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LeanPool.Superdiffusion.Algsuperdiff.Section3.Provider.CoarseEllipticity.UpperProfileExponents

UpperProfileExponents #

Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.

Exponent arithmetic for the Section 3.3 upper profile.

The percolation and wave-tail estimates are run at sigma / 4, while the exceptional exponent in the frozen theorem is Gamma_{(1-sigma)/3}. The definitions below record the arithmetic buffer needed for the extra seam and collar powers.

The reduced profile exponent used in upper coarse-ellipticity estimates.

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    The product-tail exponent associated with the reduced upper profile exponent.

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      The target exponent in the upper coarse-ellipticity tail estimate.

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        The weakest hsep-factor exponent whose product with the profile tail exponent equals the target exponent in the frozen theorem.

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          Auxiliary exponent fed to the hsep indicator theorem.

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            theorem Algsuperdiff.Section3.Provider.CoarseEllipticity.upperProfileBaseSigma_pos {sigma : ℝ} (hsigma0 : 0 < sigma) (hsigma : sigma ≤ 1 / 2) :
            theorem Algsuperdiff.Section3.Provider.CoarseEllipticity.upperProfileTailSigma_pos {sigma : ℝ} (hsigma0 : 0 < sigma) (_hsigma : sigma ≤ 1 / 2) :
            theorem Algsuperdiff.Section3.Provider.CoarseEllipticity.upperProfileHsepTau_pos {sigma : ℝ} (hsigma0 : 0 < sigma) (hsigma : sigma ≤ 1 / 2) :

            The hsep indicator product theorem at the auxiliary exponent produces the required hsep-factor exponent exactly.

            The required hsep exponent times the profile tail exponent equals the exceptional exponent in the frozen theorem.

            theorem Algsuperdiff.Section3.Provider.CoarseEllipticity.productSigma_mono_left {a b r : ℝ} (ha : 0 < a) (hab : a ≤ b) (hr : 0 < r) :
            a * r / (a + r) ≤ b * r / (b + r)

            Harmonic-product exponents are monotone in their first input.

            theorem Algsuperdiff.Section3.Provider.CoarseEllipticity.upperProfileHsepTau_le_collarPowerSigma {sigma gamma b : ℝ} (hsigma0 : 0 < sigma) (hsigma : sigma ≤ 1 / 2) (hgamma0 : 0 ≤ gamma) (hb : 0 < b) (hgamma : gamma ≤ b * sigma) :
            upperProfileHsepTau sigma ≤ upperProfileBaseSigma sigma / ((2 * gamma + 2 * b) / b)

            The direct collar power 3^((2 gamma + 2b) hsep) remains strong enough when the frozen gate has paid gamma ≤ b sigma.

            theorem Algsuperdiff.Section3.Provider.CoarseEllipticity.upperProfileTargetSigma_le_collarPower_mul_tail {sigma gamma b : ℝ} (hsigma0 : 0 < sigma) (hsigma : sigma ≤ 1 / 2) (hgamma0 : 0 ≤ gamma) (hb : 0 < b) (hgamma : gamma ≤ b * sigma) :
            upperProfileTargetSigma sigma ≤ upperProfileBaseSigma sigma / ((2 * gamma + 2 * b) / b) * upperProfileTailSigma sigma / (upperProfileBaseSigma sigma / ((2 * gamma + 2 * b) / b) + upperProfileTailSigma sigma)

            Consequently the collar power times the profile tail still reaches the exceptional exponent in the frozen theorem.