I am reading Kapranov and Vasserot's paper 'Kleinian singularities, derived categories and Hall algebras',where they proved McKay correspondence in dimension 2. In section 1.2, they constructed two functors $\Phi$ and $\Psi$
$\Phi(\mathcal{F})=(Rp_{1*}(p_2^*(\mathcal{F}\otimes\mathcal{O}_{\Sigma}))^G$
$\Psi(\mathcal{G})=Rp_{2*}R\mathcal{Hom}(\mathcal{O}_{\Sigma},p_1^*(\mathcal{G}))$
and claimed that $\Phi$ is the left adjoint of $\Psi$.
What puzzles me is that when one is taking the right adjoint of $Rp_{1*}$ and since $p_1$ is flat, we get $p^*_1(\mathcal{F})\otimes \omega_{p_1}$ under the assumption that $p_1$ is proper. Here neither the properness is assumed nor the relative differential can be seen. I cannot see how the adjunction is justified.
I would greatly appreciate any hint to clear this issue.