InformationTheory.Shannon.EPI.Case1.TwoTime.Core
EPI case-1 two-time object — Core (§0) #
Matched-time path abbreviations shared across the two-time object split
(TwoTime/Paths.lean = §1 path existence, TwoTime/GapDerivative.lean +
TwoTime/MonotonicityAndSaturation.lean + TwoTime/EntropyPowerInequality.lean = §2–§4).
Verbatim split of EPI/Case1/TwoTime.lean §0; proofs unchanged. Umbrella:
EPI/Case1/TwoTime.lean.
§0 — Matched-time path abbreviations #
The single-source heat-flow entropy power N_A(s) = entropyPower (P.map (A + √s·B)).
The matched path s(t) is the inverse of N_A solving N_A(s(t)) = N_A(0)·eᵗ.
InformationTheory.Shannon.EPICase1TwoTime.heatFlowEP
sourceSingle-source heat-flow entropy power along the perturbation A + √s·B.
N_A(0) = entropyPower (P.map A).
Equations
- InformationTheory.Shannon.EPICase1TwoTime.heatFlowEP A B P s = InformationTheory.Shannon.EntropyPowerInequality.entropyPower (MeasureTheory.Measure.map (fun (ω : Ω) => A ω + √s * B ω) P)
Instances For
Used by
InformationTheory.Shannon.EPICase1TwoTime.IsMatchedTimePath
sourceMatched-time path predicate (output of the inverse-function construction).
For a path s : ℝ → ℝ along the A-perturbation, this records that:
sstarts at0(s 0 = 0);- the entropy power grows as
eᵗ:N_A(s(t)) = N_A(0)·eᵗfort ≥ 0(the matched-timee^tcharacterization, proof-log §formulation gate); sis continuous on[0, ∞);- on the interior
t > 0,shas derivative1/J_A(s(t))(FII-matched velocity), whereJ_Ais the Fisher info of the perturbed density.
This is not a load-bearing hypothesis on the EPI conclusion: it is the
genuine output of matchedTimePath_exists (inverse-function subproject), whose
inputs are only regularity preconditions (J_A > 0, measurability, indep).
The path starts at time
0.Matched
e^tgrowth of the single-source entropy power.The path is continuous on
[0, ∞).FII-matched velocity on the interior.