Search results for "STATES"

showing 10 items of 1532 documents

Noise-induced effects in nonlinear relaxation of condensed matter systems

2015

Abstract Noise-induced phenomena characterise the nonlinear relaxation of nonequilibrium physical systems towards equilibrium states. Often, this relaxation process proceeds through metastable states and the noise can give rise to resonant phenomena with an enhancement of lifetime of these states or some coherent state of the condensed matter system considered. In this paper three noise induced phenomena, namely the noise enhanced stability, the stochastic resonant activation and the noise-induced coherence of electron spin, are reviewed in the nonlinear relaxation dynamics of three different systems of condensed matter: (i) a long-overlap Josephson junction (JJ) subject to thermal fluctuat…

PhysicsJosephson effectCondensed matter physicsStochastic processSpin polarised transport in semiconductorGeneral MathematicsApplied MathematicsQuantum noiseStochastic analysis methodsShot noiseGeneral Physics and AstronomyThermal fluctuationsResonant activationStatistical and Nonlinear PhysicsNoise processes and phenomenaSpin polarised transport in semiconductorsJosephson junctionMathematics (all)Coherent statesStochastic analysis methodSpin (physics)Noise enhanced stabilityJosephson junction; Noise enhanced stability; Noise processes and phenomena; Resonant activation; Spin polarised transport in semiconductors; Stochastic analysis methodsCoherence (physics)Chaos, Solitons & Fractals
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RESONANT ACTIVATION AND NOISE ENHANCED STABILITY IN JOSEPHSON JUNCTIONS

2005

We investigate the interplay of two noise-induced effects on the temporal characteristics of short overdamped Josephson junctions in the presence of a periodic driving. We find that: (i) the mean life time of superconductive state has a minimum as a function of driving frequency, and near the minimum it actually does not depend on the noise intensity (resonant activation phenomenon); (ii) the noise enhanced stability phenomenon increases the switching time from superconductive to the resistive state. As a consequence there is a suitable frequency range of clock pulses, at which the noise has a minimal effect on pulse propagation in RSFQ electronic devices.

PhysicsJosephson effectJosephson phaseCondensed matter physicsRSFQ CIRCUITSJosephson energyESCAPEBARRIERTIMESStability (probability)FLUCTUATING POTENTIALSPi Josephson junctionSTATESSuperconducting tunnel junctionNoise (radio)Complexity, Metastability and Nonextensivity
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Effects of Lévy noise on the dynamics of sine-Gordon solitons in long Josephson junctions

2015

We numerically investigate the generation of solitons in current-biased long Josephson junctions in relation to the superconducting lifetime and the voltage drop across the device. The dynamics of the junction is modelled with a sine-Gordon equation driven by an oscillating field and subject to an external non-Gaussian noise. A wide range of $\alpha$-stable L\'evy distributions is considered as noise source, with varying stability index $\alpha$ and asymmetry parameter $\beta$. In junctions longer than a critical length, the mean switching time (MST) from superconductive to the resistive state assumes a values independent of the device length. Here, we demonstrate that such a value is direc…

PhysicsJosephson effectStatistics and ProbabilityCondensed Matter - SuperconductivityDynamics (mechanics)large deviations in non-equilibrium systemsLarge deviations in non-equilibrium systems; mesoscopic systems (theory); metastable states; stochastic processes (theory); Statistics and Probability; Statistical and Nonlinear Physics; Statistics Probability and UncertaintyStatistical and Nonlinear Physicsstochastic processes (theory)metastable state01 natural sciencesSettore FIS/03 - Fisica Della Materia010305 fluids & plasmasLevy noiseQuantum mechanicsLarge deviations in non-equilibrium systemmesoscopic systems (theory)Condensed Matter::Superconductivitymetastable states0103 physical scienceslarge deviations in non-equilibrium systems; mesoscopic systems (theory); metastable states; stochastic processes (theory)SineStatistics Probability and Uncertainty010306 general physicsStatistical and Nonlinear Physic
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An invariant analytic orthonormalization procedure with applications

2007

We apply the orthonormalization procedure previously introduced by two of us and adopted in connection with coherent states to Gabor frames and other examples. For instance, for Gabor frames we show how to construct $g(x)\in L^2(\Bbb{R})$ in such a way the functions $g_{\underline n}(x)=e^{ian_1x}g(x+an_2)$, $\underline n\in\Bbb{Z}^2$ and $a$ some positive real number, are mutually orthogonal. We discuss in some details the role of the lattice naturally associated to the procedure in this analysis.

PhysicsLattice (group)FOS: Physical sciencesStatistical and Nonlinear PhysicsMathematical Physics (math-ph)CombinatoricsSettore MAT/05 - Analisi MatematicaCoherent statesInvariant (mathematics)Connection (algebraic framework)Gabor framesSettore MAT/07 - Fisica MatematicaMathematical PhysicsReal number
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Light-Induced Excited Spin State Trapping in Iron(II) Complexes

1987

In the course of our studies on the thermally induced high spin (HS) ↔ low spin (LS) transition in iron(II) complexes /1/, \({\!^5{\text{T}}_2}_{\text{g}}\) ↔ \({\!^1{\text{A}}_1}_{\text{g}}\) in the approximation of Oh symmetry, we have observed in 1984 a new photophysical effect /2/: If, at sufficiently low temperature, the solid spin crossover complex is irradiated with green light into the \({\!^1{\text{A}}_1}\)→ \({\!^1{\text{T}}_1}\) ligand field absorption band, the thermodynamically stable LS state can be converted to the metastable HS state and trapped with practically infinite lifetime. We have called this unusual phenomenon “Light-Induced Excited Spin State Trapping (LIESST)”.

PhysicsLigand field theoryCrystallographySpin statesSpin crossoverAbsorption bandExcited stateMetastabilitySpin (physics)LIESST
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In Silico Molecular Engineering of Dysprosocenium-Based Complexes to Decouple Spin Energy Levels from Molecular Vibrations

2019

Molecular nanomagnets hold great promise for spintronics and quantum technologies, provided that their spin memory can be preserved above liquid-nitrogen temperatures. In the past few years, the magnetic hysteresis records observed for two related dysprosocenium-type complexes have highlighted the potential of molecular engineering to decouple vibrational excitations from spin states and thereby enhance magnetic memory. Herein, we study the spin-vibrational coupling in [(CpiPr5)Dy(Cp*)]+ (CpiPr5 = pentaisopropylcyclopentadienyl, Cp* = pentamethylcyclopentadienyl), which currently holds the hysteresis record (80 K), by means of a computationally affordable methodology that combines first-pri…

PhysicsLigand field theorySpin statesSpintronics010405 organic chemistryUNESCO::QUÍMICAElectronic structure010402 general chemistryMagnetic hysteresis01 natural sciences:QUÍMICA [UNESCO]0104 chemical sciencesMolecular engineeringChemical physicsAb initio quantum chemistry methodsGeneral Materials SciencePhysical and Theoretical ChemistrySpin-½
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Lifetime measurements in 166Re : Collective versus magnetic rotation

2016

WOS: 000371740600004

PhysicsManchester Cancer Research Centreta114010308 nuclear & particles physicsResearchInstitutes_Networks_Beacons/mcrcMagnetic rotationRouthianNuclear TheoryOrder (ring theory)Semiclassical physicsState (functional analysis)rhenium01 natural sciencesNuclear shapeRecoilExcited state0103 physical scienceslifetimesAtomic physics010306 general physicsexcited statesPhysical Review C
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Generalized bloch equations for optical interactions in confined geometries

2005

By combining the field-susceptibility technique with the optical Bloch equations, a general formalism is developed for the investigation of molecular photophysical phenomena triggered by nanometer scale optical fields in the presence of complex environments. This formalism illustrate the influence of the illumination regime on the fluorescence signal emitted by a single molecule in a complex environment. In the saturated case, this signal is proportional to the optical local density of states, while it is proportional to the near-field intensity in the non-saturated case. (C) 2005 Elsevier B.V. All rights reserved.

PhysicsMicroscopyLocal density of statesGeneral Physics and AstronomySingle-Molecule SpectroscopyFluorescenceScaleFormalism (philosophy of mathematics)Bloch equationsQuantum mechanicsNear-FieldLight-SourceMoleculeDielectricsMaxwell-Bloch equationsPhysical and Theoretical ChemistryChemical Physics Letters
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Bounds on the entanglement of two-qutrit systems from fixed marginals

2019

We discuss the problem of characterizing upper bounds on entanglement in a bipartite quantum system when only the reduced density matrices (marginals) are known. In particular, starting from the known two-qubit case, we propose a family of candidates for maximally entangled mixed states with respect to fixed marginals for two qutrits. These states are extremal in the convex set of two-qutrit states with fixed marginals. Moreover, it is shown that they are always quasidistillable. As a by-product we prove that any maximally correlated state that is quasidistillable must be pure. Our observations for two qutrits are supported by numerical analysis.

PhysicsMixed statesNumerical analysisConvex setQuantum PhysicsQuantum entanglementState (functional analysis)01 natural sciences010305 fluids & plasmas0103 physical sciencesBipartite graphQuantum systemStatistical physicsQutritQuantum Entanglement010306 general physics
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Localization-delocalization transition for disordered cubic harmonic lattices.

2012

We study numerically the disorder-induced localization-delocalization phase transitions that occur for mass and spring constant disorder in a three-dimensional cubic lattice with harmonic couplings. We show that, while the phase diagrams exhibit regions of stable and unstable waves, the universality of the transitions is the same for mass and spring constant disorder throughout all the phase boundaries. The combined value for the critical exponent of the localization lengths of $\nu = 1.550^{+0.020}_{-0.017}$ confirms the agreement with the universality class of the standard electronic Anderson model of localization. We further support our investigation with studies of the density of states…

PhysicsModels MolecularPhase transitionCondensed matter physicsMolecular ConformationFOS: Physical sciencesDisordered Systems and Neural Networks (cond-mat.dis-nn)Condensed Matter - Disordered Systems and Neural NetworksRenormalization groupCondensed Matter PhysicsCondensed Matter::Disordered Systems and Neural NetworksPhase TransitionUniversality (dynamical systems)Models ChemicalDensity of statesGeneral Materials ScienceComputer SimulationWave functionCritical exponentAnderson impurity modelPhase diagramJournal of physics. Condensed matter : an Institute of Physics journal
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