"We all have to pass the time until the electoral results come in, so we might as well do some geometry..." Recall def'ns: Stein: $(M,J,\phi)$ Weinstein: $(M,\omega,\theta,\phi)$ Def'ns of complete and finite type in each case Stein: $\omega=-d(d\phi \circ J)$ is a Kahler form. Weinstein: $\omega$ symplectic, $d\theta=\omega$, $\phi$ an exhausting function; $\theta$ is associated to a "compressing" form. Weinstein, complete, of finite type => has a contact-type cone at $\infty$. Lots of Stein manifolds, all of which are Weinstein. When will they be of finite type? If $X$ is a smooth projective variety, $\L$ an ample line bundle, and $\sigma$ a nonzero holomorphic section, then $X-\sigma^{-1}(0)=X-D$ is Stein (e.g., $X \subset \C P^n$, $M=X-\C P^{n-1}$. Lemma: Suppose $D$ has normal crossings (locally, $D=\{z_1 \dots z_k=0\}$ in holomorphic coordinates, $z=(z_1,\dots,z_n)$ (i.e., if $D$ is smooth). Then $M=X-D$ is of finite type. How do we get a Stein structure to be complete? Certainly, the given Stein structure on $X-D$ isn't complete (since the symplectic form is restricted from something closed, and thus has finite volume). But we can fix this... Lemma: Suppose $(M,J,\phi)$ Stein. Let $h:\R \to \R$ be a smooth function, $h'>0$, $h'' >0$, and $h' \in O(h'')$. Then $(M,J,\tilde \phi=h(\phi))$ is Stein and complete. Clearly, $\tilde \phi$ has the same critical points as $\phi$; thus, with the new function, $M$ is of finite type iff it was originally. Pf: Let $X$ be the Liouville vector field associated to $(M,J,\phi)$, so $X=\nabla \phi$. Similarly, let $\tilde X=\nabla \tilde \phi$. Then $\tilde X=X h'(\phi)/(h'(\phi)+h''(\phi)|\nabla \phi|^2)$, where the denominator is evaluated using the original metric. Why is $\tilde \phi$ plurisubharmonic? "Obvious." We'll prove completeness. What is $d\phi(\tilde X)$? It's $|\nabla \phi|^2/(1+h''(\phi)/h'(\phi) |\nabla \phi|^2 \leq 1/\delta$, where $\delta$ is the $O$-constant. So the flow is of bounded speed; hence it's defined for all time. P.S. Suppose $(M,J,\phi)$ is already complete and of finite type. Then $(M,J,\tilde \phi)$ is isomorphic to $(M,J,\phi)$ as a Weinstein manifold: i.e., there is a diffeomorphism $f:M \to M$ such that $f^*(\tilde \theta)=\theta+dR$, $R \in C^{\infty}_c(M)$. (Thus, the isomorphism is compatible with the Liouville flow outside some compact subset.) Why is this true? By the previous proof given, we can drop the last assumption above in this case, and still get the conclusion. Do it with a collection of smooth functions interpolating between the original one and the new one, and apply Moser. Thm: Take $(M,J)$; let $\phi,\tilde \phi$ be two exhausting strictly plurisubharmonic functions on $M$. Suppose that $(M,J,\tilde \phi)$ is complete and of finite type. Then there is an embedding $i:M \to M$ such that $i^*(\tilde \theta-\theta)$ is exact. Pf: First, assume that $\tilde \ohi$ grows faster than $\phi$, in the sense that for $\delta=\tilde \phi-\phi$, $\delta \geq 1$ everywhere, $\delta$ is exhausting. Consider $U_k=\{x \in M|\delta(x)0} \times T^*(S^k \times \R^{n-k-1})$. Why is this contact? Let $\theta$ be the Liouville form; pull it back to $\bar \theta$, and let $\alpha=t \bar \theta+dt$ ($t$ is the extra variable). Then $\alpha \wedge (d\alpha)^{n-1}=t^{n-1} dt \wedge d\overline{\theta}^{n-1}$, after some algebra; this is nonzero by inspection. The contact isotropy sphere is $\{1 \times (S^k \times \{0\}\}$. Legendrian handle attachment: Assume $M$ is Weinstein, complete, and of finite type. If we take $N=\phi^{-1}(c_0)$, $\alpha=\theta|N$ is contact. Suppose $i:S^r \to N$, $K=i(S^r)$ is a framed contact isotropic sphere. Do the following 3 things: 1) Remove the cone to get a compact manifold-with-bdry 2) Attach a handle $D^{r+1} \times D^{2n-r-1}$ 3) Reattach a (different) cone. This gives another finite-type complete Weinstein manifold. Topologically, this is easy... Locally, what does this handle look like? Take $C^n$, $\omega$ standard, take $\phi=\frac{1}{4}|z|^2-\frac{1}{2} (\im(z_1))^2-\frac{1}{2}(\im(z_2))^2-\dots$. Look at the associated gradient flow; make an argument involving Morse theory and pictures I can't reproduce to make a handle. In fact, symplectically, every Stein manifold can be obtained by repeated such attachments.