Iterated Derivative Helpers #
Bounds on iterated derivatives of continuous linear maps and quadratic forms, used in the Schwartz decay proof for the equilibrium Maxwellian.
theorem
VML.iteratedFDeriv_clm_zero
{π : Type u_1}
[NontriviallyNormedField π]
{E : Type u_2}
{F : Type u_3}
[NormedAddCommGroup E]
[NormedSpace π E]
[NormedAddCommGroup F]
[NormedSpace π F]
(f : E βL[π] F)
(n : β)
(hn : 2 β€ n)
(x : E)
:
The iterated derivative of a continuous linear map vanishes at order β₯ 2.
theorem
VML.norm_iteratedFDeriv_one_clm
{π : Type u_1}
[NontriviallyNormedField π]
{E : Type u_2}
{F : Type u_3}
[NormedAddCommGroup E]
[NormedSpace π E]
[NormedAddCommGroup F]
[NormedSpace π F]
(f : E βL[π] F)
(x : E)
:
The norm of the first iterated derivative of a CLM equals the operator norm.
theorem
VML.norm_fderiv_eq_iteratedFDeriv_one
{π : Type u_1}
[NontriviallyNormedField π]
{E : Type u_2}
{F : Type u_3}
[NormedAddCommGroup E]
[NormedSpace π E]
[NormedAddCommGroup F]
[NormedSpace π F]
(f : E β F)
(v : E)
:
βfderiv f vβ = βiteratedFDeriv 1 f vβ. Converts between the ContinuousLinearMap
norm and the ContinuousMultilinearMap norm at order 1.
Derivative bound for the quadratic form q(v) = -normSq(v)/(2T). Since q is a degree-2 polynomial: fderiv is O(1+βvβ), second derivative is constant, and all higher derivatives vanish.