To Field Strength action eq sum
Electromagnetism.ElectromagneticPotential.toFieldStrength_action_eq_sum
Project documentation
This lemma expresses the component form of the transformed field strength tensor: when a Lorentz transformation Λ acts on the potential A, the resulting field strength tensor's components are given by the standard tensor transformation rule involving the Lorentz matrix elements Λ^μ_κ and Λ^ν_ρ applied to the original field components.
Exact Lean statement
lemma toFieldStrength_action_eq_sum {d} (A : ElectromagneticPotential d) (Λ : LorentzGroup d)
(hf : Differentiable ℝ A) (x : SpaceTime d) :
(Λ • A).toFieldStrength x = ∑ μ, ∑ ν,
(∑ κ, ∑ ρ, Λ.1 μ κ * Λ.1 ν ρ * toField {A.toFieldStrength (Λ⁻¹ • x) | [κ] [ρ]}ᵀ) •
Vector.basis μ ⊗ₜ[ℝ] Vector.basis νFormal artifact
Lean source
lemma toFieldStrength_action_eq_sum {d} (A : ElectromagneticPotential d) (Λ : LorentzGroup d) (hf : Differentiable ℝ A) (x : SpaceTime d) : (Λ • A).toFieldStrength x = ∑ μ, ∑ ν, (∑ κ, ∑ ρ, Λ.1 μ κ * Λ.1 ν ρ * toField {A.toFieldStrength (Λ⁻¹ • x) | [κ] [ρ]}ᵀ) • Vector.basis μ ⊗ₜ[ℝ] Vector.basis ν := by conv_lhs => rw [toFieldStrength_equivariant A Λ hf x, toFieldStrength_eq_sum_basis_eval] change Tensorial.smulLinearMap _ _ = _ simp only [map_sum, map_smul] simp [smulLinearMap, smul_prod, Vector.smul_basis, tmul_sum, sum_tmul, Finset.smul_sum, tmul_smul, smul_tmul, smul_smul] conv_lhs => enter [2, μ, 2, ν]; rw [Finset.sum_comm] conv_lhs => enter [2, μ]; rw [Finset.sum_comm] rw [Finset.sum_comm] refine Finset.sum_congr rfl (fun ν _ => ?_) conv_lhs => enter [2, μ]; rw [Finset.sum_comm] rw [Finset.sum_comm] refine Finset.sum_congr rfl (fun μ _ => ?_) simp [← Finset.sum_smul] congr 1 exact Finset.sum_congr rfl (fun κ _ => Finset.sum_congr rfl (fun κ _ => by ring))- Project
- Physlib
- License
- Apache-2.0
- Commit
- dd43e9e65791
- Source
- Physlib/Electromagnetism/Kinematics/FieldStrength.lean:214-233
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