InformationTheory.Shannon.EPI.Stam.SupplyTwoTime
InformationTheory.Shannon.EPIStamSupplyTwoTime.density_int_mass
sourceDensity facts from a withDensity law (probability-density normalization):
if P.map W = volume.withDensity (ofReal ∘ p) with P a probability measure and p ≥ 0
measurable, then p is volume-integrable with mass 1.
@audit:ok
Used by
InformationTheory.Shannon.EPIStamSupplyTwoTime.indepSum_density_ae
sourceThe independent-sum input identity, the seam of the argument: for X ⊥ Y with Lebesgue
densities pX, pY and X+Y with Lebesgue density pXY (all from probability-measure
withDensity laws), the sum density equals the convolution of the addend densities a.e.:
pXY =ᵐ[volume] convDensityAdd pX pY.
Both pXY and convDensityAdd pX pY are densities of
P.map (X+Y) = (P.map X) ∗ (P.map Y) (independence), and withDensity densities are
a.e.-unique. This is an a.e. identity at the un-smoothed input level; the consumed
density_t is pinned pointwise to the smooth convolution.
@audit:ok
Used by
InformationTheory.Shannon.EPIStamSupplyTwoTime.convDensityAdd_gaussian_asym_convDensityAdd_pos
sourceUsed by
InformationTheory.Shannon.EPIStamSupplyTwoTime.convDensityAdd_gaussian_asym_integrable_deriv_mul
sourceUsed by
InformationTheory.Shannon.EPIStamSupplyTwoTime.convDensityAdd_gaussian_asym_integrable_mul_deriv
sourceUsed by
InformationTheory.Shannon.EPIStamSupplyTwoTime.convDensityAdd_gaussian_asym_condDensityX_integrable
sourceUsed by
InformationTheory.Shannon.EPIStamSupplyTwoTime.convDensityAdd_gaussian_asym_integrable_scoreWeight_mul_condDensityX
sourceUsed by
InformationTheory.Shannon.EPIStamSupplyTwoTime.convDensityAdd_gaussian_asym_integrable_scoreWeight_sq_mul_condDensityX
sourceUsed by
InformationTheory.Shannon.EPIStamSupplyTwoTime.convDensityAdd_gaussian_asym_integrable_inner_scoreWeight_sq
sourceUsed by
InformationTheory.Shannon.EPIStamSupplyTwoTime.convDensityAdd_gaussian_asym_fisher_integrand_integrable
sourceUsed by
InformationTheory.Shannon.EPIStamSupplyTwoTime.convDensityAdd_gaussian_asym_integrable_prod_logDeriv_sq_mul
sourceUsed by
InformationTheory.Shannon.EPIStamSupplyTwoTime.convDensityAdd_gaussian_asym_integrable_prod_logDeriv_sq_shift_mul
sourceUsed by
InformationTheory.Shannon.EPIStamSupplyTwoTime.convDensityAdd_gaussian_asym_integrable_prod_deriv_mul
sourceUsed by
InformationTheory.Shannon.EPIStamSupplyTwoTime.isBlachmanConvReady_convDensityAdd_gaussian_asym
sourceThe asymmetric IsBlachmanConvReady producer (independent times σ ≠ τ):
IsBlachmanConvReady (convDensityAdd pX g_σ) (convDensityAdd pY g_τ). Faithful
generalization of EPIBlachmanGeneralDensity.isBlachmanConvReady_convDensityAdd_gaussian
(which hardcodes the same t for both arms) — every field's construction uses only the
public per-arm conv-Gaussian lemmas (convDensityAdd_gaussian_integrable / _bdd /
_deriv_bdd / convDensityAdd_fisher_integrand_integrable / convDensityAdd_pos_of_pos_cont
/ isRegularDensityV2_convDensityAdd_gaussian), each at its own arm's time, so the same-t
restriction was incidental. The only structural change is int_fisherZ: the conv-of-conv
conv(pX∗g_σ)(pY∗g_τ) is identified with conv(pX∗pY) g_{σ+τ} via the asymmetric
interchange bridge convDensityAdd_convGaussian_interchange_asym (variance σ+τ, not 2t).
All hypotheses are regularity preconditions; the conclusion (19-field integrability / boundedness / positivity bundle) is derived from them. @audit:ok
Used by
InformationTheory.Shannon.EPIStamSupplyTwoTime.twoTime_stam_supply
sourceThe two-time harmonic-Stam supply producer.
For X Y Z_X Z_Y Z : Ω → ℝ (all unit noises, sum perturbed by separate Z), independent
appropriately, with Lebesgue densities and finite second moments, and de Bruijn regularity
h_reg_X/h_reg_Y/h_reg_sum, the h_stam_supply clause of
entropyPower_add_ge_case1_of_regular_twotime holds: at every matched pair σ, τ > 0,
the three smoothed Fisher informations are positive and 1/J_S ≥ 1/J_X + 1/J_Y with
J_S the single-noise sum heat flow at σ + τ.
The conv-pin seam indepSum_density_ae
(pXY =ᵐ convDensityAdd pX pY) is proved via
IndepFun.map_add_eq_map_conv_map + conv_withDensity_eq_lconvolution
withDensitya.e.-uniqueness + the lconvolution-Bochner a.e. bridge (Tonelli finiteness + a.e.-zofReal_integral_eq_lintegral_ofReal).
@audit:ok. The honesty of the signature rests on:
(1) Core genuinely produced, not assumed: the inverse-Stam 1/J_S ≥ 1/J_X+1/J_Y is
CONSTRUCTED by isStamInequalityHyp_of_indepFun P A B (a regularity-only construction via
stamCauchySchwarzOptimal_of_indepFun, @audit:ok) then APPLIED at
density_t. The three IsDeBruijnRegularityHyp inputs are consumed only as regularity
(.pX/.pX_law/.pX_nn/.pX_meas density witnesses + .density_t_eq pointwise pins),
never as a bundled inequality core. No := h circularity, no :True, no degenerate
exploitation, no *Hypothesis-core bundling, no name laundering.
(2) a.e.→pointwise wash: the object IsStamInequalityHyp consumes is the
POINTWISE-pinned smooth density_t (density_t_eq pins to the explicit smooth
convDensityAdd pX g_t, not an a.e. rnDeriv class); the a.e. seam sits only at the
un-smoothed input (pXY =ᵐ convDensityAdd pX pY) and is washed through convDensityAdd · g
by integral_congr_ae. A skeptic cannot pick a bad pointwise representative.
(3) indepSum_density_ae sound + non-vacuous (see its tag).
(4) isBlachmanConvReady_convDensityAdd_gaussian_asym = pure 19-field regularity (see its tag).
(5) Unused hyps (hZ/hXZX/hYZY/hZX_law/hZY_law/hZ_law/hX_ac/hY_ac/hmomX/hmomY)
are OVER-hypothesized-harmless: kept to match the uniform shape EPIDensityForm passes to
entropyPower_add_ge_case1_of_regular_twotime; the de Bruijn regularity hyps already carry
the needed density data (no gap masked, proof closes without them = NOT under-hypothesized).
hpair_indep is a genuine necessary precondition (pairwise indep insufficient for
A=X+√σ·Z_X ⊥ B=Y+√τ·Z_Y; derived via .comp). sorryAx-free.