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Journal of Physics A Mathematical and Theoretical

Limits of Born approximation for unequal time correlation functions and detailed balance in open quantum systems

Katha Ganguly, Bijay Kumar Agarwalla

Published Nov 14, 2025• 0 citations
Publisher

Abstract

Abstract We show that, in general, the unequal time correlation function of system observables, when computed within the Born approximation in open quantum systems, fails to produce the temperature-dependent contributions required for thermalization in the long-time limit. As a consequence, Born approximation fails to respect the detailed balance condition in the long-time limit for arbitrary time difference. This occurs precisely due to the factorization of the total density matrix in the Born approximation, which neglects finite system–bath correlations. We demonstrate how incorporating the correction term recovers the temperature-dependent thermalization term and restores detailed balance. In contrast, we find that so-called spectral correlators, which are unrelated to detailed balance often correctly captured at the Born level to leading order in the system–bath coupling. We also provide a generic condition under which spectral correlators can be correctly predicted under Born approximation. Our approach is illustrated for two paradigmatic models of open quantum systems: (i) the dissipative Caldeira–Leggett model and (ii) the dissipative spin-boson model. We further extend our analysis for multi-bath non-equilibrium quantum transport scenario.

DOI
10.1088/1751-8121/ae1fc3

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•Jan 1, 2018•0 citations
Abstract We show that, in general, the unequal time correlation function of system observables, when computed within the Born approximation in open quantum systems, fails to produce the temperature-dependent contributions required for thermalization in the long-time limit. As a consequence, Born approximation fails to respect the detailed balance condition in the long-time limit for arbitrary time difference. This occurs precisely due to the factorization of the total density matrix in the Born approximation, which neglects finite system–bath correlations. We demonstrate how incorporating the correction term recovers the temperature-dependent thermalization term and restores detailed balance. In contrast, we find that so-called spectral correlators, which are unrelated to detailed balance often correctly captured at the Born level to leading order in the system–bath coupling. We also provide a generic condition under which spectral correlators can be correctly predicted under Born approximation. Our approach is illustrated for two paradigmatic models of open quantum systems: (i) the dissipative Caldeira–Leggett model and (ii) the dissipative spin-boson model. We further extend our analysis for multi-bath non-equilibrium quantum transport scenario.
We provide a systematic approach to compute different kinds of non-equilibrium Green's functions for open quantum systems which are essentially two-point correlation functions in time. We reveal that the definition of Green's functions based on the Born approximation does not provide the correct results in the leading order of the system-bath coupling. We next provide a systematic correction term in Green's functions by going beyond the Born approximation and incorporating a finite correlation between the system and the bath. We primarily focus on two paradigmatic models of open quantum systems, namely, the dissipative Caldeira-Leggett model and the dissipative spin-boson model. We show that the inclusion of such a correction correctly reproduces the Kadanoff-Baym type equation for the so-called lesser or greater components of the Green's functions and provides the correct long-time result up to the first non-zero order of the system-bath coupling, satisfying the detailed balance condition in thermal equilibrium. We further extend our study to a system coupled to multiple reservoirs simultaneously that are maintained at different temperatures and obtain expressions for non-equilibrium steady-state energy current, once again correct up to the first non-zero order of the system-bath coupling.
A quantum dissipation theory is constructed with the system–bath interaction being treated rigorously at the second-order cumulant level for both reduced dynamics and initial canonical boundary condition. The theory is valid for arbitrary bath correlation functions and time-dependent external driving fields, and satisfies correlated detailed-balance relation at any temperatures. The general formulation assumes a particularly simple form in driven Brownian oscillator systems in which the correlated driving-dissipation effects can be accounted for exactly in terms of local-field correction. Remarks on a class of widely used phenomenological quantum master equations that neglects the bath dispersion-induced dissipation are also made in contact with the present theory.
We consider the dynamics of a quantum system immersed in a dilute gas at thermodynamic equilibrium using a quantum Markovian master equation derived by applying the low-density limit technique. It is shown that the Gibbs state at the bath temperature is always stationary while the detailed balance condition at this state can be violated beyond the Born approximation. This violation is generically related to the absence of time-reversal symmetry for the scattering T matrix, which produces a thermalization mechanism that allows the presence of persistent probability and heat currents at thermal equilibrium. This phenomenon is illustrated by a model of an electron hopping between three quantum dots in an external magnetic field.
Within the lowest-order Born approximation, we present an exact calculation of the time dynamics of the spin-boson model in the Ohmic regime. We observe non-Markovian effects at zero temperature that scale with the system-bath coupling strength and cause qualitative changes in the evolution of coherence at intermediate times of order of the oscillation period. These changes could significantly affect the performance of these systems as qubits. In the biased case, we find a prompt loss of coherence at these intermediate times, whose decay rate is set by $\sqrt{\ensuremath{\alpha}}$, where $\ensuremath{\alpha}$ is the coupling strength to the environment. We also explore the calculation of the next-order Born approximation: we show that, at the expense of very large computational complexity, interesting physical quantities can be rigorously computed at fourth order using computer algebra, presented completely in an accompanying MATHEMATICA file. We compute the $O(\ensuremath{\alpha})$ corrections to the long time behavior of the system density matrix; the result is identical to the reduced density matrix of the equilibrium state to the same order in $\ensuremath{\alpha}$. All these calculations indicate precision experimental tests that could confirm or refute the validity of the spin-boson model in a variety of systems.
Abstract In this work we study a scenario where unitary quantum dynamics in a many-body interacting system is restricted to a single excitation subspace. We ask how dynamics within to such a subspace may in general differ from predictions of the eigenstate thermalization hypothesis (ETH). We show that for certain initial states and observables, if thermalization occurs, it will not fulfil other key predictions of the ETH; instead following differing generic behaviours. We show this by analysing long-time fluctuations, two-point correlation functions, and the out-of-time-ordered correlator; analytically detailing deviation from ETH predictions. We derive instead an ETH-like relation, with non-random off-diagonals for matrix elements of observables, with correlations which alter long-time behaviour and constrain dynamics. Further, we analytically compute the time-dependence of the decay to equilibrium, showing it is proportional to the survival probability of the initial state. We finally note the conditions studied are common in many physical scenarios, such as under the rotating-wave approximation. We show numerically our predictions are robust to perturbations which break this approximation.
The Lindblad theory of open quantum systems has been successfully applied in various fields ranging from quantum optics, condensed matter physics, and quantum thermodynamics to quantum chemistry. Nevertheless, there are situations where we can compare its predictions to those of exact methods or numerically exact results and find discrepancies between them. One example is the case where a single harmonic oscillator is coupled to a thermal bath of independent harmonic oscillators. In this case, for certain parameters, the exact master equation describes equilibration of the system to a thermal state with a temperature different from the one predicted by the Lindblad master equation. The Lindblad theory, based on a weak coupling between the system and environment as well as the Born-Markov approximation, predicts that the system will evolve to a thermal state whose temperature is equal to the initial temperature of the bath. This result is a consequence of the Born approximation, which supposes that throughout the evolution, the bath only fluctuates around its initial equilibrium state. In this master thesis we study the validity of the Born approximation as well as its consistency with other approximations. By starting from a Hamiltonian for the total system we show that, if the the Born approximation is not invoked, the dynamics of the system is determined by a hierarchy of equations for matrices which can be used to reconstruct the reduced density matrix of the system. This hierarchy approach is fundamentally different from the standard approach, which describes the system dynamics with a weak-coupling master equation, because the hierarchy does not restrict the amount of entanglement possible between the system and the environment. Furthermore, we show how invoking the Born approximation reduces to the usual result and how a generalised ansatz, which we refer to as a generalised Born approximation, reduces the hierarchy to a master equation where the bath temperature is an additional degree of freedom. Finally, we analyse the conservation of the energy of the total system and its relationship to the Markov and secular approximations, and discuss whether imposing it as a condition can fix the time-dependent temperature.