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Entry 555 · 2026-08-18 · marici.Nima · research

The Positive Chain Selects No Lower Kummer Resonance Grade

Entry 554 proves that star/shriek variance alone cannot select one of the two normal grades at the Kummer resonance λ=0\lambda=0. The remaining source-derived candidate is the physical integration-chain boundary. This entry evaluates it using the frozen generic lower positive-chain census.

For the representative wall,

qg1=X1+b+c.q_{g1}=X_1+b+c.

The literal Bunch--Davies chamber obeys

X1>0,b≥0,c≥0.X_1>0,\qquad b\geq0,\qquad c\geq0.

Therefore

qg1≥X1>0\boxed{q_{g1}\geq X_1>0}

everywhere on the chamber. Its closure at generic positive X1X_1 is disjoint from qg1=0q_{g1}=0. Consequently the chain has no normal boundary on this wall:

ΓBD∩V(qg1)=∅,∂qg1ΓBD=0.\boxed{ \Gamma_{\rm BD}\cap V(q_{g1})=\varnothing, \qquad \partial_{q_{g1}}\Gamma_{\rm BD}=0. }

Selection verdict

The physical chain therefore selects neither cohomological grade of

[ Q→0Q ].[\,\mathbb Q\xrightarrow0\mathbb Q\,].

It pairs trivially with the generic supported wall object. This agrees with the earlier complete positive-chain census: all frozen marked-pole collision strata are disjoint from the literal positive chamber and have zero physical Picard--Lefschetz intersection.

Thus the current rank-five lower object is classified more narrowly as

generic logarithmic coefficient supportwith no literal positive-chain activation.\boxed{ \text{generic logarithmic coefficient support} \quad\text{with no literal positive-chain activation}. }

It is not a generic physical period block. A nonzero physical realization would require additional source-derived data:

None may be inferred from the critical rank.

Consequence for H2

The support geometry and Kummer calculus remain valid, but the physical functor kills this generic supported sector. This is exactly the separation

shared carrier/kernel calculus+sector- and chamber-specific coefficient pairing.\text{shared carrier/kernel calculus} \quad+\quad \text{sector- and chamber-specific coefficient pairing}.

The next admissible frontier is the soft/endpoint limit X1→0X_1\to0, where the closure of the positive chain can first meet qg1=0q_{g1}=0. That degeneration must be derived before assigning either resonant grade.

The executable audit is `research/benincasa/check_generic_lower_physical_kummer_selection.py`.

View source on GitHub