1426 — The Physical Positive Sheet Selects the Odd Order-Nine Coefficient
Status
Exact termwise deck-parity theorem with replicated modular nonvanishing.
Uniform-sheet coefficient
On either uniform sheet, no non-total-energy radial constant cancels. Every one of the source terms therefore has -order nine.
Its leading coefficient is
where the product contains the nine non-total-energy denominator constants.
Exact complement relation
Global deck complement changes the sign of every one of those nine constants. Hence term by term
Thus
as a rational function wherever the leading coefficients are defined.
Nonvanishing samples
The complete source sum gives
and
In each field the entries are nonzero and exact negatives.
Physical sheet selection
Entry 1217 freezes the Euclidean loop chamber by
This selects sheet among the two uniform sheets. Therefore the physical relative current evaluates the anti-invariant order-nine line through the distinguished positive generator
The selection comes from the source Betti chamber, not from choosing a convenient algebraic basis or dividing an odd pair by two.
Consequence
The order-nine coefficient object and its physical readout have different types:
This explains how a deck-odd coefficient can contribute a nonzero physical mixed-Tate period without mixing with the even growth-four sector.
Next finite falsifier
Compare the positive-sheet exceptional integral of with Entry 1310’s exact mixed-Tate constant . The normalization must follow from the current and source orientation; modular nonvanishing alone does not identify the two coefficients.
Artifacts:
- research/benincasa/marici-gm/src/bin/five_site_two_normal_rees.rs
- research/benincasa/results/five-site-two-normal-rees.json
Allocator claim: seqclaim-d7706d52adf42ef8cb5f0b6b.