# Ch. 8: Root space decompositions (Friday, September 23) :::{.remark} Recall that the relations from last time can produce an infinite-dimensional module with basis $\ts{v_0,v_1,\cdots}$. Note that if \( m\in \ZZ_{\geq 0} \), then \( x.v_{m+1} = ( \lambda- m ) v_m = 0 \). This says that one can't raise $v_{m+1}$ back to $v_m$, so $\ts{v_{m+1},v_{m+2} \cdots}$ spans a submodule isomorphic to $M(-m-2)$. Quotienting yields $L(m) \da M(m) / M(-m-2)$, also called $V(m)$, spanned by $\ts{v_0, \cdots, v_m}$. Note that $M(-m-2)$ and $L(m)$ are irreducible. ::: :::{.remark} Let $L\in \Lie\Alg\slice\CC^{\fd, \ss}$ for this chapter. ::: ## 8.1: Maximal toral subalgebras and roots :::{.remark} Let $L\ni x = x_s + x_n \in L + L$ be the abstract Jordan decomposition. then if $x=x_n$ for every $x\in L$ then $L$ is nilpotent which contradicts Engel's theorem. Thus there exists some $x=x_s\neq 0$. ::: :::{.definition title="Toral subalgebras"} A **toral subalgebra** is any nonzero subalgebra spanned by semisimple elements. ::: :::{.example title="?"} The algebraic torus $(\CC\units)^n$ which has Lie algebra $\CC^n$, thought of as diagonal matrices. ::: :::{.lemma title="?"} Let $H$ be a maximal toral subalgebra of $L$. Any toral subalgebra $H \subseteq L$ is abelian. ::: :::{.proof title="?"} Let $T \leq L$ be toral and let $x\in T$ be a basis element. Since $x$ is semisimple, it STS $\ad_{T, x} = 0$. Semisimplicity of $x$ implies $\ad_{L, x}$ diagonalizable, so we want to show $\ad_{T, x}$ has no non-zero eigenvalues. Suppose that there exists a nonzero $y\in T$ such that $\ad_{T, x}(y) = \lambda y$ for \( \lambda \neq 0 \). Then $\ad_{T, y}(x) = [yx] = -[xy] = - \ad_{T, x} = - \lambda y\neq 0$, and since $\ad_{T, y}(y) = -[yy] = 0$, $y$ is an eigenvector with eigenvalue zero. Since $\ad_{T, y}$ is also diagonalizable and $x\in T$, write $x$ as a linear combination of eigenvectors for it, say $x = \sum a_i v_i$. Then $\ad_{T, y}(x) = \sum \lambda_i a_i v_i$ and the terms with $\lambda_i = 0$ vanish, and the remaining element is a sum of eigenvectors for $\ad_{T, y}$ with nonzero eigenvalues. $\contradiction$ ::: :::{.example title="?"} If $L = \liesl_n(\CC)$ then define $H$ to be the set of diagonal matrices. Then $H$ is toral and in fact maximal: if $L = H \oplus \CC z$ for some $z\in L\sm H$ then one can find an $h\in H$ such that $[hz] \neq 0$, making it nonabelian, but toral subalgebras must be abelian. ::: :::{.definition title="Roots"} Recall that a commuting family of diagonalizable operators on a finite-dimensional vector space can be simultaneously diagonalized. Letting $H \leq L$ be maximal toral, this applies to $\ad_L(H)$, and thus there is a basis in which all operators in $\ad_L(H)$ are diagonal. Set $L_{ \alpha} \da \ts{x\in L \st [hx] = \alpha(h) x\,\,\forall h\in H}$ where \( \alpha: H\to \CC \) is linear and thus an element of $H\dual$. Note that $L_0 = C_L(H)$, and the set $\Phi\da \ts{\alpha\in H\dual \st \alpha\neq 0, L_\alpha\neq 0}$ is called the **roots** of $H$ in $L$, and $L_\alpha$ is called a **root space**. Note that $L_0$ is not considered a root space. This induces a **root space decomposition** \[ L = C_L(H) \oplus _{ \alpha\in \Phi } L_\alpha .\] ::: :::{.remark} Note that for classical algebras, we'll show $C_L(H) = H$ and corresponds to the standard bases given early in the book. ::: :::{.example title="?"} Type $A_n$ yields $\liesl_{n+1}(\CC)$ and $\dim H = n$ for $H$ defined to be the diagonal traceless matrices. Define $\eps_i\in H\dual$ as $\eps_i \diag(a_1,\cdots, a_{n+1}) \da a_i$, the $\Phi \da \ts{\eps_i - \eps_j \st 1\leq i\neq j\leq ,n+1}$ and $L_{\eps_i - \eps_j} = \CC e_{ij}$. Why: \[ [h, e_{ij}] = \left[ \sum a_k e_{kk}, e_{ij}\right] = a_i e_{ii} e_{ij} - a_j e_{ij} e_{jj} = (a_i - a_j) e_{ij} \da (\eps_i -\eps_j)(h) e_{ij} .\] :::