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Relative-entropy decrease and convergence for a finite detailed-balance chain
A finite, time-homogeneous continuous-time rate model satisfying detailed balance; convergence is asserted only when its positive-rate graph is connected, and no general continuum or non-Markovian relaxation theorem is claimed.
Statement
Let have states, positive detailed-balance law , and connected undirected rate graph as in Finite detailed-balance rate and transition models. For every strictly positive initial probability vector , the master equation has a unique strictly positive probability solution for all . The relative entropy is nonincreasing, and for every state. No monotonicity of Shannon entropy is asserted.
Facts & Assumptions
Given: A finite state set of size , finite rates, a positive normalized detailed-balance vector , and an initially strictly positive normalized vector .
Finite detailed-balance rate and transition models: for , , and .
Finite detailed-balance rate and transition models: is positive on graph edges, and the graph is connected.
The natural logarithm has derivative 1/x and equals the integral from 1 to x of 1/t, The chain rule, in one line from Carathéodory: if is differentiable at and is differentiable at , then is differentiable at with , and Sums, scalar multiples, products and quotients: , , , and when : for , , and the ordinary chain and finite-product rules differentiate the entropy sum.
The exponential function is smooth and and The mean value theorem, as the case of Cauchy's: for continuous on with and differentiable on there is with : differentiate and infer monotonicity on an interval from a nonpositive derivative.
Cauchy-Schwarz with its equality case, the triangle inequality for , the parallelogram law and polarisation: the finite Cauchy--Schwarz inequality bounds a sum of at most edge increments by times their squared sum.
Proof
Given: [F1]--[F6] and .
Put and , where . Then has nonnegative entries and row sums one. The series and its differentiated series converge uniformly on bounded time intervals; its coefficients are nonnegative and sum to one, so it is a probability vector, starts at , and differentiates to . Its term gives . For uniqueness, the difference of two solutions satisfies ; with and , one has . Thus and force , hence .
With , detailed balance gives . By [F4], differentiating the finite entropy sum gives , since . Pairing the terms gives : if , then by [F3], and the reversed order gives the same product sign. The mean value theorem [F5] on each compact time interval makes nonincreasing.
Set , so , and . Since , differentiating and pairing the two orientations of each edge gives .
Let . Fix a root state and choose one simple path from it to each state; this is only a finite family of choices, obtainable successively, and each path has length at most . Telescoping and [F6] give . The zero-mean identity gives ; expanding yields . Since and , it follows that .
Thus with . By [F5], the derivative of is nonpositive and that function is nonincreasing, so . Since and , each .
Depends on
Finite detailed-balance rate and transition models
Order, continuity, range, and the product, quotient, and reciprocal laws for the natural logarithm
The natural logarithm has derivative 1/x and equals the integral from 1 to x of 1/t
The chain rule, in one line from Carathéodory: if is differentiable at and is differentiable at , then is differentiable at with
Sums, scalar multiples, products and quotients: , , , and when
The exponential function is smooth and
The mean value theorem, as the case of Cauchy's: for continuous on with and differentiable on there is with
Cauchy-Schwarz with its equality case, the triangle inequality for , the parallelogram law and polarisation