Search results for "quasiparticle"

showing 10 items of 280 documents

Hartree-Fock-Bogoliubov theory of polarized Fermi systems

2008

Condensed Fermi systems with an odd number of particles can be described by means of polarizing external fields having a time-odd character. We illustrate how this works for Fermi gases and atomic nuclei treated by density functional theory or Hartree-Fock-Bogoliubov (HFB) theory. We discuss the method based on introducing two chemical potentials for different superfluid components, whereby one may change the particle-number parity of the underlying quasiparticle vacuum. Formally, this method is a variant of non-collective cranking, and the procedure is equivalent to the so-called blocking. We present and exemplify relations between the two-chemical-potential method and the cranking approxi…

Condensed Matter::Quantum GasesPhysicsNuclear TheoryCondensed Matter - SuperconductivityNuclear TheoryHartree–Fock methodFOS: Physical sciencesAtomic and Molecular Physics and OpticsSuperconductivity (cond-mat.supr-con)Nuclear Theory (nucl-th)SuperfluidityQuantum mechanicsQuantum electrodynamicsAtomic nucleusQuasiparticleParity (mathematics)Nuclear theoryFermi Gamma-ray Space TelescopePhysical Review A
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Persistent currents in a circular array of Bose-Einstein condensates

2002

A ring-shaped array of Bose-Einstein condensed atomic gases can display circular currents if the relative phase of neighboring condensates becomes locked to certain values. It is shown that, irrespective of the mechanism responsible for generating these states, only a restricted set of currents are stable, depending on the number of condensates, on the interaction and tunneling energies, and on the total number of particles. Different instabilities due to quasiparticle excitations are characterized and possible experimental setups for testing the stability prediction are also discussed.

Condensed Matter::Quantum GasesPhysicsParticle numberCondensed matter physicsCondensed Matter (cond-mat)FOS: Physical sciencesCondensed MatterStability (probability)Atomic and Molecular Physics and Opticslaw.inventionCircular bufferlawQuasiparticleRelative phaseAtomic physicsBose–Einstein condensateQuantum tunnellingPhysical Review A
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Quasiparticles and quantum phase transition in universal low-temperature properties of heavy-fermion metals

2006

We demonstrate, that the main universal features of the low temperature experimental $H-T$ phase diagram of CeCoIn5 and other heavy-fermion metals can be well explained using Landau paradigm of quasiparticles. The main point of our theory is that above quasiparticles form so-called fermion-condensate state, achieved by a fermion condensation quantum phase transition (FCQPT). When a heavy fermion liquid undergoes FCQPT, the fluctuations accompanying above quantum critical point are strongly suppressed and cannot destroy the quasiparticles. The comparison of our theoretical results with experimental data on CeCoIn5 have shown that the electronic system of above substance provides a unique opp…

Condensed Matter::Quantum GasesPhysicsQuantum phase transitionStrongly Correlated Electrons (cond-mat.str-el)Condensed matter physicsCondensed Matter - SuperconductivityCondensationFOS: Physical sciencesGeneral Physics and AstronomyFermionSuperconductivity (cond-mat.supr-con)Condensed Matter - Strongly Correlated ElectronsQuantum critical pointHeavy fermionQuasiparticleCondensed Matter::Strongly Correlated ElectronsElectronic systemsPhase diagramEurophysics Letters (EPL)
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Quantum engineering of Majorana quasiparticles in one-dimensional optical lattices

2017

We propose a feasible way of engineering Majorana-type quasiparticles in ultracold fermionic gases on a one-dimensional (1D) optical lattice. For this purpose, imbalanced ultracold atoms interacting by the spin-orbit coupling should be hybridized with a three-dimensional Bose-Einstein condensate (BEC) molecular cloud. By constraining the profile of an internal defect potential we show that the Majorana-type excitations can be created or annihilated. This process is modelled within the Bogoliubov-de Gennes approach. This study is relevant also to nanoscopic 1D superconductors where modification of the internal defect potential can be obtained by electrostatic means.

Condensed Matter::Quantum GasesPhysicsSuperconductivityOptical latticeCondensed matter physicsCondensed Matter::OtherScatteringCondensed Matter - SuperconductivityFOS: Physical sciences02 engineering and technology021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesSuperconductivity (cond-mat.supr-con)Quantum technologyMAJORANACoupling (physics)Quantum Gases (cond-mat.quant-gas)Ultracold atom0103 physical sciencesQuasiparticleGeneral Materials ScienceCondensed Matter - Quantum Gases010306 general physics0210 nano-technologyJournal of Physics: Condensed Matter
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Quasiparticle Mean Field: BCS and Beyond

2007

In the previous two chapters we have laid the foundation for the BCS theory to describe open-shell nuclei. The properties of BCS solutions were compared with exact results from schematic solvable models. In this chapter we go into the details of numerical solution of the BCS equations. The implications of these solutions are discussed through applications to ds- and pf-shell nuclei.

Condensed Matter::Quantum GasesPhysicsTheoretical physicsExact resultsMean field theoryCondensed Matter::SuperconductivityNuclear TheoryQuasiparticleSchematicBCS theory
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Quantum critical point in ferromagnet

2008

Abstract The heavy-fermion metal CePd 1 - x Rh x can be tuned from ferromagnetism at x = 0 to non-magnetic state at the critical concentration x c . The non-Fermi liquid behavior at x ≃ x c is recognized by power law dependence of the specific heat C ( T ) given by the electronic contribution, susceptibility χ ( T ) and volume expansion coefficient α ( T ) at low temperatures: C / T ∝ χ ( T ) ∝ α ( T ) / T ∝ 1 / T . We show that this alloy exhibits a universal thermodynamic non-Fermi liquid behavior independent of magnetic ground state. This can be well understood utilizing the quasiparticle picture and the concept of fermion condensation quantum phase transition at the density ρ = p F 3 / …

Condensed Matter::Quantum GasesQuantum phase transitionPhysicsCondensed matter physicsFermionCondensed Matter PhysicsPower lawElectronic Optical and Magnetic MaterialsMomentumFerromagnetismQuantum critical pointQuasiparticleElectrical and Electronic EngineeringGround statePhysica B: Condensed Matter
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Asymmetrical tunneling in heavy fermion metals as a possible probe for their non-Fermi liquid peculiarities

2007

Tunneling conductivity and point contact spectroscopy between heavy fermion metal and a simple metallic point contact may serve as a convenient probing tool for non-Fermi liquid behavior. Landau Fermi liquid theory predicts that the differential conductivity is a symmetric function of voltage bias. This symmetry, in fact, holds if so called particle–hole symmetry is preserved. Here, we show that the situation can be different when one of the two metals is a heavy fermion one whose electronic system is a heavy fermion liquid. When the heavy fermion liquid undergoes fermion condensation quantum phase transition, the particle–hole symmetry in the excitation spectra is violated making both the …

Condensed Matter::Quantum GasesQuantum phase transitionPhysicsSuperconductivityCondensed matter physicsMechanical Engineeringmedia_common.quotation_subjectMetals and AlloysFermionAsymmetrySymmetry (physics)Landau theoryMechanics of MaterialsMaterials ChemistryQuasiparticleFermi liquid theorymedia_commonJournal of Alloys and Compounds
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Systematic approach toβand2νββdecays of massA=100–136nuclei

2015

In this work we perform a systematic study of pairs of single-$\ensuremath{\beta}$-decaying nuclei in the mass region $A=100--136$ to extract information on the effective value of the axial-vector coupling constant ${g}_{\mathrm{A}}$. As the many-body framework we use the quasiparticle random-phase approximation (QRPA) and its proton-neutron variant (pnQRPA) in single-particle valence bases with Woods-Saxon-calculated single-particle energies. It is found that, to a reasonable approximation, ${g}_{\mathrm{A}}$ is a linear function of the mass number $A$, with a slightly different parametrization below and above the mass $A=121$. Using the values of ${g}_{\mathrm{A}}$ extracted from the line…

Coupling constantPhysicsMass numberSemileptonic decayNuclear and High Energy PhysicsValence (chemistry)Excited stateQuasiparticleAtomic physicsGround statePhysical Review C
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Single and double beta decays in the , and triplets of isobars

2014

Abstract In this paper we analyze the ground-state-to-ground-state two-neutrino double beta ( 2 ν β β ) decays and single EC and β − decays for the A = 100 ( 100 Mo– 100 Tc– 100 Ru), A = 116 ( 116 Cd– 116 In– 116 Sn) and A = 128 ( 128 Te– 128 I– 128 Xe) triplets of isobars. We use the proton–neutron quasiparticle random-phase approximation (pnQRPA) with realistic G-matrix-derived effective interactions in very large single-particle bases. The purpose is to access the effective value of the axial-vector coupling constant g A in the pnQRPA calculations. We show that the three triplets of isobars represent systems with different characteristics of orbital occupancies and cumulative 2 ν β β nuc…

Coupling constantPhysicsNuclear and High Energy PhysicsQuasiparticleIsobarBeta (velocity)Atomic physicsNuclear Physics A
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Extracting information on the decays from the decays

2005

Abstract We have analyzed the relation between the two-neutrino ( 2 ν β β ) and neutrinoless ( 0 ν β β ) double beta decays of 76Ge, 82Se, 100Mo, and 116Cd. The relevant nuclear matrix elements have been calculated by using the proton–neutron quasiparticle random-phase approximation (pn-QRPA) with realistic two-body interactions. The dependence of the calculated matrix elements on the strength g pp of the particle–particle part of the proton–neutron two-body interaction is investigated. Recently a procedure was proposed where data on 2 ν β β -decay half-lives could be used to derive appropriate values of g pp for calculating the 0 ν β β -decay matrix elements. Following this procedure, we h…

Coupling constantPhysicsNuclear physicsNuclear and High Energy PhysicsMatrix (mathematics)Particle physicsDouble beta decayQuasiparticleObservableBeta (velocity)Nuclear Physics A
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