• 検索結果がありません。

GENERALIZATIONS OF THE STANDARD ARTIN REPRESENTATION ARE UNITARY

N/A
N/A
Protected

Academic year: 2022

シェア "GENERALIZATIONS OF THE STANDARD ARTIN REPRESENTATION ARE UNITARY"

Copied!
7
0
0

読み込み中.... (全文を見る)

全文

(1)

REPRESENTATION ARE UNITARY

MOHAMMAD N. ABDULRAHIM

Received 27 October 2004 and in revised form 24 February 2005

We consider the Magnus representation of the image of the braid group under the gener- alizations of the standard Artin representation discovered by M. Wada. We show that the images of the generators of the braid group under the Magnus representation are unitary relative to a Hermitian matrix. As a special case, we get that the Burau representation is unitary, which was known and proved by C. C. Squier.

1. Introduction

The braid groupBnhas a well-known representation due to Artin in the group Aut(Fn) of automorphisms of the free groupFngenerated byx1,...,xn. The automorphism corre- sponding to the braid generatorσitakesxitoxixi+1xi1;xi+1toxi, and fixes all other free generators. Such a representation of the braid group by automorphisms of a free group was proved to be faithful [3, page 25].

InSection 2, we present an infinite series of representations generalizing the standard Artin representation, which were discovered by Wada [8]. More precisely, for an arbitrary nonzero integerk, the automorphism corresponding to the braid generatorσitakesxito xikxi+1xik;xi+1toxi, and fixes all other free generators. Shpilrain has shown that these representations are indeed faithful [6, page 773].

InSection 3, after having defined the automorphism corresponding to the braid gen- erator, suggested by Wada, we apply the Magnus representation to these subgroups of Aut(Fn) to get linear irreducible representationsBnGLn1(C[t±1]). We show that for any nonzero integerk, the linear representations obtained are unitary relative to a Her- mitian matrix. In particular, this shows that the Burau representation, namely when k=1, is conjugate to an ordinary unitary representation; which was proved by Squier [7].

Showing that Wada’s representations are unitary might possibly help us to determine whether or not such matrix representations of the braid group are faithful. A similar argument was done in the case of the standard Artin representation (see [1, page 1257]).

It was known that fork=1, the Burau representation is not faithful forn6 [5]. It is now known that the Burau representation forn=5 is not faithful [2].

Copyright©2005 Hindawi Publishing Corporation

International Journal of Mathematics and Mathematical Sciences 2005:8 (2005) 1321–1326 DOI:10.1155/IJMMS.2005.1321

(2)

2. Definitions

The braid group onnstrings,Bn, is the abstract group with generatorsσ1,...,σn1and a presentation as follows:

σiσi+1σi=σi+1σiσi+1, i=1, 2,...,n2,

σiσj=σjσi, |ij| ≥2. (2.1) According to the standard Artin representation, the automorphism corresponding to σisendsxitoxixi+1xi1;xi+1toxi, and fixes all other free generators.

Definition 2.1. The generalizations of the standard Artin representation, discovered by Wada, assert that the automorphism corresponding toσitakes

xi−→xikxi+1xik, xi+1−→xi, xj−→xj forj=i,i+ 1.

(2.2)

By applying the Magnus representation to the image of the braid group under the gen- eralization of the standard Artin representation, we determine the linear representations BnGLn(C[t±1]) [3]. The automorphismσiis mapped onto then×nmatrix which dif- fers from the identity only by a 2×2 block with the top-left corner in the (i,i)th place.

More precisely,

σi(t)=

Ii1 0 0

0 1tk tk

1 0 0

0 0 Ini1

fori=1, 2,...,n1. (2.3)

It is clear that the subspace generated by the column vector (1, 1,..., 1)T is invariant under this representation, whereTis the transpose. Therefore, these representations, for different values ofk, are reducible.

Definition 2.2. LetkZ− {0}. Wada’s representations{φk}:BnGLn1(C[t±1]) are a family of linear irreducible representations defined asφk(σi)=In1AiBi, where

A1=

tk+ 1,1, 0, ..., 0

n3

T

, Ai=

0, ..., 0

i2

,tk,tk+ 1,1, 0,... , 0

ni2

T

,

An1=

0, ..., 0

n3

,tk,tk+ 1

T

,

(2.4)

fori=2,...,n2.

Here,{B1,...,Bn1}is the standard basis ofCn1.

(3)

These representations are irreducible by [4, Theorem 5]. Notice that the representation φ1is (conjugate to) the reduced Burau representation of the braid group as presented in [4].

3. Wada’s representations are unitary

Notation 3.1. Let () :Mm(C[t±1]) be an involution defined as follows:

fij(t)=fji

t1, fij(t)C

t±1. (3.1)

Definition 3.2. LetXandUbe elements of GLn1(C[t±1]).Uis called a unitary element (relative toX) ifUXU=X.

Now define the following (n1)×(n1) matrix,M, in a way that each column looks like (0,..., 0,tk,tk+ 1,1, 0,..., 0)T, wheretk+ 1 is a diagonal entry andTis the trans- pose. More precisely, we have

M=

tk+ 1 tk 0 ··· ··· 0

1 tk+ 1 tk 0 ··· ... 0 1 tk+ 1 tk ··· ...

0 0 1 . .. . .. 0

... ... ··· 0 tk+ 1 tk

0 0 ··· 0 1 tk+ 1

. (3.2)

For simplicity, we denote the matrixφki) corresponding to the braid generator,σi, under Wada’s representations, byXk,i, whereXk,i=In1AiBi, whereAi,Biare given by Definition 2.2.

We now prove our main theorem.

Theorem 3.3. The images of the generators of Bnunder Wada’s representations, φk, are unitary relative toM, that is, for1in1,

Xk,iMXk,i

=M. (3.3)

Proof.

Xk,iMXk,i

=

IAiBi

MIAiBi

=MAiBiMMBiAi+AiBiMBiAi. (3.4) Having done some computations, we get

AiBiM=tkAiAi, MBiAi=AiAi, AiBiMBiAi=

tk+ 1AiAi.

(3.5)

(4)

So,

Xk,iMXk,i

=M+AiAi

tk1 +tk+ 1=M. (3.6) Now we viewC[t±1] as a subring ofC[u,u1], whereu2=t. LetN=ukM, then by direct substitution, we get

N=

uk+uk uk 0 ··· ··· 0

uk uk+uk uk 0 ··· ... 0 uk uk+uk uk ··· ...

0 0 uk . .. . .. 0

... ... ··· 0 uk+uk uk

0 0 ··· 0 uk uk+uk

. (3.7)

It is clear thatN is Hermitian (N=N) andXk,iN(Xk,i)=N. Next, our objective is to show that a certain specializationNofN is equivalent to the identity matrix in some extension field, that is, for some matrixU, we have that

N=UU. (3.8)

From linear algebra, it is well known that a Hermitian matrix is positive definite if and only if each of the principal minors is positive. In that case, the matrix will be equivalent to the identity matrix.

The principal minors ofNare of the form det(Dm), where 1mn1 andDmis an m×mmatrix (upper-left corners ofN). It is then easy to see the following lemma.

Lemma3.4. Lett=u2andu=1, then under this specialization, for1mn1, detDm

=m+ 1. (3.9)

Proof. By induction onm, we get

detDm

= u2(m+1)k1

umku2k1=umku2mk+u2(m1)k+···+u2k+ 1. (3.10)

Havingu=1, we get that det(Dm)=m+ 1.

Letu=a, whereais a complex number lying in an open arc around 1 on the unit circle. By having an explicit formula for the principal minors ofNas inLemma 3.4, it is then possible to completely determine the arc around 1 whereabelongs to. The choice of this arc depends on the values ofkandn. Along the same lines as in [1, pages 1254–1255], we can easily get the following lemma.

(5)

Lemma3.5. Letabe a complex number on the unit circle. Thendet(Dm)is positive for all m=1, 2,...,n1if and only ifalies in an open arc around1bounded byeπi/knandeπi/kn. Hence, the matrixN is a positive definite Hermitian matrix under the complex spe- cializationu=abelonging to the open arc bounded byeπi/knandeπi/kn. We denote this matrix byN. By a theorem in linear algebra, there exists a matrixUsuch that

N=UU. (3.11)

As in [1, page 1255], the next theorem shows that a conjugate of Wada’s representation is unitary. Here, a matrixXis unitary ifXX=XX=I.

Theorem3.6. The complex specialization of Wada’s representation ofBn(havingt=u2= a2andais around1) is conjugate to an ordinary unitary representation.

Proof. Consider the composition map Bn φk

GLn1

C u,u1

f

GLn1(C)

(3.12)

Let f(Xk,i) be the image ofXk,iunder the complex specializationu=a, wherealies in an arc around 1 bounded byeπi/knandeπi/kn.

Having thatN=UU, we letV=U1f(Xk,i)U, then it is clear that

VV=VV=I. (3.13)

Notice that, under the casek=1,Theorem 3.6implies that the specialization of the Burau representation is conjugate to an ordinary unitary representation; which was proved by Squier [7].

Acknowledgment

This note is in final form and no version of it will be submitted for publication elsewhere.

References

[1] M. N. Abdulrahim,A faithfulness criterion for the Gassner representation of the pure braid group, Proc. Amer. Math. Soc.125(1997), no. 5, 1249–1257.

[2] S. Bigelow,The Burau representation is not faithful forn=5, Geom. Topol.3(1999), 397–404.

[3] J. S. Birman,Erratum: “Braids, Links, and Mapping Class Groups,”(Ann. of Math. Studies, no.

82, Princeton University Press, New Jersey, 1974), Princeton University Press, New Jersey, 1975.

[4] E. Formanek,Braid group representations of low degree, Proc. London Math. Soc.73(1996), no. 3, 279–322.

[5] D. D. Long and M. Paton,The Burau representation is not faithful forn6, Topology32(1993), no. 2, 439–447.

(6)

[6] V. Shpilrain,Representing braids by automorphisms, Internat. J. Algebra Comput.11(2001), no. 6, 773–777.

[7] C. C. Squier,The Burau representation is unitary, Proc. Amer. Math. Soc.90(1984), no. 2, 199–202.

[8] M. Wada,Group invariants of links, Topology31(1992), no. 2, 399–406.

Mohammad N. Abdulrahim: Department of Mathematics, Faculty of Science, Beirut Arab Uni- versity, P.O. Box 11-5020, Beirut 1107 2809, Lebanon

E-mail address:[email protected]

(7)

Special Issue on

Time-Dependent Billiards

Call for Papers

This subject has been extensively studied in the past years for one-, two-, and three-dimensional space. Additionally, such dynamical systems can exhibit a very important and still unexplained phenomenon, called as the Fermi acceleration phenomenon. Basically, the phenomenon of Fermi accelera- tion (FA) is a process in which a classical particle can acquire unbounded energy from collisions with a heavy moving wall.

This phenomenon was originally proposed by Enrico Fermi in 1949 as a possible explanation of the origin of the large energies of the cosmic particles. His original model was then modified and considered under different approaches and using many versions. Moreover, applications of FA have been of a large broad interest in many different fields of science including plasma physics, astrophysics, atomic physics, optics, and time-dependent billiard problems and they are useful for controlling chaos in Engineering and dynamical systems exhibiting chaos (both conservative and dissipative chaos).

We intend to publish in this special issue papers reporting research on time-dependent billiards. The topic includes both conservative and dissipative dynamics. Papers dis- cussing dynamical properties, statistical and mathematical results, stability investigation of the phase space structure, the phenomenon of Fermi acceleration, conditions for having suppression of Fermi acceleration, and computational and numerical methods for exploring these structures and applications are welcome.

To be acceptable for publication in the special issue of Mathematical Problems in Engineering, papers must make significant, original, and correct contributions to one or more of the topics above mentioned. Mathematical papers regarding the topics above are also welcome.

Authors should follow the Mathematical Problems in Engineering manuscript format described at http://www .hindawi.com/journals/mpe/. Prospective authors should submit an electronic copy of their complete manuscript through the journal Manuscript Tracking System athttp://

mts.hindawi.com/according to the following timetable:

Manuscript Due December 1, 2008 First Round of Reviews March 1, 2009 Publication Date June 1, 2009

Guest Editors

Edson Denis Leonel,Departamento de Estatística, Matemática Aplicada e Computação, Instituto de Geociências e Ciências Exatas, Universidade Estadual Paulista, Avenida 24A, 1515 Bela Vista, 13506-700 Rio Claro, SP, Brazil ; [email protected]

Alexander Loskutov,Physics Faculty, Moscow State University, Vorob’evy Gory, Moscow 119992, Russia;

[email protected]

Hindawi Publishing Corporation http://www.hindawi.com

参照

関連したドキュメント

In [14]-[15] it is proved the well-posedness of boundary value problems for a one-dimensional wave equation in a rectangular domain in case when boundary conditions are given on

In Section 4, we determine new representation numbers for split graphs (graphs that are the disjoint union of a complete graph and an independent set). Later in Section 5,

Keywords Jones representation, mapping class group, Torelli group, Johnson homomorphism..

Livingstone and Wagner proved that the number of orbits of G on k-subsets of is less than or equal to the number of orbits on (k + 1)-subsets.. In [7] Livingstone and Wagner proved

In Section 3, in The- orem 3.1, we show that under some additional conditions the representation theorem yields explicit asymptotic formulas for the solutions of the linear

Abstract The representation theory (idempotents, quivers, Cartan invariants, and Loewy series) of the higher-order unital peak algebras is investigated.. On the way, we obtain

A crucial physical prescription is that the field must be covariant under the action of a unitary representation U(g) of some transformation group (such as the Poincaré or Lorentz

In our previous paper [Ban1], we explicitly calculated the p-adic polylogarithm sheaf on the projective line minus three points, and calculated its specializa- tions to the d-th