亚洲免费av电影一区二区三区,日韩爱爱视频,51精品视频一区二区三区,91视频爱爱,日韩欧美在线播放视频,中文字幕少妇AV,亚洲电影中文字幕,久久久久亚洲av成人网址,久久综合视频网站,国产在线不卡免费播放

        ?

        The Mod 2 Kauffman Bracket Skein Module of Thickened Torus

        2018-01-19 02:41:24YANXINMINGANDSUNMENG

        YAN XIN-MINGAND SUN MENG

        (1.Department of Mathematics,Guangdong University of Education,Guangzhou,510303)

        (2.The China-Russian Joint Training Graduate School,Heilongjiang University,Harbin,150080)

        Communicated by Lei Feng-chun

        1 Introduction

        We are concerned with framed links in thickened torusT2×Iby using skein theory.We will extend the Kauffman bracket skein module to the mod 2 Kauffman bracket skein module and obtain an expression of a framed link as a new ambient isotopic invariant.

        Skein relations have their origin in an observation by Alexander[1],Conway found a way to calculate the Alexander polynomial of a link using a so-called skein relation[2].This is an equation that relates the polynomial of a link to the polynomial of links obtained by changing the crossings in a projection of the original link.Skein modules were introduced by Przytycki in[3].Skein modules are quotients of free modules over ambient isotopy classes of framed links in a 3-manifold by properly chosen local skein relations.The skein module based on Kauffman bracket skein relation is one of the most extensively studied object of the algebraic topology based on framed links,which is also an important invariant of 3-manifolds.There have been extensive study and application of Kauffman bracket skeinmodule(see[4]–[8]).

        If we work with regular projections of links,then the topology of links is reflected by Reidemeister moves.Regular isotopy is the equivalent relation on link projections generated by the Reidemeister moves of types II and III.The Reidemeister moves of types II and III on the cores of bands extend to the bands themselves,while the type I move dose not extend(it corresponds to a full twist on the band).Consequently,regular isotopy corresponds to ambient isotopy of framed links.

        Noted that torus knot is a kind of knot that had been investigated and used widely(see[9]).We are concerned in this paper with the torus knot,which is defined below.Given two generatorsx1,x2inπ1(T2),where

        and consider the closed curve

        If(p,q)=(0,0)orp,qare relatively prime,thenγis called a(p,q)knot inT2,denoted byK(p,q).Obviously,

        This paper is organized by two sections:In Section 2,we cover the necessary definitions and lemmas.The main result and its proof are provided in Section 3.

        2 Preliminary

        The data that determine a knot in R3are usually given by a projection onto a plane.Now we derive it in thickened surfaceF×Ias inR3.

        Definition 2.2[10]A projection ? of a framed link L is called regular if

        (1)? is an immerse;

        (2)there are only finitely many intersections in ? and all intersections are double points;

        (3)? is transverse to the every intersection point.

        Moreover,if the upper crossing line and the lower crossing line are marked at every double point in a regular projection,then this regular projection of a link is called a link projection.

        We work always in the smooth-category.We do not make any distinction between two ambient isotopic framed links,while two framed links,LandL′,inMare said to be ambient isotopic if there is a smooth orientation preserving automorphismh:M→Msuch thath(L)=L′.

        Then we give the definition of the Kauffman bracket skein module ofF×Ifor an oriented surfaceFand an intervalIas follows:

        Definition 2.3[3],[11]The Kauffman bracket skein module of3-manifold F×I,S2,∞(F×I;R,A)is defined as follows:Let L be the set of unoriented framed links in F×I(including the empty knot ?),R any commutative ring with identity and A an invertible element in R.Let RL be the free R-module generated by L,S2,∞be the submodule of RL generated by two skein expressions:L+?AL0?A?1L∞,L?T1+(A2+A?2)L,where the triple L+,L0and L∞as presented by their regular projections ?+,?0and ?∞on F are shown in Fig.2.1,which can be ambient isotopy except within the neighborhood shown,and T1denotes the trivial framed knot.Set S2,∞(F×I;R,A)=RL/S2,∞.The notation is shortened for special case:

        Fig.2.1 Link projections

        From the above definition,we have:

        Proposition 2.1For a framed link L in F×I,its expression in S2,∞(F×I)is an ambient isotopic invariant of L.

        Moreover,the expression ofLin the free module is unique.Hence,it is an ambient isotopic invariant of the framed linkL.

        The following lemmas are used later.

        Lemma 2.1[8]S2,∞(F×I;R,A)is a free R-module with a basis B(F)consisting of links in F without contractible components(but including the empty knot).

        Lemma 2.2[9]Suppose that K(p,q)and K(p′,q′)are two knots in T2.If K(p,q)∩K(p′,q′)=?,then K(p,q)=K(p′,q′)or one of them is K(0,0).

        3 Main Results

        Beginning with our main ingredient,we consider the special caseT2×I.GivenS2,∞(T2×I;R,A)the Kauffman bracket skein module ofT2×Iand

        For a framed linkLinT2×I,by Lemma 2.1,its expression in the free moduleS2,∞(T2×I)is presented as

        whereK(pi,qi)is a(pi,qi)knotinT2.

        Proof.Suppose thatLis a framed link inT2×Iwith framing(?1,···,?k).By skein expression,we have

        By the first skein expression of Definition 2.3,we also have

        it is followed that

        whereSdenotes one of the states of?;

        obviously,a(S)+b(S)=V(?);LSdenotes the framed link without crossing in the stateS,including contractible components.In fact,LSis a union of some(p,q)knots inT2.

        Nextly,by the second skein expression of Definition 2.3,we see

        wherem(S)denotes the number of contractible components,andn(S)denotes the number of uncontractible components.

        From the above analysis we obtain

        By Lemma 2.1,the expression ofLis unique after collecting the link terms.

        Without loss of generality we assume that

        which decides the direction of four paths as shown in Fig.3.1.

        Fig.3.1 The directions of four paths

        We are now in a position to discuss the following three cases:

        Case 1.Provided thatαWS(1)=αES(0),αWN(1)=αEN(0),we have

        Fig.3.2 The link projections for Case 1

        Notice that in?(xi,0),αWN?αEN∩αWS?αES=?.Using Lemma 2.2,we can now deriveαWN?αEN=αWS?αESor one ofαWN?αEN,αWS?αESisK(0,0).The results of these calculations are given in Table 3.1.

        It should be noted that the subtraction here is a formal subtraction,and the result of each subtraction is obtained by the analysis of actual?(xi,0)and?(xi,∞).Besides,for unoriented(p,q)knot,K(p,q)=K(?p,?q).

        Table 3.1 The results for Case 1

        It follows from Table 3.1 that there exists a uniqueK(p,q)∈π1(T2),such that

        Case 2.Provided thatαWS(1)=αEN(0),αWN(1)=αES(0),we have

        see Fig.3.3.

        Fig.3.3 The link projections for Case 2

        Case 3.Provided thatαWS(1)=αWN(1),αEN(0)=αES(0),we have

        Fig.3.4 The link projections for Case 3

        By Lemma 2.2,we also have the results in the Table 3.2.

        Table 3.2 The results for Case 3

        It follows from Table 3.2 that there exists a uniqueK(p,q)∈π1(T2),such that

        being an ambient isotopic invariant ofLby Proposition 2.1.

        We complete the proof.

        [1]Alexander J W.Topological invariants of knots and links.Trans.Amer.Math.Soc.,1928,30(2):275–306.

        [2]Conway J H.An enumeration of knots and links,and some of their algebraic properties.in:1970 Computational Problems in Abstract Algebra Proc.Conf.,Oxford:Pergamon,1967,pp.329–358.

        [3]Przytycki J H.Skein modules of 3-manifolds.Bull.Polish.Acad.Sci.Math.,1991,39(1-2):91–100.

        [4]Bullock D,Przytycki J H.Multiplicative structure of Kauffman bracket skein module quantizations.Proc.Amer.Math.Soc.,2000,128(3):923–931.

        [5]Bullock D.A finite set of generators for the Kauffman bracket skein algebra.Math.Z.,1999,231:91–101.

        [6]Bullock D.Rings of SL2(C)-characters and the Kauffman bracket skein module.Comment.Math.Helv.,1997,72(4):521–542.

        [7]Hoste J,Przytycki J H.Homotopy skein modules of orientable 3-manifolds.Math.Proc.Cambridge Philos.Soc.,1990,108(3):475–488.

        [8]Przytycki J H.Fundamentals of Kauffman bracket skein modules.Kobe J.Math.1999,16(1):45–66.

        [9]Rolfsen D.Knots and Links.in:Mathematics Lecture Series,No.7.Berkeley:Publish or Perish,Inc.,1976:53–55.

        [10]Yan X M.Estimating the self-intersection number of closed curves on surface by knot method.Geom.Dedicata,2015,175:65–67.

        [11]Hoste J,Przytycki J H.A survey of skein modules of 3-manifolds.in:Knots 90,Proceedings of International Conference on Knot Theory and Related Topics,Osaka(Japan),August 15–19,1990,(ed.Kawauchi A.),Berlin:Walter de Gruyter,1992:363–379.

        亚洲av极品尤物不卡在线观看| 国产精品亚洲欧美云霸高清| 国产尤物av尤物在线观看| 精品欧洲av无码一区二区| 二区三区视频| 美女露屁股无内裤视频| 国产自产二区三区精品| 手机在线看片| 免费无码黄动漫在线观看| 亚洲AV无码永久在线观看| 久久久噜噜噜噜久久熟女m| 国产在线无码精品无码| 免费观看18禁无遮挡真人网站| 丰满人妻无奈张开双腿av| 久国产精品久久精品国产四虎| 激情五月婷婷久久综合| 久久这里都是精品99| 精品国产av色一区二区深夜久久 | 精品人妻伦一二三区久久| 国产熟女露脸大叫高潮| 国产一区二区三区精品久久呦| 人妻少妇中文字幕久久hd高清 | 曰韩人妻无码一区二区三区综合部| 午夜高清福利| 国产在线高清无码不卡| 亚洲国产人成综合网站| 国产无吗一区二区三区在线欢| 丰满人妻被中出中文字幕| 精品三级久久久久久久| 久久综合激情的五月天| 精品无码国产自产拍在线观看| 成年视频国产免费观看| 日本高清一区二区在线观看| 婷婷色婷婷开心五月四| 男人扒开女人下面狂躁小视频| 欧美自拍丝袜亚洲| 狼人狠狠干首页综合网| 免费看美女被靠到爽的视频| 久久精品成人无码观看不卡| 巨爆乳中文字幕爆乳区| 日本人妻伦理片在线观看|