ConclusionSeam3 #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
Seam 3: the h_hat_sep decomposition at the b_L seam #
The per-cube Γ₁ pricing of the seam's layer object is available at a
deterministic shell pair only, and supplying the deterministic index is what
seam 3 means. Provider/Multiscale/ConclusionSeam2.lean records the same
gap: ℓ and the shell index ℓ − h_hat_sep are sample-dependent, while a
weak-Orlicz statement needs a deterministic index.
This module fixes the carrier that seam 3 is stated at: the seam's layer object
read at a deterministic index. The decomposition that would close the gap ---
split the sample space over the countably many values of h_hat_sep, apply the
deterministic-index estimate on each piece, and pay for the pieces above a
cut-off H with the proved tail of h_hat_sep --- is described below, so that the
carrier can be read against it; it is not performed here.
The shape of the answer #
There is no free lunch: the diagonal observable ω ↦ X_{h_hat_sep(ω)}(ω) is NOT
Γ_σ at the common scale of the family X_h, and nothing below claims it is.
What is true is the finite-cut-off tail bound
P[ X_{h_hat_sep(ω)}(ω) > A t ] ≤ (H+1) e^{-t^σ} + P[ h_hat_sep > H ] ,
for every H, every t ≥ 1 and every common scale A dominating the H+1
individual scales. At an abstract family and an abstract ℕ-valued index this
is a pure measure-theoretic decomposition (the events {h_hat_sep = h} for h ≤ H
together with {h_hat_sep > H} cover, and the diagonal event meets the h-th
piece inside the h-th tail event); it needs NO measurability of the index and
NO independence, only monotonicity, countable subadditivity on a finite union
and finiteness of the measure.
Two remarks on why this is the honest shape.
- The naive
∑_h P[X_h > At]over allhdiverges: each term is bounded bye^{-t^σ}uniformly inh, so the sum over the infinitely many values ofh_hat_sepis useless. The cut-offHis what makes the decomposition summable, and the price is the second term. - The second term is not an assumption: it is the proved
Percolation.measureReal_scaleSeparationFail_le_of_gates(e.hsep.tails) read throughPercolation.scaleSeparationFail_eq, givingP[h_hat_sep > H] ≤ C(σ,b) exp(−3^{(1−σ)bH})forH ≥ 1(RandomHsepAllLWaveEnvelope.measureReal_lt_hsep_le_of_gates). So the composed bound has NO undischarged probabilistic input.
The instantiation at the seam #
seamLayerObject M m h k ℓ h' L is the seam's own left-hand quantity
γ 3^{−2γℓ} ( ∑_{□ ∈ 𝒲(□_m,k)} (|□|/|□_m|) ⨍_□ |k_L − k_{ℓ−h'}|⁴ )^{1/2}
at the deterministic index h'. It is exactly the quantity the per-cube Γ₁
pricing is stated at, with n1 = ℓ − h' and n2 = L, and its scale keeps the
layer's own mass fraction 6d·3^{−k}; reading it at the DIAGONAL index
h' = h_hat_sep(ω) is what the decomposition above has to be applied to.
The composition itself is not carried out here. Its one interface datum is
hA, a common scale dominating the H+1 individual scales; that is a datum
and not a theorem because streamIncrementLpMassScale M 4 (ℓ−h) L varies with
h and this repository has no monotonicity statement for it (see "What is not
proved").
The 3^{γ h_hat_sep} re-pricing #
The other half of the seam is the pointwise split, for every nonnegative Y,
3^{γ h_hat_sep} Y ≤ 2 Y + Z Y , Z = 3^{γ h_hat_sep} 1_{γ h_hat_sep > 3^{−4}} ,
with Z carried at Γ_{(1−σ)σ₂/((1−σ)+σ₂)} and at the explicit
exp(−cγ^{−1})-sized scale of HsepReduction, which is where that half is
proved. It is the HsepReduction display multiplied by a nonnegative factor,
at the honest product index; neither Γ₄ nor Γ₂ is claimed anywhere, and no
new Orlicz input is used.
What is not proved #
hAis not discharged. A common scale forh ≤ Hrequires monotonicity (or an explicit envelope) ofh ↦ streamIncrementLpMassScale M 4 (ℓ−h) L, which is not proved. This is the precise missing input, named here rather than smuggled: it is a property ofe.kmn.bounds' envelope, not of the seam.- No
Γ_σstatement for the diagonal observable. The decomposition above yields a tail bound at a fixedt, not anIsBigOWith; converting it into one needsH = H(t). The optimization is not made in THIS file. - No
k-decay and no printed per-layer weight: blocks3^{−3k/4}independently, and nothing here approaches it. The6d·3^{−k}inside the scale is the proved Whitney layer mass fractionLayerMass.sum_cubeMassRatio_whitneyLayer_le, unchanged. - The first printed inequality of the display (per-simplex to per-cube)
remains unlanded, exactly as
ConclusionSeam2records.
Main definitions #
References #
- ABK26,
p.bfA.multiscaleboundStep 3, (the3^{γh_hat_sep}reduction) and theb_Lbranch;e.hsep.tails;p.minimal.scale.separation. Provider/Multiscale/ConclusionSeam2.lean(the layer fit and theΓ₁pricing),Provider/Multiscale/HsepReduction.lean(the Orlicz half),Provider/Percolation/MinimalScaleSeparation.lean(theh_hat_septail).
The abstract decomposition over the values of a random index #
The tail of the truncation depth #
The seam's layer object at a deterministic index #
The seam's layer object at a D shell index (ABK26, in the corrected
volume-weighted reading): γ 3^{−2γℓ} (∑_{□ ∈ 𝒲(□_m,k)} (|□|/|□_m|) ⨍_□ |k_L − k_{ℓ−h}|⁴)^{1/2}.
Equations
- One or more equations did not get rendered due to their size.