ScalingStacks

Proof. [04XT]

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Proof.

One can construct (S,s)(S,s) and ๐’ด\mathscr{Y} satisfying (1) and (2) by means of a standard argument based on spreading out and Greenberg approximation; see for instance [MN15, 5.1.2] and the proof of [NX16a, 4.2.4] (note that normality of ๐’ด\mathscr{Y} automatically follows from the fact that ๐’ดโˆ–๐’ดs\mathscr{Y}\setminus\mathscr{Y}_{s} is normal and ๐’ดsโ‰…๐’ณk\mathscr{Y}_{s}\cong\mathscr{X}_{k} is reduced). In this construction we can also spread out a global generator ฯ‰\omega of the relative canonical line bundle ฯ‰๐’ณ/R\omega_{\mathscr{X}/R}, which then induces a global generator for ฯ‰๐’ด/S\omega_{\mathscr{Y}/S}, yielding the triviality of K๐’ด/SK_{\mathscr{Y}/S}.

If NN is at least 22, then for every point xx of ๐’ณkโ‰…๐’ดs\mathscr{X}_{k}\cong\mathscr{Y}_{s}, the model ๐’ณ\mathscr{X} is regular at xx if and only if ๐’ด\mathscr{Y} is regular at xx [MN15, 5.1.2(d)]. Thus the pair (๐’ด,๐’ดs)(\mathscr{Y},\mathscr{Y}_{s}) is snc at all the points of ๐’ดs\mathscr{Y}_{s} where (๐’ณ,๐’ณk)(\mathscr{X},\mathscr{X}_{k}) is snc. Taking NN sufficiently large, we can arrange that every prime component EE of ๐’ดs\mathscr{Y}_{s} is โ„š\mathbb{Q}-Cartier in ๐’ด\mathscr{Y}. More precisely, let xx be a point of ๐’ณk\mathscr{X}_{k} and let mxm_{x} be the Cartier index of EE in ๐’ณ\mathscr{X} at xx. Let ff be a local generator for the ideal sheaf ๐’ช๐’ณโ€‹(โˆ’mxโ€‹E)\mathcal{O}_{\mathscr{X}}(-m_{x}E) at xx. Assume that N>mxN>m_{x} and let gg be any element of ๐’ช๐’ด,x\mathcal{O}_{\mathscr{Y},x} that is congruent to ff modulo tNt^{N}. Obviously, gg cannot vanish at any other component of ๐’ดs\mathscr{Y}_{s}, because tt vanishes along each of these components and ff does not. On the other hand, ff divides tmxt^{m_{x}} in ๐’ช๐’ณ,x\mathcal{O}_{\mathscr{X},x}, so that gg divides tmxt^{m_{x}} in ๐’ช๐’ด,y\mathcal{O}_{\mathscr{Y},y} since N>mxN>m_{x}. Thus the zero locus of gg is supported in ๐’ดs\mathscr{Y}_{s}, which means that g=0g=0 is a local equation for mxโ€‹Em_{x}E in ๐’ด\mathscr{Y} at xx. From now on, we assume that NN has been chosen large enough to guarantee that Nโ‰ฅ2N\geq 2 and every prime component of ๐’ดs\mathscr{Y}_{s} is โ„š\mathbb{Q}-Cartier.

Let EE be a prime component of ๐’ณk\mathscr{X}_{k}, denote by E~\widetilde{E} its normalization, and let ฮ”\Delta be the pullback of the โ„š\mathbb{Q}-Cartier divisor ๐’ณkโˆ’E\mathscr{X}_{k}-E to E~\widetilde{E}. The scheme ๐’ณ\mathscr{X} is regular in codimension two by Lemma 4.2. It follows that the different DiffE~โ€‹(๐’ณkโˆ’E)\mathrm{Diff}_{\widetilde{E}}(\mathscr{X}_{k}-E) coincides with ฮ”\Delta. Thus the pair (E~,ฮ”)(\widetilde{E},\Delta) is dlt by adjunction [Ko13, 4.8], using the same reasoning as in the proof of [Ko13, 4.16.4] (except that we have not yet established the normality of EE). Since Nโ‰ฅ2N\geq 2, the scheme ๐’ด\mathscr{Y} is regular in codimension two, as well; since it is of finite type over kk, we can apply inversion of adjunction [Ko13, 4.9] to deduce that (๐’ด,๐’ดs)(\mathscr{Y},\mathscr{Y}_{s}) is log canonical on a neighbourhood of EE, and that the log canonical centers of (๐’ด,๐’ดs)(\mathscr{Y},\mathscr{Y}_{s}) contained in EE are precisely the images of the log canonical centers of (E~,ฮ”)(\widetilde{E},\Delta). At the generic point of such a log canonical center, the pair (๐’ด,๐’ดs)(\mathscr{Y},\mathscr{Y}_{s}) is snc because the same holds for (๐’ณ,๐’ณk)(\mathscr{X},\mathscr{X}_{k}). Varying EE, we obtain that (๐’ด,๐’ดs)(\mathscr{Y},\mathscr{Y}_{s}) is dlt. This implies that every stratum of ๐’ณkโ‰…๐’ดs\mathscr{X}_{k}\cong\mathscr{Y}_{s} is normal [Ko13, 4.16]; thus, in retrospect, we see that E~=E\widetilde{E}=E. โˆŽ

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