Manuscript Em02-E@1 · Em02-E-v1.tex · section · f3795050

A quadratic coefficient is not separately the full gauge identity

Classical covariance and the quadratic kernel bridge › A quadratic coefficient is not separately the full gauge identity · lines 988–1002

Em02-E@1#eq:classical-Ward

For a compact vector field $ξ$ , put

K ξ = (L_{ξ} g_{0}, L_{ξ} ϕ_{0}) .

Classical invariance implies

L_{f} (K ξ) = 0, ⟨ H_{f}, η \otimes K ξ ⟩ + L_{f} (L_{ξ} η) = 0.

Displayed formulas in this passage

Em02-E@1#eq:classical-Ward · line 995
$L_{f} (K ξ) = 0, ⟨ H_{f}, η \otimes K ξ ⟩ + L_{f} (L_{ξ} η) = 0.$
unlabeled · line 991
$K ξ = (L_{ξ} g_{0}, L_{ξ} ϕ_{0}) .$