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LeanPool.ViscositySolutionTheory.AleksandrovDifferentiability.Analysis.LineSecondOrder

Ported for Lean Pool: imports relocated and code adapted to Lean/Mathlib v4.34.0.

Second order expansions on affine lines #

This file connects the ambient second-order expansion predicate to one-dimensional restrictions along affine lines.

theorem AleksandrovDifferentiability.HasSecondOrderExpansionAt.lineRestriction_isLittleO {E : Type u_1} [NormedAddCommGroup E] [InnerProductSpace ℝ E] {u : E → ℝ} {x p : E} {B : E →L[ℝ] E} (h : HasSecondOrderExpansionAt u x p B) (v : E) :
(fun (t : ℝ) => lineRestriction u x v t - u x - inner ℝ p v * t - 1 / 2 * inner ℝ v (B v) * t ^ 2) =o[nhds 0] fun (t : ℝ) => ‖t • v‖ ^ 2

An ambient second-order expansion restricts to a second-order expansion along every affine line, with the expected directional first and second coefficients.

theorem AleksandrovDifferentiability.HasSecondOrderExpansionAt.lineRestriction_isLittleO_of_norm_eq_one {E : Type u_1} [NormedAddCommGroup E] [InnerProductSpace ℝ E] {u : E → ℝ} {x p v : E} {B : E →L[ℝ] E} (h : HasSecondOrderExpansionAt u x p B) (hv : ‖v‖ = 1) :
(fun (t : ℝ) => lineRestriction u x v t - u x - inner ℝ p v * t - 1 / 2 * inner ℝ v (B v) * t ^ 2) =o[nhds 0] fun (t : ℝ) => ‖t‖ ^ 2

Unit-direction version of HasSecondOrderExpansionAt.lineRestriction_isLittleO, with the standard one-dimensional denominator.

theorem AleksandrovDifferentiability.HasSecondOrderExpansionAt.lineRestriction_isLittleO_standard {E : Type u_1} [NormedAddCommGroup E] [InnerProductSpace ℝ E] {u : E → ℝ} {x p : E} {B : E →L[ℝ] E} (h : HasSecondOrderExpansionAt u x p B) (v : E) :
(fun (t : ℝ) => lineRestriction u x v t - u x - inner ℝ p v * t - 1 / 2 * inner ℝ v (B v) * t ^ 2) =o[nhds 0] fun (t : ℝ) => ‖t‖ ^ 2

An ambient second-order expansion restricts to an affine line with the standard one-dimensional little-o denominator.

Ambient second-order expansions restrict to project-level second-order expansions of one-dimensional line restrictions.

Ambient second-order expansions restrict to affine lines at arbitrary line parameters.

theorem AleksandrovDifferentiability.HasSecondOrderExpansionAtCLM.lineRestriction_isLittleO {E : Type u_1} [NormedAddCommGroup E] [InnerProductSpace ℝ E] {u : E → ℝ} {x : E} {ℓ : E →L[ℝ] ℝ} {B : E →L[ℝ] E} (h : HasSecondOrderExpansionAtCLM u x ℓ B) (v : E) :
(fun (t : ℝ) => lineRestriction u x v t - u x - ℓ v * t - 1 / 2 * inner ℝ v (B v) * t ^ 2) =o[nhds 0] fun (t : ℝ) => ‖t • v‖ ^ 2

An ambient CLM-gradient second-order expansion restricts to a second-order expansion along every affine line, with the expected directional first and second coefficients.

theorem AleksandrovDifferentiability.HasSecondOrderExpansionAtCLM.lineRestriction_isLittleO_of_norm_eq_one {E : Type u_1} [NormedAddCommGroup E] [InnerProductSpace ℝ E] {u : E → ℝ} {x v : E} {ℓ : E →L[ℝ] ℝ} {B : E →L[ℝ] E} (h : HasSecondOrderExpansionAtCLM u x ℓ B) (hv : ‖v‖ = 1) :
(fun (t : ℝ) => lineRestriction u x v t - u x - ℓ v * t - 1 / 2 * inner ℝ v (B v) * t ^ 2) =o[nhds 0] fun (t : ℝ) => ‖t‖ ^ 2

Unit-direction version of HasSecondOrderExpansionAtCLM.lineRestriction_isLittleO, with the standard one-dimensional denominator.

theorem AleksandrovDifferentiability.HasSecondOrderExpansionAtCLM.lineRestriction_isLittleO_standard {E : Type u_1} [NormedAddCommGroup E] [InnerProductSpace ℝ E] {u : E → ℝ} {x : E} {ℓ : E →L[ℝ] ℝ} {B : E →L[ℝ] E} (h : HasSecondOrderExpansionAtCLM u x ℓ B) (v : E) :
(fun (t : ℝ) => lineRestriction u x v t - u x - ℓ v * t - 1 / 2 * inner ℝ v (B v) * t ^ 2) =o[nhds 0] fun (t : ℝ) => ‖t‖ ^ 2

An ambient CLM-gradient second-order expansion restricts to an affine line with the standard one-dimensional little-o denominator.

Ambient CLM-gradient second-order expansions restrict to project-level second-order expansions of one-dimensional line restrictions.

Ambient CLM-gradient second-order expansions restrict to affine lines at arbitrary line parameters.

On the real line, every scalar multiple of the identity is a symmetric operator.

Second order differentiability restricts to affine lines at arbitrary line parameters.

The preimage of a fixed ambient second-order expansion locus along a line is contained in the corresponding one-dimensional expansion locus.

The preimage of a fixed ambient CLM expansion locus along a line is contained in the corresponding one-dimensional expansion locus.

The preimage of the ambient second-order differentiability locus along a line is contained in the one-dimensional second-order differentiability locus of the line restriction.

The preimage of the ambient CLM expansion-data locus along a line is contained in the one-dimensional second-order differentiability locus of the line restriction.

On a line restriction, project-level one-dimensional second-order differentiability gives the scalar quadratic estimate format used by the one-dimensional assembly layer.

Ambient second-order differentiability along a line implies scalar quadratic estimate data for the corresponding one-dimensional line restriction.

Ambient CLM expansion data along a line implies scalar quadratic estimate data for the corresponding one-dimensional line restriction.

On a line restriction, project-level one-dimensional second-order differentiability gives the punctured scalar quotient-estimate format used by the one-dimensional assembly layer.

Ambient second-order differentiability along a line implies scalar quotient-estimate data for the corresponding one-dimensional line restriction.

Ambient CLM expansion data along a line implies scalar quotient-estimate data for the corresponding one-dimensional line restriction.