The 10 antipodal pairings of strongly involutive polyhedra on the sphere
Abstract.
It is known that strongly involutive polyhedra are closely related to self-dual maps where the antipodal function acts as duality isomorphism. Such a family of polyhedra appears in different combinatorial, topological and geometric contexts, and is thus attractive to be studied. In this note, we determine the 10 antipodal pairings among the classification of the 24 self-dual pairings of self-dual maps . We also present the orbifold associated to each antipodal pairing and describe explicitly the corresponding fundamental regions. We finally explain how to construct two infinite families of strongly involutive polyhedra (one of them new) by using their doodles and the action of the corresponding orbifolds.
1. Introduction
A polyhedron is a planar graph that is simple (without loops and multiple edges) and 3-connected. A face of an embedding of a planar graph is a region bounded by a cycle . We say that a vertex belongs to a face , denoted by , if is in the cycle . Note that every edge borders exactly two faces. The dual of , denoted by , is defined as follows: Each face in is a vertex in and two vertices in are adjacent if and only if the faces share an edge in . A polyhedron is said to be self-dual if there is an isomorphism of graphs . This isomorphism is called a duality isomorphism, and it will be called a strong involution if it satisfies the following conditions:
For each pair of vertices, if and only if and
For every vertex , we have that .
We say that a self-dual polyhedron is strongly involutive if it admits a strong involution. The above conditions are the combinatorial counterpart (in the 3-dimensional case) of a more general geometric object called strongly self-dual polytopes, introduced by Lovász [9], see also [5]. Strongly involutive polyhedra are relevant in different contexts: they are related to convex geometric problems such as the well-known Vázsonyi’s problem [4, 6], with ball polyhedra [1, 7, 16], the chromatic number of distance graphs on the sphere [9], the Reuleaux polyhedra [8, 11], constant width bodies [10] and more recently in relation with questions concerning the symmetry as well as the amphicheirality of knots [13] and projective links [14].
There are known infinite families of strongly involutive polyhedra [12, Propositions 1, 2 and 3 and Theorem 3]. Figure 1 illustrates two simple examples.

Strongly involutive isomorphisms are closely related to the notion of antipodal isometries in the 2-sphere.
A map is the image of an embedding of into where the set of vertices is a collection of distinct points in and the set of edges is a collection of arcs joining pairs of points in satisfying that for any pair of arcs, say and , we have that is either empty or an endpoint of one of the arcs. Any embedding of the topological realization of into partitions the 2-sphere into simply connected regions of called the faces of the embedding.
Recall that is the group formed by the set of all automorphisms of (i.e., the set of isomorphisms of into itself) and let be the set of all duality isomorphisms of into . We notice that is not a group since the composition of any two of them is an automorphism. Let us suppose that is a self-dual map so that there is an isomorphism . Following with the correspondence gives a permutation on which preserve incidences but reverses dimension of the elements. The collection of all such permutations generates a group in which the automorphism group is contained as a subgroup of index 2.
It is known [15, Lemma 1] that for a given map there is a homeomorphism of to itself such that for every we have that where is the group of isometries of the 2-sphere. In other words, any planar graph can be drawn on the 2-sphere such that any automorphism of the resulting map acts as an isometry of the sphere. This was extended in [15] by showing that given any self-dual planar graph and its dual can be drawn on the 2-sphere so that is realized as a group of spherical isometries.
In [2, Theorem 9] (see also [12, Corollary 2]), it was proven that if is strongly involutive then the corresponding isometry is the antipodal function , .
The couple is called the self-dual pairing of the map . In [15], all self-dual maps were enumerated and classified. In the notation of [3, page 36-38] the 24 possible pairings are:
- among the infinite classes and with positive integer, or
- among the special pairings and .
In Section 2, we classify the self-dual pairings that correspond to antipodal isometries, that is, self-dual pairings that give rise to strongly involutive polyhedra.
Theorem 1.
Every strongly involutive map corresponds to one of the following self-dual pairings: for even; for odd, .
The self-dual pairings given in Theorem 1 will be called antipodal pairings. We shall also present a short description of the orbifold associated to each antipodal pairing. We do so by explicitly giving the fundamental region for each group and its generators.
In Section 3, we study the doodle (the map restricted to its fundamental region) of two special families of strongly involutive polyhedra: the -multi hyperwheels (a new family of strongly involutive polyhedra) and the -multi wheels. We explain how these families can be constructed from their doodle via the action of the corresponding orbifold. We finally end with some concluding remarks.
2. Antipodal pairings
2.1. Spherical isometries
We quickly recall some notions on the group of spherical isometries (we refer the reader to [3] for further details and where our notation is taken from). An isometry of is either a rotation or a reflection or a composition of these two. Let be the group of isometries of the 2-sphere. We remark that any orientation reversing isometry is either a reflection or a product of three reflections. Also, it can be checked that is generated by only reflections. Moreover, any isometry is a product of at most three reflections:
[one reflection] Let be a plane passing through the center of . The reflection w.r.t. is an involutive isometry and therefore of order 2. This group is denoted by .
[two reflections] Let and be two planes with angle . The reflection and w.r.t. these planes generate the group (isomorphic to the dihedral group ) having presentation .
[three reflections] Let and be three planes inducing a spheric triangle with angles and , denoted by .

It is known that the sum of the angles of a spheric triangle is strictly larger that , therefore implying that . We take , obtaining that yielding to . By analyzing the latter, it can be found that the possible cases are :
- (corresponding to the tetrahedron),
- (corresponding to the cube and octahedron),
- (corresponding to the dodecahedron and icosahedron),
- (corresponding to a diamond polyhedron which dual is a prism with a -polygon as a base).
The group or is defined by having as a fundamental region the spherical triangle with angles and . Each of these groups has a rotational group consisting only of the possible rotations generated by pairs of reflections:
- The rotational subgroup of , consisting of the powers of , is denoted by (clearly is the trivial group),
- the rotational subgroup of , generated by the rotations and , is denoted by (these subgroups are of order 2),
- the rotational subgroup of when is even, generated by which is a rotation of order followed by the reflection , is denoted by or (these subgroups are of order 2),
- the rotational subgroup of , generated by , is denoted by (which turns out to be a cyclic group of index 2) generated by the rotatory reflection .
2.2. Detecting antipodal pairings
We first present the following lemma that identifies which groups contain the antipodal function.
Lemma 1.
Let be the antipodal function. Then,
-
(1)
for any positive integer .
-
(2)
for any positive integer .
-
(3)
if and only if or and is even.
-
(4)
for any positive integers and .
-
(5)
or if and only if or , is even and is odd.
-
(6)
if and only if , is even and is odd.
Proof. Since is an isometry without fixed points then (1) is verified. Moreover, since inverts orientation then (2) and (4) hold. Notice that (2) also follows since is a subgroup of . We can establish (3) by observing that any prism has central symmetry if and only if it has a polygon with an even number of sides as a base and similarly we see that the cube and the octahedron are the only platonic solids on the list with central symmetry.
In order to illustrate the proof of (5) and (6), let us see that . The group is generated by the reflections and such that . The subgroup is generated by the reflection and the rotation . The element is a rotatory reflection or a step, satisfying and (See Figure 3).

In the general case , if is even and is odd, then we have that and . Conversely, if , then is even and must be odd in order to express as a product of generators with an odd number of reflections, otherwise would preserve orientation, which is not the case. From this fact we can conclude also 6 since is precisely the cyclic group generated by the step . Finally, by considering (3), we just need to check the subgroup , which is generated by a reflection and a rotation . In this case, it can be verified that .
We may now prove Theorem 1.
Proof of Theorem 1. We may use Lemma 1 to identify those self-dual pairings such that and . In Table 1 we examine each case.
DualAut | Dual)? | Aut? |
---|---|---|
, -even | (3) | (1) |
(4) | (2) | |
, -odd | (5) | (1) |
, -even | (5) | (2) |
, -odd | (6) | (2) |
(1) | (1) | |
(1) | (2) | |
(1) | (1) | |
(2) | (1) | |
(2) | (2) | |
(3) | (4) | |
(3) | (5) | |
(3) | (5) | |
(3) | (3) | |
(4) | (4) | |
(5) | (4) | |
(5) | (6) | |
(5) | (6) | |
(5) | (6) | |
(5) | (5) | |
(5) | (1) | |
(3) | (3) | |
(4) | (4) | |
(5) | (4) |
2.3. Orbifolds
Given and a point we have that , that is, acts as an evaluation function in . The orbit of is the set of regions congruent to covering the sphere (the number of such regions is as many as the elements in . The stabilizer of consist of all the elements in fixing . An orbifold is defined as the fundamental region together with the points with nontrivial stabilizer.
Let be a self-duality pairing where and are finite groups of isometries of the sphere, such that is an index 2 subgroup of . In order to describe each orbifold we need fundamental regions and corresponding to the groups and , respectively as well as their corresponding generators. We observe that since is an extension of index 2, region is contained in and it will have half of its area.
In what follows we describe the fundamental regions for each antipodal self-dual pairing. We have drawn with :
- a thick line the singular elements of , i.e., sets of fixed points under the action of
- a double line the singular elements of
- continuous lines denote reflection lines
- dotted lines delimit the regions without considering a reflection and
- points marked with a circle denote a center of rotation by the marked angle.
is a group generated by reflections and through the thick lines. The fundamental region is a bigon formed by these lines. is generated by reflections and and its fundamental region is a triangle with angles . |
![]() |
The fundamental region is a bigon formed by lines with an angle and , where is a rotation for . The extension , being the reflection through the equator. |
![]() |
The fundamental region is a bigon with angle and . The region is a triangle with angles and , where is a rotation by . |
![]() |
The fundamental region consists of two triangles disposed in a way one can be obtained from the other by a rotatory reflection. This rotatory reflection is the composition of the reflection through the “I” mark and the rotation around the “C”. Then where is the rotatory reflection with order , and . |
![]() |
In this case is an equilateral triangle with internal angles of ; , is a rotation by in the midpoint of each of the sides and where is the reflection through a line and . |
![]() |
and . Here is a reflection through a line and . |
![]() |
, where is a rotatory reflection of order 4. , with a reflection through the equator and a rotation by in the north pole. Note that . |
![]() |
In this case is one hemisphere and , where is the reflection through the equator, and , where is the rotation by through the marked point (north or south pole). |
![]() |
and . Here is the reflection through the bisector or the right angle in the first triangle. |
![]() |
and . In this case, is a quadrilateral. is a reflection through one of the thick lines (the other one can be obtained by rotation), and is the rotation around the thick circle. is a triangle and is the reflection in the “horizontal” line and is the rotation around the circle with double line. |
![]() |
3. Constructing strongly involutive maps
Let us consider the orbifold of a map consisting of a fundamental region with the singular points. By construction, we have that the orbit of is a set of congruent regions covering the 2-sphere. Given a map , we may consider the part of the map which is drawn in the fundamental region and does not have any other symmetry. We call this restriction the doodle of .
Next we describe how two involutive polyhedra are constructed from their doodle by means of the action of the duality group .
3.1. The -multi hyperwheel
Let and be natural numbers. The -multi hyperwheel with levels is the graph consisting of the cycles:
as well as a vertex called the cusp and the edges and for ; see Figure 4.

If then is a strongly involutive self-dual polyhedron. Indeed, let us check this for where the strong involution is given as follows:
Note that , as duality isomorphism, associates the vertex set of the dual face to each point , while, as an isometry of the sphere, it associates the antipodal point to each point .
We may now construct the 4-multi hyperwheel which is just the 4-hyperwheel as illustrated in Figure 1 (right) by means of the action of its antipodal pairing. Figure 5 gives the fundamental region and its doodle. This doodle can generate a family of self-dual polyhedra whose pairing is .

The external circle with dotted line represents the north pole, the circle with double line represents the equator and the central point is the south pole. The graphs and appear in blue and red, respectively and there is a black vertex in each intersection of an edge in with an edge in . The join of these graphs (including the black vertices) is the graph of squares whose all faces are quadrilaterals of the form for some and .
Remark 1.
Let be any element in . We have that preserves squares. Furthermore, if and only if is color preserving; if and only if is color reversing. In any case, black vertices are mapped to black vertices.
We suppose that is the reflection in a spherical line which intersects the square . If then must pass through and and must interchange and . In this case, the reflection in the equator is a duality isomorphism since it interchanges vertices blue and red. Each automorphism can be obtained as a composition of reflections in four lines through the poles. The reflections through these lines generates the group and each one of them works as an automorphism, so we can write . The group is and it can be obtained by adding the reflection through the equator. In this way, is generated by the reflections in three planes and . Planes and intersect with angle and we can assume they are vertical planes through the poles, while is the equatorial plane and it forms angles of with each . The fundamental region is the spherical triangle with angles . The self-dual pairing for this graph is and it is determined by this triangle with three isometries: two reflections in (black lines) and one in (double line).

The above construction can be extended for each even and any : For and we have the doodle of (Figure 5). Then for and we have the doodles and the graphs in Figure 6. Here the doodle is drawn on the region between two planes forming an angle : the fundamental region of the group .
In Figure 7, we consider the embedding of both: the graph in blue and its dual graph in red. Here the reflection through the double line interchanges colors blue and red since it is a duality isomorphism of . If we let the group act on the sphere, we will have a generalization of the -multi hyperwheel. Figure 7 illustrates the case and .

3.2. The -multi wheel
Let and be natural numbers. The -multi wheel with levels is the graph consisting of the cycles
a central vertex called the cusp and edges . Figure 9 illustrates .

We notice that is actually the -wheel (a graph consisting of a -cycle with a center joined to each vertex of the cycle).
If then is a strongly involutive self-dual polyhedron. Indeed, let us check this for where the strong involution is given as follows:
We may now construct the 3-multi wheel by means of the action of its antipodal pairing. Figure 5 gives the fundamental region and its doodle. This doodle can be naturally extended to generate a family of self-dual polyhedra whose pairing is .
Let us consider an isometric embedding of the graph given in Figure 9.

In this embedding, the vertices and are in a circle while and are in another circle. These circles are concentric to the center , which we can assume to be the south pole. The red vertices correspond to the dual graph and they are also in concentric circles, in this case and are connected with the central vertex located in the north pole (dotted external line in the figure).
We can observe that the reflection on the equator does not work as duality but the rotation by around the circle in double lines in the shaded region is a duality isomorphism. This rotation is color reversing: goes to , the red point goes to and the central vertex goes to . If we call this rotation , then the group is generated by and in Coxeter notation it corresponds to . The duality pairing is .
The above construction can be extended for each odd and any . We can start by restricting the graph , which is the 5-wheel, to a fundamental region and then we can add more levels in order to obtain a simple, planar and 3-connected graph. See Figure 10.

In Figure 11 we have a fundamental region for the group . It is between two vertical planes forming an angle of . The circle in the center of the region denotes a rotation by . This rotation sends the blue lines in the doodle to the red lines in the doodle and viceversa since it is a duality isomorphism in the pairing . If we let act on we may obtain .

4. Concluding Remarks
In [2, Theorem 6], the authors showed that if is a strongly involutive polyhedron then there always exists an edge such that is also an strongly involutive polyhedron where is the strong involution and (resp. ) denotes the deletion (resp. contraction) of an edge in . It can be checked that the inverse of the delete-contraction operation corresponds to the diagonalization faces of the graph and its dual simultaneously. The latter can be settled as an add-expansion operation from to obtain .
The above implies that all strongly involutive polyhedra can be reduced to a wheel (with an odd number of vertices in the main cycle) by a finite sequence of delete-contraction operations (applied simultaneously each time), see [2, Corollary 7]. We end with the following
Question 1.
Let be a strongly involutive polyhedron and let be the strongly involutive polyhedron obtained from by applying a delete-contraction operation. Can the antipodal pairing of be determined from the antipodal pairing of ? What about the corresponding orbifolds and doodles?
References
- [1] K. Bezdek, Z. Lángi, M. Naszódi and P. Papez, Ball-polyhedra, Disc.& Comp.Geom. 38 (2007), 201–230.
- [2] J. Bracho, L. Montejano, E. Pauli and J.L. Ramírez Alfonsín, Strongly involutive self-dual polyhedra, Ars Math. Contemp. 20 (2021), 143–149.
- [3] H.S.M. Coxeter and W.O.J. Moser, Generators and Relations for Discrete Groups, Ergebnisse der Mathematik und ihrer Grenzgebiete, Bd. 13, Springer Verlag, 1972.
- [4] P. Erdös, On sets of distances of points, Amer. Math. Monthly 53 (1946) 248–250.
- [5] B. Grünbaum and G.C. Shepard, Is selfduality involutory?, Amer. Math. Monthly 95 (1985), 729–733.
- [6] B. Grünbaum, A proof of Vázsonyi’s conjecture, Bull. Res. Council Israel, Sect. A, 6 (1956), 77–78.
- [7] Y. S. Kupitz, H. Martini, and M. A. Perles, Ball polytopes and the Vázsonyi problem, Acta Math. Hungarica 126 (2010), 99–163.
- [8] G. López-Campos, D. Oliveros and J.L. Ramírez Alfonsín, Borsuk and Vázsonyi problems through Reuleaux polyhedra, (arXiv:2308.03889).
- [9] L. Lovàsz, Self-dual polytopes and the chromatic number of distance graphs on the sphere, Acta Sci. Math. 45 (1983), 317–323.
- [10] H. Martini, L. Montejano and D. Oliveros, Bodies of constant width, Birkhäuser (2019).
- [11] L. Montejano, E. Pauli, M. Raggi and E. Roldán-Pensado, The graphs behind Reuleaux polyhedra, Disc.& Comp.Geom. 64(3) (2020), 1013–1022.
- [12] L. Montejano, J.L. Ramírez Alfonsín and I. Rasskin, Self-dual maps I: antipodality, SIAM Disc. Math., 36(3) (2022), 1551–1566.
- [13] L. Montejano, J.L. Ramírez Alfonsín and I. Rasskin, Self-dual maps II : links and symmetry, SIAM Disc. Math., 37(1) (2023), 191–220.
- [14] L. Montejano, J.L. Ramírez Alfonsín and I. Rasskin, Self-dual maps III: projective links, J. Knot Th. and its Ramifications, 32(10) (2023) No 2350066, 22 pp.
- [15] B. Servatius and H. Servatius, The 24 symmetry pairings of self-dual maps on the sphere, Disc. Math. 140 (1995), 167–183.
- [16] K.J. Swanepoel, A new proof of Vázsonyi’s conjecture, J. Comb. Th. Ser. A 115 (2008), 888–892.