StepSevenEndPoincare #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
t.regularity Step 7d, part one: e.cg.Poincare.with.rhs.grad.applied #
The target #
3^{-m'}‖∇u‖_{B^{-1}_{2,2}(z'+□_{m'-1})} 1_{𝒢(m',z;·,·)}
≤ C σ_{m'}^{-1/2} ν^{1/2}‖∇u‖_{L²(z'+□_{m'-1})}
+ C σ_{m'}^{-1} 3^{sm'}[𝐠]_{H^s(z'+□_{m'-1})}
≤ C 3^{(1/2)(d+γ)(m-m')} ( σ_m^{-1/2} ν^{1/2}‖∇u‖_{L²(□_m)}
+ σ_m^{-1} 3^{sm}[𝐠]_{H^s(□_m)} ) .
Two independent inequalities, proved here as two independent theorems on the S
the display names (/ discipline), plus the C₁-largeness accounting that
absorbs the transport exponent.
The scalar carriers #
besov—3^{-m'}‖∇u‖_{B^{-1}_{2,2}(z'+□_{m'-1})}·1_{𝒢}, the left-hand side.lamInv—λ_{1/4,2}^{-1}(z+□_{m'};𝐚_{L,m'})·1_{𝒢}, the coarse-graining lemma's ellipticity weight at the lattice centre.shomMpInv/shomMinv—σ_{m'}^{-1}andσ_m^{-1}.gradLoc/gradM—ν^{1/2}‖∇u‖_{L²}onz'+□_{m'-1}and on□_m: for𝐚_L = ν I + 𝐤with𝐤antisymmetric this is the symmetric coefficient energy.dataLoc/dataM—3^{sm'}[𝐠]_{H^s(z'+□_{m'-1})}and3^{sm}[𝐠]_{H^s(□_m)}.Kg,Kd,Ks— the three transport factors of the second inequality: theL²volume ratio, theH^swindow restriction, and theσcomparison.
The conditional inputs, and nothing else #
hcg—l.coarse.graining.RHSapplied onz'+□_{m'-1}at the good scalem', in the ellipticity-weighted form the display quotes:besov ≤ C(√lamInv·gradLoc) + C(lamInv·dataLoc).hlambda—e.lambda.stability.applied, the lower leg atk' = m':λ_{1/4,2}^{-1}(z+□_{m'};𝐚_{L,m'})1_{𝒢} ≤ C σ_{m'}^{-1}. This is the first conjunct of the printed display, in exactly the rendering discipline the Step-7chlambdauses for the second conjunct (lattice centre, indicator absorbed, one scalar inequalityweight ≤ C · σ-power), so that a single future Step-7b theorem discharges both.
The three transport ingredients hgrad, hdata, hshom are not conditional
inputs of this module: they are the caller's own geometry/σ facts, and each
is supplied unconditionally elsewhere in the development
(normalizedL2On_le_of_subset for Kg, the window restriction for Kd, and
sigmaBar_le_rpow_mul_sigmaBar_of_inductionState for Ks).
The C₁-largeness accounting (the transport exponent) #
The transport exponent (1/2)(d+γ)(m-m') is absorbed into
3^{(1/4)(1-α)(m-n)} by the third and fourth C₁-largeness conditions. The
C₁ floor already carries the exact clause: stepOneC1's second maximand is
2d+2, which reads as 2(d+γ) ≤ C₁ for γ ≤ 1 — the pin whose docstring
names this transport. So
(1/2)(d+γ)(m-m') ≤ (1/2)(d+γ)·3 + 1/4 + (1/4)(1-α)(m-n)
with NO new largeness demand: the quarter-bound on (d+γ)/(2C₁) needs
exactly 2d+2 ≤ C₁ and γ ≤ 1. Nothing was enlarged.
References #
- ABK26,
e.cg.Poincare.with.rhs.grad.applied. - ABK26, graining.;
e.lambda.stability.applied.
2. The first inequality: the coarse-graining Poincaré after hlambda #
e.cg.Poincare.with.rhs.grad.applied, first inequality, on abstract reals.
l.coarse.graining.RHS produces the Besov left-hand side against the weight
λ^{-1} (square root on the gradient leg, full power on the data leg);
e.lambda.stability.applied replaces λ^{-1} by C σ_{m'}^{-1}. The two
legs are then carried by the single constant Ccg(√Clam + Clam).
3. The second inequality: the transport to □_m #
e.cg.Poincare.with.rhs.grad.applied, second inequality, on abstract
reals: the three transports
gradLoc ≤ Kg · gradM , dataLoc ≤ Kd · dataM , σ_{m'}^{-1} ≤ Ks · σ_m^{-1}
(the L² volume ratio, the H^s window restriction, and the σ
comparison) carry the weighted bracket from z'+□_{m'-1} to □_m at the two
factors √Ks·Kg and Ks·Kd.
4. The display #
e.cg.Poincare.with.rhs.grad.applied, as printed.
The two inequalities composed, at a single transport factor Ktr dominating
both legs' factors:
besov ≤ Ccg(√Clam + Clam) · Ktr · ( √σ_m^{-1}·gradM + σ_m^{-1}·dataM ) .
hcg and hlambda are the only conditional
inputs; hgrad, hdata, hshom, hKgb, hKdb are the caller's own
transport data.