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ExampleConstruction: AI-generatedVerification: AI-generatedPipeline-generatedverified 2026-10-15 (gpt-6-luna, gpt-6.1-sol, and delegated Codex review/repair agents; see completed run evidence)
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  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
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Reset bound for a biased two-state memory

Physical scope

A symbolic finite-memory calculation under the reset theorem's physical assumptions; it is not a measured reset process.

Example

Let the retained-register set be the singleton R={r0} and let the memory be a bit with probability p∈(0,1) of state 1. The register carries no information.

Facts & Assumptions

Given: A finite memory law and the endpoint assumptions of Conditional work bound for finite memory reset.

[F1]

Finite memory and retained-register reset model: ar=∑mp(m,r), q(m∣r)=p(m,r)/ar for ar>0, and H(M∣R)=∑r:ar>0ar[−∑m:q(m∣r)>0q(m∣r)log⁡q(m∣r)], with natural logarithms and entropy in nats.

[F2]

Conditional work bound for finite memory reset: W≥kBTbH(M∣R) under its stated endpoint entropy, fixed-temperature bath, unchanged endpoint energy, and total entropy nondecrease assumptions.

Verification

Given: p∈(0,1) and Tb>0.

1.1givenF1algebra

Since R={r0}, its marginal is ar0=1, and the conditional law is q(1∣r0)=p, q(0∣r0)=1−p. The entropy definition therefore gives H(M∣R)=H(M)=−plog⁡p−(1−p)log⁡(1−p).

2.1F2step 1.1algebra∎

Therefore the theorem gives W≥kBTb[−plog⁡p−(1−p)log⁡(1−p)] for this preparation. It reports no work measurement and makes no claim about an apparatus.

Depends on

Dependency tree · 2 levels

Sources