9 Lines on surfaces [03W7]
Original official author HTML, exact retained edition. Historical TeX conversion verdicts remain unchanged. Cited-edition alignment and mathematical self-containment are not assessed.
Complete original source context · Original author HTML
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 , a finite subset .
- b)
-
A -affine structure on with the standard singularities near each .
- c)
-
A set of lines. With each line there is an associated continuous map . We assume that is decomposed into a disjoint union of two subsets . Lines belonging to are called initial, while those in are called composite. We assume that for any there exists a continuous extension such that if and if .
- d)
-
A collection of covariantly constant nowhere vanishing integer-valued -forms . We assume that for in the standard coordinates near singular point we have: or for all sufficiently small , and .
- e)
-
A map (the letter stands for “parent”: one can think about these lines as “generating in a collision”).
Notice that since the form is invariant with respect to the monodromy, the condition in d) is coordinate-independent. The covector will be called a direction covector of at time . It gives rise to a half-plane
9.2 Axioms
To every we assign a pair , where is a choice of sign in (see data d) in the previous subsection). In this way we obtain a map .
- Axiom 1.
-
Map is one-to-one.
Let be a simply-connected domain, and line intersects . Let be an interval such that . Then there exists a covariantly constant closed non-zero -form in (with constant integer coefficients), such that , when both sides are restricted to .
- Axiom 2.
-
For any one has
Let , satisfy the condition . In this case we say that lines and have a collision at at the times and respectively.
- Axiom 3.
-
Under the above assumptions there are only two possibilities:
3a) either and , or
3b) covector is not proportional to . Then we may assume that . Under these conditions we require that for any coprime positive integers there exists a unique line such that , and .
In other words, and are “parents of ”, and the direction covector of at the intersection point is a primitive integral linear combination of those for and (see Figure 4).

- Axiom 4.
-
For every line there exist and such that they satisfy the condition 3b).
- Axiom 5.
-
For any there are no more than two pairs such that . In other words, there are no more than two lines intersecting at a point in .
Let mean the same as in the Axiom 3, and assume that . Let us consider the set of germs of all starting at (i.e. such that ).
- Axiom 6.
-
For any finite subset there is an orientation preserving homeomorphism of a neighborhood of onto a neighborhood of such that:
6a) Germs of oriented curves which are images of and get transformed into the germs at of coordinate axes and respectively.
6b) Germ of the image of gets transformed into the germ of the ray where .
Figure 5 illustrates this axiom.

- Axiom 7.
-
Let denotes either or . Then for any there exists such that if the line is well-defined then it belongs to .
This axiom says that any composed line appears as a result of finitely many collisions. The tree of ancestors of a given line form a tree embedded in , see Figure 6.

9.3 Example: gradient lines
Here we offer a construction of the set of lines satisfying the above axioms.
Let us use the standard as a model around each in order to fix a structure of smooth manifold on the whole surface . Let denotes the covering of such that the fiber over is .
Let us fix a generic smooth metric on . By the pull-back it gives a metric on . Notice that there is a canonical closed -form on such that , where . Using the metric we obtain dual to gradient vector field on .
For any and a choice of 1-form in local coordinates, we take the unique integral line of starting at . Set will be the set of all lines obtained in this way. Each line carries a covariantly constant closed -form . Using Axiom 2 as a definition, we obtain a canonical parametrization of each line by the time parameter . Since the metric is generic, a line cannot return to a point in .
Then we proceed inductively. If two already constructed lines meet at we produce a new integral line of with the direction covector satisfying the condition 3b) for any pair of coprime positive integers . In this way we construct a set of lines satisfying all the axioms. The only non-trivial thing to check is that for each line values of the parameter are in one-to-one correspondence with the interval . In order to see this we observe that the length of each line is infinite. Indeed, an integral curve of cannot have a limiting point in (since the flow generated by is smooth, and the lengths of tangent vectors are bounded from below because of the integrality of -forms).
We conclude that there exists a set of lines satisfying Axioms 1-7.