Search results for "conductivity"

showing 10 items of 1988 documents

FERMION CONDENSATION, T -LINEAR RESISTIVITY AND PLANCKIAN LIMIT

2019

We explain recent challenging experimental observations of universal scattering rate related to the linear-temperature resistivity exhibited by a large corps of both strongly correlated Fermi systems and conventional metals. We show that the observed scattering rate in strongly correlated Fermi systems like heavy fermion metals and high-$T_c$ superconductors stems from phonon contribution that induce the linear temperature dependence of a resistivity. The above phonons are formed by the presence of flat band, resulting from the topological fermion condensation quantum phase transition (FCQPT). We emphasize that so - called Planckian limit, widely used to explain the above universal scatteri…

Condensed Matter::Quantum GasesPhysicsSuperconductivityQuantum phase transitionQuantum PhysicsStrongly Correlated Electrons (cond-mat.str-el)Physics and Astronomy (miscellaneous)Condensed matter physicsSolid-state physicsPhononFOS: Physical sciencesFermion01 natural sciences010305 fluids & plasmasCondensed Matter - Strongly Correlated ElectronsElectrical resistivity and conductivityLattice (order)Scattering rate0103 physical sciencesCondensed Matter::Strongly Correlated ElectronsQuantum Physics (quant-ph)010306 general physicsПИСЬМА В ЖУРНАЛ ЭКСПЕРИМЕНТАЛЬНОЙ И ТЕОРЕТИЧЕСКОЙ ФИЗИКИ
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Superfluidity of fermionic pairs in a harmonic trap. Comparative studies: Local Density Approximation and Bogoliubov-de Gennes solutions

2020

Abstract Experiments with ultracold gases on the lattice give the opportunity to realize superfluid fermionic mixtures in a trapping potential. The external trap modifies the chemical potential locally. Moreover, this trap also introduces non-homogeneity in the superconducting order parameter. There are, among other approaches, two methods which can be used to describe the system of two-component mixtures loaded into an optical lattice: the Local Density Approximation (LDA) and the self-consistent Bogoliubov–de Gennes equations. Here, we compare results obtained within these two methods. We conclude that the results can be distinguishable only in the case of a small value of the pairing int…

Condensed Matter::Quantum GasesPhysicsSuperfluiditySuperconductivityOptical latticeLattice (order)Quantum mechanicsPairingGeneral Physics and AstronomyTrappingLocal-density approximationJournal of Physics Communications
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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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Refrigeration bound of heat-producing cylinders by superfluid helium

2019

In this paper we go ahead in our studies on refrigeration of nanosystems by superfluid helium, as an appealing subject for future applications to computers or astronautical precision nanodevices. We first recall the effective thermal conductivity in laminar counterflow superfluid helium through arrays of mutually parallel cylinders and we discuss the conditions for the appearance of quantum turbulence around the heat-producing cylinders. We then consider the cooling of an array of heat-producing cylindrical nanosystems by means of superfluid-helium counterflow. We discuss the upper bound on heat removal set by avoidance of quantum turbulence and avoidance of phase transition to normal He I,…

Condensed Matter::Quantum GasesPhysics::Fluid Dynamicsthermal conductivity liquid helium quantum turbulence micropores quantized vortices computer refrigeration.Mathematics; PhysicsRefrigerationExtended Thermodynamicssuperfluid heliumPhysics::Atomic and Molecular Clusterslcsh:Science (General)Settore MAT/07 - Fisica MatematicaMSC: 76A25 76F99 80A99.lcsh:Q1-390
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Pairing in a three-component Fermi gas

2006

We consider pairing in a three-component gas of degenerate fermions. In particular, we solve the finite temperature mean-field theory of an interacting gas for a system where both interaction strengths and fermion masses can be unequal. At zero temperature we find a a possibility of a quantum phase transition between states associated with pairing between different pairs of fermions. On the other hand, finite temperature behavior of the three-component system reveals some qualitative differences from the two-component gas: for a range of parameters it is possible to have two different critical temperatures. The lower one corresponds to a transition between different pairing channels, while …

Condensed Matter::Quantum GasesQuantum phase transitionPhysicsPhase transitionCondensed matter physicsCondensed Matter - SuperconductivityDegenerate energy levelsFOS: Physical sciencesFermion01 natural sciencesAtomic and Molecular Physics and Optics010305 fluids & plasmasSuperconductivity (cond-mat.supr-con)SuperfluidityMean field theoryPairingQuantum mechanics0103 physical sciences010306 general physicsFermi gasPhysical Review A
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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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Quantum critical point in high-temperature superconductors

2009

Recently, in high-T_c superconductors (HTSC), exciting measurements have been performed revealing their physics in superconducting and pseudogap states and in normal one induced by the application of magnetic field, when the transition from non-Fermi liquid to Landau Fermi liquid behavior occurs. We employ a theory, based on fermion condensation quantum phase transition which is able to explain facts obtained in the measurements. We also show, that in spite of very different microscopic nature of HTSC, heavy-fermion metals and 2D 3He, the physical properties of these three classes of substances are similar to each other.

Condensed Matter::Quantum GasesQuantum phase transitionSuperconductivityPhysicsHigh-temperature superconductivityStrongly Correlated Electrons (cond-mat.str-el)Condensed matter physicsCondensed Matter - SuperconductivityFOS: Physical sciencesGeneral Physics and AstronomyFermionElectronic structurelaw.inventionSuperconductivity (cond-mat.supr-con)Condensed Matter - Strongly Correlated ElectronslawCondensed Matter::SuperconductivityQuantum critical pointStrongly correlated materialPseudogapPhysics Letters A
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Flat Bands and Salient Experimental Features Supporting the Fermion Condensation Theory of Strongly Correlated Fermi

2020

The physics of strongly correlated Fermi systems, being the mainstream topic for more than half a century, still remains elusive. Recent advancements in experimental techniques permit to collect important data, which, in turn, allow us to make the conclusive statements about the underlying physics of strongly correlated Fermi systems. Such systems are close to a special quantum critical point represented by topological fermion-condensation quantum phase transition which separates normal Fermi liquid and that with a fermion condensate, forming flat bands. Our review paper considers recent exciting experimental observations of universal scattering rate related to linear temperature dependence…

Condensed Matter::Quantum GasesQuantum phase transitionSuperconductivityPhysicsNuclear and High Energy PhysicsCondensed matter physics010308 nuclear & particles physicsFermion01 natural sciencesAtomic and Molecular Physics and OpticsElectrical resistivity and conductivityQuantum critical pointScattering rate0103 physical sciencesFermi liquid theory010306 general physicsFermi Gamma-ray Space TelescopePhysics of Atomic Nuclei
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Fulde-Ferrell-Larkin-Ovchinnikov superfluidity in one-dimensional optical lattices

2007

Spin-polarized attractive Fermi gases in one-dimensional (1D) optical lattices are expected to be remarkably good candidates for the observation of the Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) phase. We model these systems with an attractive Hubbard model with population imbalance. By means of the density-matrix renormalization-group method we compute the pairing correlations as well as the static spin and charge structure factors in the whole range from weak to strong coupling. We demonstrate that pairing correlations exhibit quasi-long range order and oscillations at the wave number expected from FFLO theory. However, we also show by numerically computing the mixed spin-charge static struc…

Condensed Matter::Quantum GasesSuperconductivity (cond-mat.supr-con)Condensed Matter - Strongly Correlated ElectronsStrongly Correlated Electrons (cond-mat.str-el)Condensed Matter - SuperconductivityFOS: Physical sciences
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Superconducting single-electron transistor and the phi-modulation of supercurrent

2002

An analytical expression for the supercurrent of a superconducting single-electron transistor (SSET) is derived. The derivation is based on analogy between the model Hamiltonian for E_J>E_C and a discrete, one-dimensional harmonic oscillator (1DDHO). The resulting supercurrent is nearly identical to the supercurrent obtained from a continuous harmonic oscillator Hamiltonian.

Condensed Matter::Quantum GasesSuperconductivity (cond-mat.supr-con)Condensed Matter - SuperconductivityCondensed Matter::SuperconductivityFOS: Physical sciencesCondensed Matter::Mesoscopic Systems and Quantum Hall Effect
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