The real Lie algebra of the unitary group is , of real dimension . Differentiating unitarity gives necessity; exponentiating any skew-Hermitian matrix gives a curve in the group, proving sufficiency.
The real Lie algebra of the special unitary group consists of traceless skew-Hermitian matrices. Differentiating unitarity and determinant one gives the two constraints; exponentiating any such matrix proves their sufficiency. The commutator is again skew-Hermitian and traceless. Its real dimension is , and its complexification is .
With the defining two-dimensional matrix trace and inner product , the displayed Pauli matrix basis is orthonormal. The Pauli matrix multiplication law gives the indicated structure constants of a Lie algebra. With the alternative form , the orthonormal basis is and the structure constant is one. The bracket and inner-product normalizations must be kept consistent in projected gauge-field formulas.
The compact real Lie algebra consists of traceless anti-Hermitian matrices. Physicists often specify Hermitian generators instead, so the genuine Lie algebra elements are . The compact real algebra and its complexification should be distinguished.
Each root of the SU(3) Lie algebra defines an SU(2) Lie algebra generated by and in the root-length-one convention. They obey and . These subalgebras explain root strings, Weyl group reflections and the integer Dynkin labels of highest weights.
// Target: lie-theory.bigb
A real basis of the unitary Lie algebra is , and for , where are matrix units. These separately span the imaginary diagonal and real and imaginary upper off-diagonal entries.

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