Definition

For u,vC3u,v\in\mathbb C^3, their conjugated cross product is

u×v=u×v,u\mathbin{\overline\times}v=\overline{u\times v},

where u×vu\times v is the usual coordinate cross product extended complex-bilinearly and the bar denotes componentwise complex conjugation. Equivalently,

(u×v)i=j,k=13εijkujvk.(u\mathbin{\overline\times}v)_i =\sum_{j,k=1}^{3}\varepsilon_{ijk}\,\overline{u_j}\,\overline{v_k}.
Linearity and orthogonality

The operation is real-bilinear and conjugate-linear in each argument over C\mathbb C:

(λu)×v=λ(u×v),u×(λv)=λ(u×v).(\lambda u)\mathbin{\overline\times}v =\overline\lambda\,(u\mathbin{\overline\times}v), \qquad u\mathbin{\overline\times}(\lambda v) =\overline\lambda\,(u\mathbin{\overline\times}v).

It is alternating. With the Hermitian inner product convention

u,v=i=13uivi,\langle u,v\rangle=\sum_{i=1}^{3}\overline{u_i}v_i,

one has

u,u×v=v,u×v=0\langle u,u\mathbin{\overline\times}v\rangle =\langle v,u\mathbin{\overline\times}v\rangle=0

and the norm identity

u,v2+u×v2=u2v2.|\langle u,v\rangle|^2 +\lVert u\mathbin{\overline\times}v\rVert^2 =\lVert u\rVert^2\lVert v\rVert^2.
Why the conjugation is present

The ordinary complex-bilinear cross product naturally takes values in the dual representation: for gSL(3,C)g\in SL(3,\mathbb C),

(gu)×(gv)=gT(u×v).(gu)\times(gv)=g^{-T}(u\times v).

For gSU(3)g\in SU(3), one has gT=g\overline{g^{-T}}=g. Componentwise conjugation therefore turns the output into the defining representation, so

g(u×v)=(gu)×(gv)(gSU(3)).g(u\mathbin{\overline\times}v) =(gu)\mathbin{\overline\times}(gv) \qquad(g\in SU(3)).

This equivariance is precisely what makes the compatible with the standard SU(3)SU(3)-action.

Convention warning

The bar is part of the operation, not decoration. Omitting it produces a different map and breaks the displayed SU(3)SU(3)-equivariance in the defining representation. The inner product convention is also important: here it is conjugate-linear in the first argument and linear in the second.

References
  1. John C. Baez and Paul Schwahn, “The Standard Model Gauge Group from the Exceptional Jordan Algebra,” 2026. arXiv:2606.15235. Relevant: §2, especially Lemma 3.
  2. John C. Baez, “Octonions and the Standard Model (Part 2),” 2020. The n-Category Café. Relevant: the Hermitian cross product and CC3\mathbb C\oplus\mathbb C^3 multiplication convention.