SELF-DUAL MAPS III PROJECTIVE LINKS LUIS MONTEJANO1 JORGE L. RAM IREZ ALFONS IN2 AND IVAN RASSKIN Abstract. In this paper we present necessary and sucient combinatorial conditions for

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SELF-DUAL MAPS III: PROJECTIVE LINKS
LUIS MONTEJANO1, JORGE L. RAM´
IREZ ALFONS´
IN2, AND IVAN RASSKIN
Abstract. In this paper, we present necessary and sufficient combinatorial conditions for
a link to be projective, that is, a link in RP3. This characterization is closely related to
the notions of antipodally self-dual and antipodally symmetric maps. We also discuss the
notion of symmetric cycle, an interesting issue arising in projective links leading us to an
easy condition to prevent a projective link to be alternating.
1. Introduction
This paper is a continuation of the work [7] where the notions of antipodally self-dual and
antipodally symmetric maps were studied and the work [8] where these notions were applied
to investigate questions concerning symmetry and amphicharility of links. It turns out that
the above notions fit also nicely in order to understand better projective links, that is, links
in RP3.
Projective links have been studied in different contexts : in connection with the twisted
Alexander polynomial [5] and also in relation with unknotting issues [9] and possibly with
3-manifolds [10, Chapter IX]. In [2], Drobotukhina presented the analogue of the Jones
polynomial for projective links and then used it in [3] to give a classification of projective
links with at most six crossings.
In this paper, we present necessary and sufficient combinatorial conditions for a link to be
projective. The latter was done by using a characterization of projective links in terms of
some special embeddings in 3-space invariant under negative inversions.
In the next section we overview some basic notions of knots, projective links and maps
needed for the rest of the paper. In Section 3, we present our new approach and the above
mentioned characterizations. In Section 4, we discuss the notion of symmetric cycle, an
interesting issue arising in projective links leading us to an easy condition to prevent a
projective link to be alternating.
2. Knots and maps : preliminaries
2.1. Knots background. We refer the reader to [1] of [6] for standard background on knot
theory.
Alink with kcomponents consists of kdisjoint simple closed curves (S1) in R3. A knot
Kis a link with one component. A link diagram D(L) of a link Lis a regular projection of
Linto R2in such a way that the projection of each component is smooth and at most two
curves intersect at any point. At each crossing point of the link diagram the curve which
2010 Mathematics Subject Classification. Primary 57M15, 57K10.
Key words and phrases. Self-dual Maps, Projective Links.
1Partially supported by CONACyT 166306 and PAPIIT-UNAM IN112614.
2Partially supported by grant PICS07848 and INSMI-CNRS.
1
arXiv:2210.04053v1 [math.GT] 8 Oct 2022
goes over the other is specified. A shadow of a link diagram Dis a 4-regular graph if the
over/under passes of Dare ignored. Since the shadow is Eulerian (4-regular) then its faces
can be 2-colored, say with colors black and white. We thus have that each vertex is incident
to 4 faces alternatively colored around the vertex, see Figure 1.
Figure 1. (From left to right) A diagram of the Trefoil, its shadow with a
2-colored faces (vertices on white crossed circles), corresponding Black graph
(bold edges and black circles) and White graph (dotted edges and white cir-
cles).
Given such a coloring, we can define two graphs, one on the faces of each color. Let
BDdenote the graph with black faces as its vertices and two vertices are joined if the
corresponding faces share a vertex (BDis called the checkerboard graph of D). We define
the graph WDon the white faces of the shadow analogously. We notice that med(WD) is
exactly the shadow of Dand notice that med(BD) and med(WD) are the same.
An edge-signed planar graph, denoted by (G, SE), is a planar graph Gequipped with a
signature on its edges SE:E→ {+,−}. We will denote by SEthe signature of Gsatisfying
SE(e) = (SE(e)) for every eE. We write S+
E(resp. S
E) when all the signs of SEare +
(resp. ). Given a crossing of the link diagram we sign positive or negative according to the
left-over-right and right-over-left rules from point of view of black around the crossing, see
Figure 2 (Left). The latter induce an opposite signing on each crossing by the same rules
but now from point of view of white around the crossing, see Figure 2 (Right).
+_
+_
Figure 2. (Left) Left-over-right rule from black point of view. (Right) Right-
over-left rule from white point of view.
If the crossing is positive, relative to the black faces, then the corresponding edge is
declared to be positive in BDand negative in WD. Therefore, in this fashion, a link diagram
Ddetermine a dual pair of signed planar graphs (BD, SE) and (WD,SE) where the signs
on edges are swapped on moving to the dual.
Remark 1. A link diagram can be uniquely recovered from either (BD, SE)or (WD,SE).
2
We thus have that given an edge-signed planar graph (G, SE), we can associate to it (in a
canonical way) a link diagram D(L) such that (BD, SE) (and (WD,SE)) gives (G, SE). The
unsigned graph Gis called the Tait graph of the link Lwith diagram D. The construction
is easy, we just consider the med(H) with signatures on the vertices (induced by the edge-
signature SEof G). The desired diagram, denoted by D(G, SE), is obtained by determining
the under/over pass at each crossing according to Left-over-right (or Right-over-left) rule
associated to the sign of the corresponding edge of G, see Figure 3.
+
+
_
_
Figure 3. (From left to right) diagram Dof the Hopf link, denoted by 21,
signed Black graph (BD, SE) and signed White graph (WD,SE).
2.2. Diagrams for links in RP3.Aprojective n-link is the image of a smooth embedding
of ndisjoint copies of S1in RP3.
The 3-dimension real projective space RP3can be defined as the sphere S3with identified
opposite points. Since S3consists of two half-spheres then we can restrict ourselves to the
upper hemisphere of S3and merely identify antipodal points on the bounding equator. Now,
since each half-sphere is homeomorphic to the ball B3then have that RP3can be obtained
by identifying diametrically opposite points of the boundary S2=B3.
Consequently, any link Lin RP3can be defined as a set of closed curves and arcs in B3
such that the set of endpoints of arcs lies in B3. We say that the link Lin RP3is lifted to
L0in B3. Up to isotopy, we can assume that the images of the poles of B3do not belong to
L0.
A projective link Lcan be represented by projective diagrams that differ from usuals
link diagrams in R3in that they are given not on the plane but in a closed 2-disc, and
the endpoints of arcs at the boundary of the 2-disc are divided into pairs of diametrically
opposite points.
More precisely, let π:L0δbe the projection of L0to the equatorial disc ∆ B3defined
by
π(x) = Cx
where CxB3is the semicircle passing through xand the poles of the ball. Up to a small
isotopy, we can assume that Lsatisfies the following general position properties:
a) the image π(L0) does not contain any cusp, tangency point or triple point,
b) L0is a smooth submanifold of B3intersecting transversally the boundary sphere B3
c) there do not exist 2 points L0B3projecting to the same point under π.
We thus have that a link in RP3give rise a projective diagram by projecting to the
equatorial disc B2. Conversely, given a projective diagram regarding B2as the equatorial
3
disc of such a representation of RP3. At each crossing, the upper arc is pull up (and the
lower one is pull down) in order to obtain a nonintersecting curve lying inside B3. The
identification of antipodal points lying on the boundary sphere B3gives rise to a link in
RP3.
a b
a
b
ab
ba
Figure 4. Nonintersecting curves inside B3(induced by a link in RP3) and
its projective diagram in RP2.
In Table 1 we present the firs 14 nontrivial projective links among the 111 projective links
with at most 6 crossings appearing in [3, Table of links in RP3, page 102].
Table 1. First nontrivial projective links.
We notice that any projective diagram in RP2arises a projective link. However, it may
happens that two such diagrams lead to the same projective link.
4
摘要:

SELF-DUALMAPSIII:PROJECTIVELINKSLUISMONTEJANO1,JORGEL.RAMIREZALFONSIN2,ANDIVANRASSKINAbstract.Inthispaper,wepresentnecessaryandsucientcombinatorialconditionsforalinktobeprojective,thatis,alinkinRP3.Thischaracterizationiscloselyrelatedtothenotionsofantipodallyself-dualandantipodallysymmetricmaps.W...

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