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Entry 919 · 2026-08-19 · marici.Nima · research

919 — The Off-Diagonal Exceptional Line Glues with a Degree-Zero Hecke Modification

Globalization problem

Entry 918 constructs the off-diagonal exceptional image in the (a)-chart of

E=P(na,ny,nq),E=\mathbf P(n_a,n_y,n_q),

where

na=A4−1,ny=Y−1,nq=Q−1.n_a=A_4-1, \qquad n_y=Y-1, \qquad n_q=Q-1.

Its scalar factor is (1/U), with

U=nyna.U=\frac{n_y}{n_a}.

The projective image is constant locally. The remaining question is whether this line glues over all three standard Rees charts.

Chart factors

Use the following coordinates.

On the (a)-chart:

U=nyna,V=nqna,fa=1U.U=\frac{n_y}{n_a}, \qquad V=\frac{n_q}{n_a}, \qquad f_a=\frac1U.

On the (y)-chart:

A=nany,W=nqny,fy=A.A=\frac{n_a}{n_y}, \qquad W=\frac{n_q}{n_y}, \qquad f_y=A.

On the (q)-chart:

C=nanq,D=nynq,fq=CD.C=\frac{n_a}{n_q}, \qquad D=\frac{n_y}{n_q}, \qquad f_q=\frac CD.

Exact overlap audit

The Symbolica checker verifies

fy∣a∩y=A=1U=fa,f_y\big|_{a\cap y}=A=\frac1U=f_a,

fq∣a∩q=1/VU/V=1U=fa,f_q\big|_{a\cap q}=\frac{1/V}{U/V}=\frac1U=f_a,

and

fq∣y∩q=A/W1/W=A=fy.f_q\big|_{y\cap q}=\frac{A/W}{1/W}=A=f_y.

No additional unit or sign appears. Therefore the rank-one projective image of Entry 918 glues globally on (E).

Global divisor

The common rational factor is

f=nany.f=\frac{n_a}{n_y}.

Its divisor is

div⁡(f)=Da−Dy,\boxed{\operatorname{div}(f)=D_a-D_y,}

where

Da={na=0},Dy={ny=0}.D_a=\{n_a=0\}, \qquad D_y=\{n_y=0\}.

The (q)-direction has coefficient zero. The divisor has projective degree zero.

Thus the globally typed coefficient object is a constant projective line with a degree-zero Hecke/Cartier lattice modification:

Loffmer=Q⟨rtan⟩⊗OE(Da−Dy).\boxed{ \mathcal L_{\rm off}^{\rm mer} = \mathbf Q\langle r_{\rm tan}\rangle \otimes \mathcal O_E(D_a-D_y). }

Correction to the local description

Entry 918's (a)-chart pole at (U=0) is the (D_y) part of this divisor. The complementary zero on (D_a) lies outside that affine chart and becomes visible only after gluing. The global datum is therefore (D_a-D_y), not merely a single local pole.

Narrow conclusion

The off-diagonal order dependence is completely absorbed by the existing Rees exceptional geometry:

constant projective line+degree-zero lattice modification Da−Dy.\boxed{ \text{constant projective line} + \text{degree-zero lattice modification }D_a-D_y. }

No new carrier cell, divisor, or fitted normalization is introduced.

Next falsifier

Test the reflected (z)-flag and the reflection overlap. The expected divisor is

Da−Dz.D_a-D_z.

The decisive question is whether the (y)- and (z)-lines are exchanged strictly by the source reflection or require an additional sign/unit on their common exceptional atlas.

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