Search results for "master equation"

showing 10 items of 103 documents

Class of exact memory-kernel master equations

2016

A well-known situation in which a non-Markovian dynamics of an open quantum system $S$ arises is when this is coherently coupled to an auxiliary system $M$ in contact with a Markovian bath. In such cases, while the joint dynamics of $S$-$M$ is Markovian and obeys a standard (bipartite) Lindblad-type master equation (ME), this is in general not true for the reduced dynamics of $S$. Furthermore, there are several instances (\eg the dissipative Jaynes-Cummings model) in which a {\it closed} ME for the $S$'s state {\it cannot} even be worked out. Here, we find a class of bipartite Lindblad-type MEs such that the reduced ME of $S$ can be derived exactly and in a closed form for any initial produ…

PhysicsQuantum PhysicsPure mathematicsClass (set theory)Kernel (set theory)FOS: Physical sciencesState (functional analysis)open quantum systems01 natural sciencesmarkovian dynamicsSettore FIS/03 - Fisica Della Materia010305 fluids & plasmas3. Good healthopen quantum systemsOpen quantum systemcollision modelsProduct (mathematics)Quantum mechanics0103 physical sciencesMaster equationDissipative systemBipartite graphQuantum Physics (quant-ph)010306 general physicsnon markovian dynamicsPhysical Review A
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Microscopic derivation of the Jaynes-Cummings model with cavity losses

2006

In this paper we provide a microscopic derivation of the master equation for the Jaynes-Cummings model with cavity losses. We single out both the differences with the phenomenological master equation used in the literature and the approximations under which the phenomenological model correctly describes the dynamics of the atom-cavity system. Some examples wherein the phenomenological and the microscopic master equations give rise to different predictions are discussed in detail.

PhysicsQuantum PhysicsQuantum decoherenceJaynes–Cummings modelSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciCavity quantum electrodynamicsFOS: Physical sciences01 natural sciencesAtomic and Molecular Physics and OpticsSettore FIS/03 - Fisica Della Materia010305 fluids & plasmas0103 physical sciencesPhenomenological modelMaster equationQUANTUM-ELECTRODYNAMICS:AYNES-CUMMINGS MODELStatistical physicsQuantum Physics (quant-ph)010306 general physics
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Non-Markovian dissipative dynamics of two coupled qubits in independent reservoirs: a comparison between exact solutions and master equation approach…

2009

The reduced dynamics of two interacting qubits coupled to two independent bosonic baths is investigated. The one-excitation dynamics is derived and compared with that based on the resolution of appropriate non-Markovian master equations. The Nakajima-Zwanzig and the time-convolutionless projection operator techniques are exploited to provide a description of the non-Markovian features of the dynamics of the two-qubits system. The validity of such approximate methods and their range of validity in correspondence to different choices of the parameters describing the system are brought to light.

PhysicsQuantum PhysicsQuantum decoherenceMarkov processFOS: Physical sciencesAtomic and Molecular Physics and OpticsOpen quantum systemRange (mathematics)symbols.namesakeClassical mechanicsQubitMaster equationsymbolsopen quantum system master equation techniquesStatistical physicsQuantum Physics (quant-ph)BosonQuantum computer
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Collision-model-based approach to non-Markovian quantum dynamics

2013

We present a theoretical framework to tackle quantum non-Markovian dynamics based on a microscopic collision model (CM), where the bath consists of a large collection of initially uncorrelated ancillas. Unlike standard memoryless CMs, we endow the bath with memory by introducing inter-ancillary collisions between next system-ancilla interactions. Our model interpolates between a fully Markovian dynamics and the continuous interaction of the system with a single ancilla, i.e., a strongly non-Markovian process. We show that in the continuos limit one can derive a general master equation, which while keeping such features is guaranteed to describe an unconditionally completely positive and tra…

PhysicsQuantum PhysicsQuantum decoherenceQuantum dynamicsMarkov processFOS: Physical sciencesAtomic and Molecular Physics and Opticssymbols.namesakeExact solutions in general relativityClassical mechanicsSPINNon-Markovian open quantum systems collision modelsMaster equationDissipative systemsymbolsStatistical physicsQuantum informationQuantum Physics (quant-ph)Quantum
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Stimulated Raman adiabatic passage in a $\Lambda$-system in the presence of quantum noise

2011

We exploit a microscopically derived master equation for the study of STIRAP in the presence of decay from the auxiliary level toward the initial and final state, and compare our results with the predictions obtained from a phenomenological model previously used [P. A. Ivanov, N. V. Vitanov, and K. Bergmann, Phys. Rev. A 72, 053412 (2005)]. It is shown that our approach predicts a much higher efficiency. The effects of temperature are also taken into account, proving that in b-STIRAP thermal pumping can increase the efficiency of the population transfer.

PhysicsQuantum PhysicsQuantum decoherenceQuantum noiseStimulated Raman adiabatic passageAtomic and Molecular Physics and Opticssymbols.namesakeQuantum stateQuantum mechanicsMaster equationPhenomenological modelEvoluzioni adiabatiche STIRAP decoerenzasymbolsAdiabatic processRaman scattering
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Master equations for correlated quantum channels

2012

We derive the general form of a master equation describing the interaction of an arbitrary multipartite quantum system, consisting of a set of subsystems, with an environment, consisting of a large number of sub-envirobments. Each subsystem "collides" with the same sequence of sub-environments which, in between the collisions, evolve according to a map that mimics relaxations effects. No assumption is made on the specific nature of neither the system nor the environment. In the weak coupling regime, we show that the collisional model produces a correlated Markovian evolution for the joint density matrix of the multipartite system. The associated Linblad super-operator contains pairwise term…

PhysicsQuantum PhysicsQuantum decoherenceStatistical Mechanics (cond-mat.stat-mech)Lindblad equationFOS: Physical sciencesGeneral Physics and AstronomyMathematical Physics (math-ph)Settore FIS/03 - Fisica Della MateriaClassical mechanicsQuantum processMaster equationLindblad superoperatorQuantum operationQuantum algorithmQuantum Physics (quant-ph)QuantumCondensed Matter - Statistical MechanicsMathematical Physicsopen quantum systems master equations quantum correlations
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A quantum non-Markovian collision model: incoherent swap case

2013

We have recently presented a collision-model-based framework to approach non-Markovian quantum dynamics [Ciccarello F Palma G M and Giovannetti V 2013 Phys. Rev. A 87, 040103(R)]. As a distinctive feature, memory is introduced in a dynamical way by adding extra inter-ancillary collisions to a standard (memoryless) collision model. Here, we focus on the case where such intra-bath collisions are described by incoherent partial swap operations. After briefly reviewing the model, we show how to include temperature as an additional parameter by relaxing the assumption that each bath ancilla is initially in a pure state. We also calculate explicitly the dynamical map entailed by the master equati…

PhysicsQuantum PhysicsQuantum dynamicsFOS: Physical sciencesMarkov processDistinctive featureCollision modelCondensed Matter PhysicsAtomic and Molecular Physics and Opticssymbols.namesakeSPINNon-Markovian open quantum systems collision modelsMaster equationsymbolsStatistical physicsQuantum Physics (quant-ph)Swap (computer programming)QuantumMathematical Physics
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Quantum theory of heating of a single trapped ion

2003

The heating of trapped ions due to the interaction with a {\it quantized environment} is studied {\it without performing the Born-Markov approximation}. A generalized master equation local in time is derived and a novel theoretical approach to solve it analytically is proposed. Our master equation is in the Lindblad form with time dependent coefficients, thus allowing the simulation of the dynamics by means of the Monte Carlo Wave Function (MCWF) method.

PhysicsQuantum PhysicsQuantum mechanicsMonte Carlo methodMaster equationDynamics (mechanics)FOS: Physical sciencesGeneral Physics and AstronomyQuantum Physics (quant-ph)Wave functionIon
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Solution of the Lindblad equation in Kraus representation

2006

The so-called Lindblad equation, a typical master equation describing the dissipative quantum dynamics, is shown to be solvable for finite-level systems in a compact form without resort to writing it down as a set of equations among matrix elements. The solution is then naturally given in an operator form, known as the Kraus representation. Following a few simple examples, the general applicability of the method is clarified.

PhysicsQuantum PhysicsSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciLindblad equationFOS: Physical sciencesAtomic and Molecular Physics and OpticsSettore FIS/03 - Fisica Della MateriaThe so-called Lindblad equation a typical master equation describing the dissipative quantum dynamics is shown to be solvable for finite-level systems in a compact form without resort to writing it down as a set of equations among matrix elements. The solution is then naturally given in an operator form known as the Kraus representation. Following a few simple examples the general applicability of the method is clarified.Open quantum systemQuantum processMaster equationDissipative systemQuantum operationMethod of quantum characteristicsQuantum Physics (quant-ph)Quantum statistical mechanicsMathematical physics
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Reconstruction of Markovian master equation parameters through symplectic tomography

2009

In open quantum systems, phenomenological master equations with unknown parameters are often introduced. Here we propose a time-independent procedure based on quantum tomography to reconstruct the potentially unknown parameters of a wide class of Markovian master equations. According to our scheme, the system under investigation is initially prepared in a Gaussian state. At an arbitrary time t, in order to retrieve the unknown coefficients one needs to measure only a finite number (ten at maximum) of points along three time-independent tomograms. Due to the limited amount of measurements required, we expect our proposal to be especially suitable for experimental implementations.

PhysicsQuantum PhysicsSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciQuantum decoherenceTomography Markovian master equations Gaussian statesGaussianFOS: Physical sciencesMarkov processQuantum tomographyMeasure (mathematics)Atomic and Molecular Physics and Opticssymbols.namesakeQuantum mechanicsMaster equationsymbolsApplied mathematicsQuantum Physics (quant-ph)Finite setQuantumPhysical Review A
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