OAI/Analysis/CircleDomains/Sobolev/MetricInterpolation.lean
11 declarations, 0 contain sorry, 0 declared as axioms
Keeping the original metric near the retained core
The interpolated metric is an actual positive definite matrix field. Its coordinate energy is the inverse-matrix energy density, rather than an independently supplied scalar surrogate.
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OAI.CircleDomainRigidity.FiniteTransfer.PlanarMetricline 21 - def
OAI.CircleDomainRigidity.FiniteTransfer.matrixEnergyline 23 - def
OAI.CircleDomainRigidity.FiniteTransfer.blendMetricline 26 - theorem
OAI.CircleDomainRigidity.FiniteTransfer.blendMetric_zeroline 29 - theorem
OAI.CircleDomainRigidity.FiniteTransfer.blendMetric_oneline 32 - theorem
OAI.CircleDomainRigidity.FiniteTransfer.blendMetric_posDefline 35 - theorem
OAI.CircleDomainRigidity.FiniteTransfer.continuousOn_matrixEnergyline 43 - theorem
OAI.CircleDomainRigidity.FiniteTransfer.exists_core_preserving_metricline 62Source documentation
Replace a smooth positive definite metric by the identity near a compact core. The change of the actual coordinate energy outside that core is small. The transition can be confined to any prescribed open neighborhood.
theorem exists_core_preserving_metric {E : Type*} [NormedAddCommGroup E] [NormedSpace ℝ E] [FiniteDimensional ℝ E] [MeasurableSpace E] [BorelSpace E] {μ : Measure E} [IsFiniteMeasureOnCompacts μ] {K S U : Set E} (hK : IsCompact K) (hS : Bornology.IsBounded S) (hSm : MeasurableSet S) (hU : IsOpen U) (hKU : K ⊆ U) (A g : E → PlanarMetric) (hA : Continuous A) (hg : ContDiff ℝ ∞ g) (hPD : ∀ x, (g x).PosDef) {ε : ℝ} (hε : 0 < ε) : ∃ (N : Set E) (g' : E → PlanarMetric), IsOpen N ∧ K ⊆ N ∧ N ⊆ U ∧ ContDiff ℝ ∞ g' ∧ (∀ x, (g' x).PosDef) ∧ (∀ᶠ x in 𝓝ˢ K, g' x = 1) ∧ (∀ x ∉ N, g' x = g x) ∧ (∫ x in S \ K, |matrixEnergy (A x) (g' x) - matrixEnergy (A x) (g x)| ∂μ) < ε := by …Mentions: OAI.CircleDomainRigidity.FiniteTransfer.PlanarMetric, OAI.CircleDomainRigidity.FiniteTransfer.matrixEnergy
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OAI.CircleDomainRigidity.FiniteTransfer.continuous_matrixEnergyline 94 - theorem
OAI.CircleDomainRigidity.FiniteTransfer.integral_lt_of_abs_sub_ltline 100 - theorem
OAI.CircleDomainRigidity.FiniteTransfer.exists_smooth_core_gramMetricline 116Source documentation
The complete local metric step: small pairwise wedges give one smooth positive definite metric with the prescribed total energy bound, equal to the original identity metric on a full neighborhood of the retained core. The constant regularization and the transition region are both constructed.
theorem exists_smooth_core_gramMetric (x y : ℕ → (ℝ × ℝ) → ℝ) (n : ℕ) (hx : ∀ i, ContDiff ℝ ∞ (x i)) (hy : ∀ i, ContDiff ℝ ∞ (y i)) {K S U : Set (ℝ × ℝ)} (hK : IsCompact K) (hS : Bornology.IsBounded S) (hSm : MeasurableSet S) (hU : IsOpen U) (hKU : K ⊆ U) {ε : ℝ} (hε : (∫ z in S \ K, 2 * covectorWedges (fun i => x i z) (fun i => y i z) n) < ε) : ∃ (τ : ℝ) (N : Set (ℝ × ℝ)) (g : (ℝ × ℝ) → PlanarMetric), 0 < τ ∧ IsOpen N ∧ K ⊆ N ∧ N ⊆ U ∧ ContDiff ℝ ∞ g ∧ (∀ z, (g z).PosDef) ∧ (∀ᶠ z in 𝓝ˢ K, g z = 1) ∧ (∀ z ∉ N, g z = gramTensor (fun i => x i z) (fun i => y i z) n + τ • 1) ∧ (∫ z in S \ K, matrixEnergy (gramTensor (fun i => x i z) (fun i => y i z) n) (g z)) < ε := by …Mentions: OAI.CircleDomainRigidity.FiniteTransfer.covectorWedges, OAI.CircleDomainRigidity.FiniteTransfer.PlanarMetric, OAI.CircleDomainRigidity.FiniteTransfer.gramTensor, OAI.CircleDomainRigidity.FiniteTransfer.matrixEnergy