To Field Strength bare Gradient ne zero
Electromagnetism.ElectromagneticPotential.toFieldStrength_bareGradient_ne_zero
Project documentation
The field strength of the bare-gradient potential B^μ := ∂_μ χ for χ(x) = x⁰·xⁱ is nonzero (follows from fieldStrengthMatrix_bareGradient_inl_inr).
Exact Lean statement
lemma toFieldStrength_bareGradient_ne_zero {d : ℕ} (i : Fin d)
(x : SpaceTime d) :
let χ : SpaceTime d → ℝFormal artifact
Lean source
lemma toFieldStrength_bareGradient_ne_zero {d : ℕ} (i : Fin d) (x : SpaceTime d) : let χ : SpaceTime d → ℝ := fun y => y (Sum.inl 0) * y (Sum.inr i) let B : ElectromagneticPotential d := ⟨fun y μ => ∂_ μ χ y⟩ B.toFieldStrength x ≠ 0 := by intro χ B h have h2 := fieldStrengthMatrix_bareGradient_inl_inr i x dsimp only at h2 rw [fieldStrengthMatrix_eq, h] at h2 have h3 : ((Lorentz.CoVector.basis.tensorProduct Lorentz.Vector.basis).repr (0 : Lorentz.CoVector d ⊗[ℝ] Lorentz.Vector d)) = 0 := map_zero _ erw [h3, Finsupp.zero_apply] at h2 norm_num at h2- Project
- Physlib
- License
- Apache-2.0
- Commit
- dd43e9e65791
- Source
- Physlib/Electromagnetism/Kinematics/GaugeTransformation.lean:395-407
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