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Project-declaredLean 4.32.0 · mathlib@81a5d257c8e4

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 → ℝ

Formal artifact

Lean source

Canonical source
Full Lean sourceLean 4
lemma toFieldStrength_bareGradient_ne_zero {d : } (i : Fin d)    (x : SpaceTime d) :    let χ : SpaceTime d   := 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 ⊗[] 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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