Here (at the bottom of page 13) it's stated that for a smooth map $f:X\to S$, the relative Spencer complex $$\Omega_{X/S}^\bullet \otimes_{f^{-1}\mathcal{O}_S} D_X$$ is a resolution of the transfer module $$D_{S\leftarrow X} \ = \ f^{-1}(D_S \otimes_{f^{-1}\mathcal{O}_S} \Omega_S^{-1}) \otimes_{f^{-1}\mathcal{O}_S} \Omega_X$$ by left $f^{-1}D_S$-modules.
- Why is this a resolution?
- Is there a similar resolution in the case where some fibres of $f$ are singular? If so, what can we say about it?
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It's easy to show that $\Omega_{X/S}^\bullet \otimes D_X$ is a complex, but I'm not sure exactly how to get a map $$\Omega_{X/S} \otimes_{f^{-1}\mathcal{O}_S} D_X\longrightarrow D_{S\leftarrow X}$$ of left $f^{-1}D_S$-modules. I know it should be a trivial consequence of $\Omega_X\otimes_{f^{-1}\mathcal{O}_S} f^{-1}\Omega_S\simeq \Omega_{X/S}$, but for some reason I can't get it to work. I would guess something like $$\omega \otimes P \longrightarrow \phi(P) \otimes \omega$$ might work for an appropriate map $\phi:D_X\to f^{-1}D_S$.
I'm also curious about what happens when the map $f$ is smooth except at a point where the fibre is singular.