The fixed physical Sobolev order costs a polynomial in the Gevrey radius. Explicit coarse powers leave room for the source exponent C*=10(s+2), including the sum of all three particle-map fields.
Fixed cost, given by (2 : ℝ)^q*∑ j ∈ range (q+1), (j.factorial : ℝ)^2.
Equations
- EulerSobolevSourceExponent.fixedCost q = 2 ^ q * ∑ j ∈ Finset.range (q + 1), ↑j.factorial ^ 2
Instances For
theorem
EulerSobolevSourceExponent.triple_classical_bound
(q : ℕ)
(A B C : EulerLpTranslation.SmoothL2Field EulerSmoothLimit.Space)
(M R J : ℝ)
(hM : 0 ≤ M)
(hR : 0 ≤ R)
(hA : A.HasJetBound M R)
(hB : B.HasJetBound M R)
(hC : C.HasJetBound M R)
(hcost : 3 * EulerParameterWordGevrey.sobolevCoefficientAmplitude (Fin 3) q R M ≤ J)
(hrad : EulerParameterWordGevrey.sobolevCoefficientRadius (Fin 3) R ≤ J)
(n : ℕ)
:
EulerMeanClassicalWordBounds.classicalBlockSize EulerPacketParentLabelBounds.direction q A.toLp ⋯ n + EulerMeanClassicalWordBounds.classicalBlockSize EulerPacketParentLabelBounds.direction q B.toLp ⋯ n + EulerMeanClassicalWordBounds.classicalBlockSize EulerPacketParentLabelBounds.direction q C.toLp ⋯ n ≤ J ^ (n + 1) * ↑n.factorial ^ 2
theorem
EulerSobolevSourceExponent.source_triple_classical_bound
(q : ℕ)
(A B C : EulerLpTranslation.SmoothL2Field EulerSmoothLimit.Space)
(k M R : ℝ)
(hk : 12 ≤ k)
(hcost : fixedCost q ≤ k)
(hM : 0 ≤ M)
(hR : 0 ≤ R)
(hMb : M ≤ k ^ 6)
(hRb : R ≤ k ^ 5)
(hA : A.HasJetBound M R)
(hB : B.HasJetBound M R)
(hC : C.HasJetBound M R)
(n : ℕ)
:
EulerMeanClassicalWordBounds.classicalBlockSize EulerPacketParentLabelBounds.direction q A.toLp ⋯ n + EulerMeanClassicalWordBounds.classicalBlockSize EulerPacketParentLabelBounds.direction q B.toLp ⋯ n + EulerMeanClassicalWordBounds.classicalBlockSize EulerPacketParentLabelBounds.direction q C.toLp ⋯ n ≤ (k ^ (10 * (q + 2))) ^ (n + 1) * ↑n.factorial ^ 2