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Jarzynski equality for a finite protocol with stationary kernels

Physical scope

An exact ensemble identity for a finite state space, finite protocol, canonical initial law, and kernels preserving each stage's canonical law; no claim is made for general stochastic processes or for any individual path.

Statement

For the forward path law of Finite driven protocol and path work, under Canonical initial preparation for a finite protocol and Finite bath kernels preserve the stage canonical law, the finite expectation satisfies EF[e−βW]=Zm/Z0=e−βΔF. This is an ensemble identity; it does not say W=ΔF on each path.

Facts & Assumptions

Given: A nonempty finite state space, finite energies Ek, β>0, a row-stochastic Kk, initial law π0, and πkKk=πk at each stage.

[F1]

Finite driven protocol and path work: the path law is π0(i0)∏kKk(ik−1,ik), and work at quench k is Ek(ik−1)−Ek−1(ik−1).

[A1]

Canonical initial preparation for a finite protocol: the initial law is π0(i)=e−βE0(i)/Z0.

[A2]

Finite bath kernels preserve the stage canonical law: ∑iπk(i)Kk(i,j)=πk(j).

[L1]

Canonical sampling assumption for finite and normalized statistical models: the current draft postulate adopts the finite microstate law Pβ(i)=e−βE(i)/Z(β) for finite nonempty Ω with 0<Z(β)<∞ and β=(kBT)−1. Only this finite branch is used; the countable and measurable branches are not invoked.

Proof

technique · induction on protocol stages

Given: [F1], [A1], [A2], [L1], with the finite partition sums and canonical laws of the protocol.

1.1F1A1L1givenbasealgebra

For k≥1 and j∈Ω, define Sk(j) by the finite sum over i0,…,ik−1∈Ω of π0(i0)∏ℓ=1kKℓ(iℓ−1,iℓ)e−βWk, with ik=j and Wk=∑ℓ=1k[Eℓ(iℓ−1)−Eℓ−1(iℓ−1)]; put S0(j)=π0(j). Partitioning this finite sum by the state i=ik−1 gives Sk(j)=∑iSk−1(i)e−β(Ek(i)−Ek−1(i))Kk(i,j). The canonical preparation gives the base S0(j)=π0(j)=(Z0/Z0)π0(j) by [A1] and the finite branch of [L1].

2.1ihstep 1.1F1

For the induction step fix k∈{1,…,m} and suppose Sk−1(i)=(Zk−1/Z0)πk−1(i) for every i.

3.1F1A2step 1.1step 2.1algebra

Substitute this hypothesis in the recurrence from step 1.1. Since πk−1(i)=e−βEk−1(i)/Zk−1, the previous-stage Boltzmann factor cancels against the quench factor, giving Sk(j)=(Zk/Z0)∑iπk(i)Kk(i,j)=(Zk/Z0)πk(j) by [A2]. This proves the induction step at each stage.

4.1F1step 1.1step 3.1algebradischarge-induction∎

The base and induction step establish Sk(j)=(Zk/Z0)πk(j) for all stages. At k=m, summing over terminal states and using normalization of πm gives EF[e−βW]=Zm/Z0. By ΔF=−β−1log⁡(Zm/Z0), this equals e−βΔF.

Depends on

Dependency tree · 2 levels

Sources