# January 21st ## Elementary Cobordism Recall that an elementary cobordism is a cobordism that has a Morse function with exactly one critical point. Definition (Handles) : An $n\dash$dimensional $\lambda\dash$handle is a copy of $D^{\lambda} \times D^{n-\lambda}$ which is attached to $\bd M^n$ via an embedding $\phi: \bd D^\lambda \cross D^{n-\lambda} \injects \bd M$. Example : Let $\lambda = 1, n = 2, n-\lambda = 1$ and take $M^2 = D^2$ and we attach $D^1 \cross D^1$. Note that there's not necessarily a smooth structure on the resulting manifold, so we can "smooth corners": ![Image](figures/2020-01-21-11:09.png)\ Example : ![Image](figures/2020-01-21-11:12.png)\ > Note: the above is just a homeomorphism. Definition (Surgery) : Let $M$ be an $n-1$ dimensional smooth manifold, and $\rho: S^{\lambda-1} \cross D^{n-\lambda} \injects M^{n-1}$ be an embedding. Then noting that $\bd D^{n-\lambda} = S^{n-\lambda-1}$, consider the space \begin{align*} X(M, \phi) &= (M\setminus \rho(S^{\lambda-1} \cross \theset{0}) ) \cross (D^\lambda \cross S^{n-\lambda-1}) \\ & / \generators{ \rho(u, tv) \sim (tu, v) \suchthat t\in (0, 1), \forall u\in S^{\lambda-1}, \forall v\in S^{n-\lambda-1} } ,\end{align*} where we note that we can parameterize $D^{n-\lambda} = tv$ where $v$ is a point on the boundary. Note that this accomplishes the goal of smoothing, and is referred to as **surgery** (of type $\lambda, n-\lambda$) on $M$ along $\phi$. Example : ![Image](figures/2020-01-21-11:30.png) Example : $n-1 = 3$ and $\lambda = 2$ implies $\lambda-1 = 1$, and take $\rho: S^1 \cross D^2 \to S^3$, which has image a tubular neighborhood of a knot. Then $\phi(S^1 \cross\theset{0}) = K$ for some knot, and $(S^3\setminus K) \disjoint (D^2 \cross S^1) / \cdots$. Then note that $\bd \phi(\theset{u} \cross D^2) = \theset{u}\cross S^1$, which no longer bounds a disk since we have removed the core of tube. ![Image](figures/2020-01-21-11:42.png)\ Theorem (Cobordism and Morse Function Induced by Surgery) : Suppose $M' = X(M, \rho)$ is obtained from $M$ by surgery of type $\lambda$. Then there exists an elementary cobordism $(W; M, M')$ with a Morse function $f: W \to [-1, 1]$ with only one index $\lambda$ critical point. Example : Let $M=S^1$ and $\lambda = 1$. ![Image](figures/2020-01-21-11:49.png)\ ### Proof: Surgeries Come From Cobordisms With Special Morse Functions Write $\RR^n = \RR^\lambda \cross \RR^{n-\lambda}$, and $(\vector x, \vector y) \in \RR^n$. Then \begin{align*} L_\lambda = \{(\vector x, \vector y) \suchthat -1 \leq -\norm{\vector x}^2 +\norm{\vector y}^2 \leq 1,~ \norm{\vector x}\norm{\vector y} < \sinh(1) \cosh(1)\} .\end{align*} ![Image](figures/2020-01-21-11:54.png)\ The left boundary is given by $\bd_L: \norm{\vector y}^2 - \norm{\vector x}^2 = -1$, and there is a map \begin{align*} S^{\lambda-1} \cross D^{n-\lambda} &\mapsvia{\text{diffeo}} \bd_L \\ (u, tv) &\mapsto (u\cosh(t), v\sinh(t)) \quad t\in [0, 1) ,\end{align*} which is clearly invertible. The right boundary is given by $\bd_R: \norm{\vector y}^2 - \norm{\vector x}^2 = 1$, and there is a map \begin{align*} S^{\lambda-1} \cross D^{n-\lambda} &\mapsvia{\text{diffeo}} \bd_L \\ (tu, v) &\mapsto (u\sinh(t), v\cosh(t)) .\end{align*} In the above picture, we can consider the orthogonal trajectories, which are given by $y^2 - x^2 = c$, which has gradient $(-x, y)$ and $xy = c$ which has gradient $(y, x)$, so these are orthogonal. Recall that near a point $p\in M$, the morse function has the form $f(\vector x, \vector y) = f(p) - \norm{\vector x}^2 + \norm{\vector y}^2$ with a gradient-like vector field given by $\xi = (-\vector x, \vector y)$. The orthogonal trajectories will generally be of the form $\norm{\vector x}\norm{\vector y} = c$, which we can parameterize as $t \mapsto (t\vector x, \frac 1 t \vector y)$. **Construction of $W$**: Take \begin{align*} W(M, \phi) &= ( (M\setminus \phi(S^{\lambda-1} \cross \theset{0})) \cross D^1 )\disjoint L_\lambda \\ & / \generators{ \phi(u, tv) \cross c \sim (\vector x, \vector y) \suchthat \norm{\vector x}^2 - \norm{\vector y}^2 = c, (\vector x, \vector y) \in \text{orth. traj. starting from} (u\cosh(t), v\sinh(t)) } .\end{align*} ![Image](figures/2020-01-21-12:10.png)\ This amounts to closing up in the following two ways: ![Image](figures/2020-01-21-12:14.png)\ This has two boundaries: when $c = -1$, we obtain $M$, and $c=1$ yields $X(M, \phi)$. The Morse function is given by $f: W(M, \phi) \to [-1, 1]$ where \begin{align*} \begin{cases} f(z, c) = c & z \in M\setminus \phi(S^{\lambda - 1} \cross \theset{0}), c\in D^1\\ f(\vector x, \vector y) = \norm{\vector x}^2 - \norm{\vector y}^2 & (\vector x, \vector y) \in L_\lambda \end{cases} .\end{align*}