Gevrey-two composition with the outer derivatives in actual L². Only the inner positive derivatives are bounded in sup norm. The outer L² norm is transported by a measure-preserving map, so it is not replaced by a pointwise bound or by a volume of the ambient domain.
Inner partition bound, given by ∏ i, B*R^(c.partSize i)*((c.partSize i).factorial : ℝ)^2.
Equations
Instances For
theorem
EulerGevreyCompositionLp.innerPartitionBound_nonneg
{n : ℕ}
(B R : ℝ)
(hB : 0 ≤ B)
(hR : 0 ≤ R)
(c : OrderedFinpartition n)
:
theorem
EulerGevreyCompositionLp.composition_partition_bound
{E : Type u_1}
{F : Type u_2}
[NormedAddCommGroup E]
[NormedSpace ℝ E]
[NormedAddCommGroup F]
[NormedSpace ℝ F]
(f : E → E)
(g : E → F)
(n : ℕ)
(x : E)
(hf : ContDiffAt ℝ (↑n) f x)
(hg : ContDiffAt ℝ (↑n) g (f x))
(B R : ℝ)
(_hB : 0 ≤ B)
(_hR : 0 ≤ R)
(hfjet : ∀ (j : ℕ), 0 < j → j ≤ n → ‖iteratedFDeriv ℝ j f x‖ ≤ B * R ^ j * ↑j.factorial ^ 2)
:
‖iteratedFDeriv ℝ n (g ∘ f) x‖ ≤ ∑ c : OrderedFinpartition n, innerPartitionBound B R c * ‖iteratedFDeriv ℝ c.length g (f x)‖
theorem
EulerGevreyCompositionLp.composition_memLp_and_bound
{E : Type u_1}
{F : Type u_2}
[NormedAddCommGroup E]
[NormedSpace ℝ E]
[NormedAddCommGroup F]
[NormedSpace ℝ F]
[MeasurableSpace E]
(μ : MeasureTheory.Measure E)
(f : E → E)
(g : E → F)
(hf : ContDiff ℝ (↑⊤) f)
(hg : ContDiff ℝ (↑⊤) g)
(hmp : MeasureTheory.MeasurePreserving f μ μ)
(n : ℕ)
(hfg : MeasureTheory.AEStronglyMeasurable (iteratedFDeriv ℝ n (g ∘ f)) μ)
(A B R S : ℝ)
(hA : 0 ≤ A)
(hB : 0 ≤ B)
(hR : 0 ≤ R)
(hS : 0 ≤ S)
(hgLp : ∀ j ≤ n, MeasureTheory.MemLp (iteratedFDeriv ℝ j g) 2 μ)
(hgjet : ∀ j ≤ n, (MeasureTheory.eLpNorm (iteratedFDeriv ℝ j g) 2 μ).toReal ≤ A * S ^ j * ↑j.factorial ^ 2)
(hfjet : ∀ (j : ℕ), 0 < j → j ≤ n → ∀ (x : E), ‖iteratedFDeriv ℝ j f x‖ ≤ B * R ^ j * ↑j.factorial ^ 2)
:
MeasureTheory.MemLp (iteratedFDeriv ℝ n (g ∘ f)) 2 μ ∧ (MeasureTheory.eLpNorm (iteratedFDeriv ℝ n (g ∘ f)) 2 μ).toReal ≤ A * (R * (B * S + 2)) ^ n * ↑n.factorial ^ 2
A genuine L² composition estimate with factorial-square growth. The measurability premise is automatic for smooth finite-dimensional fields, and no L² premise is required for the composed derivative.