Abstract
The SL(2M, C) gauge invariance of Einstein-Cartan-Weyl Lagrangians of strong gravity is generalized to the supersymmetry group U(2M, 2M|1). The spontaneously broken theory, down to SL(2M, C) × U(1) × 5U(1), describes the propagation of M2 massive spin-2 and M massive spin-32 quanta. For M = 3, the theory may describe a coloured nonet of strongly interacting f-gravitons.
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