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Detailed balance is a strong form of equilibrium for Markov processes? and dynamical systems, stronger than stationarity and independent from ergodicity.
It can be roughly interpreted as a situation where for every two regions (of the state space, etc.) and , the amount of mass (or probability, etc.) flowing from to equals the amount of mass flowing from to .
A finite-state stationary Markov chain on with stationary measure and transition matrix? is said to satisfy detailed balance if and only if
Equivalently, if for each , the probability of the following two-state trajectories are equal:
Note that this is strictly stronger than stationarity. For example, consider a cyclic permutation on the set given by , etc. This admits the uniform measure as stationary measure (call it ), however we have that
and
Indeed, the “mass” flows in the direction , but not (at least, not in a single step). Still, the system is stationary: the amount of mass that leaves (and goes to ) is equal to the amount of mass that enters . It just does not come from .
More generally, given a measure-preserving Markov kernel , we say that the resulting process satisfies detailed balance if and only if for all measurable subsets and of ,
In other words, is its own Bayesian inverse.
The same definition can be given for a class (“semigroup”) of measure-preserving Markov kernels indexed by an arbitrary monoid.
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Wikipedia, Ergodic process
Noé Ensarguet, Paolo Perrone, Categorical probability spaces, ergodic decompositions, and transitions to equilibrium, arXiv:2310.04267
Last revised on January 31, 2025 at 18:41:16. See the history of this page for a list of all contributions to it.