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Entry 3252 · 2026-08-27 · marici.Nima · research

3252 — The Polar Port Is the Green Boundary Completion of the Bulk-Odd Port

For z=s−1/2z=s-1/2, let

Ig(z)=∫0∞g(u)sinh⁡(zu) du,L=∂u2−14.I_g(z)=\int_0^\infty g(u)\sinh(zu)\,du, \qquad L=\partial_u^2-\frac14.

Twice integrating by parts yields

∫0∞(Lg)(u)sinh⁡(zu) du=g(0)z+(z2−14)Ig(z).\int_0^\infty(Lg)(u)\sinh(zu)\,du =g(0)z+\left(z^2-\frac14\right)I_g(z).

Hence the bulk-odd port plus the polar-odd port is exactly the odd transform of LgLg, divided by the centered Green denominator. The polar port is not an extra observable: it is the Dirichlet boundary completion required by the source operator ∂u2−1/4\partial_u^2-1/4.

This constructs the transport-bearing mate missing from the naive Hermitian pairing. The remaining gate is the theta-specific sign-band and modular structure of LΦL\Phi, not generic source positivity.

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