Root space decomposition

Decomposition of a semisimple Lie algebra into a Cartan subalgebra plus root spaces for the adjoint action.
Root space decomposition

Let g\mathfrak g be a finite-dimensional complex semisimple Lie algebra (see ) and let hg\mathfrak h\subset\mathfrak g be a . For each αh\alpha\in\mathfrak h^* define the weight space

gα={Xg:[H,X]=α(H)X for all Hh}, \mathfrak g_\alpha=\{X\in\mathfrak g:[H,X]=\alpha(H)X\ \text{for all }H\in\mathfrak h\},

and let Φh\Phi\subset\mathfrak h^* be the set of nonzero α\alpha with gα0\mathfrak g_\alpha\neq 0 (the ).

The root space decomposition (sometimes called the Cartan decomposition of g\mathfrak g) is the direct sum decomposition

g  =  h    αΦgα. \mathfrak g \;=\; \mathfrak h \;\oplus\; \bigoplus_{\alpha\in\Phi}\mathfrak g_\alpha.

Conceptually, it is the simultaneous eigenspace decomposition for the commuting family of endomorphisms {ad(H)}Hh\{\mathrm{ad}(H)\}_{H\in\mathfrak h} coming from the .

Two structural bracket relations are fundamental:

  • [h,gα]gα[\mathfrak h,\mathfrak g_\alpha]\subseteq \mathfrak g_\alpha with the eigenvalue rule [H,X]=α(H)X[H,X]=\alpha(H)X;
  • [gα,gβ]gα+β[\mathfrak g_\alpha,\mathfrak g_\beta]\subseteq \mathfrak g_{\alpha+\beta} (with the convention gγ=0\mathfrak g_{\gamma}=0 if γ\gamma is not a weight), as explained in .

With the inner product induced by the , the set Φ\Phi satisfies the axioms of a . Choosing a refines this into a triangular decomposition and is the starting point for Dynkin diagram combinatorics (see ).