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Achieve Higher Efficiency at Maximum Power with Finite-time Quantum Otto Cycle
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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.
Forward citations
Cited by 2 Pith papers
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Efficiency at the maximum power of the power law dissipative Carnot-like Heat engines with non-adiabatic dissipation
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.
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Quantum Brayton Engine of Non-Interacting Fermions in a One-Dimensional Box
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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