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The group Gn2G_{n}^{2} with a parity and with points

S.Kim S.Kim, Bauman Moscow State Technical University, ksj19891120@gmail.com
Abstract.

In [8] Manturov studied groups GnkG_{n}^{k} for fixed integers nn and kk such that k<nk<n. In particular, Gn2G_{n}^{2} is isomorphic to the group of free braids of nn-stands. In [6] Manturov and the author studied an invariant valued in free groups not only for free braids but also for free tangles, which is derived from the group Gn2G_{n}^{2}. On the other hands, in [3] Manturov and Fedoseev studied groups Br2nBr_{2}^{n} of virtual braids with parity and groups BrdnBr_{d}^{n} of virtual braids with dots. They showed that there is homomorphism from Br2nBr_{2}^{n} to BrdnBr_{d}^{n} and proved the following statement:

if two braids with parity are equivalent as braids with dots, then they are equivalent as braids with parity.

By the statement it is deduced that a parity of the braid can be represented by a geometric object, dots on strands.

In this paper we study Gn2G_{n}^{2} with structures, which are corresponded to parity and points on a braid, which are denoted by Gn,p2G_{n,p}^{2} and Gn,d2G_{n,d}^{2}, respectively. In section 3, it is proved that there is a monomorphism from Gn2G_{n}^{2} to Gn,p2G_{n,p}^{2} and that there is a monomorphism from Gn,p2G_{n,p}^{2} to Gn,d2G_{n,d}^{2}. By the homomorphism from Gn2G_{n}^{2} to Gn,p2G_{n,p}^{2}, it can be deduced that a given parity of a braid has geometric representation, which is the number of points on the braid. In section 4, it can be proved that for each element β\beta in Gn,d2G_{n,d}^{2}, an element in Gn+12G_{n+1}^{2} obtained by adding another strand by tracing points on β\beta. That is, a parity of free braid of nn-stands is represented not only by points on strands, but also by an n+1n+1-th strand. Conversely, for a braid of n+1n+1-strands, a braid of nn-strands is obtained by deleting one strand of the braid of n+1n+1-strand. Finally, we will simply discuss about the way to adjust the previous observations to know whether a given braid is Brunnian or not.

1. Introduction

In [8], Manturov studied groups GnkG_{n}^{k} given by the group presentation, from which many invariants for knots and dynamical systems are derived. In [10], V.O.Manturov and I.M.Nikonov found that pure braids groups are embedded in GnkG_{n}^{k} and constructed invariants valued in free product of cyclic groups. Tangles are significant generalization of braids and we have the following question : is it possible to generalize invariants, which are asserted, to the case of tangles. By Gn2G_{n}^{2} analogously tangles can be studied. In [6], the invariants valued in free groups are extended to the case of free tangles. The groups Gn2G_{n}^{2} which are simplest case of the GnkG_{n}^{k} are known as free braid groups of nn-strands, which are known as other names, see [1] and [2].

On the other hands, in [3] V.O.Manturov and D.A.Fedoseev studied virtual braids group Br2nBr_{2}^{n} with parity and virtual braids group BrdnBr_{d}^{n} with dots. They showed that there is a homomorphism hh from Br2nBr_{2}^{n} to Brd2Br_{d}^{2}. And it was shown that Br2nBr_{2}^{n} is homomorphically embedded in BrdnBr_{d}^{n} by showing the following statement:

if two braids with parity are equivalent as braids with dots, then they are equivalent as braids with parity.

It means that the parity of braids has geometric meaning; the number of points on braids.

In this paper, analogously we will generalizethe groups Gn2G_{n}^{2} with structures; parity and points, which are denoted by Gn,p2G_{n,p}^{2} and Gn,d2G_{n,d}^{2}, respectively. We are interested in the following question:
two objects are equivalent in a lager category, then are they equivalent as themselves?
Which means that a category is embedded in the larger category. For example, the following statements are related with the above problem.

  1. (1)

    if two classical knots are equivalent as virtual knots, then they are equivalent as classical knots.

  2. (2)

    if two classical braids are equivalent as virtual briads, then they are equivalent as classical briads.

In [5] the first statement is proved and the second statement is proved in [4].

As the above question, we showed the following two statements:

  1. (1)

    if two element in Gn2G_{n}^{2} are equivalent in Gn,p2G_{n,p}^{2}, then they are equivalent in Gn2G_{n}^{2}.

  2. (2)

    if two element in Gn,p2G_{n,p}^{2} are equivalent in Gn,d2G_{n,d}^{2}, then they are equivalent in Gn,p2G_{n,p}^{2}.

From the above statements, the followings are deduced: Since Gn2G_{n}^{2} is isomorphic to group of free braids with nn strands, parity can be generalized to the case of free braids with respect to Gn,p2G_{n,p}^{2}. Moreover, parity is defined abstractly, but it can be geometrically presented by points. On the other hands point on a braid of nn strands means ’liking’ between (n+1)(n+1)-th strand and others. Moreover points on the braid of nn-strands can be considered as traces of n+1n+1-th strand and a homomorphism from Gn,d2G_{n,d}^{2} to Gn+12G_{n+1}^{2} can be defined by adding a new strand by ‘following the traces’(points) of it. By the above observations, we can find a homomorphism from Gn,p2G_{n,p}^{2} to Gn+12G_{n+1}^{2} and, roughly speaking, each value of parity of crossings of the braid of nn-strands can be represented by the number of ‘linking’ between n+1n+1-strand and the other two strands, in which a crossing is. Conversely a braid with points can be obtained from a braid of n+1n+1 strands by deleting one strand and placing points on places, on which deleted stand was.And a braid with parity can be obtained from a braid with points by counting the number of points. Then two braids can be distinguished by braids with parity. In section 2, we simply remind basic definitions and simple results. In section 3, we consider the following question:
two objects are equivalent in a larger category, then are they equivalent as themselves?
in the case of Gn2G_{n}^{2}, Gn,pG_{n,p} and Gn,d2G_{n,d}^{2}. In section 4, relations between Gn,d2G_{n,d}^{2} and Gn+1G_{n+1} are studied. And we will show geometric meanings and examples of braids of n+1n+1 strand, which are distinguished from trivial braids by braids with parity.

2. Basic definitions

Firstly, we recall basic definitions and introduce simple results.

Definition 2.1.

[9] Let Gn2G_{n}^{2} be the group given by the presentation generated by {aij|{i,j}{1,,n},i<j}\{a_{ij}~|~\{i,j\}\subset\{1,\dots,n\},i<j\} with the following relations:

  1. (1)

    aij2=1a_{ij}^{2}=1 for all iji\neq j,

  2. (2)

    aijakl=aklaija_{ij}a_{kl}=a_{kl}a_{ij} for distinct i,j,k,li,j,k,l,

  3. (3)

    aijaikajk=ajkaikaija_{ij}a_{ik}a_{jk}=a_{jk}a_{ik}a_{ij} for distinct i,j,ki,j,k.

In [9] Manturov showed that colored (pure) free braids can be presented by elements in Gn2G_{n}^{2}. In fact, the relations for Gn2G_{n}^{2} are related with Reidemeister moves for free braids.

Definition 2.2.

A free braid diagram is a graph inside a rectangle ×[0,1]\mathbb{R}\times[0,1] with the following properties:

  1. (1)

    The graph vertices of valency 11 are the points [i,0][i,0] and [i,1][i,1], i=1,,ni=1,\cdots,n.

  2. (2)

    All other vertices are 44-valent vertices.

  3. (3)

    For each 44-valent vertex, edges are split by two pairs, two edges in which are called opposite edeges. The opposite edges in such vertices are at the angle of π\pi.

  4. (4)

    The braid strands monotonously go down.

For a free braid diagram, if [i,0][i,0] and [i,1][i,1] are included in the same strand for every i{1,n}i\in\{1,\cdots n\}, then the diagram is called a pure free braid diagram.

A colored free braid diagram is a free braid diagram such that each component is enumerated. If it is a pure free braid diagram, we may assume that the enumeration agrees with xx-terms of 11-valent vertices of the strands.

Definition 2.3.

A free braid of nn strand is an equivalence class of free diagrams of n-strand braid under Artin moves for free braids in Fig. 1.

Refer to caption
Figure 1. Artin moves for free braids

This moves are related with relations of Gn2G_{n}^{2} in order. Now we construct a function from the set PBnPB_{n} of colored pure free braids with nn components to Gn2G_{n}^{2}. Let {ϵk}k=1m(0,1)\{\epsilon_{k}\}_{k=1}^{m}\subset(0,1) be a set of values such that a 44-valent vertex is placed in ×{ϵk}\mathbb{R}\times\{\epsilon_{k}\} and ϵk<ϵk+1\epsilon_{k}<\epsilon_{k+1} for each k=1,m1k=1,\cdots m-1. Without loss of generality, we assume that there is the only one vertex on ×{ϵk}\mathbb{R}\times\{\epsilon_{k}\} for each kk. Let ckc_{k} be the 44-valent vertex on ×{ϵk}\mathbb{R}\times\{\epsilon_{k}\}. Define a function ι\iota from PBnPB_{n} to Gn2G_{n}^{2} as the following: For each vertex ckc_{k}, if it contains edges in iki_{k}-th and jkj_{k}-th components, then give a generator aikjka_{i_{k}j_{k}} in Gn2G_{n}^{2}. Define ι(β)=ai1j1aimjm\iota(\beta)=a_{i_{1}j_{1}}\cdots a_{i_{m}j_{m}}, see Fig. 2.

Refer to caption
Figure 2. Example of a word for a free braid
Proposition 2.4.

[9] A function ι\iota from PBnPB_{n} to Gn2G_{n}^{2} is well-defined.

From the discovery of parity by Manturov [7], invariants for classical knots are extended to invariants for virtual knots. In [3] Fedoseev and Manturov studied classical braids with structures, which are related to parity and dots on strands of classical braids. With those structures, parity can be extended to the case of braids and generalized parity can be deduced by braids with dots. The group of braids with parity and with points are defined as follows:

Definition 2.5.

[3] A group of nn-braids with parity Brn2Br_{n}^{2} is a group generated by {σi0,σi1}i=1n1\{\sigma_{i}^{0},\sigma_{i}^{1}\}_{i=1}^{n-1} with the following relations;

  1. (1)

    σiϵ1σjϵ2=σjϵ2σiϵ1\sigma^{\epsilon_{1}}_{i}\sigma^{\epsilon_{2}}_{j}=\sigma^{\epsilon_{2}}_{j}\sigma^{\epsilon_{1}}_{i} for |ij|>2|i-j|>2,

  2. (2)

    σiϵ1σi+1ϵ2σiϵ3=σi+1ϵ3σiϵ2σi+1ϵ1\sigma_{i}^{\epsilon_{1}}\sigma_{i+1}^{\epsilon_{2}}\sigma_{i}^{\epsilon_{3}}=\sigma_{i+1}^{\epsilon_{3}}\sigma_{i}^{\epsilon_{2}}\sigma_{i+1}^{\epsilon_{1}}, where ϵ1+ϵ2+ϵ3=0\epsilon_{1}+\epsilon_{2}+\epsilon_{3}=0 mod 22.

An element in Br2nBr_{2}^{n} is called a 2\mathbb{Z}_{2}-braid.

Definition 2.6.

[3] A group of nn-braids with dots Brn2Br_{n}^{2} is a group generated by {σi|i{1,,n1}},{τi|i{1,,n}}\{\sigma_{i}~|~i\in\{1,\cdots,n-1\}\},\{\tau_{i}~|~i\in\{1,\cdots,n\}\} with the following relations;

  1. (1)

    σi2=1\sigma_{i}^{2}=1 for all i{1,n1}i\in\{1,\cdots n-1\},

  2. (2)

    σiσj=σjσi\sigma_{i}\sigma_{j}=\sigma_{j}\sigma_{i} for |ij|2|i-j|\geq 2,

  3. (3)

    σiσi+1σi=σi+1σiσi+1\sigma_{i}\sigma_{i+1}\sigma_{i}=\sigma_{i+1}\sigma_{i}\sigma_{i+1} for 1in11\leq i\leq n-1,

  4. (4)

    τi2=1\tau_{i}^{2}=1 for all i{1,n}i\in\{1,\cdots n\},

  5. (5)

    τiτj=τjτi\tau_{i}\tau_{j}=\tau_{j}\tau_{i} for all i,j{1,n}i,j\in\{1,\cdots n\},

  6. (6)

    τiτi+1σiτi+1τi=σi\tau_{i}\tau_{i+1}\sigma_{i}\tau_{i+1}\tau_{i}=\sigma_{i} for all i{1,n1}i\in\{1,\cdots n-1\},

  7. (7)

    σiτk=τkσi\sigma_{i}\tau_{k}=\tau_{k}\sigma_{i} for |ik|2|i-k|\geq 2.

In the group BrndBr_{n}^{d}, each generator τi\tau_{i} is presented by a point on ii-th strand of the braid. Now we define a mapping f:Brn2Brndf:Br_{n}^{2}\rightarrow Br_{n}^{d} by

f(σiϵ)={σiifϵ=0,τiσiτiifϵ=1.f(\sigma_{i}^{\epsilon})=\left\{\begin{array}[]{cc}\sigma_{i}&\text{if}~\epsilon=0,\\ \tau_{i}\sigma_{i}\tau_{i}&\text{if}~\epsilon=1.\\ \end{array}\right.

In [3] they proved that this mapping is injective homomorphism. Moreover the following proposition can be proved.

Proposition 2.7.

If two 2\mathbb{Z}_{2}-braids are equal as braids with dots, they are equal as 2\mathbb{Z}_{2}-braids.

In the following sections, we study Gn2G_{n}^{2} with structures which are related to parity and points algebraically.

3. Gn2G_{n}^{2} with additional structures

In this section, we get enhancements of Gn2G_{n}^{2} by adding some structures, which are related to parity and points on strands of colored pure braids. Firstly, we define a group Gn,p2G_{n,p}^{2} and we call it Gn2G_{n}^{2} with parity.

Definition 3.1.

For a positive integer nn, define Gn,p2G_{n,p}^{2} by the group presentation generated by {aijϵ|{i,j}{1,,n},i<j,ϵ{0,1}}\{a_{ij}^{\epsilon}~|~\{i,j\}\subset\{1,\dots,n\},i<j,~\epsilon\in\{0,1\}\} with the following relations;

  1. (1)

    (aijϵ)2=1(a_{ij}^{\epsilon})^{2}=1, ϵ{0,1}\epsilon\in\{0,1\} and i,j{1,,n}i,j\in\{1,\cdots,n\},

  2. (2)

    aijϵijaklϵkl=aklϵklaijϵija_{ij}^{\epsilon_{ij}}a_{kl}^{\epsilon_{kl}}=a_{kl}^{\epsilon_{kl}}a_{ij}^{\epsilon_{ij}} for 1i<j<k<ln1\leq i<j<k<l\leq n,

  3. (3)

    aijϵijaikϵikajkϵjk=ajkϵjkaikϵikaijϵija_{ij}^{\epsilon_{ij}}a_{ik}^{\epsilon_{ik}}a_{jk}^{\epsilon_{jk}}=a_{jk}^{\epsilon_{jk}}a_{ik}^{\epsilon_{ik}}a_{ij}^{\epsilon_{ij}}, for 1i<j<kn1\leq i<j<k\leq n, where ϵij+ϵik+ϵjk=0\epsilon_{ij}+\epsilon_{ik}+\epsilon_{jk}=0 mod 22.

The relations of Gn,p2G_{n,p}^{2} are closely related to the axioms of parity [7]. We call aij0a_{ij}^{0}(aij1a_{ij}^{1}) an even generator(an odd generator). If a word β\beta in Gn,p2G_{n,p}^{2} has no odd generators, then we call β\beta an even word (or an even element). Gn2G_{n}^{2} can be considered as a subgroup of Gn,p2G_{n,p}^{2} by a homomorphism ii from Gn2G_{n}^{2} to Gn,p2G_{n,p}^{2} defined by i(aij)=aij0i(a_{ij})=a_{ij}^{0}. It is easy to show that ii is well-defined. Moreover, the following statement can be proved.

Lemma 3.2.

The homomorphism i:Gn2Gn,p2i:G_{n}^{2}\rightarrow G_{n,p}^{2} is a monomorphism.

Proof.

To prove this statement, consider projection map p:Gn,p2Gn2p:G_{n,p}^{2}\rightarrow G_{n}^{2} defined by

p(aijϵ)={aijifϵ=0,1ifϵ=1.p(a_{ij}^{\epsilon})=\left\{\begin{array}[]{cc}a_{ij}&\text{if}~\epsilon=0,\\ 1&\text{if}~\epsilon=1.\\ \end{array}\right.

It is easy to show that pp is well-defined function. Let β\beta and β\beta^{\prime} be two words in Gn2G_{n}^{2} such that i(β)=i(β)i(\beta)=i(\beta^{\prime}). By the definition of ii, p(i(β))=βp(i(\beta))=\beta and p(i(β))=βp(i(\beta^{\prime}))=\beta^{\prime}. That is, β=β\beta=\beta^{\prime} in Gn2G_{n}^{2}, therefore, the proof is completed.

Corollary 3.3.

If two words β\beta and β\beta^{\prime} in Gn2G_{n}^{2} are equivalent in Gn,p2G_{n,p}^{2}, then they are equivalent in Gn2G_{n}^{2}.

Now, we define a group Gn,d2G_{n,d}^{2} and we call it Gn2G_{n}^{2} with points.

Definition 3.4.

For a positive integer nn, define Gn,d2G_{n,d}^{2} by the group presentation generated by {aij|{i,j}{1,,n},i<j}\{a_{ij}~|~\{i,j\}\subset\{1,\dots,n\},i<j\} and {τi|i{1,,n}}\{\tau_{i}~|~i\in\{1,\cdots,n\}\} with the following relations;

  1. (1)

    aij2=1a_{ij}^{2}=1 for {i,j}{1,,n},i<j\{i,j\}\subset\{1,\dots,n\},i<j,

  2. (2)

    aijakl=aklaija_{ij}a_{kl}=a_{kl}a_{ij} for distinct i,j,k,l{1,,n}i,j,k,l\in\{1,\dots,n\},

  3. (3)

    aijaikajk=ajkaikaija_{ij}a_{ik}a_{jk}=a_{jk}a_{ik}a_{ij} for distinct i,j,k{1,,n}i,j,k\in\{1,\dots,n\}

  4. (4)

    τi2=1\tau_{i}^{2}=1 for i{1,,n}i\in\{1,\dots,n\},

  5. (5)

    τiτj=τjτi\tau_{i}\tau_{j}=\tau_{j}\tau_{i} for i,j{1,,n}i,j\in\{1,\dots,n\},

  6. (6)

    τiτjaijτjτi=aij\tau_{i}\tau_{j}a_{ij}\tau_{j}\tau_{i}=a_{ij} for i,j{1,,n}i,j\in\{1,\dots,n\},

  7. (7)

    aijτk=τkaija_{ij}\tau_{k}=\tau_{k}a_{ij} for distinct i,j,k{1,,n}i,j,k\in\{1,\dots,n\}.

We call τi\tau_{i} a generator for a point on ii-th component or simply, a point on ii-th component. Geometrically, aija_{ij} is corresponded to a 4-valent vertex and τi\tau_{i} is corresponded to a point on the ii-th strand of the free braid, see Fig. 3.

Refer to caption
Figure 3. Geometrical meanigngs of aija_{ij} and τi\tau_{i}

In fact, two groups Gn,p2G_{n,p}^{2} and Gn,d2G_{n,d}^{2} are closely related to each other. Define a function ϕ\phi from Gn,p2G_{n,p}^{2} to Gn,d2G_{n,d}^{2} by

ϕ(aijϵ)={aijifϵ=0,τiaijτiifϵ=1.\phi(a_{ij}^{\epsilon})=\left\{\begin{array}[]{cc}a_{ij}&\text{if}~\epsilon=0,\\ \tau_{i}a_{ij}\tau_{i}&\text{if}~\epsilon=1.\\ \end{array}\right.

Geometrically, the image of aij1a_{ij}^{1} is a crossing between ii-th and jj-th strands of the braid with two points just before and after of the crossing on ii-th strand, see Fig. 4.

Refer to caption
Figure 4. Image of aij1a_{ij}^{1}

Notice that, since we can get τiaijτi=τjaijτj\tau_{i}a_{ij}\tau_{i}=\tau_{j}a_{ij}\tau_{j} from the relation τiτjaijτjτi=aij\tau_{i}\tau_{j}a_{ij}\tau_{j}\tau_{i}=a_{ij}, two diagrams with point in Fig. 4 are equivalent. On the other hand, the number of τi\tau_{i} and τj\tau_{j} before a given crossing ϕ(aijϵ)\phi(a_{ij}^{\epsilon}) is equal to ϵ\epsilon modulo 22, because every image of aklϵa_{kl}^{\epsilon} before ϕ(aijϵ)\phi(a_{ij}^{\epsilon}) has two points or no points.

Lemma 3.5.

The map ϕ\phi from Gn,p2G_{n,p}^{2} to Gn,d2G_{n,d}^{2} is well defined.

Proof.

To show that ϕ\phi is well defined, it is enough to show that every relation is preserved by ϕ\phi. For relations (aijϵ)2=1(a_{ij}^{\epsilon})^{2}=1, if ϵ=0\epsilon=0, then ϕ((aij0)2)=aij2=1\phi((a_{ij}^{0})^{2})=a_{ij}^{2}=1. If ϵ=1\epsilon=1, then

ϕ((aij1)2)=τiaijτiτiaijτi=τiaijaijτi=τiτi=1,\phi((a_{ij}^{1})^{2})=\tau_{i}a_{ij}\tau_{i}\tau_{i}a_{ij}\tau_{i}=\tau_{i}a_{ij}a_{ij}\tau_{i}=\tau_{i}\tau_{i}=1,

which can be presented geometrically as Fig. 5.

Refer to caption
Figure 5. ϕ(aij2)=1\phi(a_{ij}^{2})=1

For relations aijϵijaklϵkl=aklϵklaijϵija_{ij}^{\epsilon_{ij}}a_{kl}^{\epsilon_{kl}}=a_{kl}^{\epsilon_{kl}}a_{ij}^{\epsilon_{ij}} with distinct i,j,k,li,j,k,l, since ii,jj,kk, and ll are different indices, clearly the commutativity holds. For relations aijϵijaikϵikajkϵjk=ajkϵjkaikϵikaijϵija_{ij}^{\epsilon_{ij}}a_{ik}^{\epsilon_{ik}}a_{jk}^{\epsilon_{jk}}=a_{jk}^{\epsilon_{jk}}a_{ik}^{\epsilon_{ik}}a_{ij}^{\epsilon_{ij}}, where ϵij+ϵik+ϵjk=0\epsilon_{ij}+\epsilon_{ik}+\epsilon_{jk}=0 mod 22, there are only two cases: all ϵ\epsilon’s are equal to 0 or only two of them are equal to 11. If every ϵ\epsilon is 0, then

ϕ(aij0aik0ajk0)=aijaikajk=ajkaikaij=ϕ(ajk0aik0aij0).\phi(a_{ij}^{0}a_{ik}^{0}a_{jk}^{0})=a_{ij}a_{ik}a_{jk}=a_{jk}a_{ik}a_{ij}=\phi(a_{jk}^{0}a_{ik}^{0}a_{ij}^{0}).

Suppose that only two of them are equal to 11, say ϵij=1\epsilon_{ij}=1, ϵik=1\epsilon_{ik}=1 and ϵjk=0\epsilon_{jk}=0. Then

ϕ(aij1aik1ajk0)=τiaijτiτiaikτiajk=τiaijaikτiajk=τiaijaikajkτi=τiajkaikaijτi=τiajkτiτiaikτiaij=ϕ(ajk0aik1aij1),\phi(a_{ij}^{1}a_{ik}^{1}a_{jk}^{0})=\tau_{i}a_{ij}\tau_{i}\tau_{i}a_{ik}\tau_{i}a_{jk}=\tau_{i}a_{ij}a_{ik}\tau_{i}a_{jk}=\tau_{i}a_{ij}a_{ik}a_{jk}\tau_{i}=\tau_{i}a_{jk}a_{ik}a_{ij}\tau_{i}=\tau_{i}a_{jk}\tau_{i}\tau_{i}a_{ik}\tau_{i}a_{ij}=\phi(a_{jk}^{0}a_{ik}^{1}a_{ij}^{1}),

which can be presented geomerically as Fig. 6.

Refer to caption
Figure 6. ϕ(aij1aik1ajk0)=ϕ(ajk1aik1aij0)\phi(a_{ij}^{1}a_{ik}^{1}a_{jk}^{0})=\phi(a_{jk}^{1}a_{ik}^{1}a_{ij}^{0})

Therefore, ϕ\phi is well-defined.

Let Hn,d2={βGn,d2|Ni(β)=0mod2,i{1,,n}}H_{n,d}^{2}=\{\beta\in G_{n,d}^{2}~|~N_{i}(\beta)=0~\text{mod}~2,~i\in\{1,\cdots,n\}\}, where Ni(β)N_{i}(\beta) is the number of τi\tau_{i} in β\beta. Notice that, by the definition of ϕ\phi, it is clear that the image of Gn,p2G_{n,p}^{2} by ϕ\phi goes into the set Hn,d2H_{n,d}^{2}. Since every relation of Gn,d2G_{n,d}^{2} preserves the number of τ\tau’s modulo 22, Hn,d2H_{n,d}^{2} is a subgroup of Gn,d2G_{n,d}^{2}.

Lemma 3.6.

Let β=T0ai1j1T2Tk1aikjkTkTm1aimjmTmH\beta=T_{0}a_{i_{1}j_{1}}T_{2}\cdots T_{k-1}a_{i_{k}j_{k}}T_{k}\cdots T_{m-1}a_{i_{m}j_{m}}T_{m}\in H, where TkT_{k} is a product of τ\tau’s. Define a function χ:Hn,d2Gn,p2\chi:H_{n,d}^{2}\rightarrow G_{n,p}^{2} by

χ(β)=ai1j1ϵ1aikjkϵkaimjmϵm,\chi(\beta)=a_{i_{1}j_{1}}^{\epsilon_{1}}\cdots a_{i_{k}j_{k}}^{\epsilon_{k}}\cdots a_{i_{m}j_{m}}^{\epsilon_{m}},

where NikN_{i_{k}} is the number of τik\tau_{i_{k}} in T0,,Tk1T_{0},\cdots,T_{k-1} and ϵk=Nik+Njk\epsilon_{k}=N_{i_{k}}+N_{j_{k}}. Then χ\chi is well-defined.

Proof.

Consider β=T0ai1j1T2Tk1aikjkTkTm1aimjmTmH\beta=T_{0}a_{i_{1}j_{1}}T_{2}\cdots T_{k-1}a_{i_{k}j_{k}}T_{k}\cdots T_{m-1}a_{i_{m}j_{m}}T_{m}\in H. Assume that aikjka_{i_{k}j_{k}} contains in one of relations, which can be applied to β\beta. If aikjka_{i_{k}j_{k}} is contains in the relation (6) τiτjaijτjτi=aij\tau_{i}\tau_{j}a_{ij}\tau_{j}\tau_{i}=a_{ij}, then the number of τik\tau_{i_{k}} and τjk\tau_{j_{k}} in Tk1T_{k-1} preserves modulo 22 and then the sum of the numbers of τik\tau_{i_{k}} and τjk\tau_{j_{k}} in T0,,Tk1T_{0},\cdots,T_{k-1} is not changed modulo 22. Therefore ϵk=Nik+Njk\epsilon_{k}=N_{i_{k}}+N_{j_{k}} is preserved modulo 22. If aikjka_{i_{k}j_{k}} is contained in the relation (7) τkaij=aijτk\tau_{k}a_{ij}=a_{ij}\tau_{k}, then the number of τik\tau_{i_{k}} and τjk\tau_{j_{k}} in Tk1T_{k-1} is preserved, since in relation (7) i,j,ki,j,k are different respectively. Therefore the number of τik\tau_{i_{k}} and τjk\tau_{j_{k}} in T0,,Tk1T_{0},\cdots,T_{k-1} is not changed, and ϵk=Nik+Njk\epsilon_{k}=N_{i_{k}}+N_{j_{k}} is preserved modulo 22. The relation (2) aijakl=aklaija_{ij}a_{kl}=a_{kl}a_{ij} is preserved along χ\chi by relation aijϵ1aklϵ2=aklϵ2aijϵ1a_{ij}^{\epsilon_{1}}a_{kl}^{\epsilon_{2}}=a_{kl}^{\epsilon_{2}}a_{ij}^{\epsilon_{1}} for different i,j,k,li,j,k,l. Suppose that aikjka_{i_{k}j_{k}} is appeared in the relation (1) aij2=1a_{ij}^{2}=1. Then ik=ik+1i_{k}=i_{k+1}, jk=jk+1j_{k}=j_{k+1} and there are no τ\tau’s in TkT_{k}. Therefore ϵk=ϵk+1\epsilon_{k}=\epsilon_{k+1} and the relation is preserved by (aijϵ)2=1(a_{ij}^{\epsilon})^{2}=1. Suppose that aikjka_{i_{k}j_{k}} is appeared in relation (3) aijaikajk=ajkaikaija_{ij}a_{ik}a_{jk}=a_{jk}a_{ik}a_{ij}. Suppose that aikjkaik+1jk+1aik+2jk+2=aik+2jk+2aik+1jk+1aikjka_{i_{k}j_{k}}a_{i_{k+1}j_{k+1}}a_{i_{k+2}j_{k+2}}=a_{i_{k+2}j_{k+2}}a_{i_{k+1}j_{k+1}}a_{i_{k}j_{k}} and ik=ik+1i_{k}=i_{k+1}, jk=ik+2j_{k}=i_{k+2} and jk+1=jk+2j_{k+1}=j_{k+2}. It is sufficient to show that ϵk+ϵk+1+ϵk+2=0\epsilon_{k}+\epsilon_{k+1}+\epsilon_{k+2}=0 modulo 22. Then there are no τ\tau’s in TkT_{k},Tk+1T_{k+1},Tk+2T_{k+2}, and hence Nik=Nik+1N_{i_{k}}=N_{i_{k+1}}, Njk=Nik+2N_{j_{k}}=N_{i_{k+2}}, Njk+1=Njk+2N_{j_{k+1}}=N_{j_{k+2}}. Therefore

ϵk+ϵk+1+ϵk+2=Nik+Njk+Nik+1+Njk+1+Nik+2+Njk+2=0mod2.\epsilon_{k}+\epsilon_{k+1}+\epsilon_{k+2}=N_{i_{k}}+N_{j_{k}}+N_{i_{k+1}}+N_{j_{k+1}}+N_{i_{k+2}}+N_{j_{k+2}}=0~\text{mod}~2.

and the proof is completed.

Theorem 3.7.

Gn,p2G_{n,p}^{2} is isomorphic to Hn,d2H_{n,d}^{2}.

Proof.

We will show that χϕ=1Gn,p2\chi\circ\phi=1_{G_{n,p}^{2}} and ϕχ=1Hn,d2\phi\circ\chi=1_{H_{n,d}^{2}}. To show that χϕ=1Gn,p2\chi\circ\phi=1_{G_{n,p}^{2}} let β=ai1j1ϵ1aimjmϵmGn,p2\beta=a_{i_{1}j_{1}}^{\epsilon_{1}}\cdots a_{i_{m}j_{m}}^{\epsilon_{m}}\in G_{n,p}^{2}. Then

χ(ϕ(β))=χ(τi1ϵ1ai1j1τi1ϵ1τimϵmaimjmτimϵm)=ai1j1θ1aimjmθm\chi(\phi(\beta))=\chi(\tau_{i_{1}}^{\epsilon_{1}}a_{i_{1}j_{1}}\tau_{i_{1}}^{\epsilon_{1}}\cdots\tau_{i_{m}}^{\epsilon_{m}}a_{i_{m}j_{m}}\tau_{i_{m}}^{\epsilon_{m}})=a_{i_{1}j_{1}}^{\theta_{1}}\cdots a_{i_{m}j_{m}}^{\theta_{m}}.

For each kk, the number of all τ\tau’s which are appeared from ai1j1ϵ1aik1jk1ϵma_{i_{1}j_{1}}^{\epsilon_{1}}\cdots a_{i_{k-1}j_{k-1}}^{\epsilon_{m}} is even. Since θk\theta_{k} is equal to the number of all τik\tau_{i_{k}} and τjk\tau_{j_{k}} modulo 22, θk=ϵk\theta_{k}=\epsilon_{k}. Therefore χϕ=1Gn,p2\chi\circ\phi=1_{G_{n,p}^{2}}.

Now we will show that ϕχ=1Hn,d2\phi\circ\chi=1_{H_{n,d}^{2}}. Let

β=T0ai1j1T1Tk1aikjkTkTm1aimjmTmH.\beta=T_{0}a_{i_{1}j_{1}}T_{1}\cdots T_{k-1}a_{i_{k}j_{k}}T_{k}\cdots T_{m-1}a_{i_{m}j_{m}}T_{m}\in H.

Firstly we will show that β\beta is equivalent to an element in the form

τi1ϵ1ai1j1τi1ϵ1τimϵmaimjmτimϵm.\tau_{i_{1}}^{\epsilon_{1}}a_{i_{1}j_{1}}\tau_{i_{1}}^{\epsilon_{1}}\cdots\tau_{i_{m}}^{\epsilon_{m}}a_{i_{m}j_{m}}\tau_{i_{m}}^{\epsilon_{m}}.

By the relations τiτj=τjτi\tau_{i}\tau_{j}=\tau_{j}\tau_{i} and τkaij=aijτk\tau_{k}a_{ij}=a_{ij}\tau_{k}, β\beta is equivalent to the form

T0ai1j1T2Tk1aikjkTkTm1aimjmTmT_{0}a_{i_{1}j_{1}}T_{2}\cdots T_{k-1}a_{i_{k}j_{k}}T_{k}\cdots T_{m-1}a_{i_{m}j_{m}}T_{m}

such that TkT_{k} only has τik\tau_{i_{k}}, τjk\tau_{j_{k}}, τik+1\tau_{i_{k+1}} and τjk+1\tau_{j_{k+1}}. In point of aikjka_{i_{k}j_{k}}, it is a product of the following;

Aikjk=τikθikfτjkθjkfaikjkτikθikbτjkθjkb.A_{i_{k}j_{k}}=\tau_{i_{k}}^{\theta^{f}_{i_{k}}}\tau_{j_{k}}^{\theta^{f}_{j_{k}}}a_{i_{k}j_{k}}\tau_{i_{k}}^{\theta^{b}_{i_{k}}}\tau_{j_{k}}^{\theta^{b}_{j_{k}}}.

Now we claim that there is an element β\beta^{\prime} which is a product of

Aikjk=τikθikfτjkθjkfaikjkτikθikbτjkθjkb,A^{\prime}_{i_{k}j_{k}}=\tau_{i_{k}}^{\theta^{f}_{i_{k}}}\tau_{j_{k}}^{\theta^{f}_{j_{k}}}a_{i_{k}j_{k}}\tau_{i_{k}}^{\theta^{b}_{i_{k}}}\tau_{j_{k}}^{\theta^{b}_{j_{k}}},

where τikθikf=τikθikb\tau_{i_{k}}^{\theta^{f}_{i_{k}}}=\tau_{i_{k}}^{\theta^{b}_{i_{k}}} and τikθjkf=τjkθikb\tau_{i_{k}}^{\theta^{f}_{j_{k}}}=\tau_{j_{k}}^{\theta^{b}_{i_{k}}}. Suppose that ii is an index such that Aij=τiθifτjθjfaijτiθibτjθjbA_{ij}=\tau_{i}^{\theta^{f}_{i}}\tau_{j}^{\theta^{f}_{j}}a_{ij}\tau_{i}^{\theta^{b}_{i}}\tau_{j}^{\theta^{b}_{j}} is the first part in which θifθib\theta_{i}^{f}\neq\theta_{i}^{b}, say θif=1\theta_{i}^{f}=1 and θib=0\theta_{i}^{b}=0. Notice that if θib=1\theta_{i}^{b}=1 and θif=1\theta_{i}^{f}=1, then τiθib\tau_{i}^{\theta_{i}^{b}} can be move to the very next AilA_{il} and it is same to the case of θif=1\theta_{i}^{f}=1 and θib=0\theta_{i}^{b}=0. Since β\beta is in HH, the number of τi\tau_{i} should be even and there is Aik=τiθifτkθkfaikτiθibτkθkbA_{ik}=\tau_{i}^{\theta^{\prime f}_{i}}\tau_{k}^{\theta^{f}_{k}}a_{ik}\tau_{i}^{\theta^{\prime b}_{i}}\tau_{k}^{\theta^{b}_{k}} such that θif=1\theta^{\prime f}_{i}=1 or θib=1\theta^{\prime b}_{i}=1 as 3.1 and 3.2.

(3.1) β\displaystyle\beta =\displaystyle= AijAik\displaystyle\cdots A_{ij}\cdots A_{ik}\cdots
(3.2) =\displaystyle= τjθjfaijτiθibτjθjbτiθifτkθkfaikτkθkb.\displaystyle\cdots\tau_{j}^{\theta^{f}_{j}}a_{ij}\tau_{i}^{\theta^{b}_{i}}\tau_{j}^{\theta^{b}_{j}}\cdots\tau_{i}^{\theta^{f}_{i}}\tau_{k}^{\theta^{f}_{k}}a_{ik}\tau_{k}^{\theta^{b}_{k}}\cdots.

If θif=1\theta^{\prime f}_{i}=1 and there are no AilA_{il}, then by the relations aijτk=τkaija_{ij}\tau_{k}=\tau_{k}a_{ij} and τiτj=τjτi\tau_{i}\tau_{j}=\tau_{j}\tau_{i}, τi\tau_{i} can be move to the next of aija_{ij} as 3.3 and 3.4.

(3.3) β\displaystyle\beta =\displaystyle= τiτjθjfaijτjθjbAτiτkθkfaikτkθkb\displaystyle\cdots\tau_{i}\tau_{j}^{\theta^{f}_{j}}a_{ij}\tau_{j}^{\theta^{b}_{j}}\cdots A_{**}\cdots\tau_{i}\tau_{k}^{\theta^{f}_{k}}a_{ik}\tau_{k}^{\theta^{b}_{k}}\cdots
(3.4) =\displaystyle= τiτjθjfaijτiτjθjbAτkθkfaikτkθkb.\displaystyle\cdots\tau_{i}\tau_{j}^{\theta^{f}_{j}}a_{ij}\tau_{i}\tau_{j}^{\theta^{b}_{j}}\cdots A_{**}\cdots\tau_{k}^{\theta^{f}_{k}}a_{ik}\tau_{k}^{\theta^{b}_{k}}\cdots.

If θif=1\theta^{\prime f}_{i}=1 and there is a AilA_{il}’s, then by the relation τi2=1\tau_{i}^{2}=1 new τ\tau’s are appeared and by the relations aijτk=τkaija_{ij}\tau_{k}=\tau_{k}a_{ij} and τiτj=τjτi\tau_{i}\tau_{j}=\tau_{j}\tau_{i}, τi\tau_{i}’s can be move to the next of aija_{ij} and to the front of aila_{il} as 3.5, 3.6 and 3.7.

(3.5) β\displaystyle\beta =\displaystyle= τiτjθjfaijτjθjbAilτiτkθkfaikτkθkb\displaystyle\cdots\tau_{i}\tau_{j}^{\theta^{f}_{j}}a_{ij}\tau_{j}^{\theta^{b}_{j}}\cdots A_{il}\cdots\tau_{i}\tau_{k}^{\theta^{f}_{k}}a_{ik}\tau_{k}^{\theta^{b}_{k}}\cdots
(3.6) =\displaystyle= τiτjθjfaijτjθjbτiτiAilτiτkθkfaikτkθkb\displaystyle\cdots\tau_{i}\tau_{j}^{\theta^{f}_{j}}a_{ij}\tau_{j}^{\theta^{b}_{j}}\cdots\tau_{i}\tau_{i}A_{il}\cdots\tau_{i}\tau_{k}^{\theta^{f}_{k}}a_{ik}\tau_{k}^{\theta^{b}_{k}}\cdots
(3.7) =\displaystyle= τiτjθjfaijτiτjθjbτiAilτiτkθkfaikτkθkb.\displaystyle\cdots\tau_{i}\tau_{j}^{\theta^{f}_{j}}a_{ij}\tau_{i}\tau_{j}^{\theta^{b}_{j}}\cdots\tau_{i}A_{il}\tau_{i}\cdots\tau_{k}^{\theta^{f}_{k}}a_{ik}\tau_{k}^{\theta^{b}_{k}}\cdots.

Analgously the case θib=1\theta^{\prime b}_{i}=1 also can be solved.

Now assume that β=k=1m=τikθikτjkθjkaikjkτikθikτjkθjk\beta=\prod_{k=1}^{m}=\tau_{i_{k}}^{\theta_{i_{k}}}\tau_{j_{k}}^{\theta_{j_{k}}}a_{i_{k}j_{k}}\tau_{i_{k}}^{\theta_{i_{k}}}\tau_{j_{k}}^{\theta_{j_{k}}}. Then

ϕχ(β)\displaystyle\phi\circ\chi(\beta) =\displaystyle= ϕχ(k=1m=τikθikτjkθjkaikjkτikθikτjkθjk)\displaystyle\phi\circ\chi(\prod_{k=1}^{m}=\tau_{i_{k}}^{\theta_{i_{k}}}\tau_{j_{k}}^{\theta_{j_{k}}}a_{i_{k}j_{k}}\tau_{i_{k}}^{\theta_{i_{k}}}\tau_{j_{k}}^{\theta_{j_{k}}})
=\displaystyle= ϕ(k=1maikjkθikjk)=k=1m(τikθikjkaikjkτikθikjk),\displaystyle\phi(\prod_{k=1}^{m}a_{i_{k}j_{k}}^{\theta_{i_{k}j_{k}}})=\prod_{k=1}^{m}(\tau_{i_{k}}^{\theta_{i_{k}j_{k}}}a_{i_{k}j_{k}}\tau_{i_{k}}^{\theta_{i_{k}j_{k}}}),

where θikjk=θik+θjk\theta_{i_{k}j_{k}}=\theta_{i_{k}}+\theta_{j_{k}} mod 22. If θik=θjk=1\theta_{i_{k}}=\theta_{j_{k}}=1, by the relation τiτjaijτjτi=aij\tau_{i}\tau_{j}a_{ij}\tau_{j}\tau_{i}=a_{ij}, β\beta and ϕχ(β)\phi\circ\chi(\beta) are same elements in Gn,d2G_{n,d}^{2}. If θik=1\theta_{i_{k}}=1 and θjk=0\theta_{j_{k}}=0(or θik=0\theta_{i_{k}}=0 and θjk=1\theta_{j_{k}}=1, by the relation τiτjaijτjτi=aij\tau_{i}\tau_{j}a_{ij}\tau_{j}\tau_{i}=a_{ij}(in other word,τiaijτi=τjaijτj\tau_{i}a_{ij}\tau_{i}=\tau_{j}a_{ij}\tau_{j}), β\beta and ϕχ(β)\phi\circ\chi(\beta) are same elements in Gn,d2G_{n,d}^{2} and hence ϕχ=1Gn,d2\phi\circ\chi=1_{G_{n,d}^{2}}. ∎

4. Gn,d2G_{n,d}^{2} and Gn+12G_{n+1}^{2}

In [8], maps from GnkG_{n}^{k} to Gn1kG_{n-1}^{k} and from GnkG_{n}^{k} to Gn1k1G_{n-1}^{k-1} are constructed. In these maps, each generator is mapped to a generator. Here we justify these maps and extended to the case of mappings from Gn2G_{n}^{2} to Gn1,d2G_{n-1,d}^{2}. In section 3, we obtained including maps i:Gn2Gn,p2i:G_{n}^{2}\rightarrow G_{n,p}^{2} and ϕ:Gn,p2Gn,d2\phi:G_{n,p}^{2}\rightarrow G_{n,d}^{2}. To show that they are including maps, we found right inverse of them. In this section we consider relations between Gn,d2G_{n,d}^{2} and Gn+12G_{n+1}^{2}.

Let us define ψ\psi from Gn+12G_{n+1}^{2} to Gn,d2G_{n,d}^{2} by

ψ(aij)={aijifn+1{i,j},τiifj=n+1,τjifi=n+1.\psi(a_{ij})=\left\{\begin{array}[]{cc}a_{ij}&\text{if}~n+1\not\in\{i,j\},\\ \tau_{i}&\text{if}~j=n+1,\\ \tau_{j}&\text{if}~i=n+1.\\ \end{array}\right.

Then the following lemma can be proved.

Lemma 4.1.

A mapping ψ\psi from Gn+12G_{n+1}^{2} to Gn,d2G_{n,d}^{2}is well-defined.

Proof.

It is enough to show that every relation for Gn+12G_{n+1}^{2} is preserved by ψ\psi. If every index is different with n+1n+1, it is clear. Consider a relation aijakl=aklaija_{ij}a_{kl}=a_{kl}a_{ij} for distinct i,j,k,l{1,,n+1}i,j,k,l\in\{1,\cdots,n+1\}. If one of i,j,ki,j,k and ll is n+1n+1, say i=n+1i=n+1, then

ψ(a(n+1)jakl)=τjakl=aklτj=ψ(akla(n+1)j).\psi(a_{(n+1)j}a_{kl})=\tau_{j}a_{kl}=a_{kl}\tau_{j}=\psi(a_{kl}a_{(n+1)j}).

For the relations aijaikajk=ajkaikaija_{ij}a_{ik}a_{jk}=a_{jk}a_{ik}a_{ij}, if one of i,ji,j and kk is n+1n+1, say i=n+1i=n+1, then

ψ(aijaikajk)=τjτkajk=ajkτkτj=ψ(ajkaikaij).\psi(a_{ij}a_{ik}a_{jk})=\tau_{j}\tau_{k}a_{jk}=a_{jk}\tau_{k}\tau_{j}=\psi(a_{jk}a_{ik}a_{ij}).

Clearly, the relation aij2=1a_{ij}^{2}=1 is preserved along ψ\psi and the statement is proved. ∎

Now we define inverse mapping. We define ω\omega from Gn,d2G_{n,d}^{2} to Gn+12G_{n+1}^{2} by ω(aij)=aij\omega(a_{ij})=a_{ij} and ω(τi)=ai(n+1)\omega(\tau_{i})=a_{i(n+1)}, for example, see Fig. 7.

Refer to caption
Figure 7. Example of a image of the mapping ω\omega

But this mapping is not well-defined because the relation τiτj=τjτi\tau_{i}\tau_{j}=\tau_{j}\tau_{i} in Gn,d2G_{n,d}^{2} goes to ai(n+1)aj(n+1)=aj(n+1)ai(n+1)a_{i(n+1)}a_{j(n+1)}=a_{j(n+1)}a_{i(n+1)} but ai(n+1)a_{i(n+1)} and aj(n+1)a_{j(n+1)} are not commutative. However, we can modify the mapping and get the following lemma.

Lemma 4.2.

A mapping ω:Gn,d2Gn+12/ai(n+1)aj(n+1)=aj(n+1)ai(n+1)\omega:G_{n,d}^{2}\rightarrow G_{n+1}^{2}/\langle a_{i(n+1)}a_{j(n+1)}=a_{j(n+1)}a_{i(n+1)}\rangle, defined by ω(aij)=aij\omega(a_{ij})=a_{ij} and τi=ai(n+1)\tau_{i}=a_{i(n+1)}, is well-defined.

Proof.

It is sufficient to show that every relation for Gn,d2G_{n,d}^{2} goes to trivial in Gn+12/ai(n+1)aj(n+1)=aj(n+1)ai(n+1)G_{n+1}^{2}/\langle a_{i(n+1)}a_{j(n+1)}=a_{j(n+1)}a_{i(n+1)}\rangle. For relations (1),(2),(3) and (4), it is clear. Consider relation τiτj=τjτi\tau_{i}\tau_{j}=\tau_{j}\tau_{i}. Then

ω(τiτj)=ai(n+1)aj(n+1)=aj(n+1)ai(n+1)=ω(τjτi).\omega(\tau_{i}\tau_{j})=a_{i(n+1)}a_{j(n+1)}=a_{j(n+1)}a_{i(n+1)}=\omega(\tau_{j}\tau_{i}).

The relation (6) τiτjaijτjτi=aij\tau_{i}\tau_{j}a_{ij}\tau_{j}\tau_{i}=a_{ij} can be written by τiτjaij=aijτjτi\tau_{i}\tau_{j}a_{ij}=a_{ij}\tau_{j}\tau_{i}. Then

ω(τiτjaij)=ai(n+1)ajn+2aij=aijaj(n+1)ai(n+1)=ω(aijτjτi).\omega(\tau_{i}\tau_{j}a_{ij})=a_{i(n+1)}a_{jn+2}a_{ij}=a_{ij}a_{j(n+1)}a_{i(n+1)}=\omega(a_{ij}\tau_{j}\tau_{i}).

Finally, the relations (5) and (7) are preserved by the relation ai(n+1)aj(n+1)=aj(n+1)ai(n+1)a_{i(n+1)}a_{j(n+1)}=a_{j(n+1)}a_{i(n+1)} and the proof is completed. ∎

Geometrically the relations ai(n+1)aj(n+1)=aj(n+1)ai(n+1)a_{i(n+1)}a_{j(n+1)}=a_{j(n+1)}a_{i(n+1)} mean that two consecutive classical crossings pass a virtual crossing, see Fig. 8. Generally, this move in this case, is called a forbidden move by (n+1)(n+1)-th strand.

Refer to caption
Figure 8. forbidden moves
Corollary 4.3.

The groups Gn,d2G_{n,d}^{2} and Gn+12/ai(n+1)aj(n+1)=aj(n+1)ai(n+1)G_{n+1}^{2}/\langle a_{i(n+1)}a_{j(n+1)}=a_{j(n+1)}a_{i(n+1)}\rangle are isomorphic.

Proof.

We will show that ωψ=1Gn,d2\omega\circ\psi=1_{G_{n,d}^{2}} and ψω=1Gn+12/ai(n+1)aj(n+1)=aj(n+1)ai(n+1)\psi\circ\omega=1_{G_{n+1}^{2}/\langle a_{i(n+1)}a_{j(n+1)}=a_{j(n+1)}a_{i(n+1)}\rangle}. For generators aija_{ij} in Gn+12/ai(n+1)aj(n+1)=aj(n+1)ai(n+1)G_{n+1}^{2}/\langle a_{i(n+1)}a_{j(n+1)}=a_{j(n+1)}a_{i(n+1)}\rangle,

ψ(aij)={aijifn+1{i,j},τiifj=n+1,τjifi=n+1.\psi(a_{ij})=\left\{\begin{array}[]{cc}a_{ij}&\text{if}~n+1\in\{i,j\},\\ \tau_{i}&\text{if}~j=n+1,\\ \tau_{j}&\text{if}~i=n+1.\\ \end{array}\right.

By definition of ω\omega, ω(ψ(aij))=aij\omega(\psi(a_{ij}))=a_{ij}. Hence ωψ=1Gn,d2\omega\circ\psi=1_{G_{n,d}^{2}}. Analogously, it can be shown that ψω=1Gn+12/ai(n+1)aj(n+1)=aj(n+1)ai(n+1)\psi\circ\omega=1_{G_{n+1}^{2}/\langle a_{i(n+1)}a_{j(n+1)}=a_{j(n+1)}a_{i(n+1)}\rangle}. ∎

We proved that there are isomorphism from Gn,p2G_{n,p}^{2} to Hn,d2Gn,d2H_{n,d}^{2}\subset G_{n,d}^{2}(Theorem LABEL:theorem1) and isomorphism from Gn,d2G_{n,d}^{2} to Gn+12/ai(n+1)aj(n+1)=aj(n+1)ai(n+1)G_{n+1}^{2}/\langle a_{i(n+1)}a_{j(n+1)}=a_{j(n+1)}a_{i(n+1)}\rangle (Theorem LABEL:theorem2). From those theorems, it is followed that there is a monomorphism ωϕ\omega\circ\phi from Gn,p2G_{n,p}^{2} to Gn+12/ai(n+1)aj(n+1)=aj(n+1)ai(n+1)G_{n+1}^{2}/\langle a_{i(n+1)}a_{j(n+1)}=a_{j(n+1)}a_{i(n+1)}\rangle. It means that every braid of nn strands with parity can be presented by braid with (n+1)(n+1) strands up to forbidden moves by (n+1)(n+1)-th strand. That is, braids with parity are in itself. On the other hand, parity of braid has geometrical meaning: how (n+1)(n+1)-th strand is knotted with area, which is surrounded by other strans, see Fig. 9. In Fig. 9, the image of aij1a_{ij}^{1} by ωϕ\omega\circ\phi (n+1)(n+1)-th strand passes area in black, which is surrounded by ii-th and jj-th strands. Notice that the image of aij1a_{ij}^{1} by ωϕ\omega\circ\phi any relation in Gn+12G_{n+1}^{2} cannot be applied. That is, linking between (n+1)(n+1)-th strand and the area in black cannot be disappeared.

Conversely, for a braid β\beta with (n+1)(n+1) strands such that the number of crossings between ii-th and (n+1)(n+1)-th strands is even for every index in+1i\neq n+1, that is, a braid of nn strands with parity(or with points) can be obtained from βψ1(Hn,d2)\beta\in\psi^{-1}(H_{n,d}^{2}) by deleting one strand.

Refer to caption
Figure 9. The image of aij1a_{ij}^{1} by ωϕ\omega\circ\phi

Now define a mapping ψm:Gn+12Gn,d2\psi_{m}:G_{n+1}^{2}\rightarrow G_{n,d}^{2} by

ψm(aij)={τiifj=n+1,i<m,τi1ifj=n+1,i>m.aijifi,j<m,i,jn+1ai(j1)ifi<m,j>m,i,jn+1a(i1)(j1)ifi,j>m,i,jn+1\psi_{m}(a_{ij})=\left\{\begin{array}[]{cc}\tau_{i}&\text{if}~j=n+1,~i<m,\\ \tau_{i-1}&\text{if}~j=n+1,~i>m.\\ a_{ij}&\text{if}~i,j<m,~i,j\neq n+1\\ a_{i(j-1)}&\text{if}~i<m,j>m,~i,j\neq n+1\\ a_{(i-1)(j-1)}&\text{if}~i,j>m,~i,j\neq n+1\\ \end{array}\right.

Analogously ψm\psi_{m} is well-defined(see lemma 4.1). Then, for each braid β\beta of (n+1)(n+1) strands such that the number of crossings between ii-th and mm-the strands is even for each index imi\neq m, that is, βψm1(Hn,d2)\beta\in\psi_{m}^{-1}(H_{n,d}^{2}), and a braid with parity can be obtained.

Example 4.4.

Let β=a12a23a13a23a13a23a12a23\beta=a_{12}a_{23}a_{13}a_{23}a_{13}a_{23}a_{12}a_{23} in G32G_{3}^{2}. Note that ψm(β)H2,d2\psi_{m}(\beta)\in H_{2,d}^{2} for each index mm. Then

  • χ(ψ1(β))=χ(τ1a12τ2a12τ2a12τ1a12)=a121a120a121a1201,\chi(\psi_{1}(\beta))=\chi(\tau_{1}a_{12}\tau_{2}a_{12}\tau_{2}a_{12}\tau_{1}a_{12})=a_{12}^{1}a_{12}^{0}a_{12}^{1}a_{12}^{0}\neq 1,

  • χ(ψ2(β))=χ(τ1τ2a12τ2a12τ2τ1τ2)=χ(a12τ1a12τ1)=a120a1211,\chi(\psi_{2}(\beta))=\chi(\tau_{1}\tau_{2}a_{12}\tau_{2}a_{12}\tau_{2}\tau_{1}\tau_{2})=\chi(a_{12}\tau_{1}a_{12}\tau_{1})=a_{12}^{0}a_{12}^{1}\neq 1,

  • χ(ψ3(β))=χ(a12τ2τ1τ2τ1τ2a12τ2)=χ(a12τ2a12τ2)=a120a1211.\chi(\psi_{3}(\beta))=\chi(a_{12}\tau_{2}\tau_{1}\tau_{2}\tau_{1}\tau_{2}a_{12}\tau_{2})=\chi(a_{12}\tau_{2}a_{12}\tau_{2})=a_{12}^{0}a_{12}^{1}\neq 1.

Since ψm\psi_{m} is well defined, β\beta is not trivial in G32G_{3}^{2}.

As the above example, for given brad β\beta in ψm1(Hn,d2)Gn+12\psi_{m}^{-1}(H_{n,d}^{2})\subset G_{n+1}^{2}, if χ(ψm(β))1\chi(\psi_{m}(\beta))\neq 1, then β\beta is not trivial and mm-th strand of β\beta is important to be non-trivial for β\beta. And the following question is followed:
Assume that β\beta in ψm1(Hn,d2)Gn+12\psi_{m}^{-1}(H_{n,d}^{2})\subset G_{n+1}^{2} for each index mm. If β\beta it non-trivial in Gn+12G_{n+1}^{2}, then is there index mm such that χ(ψm(β))1\chi(\psi_{m}(\beta))\neq 1?

References

  • [1] V.G.Bardakov, The virtual and universal braids, Fundamenta Mathematicae, 2004, 184, 18 pages.
  • [2] V.G.Bardakov, P.Bellingeri and C.Damianti, Unrestricted virtual braids, fused links and other quotients of virtual braid group, Journal of Knot Theory and Its Ramification, 2015, vol. 24, no. 12.
  • [3] D.A.Fedoseev, V.O.Manturov, On marked braid groups, Journal of Knot Theory and Its Ramification, 2015, vol. 24, no. 13, 1541005, 12 pages.
  • [4] R.Fenn, R.Rimanyi, C.Rourke, The braid-permutation group, Topology, 1997, vol. 36, no. 1, p. 123-135.
  • [5] M.Goussarov, M.Polyak, O.Viro, Finite-type invariants of classical and virtual knots, Topology, Sep 2000 Volume 39, Issue 5, p. 1045-1068.
  • [6] S.Kim, V.O.Manturov, The group Gn2G_{n}^{2} and Invariants of free links valued in free Groups, Journal of Knot Theory and Its Ramification, 2015, vol. 24, no. 13, 1541010, 15 pages.
  • [7] V.O.Manturov, Free knots and parity, Sbornik : Mathematics, 2010, vol. 201, no. 5, p. 65-110.
  • [8] V.O.Manturov, Non-Reidemeister knot theory and its applications in dynamical systems, geometry, and topology, arXiv:1501.05208v1 [math.GT] 21 Jan 2015.
  • [9] V.O.Manturov, On groups Gn2G_{n}^{2} and Coxeter goups, arXiv:1512.09273v1 [math.GT] 31 Dec 2015.
  • [10] V.O.Manturov, I.M.Nikonov, On braids and groups GnkG_{n}^{k}, arXiv:1507.03745v1 [math.GT] 14 Jul 2015.