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Achieve Higher Efficiency at Maximum Power with Finite-time Quantum Otto Cycle

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arxiv 1904.12128 v2 pith:WOOP42XW submitted 2019-04-27 quant-ph

classification quant-ph
keywords finite-timecyclequantumefficiencymaximumottopowercarnot-like
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The optimization of finite-time thermodynamic heat engines was intensively explored recently, yet limited to few cycles, e.g. finite-time Carnot-like cycle. In this paper, we supplement a new type of finite-time engine with quantum Otto cycle and show the better performance. The current model can be widely utilized benefited from the general \mathcal{C}/\tau^{2} scaling of extra work for finite-time adiabatic process with long control time \tau. Such scaling allows analytical optimization of the generic finite-time quantum Otto cycle to surpass the efficiency at maximum power for the Carnot-like engine. We apply the current perturbation method to the quantum piston model and calculate the efficiency at maximum power, which is validated with exact solution.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Efficiency at the maximum power of the power law dissipative Carnot-like Heat engines with non-adiabatic dissipation

    cond-mat.stat-mech 2019-09 conditional novelty 4.0 of 10

    Adding non-adiabatic, power-law dissipative friction in the adiabatic branches of a Carnot-like engine leaves the universal minimum and maximum efficiency-at-maximum-power bounds unchanged.

  2. Quantum Brayton Engine of Non-Interacting Fermions in a One-Dimensional Box

    cond-mat.stat-mech 2019-08 conditional novelty 4.0 of 10

    A quantum Brayton cycle with fermions in a one-dimensional box has an efficiency set by box-length ratios alone, independent of particle number, while power scales with the number of particles.

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