Search results for "Cooper pair"

showing 10 items of 30 documents

High transparency Bi 2 Se 3 topological insulator nanoribbon Josephson junctions with low resistive noise properties

2019

Bi$_2$Se$_3$ nanoribbons, grown by catalyst-free Physical Vapour Deposition, have been used to fabricate high quality Josephson junctions with Al superconducting electrodes. The conductance spectra (dI/dV) of the junctions show clear dip-peak structures characteristic of multiple Andreev reflections. The temperature dependence of the dip-peak features reveals a highly transparent Al/Bi$_2$Se$_3$ topological insulator nanoribbon interface and Josephson junction barrier. This is supported by the high values of the Bi$_2$Se$_3$ induced gap and of I$_c$R$_n$ (I$_c$ critical current, R$_n$ normal resistance of the junction) product both of the order of 160 $\mu$eV, a value close to the Al gap. T…

010302 applied physicsSuperconductivityJosephson effectResistive touchscreenMaterials sciencePhysics and Astronomy (miscellaneous)Condensed matter physicsCondensed Matter - SuperconductivityConductanceFOS: Physical sciences02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesNoise (electronics)Superconductivity (cond-mat.supr-con)Physical vapor depositionTopological insulator0103 physical sciencesCooper pair0210 nano-technologyApplied Physics Letters
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Gauge theory of the long-range proximity effect and spontaneous currents in superconducting heterostructures with strong ferromagnets

2017

We present the generalized quasiclassical theory of the long-range superconducting proximity effect in heterostructures with strong ferromagnets, where the exchange splitting is of the order of Fermi energy. In the ferromagnet the propagation of equal-spin Cooper pairs residing on the spin-split Fermi surfaces is shown to be governed by the spin-dependent Abelian gauge field which results either from the spin-orbital coupling or from the magnetic texture. This additional gauge field enters into the quasiclassical equations in superposition with the usual electromagnetic vector potential and results in the generation of spontaneous superconducting currents and phase shifts in various geometr…

02 engineering and technology01 natural sciencesSuperposition principleCondensed Matter::Superconductivity0103 physical sciencesProximity effect (superconductivity)Boundary value problemGauge theory010306 general physicsPhysicsSuperconductivityta114Condensed matter physicsJosephson effectMeissner effectFermi energy021001 nanoscience & nanotechnologyferromagnetismcoherence lengthQuantum electrodynamicsproximity effectCondensed Matter::Strongly Correlated ElectronsCooper pair0210 nano-technologyVector potentialPhysical Review B
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Direct observation of second-order atom tunnelling

2007

Tunnelling of material particles through a classically impenetrable barrier constitutes one of the hallmark effects of quantum physics. When interactions between the particles compete with their mobility through a tunnel junction, intriguing novel dynamical behaviour can arise where particles do not tunnel independently. In single-electron or Bloch transistors, for example, the tunnelling of an electron or Cooper pair can be enabled or suppressed by the presence of a second charge carrier due to Coulomb blockade. Here we report on the first direct and time-resolved observation of correlated tunnelling of two interacting atoms through a barrier in a double well potential. We show that for we…

Condensed Matter::Quantum GasesJosephson effectQuantum PhysicsMultidisciplinaryCondensed matter physicsChemistryFOS: Physical sciencesCoulomb blockadeCondensed Matter::Mesoscopic Systems and Quantum Hall EffectCondensed Matter - Other Condensed MatterTunnel effectTunnel ionizationUltracold atomTunnel junctionCondensed Matter::SuperconductivityCooper pairQuantum Physics (quant-ph)Quantum tunnellingOther Condensed Matter (cond-mat.other)Nature
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Adiabatic transport of Cooper pairs in arrays of Josephson junctions

1999

We have developed a quantitative theory of Cooper pair pumping in gated one-dimensional arrays of Josephson junctions. The pumping accuracy is limited by quantum tunneling of Cooper pairs out of the propagating potential well and by direct supercurrent flow through the array. Both corrections decrease exponentially with the number N of junctions in the array, but give a serious limitation of accuracy for any practical array. The supercurrent at resonant gate voltages decreases with N only as sin(v/N)/N, where v is the Josephson phase difference across the array.

Josephson effectPhysicsCondensed Matter::Quantum GasesCondensed matter physicsCondensed Matter - Mesoscale and Nanoscale PhysicsCondensed Matter - SuperconductivitySupercurrentFOS: Physical sciencesCoulomb blockadeCondensed Matter::Mesoscopic Systems and Quantum Hall EffectSuperconductivity (cond-mat.supr-con)Pi Josephson junctionQuantum mechanicsCondensed Matter::SuperconductivityMesoscale and Nanoscale Physics (cond-mat.mes-hall)Superconducting tunnel junctionCooper pairAdiabatic processQuantum tunnelling
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Entanglement detection in Josephson nanocircuits

2002

We describe a possible experimental scheme to generate and detect entanglement between charge states in superconducting nanocircuits, discriminating such entanglement from classical correlations. The case of maximally entangled singlet and GHZ states of two and three coupled Josephson junctions is discussed as an example.

Josephson effectSuperconductivityPhysicsGreenberger–Horne–Zeilinger stateCondensed Matter::SuperconductivityQubitQuantum mechanicsCharge (physics)Quantum PhysicsSinglet stateQuantum entanglementCooper pairAtomic and Molecular Physics and Optics
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θ0 thermal Josephson junction

2017

We predict the thermal counterpart of the anomalous Josephson effect in superconductor/ferromagnet/superconductor junctions with noncoplanar magnetic texture. The heat current through the junction is shown to have the phase-sensitive interference component proportional to cos(θ−θ0), where θ is the Josephson phase difference and θ0 is the texture-dependent phase shift. In the generic trilayer magnetic structure with the spin-filtering tunnel barrier θ0 is determined by the spin chirality of magnetic configuration and can be considered as the direct manifestation of the energy transport with participation of spin-triplet Cooper pairs. In case of the ideal spin filter the phase shift is shown …

Josephson junctionsCondensed Matter::SuperconductivityjohteetmagnetismiCooper pairs
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Enhancing triplet superconductivity by the proximity to a singlet superconductor in oxide heterostructures

2016

We show how in principle a coherent coupling between two superconductors of opposite parity can be realized in a three-layer oxide heterostructure. Due to strong intraionic spin-orbit coupling in the middle layer, singlet Cooper pairs are converted into triplet ones and vice versa. This results in a large enhancement of the triplet superconductivity, persisting well above the native triplet critical temperature.

OxideFOS: Physical sciences02 engineering and technology01 natural sciencesSuperconductivity (cond-mat.supr-con)Condensed Matter - Strongly Correlated Electronschemistry.chemical_compound0103 physical sciencesoxide heterostructureSinglet stateTriplet state010306 general physicsPhysicsSuperconductivityStrongly Correlated Electrons (cond-mat.str-el)Condensed matter physicsta114singlet Cooper pairsCondensed Matter - SuperconductivityParity (physics)Heterojunction021001 nanoscience & nanotechnology3. Good healthchemistrySinglet fissiontriplet superconductivityCooper pair0210 nano-technologyphysicsPhysical Review B
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Connecting Berry's phase and the pumped charge in a Cooper pair pump

2003

The properties of the tunnelling-charging Hamiltonian of a Cooper pair pump are well understood in the regime of weak and intermediate Josephson coupling, i.e. when $E_{\mathrm{J}}\lesssim E_{\mathrm{C}}$. It is also known that Berry's phase is related to the pumped charge induced by the adiabatical variation of the eigenstates. We show explicitly that pumped charge in Cooper pair pump can be understood as a partial derivative of Berry's phase with respect to the phase difference $\phi$ across the array. The phase fluctuations always present in real experiments can also be taken into account, although only approximately. Thus the measurement of the pumped current gives reliable, yet indirec…

Phase differencePhysicsSuperconductivityCondensed Matter - SuperconductivityFOS: Physical sciencesObservableSuperconductivity (cond-mat.supr-con)symbols.namesakeQuantum mechanicssymbolsPartial derivativeCooper pairHamiltonian (quantum mechanics)Eigenvalues and eigenvectors
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Fermion pairing with spin-density imbalance in an optical lattice

2006

We consider pairing in a two-component atomic Fermi gas, in a three-dimensional optical lattice, when the components have unequal densities, i.e. the gas is polarized. We show that a superfluid where the translational symmetry is broken by a finite Cooper pair momentum, namely an FFLO-type state, minimizes the Helmholtz free energy of the system. We demonstrate that such a state is clearly visible in the observable momentum distribution of the atoms, and analyze the dependence of the order parameter and the momentum distribution on the filling fraction and the interaction strength.

PhysicsCondensed Matter::Quantum GasesOptical latticeCondensed Matter - Materials ScienceCondensed matter physicsCondensed Matter - SuperconductivityGeneral Physics and AstronomyMaterials Science (cond-mat.mtrl-sci)FOS: Physical sciencesFermion01 natural sciences114 Physical sciences010305 fluids & plasmasMomentumSuperfluiditySuperconductivity (cond-mat.supr-con)PairingCondensed Matter::Superconductivity0103 physical sciencesCooper pair010306 general physicsFermi gasTranslational symmetry
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Vortex mutual friction in rotating superfluid 3He

1996

The Manchester rotating cryostat has been used to measure the longitudinal and transverse coefficients of vortex mutual friction in the A and B phases of superfluid 3He. In the B phase the dominant contribution to the mutual friction is scattering of excitations off occupied bound states in the vortex core. The A phase results are explained quantitatively by assuming that doubly quantised continuous vortices are created with a dynamics determined by the equation of motion of the orbital vector I; the measurements enable us to put an upper limit on the orbital inertia of less than 0.01h{stroke} per Cooper pair. History-dependent textural effects which had to be overcome in order to make mean…

PhysicsCondensed matter physicsmedia_common.quotation_subjectPhase (waves)General Physics and AstronomyEquations of motionInertiaRotationVortexSuperfluidityClassical mechanicsBound stateCooper pairmedia_common
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