Search results for "coherence [color]"

showing 8 items of 38 documents

Scanning tunnelling spectroscopy study of paramagnetic superconducting β''-ET(4)[(H(3)O)Fe(C(2)O(4))(3)]·C(6)H(5)Br crystals.

2010

Scanning tunnelling spectroscopy (STS) and microscopy (STM) were performed on the paramagnetic molecular superconductor β''-ET(4)[(H(3)O)Fe(C(2)O(4))(3)]·C(6)H(5)Br. Under ambient pressure, this compound is located near the boundary separating superconducting and insulating phases of the phase diagram. In spite of a strongly reduced critical temperature T(c) (T(c) = 4.0 K at the onset, zero resistance at T(c) = 0.5 K), the low temperature STS spectra taken in the superconducting regions show strong similarities with the higher T(c) ET κ-derivatives series. We exploited different models for the density of states (DOS), with conventional and unconventional order parameters to take into accoun…

Superconducting coherence lengthSuperconductivityMaterials scienceCondensed matter physicsTransition temperatureOrganic superconductors order parameter scanning tunneling spectroscopyAnalytical chemistryBCS theoryCondensed Matter PhysicsParamagnetismElectrical resistivity and conductivityCondensed Matter::SuperconductivityDensity of statesGeneral Materials SciencePhase diagramJournal of physics. Condensed matter : an Institute of Physics journal
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Resistive state triggered by vortex entry in YBa 2 Cu 3 O 7−δ nanostructures

2014

We have realized YBa2Cu3O7-delta nanowires and nano Superconducting Quantum Interference Devices (nanoSQUID). The measured temperature dependence of the wire resistances below the superconducting transition temperature has been analyzed using a thermally activated vortex entry model valid for wires wider than the superconducting coherence length. The extracted zero temperature values of the London penetration depth, lambda(0) similar or equal to 270 +/- 15 nm, are in good agreement with the value obtained from critical current modulations as a function of an externally applied magnetic field in a nanoSQUID implementing two nanowires.

Superconducting coherence lengthSuperconductivityResistive touchscreenHigh-temperature superconductivityMaterials scienceCondensed matter physicsLondon penetration depthNanowireEnergy Engineering and Power TechnologyCondensed Matter PhysicsElectronic Optical and Magnetic Materialslaw.inventionVortexMagnetic fieldlawCondensed Matter::SuperconductivityElectrical and Electronic EngineeringPhysica C: Superconductivity and its Applications
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Phase Slip Phenomena in Ultra-Thin Superconducting Wires

2006

We present results on phase-slip phenomena in a superconducting wire which can be considered as quasi-one dimensional (1D) if its characteristic transverse dimension \( \sqrt \sigma\) (√ being the cross section) is smaller than the coherence length Λ(T). The shape of the bottom part of the resistive transition R(T) of a 1D superconducting strip is described by the model of phase slips activation. If the wire is infinitely long, then there is always a finite probability that a small part of the sample is instantly driven normal.

SuperconductivityPhysicsCross section (physics)Resistive touchscreenCondensed matter physicsSuperconducting wirePhase (waves)engineeringSigmaPhase slipengineering.materialCoherence length
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Nonlocal pure spin current injection via quantum pumping and crossed Andreev reflection

2005

A pure spin current injector is proposed based on adiabatic pumping and crossed normal/Andreev reflection. The device consists of a three-terminal ferromagnet-superconductor-semiconductor system in which the injection of a pure spin current is into the semiconductor which is coupled to the superconductor within a coherence length away from the ferromagnet enabling the phenomena of crossed normal /Andreev reflection to operate. Quantum pumping is induced by adiabatically modulating two independent parameters of the ferromagnetic lead, namely the magnetization strength and the strength of coupling between the ferromagnet and the superconductor. The competition between the normal/Andreev refle…

SuperconductivityPhysicsQuantum PhysicsCondensed matter physicsCondensed Matter - Mesoscale and Nanoscale Physicsbusiness.industryFOS: Physical sciencesCondensed Matter PhysicsCondensed Matter::Mesoscopic Systems and Quantum Hall EffectElectronic Optical and Magnetic MaterialsAndreev reflectionCoherence lengthMagnetizationCondensed Matter::Materials ScienceSemiconductorFerromagnetismCondensed Matter::SuperconductivityMesoscale and Nanoscale Physics (cond-mat.mes-hall)Condensed Matter::Strongly Correlated ElectronsQuantum Physics (quant-ph)businessAdiabatic processQuantum
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Electronic implementation of a non-linear oscillator subjected to noise : application to the modeling of neuronal information coding

2011

We study the nonlinear FitzHugh-Nagumo model witch describes the dynamics of excitable neural element. It is well known that this system exhibits three different possible responses. Indeed, the system can be mono-stable, oscillatory or bistable. In the oscillatory regime, the system periodically responds by generating action potential. By contrast, in the mono-stable state the system response remains constant after a transient. Under certain conditions, the system can undergo a bifurcation between the stable and the oscillatory regime via the so called Andronov-Hopf bifurcation. In this Phd thesis, we consider the FitzHugh-Nagumo model in the stable state, that is set near the Andronov-Hopf…

[SDV.MHEP] Life Sciences [q-bio]/Human health and pathologyAndronov-Hopf bifurcationBifurcation d'Andronov-HopfInfluence constructive du bruit dans un circuit électronique non linéaireAction potentialCoherence resonance and stochastic resonance phenomenonModèles neuronauxBenet of noise in nonlinear electronic circuitPhénomènes de résonance cohérente et résonance stochastique[ SDV.MHEP ] Life Sciences [q-bio]/Human health and pathologySystème non linéaire de FitzHugh-NagumoNeural model of FitzHugh-Nagumo[SDV.MHEP]Life Sciences [q-bio]/Human health and pathologyPotentiels d'action et dynamique neuronale
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Noise effect in a sine-Gordon Lattice

2013

International audience; This paper is devoted to the influence of internal noise in a sine-Gordon chain exhibiting the well known nonlinear supratransmission phenomenon. It is shown that spatiotemporal noise can trigger breather modes with a given probability in a range of parameters where they do not occur without noise. A frequency analysis is carried out to quantify the degree of coherence of the emitted breather. It is shown that there exists an appropriate amount of noise which ensures the existence of breather modes with the best coherence.

noiseBreather[PHYS.PHYS.PHYS-BIO-PH]Physics [physics]/Physics [physics]/Biological Physics [physics.bio-ph]Degree of coherence01 natural sciences010305 fluids & plasmaslaw.invention[NLIN.NLIN-PS]Nonlinear Sciences [physics]/Pattern Formation and Solitons [nlin.PS]law[ PHYS.PHYS.PHYS-BIO-PH ] Physics [physics]/Physics [physics]/Biological Physics [physics.bio-ph]Quantum mechanicsLattice (order)0103 physical sciencesPhase noise[NLIN.NLIN-PS] Nonlinear Sciences [physics]/Pattern Formation and Solitons [nlin.PS][ NLIN.NLIN-PS ] Nonlinear Sciences [physics]/Pattern Formation and Solitons [nlin.PS]Statistical physics010306 general physicsNonlinear Sciences::Pattern Formation and SolitonsBreatherPhysicsFrequency analysis[PHYS.PHYS.PHYS-BIO-PH] Physics [physics]/Physics [physics]/Biological Physics [physics.bio-ph]Quantum noiseShot noisecoherence resonance[SPI.TRON] Engineering Sciences [physics]/Electronics[SPI.TRON]Engineering Sciences [physics]/Electronics[ SPI.TRON ] Engineering Sciences [physics]/ElectronicsNonlinear systemStochastic resonance
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Algorithms for coherence checking and propagation of conditional probability bounds

2001

In this paper, we propose some algorithms for the checking of generalized coherence (g-coherence) and for the extension of imprecise conditional probability assessments. Our concept of g-coherence is a generalization of de Finetti’s coherence principle and is equivalent to the ”avoiding uniform loss” property for lower and upper probabilities (a la Walley). By our algorithms we can check the g-coherence of a given imprecise assessment and we can correct it in order to obtain the associated coherent assessment (in the sense of Walley and Williams). Exploiting some properties of the random gain we show how, in the linear systems involved in our algorithms, we can work with a reduced set of va…

reduced sets of variables and constraintsSettore MAT/06 - Probabilita' E Statistica MatematicaUncertain knowledgeUncertain knowledge probabilistic reasoning under coherence imprecise conditional probability assessments g-coherence checking g-coherent extension algorithms computational aspects reduced sets of variables reduced sets of linear constraints.g-coherent extensionimprecise conditional probability assessmentsg-coherence checkingUncertain knowledge; probabilistic reasoning under coherence; imprecise conditional probability assessments; g-coherence checking; g-coherent extension; algorithms.; computational aspects; reduced sets of variables and constraints.algorithmsprobabilistic reasoning under coherencecomputational aspects
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Field dependence of the vortex-core sizes in dirty two-band superconductors

2019

We study the structure of Abrikosov vortices in two-band superconductors for different external magnetic fields and different parameters of the bands. The vortex core size determined by the coherence lengths are found to have qualitatively different behaviour from that determined by the quasiparticle density of states spatial variation. These different vortex core length scales coincide near the upper critical field, while the discrepancy between them becomes quite significant at lower fields. Within the diffusive approximation we demonstrate several generic regimes in the field dependence of the vortex core sizes determined by the disparity of diffusion constants in the two bands.

suprajohtavuusmultiband superconductivityFOS: Physical sciences02 engineering and technology01 natural sciencessuprajohteetSuperconductivity (cond-mat.supr-con)disordered systemsCondensed Matter::Superconductivity0103 physical sciences010306 general physicsCritical fieldPhysicsSuperconductivityCondensed matter physicsCondensed Matter - Superconductivityvortices in superconductors021001 nanoscience & nanotechnologycoherence lengthMagnetic fieldVortexScattering ratePairingDensity of statesQuasiparticle0210 nano-technology
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