Entry 3614 · 2026-08-27 · marici.Figueiredo · research

Oriented Inflow Fixes the Primitive Charge, Not the Gauge Coupling

The integer incidence

$$B= \begin{pmatrix} 2&-1&0\\ 3&0&-1 \end{pmatrix}$$

has primitive kernel $\pm(1,2,3)^T$. On the kernel $q=s(1,2,3)^T$, the cubic anomaly is $36s^3$. An oriented quantized inflow $k=36$ therefore selects

$$q=(1,2,3)^T, \qquad q_3-q_2=1.$$

The reversed bulk selects the mirror orientation. Conditional on independent incidence and bulk authority, this is a genuine relational selector of charge direction, sign, and primitive normalization.

The physical portal remains $e(q_3-q_2)=e$. Positive one-loop Abelian running has no nonzero fixed point and preserves initial-coupling dependence. Wess–Zumino matching preserves total anomaly through thresholds without freezing the numerical amplitude. Physical16 descent and calibrated detector gain remain absent.

Evidence

• Packet: research/flavor/flavor-integer-incidence-anomaly-inflow-selector.md
• Checker: research/flavor/checkers/wp820_integer_incidence_anomaly_inflow_selector.py
• Generated result: research/flavor/results/wp820_integer_incidence_anomaly_inflow_selector.json
• Exact result: 22 of 22 checks passed.
• Ledger-sequence claim: seqclaim-af462cf81738b6af0120513e, value 3614.
• Graph admission: ev-000000007757-b76073f6-16ad-4bcc-9033-1458bab3dc8f.

Claim boundary

The result is conditional on a declared chiral cubic-anomaly model and independently derived incidence and oriented bulk inflow. It does not derive the continuous gauge coupling, a nonzero RG basin, numerical threshold matching, quotient descent, or a detector instrument.

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