Given a kahler manifold $(X, w)$ without boundary, we can define the laplacian $\Delta$ acting on a smooth function $f$ to be $\Delta f = g^{j \bar i} \partial_i \partial_{\bar j} f$, where $g^{j\bar i}$ is the component of the inverse of the metric $w$. Now I want to prove the following integration by parts formula(integrating with respect to the kahler volume form $w^n$):
$\int \Delta f h \omega^n = \int \Delta h f \omega^n$
Starting by writing the left hand side in local coordinates:
$\int g^{j \bar i} \partial_i \partial_{\bar j} f g = -\int \partial_i g^{i\bar j} h \partial_{\bar i} f = \int \partial_{i} \partial_{\bar j}( g^{j \bar i} h)f$
Some of the derivatives will hit on the metric producing extra terms. How do I bring it into the form on the right hand side?
Your definition of the Laplacian is incorrect. I suggest you try to modify it in order for the integration by parts to work, but you can look out the correct expression in coordinates on the Wikipedia page for the Laplace-Beltrame operator: https://en.m.wikipedia.org/wiki/Laplace%E2%80%93Beltrami_operator