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We propose a new non-Hermitian chiral random matrix model that describessingle-flavor spin-one Cooper pairing of quarks. For three colors the modelshows spontaneous breaking of color $\mathrm{SU}(3)_C$ and spin$\mathrm{SO}(3)_J$ symmetries down to the diagonal $\mathrm{SO}(3)_{C+J}$subgroup, in striking analogy to the color-spin locked phase of one-flavor QCDat high density. For two colors, color-singlet spin-one diquarks condense andtrigger symmetry breaking $\mathrm{U}(1) \times \mathrm{SO}(3)_J \to\mathrm{SO}(2)_J$. In both cases the microscopic large-$N$ limit is rigorouslytaken and the effective theory of Nambu-Goldstone modes is derived.

Chiral random matrix theory for single-flavor spin-one Cooper pairing