Geometrical Equivalence and Action Type Geometrical Equivalence of Group Representations
J. Simoes da Silva, A. Tsurkov

TL;DR
This paper demonstrates that action-type geometrical equivalence and group geometrical equivalence do not necessarily imply overall geometrical equivalence of group representations, highlighting limitations in current equivalence criteria.
Contribution
It provides a counterexample showing the non-implication between different types of geometrical equivalences in group representations.
Findings
Counterexample disproves the implication from action-type to overall geometrical equivalence.
Highlights the independence of different geometrical equivalence notions in group representations.
Clarifies limitations in the criteria for classifying group representations based on geometrical equivalence.
Abstract
In this paper we present the example which proves that we can not conclude the geometrical equivalence of group representations from the corresponding action-type geometrical equivalence and group geometrical equivalence.
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Taxonomy
TopicsGeometric and Algebraic Topology · Homotopy and Cohomology in Algebraic Topology · Advanced Operator Algebra Research
Geometrical Equivalence and Action Type Geometrical Equivalence of
Group Representations
J. Simões da Silva
A. Tsurkov.
Mathematical Department, CCET,
Federal University of Rio Grande do Norte (UFRN),
Av. Senador Salgado Filho, 3000,
Campus Universitário, Lagoa Nova,
Natal - RN - Brazil - CEP 59078-970,
Abstract
The universal algebraic geometry of group representations was considered in [10]. Thereat the concepts of geometrical equivalence and action type geometrical equivalence of group representations were defined. It was proved [10, Corollary 2 from Proposition 4.2.] that if two representations are geometrically equivalent then they are action type geometrically equivalent. Also it was remarked [10, Remark 5.1] that if two representations and are action type geometrically equivalent and groups and are geometrically equivalent, the representations and are not necessarily geometrically equivalent. But some specific counterexample was not presented. In this paper we present the example of two representations and which are action type geometrically equivalent and groups and are geometrically equivalent, but the representations and are not geometrically equivalent.
1 Introduction
All definitions of the basic notions of the universal algebraic geometry can be found, for example, in [5], [6], [7] and [8]. Also, there are fundamental papers [1], [4] and [2], [3].
Some problems of the universal algebraic geometry of many-sorted universal algebras were considered also in [10], [12], [13] and [14].
We consider the representations of groups over vector spaces over an arbitrary fixed field . This field is fixed in all our considerations. In this article the representation of group is a pair , where is a vector space over field and is a group. The signature of this algebraic object includes all the operations in the vector spaces (multiplication by every scalar we consider as unary operation), all the operations in the group and the operation of action of the on vector spaces . We denote this operation by :
[TABLE]
From here and below we will write briefly ”representation” instead ”representation of group”. The homomorphism : from representation to representation is a pair, where is a linear mapping and is homomorphism of groups, such that for every and every the equality
[TABLE]
holds. The reader can see that we consider representations as -sorted universal algebras: the first sort is a sort of vectors of vector spaces and the second sort is a sort of elements of groups. This approach to the representations the reader can find also in [11], [15], [10], [13].
The variety of all the representations of groups over a fixed field will be denoted by .
As usually, we say that
Definition 1.1
The representation is called the free representation generated by the sets and if, for every and every mappings and , there is only one homomorphism of representations , such that , .
It is easy to prove [11], that , where is the free group with the free set of generators , is the group ring over this group and is the free -module with the free basis .
2 Basic notions of the algebraic geometry of representations.
From here and below we suppose that the sets and of generators of the free representations are finite. Every equation in the algebraic geometry of representation is equivalent to the equation , where or to the equation , where for arbitrary and . So, in algebraic geometry of representations we can consider the system of equations , where , , or, briefly, . If we will resolve this system of equations in the representation , then the set has for us the role of the affine space. The solution of the system in will be the set
[TABLE]
[TABLE]
The algebraic -closure of the system will be the set
[TABLE]
[TABLE]
This is the maximal system of equations, which has the same solutions as the system .
Definition 2.1
Let . We say that and are geometrically equivalent if , for every and every and . We use the notation .
The notion of geometric equivalence can be defined in arbitrary variety of universal algebras, as one-sorted, as many-sorted. The reader can consult in [5].
In our theory
Definition 2.2
The logic formulas which have the form:
[TABLE]
where can be either or , for or ,, , are called quasi-identities.
Definition 2.3
Let We say that fulfills the quasi-identity (2.1) if, for every such that , when is , or , when is , , we have that , when is , or , when is . We denote:
[TABLE]
By [9, Theorem 2] we have the
Proposition 2.1
Let and then and fulfill same quasi-identities.
By [5, Proposition 13] we also have the
Proposition 2.2
Let some variety of universal algebras, are finitely generated. Then if and only if exist injections and , where are some sets of indexes and corresponding Cartesian powers of algebras and .
In [10] the action type algebraic geometry of representations was also considered. This geometry was elaborated on in order to avoid the influence of the algebraic geometry of the acting group on the algebraic geometry of representation.
In this geometry we consider only system of action type equations, i.e., system of equations which have form . The set of solutions of this system in the representation is the set
[TABLE]
The action type -closure of the system of equations is a set
[TABLE]
This is the maximal system of action type equations, which has the same solutions as the system .
Definition 2.4
Let . We say that and are action type geometrically equivalent if , for every and every and . We use the notation .
By [10, Corollary 2 from Proposition 4.2], if two representations and are geometrically equivalent then they are action type geometrically equivalent.
If , for every we can consider the stabilizer of , defined by
[TABLE]
and the , defined by
[TABLE]
It is easy to check that is a normal subgroup of . We denote by the quotient group and by the natural epimorphism . It also is easy check that we obtain the representation over the vector spaces if we define the action of the group over the vector spaces thusly
[TABLE]
where ,.
Definition 2.5
The representation is called the faithful image of the representation .
By [10, Corollary 4 from Theorem 5.1], we have the
Proposition 2.3
Every representation is action type geometrically equivalent to its faithful image .
3 The relation between geometrical equivalence and action type
geometrical equivalence ofgroup representations.
In this Section we will discuss the following question:
Problem 1
Let . Can we conclude the geometrical equivalence from the action type geometrical equivalence and the geometrical equivalence of groups ?
The negative answer to this question was remarked by [10, Remark 5.1], but no counterexample was presented. This question has a sense, because in the action type algebraic geometry of representations we only consider the specific systems of equations which have form and the specific form of the algebraic closure (2.2). By this restriction we avoid the influence of the algebraic geometry of action groups. But one question which comes naturally is whether we are losing some important information about representations by this restriction. The negative answer to the Problem 1 shows that we indeed lose some information.
Theorem 3.1
Let . From conditions
* and* 2. 2.
**
we can not conclude .
Proof. We consider a vector space over arbitrary field , such that , with the basis . We also consider the groups and . We define the action of and over thusly:
[TABLE]
[TABLE]
Hence, we obtain the representations and . . . Therefore, the faithful image of the representation is isomorphic to the representation . So, by Proposition 2.3 .
The injections and exist. Therefore, by Proposition 2.2, .
Now, we consider the quasi-identity
[TABLE]
We have that
[TABLE]
because , and
[TABLE]
because . It means by Proposition 2.1 that .
4 Acknowledgements
We acknowledge the support of Coordenação de Aperfeiçoamento de Pessoal de Nível Superior - CAPES (Coordination for the Improvement of Higher Education Personnel, Brazil).
We are thankful to Prof. E. Aladova for her important remarks, which helped a lot in writing this article.
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