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6.5 ๐™ -affine version of Gauss-Bonnet theorem [03V2]

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6.5 ๐™{\bf Z}-affine version of Gauss-Bonnet theorem

Let BB be a connected compact oriented topological surface, Bsโ€‹iโ€‹nโ€‹gโŠ‚BB^{sing}\subset B a finite set. Assume that Bsโ€‹m=Bโˆ–Bsโ€‹iโ€‹nโ€‹gB^{sm}=B\setminus B^{sing} carries a ๐™{\bf Z}-affine structure such that for any xโˆˆBsโ€‹iโ€‹nโ€‹gx\in B^{sing} there exists a small neighborhood UU such that U=โˆชiโˆˆIUiU=\cup_{i\in I}U_{i} where II is a finite set and each UiU_{i} is affine equivalent to a germ of an angle in ๐‘2{{\bf R}}^{2}, with xx being the apex of each angle.

The aim of this section is to define a map ilโ€‹oโ€‹c:Bsโ€‹iโ€‹nโ€‹gโ†’112โ€‹๐™i_{loc}:B^{sing}\to{\frac{1}{12}}{{\bf Z}} (which depends only on ๐™{\bf Z}-affine structure near Bsโ€‹iโ€‹nโ€‹gB^{sing}) and prove the following result (a kind of Gauss-Bonnet theorem).

Theorem 2

The following equality holds

โˆ‘xโˆˆBsโ€‹iโ€‹nโ€‹gilโ€‹oโ€‹cโ€‹(x)=ฯ‡โก(B),\sum_{x\in B^{sing}}i_{loc}(x)=\chi(B)\,\,,

where ฯ‡โก(B)\chi(B) is the Euler characteristic of BB.

We start with the construction of ilโ€‹oโ€‹ci_{loc}. Let us denote by Sโ€‹Lโ€‹(2,๐™)~\widetilde{SL(2,{{\bf Z}})} the pre-image of Sโ€‹Lโ€‹(2,๐™)SL(2,{{\bf Z}}) in the universal covering Sโ€‹Lโ€‹(2,๐‘)~\widetilde{SL(2,{{\bf R}})} of the group Sโ€‹Lโ€‹(2,๐‘)SL(2,{{\bf R}}). The group Sโ€‹Lโ€‹(2,๐‘)~\widetilde{SL(2,{{\bf R}})} contains ฯ€1โ€‹(Sโ€‹Lโ€‹(2,๐‘))โ‰ƒ๐™\pi_{1}(SL(2,{{\bf R}}))\simeq{{\bf Z}}. Let uu be a generator of the latter (it belongs also to Sโ€‹Lโ€‹(2,๐™)~\widetilde{SL(2,{{\bf Z}})}).

We have an exact sequence of groups

1โ†’๐™โ†’Sโ€‹Lโ€‹(2,๐™)~โ†’Pโ€‹Sโ€‹Lโ€‹(2,๐™)โ†’1.1\to{{\bf Z}}\to\widetilde{SL(2,{{\bf Z}})}\to PSL(2,{{\bf Z}})\to 1\,\,.

Notice that Pโ€‹Sโ€‹Lโ€‹(2,๐™)PSL(2,{{\bf Z}}) is a free product ๐™/2โˆ—๐™/3{{\bf Z}}/2*{{\bf Z}}/3. Moreover, in the above exact sequence ๐™{{\bf Z}} is embedded into the center of Sโ€‹Lโ€‹(2,๐™)~\widetilde{SL(2,{{\bf Z}})}. Notice that uu is the image of 2โˆˆ๐™2\in{{\bf Z}}. One can choose representatives a2,a3a_{2},a_{3} of the standard generators of Pโ€‹Sโ€‹Lโ€‹(2,๐™)PSL(2,{{\bf Z}}) in such a way that Sโ€‹Lโ€‹(2,๐™)~\widetilde{SL(2,{{\bf Z}})} is generated by u,a2,a3u,a_{2},a_{3} subject to the relations a22=a33,a24=a36=ua_{2}^{2}=a_{3}^{3},a_{2}^{4}=a_{3}^{6}=u. This gives a homomorphism of groups ฯ•:Sโ€‹Lโ€‹(2,๐™)~โ†’๐™\phi:\widetilde{SL(2,{{\bf Z}})}\to{{\bf Z}} such that ฯ•โก(a2)=3,ฯ•โก(a3)=2,ฯ•โก(u)=12\phi(a_{2})=3,\phi(a_{3})=2,\phi(u)=12. Dividing by 1212 we obtain a homomorphism i:Sโ€‹Lโ€‹(2,๐™)~โ†’112โ€‹๐™i:\widetilde{SL(2,{{\bf Z}})}\to{\frac{1}{12}}{{\bf Z}} such that iโก(u)=1i(u)=1.

Let us consider a topological S1S^{1}-bundle EE over BB, such that the fiber over xโˆˆBx\in B is the union of all affine rays outcoming of xx. Then the restriction of EE to Bsโ€‹mB^{sm} is just the spherical bundle. Let us pick x0โˆˆBsโ€‹mx_{0}\in B^{sm} and remove it from BB together with small neighborhoods of all points Bsโ€‹iโ€‹nโ€‹gB^{sing}. We denote by B1B_{1} the topological space obtained in this way. We can trivialize the tangent bundle over B1B_{1} (we choose a CโˆžC^{\infty}-trivialization, compatible with Sโ€‹Lโ€‹(2,๐‘)SL(2,{{\bf R}})-structure) in such a way that it extends to a continuous trivialization of S1S^{1}-bundle EE over Bโˆ–{x0}B\setminus\{x_{0}\}. Let ฮฑโˆˆฮฉ1โ€‹(B1)โŠ—sโ€‹lโ€‹(2,๐‘)\alpha\in\Omega^{1}(B_{1})\otimes sl(2,{{\bf R}}) be a 11-form defined by means of the affine structure โˆ‡\nabla on B1B_{1}. Then dโ€‹ฮฑ+12โ€‹[ฮฑ,ฮฑ]=0d\alpha+{\frac{1}{2}}[\alpha,\alpha]=0 and ฮฑ\alpha defines a flat connection on a trivial Sโ€‹Lโ€‹(2,๐‘)~\widetilde{SL(2,{{\bf R}})}-bundle on B1B_{1}. It gives a a monodromy representation ฯ€1โ€‹(B1)โ†’Sโ€‹Lโ€‹(2,๐™)~\pi_{1}(B_{1})\to\widetilde{SL(2,{{\bf Z}})} defined up to a conjugation. Composing it with the homomorphism ii we obtain a homomorphism ฯ€1โ€‹(B1)โ†’112โ€‹๐™\pi_{1}(B_{1})\to{\frac{1}{12}}{{\bf Z}}. Since 112โ€‹๐™{\frac{1}{12}}{{\bf Z}} is an abelian group, the latter homomorphism is a composition ฯ€1โ€‹(B1)โ†’H1โ€‹(B1,๐™)โ†’112โ€‹๐™\pi_{1}(B_{1})\to H_{1}(B_{1},{\bf Z})\to{\frac{1}{12}}{{\bf Z}}. Let us pick small circles [ฮณx]โˆˆH1โ€‹(B,๐™)[\gamma_{x}]\in H_{1}(B,{\bf Z}) for each xโˆˆBsโ€‹iโ€‹nโ€‹gx\in B^{sing}. Then the above homomorphism gives us a number denoted by ilโ€‹oโ€‹cโ€‹(x)โˆˆ112โ€‹๐™i_{loc}(x)\in{\frac{1}{12}}{{\bf Z}}.

Proof of the Theorem. Let us pick up a small circle [ฮณx0]โˆˆH1โ€‹(B1,๐™)[\gamma_{x_{0}}]\in H_{1}(B_{1},{\bf Z}) around x0x_{0}. Then โˆ‘xโˆˆBsโ€‹iโ€‹nโ€‹g[ฮณx]+[ฮณx0]=0\sum_{x\in B^{sing}}[\gamma_{x}]+[\gamma_{x_{0}}]=0. The monodromy around x0x_{0} can be easily computed via the winding number of the induced vector field (section of E|ฮณx0E_{|\gamma_{x_{0}}}) and is equal to โˆ’ฯ‡โก(B)โ€‹u-\chi(B)u. Applying homomorphism ii we obtain the result. โ– \blacksquare

Corollary 2

Suppose that the monodromy for each point xโˆˆBsโ€‹iโ€‹nโ€‹gx\in B^{sing} is the standard one (see Section 6.4). Then one has two possibilities:

a) Bsโ€‹iโ€‹nโ€‹g=โˆ…B^{sing}=\emptyset and B=Bsโ€‹mB=B^{sm} is a 22-dimensional torus;

b) the set Bsโ€‹iโ€‹nโ€‹gB^{sing} consists of 2424 distinct points on the sphere S2S^{2}.

Proof. It is easy to see that for each point xโˆˆBsโ€‹iโ€‹nโ€‹gx\in B^{sing} one has ilโ€‹oโ€‹cโ€‹(x)=112i_{loc}(x)={\frac{1}{12}}. Then from Gauss-Bonnet theorem one deduces that ฯ‡โก(B)=2โˆ’2โ€‹g\chi(B)=2-2g, where gg is the genus of the Riemann surface BB. Then we have

|Bsโ€‹iโ€‹nโ€‹g|12=2โˆ’2โ€‹g.{\frac{|B^{sing}|}{12}}=2-2g\,\,.

Since LHS is non-negative we conclude that either g=1g=1 or g=0g=0. In the first case |Bsโ€‹iโ€‹nโ€‹g|=0|B^{sing}|=0 and we have a ๐™{\bf Z}-affine structure on a torus. In the second case we have |Bsโ€‹iโ€‹nโ€‹g|=24|B^{sing}|=24 and g=0g=0. โ– \blacksquare

Remark 2

This corollary was proved in [LeS] by different methods.

Similarly, for the affine structure with the monodromy at each point conjugate to

(1401)\left(\begin{array}[]{cc}1&4\\ 0&1\end{array}\right)

one has ilโ€‹oโ€‹cโ€‹(x)=13i_{loc}(x)=\frac{1}{3}, and we have six singular points on S2S^{2} (see Section 4.2.5).

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