Search results for "conductivity"

showing 10 items of 1988 documents

The quantum phase slip phenomenon in superconducting nanowires with a low-Ohmic environment

2012

In a number of recent experiments it has been demonstrated that in ultra-narrow superconducting channels quantum fluctuations of the order parameter, alternatively called quantum phase slips, are responsible for the finite resistance well below the critical temperature. The acceptable agreement between those experiments and the models describing quantum fluctuations in quasi-one-dimensional superconductors has been established. However the very concept of the phase slip is justified when these fluctuations are the relatively rare events, meaning that the effective resistance of the system should be much smaller than the normal state equivalent. In this paper we study the limit of the strong…

SuperconductivityPhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed matter physicsMagnetoresistanceCondensed Matter - SuperconductivityMetals and AlloysNanowireFOS: Physical sciencesCondensed Matter PhysicsMagnetic fieldSuperconductivity (cond-mat.supr-con)Phase (matter)Mesoscale and Nanoscale Physics (cond-mat.mes-hall)Materials ChemistryCeramics and CompositesElectrical and Electronic EngineeringQuantumOhmic contactQuantum fluctuation
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Dynamics of a Ferromagnetic Particle Levitated Over a Superconductor

2018

Under conditions where the angular momentum of a ferromagnetic particle is dominated by intrinsic spin, applied torque is predicted to cause gyroscopic precession of the particle. If the particle is sufficiently isolated from the environment, a measurement of spin precession can potentially yield sensitivity to torque beyond the standard quantum limit. Levitation of a micron-scale ferromagnetic particle above a superconductor is a possible method of near frictionless suspension enabling observation of ferromagnetic particle precession and ultrasensitive torque measurements. We experimentally investigate the dynamics of a micron-scale ferromagnetic particle levitated above a superconducting …

SuperconductivityPhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed matter physicsSpinsQuantum limitGeneral Physics and AstronomyFOS: Physical sciencesPhysics - Applied Physics02 engineering and technologyApplied Physics (physics.app-ph)021001 nanoscience & nanotechnology01 natural sciencesPhysics::Fluid DynamicsFerromagnetismCondensed Matter::Superconductivity0103 physical sciencesMesoscale and Nanoscale Physics (cond-mat.mes-hall)PrecessionLevitationTorque010306 general physics0210 nano-technologyMicroscale chemistry
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Interference of nonequilibrium quasiparticles in a superconductor

2003

Abstract We have observed an interference of nonequilibrium quasiparticles, injected from a copper electrode into an aluminium loop through a tunnel barrier. At temperatures below 1K the tunnel current at fixed voltage bias is periodically modulated by external magnetic field. The amplitude of the modulation reaches maximum at a bias slightly below the gap energy, and decreases with the further increase of the bias voltage. For a given voltage bias the amplitude of the current oscillations decreases with increase of the temperature and the loop circumference.

SuperconductivityPhysicsCondensed matter physicsBiasingCondensed Matter::Mesoscopic Systems and Quantum Hall EffectCondensed Matter PhysicsInterference (wave propagation)Electronic Optical and Magnetic MaterialsMagnetic fieldAmplitudeCondensed Matter::SuperconductivityQuasiparticleElectrical and Electronic EngineeringCurrent (fluid)VoltagePhysica B: Condensed Matter
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Spin–orbit coupling effects on the electronic properties of the pressure-induced superconductor CrAs

2019

We present the effects of spin-orbit coupling on the low-energy bands and Fermi surface of the recently discovered pressure-induced superconductor CrAs. We apply the L\"owdin down-folding procedure to a tight-binding hamiltonian that includes the intrinsic spin-orbit interaction, originating from the Cr 3d electrons as well as from As 4p ones. Our results indicate that As contributions have negligible effects, whereas the modifications to the band structure and the Fermi surface can be mainly ascribed to the Cr contribution. We show that the inclusion of the spin-orbit interaction allows for a selective removal of the band degeneracy due to the crystal symmetries, along specific high symmet…

SuperconductivityPhysicsCondensed matter physicsCondensed Matter - SuperconductivityFOS: Physical sciencesGeneral Physics and AstronomyFermi surface02 engineering and technologyElectronSpin–orbit interaction021001 nanoscience & nanotechnology01 natural sciencesSuperconductivity (cond-mat.supr-con)symbols.namesake0103 physical sciencesHomogeneous spacesymbolsGeneral Materials SciencePhysical and Theoretical Chemistry010306 general physics0210 nano-technologyElectronic band structureHamiltonian (quantum mechanics)Electronic propertiesThe European Physical Journal Special Topics
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Andreev Reflection at Point Contacts with Heavy-FermionUBe13?

2000

We comment on a recent Letter by Waelti et al. (PRL 84, 5616 (2000)) on 'Spectroscopic evidence for unconventional superconductivity in UBe13'. We show - by using the basic Wexler formula - that it is unlikely to observe Andreev reflection at point contacts between UBe13 and a normal metal. The large superconducting anomalies usually found for those contacts are mainly due to the resistive Maxwell resistance vanishing below Tc of UBe13.

SuperconductivityPhysicsCondensed matter physicsCondensed Matter::SuperconductivityHeavy fermionQuantum mechanicsGeneral Physics and AstronomyPoint (geometry)Andreev reflectionPhysical Review Letters
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Magnetic phase diagrams in heavy-fermion compounds

1990

Magnetic phase diagrams have been explored in heavy-fermion (HF) compounds by controlled changes of the stoichiometry (UCu4+xAl8−x), dopant concentration (Ce(Cu1−xNix)2Ge2) and magnetic field (CeCu2Si2). The results demonstr competition (i) between Kondo and RKKY interactions in the former two compounds and (ii) between HF superconductivity and some cooperative state, presumably HF band magnetism, in the latter.

SuperconductivityPhysicsCondensed matter physicsDopantMagnetismHeavy fermionMagnetic phaseCondensed Matter PhysicsStoichiometryElectronic Optical and Magnetic MaterialsMagnetic fieldJournal of Magnetism and Magnetic Materials
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Electronic Properties, Band Structure, and Fermi Surface Instabilities ofNi1+/Ni2+NickelateLa3Ni2O6, Isoelectronic with Superconducting Cuprates

2009

Electronic structure calculations were performed for the mixed-valent Ni(1+)/Ni(2+) nickelate La3Ni2O6, which exhibits electronic instabilities of the Fermi surface similar to that of the isostructural superconducting La2CaCu2O6 cuprate. La3Ni2O6 shows activated hopping, which fits to Mott's variable-range-hopping model with localized states near the Fermi level. However, a simple local spin density approximation calculation leads to a metallic ground state. The calculations including local density approximation+Hubbard U and hybrid functionals indicate a multiply degenerate magnetic ground state. For electron-doped La2ZrNi2O6, which is isoelectronic with La2CaCu2O6, an antiferromagnetic in…

SuperconductivityPhysicsCondensed matter physicsFermi levelGeneral Physics and AstronomyFermi surfaceElectronic structureHybrid functionalsymbols.namesakesymbolsCondensed Matter::Strongly Correlated ElectronsLocal-density approximationElectronic band structureGround statePhysical Review Letters
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Time evolution of the microwave second-harmonic response of MgB2 superconductor

2003

We report on transient effects in the microwave second-order response of two ceramic MgB2 samples. The time evolution of the second-harmonic signal is investigated for about 500 s after the sample has been exposed to a variation of the dc magnetic field. We suggest that during the first seconds the response is determined by diffusive motion of fluxons, while in the time scale of minutes it is ruled by magnetic relaxation over the surface barrier.

SuperconductivityPhysicsCondensed matter physicsFluxonCondensed Matter - SuperconductivityTime evolutionFOS: Physical sciencesEnergy Engineering and Power TechnologySecond-harmonic generationCondensed Matter PhysicsSignalElectronic Optical and Magnetic MaterialsMagnetic fieldSuperconductivity (cond-mat.supr-con)Condensed Matter::SuperconductivityTransient (oscillation)Electrical and Electronic EngineeringMicrowavePhysica C: Superconductivity
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Force-free state in a superconducting single crystal and angle-dependent vortex helical instability

2017

Superconducting 2H-NbSe2 single crystals show intrinsic low pinning values. Therefore, they are ideal materials with which to explore fundamental properties of vortices. (V, I) characteristics are the experimental data we have used to investigate the dissipation mechanisms in a rectangular shape 2H-NbSe2 single crystal. Particularly, we have studied dissipation behavior with magnetic fields applied in the plane of the crystal and parallel to the injected currents, i.e. in the force-free state where the vortex helical instability governs the vortex dynamics. In this regime, the data follow the elliptic critical state model and the voltage dissipation shows an exponential dependence.Moreover,…

SuperconductivityPhysicsCondensed matter physicsFísica de materialesCondensed Matter - SuperconductivityFísicaFOS: Physical sciencesVorticityDissipationCiència dels materials01 natural sciencesInstability010305 fluids & plasmasVortexMagnetic fieldCrystalSuperconductivity (cond-mat.supr-con)Condensed Matter::Superconductivity0103 physical sciencesFísica del estado sólido010306 general physicsSingle crystal
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Anisotropic transport properties ofUNi2Al3thin films

2007

Experimental results on the transport anisotropy in thin films of the heavy fermion superconductor $\mathrm{U}{\mathrm{Ni}}_{2}{\mathrm{Al}}_{3}$ are presented. They show that the eletronic transport in $\mathrm{U}{\mathrm{Ni}}_{2}{\mathrm{Al}}_{3}$ for different directions is strongly dominated by different sheets of the Fermi surface, and that the magnetic moments must be assigned to a cylindrical part around the $c$ axis. Founded on the findings about the Fermi surface, the dependence of the resistive superconducting transition temperature ${T}_{c}$ on the current direction in $\mathrm{U}{\mathrm{Ni}}_{2}{\mathrm{Al}}_{3}$ can be explained as the result of weakly coupled superconducting …

SuperconductivityPhysicsCondensed matter physicsMagnetic momentSuperconducting transition temperatureFermi surfaceHeavy fermion superconductorThin filmCondensed Matter PhysicsAnisotropyElectronic Optical and Magnetic MaterialsPhysical Review B
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