nLab detailed balance

Contents

Context

Physics

physics, mathematical physics, philosophy of physics

Surveys, textbooks and lecture notes


theory (physics), model (physics)

experiment, measurement, computable physics

Measure and probability theory

Contents

Idea

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.) AA and BB, the amount of mass (or probability, etc.) flowing from AA to BB equals the amount of mass flowing from BB to AA.

Definition

For discrete Markov chains

A finite-state stationary Markov chain on XX with stationary measure pp and transition matrix? kk is said to satisfy detailed balance if and only if

p(x)k(y|x)=p(y)k(x|y). p(x)\,k(y|x) \;=\; p(y)\,k(x|y) .

Equivalently, if for each x,yXx,y\in X, the probability of the following two-state trajectories are equal:

P(x,y)=P(y,x). P(x,y) \;=\; P(y,x) .

Note that this is strictly stronger than stationarity. For example, consider a cyclic permutation kk on the set {a,b,c,d}\{a,b,c,d\} given by ab,bca\mapsto b, b\mapsto c, etc. This admits the uniform measure as stationary measure (call it pp), however we have that

p(a)k(b|a)=141=14 p(a)\cdot k(b|a) \;=\; \frac{1}{4} \cdot 1 \;=\; \frac{1}{4}

and

p(b)k(a|b)=140=0. p(b)\cdot k(a|b) \;=\; \frac{1}{4} \cdot 0 \;=\; 0 .

Indeed, the “mass” flows in the direction aba\to b, but not bab\to a (at least, not in a single step). Still, the system is stationary: the amount of mass that leaves aa (and goes to bb) is equal to the amount of mass that enters aa. It just does not come from bb.

General case

More generally, given a measure-preserving Markov kernel k:(X,p)(X,p)k:(X,p)\to(X,p), we say that the resulting process satisfies detailed balance if and only if for all measurable subsets AA and BB of XX,

Ak(B|x)p(dx)= Bk(A|x)p(dx). \int_A k(B|x)\,p(d x) \;=\; \int_B k(A|x)\,p(d x) .

In other words, kk 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.

Properties

  • A Markov process satisfies detailed balance if and only if it is time-reversible.

Examples

  • Every idempotent Markov chain? satisfies detailed balance.

(…)

References

category: probability

Last revised on January 31, 2025 at 18:41:16. See the history of this page for a list of all contributions to it.