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10 Groups and symplectomorphisms [03WB]

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10 Groups and symplectomorphisms

In this section we are going to discuss the sheaf of groups of symplectomorphisms S​y​m​p:=S​y​m​p​(𝒪Yc​a​n)Symp:=Symp({\cal O}_{Y}^{can}) of the sheaf 𝒪Yc​a​n{\cal O}_{Y}^{can}. Let U⊂YU\subset Y be an open convex subset. By definition, a symplectomorphism of 𝒪Yc​a​n​(U){\cal O}_{Y}^{can}(U) is an automorphism of KK-algebra 𝒪Yc​a​n​(U){\cal O}_{Y}^{can}(U) preserving projection to YY and the canonical symplectic form Ω=d​ξ∧d​ηξ​η\Omega={d\xi\wedge d\eta\over{\xi\eta}} (the latter is understood as an element of the algebra of Kähler differential forms). To each line ll we will assign a symplectomorphism of the restriction of 𝒪Yc​a​n{\cal O}_{Y}^{can} to ll, so that the assignment will be compatible with the collision of lines. Then we are going to modify the sheaf 𝒪Yc​a​n{\cal O}_{Y}^{can} using symplectomorphisms, associated with lines and obtain the sheaf 𝒪Ym​o​d​i​f{\cal O}_{Y}^{modif}. This sheaf will be glued with the sheaf 𝒪𝐑2m​o​d​e​l{\cal O}^{model}_{{\bf R}^{2}} near each point of Bs​i​n​gB^{sing}.

10.1 Pro-nilpotent Lie algebra

Here it will be convenient to work in local coordinates (x,y)=(log⁡|ξ|,log⁡|η|)(x,y)=(\log|\xi|,\log|\eta|) on YY.

Let (x0,y0)∈𝐑2(x_{0},y_{0})\in{\bf R}^{2} be a point, α1,α2∈(𝐙2)∗\alpha_{1},\alpha_{2}\in({\bf Z}^{2})^{\ast} be 11-covectors such that α1∧α2>0\alpha_{1}\wedge\alpha_{2}>0. Denote by V=V(x0,y0),α1,α2V=V_{(x_{0},y_{0}),\alpha_{1},\alpha_{2}} the closed angle

{(x,y)∈𝐑2|⟨αi,(x,y)−(x0,y0)⟩≥0,i=1,2}.\{(x,y)\in{\bf R}^{2}|\langle\alpha_{i},(x,y)-(x_{0},y_{0})\rangle\geq 0,i=1,2\,\}\,\,.

Let 𝒪⁡(V){\cal O}(V) be a KK-algebra consisting of series f=∑n,m∈𝐙cn,m​ξn​ηmf=\sum_{n,m\in{\bf Z}}c_{n,m}\xi^{n}\eta^{m}, such that cn,m∈Kc_{n,m}\in K and for all (x,y)∈V(x,y)\in V we have:

  1. 1.

    if cn,m≠0c_{n,m}\neq 0 then ⟨(n,m),(x,y)−(x0,y0)⟩≤0\langle(n,m),(x,y)-(x_{0},y_{0})\rangle\leq 0, where we identified (n,m)∈𝐙2(n,m)\in{\bf Z}^{2} with a covector in (Tp∗​Y)𝐙(T_{p}^{\ast}Y)^{{\bf Z}};

  2. 2.

    log⁡|cn,m|+n​x+m​y→−∞\log|c_{n,m}|+nx+my\to-\infty as long as |n|+|m|→+∞|n|+|m|\to+\infty.

Algebra 𝒪⁡(V){\cal O}(V) is a Poisson algebra with respect to the bracket {ξ,η}=ξ​η\{\xi,\eta\}=\xi\eta.

For an integer covector μ=a​d​x+b​d​y∈(𝐙2)∗\mu=adx+bdy\in({\bf Z}^{2})^{*} we denote by RμR_{\mu} the monomial ξa​ηb\xi^{a}\eta^{b}.

Let us consider a pro-nilpotent Lie algebra 𝐠:=𝐠α1,α2,V⊂𝒪⁡(V){\bf g}:={\bf g}_{\alpha_{1},\alpha_{2},V}\subset{\cal O}(V) consisting of series

f=∑n1,n2≥0,n1+n2>0cn1,n2​Rα1−n1​Rα2−n2f=\sum_{n_{1},n_{2}\geq 0,n_{1}+n_{2}>0}c_{n_{1},n_{2}}R_{\alpha_{1}}^{-n_{1}}R_{\alpha_{2}}^{-n_{2}}

satisfying the condition

log⁡|cn,m|−n1​⟨α1,(x,y)⟩−n2​⟨α2,(x,y)⟩≤0​∀(x,y)∈V.\log|c_{n,m}|-n_{1}\langle\alpha_{1},(x,y)\rangle-n_{2}\langle\alpha_{2},(x,y)\rangle\leq 0\,\,\,\,\forall\,(x,y)\in V\,\,.

The latter condition is equivalent to log⁡|cn,m|−⟨n1​α1+n2​α2,(x0,y0)⟩≤0\log|c_{n,m}|-\langle n_{1}\alpha_{1}+n_{2}\alpha_{2},(x_{0},y_{0})\rangle\leq 0.

Lie algebra 𝐠{\bf g} admits a filtration by Lie subalgebras 𝐠≥k,k∈𝐙,k≥1{\bf g}^{\geq k},k\in{\bf Z},k\geq 1, 𝐠=𝐠≥1{\bf g}={\bf g}^{\geq 1}, such that 𝐠≥k{\bf g}^{\geq k} consists of the above series which satisfy the condition n1+n2≥kn_{1}+n_{2}\geq k. Clearly [𝐠≥k1,𝐠≥k2]⊂𝐠≥k1+k2[{\bf g}^{\geq k_{1}},{\bf g}^{\geq k_{2}}]\subset{\bf g}^{\geq k_{1}+k_{2}}, and 𝐠=lim←k→+∞⁡𝐠/𝐠≥k{\bf g}=\varprojlim_{k\to+\infty}{\bf g}/{\bf g}^{\geq k}.

Thus, 𝐠{\bf g} is a topological complete pro-nilpotent Lie algebra over KK. We denote by GG the corresponding pro-nilpotent Lie group exp⁡(𝐠)\exp({\bf g}). It inherits the filtration by normal subgroups G≥kG^{\geq k} obtained from the corresponding Lie algebras.

10.2 Lie groups GλG_{\lambda}

For each λ∈[0,+∞]𝐐:=𝐐≥0∪∞\lambda\in[0,+\infty]_{{\bf Q}}:={\bf Q}_{\geq 0}\cup\infty we define a Lie subalgebra

𝐠λ={∑n1,n2cm,nRα1−n1Rα2−n2∈𝐠|cn1,n2∈K,n2n1=λ}.{\bf g}_{\lambda}=\left\{\sum_{n_{1},n_{2}}c_{m,n}R_{\alpha_{1}}^{-n_{1}}R_{\alpha_{2}}^{-n_{2}}\in{\bf g}\,|\,\,c_{n_{1},n_{2}}\in K,\,\,{n_{2}\over{n_{1}}}=\lambda\,\right\}\,\,.

Each 𝐠λ{\bf g}_{\lambda} is an abelian Lie algebra. It carries the induced filtration by Lie algebras 𝐠λ≥k=𝐠λ∩𝐠≥k{\bf g}_{\lambda}^{\geq k}={\bf g}_{\lambda}\cap{\bf g}^{\geq k}. Denote by Gλ=exp⁡(𝐠λ)G_{\lambda}=\exp({\bf g}_{\lambda}) the corresponding pro-nilpotent group.

Lemma 4

For any given k≥1k\geq 1 there exist finitely many λ1<λ2<⋯<λNk\lambda_{1}<\lambda_{2}<\dots<\lambda_{N_{k}} such that 𝐠λ/𝐠λ≥k=0{\bf g}_{\lambda}/{\bf g}^{\geq k}_{\lambda}=0 for λ≠λi,1≤i≤Nk\lambda\neq\lambda_{i},1\leq i\leq N_{k}.

Proof. Indeed, for the monomial Rα1−n1​Rα2−n2∈𝐠λR_{\alpha_{1}}^{-n_{1}}R_{\alpha_{2}}^{-n_{2}}\in{\bf g}_{\lambda} which maps non-trivially to the quotient 𝐠λ/𝐠λ≥k{\bf g}_{\lambda}/{\bf g}^{\geq k}_{\lambda} we have: n1+n2≤k,n1/n2=λn_{1}+n_{2}\leq k,n_{1}/n_{2}=\lambda, where n1,n2n_{1},n_{2} are non-negative integers. There are finitely many such non-negative integers n1n_{1} and n2n_{2}. ■\blacksquare

It follows from the Lemma that we have a natural isomorphism of vector spaces ∏λ∈[0,+∞]𝐐𝐠λ/𝐠λ≥k→𝐠/𝐠≥k\prod_{\lambda\in[0,+\infty]_{{\bf Q}}}{\bf g}_{\lambda}/{\bf g}_{\lambda}^{\geq k}\to{\bf g}/{\bf g}^{\geq k}, hence the map

(fλ)λ∈[0,+∞]𝐐↦∑λfλ=∑i=1Nifλi, where fλ∈𝐠λ/𝐠λ≥k∀λ∈[0,+∞]𝐐(f_{\lambda})_{\lambda\in[0,+\infty]_{{\bf Q}}}\mapsto\sum_{\lambda}f_{\lambda}=\sum_{i=1}^{N_{i}}f_{\lambda_{i}},\,\,\,\,\mbox{ where }f_{\lambda}\in{\bf g}_{\lambda}/{\bf g}_{\lambda}^{\geq k}\,\,\,\forall\lambda\in[0,+\infty]_{{\bf Q}}

is well-defined and gives rise (after taking the projective limit as k→+∞k\to+\infty) to the isomorphism 𝐠≃∏λ∈[0,+∞]𝐐𝐠λ{\bf g}\simeq\prod_{\lambda\in[0,+\infty]_{{\bf Q}}}{\bf g}_{\lambda}.

In a similar way we define the map ∏→:∏λ∈[0,+∞]𝐐Gλ→G\prod_{\to}:\prod_{\lambda\in[0,+\infty]_{{\bf Q}}}G_{\lambda}\to G, the product is taken with respect to the natural order on 𝐐{\bf Q}. Namely, for any k≥1k\geq 1 we define

∏→(k):∏i=1NkGλi/Gλi≥k→G/G≥k,(g1,…,gNk)↦g1​…​gNk, for ​gi∈Gλi/Gλi≥k{\textstyle\prod_{\to}^{(k)}}:\prod_{i=1}^{N_{k}}G_{\lambda_{i}}/G_{\lambda_{i}}^{\geq k}\to G/G^{\geq k}\,,\,(g_{1},\dots,g_{N_{k}})\mapsto g_{1}\dots g_{N_{k}},\,\mbox{ for }g_{i}\in G_{\lambda_{i}}/G_{\lambda_{i}}^{\geq k}

and then set ∏→:=lim←k∏→(k)\prod_{\to}:=\varprojlim_{k}\prod_{\to}^{(k)}\,.

Theorem 6

Map ∏→\prod_{\to} is a bijection of sets.

Proof. Let k≥1k\geq 1 be an integer. We claim that ∏→(k)\prod_{\to}^{(k)} is a bijection of sets (this implies the proposition by taking the projective limit as k→+∞k\to+\infty). We will prove the bijection by induction in kk . Case k=1k=1 is obvious because all the groups under considerations are trivial.

We would like to prove that ∏→(k+1)\prod_{\to}^{(k+1)} is a bijection assuming that ∏→(k)\prod_{\to}^{(k)} is a bijection. Let hh be an element of G/G≥k+1G/G^{\geq k+1} and h¯\overline{h} its image in G/G≥kG/G^{\geq k}. By the induction assumption there exist unique h¯i∈Gλi/Gλi≥k+1,1≤i≤Nk+1\overline{h}_{i}\in G_{\lambda_{i}}/G_{\lambda_{i}}^{\geq k+1},1\leq i\leq N_{k+1} such that h¯1​…​h¯Nk+1=h¯\overline{h}_{1}\dots\overline{h}_{N_{k+1}}=\overline{h}. Let hi,1≤i≤Nk+1h_{i},1\leq i\leq N_{k+1} be any liftings of h¯i\overline{h}_{i} to Gi/Gi≥kG_{i}/G_{i}^{\geq k}. Then h1​…​hNk+1=h(modG≥k)h_{1}\dots h_{N_{k+1}}=h\pmod{G^{\geq k}}, hence c:=h1​…​hNk+1​h−1c:=h_{1}\dots h_{N_{k+1}}h^{-1} belongs to G≥k/G≥k+1⊂C​e​n​t​e​r​(G/G≥k+1)G^{\geq k}/G^{\geq k+1}\subset Center(G/G^{\geq k+1}). The last inclusion holds because [𝐠,𝐠≥k]=[𝐠≥1,𝐠≥k]⊂𝐠≥k+1[{\bf g},{\bf g}^{\geq k}]=[{\bf g}^{\geq 1},{\bf g}^{\geq k}]\subset{\bf g}^{\geq k+1}.

Next we observe that the isomorphism of abelian Lie algebras

⨁1≤i≤Nk+1𝐠λi≥k/𝐠λi≥k+1≃𝐠≥k/𝐠≥k+1\bigoplus_{1\leq i\leq{N_{k+1}}}{\bf g}_{\lambda_{i}}^{\geq k}/{\bf g}_{\lambda_{i}}^{\geq k+1}\simeq{\bf g}^{\geq k}/{\bf g}^{\geq k+1}

implies an isomorphism of the corresponding abelian groups

∏1≤i≤Nk+1Gi≥k/Gi≥k+1≃G≥k/G≥k+1.\prod_{1\leq i\leq{N_{k+1}}}G_{i}^{\geq k}/G_{i}^{\geq k+1}\simeq G^{\geq k}/G^{\geq k+1}\,\,.

Hence we can write uniquely c=c1​…​cNk+1c=c_{1}\dots c_{N_{k+1}}, where ci∈G≥k/G≥k+1⊂C​e​n​t​e​r​(G/G≥k+1)c_{i}\in G^{\geq k}/G^{\geq k+1}\subset Center(G/G^{\geq k+1}). It follows that ∏→(k+1)((hi​ci−1))=h\prod_{\to}^{(k+1)}\left((h_{i}c_{i}^{-1})\right)=h. Also it is now clear that this decomposition of hh is unique. This concludes the proof. ■\blacksquare

10.3 Function o​r​dlord_{l}

For l∈ℒl\in{\cal L} we will define an order function

o​r​dl∈Γ⁡((0,+∞),fl∗​(A​f​f𝐙,Y))ord_{l}\in\Gamma((0,+\infty),f_{l}^{\ast}(Aff_{{\bf Z},Y}))

(its meaning will become clear later) by the following inductive procedure:

  1. 1.

    Let l∈ℒi​nl\in{\cal L}_{in} and t>0t>0 be sufficiently small. Then in the standard affine coordinates near s=fl​(0)s=f_{l}(0) one has αl=±fl∗​(d​y)\alpha_{l}=\pm f_{l}^{\ast}(dy). We define o​r​dl=±fl∗​(y)ord_{l}=\pm f_{l}^{\ast}(y). Then d⁡(o​r​dl)=αld(ord_{l})=\alpha_{l}, and we can extend uniquely o​r​dlord_{l} for all t∈(0,+∞)t\in(0,+\infty).

  2. 2.

    Let l∈ℒc​o​ml\in{\cal L}_{com} and l1,l2l_{1},l_{2} be parents of ll. In the notation of Axiom 3 we have fl1​(t1)=fl2​(t2)=fl​(0)f_{l_{1}}(t_{1})=f_{l_{2}}(t_{2})=f_{l}(0) and αl​(0)=n1​αl1​(t1)+n2​αl2​(t2)\alpha_{l}(0)=n_{1}\alpha_{l_{1}}(t_{1})+n_{2}\alpha_{l_{2}}(t_{2}). Then we define o​r​dl​(0):=n1​o​r​dl1​(t1)+n2​o​r​dl2​(t2)ord_{l}(0):=n_{1}ord_{l_{1}}(t_{1})+n_{2}ord_{l_{2}}(t_{2}). Again, using the condition d⁡(o​r​dl)=αld(ord_{l})=\alpha_{l} and the knowledge of o​r​dl​(0)ord_{l}(0) we can extend o​r​dlord_{l} for t>0t>0.

Notice that o​r​dl​(t)ord_{l}(t) can be thought of as affine function on the tangent space Tfl​(t)​YT_{f_{l}(t)}Y (in the induced integral affine structure). In particular, we have a half-plane Pl,t⊂Tfl​(t)​YP_{l,t}\subset T_{f_{l}(t)}Y defined by the inequality o​r​dl​(t)>0ord_{l}(t)>0. The family of half-planes Pl,tP_{l,t} is covariantly constant with respect to ∇a​f​f\nabla^{aff}.

Each half-plane Pl,tP_{l,t} contains 0∈Tfl​(t)​Y0\in T_{f_{l}(t)}Y strictly in its interior. Recall that at the end of Section 9.1 we defined another half-plane Pl,t(0)⊂Tfl​(t)​YP_{l,t}^{(0)}\subset T_{f_{l}(t)}Y. It is easy to see that Pl,t(0)P_{l,t}^{(0)} is the half-plane parallel to Pl,tP_{l,t} such that 0∈Tfl​(t)​Y0\in T_{f_{l}(t)}Y is on the boundary of Pl,t(0)P_{l,t}^{(0)}.

10.4 Symplectomorphisms assigned to lines

In this section we are going to assign to each line l∈ℒl\in{\cal L} a symplectomorphism

φl∈Γ⁡((0,+∞),fl∗​(S​y​m​p))\varphi_{l}\in\Gamma\left((0,+\infty),f_{l}^{*}\left(Symp\right)\right)

giving for each t>0t>0 a transformation φl​(t):𝒪Y,fl​(t)c​a​n→𝒪Y,fl​(t)c​a​n\varphi_{l}(t):{\cal O}^{can}_{Y,f_{l}(t)}\to{\cal O}^{can}_{Y,f_{l}(t)}. This symplectomorphism in local coordinates will belong to the subgroup GλG_{\lambda} where λ\lambda is the slope of αl​(t)\alpha_{l}(t). More precisely, we demand that φl​(t)\varphi_{l}(t) is of the form

φl​(t)=exp⁡{Fl,t​(ξ−a​η−b),⋅},\varphi_{l}(t)=\exp\{F_{l,t}(\xi^{-a}\eta^{-b}),\cdot\}\,\,,

where αl​(t)=a​d​x+b​d​y\alpha_{l}(t)=adx+bdy, operation {⋅,⋅}\{\cdot,\cdot\} is the Poisson bracket on 𝒪Y,fl​(t)c​a​n{\cal O}^{can}_{Y,f_{l}(t)} and Fl,t​(z)∈z​K​[[z]]F_{l,t}(z)\in zK[[z]] is an analytic function of one variable satisfying the following condition. Let us consider the pullback (by the exponential map) of the function Fl,t​(ξ−a​η−b)F_{l,t}(\xi^{-a}\eta^{-b}) to a section of the sheaf 𝒪c​a​n{\cal O}^{can} on vector space Tfl​(t)​Y≃𝐑2T_{f_{l}(t)}Y\simeq{\bf R}^{2} considered as a manifold with 𝐙{\bf Z}-affine structure. Then this pullback should admit an analytic continuation from 0∈Tfl​(t)0\in T_{f_{l}(t)} to the half-plane Pl,tP_{l,t}, and obey there the bound

|Fl,t​(ξ−a​η−b)|≤exp⁡(−o​r​dl​(t)).|F_{l,t}(\xi^{-a}\eta^{-b})|\leq\exp(-ord_{l}(t))\,\,.

Let us explain the construction of φl​(t)\varphi_{l}(t), leaving the justification for the next sections.

Symplectomorphisms φl\varphi_{l} are constructed by an inductive procedure. Let l=l+∈ℒi​nl=l_{+}\in{\cal L}_{in} be (in standard affine coordinates) a line in the half-plane y>0y>0 emerging from (0,0)(0,0) (there is another such line l−l_{-} in the half-plane y<0y<0). Assume that tt is sufficiently small. Then we define φl​(t)∈S​y​m​pfl​(t)\varphi_{l}(t)\in Symp_{f_{l}(t)} on topological generators ξ,η\xi,\eta by the formula (as in Section 8)

φl​(t)​(ξ,η)=(ξ⁡(1+1/η),η).\varphi_{l}(t)(\xi,\eta)=(\xi(1+1/\eta),\eta)\,\,.

Notice that φl​(t)=exp⁡{F⁡(η−1),⋅}\varphi_{l}(t)=\exp\{F(\eta^{-1}),\cdot\}, where F⁡(z)=∑n>0(−1)n​zn/n2F(z)=\sum_{n>0}(-1)^{n}z^{n}/n^{2} is convergent for |z|<1|z|<1.

In order to extend φl​(t)\varphi_{l}(t) to the interval (0,t0)(0,t_{0}), where t0t_{0} is not small, we cover the corresponding segment of ll by open charts. Notice that change of affine coordinates transforms η\eta into a monomial multiplied by a constant from K×K^{\times}. Therefore η\eta extends analytically in a unique way to a global section over (0,+∞)(0,+\infty) of the sheaf fl∗​((𝒪c​a​n)×)f_{l}^{\ast}(({\cal O}^{can})^{\times}). Moreover, the norm |η||\eta| strictly decreases as tt increases, and remains strictly smaller than 11. Hence F⁡(η)F(\eta) can be canonically extended for all t>0t>0.

Each symplectomorphism φl​(t)\varphi_{l}(t) is defined by a series which converges in the half-plane Pl,tP_{l,t}. Using the exponential map associated with the affine structure as well as estimates of o​r​dl​(t)ord_{l}(t), we can extend analytically φl​(t)\varphi_{l}(t) into a neighborhood of fl​(t)f_{l}(t).

Let us now assume that l1l_{1} and l2l_{2} collide at p=fl1​(t1)=fl2​(t2)p=f_{l_{1}}(t_{1})=f_{l_{2}}(t_{2}), generating the line l∈ℒc​o​ml\in{\cal L}_{com}. Then φl​(0)\varphi_{l}(0) is defined with the help of factorization theorem in the group GG. More precisely, we set αi:=αli(ti),i=1,2\alpha_{i}:=\alpha_{l_{i}}(t_{i}),\,\,i=1,2 and the angle VV to be the intersection of half-planes Pl1,t1∩Pl2,t2P_{l_{1},t_{1}}\cap P_{l_{2},t_{2}}. By construction elements g0:=φl1​(t1)g_{0}:=\varphi_{l_{1}}(t_{1}) and g+∞:=φl2​(t2)g_{+\infty}:=\varphi_{l_{2}}(t_{2}) belong respectively to G0G_{0} and G+∞G_{+\infty}. Then we can use the factorization Theorem 6 and write down the formula

g+∞​g0=∏→((gλ)λ∈[0,+∞]𝐐)=g0​…​g1/2​…​g1​…​g+∞,g_{+\infty}g_{0}={\textstyle\prod_{\to}}\left((g_{\lambda})_{\lambda\in[0,+\infty]_{\bf Q}}\right)=g_{0}\dots g_{1/2}\dots g_{1}\dots g_{+\infty}\,\,,

where gλ∈Gλg_{\lambda}\in G_{\lambda} and the product on the right is in the increasing order. There is no clash of notations because it is easy to see that the boundary factors in the decomposition from above are indeed equal to g0g_{0} and g+∞g_{+\infty}. Each term gλg_{\lambda} with 0<λ=n1/n2<+∞0<\lambda=n_{1}/n_{2}<+\infty corresponds to the newborn line ll with the direction covector n1​αl1​(t1)+n2​αl2​(t2)n_{1}\alpha_{l_{1}}(t_{1})+n_{2}\alpha_{l_{2}}(t_{2}). Then we set φl​(0):=gλ\varphi_{l}(0):=g_{\lambda}. This transformation is defined by a series which is convergent in a neighborhood of pp, and using the analytic continuation as above, we obtain φl​(t)\varphi_{l}(t) for t>0t>0. The decomposition identity can be rewritten as

g0​…​g1/2​…​g1​…​g+∞​g0−1​g+∞−1=i​dg_{0}\dots g_{1/2}\dots g_{1}\dots g_{+\infty}g_{0}^{-1}g_{+\infty}^{-1}=id

where each factor corresponds to half-lines at the collision point (see Figure 5), and the meaning of the identity is that the infinite composition of symplectomorphisms in the natural cyclic order on half-lines, is trivial.

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