Admissibility frontier · Edition 3

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The free-Majorana relation-defect operator is fixed

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corpus/programmes/moonshine-program-lattice/relation-defect-free-majorana-multiplier.md
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Why this page is here: the shortest known corpus-link route from an Edition 3 source is:

  1. The robust phase target is relative, not absolute
  2. The free-Majorana relation-defect operator is fixed

The free-Majorana relation-defect operator is fixed

Date: 25 October 2026

Status: complete for the reduced free-Majorana characteristic action and eta normalization; subsequent Arf conjugation fixes the compensating Baby-Monster multiplier

Evidence: machine-readable multiplier ledger

Certificate: word-composition verifier

Result

The corpus's existing first-handle \(T_1/S_1\) phase rules are sufficient to compute the free-Majorana part of the relation-defect operator. The explicit integral lift has the word

\[ R=S\,T^{-5}S\,T^{-3}S\,T^{-2}S^3T^4, \]

and

\[ K=S^2R^{-11}. \]

Composing the certified reduced theta-characteristic actions gives the following result on each of the three 3-cycles:

\[ \text{edge exponents }(3,6,1)\pmod8, \qquad \text{cycle product } \zeta_8^{10}=\zeta_8^2=i. \]

The fixed odd--odd characteristic has reduced eigenphase \(\zeta_8^2=i\) as well.

The common Dedekind eta multiplier contributes \(v_\eta(K)=i=\zeta_8^2\) to every sector. With that normalization, each 3-cycle has total product

\[ i\cdot i^3=1, \]

while the fixed odd--odd sector has eigenvalue

\[ i\cdot i=-1. \]

Thus the eta-normalized free-Majorana operator has the exact spectral form

\[ \boxed{ \rho_{\mathrm{free}}(K): \quad 3\text{ cycles with product }1, \quad 1\text{ fixed sector with eigenvalue }-1. } \]

Its determinant on the ten even-characteristic sectors is \(-1\).

1. Exact monomial action

Using the characteristic ordering in the seam-permutation audit, the reduced action is

sourcetargetexponent of \(\zeta_8\)
\(00\mid00\)\(00\mid10\)3
\(00\mid10\)\(10\mid00\)6
\(10\mid00\)\(00\mid00\)1
\(00\mid01\)\(00\mid11\)3
\(00\mid11\)\(10\mid01\)6
\(10\mid01\)\(00\mid01\)1
\(01\mid00\)\(01\mid10\)3
\(01\mid10\)\(11\mid00\)6
\(11\mid00\)\(01\mid00\)1
\(11\mid11\)\(11\mid11\)2

Adding the common eta exponent \(2\) produces normalized edge exponents \((5,0,3)\) on each 3-cycle and exponent \(4\) on the fixed sector.

This is invariantly summarized by the closed-cycle products and fixed-sector eigenvalue; diagonal rephasings of individual sectors cannot change them.

2. Why this is more than the permutation

The bare permutation has sign \(+1\), so the determinant quotient misses \(K\). The reduced phase matrix also has determinant \(+1\): its total exponent is zero modulo eight. The eta normalization changes the ten-sector determinant to

\[ i^{10}=-1. \]

The lost sign is therefore restored only after retaining the metaplectic anomaly line. This is a literal example of the corpus's admissibility rule: the label permutation and phase extension are separately insufficient, while their joined operator has a new invariant.

3. The remaining Monster gate

The \(2A\) fermionization splits into a free Majorana--Weyl factor and a fermionic Baby-Monster factor. This calculation completes only the free factor. Let the unknown Baby-Monster action on the same cycles be \(\rho_{\mathrm{Baby}}(K)\). The complete \(2A\) seam requires

\[ \rho_{2A}(K) =\rho_{\mathrm{free}}(K)\otimes\rho_{\mathrm{Baby}}(K) \]

with compatible anomaly trivialization and separating degeneration.

The subsequent Arf-conjugation calculation fixes this multiplier to the edgewise inverse of the free action. What remains source-gated is the genus-two fermionic Baby-Monster amplitude vector, or an equivalent sewn defect module, carrying that multiplier and satisfying the required degeneration.

Boundary

The result is exact for the reduced free-Majorana \(T_1/S_1\) conventions and the declared eta normalization. It is not yet the full Monster \(2A\) multiplier, a \(2B\) Leech-seam result, or a physical detector prediction.

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