Abstract
The work required to drive a system from one state to another comprises both the equilibrium free energy difference and the dissipation associated with irreversibility. As physical processes—such as computing—approach fast limits, calculating this excess dissipation becomes increasingly critical. Yet, precisely quantifying dissipation, more specifically, entropy production, in strongly driven, time-dependent, realistic nanoscale systems remains a considerable challenge. Consequently, previous studies have largely been limited to either idealized Markovian systems under time-dependent driving or non-Markovian steady-state systems under constant driving. Here we measure the full dynamics of trajectory-level entropy production in a non-stationary, non-Markovian material arising from time-dependent driving. We use machine learning to extract the entropy produced by a quantum dot stochastically blinking under a stepwise control protocol. The entropy produced corresponds to the loss of memory in the material as the carrier distribution evolves. In addition, our approach quantifies both information insertion and dissipation under a quenched protocol. This work demonstrates a simple and effective approach for visualizing dissipation dynamics following a fast quench and serves as a stepping stone towards optimizing energy costs in the control of real materials and devices.
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Data availability
The data that support the findings of this study are available from the corresponding author upon request.
Code availability
The codes used in this work are available publicly at http://codeocean.com/signup/nature?token=0bf0606b4f9e4cd59b0ed7b9efcc731d.
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Acknowledgements
This work was supported primarily by the US Department of Energy, Office of Basic Energy Sciences, Division of Materials Sciences and Engineering (Contract No. DE-AC02-76SF00515). F.L. acknowledges support from the US Department of Energy, Office of Science, Basic Energy Sciences, CPIMS Program (Award No. DE-SC0026181). We thank P. H. Bucksbaum for generously providing access to his laboratory and the laser facilities used in this work. We are grateful to H. Qin and X. Peng for supplying the QD samples and to Z. Jiang (Karunadasa Group) for providing the PMMA for sample preparation. We also acknowledge valuable discussions with Y. Huang, Y. Jiang and Y. Du regarding the QD identification algorithm and machine learning approaches.
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Y.S., J.S. and A.M.L. conceived the project and initiated the experimental effort. C.C., Y.S. and G.M.R. developed the theoretical framework and constructed the model. Y.S. and H.M. performed the data acquisition. Y.S., A.P.S. and F.L. were responsible for sample preparation. C.H. optimized the laser system. Y.S. and C.C. led the writing of the paper. A.M.L. supervised the project.
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Extended data
Extended Data Fig. 1 The workflow of optimizing the parameters for the HMM.
Experimental data are split into train and test sets. Model parameters are optimized by minimizing the loss (top left) on the train data and validated by comparing losses on train and test sets. Bottom left: field-off parameters are optimized first and used for subsequent field-on optimization.
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Supplementary Notes 1–7, Figs. 1–12 and Table 1.
Supplementary Video 1 (download MP4 )
A viscous system under pulsed excitations.
Supplementary Video 2 (download AVI )
PL measurement of QD blinking under a periodically applied NIR field.
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Shen, Y., Chen, C., Ma, H. et al. Non-equilibrium entropy production and information dissipation in a non-Markovian quantum dot. Nat. Phys. 22, 374–381 (2026). https://doi.org/10.1038/s41567-026-03177-8
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DOI: https://doi.org/10.1038/s41567-026-03177-8


