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2.4. Polarized dynamical systems [01JJ]

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2.4. Polarized dynamical systems

We now explain another example of metrized line bundles : the canonical metrics associated to dynamical system.

Lemma 2.4.1.

Let X\mathrm{X} be the analytic space associated to a proper KK-scheme and let f:X→Xf\colon\mathrm{X}\rightarrow\mathrm{X} be a finite morphism. Let LL be a line bundle on X\mathrm{X}, dd an integer such that d≥2d\geq 2 and an isomorphism ε:f∗​L≃Ld\varepsilon\colon f^{*}L\simeq L^{d}. The line bundle LL possesses a unique continuous metric such that the isomorphism ε\varepsilon is an isometry. If LL is ample, then this metric is semi-positive.

In essence, this result, or at least its proof, goes back to Tate’s construction of the “Néron–Tate” canonical height for abelian varieties. In the slightly different language of local heights and Néron functions, it has been proved by Call–Silverman [16]. In the asserted form, it is due to Zhang [59].

Démonstration.

Let us first prove uniqueness. If L¯\overline{L} and L¯′\overline{L}^{\prime} are two metrics on LL, let φ\varphi be the continuous function such that ‖⋅‖′=e−φ​‖⋅‖\left\|{\cdot}\right\|^{\prime}=e^{-\varphi}\left\|{\cdot}\right\|. Assuming that ε\varepsilon is an isometry for these two metrics, one obtains the following equation

φ⁡(f⁡(x))=d​φ​(x),\varphi(f(x))=d\varphi(x),

for any x∈Xx\in\mathrm{X}. Since X\mathrm{X} is compact, φ\varphi is bounded and this equation implies that ‖φ‖∞≤1d​‖φ‖∞\left\|{\varphi}\right\|_{\infty}\leq\frac{1}{d}\left\|{\varphi}\right\|_{\infty}. Since d≥2d\geq 2, one concludes that φ≡0\varphi\equiv 0.

For the existence, one begins with any continuous metric L¯0\overline{L}_{0} on LL. Let us then consider the sequence of metrics (L¯n)(\overline{L}_{n}) on LL induced by the pull-backs on Ld=ε​f∗​LL^{d}=\varepsilon f^{*}L, Ld2=(ε​f∗)2​LL^{d^{2}}=(\varepsilon f^{*})^{2}L, etc., hence on LL. Since d≥2d\geq 2, a similar contraction argument as the one used for uniqueness shows that this is a Cauchy sequence of metrics on LL ; consequently, it converges to a continuous metric on LL. If L¯0\overline{L}_{0} is chosen to be semi-positive, which we may if LL is ample, then all al of the metrized line bundles L¯n\overline{L}_{n} are semi-positive, hence the canonical metric is semi-positive.

Concretely, in the non-archimedean case, one begins with a model (𝔛0,𝔏0,e)(\mathfrak{X}_{0},\mathfrak{L}_{0},e) such that 𝔏0\mathfrak{L}_{0} is numerically effective. Then one considers the map f:X→𝔛0f\colon X\rightarrow\mathfrak{X}_{0} and the normalization 𝔛1\mathfrak{X}_{1} of 𝔛0\mathfrak{X}_{0} in XX ; this is a projective model 𝔛1\mathfrak{X}_{1}, equiped with a finite morphism f1:𝔛1→𝔛0f_{1}\colon\mathfrak{X}_{1}\rightarrow\mathfrak{X}_{0} extending ff. Moreover, 𝔏1=f1∗​𝔏0\mathfrak{L}_{1}=f_{1}^{*}\mathfrak{L}_{0} is a model of f∗​Lef^{*}L^{e} which is identified with Le​dL^{ed} via the fixed isomorphism ε\varepsilon. Iterating this construction defines a sequence (𝔛n,𝔏n,e​dn)(\mathfrak{X}_{n},\mathfrak{L}_{n},ed^{n}) of models of (X,L)(X,L), with finite morphisms fn:𝔛n→𝔛n−1f_{n}\colon\mathfrak{X}_{n}\rightarrow\mathfrak{X}_{n-1} such that fn∗​𝔏n−1=𝔏nf_{n}^{*}\mathfrak{L}_{n-1}=\mathfrak{L}_{n}. The metric on LL defined by any of these models is semi-positive, hence so is their uniform limit. ∎

The canonical measure

The measure c1​(L¯)nc_{1}(\overline{L})^{n} on X\mathrm{X} defined by the metrized line bundle L¯\overline{L} is a very important invariant of the dynamical system. It satisfies the functional equations

f∗​c1​(L¯)n=dn​c1​(L¯)nandf∗​c1​(L¯)n=c1​(L¯)n.f^{*}c_{1}(\overline{L})^{n}=d^{n}c_{1}(\overline{L})^{n}\quad\text{and}\quad f_{*}c_{1}(\overline{L})^{n}=c_{1}(\overline{L})^{n}.

The first follows by a general functorial property proved in [18] ; it implies the second. The support of the canonical measure is therefore totally invariant under ff.

The Fatou set

Generalizing results of Kawaguchi–Silverman in [42] and Baker–Rumely [6], we want to show here that the canonical measure vanishes on any open set U\mathrm{U} of X\mathrm{X} where the sequence (fn|U)(f^{n}|_{\mathrm{U}}) of iterates of ff is equicontinuous.

Let U\mathrm{U} be an open set in X\mathrm{X} and ℱ\mathscr{F} be a family of continuous maps from U\mathrm{U} to X\mathrm{X}. One says that this family is equicontinuous if for any x∈Ux\in\mathrm{U} and any finite covering (Vj)(\mathrm{V}_{j}) of X\mathrm{X} by affinoid spaces, there exists a neighbourhood Ux\mathrm{U}_{x} of xx in U\mathrm{U} such that for any φ∈ℱ\varphi\in\mathscr{F}, there exists an index jj such that φ⁡(Ux)⊂Vj\varphi(\mathrm{U}_{x})\subset\mathrm{V}_{j}. (This definition is adapted from Definition 10.63 in [6] ; it is the definition of equicontinuity associated to the canonical uniform structure of the compact space X\mathrm{X}.)

We define the equicontinuous locus of ff as the largest open subset Ef\mathrm{E}_{f} of X\mathrm{X} over which the sequence of iterates of ff is equicontinuous.

Proposition 2.4.2.

If LL is ample, then the metric L¯\overline{L} is strongly pluriharmonic on Ef\mathrm{E}_{f}.33 3 The ampleness assumption should not be necessary for the result to hold.

Démonstration.

The proof is inspired from the above-mentioned sources, which in turns is an adaptation of the complex case [41] (see also [52]).

We may replace LL by a positive power of itself and assume that it is very ample, induced by a closed embedding of X\mathrm{X} in Pn\mathrm{P}^{n}, and that the natural map Γ⁡(𝐏n,𝒪⁡(d))→Γ⁡(X,𝒪⁡(d))\Gamma(\mathrm{{\mathbf{P}}}^{n},\mathscr{O}(d))\rightarrow\Gamma(\mathrm{X},\mathscr{O}(d)) is surjective. Then, there are homogeneous polynomials (F0,…,Fn)(F_{0},\dots,F_{n}), of degree dd, with coefficients in KK, and without common zeroes on X\mathrm{X}, such that f([x0:…:xn])=[F0(x):…:Fn(x)]f([x_{0}:\dots:x_{n}])=[F_{0}(x):\dots:F_{n}(x)] for any x=[x0:…:xn]∈Pnx=[x_{0}:\dots:x_{n}]\in\mathrm{P}^{n}. One considers the polynomial map F:An+1→An+1F\colon\mathrm{A}^{n+1}\rightarrow\mathrm{A}^{n+1} ; it lifts a rational map on Pn\mathrm{P}^{n} which extends the morphism ff.

For (x0,…,xn)∈An+1(x_{0},\dots,x_{n})\in\mathrm{A}^{n+1}, define ‖x‖=max⁡(|x0|,…,|xn|)\left\|{x}\right\|=\max(\left|{x_{0}}\right|,\dots,\left|{x_{n}}\right|). The Weil metric on 𝒪⁡(1)\mathscr{O}(1) is given by

log⁡‖sP​(x)‖−1=log⁡|P⁡(x)|−1+deg⁡(P)​log​‖x‖,\log\left\|{s_{P}(x)}\right\|^{-1}=\log\left|{P(x)}\right|^{-1}+\deg(P)\log\left\|{x}\right\|,

where PP is an homogeneous polynomial, sPs_{P} the corresponding global section of 𝒪⁡(deg⁡(P))\mathscr{O}(\deg(P)), and xx is a point of An+1\mathrm{A}^{n+1} such that P⁡(x)≠0P(x)\neq 0. The restriction to X\mathrm{X} of this metric is a semi-positive metric ‖⋅‖0\left\|{\cdot}\right\|_{0} on LL. The construction of the canonical metric on LL introduces a sequence of semi-positive metrics ‖⋅‖n\left\|{\cdot}\right\|_{n} on LL ; these metrics are given by the following explicit formula

log⁡‖sP​(x)‖k−1=log⁡|P⁡(x)|−1+deg⁡(P)​d−k​log​‖F(k)​(x)‖,\log\left\|{s_{P}(x)}\right\|_{k}^{-1}=\log\left|{P(x)}\right|^{-1}+\deg(P)d^{-k}\log\left\|{F^{(k)}(x)}\right\|,

where F(k):An+1→An+1F^{(k)}:\mathrm{A}^{n+1}\rightarrow\mathrm{A}^{n+1} is the kkth iterate of FF.

The convergence of this sequence is therefore equivalent to the convergence of the sequence (d−k​log⁡‖F(k)‖)k(d^{-k}\log\left\|{F^{(k)}}\right\|)_{k} towards a continuous fonction on the preimage of X\mathrm{X} under the projection map An+1∖{0}→Pn\mathrm{A}^{n+1}\setminus\{0\}\rightarrow\mathrm{P}^{n}. The limit is usually called the homogeneous Green function.

For 0≤i≤n0\leq i\leq n, let Vi\mathrm{V}_{i} be the open set of points x=[x0:…:xn]∈Pnx=[x_{0}:\dots:x_{n}]\in\mathrm{P}^{n} such that |xi|>12​‖x‖\left|{x_{i}}\right|>\frac{1}{2}\left\|{x}\right\|. They form an open covering of Pn\mathrm{P}^{n} ; their intersections with X\mathrm{X} form an open covering of X\mathrm{X}.

Fix x∈Efx\in\mathrm{E}_{f} and let U\mathrm{U} be an open neighbourhood of xx such that for any positive integer kk, there exists i∈{0,…,n}i\in\{0,\dots,n\} such that fk​(U)⊂Vif^{k}(\mathrm{U})\subset\mathrm{V}_{i}. For any ii, let NiN_{i} be the set of integers kk such that fk​(U)⊂Vif^{k}(\mathrm{U})\subset\mathrm{V}_{i}. Let us consider any index ii such that NiN_{i} is infinite ; to fix ideas, let us assume that i=0i=0. The canonical norm of a section sPs_{P} at a point y∈Uy\in\mathrm{U} is given by

log⁡‖sP​(y)‖−1\displaystyle\log\left\|{s_{P}(y)}\right\|^{-1} =log⁡|P⁡(y)|−1+deg⁡(P)​limk→∞k∈N0d−k​log​‖F(k)​(y)‖\displaystyle=\log\left|{P(y)}\right|^{-1}+\deg(P)\lim_{\begin{subarray}{c}k\rightarrow\infty\\ k\in N_{0}\end{subarray}}d^{-k}\log\left\|{F^{(k)}(y)}\right\|
=log⁡|P⁡(y)|−1\displaystyle=\log\left|{P(y)}\right|^{-1}
+deg(P)limk→∞k∈N0d−k(log|F0(k)(y)|+logmax0≤i≤m|Fi(k)(y)/F0(k)(y)|).\displaystyle\quad+\deg(P)\lim_{\begin{subarray}{c}k\rightarrow\infty\\ k\in N_{0}\end{subarray}}d^{-k}\left(\log\left|{F_{0}^{(k)}(y)}\right|+\log\max_{0\leq i\leq m}\left|{F_{i}^{(k)}(y)/F_{0}^{(k)}(y)}\right|\right).

Observe that [F0(k)(y):…:Fm(k)(y)][F_{0}^{(k)}(y):\dots:F^{(k)}_{m}(y)] are the homogeneous coordinates of the point fk​(y)f^{k}(y). Since y∈Uy\in\mathrm{U} and fk​(U)⊂V0f^{k}(\mathrm{U})\subset\mathrm{V}_{0}, one has |Fi(k)​(y)|≤2​|F0(k)​(y)|\left|{F^{(k)}_{i}(y)}\right|\leq 2\left|{F^{(k)}_{0}(y)}\right|, so that the last term is bounded by d−k​log⁡2d^{-k}\log 2 and uniformly converges to 00 on U\mathrm{U}. Finally, uniformly on U\mathrm{U},

log⁡‖sP​(y)‖−1=log⁡|P⁡(y)|−1+deg⁡(P)​limk→∞k∈N0d−k​log​|F0(k)​(y)|.\log\left\|{s_{P}(y)}\right\|^{-1}=\log\left|{P(y)}\right|^{-1}+\deg(P)\lim_{\begin{subarray}{c}k\rightarrow\infty\\ k\in N_{0}\end{subarray}}d^{-k}\log\left|{F_{0}^{(k)}(y)}\right|.

This shows that log⁡‖sP‖−1\log\left\|{s_{P}}\right\|^{-1} is strongly harmonic on U\mathrm{U}, as claimed. ∎

Corollary 2.4.3.

The canonical measure c1​(L¯)nc_{1}(\overline{L})^{n} vanishes on Ef\mathrm{E}_{f}.

Démonstration.

It suffices to apply Prop. 2.3.3. ∎

Remarks

1) The particular case X=Pn\mathrm{X}=\mathrm{P}^{n} generalizes Theorem 6 in [42] according to which canonical metrics are locally constant on the classical Fatou set (meaning that the norm of a non-vanishing local section is locally constant). Indeed, the restriction to the set of smooth rigid points of a strongly harmonic function is locally constant. This follows from the fact that any such point has an affinoid neighbourhood U\mathrm{U} which is a polydisk, so that the absolute value of any invertible function on U\mathrm{U}, hence any harmonic function on U\mathrm{U} is constant.

2) In the case X=P1\mathrm{X}=\mathrm{P}^{1}, Fatou and Julia sets in the Berkovich framework have been studied by Rivera-Letelier [48] and Benedetto [9] ; see also [6] for a detailed exposition of the theory and further references. An example of Rivera-Letelier on the projective line (Example 10.70 of [6]) shows that the equicontinuity locus Ef\mathrm{E}_{f} may be smaller than the complement of the support of the measure c1​(L¯)c_{1}(\overline{L}).

Anyway, this proposition suggests the interest of a general study of Fatou sets and of pluripotential theory on Berkovich spaces. For example, is there an interesting theory of pseudoconvexity for Berkovich spaces ? Is it related to Stein spaces ? By analogy to the complex case (see [52]), are Berkovich Fatou components pseudoconvex ? Stein ?

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