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A topological fluctuation theorem

Abstract:
Fluctuation theorems specify the non-zero probability to observe negative entropy production, contrary to a naive expectation from the second law of thermodynamics. For closed particle trajectories in a fluid, Stokes theorem can be used to give a geometric characterization of the entropy production. Building on this picture, we formulate a topological fluctuation theorem that depends only by the winding number around each vortex core and is insensitive to other aspects of the force. The probability is robust to local deformations of the particle trajectory, reminiscent of topologically protected modes in various classical and quantum systems. We demonstrate that entropy production is quantized in these strongly fluctuating systems, and it is controlled by a topological invariant. We demonstrate that the theorem holds even when the probability distributions are non-Gaussian functions of the generated heat.
Publication status:
Published
Peer review status:
Peer reviewed

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Publisher copy:
10.1038/s41467-022-30644-6

Authors

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Role:
Author
ORCID:
0000-0001-9915-0233
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Role:
Author
ORCID:
0000-0002-8274-8850
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Institution:
University of Oxford
Role:
Author
ORCID:
0000-0002-3149-4002


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Funder identifier:
10.13039/501100004189


Publisher:
Nature Research
Journal:
Nature Communications More from this journal
Volume:
13
Issue:
1
Pages:
3036-3036
Article number:
3036
Publication date:
2022-05-31
DOI:
EISSN:
2041-1723
ISSN:
2041-1723


Language:
English
Keywords:
Pubs id:
1261992
Local pid:
pubs:1261992
Source identifiers:
W3196248348
Deposit date:
2026-04-24
ARK identifier:
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