We know that the the roots of $\mathbb{g} = sl(3,C)$ under the adjoint action are
given by $L_i - L_j$ where $L_i (diag(a_1, a_2, a_3))=a_i$ for $i = 1,2,3$.
If $V$ is any irreducible representation of $sl(3,C)$, then clearly $V$ is the direct sum of its simultaneous eigenspaces given by $V_\beta$ = { $v \in V$ : $H.v$ = $\beta(H)v$ $\forall$ H $\in \mathbb{h}$ } where $\mathbb{h}$ is the subalgebra of diagonal matrices in $sl(3,C)$.In this case, $\beta$ is called the eigenvalue for the representation $V$. If $X$ $\in \mathbb{g_{\alpha}}$ and $v \in V_{\beta}$, then we know that
$\mathbb{g_{\alpha}}$ carries $V_{\beta}$ to $V_{\alpha + \beta}$
where $\mathbb{g_{\alpha}}$ = $\{ X_{\alpha} \in sl(3,C) : adH(X_{\alpha}) = \alpha(H) X_{\alpha} \forall H \in \mathbb{h}\}$.
I want to now show that the eigenvalues $\alpha$ occuring in the representation $V$ differ from one another by integral linear combinations of the vectors $L_i - L_j \in \mathbb{h^*}$.
Note - $adH(X) = [H,X] = HX - XH$.
Thanks for any help.
2026-05-04 21:23:46.1777929826