2014
DOI: 10.1103/physrevlett.112.030602
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Nanoscale Heat Engine Beyond the Carnot Limit

Abstract: We consider a quantum Otto cycle for a time-dependent harmonic oscillator coupled to a squeezed thermal reservoir. We show that the efficiency at maximum power increases with the degree of squeezing, surpassing the standard Carnot limit and approaching unity exponentially for large squeezing parameters. We further propose an experimental scheme to implement such a model system by using a single trapped ion in a linear Paul trap with special geometry. Our analytical investigations are supported by Monte Carlo s… Show more

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Cited by 626 publications
(650 citation statements)
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References 60 publications
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“…Such a study helps us to understand the special behavior of thermodynamic quantities like work, heat, and efficiency in the quantum regime due to the presence non-classical features such as entanglement, quantum superposition, squeezing, etc. [19][20][21]. The quantum heat devices can show interesting atypical behaviors such as exceeding Carnot limit [19,21] when they act as heat engines.…”
Section: Introductionmentioning
confidence: 99%
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“…Such a study helps us to understand the special behavior of thermodynamic quantities like work, heat, and efficiency in the quantum regime due to the presence non-classical features such as entanglement, quantum superposition, squeezing, etc. [19][20][21]. The quantum heat devices can show interesting atypical behaviors such as exceeding Carnot limit [19,21] when they act as heat engines.…”
Section: Introductionmentioning
confidence: 99%
“…[19][20][21]. The quantum heat devices can show interesting atypical behaviors such as exceeding Carnot limit [19,21] when they act as heat engines. However, these apparent behaviors are found to be compatible with the second law of thermodynamics when all the preparation costs are considered [22].…”
Section: Introductionmentioning
confidence: 99%
“…In a first line of experiments, we construct an Otto cycle between a hot squeezed thermal reservoir with effective temperature T h ¼ 10 000 K and squeezing factor r ¼ 0.4 and a cold purely thermal bath at T c ¼ 9500 K under maximum power condition [19]. The four strokes include an adiabatic compression, isochoric heat addition, adiabatic expansion, and isochoric heat rejection.…”
Section: Otto Cycle With Squeezed Thermal Reservoirsmentioning
confidence: 99%
“…In the future, the exploitation of novel sources of work could have a large impact on the design of efficient and powerful engines at the microscale and nanoscale. By employing nonequilibrium reservoirs, it is expected that the efficiency of work generation can surpass standard thermodynamic bounds, as has been theoretically suggested for quantum coherent [12], quantum correlated [13,14], quantum-measurement-induced [15][16][17], and squeezed thermal reservoirs [18][19][20][21][22][23]. The realization of such engines not only extends our knowledge of finite-size, nonequilibrium, and quantum effects in thermodynamics, but could also lead to important applications in nanotechnology and in the life sciences [24].…”
Section: Introductionmentioning
confidence: 98%
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