Statement

For a labeled defining weight wkw_k in the , let

Φk={rΦ(E7):π(r)=±wk},Nk:=rΦk(e7)r.\Phi_k=\{r\in\Phi(E_7):\pi(r)=\pm w_k\}, \qquad N_k:=\bigoplus_{r\in\Phi_k}(\mathfrak e_7)_r.

Then NkN_k is a 3030-dimensional sl6SM\mathfrak{sl}_6^{\mathrm{SM}}-submodule of the adjoint e7\mathfrak e_7-module, and

NkΛ2C6Λ4C6N_k\cong \Lambda^2\mathbb C^6\oplus\Lambda^4\mathbb C^6

as sl6SM\mathfrak{sl}_6^{\mathrm{SM}}-modules, where the summands are .

This is a and vector-space decomposition. In general NkN_k is not a of e7\mathfrak e_7.

Restriction to the standard sl5

Using the defining-module splitting C6C5C\mathbb C^6\cong\mathbb C^5\oplus\mathbb C, restriction to gives

NkΛ1C5Λ2C5Λ3C5Λ4C5.N_k\cong \Lambda^1\mathbb C^5 \oplus\Lambda^2\mathbb C^5 \oplus\Lambda^3\mathbb C^5 \oplus\Lambda^4\mathbb C^5.

The formula follows from the and its degree decomposition.

Standard Model interpretation

On restriction to gSM\mathfrak g_{\mathrm{SM}}, this is the with the degree-zero and degree-five singlets omitted. These two missing one-dimensional summands are the right-handed neutrino and its antiparticle, both . Adding the two generation-root spaces produces the .

Dependence on choices and conventions

The three spaces NkN_k require a compatible and a labeling of the three defining weights. Reversing highest-weight conventions exchanges Λ2C6\Lambda^2\mathbb C^6 with its dual Λ4C6\Lambda^4\mathbb C^6; their direct sum is unaffected. The particle/antiparticle and chirality labels additionally depend on the chosen Standard Model representation conventions.

References
  1. John C. Baez, “Three Generations in E7,” 2026, Lemma 9 and Theorem 10. arXiv:2608.06271.
  2. John C. Baez and John Huerta, “The Algebra of Grand Unified Theories,” Bulletin of the American Mathematical Society 47 (2010), 483–552, especially the exterior-algebra description of fermions. arXiv:0904.1556.