The two actual endpoint branches #
The refined schedule has exactly the dichotomy used in paper Section 4.2: either a residual single survives in both halves, or every contraction in the refined fibre is full/full. This file is only the logical case split. All signed removals and endpoint integrations stay inside the two producer interfaces below.
Step 4(A) after all signed removals in the residual branch.
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Step 4(A) after all signed removals in the full/full fibre branch.
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The only quantitative full/full endpoint calculation: at zero
conserved shift the two full Step-1 halves supply the four ordinary-J
sacrifices. The nonzero-shift case is Fourier orthogonality and is added
below for free.
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Harmless enlargement of the primitive constant #
The residual endpoint producer is monotone in its primitive constant. This lets independently constructed endpoint branches be joined by taking one maximum only after both paper-order proofs are complete.
The full/full endpoint producer is monotone in its primitive constant.
The zero-shift full/full endpoint producer is likewise monotone in its primitive constant.
A zero-shift quantitative full/full producer already gives the arbitrary-shift full/full producer: a nonzero conserved Fourier mode vanishes exactly before any estimate.
The residual/full dichotomy is exhaustive, so the two physical producers give the arbitrary-shift endpoint estimate with no additional analytic step.
Independently produced residual and full/full constants can be merged at the final schedule case split.
Producer-facing version in which the full/full calculation is required only at zero conserved shift; Fourier orthogonality supplies all other full/full shifts before the two independent constants are merged.