2018
DOI: 10.1103/physreve.98.012131
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Refrigeration beyond weak internal coupling

Abstract: We investigate the performance of a three-spin quantum absorption refrigerator using a refined open quantum system model valid across all interspin coupling strengths. It describes the transition between previous approximate models for the weak and the ultrastrong coupling limit, and it predicts optimal refrigeration for moderately strong coupling, where both approximations are inaccurate. Two effects impede a more effective cooling: the coupling between the spins no longer reduces to a simple resonant energy … Show more

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Cited by 52 publications
(69 citation statements)
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“…While the first distinction arises from the type of coupling considered in the system-reservoir interaction the second distinguishes between the different approximations leading to a final form of the master equation which depends on the magnitude of the inter-system coupling. For example, the Lindbladians obtained in equation (4) with the operators in equation (5) are fundamentally different from the ones obtained for the case of separate reservoirs under the global approach [31,35].…”
Section: Master Equation In the Local Approachmentioning
confidence: 75%
See 1 more Smart Citation
“…While the first distinction arises from the type of coupling considered in the system-reservoir interaction the second distinguishes between the different approximations leading to a final form of the master equation which depends on the magnitude of the inter-system coupling. For example, the Lindbladians obtained in equation (4) with the operators in equation (5) are fundamentally different from the ones obtained for the case of separate reservoirs under the global approach [31,35].…”
Section: Master Equation In the Local Approachmentioning
confidence: 75%
“…Henceforth, another figure of merit to characterize the performance of the refrigerator is the COP at maximum cooling power, which we denote by h * . This quantity has been extensively studied within the global approach in [31,35], and shown to be bounded by a fraction of h C only depending on the dimensionality of the cold reservoir [31,32].…”
Section: Characterization Of the Performancementioning
confidence: 99%
“…The origin of these effects, as shown in [75], lies in the fact that the heat fluxes become of the same order of magnitude as the neglected nonlocal terms They thus suggest to use the GME to fix such thermodynamic anomalies. These findings generated a considerable stream of investigations on the comparison between global and LMEs [49,52,53,61,[76][77][78][79][80][81][82] as well as clever possible alternatives [83,84].Recent results indicate, however, that it is possible to construct a consistent thermodynamic framework for LMEs, resolving these seeming contradictions. First and foremost, it is important to mention that, unlike Redfield equations, LMEs are in Lindblad form and therefore generate completely positive trace preserving (CPTP) maps.…”
mentioning
confidence: 99%
“…More precisely, this assertion is due to a restrictive consideration of the global master equation as limited by a full secular approximation, which also the authors recognize as responsible for the breakdown of the master equation. In [27] the possibility for a partial secular approximation is also suggested in order to cure such deficiency, and many other papers have pointed out why the full secular approximation may not be valid in some parameters ranges of different scenarios [25,34,56,64,69,70]. In the following, we therefore analyze in detail both local and global approach and show that the partial secular approximation allows to derive a global master equation that never leads to unphysical results, given that in the limit l  0 it coincides with the local master equation.…”
Section: Local Versus Global: An In-depth Discussionmentioning
confidence: 99%
“…In the master equation, the absence of counter-rotating terms eliminates all the 'double emission' or 'double absorption' jump operators, namely s w  ( ) j z III in equation (C.2). Without these terms important effects do not arise, such as stationary entanglement [23], or are not properly described, as the refrigerator performance analyzed in [70]. (20), where with abuse of notation α=c 1 =c 2 =c.…”
Section: A2 Further Qubit-qubit Couplingsmentioning
confidence: 99%