Manuscript XIV-G@1 · XIV-G.tex · section · 791c6644

Negative freeze

G1: operator and pullback calculus without a common phase › Negative freeze · lines 914–924

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There is no cutoff of , restoring limit, characteristic subtraction, new contact class, or change of propagator.

The tangent defect is not renamed as an excess fiber. The fourteen-dimensional image of is not used as a Lagrangian relation in . No branch numerator is promoted to a joint section.