We propose a new non-Hermitian chiral random matrix model that describes single-flavor spin-one Cooper pairing of quarks. For three colors the model shows spontaneous breaking of color SU ( 3 ) C and spin SO ( 3 ) J symmetries down to the diagonal SO ( 3 ) C + J subgroup, in striking analogy to the color-spin locked phase of one-flavor QCD at high density. For two colors, color-singlet spin-one diquarks condense and trigger symmetry breaking U ( 1 ) × SO ( 3 ) J → SO ( 2 ) J . In both cases the microscopic large- N limit is rigorously taken and the effective theory of Nambu-Goldstone modes is derived.
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