2016
DOI: 10.1103/physreve.94.062109
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Speed and efficiency limits of multilevel incoherent heat engines

Abstract: We present a comprehensive theory of heat engines (HE) based on a quantum-mechanical "working fluid" (WF) with periodically-modulated energy levels. The theory is valid for any periodicity of driving Hamiltonians that commute with themselves at all times and do not induce coherence in the WF. Continuous and stroke cycles arise in opposite limits of this theory, which encompasses hitherto unfamiliar cycle forms, dubbed here hybrid cycles. The theory allows us to discover the speed, power and efficiency limits a… Show more

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Cited by 23 publications
(21 citation statements)
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“…Thus, if one starts from a high w k ( w > k *) and progressively lowers its value, a transition from QR to QHE occurs at w k *, followed by a transition to the accelerator regime. On a related note, the above QHE-QR transition has also been shown in four-stroke [61] and continuous thermal machines [50,54,62]. Note that, while Q h and Q c reverse their sign only at the first transition (QR-QHE), W undergoes sign reversal at the QHE-accelerator transition as well.…”
Section: Thermalization Stroke ( T )mentioning
confidence: 54%
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“…Thus, if one starts from a high w k ( w > k *) and progressively lowers its value, a transition from QR to QHE occurs at w k *, followed by a transition to the accelerator regime. On a related note, the above QHE-QR transition has also been shown in four-stroke [61] and continuous thermal machines [50,54,62]. Note that, while Q h and Q c reverse their sign only at the first transition (QR-QHE), W undergoes sign reversal at the QHE-accelerator transition as well.…”
Section: Thermalization Stroke ( T )mentioning
confidence: 54%
“…Depending on the sign of Q h , Q c and W, TTMs may depict four distinct regimes of operation [53,54],…”
Section: Thermalization Stroke ( T )mentioning
confidence: 99%
“…To obtain the efficiency bound, we need to extract the ergotropy from the WF (by the piston via a suitable unitary transformation) before its interaction with the cold bath. In continuous cycles where both baths are simultaneously coupled to the WF [19,26,63], part of the ergotropy may then be dissipated into the cold bath, so that such cycles are inherently less efficient than stroke cycles. For time-dependent Hamiltonians, the requirement that H(t) commutes with itself at all times, e.g., a HO with time-independent eigenstates, will be adopted in this chapter for any interaction of a system with a bath, since Hamiltonians that do not commute with themselves at different times reduce the efficiency via "quantum friction" [20,64].…”
Section: Efficiency Bound Of Cyclic Quantum Engines Powered By Thmentioning
confidence: 99%
“…These quantum processes with a finite time duration can be also interesting as a non-adiabatic counterpart to a local quench dynamics of a suddenly cut and stitched spin chains [15], and for bond impurity chain cutting [16]. Another related field is the quantum thermodynamics [17], or the physics of quantum heat machines [18][19][20][21], where one part of the spin chain can be considered as a working medium, connected to and disconnected from the other part, which plays the role of a thermal reservoir.…”
Section: Introductionmentioning
confidence: 99%