Search results for "Condensed Matter::Superconductivity"

showing 10 items of 632 documents

Electron–phonon coupling in degenerate silicon-on-insulator film probed using superconducting Schottky junctions

2002

Abstract Energy flow rate in degenerate n-type silicon-on-insulator (SOI) film is studied at low temperatures. The electrons are heated above the lattice temperature by electric field and the electron temperature is measured via semiconductor–superconductor quasiparticle tunneling. The energy flow rate in the system is found to be proportional to T 5 , indicating that electron–phonon relaxation rate and electron–phonon phase breaking rate are proportional to T 3 . The electron–phonon system in the SOI film is in the “dirty limit” where the electron mean free path is smaller than the inverse of the thermal phonon wave vector.

SuperconductivityPhysicsCondensed matter physicsPhononsuperconductivityelectron phonon couplingelectron energy relaxationElectronCondensed Matter::Mesoscopic Systems and Quantum Hall EffectCondensed Matter PhysicsAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic Materialssilicon-on-insulatorCondensed Matter::Materials ScienceCondensed Matter::SuperconductivityElectric fieldQuasiparticleElectron temperatureCondensed Matter::Strongly Correlated ElectronsWave vectorQuantum tunnellingPhysica E: Low-dimensional Systems and Nanostructures
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Superconductivity in palladium-based Heusler compounds

2009

This work reports on four more Heusler superconductors: ${\text{Pd}}_{2}\text{ZrAl}$, ${\text{Pd}}_{2}\text{HfAl}$, ${\text{Pd}}_{2}\text{ZrIn}$, and ${\text{Pd}}_{2}\text{HfIn}$. These compounds exhibit superconducting transition temperatures ranging from 2.4--3.8 K as determined by resistivity measurements. According to their behavior in an external magnetic field, all compounds are type II bulk superconductors. The occurrence of superconductivity was predicted for these compounds using electronic structure calculations. The electronic structures exhibit van Hove singularities (saddle points) at the $L$ point. These lead to a maximum in the corresponding density of states and superconduct…

SuperconductivityPhysicsCondensed matter physicsScatteringTransition temperatureFermi energyElectronic structureCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsElectrical resistivity and conductivityCondensed Matter::SuperconductivityDensity of statesCondensed Matter::Strongly Correlated ElectronsElectron scatteringPhysical Review B
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Strong-coupling effects in the heavy-fermion superconductor UPd2Al3

2000

Abstract Recent results of superconducting tunneling spectroscopy on epitaxial thin films of the antiferromagnetic heavy-fermion superconductor UPd 2 Al 3 are presented. Strong-coupling effects in the tunneling density of states are analyzed within the framework of the anisotropic Eliashberg theory for a pair-coupling mechanism based on the exchange of antiferromagnetic spin excitations. The multi-sheeted Fermi surface of UPd 2 Al 3 is taken into account.

SuperconductivityPhysicsCondensed matter physicsType-I superconductorScanning tunneling spectroscopyFermi surfaceHeavy fermion superconductorCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsCondensed Matter::SuperconductivityDensity of statesAntiferromagnetismCondensed Matter::Strongly Correlated ElectronsElectrical and Electronic EngineeringSpin-½Physica B: Condensed Matter
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Change of the vortex core structure in two-band superconductors at the impurity-scattering-driven s±/s++ crossover

2017

We report a nontrivial transition in the core structure of vortices in two-band superconductors as a function of interband impurity scattering. We demonstrate that, in addition to singular zeros of the order parameter, the vortices there can acquire a circular nodal line around the singular point in one of the superconducting components. It results in the formation of the peculiar ``moat''-like profile in one of the superconducting gaps. The moat-core vortices occur generically in the vicinity of the impurity-induced crossover between ${s}_{\ifmmode\pm\else\textpm\fi{}}$ and ${s}_{++}$ states.

SuperconductivityPhysicsCondensed matter physicsta114ScatteringCrossovermultiband superconductivityOrder (ring theory)vortices in superconductors02 engineering and technologySingular point of a curve021001 nanoscience & nanotechnology01 natural sciencesVortexImpurityCondensed Matter::Superconductivityimpurities in superconductors0103 physical sciencess-wave010306 general physics0210 nano-technologyLine (formation)Physical Review B
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Spatially resolved measurement of nonequilibrium quasiparticle relaxation in superconducting Al

2011

Spatially resolved relaxation of nonequilibrium quasiparticles in a superconductor at ultralow temperatures was experimentally studied. It was found that the quasiparticle injection through a tunnel junction results in the modification of the shape of the I-V characteristic of a remote ``detector'' junction. The effect depends on the temperature, injection current, and proximity to the injector. The phenomena can be understood in terms of the creation of quasiparticle charge and energy disequilibrium characterized by two different length scales ${\ensuremath{\Lambda}}_{{Q}^{*}}~5$ and ${\ensuremath{\Lambda}}_{{T}^{*}}~40$ $\ensuremath{\mu}$m. The findings are in good agreement with existing…

SuperconductivityPhysicsCondensed matter physicsta114ta221Charge (physics)Condensed Matter::Mesoscopic Systems and Quantum Hall EffectCondensed Matter PhysicsLambdaElectronic Optical and Magnetic MaterialsTunnel junctionCondensed Matter::SuperconductivityQuasiparticleRelaxation (physics)Microscopic theoryEnergy (signal processing)Physical Review B
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Energy dependence of the electron-boson coupling strength in the electron-doped cuprate superconductor Pr1.85Ce0.15CuO4−δ

2017

In the conventional theory of superconductivity the critical temperature Tc is determined by the electron-phonon coupling constant and the phonon cut-off frequency. The hallmark experiments of McMillan and Rowell demonstrated that bosons (phonons) responsible for pairing can be observed through the frequency dependence of the gap parameter. Determination of the electron-boson coupling strength in high-${T}_{c}$ cuprates is, however, not an easy task. One of the promising ways is to measure the energy relaxation rate of photoexcited carriers by using femtosecond real-time techniques. Here, considering the electron relaxation process within the conduction band, it is commonly assumed that the…

SuperconductivityPhysicsCoupling constantCondensed matter physicsPhononElectronCoupling (probability)01 natural sciences010305 fluids & plasmasCondensed Matter::SuperconductivityPairing0103 physical sciencesCuprate010306 general physicsEnergy (signal processing)Physical Review B
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Flat Bands as a Route to High-Temperature Superconductivity in Graphite

2016

Superconductivity is traditionally viewed as a low-temperature phenomenon. Within the BCS theory this is understood to result from the fact that the pairing of electrons takes place only close to the usually two-dimensional Fermi surface residing at a finite chemical potential. Because of this, the critical temperature is exponentially suppressed compared to the microscopic energy scales. On the other hand, pairing electrons around a dispersionless (flat) energy band leads to very strong superconductivity, with a mean-field critical temperature linearly proportional to the microscopic coupling constant. The prize to be paid is that flat bands can probably be generated only on surfaces and i…

SuperconductivityPhysicsCoupling constantHigh-temperature superconductivityCondensed matter physicsFermi surface02 engineering and technologyBCS theory021001 nanoscience & nanotechnology01 natural sciences7. Clean energylaw.inventionlawCondensed Matter::SuperconductivityTopological insulatorPairing0103 physical sciences010306 general physics0210 nano-technologyTopological quantum number
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Irreversibility of the threshold field for dendritic flux avalanches in superconductors

2010

Hysteretic effects are seen in the upper and lower threshold fields for the appearance of dendritic flux instabilities, first explained in Yurchenko et al. [Phys. Rev. B 76 (2007) 092504], in NbN-films. We have measured the threshold fields at increasing and decreasing applied fields at different temperatures and proposed a mechanism explaining how the hysteresis arises by analyzing the field profiles inside the sample.

SuperconductivityPhysicsField (physics)Condensed matter physicsEnergy Engineering and Power TechnologyFluxCondensed Matter PhysicsInstabilityMagnetic fluxElectronic Optical and Magnetic MaterialsHysteresisLower thresholdCondensed Matter::SuperconductivityElectrical and Electronic EngineeringPhysica C: Superconductivity
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History dependence of the magnetization of thin HTSC films: an explanation for distorted SQUID signals

1997

Abstract The magnetizations of thin film disk-shaped type-II superconductors in perpendicular magnetic fields are considered by aid of Mikheenko's critical state model which has been corrected by Zhu for the case of a time-varying periodic field. This paper presents the application of this scheme to an arbitrary nonperiodic time dependence H ( t ). We calculate the influence of field inhomogeneities in a magnetometer on the current density distribution of a disk-shaped type-II superconductor. The resulting SQUID pickup signals and magnetic moments are compared to measurements performed on a 200 nm thick YBa 2 Cu 3 O 7 film in the irreversible regime of the phase diagram. Theory and experime…

SuperconductivityPhysicsField (physics)Condensed matter physicsMagnetic momentMagnetometerEnergy Engineering and Power TechnologyCondensed Matter PhysicsElectronic Optical and Magnetic Materialslaw.inventionMagnetic fieldSQUIDMagnetizationScanning SQUID microscopylawCondensed Matter::SuperconductivityElectrical and Electronic EngineeringPhysica C: Superconductivity
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Superconductor-Diamond Hybrid Quantum System

2016

This chapter describes recent progress on research into superconducting flux qubit, NV diamond, and superconductor-diamond hybrid quantum systems. First, we describe important physical properties of superconducting macroscopic artificial atoms i.e., the tunability of the qubit energy level spacing, the coherence property, an example of strong coupling to another quantum system such as an LC harmonic oscillator, and qubit state readout through a Josephson bifurcation amplifier. We then introduce the NV center in diamond as an intriguing candidate for quantum information processing, which offers excellent multiple accessibility via visible light, microwaves and magnetic fields. Finally, we de…

SuperconductivityPhysicsFlux qubitbusiness.industryDiamond02 engineering and technologyengineering.material021001 nanoscience & nanotechnology01 natural sciencesDark stateCondensed Matter::SuperconductivityQubit0103 physical sciencesQuantum systemengineeringOptoelectronics010306 general physics0210 nano-technologybusinessQuantumCoherence (physics)
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