Retained bins as a band family #
Lowest retained bin index: the bin containing L.
Equations
- CommutingRepetition.binLo r θ L = CommutingRepetition.binIdx r θ L
Instances For
Highest retained bin index: the bin containing H.
Equations
- CommutingRepetition.binHi r θ H = CommutingRepetition.binIdx r θ H
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Number of retained bins (those meeting the window [L, H]).
Equations
- CommutingRepetition.binCount r θ L H = (CommutingRepetition.binHi r θ H - CommutingRepetition.binLo r θ L + 1).toNat
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The k-th retained bin I_j^θ ∩ [L, H], j = binLo + k
(06_otqcs.tex, eq N1-Z "the finite retained bin set").
Equations
- CommutingRepetition.retainedBin r θ L H k = CommutingRepetition.binIdx r θ ⁻¹' {CommutingRepetition.binLo r θ L + ↑↑k} ∩ Set.Icc L H
Instances For
Its band value: the upper endpoint t_j^θ = r^(j+1+θ) (eq shifted-bins).
Equations
- CommutingRepetition.retainedVal r θ L H k = r ^ (↑(CommutingRepetition.binLo r θ L + ↑↑k) + 1 + θ)
Instances For
The retained index of a point of the window.
Equations
- CommutingRepetition.retainedIdx hr hL ha = ⟨(CommutingRepetition.binIdx r θ a - CommutingRepetition.binLo r θ L).toNat, ⋯⟩
Instances For
The retained rounded square regroups over the retained bins:
roundSq a = ∑_k t_k² 1_{B_k}(a) (eq abcGamma, finite retained-bin form).
The same-bin joint rounded square regroups over the retained bins:
jointRoundSq a b = ∑_k t_k² 1_{B_k × B_k}(a, b).
The retained bins form a band family.
Each retained bin sits inside [t_k / r, t_k] (the shifted-bin geometry,
as consumed by selSharp_round).
The retained bins cover exactly the window [L, H].
The grid functionals as band sums #
Band-mass inequalities (eq c-min and a + b − c ≤ Z) #
Per bin: μ_A(B) + μ_B(B) − ν(B×B) = ν((B×ℝ) ∪ (ℝ×B)) ≤ 1.
a_s + b_t − c_{st} ≤ Z (the per-trial progress is a probability).
Second-moment facts for the spectral distributions #
The retained-window second moment of a spectral distribution supported on
[0, ∞) with unit second moment and high tail at most ρ is at least
1 − ρ − L² (06_otqcs.tex, eq rounding-tails: the omitted region is the low
window [0, L) of mass at most L² and the high tail).
One finite cutoff H > L makes every high squared tail of a finite family of
probability measures with finite second moment at most ρ (06_otqcs.tex, "for each
ρ > 0 one finite H makes the two high-tail bounds hold for every member").