OAI/MathematicalPhysics/Elasticity/LocalRegularity.lean
35 declarations, 0 contain sorry, 0 declared as axioms
- def
OAI.ElasticityRegularity.LocalEqualline 19 - lemma
OAI.ElasticityRegularity.LocalEqual.reflline 23 - lemma
OAI.ElasticityRegularity.LocalEqual.symmline 24 - lemma
OAI.ElasticityRegularity.LocalEqual.transline 25 - lemma
OAI.ElasticityRegularity.LocalEqual.addline 27 - lemma
OAI.ElasticityRegularity.LocalEqual.subline 30 - lemma
OAI.ElasticityRegularity.LocalEqual.smulline 33 - lemma
OAI.ElasticityRegularity.LocalEqual.sumline 36 - lemma
OAI.ElasticityRegularity.LocalEqual.derivativeline 41 - lemma
OAI.ElasticityRegularity.LocalEqual.cutoffline 50 - lemma
OAI.ElasticityRegularity.LocalEqual.localSobolevline 61 - lemma
OAI.ElasticityRegularity.LocalSobolev.addline 69 - lemma
OAI.ElasticityRegularity.LocalSobolev.subline 73 - lemma
OAI.ElasticityRegularity.LocalSobolev.smulline 77 - lemma
OAI.ElasticityRegularity.LocalSobolev.sumline 81 - lemma
OAI.ElasticityRegularity.LocalSobolev.coeffline 86 - lemma
OAI.ElasticityRegularity.LocalSobolev.derivativeline 91 - lemma
OAI.ElasticityRegularity.local_laplacian_gain_basisline 96 - lemma
OAI.ElasticityRegularity.schwartz_dist_injectiveline 121 - lemma
OAI.ElasticityRegularity.distribution_schwartz_productline 129 - lemma
OAI.ElasticityRegularity.LocalEqual.cutoff_oneline 139 - lemma
OAI.ElasticityRegularity.LocalEqual.schwartz_eqOnline 152 - lemma
OAI.ElasticityRegularity.smooth_Linfty_productline 179 - theorem
OAI.ElasticityRegularity.local_schwartz_representativeline 196Source documentation
Interior cutoff regularity yields an actual Schwartz representative on the smaller open set; this is what is needed to construct physical smooth CGO solutions on a ball from an L2 weak solution on a larger ball.
theorem local_schwartz_representative {Ω Ω' : Set E} (u : 𝓢'(E,ℂ)) (hu : ∀ N : ℕ, LocalSobolev Ω N u) {g : E → ℂ} (hg : ContDiff ℝ (⊤ : ℕ∞) g) (hc : HasCompactSupport g) (hs : tsupport g ⊆ Ω) (h1 : Set.EqOn g 1 Ω') : ∃ v : 𝓢(E,ℂ), LocalEqual Ω' u (v : 𝓢'(E,ℂ)) := by …Mentions: OAI.ElasticityRegularity.LocalSobolev, OAI.ElasticityRegularity.LocalEqual
- lemma
OAI.ElasticityRegularity.LocalEqual.lp_aeline 215 - theorem
OAI.ElasticityRegularity.local_schwartz_l2_representativeline 251Source documentation
The smooth local representative really is the original L2 function almost everywhere, so the HB solution's L2 estimate is not lost in regularization.
theorem local_schwartz_l2_representative {Ω Ω' : Set E} (hΩ' : IsOpen Ω') (u : Lp ℂ 2 (volume : Measure E)) (hu : ∀ N : ℕ, LocalSobolev Ω N (u : 𝓢'(E,ℂ))) {g : E → ℂ} (hg : ContDiff ℝ (⊤ : ℕ∞) g) (hc : HasCompactSupport g) (hs : tsupport g ⊆ Ω) (h1 : Set.EqOn g 1 Ω') : ∃ v : 𝓢(E,ℂ), LocalEqual Ω' (u : 𝓢'(E,ℂ)) (v : 𝓢'(E,ℂ)) ∧ ∀ᵐ x ∂(volume : Measure E), x ∈ Ω' → u x=v x := by …Mentions: OAI.ElasticityRegularity.LocalSobolev, OAI.ElasticityRegularity.LocalEqual
- lemma
OAI.ElasticityDistribution.coe_schwartz_addline 272 - lemma
OAI.ElasticityDistribution.coe_schwartz_smulline 273 - lemma
OAI.ElasticityDistribution.coe_schwartz_sumline 274 - lemma
OAI.ElasticityDistribution.sd_schwartzline 276 - lemma
OAI.ElasticityDistribution.coeff_schwartzline 281 - lemma
OAI.ElasticityDistribution.divd_schwartzline 283 - lemma
OAI.ElasticityDistribution.phys_schwartzline 287 - lemma
OAI.ElasticityDistribution.LocalEq.physicalline 292 - theorem
OAI.ElasticityDistribution.classical_representativeline 300Source documentation
A genuinely classical physical solution on an interior open set is obtained from the actual weak solution, and represents that same L2 unknown there.
theorem classical_representative {Ω Ω' : Set X} (hΩ' : IsOpen Ω') (hsub : Ω' ⊆ Ω) (z : Fin 3 → ℂ) (lam m n o : Coeff) (hn : n*m=1) (ho : o*(lam+m+m)=1) (w : ElasticityPhysicalDual.H) (F : Fin 3 → S) (heq : ∀ i, LocalEq Ω (phys z lam m (fun j => (w j : Dist)) i) (F i : Dist)) {g : X → ℂ} (hg : ContDiff ℝ (⊤ : ℕ∞) g) (hc : HasCompactSupport g) (hs : tsupport g ⊆ Ω) (h1 : Set.EqOn g 1 Ω') : ∃ v : Fin 3 → S, (∀ i, ∀ᵐ x ∂(volume : Measure X), x ∈ Ω' → w i x=v i x) ∧ ∀ i, Set.EqOn (physical z (eval lam) (eval m) v i : X → ℂ) (F i : X → ℂ) Ω' := by …Mentions: OAI.ElasticityDistribution.X, OAI.ElasticityDistribution.Coeff, OAI.ElasticityPhysicalDual.H, OAI.ElasticityDistribution.S, OAI.ElasticityDistribution.LocalEq, OAI.ElasticityDistribution.phys, OAI.ElasticityDistribution.Dist, OAI.ElasticityDistribution.eval