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arXiv:2605.01719 · Advanced Quantum Technologies

Coherence-Preserving Fluctuation Diagnostics for an Engineered Population-Inverted Qubit Otto Engine

Gabriella G. Damas, Norton G. de Almeida, Gao Xianlong, G. D. de Moraes Neto

quant-phSubmitted May 3, 2026• Announced May 5, 2026• 0 citations
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Abstract

Finite-time quantum thermal machines require diagnostics beyond average work and efficiency, because microscopic engines operate in regimes where fluctuations, incomplete thermalization, and coherence are equally important. Here we develop a measurement-backaction-free (coherence-preserving) fluctuation diagnostic for an engineered qubit Otto engine coupled to an actively maintained population-inverted hot channel. The engine is analyzed using a dynamic Bayesian network (DBN) reconstruction of the unmeasured coherent cycle, yielding work, heat, power, and normalized efficiency-proxy fluctuations without imposing the projective dephasing inherent in two-point energy measurements. The inverted channel is treated as an active reduced-model resource; accordingly, all reported power and efficiency enhancements represent gross working-medium advantages, not net device efficiencies. In the full-thermalization limit, population inversion enhances extracted work and output power while opening a stability sector with markedly reduced relative power fluctuations. When finite-duration isochores are implemented, this gross enhancement reorganizes into a structured operating landscape with distinct high-power, high-efficiency, and low-relative-noise sectors, whose boundaries are governed by the competing timescales of nonadiabatic driving and thermalization rates. A direct comparison reveals that DBN and conventional two-point measurement predictions diverge precisely in coherence-rich regimes, identifying where a backaction-free reconstruction is essential. A coherence-sensitive analysis further shows that the positive-temperature reference operates optimally in an almost decohered region, whereas the inverted high-efficiency branch remains aligned with the dominant post-hot-bath coherence ridge. These results provide a reduced-model benchmarking framework for engineered qubit thermal machines.

AI Summary

The paper asks how population inversion, incomplete thermalization, and coherence affect the output and fluctuations of a finite-time qubit Otto engine. It models noncommuting hot and cold Hamiltonians, driven unitary strokes, and Lindblad isochores with an actively maintained inverted hot-channel stationary state. A dynamic Bayesian network (DBN) reconstructs positive energy-history probabilities from corner-state eigenprojectors, preserving unmeasured-cycle mean energetics rather than imposing energy-measurement dephasing. Numerical stationary-cycle scans identify distinct output–noise sectors. In the ideal-reset benchmark, the inverted performance optimum gives roughly $2.3$ times the work and power of the best positive-temperature point, with gross efficiency $0.979$ versus $0.493$. A separate inverted stability point has comparable power and relative power fluctuation $\phi_P=\sigma(P)/|\langle P\rangle|=0.338$, versus $1.38$ for the positive-temperature optimum. With finite isochores, maximum power is approximately seven times the inverted reset benchmark; the maximum-efficiency point reaches $0.980$ but has $\phi_P=14.3$. The inverted high-efficiency sector aligns with residual post-hot-stroke coherence. An average-level DBN–TPM comparison finds discrepancies in short-time coherent regimes and convergence at long driving times. These are gross working-medium results: inversion-maintenance costs, implementation-specific reservoir physics, and tomography errors are excluded. The Markovian approximation may fail at short contacts. The efficiency-fluctuation variable is normalized work, $-W/\langle Q_h\rangle$, not trajectory efficiency; its relative noise equals $\phi_P$. DBN is an ensemble reconstruction, not a backaction-free single-shot measurement, and no distribution-level DBN–TPM comparison is provided.

Likely largely AI-generatedIncrementalSmall numerics onlyStrong assumptionsMissing comparison

Error found: The ideal-reset powers in Table I imply cycle durations near 25,000, contradicting the minimum duration of 100,000 required by the stated two 50,000-duration isochores. Using the stated ideal-reset duration, the reported finite-time maximum power exceeds the inverted reset benchmark by at least approximately 27-fold, not the claimed nearly sevenfold. The quoted inverted-branch coherence values are approximately 19–27 times below ln(2), not roughly two orders of magnitude below it.

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Finite-time quantum thermal machines require diagnostics beyond average work and efficiency, because microscopic engines operate in regimes where fluctuations, incomplete thermalization, and coherence are equally important. Here we develop a measurement-backaction-free (coherence-preserving) fluctuation diagnostic for an engineered qubit Otto engine coupled to an actively maintained population-inverted hot channel. The engine is analyzed using a dynamic Bayesian network (DBN) reconstruction of the unmeasured coherent cycle, yielding work, heat, power, and normalized efficiency-proxy fluctuations without imposing the projective dephasing inherent in two-point energy measurements. The inverted channel is treated as an active reduced-model resource; accordingly, all reported power and efficiency enhancements represent gross working-medium advantages, not net device efficiencies. In the full-thermalization limit, population inversion enhances extracted work and output power while opening a stability sector with markedly reduced relative power fluctuations. When finite-duration isochores are implemented, this gross enhancement reorganizes into a structured operating landscape with distinct high-power, high-efficiency, and low-relative-noise sectors, whose boundaries are governed by the competing timescales of nonadiabatic driving and thermalization rates. A direct comparison reveals that DBN and conventional two-point measurement predictions diverge precisely in coherence-rich regimes, identifying where a backaction-free reconstruction is essential. A coherence-sensitive analysis further shows that the positive-temperature reference operates optimally in an almost decohered region, whereas the inverted high-efficiency branch remains aligned with the dominant post-hot-bath coherence ridge. These results provide a reduced-model benchmarking framework for engineered qubit thermal machines.
The paper asks how population inversion, incomplete thermalization, and coherence affect the output and fluctuations of a finite-time qubit Otto engine. It models noncommuting hot and cold Hamiltonians, driven unitary strokes, and Lindblad isochores with an actively maintained inverted hot-channel stationary state. A dynamic Bayesian network (DBN) reconstructs positive energy-history probabilities from corner-state eigenprojectors, preserving unmeasured-cycle mean energetics rather than imposing energy-measurement dephasing.
Numerical stationary-cycle scans identify distinct output–noise sectors. In the ideal-reset benchmark, the inverted performance optimum gives roughly 2.32.32.3 times the work and power of the best positive-temperature point, with gross efficiency 0.9790.9790.979 versus 0.4930.4930.493. A separate inverted stability point has comparable power and relative power fluctuation ϕP=σ(P)/∣⟨P⟩∣=0.338\phi_P=\sigma(P)/|\langle P\rangle|=0.338ϕP​=σ(P)/∣⟨P⟩∣=0.338, versus 1.381.381.38 for the positive-temperature optimum. With finite isochores, maximum power is approximately seven times the inverted reset benchmark; the maximum-efficiency point reaches 0.9800.9800.980 but has ϕP=14.3\phi_P=14.3ϕP​=14.3. The inverted high-efficiency sector aligns with residual post-hot-stroke coherence. An average-level DBN–TPM comparison finds discrepancies in short-time coherent regimes and convergence at long driving times.
These are gross working-medium results: inversion-maintenance costs, implementation-specific reservoir physics, and tomography errors are excluded. The Markovian approximation may fail at short contacts. The efficiency-fluctuation variable is normalized work, −W/⟨Qh⟩-W/\langle Q_h\rangle−W/⟨Qh​⟩, not trajectory efficiency; its relative noise equals ϕP\phi_PϕP​. DBN is an ensemble reconstruction, not a backaction-free single-shot measurement, and no distribution-level DBN–TPM comparison is provided.
Population inversion and collective relaxation can both enhance the performance of a quantum heat engine, but through distinct mechanisms. We study a quantum Otto engine whose working medium is a symmetric collective spin of NNN two-level constituents. For commuting work strokes and collective reservoir coupling, the dynamics reduces exactly to a finite birth--death process on the Dicke ladder, allowing a unified treatment of stationary operation, work fluctuations, and finite-time relaxation. In the complete-reset limit, passive work per cycle saturates with system size, whereas population inversion yields work that grows linearly with NNN. The work reliability shows the same linear scaling, exceeding the square-root behavior of NNN independent engines. This enhancement originates from a macroscopic polarization displacement between hot and cold states, while collective coupling instead accelerates the finite-time dynamics through Dicke transition rates. For matched passive and inverted hot states, the extra gross work equals the Otto efficiency times the ergotropy of the inverted state. Charging the corresponding reversible excess state-formation cost removes this advantage, showing that the enhanced output converts a pre-existing active-state resource rather than generating a free thermodynamic gain. Exact finite-contact trajectory statistics further quantify how collective kinetics, fluctuations, correlations, and resource accounting remain linked away from complete reset.
Measurement-based quantum heat engines have attracted significant interest as alternatives to conventional thermal engines, as they replace the hot thermal reservoir with quantum measurements, thereby offering greater controllability and simpler implementation. Motivated by these advantages, we investigate a measurement-driven quantum Otto engine with a qubit working substance and study the optimal work extractable from such engines, including whether their performance can surpass that of conventional quantum Otto cycles. We analyze the engine in both the infinite-time (adiabatic) and finite-time (non-adiabatic) regimes, considering two distinct implementations obtained through optimization over all projection-valued measurements (PVMs) and over all two-outcome positive operator-valued measurements (POVMs). We show that measurement-based engines can outperform conventional quantum Otto engines within specific parameter regimes and that POVM-based engines can yield higher optimal work extraction than PVM-based ones. Furthermore, by incorporating the thermodynamic cost associated with resetting the auxiliary system required for POVM implementation, we demonstrate that the resulting net work output can still exceed that of PVM-based engines under suitable conditions on the spectral gaps and cold bath temperature. We also identify regimes in which non-adiabatic implementations can yield higher work output and efficiency than their adiabatic counterparts. Our study provides operational guidelines for designing improved measurement-driven quantum Otto engines.
Determining the work statistics of quantum engines is challenging due to measurement backaction. We here show that a dynamic Bayesian network-based measurement scheme, which preserves quantum coherence within an engine cycle, is minimally invasive, in the sense that the averaged measured state over one cycle exactly coincides with the unmeasured state. It therefore provides a general framework to investigate energy exchange statistics in quantum machines. This stands in contrast to the standard two-point measurement protocol, whose backaction can be so strong that it generally fails to reproduce the average work output of a coherent motor. It may even alter its mode of operation, causing it to cease functioning as an engine under observation. We further demonstrate that recently proposed universal fluctuation bounds do not necessarily apply to coherent machines.
With the development of any quantum technology comes a need for precise control of quantum systems. Here, we evaluate the impact of control noise on a quantum Otto cycle. While it is postulated that noiseless quantum engines can approach maximal Otto efficiency in finite times, the existence of white noise on the controls is shown to negatively affect average engine performance. Two methods of quantum enhancement, counterdiabatic driving and quantum lubrication, are implemented and found to improve the performance of the noisy cycle only in specified parameter regimes. To gain insight into performance fluctuations, projective energy measurements are used to construct a noise-averaged probability distribution without assuming full thermalization or adiabaticity. From this, the variances in thermodynamic currents are observed to increase as average power and efficiency improve, and are also shown to be consistent with known bounds from thermodynamic uncertainty relations. Lastly, by comparing the average functioning of the unmonitored engine to a projectively measured engine cycle, the role of coherence in work extraction for this quantum engine model is investigated.
We investigate a quantum Otto engine (QOE) constructed from the two-qubit quantum Rabi model, operating within a cavity quantum electrodynamics (QED) architecture. The engine operates with two qubits as the working substance and a single non-Markovian hot thermal bath, modeled via the hierarchical equations of motion (HEOM) formalism. In place of a conventional cold thermal reservoir, the cooling stroke is realized through a projective measurement protocol on the cavity mode, which acts as an ancillary subsystem and effectively mimics a cold bath for the qubit working medium via measurement back-action. A squeezing drive applied to the cavity mode serves as a quantum fuel. We demonstrate that cavity squeezing systematically enhances both the power output and operational efficiency of the engine - the work extracted per unit of heat drawn from the hot bath-driving it above the standard quantum Otto limit. In the limit-cycle regime, the efficiency, while remaining above the Otto bound throughout, asymptotically converges to it from above. This identifies squeezing as a controllable quantum resource for thermodynamic optimization. Our results reveal that the interplay between qubit-cavity coupling, measurement-induced cooling, and non-equilibrium squeezing gives rise to a multi-resource thermodynamic architecture with performance characteristics inaccessible to conventional two-bath quantum Otto engines, thereby providing a concrete route toward experimentally realizable quantum heat engines in cavity QED platforms.
Recently, measurement-based quantum thermal machines have drawn more attention in the field of quantum thermodynamics. However, the previous results on quantum Otto heat engines were either limited to special unital and nonunital channels in the bath stages, or a specific driving protocol at the work strokes and assuming the cycle being time-reversal symmetric, i.e., V^{†}=U (or V=U). In this paper, we consider a single spin-1/2 quantum Otto heat engine, by first replacing one of the heat baths by an arbitrary unital channel, and then we give the exact analytical expression of the characteristic function from which all the cumulants of heat and work emerge. We prove that under the effect of monitoring, ν_{2}>ν_{1} is a necessary condition for positive work, either for a symmetric or asymmetric-driven Otto cycle. Furthermore, going beyond the average we show that the ratio of the fluctuations of work and heat is lower and upper-bounded when the system is working as a heat engine. However, differently from the previous results in the literature, we consider the third and fourth cumulants as well. It is shown that the ratio of the third (fourth) cumulants of work and heat is not upper-bounded by unity nor lower-bounded by the third (fourth) power of the efficiency, as is the case for the ratio of fluctuations. Finally, we consider applying a specific unital map that plays the role of a heat bath in a coherently superposed manner, and we show the role of the initial coherence of the control qubit on efficiency, on the average work and its relative fluctuations.