Plain-English statement
Log-Sobolev coercivity turns entropy dissipation into exponential KL decay.
Mathematical statement
If KL'(t)=-FI(t) and KL(t)≤(C/2)FI(t), then KL(t)≤KL(0)exp(-2t/C).
Intuition
LSI lower-bounds the available Fisher dissipation by a multiple of the current KL divergence, so entropy cannot decay slower than the corresponding exponential curve.
Conditions
- C is positive
- the entropy curve has derivative minus Fisher information
- the LSI bound holds along the curve
Why these conditions cannot be dropped
- density regularity and entropy differentiation are genuine analytic obligations
- the factor C/2 determines the rate 2/C
Proof route
- multiply KL≤(C/2)FI by 2/C
- obtain (2/C)KL≤FI
- invoke the generic scaled-dissipation decay theorem
Lean interface notes
- the existing KL/FI scalar bookkeeping can later instantiate this curve
- the converse LSI criterion remains a separate theorem
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Lean statement
theorem chewi_theorem_1_2_26_forward
{C : ℝ} (hC : 0 < C) (curve : DissipationCurve 1)
(hLSI : ∀ s : ℝ,
curve.energy s ≤ (C / 2) * curve.dissipation s)
{t : ℝ} (ht : 0 ≤ t) :
curve.energy t ≤
curve.energy 0 * Real.exp (-(2 / C) * t) := by
simpa [sub_zero] using
chewi_theorem_1_2_26_forward_from hC curve hLSI ht
/-- Backward scalar direction of Chewi, Theorem 1.2.26. -/
Open AutoSamplingTheory/TechnicalLemmas/FunctionalInequalities/SemigroupDecay.lean:327published source at 7bcd37294df1