, S.; Mielke, M.; Mikirtytchiants, S.; Ohm, H.; Papenbrock, M.; Polyanskiy, A.; Serdyuk, V.; Stein, H. J.; Ströher, H.; Trusov, S.; Valdau, Yu.; Wilkin, C.; Wüstner, P.
2013-06-01T23:59:59.000Z
The pp?ppK?K? reaction was measured below the ? threshold at a beam energy of 2.568 GeV using the COSY-ANKE magnetic spectrometer. By assuming that the four-body phase space is distorted only by the product of two-body final-state interactions, fits to a variety of one-dimensional distributions permit the evaluation of differential and total cross sections. The shapes of the distributions in the K_{p} and K_{pp} invariant masses are reproduced only if the K?_{p} interaction is even stronger than that found at higher energy. The cusp effect in the K?K? distribution at the K?K¯¯¯? threshold is much more clear and some evidence is also found for coupling between the K?_{p} and K¯¯¯?n channels. However, the energy dependence of the total cross section cannot be reproduced by considering only a simple product of such pairwise final-state interactions.
Production of K?K? pairs in proton-proton collisions below the ? meson threshold
DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)
Ye, Q. J.; Hartmann, M.; Chiladze, D.; Dymov, S.; Dzyuba, A.; Gao, H.; Gebel, R.; Hejny, V.; Kacharava, A.; Lorentz, B.; et al
2013-06-01T23:59:59.000Z
The pp?ppK?K? reaction was measured below the ? threshold at a beam energy of 2.568 GeV using the COSY-ANKE magnetic spectrometer. By assuming that the four-body phase space is distorted only by the product of two-body final-state interactions, fits to a variety of one-dimensional distributions permit the evaluation of differential and total cross sections. The shapes of the distributions in the Kp and Kpp invariant masses are reproduced only if the K?p interaction is even stronger than that found at higher energy. The cusp effect in the K?K? distribution at the K?K¯¯¯? threshold is much more clear and some evidencemore »is also found for coupling between the K?p and K¯¯¯?n channels. However, the energy dependence of the total cross section cannot be reproduced by considering only a simple product of such pairwise final-state interactions.« less
The WA102 Collaboration; D. Barberis et al
1999-07-28T23:59:59.000Z
A coupled channel analysis of the centrally produced K+K- and pi+pi- final states has been performed in pp collisions at an incident beam momentum of 450 GeV/c. The pole positions and branching ratios to pipi and KK of the f0(980), f0(1370), f0(1500) and f0(1710) have been determined. A systematic study of the production properties of all the resonances observed in the pi+pi- and K+K- channels has been performed.
A study of the centrally produced K*K* and phi omega systems in pp interactions at 450 GeV/c
The WA102 Collaboration; D. Barberis et al
1998-07-21T23:59:59.000Z
A study of the reactions pp -> pfps(K+K-pi+pi-) and pp -> pfps(K+K-pi+pi-pi0) shows evidence for the K*K* and phi omega channels respectively. The K*K* mass spectrum shows a broad distribution with a maximum near threshold and an angular analysis shows that it is compatible with having JP = 2+. The behaviour of the cross-section as a function of centre of mass energy, and the four momentum transfer dependence, are compatible with what would be expected if the K*K* system was produced via double Pomeron exchange. The dPT behaviour of the phi omega channel is similar to what has been observed for all the undisputed qqbar states. In contrast, the dPT behaviour of the K*K* final state is similar to what has been observed for the phi phi final state and for previously observed glueball candidates.
Comprehensive amplitude analysis of ????+??,?0?0 and K¯K below 1.5 GeV
DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)
Dai, Ling-Yun; Pennington, M.? R.
2014-08-01T23:59:59.000Z
In this paper we perform an amplitude analysis of essentially all published pion and kaon pair production data from two photon collisions below 1.5 GeV. This includes all the high statistics results from Belle, as well as older data from Mark II at SLAC, CELLO at DESY, Crystal Ball at SLAC. The purpose of this analysis is to provide as close to a model-independent determination of the ?? to meson pair amplitudes as possible. Having data with limited angular coverage, typically |cos?| more »the underlying amplitudes might appear an intractable problem. However, imposing the basic constraints required by analyticity, unitarity, and crossing-symmetry makes up for the experimentally missing information. Above 1.5 GeV multi-meson production channels become important and we have too little information to resolve the amplitudes. Nevertheless, below 1.5 GeV the two photon production of hadron pairs serves as a paradigm for the application of S-matrix techniques. Final state interactions among the meson pairs is critical to this analysis. To fix these, we include the latest ?? ? ??, K?K scattering amplitudes given by dispersive analyses, supplemented in the K?K threshold region by the recent precision Dalitz plot analysis from BaBar. With these hadronic amplitudes built into unitarity, we can constrain the overall description of ?? ? ?? and K?K datasets, both integrated and differential cross-sections, including the high statistics charged and neutral pion data from Belle. A region of solutions is found for the ?? ? ?? partial waves with both isospin 0 and 2. Since this analysis invokes coupled hadronic channels, even the relatively poor integrated cross-section data on ?? ? K?K narrows the patch of solutions to essentially a single form. For this we present the complete partial wave amplitudes, show how well they fit all the available data, and give the two photon couplings of scalar and tensor resonances that appear.« less
Comprehensive Amplitude Analysis of ????+?-, ?0?0 and K?K below 1.5 GeV
DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)
Dai, Lingyun; Pennington, Michael R.
2014-08-01T23:59:59.000Z
In this paper we perform an amplitude analysis of essentially all published pion and kaon pair production data from two photon collisions below 1.5 GeV. This includes all the high statistics results from Belle, as well as older data from Mark II at SLAC, CELLO at DESY, Crystal Ball at SLAC. The purpose of this analysis is to provide as close to a model-independent determination of the ?? to meson pair amplitudes as possible. Having data with limited angular coverage, typically |cos?| more »the underlying amplitudes might appear an intractable problem. However, imposing the basic constraints required by analyticity, unitarity, and crossing-symmetry makes up for the experimentally missing information. Above 1.5 GeV multi-meson production channels become important and we have too little information to resolve the amplitudes. Nevertheless, below 1.5 GeV the two photon production of hadron pairs serves as a paradigm for the application of S-matrix techniques. Final state interactions among the meson pairs is critical to this analysis. To fix these, we include the latest ?? ? ??, K?K scattering amplitudes given by dispersive analyses, supplemented in the K?K threshold region by the recent precision Dalitz plot analysis from BaBar. With these hadronic amplitudes built into unitarity, we can constrain the overall description of ?? ? ?? and K?K datasets, both integrated and differential cross-sections, including the high statistics charged and neutral pion data from Belle. A region of solutions is found for the ?? ? ?? partial waves with both isospin 0 and 2. Since this analysis invokes coupled hadronic channels, even the relatively poor integrated cross-section data on ?? ? K?K narrows the patch of solutions to essentially a single form. For this we present the complete partial wave amplitudes, show how well they fit all the available data, and give the two photon couplings of scalar and tensor resonances that appear.« less
Production of K+K? pairs in proton-proton collisions below the ? meson threshold
DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)
Ye, Q. J.; Hartmann, M.; Chiladze, D.; Dymov, S.; Dzyuba, A.; Gao, H.; Gebel, R.; Hejny, V.; Kacharava, A.; Lorentz, B.; Mchedlishvili, D.; Merzliakov, S.; Mielke, M.; Mikirtytchiants, S.; Ohm, H.; Papenbrock, M.; Polyanskiy, A.; Serdyuk, V.; Stein, H. J.; Ströher, H.; Trusov, S.; Valdau, Yu.; Wilkin, C.; Wüstner, P.
2013-06-01T23:59:59.000Z
The pp?ppK+K? reaction was measured below the ? threshold at a beam energy of 2.568 GeV using the COSY-ANKE magnetic spectrometer. By assuming that the four-body phase space is distorted only by the product of two-body final-state interactions, fits to a variety of one-dimensional distributions permit the evaluation of differential and total cross sections. The shapes of the distributions in the Kp and Kpp invariant masses are reproduced only if the K?p interaction is even stronger than that found at higher energy. The cusp effect in the K+K? distribution at the K0K{bar}0 threshold is much more clear and some evidence is also found for coupling between the K?p and K?0n channels. However, the energy dependence of the total cross section cannot be reproduced by considering only a simple product of such pairwise final-state interactions.
Tebo, Brad
, MnxG was overexpressed in Escherichia coli and used to generate polyclonal antibodies. Western blotAbstract Dormant spores of the marine Bacillus sp. strain SG-1 catalyze the oxidation of manganese Introduction Mature spores of the marine Bacillus sp. strain SG-1 oxi- dize soluble manganese [Mn(II)], thereby
Comprehensive Amplitude Analysis of ????+?-, ?0?0 and K?K below 1.5 GeV
DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)
Dai, Lingyun; Pennington, Michael R. [JLAB
2014-08-01T23:59:59.000Z
In this paper we perform an amplitude analysis of essentially all published pion and kaon pair production data from two photon collisions below 1.5 GeV. This includes all the high statistics results from Belle, as well as older data from Mark II at SLAC, CELLO at DESY, Crystal Ball at SLAC. The purpose of this analysis is to provide as close to a model-independent determination of the ?? to meson pair amplitudes as possible. Having data with limited angular coverage, typically |cos?| < 0.6-0.8, and no polarization information for reactions in which spin is an essential complication, the determination of the underlying amplitudes might appear an intractable problem. However, imposing the basic constraints required by analyticity, unitarity, and crossing-symmetry makes up for the experimentally missing information. Above 1.5 GeV multi-meson production channels become important and we have too little information to resolve the amplitudes. Nevertheless, below 1.5 GeV the two photon production of hadron pairs serves as a paradigm for the application of S-matrix techniques. Final state interactions among the meson pairs is critical to this analysis. To fix these, we include the latest ?? ? ??, K?K scattering amplitudes given by dispersive analyses, supplemented in the K?K threshold region by the recent precision Dalitz plot analysis from BaBar. With these hadronic amplitudes built into unitarity, we can constrain the overall description of ?? ? ?? and K?K datasets, both integrated and differential cross-sections, including the high statistics charged and neutral pion data from Belle. A region of solutions is found for the ?? ? ?? partial waves with both isospin 0 and 2. Since this analysis invokes coupled hadronic channels, even the relatively poor integrated cross-section data on ?? ? K?K narrows the patch of solutions to essentially a single form. For this we present the complete partial wave amplitudes, show how well they fit all the available data, and give the two photon couplings of scalar and tensor resonances that appear.
Predicting Functional Regions of Objects Chaitanya Desai
Ramanan, Deva
regions. We compare "blind" approaches that ig- nore image data, bottom-up approaches that reason about). We benchmark a wide variety of algo- rithms for producing such outputs, including blind baselines- fords little use to an observer. The central thesis of this work is that functional regions
Precision measurement of $CP$ violation in $B_s^0 \\to J/\\psi K^+K^-$ decays
Aaij, Roel; Adinolfi, Marco; Affolder, Anthony; Ajaltouni, Ziad; Akar, Simon; Albrecht, Johannes; Alessio, Federico; Alexander, Michael; Ali, Suvayu; Alkhazov, Georgy; Alvarez Cartelle, Paula; Alves Jr, Antonio Augusto; Amato, Sandra; Amerio, Silvia; Amhis, Yasmine; An, Liupan; Anderlini, Lucio; Anderson, Jonathan; Andreassen, Rolf; Andreotti, Mirco; Andrews, Jason; Appleby, Robert; Aquines Gutierrez, Osvaldo; Archilli, Flavio; Artamonov, Alexander; Artuso, Marina; Aslanides, Elie; Auriemma, Giulio; Baalouch, Marouen; Bachmann, Sebastian; Back, John; Badalov, Alexey; Baesso, Clarissa; Baldini, Wander; Barlow, Roger; Barschel, Colin; Barsuk, Sergey; Barter, William; Batozskaya, Varvara; Battista, Vincenzo; Bay, Aurelio; Beaucourt, Leo; Beddow, John; Bedeschi, Franco; Bediaga, Ignacio; Belogurov, Sergey; Belous, Konstantin; Belyaev, Ivan; Ben-Haim, Eli; Bencivenni, Giovanni; Benson, Sean; Benton, Jack; Berezhnoy, Alexander; Bernet, Roland; Bertolin, Alessandro; Bettler, Marc-Olivier; van Beuzekom, Martinus; Bien, Alexander; Bifani, Simone; Bird, Thomas; Bizzeti, Andrea; Bjørnstad, Pål Marius; Blake, Thomas; Blanc, Frédéric; Blouw, Johan; Blusk, Steven; Bocci, Valerio; Bondar, Alexander; Bondar, Nikolay; Bonivento, Walter; Borghi, Silvia; Borgia, Alessandra; Borsato, Martino; Bowcock, Themistocles; Bowen, Espen Eie; Bozzi, Concezio; Brett, David; Britsch, Markward; Britton, Thomas; Brodzicka, Jolanta; Brook, Nicholas; Bursche, Albert; Buytaert, Jan; Cadeddu, Sandro; Calabrese, Roberto; Calvi, Marta; Calvo Gomez, Miriam; Campana, Pierluigi; Campora Perez, Daniel; Carbone, Angelo; Carboni, Giovanni; Cardinale, Roberta; Cardini, Alessandro; Carson, Laurence; Carvalho Akiba, Kazuyoshi; Casanova Mohr, Raimon; Casse, Gianluigi; Cassina, Lorenzo; Castillo Garcia, Lucia; Cattaneo, Marco; Cauet, Christophe; Cenci, Riccardo; Charles, Matthew; Charpentier, Philippe; Chefdeville, Maximilien; Chen, Shanzhen; Cheung, Shu-Faye; Chiapolini, Nicola; Chrzaszcz, Marcin; Cid Vidal, Xabier; Ciezarek, Gregory; Clarke, Peter; Clemencic, Marco; Cliff, Harry; Closier, Joel; Coco, Victor; Cogan, Julien; Cogneras, Eric; Cogoni, Violetta; Cojocariu, Lucian; Collazuol, Gianmaria; Collins, Paula; Comerma-Montells, Albert; Contu, Andrea; Cook, Andrew; Coombes, Matthew; Coquereau, Samuel; Corti, Gloria; Corvo, Marco; Counts, Ian; Couturier, Benjamin; Cowan, Greig; Craik, Daniel Charles; Crocombe, Andrew Christopher; Cruz Torres, Melissa Maria; Cunliffe, Samuel; Currie, Robert; D'Ambrosio, Carmelo; Dalseno, Jeremy; David, Pascal; David, Pieter; Davis, Adam; De Bruyn, Kristof; De Capua, Stefano; De Cian, Michel; De Miranda, Jussara; De Paula, Leandro; De Silva, Weeraddana; De Simone, Patrizia; Dean, Cameron Thomas; Decamp, Daniel; Deckenhoff, Mirko; Del Buono, Luigi; Déléage, Nicolas; Derkach, Denis; Deschamps, Olivier; Dettori, Francesco; Di Canto, Angelo; Di Domenico, Antonio; Dijkstra, Hans; Donleavy, Stephanie; Dordei, Francesca; Dorigo, Mirco; Dosil Suárez, Alvaro; Dossett, David; Dovbnya, Anatoliy; Dreimanis, Karlis; Dujany, Giulio; Dupertuis, Frederic; Durante, Paolo; Dzhelyadin, Rustem; Dziurda, Agnieszka; Dzyuba, Alexey; Easo, Sajan; Egede, Ulrik; Egorychev, Victor; Eidelman, Semen; Eisenhardt, Stephan; Eitschberger, Ulrich; Ekelhof, Robert; Eklund, Lars; El Rifai, Ibrahim; Elsasser, Christian; Ely, Scott; Esen, Sevda; Evans, Hannah Mary; Evans, Timothy; Falabella, Antonio; Färber, Christian; Farinelli, Chiara; Farley, Nathanael; Farry, Stephen; Fay, Robert; Ferguson, Dianne; Fernandez Albor, Victor; Ferreira Rodrigues, Fernando; Ferro-Luzzi, Massimiliano; Filippov, Sergey; Fiore, Marco; Fiorini, Massimiliano; Firlej, Miroslaw; Fitzpatrick, Conor; Fiutowski, Tomasz; Fol, Philip; Fontana, Marianna; Fontanelli, Flavio; Forty, Roger; Francisco, Oscar; Frank, Markus; Frei, Christoph; Frosini, Maddalena; Fu, Jinlin; Furfaro, Emiliano; Gallas Torreira, Abraham; Galli, Domenico; Gallorini, Stefano; Gambetta, Silvia; Gandelman, Miriam; Gandini, Paolo; Gao, Yuanning; García Pardiñas, Julián; Garofoli, Justin; Garra Tico, Jordi; Garrido, Lluis; Gascon, David; Gaspar, Clara; Gastaldi, Ugo; Gauld, Rhorry; Gavardi, Laura; Gazzoni, Giulio; Geraci, Angelo; Gersabeck, Evelina; Gersabeck, Marco; Gershon, Timothy; Ghez, Philippe; Gianelle, Alessio; Gianì, Sebastiana; Gibson, Valerie; Giubega, Lavinia-Helena; Gligorov, Vladimir; Göbel, Carla; Golubkov, Dmitry; Golutvin, Andrey; Gomes, Alvaro; Gotti, Claudio; Grabalosa Gándara, Marc; Graciani Diaz, Ricardo; Granado Cardoso, Luis Alberto; Graugés, Eugeni; Graverini, Elena; Graziani, Giacomo
2015-01-01T23:59:59.000Z
The time-dependent $CP$ asymmetry in $B_s^0 \\to J/\\psi K^+K^-$ decays is measured using $pp$ collision data, corresponding to an integrated luminosity of $3.0$fb$^{-1}$, collected with the LHCb detector at centre-of-mass energies of $7$ and $8$TeV. In a sample of 96 000 $B_s^0 \\to J/\\psi K^+K^-$ decays, the $CP$-violating phase $\\phi_s$ is measured, as well as the decay widths $\\Gamma_{L}$ and $\\Gamma_{H}$ of the light and heavy mass eigenstates of the $B_s^0-\\bar{B}_s^0$ system. The values obtained are $\\phi_s = -0.058 \\pm 0.049 \\pm 0.006$ rad, $\\Gamma_s \\equiv (\\Gamma_{L}+\\Gamma_{H})/2 = 0.6603 \\pm 0.0027 \\pm 0.0015$ps$^{-1}$, and$\\Delta\\Gamma_s \\equiv \\Gamma_{L} - \\Gamma_{H} = 0.0805 \\pm 0.0091 \\pm 0.0032$ps$^{-1}$, where the first uncertainty is statistical and the second systematic. These are the most precise single measurements of those quantities to date. A combined analysis with $B_s^{0} \\to J/\\psi \\pi^+\\pi^-$ decays gives $\\phi_s = -0.010 \\pm 0.039 $rad. All measurements are in agreement with the Sta...
Banaji,. Murad
2008-01-01T23:59:59.000Z
Großmann, H., Schwabe, R. & Gilmour S.G. (2009). Some new designs for firstorder interactions in 2K). Optimal design of factorial paired comparison experiments in the presence of withinpair order effects threelevel response surface designs. Großmann, H. & Schwabe, R. (2007). The relationship between optimal
DIRECT STEAM GENERATION USING THE SG4 500m2 PARABOLOIDAL DISH CONCENTRATOR
steam turbine power block. As well as DSG, the ANU group is investigating energy conversion options conveyed the steam to our 50 kWe steam turbine; the new dish is oversized for the current engine, so someDIRECT STEAM GENERATION USING THE SG4 500m2 PARABOLOIDAL DISH CONCENTRATOR Greg Burgess 1 , Keith
Domenico Solution--Is It Valid? by V. Srinivasan1, T.P. Clement2, and K.K. Lee3
Clement, Prabhakar
Domenico Solution--Is It Valid? by V. Srinivasan1, T.P. Clement2, and K.K. Lee3 Abstract +82-2-874- 1226; kklee@snu.ac.kr Received May 2006, accepted August 2006. Copyright Âª 2007 The Author
Gan, K. K.
that the main radiation effect is bulk damage in the VCSEL and PIN with the displacement of atoms. After five and VCSEL arrays coupled to radiation-hard ASICs produced for the current pixel optical link [5], the DORIC1 STUDY OF THE RADIATION HARDNESS OF VCSEL AND PIN ARRAYS K.K. GAN, W. FERNANDO, H.P. KAGAN, R
Measurement of D0-D0bar Mixing using the Ratio of Lifetimes for the Decays D0->K-pi+ and K+K-
The BABAR Collaboration; B. Aubert
2009-08-05T23:59:59.000Z
We measure the rate of D0-D0bar mixing with the observable yCP=(tauKpi/tauKK)-1, where tauKK and tauKpi are respectively the mean lifetimes of CP-even D0->K+K- and CP-mixed D0->K-pi+ decays, using a data sample of 384/fb collected by the Babar detector at the SLAC PEP-II asymmetric-energy B Factory. From a sample of D0 and D0bar decays where the inital flavor of the decaying meson is not determined, we obtain yCP = [1.12 +/- 0.26 (stat) +/- 0.22 (sys)]%, which excludes the no-mixing hypothesis at 3.3 sigma, including both statistical and systematic uncertainties. This result is in good agreement with a previous Babar measurement of yCP obtained from a sample of D*+->D0pi+ events, where the D0 decays to K-pi+, K+K-, and pi+pi-, which is disjoint with the untagged D0 events used here. Combining the two results taking into account statistical and systematic uncertainties, where the systematic uncertainties are assumed to be 100% correlated, we find yCP = [1.16 +/- 0.22 (stat) +/- 0.18 (sys)]%, which excludes the no-mixing hypothesis at 4.1 sigma.
Copy of FINAL SG Demo Project List 11 13 09-External.xls | Department of
Office of Environmental Management (EM)
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: Alternative1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level: National5Sales for4,645 3,625 1,006 492 742 33 1112011AT&T, Inc.'sEnergyTexas1.SpaceFluorControlsEnergy Copy of FINAL SG Demo
Ecosystem Approaches for Fisheries Management 609 Alaska Sea Grant College Program AK-SG-99-01, 1999
Ecosystem Approaches for Fisheries Management 609 Alaska Sea Grant College Program · AK-SG-99-01, 1999 Ecosystem Considerations and the Limitations of Ecosystem Models in Fisheries Management: Insights for the implementation of ecosystem approaches. The major criticism of single- species models is that they cannot predict
Comprehensive Amplitude Analysis of ????^{+}?^{-}, ?^{0}?^{0} and K?K below 1.5 GeV
Dai, Lingyun; Pennington, Michael R. [JLAB
2014-08-01T23:59:59.000Z
In this paper we perform an amplitude analysis of essentially all published pion and kaon pair production data from two photon collisions below 1.5 GeV. This includes all the high statistics results from Belle, as well as older data from Mark II at SLAC, CELLO at DESY, Crystal Ball at SLAC. The purpose of this analysis is to provide as close to a model-independent determination of the ?? to meson pair amplitudes as possible. Having data with limited angular coverage, typically |cos?| < 0.6-0.8, and no polarization information for reactions in which spin is an essential complication, the determination of the underlying amplitudes might appear an intractable problem. However, imposing the basic constraints required by analyticity, unitarity, and crossing-symmetry makes up for the experimentally missing information. Above 1.5 GeV multi-meson production channels become important and we have too little information to resolve the amplitudes. Nevertheless, below 1.5 GeV the two photon production of hadron pairs serves as a paradigm for the application of S-matrix techniques. Final state interactions among the meson pairs is critical to this analysis. To fix these, we include the latest ?? ? ??, K?K scattering amplitudes given by dispersive analyses, supplemented in the K?K threshold region by the recent precision Dalitz plot analysis from BaBar. With these hadronic amplitudes built into unitarity, we can constrain the overall description of ?? ? ?? and K?K datasets, both integrated and differential cross-sections, including the high statistics charged and neutral pion data from Belle. A region of solutions is found for the ?? ? ?? partial waves with both isospin 0 and 2. Since this analysis invokes coupled hadronic channels, even the relatively poor integrated cross-section data on ?? ? K?K narrows the patch of solutions to essentially a single form. For this we present the complete partial wave amplitudes, show how well they fit all the available data, and give the two photon couplings of scalar and tensor resonances that appear.
DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)
Aaltonen, T. [Helsinki Inst. of Physics; Gonzalez, Alvarez B. [Oviedo U., Cantabria Inst. of Phys.; Amerio, S. [INFN, Padua; Amidei, D. [Michigan U.; Anastassov, A. [Northwestern U.; Annovi, A. [Frascati; Antos, J [Comenius U.; Apollinari, G. [Fermilab; Appel, J. A [Fermilab; Apresyan, A. [Purdue; Arisawa, T. [Waseda U., Dubna, JINR
2011-08-01T23:59:59.000Z
We report the first reconstruction in hadron collisions of the suppressed decays B-? D(? K+?-)K- and B-? D(? K+?-)?- decays, sensitive to the CKM phase {gamma}, using data from 7 fb-1 of integrated luminosity collected by the CDF II detector at the Tevatron collider. We reconstruct a signal for the B-? D(? K+?-)K- suppressed mode with a significance of 3.2 standard deviations, and measure the ratios of the suppressed to favored branching fractions R(K) = [22.0 ± 8.6(stat) ± 2.6(syst)] x 10-3, R+(K) = [42.6 ± 13.7(stat) ± 2.8(syst)] x 10-3, R-(K) = [3.8 ± 10.3(stat) ± 2.7(syst)] x 10-3 as well as the direct CP-violating asymmetry A(K) = -0.82±0.44(stat)±0.09(syst) of this mode. Corresponding quantities for B- ? D(? K+?-)?- decay are also reported.
S. Giridhar; D. L. Lambert; G. Gonzalez
2000-08-28T23:59:59.000Z
Chemical compositions are derived from high-resolution spectra for five field SRd variables. These supergiants not previously analysed are shown to be metal-poor: KK Aql with [Fe/H] = -1.2, AG Aur with [Fe/H] = -1.8, Z Aur with [Fe/H] = -1.4, W LMi with [Fe/H] = -1.1, and WW Tau with [Fe/H] = -1.1. Their compositions are, except for two anomalies, identical to within the measurement errors with the compositions of subdwarfs, subgiants, and less evolved giants of the same [Fe/H]. One anomaly is an s-process enrichment for KK Aql, the first such enrichment reported for a SRd variable. The second and more remarkable anomaly is a strong lithium enrichment for W LMi, also a first for field SRds. The Li I 6707 A profile is not simply that of a photospheric line but includes strong absorption from red-shifted gas, suggesting, perhaps, that lithium enrichment results from accretion of Li-rich gas. This potential clue to lithium enrichment is discussed in light of various proposals for lithium synthesis in evolved stars.
Seismic Tomography Of Pg And Sg/lg And Its Use For Average Upper Crust Structure In Eurasia
Steck, Lee K [Los Alamos National Laboratory; Phillips, W Scott [Los Alamos National Laboratory; Rowe, C A [Los Alamos National Laboratory; Stead, R J [Los Alamos National Laboratory; Begnaud, M L [MSU
2008-01-01T23:59:59.000Z
Tomographic inversion oftravel times from first arriving compressional and shear waves for velocity structure has been applied with great success at all length scales, ranging from the laboratory bench-top to the entire Earth. Inversion of later arriving phases has seen a much more limited application. In this paper we present inversion results for regional Pg and Sg for the Eurasian continent to explore its use for understanding average upper crustal velocity structure. Inversion is performed using a damped, smoothed LSQR implementation that solves for site and event terms as well as for velocity along great circle paths between the source and receiver. Results are broadly consistent with published upper crustal velocities for the region. A spotcomparison of Vp/Vs from local and regional studies also compares well with the ratio of observed Pg to Sg velocities from our study where resolution is high. Resolution is determined through the use of checkerboard tests, and these suggest that in regions where data density is high we can resolve features down to at least 2 deg, with 4 deg possible over broader areas. RMS residual reductions are on the order of25% for Sg and 30% for Pg.
Pion Freeze-Out Time in Pb+Pb Collisions at 158 A GeV/c Studied via pi-/pi+ and K-/K+ Ratios
WA98 Collaboration
2006-07-16T23:59:59.000Z
The effect of the final state Coulomb interaction on particles produced in Pb+Pb collisions at 158 A GeV/c has been investigated in the WA98 experiment through the study of the pi-/pi+ and K-/K+ ratios measured as a function of transverse mass. While the ratio for kaons shows no significant transverse mass dependence, the pi-/pi+ ratio is enhanced at small transverse mass values with an enhancement that increases with centrality. A silicon pad detector located near the target is used to estimate the contribution of hyperon decays to the pi-/pi+ ratio. The comparison of results with predictions of the RQMD model in which the Coulomb interaction has been incorporated allows to place constraints on the time of the pion freeze-out.
CDF Collaboration; T. Aaltonen; S. Amerio; D. Amidei; A. Anastassov; A. Annovi; J. Antos; G. Apollinari; J. A. Appel; T. Arisawa; A. Artikov; J. Asaadi; W. Ashmanskas; B. Auerbach; A. Aurisano; F. Azfar; W. Badgett; T. Bae; A. Barbaro-Galtieri; V. E. Barnes; B. A. Barnett; P. Barria; P. Bartos; M. Bauce; F. Bedeschi; S. Behari; G. Bellettini; J. Bellinger; D. Benjamin; A. Beretvas; A. Bhatti; K. R. Bland; B. Blumenfeld; A. Bocci; A. Bodek; D. Bortoletto; J. Boudreau; A. Boveia; L. Brigliadori; C. Bromberg; E. Brucken; J. Budagov; H. S. Budd; K. Burkett; G. Busetto; P. Bussey; P. Butti; A. Buzatu; A. Calamba; S. Camarda; M. Campanelli; F. Canelli; B. Carls; D. Carlsmith; R. Carosi; S. Carrillo; B. Casal; M. Casarsa; A. Castro; P. Catastini; D. Cauz; V. Cavaliere; A. Cerri; L. Cerrito; Y. C. Chen; M. Chertok; G. Chiarelli; G. Chlachidze; K. Cho; D. Chokheli; A. Clark; C. Clarke; M. E. Convery; J. Conway; M. Corbo; M. Cordelli; C. A. Cox; D. J. Cox; M. Cremonesi; D. Cruz; J. Cuevas; R. Culbertson; N. d'Ascenzo; M. Datta; P. de Barbaro; L. Demortier; L. Marchese; M. Deninno; F. Devoto; M. D'Errico; A. Di Canto; B. Di Ruzza; J. R. Dittmann; M. D'Onofrio; S. Donati; M. Dorigo; A. Driutti; K. Ebina; R. Edgar; A. Elagin; R. Erbacher; S. Errede; B. Esham; S. Farrington; J. P. Fernández Ramos; R. Field; G. Flanagan; R. Forrest; M. Franklin; J. C. Freeman; H. Frisch; Y. Funakoshi; C. Galloni; A. F. Garfinkel; P. Garosi; H. Gerberich; E. Gerchtein; S. Giagu; V. Giakoumopoulou; K. Gibson; C. M. Ginsburg; N. Giokaris; P. Giromini; V. Glagolev; D. Glenzinski; M. Gold; D. Goldin; A. Golossanov; G. Gomez; G. Gomez-Ceballos; M. Goncharov; O. González López; I. Gorelov; A. T. Goshaw; K. Goulianos; E. Gramellini; C. Grosso-Pilcher; R. C. Group; J. Guimaraes da Costa; S. R. Hahn; J. Y. Han; F. Happacher; K. Hara; M. Hare; R. F. Harr; T. Harrington-Taber; K. Hatakeyama; C. Hays; J. Heinrich; M. Herndon; A. Hocker; Z. Hong; W. Hopkins; S. Hou; R. E. Hughes; U. Husemann; M. Hussein; J. Huston; G. Introzzi; M. Iori; A. Ivanov; E. James; D. Jang; B. Jayatilaka; E. J. Jeon; S. Jindariani; M. Jones; K. K. Joo; S. Y. Jun; T. R. Junk; M. Kambeitz; T. Kamon; P. E. Karchin; A. Kasmi; Y. Kato; W. Ketchum; J. Keung; B. Kilminster; D. H. Kim; H. S. Kim; J. E. Kim; M. J. Kim; S. B. Kim; S. H. Kim; Y. K. Kim; Y. J. Kim; N. Kimura; M. Kirby; K. Knoepfel; K. Kondo; D. J. Kong; J. Konigsberg; A. V. Kotwal; M. Kreps; J. Kroll; M. Kruse; T. Kuhr; M. Kurata; A. T. Laasanen; S. Lammel; M. Lancaster; K. Lannon; G. Latino; H. S. Lee; J. S. Lee; S. Leo; S. Leone; J. D. Lewis; A. Limosani; E. Lipeles; A. Lister; H. Liu; Q. Liu; T. Liu; S. Lockwitz; A. Loginov; A. Lucà; D. Lucchesi; J. Lueck; P. Lujan; P. Lukens; G. Lungu; J. Lys; R. Lysak; R. Madrak; P. Maestro; S. Malik; G. Manca; A. Manousakis-Katsikakis; F. Margaroli; P. Marino; K. Matera; M. E. Mattson; A. Mazzacane; P. Mazzanti; R. McNulty; A. Mehta; P. Mehtala; C. Mesropian; T. Miao; D. Mietlicki; A. Mitra; H. Miyake; S. Moed; N. Moggi; C. S. Moon; R. Moore; M. J. Morello; A. Mukherjee; Th. Muller; P. Murat; M. Mussini; J. Nachtman; Y. Nagai; J. Naganoma; I. Nakano; A. Napier; J. Nett; C. Neu; T. Nigmanov; L. Nodulman; S. Y. Noh; O. Norniella; L. Oakes; S. H. Oh; Y. D. Oh; I. Oksuzian; T. Okusawa; R. Orava; L. Ortolan; C. Pagliarone; E. Palencia; P. Palni; V. Papadimitriou; W. Parker; G. Pauletta; M. Paulini; C. Paus; T. J. Phillips; E. Pianori; J. Pilot; K. Pitts; C. Plager; L. Pondrom; S. Poprocki; K. Potamianos; F. Prokoshin; A. Pranko; F. Ptohos; G. Punzi; I. Redondo Fernández; P. Renton; M. Rescigno; F. Rimondi; L. Ristori; A. Robson; T. Rodriguez; S. Rolli; M. Ronzani; R. Roser; J. L. Rosner; F. Ruffini; A. Ruiz; J. Russ; V. Rusu; W. K. Sakumoto; Y. Sakurai; L. Santi; K. Sato; V. Saveliev; A. Savoy-Navarro; P. Schlabach; E. E. Schmidt; T. Schwarz; L. Scodellaro; F. Scuri; S. Seidel; Y. Seiya; A. Semenov; F. Sforza; S. Z. Shalhout; T. Shears; P. F. Shepard; M. Shimojima; M. Shochet; I. Shreyber-Tecker; A. Simonenko; K. Sliwa; J. R. Smith; F. D. Snider; V. Sorin; H. Song; M. Stancari; R. St. Denis; D. Stentz; J. Strologas; Y. Sudo; A. Sukhanov; I. Suslov; K. Takemasa; Y. Takeuchi; J. Tang; M. Tecchio; P. K. Teng; J. Thom; E. Thomson; V. Thukral; D. Toback; S. Tokar; K. Tollefson; T. Tomura; D. Tonelli; S. Torre; D. Torretta; P. Totaro; M. Trovato; F. Ukegawa; S. Uozumi; F. Vázquez; G. Velev; C. Vellidis; C. Vernieri; M. Vidal; R. Vilar; J. Vizán; M. Vogel; G. Volpi; P. Wagner; R. Wallny; S. M. Wang; D. Waters; W. C. Wester III; D. Whiteson; A. B. Wicklund; S. Wilbur; H. H. Williams; J. S. Wilson; P. Wilson; B. L. Winer; P. Wittich; S. Wolbers; H. Wolfe; T. Wright; X. Wu; Z. Wu; K. Yamamoto; D. Yamato; T. Yang; U. K. Yang; Y. C. Yang; W. -M. Yao; G. P. Yeh; K. Yi; J. Yoh; K. Yorita; T. Yoshida; G. B. Yu; I. Yu; A. M. Zanetti; Y. Zeng; C. Zhou; S. Zucchelli
2015-01-06T23:59:59.000Z
We report a measurement of the indirect CP-violating asymmetries ($A_{\\Gamma}$) between effective lifetimes of anticharm and charm mesons reconstructed in $D^0\\to K^+ K^-$ and $D^0\\to \\pi^+\\pi^-$ decays. We use the full data set of proton-antiproton collisions collected by the Collider Detector at Fermilab experiment and corresponding to $9.7$~fb$^{-1}$ of integrated luminosity. The strong-interaction decay $D^{*+}\\to D^0\\pi^+$ is used to identify the meson at production as $D^0$ or $\\overline{D}^0$. We statistically subtract $D^0$ and $\\overline{D}^0$ mesons originating from $b$-hadron decays and measure the yield asymmetry between anticharm and charm decays as a function of decay time. We measure $A_\\Gamma (K^+K^-) = (-0.19 \\pm 0.15 (stat) \\pm 0.04 (syst))\\%$ and $A_\\Gamma (\\pi^+\\pi^-)= (-0.01 \\pm 0.18 (stat) \\pm 0.03 (syst))\\%$. The results are consistent with the hypothesis of CP symmetry and their combination yields $A_\\Gamma = (-0.12 \\pm 0.12)\\%$.
Vazquez Sierra, Carlos
2015-01-01T23:59:59.000Z
CP violating phase ?s appears in b ? anti(c)cs transitions due to the interference between the direct decay and the decay after the Bs?-anti(Bs?) mixing. In SM, ?s = -2?s + ?P, where -2?s is related to CKM matrix elements and ?P is the penguin phase where contributions due to penguin diagrams are taken into account, being this ?P phase also the main source of theoretical uncertainty in ?s. This ?s phase is very sensitive to possible NP (new particles contributing to box diagrams during the mixing, several possible BSM scenarios are presented), so ?P should be estimated in order to disentangle these penguin pollution contributions from possible NP contributions, ?s(LHCb) = -2?s + ?P + ?NP. The decay Bs? ? J/? K?K? is a golden decay for ?s measurement: latest LHCb combined result also including Bs? ? J/? ???? measurements is ?s = -0.010 ± 0.039 rad, which is in excellent agreement with SM. The penguin pollution phase ?P can be estimated using B? ? J/? ?? and B...
Seul, K.W.; Bang, Y.S.; Lee, S.; Kim, H.J. [Korea Inst. of Nuclear Safety, Taejon (Korea, Republic of)
1996-09-01T23:59:59.000Z
The objective of the present work is to identify the predictability of RELAP5/MOD3.1 regarding thermal-hydraulic behavior during a steam generator tube rupture (SGTR). To evaluate the computed results, LSTF SB-SG-06 test data simulating the SGTR that occurred at the Mihama Unit 2 in 1991 are used. Also, some sensitivity studies of the code change in RELAP5, the break simulation model, and the break valve discharge coefficient are performed. The calculation results indicate that the RELAP5/MOD3.1 code predicted well the sequence of events and the major phenomena during the transient, such as the asymmetric loop behavior, reactor coolant system (RCS) cooldown and heat transfer by natural circulation, the primary and secondary system depressurization by the pressurizer auxiliary spray and the steam dump using the intact loop steam generator (SG) relief valve, and so on. However, there are some differences from the experimental data in the number of the relief valve cycling in the affected SG, and the flow regime of the hot leg with the pressurizer, and the break flow rates. Finally, the calculation also indicates that the coolant in the core could remain in a subcooled state as a result of the heat transfer caused by the natural circulation flow even if the reactor coolant pumps (RCPs) turned off and that the affected SG could be properly isolated to minimize the radiological release after the SGTR.
The WA102 Collaboration; D. Barberis et al
1999-03-18T23:59:59.000Z
A partial wave analysis of the centrally produced K+K- and K0K0 channels has been performed in pp collisions using an incident beam momentum of 450 GeV/c. An unambiguous physical solution has been found in each channel. The striking feature is the observation of peaks in the S-wave corresponding to the f0(1500) and fJ(1710) with J = 0. The D-wave shows evidence for the f2(1270)/a2(1320), the f2(1525) and the f2(2150) but there is no evidence for a statistically significant contribution in the D-wave in the 1.7 GeV mass region.
Allen, Bruce D.
107 Lucas, S.G., Morgan, G.S. and Zeigler, K.E., eds., 2005, New Mexico's Ice Ages, New Mexico of the large, topographically closed basins in New Mexico during the last ice age (Fig. 1). Compli- mentary-age Southwest. A comprehensive review of the known distribution of latest Pleis- tocene lakes in New Mexico
Dunbar, Nelia W.
95 Lucas, S.G., Morgan, G.S. and Zeigler, K.E., eds., 2005, New Mexico's Ice Ages, New Mexico a significant role in the geological evolution of New Mexico during the Quaternary. The extensional tec- tonic setting of New Mexico, together with pre-existing, long-lived zones of crustal weakness, has allowed
Barber, James R.
2013-01-01T23:59:59.000Z
/PICJ/Vol00000/130325/APPFile/SG-PICJ130325.3d (PIC) [PREPRINTER stage] Original Article The use the detailed implementation of the contact and friction laws. The reduced stiffness matrix is also an essential loading. Keywords Contact problems, static reduction, shakedown, Coulomb friction, substructuring, finite
Reif, John H.
a distribution channel. His articles on these topics have appeared in top-tier academic journals of Duke's academic council and also serves on the Academic Committee on Online Education (ACOE). #12;
Office of Energy Efficiency and Renewable Energy (EERE) 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: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels DataDepartment of Energy Your Density Isn'tOrigin ofEnergy atLLC - FE DKT. 10-160-LNG - ORDER 2913| Department of Energy PATRICIA
Canadian Solar Japan KK | Open Energy Information
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Toyo Aluminium KK | 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 onYou are now leaving Energy.gov You are now leaving Energy.gov You are beingZealand Jump to:Ezfeedflag JumpID-f <MaintainedInformationThePtyTown Hall Meeting JulyTown
Hao, Liang; Zhao, Yiqing; Hu, Xiaoyan; Zou, Shiyang [Institute of Applied Physics and Computational Mathematics, Beijing 100094 (China); Yang, Dong; Wang, Feng; Peng, Xiaoshi; Li, Zhichao; Li, Sanwei; Xu, Tao; Wei, Huiyue [Research Center of Laser Fusion, China Academy of Engineering Physics, Mianyang, Sichuan 621900 (China); Liu, Zhanjun; Zheng, Chunyang, E-mail: zheng-chunyang@iapcm.ac.cn [Institute of Applied Physics and Computational Mathematics, Beijing 100094 (China); Key Laboratory of HEDP of the Ministry of Education, CAPT, Peking University, Beijing 100871 (China)
2014-07-15T23:59:59.000Z
Experiments about the observations of stimulated Raman backscatter (SRS) and stimulated Brillouin backscatter (SBS) in Hohlraum were performed on Shenguang-III (SG-III) prototype facility for the first time in 2011. In this paper, relevant experimental results are analyzed for the first time with a one-dimension spectral analysis code, which is developed to study the coexistent process of SRS and SBS in Hohlraum plasma condition. Spectral features of the backscattered light are discussed with different plasma parameters. In the case of empty Hohlraum experiments, simulation results indicate that SBS, which grows fast at the energy deposition region near the Hohlraum wall, is the dominant instability process. The time resolved spectra of SRS and SBS are numerically obtained, which agree with the experimental observations. For the gas-filled Hohlraum experiments, simulation results show that SBS grows fastest in Au plasma and amplifies convectively in C{sub 5}H{sub 12} gas, whereas SRS mainly grows in the high density region of the C{sub 5}H{sub 12} gas. Gain spectra and the spectra of backscattered light are simulated along the ray path, which clearly show the location where the intensity of scattered light with a certain wavelength increases. This work is helpful to comprehend the observed spectral features of SRS and SBS. The experiments and relevant analysis provide references for the ignition target design in future.
Regulating User Arrivals at a Mobile IP Home Maulik Desai Thyaga Nandagopal
Shepard, Kenneth
. They require new hardware, which increases the capex and opex of the network operators, in addition
Zhou, Yaoqi
A Systematic Analysis of Epigenetic Genes across Different Stages of Lung Adenocarcinoma Akshay across different stages of lung adenocarcinoma (LUAD). Method: An integrative system biology approach
Hybrid fiber reinforced Composite Phenolic foam Amit Desai, Steven R. Nutt
Southern California, University of
Composite Center Hybrid Composite Phenolic foams were reinforced with glass and aramid fibers in different the hybrid foams exhibited higher strength and modulus as compared to foams reinforced with only glass with only glass fibers of different length , the elastic properties of foam such as modulus and density do
Credibility and flexibility : political institutions and foreign direct investment
Zheng, Yu
2007-01-01T23:59:59.000Z
Desai, Mihir, Fritz Foley, and James Hines. 2004, ForeignDesai, Mihir, Fritz Foley, and James Hines. 2005. ForeignDesai, Mihir, Fritz Foley, and James Hines. 2006. Capital
Nonroutine tasks in international trade
Oldenski, Lindsay
2009-01-01T23:59:59.000Z
4269. Desai, Mihir, Fritz Foley and James Hines Jr. , 2001,Desai, Mihir, Fritz Foley, and James Hines Jr. , 2002,W9224. Desai, Mihir, Fritz Foley and James Hines Jr. , 2001,
On the relationship of gravitational constants in KK reduction
Lu, J X
2000-01-01T23:59:59.000Z
In this short note, we try to clarify a seemly trivial but often confusing question in relating a higher-dimensional physical gravitational constant to its lower-dimensional correspondence in Kaluza-Klein reduction. In particular, we re-derive the low-energy M-theory gravitational constant in terms of type IIA string coupling $g_s$ and constant $\\alpha'$ through the metric relation between the two theories.
Resonances in Coupled ?K??K Scattering from Quantum Chromodynamics
DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)
Dudek, Jozef J.; Edwards, Robert G.; Thomas, Christopher E.; Wilson, David J.
2014-10-01T23:59:59.000Z
Using first-principles calculation within Quantum Chromodynamics, we are able to reproduce the pattern of experimental strange resonances which appear as complex singularities within coupled ?K, ?K scattering amplitudes. We make use of numerical computation within the lattice discretized approach to QCD, extracting the energy dependence of scattering amplitudes through their relation- ship to the discrete spectrum of the theory in a finite-volume, which we map out in unprecedented detail.
FIBERWISE KK-EQUIVALENCE OF CONTINUOUS FIELDS OF C ...
2008-01-04T23:59:59.000Z
Abstract. Let A and B be separable nuclear continuous C(X)-algebras over a fi- nite dimensional compact metrizable space X. It is shown that an element ? of the
ON THE KK-THEORY OF STRONGLY SELF-ABSORBING ...
2007-05-29T23:59:59.000Z
be simple and nuclear; moreover, they are either purely infinite or stably finite. The only known examples of strongly self-absorbing C?-algebras are the UHF ...
Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)
on the secondary side. The primary coolant is then returned to the reactor core via the coolant pump and the cycle is repeated. Feedwater (secondary coolant) is pumped into the...
Dorsett, D., and Merkenschlager, M. (2013). Curr. Opin. Cell Biol. 25, 327333.
von Andrian, Ulrich H.
2013-01-01T23:59:59.000Z
, M.B., Kundaje, A., Hariharan, M., Landt, S.G., Yan, K.K., Cheng, C., Mu, X.J., Khurana, E., Rozowsky.M., Acht- man, J.C., Jain, D.P., Cheng, Y., Hardison, R.C., and Blobel, G.A. (2012). Cell 150, 725. (2009). Genome Biol. 10, R80. Schaaf, C.A., Kwak, H., Koenig, A., Misulovin, Z., Gohara, D.W., Watson, A
Chen, Christopher S.
, Sophia Chen and Christopher S. Chen versus collective cell migration Contact inhibition of locomotion, Sophia Chen1 and Christopher S. Chen1, 1 Department of Bioengineering, University of Pennsylvania
A Data Mining and CIDF Based Approach for Detecting Novel and Distributed Intrusions
Lee, Wenke
, Rahul A. Nimbalkar 1 , Kam K. Yee 1 , Sunil B. Patil 1 , Pragneshkumar H. Desai 1 , Thuan T. Tran 1
6d (2, 0) Theory and M5 Branes: A KK Mode Approach
Hu, Shan
2013-07-16T23:59:59.000Z
C4 ! Z d2 Ba2 : (1.4) The tension of teh string is still proportional to the volume of Ca2 and will become tensionless when the volume of Ca2 approaches 0. Both C4 and D3 are selfdual, so in 6d, the tensor Ba2 and the strings are also selfdual... will appear as the strings. At the origin of moduli space, the M5-branes coincide and the strings become tensionless, in parallel with the Type IIB picture. Aside from the A-series, the D-series 6d (2, 0) theory can also be described in M theory...
The Case for Semantic Aware Remote Replication Xiaotao Liu, Gal Niv, K.K. Ramakrishnan
Fisher, Kathleen
efficiency and safe remote replication with tight recovery-point and recovery-time objectives. Using sys- tems is a high priority. However, these desirable proper- ties come at a price. First, because
S09 Symposium KK, Structure-Property Relationships in Biomineralized and Biomimetic Composites
David Kisailus; Lara Estroff; Himadri S. Gupta; William J. Landis; Pablo D. Zavattieri
2010-06-07T23:59:59.000Z
The technical presentations and discussions at this symposium disseminated and assessed current research and defined future directions in biomaterials research, with a focus on structure-function relationships in biological and biomimetic composites. The invited and contributed talks covered a diverse range of topics from fundamental biology, physics, chemistry, and materials science to potential applications in developing areas such as light-weight composites, multifunctional and smart materials, biomedical engineering, and nanoscaled sensors. The invited speakers were chosen to create a stimulating program with a mixture of established and junior faculty, industrial and academic researchers, and American and international experts in the field. This symposium served as an excellent introduction to the area for younger scientists (graduate students and post-doctoral researchers). Direct interactions between participants also helped to promote potential future collaborations involving multiple disciplines and institutions.
2012 SG Peer Review - Recovery Act: Secure Interoperable Open...
Broader source: Energy.gov (indexed) [DOE]
Project Objective Life-cycle Funding FY10 - FY13 45.4 m Technical Scope (Insert graphic here) 2 *Integrate Legacy and Smart Grid information systems *Integrate external...
2012 SG Peer Review - Recovery Act: Irvine Smart Grid Demonstration...
Broader source: Energy.gov (indexed) [DOE]
RD&D Needs Technical Challenges g Energy Smart Customer Devices * Impact of multiple Zero Net Energy technologies (grid and residential load) * PEV load management using...
Defect specific maintenance of SG tubes -- How safe is it?
Cizelj, L.; Mavko, B.; Dvorsek, T. [Jozef Stefan Institute, Ljubljana (Slovenia)
1997-02-01T23:59:59.000Z
The efficiency of the defect specific plugging criterion for outside diameter stress corrosion cracking at tube support plates is assessed. The efficiency is defined by three parameters: (1) number of plugged tubes, (2) probability of steam generator tube rupture and (3) predicted accidental leak rate through the defects. A probabilistic model is proposed to quantify the probability of tube rupture, while procedures available in literature were used to define the accidental leak rates. The defect specific plugging criterion was then compared to the performance of traditional (45%) plugging criterion using realistic data from Krsko nuclear power plant. Advantages of the defect specific approach over the traditional one are clearly shown. Some hints on the optimization of safe life of steam generator are also given.
Materials Data on VPO4 (SG:63) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Nd (SG:229) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on VP (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on P (SG:2) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on BPO4 (SG:152) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ge (SG:96) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ge (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ge (SG:148) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ge (SG:96) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on UGe2 (SG:63) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on UGe2 (SG:65) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ge (SG:69) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Microsoft Word - BBEE_BPA_in_template_SG__011013.doc
Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)
energy use and improve operating performance through building or equipment tune-ups and changes to O&M routines. Innovative Behavior-based Energy Efficiency Pilots -...
Materials Data on Nd (SG:229) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
2012 SG Peer Review - Recovery Act: LADWP Smart Grid Regional...
Funding (K) FY1011 - FY1516 60,280K Match Grant Technical Scope *Integrate Electric Vehicles into the LADWP grid *Demonstrate integrated Demand Response operation and...
Materials Data on Tc (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Er (SG:229) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on YB2 (SG:191) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on La (SG:229) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Tb (SG:229) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Dy (SG:229) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on YZn (SG:225) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Tm (SG:229) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Lu (SG:229) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
2012 SG Peer Review - Recovery Act: Pacific Northwest Smart Grid...
Broader source: Energy.gov (indexed) [DOE]
Management Approach 6 Metrics & Benefits Plan Conceptual Design Equipment Planning Data Collection and Reporting Asset System Non- Transactive Final Reporting & Operational...
Materials Data on B (SG:166) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Fe (SG:194) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on YS (SG:225) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Nd (SG:225) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on KC10 (SG:204) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Se (SG:148) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on VPt2 (SG:71) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ga (SG:139) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on S (SG:221) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Microsoft PowerPoint - Create Business Case for SG Implement...
Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)
(IT) A CIS Upgrade to accommodate AMI and DR functionality & Outage Management Demand Response (DR) The aggregated sum of 104 MW of DR from Residential, Commercial, and...
Materials Data on UAl2 (SG:227) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
SG Network System Requirements Specification- Interim Release 3 |
Office of Energy Efficiency and Renewable Energy (EERE) 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: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels DataDepartment of Energy Your Density Isn'tOrigin ofEnergy atLLC - FE DKT. 10-160-LNG - ORDER 2913| Department of Energy
Microsoft Word - SG_Roadmap_9-16.doc
Office of Environmental Management (EM)
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: Alternative1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level: National5Sales for4,645 3,625 1,006 492 742 33Frequently Asked Questions forCheneyNovemberi CONTENTS Executive U.S.and Geochemical3G-1Smart Grid
Microsoft Word - BBEE_BPA_in_template_SG__011013.doc
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: Alternative1 First Use of Energy for All Purposes (Fuel and Nonfuel), 2002; Level: National5Sales for4,645U.S. DOEThe Bonneville PowerCherries 82981-1cnHighandSWPA / SPRA / USACE SWPAURTeC:8 3. March 3, 20155-12, 2010DayWhat
Corporate Governance and Taxation
Dyck, Alexander
2004-01-01T23:59:59.000Z
Accounting and Corporate Governance,” Journal of Accounting1997) “A Survey of Corporate Governance” Journal of FinanceCorporate Governance and Taxation Mihir A. Desai* Harvard
Production of K?K? pairs in proton-proton collisions at 2.83 GeV
DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)
Ye, Q. J.; Hartmann, M.; Maeda, Y.; Barsov, S.; Büscher, M.; Chiladze, D.; Dymov, S.; Dzyuba, A.; Gao, H.; Gebel, R.; et al
2012-03-01T23:59:59.000Z
Differential and total cross sections for the pp?ppK?K? reaction have been measured at a proton beam energy of 2.83 GeV using the COSY-ANKE magnetic spectrometer. Detailed model descriptions fitted to a variety of one-dimensional distributions permit the separation of the pp?pp? cross section from that of non-? production. The differential spectra show that higher partial waves represent the majority of the pp?pp? total cross section at an excess energy of 76 MeV, whose energy dependence would then seem to require some s-wave ?p enhancement near threshold. The non-? data can be described in terms of the combined effects of two-bodymore »final state interactions using the same effective scattering parameters determined from lower energy data.« less
Production of K?K? pairs in proton-proton collisions at 2.83 GeV
DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)
Ye, Q. J.; Hartmann, M.; Maeda, Y.; Barsov, S.; Büscher, M.; Chiladze, D.; Dymov, S.; Dzyuba, A.; Gao, H.; Gebel, R.; Hejny, V.; Kacharava, A.; Keshelashvili, I.; Kiselev, Yu. T.; Khoukaz, A.; Koptev, V. P.; Kulessa, P.; Kulikov, A.; Lorentz, B.; Mersmann, T.; Merzliakov, S.; Mikirtytchiants, S.; Nekipelov, M.; Ohm, H.; Paryev, E. Ya.; Polyanskiy, A.; Serdyuk, V.; Stein, H. J.; Ströher, H.; Trusov, S.; Valdau, Yu.; Wilkin, C.; Wüstner, P.
2012-03-01T23:59:59.000Z
Differential and total cross sections for the pp?ppK?K? reaction have been measured at a proton beam energy of 2.83 GeV using the COSY-ANKE magnetic spectrometer. Detailed model descriptions fitted to a variety of one-dimensional distributions permit the separation of the pp?pp? cross section from that of non-? production. The differential spectra show that higher partial waves represent the majority of the pp?pp? total cross section at an excess energy of 76 MeV, whose energy dependence would then seem to require some s-wave ?p enhancement near threshold. The non-? data can be described in terms of the combined effects of two-body final state interactions using the same effective scattering parameters determined from lower energy data.
Orion: A Software Project Search Engine with Integrated Diverse Software Artifacts
Paris-Sud XI, Université de
@labri.fr, ferdianthung@smu.edu.sg, davidlo@smu.edu.sg, lxjiang@smu.edu.sg, reveillere@labri.fr Abstract
Desai, Narayan [ANL] [ANL
2011-10-12T23:59:59.000Z
Argonne National Lab's Narayan Desai on "Scaling MG-RAST to Terabases" at the Metagenomics Informatics Challenges Workshop held at the DOE JGI on October 12-13, 2011.
Chapman, Edwin R.
with the ex- domains (Brose et al., 1992; Davletov and Sudhof, 1993; Desai et al., 2000; Fernandez et al and SNAP-25/syntaxin. (Bai et al., 2002; Brose et al., 1992), syt·syt oligomeriza- tion (Wu et al., 2003
UCR Physics Grad School Welcome to UC Riverside!
Mills, Allen P.
Kawakami Jeanie Lau Doug MacLaughlinAllen P. Mills Umar Mohideen Jing Shi Harry Tom Roya Zandi Chandra Clare Bipin Desai John Ellison Bill Gary Gail Hanson Owen Long Ernest Ma Rich Seto Steve Wimpenny Jose
FIELD WORK (TD 609) Palsunda Village
Sohoni, Milind
PRA, Household survey, Water Resources Survey, Road and Transport Survey, Energy Survey, Agriculture thank Prof. Puru Kulkarni, Prof. Milind Sohoni, Raj Desai Sir and Hemant for providing valuable inputs
Desai, Narayan [ANL
2013-01-22T23:59:59.000Z
Argonne National Lab's Narayan Desai on "Scaling MG-RAST to Terabases" at the Metagenomics Informatics Challenges Workshop held at the DOE JGI on October 12-13, 2011.
Prescription Drug Monitoring Programs: Examining Limitations and Future Approaches
Griggs, Christopher A.; Weiner, Scott G.; Feldman, James A.
2015-01-01T23:59:59.000Z
Li G, Brady JE, Lang B, et al. Prescription drug monitoringand drug overdose mortality. Inj Epidemiol. 2014;1:1-9.EM, Desai HA. Prescription drug monitoring programs and
Materials Data on LaTl3 (SG:221) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ba3P4 (SG:43) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Sr3P4 (SG:43) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on K3Sb (SG:225) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Rb2Se (SG:225) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
2012 SG Peer Review - Recovery Act: AEP Ohio gridSMART Demonstration...
Broader source: Energy.gov (indexed) [DOE]
national impact. Life-cycle Funding 2010 - 2013 73,660,317 Technical Scope (Insert graphic here) * 110,000 AMI meters and associated infrastructure * Consumer Managed Energy...
Satisfying Real-Time Constraints with Custom Instructions panyu@comp.nus.edu.sg
Mitra, Tulika
have become popular as they strike the right balance between challenging perfor- mance requirement to lists, requires prior specific permission and/or a fee. CODES+ISSS'05, Sept. 1921, 2005, Jersey City instructions help simple embedded processors achieve con- siderable performance and energy efficiency
Materials Data on EuB6 (SG:221) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
U-068:Linux Kernel SG_IO ioctl Bug Lets Local Users Gain Elevated...
Broader source: Energy.gov (indexed) [DOE]
Linux Desktop (v. 6) Red Hat Enterprise Linux HPC Node (v. 6) Red Hat Enterprise Linux Server (v. 6) Red Hat Enterprise Linux Server AUS (v. 6.2) Red Hat Enterprise Linux Server...
Materials Data on LiCoPO4 (SG:62) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on HfCr2 (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on DyNi (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on ThRe2 (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Dy2SO2 (SG:164) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on MgPt (SG:198) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on FeClO (SG:59) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on PuCo3 (SG:166) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Fe3(O2F)2 (SG:1) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on FeS2 (SG:58) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Co3S4 (SG:227) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Mn2Nb (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Er(NiGe)2 (SG:139) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SrO (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ba2FeReO6 (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Al5Co2 (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ho2SO2 (SG:164) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on TbIr2 (SG:227) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on InN (SG:186) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ti5Sn3 (SG:193) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on PuGe2 (SG:141) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ba2CoReO6 (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ni3Sn (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Mn3O4 (SG:141) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Na2BHO3 (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Pr3GaC (SG:221) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on USnPt (SG:216) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CrO3 (SG:40) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Pb(CO2)2 (SG:2) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Er2C(NO)2 (SG:164) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SnPd (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ba2ReNiO6 (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on TaBe12 (SG:139) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on TiCo2Sn (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on HfAl2 (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ba2MgReO6 (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on ZrSnRh (SG:190) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on TbGaPd (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Pr2SO2 (SG:164) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CsIO3 (SG:221) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on GdGe (SG:63) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on YCrO3 (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Si2H2O3 (SG:148) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on BaTiO3 (SG:123) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ba2ZnReO6 (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Pu2Co (SG:189) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Tb2SO2 (SG:164) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Bi2O3 (SG:224) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Lu2SO2 (SG:164) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CdO2 (SG:205) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on TaMn2 (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on PrNbO4 (SG:15) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ba2MnReO6 (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CrO (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on GdNbO4 (SG:15) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ti2Be17 (SG:166) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CeInAu2 (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on U2Se3 (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LuB6 (SG:221) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on ErNbO4 (SG:15) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Na2O2 (SG:189) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LaSiIr (SG:198) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Er2SO2 (SG:164) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on La2SiO5 (SG:14) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Yb2SO2 (SG:164) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on UH12C4N4O11 (SG:14) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Mg5Si6 (SG:12) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Hierarchical Dirichlet Processes Yee Whye Teh tehyw@comp.nus.edu.sg
Kaski, Samuel
University of New York at Buffalo, Buffalo NY 14260-2000, USA David M. Blei blei@eecs.berkeley.edu Department. Beal is Assistant Professor of Computer Science and Engineering, SUNY Buffalo, NY; and David M. Blei
Materials Data on AlPt3C (SG:221) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Hierarchical Dirichlet Processes # Yee Whye Teh tehyw@comp.nus.edu.sg
Rattray, Magnus
, State University of New York at Buffalo, Buffalo NY 142602000, USA David M. Blei blei. Blei is Assistant Professor of Computer Science, Princeton University, NJ. Correspondences should
On the possible Uralic source for the gen. sg. a-stem desinence in Slavic
Greenberg, Marc L.
2003-01-01T23:59:59.000Z
The paper proposes that contact with Finnic languages led to reshaping of the genitive and possessive markers in Proto-Slavic.
Materials Data on AlPt3 (SG:221) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on GdGe (SG:63) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ba2MgReO6 (SG:225) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ba2ZnReO6 (SG:225) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Nb5(NiP)4 (SG:87) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ca3PN (SG:221) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on EuKPSe4 (SG:11) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LiZr2(PO4)3 (SG:14) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on KCa(PO3)3 (SG:188) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on NaPF6 (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CaPSe3 (SG:14) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Pr(ZnP)3 (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CoPSe (SG:61) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on P2W (SG:36) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Pr(CdP)3 (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SrAgP (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on NiMoP2 (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LiZnP (SG:216) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on ZnP2 (SG:96) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LuPPt (SG:187) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LiScP2O7 (SG:4) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Sr2Cu(PO4)2 (SG:12) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LiCdP (SG:216) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Cs(MnP)2 (SG:139) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Mg(P2Rh3)2 (SG:187) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on P2W (SG:12) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on ErP (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Sm(PRu)2 (SG:139) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Mg2Co12P7 (SG:174) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ce(P3Ru)4 (SG:204) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Na3PS3O (SG:36) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on BaPSe3 (SG:14) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ba(POs)2 (SG:139) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on NaErPO4F (SG:12) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Na2MgPO4F (SG:60) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Mo3P (SG:121) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on NpP (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on KVP2S7 (SG:5) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SrLiP (SG:187) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on MoP4 (SG:15) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on ZrP (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Zr(NiP)2 (SG:139) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LuP (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ni12P5 (SG:87) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on TiPRu (SG:189) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on ScNiP (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on NaYPO4F (SG:12) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on K4ZnP2 (SG:166) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on ZrMoP (SG:189) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ba3P14 (SG:14) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ca(PIr)2 (SG:154) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on P2Ir (SG:14) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SmPPd (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Er(PRu)2 (SG:139) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SrSnP (SG:129) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LiMgP (SG:216) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Nb5(PPd)4 (SG:87) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ba(PIr)2 (SG:139) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on FeP (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SrP3 (SG:12) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LiZnPS4 (SG:82) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CaPAu (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on BaAg(PO3)3 (SG:19) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Li2CuP (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Mg(Co3P2)2 (SG:187) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on NaPN2 (SG:122) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SmPPt (SG:187) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on YbNa(PS3)2 (SG:2) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ca2Co12P7 (SG:174) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ca5P12Rh19 (SG:189) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on PrPPd (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ni2P (SG:189) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on TiCrP (SG:189) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Na3Sr3GaP4 (SG:186) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on K2Mg(PSe3)2 (SG:14) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on BaPS3 (SG:14) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on BaLiP (SG:187) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CoH6(CO3)2 (SG:14) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on NdMg3 (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on KCd3H8Cl7O4 (SG:11) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Na3H5(CO2)4 (SG:2) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on InH8C4NO10 (SG:180) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on H4Pb(CO3)2 (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Sc2PbS4 (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Nb3H12C4NCl9 (SG:164) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ca(ScS2)2 (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CsTiF4 (SG:129) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on PbSO4 (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CuH3C2NO4 (SG:61) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on TiH8C4NO10 (SG:181) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LaH4C4NO8 (SG:14) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on TiH8C4NO10 (SG:180) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on H12W3C4NCl9 (SG:164) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SrCu2GeSe4 (SG:40) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on K2ZrGe2O7 (SG:15) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CdGeP2 (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SrLiGe2 (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Th(GeAu)2 (SG:139) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ca(GeRh)2 (SG:139) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ge(Te2As)2 (SG:166) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on K2ZrGe2O7 (SG:15) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Li(NiGe)6 (SG:191) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on PuGe2 (SG:141) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LiInGe (SG:216) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LaGe3Rh (SG:107) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ag6Ge2O7 (SG:4) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Mg(CoGe)6 (SG:191) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ge(Te2As)2 (SG:166) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on TiGePd (SG:189) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Tm2Ge2O7 (SG:92) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CaMgGe (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CeGe3Rh (SG:107) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LaCrGe3 (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on ZnAg2GeO4 (SG:7) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Tb2Ge2O7 (SG:92) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ge2Te5As2 (SG:164) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LiNdGe (SG:189) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CeScGe (SG:139) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LiSmGe (SG:189) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ho2Ge2Os (SG:12) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Zn3Ni2Ge (SG:227) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Tm2Ge2O7 (SG:92) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Lu4Zn5Ge6 (SG:36) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SrNi2Ge (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ca(GeIr)2 (SG:139) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SrCaGe (SG:62) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on NaAlGeO4 (SG:14) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Sm5Ge4 (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SrGe2 (SG:62) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on TmGe2 (SG:63) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on ZnNi2Ge (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SrMgGe (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Co2Ge (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on ZnAg2GeO4 (SG:7) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CaZn(GeO3)2 (SG:15) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on BaCaGe (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SrCaGe (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ca(GePd)2 (SG:139) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on PrCrGe3 (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Li2HgGe (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Th(GeAu)2 (SG:139) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SrCu2GeSe4 (SG:40) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Er(NiGe)2 (SG:139) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Li2ZnGe (SG:216) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Np(GeRh)2 (SG:139) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ni2Ge (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Cu2GeS3 (SG:9) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CaZn(GeO3)2 (SG:15) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Tb5Ge4 (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CeGe3Ir (SG:107) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on NdCoGe3 (SG:107) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Tm4Zn5Ge6 (SG:36) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on TiNiGe (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Tl2Ge2S5 (SG:15) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Li2GeO3 (SG:36) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CdGeO3 (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Na5GeAs3 (SG:14) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Tb2Ge2O7 (SG:92) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on La3(GeRh)4 (SG:71) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CaZnGe (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Er(AlGe)2 (SG:164) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on GePt3 (SG:140) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SrGe2 (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Dy(CrGe)2 (SG:139) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on NaAlGeO4 (SG:14) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LiNi2Ge (SG:225) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on ThGe2 (SG:63) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on ThGe2 (SG:65) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Np(GeRh)2 (SG:139) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on RbNa2Ge17 (SG:227) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ge9Pd25 (SG:147) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ho3Ge4 (SG:63) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on PrNiGe3 (SG:65) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Th2Ge (SG:140) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Nd5Ge3 (SG:193) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ho2InGe2 (SG:127) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Er3Al3NiGe2 (SG:189) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on TmTiGe (SG:129) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ge2Te5As2 (SG:164) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ge2Pt (SG:58) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Zr3(Cu2Ge)2 (SG:189) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on RbNa2Ge17 (SG:227) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CaCdGe (SG:189) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Nb5Ge3 (SG:140) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on CaCdGe (SG:189) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on BaCaGe (SG:62) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Zn3Ni2Ge (SG:227) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on HoGe (SG:63) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Lu4Zn5Ge6 (SG:36) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ca7Ge6 (SG:62) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SrNi3Ge2 (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ge3Os2 (SG:60) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SmCrGe3 (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on NdCrGe3 (SG:194) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on La3(GeRh)4 (SG:71) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LiHoGe (SG:189) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ca(GeIr)2 (SG:139) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Li(NiGe)6 (SG:191) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Li2SnGe (SG:216) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on PrGe3Rh (SG:107) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Dy(CrGe)2 (SG:139) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Na5GeAs3 (SG:14) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Tl2Ge2S5 (SG:15) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Tm4Zn5Ge6 (SG:36) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on PrCoGe3 (SG:107) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ge3Os2 (SG:60) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
2012 SG Peer Review - Recovery Act: KCP&L Green Impact Zone Smart...
Broader source: Energy.gov (indexed) [DOE]
Framework and Standards to accelerate industry adoption *IEC 61850 (substation protection & automation) *IEC 61850 (substation - control center) *DNPIP (field device to...
Measurement of the 208Pb(52Cr, n)259Sg Excitation Function
Folden III, C.M.
2010-01-01T23:59:59.000Z
of other measured cold fusion excitation functions (see Fig.in agreement with other cold fusion excitation functions,+b I. INTRODUCTION “Cold” nuclear fusion reactions, using Pb
Materials Data on K2Ni2(SO4)3 (SG:198) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on K2Ca2(SO4)3 (SG:19) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on K2Ca2(SO4)3 (SG:198) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on DyTh (SG:221) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Cd3In (SG:221) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on AlPt3 (SG:221) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Microsoft PowerPoint - E_forum_2_SG Benefits and Challenges_APPROVED...
Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)
natural disaster" Physical and cyber security built in from the ground up Reduces threat, vulnerability, consequences Deters, detects, mitigates, responds, and restores Less...
Materials Data on UB2Ir3 (SG:191) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Nb3Si (SG:221) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on ThB2Ir3 (SG:191) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SrTcO3 (SG:221) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Rb4Tc6S13 (SG:15) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Al12Tc (SG:204) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Tc2P3 (SG:12) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on TaTc (SG:221) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Al6Tc (SG:63) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on TiTc (SG:221) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Tc3P (SG:82) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on HfTc (SG:221) by Materials Project
DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]
Kristin Persson
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SmCuSe2 (SG:14) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on PrCuSe2 (SG:14) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LaCuSe2 (SG:14) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Field Enhancement of a Superconducting Helical Undulator with K. Flttmann, S.G. Wipf
. Geometry of a helical undulator with iron A helical field can be produced by a pair of conductors wound to form a double helix as sketched in Figure 1. The current in the two conductors is equal and of opposite of the coil ro= outer radius of the coil B = on axis field amplitude (1) A width of 1/3 is assumed
Materials Data on BaLaCuTe3 (SG:62) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on HoCd (SG:221) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on BaYCuTe3 (SG:63) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Yb(SiAu)2 (SG:139) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Y6Mn23 (SG:225) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Lu3InN (SG:221) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LuSi2 (SG:191) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on TmHg (SG:221) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LuIr (SG:221) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on TbSi2 (SG:191) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Lu2O3 (SG:206) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Er(PRu)2 (SG:139) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on YbSbPd (SG:216) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on BaYAgTe3 (SG:63) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Nd(FeSb3)4 (SG:204) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on YbTl (SG:221) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on La(SiAu)2 (SG:139) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on ErCd2 (SG:191) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on HoGa2 (SG:191) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LuZn (SG:221) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Sm(PRu)2 (SG:139) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on TmCd2 (SG:191) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on HoCd2 (SG:191) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LuN (SG:225) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LuB6 (SG:221) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on YbO (SG:225) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on HoPb3 (SG:221) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Sm(SiAu)2 (SG:139) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on HoSi2 (SG:191) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on La(SiAg)2 (SG:139) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on NdHg2 (SG:191) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Ho5Ni19P12 (SG:189) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on EuZn (SG:221) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on DyN (SG:225) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on YbSiAg (SG:189) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Yb(SiAg)2 (SG:139) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SrO (SG:225) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on V3Te4 (SG:12) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on InN (SG:186) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on BaGa2 (SG:191) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on KAg2PS4 (SG:121) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Sm(CoSi)2 (SG:139) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on MgS (SG:225) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on As2Ir (SG:14) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on MgTe (SG:216) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on FeS2 (SG:58) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Tm2CdSe4 (SG:227) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Sc3SnC (SG:221) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on ZnSnO3 (SG:161) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SrAl9Co2 (SG:191) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on La3Sn (SG:221) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on SnS (SG:63) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on MgSeO3 (SG:62) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on AlCrCu2 (SG:225) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on LiRhO2 (SG:166) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on PrPd3 (SG:221) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on TbPt3 (SG:221) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on Cs2Pt3S4 (SG:69) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations
Materials Data on BaO (SG:225) by Materials Project
Kristin Persson
2014-11-02T23:59:59.000Z
Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations