GammaTenGaugeScalarCap #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
The two scalar gauge factors of the Besov legs are capped #
ABK26, e.shom.h.bounds, read at Step 2 of l.approximate.recurrence.formula,
e.Fz.def.
The gap this module fills #
cubeBesovPositiveVectorPartialSeminormTwo_gauged_localizationFz_potential
and ..._flux identify the Besov tower of each gauged leg of bfF_z with a
scalar multiple of the tower of the raw field, the two scalars being
c_1 = sqrt(sigma_0) . sqrt(shom_n)^{-1} , c_2 = sqrt(sigma_0)^{-1} . sqrt(shom_n) ,
at sigma_0 = shom_{n+h-1}. Closure.GammaTenStripEnvelopeTwoLeg carries
|c_1| <= C_g and |c_2| <= C_g as binders and no producer exists. The
proved PrincipalResponseComposeDisplayTwo.gaugeRatio_sigmaBar_le_readingConst
caps the ratio max(shom_{n+h-1}/shom_n, shom_n/shom_{n+h-1}) by the
absolute 4 . 3^9; each |c_i| is the square root of one of those two
quotients, and a square root of a number above 1 is below the number itself.
That is the whole content.
What is proved #
sqrt_le_self_of_one_le---sqrt C <= Cfor1 <= C.abs_sqrt_mul_inv_sqrt_le---|sqrt a . (sqrt b)^{-1}| <= Cfroma / b <= Cand1 <= C, for positivea,b.abs_gaugeScalar_potential_le,abs_gaugeScalar_flux_le--- the two caps at the closure's own pair of gauges, from the proved ratio cap carried as the binderhgauge.
Binders #
Only hgauge, the same binder
Closure.GammaTenCloserGauge.blockVecNormSum_blockGaugeUp_le_gammaTenGaugeConst
already carries and which Closure.ClosureInteriorSplit discharges inline from
PrincipalResponseComposeDisplayTwo.gaugeRatio_sigmaBar_le_readingConst. No
smallness gate, no moment, no measurability and no sample-space proposition
occurs.
Scope #
Internal Provider infrastructure for the Step-2 fluctuation estimate. There is
no sorry, no admit, no custom axiom and no set_option maxHeartbeats.
References #
- ABK26,
e.shom.h.bounds,l.approximate.recurrence.formulaStep 2,e.Fz.def.
Two elementary steps #
The scalar gauge factor is the square root of the gauge quotient, hence
capped by any cap at least 1 on that quotient.
on ha, hb, hC and hab.
The two caps at the closure's pair of gauges #
The potential leg's scalar gauge factor is capped by 4 . 3^9.
on hgauge.
The flux leg's scalar gauge factor is capped by 4 . 3^9.
on hgauge.