[guided]The purpose of this step is to justify that contraction is not merely a pointwise bundle isomorphism; it is compatible with the differential used to define Dolbeault cohomology. For every $q\ge 0$, let $A^{0,q}(X,T_X)$ be the complex vector space of smooth $T_X$-valued $(0,q)$-forms, let $A^{n-1,q}(X)$ be the complex vector space of smooth scalar-valued $(n-1,q)$-forms, and let $\bar\partial_{T_X}:A^{0,q}(X,T_X)\to A^{0,q+1}(X,T_X)$ be the Dolbeault operator induced by the holomorphic structure on $T_X$. Define
\begin{align*}
C_q:A^{0,q}(X,T_X)&\longrightarrow A^{n-1,q}(X)
\end{align*}
by
\begin{align*}
C_q(\varphi)&=\varphi\lrcorner\Omega.
\end{align*}
Since $C:T_X\to\Omega_X^{n-1}$ is already a holomorphic vector bundle isomorphism, tensoring with $(0,q)$-forms gives an isomorphism on smooth sections, so each $C_q$ is bijective.
We must verify that this bijection sends $\bar\partial_{T_X}$-closed forms to $\bar\partial$-closed forms and $\bar\partial_{T_X}$-exact forms to $\bar\partial$-exact forms. This is equivalent to the identity
\begin{align*}
\bar\partial(\varphi\lrcorner\Omega)=(\bar\partial_{T_X}\varphi)\lrcorner\Omega
\end{align*}
for every $\varphi\in A^{0,q}(X,T_X)$.
We verify the identity in local holomorphic coordinates. Let $(U,z)$ be a holomorphic coordinate chart with coordinates $z_1,\dots,z_n$. Since $\Omega$ is a holomorphic section of $K_X$, there is a [holomorphic function](/page/Holomorphic%20Function) $f:U\to\mathbb C$ such that
\begin{align*}
\Omega|_U=f\,dz_1\wedge\cdots\wedge dz_n.
\end{align*}
The nowhere-vanishing hypothesis says $f(p)\ne 0$ for every $p\in U$, but the commutation with $\bar\partial$ uses the holomorphicity condition $\bar\partial f=0$.
Write a local $T_X$-valued $(0,q)$-form as
\begin{align*}
\varphi=\sum_{i,J}\varphi_{i,J}\,d\bar z_J\otimes\partial_{z_i},
\end{align*}
where $J$ ranges over increasing $q$-tuples and each $\varphi_{i,J}:U\to\mathbb C$ is smooth. Contracting with $\Omega$ gives a finite sum whose coefficients are products of the smooth functions $\varphi_{i,J}$ with the holomorphic function $f$, multiplied by fixed coordinate forms. Applying $\bar\partial$ differentiates only in the anti-holomorphic directions. Since $\bar\partial f=0$ and the coordinate holomorphic forms are $\bar\partial$-closed, the only differentiated coefficients are the $\varphi_{i,J}$. Therefore
\begin{align*}
\bar\partial(\varphi\lrcorner\Omega)=(\bar\partial_{T_X}\varphi)\lrcorner\Omega.
\end{align*}
This proves that the family $(C_q)_{q\ge 0}$ is an isomorphism of complexes
\begin{align*}
(A^{0,*}(X,T_X),\bar\partial_{T_X})\cong (A^{n-1,*}(X),\bar\partial).
\end{align*}[/guided]