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9 Lines on surfaces [03W7]

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9 Lines on surfaces

In this section we are going to describe axiomatically the notion of collection of lines on a surface.

9.1 Data

a)

A compact oriented surface BB, a finite subset Bs​i​n​g⊂BB^{sing}\subset B.

b)

A 𝐙{\bf Z}-affine structure on Y=Bs​m=B∖Bs​i​n​gY=B^{sm}=B\setminus B^{sing} with the standard singularities near each b∈Bs​i​n​gb\in B^{sing}.

c)

A set ℒ{\cal L} of lines. With each line l∈ℒl\in{\cal L} there is an associated continuous map fl:(0,+∞)→Yf_{l}:(0,+\infty)\to Y. We assume that ℒ{\cal L} is decomposed into a disjoint union of two subsets ℒ=ℒi​n⊔ℒc​o​m{\cal L}={\cal L}_{in}\sqcup{\cal L}_{com}. Lines belonging to ℒi​n{\cal L}_{in} are called initial, while those in ℒc​o​m{\cal L}_{com} are called composite. We assume that for any l∈ℒl\in{\cal L} there exists a continuous extension fl:[0,+∞)→Bf_{l}:[0,+\infty)\to B such that fl​(0)∈Bs​i​n​gf_{l}(0)\in B^{sing} if l∈ℒi​nl\in{\cal L}_{in} and fl​(0)∈Y=Bs​mf_{l}(0)\in Y=B^{sm} if l∈ℒc​o​ml\in{\cal L}_{com}.

d)

A collection of covariantly constant nowhere vanishing integer-valued 11-forms αl∈Γ⁡((0,+∞),fl∗​((T∗)𝐙),l∈ℒCLOSE\alpha_{l}\in\Gamma((0,+\infty),f_{l}^{\ast}((T^{\ast})^{\bf Z}),l\in{\cal L}. We assume that for l∈ℒi​nl\in{\cal L}_{in} in the standard coordinates (x,y)(x,y) near singular point fl​(0)f_{l}(0) we have: fl​(t)=(0,t)f_{l}(t)=(0,t) or fl​(t)=(0,−t)f_{l}(t)=(0,-t) for all sufficiently small t>0t>0, and αl​(t)=±fl∗​(d​y)\alpha_{l}(t)=\pm f_{l}^{\ast}(dy).

e)

A map ℒ→ℒ×ℒ,l↦(pl​e​f​t​(l),pr​i​g​h​t​(l)){\cal L}\to{\cal L}\times{\cal L},\,\,\,l\mapsto(p_{left}(l),p_{right}(l)) (the letter pp stands for “parent”: one can think about these lines as “generating ll in a collision”).

Notice that since the form d​ydy is invariant with respect to the monodromy, the condition in d) is coordinate-independent. The covector αl​(t)\alpha_{l}(t) will be called a direction covector of ll at time tt. It gives rise to a half-plane

Pl,t(0)={v∈Tfl​(t)​Y|⟨αl​(t),v⟩>0}.P_{l,t}^{(0)}=\{v\in T_{f_{l}(t)}Y|\langle\alpha_{l}(t),v\rangle>0\}\,\,.

9.2 Axioms

To every l∈ℒi​nl\in{\cal L}_{in} we assign a pair (fl​(0),s​g​n​(αl​(0)))∈Bs​i​n​g×{±1}\left(f_{l}(0),sgn\left(\alpha_{l}(0)\right)\right)\in B^{sing}\times\{\pm 1\}, where s​g​n​(αl​(0))sgn(\alpha_{l}(0)) is a choice of sign in ±fl∗​(d​y)\pm f_{l}^{\ast}(dy) (see data d) in the previous subsection). In this way we obtain a map r:ℒi​n→Bs​i​n​g×{±1}r:{\cal L}_{in}\to B^{sing}\times\{\pm 1\}.

Axiom 1.

Map rr is one-to-one.

Let U⊂YU\subset Y be a simply-connected domain, and line ll intersects UU. Let I⊂𝐑+I\subset{\bf R}_{+} be an interval such that fl​(I)⊂Uf_{l}(I)\subset U. Then there exists a covariantly constant closed non-zero 11-form βU\beta_{U} in UU (with constant integer coefficients), such that fl∗​(βU)=αlf_{l}^{\ast}(\beta_{U})=\alpha_{l}, when both sides are restricted to II.

Axiom 2.

For any t1,t2∈It_{1},t_{2}\in I one has

∫fl​(t1)fl​(t2)βU=t2−t1.\int_{f_{l}(t_{1})}^{f_{l}(t_{2})}\beta_{U}=t_{2}-t_{1}\,\,.

Let l1,l2∈ℒl_{1},l_{2}\in{\cal L}, t1,t2>0t_{1},t_{2}>0 satisfy the condition fl1​(t1)=fl2​(t2)=x∈Yf_{l_{1}}(t_{1})=f_{l_{2}}(t_{2})=x\in Y. In this case we say that lines l1l_{1} and l2l_{2} have a collision at xx at the times t1t_{1} and t2t_{2} respectively.

Axiom 3.

Under the above assumptions there are only two possibilities:

3a) either l1=l2l_{1}=l_{2} and t1=t2t_{1}=t_{2}, or

3b) covector αl1​(t1)\alpha_{l_{1}}(t_{1}) is not proportional to αl2​(t2)\alpha_{l_{2}}(t_{2}). Then we may assume that αl1​(t1)∧αl2​(t2)>0\alpha_{l_{1}}(t_{1})\wedge\alpha_{l_{2}}(t_{2})>0. Under these conditions we require that for any coprime positive integers n1,n2n_{1},n_{2} there exists a unique line l∈ℒl\in{\cal L} such that l1=pl​e​f​t​(l),l2=pr​i​g​h​t​(l)l_{1}=p_{left(l)},l_{2}=p_{right}(l), fl​(0)=xf_{l}(0)=x 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}).

In other words, l1l_{1} and l2l_{2} are “parents of ll”, and the direction covector of ll at the intersection point is a primitive integral linear combination of those for l1l_{1} and l2l_{2} (see Figure 4).

Refer to caption

Figure 4: Line ll and its two parents l1,l2l_{1},l_{2}. Dashed half-planes are domains in tangent planes where 11-forms α\alpha take positive values.
Axiom 4.

For every line l∈ℒc​o​ml\in{\cal L}_{com} there exist l1l_{1} and l2l_{2} such that they satisfy the condition 3b).

Axiom 5.

For any x∈Yx\in Y there are no more than two pairs (l,t)∈ℒ×(0,+∞)(l,t)\in{\cal L}\times(0,+\infty) such that x=fl​(t)x=f_{l}(t). In other words, there are no more than two lines intersecting at a point in YY.

Let l1,l2,t1,t2,xl_{1},l_{2},t_{1},t_{2},x mean the same as in the Axiom 3, and assume that αl1​(t1)∧αl2​(t2)>0\alpha_{l_{1}}(t_{1})\wedge\alpha_{l_{2}}(t_{2})>0. Let us consider the set ℒ(x){\cal L}_{(x)} of germs of all l∈ℒc​o​ml\in{\cal L}_{com} starting at xx (i.e. such that fl​(0)=xf_{l}(0)=x).

Axiom 6.

For any finite subset ℒ′⊂ℒ(x){\cal L}^{\prime}\subset{\cal L}_{(x)} there is an orientation preserving homeomorphism of a neighborhood of xx onto a neighborhood of (0,0)∈𝐑2(0,0)\in{\bf R}^{2} such that:

6a) Germs of oriented curves which are images of l1l_{1} and l2l_{2} get transformed into the germs at (0,0)(0,0) of coordinate axes (x,0)(x,0) and (0,y)(0,y) respectively.

6b) Germ of the image of l∈ℒ′l\in{\cal L}^{\prime} gets transformed into the germ of the ray {(n1​t,n2​t)|t>0}\{(n_{1}t,n_{2}t)\,|\,t>0\} where 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}).

Figure 5 illustrates this axiom.

Refer to caption

Figure 5: Two intersecting lines and some of new lines obtained as a result of collision. All lines are straightened by a homeomorphism of 𝐑2{\bf R}^{2}.
Axiom 7.

Let pip_{i} denotes either pl​e​f​tp_{left} or pr​i​g​h​tp_{right}. Then for any l∈ℒl\in{\cal L} there exists N≥1N\geq 1 such that if the line p1​(p2​(…​pN​(l)​…)CLOSEp_{1}(p_{2}(\dots p_{N}(l)\dots) is well-defined then it belongs to ℒi​n{\cal L}_{in}.

This axiom says that any composed line l∈ℒc​o​ml\in{\cal L}_{com} appears as a result of finitely many collisions. The tree of ancestors of a given line form a tree embedded in BB, see Figure 6.

Refer to caption

Figure 6: Tree of ancestors of line ll starting from 33 singular points s1,s2,s3∈Bs​i​n​gs_{1},s_{2},s_{3}\in B^{sing}.

9.3 Example: gradient lines

Here we offer a construction of the set of lines satisfying the above axioms.

Let us use the standard 𝐑2{\bf R}^{2} as a model around each b∈Bs​i​n​gb\in B^{sing} in order to fix a structure of smooth manifold on the whole surface BB. Let Y~\widetilde{Y} denotes the covering of YY such that the fiber over y∈Yy\in Y is (Ty∗​Y)𝐙∖{0}(T_{y}^{\ast}Y)^{{\bf Z}}\setminus\{0\}.

Let us fix a generic smooth metric on BB. By the pull-back it gives a metric on Y~\widetilde{Y}. Notice that there is a canonical closed 11-form β\beta on Y~\widetilde{Y} such that β|(y,μ)=μ\beta_{|(y,\mu)}=\mu, where y∈Y,μ∈(Ty∗​Y)𝐙y\in Y,\,\,\mu\in(T_{y}^{\ast}Y)^{{\bf Z}}. Using the metric we obtain dual to β\beta gradient vector field vv on Y~\widetilde{Y}.

For any s∈Bs​i​n​gs\in B^{sing} and a choice of 1-form α⁡(0)=±d​y\alpha(0)=\pm dy in local coordinates, we take the unique integral line of vv starting at (s,α⁡(0))(s,\alpha(0)). Set ℒi​n{\cal L}_{in} will be the set of all lines obtained in this way. Each line l∈ℒi​nl\in{\cal L}_{in} carries a covariantly constant closed 11-form αl\alpha_{l}. Using Axiom 2 as a definition, we obtain a canonical parametrization of each line by the time parameter tt. Since the metric is generic, a line cannot return to a point in Bs​i​n​gB^{sing}.

Then we proceed inductively. If two already constructed lines l1,l2∈ℒl_{1},l_{2}\in{\cal L} meet at x∈Yx\in Y we produce a new integral line ll of vv with the direction covector satisfying the condition 3b) for any pair of coprime positive integers n1,n2n_{1},n_{2}. In this way we construct a set of lines ℒ{\cal L} satisfying all the axioms. The only non-trivial thing to check is that for each line values of the parameter tt are in one-to-one correspondence with the interval (0,+∞)(0,+\infty). In order to see this we observe that the length of each line is infinite. Indeed, an integral curve of vv cannot have a limiting point in YY (since the flow generated by vv is smooth, and the lengths of tangent vectors are bounded from below because of the integrality of 11-forms).

We conclude that there exists a set ℒ{\cal L} of lines satisfying Axioms 1-7.

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