Lemma 50.20.1. Let k be a field. Let X be a nonempty smooth proper scheme over k equidimensional of dimension d. There exists a k-linear map
t : H^ d(X, \Omega ^ d_{X/k}) \longrightarrow k
unique up to precomposing by multiplication by a unit of H^0(X, \mathcal{O}_ X) with the following property: for all p, q the pairing
H^ q(X, \Omega ^ p_{X/k}) \times H^{d - q}(X, \Omega ^{d - p}_{X/k}) \longrightarrow k, \quad (\xi , \xi ') \longmapsto t(\xi \cup \xi ')
is perfect.
Proof.
By Duality for Schemes, Lemma 48.27.1 we have \omega _ X^\bullet = \Omega ^ d_{X/k}[d]. Since \Omega _{X/k} is locally free of rank d (Morphisms, Lemma 29.34.12) we have
\Omega ^ d_{X/k} \otimes _{\mathcal{O}_ X} (\Omega ^ p_{X/k})^\vee \cong \Omega ^{d - p}_{X/k}
Thus we obtain a k-linear map t : H^ d(X, \Omega ^ d_{X/k}) \to k such that the statement is true by Duality for Schemes, Lemma 48.27.4. In particular the pairing H^0(X, \mathcal{O}_ X) \times H^ d(X, \Omega ^ d_{X/k}) \to k is perfect, which implies that any k-linear map t' : H^ d(X, \Omega ^ d_{X/k}) \to k is of the form \xi \mapsto t(g\xi ) for some g \in H^0(X, \mathcal{O}_ X). Of course, in order for t' to still produce a duality between H^0(X, \mathcal{O}_ X) and H^ d(X, \Omega ^ d_{X/k}) we need g to be a unit. Denote \langle -, - \rangle _{p, q} the pairing constructed using t and denote \langle -, - \rangle '_{p, q} the pairing constructed using t'. Clearly we have
\langle \xi , \xi ' \rangle '_{p, q} = \langle g\xi , \xi ' \rangle _{p, q}
for \xi \in H^ q(X, \Omega ^ p_{X/k}) and \xi ' \in H^{d - q}(X, \Omega ^{d - p}_{X/k}). Since g is a unit, i.e., invertible, we see that using t' instead of t we still get perfect pairings for all p, q.
\square
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