We ask what it means, precisely, for the quantum curvature representation space at a spin network vertex to be compatible with classical general relativity. Requir-ing (i) that the spin-2 gravitational degrees of freedom are present, and (ii) that no curvature representations of spin k > 2 appear—together constituting a condition ofclassical curvature compatibility—we prove that the curvature representation space Hcurv(j) = V1 ⊗ Vj satisfies both conditions for a unique value: j = 1. The uniquenessis non-trivial: it was not a priori guaranteed that any j would satisfy both conditions simultaneously, nor that exactly one would. The result establishes j = 1 as the uniquekinematically admissible vacuum edge label under classical curvature compatibility, recovering the adjoint representation of the classical Ashtekar–Barbero connection as the unique kinematically admissible choice. This provides a kinematic foundation for the role of j = 1 in spin foam models and complements semiclassical analyses that recover Regge gravity from EPRL vertex amplitudes in the large-spin limit.
John van Hemert (Tue,) studied this question.
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