2013
DOI: 10.1140/epjd/e2013-30763-8
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Negentropy as a source of efficiency: a nonequilibrium quantum Otto cycle

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Cited by 16 publications
(11 citation statements)
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“…along with the normalization condition Equation (24). The integral of Equation (36) from B γ → B δ yields:…”
Section: The Iso-energetic Cyclementioning
confidence: 99%
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“…along with the normalization condition Equation (24). The integral of Equation (36) from B γ → B δ yields:…”
Section: The Iso-energetic Cyclementioning
confidence: 99%
“…with p 2 (B) = 1 − p 1 (B) after the normalization condition Equation (24). The heat exchanged by the system with the environment during the iso-energetic trajectory connecting the initial and final states B 1 → B 2 is given by the expression:…”
Section: The Iso-energetic Cyclementioning
confidence: 99%
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“…Phaseonium engine could work with a single heat bath and a phaseonium reservoir [4][5][6][7]. This proposal stimulated much interest to quantum heat engines [8][9][10][11][12][13][14][15][16][17][18][19][20]. It was later argued that existing resonator systems can not implement such an engine, due to high cavity losses and atomic dephasing [21].…”
Section: Introductionmentioning
confidence: 99%
“…These include entangled states in a qubit, 10 as well as quantum mechanical versions of the diesel 6 and Otto cycles (i.e., the operating principles of dieselfueled and gasoline-fueled car engines, respectively). 7,[11][12][13] In general, idealized reciprocating QHENs involve a stationary limit cycle 3,14 consisting of a sequence of intermediate equilibrium states that can be described microscopically by a density matrix operator that depends on a minimal set of macroscopic variables. 14,15 As part of these developments, we have recently proposed a magnetically driven QHEN that combines the effects of a parabolic confining potential (which can be provided by a semiconductor quantum dot) with an external magnetic field.…”
mentioning
confidence: 99%