For the usual colour SU(3) fixing the fourth coordinate of the SU(4) defining representation,
Taking the exterior square gives
The identification follows by contracting an antisymmetric tensor with the invariant three-index Levi-Civita symbol. Combining this with c gives all colour multiplets:
A colour triplet has the color charge transformation law of a quark, an antitriplet that of an antiquark, and a colour singlet is colour-neutral, as a lepton is. Thus both parent representations permit quark-like and antiquark-like colour sectors; the vector has one neutral sector and the spinor two. These are colour assignments only. They do not determine particle spin, statistics, electric charge, weak quantum numbers or a full generation of the Standard Model. In a real parent field the conjugate colour sectors may describe one complex colour field and its conjugate, rather than independent particle species.
Global group qualification. The printed chain is correct at the Lie algebra level, . Globally its simply connected form is . The standard map of SU(4) into through has a nontrivial kernel: the concrete central element acts as on and trivially on the singlet representation. Its image is , rather than an injective copy of SU(4) under this map.
The global form obstruction for the Spin7 spinor is explicit: the central element of the Spin group maps to the identity in but acts as on the eight-dimensional spin representation. Equivalently acts as on both and in its restriction. Therefore the spinor does not descend to a genuine SO(7) group representation. A theory containing that spinor needs the Spin group global form, or must understand the source's notation as specifying only its Lie algebra. The displayed colour branchings remain valid with this correction.

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