Let g\mathfrak g be a split over a characteristic-zero field, with split t\mathfrak t, Φ\Phi, and Δ={α1,,α}\Delta=\{\alpha_1,\ldots,\alpha_\ell\}. A Chevalley basis is

{h1,,h}{eα}αΦ,\{h_1,\ldots,h_\ell\}\cup\{e_\alpha\}_{\alpha\in\Phi},

where hih_i represents the and eαe_\alpha spans gα\mathfrak g_\alpha, normalized so that

[hi,eα]=α,αieα,[eα,eα]=hα,[h_i,e_\alpha] = \langle\alpha,\alpha_i^\vee\rangle e_\alpha, \qquad [e_\alpha,e_{-\alpha}]=h_\alpha,

and

[eα,eβ]=Nα,βeα+β[e_\alpha,e_\beta] = N_{\alpha,\beta}e_{\alpha+\beta}

when α+β\alpha+\beta is a root, with Nα,βZN_{\alpha,\beta}\in\mathbb Z.

Root-string normalization

The root-vector signs can be chosen so that

Nα,β=±(p+1),N_{\alpha,\beta}=\pm(p+1),

where pp is the largest nonnegative integer such that βpαΦ\beta-p\alpha\in\Phi. The sign choices are not canonical, but the existence of integral structure constants is.

Integral Lie form

The Z\mathbb Z-span

gZ=iZhiαΦZeα\mathfrak g_{\mathbb Z} = \bigoplus_i\mathbb Zh_i \oplus \bigoplus_{\alpha\in\Phi}\mathbb Ze_\alpha

is closed under the bracket. It is the Chevalley Lie form. Constructing integral representations and a scheme additionally uses divided powers and the full root datum; see the .

Role in the letter

Root-vector normalization rigidifies the and gives integral structures from which almost-all local integral models and can be obtained.

References
  1. Claude Chevalley, “Sur certains groupes simples,” Tohoku Mathematical Journal 7 (1955), 14–66.
  2. Robert Steinberg, Lectures on Chevalley Groups, AMS, 2016.