Search results for "Pauli exclusion principle"

showing 10 items of 52 documents

Composite Operator Method analysis of the underdoped cuprates puzzle

2014

The microscopical analysis of the unconventional and puzzling physics of the underdoped cuprates, as carried out lately by means of the Composite Operator Method (COM) applied to the 2D Hubbard model, is reviewed and systematized. The 2D Hubbard model has been adopted as it has been considered the minimal model capable to describe the most peculiar features of cuprates held responsible for their anomalous behavior. COM is designed to endorse, since its foundations, the systematic emergence in any SCS of new elementary excitations described by composite operators obeying non-canonical algebras. In this case (underdoped cuprates - 2D Hubbard model), the residual interactions - beyond a 2-pole…

PhysicsSuperconductivityCondensed Matter::Quantum GasesStrongly Correlated Electrons (cond-mat.str-el)Hubbard modelCondensed matter physicsCondensed Matter - SuperconductivityFOS: Physical sciencesFermi surfaceCondensed Matter Physicslcsh:QC1-999Superconductivity (cond-mat.supr-con)Minimal modelsymbols.namesakeCondensed Matter - Strongly Correlated ElectronsPauli exclusion principleCondensed Matter::SuperconductivitysymbolsAntiferromagnetismCuprateCondensed Matter::Strongly Correlated ElectronsPseudogaplcsh:Physics
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Shell structure in mixed3He−4Hedroplets

2004

Due to the immiscibility of ${}^{3}\mathrm{He}$ into ${}^{4}\mathrm{He}$ at very low temperatures, mixed helium droplets consist of a core of ${}^{4}\mathrm{He}$ atoms coated by a ${}^{3}\mathrm{He}$ layer whose thickness depends on the number of atoms of each isotope. When these numbers are such that the centrifugal kinetic energy of the ${}^{3}\mathrm{He}$ atoms is small and can be considered as a perturbation to the mean-field energy, a novel shell structure arises, with magic numbers different from these of pure ${}^{3}\mathrm{He}$ droplets. If the outermost shell is not completely filled, the valence atoms align their spins up to the maximum value allowed by the Pauli principle.

PhysicsValence (chemistry)Spinschemistry.chemical_elementKinetic energyAtomic and Molecular Physics and Opticssymbols.namesakeHelium-4Pauli exclusion principlechemistryMean field theoryHelium-3Physics::Atomic and Molecular ClusterssymbolsPhysics::Atomic PhysicsAtomic physicsHeliumPhysical Review A
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The Pauli Principle and Systems Consisting of Composite Particles

1993

In nature we often deal with many-body systems that are described in terms of particles that are not elementary but themselves composite. Examples of such composite particles are hadrons, atoms, phonons, and Cooper pairs. For the description of systems consisting of such composite particles in terms of the underlying degrees of freedom group theory plays an important role, in particular the symmetric group to describe the permutational symmetry of the wave function of the system, and unitary groups to describe the symmetry forced on the system by the interaction between the particles.

Physicssymbols.namesakeTheoretical physicsPauli exclusion principleSymmetric groupsymbolsDegrees of freedom (physics and chemistry)Cooper pairPermutation groupWave functionGroup theorySymmetry (physics)
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Magnetic properties of quantum dots and rings

2001

Exact many-body methods as well as current-spin-density functional theory are used to study the magnetism and electron localization in two-dimensional quantum dots and quasi-one-dimensional quantum rings. Predictions of broken-symmetry solutions within the density functional model are confirmed by exact configuration interaction (CI) calculations: In a quantum ring the electrons localize to form an antiferromagnetic chain which can be described with a simple model Hamiltonian. In a quantum dot the magnetic field localizes the electrons as predicted with the density functional approach.

Quantum phase transitionPhysicssymbols.namesakePauli exclusion principleCondensed matter physicsQuantum dotJelliumPrincipal quantum numbersymbolsElectronic structureMagnetic quantum numberQuantum numberAtomic and Molecular Physics and OpticsThe European Physical Journal D
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Dirac and Pauli form factors from lattice QCD

2011

We present a comprehensive analysis of the electromagnetic form factors of the nucleon from a lattice simulation with two flavors of dynamical O(a)-improved Wilson fermions. A key feature of our calculation is that we make use of an extensive ensemble of lattice gauge field configurations with four different lattice spacings, multiple volumes, and pion masses down to m_\pi ~ 180 MeV. We find that by employing Kelly-inspired parametrizations for the Q^2-dependence of the form factors, we are able to obtain stable fits over our complete ensemble. Dirac and Pauli radii and the anomalous magnetic moments of the nucleon are extracted and results at light quark masses provide evidence for chiral …

QuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeLattice field theoryNuclear TheoryFOS: Physical sciences7. Clean energy01 natural sciencessymbols.namesakePauli exclusion principleHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesddc:530Quantum field theory010306 general physicsQuantum chromodynamicsPhysics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)FermionLattice QCDJHigh Energy Physics - PhenomenologysymbolsNucleon
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Nucleon structure from Lattice QCD using a nearly physical pion mass

2014

We report the first Lattice QCD calculation using the almost physical pion mass mpi=149 MeV that agrees with experiment for four fundamental isovector observables characterizing the gross structure of the nucleon: the Dirac and Pauli radii, the magnetic moment, and the quark momentum fraction. The key to this success is the combination of using a nearly physical pion mass and excluding the contributions of excited states. An analogous calculation of the nucleon axial charge governing beta decay has inconsistencies indicating a source of bias at low pion masses not present for the other observables and yields a result that disagrees with experiment.

QuarkNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryLattice field theoryFOS: Physical sciencesLattice QCDNuclear Theory (nucl-th)Nucleon structureNuclear physicssymbols.namesakeHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Pauli exclusion principlePionddc:530Nuclear ExperimentPhysicsQuantum chromodynamicsIsovectorHigh Energy Physics - Lattice (hep-lat)Form factorsLattice QCDHigh Energy Physics - PhenomenologysymbolsHigh Energy Physics::ExperimentNucleonPhysics Letters B
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On the Pauli-Villars regularisation scheme in the NJL model

1993

Abstract We consider the Nambu-Jona-Lasinio model with a Pauli-Villars cutoff. We point out that previous attempts to use this regularisation have not been consistent and it is shown that if used correctly this approach yields very reasonable values for the cutoff parameter and quark condensate when we demand that ƒπ is fixed to its experimental value. Finally it is argued that because of its covariance and smooth nature this regularisation scheme has significant advantages over other regulators on the market.

QuarkPhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryStrong interactionElementary particleCovariancesymbols.namesakePauli exclusion principleRegularization (physics)Quantum electrodynamicssymbolsApplied mathematicsCutoffGauge theoryPhysics Letters B
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Quark exchange in deep inelastic scattering

1995

We use a model for baryons that links the constituent structure to the deep inelastic (current) properties. The approach consists in a laboratory partonic description (based on a model of hadron structure), to which a low momentum scaleQ 0 is adscribed, which is evolved to high momenta by means of the renormalization group. A generalization of the model by means of the hadronic quark cluster decomposition, provides a description of the structure functions of nuclei and is the starting point to study the effects that the antisymmetrization at the quark level has on the structure function of a model deuteron. The analysis contains conventional and high momentum partonic components. We next st…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHadronHigh Energy Physics::PhenomenologyNuclear TheoryFísicaRenormalization groupDeep inelastic scatteringBaryonNuclear physicsMomentumsymbols.namesakePauli exclusion principlesymbolsNuclear fusionHigh Energy Physics::ExperimentNuclear ExperimentParticle Physics - Phenomenology
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Microscopic description of the nucleon- Delta interaction in the quark cluster model.

1995

By using a nonrelativistic quark cluster model to describe baryonic systems, we generate a nucleon-{Delta} potential from the elementary interaction between constituents. The basic quark-quark potential used provides, when applied to the nucleon-nucleon system, an adequate description of the scattering phase shifts, the deuteron properties and the nonstrange baryonic spectroscopy. Special attention is paid to the short-range behavior of the interaction and its connection to the quark Pauli principle. This establishes a conceptual difference with meson-exchange models where the interaction, due to the lack of data, is not even well defined.

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryFew-body systemsBottom quarkDelta baryonBaryonsymbols.namesakePauli exclusion principlesymbolsCluster (physics)High Energy Physics::ExperimentNuclear ExperimentNucleonPhysical review. C, Nuclear physics
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About two equivalent descriptions of quark antisymmetrization

1992

We analyze the wave function for a two-hadron system when the quark symmetrization principle is incorporated. Two alternative mathematical descriptions are considered. The representation method of Hund constructs a system of generators of thesinglet⊗singlet type. The method of Young-Froebenius incorporates hidden-color components in order to describe the representation basis. By taking a naive model we show that the two descriptions, are equivalent and thus no physical meaning should be attached to their mathematical differences. The results of our analysis are then applied to the more realisticN-N (deuteron) system. We end by discussing the structure of the Pauli correlations which we comp…

QuarkPhysicsTheoretical physicssymbols.namesakeClassical mechanicsPauli exclusion principleBasis (linear algebra)symbolsSymmetrizationFunction (mathematics)Quantum field theoryRepresentation (mathematics)Wave functionIl Nuovo Cimento A
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