Core idea

For an idempotent ee in a JJ, the Peirce-one corner is

J1(e)={x∈J:e∘x=x}.J_1(e)=\{x\in J:e\circ x=x\}.

It is a of JJ, and ee is its unit. Notice that the defining equation is e∘x=xe\circ x=x, not e∘x=1e\circ x=1.

Hermitian 33-by-33 case

Let K\mathbb K be one of the normed real division algebras R,C,H,O\mathbb R,\mathbb C,\mathbb H,\mathbb O, and let J=H3(K)J=H_3(\mathbb K). If ℓ∈J\ell\in J is an idempotent of matrix trace 22, then

J1(ℓ)≅H2(K)J_1(\ell)\cong H_2(\mathbb K)

as a unital Jordan algebra. After an automorphism takes ℓ\ell to E11+E22E_{11}+E_{22}, this corner consists exactly of matrices

(αx0x∗β0000),α,β∈R,x∈K.\begin{pmatrix} \alpha&x&0\\ x^*&\beta&0\\ 0&0&0 \end{pmatrix}, \qquad \alpha,\beta\in\mathbb R,\quad x\in\mathbb K.

Conversely, every of H3(K)H_3(\mathbb K) isomorphic to H2(K)H_2(\mathbb K) is J1(ℓ)J_1(\ell) for a unique trace-two idempotent ℓ\ell: namely, the unit of that subalgebra viewed inside JJ.

References
  1. John C. Baez and Paul Schwahn, “The Standard Model Gauge Group from the Exceptional Jordan Algebra,” 2026, Lemmas 7–10. arXiv:2606.15235.
  2. Nathan Jacobson, Structure and Representations of Jordan Algebras, American Mathematical Society, 1968, Chapter III, §1. Publisher record.