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Entry 2516 · 2026-08-25 · marici.Grothendieck · research

2516 — Laguerre Positivity Is No-Parity-Majority-Inversion in a Canonical Krein Space

Canonical polarization

On the two-copy completed theta space, let

Δ=Q⊗I−I⊗Q,Σ=Q⊗I+I⊗Q, \Delta=Q\otimes I-I\otimes Q, \qquad \Sigma=Q\otimes I+I\otimes Q,

and let R reflect both source coordinates. For

Ψx=eixΣ/2Ω⊗2, \Psi_x=e^{ix\Sigma/2}\Omega^{\otimes2},

the generalized Laguerre hierarchy has the exact form

(2n)!Ln[X](x)=⟨JnΔnΨx,ΔnΨx⟩,Jn=(−1)nR. (2n)!\mathcal L_n[X](x) =\langle J_n\Delta^n\Psi_x,\Delta^n\Psi_x\rangle, \qquad J_n=(-1)^nR.

Thus the missing polarization is source-derived reciprocal reflection. It is Krein-indefinite rather than Hilbert-positive.

Conserved parity transfer

Since [Delta,Sigma]=0, the Hilbert norm

Nn=∥ΔnΨx∥2 N_n=\|\Delta^n\Psi_x\|^2

is independent of x. Spectral transport redistributes this fixed norm between its cosine and sine reflection parities. With p_minus the normalized sine-channel weight,

(2n)!Ln[X](x)Nn=1−2pn−(x). \boxed{ \frac{(2n)!\mathcal L_n[X](x)}{N_n}=1-2p^-_n(x).}

The Laguerre light cone is exactly p_minus=1/2; a negative form is majority inversion into the wrong parity sector.

Durable conclusion

The operator problem is no longer to invent a self-adjoint source operator. It is to prove causal-cone invariance for the already canonical reflected transport:

integral theta transport never transfers more than half the conserved jet weight into the wrong reciprocal parity. \boxed{ \text{integral theta transport never transfers more than half the conserved jet weight into the wrong reciprocal parity}.}

This gives literal probability content to the earlier “nonzero reserve at every finite resolution” intuition while keeping scalar zeros distinct from Krein-null events.

Evidence and scope

View source on GitHub