Step1Assembly #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
The two interchanges and the centre closure of Step 1 #
ABK26, Section 4.1, e.mathcalE.annular.decomp.pre, Step 1.
Step1.annularDecompPre_of reduces the Step-1 shape to three caller
obligations: hgrid (the cover split), hcov (the cover interchange) and
hcen (the resummed centre term). This module proves the last two
abstractly, in the weight the manuscript uses, so that the concrete
producer only has to supply the geometry.
What is proved #
tsum_annFam_row-- then-row of the guarded annular family is a finite sum overj ∈ [n+1, m]. This is the manuscript's interchangeΣ_{n ≤ m} Σ_{j=n+1}^m = Σ_{j ≤ m} Σ_{n ≤ j-1}, and it is an identity, so the cover leg costsC_cov = 1with no loss.annDouble_eq_tsum_rows,summable_annFam_rows-- the transposed iterated form of the annular double sum, and the summability of its rows.tsum_centre_le-- the centre closure. Given only the one-step subadditivity recursionJcen n ≤ A n + ρ^{-1} Jcen (n-1)and a uniform bound on both families, the weighted centre sum is at most3times the diagonal slice of the annular double sum.C_cen = 3is an absolute numeral on the printed windows ≤ 1/4,ρ ≥ 9.
The centre closure, and why it does not iterate #
The manuscript iterates the one-step recursion into an infinite series and then
computes Σ_{n=k+1}^m 3^{-2s(m-n) - d(n-1-k)} ≤^{-2s(m-k)}. The same constant
is obtained here without any iteration: the weighted centre sum S is (the
uniform bound plus the geometric weight), the weight satisfies w(n) = 3^{2s} w(n-1) exactly, and the ℤ-shift is a tsum bijection, so summing the
one-step recursion gives
S ≤ T + 3^{2s} ρ^{-1} S ,
with T the weighted diagonal sum. On s ≤ 1/4 and ρ ≥ 9 the contraction
factor is at most 7/36, whence S ≤ (36/29) T, and T = 3^{2s} times the
diagonal slice in the spelling Step1.annularDecompPre_of expects. Since
(36/29)·(7/4) = 63/29 < 3, C_cen = 3 closes it. This is exactly the geometric
factor 3^{2s}(1 - 3^{2s-d})^{-1} of the centre interchange, evaluated with
slack on the printed window; the honest convergence condition 2s < d is what
s ≤ 1/4 < 1 ≤ d/2 supplies.
The tolerance #
The printed W(p) = 3^{-dp} at C₀ = 1 -- which is what the one-step
recursion at ρ = 3^d produces -- sits far inside that condition; the numerals
7/4, 1/9, 7/36, 36/29, 3 above are the explicit margin.
References #
- ABK26, (Step 1); (the cover interchange); (the centre resummation).
Part A -- the lower-half reindexing n = m − u #
The guarded geometric criterion. A nonnegative family that is uniformly
bounded on {n ≤ m} is summable against the Step-1 weight 3^{−2s(m−n)}.
Part B -- the cover interchange #
The n-row of the guarded annular family. For n ≤ m the row is the
finite sum over the annulus indices j ∈ [n+1, m]; for n > m it vanishes.
The manuscript's interchange of the order of summation is exactly this identity
together with annDouble_eq_tsum_rows.
Part C -- the two numerals of the centre closure #
Part D -- the centre closure #
The Step-1 centre closure, at the absolute constant 3.
Jcen is the centre leg J(□_n) and A n the annulus maximum at step n
(the manuscript's max_{z' ∈ 3^{n-1}ℤ^d ∩ (□_n ∖ □_{n-1})} J(z' + □_{n-1})). The
only structural input is the one-step subadditivity recursion hstep; the uniform
bounds make the weighted sums finite, which is what lets the recursion be summed
instead of iterated.
The conclusion is exactly the hcen slot of Step1.annularDecompPre_of at
Ccen = 3, once A is instantiated at fun n ↦ Jann n (n-1).