[guided]We now verify the condition that makes the CR structure integrable: sections of $T_{1,0}M$ must be closed under the Lie bracket.
Let $U\subset M$ be open, and let
\begin{align*}
X,Y\in \Gamma(U,T_{1,0}M)
\end{align*}
be smooth local sections. Fix $p\in U$. The argument is local on $U$, so we replace $U$ by a smaller neighbourhood of $p$ in $M$. Choose an ambient open neighbourhood $\widetilde U\subset \mathbb C^N$ with embedded-submanifold coordinates in which $M\cap\widetilde U$ is a coordinate slice and the smaller $U$ equals $M\cap\widetilde U$. In these coordinates, coefficient functions of sections along the slice extend smoothly to $\widetilde U$ by keeping them constant in the normal coordinate directions. Since $X$ and $Y$ are restrictions of sections of the smooth ambient bundle $T_{1,0}\mathbb C^N$, we may extend them locally to ambient smooth type $(1,0)$ vector fields
\begin{align*}
\widetilde X,\widetilde Y\in \Gamma(\widetilde U,T_{1,0}\mathbb C^N).
\end{align*}
First we check the type. In standard holomorphic coordinates $(z_1,\dots,z_N):\mathbb C^N\to\mathbb C^N$, every smooth type $(1,0)$ vector field is a smooth linear combination of the coordinate fields $\partial/\partial z_j$. Thus there are smooth functions $a_j,b_j:\widetilde U\to\mathbb C$ such that
\begin{align*}
\widetilde X=\sum_{j=1}^N a_j\frac{\partial}{\partial z_j},\qquad \widetilde Y=\sum_{j=1}^N b_j\frac{\partial}{\partial z_j}.
\end{align*}
Using the definition of the Lie bracket as the commutator of derivations, and using that the coordinate fields $\partial/\partial z_j$ commute with one another, we get
\begin{align*}
[\widetilde X,\widetilde Y]=\sum_{j=1}^N\left(\widetilde X(b_j)-\widetilde Y(a_j)\right)\frac{\partial}{\partial z_j}.
\end{align*}
This is again a smooth linear combination of the fields $\partial/\partial z_j$, so it is again of ambient type $(1,0)$.
Second we check tangency to $M$. Let
\begin{align*}
I_M(\widetilde U):=\{f\in C^\infty(\widetilde U;\mathbb C):f|_{M\cap \widetilde U}=0\}
\end{align*}
be the ideal of smooth complex-valued functions vanishing on $M$. A vector field along $M$ is tangent to $M$ exactly when it sends every function in this vanishing ideal to a function that also vanishes on $M$. Since $X$ and $Y$ are tangent to $M$, for every $f\in I_M(\widetilde U)$ we have
\begin{align*}
(\widetilde Xf)|_U=0,\qquad (\widetilde Yf)|_U=0.
\end{align*}
Now use tangency one more time. The function $\widetilde Yf$ vanishes on $M\cap\widetilde U$, and $\widetilde X|_U=X$ is tangent to $M$, so $(\widetilde X(\widetilde Yf))|_U=0$. Similarly, $\widetilde Xf$ vanishes on $M\cap\widetilde U$, and $\widetilde Y|_U=Y$ is tangent to $M$, so $(\widetilde Y(\widetilde Xf))|_U=0$. Applying the commutator to such an $f$, we obtain
\begin{align*}
([\widetilde X,\widetilde Y]f)|_U=(\widetilde X(\widetilde Yf)-\widetilde Y(\widetilde Xf))|_U=0.
\end{align*}
Thus $[\widetilde X,\widetilde Y]|_U$ is tangent to $M$.
We have shown both required properties: the bracket is of ambient type $(1,0)$ and tangent to $M$. Therefore
\begin{align*}
[\widetilde X,\widetilde Y]|_U\in \Gamma(U,T_{1,0}\mathbb C^N|_U)\cap \Gamma(U,TM\otimes_{\mathbb R}\mathbb C)=\Gamma(U,T_{1,0}M).
\end{align*}
The restricted bracket is the intrinsic bracket $[X,Y]$ on $U$: for every smooth function $g:U\to\mathbb C$, extend $g$ locally to a smooth function $\widetilde g:\widetilde U\to\mathbb C$; then $X(g)=(\widetilde X\widetilde g)|_U$ and $Y(g)=(\widetilde Y\widetilde g)|_U$, so the commutator derivation induced on $U$ is $[X,Y]$. The ideal calculation above proves that this commutator is tangent to $M$, hence $[X,Y]$ is a section of $T_{1,0}M$, which is precisely formal integrability.[/guided]