- Commit
- 44628b7f88a599c910e33a7a169ef30d986fe91a
- Parent
- 86586de251558363548f06d941489836707028fd
- Author
- Pablo <pablo-escobar@riseup.net>
- Date
Revised the first chapter
Source code for my notes on representations of semisimple Lie algebras and Olivier Mathieu's classification of simple weight modules
Revised the first chapter
1 file changed, 38 insertions, 38 deletions
Status | File Name | N° Changes | Insertions | Deletions |
Modified | sections/introduction.tex | 76 | 38 | 38 |
diff --git a/sections/introduction.tex b/sections/introduction.tex @@ -158,7 +158,7 @@ this last construction. f & = \begin{pmatrix} 0 & 0 \\ 1 & 0 \end{pmatrix} & h & = \begin{pmatrix} 1 & 0 \\ 0 & -1 \end{pmatrix} \end{align*} - form a basis for \(\mathfrak{sl}_2(K)\) and subject to the following + form a basis for \(\mathfrak{sl}_2(K)\) and are subject to the following relations. \begin{align*} [e, f] & = h & [h, f] & = -2 f & [h, e] = 2 e @@ -186,8 +186,7 @@ this last construction. \[ \mathfrak{sp}_{2 n}(K) = \left\{ - X \in \mathfrak{gl}_{2 n}(K) : - X^{\operatorname{T}} + X \in \mathfrak{gl}_{2 n}(K) : X^\top \begin{pmatrix} 0 & \operatorname{Id}_n \\ - \operatorname{Id}_n & 0 @@ -397,8 +396,8 @@ also share structural features with groups. For example\dots \end{example} \begin{definition} - A Lie algebra \(\mathfrak{g}\) is called \emph{nilpotent} if its derived - series + A Lie algebra \(\mathfrak{g}\) is called \emph{nilpotent} if its lower + central series \[ \mathfrak{g} \supseteq [\mathfrak{g}, \mathfrak{g}] @@ -436,7 +435,7 @@ Other interesting classes of Lie algebras are the so called \emph{simple} and \mathfrak{a}\), so again \(\mathfrak{a} = \mathfrak{sl}_2(K)\). Similarly, if \(f \in \mathfrak{a}\) then \([e, f] = h \in \mathfrak{a}\) and \(\mathfrak{a} = \mathfrak{sl}_2(K)\). More generally, the Lie algebra - \(\mathfrak{sl}_n(K)\) is simple for each \(n > 0\) -- see the section of + \(\mathfrak{sl}_n(K)\) is simple for each \(n > 1\) -- see the section of \cite[ch. 6]{kirillov} on invariant bilinear forms and the semisimplicity of classical Lie algebras. \end{example} @@ -461,7 +460,7 @@ A slight generalization is\dots \end{definition} \begin{example} - The Lie algebra \(\mathfrak{gl}_n(K)\) is reducible. Indeed, + The Lie algebra \(\mathfrak{gl}_n(K)\) is reductive. Indeed, \[ X = @@ -514,8 +513,6 @@ semisimple and reductive algebras by modding out by certain ideals, known as \] \end{definition} -As promised, we finds\dots - \begin{proposition}\label{thm:quotients-by-rads} Let \(\mathfrak{g}\) be a Lie algebra. Then \(\mfrac{\mathfrak{g}}{\mathfrak{rad}(\mathfrak{g})}\) is semisimple and @@ -671,9 +668,9 @@ The construction of \(\mathcal{U}(\mathfrak{g})\) may seem like a purely algebraic affair, but the universal enveloping algebra of the Lie algebra of a Lie group \(G\) is in fact intimately related with the algebra \(\operatorname{Diff}(G)\) of differential operators \(C^\infty(G) \to -C^\infty(G)\) -- \(\mathbb{R}\)-linear endomorphisms \(C^\infty(G) \to -C^\infty(G)\) of finite order as defined in Coutinho's \citetitle{coutinho} -\cite[ch.~3]{coutinho}, for example. Algebras of differential operators and +C^\infty(G)\) -- i.e. \(\mathbb{R}\)-linear endomorphisms \(C^\infty(G) \to +C^\infty(G)\) of finite order, as defined in Coutinho's \citetitle{coutinho} +\cite[ch.~3]{coutinho} for example. Algebras of differential operators and their modules are the subject of the theory of \(D\)-modules, which has seen remarkable progress in the past century. Specifically, we find\dots @@ -689,12 +686,12 @@ remarkable progress in the past century. Specifically, we find\dots \begin{proof} An order \(0\) \(G\)-invariant differential operator in \(G\) is simply - multiplication by a constant in \(\mathbb{R}\). An order \(1\) + multiplication by a constant in \(\mathbb{R}\). A homogeneous order \(1\) \(G\)-invariant differential operator in \(G\) is simply a left invariant derivation \(C^\infty(G) \to C^\infty(G)\). All other \(G\)-invariant differential operators are generated by invariant operators of order \(0\) and \(1\). Hence \(\operatorname{Diff}(G)^G\) is generated by - \(\operatorname{Der}(G)^G\) -- here \(\operatorname{Der}(G)^G \subset + \(\operatorname{Der}(G)^G + K\) -- here \(\operatorname{Der}(G)^G \subset \operatorname{Der}(G)\) denotes the Lie subalgebra of invariant derivations. Now recall that there is a canonical isomorphism of Lie algebras @@ -718,7 +715,7 @@ remarkable progress in the past century. Specifically, we find\dots Since \(\mathcal{U}(\mathfrak{g})\) is generated by the image of the inclusion \(\mathfrak{g} \to \mathcal{U}(\mathfrak{g})\), this implies \(\ker \tilde f = 0\). Given that \(\operatorname{Diff}(G)^G\) is generated by - \(\operatorname{Der}(G)^G\), this also goes to show \(\tilde f\) is + \(\operatorname{Der}(G)^G + K\), this also goes to show \(\tilde f\) is surjective. \end{proof} @@ -745,21 +742,23 @@ First introduced in 1896 by Georg Frobenius in his paper \citetitle{frobenius} one of the cornerstones of modern mathematics. In this section we provide a brief overview of basic concepts of the representation theory of Lie algebras. We should stress, however, that the representation theory of Lie algebras is -only a small fragment of what is today known as representation theory, which is -in general concerned with a diverse spectrum of algebraic and combinatorial -structures -- such as groups, quivers and associative algebras. An introductory -exploration of some of this structures can be found in \cite{etingof}. +only a small fragment of what is today known as ``representation theory'', +which is in general concerned with a diverse spectrum of algebraic and +combinatorial structures -- such as groups, quivers and associative algebras. +An introductory exploration of some of this structures can be found in +\cite{etingof}. We begin by noting that any \(\mathcal{U}(\mathfrak{g})\)-module \(V\) may be regarded as a \(K\)-vector space endowed with a ``linear action'' of \(\mathfrak{g}\). Indeed, by restricting the action map -\(\mathcal{U}(\mathfrak{g}) \to \operatorname{End}(V)\) to \(\mathfrak{g}\) -yields a homomorphism of Lie algebras \(\mathfrak{g} \to \mathfrak{gl}(V) = -\operatorname{End}(V)\). In fact proposition~\ref{thm:universal-env-uni-prop} -implies that given a vector space \(V\) there is a one-to-one correspondence -between \(\mathcal{U}(\mathfrak{g})\)-module structures for \(V\) and -homomorphisms \(\mathfrak{g} \to \mathfrak{gl}(V)\). This leads us to the -following definition. +\(\mathcal{U}(\mathfrak{g}) \to \operatorname{End}(V)\) to \(\mathfrak{g} +\subset \mathcal{U}(\mathfrak{g})\) yields a homomorphism of Lie algebras +\(\mathfrak{g} \to \mathfrak{gl}(V) = \operatorname{End}(V)\). In fact +proposition~\ref{thm:universal-env-uni-prop} implies that given a vector space +\(V\) there is a one-to-one correspondence between +\(\mathcal{U}(\mathfrak{g})\)-module structures for \(V\) and homomorphisms +\(\mathfrak{g} \to \mathfrak{gl}(V)\). This leads us to the following +definition. \begin{definition} Given a Lie algebra \(\mathfrak{g}\) over \(K\), \emph{a representation \(V\) @@ -927,7 +926,8 @@ define\dots Given a Lie algebra \(\mathfrak{g}\) and representations \(V\) and \(W\) of \(\mathfrak{g}\), the exterior and symmetric products \(V \wedge W\) and \(V \odot W\) are both representations of \(\mathfrak{g}\): they are quotients of - \(V \otimes W\). + \(V \otimes W\). In particular, the exterior and symmetric powers \(\wedge^n + V\) and \(\operatorname{Sym}^n V\) are \(\mathfrak{g}\)-modules. \end{example} \begin{example} @@ -946,7 +946,7 @@ separate algebras. In particular, we may define\dots \(\operatorname{Res}_{\mathfrak{h}}^{\mathfrak{g}} V = V\) the representation of \(\mathfrak{h}\) where the action of \(\mathfrak{h}\) is given by restricting the map \(\mathfrak{g} \to \mathfrak{gl}(V)\) to - \(\mathfrak{g}\). Any homomorphism of \(\mathfrak{g}\)-modules \(V \to W\) is + \(\mathfrak{h}\). Any homomorphism of \(\mathfrak{g}\)-modules \(V \to W\) is also a homomorphism of \(\mathfrak{h}\)-modules and this construction is clearly functorial. \[ @@ -958,12 +958,11 @@ separate algebras. In particular, we may define\dots \begin{example} Given a Lie algebra \(\mathfrak{g}\), the adjoint representation of - \(\mathfrak{g}\) is a subrepresentation of - \(\operatorname{Res}_{\mathfrak{g}}^{\mathcal{U}(\mathfrak{g})} - \mathcal{U}(\mathfrak{g})\). + \(\mathfrak{g}\) is a subrepresentation of the restriction of the adjoint + representation of \(\mathcal{U}(\mathfrak{g})\) to \(\mathfrak{g}\). \end{example} -Surprisingly, this functor has right adjoint. +Surprisingly, this functor has a right adjoint. \begin{example} Let \(\mathfrak{g}\) be a Lie algebra and \(\mathfrak{h}\) be a subalgebra. @@ -971,10 +970,11 @@ Surprisingly, this functor has right adjoint. \(\operatorname{Ind}_{\mathfrak{h}}^{\mathfrak{g}} V\) the representation of \(\mathfrak{h}\) corresponding to the \(\mathcal{U}(\mathfrak{g})\)-module \(\mathcal{U}(\mathfrak{g}) \otimes_{\mathcal{U}(\mathfrak{h})} V\) -- where - the action of \(\mathfrak{h}\) in \(\mathcal{U}(\mathfrak{g})\) is given by - left multiplication. Any homomorphism of \(\mathfrak{h}\)-modules \(T : V \to - W\) induces a homomorphism \(\operatorname{Ind}_{\mathfrak{h}}^{\mathfrak{g}} - T = \operatorname{Id} \otimes T : + the right \(\mathcal{U}(\mathfrak{h})\)-module structure of + \(\mathcal{U}(\mathfrak{g})\) is given by right multiplication. Any + homomorphism of \(\mathfrak{h}\)-modules \(T : V \to W\) induces a + homomorphism \(\operatorname{Ind}_{\mathfrak{h}}^{\mathfrak{g}} T = + \operatorname{Id} \otimes T : \operatorname{Ind}_{\mathfrak{h}}^{\mathfrak{g}} V \to \operatorname{Ind}_{\mathfrak{h}}^{\mathfrak{g}} W\) and this construction is clearly functorial. @@ -1037,7 +1037,7 @@ Surprisingly, this functor has right adjoint. \end{proof} This last proposition is known as \emph{Frobenius reciprocity}, and was first -proved by Frobenius himself in the context of finite-groups. Another +proved by Frobenius himself in the context of finite groups. Another interesting construction is\dots \begin{example} @@ -1053,4 +1053,4 @@ interesting construction is\dots This concludes our initial remarks on representations. In the following chapters we will explore the fundamental problem of representation theory: that -of classifying all representations up to isomorphism. +of classifying all representations of a given algebra up to isomorphism.