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IJMMS 2004:7, 373–375 PII. S0161171204304047 http://ijmms.hindawi.com

© Hindawi Publishing Corp.

POWERS OF A PRODUCT OF COMMUTATORS AS PRODUCTS OF SQUARES

ALIREZA ABDOLLAHI Received 1 April 2003

We prove that for any odd integerNand any integern >0, theNth power of a product of ncommutators in a nonabelian free group of countable infinite rank can be expressed as a product of squares of 2n+1 elements and, for all such oddNand integersn, there are commutators for which the number 2n+1 of squares is the minimum number such that the Nth power of its product can be written as a product of squares. This generalizes a recent result of Akhavan-Malayeri.

2000 Mathematics Subject Classification: 20F12, 20F99.

1. Introduction. Lyndon et al. [2] have shown that the product ofncommutators in a nonabelian free group can be written as a product of 2n+1 squares of elements and there are commutators for which the number 2n+1 of squares is the minimum number such that the product of these commutators can be written as a product of squares. Recently, Akhavan-Malayeri [1] proved, for an odd integern, that[x,y]n of two distinct elements of a free generating set of a nonabelian free group is not a product of two squares but it is the product of three squares. We generalize these results in the following theorem.

Theorem1.1. LetFbe a free group with a basis of distinct elementsx1,...,x2n, and Nany odd integer. Then there exist elementsu1,...,uminF such that

x1,x2

···

x2n−1,x2nN=u21···u2m (1.1) if and only ifm≥2n+1.

Note that the theorem for evenNis not true since the element in the left-hand side of the above equation is actually a square. The proof of this theorem is almostmutatis mu- tandisas the proof of the main result of [2]. Throughout this note,[x,y]=x−1y−1xy and [x,y,z]=[[x,y],z]for all elementsx,y, zof a groupG, andGdenotes the derived subgroup ofG.

2. Proof of the main result

Proof ofTheorem1.1. We show first that this equation has a solution form= 2n+1, hence trivially form≥2n+1. SinceNis odd, there is an integerksuch that N=2k+1. Thus it is enough to show that, for any elementv ofF, we can express the elementv2[x1,x2]···[x2n−1,x2n]as a product of 2n+1 squares. We argue by

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374 ALIREZA ABDOLLAHI

induction onn. Ifn=1, then by the following well-known identity this case is proved:

A2[B,C]=

A2B1A12

ABA1C1A12

(AC)2. (2.1)

Assumen >1 and suppose inductively that v2

x1,x2

···

x2n−3,x2n−2

=u21···u22n−1 (2.2)

for some elementsu1,...,u2n−1inF. Now by the identity (2.1) we can write u22n−1

x2n−1,x2n

=U2V2W2 (2.3)

for some elementsU,V, andWinF, and so v2

x1,x2

···

x2n−1,x2n

=u21···u22n−2U2V2W2, (2.4) which completes the induction. This first part of the proof is essentially well known in a topological context: the nonorientable surface formed by attaching one cross-cap and n handles to a sphere (the connected sum of 1 projective plane and ntori) is homeomorphic to the surface obtained by attaching 2n+1 cross-caps (the connected sum of 2n+1 projective planes). In this context, the identity (2.1) is just the handle calculus that says cross-cap + handle=3 cross-caps.

For the converse, we suppose that the equation holds. LetGbe the group with the following presentation:

yi|yi2=

yi,yj,yk

=1∀i,j,k∈ {1,2,...,2n}

. (2.5)

The equation would also hold inGsinceGis a quotient ofF. So we have y1,y2

···

y2n−1,y2n

N

=v12···vm2 (2.6) for some elementsv1,...,vminG. SinceNis odd,N=2t+1 for some integert. Since Gis nilpotent of class 2 andyi2=1 for eachi, we have[yi,yj]2=1 and all the com- mutators are in the center ofG, so the latter equation can be rewritten as

y1,y2

···

y2n−1,y2n

=v12···vm2. (2.7)

Letcij=[yi,yj]. Then each elementvofGhas a unique expression v=y1a1···y2na2n

i<j

cijdij forai,dijZ2. (2.8)

Let

vk=y1a1k···y2na2nkzk, (2.9) whereaikZ2andzk∈Gfor alli∈ {1,...,2n}and allk∈ {1,...,m}. Sincez2k=1 for allk, we have

v12···vm2 =

i<j

c

m k=1aikajk

ij . (2.10)

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A PRODUCT OF COMMUTATORS 375 IfA is the matrixA=(aij)overZ2, andAi=(ai1,...,aim)is the ith row ofA, then from the relationv12···vm2 =[y1,y2]···[y2n−1,y2n]we conclude that, taking inner products,

Ai·Aj=



1 if{i,j} = {2h−1,2h}for 1≤h≤n,

0 otherwise. (2.11)

We conclude thatA·AT=B, whereAT is the transpose ofA, andBis the direct sum of nmatrices of the form1 0

0 1

, and hence has rank 2n. It follows that rank(A)≥2n. But the equationAi·Ai=m

j=1aijaij=0 for eachiimplies that the sum of the columns of Ais 0, whence rank(A)≤m−1. Thereforem−12n.

References

[1] M. Akhavan-Malayeri,Powers of commutators as products of squares, Int. J. Math. Math. Sci.

31(2002), no. 10, 635–637.

[2] R. Lyndon, T. McDonough, and M. Newman,On products of powers in groups, Proc. Amer.

Math. Soc.40(1973), 419–420.

Alireza Abdollahi: Department of Mathematics, University of Isfahan, Isfahan 81746-73441, Iran

E-mail address:[email protected]

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Mathematical Problems in Engineering

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 at

http://

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]

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

[email protected]

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

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