Search results for "quantum [statistics]"

showing 10 items of 4295 documents

Systematic trends in (0 0 1) surface ab initio calculations of ABO 3 perovskites

2018

This work was supported by the Latvian Council of Science Grant No. 374/2012 and the Latvian National Research Program IMIS2. Many stimulating discussions with D. Vanderbilt, K.M. Rabe, M. Rohlfing, E. Heifets, J. Maier, G. Borstel and E.A. Kotomin are greatly acknowledged.

B3LYPBand gapABO3 perovskitesPopulation02 engineering and technology01 natural scienceslcsh:ChemistryCrystalAb initio quantum chemistry methodsComputational chemistry0103 physical sciences:NATURAL SCIENCES:Physics [Research Subject Categories]Surface layer010306 general physicseducationPerovskite (structure)(0 0 1) surfaceseducation.field_of_studyCondensed matter physicsChemistryRelaxation (NMR)General Chemistry021001 nanoscience & nanotechnologyB3PWlcsh:QD1-999Chemical bondAb initio calculations0210 nano-technologyJournal of Saudi Chemical Society
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Comparative Ab Initio Calculations of ReO3, SrZrO3, BaZrO3, PbZrO3 and CaZrO3 (001) Surfaces

2020

We performed, for first time, ab initio calculations for the ReO2-terminated ReO3 (001) surface and analyzed systematic trends in the ReO3, SrZrO3, BaZrO3, PbZrO3 and CaZrO3 (001) surfaces using first-principles calculations. According to the ab initio calculation results, all ReO3, SrZrO3, BaZrO3, PbZrO3 and CaZrO3 (001) surface upper-layer atoms relax inwards towards the crystal bulk, all second-layer atoms relax upwards and all third-layer atoms, again, relax inwards. The ReO2-terminated ReO3 and ZrO2-terminated SrZrO3, BaZrO3, PbZrO3 and CaZrO3 (001) surface band gaps at the &Gamma

B3LYPMaterials scienceReO<sub>3</sub>Band gapABO3 perovskitesGeneral Chemical EngineeringPopulationab initio methodsAb initio02 engineering and technology010402 general chemistry01 natural sciencesMolecular physicsInorganic ChemistryCrystalABO<sub>3</sub> perovskitesAb initio quantum chemistry methodsAtomlcsh:QD901-999:NATURAL SCIENCES:Physics [Research Subject Categories]ReO3General Materials ScienceeducationPerovskite (structure)education.field_of_studyAb initio methods021001 nanoscience & nanotechnologyCondensed Matter Physics0104 chemical sciencesB3PWChemical bond(001) surfacelcsh:Crystallography0210 nano-technologyCrystals
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The Belle II Physics Book

2019

cd. autorów: L. Cao48,‡, G. Caria145,‡, G. Casarosa57,‡, C. Cecchi56,‡,D. Cˇ ervenkov10,‡,M.-C. Chang22,‡, P. Chang92,‡, R. Cheaib146,‡, V. Chekelian83,‡, Y. Chen154,‡, B. G. Cheon28,‡, K. Chilikin77,‡, K. Cho70,‡, J. Choi14,‡, S.-K. Choi27,‡, S. Choudhury35,‡, D. Cinabro170,‡, L. M. Cremaldi146,‡, D. Cuesta47,‡, S. Cunliffe16,‡, N. Dash33,‡, E. de la Cruz Burelo9,‡, E. de Lucia52,‡, G. De Nardo54,‡, †Editor. ‡Belle II Collaborator. §Theory or external contributing author. M. De Nuccio16,‡, G. De Pietro59,‡, A. De Yta Hernandez9,‡, B. Deschamps129,‡, M. Destefanis60,‡, S. Dey116,‡, F.Di Capua54,‡, S.Di Carlo75,‡, J. Dingfelder129,‡, Z. Doležal10,‡, I. Domínguez Jiménez125,‡, T.V. Dong30,26,…

B: semileptonic decayPhysics beyond the Standard ModelHadronelectroproduction [charmonium]General Physics and AstronomyComputingMilieux_LEGALASPECTSOFCOMPUTINGB: radiative decayannihilation [electron positron]7. Clean energy01 natural sciencescharmonium: electroproductionB physicsHigh Energy Physics - Experimentlaw.inventionHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Z'law[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Charm (quantum number)dark sector searchesPhysicslifetimeradiative decay [B]doublet [Higgs particle]new physicsPhysicsHigh Energy Physics - Lattice (hep-lat)ddc:530Electroweak interactionlepton: flavor: violationhep-phParticle Physics - LatticeMonte Carlo [numerical calculations]electron positron: colliding beamsQuarkoniumasymmetry: CPquarkonium physicselectroweak interaction: penguinHigh Energy Physics - PhenomenologyImproved performancecolliding beams [electron positron]CP violationinterfaceelectroproduction [quarkonium]electroweak precision measurementsnumerical calculations: Monte CarlophysicsParticle Physics - ExperimentperformanceParticle physicsflavor: violation [lepton]reviewhep-latFOS: Physical sciencesBELLEHigh Energy Physics - Experiment; High Energy Physics - Experiment; High Energy Physics - Lattice; High Energy Physics - Phenomenologyelectron positron: annihilationquarkonium: electroproductionCP [asymmetry]E(6)Higgs particle: doubletmixing [D0 anti-D0]Theoretical physicsCP: violation: time dependenceHigh Energy Physics - LatticeKEK-B0103 physical sciencesquantum chromodynamicshidden sector [photon]ddc:530composite010306 general physicsColliderParticle Physics - PhenomenologyHigh Energy Physics - Experiment; High Energy Physics - Lattice; High Energy Physics - Phenomenologyphoton: hidden sectorhep-ex010308 nuclear & particles physics[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat]C50 Other topics in experimental particle physicsviolation: time dependence [CP]D0 anti-D0: mixingB2TiP530 PhysikExperimental physicsB: leptonic decayCKM matrix[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]penguin [electroweak interaction]leptonic decay [B]semileptonic decay [B]charmparticle identificationexperimental results
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Top-quark pair + 1-jet production at next-to-leading order QCD

2008

Top-quark pair production with an additional jet is an important signal and background process at the LHC. We present the next-to-leading order QCD calculation for this process and show results for integrated as well as differential cross sections.

Background processQuantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsTop quarkLarge Hadron ColliderHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyOrder (ring theory)FOS: Physical sciencesJet (particle physics)Atomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyPair productionHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentDifferential (infinitesimal)
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Bader’s topological analysis of the electron density in the pressure-induced phase transitions/amorphization in α-quartz from the catastrophe theory …

2013

In this work, the Bader's topological analysis of the electron density, coupled with Thom's catastrophe theory, was used to characterize the pressure-induced transformations in α-quartz. In particular, ab initio calculations of the α-quartz structures in the range 0-105 Gpa have been performed at the HF/DFT exchange-correlation terms level, using Hamiltonians based on a WC1LYP hybrid scheme. The electron densities calculated throughout the ab initio wave functions have been analysed by means of the Bader's theory, seeking for some catastrophic mechanism in the sense of Thom's theory. The analysis mainly showed that there is a typical fold catastrophe feature involving an O-O interaction at …

Bader's topological analysiSettore GEO/06 - MineralogiaPhase transitionElectron densityCondensed matter physicsChemistryCatastrophe theoryAb initioQuartzElectronTopologyAmorphizationHigh pressureCondensed Matter::Materials ScienceGeochemistry and PetrologyAb initio quantum chemistry methodsGeneral Materials ScienceVector fieldCatastrophe theoryWave functionPhase transitionPhysics and Chemistry of Minerals
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Ab initio calculations of the atomic and electronic structure of BaZrO3 (111) surfaces

2013

Abstract The paper presents and discusses the results of calculations of surface relaxations and energetics for the polar (111) surface of BaZrO 3 using a hybrid B3LYP description of exchange and correlation. On the (111) surface, both Zr- and BaO 3 -terminations were analyzed. For both Zr and BaO 3 -terminated BaZrO 3 (111) surface upper layer atoms, with the sole exception of BaO 3 -terminated surface Ba atoms, relax inwards. The Zr-terminated BaZrO 3 (111) surface second layer Ba atoms exhibit the strongest relaxation between all Zr and BaO 3 -terminated BaZrO 3 (111) surface atoms. The calculated surface relaxation energy for Zr-terminated BaZrO 3 (111) surface is almost fifteen times l…

Band gapAb initio quantum chemistry methodsChemistryRelaxation (NMR)Ab initioGeneral Materials ScienceGeneral ChemistrySurface phononElectronic structureAtomic physicsCondensed Matter PhysicsSurface energySurface statesSolid State Ionics
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On-surface Synthesis of a Chiral Graphene Nanoribbon with Mixed Edge Structure.

2020

Abstract Chiral graphene nanoribbons represent an important class of graphene nanomaterials with varying combinations of armchair and zigzag edges conferring them unique structure‐dependent electronic properties. Here, we describe the on‐surface synthesis of an unprecedented cove‐edge chiral GNR with a benzo‐fused backbone on a Au(111) surface using 2,6‐dibromo‐1,5‐diphenylnaphthalene as precursor. The initial precursor self‐assembly and the formation of the chiral GNRs upon annealing are revealed, along with a relatively small electronic bandgap of approximately 1.6 eV, by scanning tunnelling microscopy and spectroscopy.

Band gapAnnealing (metallurgy)530 Physics010402 general chemistry01 natural sciencesBiochemistrygraphene nanoribbonNanomaterialslaw.inventionlawchiral edge540 Chemistrypolycyclic aromatic hydrocarbonon-surface synthesisSpectroscopyQuantum tunnelling010405 organic chemistryChemistryGraphenescanning tunneling microscopy and spectroscopyCommunicationOrganic ChemistryGeneral ChemistryCommunications0104 chemical sciencesZigzagChemical physics570 Life sciences; biologyGraphene nanoribbonsChemistry, an Asian journal
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First principles calculations of SrZrO3 bulk and ZrO2-terminated (001) surface F centers

2016

Abstract Using a supercell model and B3PW hybrid exchange-correlation functional in the framework of the density functional theory (DFT), as it is implemented in the CRYSTAL computer code, we performed ab initio calculations for the F -center located in the SrZrO 3 bulk and on the ZrO 2 -terminated (001) surface. According to the results of performed relaxation of atoms around the defect, two nearest Zr and four Sr atoms are repulsed, but all oxygen atoms are attracted towards both, the bulk and (001) surface F -center. The displacement magnitudes of atoms surrounding the bulk F -center are smaller than around the (001) surface F -center. The B3PW calculated SrZrO 3 bulk optical band gap (5…

Band gapChemistryMaterials Science (miscellaneous)Ab initioBulk F center02 engineering and technology021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesSrZrO3Electronic Optical and Magnetic Materials(001) surface F-CenterCrystalChemical bondAb initio quantum chemistry methodsVacancy defect0103 physical sciencesMaterials ChemistryDensity functional theoryAb initio calculationsAtomic physics010306 general physics0210 nano-technologyPerovskite (structure)Computational Condensed Matter
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Electron delocalization in mixed-valence Keggin polyoxometalates. Ab initio calculation of the local effective transfer integrals and its consequence…

2002

We present a quantitative evaluation of the influence of the electron transfer on the magnetic properties of mixed-valence polyoxometalates reduced by two electrons. For that purpose, we extract from valence-spectroscopy ab initio calculations on embedded fragments the value of the transfer integrals between W nearest-neighbor atoms in a mixed-valence alphaPW(12)O(40) polyoxowolframate Keggin anion. In contradiction with what is usually assumed, we show that the electron transfer between edge-sharing and corner-sharing WO(6) octahedra have very close values. Considering fragments of various ranges, we analyze the accuracy of calculations on fragments based on only two WO(5) pyramids which s…

Band gapelectron delocalizationAb initioElectronic structureElectron010402 general chemistry01 natural sciencesBiochemistryMolecular physicsCatalysisIonElectron transferColloid and Surface ChemistryAb initio quantum chemistry methodsComputational chemistrypolyoxometalesmixed-valenceValence (chemistry)010405 organic chemistryChemistryGeneral MedicineGeneral ChemistryConfiguration interaction0104 chemical sciencesmagnetismDiamagnetism[PHYS.COND.CM-SCE]Physics [physics]/Condensed Matter [cond-mat]/Strongly Correlated Electrons [cond-mat.str-el]
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From CCSD(T)/aug-cc-pVTZ-J to CCSD(T) complete basis set limit isotropic nuclear magnetic shieldings via affordable DFT/CBS calculations

2011

It is shown that a linear correlation exists between nuclear shielding constants for nine small inorganic and organic molecules (N2, CO, CO2, NH3, CH4, C2H2, C2H4, C2H6 and C6H6) calculated with 47 methods (42 DFT methods, RHF, MP2, SOPPA, SOPPA(CCSD), CCSD(T)) and the aug-cc-pVTZ-J basis set and corresponding complete basis set results, estimated from calculations with the family of polarization-consistent pcS-n basis sets. This implies that the remaining basis set error of the aug-cc-pVTZ-J basis set is very similar in DFT and CCSD(T) calculations. As the aug-cc-pVTZ-J basis set is significantly smaller, CCSD(T)/aug-cc-pVTZ-J calculations allow in combination with affordable DFT/pcS-n com…

Basis (linear algebra)ChemistryComputational chemistryIsotropyGeneral Materials ScienceGeneral ChemistryLimit (mathematics)Linear correlationScalingMolecular physicsQuantum chemistryBasis setOrganic moleculesMagnetic Resonance in Chemistry
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