We prove that the spin-1 (adjoint) representation is the unique SU(2) representation j for which the curvature representation space V₁ ⊗ Vⱼ at a 4-valent vertex in loop quantum gravity (LQG) (i) contains the spin-2 representation, and (ii) contains no representation of spin greater than 2. The proof is a direct application of the Clebsch–Gordan decomposition. We discuss the physical motivations for these conditions, emphasizing their role in ensuring compatibility with the spin-2 gravitational degrees of freedom and the classical structure of the Ashtekar–Barbero curvature. This result recovers the adjoint representation carried by the classical Ashtekar–Barbero connection and provides a kinematic rationale for preferring low-spin representations in dynamical studies of LQG. This uniqueness provides a representation-theoretic foundation for the role of low-spin vacuum states in spin foam models, complementing semiclassical analyses that recover Regge gravity from vertex amplitudes.
John van Hemert (Tue,) studied this question.
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