The combined decay inequality with an absolute leading constant #
Paper label lem:theta-decay (eq:theta-decay-1 and eq:theta-decay-2):
there are an absolute constant C₂₇ and a constant C₂₈ = C₂₈(q) such
that the combined quantity θ = α + β + κ⁻⁴δ² decays from scale ρ to scale
κρ. The order of the two constants matters downstream: κ, η and ε_*
of conv:kappa are built from C₂₇ alone, so C₂₇ has to be fixed before
the integrability exponent q of the force.
Stating the same two displays with q quantified first would only give
∀ q, ∃ C₂₇. The theorem below exchanges the two quantifiers: the witness,
thetaDecayC₂₇ gagliardoConstant √(2 · max pressureP12Constant czP1ThetaDecayConstant) caccioppoliC₂₅, mentions no q, so it can be
produced before q is introduced. The Calderón–Zygmund input of
thm:pressure-decay is discharged from the solution by
CKN.theoremA_hCZ_p1_of_sws.
Following conv:kappa the displays are taken at κ = iterationKappa C₂₇.
Paper label lem:theta-decay, displays eq:theta-decay-1 and
eq:theta-decay-2, with the leading constant C₂₇ absolute (fixed before the
force exponent q) and C₂₈ = C₂₈(q), at the scale ratio κ of
conv:kappa.