- Commit
- 0e1431c14f50b0e751ce3d5de0774dd80765ca88
- Parent
- 19e1433e29d6cee5a45673518a4fa6beaf4550b6
- Author
- Pablo <pablo-escobar@riseup.net>
- Date
Added comments on the lack of functoriality of some of the constructions in the last chapter
Source code for my notes on representations of semisimple Lie algebras and Olivier Mathieu's classification of simple weight modules
Added comments on the lack of functoriality of some of the constructions in the last chapter
1 file changed, 28 insertions, 15 deletions
Status | File Name | N° Changes | Insertions | Deletions |
Modified | sections/mathieu.tex | 43 | 28 | 15 |
diff --git a/sections/mathieu.tex b/sections/mathieu.tex @@ -527,15 +527,8 @@ follows. \begin{definition} A coherent family \(\mathcal{M}\) is called \emph{simple} if it contains no proper coherent subfamilies -- i.e. \(\mathcal{M}\) is a simple object in the - full subcategory of coherent families. Equivalently\footnote{It is easy to - see that if $\mathcal{M}_\lambda$ is a simple - $\mathcal{U}(\mathfrak{g})_0$-module for some $\lambda \in \mathfrak{h}^*$ - then $\mathcal{M}$ is a simple object in the category of coherent families, - for if $\mathcal{N} \subset \mathcal{M}$ is a nonzero coherent subfamily - $\mathcal{N}_\lambda = \mathcal{M}_\lambda$ and therefore $\deg \mathcal{N} = - \deg \mathcal{M}$, which implies $\mathcal{N} = \mathcal{M}$. The converse is - also true, but its proof was deemed too technical to be included in here.}, - we call \(\mathcal{M}\) simple if \(\mathcal{M}_\lambda\) is a simple + full subcategory of coherent families. Equivalently, we call \(\mathcal{M}\) + simple if \(\mathcal{M}_\lambda\) is a simple \(\mathcal{U}(\mathfrak{g})_0\)-module for some \(\lambda \in \mathfrak{h}^*\). \end{definition} @@ -556,8 +549,6 @@ to a completely reducible coherent extension of \(V\). \(\mathcal{M}[\lambda]\) has finite length as a \(\mathfrak{g}\)-module. \end{lemma} -% TODOO: Point out this construction is NOT functorial, since it depends on the -% choice of composition series \begin{corollary} Let \(\mathcal{M}\) be a coherent family of degree \(d\). There exists a unique completely reducible coherent family @@ -568,7 +559,13 @@ to a completely reducible coherent extension of \(V\). Namely, if \(\lambda \in \mathfrak{h}^*\) and \(0 = \mathcal{M}_{\lambda 0} \subset \mathcal{M}_{\lambda 1} \subset \cdots \subset \mathcal{M}_{\lambda - n_\lambda} = \mathcal{M}[\lambda]\) is a composition series, + n_\lambda} = \mathcal{M}[\lambda]\) is a composition series\footnote{Notice + that $\mathcal{M}[\lambda] = \mathcal{N}[\mu]$ for any $\mu \in \lambda + Q$. + Hence the sum $\bigoplus_{\lambda + Q \in \mfrac{\mathfrak{h}^*}{Q}} + \bigoplus_i \mfrac{\mathcal{M}_{\lambda i + 1}}{\mathcal{M}_{\lambda i}}$ is + independant of the choice of representative for $\lambda + Q$ -- at least as + long as we choose $\mathcal{M}_{\lambda i} = \mathcal{M}_{\mu i}$ for all + $\mu \in \lambda + Q$ and $i$.}, \[ \mathcal{M}^{\operatorname{ss}} \cong \bigoplus_{\substack{\lambda + Q \in \mfrac{\mathfrak{h}^*}{Q} \\ i}} @@ -636,6 +633,20 @@ to a completely reducible coherent extension of \(V\). is polynomial in \(\mu \in \mathfrak{h}^*\). \end{proof} +\begin{note} + Althought we have provided an explicit construction of + \(\mathcal{M}^{\operatorname{ss}}\) in terms of \(\mathcal{M}\), we should + point out this construction is not fuctorial. First, given an intertwiner \(T + : \mathcal{M} \to \mathcal{N}\) between coherent families, it is unclear what + \(T^{\operatorname{ss}} : \mathcal{M}^{\operatorname{ss}} \to + \mathcal{N}^{\operatorname{ss}}\) is supposed to be. Secondly, and this is + more relevant, our construction depends on the choice of composition series + \(0 = \mathcal{M}_{\lambda 0} \subset \cdots \subset \mathcal{M}_{\lambda + n_\lambda} = \mathcal{M}[\lambda]\). While different choices of composition + series yield isomorphic results, there is no canonical isomorphism. + In addition, there is no canonical choice of composition series. +\end{note} + As promised, if \(\mathcal{M}\) is a coherent extension of \(V\) then so is \(\mathcal{M}^{\operatorname{ss}}\). @@ -1290,10 +1301,12 @@ It should now be obvious\dots There exists a coherent extension \(\mathcal{M}\) of \(V\). \end{proposition} -% TODOO: Point out that here we have to fix representatives of the cosets, so -% this construction is, once again, not functorial \begin{proof} - Take + Take\footnote{Here we fix some $\lambda_t \in t$ for each $Q$-coset $t \in + \mfrac{\mathfrak{h}^*}{Q}$. While there is a natural isomorphism + $\theta_\lambda \Sigma^{-1} V \isoto \theta_\mu \Sigma^{-1} V$ for each $\mu + \in \lambda + Q$, they are not the same representation strictly speaking. + This is yet another obstruction to the functoriality of our constructions.} \[ \mathcal{M} = \bigoplus_{\lambda + Q \in \mfrac{\mathfrak{h}^*}{Q}}