Graphs with Eulerian unit spheres
-spheres are defined graph theoretically and inductively as the empty graph in dimension and -dimensional graphs for which all unit spheres are -spheres and such that for the removal of one vertex renders the graph contractible. Eulerian -spheres are geometric -spheres which can be colored with colors. They are Eulerian graphs in the classical sense and for , all unit spheres of an Eulerian sphere are Eulerian spheres. We prove here that is an Eulerian sphere if and only if the degrees of all the -dimensional sub-simplices in are even. This generalizes a result of Kempe-Heawood for and is work related to the conjecture that all -spheres have chromatic number or which is based on the geometric conjecture that every -sphere can be embedded in an Eulerian -sphere. For , such an embedding into an Eulerian 3-sphere would lead to a geometric proof of the 4 color theorem, allowing to see “why 4 colors suffice”. To achieve the goal of coloring a -sphere with colors, we hope to embed it into a -sphere and refine or thin out the later using special homotopy deformations without touching the embedded sphere. Once rendered Eulerian and so -colorable, it colors the embedded graph . In order to define the degree of a simplex, we introduce a notion of dual graph of a subgraph in a general finite simple graph . This leads to a natural sphere bundle over the simplex graph. We look at geometric graphs which admit a unique geodesic flow: their unit spheres must be Eulerian. We define Platonic spheres graph theoretically as -spheres for which all unit spheres are graph isomorphic Platonic -spheres. Gauss-Bonnet allows a straightforward classification within graph theory independent of the classical Schläfli-Schoute-Coxeter classification: all spheres are Platonic for , the octahedron and icosahedron are the Platonic -spheres, the sixteen and six-hundred cells are the Platonic -spheres. The cross polytope is the unique Platonic -sphere for . It is Eulerian.
Key words and phrases:Geometric graphs, Graph coloring, Eulerian graphs, discrete Hopf-Rinov, Platonic solids, Billiards in graphs
1991 Mathematics Subject Classification:Primary: 05C15, 05C10, 57M15
1. The geometry of graphs
When studying geometric graphs in a purely graph theoretical manner, there is no need to
carrying around Euclidean spaces. This is analogue to look at groups detached from
concrete representations given by transformations in Euclidean space. This detachment from
Euclidean structures can be pedagogically helpful: abstract group theory can be grasped early
by students as symmetry groups or Rubik type puzzles which are intuitive.
Kids without abstract training in algebra can solve these finitely
presented groups and do so often more successfully than adults with abstract mathematical training.
Graphs are intuitive too, as they can be drawn.
Place five dots on paper and connect them all: this is the hyper-tetrahedron, an example of a four
dimensional graph. Want to see a 3-dimensional sphere? Draw a regular 8-gon, then connect all
diagonals except the main diagonals. You might not see the sphere structure yet, but it can be done
by looking at a unit sphere of a vertex . It is the subgraph formed by all points
connected to . If we draw this
sphere, it can be represented as the regular hexagon, where all diagonals except the main diagonals
are placed. Why is this a 2-sphere? Because after removing one point, the remaining graph can be collapsed
and because the unit spheres are spheres: each unit sphere is a -gon, which is
an example of a -sphere. How so? Because removing one point in this quadrangle produces an
interval graph with vertices which can be collapsed and because every unit sphere in this graph is a
-sphere consisting of two disconnected points. Why is the graph consisting of two disconnected points a -sphere:
because removing one point has made the graph collapsed to one point
and because every unit sphere is empty. We just have to impose the initial induction assumption that the empty
graph is the -sphere and we have defined inductively a concept of “sphere” in arbitrary dimension .
This construction illustrates how important dimension is: the dimension of a graph is inductively defined
as plus the average dimension of its unit spheres. An other important ingredient has entered in the definition of spheres:
the notion of homototopy is based on the notion of reduction steps and also inductive: a graph can be collapsed
to a point, if there exists a vertex such that both its unit sphere as well as the graph obtained by
removing the point can be collapsed to a point.
Our 4 dimensional simplex drawn before can be collapsed to a point because every unit sphere
is a 3-dimensional simplex and also because removing the vertex deforms the graph to a 3-dimensional simplex.
So, by induction a complete -simplex is collapsible if the -simplex is collapsible. If as an induction
base, the one point graph is assumed to be collapsible, we are done. Why is a punctured
sphere collapsible? Take the octahedron; removing a single vertex produces the wheel graph with a 4-gon
boundary. The later is collapsible because we take away any outer vertex we get the kite graph, two triangles
glued along an edge. And the kite graph is collapsible, because we can get from it a triangle after removing a vertex.
The triangle is collapsible because it is a simplex.
As in the continuum, one would have to distinguish collapsibility with contractibility. The later means homotopic
to a point, where homotopy is a chain of collapse or inverse collapsing steps and is not equivalent. There
are graphs like the dunce hat which first need to be enlarged before one can contract them to a point. Also this
is analogue to the continuum . But this subtlety is not relevant for spheres.
Why has this simple setup for geometric graphs not appeared earlier? Maybe because it would not have been right:
only since the Poincaré conjecture was proven, we know that spheres are homotopy spheres. Since it is a theorem
that topological -spheres can be characterized as geometric objects of dimension which have the homotopy
type of spheres, this is a valid way how to define spheres in graph theory.
An intuitive definition of dimension for graphs is to add to the average dimension of the
unit spheres. This definition is motivated by a classical Menger-Urysohn dimension but the later
assigns to graphs dimension , because the topology generated by the usual distance metric
renders graphs -dimensional: the topology on a graph is the discrete topology. One has to refer to pointless topology
to get a useful notion of homeomorphism .
Graphs are usually perceived as low dimensional objects: they are usually treated as one-dimensional
simplicial complexes with zero and one-dimensional cohomology only, despite the fact that the higher
dimensional nature is acknowledged in computer graphics or computational topology. We read for example in
: “a one-dimensional complex is a graph”.
Without having to impose more structure, graphs already have a natural simplicial complex associated with them.
This structure of complete subgraphs inside the graph
allows also conveniently to compute cohomology: less than two dozen lines of computer
algebra code are needed to compute a basis for any cohomology group of a general finite simple graph. Without
additional libraries. The key is to build a matrix and to find the kernels of the block matrices of
. For code see .
As early steps in geometry show, the notions of spheres and lines are pivotal for our understanding of a geometric
space. Both are based on distance: spheres are points with equal distance to a given point and lines are
curves which locally minimize distance. They can already be complicated in simple situations like a non-flat
surface, where spheres are wave fronts and lines are geodesics. Also spheres of codimension larger than 1 like a circle in space are
important. We will see that in geometric graphs, graphs for which all unit spheres are graph theoretically defined abstract spheres,
there is a natural way to get spheres as dual graphs to complete subgraphs. The notion of “line” in geometry
is superseded by the notion of “geodesic”, shortest connections between points. For general geometric
graphs, there is no natural geodesic flow. Already for spheres like the icosahedron, we have to tell
how to propagate a light ray through a disc. This requires to tell which “in” direction goes to which “out” direction.
There is a problem in general. Assume we hit cross road, where 5 streets meet. Which of the
two “opposite streets” do we chose? We could throw a dice each time when hitting such an odd degree vertex
but that would render the geodesic flow a random walk. For two dimensional graphs there is a natural geodesic
flow if the graph has even degree at every point. In other words, -dimensional graphs for which a geodesic flow
exists, have to be Eulerian.
This already leads us to the topic studied here and it merges with an other topic in graph theory,
the theory of colorings. The connection is that Eulerian spheres are exactly the spheres which can be colored
with 3 colors. But is pretty clear that in order to define a geodesic flow in higher dimensions which has the property
that is unique, we need the unit spheres to have a bit of symmetry. We need a fixed point free involution
on the unit sphere , telling how to get from the incoming ray to the outgoing ray.
This existence of a fixed point free involution
is a weak form of “projective” as if the graph is large enough, the quotient is then again a graph,
a projective plane. In any case, weakly projective -spheres are Eulerian in the sense that they can be colored
When investigating the class of -spheres which allow a minimal coloring with colors, it is
important also to understand spheres of positive co-dimension. Examples are -dimensional unit spheres or
-dimensional intersections of neighboring unit spheres. This naturally leads to a notion of duality, as
the dual graph of a vertex is , and the dual graph of an edge is the intersection ,
the dual of a triangle the intersection of three spheres etc.
In the case , the dual sphere of an edge is a one-dimensional circular graph and its length is what we
called edge degree. In the case , the dual sphere of a triangle is a circular graph and its length is called
the degree of the triangle. In this case, degree is the number of hyper-tetrahedra “hinging” at the triangle.
When subdividing an edge, the degrees of the maximal simplices in the dual of the edge changes
parity. We are interested in these numbers because if in a -sphere, all
the -dimensional simplices in are even, then the graph can be minimally colored. While we can not
color it initially with colors, we aim to get there eventually using refinement or collapsing processes
To understand this in higher dimensions, it is necessary to look at spheres in graphs a bit more generally.
It turns out that we can define for any subgraph of a finite simple graph a -dual graph .
Unlike the dual graph for the geometric graph itself which is defined by the intersection
properties of its highest dimensional simplices, the -dual graph depends on the host graph
. If is a subgraph of and is a subgraph of then the -dual graph of
is a subgraph of the -dual graph of . As often in duality, the involution property does not kick in directly
but it applies after applying the dual operation once. The reason is that for many subgraphs , the dual graph will
be empty so that the dual operation lock many subgraphs into the cycle. This happens for
every subgraph of which has diameter larger than in . What is important for us is that for
complete subgraphs of dimension , the dual graph is a sphere of dimension .
The notion of complementary duality is motivated by school geometry, where we construct a line
perpendicular to a given line with the compass by intersecting spheres located at the end
points of an interval and end points of an intervals form a - sphere, the two new intersection
points gave us a dual object. Doing the construction again at the dual line brings back the original -sphere.
The same construction can be done in graph theory. The “compass” is now the ability to
draw spheres. It is essentially the only tool at our disposition in the discrete. But sphere geometry
is such a mighty instrument that we do not lose much. Actually, it is surprising how much of geometry
goes over to graph theory, not only to geometric graphs, but to the full class of finite simple graphs.
There is a inductively defined class of -spheres, graphs which have all the properties of -dimensional
spheres in the continuum. Geometric graphs in dimension are defined as graphs for which every unit sphere is a
-sphere. Induction is important because also lower dimensional spheres are relevant in geometry.
In graph theory, they can be constructed by intersecting unit spheres. For example,
the intersection of two neighboring unit spheres in a -dimensional graph produces a -sphere because
is a unit sphere in the unit sphere and because the definition of spheres has been
done recursively. As we will see, if we take a -dimensional simplex in a -dimensional geometric
graph and intersect all these unit spheres centered at vertices in , we obtain a sphere of
The idea to use higher dimensional geometry to color planar graphs has emerged in the late 70’ies in particular
through the work of Steve Fisk .
The excitement and repercussions about the computer assisted proof of the 4-color theorem which was achieved
at just about the same time when  was written, might have dampened a brisker development using geometric
ideas even so it has not stopped. One difficulty with the Fisk approach as well as others following his work
is that it based on more difficult definitions from topology, in particular the notion of
“triangulation” which is complicated and which can carry surprises, especially in higher dimensions.
Coloring questions of triangulations in
higher dimensions in particular are expected to depend on the class of triangulations. We bypass the continuum
and define what a “geometric graph”, a ”sphere” or a ”ball” is entirely within graph theory in a recursive
way. Avoiding definitions from the continuum does not mean to ignore Riemannian geometry; almost all intuition from the
continuum can be carried over almost verbatim from differential topology to graph theory if one lets go the usual
assumption treating graphs as one-dimensional objects. And almost all definitions are motivated from continuum notions.
And there are not only plenty of questions but plenty of entire research areas which have not yet been carried over
from the continuum to this combinatorial setting .
The fresh start with clear and simple definitions allows for bolder conjectures in  like
The later is settled for , where it is known to be equivalent to the 4-color theorem . The reason why these statements are likely to hold true is because of the conjectured picture that every orientable -dimensional geometric graph can be embedded in an Eulerian three sphere bounding a four dimensional ball of dimension , which has a simply connected interior (in the non-orientable case, a Moebius turn needs to to leave into the 4-ball but this does not affect its simply connectivity) and that every -sphere can be embedded in an Eulerian -sphere. In order to investigate this further, we have to understand Eulerian spheres in any dimension and understand a special class of homotopy transformations called edge subdivision or edge collapses. We would eventually like to know whether any two spheres can be deformed into each other by such homotopies and whether we can perform this talk under the “handicap” of not modifing an embedded smaller dimensional surface.
2. Graphs with Eulerian spheres
The definition of geometric graphs and spheres is by induction, starting with the assumption
that the empty graph is the -dimensional sphere so that
and that is empty. The classes of geometric graphs, balls
and spheres are now defined inductively as follows: is the set of graphs for which all unit spheres
in which case or in which case .
The set consists of graphs for which removing one vertex produces
a graph in . Finally, is the set of contractible graphs for which
the boundary is in . A graph is contractible if there exists a vertex such
that and are both contractible.
With these definitions, all graphs in satisfy for and all -spheres have Euler characteristic for dimension . On can characterize in as the class of graphs which admit a function with exactly one critical point and in . For , is the class of graphs in for which the minimal number of critical points is exactly .
1) -spheres are cyclic graphs with . Such a graph is a geometric -sphere, if and only if is even.
2) A graph is a -sphere if and only if it is both 4-connected and maximally planar. . The 4-connectivity implies 3-connectivity which by the Steinitz theorem implies that the planar graph can be realized as a convex polyhedron in . The maximal planarity then implies that this polyhedron has triangular faces. Examples are the octahedron or icosahedron. A -sphere is Eulerian if an only if it is an Eulerian graph, hence our nomenclature.
3) The -cell is an example of an Eulerian -sphere. But not all -spheres are Eulerian spheres in our sense: the -cell is an example of a -sphere which is not an Eulerian sphere. Its chromatic number is .
4) Removing a vertex from an Eulerian sphere produces an Eulerian disk. Every interval graph is an Eulerian disk as we can color an interval with colors.
5) Gluing two Eulerian disks in along the circular boundary produces an Eulerian sphere. An Eulerian disk does not need to be an Eulerian graph. An example is the wheel graph with boundary . It can be colored with colors but the boundary points in a wheel graph have degree which is odd so that wheel graphs are never Eulerian graphs.
Lets start with the trivial case as it matches the following statements. For , define the degree of the empty graph as the number of vertices in . We can look in general at itself as the dual graph of the empty graph, which can for be seen as a -dimensional sphere within . Lets formulate this special case too as it will matches the higher dimensional situation:
The following result is the classical Euler-Hierholzer result:
1) The octahedron is Eulerian.
2) The stellated -cube with vertex degrees and is Eulerian.
3) The icosahedron has vertex degrees and is not Eulerian.
4) Take two Eulerian spheres which contain both a vertex or of degree . By the connected sum construction, we can glue the two spheres along the unit ball to get a larger Eulerian sphere.
In , we have defined the edge degree of as the number of tetrahedra attached to an edge . The union of the vertices of these tetrahedra minus the vertices of the edge form a circular graph.
1) The 16 cell, the three-dimensional analogue of the octahedron is Eulerian. Its clique volume vector is .
2) The 600 cell, the three dimensional analogue of the icosahedron is not Eulerian.
3) The stellated -cube is the tesseract, where the -dimensional ”solid cube faces” are stellated. It is a graph containing vertices, edges, triangles and tetrahedra. It is an Eulerian graph for which all edge degrees are either or .
4) Using connected sum constructions, stacking together such cubes along common faces, we can get larger and larger classes of such graphs and get graphs in which have arbitrary large but which are minimally colorable with colors.
5) If is an Eulerian -sphere, then the double suspension construction produces an Eulerian 3-sphere. For example, the -cell is obtained from the octahedron by a double suspension.
If some would need more than colors, then would need more than colors to be colored. ∎
The -volumes are known to be a basis for all isomorphism invariant additive functionals on graphs satisfying for . The Euler characteristic is as a super volume an example of a linear combination of the volumes.
Use induction with respect to and use the handshaking formula
which in the case agrees with the classical Euler handshaking result telling that twice the number of edges is the sum of the number of edge degrees. Since by induction, all are even for , the result follows if we can show that is even. But since the Euler characteristic of spheres is either or and so even, the evenness of follows from the formula . ∎
One could ask whether the reverse is true and whether the condition that all the volumes are even, assures that is Eulerian. But this is not the case. Make two edge refinements at different but intersecting edges for . Each edge refinement changes the parity of the number of vertices and edges but not for triangles. After the two refinements we have two vertices of odd degree so that the new graph is no more Eulerian, even so all volumes are even. We do not believe that one can read off the Eulerian property from volumes. But one can still ask:
Of course we do not mean silly conditions like for , where forces the graph to be a 16-cell and so to be Eulerian. One could imagine a computer building lots of random geometric graphs and color in the grid the points given by gometric graphs with one color, the others with an other color. It looks like a formidable problem also to find the number of geometric graphs in which have a given volume vector .
Eulerian spheres are Eulerian graphs:
By Euler-Hierholzer, we only need to know that every unit sphere has an even number of vertices. But that follows from the previous corollary. ∎
Because every unit sphere in must be minimally colorable with colors,
the class of Eulerian spheres could be defined recursively as
the class of spheres for which every unit sphere is in with the inductive assumption
for , the spheres are Eulerian.
Since spheres and especially Eulerian spheres are orientable, the coloring of each of the maximal simplices defines a sign of the permutation of the colors. This signature partitions the dual graph into two sets. Adjacent simplices have opposite signatures. ∎
1) A -sphere has the same dual graph and is bipartite if and only if is even.
2) For the octahedron graph, the dual graph is the cube graph. It is bipartite.
3) There are projective planes with chromatic number . In that case the dual graph is not bipartite.
If is an Eulerian sphere, then by the previous lemma, we have a bipartite dual graph. If is bipartite we can constructively color the graph with colors. ∎
This does not generalize to non-simply connected graphs as
the coloring will then also depend on holonomy conditions. The torus
for example is in but the torus is not. For spheres which
are simply connected for , these difficulties are absent.
We have seen that every Eulerian sphere is an Eulerian graph and that for , Eulerian spheres agree with Eulerian graphs. Of course, for , every sphere is an Eulerian graph but only graphs of the form are Eulerian graphs.
We believe the answer is “yes” and that holds in general
but that examples might only exist in 4 or higher dimension. We tried
to explore the answer ”no” by using an Eulerian path visiting all edges of and
use this path to color all the vertices with a colors. But more likely is that there
is a counter example. It would be surprising if because then, we could
focus on vertex degrees rather than -dimensional simplex degrees during
the graph modification process which could be easier.
Geometric graphs have spheres as unit spheres. One can look at a larger class of graphs, where we just ask that unit spheres are in . Lets weaken this:
One could start even earlier and allow . This would lead to an even larger class of graphs which contains discrete varieties defined in . But this would lead too far away evenso we believe that for varieties, the coloring questions are similar to graphs in as singularities should not matter much. Lets go back to as just defined. Clearly, it follows from that . There are no exotic -dimensional spaces. But already is larger as we can look for example at the double suspension of a higher degree surface. But this example is not homeomorphic to a standard sphere where homeomorphic is in the sense of . Since we have a notion of homemorphism for graphs and because exotic spheres exist in classical topology, it is obvious to ask about the existence of “discrete exotic spheres”:
Such spheres could exist in higher dimensions. We would have to build a graph for which some unit spheres are not spheres but for which there is a cover which has a nerve graph which is graph isomorphic to a nerve graph of a standard sphere. If the answer to the above question is yes, one has course to wonder whether there is a relation with exotic spheres in topology, examples of spheres which are homeomorphic to a unit sphere in Euclidean space but not diffeomorphic to it.
3. Complementary dual graphs
The following definition is done for any subgraph of a finite simple graph .
1) The dual graph of the empty graph in is the graph it self. The dual graph of is the empty graph.
2) The dual graph of a -vertex subgraph is the unit sphere of in .
3) The dual graph of a complete graph in is the complete graph formed by the complementary vertices of .
For , the complete graph is a single vertex and the dual graph is its unit sphere, which is a -sphere: the empty graph. In general, use induction with respect to to : given a subgraph , take a point off from to get a complete subgraph . The dual graph of is now a -dimensional graph containing . By induction assumption, it is a sphere. The dual graph of is the unit sphere of in which (because is a sphere) by definition is again a -dimensional sphere. ∎
1) For a vertex in the octahedron, the dual graph is the -dimensional unit sphere which is in this case.
2) For an edge in a -dimensional geometric graph, the dual graph consists of the zero-dimensional sphere consisting of two edges , where and are the two triangles adjacent to .
The following statement justifies the name duality:
Given a vertex . Every vertex in has distance from . Therefore is in the dual graph of . This shows that . Applying this to shows that . (1) We know that , then as consists of less intersections. Applying this to and shows that (2). From (1) and (2) we see if is a dual graph. ∎
Is every subgraph of a graph a dual graph of some graph? No. Otherwise, the dual operation would be bijective but there are many subgraphs of for which is the empty graph. Examples are graphs of diameter larger than . In a geometric situation we can characterize dual graphs as follows:
For the empty graph , the dual graph is the entire graph . Graphs of diameter are complete subgraphs for which the dual is a sphere. If the diameter is (within ) we deal with subsets of spheres and the dual is a sphere together with the center which is a disk or a complete subgraph. For a graph of diameter or more, two spheres do not intersect and the dual graph is empty. ∎
1) If the host graph is a complete graph, every subgraph has the dual graph graph and these two complete graphs are dual to each other.
2) In , the graph , the empty graph , the one point graphs and their spheres are the only dual graphs. The dual graph of a unit ball is the empty graph.
3) For a 3-sphere, the dual graph of an edge is a circular graph . If we take a sufficiently large part of that circular graph, then the dual is already the edge again. But . For a complete subgraph it is a sphere . Now complete this sphere to a ball . The complementary graph of this ball is a -dimensional sphere . The two spheres and are dual spheres in in the sense that the dual sphere of the ball of is and the dual sphere of the ball of is .
4) For an edge in a -sphere, the dual graph is a -sphere , the intersection of two -spheres and . The dual of is again .
5) For a vertex in the dual graph is a sphere and the dual of is again a complete graph.
4. Degree condition for Eulerian
We have seen that the degree of the empty graph is the order of the graph, that the degree of a vertex in a -dimensional graph is the degree of the vertex and that the degree of an edge in a -dimensional graph is the edge degree, the order of the dual graph of . In general, we have:
Here is the main result. It generalizes what we know already for and :
Let be a -dimensional simplex and let be its dual sphere which we know to be a -dimensional circular graph. If is the number of vertices in , it is the degree of . Let be a -dimensional simplex which contains . It is given by the vertices in as well as two adjacent vertices in . It follows that the set of -dimensional simplices which hinge at form a circular chain of length . Now pick a simplex in this set and color it with colors. The coloring of the adjacent simplices in the circular chain is now determined. Since is even we can continue through and color all the simplices with colors. Now pick an other dimensional simplex which is the intersection of two simplices. It again produces a chain of simplices. In the same way, we can continue the coloring. Since the graph is simply connected, we can color the entire graph with colors. ∎
5. Edge refinement and collapse
There are many refinements of Eulerian graphs which
keep the graph Eulerian. The already mentioned connected sum construction
can be seen as such: chose a unit ball inside and glue two
copies of the graph together along the boundary. This can be seen as a refinement,
as we can see the second graph glued into the unit ball of the first. We are more
interested in refinements which do modify the Eulerian structure as we want
to get to the Eulerian graphs eventually. One example is to do an edge division and
the inverse, the edge collapse.
Given a -sphere and a -dimensional complete subgraph . The dual graph is a cyclic graph. We want to find a subdivision algorithm which renders all degrees even.
The reverse of an edge division can be identified with edge collapse, which is often used in graph theory but which does not always preserve dimension and so the class of geometric class.
Each edge subdivision preserves the class of spheres and is an Ivashchenko homotopy:
This is seen by induction with respect to . The sphere of the new vertex dividing the edge is a double suspension of the sphere and so a sphere. The spheres and do not change topologically. For the sphere , the vertex is just replaced with the vertex . The other affected vertices are vertices in . For such a vertex , the sphere contains originally the edge and afterwards the edge and where is replaced with any vertex in . In other words, the sphere has undergone an edge refinement too and by induction this is again is a sphere.
(b) is homotopic to .
The edge division can be split up into two parts. First by adding a new vertex and attaching it to the contractible subgraph . This does not leave spheres invariant but it is a homotopy step. Now remove the edge . This is possible since is now contractible. By the way, this is the original Ivashchenko notion of I-contractibility which additionally included that deformation.
(c) : since by b), the graph is homotopic to a sphere, it must be in .
(d) Edge collapse. If and was the newly added vertex in the edge, then either collapsing the new edge or collapsing produces a graph isomorphic to the old graph . ∎
Note that unlike edge refinements and the fact that edge collapse
reverses an edge refinement, an edge collapse in general is not a homotopy.
An example is the graph which is not simply connected and has Euler characteristic
. After an edge collapse we have a triangle which is contractible and has
Euler characteristic . If we do an edge subdivision for the triangle,
we obtained the kite graph.
What is the effect of an edge division or edge collapse?
Given a simplex in , it gives together with the edges a -dimensional simplex which counts to the degree of . When splitting to , we get two simplices, one with added to the vertices of , the other with added. ∎
1) For , the dual graph of any edge is empty. There are no -simplices in the graph. The subdivision changes the degree of the entire graph. This is a special case; not at least because -dimensional spheres are not simply connected.
2) For , the dual graph consists of two vertices. The subdivision changes the degree of these two vertices.
3) For , the dual graph consists of a circular graph. The subdivision changes the degree of each of the edges of this circle.
4) For , the dual graph consists of a -sphere, a polyhedron. The subdivision changes the degrees of each triangle in that sphere. Remember that the degree of the triangle is the number of elements in the -dimensional circle dual to that triangle.
We believe that every -sphere can be modified by refinements or collapses within the class so that it becomes Eulerian but we only know this in the case .
Chose two vertices of odd degree. Find a path of even length connecting the two and cut the triangles. Possibly first make a subdivision first. ∎
In the following, an edge collapse only refers to edge collapses which keeps the graph in . Irreducible graphs to be defined below would not allow an edge collapse. The following statement would provide a proof of the 4-color theorem:
The following statement would provide a proof of the conjecture that every graph in can be colored with or colors.
The following statement would provide a proof of the conjecture
6. Projective spheres and irreducibility
Spheres in spheres play the role of linear subspaces of the tangent space in classical geometry: the reason is that if we take a linear subspace and intersect it with the sphere, we get a lower dimensional sphere. Since in the discrete, we only have spheres and no notion of linear subspaces, we work with the later similarly as classical geometry can be dealt with by compactifying Euclidean space leading to projective geometry. Since we use edge subdivision to modify graphs aiming to make them Eulerian, we are interested in graphs which can not be obtained from edge subdivision steps.
There is a different notion of irreducibility in discussions about the 4 color theorem but
should be no confusion.
1) An octahedron is irreducible because it is the smallest graph in .
2) The octahedron is a double suspension of . Any double suspension of with is reducible. The reason is that is obtained from by an edge refinement.
3) The icosahedron is reducible as we can collapse one edge and still keep it geometric.
4) All higher dimensional cross polytopes in are irreducible.
5) There is exactly one irreducible sphere in : it is .
6) Irreducibility is also defined for graphs in . A hexagonal flat torus for example is irreducible since an edge refinement steps produces a vertex of degree .
Can we classify irreducible spheres? Yes, in dimension , where only is irreducible and also in dimension : after an edge refinement step, we always have a vertex of degree so that if there are no degree vertices, we can not collapse:
Let be the neighbors of and a pair of elements in . Remove the edges and add the edge . By the radius of injectivity condition, this edge collapse still produces a graph in . ∎
Graph modifications are important in the four color theorem. One can restrict to graphs in for which all vertex degrees are larger or equal to . Kempe used his chains to avoid degree 4 vertices and overlooked a case when trying to avoid degree-5 vertices which by Gauss-Bonnet always exist for if degree-4 vertices have been excluded.
1) For a cell, every unit sphere is an octahedron which is projective but not strongly projective. It admits an involution but the quotient is no more geometric. There are no strictly positive curvature projective planes in the discrete.
2) If every cyclic graph is , then is strongly projective. It has an involution such that is again a cyclic graph.
3) Graphs containing an unit sphere with an odd number of vertices can not be projective. Therefore, the degree has to be even for all vertices.
4) Strongly projective spheres can be constructed by taking a discrete projective space , for example by taking a nice triangulation of a classical projective space, then take a double cover.
5) A decahedron, the polyhedron obtained by doing a double suspension on is an example of a weakly projective space. There is an antipodal map, which assigns to each vertex the unique point with largest distance from . But this map can not be fixed point free as the restriction to the equator shows, where the odd number of vertices prevent a fixed point free involution.
1) A graph in which is projective then it is in because all unit spheres have then even degree.
2) A graph in is projective then every unit sphere in is projective and so Euclidean. This means that contains the projective -spheres.
3) There are Eulerian graphs which are not projective. A simple example is obtained by taking an octahedron and subdividing the same edge twice. This produces a new Eulerian graph but it does not admit a fixed point free involution.
1) The icosahedron is generic in .
2) The cell is generic in .
3) Any flat torus with hexagonal tiling is generic in .
In other words, is weakly projective if all unit spheres are a double cover of a disc ramified over its boundary or even a double cover over a projective space. Two weakly projective spheres can be added with the direct sum construction so that . A generic sphere does not allow a nontrivial involution on each of its spheres. Strongly projective spheres are spheres which are double covers of projective spaces. Any large enough projective sphere is strongly projective.
We prove that if is not irreducible, then the graph is not generic. If is not irreducible, it is obtained from an other graph by an edge division. This edge refinement step has added a vertex in the middle of an edge and produced a projective sphere within : the involution switches and leaves the sphere invariant. The graph is not generic. ∎
If , then is the unit sphere . We know that contains . Assume it contains and an additional vertex then is also the unit sphere of . But then there is an involution which maps and and leaves invariant. In other words, would be reducible and so be not generic. In general, the fact follows by the recursive definition of genericity. If , take a vertex in and look at the unit sphere. It is a sphere of dimension less and the dual of in is the dual of in . By induction, its dual is . ∎
The sphere bundle over the simplex set comes handy when filling the interior
structure of the faces of the dual graph of . This is needed
when we want to get the completion as a graph in with
dual Betti data. For the sphere bundle reveals the dual geometric graph of
as probably Whitney first made clear, of course using different language. We want to see this
graph theoretically. The spheres in the sphere bundle have dimension .
It is the dual graph which is the skeleton containing the -dimensional simplices of
as vertices. The sphere bundle helps to fill this skeleton with a triangulation
in order to get as a geometric graph in . First of all we need additional
vertices in . Take for that the set of spheres . The dual graph has now
vertices. Connect a vertex with all maximal simplices which contain it. This produces
edges additionally to the already existing ones in . We see that these new edges
correspond to vertices in the dual graph of . Now we have to complewte the dual
graph of . But that is a lower dimensional problem which shows that all the filling can be done
inductively. In two dimensions, the task was so easy because the dual graph of is again a circular graph
which does not need to be completed.
If is orientable, then is again a graph in and Poincaré duality holds. For example, the dual graph of the octahedron is the cube, a one-dimensional graph with square faces which can be caped in a compatible way. For a non-orientable graph but we can not fill the interiors in a compatible way to get a dual completion in . To prove the Poincaré duality, one needs to write down the incidence matrices of the dual graph and relate the kernel of the Laplacians with the kernel of which is not obvious as the matrices have completely different size. The new for example is matrix. We have not shown yet Poincaré duality purely graph theoretically.
Proof by induction for . For , it is clear as the dual graph is isomorphig to the graph itself. Look at the unit spheres in the completed graph. For the vertices belonging to the maximal simplices, it is the completion of the dual graph of the sphere . By induction and using that is Eulerian, also the dual is Eulerian if and only if is Eulerian. For each of the virtual vertices added, the unit sphere is isomorphic to and so Eulerian. ∎
1) For , we always have .
2) For , the volumes of the graph are and . The graph now has vertex degrees or , which are all even.
3) For the 16-cell , the dual graph is the stellated three dimensional cube which is Eulerian as every unit sphere is either an octahedron or stellated cube.
4) We see already when looking at the two dimensional spheres that when taking the double dual, the volumes grow exponentially.
7. Sphere bundles over the simplex graph
Simplices play an important role in graph theory. In geometric setups, this has been
realized most prominently by Forman  who built discrete Morse theory.
Calculus and cohomology are other reasons as differential forms are just functions
on simplices in such a way that an pre-described ordering of the vertices in each
simplex produces functions on the simplices.
An other indication comes from fixed point results like the Lefshetz fixed point
formula  which equates the sum of the
degrees of fixed simplices with the Lefshetz number of the graph automorphism .
This result holds in full generality for all finite simple graphs.
In a geometric setup, if , then the degree of the map on a simplex
can be seen in a more general way as we have now a natural sphere bundle on the set of simplices.
We have just seen that under some genericity condition, the sphere recovers the simplex.
Assume now that is in and that denotes the sphere associated to a complete subgraph which we consider as in the Brouwer story to be an atomic quantity.
As , the permuted has the same sphere. Let are vertices in which are cyclically permuted, this cyclically permutes the corresponding spheres , leaving the intersection invariant. It therefore produces a map on the sphere . As is an automorphism, it induces an automorphism on the subgraph . ∎
1) If is the octahedron and is a rotation of this sphere with fixed vertices, then these are the only simplices fixed and their degree is one. The degree of the rotation on is . The Lefshetz number of on is as the map induces the identity on and and has no contribution from as is simply connected.
2) If is the octahedron and is the antipodal map, then is orientation reversing and has trace on . Therefore, its Lefshetz number is zero. There is no fixed point.
This leads to a reformulation of the Brouwer-Lefshetz story as if is a fixed simplex, then the dual graph is fixed too.
The Brouwer-Lefshetz fixed point theorem  can now be formulated in that the sum of the degrees
of induced on spheres is the Lefshetz number. In some sense this is closer to the
continuum geometry, but its not clear yet how things are linked. The Lefshetz number of
a sphere is either or depending on the dimension and whether is orientation preserving
or not. If is even and is orientation preserving on the sphere or is odd and is orientation
reversing on the sphere then , otherwise, it is .
The degree of is if is even and is orientation preserving on or if is odd and
is orientation reversing on . We see that the situation is completely parallel.
It is surprisingly tricky to define without intersecting spheres what a “lower dimensional unit sphere” is in a graph. In the case of one dimensional spheres, we can not just say it to be a subgraph isomorphic to for which the diameter in is as any closed curve on the unit sphere of a vertex would qualify as a -dimensional unit sphere. Duality provided us with a convenient way: -dimensional sphere in a -dimensional geometric graph is the dual graph of a subgraph. For example, for , a dimensional subgraph is the dual of a , an edge. The sphere bundle of the set of simplices is therefore a natural construct and produces all the small spheres we ever need in a geometric setup.
8. Geodesics and Hopf-Rinov
There will never be a completely satisfactory classical geodesic flow for finite simple
graphs simply because the unit sphere at a point is in general
smaller than the number of vertices different from . Even if a unique geodesic
flow can be defined in such a way that two points in distance have a unique geodesic connection,
still many graphs have the property that for some point , the union of all geodesics starting
at will not cover the entire graph. The true geodesic flow is quantum in nature, as it is in the
real world: we have to look at the wave equation on a graph. It is then possible for two points
to start with a wave located on the vertex at time and find a velocity vector
of length (a function on vertices and edges) and a time such that .
The reason why this is possible is simply linear algebra: because
the wave equation with scalar Laplacian of the
graph is part of the wave equation on the simplex space, where with
a matrix so that we can write which is the
d’Alemberg solution. We now only have to solve for and in the ortho-complement of the kernel
of to solve the equation for given and . The smallest time which leads to a solution gives
us a notion of “how fast particles travel” in the graph.
Mathematically, there is no problem in the simply connected connected case as we only have to
look for velocities for which the total velocity is zero, to make sense of.
As is a symmetric matrix, there is no need even to involve the theory of pseudo inverses. In any case,
this solution of the wave equation is quantum in nature because we can write also
with complex wave function vectors
. So, waves on a graph are described by the Schrödinger equation
for the Dirac operator.
For a physicist, this story really becomes exciting when looking at the
propagation of waves on higher forms. For example, if is an initial wave located on an edge,
then we look at the propagation of -forms which is electromagnetism. For forms given by functions
on triangles, the symmetry group of the triangle is already non-Abelian. How fast do things travel there
answers the question “how heavy” the particles under consideration are. In any case,
the mathematics of propagating waves (= quantum particles) in this finite universe is simple
linear algebra even so the matrices can become large. For the icosahedron already, the matrix
is a matrix as . For a three dimensional graph modeling
more realistic physics, the matrices are much larger.
If we go back to draw circles and look for a classical notion of “line” we need to say what a geodesic is
in the graph. We can look for a weaker form of Hopf-Rinov and not ask to be able to connect two
arbitrary points with a line - which as we have just seen is impossible - but to extend a line
segment of length one indefinitely. In other words, we only want to find a dynamical system on the
unit sphere bundle which has global existence of solutions. Here is where the relation with
chromatology comes in. If we look at a polyhedron which has a vertex with an
odd number of edges attached and a light ray comes in, then how do we tell, where it goes out?
We could chose randomly but we can never do that in a reversible manner except bouncing
back some light ray from one direction which is highly unphysical and contradicts anything
we know about light. Mathematically, the reason why we can not find a local deterministic
reversible propagation rule on a unit ball of an odd degree vertex is that on with odd
there is no fixed point free involution. So, we need each vertex to have even degree. That means
the polyhedron has to be Eulerian or equivalently to be colorable. In higher dimensions,
where unit spheres have dimension larger than , the unit spheres can become already complicated
and we need a bit more than the graph just to be Eulerian. This is why we have looked at
projective graphs. This is a natural as for large enough unit spheres, the notion of projective
means that the unit sphere is a double cover of a projective space as in Euclidean geometry.
The problem of computing geodesic paths in graphs was our very first
entry point to the field of graph theory while investigating
classical geodesic evolutions in a HCRP project with
Michael Teodorescu in the fall of 2008 and spring 2009, especially in the
context of the open Jacobi conjecture about caustics in ellipsoids.
In any case, the notion of projective spheres is crucial for getting graphs which have geodesic flow without having to refer to the quantum world, where waves are computed on graphs. For geometric purposes, it is desirable to have a classical Hopf-Rinov type statement. And there is almost nothing to show:
The involution in the unit sphere describes the propagation of the path in each unit ball: an incoming ray is propagated to a well defined outgoing ray . ∎
This is natural since if there exists a fixed point free involution on a sphere, it is unique among this kind. Comparing with differential geometry, it is a Levi-Civita statement telling that under some conditions, there is a unique connection, or notion of parallel transport:
Use induction with respect to . For , it is clear as the automorphism group of a circular graph is the dihedral group containing only one involution which is fixed point free and that is the antipodal map. Assume , since is by induction uniquely determined on , we can extend the map uniquely to the disc from there to a larger neighborhood etc until it fixes the map on all the sphere. ∎
9. Billiards and caustics
There is therefore exactly one geodesic flow on a projective geometric graph. The
projective condition plays the analogue role of zero-torsion for the connection as
the later also assures uniqueness of the connection.
And so, we can get geometric graphs with the Hopf-Rinov property if the unit
spheres are double covers of Eulerian projective spaces. The graph itself does not
have to have this property.
We have investigated in  a very special case of the question:
Here is something we know about “curvature 60”:
By the classical Gauss-Bonnet known since the 19th century for polyhedra, there are exactly 12 degree 5 vertices. Since all neighbors have degree 6, the second order curvature is 5 at each of these vertices. For vertices in distance 2 or larger to the degree 5 vertices, the curvature is 0 as the 2-disk is then completely flat. Also in the immediate neighborhood of a degree vertex, the curvature is zero, if the vertex has degree 6. ∎
We do no know under which conditions such a second order Gauss-Bonnet result holds and therefore
have stuck to first order curvatures, also in higher dimensions. The constant for the second
order curvature formula is obtained for the icosahedron, where for
all 12 vertices. One problem is to define the second sphere as there are already
points in distance which can not be reached by geodesics starting at if the degree of
is and positive curvature implies for Eulerian graphs the presence of degree 4 vertices
and so large curvature. It might therefore be that we need non-positive curvature for the second
curvature to be a good but this just seems to lead to Buckyball examples like treated in the
previous lemma. In general, we have had little luck with getting total curvature 60 if there are
negative curvature vertices. In this context there are interesting constraints:
 for example showed recently that (1/6,-1/6) curvature pairs can not be realized alone on
a torus, even so Gauss-Bonnet would allow for that (thanks to Ivan Izmestiev for sending us
1) For the stellated cube which is a Catalan solid, not all second spheres are circles. The second order curvatures are at eight vertices and zero else. The total curvature is 48.
2) From the 13 Catalan solids, the duals of the Archimedean solids, there are 4 which are geometric and 3 of them are Eulerian. For none of them, the second spheres are spheres. The history of Archimedean solids is a bit murky since Archimedan’s own account is lost  but where Archimedes has referred to the cuboctahedron as already been studied by Plato. The duality might have been first understood in the 14th century by Maurolycus.
3) For all “Buckminsterfullerene” type graphs with degree 5 and 6 vertices the total second order curvature is 60: the proof is that the isosahedral symmetry forces all the 12 degree 5 vertices to be separated apart and the second order curvature is 5 in each of these cases and zero else. Examples are “golf balls”. Degree 4 vertices do not work as the second spheres are no spheres. In some sense, degree 4 vertices have the effect that the graph is not “smooth enough” for second order curvatures.
This is a standard motivation for billiards : classical
billiards can be seen as a limiting case of a geodesic flow. In the discrete
we do not have to take a limit. The geodesic flow on the double cover of the
billiard table with boundary is equivalent to the billiard situation, where
the ball changes direction at each boundary point.
One can also look at notions of caustic. There are caustics known in billiards as well as in geodesic flows are sometimes related as  illustrates.
A point in the caustic is also called conjugate point but it is not the same.
Classically, conjugate points are points for which a nonzero Jacobi field exists along
the geodesics which has a root at the end points. It is a common theme in differential
geometry to give curvature conditions estimating the radius of injectivity in terms
of curvature (see e.g. ).
The caustics are difficult to understand in differential geometry is illustrated by the unsolved
Jacobi’s last theorem asking whether on a general ellipsoid, all primary caustics
have 4 cusps. This is rather embarrassing since the geodesic flow on the ellipsoid is integrable.
It is the prototype of a system which is “solvable”. Still we have no clue about the caustics.
One can look at secondary and ternary caustics etc. In general, even in integrable situations, the
union of all caustics is expected to become dense except in very special cases like the round sphere
where the caustic is always a point. It was this story of caustics which brought us originally
to the journey to consider at discrete versions of the problem.
Having a geodesic flow on surfaces or billiards allows to investigate questions in the discrete in a completely combinatorial way which are difficult in the continuum. There are questions about the existence of periodic orbits, the existence of geodesics which visit all points. An other important question is how to model the continuum with discrete structures. One has to break symmetries in order to have geometries which are not too rigid. A first possibility is by refining randomly, an other is to use almost periodicity. The Penrose graph for example is a graph which is Eulerian, as all vertex degrees are 4,6,8 or 10. Taking two such Penrose patches with smooth boundary and gluing the boundaries together produces a Penrose sphere in .
10. Platonic spheres and symmetries
The story of regular polytopes is one of the oldest in mathematics. As pointed out
in , the story went through an evolution of failures. The culprit is
the notion of “polytope”, a generalization of polygon and polyhedron for which is surprisingly
hard to find a precise definition. Already in school
geometry there is a mesmerizing variety of notions about what a polygon is: does it have to be
a simple polygon or convex? For polyhedra in three dimension, one does not know whether to see
the story as a comedy or tragedy 
as “theorems” like the Euler polyhedron formula had to go through a chain of improvements
when new counter examples to the formula appeared. Examples like the Kepler-Poinsot polyhedra with
negative Euler characteristic illustrate this. Of course the dust has settled today.
In higher dimensions, one usually restricts now to convex polyopes .
The story of polytopes in higher dimensions is by far settled. It is historically
interesting that early pioneer research of polytopes in higher dimensions has been done by
non-mainstream mathematicians like Alicia Boole Stott who had a great influence on
Schoute  similarly than Ludwig Schläfli  who influenced
When leaving the Euclidean embedding questions off the table, the story of polytopes becomes combinatorial: polygon are -spheres, polyhedra are -spheres and polytopes are -sphere. Yes there are graphs in of higher genus which have natural immersions in as regular polytopes but this is exactly what makes the classical story difficult. Lets illustrate how untangled everything becomes when giving a graph theoretical definition of Platonic solid.
Unlike the classical classification of regular polyhedra done by mathematicians like Schläfli  Scott, Schoute or Coxeter, the classification of Platonic spheres in graph theory is easy to give in an independent way. We only need Gauss-Bonnet :
The case is clear. For , the curvature has to be the same at every vertex and add up to . It therefore better has to be positive. As it is a fraction of , it is either (leading to the octahedron) or (leading to the icosahedron). As all unit spheres for a graph in have to be regular, we know that there are two possibilities: either the unit sphere is the octahedron, or the icosahedron. Both are possible, the first is the 16 cell, the second the 600 cell. We do not have to invoke Gauss-Bonnet as it would be useless: the sum of curvatures would be zero as for all . This shows inductively that in higher dimensions also,, there are maximally two polyhedra. But in , by Gauss-Bonnet again, the curvatures have to add up to . Since the curvature at a vertex is , where are the -volumes in . The numbers are integers so that the curvature must be of the form . Indeed, for , we can realize it with the -dimensional cross polytope (the octahedron embedded in ), which has the volume data , leading to Euler characteristic . If it is the unit of a 5-dimensional solid, then the curvature is which is no surprise as every -dimensional sphere has zero Euler characteristic. Can we get a 4-dimensional Platonic solid in for which the unit sphere is the 600-cell? Lets compute the curvature. The volume data of the 600-cell are leading to the curvature . Since the curvature adds up to and must be the same at every vertex, this is not possible. We see that we are locked in to cross polytopes from now on. ∎
We see that when looking at Platonic solids in , we can
explain easily why the number of Platonic solids “thins out” in higher
dimensions: the number of Platonic solids can not increase and Gauss-Bonnet
is the reason why we the drop from to and from to .
Since odd dimensional geometric graphs have zero Euler characteristic, these
drops could can easily take place when moving from odd to even dimensions. And
since at dimensions , we are already down to one, there is nothing to do
any more. We don’t miss much as classically, only the duals of the platonic solids
like the hypercube have to be placed into the picture.
The hyper-tetrahedra do not count for us as Platonic solids
because they are not spheres. Indeed, they are contractible.
What about semi-regular polytopes? Classically this is already a bit more
difficult to analyze as one asks that the vertex degrees are the same
everywhere and that the faces are regular polytopes. A classification
in higher dimensions has not yet been done .
Lets try to give a definition which is close to the definition of uniform polyhedra seen classically. Of course we can not have the same notions as we only look at geometric graphs. Denote with the automorphism group of a graph. It consists of all graph isomorphisms . This group plays an important role also in the continuum, when analyzing semi regular polytopes as it plays the role of reflection and rotational symmetries in the continuum.
1) Every Platonic spheres (octahedron, icosahedron) is uniform.
2) In two dimensions, all the completions of Archimedean solids are uniform.
3) The completions of a Catalan solid for which this completion is in are uniform spheres.
Uniform spheres can also become non-Eulerian spheres, as the completion of the
dodecahedraon or the icosahedron show.
Assume is a uniform sphere. Is the dual completion also uniform?
We tried to prove this for a while until we realized that the dual completion dynamics
would produce larger and larger examples of graphs with the same automorphism group
for which the transitivity of the automorphism group can not hold any more.
Classification of these graphs is not yet done. Besides prismatic families of graphs, there
should be only a finite set.
1) The dual completion of the icosahedron is the ”small stellated dodecahedron”. In an Euclidean setting, this solid is looked at differently as see it to be embedded in Euclidean space with 12 faces. We look at it as an element in : there are faces (each of the original faces is replaced with ), vertices (the 20 original vertices together with the 12 new centers) and edges (the 30 original edges plus 5 for each of the original faces). The Euler characteristic is . The positive curvature is located on 12 new centers where it is .
2) The completion of the dual of the octahedron is the stellated cube, which is also known under the name ”Tetrakishexahedron”. It is an example of a Catalan solid which happens to be in . The curvature is zero except for the 6 new faces vertices of curvature .
11. Summary and conclusion
We have looked here at the class of Eulerian spheres, spheres which can be colored
minimally. More generally, we were interested in Eulerian geometric graphs, geometric graphs for which all unit spheres are
Eulerian. They are all Eulerian graphs in the classical sense that there exists a closed path visiting all edges exactly once.
We can recursively characterize as the class of spheres for which all are
in and bipartite graphs is the class of bipartite circular graphs.
We have also seen that
and that .
We do not know yet whether .
While we have seen that all -volumes are even for ,
we do not know yet which volume data are achievable satisfying .
We have characterized as the class of spheres for which all degrees of -dimensional simplices are even
where the degree is defined as the length of .
We have defined edge refinements, which are transformations from . The reverse of an edge
refinement is an edge collapse.
An edge refinement or collapse (in the later case of course assuming that we stay in )
for is a homotopy which has the effect that all degrees of maximal simplices in the -dimensional
sphere change parity. We know by definition that any two spheres are homotopic.
One question is whether any two spheres can be transformed into
each other by edge refinements and collapses within and more generally, if any two -spheres containing
a common dimensional sphere can be transformed into each other by such transformations without
touching edges in . A positive answer would verify the conjecture
which in the case is equivalent to the 4-color theorem.
Finally, we indicated that the class of Eulerian graphs can be of interest beyond graph coloring. We characterized the
class of geometric graphs for which a Hopf-Rinov theorem holds as the class of graphs for which all unit spheres are
projective, and especially Eulerian. In two dimensions, these graphs agree with the graphs in which are
Eulerian graphs in the classical sense. Having graphs with geodesic flows allows to carry virtually any question from the
continuum to the discrete. There are questions about geodesic flows and billiards, the structure of caustics
and their relation with curvature, the size of the lengths of minimal geodesics and all within a combinatorial
framework. Finally we have seen that in for , Platonic spheres, spheres for which all unit spheres
are Platonic spheres, are unique and given by the Eulerian cross-polytopes.
The geometry of graphs and especially spheres still needs to be investigated more.
We have seen that the question of “drawing lines and circles” in geometry is fundamental in order to understand
the geometry of geometric graphs, graphs for which the unit spheres are graph theoretically defined graphs.
To “draw lines” we need to have an exponential map which is globally defined and unique. This leads to mild
restrictions of unit spheres which are however not as severe as we just ask for a projective structure on all
The most prominent question remains embedding question. Can any -dimensional sphere be embedded in an Eulerian
dimensional sphere? Answering this question positively
in dimension would prove the 4 color theorem in a geometric way.
In higher dimensions it would lead to the conjectured bound that all -spheres are either Eulerian spheres
or spheres which can be colored by colors.
And since two dimensional manifolds can be embedded in the closed 4-dimensional Euclidean ball in such a way that the complement intersected with the interior is simply connected, one can expect that all to have chromatic number 3,4 or 5. The reason is that orientable surfaces like the torus can be embedded into the three sphere, the boundary of the four dimensional ball whose interior is simply connected. In the non-orientable case, we need the interior of a Möbius strip to temporarily leave the boundary 3 sphere and “hang out” into the four dimensional interior to make a turn, but this keeps the interior simply connected. Coloring the four-dimensional inside with 5 colors now colors also the surface with 5 colors.
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