Abstract:Understanding and simulating how a quantum system interacts and exchanges information or energy with its surroundings is a ubiquitous problem, one which must be carefully addressed in order to establish a coherent framework to describe the dynamics and thermodynamics of quantum systems. Significant effort has been invested in developing various methods for tackling this issue and in this Perspective paper we focus on one such technique, namely collision models, which have emerged as a remarkably flexible appro… Show more
“…Sketch of the information backflow in open quantum system dynamics, which is at the basis of the notion of quantum non-Markovianity used in this paper: initially the reduced states ρ, σ approach each other since the information is flowing out of the reduced system to the environment or to the correlations between the system and the environment (left); on the other hand, an information backflow makes the two states diverge from each other at a later time (right), as can be witnessed via proper state distinguishability quantifiers. This behaviour was observed in fundamental open system models[27,[62][63][64] as well as in general classes of dynamics arising by repeated random interactions as those that are considered in this paper[27,60].…”
mentioning
confidence: 65%
“…Note that, even though the definition of non-Markovianity used here has an interpretation in terms of information flow between the system and environment as explained above, it can be directly used at the level of the reduced evolution without the necessity to specify an underlying microscopical model. With this, it can also be applied to our phenomenological approach, where we construct the proper dynamical maps without directly starting from the total Hamiltonian, although realisations-for example, with collisional models-are possible [60,61]. approach each other since the information is flowing out of the reduced system to the environment or to the correlations between the system and the environment (left); on the other hand, an information backflow makes the two states diverge from each other at a later time (right), as can be witnessed via proper state distinguishability quantifiers.…”
Section: Memory Effects In Quantum Dynamicsmentioning
Simple, controllable models play an important role in learning how to manipulate and control quantum resources. We focus here on quantum non-Markovianity and model the evolution of open quantum systems by quantum renewal processes. This class of quantum dynamics provides us with a phenomenological approach to characterise dynamics with a variety of non-Markovian behaviours, here described in terms of the trace distance between two reduced states. By adopting a trajectory picture for the open quantum system evolution, we analyse how non-Markovianity is influenced by the constituents defining the quantum renewal process, namely the time-continuous part of the dynamics, the type of jumps and the waiting time distributions. We focus not only on the mere value of the non-Markovianity measure, but also on how different features of the trace distance evolution are altered, including times and number of revivals.
“…Sketch of the information backflow in open quantum system dynamics, which is at the basis of the notion of quantum non-Markovianity used in this paper: initially the reduced states ρ, σ approach each other since the information is flowing out of the reduced system to the environment or to the correlations between the system and the environment (left); on the other hand, an information backflow makes the two states diverge from each other at a later time (right), as can be witnessed via proper state distinguishability quantifiers. This behaviour was observed in fundamental open system models[27,[62][63][64] as well as in general classes of dynamics arising by repeated random interactions as those that are considered in this paper[27,60].…”
mentioning
confidence: 65%
“…Note that, even though the definition of non-Markovianity used here has an interpretation in terms of information flow between the system and environment as explained above, it can be directly used at the level of the reduced evolution without the necessity to specify an underlying microscopical model. With this, it can also be applied to our phenomenological approach, where we construct the proper dynamical maps without directly starting from the total Hamiltonian, although realisations-for example, with collisional models-are possible [60,61]. approach each other since the information is flowing out of the reduced system to the environment or to the correlations between the system and the environment (left); on the other hand, an information backflow makes the two states diverge from each other at a later time (right), as can be witnessed via proper state distinguishability quantifiers.…”
Section: Memory Effects In Quantum Dynamicsmentioning
Simple, controllable models play an important role in learning how to manipulate and control quantum resources. We focus here on quantum non-Markovianity and model the evolution of open quantum systems by quantum renewal processes. This class of quantum dynamics provides us with a phenomenological approach to characterise dynamics with a variety of non-Markovian behaviours, here described in terms of the trace distance between two reduced states. By adopting a trajectory picture for the open quantum system evolution, we analyse how non-Markovianity is influenced by the constituents defining the quantum renewal process, namely the time-continuous part of the dynamics, the type of jumps and the waiting time distributions. We focus not only on the mere value of the non-Markovianity measure, but also on how different features of the trace distance evolution are altered, including times and number of revivals.
“…The PReB process may be thought of as a collisional or repeated-interaction model [35][36][37][38][39], where the system repeatedly interacts with multiple finite-sized chains. Collisional or repeated-interaction models have provided valuable insight in a diverse range of settings, with quantum thermodynamics [40][41][42][43] and non-Markovian dynamics [44][45][46][47][48][49] being particularly elegant examples.…”
Section: Preb As a Collisional Or Repeated Interaction Modelmentioning
confidence: 99%
“…Obtaining the numerically exact dynamics of interacting quantum many-body chains in such two-terminal setups has been an outstanding problem, despite its relevance in a wide range of contexts, such as quantum transport, localization, integrability breaking [24][25][26][27][28][29][30][31][32][33][34], quantum heat engines, and refrigerators [2]. Further, we discuss the relationship between our formalism and collisional (or repeated interaction) models [35][36][37][38][39][40][41][42][43][44][45][46][47][48][49][50], highlighting how our results extend these notions, significantly advancing this highly active field of research. Finally, to demonstrate that our formalism can be combined with not one but any of the existing techniques for numerically exact non-Markovian dynamics [10][11][12][13][14][15][16][17][18][19][20][21][22][23], we also apply our formalism to a spin-boson model employing a completely different numerical technique [17] compared to the one used for the many...…”
“…We, in the framework of collision model (or repeated interaction model), will investigate the behaviors of steady heat current between the system and the TTB (also named target heat current-THC, hereafter) and thermal functions of the system with a CAB. Here, it is pointed out that the collision model has become a convenient and powerful tool for studying the dynamics of open quantum system [74], especially for the situations of non-equilibrium bath with quantum effects [75][76][77]. Thus, so far, the general thermodynamic framework of collision models has been explored deeply and established [35,[78][79][80].…”
We study a scheme of thermal management where a three-qubit system assisted with a coherent auxiliary bath (CAB) is employed to implement heat management on a target thermal bath (TTB). We consider the CAB/TTB being ensemble of coherent/thermal two-level atoms (TLAs), and within the framework of collision model investigate the characteristics of steady heat current (also called target heat current (THC)) between the system and the TTB. It demonstrates that with the help of the quantum coherence of ancillae the magnitude and direction of heat current can be controlled only by adjusting the coupling strength of system-CAB. Meanwhile, we also show that the influences of quantum coherence of ancillae on the heat current strongly depend on the coupling strength of system—CAB, and the THC becomes positively/negatively correlated with the coherence magnitude of ancillae when the coupling strength below/over some critical value. Besides, the system with the CAB could serve as a multifunctional device integrating the thermal functions of heat amplifier, suppressor, switcher and refrigerator, while with thermal auxiliary bath it can only work as a thermal suppressor. Our work provides a new perspective for the design of multifunctional thermal device utilizing the resource of quantum coherence from the CAB.
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