Abstract
Hypergroups represent a generalization of groups, introduced by Marty, that are rich in applications in several sectors of mathematics and in other fields. An important class of hypergroups called join spaces is presented in this paper, along with some connections to lattice theory, in particular, to modular and to distributive lattices. In particular, we study join spaces associated with chains through functions and we analyze when such join spaces are isomorphic. Moreover, a combinatorial problem is presented for a finite context, focusing on calculating the number of isomorphisms classes of join spaces.
MSC:
20N20
1. Introduction
The composition of two elements is an element in groups, while in an algebraic hypergroup, the composition of two elements is a nonempty subset. F. Marty observed that the elements of a factor group are subsets and this was the starting point for hypergroup theory, see [1].
He introduced the hypergroup concept in 1934 at the 8th Congress of the mathematicians from the Scandinavian countries. Over time, new results have also appeared interesting, but especially since the 1970s, this theory developed a lot in Europe, the United States, Asia, and Australia. Some sound names in this field such as Dresher, Ore, Koskas, and Krasner made contributions in the field of homomorphisms of hypergroups and in the theory of subhypergroups.
Hypergroups have applications in several sectors of mathematics and in other fields, see [2]. Complete parts were studied by Koskas, then by Corsini, Leoreanu, Davvaz, Vougiouklis, and Freni.
Fundamental equivalence relations are important in algebraic hyperstructures because they establish a natural connection between algebraic hyperstructures and classical algebraic structures. The relation connects the class of hypergroups to the class of groups. More exactly, the quotient of a hypergroup has a group structure. Using relation , Migliorato defines the notion of an n-complete hypergroup.
In [3], basic notions and results about algebraic hypergroups are presented, in particular about semihypergroups, hypergroups, subhypergroups, homomorphisms and isomorphisms, fundamental relations and the corresponding quotient structures, join spaces, canonical hypergroups, Rosenberg hypergroups, topological hypergroups, and also connections with hypergraphs and n-ary relations, while in [4] hyperstructures and their representations are studied.
Hyperlattices were introduced in 1994 by Mittas and Konstantinidou, see [5], and later on they were studied by many mathematicians, see, e.g., [6,7]. Connections between hypergroups and lattices or hyperlattices have been considered and analyzed by Nakano [8] and Varlet [9], then by Comer [10] and later by Kehagias, Konstantinidou, and Serafimidis [11,12], Călugăreanu and Leoreanu [13], Tofan and Volf [14], and Njionou, Ngapeya and Leoreanu-Fotea [15].
2. Join Spaces and Connections with Lattices
In this section, we present the join space notion and we analyze some connections with lattice theory.
Let A function is called a hyperoperation, where denotes the set of nonempty subsets of H.
If are subsets of H, then
The structure is a hypergroup if for all of H we have
For all elements , denote
Definition 1.
A hypergroup is called a join space if it is commutative and for all of H, we have
In other words,
The condition (1) is often called the join space condition.
Join spaces were defined by W. Prenowitz. He and J. Jantosciak applied them in both Euclidean and non-Euclidean geometry, see [16]. Using join spaces, descriptive, projective, and spherical geometry were subsequently rebuilt.
Join spaces can be also studied in connections with binary relations, fuzzy sets, or rough sets, see [2,17].
We present here some examples of join spaces:
Example 1.
Let H be a non-empty set. If R is an equivalence relation on it, then denote the equivalence class of by and define the next hyperoperation on H:
Then, is a join space.
For all we have whence is a commutative hypergroup. Moreover, if and there is such that then
If then Similarly, if then
If and then and whence hence Therefore, is a join space.
Example 2.
Let be a commutative group. For all consider a nonempty set such that if , then
Set and
For all we define Then, is a join space.
Indeed, it can be checked that and
Now, if are such that then and , whence and .
Hence, , so Thus, is a join space.
Example 3.
Consider a hypergroup and a commutative group. Consider a family of nonempty sets, such that and for We define the next hyperoperation on
Then, is a join space if and only if is a join space.
Let be a join space.
We have , since is a group. The associativity law holds.
Moreover, if then
Similarly, if then Thus, , whence .
If , then
If , then we use the fact is a join space.
Therefore, is a join space.
Conversely, suppose that is a join space. If and , then , whence which means that Thus, is a join space.
The study of algebraic hypergroups and connections with lattices and ordered sets was initiated by J. Mittas and then by M. Konstantinidou and K. Serafimidis, Ch. Massouros, G. Massouros, and later by Ath. Kehagias. Connections between ordered sets, quasi-orders, and hypergroups were also studied by Chvalina.
In what follows, we present some connections with lattice theory, see [18]. Two important classes of lattices are characterized using hypergroups: distributive and modular lattices, see [9,10,19].
Connection 1.
In [9], J.Varlet provided the following characterization of distributive lattices:
Consider the next hyperoperation on a lattice :
we set
Theorem 1.
is a distributive lattice if and only if is a join space.
In [19], we considered and analyzed a family of hyperoperations defined as follows.
Let be arbitrary. For all set
Theorem 2.
If the lattice is distributive and , then is a join space.
We mention some important steps from the proof of this theorem:
First, check that
In order to prove “⊇”, we consider an arbitrary element and we set Thus, whence
Now, we consider that satisfy and
Set We obtain .
Hence, and so is a join space.
Connection 2.
The next example of a join space is useful to characterize modular lattices.
Let be a lattice. In [8] H. Nakano introduced the following hyperoperation on L:
Later, S. Comer [10] showed that:
Theorem 3.
is a modular lattice if and only if is a join space.
Another interesting proof of the above theorem is given in [2]. Several properties of this join space were presented in [13].
In [19], a new family of hyperoperations determined by a lattice is analyzed. For all set
Notice that , since
For set and denote by the restriction of to .
Theorem 4.
Let . If is modular, then is a join space.
Similar results can be obtained by considering the hyperoperation:
The hyperproduct is not empty since
Connection 3.
Another connection between join spaces and lattices was highlighted by Tofan and Volf [14], as follows:
If is a lattice and is a function, such that is a distributive sublattice of , then define
We obtain a commutative hypergroup .
Indeed, in the above conditions, the next equality is checked:
Moreover, we shall prove here the next result, as follows:
Theorem 5.
The next statements are equivalent:
- is a distributive sublattice.
- satisfies the join space condition.
Proof.
First, let us check that the join space condition is satisfied for a distributive sublattice Let : ,
Then, we shall check that there is
Since and
, according to the distributivity, it follows that
From here we obtain
Similarly, we have
Hence,
Therefore,
Now, let us note that the reciprocal statement also holds: if the join space condition is satisfied, then is a distributive sublattice.
Indeed, if is not distributive, then it will contain a sublattice
and of are not comparable two by two.
In both situations, , since
and
Thus, and a contradiction. Thus, the sublattice is distributive. □
Canonical hypergroups are an important class of join spaces and were introduced by J. Mittas [20]. They are the additive structures of Krasner hyperrings and were used by R. Roth to obtain results in the finite group character theory, see [21]. McMullen and Price studied finite abelian hypergroups over splitting fields [22].
More recent studies of canonical hypergroups were conducted by C and G. Massouros (in connection with automata), P. Corsini (sd-hypergroups), and K. Serafimidis, M. Konstantinidou, and J. Mittas, while feebly canonical hypergroups were analyzed by P. Corsini and M. De Salvo.
Canonical hypergroups are exactly join spaces with a scalar identity e, which means that . Obviously, commutative groups are canonical hypergroups. Other examples of canonical hypergroups are given in [3].
More general structures were also considered, namely polygroups, also called quasi-canonical hypergroups, by Bonansinga, Corsini, and Ch. Massouros. Comer analyzed the applications of polygroups in the theory of graphs, relations, Boolean, and cylindrical algebras.
A particular type of polygroup, namely the hypergroup of bilateral classes, was investigated by Drbohlav, Harrison. and Comer. Polygroups satisfy the same conditions as canonical hypergroups, with the exception of commutativity.
In the next two sections, we associate join spaces with chains and we analyze when they are isomorphic. Moreover, a combinatorial problem is presented: we calculate how many isomorphism classes of join spaces are.
3. Join Spaces Associated with a Chain: The Finite Case
In what follows, we associate a join space structure with a chain, through a function. We then study under what conditions such join spaces, considered for different functions, are isomorphic, for the finite case.
Let H be finite and where C is a chain. Consider the next hyperoperation on H:
We have
According to Theorem 5 or by a direct check, we then utilize the following theorem.
Theorem 6.
The structure is a join space.
Set We define the next equivalence relation on H:
Denote and order as follows: for
We denote where
For all set . We have
Denote the ordered partition of n into s parts and where
Theorem 7.
If are two maps, then or .
Proof.
“⇐”
Suppose Set where for all ,
Set ,
We order H as follows:
For we have
Consider the map:
We have
which means that
Suppose now that
We have where
Moreover, , and with
Consider the function: We obtain
.
Therefore,
“⇒”
Let be defined as follows: such that Similarly, is defined, where
Denote the isomorphism by .
Denote the set by . For all we have
On the other hand,
For every and every we have
Consider the function We obtain
is injective:
Indeed, if then . Hence, for every there exists such that whence which means that is injective.
is surjective:
Indeed, for each , there is for which since
Therefore, is a bijective function from to
Particularly, We have
So, whence it follows that We have
Hence,
Moreover, for all we have
From it follows that
so
Hence,
Denote by B the set of bijections of defined to itself.
We show that or Denote by
For , we have
If and we suppose that , then so which is a contradiction.
Similarly, for we obtain a contradiction.
Suppose now that there is such that
We obtain
whence
Therefore, which means that
If then
whence Thus, that is
Hence, or □
Now we calculate how many isomorphism classes for join spaces can be constructed in this way.
Denote by the quotient set which contains classes of join spaces associated with maps .
Theorem 8.
(i) If then
- (ii)
- If then .
Proof.
Denote by the set of ordered partitions of n.
According to [23], we have
Let us number the symmetrical ordered partitions of n, that is partitions for which
Set the set of all symmetrical ordered partitions of n.
We have the two cases:
Case 1.
If and if , then or , where and
We have
According to [23], for all t we have Hence,
Case 2.
If and if , then or , where and
We obtain
According to [23], for all t we have
Hence,
Therefore, we can conclude:
- If then ;
- If then .
□
4. Join Spaces Associated with a Chain: The General Case
In this section, we consider an arbitrary set H and we analyze when the join spaces associated with a chain are isomorphic.
Let us present first the context:
Let and consider the equivalence relation on H:
We order as follows: for
Denote and by for all
We order I as follows:
Since C is a chain, it follows that is a chain, too.
Moreover, for all denote
If , then Similarly,
and for all denote We have that is a chain, too.
Theorem 9.
If are two functions, then if and only if there exists a strictly monotonous bijection
Proof.
“⇐”
For all Define
as follows: where we choose . Now, , we have
If is strictly increasing, then
Since is a bijective function, we have
Hence,
If is strictly decreasing, then
Since is a bijection, we have
Hence,
Therefore, is an isomorphism.
“⇒”
Denote by the isomorphism from to Set and , where for all , we obtain and
For we obtain , whence
Hence,
Define by : where
We check that is a bijective function.
Suppose that there are such that
Thus, , which is a contradiction with
On the other hand, since we obtain
whence Hence, is bijective and
Thus,
Hence, Let us prove now that is strictly monotonous.
If are elements of I, then we denote and for then
If and , then whence
We obtain that
For we have or
If , then is strictly increasing on Indeed, it follows from (3).
Similarly, if , then is strictly decreasing on
Therefore, we obtain the thesis. □
Let us present some examples.
Example 4.
If , where is a real interval and , then , whence and φ is the identity function. Hence,
Example 5.
If , where is the real number set and , then , and again , φ is the identity function and
Example 6.
If are such that , , such that , , and so on.
In general, for all .
Then, and is a strictly decreasing function. Hence,
5. Conclusions
We study classes of isomorphism for join spaces associated with chains and a combinatorial problem is analyzed for the finite case, which is to determine the number of the classes of isomorphism.
As a future problem, we can study classes of isomorphism for join spaces associated with lattices. For two maps , where is a lattice, we intend to determine when , to consider the corresponding equivalence classes and examine the finite case.
Another study problem would be to determine hypergroups/join spaces associated with other classes of lattices, such as Boolean lattices and to obtain characterizations of these classes of lattices. In this way, some results of the lattice theory could be demonstrated with the help of the hypergroup theory. For example, in a modular lattice, the ideals are exactly the subhypergroups of the associated join space structure.
Author Contributions
Conceptualization, V.L.-F. and S.H.-M.; methodology, V.L.-F. and S.H.-M.; investigation, V.L.-F.; resources, V.L.-F.; writing—original draft preparation, V.L.-F.; writing—review and editing, V.L.-F. and S.H.-M.; project administration S.H.-M.; funding acquisition, S.H.-M. All authors have read and agreed to the published version of the manuscript.
Funding
The second author thanks to the Ministry of Defence of the Czech Republic for the support under the grant VAROPS.
Institutional Review Board Statement
Not applicable.
Informed Consent Statement
Not applicable.
Data Availability Statement
No new data were created or analyzed in this study. Data sharing is not applicable to this article.
Conflicts of Interest
The authors declare no conflicts of interest.
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