 Chevalley basis

A Chevalley basis of a complex semisimple Lie algebra consists of suitable coroot elements and one vector $e_{\alpha }$ in each root space, chosen so all Lie bracket structure constants are integers. In particular $[e_{\alpha },e_{\beta }]=N_{\alpha ,\beta }{e}_{\alpha +\beta }$ when the sum is a root, with $N_{\alpha ,\beta }=\pm (p+1)$ where $\beta -p\alpha$ is the last negative-direction root in the root string. For independent roots with no root sum the bracket is zero. The integral lattice makes reduction to other fields possible.

A Chevalley basis is a particular kind of basis for the root system associated with a semisimple Lie algebra. It provides a way to represent elements of the Lie algebra that are closely related to the algebra's structure and the geometry of its representation theory.