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
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.