Example 2.31 in these notes of Milne is about real Hodge structures and the fact that they can be seen as representations of the Deligne torus $\mathbb{S}$. The pace is a bit too fast for me. I have the following two questions:
- Why does $z \in \mathbb{C}^\times$ have to act on $V^{p,q}$ as multiplication by $z^{-p}\overline{z}^{-q}$ and cannot just be multiplication by $z^{p}\overline{z}^{q}$? Would the corresponding map $\mathbb{G}_m \to \mathbb{S}$ be the usual inclusion of $\mathbb{R}$ into $\mathbb{C}$ in that case, rather than being $t \mapsto t^{-1}$?
- How is the action on $V$ defined exactly? So far I have only an action on $V \otimes \mathbb{C}$, without knowledge of what happens to pure tensors of the form $v \otimes 1$. If I want to know what $z \cdot v$ is, should I take the real part of $z \cdot (v \otimes 1)$, or the imaginary part, or split $v \otimes 1$ into components of pure weight and do something with them? Or should I just take the $V_{p,p}$ components of $v \otimes 1$ and take their image, since $z$ acts on $V_{p,p}$ as multiplication by $|z|^{-2p} \in \mathbb{R}^\times$? None of these options seems to give the right action (or an action at all).