Observational entropy with general quantum priors
1Centre for Quantum Technologies, National University of Singapore, 3 Science Drive 2, Singapore 117543
2Center for Theoretical Physics of Complex Systems, Institute for Basic Science (IBS), Daejeon 34126, Korea
3Basic Science Program, Korea University of Science and Technology (UST), Daejeon - 34113, Korea
4Física Teòrica: Informació i Fenòmens Quàntics, Departament de Física, Universitat Autònoma de Barcelona, 08193 Bellaterra, Spain
5Department of Mathematical Informatics, Nagoya University, Furo-cho Chikusa-ku, Nagoya 464-8601, Japan
6Department of Physics, National University of Singapore, 2 Science Drive 3, Singapore 117542
| Published: | 2024-11-14, volume 8, page 1524 |
| Eprint: | arXiv:2308.08763v3 |
| Doi: | https://doi.org/10.22331/q-2024-11-14-1524 |
| Citation: | Quantum 8, 1524 (2024). |
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Abstract
Observational entropy captures both the intrinsic uncertainty of a thermodynamic state and the lack of knowledge due to coarse-graining. We demonstrate two interpretations of observational entropy, one as the statistical deficiency resulting from a measurement, the other as the difficulty of inferring the input state from the measurement statistics by quantum Bayesian retrodiction. These interpretations show that the observational entropy implicitly includes a uniform reference prior. Since the uniform prior cannot be used when the system is infinite-dimensional or otherwise energy-constrained, we propose generalizations by replacing the uniform prior with arbitrary quantum states that may not even commute with the state of the system. We propose three candidates for this generalization, discuss their properties, and show that one of them gives a unified expression that relates both interpretations.

Featured image: A quantum system, like a cat, has intrinsic uncertainties. Observational entropy characterizes both the intrinsic uncertainty of the system and additional uncertianty introduced by the lens we use to observe it.
Popular summary
Typically, the definition of OE assumes a "uniform prior," i.e., it starts with an assumption of maximum uncertainty about the state of the system. However, this assumption is not always tenable, especially in more complex systems, such as those influenced by energy constraints or infinite dimensional systems, where instead other priors, such as the Gibbs distribution, would be preferable, both physically and mathematically.
To fill this gap and extend OE to arbitrary priors, we first show how OE can be interpreted in two ways: as a measure of how much a measurement scrambles the true state of a system (statistical deficiency), and as the difficulty of inferring the original state from the measurement results (irretrodictability). These two aspects provide complementary insights into how much we lose or gain in our knowledge of the original state of a system when we make observations on it.
This conceptual insight leads us to introduce three generalized versions of OE: two that capture either statistical deficiency or irretrodictability, but are inherently incompatible; and a third, based on Belavkin-Staszewski relative entropy, that instead is able to combine both perspectives and provide a unified view of commuting and non-commuting priors alike. We expect that our results will pave the way for a consistent treatment of the second law of thermodynamics and fluctuation relations in fully quantum scenarios.
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[2] Teruaki Nagasawa, Eyuri Wakakuwa, Kohtaro Kato, and Francesco Buscemi, "Macroscopicity and observational deficit in states, operations, and correlations* ", Reports on Progress in Physics 88 11, 117601 (2025).
[3] Shintaro Minagawa, M. Hamed Mohammady, Kenta Sakai, Kohtaro Kato, and Francesco Buscemi, "Universal validity of the second law of information thermodynamics", npj Quantum Information 11 1, 18 (2025).
[4] Teruaki Nagasawa, Kohtaro Kato, Eyuri Wakakuwa, and Francesco Buscemi, "Generic increase of observational entropy in isolated systems", Physical Review Research 6 4, 043327 (2024).
[5] Ge Bai, Francesco Buscemi, and Valerio Scarani, "Quantum Bayes’ Rule and Petz Transpose Map from the Minimum Change Principle", Physical Review Letters 135 9, 090203 (2025).
[6] Joseph Schindler, Philipp Strasberg, Niklas Galke, Andreas Winter, and Michael G. Jabbour, "Unification of observational entropy with maximum entropy principles", arXiv:2503.15612, (2025).
[7] Leonardo Rossetti, Stefano Mancini, Andreas Winter, and Joseph Schindler, "Observational entropy of quantum correlations and entanglement", arXiv:2510.10058, (2025).
[8] Clive Cenxin Aw, "Classical and quantum reverse processes through Bayesian inference", International Journal of Quantum Information 24 2, 2530004-650 (2026).
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