ScalingStacks

Gubler’s description [01JX]

Original official author HTML, exact retained edition. Historical TeX conversion verdicts remain unchanged. Cited-edition alignment and mathematical self-containment are not assessed.

Complete original source context · Original author HTML

Gubler’s description

In the case of bad reduction, the description of the canonical measures has been established by W. Gubler [39].

Up to replacing KK by a finite extension, we assume that X\mathrm{X} has split semi-stable reduction. Raynaud’s uniformization involves an analytic group E\mathrm{E} which is an extension of an abelian variety with good reduction Y\mathrm{Y} by a split torus T≃𝐆mt\mathrm{T}\simeq{\mathbf{G}_{\mathrm{m}}}^{t}, where t∈{1,…,n}t\in\{1,\dots,n\} — the so-called Raynaud extension of X\mathrm{X}. One has t≥1t\geq 1 since we assume bad reduction ; moreover, dim⁡Y=dim⁡E−t=n−t\operatorname{dim}\mathrm{Y}=\operatorname{dim}\mathrm{E}-t=n-t. There is a morphism p:E→Xp\colon\mathrm{E}\rightarrow\mathrm{X}, whose kernel is a discrete subgroup MM of E⁡(K)\mathrm{E}(K), so that the induced map E/Λ→X\mathrm{E}/\Lambda\rightarrow\mathrm{X} is an isomorphism. When t=nt=n, one says that X\mathrm{X} has totally degenerate reduction, and the morphism pp is the rigid analytic uniformization of the abelian variety X\mathrm{X}.

Moreover, E\mathrm{E} is constructed as a contracted product (E1×T)/T1(\mathrm{E}_{1}\times\mathrm{T})/\mathrm{T}_{1} from an extension E1\mathrm{E}_{1} of Y\mathrm{Y} by the “unit subtorus” T1\mathrm{T}_{1} of T\mathrm{T} (defined by the equalities |Tj​(x)|=1\left|{T_{j}(x)}\right|=1 for j∈{1,…,t}j\in\{1,\dots,t\} and x∈Tx\in\mathrm{T}). The natural map λT:T→𝐑t\lambda_{\mathrm{T}}\colon\mathrm{T}\rightarrow{\mathbf{R}}^{t} defined by

x↦(−log⁡|T1​(x)|,…,−log⁡|Tt​(x)|)x\mapsto(-\log\left|{T_{1}(x)}\right|,\dots,-\log\left|{T_{t}(x)}\right|)

is continuous and surjective ; it admits a canonical section ιT\iota_{\mathrm{T}} which maps a point (u1,…,ut)∈𝐑t(u_{1},\dots,u_{t})\in{\mathbf{R}}^{t} to the semi-norm

f↦sup𝐦∈𝐙ta𝐦​e−m1​u1−⋯−mt​ut,for f=∑𝐦a𝐦​T1m1​…​Ttmt∈𝒪⁡(T).f\mapsto\sup_{\mathbf{m}\in{\mathbf{Z}}^{t}}a_{\mathbf{m}}e^{-m_{1}u_{1}-\dots-m_{t}u_{t}},\qquad\text{for $f=\sum_{\mathbf{m}}a_{\mathbf{m}}T_{1}^{m_{1}}\dots T_{t}^{m_{t}}\in\mathscr{O}(\mathrm{T}).$}

The map λT\lambda_{\mathrm{T}} extends uniquely to a morphism λ:E→𝐑t\lambda\colon\mathrm{E}\rightarrow{\mathbf{R}}^{t} whose kernel contains E1\mathrm{E}_{1}. The image Λ=λ⁡(M)\Lambda=\lambda(M) is a lattice of 𝐑t{\mathbf{R}}^{t}, and the morphism pp induces a continuous proper morphism ρ:X→𝐑t/Λ\rho\colon\mathrm{X}\rightarrow{\mathbf{R}}^{t}/\Lambda. Composing the section ιT\iota_{\mathrm{T}} with the projection pp furnishes a section ι:𝐑t/Λ→X\iota\colon{\mathbf{R}}^{t}/\Lambda\rightarrow\mathrm{X} of ρ\rho. Its image is the skeleton of X\mathrm{X}. Gubler’s theorem ([39], Cor. 7.3) is the following :

Theorem 2.5.1.

Let L1,…,LnL_{1},\dots,L_{n} be line bundles on X\mathrm{X}. The canonical measure c1​(L¯1)​…​c1​(L¯n)c_{1}(\overline{L}_{1})\dots c_{1}(\overline{L}_{n}) is the direct image by ι\iota of the unique Haar measure on 𝐑t/Λ{\mathbf{R}}^{t}/\Lambda whose total mass is deg⁡(L1​…​Ln)\deg(L_{1}\dots L_{n}).

Original mathematics by the credited authors. Source-backed reader collection; mathematical self-containment is not assessed.