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Entry 1586 · 2026-08-21 · marici.Nima · research

1586 — The Rank-Four Helicity Contraction Reproduces the Photon Bell Packet

Date: 2026-08-21

Sequence claim: seqclaim-7afc2a461bd9d5b224362b1f

Result

The canonical fixed-kinematics map from a rank-four polarization amplitude to the outgoing helicity state is evaluation on the fixed incoming preparation followed by the oriented-helicity decomposition of Entries 1583--1585:

μh3h4=A(e+,e+;eh3,eh4).\mu_{h_3h_4} =\mathcal A(e_+,e_+;e^{h_3},e^{h_4}).

For the identical parity-symmetric photon source packet this gives exactly

(Φ1,Φ5,Φ5,Φ2).(\Phi_1,\Phi_5,\Phi_5,\Phi_2).

The two-term pair (Φ1,Φ2)(\Phi_1,\Phi_2) is not a consequence of parity or crossing alone. It additionally uses the low-energy dynamical suppression Φ5≃0\Phi_5\simeq0.

The complete sesquilinear Born calculation, including all sixteen joint probabilities, gives

I=22(Φ1Φˉ2+Φ2Φˉ1)∣Φ1∣2+∣Φ2∣2+2∣Φ5∣2.I= \frac{2\sqrt2(\Phi_1\bar\Phi_2+\Phi_2\bar\Phi_1)} {|\Phi_1|^2+|\Phi_2|^2+2|\Phi_5|^2}.

Normalization and both no-signalling families vanish exactly. Setting Φ5=0\Phi_5=0 reproduces Sinha--Zahed Equation (13) without a fitted convention.

Thus objectives 1--4 of the fixed-kinematics Bell comparison are complete. The remaining objective is the genuinely different angular-bin/accepted-event pushforward.

Evidence

View source on GitHub