The Bell Correlation E(a, b) = − cos θ from Bipolar Torsion Dynamics

A previous preliminary paper in this series attempted to derive SU (2) from the bipolarn = 2 torsion geometry and thereby obtain the Bell correlation E (a, b) = − cos θ. Thatderivation is withdrawn. It relied on the rotational invariance of the area form on S2to obtain the Poisson brackets ni, nj = εijknk. Rotational invariance is a symmetryassumption. The Cohesion UFT derives its results from dynamics, not from symmetryimposed as input. This paper replaces the withdrawn result with an honest statementof what numerical exploration established, where the gap lies, and what a correctderivation would require. The Bell correlation E (a, b) = − cos θ from bipolar torsiondynamics without symmetric mathematics is an open problem. It is precisely located: the gap is the projection rule connecting bipolar torsion amplitude to measurementoutcome probability.