Search results for "Many-Body"

showing 10 items of 87 documents

The composite operator method route to the 2D Hubbard model and the cuprates

2018

In this review paper, we illustrate a possible route to obtain a reliable solution of the 2D Hubbard model and an explanation for some of the unconventional behaviours of underdoped high-$T_\text{c}$ cuprate superconductors within the framework of the composite operator method. The latter is described exhaustively in its fundamental philosophy, various ingredients and robust machinery to clarify the reasons behind its successful applications to many diverse strongly correlated systems, controversial phenomenologies and puzzling materials.

Electronic structureСильно скорельованi системиHubbard modelPhysics and Astronomy (miscellaneous)Hubbard modelFOS: Physical sciencesЕлектронна структура01 natural sciencesComposite operatorПсевдощiлинаTheoretical physicsCondensed Matter - Strongly Correlated ElectronsCupratesCondensed Matter::Superconductivity0103 physical sciencesCuprateбагаточастинковi методи010306 general physicsStrongly correlated systemsКупрати010302 applied physicsPhysicsPseudogapCuprates; Electronic structure; Hubbard model; Many-body techniques; Pseudogap; Strongly correlated systems; багаточастинковi методи; Електронна структура; Купрати; Модель Хаббарда; Псевдощiлина; Сильно скорельованi системи;Strongly Correlated Electrons (cond-mat.str-el)Many-body techniquesCondensed Matter Physicslcsh:QC1-999Модель ХаббардаCondensed Matter::Strongly Correlated Electronslcsh:Physics
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Computational nuclear quantum many-body problem: The UNEDF project

2013

The UNEDF project was a large-scale collaborative effort that applied high-performance computing to the nuclear quantum many-body problem. The primary focus of the project was on constructing, validating, and applying an optimized nuclear energy density functional, which entailed a wide range of pioneering developments in microscopic nuclear structure and reactions, algorithms, high-performance computing, and uncertainty quantification. UNEDF demonstrated that close associations among nuclear physicists, mathematicians, and computer scientists can lead to novel physics outcomes built on algorithmic innovations and computational developments. This review showcases a wide range of UNEDF scien…

Energy density functionalNuclear Theoryta114Computer scienceFOS: Physical sciencesGeneral Physics and AstronomyComputerApplications_COMPUTERSINOTHERSYSTEMSSupercomputerNuclear Theory (nucl-th)Many-body problemRange (mathematics)Hardware and ArchitectureSystems engineeringStatistical physicsUncertainty quantificationQuantumNuclear theoryComputer Physics Communications
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Large-N kinetic theory for highly occupied systems

2018

We consider an effective kinetic description for quantum many-body systems, which is not based on a weak-coupling or diluteness expansion. Instead, it employs an expansion in the number of field components N of the underlying scalar quantum field theory. Extending previous studies, we demonstrate that the large-N kinetic theory at next-to-leading order is able to describe important aspects of highly occupied systems, which are beyond standard perturbative kinetic approaches. We analyze the underlying quasiparticle dynamics by computing the effective scattering matrix elements analytically and solve numerically the large-N kinetic equation for a highly occupied system far from equilibrium. T…

Field (physics)Lattice field theoryFOS: Physical sciencesFixed point01 natural sciencesMany-body problemHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencessirontanonperturbative effects in field theoryQuantum field theory010306 general physicsdynamiikkaPhysicsta114010308 nuclear & particles physicsScalar (physics)finite temperature field theoryultracold gasesHigh Energy Physics - PhenomenologyDistribution functionClassical mechanicsQuantum Gases (cond-mat.quant-gas)Kinetic theory of gaseskvanttikenttäteoriaCondensed Matter - Quantum Gasesrelativistic heavy-ion collisions
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Approximate energy functionals for one-body reduced density matrix functional theory from many-body perturbation theory

2018

We develop a systematic approach to construct energy functionals of the one-particle reduced density matrix (1RDM) for equilibrium systems at finite temperature. The starting point of our formulation is the grand potential $\Omega [\mathbf{G}]$ regarded as variational functional of the Green's function $G$ based on diagrammatic many-body perturbation theory and for which we consider either the Klein or Luttinger-Ward form. By restricting the input Green's function to be one-to-one related to a set on one-particle reduced density matrices (1RDM) this functional becomes a functional of the 1RDM. To establish the one-to-one mapping we use that, at any finite temperature and for a given 1RDM $\…

Grand potentialSolid-state physicsComplex systemFOS: Physical sciencesdensity matrix functional theory01 natural sciencesCondensed Matter - Strongly Correlated Electronssymbols.namesakePhysics - Chemical Physics0103 physical sciencesSDG 7 - Affordable and Clean Energy010306 general physicsMathematical physicsEnergy functionalChemical Physics (physics.chem-ph)PhysicsQuantum Physics/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyStrongly Correlated Electrons (cond-mat.str-el)010304 chemical physicstiheysfunktionaaliteoriamany-body perturbation theory16. Peace & justiceCondensed Matter PhysicsStationary pointElectronic Optical and Magnetic MaterialsCondensed Matter - Other Condensed Matterapproximate energy functionalssymbolsReduced density matrixapproksimointiQuantum Physics (quant-ph)Hamiltonian (quantum mechanics)Ground stateOther Condensed Matter (cond-mat.other)The European Physical Journal B
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Soft-dielectron excess in proton-proton collisions at $\sqrt{s}$ = 13 TeV

2021

Physical review letters 127(4), 042302 (2021). doi:10.1103/PhysRevLett.127.042302

HadronGeneral Physics and Astronomylow [transverse momentum]dielectron productionscattering [hadron hadron]01 natural sciencesSpectral lineQUARK-GLUON PLASMAHigh Energy Physics - ExperimentMany-body problemHigh Energy Physics - Experiment (hep-ex)ALICEscattering [p p][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]multiplicityInvariant massDielectronNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear Experimenthadron-hadron scatteringAU COLLISIONSPhysicsQuantum chromodynamicsbremsstrahlung: hadronicLarge Hadron Colliderradiation: thermalPhysicsMUON PAIRSPHOTON PRODUCTIONBremsstrahlungELECTRON-PAIR PRODUCTIONddc:hadron: decayCERN LHC CollkinematicsMASS DILEPTON PRODUCTIONmany-body problemMASS DILEPTON PRODUCTION; ELECTRON-PAIR PRODUCTION; SPACE-TIME EVOLUTION; ETA-MESON PRODUCTION; QUARK-GLUON PLASMA; PHOTON PRODUCTION; NUCLEUS COLLISIONS; AU COLLISIONS; P-BE; MUON PAIRShadron hadron: scatteringParticle Physics - ExperimentParticle physicsp p: scatteringETA-MESON PRODUCTIONtransverse momentum: lowFOS: Physical sciencesthermal [radiation]Physics and Astronomy(all)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]5300103 physical sciencesSPACE-TIME EVOLUTIONddc:530Nuclear Physics - ExperimentMultiplicity (chemistry)010306 general physicsenhancementp nucleus: scatteringP-BEhadronic [bremsstrahlung]ALICE particle physics010308 nuclear & particles physicsALICE experimentparametrizationscattering [p nucleus]p p: scattering ; bremsstrahlung: hadronic ; transverse momentum: low ; p nucleus: scattering ; radiation: thermal ; hadron: decay ; hadron hadron: scattering ; CERN LHC Coll ; enhancement ; ALICE ; many-body problem ; parametrization ; multiplicity ; acceptance ; kinematics ; experimental results ; 13000 GeV-cms/nucleon13000 GeV-cms/nucleonHigh Energy Physics::ExperimentNUCLEUS COLLISIONSdecay [hadron]ALICE experiment dielectron production hadron-hadron scatteringacceptanceexperimental results
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Elementary presentation of self‐consistent intermediate Hamiltonians and proposal of two totally dressed singles and doubles configuration interactio…

1994

Intermediate Hamiltonians are effective Hamiltonians which are defined on an N‐dimensional model space but which only provide n<N exact eigenvalues and the projections of the corresponding eigenvectors onto the model space. For a single root research, the intermediate Hamiltonian may be obtained from the restriction of the Hamiltonian to the model space by an appropriate, uniquely defined dressing of the diagonal energies or of the first column. Approximate self‐consistent dressings may be proposed. The simplest perturbative form gives the same result as the original 2nd order intermediate Hamiltonian or the ‘‘shifted Bk’’ technique but it is of easier implementation. Self‐consistent inclus…

HamiltoniansHamiltonians ; Configuration Interaction ; Scf Calculations ; Eigenvalues ; Eigenvectors ; Degeneration ; Many−Body Problem ; Electronic StructureDiagonalGeneral Physics and AstronomyElectronic structureMany−Body ProblemMany-body problemsymbols.namesakePauli exclusion principleQuantum mechanicsPhysical and Theoretical Chemistry:FÍSICA::Química física [UNESCO]Eigenvalues and eigenvectorsMathematical physicsMathematicsDegenerate energy levelsEigenvaluesScf CalculationsConfiguration interactionUNESCO::FÍSICA::Química físicaConfiguration InteractionElectronic StructureDegenerationsymbolsEigenvectorsHamiltonian (quantum mechanics)The Journal of Chemical Physics
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Spectroscopy of short-lived radioactive molecules: A sensitive laboratory for new physics

2019

The study of molecular systems provides exceptional opportunities for the exploration of the fundamental laws of nature and for the search for physics beyond the Standard Model of particle physics. Measurements of molecules composed of naturally occurring nuclei have provided the most stringent upper bounds to the electron electric dipole moment to date, and offer a route to investigate the violation of fundamental symmetries with unprecedented sensitivity. Radioactive molecules - where one or more of their atoms possesses a radioactive nucleus - can contain heavy and deformed nuclei, offering superior sensitivity for EDM measurements as well as for other symmetry-violating effects. Radium …

High Energy Physics - TheoryexceptionalNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]collinearFOS: Physical sciencesnucleus: structure function[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)ionizationPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear Experimentenhancementnew physics[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]stabilitysensitivitylaserradiumelectron: electric momentHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)radioactivity[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]many-body problemnucleus: deformation
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Challenges in truncating the hierarchy of time-dependent reduced density matrices equations

2012

In this work, we analyze the Born, Bogoliubov, Green, Kirkwood, and Yvon (BBGKY) hierarchy of equations for describing the full time evolution of a many-body fermionic system in terms of its reduced density matrices (at all orders). We provide an exhaustive study of the challenges and open problems linked to the truncation of such a hierarchy of equations to make them practically applicable. We restrict our analysis to the coupled evolution of the one- and two-body reduced density matrices, where higher-order correlation effects are embodied into the approximation used to close the equations. We prove that within this approach, the number of electrons and total energy are conserved, regardl…

Hubbard modelta114PhysicsComplex systemdensity matricesmany-body fermionic systemElectronCondensed Matter PhysicsBBGKY hierarchy01 natural sciencesInstability010305 fluids & plasmasElectronic Optical and Magnetic MaterialsequationsQuantum mechanics0103 physical sciencesCompatibility (mechanics)Strongly correlated materialStatistical physics010306 general physicsMathematicsElectronic density
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Correlating Schiff Moments in the Light Actinides with Octupole Moments

2018

We show that the measured intrinsic octupole moments of $^{220}$Rn, $^{224}$Ra, and $^{226}$Ra constrain the intrinsic Schiff moments of $^{225}$Ra$^{221}$Rn, $^{223}$Rn, $^{223}$Fr, $^{225}$Ra, and $^{229}$Pa. The result is a dramatically reduced uncertainty in intrinsic Schiff moments. Direct measurements of octupole moments in odd nuclei will reduce the uncertainty even more. The only significant source of nuclear-physics error in the laboratory Schiff moments will then be the intrinsic matrix elements of the time-reversal non-invariant interaction produced by CP-violating fundamental physics. Those matrix elements are also correlated with octupole moments, but with a larger systematic u…

INTRINSIC REFLECTION ASYMMETRYPARAMETRIZATIONnuclear many-body theoryODDNuclear TheoryNUCLEInuclear density functional theorySKYRME INTERACTIONFOS: Physical sciencesRA-225114 Physical sciencesnuclear structure and decays3100Nuclear Theory (nucl-th)FORCESydinfysiikkanuclear tests of fundamental interactions
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Relativistic corrections and unitary equivalence in elastic electron deuteron scattering.

1993

The role of unitary equivalence of relativistic corrections in elastic electron deutron scattering is studied, starting from a class of approximately, unitarily equivalent Hamiltonians and using consistent charge density operators. The connection of various formal approaches for deriving the relativistic corrections to wave functions and operators are discussed in detail. For reasons of simplicity, we have chosen a pure one-pion-exchange model and calculated the charge and quadrupole form factors of the deuteron. The numerical results show that the unitary equivalence holds at small momentum transfers, but breaks down rather soon with increasing momentum transfers (\ensuremath{\lesssim}5 ${…

Many-body problemElastic scatteringMomentumPhysicsNuclear and High Energy PhysicsScatteringQuantum mechanicsCharge (physics)Connection (algebraic framework)Few-body systemsWave functionPhysical review. C, Nuclear physics
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