Dist Deriv comp lorentz action
SpaceTime.distDeriv_comp_lorentz_action
Project documentation
Given a distribution (function) f : Space d →d[ℝ] M the derivative of f in direction μ. -/ noncomputable def distDeriv {M d} [NormedAddCommGroup M] [NormedSpace ℝ M] (μ : Fin 1 ⊕ Fin d) : ((SpaceTime d) →d[ℝ] M) →ₗ[ℝ] (SpaceTime d) →d[ℝ] M where toFun f := let ev : (SpaceTime d →L[ℝ] M) →L[ℝ] M := { toFun v := v (Lorentz.Vector.basis μ) map_add' v1...
Exact Lean statement
lemma distDeriv_comp_lorentz_action {μ : Fin 1 ⊕ Fin d} (Λ : LorentzGroup d)
(f : (SpaceTime d) →d[ℝ] M) :
distDeriv μ (Λ • f) = ∑ ν, Λ⁻¹.1 ν μ • (Λ • distDeriv ν f)Formal artifact
Lean source
lemma distDeriv_comp_lorentz_action {μ : Fin 1 ⊕ Fin d} (Λ : LorentzGroup d) (f : (SpaceTime d) →d[ℝ] M) : distDeriv μ (Λ • f) = ∑ ν, Λ⁻¹.1 ν μ • (Λ • distDeriv ν f) := by symm trans (∑ ν, Λ • Λ⁻¹.1 ν μ • (distDeriv ν) f) · congr funext i rw [SMulCommClass.smul_comm] trans Λ • (∑ ν, Λ⁻¹.1 ν μ • (distDeriv ν) f) · exact Eq.symm Finset.smul_sum ext η rw [lorentzGroup_smul_dist_apply, distDeriv_apply, fderivD_apply, lorentzGroup_smul_dist_apply] rw [← smul_neg] congr rw [_root_.sum_apply] simp only [FunLike.coe_smul, Pi.smul_apply] conv_lhs => enter [2, x] rw [distDeriv_apply, fderivD_apply] simp only [smul_neg] rw [← map_smul] rw [Finset.sum_neg_distrib] congr rw [← map_sum] congr /- Reduced to Schwartz maps -/ ext x rw [_root_.sum_apply] symm simp [schwartzAction_apply] change ∂_ μ η (Λ • x) = ∑ ν, Λ⁻¹.1 ν μ • ∂_ ν (schwartzAction Λ⁻¹ η) (x) obtain ⟨η, rfl⟩ := schwartzAction_surjective Λ η simp only [smul_eq_mul] rw [schwartzAction_mul_apply] simp only [inv_mul_cancel, map_one, one_apply_eq_self] change ∂_ μ (fun x => η (Λ⁻¹ • x)) (Λ • x) = _ rw [deriv_comp_lorentz_action] simp only [inv_smul_smul, smul_eq_mul] exact SchwartzMap.differentiable η- Project
- Physlib
- License
- Apache-2.0
- Commit
- dd43e9e65791
- Source
- Physlib/SpaceAndTime/SpaceTime/Derivatives.lean:403-442
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