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7 K -affine structures [03VK]

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7 KK-affine structures

7.1 Definitions

Let Bs​mB^{sm} be a manifold with 𝐙{\bf Z}-affine structure. The sheaf of 𝐙{\bf Z}-affine functions A​f​f𝐙:=A​f​f𝐙,Bs​mAff_{{\bf Z}}:=Aff_{{{\bf Z}},B^{sm}} gives rise to an exact sequence of sheaves of abelian groups

0→𝐑→A​f​f𝐙→(Tβˆ—)𝐙→0.0\to{{\bf R}}\to Aff_{{\bf Z}}\to(T^{\ast})^{{\bf Z}}\to 0\,\,.

Let KK be a complete non-archimedean field with a valuation map v​a​lval. We give two equivalent definitions of a KK-affine structure on Bs​mB^{sm} compatible with a given 𝐙{\bf Z}-affine structure.

Definition 11

A KK-affine structure on Bs​mB^{sm} compatible with the given 𝐙{\bf Z}-affine structure is a sheaf A​f​fKAff_{K} of abelian groups on Bs​mB^{sm}, an exact sequence of sheaves

0β†’KΓ—β†’A​f​fKβ†’(Tβˆ—)𝐙→0,0\to K^{\times}\to Aff_{K}\to(T^{\ast})^{{\bf Z}}\to 0\,\,,

together with a homomorphism Ξ¦\Phi of this exact sequence to the exact sequence of sheaves of abelian groups

0→𝐑→A​f​f𝐙→(Tβˆ—)𝐙→0,0\to{{\bf R}}\to Aff_{{\bf Z}}\to(T^{\ast})^{{\bf Z}}\to 0\,\,,

such that Ξ¦=i​d\Phi=id on (Tβˆ—)𝐙(T^{\ast})^{{\bf Z}} and Ξ¦=v​a​l\Phi=val on KΓ—K^{\times}.

Since Bs​mB^{sm} carries a 𝐙{\bf Z}-affine structure, we have an associated G​L​(n,𝐙)⋉𝐑nGL(n,{{\bf Z}})\ltimes{{\bf R}}^{n}-torsor on Bs​mB^{sm}, whose fiber over a point xx consists of all 𝐙{\bf Z}-affine coordinate systems at xx.

Definition 12

A KK-affine structure on Bs​mB^{sm} compatible with the given 𝐙{\bf Z}-affine structure is a G​L​(n,𝐙)⋉(KΓ—)nGL(n,{{\bf Z}})\ltimes(K^{\times})^{n}-torsor on Bs​mB^{sm} such that the application of v​a​lΓ—nval^{\times n} to (KΓ—)n(K^{\times})^{n} gives the initial G​L​(n,𝐙)⋉𝐑nGL(n,{{\bf Z}})\ltimes{{\bf R}}^{n}-torsor.

Equivalence of two definitions from above is obvious in local 𝐙{\bf Z}-affine coordinates. The reason is that the set of automorphisms of the exact sequence of groups

0β†’KΓ—β†’K××𝐙n→𝐙nβ†’00\to K^{\times}\to K^{\times}\times{{\bf Z}}^{n}\to{{\bf Z}}^{n}\to 0

identical on KΓ—K^{\times} coincides with the group G​L​(n,𝐙)⋉(KΓ—)nGL(n,{{\bf Z}})\ltimes(K^{\times})^{n}.

Finally, we can formulate the Fixed Point Property for KK-affine structures (see Section 3.1 for 𝐙{\bf Z}-affine case):
Fixed Point Property for KK-affine structures. In the notation of the end of Section 3.1, for any b∈Bs​i​n​gb\in B^{sing} and sufficiently small neighborhood UU of bb the lifted monodromy representation Ο€1​(U)β†’G​L​(n,𝐙)⋉(KΓ—)n\pi_{1}(U)\to GL(n,{{\bf Z}})\ltimes(K^{\times})^{n} has fixed vectors in KΓ—nK^{\times n}, and the 𝐑{{\bf R}}-affine span of the corresponding (under the valuation map) vectors in 𝐑n{{\bf R}}^{n} coincides with the set of fixed points of the monodromy representation Ο€1​(U)β†’G​L​(n,𝐙)⋉𝐑n\pi_{1}(U)\to GL(n,{{\bf Z}})\ltimes{{\bf R}}^{n}.

7.2 KK-affine structure on smooth points

Starting from this section till the end of the paper (except of the Section 11.7) we will assume the following
Zero Charactersistic Assumption. KK is a complete non-archimedean local field such that its residue field has characteristic zero.

Let XX be a KK-analytic manifold of dimension nn and we are given a continuous map Ο€:Xβ†’B\pi:X\to B, where BB is a topological space. Then Bs​mB^{sm} carries a 𝐙{\bf Z}-affine structure (Theorem 1). Suppose that there is an open KK-analytic submanifold UβŠ‚XU\subset X such that Ο€βˆ’1​(Bs​m)βŠ‚U\pi^{-1}(B^{sm})\subset U and there is a nonwhere vanishing analytic form Ξ©βˆˆΞ“β‘(U,Ξ©Xn)\Omega\in\Gamma(U,\Omega_{X}^{n}). We are going to define a 𝐙{\bf Z}-affine function V​a​l​(Ξ©)Val(\Omega) similarly to the definition of the function V​a​l​(Ο†)Val(\varphi) in Section 4.1. Namely, in local coordinates (z1,…,zn)(z_{1},...,z_{n}) we consider the expression Ο†:=Ξ©/β‹€1≀i≀n(d​zi/zi)\varphi:=\Omega/\bigwedge_{1\leq i\leq n}(dz_{i}/z_{i}). This is an invertible function, and we define V​a​l​(Ξ©)Val(\Omega) as V​a​l​(Ο†)Val(\varphi). The independence on the choice of coordinates follows from the following lemma

Lemma 2

Let (zi)i=1,…,n,(ziβ€²)i=1,…,n(z_{i})_{i=1,\dots,n},\,\,(z^{\prime}_{i})_{i=1,\dots,n} be two systems of invertible coordinates on Ο€βˆ’1​(U)\pi^{-1}(U) for some connected open UβŠ‚Bs​mU\subset B^{sm}. Then

|(β‹€1≀i≀n(d​zi/zi))/(β‹€1≀i≀n(d​ziβ€²/ziβ€²))|x=1β€‹βˆ€xβˆˆΟ€βˆ’1​(U).\left|\left({\textstyle\bigwedge_{1\leq i\leq n}(dz_{i}/z_{i})}\right)/\left({\textstyle\bigwedge_{1\leq i\leq n}(dz^{\prime}_{i}/z^{\prime}_{i})}\right)\right|_{x}=1\,\,\,\forall x\in\pi^{-1}(U)\,\,.

Proof: By Lemma 1 from Section 4.1 we know that ziβ€²z_{i}^{\prime} as any invertible function can be written in form ci​zI(i)​(1+o⁑(1))c_{i}z^{I^{(i)}}(1+o(1)) for some nonzero ci∈Kc_{i}\in K and a multi-index I(i)βˆˆπ™nI^{(i)}\in{\bf Z}^{n}. Vectors I(1),…,I(n)I^{(1)},\dots,I^{(n)} form a basis of 𝐙n{\bf Z}^{n}, as follows from the condition that z1β€²,…,znβ€²z_{1}^{\prime},\dots,z_{n}^{\prime} form a coordinate system. Therefore, after applying the change of coordinates zi↦ci​zI(i)z_{i}\mapsto c_{i}z^{I^{(i)}} preserving form β‹€id​zi/zi\bigwedge_{i}dz_{i}/z_{i} up to sign, we may assume that ziβ€²=(1+o⁑(1))​ziz_{i}^{\prime}=(1+o(1))z_{i}. The Jacobian matrix of the transformation (zi)β†’(ziβ€²)(z_{i})\to(z_{i}^{\prime}) is the identity matrix plus terms of size o⁑(1)o(1). Therefore its determinant has norm equal to 1. β– \blacksquare

Now we make the following
Constant Norm Assumption. The function V​a​l​(Ο†)Val(\varphi) is locally constant.

Theorem 4

If the Constant Norm Assumption is satisfied then there is a KK-affine structure on Bs​mB^{sm} compatible with the 𝐙{\bf Z}-affine structure A​f​f𝐙,Bs​mc​a​nAff_{{{\bf Z}},B^{sm}}^{can} (see Section 4.1).

Proof. Let us write in local coordinates Ξ©=φ⁑(z1,…​zn)​⋀1≀i≀nd​zizi\Omega=\varphi(z_{1},...z_{n})\bigwedge_{1\leq i\leq n}{dz_{i}\over z_{i}}. Define residue R​e​s​(Ξ©)∈KRes(\Omega)\in K as the constant term Ο†0\varphi_{0} in the Laurent expansion φ⁑(z1,…​zn)=βˆ‘Iβˆˆπ™nΟ†I​zI\varphi(z_{1},...z_{n})=\sum_{I\in{\bf Z}^{n}}\varphi_{I}z^{I}. It is easy to see that R​e​s​(Ξ©)Res(\Omega) does not depend (up to a sign) on the choice of local coordinates. For non-vanishing everywhere Ξ©\Omega satisfying Constant Norm Assumption we have exp⁑(βˆ’V​a​l​(Ο†))=|Ο†|=|Ο†0|\exp(-Val(\varphi))=|\varphi|=|\varphi_{0}|. Therefore we have R​e​s​(Ξ©)β‰ 0Res(\Omega)\neq 0.

Let us return to the proof of the Theorem. Let FF be the sheaf of abelian groups FβŠ‚Ο€βˆ—β€‹(π’ͺXΓ—)F\subset\pi_{\ast}({\cal O}_{X}^{\times}) consisting of ff such that V​a​l​(f)=0Val(f)=0. Then we have an exact sequence of sheaves

0β†’KΓ—/π’ͺKΓ—β†’Ο€βˆ—β€‹(π’ͺXΓ—)/Fβ†’(TXβˆ—)𝐙→0,0\to K^{\times}/{\cal O}_{K}^{\times}\to\pi_{\ast}({\cal O}_{X}^{\times})/F\to(T_{X}^{\ast})^{{\bf Z}}\to 0\,\,\,,

where π’ͺK{\cal O}_{K} denotes the constant sheaf with the fiber being the ring of integers of KK. Indeed we embed KΓ—/π’ͺKΓ—K^{\times}/{\cal O}_{K}^{\times} into Ο€βˆ—β€‹(π’ͺXΓ—)/F\pi_{\ast}({\cal O}_{X}^{\times})/F as constant functions. The projection Ο€βˆ—β€‹(π’ͺXΓ—)/Fβ†’(TXβˆ—)𝐙\pi_{\ast}({\cal O}_{X}^{\times})/F\to(T_{X}^{\ast})^{{\bf Z}} assigns to the function ff the linear part of the corresponding 𝐙{\bf Z}-affine function V​a​l​(f)Val(f).

Notice that if UβŠ‚Bs​mU\subset B^{sm} is a connected domain then any fβˆˆΞ“β‘(U,F)f\in\Gamma(U,F) can be written (non-canonically) as f=a⁑(1+r)f=a(1+r), where a∈π’ͺKΓ—a\in{\cal O}_{K}^{\times} and r=o⁑(1)r=o(1) in Ο€βˆ’1​(U)\pi^{-1}(U).

We define an epimorphism of sheaves pΞ©:Fβ† π’ͺKΓ—p_{\Omega}:F\twoheadrightarrow{\cal O}_{K}^{\times} by formula

pΩ​(f)=pΩ​(a⁑(1+r))=a​exp⁑(R​e​s​(Ω​log⁑(1+r))R​e​s​(Ξ©)).p_{\Omega}(f)=p_{\Omega}(a(1+r))=a\,\exp\left({Res(\Omega\,\log(1+r))\over{Res(\Omega)}}\right)\,\,.

Here exp\exp and log\log are understood as infinite convergent series (in order to make sense of them we use Zero Characteristic Assumption).

It is easy to see that pΞ©p_{\Omega} is well-defined. Then the exact sequence of sheaves

1β†’KΓ—β†’Ο€βˆ—β€‹(π’ͺXΓ—)/ker⁑(pΞ©)β†’(TXβˆ—)𝐙→11\to K^{\times}\to\pi_{\ast}({\cal O}_{X}^{\times})/\ker(p_{\Omega})\to(T_{X}^{\ast})^{{\bf Z}}\to 1

defines a KK-affine structure on Bs​mB^{sm} compatible with A​f​f𝐙,Bs​mc​a​nAff_{{{\bf Z}},B^{sm}}^{can}. This concludes proof of the Theorem. β– \blacksquare

Notice that the above proof gives an explicit construction of the KK-affine structure. We will denote it by A​f​fK,Bs​mΞ©Aff_{K,B^{sm}}^{\Omega}. It is easy to see that this KK-affine structure does not change if we make a rescaling Ω↦c​Ω,c∈KΓ—\Omega\mapsto c\Omega,c\in K^{\times}.

7.3 Lifting Problem

Let KK be as in Section 7.2, BβŠƒBp​r​eβˆ’s​i​n​gB\supset B^{pre-sing} be a space with singular 𝐙{\bf Z}-affine structure (see Section 6.3), and an extension of 𝐙{\bf Z}-affine structure on Bβˆ–Bp​r​eβˆ’s​i​n​gB\setminus B^{pre-sing} to a KK-affine structure satisfying fixed point property (see 7.1). We assume that 𝐙{\bf Z}-affine structure cannot be extended to a larger open set UβŠƒBβˆ–Bp​r​eβˆ’s​i​n​g,Uβ‰ Bβˆ–Bp​r​eβˆ’s​i​n​gU\supset B\setminus B^{pre-sing},U\neq B\setminus B^{pre-sing}. Slightly abusing notation we will denote Bβˆ–Bp​r​eβˆ’s​i​n​gB\setminus B^{pre-sing} simply by Bs​mB^{sm}. We want to have a KK-analytic space XX, meromorphic non-zero top degree form Ξ©\Omega and a continuous proper (and maybe also Stein) map Ο€:Xβ†’B\pi:X\to B such that:

  1. 1.

    Bp​r​eβˆ’s​i​n​gB^{pre-sing} coincides with Bs​i​n​gB^{sing}, and 𝐙{\bf Z}-affine structure on Bs​mB^{sm} arising from the projection Ο€\pi coincides with the given one;

  2. 2.

    the restriction Ξ©|Ο€βˆ’1(Bs​m)\Omega_{|\pi^{-1}(B^{sm})} is a nowhere vanishing analytic form which satisfies the Constant Norm Assumption;

  3. 3.

    the KK-affine structure on Bs​mB^{sm} arising from the pair (X,Ξ©)(X,\Omega) coincides with the initial one.

We call the problem of finding such data Lifting Problem.

Remark 3

If a solution of the Lifting Problem exists then Bs​mB^{sm} is orientable. Indeed, R​e​s​(Ξ©)Res(\Omega) is locally a constant defined up to a sign which depends on the orientation of Bs​mB^{sm}. Global choice of the constant gives an orientation. For oriented Bs​mB^{sm} we can rescale Ξ©\Omega canonically in such a way that R​e​s​(Ξ©)=1Res(\Omega)=1

Question. What restrictions on the behavior of the KK-affine structure near Bp​r​eβˆ’s​i​n​g=Bs​i​n​gB^{pre-sing}=B^{sing} should we impose in order to guarantee the existence of a solution of the Lifting Problem?

Let B=Bs​mB=B^{sm} be a flat torus (see Section 3.2.1). Then the Lifting Problem has a solution (canonical up to rescaling of Ξ©\Omega) for any compatible KK-affine structure. More precisely, the groupoid of Tate tori and isomorphisms between them is equivalent to the groupoid of KK-affine structures on real flat tori.

In Sections 8-11 we are going to discuss a solution of the Lifting Problem for K3 surfaces. In that case Bs​i​n​gβ‰ βˆ…B^{sing}\neq\emptyset.

If we restrict ourselves only to the smooth part Bs​mB^{sm} (i.e. we allow non-compact XX) then there is a canonical solution of this β€œreduced” Lifting Problem. In other words one can construct a smooth KK-analytic space Xβ€²X^{\prime} with an analytic top degree form Ξ©β€²\Omega^{\prime} and a map Ο€β€²:Xβ€²β†’Bs​m\pi^{\prime}:X^{\prime}\to B^{sm} satisfying the above conditions 1–3. Let us explain this construction assuming that Bs​mB^{sm} is oriented.

First of all we notice that the orientation of Bs​mB^{sm} gives a reduction to S​L​(n,𝐙)⋉(KΓ—)nSL(n,{{\bf Z}})\ltimes(K^{\times})^{n} of the structure group of the torsor defining the KK-affine structure. The reduced group naturally acts by automorphisms of the fibration Ο€c​a​n:(𝐆ma​n)n→𝐑n\pi_{can}:({\bf G}_{m}^{an})^{n}\to{{\bf R}}^{n} preserving the form β‹€1≀i≀nd​zizi\bigwedge_{1\leq i\leq n}{dz_{i}\over z_{i}}. The action on (𝐆ma​n)n({\bf G}_{m}^{an})^{n} is induced from the action on monomials. Namely, the inverse to an element (A,Ξ»1,…,Ξ»n)∈S​L​(n,𝐙)⋉(KΓ—)n(A,\lambda_{1},...,\lambda_{n})\in SL(n,{{\bf Z}})\ltimes(K^{\times})^{n} acts on monomials as

zI=z1I1​…​znIn↦(∏i=1nΞ»iIi)​zA⁑(I).z^{I}=z_{1}^{I_{1}}\dots z_{n}^{I_{n}}\mapsto\left({\textstyle\prod_{i=1}^{n}}\lambda_{i}^{I_{i}}\right)\,\,z^{A(I)}\,\,\,.

The action of the same element on 𝐑n{{\bf R}}^{n} is given by the similar formula

x=(x1,…,xn)↦A⁑(x)βˆ’(v​a​l​(Ξ»1),…,v​a​l​(Ξ»n)).x=(x_{1},\dots,x_{n})\mapsto A(x)-(val(\lambda_{1}),\dots,val(\lambda_{n}))\,\,\,.

Let Bs​m=βˆͺΞ±UΞ±B^{sm}=\cup_{\alpha}U_{\alpha} be an open covering by coordinate charts Uα≃VΞ±βŠ‚π‘nU_{\alpha}\simeq V_{\alpha}\subset{{\bf R}}^{n} such that for any Ξ±,Ξ²\alpha,\beta we are given elements gΞ±,β∈S​L​(n,𝐙)⋉(KΓ—)ng_{\alpha,\beta}\in SL(n,{{\bf Z}})\ltimes(K^{\times})^{n} satisfying the 11-cocycle condition for any triple Ξ±,Ξ²,Ξ³\alpha,\beta,\gamma. Then the space Xβ€²X^{\prime} is obtained from Ο€c​a​nβˆ’1​(VΞ±)\pi_{can}^{-1}(V_{\alpha}) by gluing by means of the transformations gΞ±,Ξ²g_{\alpha,\beta}. The form β‹€1≀i≀nd​zizi\bigwedge_{1\leq i\leq n}{dz_{i}\over z_{i}} gives rise to a nowhere vanishing analytic top degree form Ξ©β€²\Omega^{\prime} on Xβ€²X^{\prime}. Thus we have obtained a solution of the reduced Lifting Problem. The sheaf Ο€βˆ—β€‹(π’ͺXβ€²):=π’ͺBs​mc​a​n\pi_{\ast}({\cal O}_{X^{\prime}}):={\cal O}_{B^{sm}}^{can} is called the canonical sheaf.

In the case Bp​r​eβˆ’s​i​n​gβ‰ βˆ…B^{pre-sing}\neq\emptyset this solution seems to be a β€œwrong” one, i.e. it cannot be extended to a solution Ο€:Xβ†’B\pi:X\to B, where XX and BB are compact. In the case of K3 surfaces we will show later how to modify it in order to obtain a β€œtrue” solution of the Lifting Problem.

7.4 Flat coordinates and periods

Here we are going to discuss a relation between KK-affine structures and so-called flat coordinates on the moduli space of complex structures on Calabi-Yau manifolds. We assume the picture of collapse from Section 5.1.

7.4.1 Flat coordinates for degenerating complex Calabi-Yau manifolds

Let Xm​e​r=(Xt)tβ†’0{X}_{mer}=(X_{t})_{t\to 0} be a maximally degenerating algebraic Calabi-Yau manifold of dimension nn over 𝐂tm​e​r{{\bf C}}_{t}^{mer}. We denote by BB the Gromov-Hausdorff limit of our family (see Conjecture 1, Section 5.1). Its connected oriented open dense part Bs​mB^{sm} carries a 𝐙{\bf Z}-affine structure with the covariant lattice T𝐙T^{{\bf Z}}.

Recall that according to the picture of collapse presented in Section 5.1 there is a canonical isotopy class of embeddings from a torus bundle p:Xtβ€²β†’Bs​mp:X_{t}^{\prime}\to B^{sm} to the complex manifold XtX_{t} for all sufficiently small tβ‰ 0t\neq 0. Let us denote by [Ξ³0]∈Hn​(Xtβ€²,𝐙)[\gamma_{0}]\in H_{n}(X_{t}^{\prime},{{\bf Z}}) the fundamental class of the fiber of pp. This is the homology class of a singular chain in Xtβ€²X_{t}^{\prime} which projects to a point by pp.

Let Hn≀1​(Xtβ€²,𝐙)βŠ‚Hn​(Xtβ€²,𝐙)H_{n}^{\leq 1}(X_{t}^{\prime},{{\bf Z}})\subset H_{n}(X_{t}^{\prime},{{\bf Z}}) be the subgroup generated by homology classes of chains which are projected into graphs in Bs​mB^{sm}. It follows from the definition that we have an epimorphism

Ja:H1​(Bs​m,β‹€nβˆ’1T𝐙)β† Hn≀1​(Xtβ€²,𝐙)/𝐙⁑[Ξ³0]J_{a}:H_{1}(B^{sm},{\textstyle\bigwedge^{n-1}}T^{{\bf Z}})\twoheadrightarrow H_{n}^{\leq 1}(X_{t}^{\prime},{{\bf Z}})/{{\bf Z}}[\gamma_{0}]

similar to the homomorphims JsJ_{s} defined in the symplectic case (see Section 3.1.1). The following formula defines a homomorphism of groups

P:Hn≀1​(Xtβ€²,𝐙)/𝐙⁑[Ξ³0]β†’(𝐂tm​e​r)Γ—,[Ξ³]↦exp⁑(2​π​iβ€‹βˆ«[Ξ³]Ξ©t∫[Ξ³0]Ξ©t).P:H_{n}^{\leq 1}(X_{t}^{\prime},{{\bf Z}})/{{\bf Z}}[\gamma_{0}]\to({{\bf C}}_{t}^{mer})^{\times},\,\,\,\,[\gamma]\mapsto\exp\left(2\pi i{\int_{[\gamma]}\Omega_{t}\over\int_{[\gamma_{0}]}\Omega_{t}}\right)\,\,.

We will call PP the period map. Notice that 𝐙⁑[Ξ³0]:=Hn≀0​(Xtβ€²,𝐙)βŠ‚Hn≀1​(Xtβ€²,𝐙){{\bf Z}}[\gamma_{0}]:=H_{n}^{\leq 0}(X_{t}^{\prime},{{\bf Z}})\subset H_{n}^{\leq 1}(X_{t}^{\prime},{{\bf Z}}) is a low degree part of the limiting Hodge filtration on the homology of Calabi-Yau manifold XtX_{t}. Non-zero complex numbers

exp⁑(2​π​iβ€‹βˆ«[Ξ³i]Ξ©t∫[Ξ³0]Ξ©t),\exp\left(2\pi i{\int_{[\gamma_{i}]}\Omega_{t}\over\int_{[\gamma_{0}]}\Omega_{t}}\right)\,\,,

where Ξ³i\gamma_{i} is a set of generators of Hn≀1​(Xtβ€²,𝐙)/Hn≀0​(Xtβ€²,𝐙)H_{n}^{\leq 1}(X_{t}^{\prime},{{\bf Z}})/H_{n}^{\leq 0}(X_{t}^{\prime},{{\bf Z}}) are called flat coordinates in Mirror Symmetry (see e.g. [Mor]). Those are local coordinates near a point close to the β€œcusp” of the moduli space of complex structures (local Torelli theorem).

The orientation of Bs​mB^{sm} gives rise to an isomorphism β‹€nβˆ’1T𝐙≃(Tβˆ—)𝐙\bigwedge^{n-1}T^{{\bf Z}}\simeq(T^{\ast})^{{\bf Z}}. Therefore, combining maps Ja,PJ_{a},P and the above isomorphism we obtain a homomorphism

P~:H1​(Bs​m,(Tβˆ—)𝐙)β†’(𝐂tm​e​r)Γ—.\widetilde{P}:H^{1}(B^{sm},(T^{\ast})^{{\bf Z}})\to\left({{\bf C}}_{t}^{mer}\right)^{\times}\,\,.
7.4.2 Non-archimedean periods

Let Xa​n{X}^{an} be a smooth analytic Calabi-Yau manifold associated with Xm​e​rX_{mer}. Assuming the equivalence of Gromov-Hausdorff and non-archimedean pictures of collapse presented in Section 5 we have a continuous map Ο€:Xa​nβ†’B\pi:{X}^{an}\to B. It gives a KK-affine structure on Bs​mB^{sm}. The corresponding exact sequence

0β†’KΓ—β†’A​f​fKβ†’(Tβˆ—)𝐙→00\to K^{\times}\to Aff_{K}\to(T^{\ast})^{{\bf Z}}\to 0

represents a class in H1​(Bs​m,Tπ™βŠ—KΓ—)≃E​x​t1​((Tβˆ—)𝐙,KΓ—)H^{1}(B^{sm},T^{{\bf Z}}\otimes K^{\times})\simeq Ext^{1}((T^{\ast})^{{\bf Z}},K^{\times}). Pairing with this class gives another homomorphism

Pβ€²:H1​(Bs​m,(Tβˆ—)𝐙)β†’KΓ—=H0​(Bs​m,KΓ—).P^{\prime}:H_{1}(B^{sm},(T^{\ast})^{{\bf Z}})\to K^{\times}=H_{0}(B^{sm},K^{\times})\,\,.
Conjecture 10

Homomorphism Pβ€²P^{\prime} is equal to the composition of P~\widetilde{P} with the embedding (𝐂tm​e​r)Γ—β†ͺKΓ—\left({{\bf C}}_{t}^{mer}\right)^{\times}\hookrightarrow K^{\times}.

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