% % file: oostende.tex % purpose: talk at Oostende conf., 2011 % created: pasha may 21-22,24-25 2011 % modified: % modification: % \documentclass{beamer} %\usepackage{mathrsfs} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% % to display sets { ... | ... } \newcommand{\set}[2]{\ensuremath{\{ #1 \>|\> #2 \}}} \def\liebrack{\ensuremath{[\,\cdot\, , \cdot\,]}} % to display nicely [.,.] \hyphenation{al-geb-ras} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \setbeamertemplate{headline} { \vskip2pt\hskip1pt\insertframenumber / \inserttotalframenumber } \setbeamertemplate{navigation symbols}{} \title{Novikov structures on Kac-Moody and modular semisimple Lie algebras} \author{Pasha Zusmanovich} \institute{Tallinn University of Technology} \date{May 30, 2011} \begin{document} \setcounter{framenumber}{-1} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame} \titlepage \end{frame} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}{What is a left-symmetric structure?} Left-symmetric (aka Vinberg, pre-Lie, chronological) identity: $$ x(yz) - (xy)z = y(xz) - (yx)z $$ Equivalently: \begin{itemize} \item $(x,y,z) = (y,x,z)$, where $(x,y,z) = (xy)z - x(yz)$ is the associator. \item $[L_x,L_y] = L_{[x,y]}$, where $L_x(a) = xa$. \end{itemize} \uncover<2->{ Left-symmetricity $\Rightarrow$ Lie-admissibility: $$ [x,y] = xy - yx $$ satisfies the Jacobi identity. \begin{block}{Question} Describe left-symmetric structures on a given Lie algebra. \end{block} \begin{block}{Origin} Theory of affine manifolds (Auslander, Milnor). \end{block} } \end{frame} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}{What is a Novikov structure?} Left-symmetric + $$ (xy)z = (xz)y $$ Equivalently: $$ [R_x,R_y] = 0 $$ where $R_x(a) = ax$. \begin{block}{Question} Describe Novikov structures on a given Lie algebra. \end{block} \begin{block}{Origin (of Novikov algebras)} \begin{itemize} \item Integrability of dynamical systems (Gelfand \& Dorfman). \item Poisson brackets of hydrodynamic type (Balinsky \& Novikov). \end{itemize} \end{block} \end{frame} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}{What is known about Novikov structures?} ($p=0$, finite-dimensional, unless stated otherwise) \begin{itemize} \item Helmstetter (1979): a Lie algebra admitting a left-symmetric structure is not perfect ($[L,L] \ne L$). \item Osborn (1992) and Xu (1996): Novikov structures on the Zassenhaus algebra $W_1(n)$ ($p>0$). \item Osborn \& Zelmanov (1995): an inverse problem: Lie structures on some infinite-dimensional Novikov Witt-type algebras. \item Xu (2000): same inverse problem; Novikov structures on the infinite-dimensional Witt algebra. \item Bai \& Meng (2001): Novikov structures on $4$-dimensional nilpotent Lie algebras. \item Burde (2006): a Lie algebra admitting a Novikov structure is solvable. \item Burde, Dekimpe \& Vercammen (2008): Novikov structures on Lie algebras of (strictly) upper triangular $n \times n$ matrices exist only for small $n$. \end{itemize} \end{frame} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}{Quadratic vs. linear problems} Suppose a Lie-admissible algebra satisfies a number of identities: \begin{equation*} \sum_{\sigma\in S_3} \Big(\alpha_\sigma^i (x_{\sigma(1)} x_{\sigma(2)}) x_{\sigma(3)} + \beta_\sigma^i x_{\sigma(1)} (x_{\sigma(2)} x_{\sigma(3)}) \Big) = 0, \quad i=1, \dots, n \end{equation*} Rewrite these identities in terms of $\liebrack$ and $\circ$, where $$ xy = \frac 12 [x,y] + \frac 12 x \circ y \qquad \text{(so $x \circ y = xy + yx$)}: $$ \begin{align*} & (\alpha_e^i + \alpha_{(12)}^i + \beta_e^i + \beta_{(12)}^i) (x_1 \circ x_2) \circ x_3 \\ + & (\alpha_{(23)}^i + \alpha_{(132)}^i + \beta_{(23)}^i + \beta_{(132)}^i) (x_3 \circ x_1) \circ x_2 \\ + & (\alpha_{(13)}^i + \alpha_{(123)}^i + \beta_{(13)}^i + \beta_{(123)}^i) (x_2 \circ x_3) \circ x_1 \\ + &\text{(terms linear with respect to $\circ$)} = 0. \end{align*} \begin{block}{Quadratic problem} For a given Lie algebra $(L, \liebrack)$, find symmetric maps $L \circ L \to L$, satisfying these identities. \end{block} \end{frame} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}{Quadratic vs. linear problems (continuation)} If $$ rk {\tiny \begin{pmatrix} \alpha_e^1 + \alpha_{(12)}^1 + \beta_e^1 + \beta_{(12)}^1 & \alpha_{(23)}^1 + \alpha_{(132)}^1 + \beta_{(23)}^1 + \beta_{(132)}^1 & \alpha_{(13)}^1 + \alpha_{(123)}^1 + \beta_{(13)}^1 + \beta_{(123)}^1 \\ \\ \dots & \dots & \dots \\ \\ \alpha_e^n + \alpha_{(12)}^n + \beta_e^n + \beta_{(12)}^n & \alpha_{(23)}^n + \alpha_{(132)}^n + \beta_{(23)}^n + \beta_{(132)}^n & \alpha_{(13)}^n + \alpha_{(123)}^n + \beta_{(13)}^n + \beta_{(123)}^n \end{pmatrix} } < n $$ then this quadratic problem has a \textbf{linear} consequence. \medskip \uncover<2->{ {\bf Left-symmetric structures - quadratic \smallskip Novikov (and LR, and probably some others?) structures - linear! } } \end{frame} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}{2-sided Alia algebras} \hskip -20pt (Dzhumadil'daev, 2009) \begin{align*} [x,y]z + [z,x]y + [y,z]x &= 0 \\ z[x,y] + y[z,x] + x[y,z] &= 0 \end{align*} $$ \begin{array}{l} \text{commutative} \\ \text{Lie} \\ \text{Novikov} \\ \text{LR} \end{array} \Rightarrow \text{2-sided Alia} \Rightarrow \text{Lie-admissible} $$ \begin{block}{Question} Describe 2-sided Alia structures on a given Lie algebra. \end{block} \uncover<2->{ \begin{block}{Equivalent question} Describe commutative $2$-cocycles on a given Lie algebra. \end{block} } \end{frame} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}{What are commutative $2$-cocycles?} Each 2-sided Alia structure on a Lie algebra $L$ is given by $$ xy = [x,y] + \varphi(x,y) $$ where $\varphi: L \times L \to K$ is a \textbf{commutative $2$-cocycle} on $L$, i.e.: \begin{enumerate} \item $\varphi$ is symmetric \item $\varphi([x,y],z) + \varphi([z,x],y) + \varphi([y,z],x) = 0$ \end{enumerate} Cocycles with $\varphi([L,L],L) = 0$ are called \textbf{trivial}. \medskip The space of all $K$-valued commutative $2$-cocycles on $L$ is denoted as $Z^2_{comm}(L)$. \end{frame} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}{Commutative $2$-cocycles on current Lie algebras} A \textbf{current Lie algebra} is a Lie algebra of the form $L \otimes A$, where $L$ is a Lie algebra, $A$ is an associative commutative algebra, with the Lie bracket $$ [x \otimes a, y \otimes b] = [x,y] \otimes ab $$ for $x,y\in L$, $a,b\in A$. \begin{block}{Fact} Under some technical assumptions, \begin{align*} &Z^2_{comm} (L\otimes A) \\ &\simeq Z^2_{comm}(L) \otimes A^* \\ &\oplus \set{\varphi: L \times L \to K}{\varphi \text{ is skew; } \varphi([x,y],z) = \varphi([z,x],y)} \otimes HC^1(A) \\ &\oplus \text{(trivial cocycles)} \end{align*} \end{block} \end{frame} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}{No Novikov structures on Kac-Moody} Kac--Moody: $$ \mathfrak g \otimes \mathbb C[t,t^{-1}] + \mathbb C t\frac{d}{dt} + \mathbb C z $$ \begin{block}{Corollary} All commutative $2$-cocycles on affine Kac-Moody algebras are trivial. \end{block} \begin{block}{Fact} A Lie algebra which is not $2$-step solvable and all whose commutative $2$-cocycles are trivial, do not admit a Novikov structure. \end{block} \begin{block}{Theorem} Affine Kac--Moody algebras do not admit Novikov structures. \end{block} \end{frame} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}{Novikov structures on modular semisimples} Modular semisimple Lie algebras: $$ S \otimes K[t_1, \dots, t_n]/(t_1^p, ..., t_n^p) + 1 \otimes D $$ \begin{block}{Another corollary} $Z^2_{comm}$ of such algebras is isomorphic to $Z^2_{comm}(D)$. \end{block} \begin{block}{Another theorem} A modular semisimple Lie algebra admits a Novikov structure if and only if $W_1(n)$ is ``involved''. \end{block} \uncover<2->{ Simples: \begin{itemize} \item Burde (1994): left-symmetric structures on classical, examples for Cartan type. \item Dzhumadil'daev \& Zusmanovich (2010): nonzero commutative $2$-cocycles exist only on $sl(2)$ and $W_1(n)$. \end{itemize} Semisimples: by the corollary above. } \end{frame} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% % don't include this final frame into the total count; % TeX twice for that! \newcounter{finalframe} \setcounter{finalframe}{\value{framenumber}} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \begin{frame}{} \begin{center} {\Huge That's all. Thank you.} \bigskip Slides at \texttt{http://justpasha.org/math/oostende.pdf} \end{center} \end{frame} %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% \setcounter{framenumber}{\value{finalframe}} \end{document} % end of oostende.tex