BadEventFrozenApplication #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
The per-cube bad-event tail at the dimension floor, from the frozen estimate #
This module consumes Algsuperdiff.Frozen.Section3.bad_event_estimate and
delivers the per-cube tail at a constant that clears the dimension floor
(d : ℝ) ^ 6, which is what the Section 3.4 good-event display needs. It is
the consuming half of the scale-shift bridge whose geometric core is
Provider.Diffusivity.ApproximateRecurrence.BadEventScaleShiftBridge.
The mechanism #
The frozen export publishes only 1 ≤ Ccg, and goodLocalEvent is not monotone
in that constant. The bridge trades the constant against the cube scale: with
k := badEventScaleShiftExp d = 6 d,
good (2 Ccg, cu_m, n) ∩ good (2 Ccg, cu_{m + 2k}, n) ⊆ good (2 · 3^k · Ccg, cu_m, n)
(goodLocalEvent_inter_subset_scaleShift_le), and 3 ^ k ≥ (d : ℝ) ^ 6
(dim_pow_six_le_three_pow_scaleShiftExp). The frozen export is applied twice
at the same translate triadicCubeShift R, once at the cube scale R.scale
and once at the enlarged scale R.scale + 2 k, and the union bound produces the
factor 2 that the consumer absorbs through its Hoelder 3/8 power.
The two guarded rate gates #
The first application sits in the ¬ (n < m) regime, so both of its guarded
gates are vacuous. The second one need not: the Section 3.4 grid is indexed by
a free recurrence multiplier a ≤ 32, and at a = 0 the cube scale equals the
field scale, leaving no headroom at all. The two gates are therefore discharged
on their own terms, using only R.scale ≤ n, which caps the enlarged gap at
m - n ≤ 2 k:
- the rate gate
3 ^ (5 (m - n)) ≤ c · cstar · gamma⁻¹follows from the admissibility premisec⁻¹ cstar⁻¹ ≤ E ≤ gamma⁻¹once the exportedcis the dimension-only shrinkc₀ · 3 ^ (-12 k); - the ellipticity gate
d (m - n) log 3 + exp (X / 8) ≤ exp (X / 4),X := Ccg⁻¹ E⁻² gamma⁻¹, follows fromu ^ 2 + exp u ≤ exp (2 u)atu = X / 8onceXis above the dimension-only thresholdKgate := 40 (d + k + 1) Ccg, which is exported as a binder and discharged by the consumer from its own window premise.
Both gates are derived, never assumed of the source: Kgate is an exported
existential witness, and the consumer discharges Kgate ≤ E⁻² gamma⁻¹ from the
window premise gamma / 2 + exp (-(C⁻¹ E⁻² gamma⁻¹)) ≤ gamma at its own
enlarged constant C.
References #
- ABK26,
l.bad.event.lemma;e.good.local.events. - The gate
R.scale + 2 k ≤ nthat §5.3 proposes is not available at the consumer, whose public statement quantifies the recurrence multiplier freely; the two gates are discharged non-vacuously instead, and no public statement changes.
One elementary exponential inequality #
The frozen application #
The per-cube bad-event tail at a floor-normalized constant, derived from
the frozen Algsuperdiff.Frozen.Section3.bad_event_estimate.
The frozen export is applied twice at the same translate triadicCubeShift R,
once at the cube scale R.scale and once at the enlarged scale
R.scale + 2 * badEventScaleShiftExp d; the scale-shift inclusion turns the two
events into the single event at the enlarged constant 2 * 3 ^ k * Ccg, whose
floor (d : ℝ) ^ 6 is cleared by dim_pow_six_le_three_pow_scaleShiftExp, and
the union bound produces the factor 2.
The exported Kgate is a dimension-only lower threshold on E⁻² gamma⁻¹: it is
what discharges the frozen ellipticity gate at the enlarged scale, and the
consumer derives it from its own window premise.
: this statement holds only under the propositions supplied by its binders. It is a provider A, not a source-facing frozen declaration.