Search results for "ASIP"

showing 10 items of 322 documents

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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Modified mode-coupling theory for the collective dynamics of simple liquids

2011

Recently it has been shown that mode-coupling theory, which accounts for the salient features of glassy relaxation near the liquid–glass transition, is also capable of describing the collective excitations of simple liquids away from the glass transition. In order to further improve the agreement between theory and computer simulations on Lennard-Jones argon we modify MCT by taking binary collisions into account. This, in fact, improves the agreement. We also show that multiplying the memory function of the original theory with a reduction factor leads to similar results.

CouplingChemistryFunction (mathematics)Condensed Matter PhysicsCondensed Matter::Disordered Systems and Neural NetworksCondensed Matter::Soft Condensed MatterReduction (complexity)Mode couplingQuasiparticleRelaxation (physics)General Materials ScienceStatistical physicsGlass transitionExcitationJournal of Physics: Condensed Matter
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Stability of chiral geometry in the odd–odd Rh isotopes: spectroscopy of 106Rh

2004

International audience; 136 P. Joshi et al. / Physics Letters B 595 (2004) 135–142AbstractThe nucleus 106Rh was populated using the reaction 96Zr(13C, p2n) at a beam energy of 51 MeV. γ -ray transitions wereidentified using the EUROBALL-IV γ -ray spectrometer and the DIAMANT charged particle array. The yrast band, which isbased upon a πg−19/2 ⊗ νh11/2 configuration, has been extended to I π = (22−). A new I = 1 band has been identified whichresides ∼ 300 keV above the yrast band. Core–quasiparticle coupling model calculations show reasonably good agreement withthe data. The properties of the two pairs of strongly coupled bands are consistent with a chiral interpretation for these states. 2…

CouplingPhysicsNuclear and High Energy PhysicsIsotopeSpectrometer010308 nuclear & particles physicsYrast[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesStability (probability)Charged particle0103 physical sciencesQuasiparticleAtomic physics010306 general physicsSpectroscopyNuclear ExperimentPhysics Letters B
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Microscopic quasiparticle–phonon description of beta decays of 113Cd and 115In using proton–neutron phonons

2007

Abstract The fourth-forbidden non-unique ground-state-to-ground-state beta decays of 113 Cd and 115 In are calculated using a realistic microscopic two-body interaction and a realistic single-particle model space. To describe the involved initial and final nuclear states we introduce a proton–neutron variant of the microscopic quasiparticle–phonon model (MQPM), the proton–neutron MQPM (pnMQPM). The states of the pnMQPM are created by coupling quasiparticles with phonons of the proton–neutron quasiparticle random-phase approximation (pnQRPA). The computed half-lives and log f t values are found to be in excellent agreement with experimental data. Computed beta spectra of the decays are also …

CouplingPhysicsNuclear and High Energy PhysicsProtonPhononNuclear TheorySpace (mathematics)Spectral lineNuclear physicsCondensed Matter::SuperconductivityBeta (plasma physics)QuasiparticleNeutronNuclear ExperimentPhysics Letters B
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