2701 — The Canonical Rank-Twenty-Six Source Derivative Is Fixed Coefficientwise
Frozen source
Write the coefficient of the five-pole source form as
The canonical first-order source extension in external direction (j) is obtained without choosing a quotient representative:
Exact coefficient audit
The complete unspecialized formulas give:
- in the (x)-direction, (partial_xN=-1), with marked-pole derivatives on (q_{\mathcal G_2}) and (q_{\mathcal G_{23}});
- in the (y)-direction, (partial_yN=-1), with marked-pole derivatives on (q_{\mathcal G_1}) and (q_{\mathcal G_{31}});
- in the (z)-direction, (partial_zN=0), with marked-pole derivatives on (q_{\mathcal G_1},q_{\mathcal G_2},q_{\mathcal G_3}).
Symbolic differentiation verifies that (K_{\rm CM}) has total degree (6), every (q_i) and (N) has degree (1), and their derivatives have degrees (5) and (0), respectively.
The source coefficient has weight
Including (da\wedge db) gives source-form weight (28). Every canonical external derivative has coefficient weight (25), hence form weight (27).
Result
The dual-number coefficient required by Entry 2697 is now fixed term-by-term by the frozen source. It is not selected by the desired Euler recurrence, by sparsity, or by a quotient section.
This establishes the characteristic-zero source derivative but not yet its equality with the finite de Rham connection implementation.
Artifacts
research/benincasa/check_rank26_canonical_source_derivative.pyresearch/benincasa/rank26-canonical-source-derivative.json
Run the checker with:
uv run --with sympy python research/benincasa/check_rank26_canonical_source_derivative.py
Next falsifier
Insert the canonical coefficient derivatives into the complete finite presentation and verify in all three directions that
after quotient reduction. A mismatch would localize the failure in the finite Gauss--Manin adapter rather than in source homogeneity.