In
mathematics, each closed
surface in the sense of
geometric topology can be constructed from an even-sided oriented
polygon, called a 'fundamental polygon', by pairwise identification of its edges.

Fundamental parallelogram defined by a pair of vectors, generates the torus.
This construction can be represented as a string of length 2''n'' of ''n'' distinct symbols where each symbol appears
twice with exponent either +1 or -1. The exponent -1
signifies that the corresponding edge has the orientation opposing the one of the fundamental polygon.
Examples
★
sphere:
or
★
real projective plane:
or
★
Klein bottle:
or
★
torus:
or
Group generators
For the set of standard, symmetrical shapes, the edges of the polygon may be understood to the
generators of a
group. Then, the polygon, written in terms of group elements, becomes a constraint on the
free group generated by the edges, giving a
group presentation with one constraint.
Thus, for example, given the Euclidean plane
, let the group element
act on the plane as
while
. Then
generate the
lattice , and the torus is given by the
quotient space (a
homogeneous space)
. More generally, the two generators
can be taken to generate a parallelogram tiling, of
fundamental parallelograms.
For the torus, the constraint on the free group in two letters is given by
. This constraint is trivially embodied in the action on the plane given above. Alternately, the plane can be tiled by
hexagons, and the centers of the hexagons form a hexagonal lattice. Identifying opposite edges of the hexagon again leads to the torus, this time, with the constraint
describing the action of the
hexagonal lattice generators on the plane.
In practice, most of the interesting cases are surfaces with negative curvature, and are thus realized by a discrete lattice
in the group
acting on the
upper half-plane. Such lattices are known as
Fuchsian groups.
Standard fundamental polygons
An orientable closed surface of
genus ''n'' has the following standard fundamental polygon:
:
A non-orientable closed surface of (non-orientable) genus ''n'' has the following standard fundamental polygon:
:
Alternately, the non-orientable surfaces can be given on one of two forms, the genus ''n''
Klein bottle, and the genus ''n''
real projective plane. The genus 2''n'' Klein bottle is given by the 4''n''-sided polygon
:
(note the final
is missing the superscript -1; this flip, as compared to the orientable case, being the source of the non-orientability). The genus 2''n''+1 projective plane is given by the 4''n''+2-sided polygon
:
That these two cases exhaust all the possibilities for a non-orientable surface was shown by
Henri Poincaré.
Fundamental polygon of a compact Riemann surface
The fundamental polygon of a (hyperbolic)
compact Riemann surface has a number of important properties that relate the surface to its
Fuchsian model. That is, a hyperbolic compact Riemann surface has the
upper half-plane as the
universal cover, and can be represented as a quotient
manifold 'H'/Γ where Γ is a
non-Abelian group isomorphic to the
deck transformation group of the surface. The cosets of the quotient space have the standard fundamental polygon as a representative element. In the following, note that all Riemann surfaces are orientable.
Metric fundamental polygon
Given a point
in the
upper half-plane 'H', and a discrete
subgroup Γ of PSL(2,'R') that acts
freely discontinuously on the upper half-plane, then one can define the 'metric fundamental polygon' as the set of points
:
Here, ''d'' is a hyperbolic
metric on the upper half-plane. The metric fundamental polygon is also sometimes called the 'Dirichlet region' or the '
Voronoi polygon'.
★ This fundamental polygon is a
fundamental domain.
★ This fundamental polygon is
convex in that the
geodesic joining any two points of the polygon is contained entirely inside the polygon.
★ The
diameter of ''F'' is less than or equal to the diameter of 'H'/Γ. In particular, the closure of ''F'' is compact.
★ If Γ has no fixed points in 'H' and 'H'/Γ is compact, then ''F'' will have finitely many sides.
★ Each side of the polygon is a
geodesic arc.
★ For every side ''s'' of the polygon, there is precisely one other side ''s' '' such that ''gs=s' '' for some ''g'' in Γ. Thus, this polygon will have an even number of sides.
★ The set of group elements ''g'' that join sides to each other are
generators of Γ, and there is no smaller set that will generate Γ.
★ The upper half-plane is tiled by the closure of ''F'' under the action of Γ. That is,
where
is the closure of ''F''.
Standard fundamental polygon
Given any metric fundamental polygon ''F'', one can construct, with a finite number of steps, another fundamental polygon, the 'standard fundamental polygon', which has an additional set of noteworthy properties:
★ The vertices of the standard polygon are all equivalent. By ''vertex'' is meant the point where two sides meet. By ''equivalent'', it is meant that each vertex can be carried to any of the other vertices by some ''g'' in Γ.
★ The number of sides is divisible by four.
★ A given element ''g'' of Γ will carry at most one side of the polygon to another. Thus, the sides can be marked off in pairs. Since the action of Γ is orientation-preserving, if one side is called
, then the other of the pair can be marked with the opposite orientation
.
★ The edges of the standard polygon can be arranged so that the list of adjacent sides takes the form
. That is, pairs of sides can be arranged so that they interleave in this way.
★ The standard polygon is convex.
★ The sides can be arranged to be geodesic arcs.
The above construction is sufficient to guarantee that each side of the polygon is a closed (non-trivial) loop in the manifold 'H'/Γ. As such, each side can thus an element of the
fundamental group . In particular, the fundamental group
has 2''n'' generators
, with exactly one defining constraint,
:
.
The genus of the resulting manifold 'H'/Γ is ''n''.
Example
The metric fundamental polygon and the standard fundamental polygon will usually have a different number of sides. Thus, for example, the standard fundamental polygon on a
torus is a
fundamental parallelogram. By contrast, the metric fundamental polygon is six-sided, a
hexagon. This can be most easily seen by noting that the sides of the hexagon are perpendicular bisectors of the edges of the parallelogram. That is, one picks a point in the lattice, and then considers the set of straight lines joining this point to nearby neighbors. Bisecting each such line by another perpendicular line, the smallest space walled off by this second set of lines is a hexagon.
In fact, this last construction works in generality: picking a point ''x'', one then considers the geodesics between ''x'' and ''gx'' for ''g'' in Γ. Bisecting these geodesics is another set of curves, the
locus of points equidistant between ''x'' and ''gx''. The smallest region enclosed by this second set of lines is the metric fundamental polygon.
Area
The area of the standard fundamental polygon is
where ''n'' is the genus of the Riemann surface (equivalently, where 4''n'' is the number of the sides of the polygon). Since the standard polygon is a representative of 'H'/Γ, the total area of the Riemann surface is equal to the area of the standard polygon. The area formula follows from the
Gauss-Bonnet theorem and is in a certain sense generalized through the
Riemann-Hurwitz formula.
Explicit form for standard polygons
Explicit expressions can be given for the standard polygons. One of the more useful forms is in terms of the group
associated with the standard polygon. For a genus
oriented surface, the group may be given by
generators
. These generators are given by the following
fractional linear transforms acting on the
upper half-plane:
:
for
. The parameters are given by
:
and
:
and
:
It may be verified that these generators obey the constraint
:
which gives the totality of the
group presentation.
Generalizations
In higher dimensions, the idea of the fundamental polygon is captured in the articulation of
homogeneous spaces.
See also
★
Cayley graph
★
Euclidean domain
★
Voronoi diagram
References
★ Hershel M. Farkas and Irwin Kra, ''Riemann Surfaces'' (1980), Springer-Verlag, New York. ISBN 0-387-90465-4.
★ Jurgen Jost, ''Compact Riemann Surfaces'' (2002), Springer-Verlag, New York. ISBN 3-540-43299-X.