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Exact Redfield description for open non-interacting quantum systems and failure of the Lindblad approach  [PDF]
Archak Purkayastha,Manas Kulkarni,Abhishek Dhar
Physics , 2015,
Abstract: We present the Redfield quantum master equation (RQME) description for an open system of non-interacting particles (bosons or fermions) on an arbitrary lattice of $N$ sites in any dimension and connected to multiple reservoirs at different temperatures and chemical potentials. For the $N=2$ case, we show that RQME is robust against pathologies one sees in the conventional Lindblad equation approaches. It gives results which agree with exact analytical results for steady state properties and with exact numerics for time-dependent properties. These results can be experimentally relevant for cold atoms, cavity QED and far-from-equilibrium quantum dot experiments.
Exact Nonequilibrium Steady State of an Open Hubbard Chain  [PDF]
Tomaz Prosen
Physics , 2013, DOI: 10.1103/PhysRevLett.112.030603
Abstract: We discuss current carrying non-equilibrium steady state of an open fermionic Hubbard chain that is strongly driven by markovian incoherent processes localized at the chain ends. An explicit form of exact many-body density operator for any value of the coupling parameter is presented. The structure of a matrix product form of the solution is encoded in terms of a novel diagrammatic technique which should allow for generalization to other integrable non-equillibrium models.
On the steady state correlation functions of open interacting systems  [PDF]
Horia D. Cornean,Claude-Alain Pillet,Valeriu Moldoveanu
Physics , 2013, DOI: 10.1007/s00220-014-1925-0
Abstract: We address the existence of steady state Green-Keldysh correlation functions of interacting fermions in mesoscopic systems for both the partitioning and partition-free scenarios. Under some spectral assumptions on the non-interacting model and for sufficiently small interaction strength, we show that the system evolves to a NESS which does not depend on the profile of the time-dependent coupling strength/bias. For the partitioned setting we also show that the steady state is independent of the initial state of the inner sample. Closed formulae for the NESS two-point correlation functions (Green-Keldysh functions), in the form of a convergent expansion, are derived. In the partitioning approach, we show that the 0th order term in the interaction strength of the charge current leads to the Landauer-Buettiker formula, while the 1st order correction contains the mean-field (Hartree-Fock) results.
Power-law approach to steady state in open lattices of non-interacting electrons  [PDF]
M. V. Medvedyeva,S. Kehrein
Physics , 2014, DOI: 10.1103/PhysRevB.90.205410
Abstract: We address the question of how a non-equilibrium steady state (NESS) is reached in the Linbdladian dynamics of an open quantum system. We develop an expansion of the density matrix in terms of the NESS-excitations, each of which has its own (exponential) decay rate. However, when the decay rates tend to zero for many NESS-excitations (the spectral gap of the Liouvillian is closed in the thermodynamic limit), the long-time dynamics of the system can exhibit a power-law behaviour. This relaxation to NESS expectation values is determined by the density of states close to zero spectral gap and the value of the operator in these states. We illustrate this main idea on the example of the lattice of non-interacting fermions coupled to Markovian leads at infinite bias voltage. The current comes towards its NESS value starting from a typical initial state as $\tau^{-3/2}$. This behaviour is universal and independent of the space dimension.
Exact nonequilibrium steady state of a strongly driven open XXZ chain  [PDF]
Tomaz Prosen
Physics , 2011, DOI: 10.1103/PhysRevLett.107.137201
Abstract: An exact and explicit ladder-tensor-network ansatz is presented for the non-equilibrium steady state of an anisotropic Heisenberg XXZ spin-1/2 chain which is driven far from equilibrium with a pair of Lindblad operators acting on the edges of the chain only. We show that the steady-state density operator of a finite system of size n is - apart from a normalization constant - a polynomial of degree 2n-2 in the coupling constant. Efficient computation of physical observables is faciliated in terms of a transfer operator reminiscent of a classical Markov process. In the isotropic case we find cosine spin profiles, 1/n^2 scaling of the spin current, and long-range correlations in the steady state. This is a fully nonperturbative extension of a recent result [Phys. Rev. Lett. 106, 217206 (2011)].
Exact solutions of open integrable quantum spin chains  [PDF]
Enej Ilievski
Physics , 2014,
Abstract: In the thesis we present an analytic approach towards exact description for steady state density operators of nonequilibrium quantum dynamics in the framework of open systems. We employ the so-called quantum Markovian semi-group evolution, i.e. a general form of time-autonomous positivity and trace-preserving dynamical equation for reduced density operators, by only allowing unitarity-breaking dissipative terms acting at the boundaries of a system. Such setup enables to simulate macroscopic reservoirs for different values of effective thermodynamic potentials, causing incoherent transitions between quantum states which are modeled with aid of the Lindblad operators. This serves as a simple minimalistic model for studying quantum transport properties, either in the linear response domain or in more general regimes far from canonical equilibrium. We are mainly exploring possibilities of identifying nonequilibrium situations which are amenable to exact description within matrix product state representation, by exclusively focusing on steady states, i.e. fixed points of the Lindblad equation, of certain prototypic interacting integrable spin chains driven by incoherent polarizing processes. Finally, we define a concept of pseudo-local extensive almost-conserved quantities by allowing a violation of time-invariance up to boundary-localized terms. We elucidate the role of such quantities on non-ergodic behaviour of temporal correlation functions rendering anomalous transport properties. It turns out that such conservation laws can be generated by means of boundary universal quantum transfer operators of the fundamental integrable models.
Exact solution for a diffusive nonequilibrium steady state of an open quantum chain  [PDF]
Marko Znidaric
Statistics , 2010, DOI: 10.1088/1742-5468/2010/05/L05002
Abstract: We calculate a nonequilibrium steady state of a quantum XX chain in the presence of dephasing and driving due to baths at chain ends. The obtained state is exact in the limit of weak driving while the expressions for one- and two-point correlations are exact for an arbitrary driving strength. In the steady state the magnetization profile and the spin current display diffusive behavior. Spin-spin correlation function on the other hand has long-range correlations which though decay to zero in either the thermodynamical limit or for equilibrium driving. At zero dephasing a nonequilibrium phase transition occurs from a ballistic transport having short-range correlations to a diffusive transport with long-range correlations.
Perturbative treatment of the multichannel interacting resonant level model in steady state non-equilibrium  [PDF]
L. Borda,A. Zawadowski
Physics , 2009, DOI: 10.1103/PhysRevB.81.153303
Abstract: We consider the steady state non-equilibrium physics of the multichannel interacting resonant level model in the weak coupling regime. By using the scattering state method we show in agreement with the rate equations that the negative differential conductance at large enough voltages is due to the renormalization of the hopping amplitude thus of the vertex.
Exact solution of Markovian master equations for quadratic fermi systems: thermal baths, open XY spin chains, and non-equilibrium phase transition  [PDF]
Tomaz Prosen,Bojan Zunkovic
Physics , 2009, DOI: 10.1088/1367-2630/12/2/025016
Abstract: We generalize the method of third quantization to a unified exact treatment of Redfield and Lindblad master equations for open quadratic systems of n fermions in terms of diagonalization of 4n x 4n matrix. Non-equilibrium thermal driving in terms of the Redfield equation is analyzed in detail. We explain how to compute all physically relevant quantities, such as non-equilibrium expectation values of local observables, various entropies or information measures, or time evolution and properties of relaxation. We also discuss how to exactly treat explicitly time dependent problems. The general formalism is then applied to study a thermally driven open XY spin 1/2 chain. We find that recently proposed non-equilibrium quantum phase transition in the open XY chain survives the thermal driving within the Redfield model. In particular, the phase of long-range magnetic correlations can be characterized by hypersensitivity of the non-equilibrium-steady state to external (bath or bulk) parameters. Studying the heat transport we find negative thermal conductance for sufficiently strong thermal driving, as well as non-monotonic dependence of the heat current on the strength of the bath coupling.
An exact stochastic field method for the interacting Bose gas at thermal equilibrium  [PDF]
Iacopo Carusotto,Yvan Castin
Physics , 2001, DOI: 10.1088/0953-4075/34/23/305
Abstract: We present a new exact method to numerically compute the thermodynamical properties of an interacting Bose gas in the canonical ensemble. As in our previous paper (Phys. Rev. A, 63 023606 (2001)), we write the density operator $\rho$ as an average of Hartree dyadics $\ketbra{N:\phi_1}{N:\phi_2}$ and we find stochastic evolution equations for the wave functions $\phi_{1,2}$ such that the exact imaginary-time evolution of $\rho$ is recovered after average over noise. In this way, the thermal equilibrium density operator can be obtained for any temperature $T$. The method is then applied to study the thermodynamical properties of a homogeneous one-dimensional $N$-boson system: although Bose-Einstein condensation can not occur in the thermodynamical limit, a macroscopic occupation of the lowest mode of a finite system is observed at sufficiently low temperatures. If $k_B T \gg \mu$, the main effect of interactions is to suppress density fluctuations and to reduce their correlation length. Different effects such as a spatial antibunching of the atoms are predicted for the opposite $k_B T\leq \mu$ regime. Our exact stochastic calculations have been compared to existing approximate theories.
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