# Friday February 7th So far, we have $\chi_\lambda = \chi_{w.\cdot \lambda}$ if $\lambda \in \Lambda$ and $w\in W$. We have $\lieh\dual \supset \Lambda$ which is topologically equivalent to $\AA^\ell \supset \ZZ^\ell$, where $\ZZ^\ell$ is dense in the Zariski topology. For $z\in \mcz(\lieg)$, we have $\chi_\lambda(z) = \chi_{W\cdot \lambda} (z)$ and so $\lambda(\xi(z)) = (w\cdot \lambda )(\xi(z))$ where $\xi: \mcz(\lieg) \to U(\lieh) = S(\lieh) \cong P(\lieh\dual)$ where we send $\lambda(f)$ to $f(\lambda)$. Then $\xi(z)(\lambda) = \xi(z)(w\cdot \lambda)$ for all $\lambda \in \Lambda$, and so $\xi(z) = w\inv \xi(z)$ on $\Lambda$. But both sides here are polynomials and thus continuous, and $\Lambda \subset \lieh\dual$ is dense, so $\xi(z) = w\inv \xi(z)$ on all of $\lieh\dual$. I.e., $\chi_\lambda = \chi_{w\cdot } \lambda$ for all $\lambda \in \lieh\dual$. This in fact shows that the image of $\mcz(\lieg)$ under $\xi$ consists of $W\dash$invariant polynomials. It's customary to state this in terms of the natural action of $W$ on polynomials without the row-shift. We do this by letting $\tau_\rho: S(\lieh) \mapsvia{\cong} S(\lieh)$ be the algebra automorphism induced by $f(\lambda) \mapsto f(\lambda - \rho)$. This is clearly invertible by $f(\lambda) \mapsto f(\lambda + \rho)$. We then define $$\psi: \mcz(\lieg) \mapsvia{\xi} S(\lieh) \mapsvia{\tau_\rho} S(\lieh)$$ as this composition; this is referred to as the **Harish-Chandra** (HC) homomorphism. Exercise : Show $\chi_\lambda(z) = (\lambda + \rho) (\psi(z))$ and $\chi_{w\cdot \lambda} (w(\lambda+\rho))(\psi(z))$, where $w(\wait)$ is the usual $w\dash$action. Replacing $\lambda$ by $\lambda + \rho$ and $w$ by $w\inv$, we get $$ w\psi(z) = \psi(z) $$ for all $z\in \mcz(\lieg)$ and all $w\in W$ where $(w\psi(z))(\lambda) = \psi(z)(w\inv \lambda)$. We've proved that Theorem (Character Linkage and Image of the HC Morphism) : \hfill a. If $\lambda, \mu \in \lieh\dual$ that are linked, then $\chi_\lambda = \chi_\mu$. b. The image of the twisted HC homomorphism $\psi: \mcz(\lieg) \to U(\lieh) = S(\lieh)$ lies in the subalgebra $S(\lieh)^W$. Example : Let $\lieg = \liesl_2$. Recall from finite-dimensional representations there is a canonical element $c\in \mcz(\lieg)$ called the Casimir element. For $\OO$, we need information about the full center $\mcz(\lieg)$ (hence introducing infinitesimal characters). Expressing $c$ in the PBW basis yields $c = h^2 + 2h + 4yx$, where $h^2 + 2h \in U(\lieh)$ and $4yx \in \lien^- U(\lieg) + U(\lieg) \lien$. > Enveloping algebra convention: $x$s, $h$s, $y$s Then $\xi(c) = \pr(c) = h^2 + 2h$, and under the identification $\lieh\dual \iff \CC$ where $\lambda \iff \lambda(h)$, we can identify $\rho \iff \rho(h) = 1$. The row shift is given by $\psi(c) = (h-1)^2 + 2(h-1) = h^2 - 1$. This is $W\dash$invariant, since $s_{\alpha_h} = -h$. But $W = \generators{s_\alpha, 1}$, so $s_\alpha$ generates $W$. We also have $\chi_\lambda(c) = (\lambda + \rho) (\psi(c)) = (\lambda+1)^2 - 1$. Then $$ \chi_\lambda(c) = \chi_\mu(c) \iff (\lambda+1)^2 - 1 = (\mu + 1)^2 \iff \mu = \lambda \text{ or } \mu = -\lambda - 2 $$ But $\lambda = 1 \cdot \lambda$ and $-\lambda - 2 = s_\alpha \cdot \lambda$, so $\mcz(\lieg) = \generators{c} \definedas \CC[c]$ as an algebra. So these characters are equal iff $\mu = w\cdot \lambda$ for $w\in W$. # Section 1.10: Harish-Chandra's Theorem Goal: prove the converse of the previous theorem. Theorem (Harish-Chandra) : Let $\psi: \mcz(\lieg) \to S(\lieh)$ be the twisted HC homomorphism. Then a. $\psi$ is an *isomorphism* of $\mcz(\lieg)$ onto $S(\lieh)^W$. b. For all $\lambda, \mu \in \lieh\dual$, $\chi_\lambda = \chi_\mu$ iff $\mu = w\cdot \lambda$ for some $w\in W$. c. Every central character $\chi: \mcz(\lieg) \to \CC$ is a $\chi_\lambda$. Proof (of (a)) : Relies heavily on the *Chevalley Restriction Theorem* (which we won't prove here). Initially we have a restriction map on polynomial functions $\theta: P(\lieg) \to P(\lieh)$. We identified $P(\lieg) = S(\lieg\dual)$, the formal polynomials on $\lieg\dual$. However, for $\lieg$ semisimple, we can identify $S(\lieg\dual) \cong S(\lieg)$ via the Killing form. By the Chinese Remainder Theorem, $\theta: S(\lieg)^G \to S(\lieh)^W$ is an isomorphism, where the subgroup $G \leq \aut(\lieg)$ is the *adjoint group* generated by $\theset{\exp \ad_x \suchthat x \text{ is nilpotent}}$. It turns out that $S(\lieg)^G$ is very close to $\mcz(\lieg)$ -- it is the associated graded of a natural filtration on $\mcz(\lieg)$. This is enough to show that $\psi$ is a bijection. Proof (of (b)) : We'll prove the contrapositive of the converse. Suppose $W\cdot \lambda \intersect W\cdot \mu = \emptyset$ and both are in $\lieh\dual$. Since these are finite sets, Lagrange interpolation yields a polynomial that is 1 on $W\cdot \lambda$ and 0 on $W\cdot \mu$. Let $g = \frac{1}{\abs W} \sum_{w\in W} w\cdot f$. > Note: definitely the dot action here, may be a typo in the book. Then $g$ is a $W\cdot$ invariant polynomial with the same properties. By part (a), we can get rid of the row shift to obtain an isomorphism $\xi: \mcz(\lieg) \to S(\lieh)^(W\cdot)$, the $W\cdot$ invariant polynomials. Choose $z\in \mcz(\lieg)$ such that $\xi(z) = g$, then $\chi_\lambda(z) = \lambda(\xi(z)) = \lambda(g) = g(\lambda) = 1$. So $\chi_\mu(z) = 0$ similarly, and $\chi_\lambda = \chi_\mu$. Proof (of (c)) : This follows from some commutative algebra, we won't say much here. Look at maximal ideals in $\CC[x, y,\cdots]$ which correspond to evaluating on points in $\CC^\ell$. $\qed$ Remark : Chevalley actually proved that $S(\lieh)^W \cong \CC(p_1, \cdots, p_\ell)$ where the $p_i$ are homogeneous polynomials of degrees $d_1 \leq \cdots \leq d_\ell$. These numbers satisfy some remarkable properties: $\prod d_i = \abs{W}$ and $d_1 = 2$ (these are called the *degrees of $W$*) # Section 1.11 Theorem (Category O is Artinian) : Category $\OO$ is *artinian*, i.e. every $M \in \OO$ is Artinian (DCC) and $\dim \hom_\lieg(M, N) < \infty$ for every $M, N$. Recall that $\OO$ is known to be Noetherian from an earlier theorem. This will imply that **every $M$ has a composition/Jordan-Holder series**, so we can take composition factors and multiplicities. Most interesting question: what are the factors/multiplicities of the simple modules and Verma modules?