\documentclass[11pt]{article} \usepackage{cancel} \usepackage{amsmath} \usepackage{amsthm} \usepackage{amssymb} \usepackage{epsfig} \usepackage{pstricks} \newcommand{\handout}[5]{ \noindent \begin{center} \framebox{ \vbox{ \hbox to 5.78in { {\bf 18.745 Introduction to Lie Algebras } \hfill #2 } \vspace{4mm} \hbox to 5.78in { {\Large \hfill #5 \hfill} } \vspace{2mm} \hbox to 5.78in { {\em #3 \hfill #4} } } } \end{center} \vspace*{4mm} } \newcommand{\lecture}[4]{\handout{#1}{#2}{#3}{Scribe: #4}{Lecture #1}} \newcommand{\F}{\mathbb{F}} \newcommand{\Z}{\mathbb{Z}} \newcommand{\Q}{\mathbb{Q}} \newcommand{\sll}{\mbox{sl}} \newcommand{\gl}{\mbox{gl}} \newcommand{\so}{\mbox{so}} \newcommand{\spl}{\mbox{sp}} \newcommand{\tr}{\mbox{tr}} \newcommand{\diag}{\mbox{diag}} \newcommand{\ad}{\mbox{ad}} \newcommand{\charr}{\mbox{char}} \newcommand{\centerr}{\mbox{center}} \newcommand{\g}{\mathfrak{g}} \newcommand{\gb}{\overline{\g}} \newcommand{\h}{\mathfrak{h}} \newcommand{\hb}{\overline{\h}} \newcommand{\m}{\mathfrak{m}} \newcommand{\p}{\mathfrak{p}} \newcommand{\D}{\mathfrak{D}} \newcommand{\He}{\mathcal{H}} \newcommand{\sk}{\vspace*{1em}} \newtheorem{defn}{Definition} \newtheorem{remark}{Remark} \newtheorem{example}{Example} \newtheorem{thm}{Theorem} \newtheorem{lem}{Lemma} \newtheorem{cor}{Corollary} % 1-inch margins, from fullpage.sty by H.Partl, Version 2, Dec. 15, 1988. \topmargin 0pt \advance \topmargin by -\headheight \advance \topmargin by -\headsep \textheight 8.9in \oddsidemargin 0pt \evensidemargin \oddsidemargin \marginparwidth 0.5in \textwidth 6.5in \parindent 0in \parskip 1.5ex %\renewcommand{\baselinestretch}{1.25} \begin{document} \lecture{10 --- October 12, 2004}{Fall 2004}{Prof.\ Victor Ka\v{c}}{Steven Sivek} Recall that a \emph{trace form} on a Lie algebra $\g$, given a representation $\pi$ of $\g$ in a finite dimensional vector space $V$, is defined as $(a,b)_V = \tr_V(\pi(a)\pi(b))$. \begin{defn} The \emph{Killing form} on a finite-dimensional Lie algebra $\g$ is the trace form $K(a,b) = \tr_{\g}((\ad\ a)(\ad\ b))$ in the adjoint representation of $\g$. \end{defn} \paragraph{Exercise 10.1.} Show that the trace form for the defining representation of $\gl_n(\F)$, $\sll_n(\F)$, $\so_n(\F)$, $\spl_n(\F)$ is nondegenerate. \paragraph{Solution.} Let $e_{xy}$ denote the $n$x$n$ matrix with the element in row $x$, column $y$ equal to 1 and all other elements 0. We note that $\tr(e_{ij}e_{kl}) = \tr(\delta_{jk}e_{il}) = \delta_{jk}\delta_{il}$. To show that this form is nondegenerate for a Lie algebra $\g \subset \gl_n(\F)$, it suffices to show for any $a \in \g$ that $\tr(ab) \not= 0$ for some $b \in \g$, so this is how we will proceed. (We will assume that $\charr(\F) = 0$ for simplicity, since e.g. the trace form for $\sll_n(\F)$ is degenerate when $\charr(F)\ |\ n$.) $\g = \gl_n(\F)$: Take nonzero $a = (a_{ij}) \in \g$, and pick $x,y$ such that $a_{xy} \not= 0$. Then $\tr(a e_{yx}) = a_{xy} \not= 0$. $\g = \sll_n(\F)$: Choose nonzero $a = (a_{ij}) \in \g$. If $a$ is not a diagonal matrix, then we may pick $x \not= y$ such that $a_{xy} \not= 0$, and as before we have $\tr(a e_{yx}) \not= 0$. Otherwise, let $a = \diag(b_1, \dots, b_n)$. Then $a \not= \alpha I_n$ for any $\alpha$, since otherwise we would have either $a=0$ or $\tr(a) = n\alpha$ with $n,\alpha \not= 0$. It follows that for some $k < n$ we must have $b_k \not= b_{k+1}$; we calculate that $\tr(a (e_{kk} - e_{k+1}{k+1})) = b_k-b_{k+1} \not= 0$. $\g = \so_n(\F)$: Pick a basis for $\F^n$ such that $\so_n(\F)$ is the algebra of skew-symmetric matrices, i.e. $\so_n(\F) = \{ a \in \gl_n(\F)\ |\ a^T = -a \}$. Then $\g$ has as a basis $\mathcal{B} = \{ e_{ij}-e_{ji}\ |\ i 0$, so $\lambda(h) = \frac{-Q}{P} \alpha(h)$, where the ratio $\frac{-Q}{P}$ depends only on $\lambda$ and $\alpha$, as desired. \end{proof} We may use this to describe solvable subalgebras of $\gl_V$ in several ways in terms of trace forms. \begin{thm}[Cartan's criterion] Let $\g$ be a subalgebra of $\gl_V$ for $V$ a finite-dimensional vector space over a an algebraically closed field $\F$ of characteristic 0. Then the following are equivalent: \begin{enumerate} \item $(\g, [\g,\g])_V = 0$. \item $(a,a)_V = 0$ for any $a \in [\g,\g]$. \item $\g$ is a solvable Lie algebra. \end{enumerate} \begin{proof} $(1) \Rightarrow (2)$: Take $a \in [\g,\g]$, and write $a=[b,c]$. Then since $(a,[b,c])_V = 0$, we have $(a,a)_V=0$. $(2) \Rightarrow (3)$: Suppose that $\g$ is not solvable. Then the derived series of $\g$ stabilizes to some nonzero subalgebra $\p = \g^{(N)} = \g^{(N+1)} = \cdots$, so $[\p, \p] = \p$. In particular, since $\p \subset \g$, we have $(a,a)_V = 0$ for any $a \in [\p,\p] = \p$ by our assumption. Let $\h$ be a Cartan subalgebra of $\p$, and consider the root and weight space decompositions \begin{eqnarray*} \p = \bigoplus_{\alpha \in \h^*} \p_\alpha,\ V = \bigoplus_{\lambda \in \h^*} V_\lambda. \end{eqnarray*} Since $[\p_\alpha, \p_\beta] \subset \p_{\alpha+\beta}$ and $[\p,\p] = \p$, we conclude that $\h = \p_0 = \sum_\alpha [\p_\alpha, \p_{-\alpha}]$; that is, $\h$ is a span of elements of the form $h_{\alpha,i} = [e_{\alpha,i}, f_{\alpha,i}]$, where $e_{\alpha,i} \in \p_\alpha$ and $f_{\alpha,i} \in \p_{-\alpha}$. Suppose that $V_\lambda \not= 0$ for some fixed $\lambda \in \h^*$. By Cartan's lemma, we can write $\lambda(h_{\alpha,i}) = r_{\alpha,\lambda} \alpha(h_{\alpha,i})$ for all $\alpha$ and $i$, where $r_{\alpha,\lambda} \in \Q$. Since we are assuming (2), $(h_{\alpha,i}, h_{\alpha,i})_V = 0$. But we compute that $(h_{\alpha,i}, h_{\alpha,i})_V = \sum_\lambda \lambda(h_{\alpha,i})^2\dim(V_\lambda)$ by considering the restriction of $h_{\alpha,i}$ to each subspace $V_\lambda$ as in the proof of Cartan's lemma; this is then equal to $\sum_\lambda r_{\alpha,\lambda}^2 \alpha(h_{\alpha,i})^2 \dim(V_\lambda)$ by the lemma, so $\alpha(h_{\alpha,i})^2 \left( \sum_\lambda r_{\alpha,\lambda}^2 \dim(V_\lambda) \right) = 0$. Hence, since all the $r_{\alpha,\lambda}$ are rational numbers, either $\alpha(h_{\alpha,i}) = 0$, or $r_{\alpha,\lambda} = 0$ whenever $V_\lambda \not= 0$, and in either case we have $\lambda(h_{\alpha,i}) = r_{\alpha,\lambda} \alpha(h_{\alpha,i}) = 0$ whenever $V_\lambda \not= 0$. For any $\lambda \in \h^*$ such that $V_\lambda \not= 0$, since the elements $\{h_{\alpha,i}\}$ span $\h$, and $\lambda = 0$ on all of these elements, we conclude that $\lambda \equiv 0$ on $\h$. Therefore the weight space decomposition of $V$ is $V = V_0$. But for any $\alpha \not= 0$ we have $\p_\alpha V_0 \subset V_\alpha = 0$, so $\p_\alpha = 0$; hence $\p = \p_0 = \h$. But if $\p = \h$ then $\p$ is nilpotent, and so $[\p, \p]$ is a proper subset of $\p$. This is a contradiction, so $\g$ must in fact be solvable. $(3) \Rightarrow (1)$: By a corollary to Lie's theorem, we may pick a basis of $V$ such that all of the matrices in $\g$ are upper triangular, hence all matrices in $[\g,\g]$ are strictly upper triangular. Then $\tr_V(ab) = 0$ for any $a \in \g$ and $b \in [\g,\g]$, since $ab$ is strictly upper triangular, and so $(\g,[\g,\g])_V = 0$. \end{proof} \end{thm} This theorem leads almost immediately to a characterization of solvable Lie algebras, as follows: \begin{cor} A finite dimensional Lie algebra $\g$ over an algebraically closed field of characteristic 0 is solvable if and only if $K(\g,[\g,\g]) = 0$. \begin{proof} We know that $\g$ is solvable if and only if $\g/\centerr(\g)$ and $\centerr(\g)$ are both solvable, hence if and only if $\g/\centerr(\g)$ is solvable. Consider the adjoint representation $\ad: \g \rightarrow \gl_{\g}$. Since $\ker(\ad) = \centerr(\g)$, this proof reduces to consideration of the subalgebra $\ad\ \g \subset \gl_\g$; we now apply the fact that conditions (1) and (3) of Cartan's criterion are equivalent, and we are done. \end{proof} \end{cor} Up until this point, we have restricted many of our results to Lie algebras over algebraically closed fields $\F$ of characteristic zero, since root space and weight space decompositions exist for such algebras. Requiring $\F$ to be algebraically closed is not always necessary, as we shall see: \begin{remark} Let $\F$ be a field of characteristic zero which is not necessarily algebraically closed, and let $\g$ be a Lie algebra over $\F$. Then the following are true: \begin{enumerate} \item Cartan's criterion and the corollary which followed it are both true over $\F$. \item $\h_0^a$ is a Cartan subalgebra of $\g$ if $a \in \g$ is regular. \item $[\g,\g]$ is nilpotent if $\g$ is finite-dimensional and solvable. \end{enumerate} \end{remark} In order to show this, we will introduce some notation: let $\overline{\F}$ be the algebraic closure of $\F$, and let $\gb = \overline{\F} \otimes_\F \g$. \paragraph{Exercise 10.3.} (a) Show that $\g$ is solvable (resp. nilpotent, abelian) if and only if $\gb$ is, and that $\overline{[\g,\g]} = [\gb, \gb]$. (b) Prove the above remark for $\F$ not algebraically closed. \paragraph{Solution.} Given two Lie algebras $\g$ and $\h$ over $\F$, we claim that $[\gb, \hb] = \overline{[\g,\h]}$. Clearly since $\g \subset \gb$ and $\h \subset \hb$, we have $\overline{[\g,\h]} \subset \overline{[\gb,\hb]} = [\gb, \hb]$. Given bases $\{ g_\alpha \}_{\alpha \in I}$ of $\g$ and $\{ h_\beta \}_{\beta \in J}$ of $\h$, these same bases generate $\gb$ and $\hb$ when combined over $\overline{\F}$ rather than $\F$. Hence the set $\{[g_\alpha, h_\beta]\}_{\alpha \in I, \beta \in J}$ generates $[\gb,\hb]$ over $\overline{\F}$. But this set also generates $[\g,\h]$ with coefficients in $\F$, so when we extend this to $\overline{F}$ we get $[\gb,\hb] \subset \overline{[\g,\h]}$. Thus $[\gb, \hb] = \overline{[\g,\h]}$. Part (a) now follows easily, since we note that $\gb^i = \overline{\g^i}$ and $\gb^{(i)} = \overline{\g^{(i)}}$ for all $i$. Then $\g$ is solvable if and only if $\g^{(n)} = 0$ for some $n$; but this is equivalent to $\overline{\g^{(n)}} = 0$, or $\gb^{(n)} = 0$, and so $\g$ is solvable iff $\gb$ is. The same is true of nilpotency, as we see by replacing $g^{(n)}$ with $g^n$ in this argument, and abelianness, which comes from the solvability argument with $n = 1$. In particular, letting $\h = \g$ above yields $\overline{[\g,\g]} = [\gb,\gb]$. For part (b), we first look at Cartan's criterion. Since $\g$ is solvable if and only if $\gb$ is, we have the equivalent conditions (1) $(\gb, [\gb,\gb]_V = 0$; (2) $(a,a)_V = 0$ for all $a \in [\gb,\gb]$; and (3) $\g$ is solvable. But $(\gb, [\gb,\gb])_V = (\gb, \overline{[\g,\g]})_V = \overline{(\g,[\g,\g])_V}$, so $(\g,[\g,\g])_V = 0$ if and only if $(\gb,[\gb,\gb])_V = 0$. Furthermore, $(a,a)_V = 0$ for all $a \in [\gb,\gb] = \overline{[\g,\g]}$ iff it does for all $a \in [\g,\g]$, since $[\g,\g]$ and $\overline{[\g,\g]}$ share the same basis over different fields and thus $(a,a)_V = 0$ for all $a$ in one iff it does for all $a$ in the other. Therefore Cartan's criterion holds for $\g$ given that it does for $\gb$; the corollary's proof over $\g$ is identical to its original proof, since it only needed algebraic closure to satisfy Cartan's criterion. Next, we consider the proof that $\h_0^a$ is a Cartan subalgebra if $a$ is regular. If $a \in \g$ is regular, it is regular in $\gb$, so we know that $\overline{\h_0^a}$ is a Cartan subalgebra of $\gb$, or $\overline{\h_0^a} = N_{\gb}(\overline{\h_0^a})$. Since $[b, \overline{\h_0^a}] \subset \overline{\h_0^a}$ if and only if $[b, \h_0^a] \subset \h_0^a$ for any $b \in \g$, we conclude that $N_{\g}(\h_0^a) = \h_0^a$, and so $\h_0^a$ is a Cartan subalgebra of $\g$. Finally, assume $\g$ is finite dimensional and solvable. Then $\gb$ is finite dimensional and solvable, so we know that $[\gb,\gb]$ is nilpotent. But $[\gb,\gb] = \overline{[\g,\g]}$, so $\overline{[\g,\g]}$ is nilpotent, hence $[\g,\g]$ is nilpotent. \paragraph{} \begin{remark} The basic properties of a trace form are that it is symmetric (i.e. $(a,b)_V = (b,a)_V$) and invariant (i.e. $([a,b],c)_V = (a,[b,c])_V$). The basic results on trace forms (like Cartan's criterion) fail, however, if we assume only that the bilinear forms involved are symmetric and invariant. \end{remark} We can construct an example of this as follows: \paragraph{Exercise 10.4.} Consider the 4-dimensional Lie algebra $\D = \F p + \F q + \F c + \F d$, where $[p,q] = c$, $c$ is central, $[d,p] = p$, and $[d,q] = d$. Construct a nondegenerate symmetric invariant bilinear form on $\D$. \paragraph{Solution.} Define a bilinear form $B(x,y)$ on $\D$ by the values $B(p,q) = B(q,p) = 1$; $B(c,d) = B(d,c) = 1$; $B = 0$ on all other pairs of basis elements; and all other values of $B$ follow by symmetry and bilinearity. Then $B$ is nondegenerate, since it has matrix {\tiny $\left( \begin{array}{cccc} 0&1&0&0 \\ 1&0&0&0 \\ 0&0&0&1 \\ 0&0&1&0 \end{array} \right)$ } with respect to the basis $\{p,q,c,d\}$ and this matrix is invertible. Invariance is also easy to check, so we are done. \paragraph{} The algebra $\D$ is solvable, since $[\D,\D] = \He_1$ is solvable, so by Cartan's criterion, any trace form on $\D$ must satisfy $(\D, \He_1)_V = 0$. But $B(d,c) = 1$, so $B$ cannot be a trace form. \paragraph{} We conclude the lecture by defining a new class of Lie algebras: \begin{defn} A Lie algebra $\g$ is called \emph{semisimple} if it contains no nonzero solvable ideals. Equivalently, $\g$ is semisimple if it contains no nonzero abelian ideals. \end{defn} Equivalence can be proved as follows: If $\g$ has a nonzero abelian ideal, then it has a nonzero solvable ideal, since abelian ideals are solvable. Conversely, if $\g$ has a nonzero solvable ideal $\h$, take $n$ such that $\h^{(n)} \not= 0$ but $\h^{(n+1)} = 0$; then $\h^{(n)}$ is a nonzero abelian ideal. In the next lecture, we'll prove that a finite-dimensional Lie algebra $\g$ over a field of characteristic zero is semisimple if and only if the Killing form on $\g$ is nondegenerate. \end{document}