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The linear deformation of discrete groups
by
Petr Yagodovsky
Moscow State University
The report informs about the construction of deformation of discrete groups in the class of multivalued groups.
Defenition ([]). The set S with maping \mu: S×S --> (S)n (here (S)n is the symmetric power of S) is called the n-valued group if S and \mu obey the following laws. (1) The law of assoctativety: for allx, y, z in S \mu(x, \mu(y, z)) = \mu(\mu(x, y), z). (2) The law of groups unit: existse in S for allx in S \mu(e, x) = \mu(x, e) = (x, ... , x). (3) The law of inverse element existence. for allx in S existsx' in S Cex, x' > 0 and Cex', x > 0. Here Czx, y > 0 is the multiplicity of z in \mu(x, y). The mapping \mu is called the production.
Defenition ([]). Let A be an algebra with a fixed basis and S be some n-valued group. Let elements of this basis are one to one correspond to elements of S. We will denote as [x\tilde] the basis element of A corresponding to x in S. Let the structural constants c[z\tilde][x\tilde], [y\tilde] be equal to [ 1/n]Czx, y > 0. Then the algebra is called the group algebra of the n-valued group S.
The main construction ([]). Let us consider V = RN(N-1)2 with coordinates cki, l . Let us define the manifold of associative algebras dimension N with a unit and a fixed basis MNass as the surface in V corresponding to solutions of equations of associativety. Let A be a group algebra of some n-valued group S and x be the point on the surface MNass which correspondents to the algebra A. Let us consider the set of lines, which is tangential to MNass in the point x. There are a lot of examples, when some of such lines are lines on the surface MNass.
Defenition . Let A and B be two group algebras of multivalued groups S and C. Let x and y be the points on the surface MNass, which correspondent to A and B. Let the line which passes through the points x and y in the space V lie on MNass. Then the group C is called the linear deformation of the group S.
Let G be a discrete group in the
usual sense. Then a linear deformation of the
group G may be written on the form:
where L = \sumr in GLr
is a 2-cocycle of G with the coefficients in the
ad-representation of G.
i*j=
Е
r in G
Lr(i, j)(r·i·j) i, j in G,
Is the case of abelian group G, there is the special class of cocycles L(i, j) = (1-Lr(i, j))e-Lr(i, j)r. Linear deformations corresponding to the cocycles are called regular deformations. It turns, for for alli in N there is the cocycle Li of the group Zi, such that for any regular deformation of a finite abelian group G defining by a pair (L, r) there are the integer number i and projection pi: G --> Zi, with L = pi*Li, and either pi(r) = 0 or pi(r) = 1. If G is Z then pairs (L, r) (where L = pi*Li and either p(r) = 0 or p(r) = 1) defines periodic regular deformations. Any regular deformations of group Z which is not periodic may be build by appicating the special construction to periodic regular deformations.
Linear deformations of the groups Z3, Z4 and Z2\otimesZ2 are classified. It is interesting, that Z4 is the linear deformation of Z2\otimesZ2. The following diagrams describe the sets of deformations of Z4 (see a)) and Z2\otimesZ2 (see b)).
Date received: June 16, 1999
Copyright © 1999 by the author(s). The author(s) of this document and the organizers of the conference have granted their consent to include this abstract in Atlas Conferences Inc. Document # cacy-41.