Lemma 53.6.7. In Situation 53.6.2. Let \mathcal{L} be a very ample invertible \mathcal{O}_ X-module with \deg (\mathcal{L}) \geq 2. Then \omega _ X \otimes _{\mathcal{O}_ X} \mathcal{L} is globally generated.
Proof. Assume k is algebraically closed. Let x \in X be a closed point. Let C_ i \subset X be the irreducible components and for each i let x_ i \in C_ i be the generic point. By Varieties, Lemma 33.22.2 we can choose a section s \in H^0(X, \mathcal{L}) such that s vanishes at x but not at x_ i for all i. The corresponding module map s : \mathcal{O}_ X \to \mathcal{L} is injective with cokernel \mathcal{Q} supported in finitely many points and with H^0(X, \mathcal{Q}) \geq 2. Consider the corresponding exact sequence
By Lemma 53.6.5 we see that the module generated by global sections surjects onto \omega _ X \otimes \mathcal{Q}. Since x was arbitrary this proves the lemma. Some details omitted.
We will reduce the case where k is not algebraically closed, to the algebraically closed field case. We suggest the reader skip the rest of the proof. Choose an algebraic closure \overline{k} of k and consider the base change X_{\overline{k}}. Let us check that X_{\overline{k}} \to \mathop{\mathrm{Spec}}(\overline{k}) is an example of Situation 53.6.2. By flat base change (Cohomology of Schemes, Lemma 30.5.2) we see that H^0(X_{\overline{k}}, \mathcal{O}) = \overline{k}. The scheme X_{\overline{k}} is proper over \overline{k} (Morphisms, Lemma 29.41.5) and equidimensional of dimension 1 (Morphisms, Lemma 29.28.3). The pullback of \omega _ X to X_{\overline{k}} is the dualizing module of X_{\overline{k}} by Lemma 53.4.4. The pullback of \mathcal{L} to X_{\overline{k}} is very ample (Morphisms, Lemma 29.38.8). The degree of the pullback of \mathcal{L} to X_{\overline{k}} is equal to the degree of \mathcal{L} on X (Varieties, Lemma 33.44.2). Finally, we see that \omega _ X \otimes \mathcal{L} is globally generated if and only if its base change is so (Varieties, Lemma 33.22.1). In this way we see that the result follows from the result in the case of an algebraically closed ground field. \square
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