# Wednesday, August 26 ## Review - $G$ a reductive algebraic group over $k$ - $T = \prod_{i=1}^n \GG_m$ a maximal split torus - $\lieg = \mathrm{Lie}(G)$ - There's an induced root space decomposition $\lieg = t\oplus \bigoplus_{\alpha\in \Phi}\lieg_\alpha$ - When $G$ is simple, $\Phi$ is an *irreducible* root system - There is a classification of these by Dynkin diagrams :::{.example} $A_n$ corresponds to $\liesl(n+1, k)$ (mnemonic: $A_1$ corresponds to $\liesl(2)$) ::: - We have representations $\rho: G\to \GL(V)$, i.e. $V$ is a $G\dash$module - For $T\subseteq G$, we have a weight space decomposition: $V = \bigoplus_{\lambda \in X(T)} V_\lambda$ where $X(T) = \hom(T, \GG_m)$. > Note that $X(T) \cong \ZZ^n$, the number of copies of $\GG_m$ in $T$. ## Root Systems and Weights :::{.example} Let $\Phi = A_2$, then we have the following root system: ![Image](figures/image_2020-08-26-14-05-58.png) ::: In general, we'll have $\Delta = \ts{\alpha_1, \cdots, \alpha_n}$ a basis of *simple roots*. :::{.remark} Every root $\alpha\in I$ can be expressed as either positive integer linear combination (or negative) of simple roots. ::: For any $\alpha\in \Phi$, let $s_\alpha$ be the reflection across $H_\alpha$, the hyperplane orthogonal to $\alpha$. Then define the *Weyl group* $W = \ts{s_\alpha \st \alpha\in \Phi}$. :::{.example} Here the Weyl group is $S_3$: ![Image](figures/image_2020-08-26-14-10-24.png) ::: :::{.remark} $W$ acts transitively on bases. ::: :::{.remark} $X(T) \subseteq \ZZ\Phi$, recalling that $X(T) = \hom(T, \GG_m) = \ZZ^n$ for some $n$. Denote $\ZZ\Phi$ the *root lattice* and $X(T)$ the *weight lattice*. ::: :::{.example} Let $G = \liesl(2, \CC)$ then $X(T) = \ZZ\omega$ where $\omega = 1$, $\ZZ \Phi = \ZZ\ts{\alpha}$ Then there is one weight $\alpha$, and the root lattice $\ZZ\Phi$ is just $2\ZZ$. However, the weight lattice is $\ZZ\omega = \ZZ$, and these are not equal in general. ::: :::{.remark} There is partial ordering on $X(T)$ given by $\lambda \geq \mu \iff \lambda - \mu = \sum_{\alpha\in \Delta} n_\alpha \alpha$ where $n_\alpha \geq 0$. (We say $\lambda$ *dominates* $\mu$.) ::: :::{.definition title="Fundamental Dominant Weights"} We extend scalars for the weight lattice to obtain $E \da X(T) \tensor_\ZZ \RR \cong \RR^n$, a Euclidean space with an inner product $\inner{\wait}{\wait}$. For $\alpha\in \Phi$, define its *coroot* $\alpha\dual \da {2\alpha \over \inner{\alpha}{\alpha}}$. Define the *simple coroots* as $\Delta\dual \da \ts{\alpha_i\dual}_{i=1}^n$, which has a dual basis $\Omega \da \ts{\omega_i}_{i=1}^n$ the *fundamental weights*. These satisfy $\inner{\omega_i}{\alpha_j\dual} = \delta_{ij}$. \todo[inline]{What is the notation for fundamental weights? Definitely not $\Omega$ usually!} > Important because we can index irreducible representations by fundamental weights. A weight $\lambda\in X(T)$ is *dominant* iff $\lambda \in \ZZ^{\geq 0} \Omega$, i.e. $\lambda = \sum n_i \omega_i$ with $n_i \in \ZZ^{\geq 0}$. ::: If $G$ is simply connected, then $X(T) = \bigoplus \ZZ \omega_i$. > See Jantzen for definition of simply-connected, $\SL(n+1)$ is simply connected but its adjoint $PGL(n+1)$ is not simply connected. ## Complex Semisimple Lie Algebras When doing representation theory, we look at the Verma modules $Z(\lambda) = U(\lieg) \tensor_{U(\lieb^+)} \lambda \surjects L(\lambda)$. :::{.theorem title="?"} $L(\lambda)$ as a finite-dimensional $U(\lieg)\dash$module $\iff$ $\lambda$ is dominant, i.e. $\lambda \in X(T)_+$. ::: Thus the representations are indexed by lattice points in a particular region: ![Image](figures/image_2020-08-26-14-36-44.png) **Question 1**: Suppose $G$ is a simple (simply connected) algebraic group. How do you parameterize *irreducible* representations? For $\rho: G\to \GL(V)$, $V$ is a *simple module* (an *irreducible representation*) iff the only proper $G\dash$submodules of $V$ are trivial. **Answer 1**: They are also parameterized by $X(T)_+$. We'll show this using the induction functor $\ind_B^G \lambda =H^0(G/B, \mathcal{L}(\lambda))$ (sheaf cohomology of the flag variety with coefficients in some line bundle). > We'll define what $B$ is later, essentially upper-triangular matrices. **Question 2**: What are the dimensions of the irreducible representations for $G$? **Answer 2**: Over $k=\CC$ using Weyl's dimension formula. For $k = \bar{\FF}_p$: conjectured to be known for $p\geq h$ (the *Coxeter number*), but by Williamson (2013) there are counterexamples. Current work being done!