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2.2. The hybrid topology [0155]

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2.2. The hybrid topology

Next we define a natural topology on the disjoint union

𝒳hyb:=(π’³βˆ–D)β€‹βˆΞ”β‘(D).{\mathcal{X}}^{\mathrm{hyb}}:=({\mathcal{X}}\setminus D)\coprod\Delta(D).

Consider a connected open set π’°βŠ‚π’³{\mathcal{U}}\subset{\mathcal{X}} meeting DD and local coordinates z=(z0,…,zn)z=(z_{0},\dots,z_{n}) on 𝒰{\mathcal{U}}. We say that the pair (𝒰,z)({\mathcal{U}},z) is adapted (to DD) if the following conditions hold:

  • (i)

    if E0,…,EpE_{0},\dots,E_{p} are the irreducible components of DD intersecting 𝒰{\mathcal{U}}, then we have π’°βˆ©E0βˆ©β‹―βˆ©Ep=π’°βˆ©Y̊{\mathcal{U}}\cap E_{0}\cap\dots\cap E_{p}={\mathcal{U}}\cap\mathring{Y} for a component YY of E0βˆ©β‹―βˆ©EpE_{0}\cap\dots\cap E_{p};

  • (ii)

    ziz_{i} is an equation of Eiβˆ©π’°E_{i}\cap{\mathcal{U}} with |zi|<1|z_{i}|<1, 0≀i≀p0\leq i\leq p.

We call Y=Y𝒰Y=Y_{\mathcal{U}} the stratum of 𝒰{\mathcal{U}}, and denote by

σ𝒰={wβˆˆβ„p+1βˆ£βˆ‘i=0pbi​wi=1}\sigma_{\mathcal{U}}=\left\{w\in{\mathbb{R}}^{p+1}\mid\sum_{i=0}^{p}b_{i}w_{i}=1\right\}

the corresponding face of Δ⁑(D)\Delta(D). The function f𝒰,z:=∏i=0pzibif_{{\mathcal{U}},z}:=\prod_{i=0}^{p}z_{i}^{b_{i}} is an equation of DD in 𝒰{\mathcal{U}}, with |f𝒰,z|<1|f_{{\mathcal{U}},z}|<1, and we get a continuous map Log𝒰:π’°βˆ–Dβ†’ΟƒY\operatorname{Log}_{{\mathcal{U}}}\colon{\mathcal{U}}\setminus D\to\sigma_{Y} by setting

Log𝒰=(log⁑|zi|log⁑|f𝒰|)0≀i≀p.\operatorname{Log}_{{\mathcal{U}}}=\left(\frac{\log|z_{i}|}{\log|f_{\mathcal{U}}|}\right)_{0\leq i\leq p}.

For any two adapted coordinate charts (𝒰,z)({\mathcal{U}},z), (𝒰′,zβ€²)({\mathcal{U}}^{\prime},z^{\prime}), with the same stratum YY, we have ziβ€²=ui​ziz^{\prime}_{i}=u_{i}z_{i} with uiu_{i} nonvanishing on π’°βˆ©π’°β€²{\mathcal{U}}\cap{\mathcal{U}}^{\prime}, for i=0,…,pi=0,\dots,p (after a possible reindexing); it follows that

Log𝒰′=Log𝒰+O⁑(1log⁑|f𝒰,z|βˆ’1)\operatorname{Log}_{{\mathcal{U}}^{\prime}}=\operatorname{Log}_{{\mathcal{U}}}+O\left(\frac{1}{\log|f_{{\mathcal{U}},z}|^{-1}}\right) (2.1)

locally uniformly on π’°βˆ©π’°β€²{\mathcal{U}}\cap{\mathcal{U}}^{\prime}. We next show how to globalize this construction.

Proposition 2.1.

There exists an open neighborhood π’±βŠ‚π’³{\mathcal{V}}\subset{\mathcal{X}} of DD and a continuous map Log𝒱:π’±βˆ–D→Δ⁑(D)\operatorname{Log}_{\mathcal{V}}\colon{\mathcal{V}}\setminus D\to\Delta(D) such that for each adapted coordinate chart (𝒰,z)({\mathcal{U}},z) with π’°βŠ‚π’±{\mathcal{U}}\subset{\mathcal{V}} we have Log𝒱⁑(π’°βˆ–D)βŠ‚Οƒπ’°\operatorname{Log}_{\mathcal{V}}({\mathcal{U}}\setminus D)\subset\sigma_{\mathcal{U}} and

Log𝒱=Log𝒰+O⁑(1log⁑|f𝒰,z|βˆ’1)\operatorname{Log}_{\mathcal{V}}=\operatorname{Log}_{{\mathcal{U}}}+O\left(\frac{1}{\log|f_{{\mathcal{U}},z}|^{-1}}\right) (2.2)

uniformly on compact subsets of 𝒰{\mathcal{U}}.

This will be accomplished by means of a partition of unity, using the following elementary special case ofΒ [Cle77, Theorem 5.7].

Lemma 2.2.

There exists a family ((𝒱α,zΞ±))α∈A(({\mathcal{V}}_{\alpha},z_{\alpha}))_{\alpha\in A} of adapted coordinate charts, such that (𝒱α)Ξ±({\mathcal{V}}_{\alpha})_{\alpha} forms a locally finite covering of DD and such that the strata YΞ±Y_{\alpha} of the 𝒱α{\mathcal{V}}_{\alpha} satisfy

β‹‚Ξ²βˆˆBπ’±Ξ²β‰ βˆ…βŸΉβ‹‚Ξ²βˆˆBYΞ²β‰ βˆ…\bigcap_{\beta\in B}{\mathcal{V}}_{\beta}\neq\emptyset\Longrightarrow\bigcap_{\beta\in B}Y_{\beta}\neq\emptyset (2.3)

for every finite BβŠ‚AB\subset A.

Proof of PropositionΒ 2.1.

Pick an open cover (𝒱α)Ξ±({\mathcal{V}}_{\alpha})_{\alpha} as in LemmaΒ 2.2, and denote by LogΞ±:π’±Ξ±βˆ–D→σα\operatorname{Log}_{\alpha}\colon{\mathcal{V}}_{\alpha}\setminus D\to\sigma_{\alpha} the corresponding maps. Set 𝒱:=⋃α𝒱α{\mathcal{V}}:=\bigcup_{\alpha}{\mathcal{V}}_{\alpha}, and pick a partition of unity (χα)(\chi_{\alpha}) subordinate to (𝒱α)({\mathcal{V}}_{\alpha}). We claim that for each ΞΎβˆˆπ’±\xi\in{\mathcal{V}} there exists an open neighborhood WW of ΞΎ\xi and a face ΟƒW\sigma_{W} of Δ⁑(D)\Delta(D) such that

W∩suppβ‘Ο‡Ξ±β‰ βˆ…βŸΉΟƒΞ±βŠ‚ΟƒWW\cap\operatorname{supp}\chi_{\alpha}\neq\emptyset\Longrightarrow\sigma_{\alpha}\subset\sigma_{W}

for any α∈A\alpha\in A. Indeed, using (2.3) it is easy to see that

W:=β‹‚Ξ±|ΞΎβˆˆπ’°Ξ±π’±Ξ±βˆ–β‹ƒΞ±|ΞΎβˆ‰supp⁑χβsupp⁑χβW:=\bigcap_{\alpha\mid\xi\in{\mathcal{U}}_{\alpha}}{\mathcal{V}}_{\alpha}\setminus\bigcup_{\alpha\mid\xi\notin\operatorname{supp}\chi_{\beta}}\operatorname{supp}\chi_{\beta}

satisfies this property. By convexity of ΟƒW\sigma_{W}, it follows that Log𝒱:=βˆ‘Ξ±Ο‡Ξ±β€‹Log𝒱α\operatorname{Log}_{\mathcal{V}}:=\sum_{\alpha}\chi_{\alpha}\operatorname{Log}_{{\mathcal{V}}_{\alpha}} is well-defined on Wβˆ–DW\setminus D, and hence yields a continuous map Log𝒱:π’±βˆ–D→Δ⁑(D)\operatorname{Log}_{\mathcal{V}}\colon{\mathcal{V}}\setminus D\to\Delta(D). The last property is a direct consequence ofΒ (2.1). ∎

We extend the previous map as

Log𝒱:𝒱hyb:=(π’±βˆ–D)βˆͺΔ⁑(D)→Δ⁑(D)\operatorname{Log}_{\mathcal{V}}\colon{\mathcal{V}}^{\mathrm{hyb}}:=({\mathcal{V}}\setminus D)\cup\Delta(D)\to\Delta(D)

by setting Log𝒱=id\operatorname{Log}_{\mathcal{V}}=\operatorname{id} on Δ⁑(D)\Delta(D).

Definition 2.3.

The hybrid topology on 𝒳hyb:=(π’³βˆ–D)βˆͺΔ⁑(D){\mathcal{X}}^{\mathrm{hyb}}:=({\mathcal{X}}\setminus D)\cup\Delta(D) is defined as the coarsest topology such that:

  • (i)

    π’³βˆ–Dβ†ͺ𝒳hyb{\mathcal{X}}\setminus D\hookrightarrow{\mathcal{X}}^{\mathrm{hyb}} is an open embedding;

  • (ii)

    For every open neighborhood 𝒱{\mathcal{V}} of DD in 𝒳{\mathcal{X}}, the set (π’±βˆ–D)βˆͺΔ⁑(𝒳)({\mathcal{V}}\setminus D)\cup\Delta({\mathcal{X}}) is open in 𝒳hyb{\mathcal{X}}^{\mathrm{hyb}};

  • (iii)

    Log𝒱:𝒱hyb→Δ⁑(D)\operatorname{Log}_{\mathcal{V}}\colon{\mathcal{V}}^{\mathrm{hyb}}\to\Delta(D) is continuous.

UsingΒ (2.2), this definition is easily seen to be independent of the choice of map Log𝒱\operatorname{Log}_{\mathcal{V}}. If DD is compact and KβŠ‚π’³K\subset{\mathcal{X}} is a compact neighborhood of DD, then one easily checks that the corresponding subset Khyb=(Kβˆ–D)βˆͺΔ⁑(D)K^{\mathrm{hyb}}=(K\setminus D)\cup\Delta(D) is compact (Hausdorff). When D=b0​E0D=b_{0}E_{0} has only one irreducible component, KhybK^{\mathrm{hyb}} is simply the Tychonoff one-point compactification of Kβˆ–DK\setminus D.

Example 2.4.

Set 𝒳=𝔻2{\mathcal{X}}={\mathbb{D}}^{2} and D=E0+E1D=E_{0}+E_{1} the union of the coordinate axes, with coordinates (z0,z1)(z_{0},z_{1}). Then 𝒰=𝒳{\mathcal{U}}={\mathcal{X}} is itself an adapted coordinate chart. In these coordinates, Log𝒰:π’°βˆ–D→σ𝒰\operatorname{Log}_{{\mathcal{U}}}\colon{\mathcal{U}}\setminus D\to\sigma_{\mathcal{U}} becomes the map (π”»βˆ—)2β†’[0,1]({\mathbb{D}}^{*})^{2}\to[0,1] sending (z0,z1)(z_{0},z_{1}) to log⁑|z1|/log⁑|z0​z1|\log|z_{1}|/\log|z_{0}z_{1}|. As a consequence, given tβˆˆβ„+βˆ—t\in{\mathbb{R}}_{+}^{*} and 0<Ξ΅β‰ͺ10<\varepsilon\ll 1, the closure in 𝒳hyb{\mathcal{X}}^{\mathrm{hyb}} of the closed subset

FΞ΅:={0<|z0|,|z1|≀Ρ,|z0|t+Ρ≀|z1|≀|z0|tβˆ’Ξ΅}βŠ‚π”»2F_{\varepsilon}:=\{0<|z_{0}|,|z_{1}|\leq\varepsilon,|z_{0}|^{t+\varepsilon}\leq|z_{1}|\leq|z_{0}|^{t-\varepsilon}\}\subset{\mathbb{D}}^{2}

is given by FΒ―Ξ΅=FΞ΅βˆͺIΞ΅{\bar{F}}_{\varepsilon}=F_{\varepsilon}\cup I_{\varepsilon}, where IΞ΅:={t∈[0,1]∣tβˆ’Ξ΅1+tβˆ’Ξ΅β‰€t≀t+Ξ΅1+t+Ξ΅}I_{\varepsilon}:=\{t\in[0,1]\mid\frac{t-\varepsilon}{1+t-\varepsilon}\leq t\leq\frac{t+\varepsilon}{1+t+\varepsilon}\}. Further, the sets FΒ―Ξ΅{\bar{F}}_{\varepsilon}, for 0<Ξ΅β‰ͺ10<\varepsilon\ll 1 form a basis of closed neighborhoods of the point t1+t∈[0,1]\frac{t}{1+t}\in[0,1] in 𝒳hyb{\mathcal{X}}^{\mathrm{hyb}}. See FigureΒ 1.

Original source figure
Figure 1. The figure shows the closed subset FΞ΅F_{\varepsilon} in ExampleΒ 2.4.

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