Norm-level cutoff existence #
This file proves the existence form of apd:thm:truncation_threshold_entangled at norm level:
for a decay base 0 ≤ q < 1, the majorant q^(m+1) (e(m+1))^c M supplied by
total_truncation_error_product_bound tends to zero in the rung m, so every sufficiently large
rung m ≥ 1 brings it below any tolerance ε > 0.
Main results #
norm_majorant_tendsto_zero:q^(m+1) (e(m+1))^c M → 0asm → ∞, for0 ≤ q < 1.exists_eventual_norm_threshold,exists_norm_threshold: a rungm ≥ 1meeting the tolerance exists, and so does every larger rung.exists_uniform_norm_threshold,exists_uniform_weight_cutoff: one rung, respectively one weight cutoffw = k_o + (k_h − 1)m, for a whole family sharing the sameq, c, M.exists_model_norm_threshold: the caseq = decayBase G kh α twitht < tZeroModel G kh α.exists_admissible_step_count: a step countrcan be chosen after the rung.
Scope #
apd:thm:truncation_threshold_entangled and eq:truncation_weight_bound use exponential decay
to dominate the polynomial factor. Here the norm-level majorant q^(m+1) (e(m+1))^c M tends to
zero when 0 ≤ q < 1; for c ≥ 0 its factor (e(m+1))^c is smaller than the factor
(m*+2)(e(m*+2))^c of apd:eq:total_truncation_error. The analytic limit permits any real
c, M; physical applications use the nonnegative constants supplied by the norm bound. Mathlib's
real-power/exponential asymptotic is reused directly.
The conclusions are cutoff existence, a conservative form of the paper's corollary: the explicit
logarithmic/log-log estimate of m*, the runtime statement (apd:thm:runtime) and the
conversion to an error in expectation are not formalized here. The uniform-family corollary
requires one common q,c,M bound for the entire family; dimension independence is not inferred
when those parameters, especially the observable norm bound, grow with dimension.
Converting a uniform rung to a uniform weight also requires fixed k_o,k_h; the weight
corollary keeps these outside the family quantifier explicitly.
Choosing a larger numerical step count is separate from constructing the corresponding gate
angles. Nothing here assumes a fixed angle family still satisfies a ≤ αt/r after r changes.
The analytic decay behind apd:thm:truncation_threshold_entangled, applied to the norm-level
majorant of total_truncation_error_product_bound: for 0 ≤ q < 1 and all real c, M,
q^(m+1) (e(m+1))^c M → 0 as m → ∞. The exponential decay of q^(m+1) dominates the
polynomial factor.
Every sufficiently large natural rung meets the norm tolerance, the existence part of
apd:thm:truncation_threshold_entangled. No explicit logarithmic formula for the rung is
asserted, and no hypothesis on the input state is involved.
The cutoff can be chosen independently of the family index when the same q,c,M
majorizes the whole family. This is the qualified dimension-independent interpretation of
apd:thm:truncation_threshold_entangled, for absolute norm tolerance.
A single weight cutoff works for the whole family when k_o,k_h,q,c,M are all fixed
uniform data. This is the norm-level, absolute-tolerance form of
eq:truncation_weight_bound, not a runtime or expectation theorem.
The model-only short-time condition t < tZeroModel G kh α supplies 0≤q<1 for
q = decayBase G kh α t, so the norm-level cutoff exists. This is the model-threshold
counterpart of apd:thm:truncation_threshold_entangled; it concerns the norm-level majorant
only, so no hypothesis on the input state is involved.
Numerical step counts can be chosen after the rung: an Archimedean helper for the conditions
of apd:eq:multijump_factor. The two real lower bounds B₁, B₂ may encode the paper's
finite-step conditions r ≥ 8(m*+1)²/Γ and r ≥ 8e²·w₂·αt; satisfying them does not construct
or update any gate-angle family.