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- 4127c23b2acd5c54bccffff057640c690cd118eb
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- 3dcf4f4eaab8cc8674f4c1d03b1cc9c257c5525c
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- Pablo <pablo-pie@riseup.net>
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Hydrated chapter 4
My M2 Memoire on mapping class groups & their representations
Hydrated chapter 4
5 files changed, 349 insertions, 175 deletions
Status | File Name | N° Changes | Insertions | Deletions |
Modified | references.bib | 38 | 38 | 0 |
Modified | sections/introduction.tex | 2 | 1 | 1 |
Modified | sections/presentation.tex | 45 | 28 | 17 |
Modified | sections/representations.tex | 431 | 278 | 153 |
Modified | sections/twists.tex | 8 | 4 | 4 |
diff --git a/references.bib b/references.bib @@ -23,6 +23,44 @@ year = {2023}, } +@article{funar, + author = {Louis Funar}, + doi = {10.1090/S0002-9939-2010-10555-5}, + journal = {Proceedings of the American Mathematical Society}, + language = {English}, + number = 1, + pages = {375--382}, + title = {Two Questions on Mapping Class Groups}, + volume = {139}, + year = {2011}, +} + +@article{franks-handel, + author = {Franks, John and Handel, Michael}, + doi = {10.1090/S0002-9939-2013-11556-X}, + issn = {0002-9939}, + journal = {Proceedings of the American Mathematical Society}, + number = 9, + pages = {2951--2962}, + title = {Triviality of Some Representations of $\operatorname{MCG}(S_g)$ in $GL(n, \mathbb{C})$, $\operatorname{Diff}(S^2)$ and $\operatorname{Homeo}(\mathbb{T}^2)$}, + volume = {141}, + year = {2013}, +} + +@article{kasahara, + author = {Kasahara, Yasushi}, + doi = {10.1090/tran/9037}, + issn = {1088-6850}, + journal = {Transactions of the American Mathematical Society}, + month = oct, + number = 2, + pages = {1183--1218}, + publisher = {American Mathematical Society (AMS)}, + title = {Crossed homomorphisms and low dimensional representations of mapping class groups of surfaces}, + volume = {377}, + year = {2023}, +} + @incollection{julien, author = {Marché, Julien}, booktitle = {Topology and geometry. A collection of essays dedicated to Vladimir G. Turaev},
diff --git a/sections/introduction.tex b/sections/introduction.tex @@ -61,7 +61,7 @@ \(\Mod(S) \actson H_k(S, \mathbb{R})\) \end{example} -\begin{example} +\begin{example}\label{ex:symplectic-rep} The symplectic representation. \end{example}
diff --git a/sections/presentation.tex b/sections/presentation.tex @@ -1,15 +1,16 @@ \chapter{Relations Among Twists \& Wajnryb's Presentation} -\begin{proposition}[Lantern relation] -\end{proposition} +\begin{example} + Lantern relation +\end{example} -\begin{corollary} - If \(g \ge 3\) then the Abelianization \(\Mod(S_g)^\ab = - \mfrac{\Mod(S_g)}{[\Mod(S_g), \Mod(S_g)]}\) is trivial. In other words, - \(\Mod(S_g) = \Mod(S_g)'\) is a perfect group for \(g \ge 3\). -\end{corollary} +\begin{proposition}\label{thm:trivial-abelianization} + If \(g \ge 3\) then the Abelianization \(\Mod(S_g^b)^\ab = + \mfrac{\Mod(S_g^b)}{[\Mod(S_g), \Mod(S_g)]}\) is trivial. In other words, + \(\Mod(S_g) = [\Mod(S_g), \Mod(S_g)]\) is a perfect group for \(g \ge 3\). +\end{proposition} -% TODO: Explain to get the groups in the low-genus settings we use explicit +% TODO: Explain how to get the groups in the low-genus settings we use explicit % presentations of Mod(S_g) \begin{center} \begin{tabular}{ r|c|l } @@ -23,17 +24,17 @@ % TODO: Look for a proof of this? In any case, cite a reference \begin{proposition}\label{thm:commutator-is-perfect} - Given \(b \ge 0\) the commutator subgroup \(\Mod(S_2^b)' = [\Mod(S_2^b), - \Mod(S_2^b)]\) is perfect -- i.e. \(\Mod(S_2^b)^{(2)} = [\Mod(S_2^b)', - \Mod(S_2^b)']\) is the whole of \(\Mod(S_2^b)'\). + The commutator subgroup \(\Mod(S_2^b)' = [\Mod(S_2^b), \Mod(S_2^b)]\) is + perfect -- i.e. \(\Mod(S_2^b)^{(2)} = [\Mod(S_2^b)', \Mod(S_2^b)']\) is the + whole of \(\Mod(S_2^b)'\). \end{proposition} % TODO: Comment on the proof of this? \begin{proposition}\label{thm:commutator-normal-gen} If \(g \ge 2\) and \(\alpha, \beta \subset S_g\) are simple closed curves - with \(\#(\alpha \cap \beta) = 1\) then \(\Mod(S_g)'\) is normally generated - by \(\tau_\alpha \tau_\beta^{-1}\) -- i.e. if \(\tau_\alpha \tau_\beta^{-1} - \in N \normal \Mod(S_g)'\) then \(\Mod(S_g)' \subset N\). + with \(\#(\alpha \cap \beta) = 1\) then \(\Mod(S_g)'\) is \emph{normally + generated} by \(\tau_\alpha \tau_\beta^{-1}\) -- i.e. if \(\tau_\alpha + \tau_\beta^{-1} \in N \normal \Mod(S_g)'\) then \(\Mod(S_g)' \subset N\). \end{proposition} \section{The Birman-Hilden Theorem} @@ -46,8 +47,18 @@ % TODO: Cite the paper by Artin \begin{theorem}[Artin] - \(B_n = \langle \sigma_1, \ldots, \sigma_{n - 1} : \sigma_i \sigma_{i + 1} - \sigma_i = \sigma_{i + 1} \sigma_i \sigma_{i + 1} \forall i \rangle\). + \[ + B_n = + \left\langle + \sigma_1, \ldots, \sigma_{n - 1} : + \begin{aligned} + \sigma_i \sigma_{i+1} \sigma_i & = \sigma_{i+1} \sigma_i \sigma_{i+1} + \ \text{for all} \ i, \\ + \sigma_i \sigma_j & = \sigma_j \sigma_i + \ \text{for} \ j \ne i + 1 \ \text{and} \ j \ne i - 1 + \end{aligned} + \right\rangle + \] \end{theorem} \begin{corollary} @@ -102,7 +113,7 @@ \end{example} % TODO: Cite the original paper? -\begin{theorem}[Wajnryb] +\begin{theorem}[Wajnryb]\label{thm:wajnryb-presentation} If \(\alpha_0, \ldots, \alpha_g\) are as in % TODO: Reference the drawing of the curves somewhere and \(a_i = \tau_{\alpha_i} \in \Mod(S_g)\) are the Humphreys generators then
diff --git a/sections/representations.tex b/sections/representations.tex @@ -1,50 +1,59 @@ \chapter{Low-Dimensional Representations} -\begin{theorem}[Korkmaz \cite{korkmaz}]\label{thm:low-dim-reps-are-trivial} +Having built a solid understanding of the combinatorics of Dehn twists, we are +now ready to attack the problem of classifying the representations of +\(\Mod(S_g)\). Indeed, in light of the Wajnryb presentation, a representation +\(\rho : \Mod(S_g) \to \GL_n(\mathbb{C})\) is nothing other than a choice of +\(2g + 1\) matrices \(\rho(\tau_{\alpha_1}), \ldots, \rho(\tau_{\alpha_{2g}}) +\in \GL_n(\mathbb{C})\) satisfying the relations \strong{(i)} to \strong{(v)} +from Theorem~\ref{thm:wajnryb-presentation}. + +Historically, these relations have been exploited by Funar \cite{funar}, +Franks-Handel \cite{franks-handel} and others to establish the triviality of +low-dimensional representions, culminating Korkmaz' recent classification of +representations of dimension \(n \le 2 g\) for \(g \ge 3\) \cite{korkmaz}. The +goal of this chapter is providing a concise account of Korkmaz' results, +starting by\dots + +\begin{theorem}[Korkmaz]\label{thm:low-dim-reps-are-trivial} Let \(S_g^b\) be the surface of genus \(g \ge 1\) and \(b\) boundary - components and \(\rho : \Mod(S_g^b) \to \GL(V)\) be an \(m\)-dimensional - linear representation for some \(m < 2 g\). Then the image of \(\rho\) is - Abelian. In particular, if \(g \ge 3\) then \(\rho\) is trivial. + components and \(\rho : \Mod(S_g^b) \to \GL_n(\mathbb{C})\) be a linear + representation with \(n < 2 g\). Then the image of \(\rho\) is Abelian. In + particular, if \(g \ge 3\) then \(\rho\) is trivial. \end{theorem} -% TODO: Explain the setup of the proof: induction in m and case analysis on the -% Jordan form +Like so many of the results we have encountered so far, the proof of +Theorem~\ref{thm:low-dim-reps-are-trivial} is elementary in nature: we proceed +by induction on \(g\) and tedious case analysis. We begin by the base case \(g += 2\). -% TODO: Explain this is the base case \begin{proposition}\label{thm:low-dim-reps-are-trivial-base-case} - Let \(\rho : \Mod(S_2^b) \to \GL(V)\) be an \(m\)-dimensional representation, - \(m \le 3\). Then the image of \(\rho\) is a quotient of \(\mathbb{Z}/10\). + Given \(\rho : \Mod(S_2^b) \to \GL_n(\mathbb{C})\) with \(n \le 3\), the + image of \(\rho\) is Abelian. \end{proposition} -% I don't think it's worth including the whole proof in here: the case analysis -% is too boring and takes too much space \begin{proof}[Sketch of proof] - % TODO: You haven't commented on the Abelianization in the case with boundary - % It is easy to see that Mod(S_2^b)^ab is a quotient of ℤ/10: the map - % Mod(S_2^b)^ab → Mod(S_2)^ab induced by the inclusion morphism is surjective - Since \(\Mod(S_2^b)^\ab \cong \mathbb{Z}/10\), it suffices to show - \(\rho(\Mod(S_2^b))\) is Abelian, so that \(\rho\) factors through the - Abelianization map \(\Mod(S_2^b) \to \Mod(S_2^b)^\ab\). Equivalenty, it - suffices to show that \(\rho(\Mod(S_2^b)') = 1\). Given \(\alpha \subset - S_2^b\), denote \(L_\alpha = \rho(\tau_\alpha)\). Let \(\alpha_1, - \alpha_2, \mu_1, \mu_2, \gamma, \eta_1, \ldots, \eta_{b - 1} \subset - S_2^b\) be the curves of the Lickorish generators from - Theorem~\ref{thm:lickorish-gens}. + Given \(\alpha \subset S_2^b\), let \(L_\alpha = \rho(\tau_\alpha)\) and + denote by \(E_{\alpha = \lambda} = \{ v \in \mathbb{C}^n : L_\alpha v = + \lambda v \}\) its eigenspaces. Let \(\alpha_1, \alpha_2, \mu_1, \mu_2, + \gamma, \eta_1, \ldots, \eta_{b - 1} \subset S_2^b\) be the curves of the + Lickorish generators from Theorem~\ref{thm:lickorish-gens}. \begin{center} \includegraphics[width=.25\linewidth]{images/lickorish-gens-gen-2.eps} \end{center} - If \(m = 1\) then \(\GL(V) = \mathbb{C}^\times\) is Abelian and hence so is - \(\rho(\Mod(S_2^b))\). Now if \(m = 2\) or \(3\), by + If \(n = 1\) then \(\rho(\Mod(S_2^b)) \subset \GL_1(\mathbb{C}) = + \mathbb{C}^\times\) is Abelian. Now if \(n = 2\) or \(3\), by Propositon~\ref{thm:commutator-normal-gen} it suffices to show \(L_{\alpha_1} = L_{\mu_1}\), so that \(\tau_{\alpha_1} \tau_{\mu_1}^{-1} \in \ker \rho\) - and thus \(\Mod(S_2^b)' \subset \ker \rho\). Given the braid relation + and thus \(\Mod(S_2^b)' \subset \ker \rho\) -- i.e. \(\rho(\Mod(S_2^b))\) is + Abelian. Given the braid relation \begin{equation}\label{eq:braid-rel-induction-basis} L_{\alpha_1} L_{\mu_1} L_{\alpha_1} = L_{\mu_1} L_{\alpha_1} L_{\mu_1}, \end{equation} this amounts to showing \(L_{\alpha_1}\) and \(L_{\mu_1}\) commute. - To that end, we exhausively analyse all of the possible Jordan decompositions + To that end, we exhausively analyse all of the possible Jordan forms \begin{align*} \begin{pmatrix} \lambda & 0 \\ @@ -106,25 +115,25 @@ \end{pmatrix} & \quad{\normalfont(9)} \end{align*} - of \(L_{\mu_2}\) in some basis \(\mathcal{B}\) -- where \(\lambda, \mu, - \nu \in \mathbb{C}^\times\) are all distinct. + of \(L_{\mu_2}\) -- where \(\lambda, \mu, \nu \in \mathbb{C}^\times\) are all + distinct. By changing basis we may assume without loss of generality that the + matrix \(L_{\mu_2}\) is exactly its Jordan form, so that \(E_{\mu_2 = + \lambda} = \mathbb{C} e_1 \oplus \mathbb{C} e_2\). For cases (1) to (7) we use the change of coordinates principle and the braid - relation (\ref{eq:braid-rel-induction-basis}) to show that the matrices of - \(L_{\alpha_1}\) and \(L_{\mu_1}\) in the basis \(\mathcal{B}\) lie in - some Abelian subgroup of \(\GL_m(\mathbb{C})\), \(m = 2\) or \(3\) -- hence - they commute. See \cite[Proposition~5.1]{korkmaz} for further details. - For cases (8) and (9) we consider the curve \(\alpha_2\). In these cases, - the eigenspace \(V_{L_{\mu_2} = \lambda}\) is \(2\)-dimensional. Since - \(L_{\mu_2}\) and \(L_{\alpha_2}\) are conjugate, so is \(V_{L_{\alpha_2} - = \lambda}\) -- indeed, conjugate operators have the same Jordan form. Now - either \(V_{L_{\mu_2} = \lambda} = V_{L_{\alpha_2} = \lambda}\) or - \(V_{L_{\mu_2} = \lambda} \ne V_{L_{\alpha_2} = \lambda}\). We begin by - the first case. - - We claim that if \(V_{L_{\mu_2} = \lambda} = V_{L_{\alpha_2} = \lambda}\) - then \(V_{L_{\alpha_0} = \lambda}\) is \(\Mod(S_2^b)\)-invariant. Indeed, by - change of coordinates we can always find \(f, g, h_i \in \Mod(S_2^b)\) with + relation (\ref{eq:braid-rel-induction-basis}) to show that \(L_{\alpha_1}\) + and \(L_{\mu_1}\) lie in some Abelian subgroup of \(\GL_n(\mathbb{C})\) -- + hence they commute. See \cite[Proposition~5.1]{korkmaz} for further details. + For cases (8) and (9) we consider the curve \(\alpha_2\). In these cases, the + eigenspace \(E_{\mu_2 = \lambda}\) is \(2\)-dimensional. Since \(L_{\mu_2}\) + and \(L_{\alpha_2}\) are conjugate, \(E_{\alpha_2 = \lambda}\) is also + \(2\)-dimensional -- indeed, conjugate operators have the same Jordan form. + Now either \(E_{\mu_2 = \lambda} = E_{\alpha_2 = \lambda}\) or \(E_{\mu_2 = + \lambda} \ne E_{\alpha_2 = \lambda}\). We begin by the first case. + + We claim that if \(E_{\mu_2 = \lambda} = E_{\alpha_2 = \lambda}\) + then \(E_{\mu_2 = \lambda}\) is \(\Mod(S_2^b)\)-invariant. Indeed, by change + of coordinates we can always find \(f, g, h_i \in \Mod(S_2^b)\) with \begin{align*} f \cdot [\mu_2] & = [\mu_1] & @@ -152,136 +161,141 @@ \end{align*} and thus \begin{align*} - V_{L_{\mu_1} = \lambda} - = \rho(f) V_{L_{\mu_2} = \lambda} - & = \rho(f) V_{L_{\alpha_2} = \lambda} - = V_{L_{\alpha_1} = \lambda} + E_{\mu_1 = \lambda} + = \rho(f) E_{\mu_2 = \lambda} + & = \rho(f) E_{\alpha_2 = \lambda} + = E_{\alpha_1 = \lambda} \\ - V_{L_{\alpha_1} = \lambda} - = \rho(g) V_{L_{\mu_2} = \lambda} - & = \rho(g) V_{L_{\alpha_2} = \lambda} - = V_{L_\gamma = \lambda} + E_{\alpha_1 = \lambda} + = \rho(g) E_{\mu_2 = \lambda} + & = \rho(g) E_{\alpha_2 = \lambda} + = E_{\gamma = \lambda} \\ - V_{L_{\eta_i} = \lambda} - = \rho(h_i) V_{L_{\mu_2} = \lambda} - & = \rho(h_i) V_{L_{\alpha_2} = \lambda} - = V_{L_{\alpha_2} = \lambda}. + E_{\eta_i = \lambda} + = \rho(h_i) E_{\mu_2 = \lambda} + & = \rho(h_i) E_{\alpha_2 = \lambda} + = E_{\alpha_2 = \lambda}. \end{align*} - In other words, \(V_{L_{\alpha_1} = \lambda} = V_{L_{\alpha_2} = \lambda} = - V_{L_{\mu_1} = \lambda} = V_{L_{\mu_2} = \lambda} = V_{L_\gamma = \lambda} = - V_{L_{\eta_1} = \lambda} = \cdots = V_{L_{\eta_{b - 1}} = \lambda}\) is + In other words, \(E_{\alpha_1 = \lambda} = E_{\alpha_2 = \lambda} = + E_{\mu_1 = \lambda} = E_{\mu_2 = \lambda} = E_{\gamma = \lambda} = + E_{\eta_1 = \lambda} = \cdots = E_{\eta_{b - 1} = \lambda}\) is invariant under the action of all Lickorish generators. Hence \(\rho\) restricts to a subrepresentation \(\bar \rho : \Mod(S_2^b) \to - \GL(V_{L_{\mu_2} = \lambda})\). By case (2), \(\bar \rho(f) = 1\) for all - \(f \in \Mod(S_2^b)'\), for \(\bar \rho(\Mod(S_2^b))\) is Abelian. In other - words, the matrix of \(\rho(f)\) in the basis \(\mathcal{B}\) has the form + \GL(E_{\mu_2 = \lambda}) = \GL_2(\mathbb{C})\) -- recall \(E_{\mu_2 = + \lambda} = \mathbb{C} e_1 \oplus \mathbb{C} e_2\). By case (2), \(\bar + \rho(f) = 1\) for all \(f \in \Mod(S_2^b)'\), given that \(\bar + \rho(\Mod(S_2^b))\) is Abelian. Thus \[ + \rho(\Mod(S_2^b)') \subset \begin{pmatrix} 1 & 0 & * \\ 0 & 1 & * \\ 0 & 0 & * \end{pmatrix} \] - and, in particular, it lies inside the group of upper triangular matrices -- - a solvalbe subgroup of \(\GL_3(\mathbb{C})\). Now by - Proposition~\ref{thm:commutator-is-perfect} we get \(\rho(\Mod(S_2^b)') = - 1\): any homomorphism from a perfect group to a solvable group is trivial. + lies inside the group of upper triangular matrices, a solvalbe subgroup of + \(\GL_3(\mathbb{C})\). Now by Proposition~\ref{thm:commutator-is-perfect} we + get \(\rho(\Mod(S_2^b)') = 1\): any homomorphism from a perfect group to a + solvable group is trivial. - Finally, if \(V_{L_{\mu_2} = \lambda} \ne V_{L_{\alpha_2} = \lambda}\) and + Finally, if \(E_{\mu_2 = \lambda} \ne E_{\alpha_2 = \lambda}\) and the Jordan form of \(L_{\mu_2}\) is given by (8) then \[ 0 - \subsetneq V_{L_{\mu_2} = \lambda} \cap V_{L_{\alpha_2} = \lambda} - \subsetneq V_{L_{\mu_2} = \lambda} + \subsetneq E_{\mu_2 = \lambda} \cap E_{\alpha_2 = \lambda} + \subsetneq E_{\mu_2 = \lambda} \subsetneq V \] is a flag of subspaces invariant under \(L_{\mu_1}\) and \(L_{\alpha_1}\), for \(\mu_2\) is disjoint from \(\mu_1 \cup \alpha_1\) and thus \([\tau_{\mu_2}, \tau_{\mu_1}] = [\tau_{\mu_2}, \tau_{\alpha_1}] = 1\). In - this case we can find a basis \(\mathcal{B}'\) for \(V\) in wich the matrices - of \(L_{\mu_1}\) and \(L_{\alpha_1}\) are both upper triangular with - \(\lambda\) along the diagonal: take \(\mathcal{B}' = \{v_1, v_2, v_3\}\) - with \(v_1 \in V_{L_{\mu_2} = \lambda} \cap V_{L_{\alpha_2} = \lambda}\), - \(v_2 \in V_{L_{\mu_2}}\) and adjust \(v_3\) to get the desired diagonal - entry. Any such pair of matrices satisfying the braid relation + this case we can find a basis for \(\mathbb{C}^3\) with respect to wich the + matrices of \(L_{\mu_1}\) and \(L_{\alpha_1}\) are both upper triangular with + \(\lambda\) along the diagonal: take \(v_1, v_2, v_3 \in \mathbb{C}^3\) with + \(v_1 \in E_{\mu_2 = \lambda} \cap E_{\alpha_2 = \lambda}\), \(v_2 \in + V_{L_{\mu_2}}\) and adjust \(v_3\) to get the desired diagonal entry. Any + such pair of matrices satisfying the braid relation (\ref{eq:braid-rel-induction-basis}) commute. - Similarly, if \(L_{\mu_2}\) has Jordan form (9) and \(V_{L_{\mu_2} = \lambda} - \ne V_{L_{\alpha_2} = \lambda}\) we use (\ref{eq:braid-rel-induction-basis}) - to conclude \([L_{\mu_1}, L_{\alpha_1}] = 1 \in \GL(V)\) -- again, see - \cite[Proposition~5.1]{korkmaz} for further details. We are done. + Similarly, if \(L_{\mu_2}\) has Jordan form (9) and \(E_{\mu_2 = \lambda} + \ne E_{\alpha_2 = \lambda}\) we use (\ref{eq:braid-rel-induction-basis}) + to conclude \(L_{\mu_1}\) and \(L_{\alpha_1}\) commute -- again, see + \cite[Proposition~5.1]{korkmaz}. We are done. \end{proof} -\begin{proof}[Proof of Theorem~\ref{thm:low-dim-reps-are-trivial}] - Let \(g \ge 3\), \(b \ge 0\) and \(\rho : \Mod(S_g^b) \to \GL(V)\) be an - \(m\)-dimensional representation with \(m < 2g\). +We are now ready to establish the triviality of low-dimensional +representations. - As promised, we proceed by induction on \(g\). If \(g = 1\) then \(m = 1\) - and thus \(\rho(\Mod(S_g^b)) \subset \GL(V) = \mathbb{C}^\times\) is Abelian. - The base case \(g = 2\) was also established in - Proposition~\ref{thm:low-dim-reps-are-trivial-base-case}. Now suppose \(g \ge - 3\) and every \(n\)-dimensional representation of \(S_{g - 1}^c\) has Abelian - image for \(n < 2(g - 1)\) and \(c \ge 0\). Let us show \(\rho\) has Abelian - image. +\begin{proof}[Proof of Theorem~\ref{thm:low-dim-reps-are-trivial}] + Let \(g \ge 1\), \(b \ge 0\) and fix \(\rho : \Mod(S_g^b) \to + \GL_n(\mathbb{C})\) with \(n < 2g\). As promised, we proceed by induction on + \(g\). The base case \(g = 1\) is again clear from the fact \(n = 1\) and + \(\GL_1(\mathbb{C}) = \mathbb{C}^\times\). The case \(g = 2\) was also + established in Proposition~\ref{thm:low-dim-reps-are-trivial-base-case}. Now + suppose \(g \ge 3\) and every \(m\)-dimensional representation of \(S_{g - + 1}^{b'}\) has Abelian image for \(m < 2(g - 1)\). Let us show \(\rho\) has + Abelian image. Let \(\alpha_1, \ldots, \alpha_g, \mu_1, \ldots, \mu_g, \gamma_1, \ldots, \gamma_{g - 1}, \beta_1, \ldots, \beta_{b - 1} \subset S_g^b\) be the curves from the Lickorish generators of \(\Mod(S_g^b)\), as in - Theorem~\ref{thm:lickorish-gens}. Once again, denote \(L_\alpha = - \rho(\tau_\alpha)\) for any closed \(\alpha \subset S_g^b\). Let \(R \cong - S_{g - 1}^1\) be the closed subsurface highlighted in the following picture. + Theorem~\ref{thm:lickorish-gens}. Once again, let \(L_\alpha = + \rho(\tau_\alpha)\) and denote by \(E_{\alpha = \lambda}\) the eigenspace of + \(L_\alpha\) associated to \(\lambda \in \mathbb{C}\). Let \(R \cong S_{g - + 1}^1\) be the closed subsurface highlighted in the following picture. \begin{center} \includegraphics[width=.5\linewidth]{images/lickorish-gens-korkmaz-proof.eps} \end{center} % TODO: Add more comments on the injectivity of this map? - We claim that it suffices to find a \(\Mod(R)\)-invariant\footnote{Here we - view $\Mod(R)$ as a subgroup of $\Mod(S_g^b)$ via the inclusion homomorphism - $\Mod(R) \to \Mod(S_g^b)$ from Example~\ref{ex:inclusion-morphism}, which can - be shown to be injective in this particular case.} subspace \(W \subset V\) - of dimension \(n\) with \(2 \le n \le m - 2\). Indeed, in this case \(n < 2(g - - 1)\) and \(\dim \mfrac{V}{W} = m - n < 2(g - 1)\). Thus both - representations + We claim that it suffices to find a \(m\)-dimensional + \(\Mod(R)\)-invariant\footnote{Here we view $\Mod(R)$ as a subgroup of + $\Mod(S_g^b)$ via the inclusion homomorphism $\Mod(R) \to \Mod(S_g^b)$ from + Example~\ref{ex:inclusion-morphism}, which can be shown to be injective in + this particular case.} subspace \(W \subset \mathbb{C}^n\) with \(2 \le m \le + n - 2\). Indeed, in this case \(m < 2(g - 1)\) and \(\dim + \mfrac{\mathbb{C}^n}{W} = n - m < 2(g - 1)\). Thus both representations \begin{align*} - \rho_1 : \Mod(R) & \to \GL(W) & \rho_2 : \Mod(R) & \to \GL(\mfrac{V}{W}) + \rho_1 : \Mod(R) & \to \GL(W) \cong \GL_m(\mathbb{C}) + & + \rho_2 : \Mod(R) & \to \GL(\mfrac{\mathbb{C}^n}{W}) + \cong \GL_{n - m}(\mathbb{C}) \end{align*} fall into the induction hypotesis -- i.e. \(\rho_i(\Mod(R))\) is Abelian. In particular, \(\rho_i(\Mod(R)') = 1\) and we can find some - basis for \(V\) under which + basis for \(\mathbb{C}^n\) with respect to which \[ - % TODO: Make this prettier: somehow format the block sizes in the equation \rho(f) = \left( \begin{array}{c|c} - 1 & * \\ \hline - 0 & 1 + 1_m & * \\ \hline + 0 & 1_{n - m} \end{array} \right) \] - for any \(f \in \Mod(R)'\) -- where the first and second diaogonal blocks are - \(n \times n\) and \((m - n) \times (m - n)\). Since the group of upper - triangular matrices is solvable, it follows from - Proposition~\ref{thm:commutator-is-perfect} that \(\rho\) annihilates all - \(\Mod(R)'\) and, in particular, \(\tau_{\alpha_1} \tau_{\mu_1}^{-1} \in \ker - \rho\). But recall from Proposition~\ref{thm:commutator-normal-gen} that - \(\Mod(S_g^b)'\) is normally generated by \(\tau_{\alpha_1} - \tau_{\mu_1}^{-1}\), from which we conclude \(\rho(\Mod(S_g^b)') = 1\), as - desired. - - As before, we exhaustively analyse all possible Jordan forms for + for all \(f \in \Mod(R)'\) -- where \(1_k\) denotes the \(k \times k\) + identity matrix. Since the group of upper triangular matrices is solvable, it + follows from Proposition~\ref{thm:commutator-is-perfect} that \(\rho\) + annihilates all of \(\Mod(R)'\) and, in particular, \(\tau_{\alpha_1} + \tau_{\mu_1}^{-1} \in \ker \rho\). But recall from + Proposition~\ref{thm:commutator-normal-gen} that \(\Mod(S_g^b)'\) is normally + generated by \(\tau_{\alpha_1} \tau_{\mu_1}^{-1}\), from which we conclude + \(\rho(\Mod(S_g^b)') = 1\), as desired. + + As before, we exhaustively analyse all possible Jordan forms of \(L_{\mu_g}\). First, consider the case where we can find eigenvalues \(\lambda_1, \ldots, \lambda_k\) of \(L_{\mu_g}\) such that the sum \(W = - \bigoplus_i V_{L_{\mu_g} = \lambda_i}\) of the corresponding eigenspaces has - dimension \(n\) with \(2 \le n \le m - 2\). In this case, it suffices to - observe that since \(\mu_g\) lies outside of \(R\), each \(V_{L_{\mu_g} = + \bigoplus_i E_{\mu_g = \lambda_i}\) of the corresponding eigenspaces has + dimension \(m\) with \(2 \le m \le n - 2\). In this case, it suffices to + observe that since \(\mu_g\) lies outside of \(R\), each \(E_{\mu_g = \lambda_i}\) is \(\Mod(R)\)-invariant: the Lickorish generators \(\tau_{\alpha_1}, \ldots, \tau_{\alpha_{g - 1}}, \tau_{\mu_1}, \ldots, - \tau_{\mu_{g - 1}}, \tau_{\gamma_1}, \ldots, \tau_{\gamma_{g - 2}}\) of \(R - \cong S_{g - 1}^1\) all commute with \(\tau_{\mu_g}\) and thus preserve the - eigenspaces of it's action on \(V\). + \tau_{\mu_{g - 1}}\), \(\tau_{\gamma_1}, \ldots, \tau_{\gamma_{g - 2}}\) of + \(R \cong S_{g - 1}^1\) all commute with \(\tau_{\mu_g}\) and thus preserve + the eigenspaces of its action on \(\mathbb{C}^n\). - If no sum of the form \(\bigoplus_i V_{L_{\mu_g} = \lambda_i}\) has + If no sum of the form \(\bigoplus_i E_{\mu_g = \lambda_i}\) has dimension lying between \(2\) and \(m - 2\) there must be at most \(2\) distinct eigenvalues and all eigenspaces must be either \(1\)-dimensional or \((m - 1)\)-dimensional. Hence then the Jordan form of \(L_{\mu_g}\) has to @@ -323,29 +337,27 @@ \end{pmatrix} & \quad{\normalfont(4)} \end{align*} - for \(\lambda \ne \mu\). We now analyze each one of these sporadic cases + for \(\lambda \ne \mu\). We analyze each one of these sporadic cases individually. For case (1), we use the change of coordinates principle: each \(L_{\alpha_i}, L_{\mu_i}, L_{\gamma_i}, L_{\eta_i}\) is conjugate to \(L_{\mu_g} = \lambda\), so all Lickorish generators of \(\Mod(S_g^b)\) act - on \(V\) as scalar multiplication by \(\lambda\) as well. Hence - \(\rho(\Mod(S_g^b))\) is cyclic and thus Abelian. In case (2) \(W = \ker - (L_{\alpha_{2 - g}} - \lambda)^2\) is a \(2\)-dimensional - \(\Mod(R)\)-invariant subspace. - - For cases (3) and (4) we consider two situations: \(V_{L_{\mu_g} = - \lambda} \ne V_{L_{\alpha_g} = \lambda}\) or \(V_{L_{\mu_g} = - \lambda} = V_{L_{\alpha_g} = \lambda}\). In the first case, \(W = - V_{L_{\mu_g} = \lambda} \cap V_{L_{\alpha_g} = \lambda}\) is a - \((m - 2)\)-dimensional \(\Mod(R)\)-invariant subspace: since \(L_{\alpha_{2 - - g}}\) and \(L_{\alpha_g}\) are conjugate and \(\alpha_g\) lies - outside of \(R\), both \(V_{L_{\mu_g} = \lambda}\) and - \(V_{L_{\alpha_g} = \lambda}\) are \(\Mod(R)\)-invariant \((m - - 1)\)-dimensional subspaces. - - Finally, we consider the case where \(V_{L_{\mu_g} = \lambda} = - V_{L_{\alpha_g} = \lambda}\). In this situation, as in the proof of + on \(\mathbb{C}^n\) as scalar multiplication by \(\lambda\) as well. Hence + \(\rho(\Mod(S_g^b))\) is cyclic and thus Abelian. In case (2), \(W = \ker + (L_{\mu_g} - \lambda)^2\) is a \(2\)-dimensional \(\Mod(R)\)-invariant + subspace. + + For cases (3) and (4) we consider two situations: \(E_{\mu_g = \lambda} \ne + E_{\alpha_g = \lambda}\) or \(E_{\mu_g = \lambda} = E_{\alpha_g = \lambda}\). + In the first case, \(W = E_{\mu_g = \lambda} \cap E_{\alpha_g = \lambda}\) is + a \((m - 2)\)-dimensional \(\Mod(R)\)-invariant subspace: since \(L_{\mu_g}\) + and \(L_{\alpha_g}\) are conjugate and \(\alpha_g\) lies outside of \(R\), + both \(E_{\mu_g = \lambda}\) and \(E_{\alpha_g = \lambda}\) are + \(\Mod(R)\)-invariant \((m - 1)\)-dimensional subspaces. + + Finally, we consider the case where \(E_{\mu_g = \lambda} = + E_{\alpha_g = \lambda}\). In this situation, as in the proof of Proposition~\ref{thm:low-dim-reps-are-trivial-base-case} it follows from the change of coordinates principle that there are \(f_i, g_i, h_i \in \Mod(S_g^b)\) with @@ -364,14 +376,14 @@ \end{align*} and thus \[ - V_{L_{\alpha_1} = \lambda} = \cdots = V_{L_{\alpha_g} = \lambda} - = V_{L_{\mu_1} = \lambda} = \cdots = V_{L_{\mu_g} = \lambda} - = V_{L_{\gamma_1} = \lambda} = \cdots = V_{L_{\gamma_{g - 1}} = \lambda} - = V_{L_{\eta_1} = \lambda} = \cdots = V_{L_{\eta_{b - 1}} = \lambda}. + E_{\mu_1 = \lambda} = \cdots = E_{\mu_g = \lambda} + = E_{\alpha_1 = \lambda} = \cdots = E_{\alpha_g = \lambda} + = E_{\gamma_1 = \lambda} = \cdots = E_{\gamma_{g - 1} = \lambda} + = E_{\eta_1 = \lambda} = \cdots = E_{\eta_{b - 1} = \lambda}. \] - In particular, we can find a basis for \(V\) under which the matrix of all - Lickorish generators has the form + In particular, we can find a basis for \(\mathbb{C}^n\) with respect to which + the matrix of any Lickorish generators has the form \[ \begin{pmatrix} \lambda & 0 & \cdots & 0 & * \\ @@ -382,15 +394,128 @@ \end{pmatrix}. \] Since the group of upper triangular matrices is solvable and \(\Mod(S_g^b)\) - is perfect, it follows that \(\rho(\Mod(S_g^b))\) is trivial. We are done. + is perfect, it follows that \(\rho(\Mod(S_g^b))\) is trivial. This concludes + the proof \(\rho(\Mod(S_g^b))\) is Abelian. + + To see that \(\rho(\Mod(S_g^b)) = 1\) for \(g \ge 3\) we note that, since + \(\rho(\Mod(S_g^b))\) is Abelian, \(\rho\) factors though the Abelinization + map \(\Mod(S_g^b) \to \Mod(S_g^b)^\ab = \mfrac{\Mod(S_g^b)}{[\Mod(S_g^b), + \Mod(S_g^b)]}\) Now recall from Proposition~\ref{thm:trivial-abelianization} + that \(\Mod(S_g^b)^\ab = 0\) for \(g \ge 3\). In other words, \(\rho\) + factors though the homomorphism \(1 \to \GL_n(\mathbb{C})\). We are done. \end{proof} -\begin{theorem}[Korkmaz \cite{korkmaz}] - Let \(g \ge 3\) and \(\rho : \Mod(S_g^b) \to \GL(V)\) be a \(2g\)-dimensional - linear representation. Then either \(\rho\) is either trivial or conjugate to - the symplectic representation\footnote{Here the map \(\Mod(S_g^b) \to - \operatorname{Sp}_{2g}(\mathbb{Z})\) is given by the composition of the - inclusion morphism \(\Mod(S_g^b) \to \Mod(S_g)\) with the usual symplect - representation \(\psi : \Mod(S_g) \to \operatorname{Sp}_{2g}(\mathbb{Z})\).} +Having established the triviality of the low-dimensional representations \(\rho +: \Mod(S_g^b) \to \GL_n(\mathbb{C})\), all that remains for us is to understand +the \(2g\)-dimensional reprensentations of \(\Mod(S_g^b)\). We certainly know a +nontrivial example of such, namely the symplectic representation \(\psi : +\Mod(S_g) \to \operatorname{Sp}_{2g}(\mathbb{Z})\) from +Example~\ref{ex:symplectic-rep}. Surprinsgly, this turns out to be +\emph{essentially} the only example of a nontrivial \(2g\)-dimensional +representation in the compact case. More precisely, + +\begin{theorem}[Korkmaz]\label{thm:reps-of-dim-2g-are-symplectic} + Let \(g \ge 3\) and \(\rho : \Mod(S_g^b) \to \GL_{2g}(\mathbb{C})\). Then + \(\rho\) is either trivial or conjugate to the symplectic + representation\footnote{Here the map $\Mod(S_g^b) \to + \operatorname{Sp}_{2g}(\mathbb{Z})$ is given by the composition of the + inclusion morphism $\Mod(S_g^b) \to \Mod(S_g)$ with the usual symplect + representation $\psi : \Mod(S_g) \to \operatorname{Sp}_{2g}(\mathbb{Z})$.} \(\Mod(S_g^b) \to \operatorname{Sp}_{2g}(\mathbb{Z})\) of \(\Mod(S_g^b)\). \end{theorem} + +Unfortunately, the limited scope of these master thesis does not allow us to +dive into the proof of Theorem~\ref{thm:reps-of-dim-2g-are-symplectic}. The +heart of this proof lies in a somewhat technical result about representations +of the product \(B_3^n = B_3 \times \cdots \times B_3\), which Korkmaz refers +to as \emph{the main lemma}. Namely\dots + +\begin{lemma}[Korkmaz' Main Lemma]\label{thm:main-lemma} + Given \(i = 1, \ldots, n\), denote by \newline \(a_i = (1, \ldots, 1, + \sigma_1, 1, \ldots 1)\) and \(b_i = (1, \ldots, 1, \sigma_2, 1, \ldots, 1)\) + the \(n\)-tuples in \(B_3^n\) whose \(i\)-th coordinates are \(\sigma_1\) and + \(\sigma_2\), respectively, and with all other coordinates equal to \(1\). + Let \(m \ge 2n\) and \(\rho : B_3^n \to \GL_m(\mathbb{C})\) be a + representation satisfying: + \begin{enumerate} + \item The only eigenvalue of \(\rho(a_i)\) is \(1\) and it's eigenspace is + \((2g - 1)\)-dimensional. + \item The eigenspaces of \(\rho(a_i)\) and \(\rho(b_i)\) associated to the + eigenvalue \(1\) do not coincide. + \end{enumerate} + Then \(\rho\) is conjugate to the representation + \begin{align*} + B_3^n & \to \GL_m(\mathbb{C}) \\ + a_i + & \mapsto + \left( + \begin{array}{c|c|c} + 1_{2(i-1)} & 0 & 0 \\ \hline + 0 & \begin{array}{cc} 1 & 1 \\ 0 & 1 \end{array} & 0 \\ \hline + 0 & 0 & 1_{m-2i} + \end{array} + \right) \\ + b_i + & \mapsto + \left( + \begin{array}{c|c|c} + 1_{2(i-1)} & 0 & 0 \\ \hline + 0 & \begin{array}{cc} 1 & 0 \\ -1 & 1 \end{array} & 0 \\ \hline + 0 & 0 & 1_{m-2i} + \end{array} + \right), + \end{align*} + where \(1_k\) denotes the \(k \times k\) identity matrix. +\end{lemma} + +This is proved in \cite[Lemma 7.6]{korkmaz} using the braid relations. Notice +that for \(n = g\) and \(m = 2g\) the matrices in +Lemma~\ref{thm:main-lemma} coincide with the action of +the Lickrish generators \(\tau_{\mu_1}, \ldots, \tau_{\mu_g}, \tau_{\alpha_1}, +\ldots, \tau_{\alpha_g} \in \Mod(S_g^b)\) on \(H_1(S_g, \mathbb{C}) \cong +\mathbb{C}^{2g}\) -- represented in the standard basis \([\mu_1], \ldots, +[\mu_g], [\alpha_1], \ldots, [\alpha_g]\) for \(H_1(S_g, \mathbb{C})\). +\begin{align*} + (\tau_{\mu_i})_* & = + \left( + \begin{array}{c|c|c} + 1 & 0 & 0 \\ \hline + 0 & \begin{array}{cc} 1 & 1 \\ 0 & 1 \end{array} & 0 \\ \hline + 0 & 0 & 1 + \end{array} + \right) & + (\tau_{\alpha_i})_* & = + \left( + \begin{array}{c|c|c} + 1 & 0 & 0 \\ \hline + 0 & \begin{array}{cc} 1 & 0 \\ -1 & 1 \end{array} & 0 \\ \hline + 0 & 0 & 1 + \end{array} + \right) +\end{align*} + +Hence by embeding \(B_3^g\) in \(\Mod(S_g^b)\) via +\begin{align*} + B_3^g & \to \Mod(S_g^b) \\ + a_i & \mapsto \tau_{\mu_i} \\ + b_i & \mapsto \tau_{\alpha_i} +\end{align*} +we can see that any \(\rho : \Mod(S_g^b) \to \GL_{2g}(\mathbb{C})\) in a +certain class of representation satisfying some technical conditions must be +conjugate to the symplectic representation \(\Mod(S_g^b) \to +\operatorname{Sp}_{2g}(\mathbb{Z})\) when restricted to \(B_3^g\). + +Korkmaz then goes on to show that such technical conditions are met for any +nontrivial \(\rho : \Mod(S_g^b) \to \GL_{2g}(\mathbb{C})\). Furthermore, +Korkmaz also argues that we can find a basis for \(\mathbb{C}^{2g}\) with +respect to which the matrices of \(\rho(\tau_{\gamma_1}), \ldots, +\rho(\tau_{\gamma_{g - 1}}), \rho(\tau_{\eta_1}), \ldots, +\rho(\tau_{\eta_{b-1}})\) also agrees with the action of \(\Mod(S_g^b)\) on +\(H_1(S_g, \mathbb{C})\), concluding the classification of \(2g\)-dimensional +representations. + +% TODO: Add some final comments about how the rest of the landscape of +% representations is generally unknown and how there is a lot to study in here +Recently, Kasahara also classified the \((2g+1)\)-dimensional representations +of \(\Mod(S_g^b)\) for \(g \ge 7\) in terms of certain twisted \(1\)-cohomology +groups \cite{kasahara}.
diff --git a/sections/twists.tex b/sections/twists.tex @@ -178,13 +178,13 @@ each corresponding to one of the standard generators \begin{align*} \begin{pmatrix} - 1 & -1 \\ - 0 & 1 + 1 & 1 \\ + 0 & 1 \end{pmatrix} && \begin{pmatrix} - 1 & 0 \\ - 1 & 1 + 1 & 0 \\ + -1 & 1 \end{pmatrix} \end{align*} of \(\operatorname{SL}_2(\mathbb{Z})\).