Search results for "Geometric phase"

showing 10 items of 40 documents

The quantum trajectory approach to geometric phase for open systems

2005

The quantum jump method for the calculation of geometric phase is reviewed. This is an operational method to associate a geometric phase to the evolution of a quantum system subjected to decoherence in an open system. The method is general and can be applied to many different physical systems, within the Markovian approximation. As examples, two main source of decoherence are considered: dephasing and spontaneous decay. It is shown that the geometric phase is to very large extent insensitive to the former, i.e. it is independent of the number of jumps determined by the dephasing operator.

Quantum phase transitionPhysicsNuclear and High Energy PhysicsQuantum decoherenceDecoherence-free subspacesDephasingquantum computationGeometric phaseGeneral Physics and AstronomyAstronomy and AstrophysicsOpen quantum systemClassical mechanicsQuantum error correctionQuantum processQuantum dissipationdecoherence
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Geometry of quantum phase transitions

2020

In this article we provide a review of geometrical methods employed in the analysis of quantum phase transitions and non-equilibrium dissipative phase transitions. After a pedagogical introduction to geometric phases and geometric information in the characterisation of quantum phase transitions, we describe recent developments of geometrical approaches based on mixed-state generalisation of the Berry-phase, i.e. the Uhlmann geometric phase, for the investigation of non-equilibrium steady-state quantum phase transitions (NESS-QPTs ). Equilibrium phase transitions fall invariably into two markedly non-overlapping categories: classical phase transitions and quantum phase transitions, whereas i…

Quantum phase transitionPhysicsPhase transitionQuantum PhysicsDissipative phase transitions Geometric phase Quantum geometric information Quantum metrology Quantum phase transitionsStatistical Mechanics (cond-mat.stat-mech)010308 nuclear & particles physicsCritical phenomenaGeneral Physics and AstronomyFOS: Physical sciences01 natural sciencesTheoretical physicssymbols.namesakeGeometric phase0103 physical sciencesQuantum metrologyDissipative systemsymbols010306 general physicsHamiltonian (quantum mechanics)Quantum Physics (quant-ph)QuantumCondensed Matter - Statistical Mechanics
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Geometric phases and criticality in spin chain systems

2005

A relation between geometric phases and criticality of spin chains is established. As a result, we show how geometric phases can be exploited as a tool to detect regions of criticality without having to undergo a quantum phase transition. We analytically evaluate the geometric phase that correspond to the ground and excited states of the anisotropic XY model in the presence of a transverse magnetic field when the direction of the anisotropy is adiabatically rotated. Ultra-cold atoms in optical lattices are presented as a possible physical realization.

Quantum phase transitionPhysicsQuantum PhysicsCondensed matter physicsCondensed Matter - Mesoscale and Nanoscale PhysicsPhase (waves)General Physics and AstronomyFOS: Physical sciencesQuantum phase transitionClassical XY modelSpin-chain systemsGeometric phaseCriticalityUltracold atomQuantum mechanicsMesoscale and Nanoscale Physics (cond-mat.mes-hall)AnisotropyQuantum Physics (quant-ph)Spin-½
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Scaling of Berry's phase close to the Dicke quantum phase transition

2006

We discuss the thermodynamic and finite size scaling properties of the geometric phase in the adiabatic Dicke model, describing the super-radiant phase transition for an $N$ qubit register coupled to a slow oscillator mode. We show that, in the thermodynamic limit, a non zero Berry phase is obtained only if a path in parameter space is followed that encircles the critical point. Furthermore, we investigate the precursors of this critical behavior for a system with finite size and obtain the leading order in the 1/N expansion of the Berry phase and its critical exponent.

Quantum phase transitionPhysicsQuantum PhysicsPhase transitionFOS: Physical sciencesGeneral Physics and AstronomyGeometric phaseCritical point (thermodynamics)Quantum mechanicsQubitThermodynamic limitQuantum phase transition Berry phaseQuantum Physics (quant-ph)Adiabatic processCritical exponentEurophysics Letters (EPL)
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Berry Phase and Parametric Harmonic Oscillator

2001

Our concern in this section is once more with the time-dependent harmonic oscillator with Lagrangian $$\displaystyle{ L = \frac{1} {2}\dot{x}^{2} -\frac{1} {2}\omega ^{2}(t)x^{2}\;. }$$ To present a coherent picture of the whole problem, let us briefly review some of the results of Chap. 21. There we found the propagation function

Section (fiber bundle)PhysicsVackář oscillatorGeometric phaseQuantum mechanicsAnharmonicityFunction (mathematics)Parametric oscillatorOmegaHarmonic oscillator
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GEOMETRY OF DISSIPATIVE PHASE TRANSITIONS

The main objective of this thesis is the development of geometrical methods for the investigation of critical phenomena. In particular, a novel approach based on the Uhlmann curvature is introduced for the investigation of non-equilibrium steady-state quantum phase transitions (NESS-QPTs). Equilibrium phase transitions fall invariably into two markedly non-overlapping categories: classical phase transitions and quantum phase transitions. NESS-QPTs offer a unique arena where such a distinction fades off. We propose a method to reveal and quantitatively assess the quantum character of such critical phenomena. We apply this tool to a paradigmatic class of lattice fermion systems with local res…

Settore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciQuantum phase transition. Non-equilibrium phase transition. Geometric phase. Information geometry. Quantum information. Quantum parameter estimation.
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Haldane Model at finite temperature

2019

We consider the Haldane model, a 2D topological insulator whose phase is defined by the Chern number. We study its phases as temperature varies by means of the Uhlmann number, a finite temperature generalization of the Chern number. Because of the relation between the Uhlmann number and the dynamical transverse conductivity of the system, we evaluate also the conductivity of the model. This analysis does not show any sign of a phase transition induced by the temperature, nonetheless it gives a better understanding of the fate of the topological phase with the increase of the temperature, and it provides another example of the usefulness of the Uhlmann number as a novel tool to study topolog…

Statistics and ProbabilityPhase transitionGeneralizationFOS: Physical sciencesConductivity01 natural sciences010305 fluids & plasmasCondensed Matter - Strongly Correlated ElectronsPhase (matter)0103 physical sciencesStatistical physics010306 general physicsCondensed Matter - Statistical MechanicsPhysicstopological insulatorQuantum PhysicsChern classStatistical Mechanics (cond-mat.stat-mech)Strongly Correlated Electrons (cond-mat.str-el)Topological phase of matter phase transition geometric phase quantum transportStatistical and Nonlinear PhysicsTransverse planeTopological insulatorStatistics Probability and UncertaintyQuantum Physics (quant-ph)Sign (mathematics)
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On critical properties of the Berry curvature in the Kitaev honeycomb model

2019

We analyse the Kitaev honeycomb model, by means of the Berry curvature with respect to Hamiltonian parameters. We concentrate on the ground-state vortex-free sector, which allows us to exploit an appropriate Fermionisation technique. The parameter space includes a time-reversal breaking term which provides an analytical headway to study the curvature in phases in which it would otherwise vanish. The curvature is then analysed in the limit in which the time-reversal-symmetry-breaking perturbation vanishes. This provides remarkable information about the topological phase transitions of the model. The Berry curvature in itself exhibits no singularities at criticality, nevertheless it distingui…

Statistics and ProbabilityQuantum phase transitionPhysicsCondensed matter physicsHoneycomb (geometry)Statistical and Nonlinear PhysicsBerry connection and curvatureStatistics Probability and UncertaintyTopological phases of Matter geometric phase phase transition anyons and fractional statistical models quantum phase transitionsJournal of Statistical Mechanics: Theory and Experiment
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Implementation of single-qubit quantum gates by adiabatic passage and static laser phases

2006

International audience; We propose and analyse experimentally feasible implementations of single-qubit quantum gates based on stimulated Raman adiabatic passage (STIRAP) between magnetic sublevels in atoms coupled by elliptically polarized pulsed laser fields, in part based on a proposal by Kis and Renzoni [Z. Kis, F. Renzoni, Phys. Rev. A 65 (2002) 032318]. These techniques require only the control of the relative phase of the driving fields but do not involve any dynamical or geometric phases, which makes it independent of the other interaction details: detuning, pulse shapes, pulse areas and pulse durations. The suggested techniques are immune to spontaneous emission since the qubit mani…

[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]Stimulated Raman adiabatic passage7. Clean energy01 natural sciences010305 fluids & plasmasQuantum gateOptics[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]Quantum mechanics0103 physical sciencesSpontaneous emissionElectrical and Electronic EngineeringPhysical and Theoretical Chemistry010306 general physicsAdiabatic processComputingMilieux_MISCELLANEOUS[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]Quantum computerPhysics[PHYS.PHYS.PHYS-AO-PH]Physics [physics]/Physics [physics]/Atmospheric and Oceanic Physics [physics.ao-ph]business.industryAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsPulse (physics)Geometric phase[ PHYS.PHYS.PHYS-AO-PH ] Physics [physics]/Physics [physics]/Atmospheric and Oceanic Physics [physics.ao-ph]Qubitbusiness
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Non-adiabatic vacuum induced berry phase

2016

We investigate quantum effects in geometric phases arising when a two-level system is interacting with a quantized electromagnetic field.

non-adiabaticQuantum FieldGeometric phase: vacuum
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