The goal of this paper is to determine the braid index of two types of complicated DNA polyhedral links introduced by chemists and biologists in recent years. We shall study it in a more broad context and actually consider so-called Jaeger's links (more general Traldi's links) which contain, as special cases, both four types of simple polyhedral links whose braid indexes have been determined and the above two types of complicated DNA polyhedral links. Denote by and the braid index and crossing number of an oriented link , respectively. Roughly speaking, in this paper, we prove that for any link in a family including Jaeger's links and contained in Traldi's links, which is obtained by combining the MFW inequality and an Ohyama's result on upper bound of the braid index. Our result may be used to to characterize and analyze the structure and complexity of DNA polyhedra and entanglement in biopolymers.
Citation: Cheng X-S, Jin X (2012) The Braid Index of Complicated DNA Polyhedral Links. PLoS ONE 7(11): e48968. doi:10.1371/journal.pone.0048968
Editor: Laurent Kreplak, Dalhousie University, Canada
Received: July 31, 2012; Accepted: October 3, 2012; Published: November 20, 2012
Copyright: © 2012 Cheng, Jin. This is an open-access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are credited.
Funding: XSC was supported by grants from the National Natural Science Foundation of China (number 11101174), Natural Science Foundation of Guangdong Province of China (number S2011040003984) and Foundation for Distinguished Young Talents in Higher Education of Guangdong, China (number LYM11120). XJ was supported by grants from the National Natural Science Foundation of China (numbers 10831001 and 11271307), Natural Science Foundation of Fujian Province of China (number 2012J01019) and the Fundamental Research Funds for the Central Universities (number 2010121007). The funders had no role in study design, data collection and analysis, decision to publish, or preparation of the manuscript.
Competing interests: The authors have declared that no competing interests exist.
The braid index of links has some applications in chemistry and molecular biology. For example, representing knotted hydrocarbon complexes as closed braids  can facilitate the study of their properties. In recent 20 years, many DNA polyhedral links such as DNA cube , DNA tetrahedron , DNA octahedron , DNA truncated octahedron , DNA bipyramid , DNA dodecahedron , DNA icosahedron and buckyballs  etc, have been synthesized in laboratories or schemes for synthesizing them have been designed by chemists and biologists. In addition, several novel types of polyhedral links have also been posed by mathematicians as a potential object to be synthesized. For four types of simple polyhedral links, their braid indexes have been determined in . The purpose of this paper is to determine braid index of another two types of more complicated polyhedral links appeared in , , , ,  and , respectively. We shall study it in a more broad context and actually consider so-called Jaeger's links and more general Traldi's links.
In , Jaeger associated to a plane graph an oriented link diagram by replacing each edge of the graph by an oriented clasp as illustrated in of Figure 1. Then he established a relation between the Tutte polynomial  of the graph and the HOMFLY polynomial ,  of the associated oriented link. Moreover, about one year later, both the construction and the relation were extended by Traldi in , Traldi constructed his oriented link diagram based on a plane graph via replacing each edge by one of four types of oriented clasps and , as illustrated in Figure 1. By assigning four different weights to edges of the plane graph according to the four types of oriented clasps he built a relation between the weighted dichromatic polynomial  of the graph and the HOMFLY polynomial of the associated oriented link.
Formally, let be an oriented link, we call to be a Jaeger's link if , or its reverse, or its mirror image, or its inverse (i.e. the composition of the reverse and the mirror image), has an oriented diagram which can be obtained from a connected plane graph by replacing each edge of the graph by an oriented clasp in Figure 1. According to the above definition, Jaeger's links will be all alternating. Analogously, we call to be a Traldi's link if , or its reverse, has an oriented diagram which can be obtained from a connected plane graph by replacing each edge of the graph by one of four types of oriented clasps in Figure 1. Note that different edges may be replaced by different types of oriented clasps. Traldi's links may not be alternating, say, the link in the Thistlethwaite Link Table . Clearly, Traldi's links contain Jaeger's links as special cases.
The braid index of an oriented link is the minimum number of strings among all closed braid representatives for the given oriented link. We point out that the braid index depends on orientations of links. See Page 215 of . Let be an oriented link. We denote by the braid index of . It is, in general, very hard to determine this geometric and numerical invariant . Let be the HOMFLY polynomial of the oriented link . In  and , Franks, Williams and Morton gave independently a lower bound for the braid index of an oriented link in terms of as follows:(1)where = , and and denote, respectively, the maximal degree and minimal degree of in the polynomial . This inequality is usually called MFW inequality. The MFW inequality was the first known result relating the braid index to the HOMFLY polynomial. To date, we have known that the MFW inequality for many link families is sharp. For example, the inequality is sharp for all torus links, closed positive n-braids with a full twist , 2-bridge links , alternating fibred links  and a certain family of closed positive braids . In this paper we shall prove the sharpness of the MFW inequality for a family of links including Jaeger's links and contained in Traldi's links. We shall make use of the following result obtained by Ohyama in 1993  which states that for a non-splittable oriented link ,(2)where is the crossing number of . In fact, you will see this upper bound and the MFW lower bound coincide for a family of links including Jaeger's links, but do not coincide for general Traldi's links.
Note that many types of polyhedral links are, in fact, Jaeger's links defined above. Four types of simple polyhedral links considered in  are actually all Jaeger's links constructed from subdivisions of (convex) polyhedral graphs or their duals. Note that the dual of a polyhedral graph is also a polyhedral graph and Steinitz's theorem states that a polyhedral graph is a 3-connected simple (i.e. no loops and no multiple edges) planar graph. Thus the result in  can not be used to deal with general Jaeger's links. Roughly speaking, in this paper we prove that for any link in a family including Jaeger's links and contained in Traldi's links and thus extend the result in . This extension enables us to determine the braid index of another two types of more complicated polyhedral links in ,  and  as well as four types of polyhedral links in . It is probable that our result be used to determine braid indexes of new types of polyhedral links to be synthesized in the future. Our research demonstrates that using the braid index or crossing index to describe the complexity of some polyhedral links are equivalent and it may open a door to characterize, analyze the structure and complexity of DNA polyhedra and entanglement in biopolymers.
Before analyzing the braid index of polyhedral links, we give some preliminary knowledge on links, the HOMFLY polynomial, graphs and the dichromatic polynomial.
A knot is a simple closed curve in , i.e. the image of the embedding of into . A link of components is a disjoint union of knots: . A knot is a link with one component. An oriented link is a link with each of its component assigned an orientation. A link diagram is a (regular) projection of a link onto a plane with the under-strand specified by using gaps at each crossing. When the link is oriented, the link diagram will inherit the orientation of the link in a natural way and called oriented link diagram. The crossing number or crossing index of a link , denoted by , is the least number of crossings that occur in any diagram of the link. A diagram with fewest number of crossings for a given link is called a minimal diagram for the link.
An -string braid is a set of strings in a 3-dimensional cube , where , all of which are attached to a horizontal bar at the top and at the bottom such that each , , meets the strings in exactly points. A closed -string braid is a set of strings embedded in such that each , , meets the strings in exactly points. An example is illustrated in Figure 2.
It is clear that a closed -string braid is an oriented link with the convention that we always orient from the top to the bottom. Conversely, Alexander , in 1923, showed that every oriented link in can be represented as a closed -string braid. The braid index for an oriented link is the smallest positive integer such that can be represented as a closed -string braid.
Let be an oriented link. We denote by and the reverse (reversing the orientation of each component of ) and the mirror image of , respectively. Then it is obvious that .
2. The HOMFLY polynomial
The HOMFLY polynomial is an invariant of oriented links, introduced in  and  independently. Now we recall the definition of the HOMFLY polynomial. The HOMFLY polynomial of an oriented link , denoted by , can be defined by the three following axioms .
- is invariant under ambient isotopy of L.
- If is the trivial knot then .
- It satisfies the skein relation: , where , and are link diagrams which are identical except near one crossing where they are as in Figure 3 and are called a skein triple.
It possesses the following basic properties , which imply that .
- If is the reverse of , then .
- If is the mirror image of , then .
Let be a graph. We denote by and the numbers of vertices and edges, respectively, of the graph . A graph is said to be connected if it has a path with two distinct vertices and whenever and is said to be disconnected otherwise. A component of a graph is a subgraph that is connected and is not properly contained in any other connected subgraph of . We denote by the number of components of the graph . An edge of is said to be a bridge if . If has no bridges, is said to be bridgeless. An edge of is said to be a loop if its two end-vertices are the same. Iff has no loops, is said to be loopless. The rank and nullity of the graph is defined to be and , respectively. It is well known that and are exactly the dimensions of cycle space and cut space, respectively, of the graph and hence, are both non-negative integers. See, for example, .
Given a graph and an edge of , we write for the graph obtained from by deleting the edge , and for the graph obtained from by contracting , i.e. deleting firstly and then identifying its two endvertices. A planar graph is a graph which can be embedded in the plane or equivalently, the sphere . A specific embedding of a planar graph is called a plane graph. For undefined notations and terminologies on graph theory, we refer the readers to .
4. The dichromatic polynomial
A weighted graph is a graph together with a function mapping into some commutative ring with unity 1. If is an edge of the weighted graph , then is the weight of the edge . The dichromatic polynomial for weighted graphs was introduced by Traldi in , which is a generalization of the Tutte polynomial for signed graphs introduced by Kauffman in . We point out there are actually several weighted versions of the Tutte polynomial.
The dichromatic polynomial of a weighted graph G can be defined as(3)where the summation is over all edge subsets, , of , and are the number of components and the nullity, respectively, of the spanning subgraph , induced by , of . It can also be defined by using the following recursive relations:
- If is an edgeless graph with vertices
- If is a loop of , then
- If is not a loop of , then .
Just as the Tutte polynomial, it also has a spanning tree expansion and we do not explain it here.
Now we start to analyze the braid index of polyhedral links. We first consider a family of Jaeger's links.
Let be a connected plane graph. Let be the oriented link diagram constructed based on by covering each edge of with oriented clasp in Figure 1. Oriented link diagrams and can be defined similarly. Let be the oriented link diagram constructed based on by covering some edges of with oriented clasp and other edges with oriented clasp in Figure 1. Oriented link diagrams can be defined similarly. Note that (resp. ) contains (resp. ) as special cases. More generally, is defined to be the oriented link diagram obtained from by covering each edge with one of four types of clasps and . In , Traldi obtained the following general formula.
Let be a plane graph. Let be the Traldi's oriented link diagram. Let the weight of the edge replaced by oriented clasp and be , , and , respectively. Then(4)where and are numbers of edges of which are replaced by oriented clasp and , respectively.
The following theorem is a main theoretical tool for determining the braid index of polyhedral links.
Note that is the mirror image of some and taking the mirror image does not change the braid index and the crossing index. It suffices for us to prove Eq. (5). When is bridgeless and loopless, it is not hard to observe that is a connected alternating oriented link diagram without nugatory crossings. According to the famous result , ,  due to Kauffman, Murasugi and Thistlethwaite: A connected alternating link diagram without nugatory crossings is minimal, we obtain that(7)where is the link that the link diagram represents. In addition, by a result  due to Menasco that states that a link with an alternating diagram will be non-splittable if and only if the diagram is connected, we know that is non-splittable. Thus, by Eq. (2), we have(8)
where and are numbers of edges in covered by clasps of types and , respectively. It is clear that .
Now we compute the highest and lowest degrees in of Eq. (9). Note that the power of is . Thus we haveThe third equation holds since attains maximality if and only if because of is bridgeless. Similarly, we haveThe second equation holds since attains maximality if and only if since is loopless. Thus,Hence, by Eq. (1), we obtain(10)
By checking the proof of Theorem 2, we find that the condition “loopless” is actually not necessary for the special case . Hence, Eq. (11) holds. Eq. (12) follows from Eq. (11) and the fact . Let be a connected loopless plane graph and be the planar dual of . Then is connected and bridgeless. Note that (see Figure 4 for an example) and and reversing orientations do not change braid index and crossing index. Hence, Eqs. (13) and (14) hold. By the definition of a Jaeger's link , we know that there is a connected plane graph such that is equivalent to one of the four links: , , and . It will suffice to prove that for any connected plane graph . Firstly, for any connected bridgeless plane graph . Secondly, if has bridges, let be the connected plane graph obtained from by contracting all bridges of . Note that is equivalent to via untwisting oriented clasps covering bridges. Hence, we have .
To conclude the section, we point out that the braid index of general Traldi's links (even for alternating Traldi's links) can not be determined similarly since the upper and lower bounds are not always equal in general. An example of alternating Traldi's links, denoted by , is shown in Figure 5 which is constructed from a theta graph by replacing edges by oriented clasp and by clasp . On the one hand, by using the software KnotGTK, we obtain(16)and hence, . On the other hand, we have . Therefore,(17)
It is obvious that by the Corollary the braid index of four types of polyhedral links (see Fig. 2 of ) can be determined. In this section, we determine the braid index of two types of complicated DNA polyhedral links. However, braid indexes of these two new types of polyhedral links can not be obtained by the previous result in . You will see these new types of polyhedral links are all alternating and hence their crossing numbers are easily obtained. By the Corollary, in order to obtain the braid index, we only need to show that these links are Jaeger's links, and equivalently to find their associated plane graphs. Note that two strands of DNA have antiparallel orientations which are consistent with Jaeger's orientations. For simplicity, we do not draw orientations in the following any more.
1. Double crossover DNA polyhedral links
Recent years, in , , , , , the authors, in laboratory, designed and synthesized some fancy double crossover DNA polyhedra, such as DNA tetrahedron, cube, octahedron, dodecahedron, icosahedron and buckyball, by covering each vertex of degree of the polyhedron by “-point star motif (tiles)” and through sticky-end association between the tiles. The “-point star motif” has an -fold rotational symmetry and consists of single strands: a long repetitive central DNA strand (colored red and yellow), identical medium DNA strands (colored green) and identical short DNA strands (colored black). The colored yellow part at the center of the motif represents unpaired DNA single-strands whose lengths can be adjusted to change bending degree of the whole structure. See Figure 6.
We point out in Figure 6 the tiles are a little different in the ends of tiles from the actual assemblies of such DNA polyhedra. For actual assemblies, we refer the reader to Fig. 1 of  for DNA tetrahedron, dodecahedron and buckyball, Fig. 4 of  for DNA cube, Fig. 1 of  for DNA octahedron and Fig. 4(f) of  and Fig. 1 of  for DNA icosahedron. However, one will obtain the same polyhedron links based on our drawings as actual assemblies, and hence do not affect the analysis of their braid indexes.
Now we take double crossover DNA cube as an example to show double crossover DNA polyhedra are all Jaeger's links. The planar form of double crossover DNA cube link and its associated plane graph are shown in Figure 7 (upper and right) and (lower), respectively. In general, the associated plane graph can be obtained from the polyhedron by the following steps:
Step 1: Truncating the polyhedron , i.e. cutting each corner of the polynhedron , we obtain a polyhedral graph .
Step 2: Inflating edges of corresponding to edges of , i.e. converting a single edge into two parallel edges, we obtain a plane graph .
Step 3: Subdividing each edge of by inserting a vertex, we obtain the associated graph .
Let be a polyhedron with edges. Then, by simple calculation, the associated plane graph has edges and thus the braid index of the corresponding double crossover DNA polyhedral link is .
2. Cycle-crossover polyhedral links
This type of polyhedral links was introduced in , designed as a potential object for synthesising, which can be constructed from a polyhedron by replacing each edge of the polyhedron by a “cycle-crossover” and replacing each vertex of degree by an -branched curve. See Figure 8. The planar form of the cycle-crossover cube link is shown in Figure 9 (upper and right) and its associated plane graph is shown in Figure 9 (lower).
In general, cycle-crossover polyhedral links are all Jaeger's links. The associated plane graph can be obtained from the polyhedron by the following steps:
Step 1: Computing the planar dual of , we obtain a plane graph
Step 2: Inflating edges of , i.e. converting a single edge into several parallel edges, we obtain the associated graph .
In this case suppose that the total lengths of cycle-crossovers used to construct cycle-crossover polyhedral links are . Then the associated plane graph has edges and thus the braid index of the corresponding cyle-crossover DNA polyhedral link is .
Firstly, note that the two associated plane graphs in Figures 7 and 9 are both not subdivisions of polyhedral graphs and for both types of polyhedral links. This means that the method used in  can not be used here. Secondly, it is easy to find that the braid index of two types of complicated polyhedral links does not depend on the structure of the polyhedron. Thirdly, as the referee points out that there are two types of DNA cube: 4 turns and 4.5 turns. See Figure 4 and Figure 1, respectively, of , we only consider the 4-turn DNA cube in this paper. It deserves to study the braid index of 5-turn DNA cube and more general 5-turn DNA polyhedra. Finally, in fact Theorem 2 is more powerful than it has been used, and hence may be used to determine the braid index of more complicated polyhedral links in the future.
Conceived and designed the experiments: XSC XJ. Performed the experiments: XSC XJ. Analyzed the data: XSC XJ. Contributed reagents/materials/analysis tools: XSC XJ. Wrote the paper: XSC XJ.
- 1. Cox MA, Hughes TS, Ellis-Monaghan JA, Mondanaro KR (2008) Hydrocarbon links in an octet truss. J Math Chem 43: 874–891.
- 2. Chen J, Seeman NC (1991) Synthesis from DNA of a molecule with the connectivity of a cube. Nature 350: 631–633.
- 3. Goodman RP, Berry RM, Turberfield AJ (2004) The single-step synthesis of a DNA tetrahedron. Chem Commun 12: 1372–1373.
- 4. Shih WM, Quispe JD, Joyce GF (2004) A 1.7-kilobase single-stranded DNA that folds into a nanoscale octahedron. Nature 427: 618–621.
- 5. Zhang Y, Seeman NC (1994) The construction of a DNA truncated octahedron. J Am Chem Soc 116: 1661–1669.
- 6. Erben CM, Goodman RP, Turberfield AJ (2007) A Self-Assembled DNA Bipyramid. J Am Chem Soc 129: 6992–6993.
- 7. Zimmermann J, Cebulla MPJ, Mönninghoff S, Kiedrowski GV (2008) Self-Assembly of a DNA Dodecahedron from 20 Trisoligonucleotides with C3h Linkers. Angew Chem Int Ed 47: 3626–3630.
- 8. He Y, Ye T, Su M, Zhang C, Ribbe AE, et al. (2008) Hierarchical self-assembly of DNA into symmetric supramolecular polyhedra. Nature 452: 198–202.
- 9. Cheng XS, Jiang X, Dai H (2012) The braid index of polyhedral links. J Math Chem 50: 1386–1397.
- 10. Lin C, Liu Y, Yan H (2009) Designer DNA Nanoarchitectures. Biochemistry 48 (8) 1663–1674.
- 11. Zhang C, Ko SH, Su M, Leng Y, Ribbe AE, et al. (2009) Symmetry Controls the Face Geometry of DNA Polyhedra. J Am Chem Soc 131: 1413–1415.
- 12. Zhang C, Su M, He Y, Zhao X, Fang P, et al. (2008) Conformational flexibility facilitates selfassembly of complex DNA nanostructures. Proc Natl Acad Sci USA 105: 10665–10669.
- 13. He Y, Su M, Fang P, Zhang C, Ribbe AE, et al. (2010) On the chirality of self-assembled DNA octahedra. Angew Chem Int Ed 49: 748–751.
- 14. Cheng XS, Zhang HP, Hu G, Qiu WY (2010) The architecture and Jones polynomials of cycle-crossover polyhedral links. MATCH Commun Math Comput Chem 63: 637–635.
- 15. Jaeger F (1988) On Tutte polynomials and link polynomials. Proc Amer Math Soc 103: 647–654.
- 16. Tutte WT (1954) A contribution to the theory of chromatic polynomials. Canad J Math 6: 80–91.
- 17. Freyd P, Yetter D, Hoste J, Lickorish WBR, Millett K, et al. (1985) A new polynomial invariant of knots and links. Bull Amer Math Soc (NS) 12: 239–246.
- 18. Przytycki JH, Traczyk P (1987) Invariants of links of Conway type. Kobe J Math 4: 115–139.
- 19. Traldi L (1989) A dichromatic polynomial for weighted graphs and link polynomials. Proc Amer Math Soc 106: 279–286.
- 20. Math.toronto.edu. Available: http://katlas.math.toronto.edu/wiki/The Thistlethwaite Link Table. Accessed 2012 Oct 11.
- 21. Murasugi K (1996) Knot theory and its applications. Boston: Birkhauser. 341 p.
- 22. Franks J, Williams RF (1987) Braids and the Jones polynomial. Trans Amer Math Soc 303: 97–108.
- 23. Morton HR (1986) Seifert circles and knot polynomials. Math. Proc. Cambridge Philos Soc 99: 107–109.
- 24. Murasugi K (1991) On the braid index of alternating links. Trans Amer Math Soc 326: 237–260.
- 25. Nakamura T (2004) Notes on the braid index of closed positive braids. Topology Appl 135: 13–31.
- 26. Ohyama Y (1993) On the minimal crossing number and the braid index of links. Canad J Math 45: 117–131.
- 27. Alexander JW (1923) A lemma on systems of knotted curves. Proc Natl Acad Sci USA 9: 93–95.
- 28. Cromwell PG (2004) Knots and Links. Cambridge University Press. 328 p.
- 29. Bondy JA, Murty USR (1976) Graph theory with applications. London and Basingstoke: The Macmillan Press Ltd. 264 p.
- 30. Kauffman LH (1989) A Tutte polynomial for signed graphs. Discrete Appl Math 25: 105–127.
- 31. Kauffman LH (1987) State models and the Jones polynomial. Topology 26: 395–407.
- 32. Thistlethwaite MB (1987) A spanning tree expansion of the Jones polynomial. Topology 26: 297–309.
- 33. Murasugi K (1987) Jones polynomial and classical conjectures in knot theory. Topology 26: 187–194.
- 34. Menasco W (1984) Closed incompressible surfaces in alternating knot and link complements. Topology 23 (1) 37–44.