2022
DOI: 10.1103/physrevx.12.031025
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Thermodynamic Inference in Partially Accessible Markov Networks: A Unifying Perspective from Transition-Based Waiting Time Distributions

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Cited by 43 publications
(48 citation statements)
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“…If a network has internal cycles, the densities could exhibit multimodal behaviour. 75 For a second-order semi-Markov process, the waiting time distributions are direction-time dependent. Thus, the mean dwell-times that the system spends at a particular state for the forward and the reverse transitions are not necessarily identical, and a deviation of their ratio from one provides information regarding the irreversible nature of the process.…”
Section: Coarse-graining Lower Bound On the Total Entropy Production ...mentioning
confidence: 99%
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“…If a network has internal cycles, the densities could exhibit multimodal behaviour. 75 For a second-order semi-Markov process, the waiting time distributions are direction-time dependent. Thus, the mean dwell-times that the system spends at a particular state for the forward and the reverse transitions are not necessarily identical, and a deviation of their ratio from one provides information regarding the irreversible nature of the process.…”
Section: Coarse-graining Lower Bound On the Total Entropy Production ...mentioning
confidence: 99%
“…An estimator based on the KLD between waiting time distributions of the time forward and the time backward transitions between discrete states was shown to provide a lower bound on the total EPR, 64 given that the time-reversal operator does not lead to kinetic hysteresis. [72][73][74][75] Applied to a second-order semi-Markov process, this KLD estimator of the EPR breaks into two contributions, 64 the affinity EPR, EPR aff , which accounts for the net flux and affinity or the thermodynamic force, 68,70 and the waiting-time-distribution (WTD) EPR, EPR WTD , which accounts for the broken time-reversal symmetry in the waiting time distributions. 64 For second-order semi-Markov processes, which naturally emerge when ''lumping'' adjacent states, 64,76 the EPR WTD can provide a lower bound on the total EPR, even when the system does not have any net current observed and EPR aff = 0.…”
Section: Introductionmentioning
confidence: 99%
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“…Furthermore, as proven in Ref. [87], when the hidden network either has no cycles or satisfies detailed balance, σ t vanishes and σ L = σ The current is defined as the number of times the system jumps from a given state to another one, without going through any other states in between, minus the number of opposite jumps.…”
Section: Visible Irreversibilitymentioning
confidence: 98%