1. Introduction
We refer to hypercompositional algebra as the branch of algebra concerned with hypercompositional structures, that is, algebraic structures where the composition of two elements is a nonempty set rather than a single element [1]. Although hypercompositional algebra differs from classic algebra in its subjects, methods, and goals, the two fields are connected by certain equivalence relations, called fundamental relations [2,3]. Through the fundamental relations, hypercompositional algebra can make use of the wealth of tools typical of traditional algebra.
A fundamental relation is the smallest equivalence relation defined on a hypercompositional structure such that the corresponding quotient is a classic structure whose operational properties are analogous to those of the original structure [4,5]. For example, the quotient of a hypergroup modulo the equivalence is isomorphic to a group [6,7,8]. On the other hand, given a group G and a family of nonempty and pairwise disjoint sets, the set equipped with the hyperproduct , for all and , is a hypergroup. Hypergroups built in this way are called complete [4] and have the property that the -classes are the sets . For any nonempty subset A of a hypergroup , the set is the complete closure of A. Hence, a hypergroup is complete if and only if , for all . Complete hypergroups have been the subject of many studies, see, e.g., [9,10,11,12], because they have a variety of group-like properties. Notably, in [13], the authors define the commutativity degree of complete hypergroups and characterize it with an identity that is analogous to the class equation for groups. Recall that the commutativity degree of a finite group G was defined by W. Gustafson in [14] as the probability that two randomly chosen elements commute,
Inspired by this concept, in [13] the commutativity degree of a finite hypergroup is defined as
The probabilistic interpretation of this number is completely analogous to that for groups. In this paper, we define the completeness degree of a finite hypergroup as the number
and determine some formulas which allow us to compute the previous numbers for a special class of hypergroups, called weakly complete, that include complete hypergroups.The plan of this paper is the following: In Section 2, we introduce definitions, notations, and fundamental facts to be used throughout the paper. In Section 3, we give the definition of product-free relations on a group G and study their main characteristics. In particular, we characterize product-free relations that are maximal with respect to inclusion. In Section 4, we present a new construction of hypergroups. These hypergroups are called weakly complete and are defined using a product-free relation I on a group G, a family of nonempty and pairwise disjoint sets and a special family of functions . The main features of these hypergroups are discussed in this section. The completeness degree of finite weakly complete hypergroups is defined and analyzed in Section 5. There, we prove lower bounds for that depend only on the size of the -classes of H. Finally, in Section 6, we discuss the commutativity degree of finite weakly complete hypergroups, and establish relations between and . In particular, in our last theorem we prove that, if the cardinality of does not depend on k, then .
2. Basic Definitions and Notations
We adopt from known texbooks [1,4,5] standard definitions of basic concepts in hypercompositional algebra, such as semihypergroups and hypergroups. For the reader’s convenience, we present below a few concepts that are needed in this work.
Given a semihypergroup , the relation is defined as , where is the diagonal relation in H and, for every integer , is defined as follows:
(1)
see, e.g., [2,3]. This relation is one of the main fundamental relations alluded to in the Introduction. For some special families of semihypergroups, is transitive; see, e.g., [15,16]. In particular, if , is a hypergroup then is an equivalence relation, see [7,8], and we have the chain of inclusions(2)
Moreover, the quotient set equipped with the operation for all and , is a group. More precisely, is the smallest strongly regular equivalence on H such that the quotient is a group [2]. The canonical epimorphism fulfills the identity for all , and the kernel of is the heart of .
Let be a hypergroup. We say that a nonempty subset is a complete part if for every and ,
The complete closure of A is the intersection of all complete parts containing A and is denoted with . Using the canonical projection , the complete closure of A can be characterized as follows:
A hypergroup is complete if for all . In other words, is a complete hypergroup if for every and .
Finally, let G be a group and let be a binary relation on G. We denote the transpose relation of , that is, . Furthermore, we associate with I the span and support sets defined below:
Here and in the following, denotes the set .
3. Product-Free Relations on a Group
The class of complete hypergroups is among the best known in hypergroup theory, and is characterized by the fact that the hyperproduct of any two elements is a -class. These hypergroups were introduced by P. Corsini in [4] and can be built by considering a group G and a family of nonempty and pairwise disjoint sets. The set is endowed with the product for and . Then, is a complete hypergroup and the -classes of are the sets . In this section, we introduce a special family of binary relations in a group G. These relations will allow us to define in the next section the class of hypergroups that generalize that of complete hypergroups and is the main subject of this work.
Let G be a group. A binary relation is called product-free or PF-relation if, for all ,
denotes the family of all -relations in the group G. If and , then the elements are different from . Otherwise, if, for example, , then we have the contradiction . As a consequence, if , then reduces to the empty relation. Hence, if , then and .
Our first result provides a characterization of -relations in terms of support and span sets. Subsequently, we analyze the structure of and provide some examples.
Let . Then, if and only if .
If , then or for some and there exists such that . We obtain or , a contradiction. Conversely, if , then there exists and such that or . However, then we have . □
Below we provide a couple of examples of how -relations can be built.
Let G be a group. For any subset , let be the relation
It is can be seen that and . Hence, by Lemma 1. For example, is the relation consisting of the pairs for . On the other hand, is the empty relation.
Let G and be groups. Moreover, let and . Then, the direct product relation
is a -relation on the direct product . Indeed, and , so the claim follows from Lemma 1.
The following features of -relations are self-evident, so we refrain from including a proof.
Every subset of a -relation is a -relation.
If , then .
Let G be abelian. Then, if and only if .
Hereafter, we show that no -relation can contain more than a quarter of all possible pairs of elements in the group. This result will play an important role in the forthcoming sections.
Let G be a finite group and . Then, .
For notational simplicity, let . For any element , let and . Obviously, and have the same cardinality, since the application such that is bijective. Since , we have
Moreover,
To maximize the rightmost quantity, we set , and we have the claim. □
The following example shows that the inequality in the preceding theorem is the best possible, since it can hold as an equality.
Let , where is even. Consider the following relation :
It is easy to see that and . Hence, by Lemma 1. Finally, and .
Maximal PF-Relations
-relations can be semi-ordered by inclusion; hence, it is worth considering maximal elements in , with regard to their existence and characterization. The existence of maximal relations is shown in the forthcoming result.
The family of -relations on G has at least one maximal element.
The family is nonempty because it contains the empty relation. Moreover, for each chain in the partially ordered set , the relation is product free. Indeed, if and by chance there exists such that , then there exist such that and . Since is a chain, we can assume that , and so , which is impossible because . Hence, is a upper bound of . By Zorn’s Lemma, in there exists a maximal element. □
Using an argument similar to the previous one, we also have that every -relation I on a group G is contained in a maximal -relation M. It suffices to apply Zorn’s lemma to the family of -relations that contain I. Hence, we have the following result:
Let . Then, there exists a maximal -relation such that .
Every maximal -relation M in an abelian group G is symmetric. Indeed, if and , then is a -relation and . The same fact is not true if the group is not abelian, as shown in the following example. Let G be a noncommutative group with two elements such that , and , e.g., the symmetric group . In these hypotheses, and the relation are product free. If is maximal and , then we have since .
The empty relation is maximal if and only if G is trivial. In the next result, we give a necessary and sufficient condition for a -relation to be maximal.
Let G be a group and let . Moreover, let
Then, we have
-
1.
;
-
2.
I is maximal if and only if .
If then the claim is trivial, so suppose . Note that admits the alternative definition
Let . By hypotesis, there exists such that or . If (resp., ), then (resp., ), which contradicts . Similarly, if (resp., ) then (resp., ), which contradicts .
By point 1, if , then I is maximal. On the other hand, let I be maximal and with . Since is not a -relation, two cases are possible:
(a). There exist and such that or .
(b). There exists such that or .
In the first case, we obtain or ; hence, . In the second case, we have because . In both cases, we obtain . □
We observe that if I and are maximal -relations, then the tensor product relation is not necessarily maximal. For example, let and be groups isomorphic to and , respectively. Moreover, let and . The relations I and are maximal -relations. However, the tensor product relation is not maximal because it is contained in the following -relation on :
4. Weakly Complete Hypergroups
In this section, we introduce a new class of hypergroups, whose construction is fundamentally based on -relations. We introduce a few auxiliary concepts and notations for background information. In what follows, we denote the collection of nonempty subsets of the set X.
Let be nonempty sets. A function is a double covering, or bi-covering for short, if for all and we have
(3)
A bi-covering is called trivial if for all and , and proper if for all and .
Bi-covering functions can be constructed by considering a group G and three nonempty sets A, B, C of size . If , and are three surjective functions; then, the function such that , for all , is bi-covering. Indeed, we trivially have , for all . Moreover, if , then, taking , we have and we obtain
Hence, for all . Analogous arguments prove that , for all . Thus, φ is a bi-covering. We note in passing that in the previous construction the role of the group G can be played by an arbitrary hypergroup.
Let G be a group and let I be a relation on G. Consider a family of nonempty and pairwise disjoint sets, and let be a family of bi-coverings . In particular, if , then . In the set, introduce the hyperproduct , defined as follows:
(4)
for all . This hyperproduct is well defined because the sets in the family are nonempty and pairwise disjointed. The hyperproduct is naturally extended to nonempty subsets of H as usual: For letIn particular, for every and , we have
(5)
Indeed, if then . Otherwise, if , then from (3) we obtain . Analogously we can deduce that . From this observation, it is not difficult to derive that if or all functions are trivial; for every , then is a complete hypergroup. The following result shows that is always a hypergroup under the sole condition that .
Let . Then, in the previous notations,
-
(a)
for every , , and , we have
-
(b)
for every integer and for every there exists such that ;
-
(c)
is a hypergroup such that ;
Let , , and . If and , then we have , . Consequently, by (5) we obtain
If and , we have , and . Moreover, for every we have . Hence,
Moreover, by (5), we obtain . Therefore, . We obtain same result also when and . Finally, if and , we have and . Since I is product free, we have and . Thus,
Hence, also in this case .
It suffices to apply (5) and the previous part and proceed by induction on n.
To prove that is a hypergroup, we only need to show that ∘ is reproducible. Let and . Clearly, for all and, by Equation (5), we obtain
The identity follows analogously for every , so is a hypergroup. Finally, let . By (2), there exists such that . By point , there exists such that . Now, let . Since , by (4) we have and we deduce . □
Let G be a group and let be a relation on G. Consider a family of nonempty and pairwise disjoint sets such that , for all . Moreover, let be a family of surjective functions. Proceeding as in Example 4, we obtain a family of bi-covering functions . If , then Theorem 3 provides a hypergroup .
Product-free relations have a kind of optimality with respect to the rule (4). As shown in Theorem 3, every hyperproduct defined in terms of a -relation is associative and reproducible, independent of families and . The same property does not hold in general if the relation I is not a -relation. For example, consider the group , the relation , the sets , , and the bi-coverings defined as follows:
c | d | e | f | g | h | f | g | h | |||||
c | f | f | c | ||||||||||
d | g | g | |||||||||||
e | h | h |
a | ||||||||
b | ||||||||
c | ||||||||
d | ||||||||
e | ||||||||
f | ||||||||
g | ||||||||
h |
a | ||||||||
b | ||||||||
c | ||||||||
d | ||||||||
e | ||||||||
f | c | |||||||
g | ||||||||
h |
Let G be a group and suppose that is not product free. Then, there exists a family of nonempty and pairwise disjoint sets and there exists a family of bi-coverings such that the hyperproduct defined in (4) is not associative.
Firstly, note that we have as . The proof can be reduced to the analysis of two cases: (a) there exists such that ; and (b) there exists such that and (or, equivalently, ).
(a) If then it suffices to consider arbitrary families and where and the function is described by the following table:
a | b | a |
b |
Hence, . On the other hand, ; hence .
(b) Let and be arbitrary families verifying the following conditions: (b1) for every ; (b2) if then for every and ; in all remaining cases. Let , , and . Then,
Since , then and . Hence, by (b2). On the other hand, for some , we have
By (b1) we can conclude that . (The proof proceeds in a similar way if .) □
The hypergroups defined as in (4) with a -relation I are called weakly complete. A weakly complete hypergroup is n-uniform if for all ; if the size n is not relevant, then we simply call it uniform.
The term “weakly complete” originates from the following observations: Let be a weakly complete hypergroup built from families and , and let ⋄ be the hyperproduct obtained from the same set family using only trivial bi-coverings. Then, is a complete hypergroup and for all . We also obtain the same conclusion by replacing the given relation I with the empty relation. Furthermore, both in complete hypergroups and weakly complete hypergroups, the fundamental relation coincides with , as shown in Theorem 3.
In the following, we use the notation to indicate a weakly complete hypergroup whose hyperproduct ∘ is defined as (4) from and the families and . We call a representation of . It is worth noting that a weakly complete hypergroup may have multiple representations. Indeed, let and let . If the relation is product free, then the same hypergroup admits the representation where and for every and . However, all possible representations of a given weakly complete hypergoup share the same group G and family . This fact should be evident from the following proposition, where we explain the algebraic role of the parameters of a representation of a weakly complete hypergroup.
Let . Then, we have:
-
1.
The sets are the β-classes of H, i.e, for every , .
-
2.
and .
-
3.
Every subhypergroup K of is a complete part of H, that is, .
-
4.
A subset is a subhypergroup of if and only if there exists a subgroup of G such that .
Let and . Then, , and so implies . Conversely, if , then there exist such that . By construction, there exists such that . Therefore, since and the sets of the family are pairwise disjoint, we obtain . Hence, if and only if . By Theorem 3, we conclude .
The map such that , for every , is a group isomorphism. Moreover, we have since .
We must prove that , for all . By reproducibility of K, if then there exists such that . Considering the canonical epimorphism , we obtain and so . Hence, from point , we have . Consequently, and , for all .
Since , for all , the proof of the implication ⇐ is similar to the one used in point of Theorem 3 to prove that is a hypergroup. Now, we prove the implication ⇒. By point , the -classes of are the sets , for all . Let be the canonical epimorphism and be the isomorphism such that , for all . If K is a subhypergroup of , then is a subgroup of G. Moreover, if then there exists such that . By point , we have and . Hence, . On the other hand, if , there exists such that . Clearly, there exists such that . If we suppose that , then we have and . Finally, by point , . Therefore, . □
The following result, which follows from the definition of hyperproduct in (4) and point 1 in Proposition 3, describes all cases where a weakly complete hypergroup is complete.
Let .
-
1.
If , then is complete;
-
2.
if , then is complete is trivial, for every .
Let such that for some and for . Then, is complete, as a consequence of the previous corollary. Indeed, if and , then and is trivial. On the other hand, if then because I is product free. Thus, and are trivial since it is a bi-covering.
The next example shows a weakly complete hypergroup that contains both complete and noncomplete subhypergroups.
Let be a group isomorphic to the Klein group where . Consider , , , and . In the set , define the hyperproduct represented in the following table:
∘ | |||||||
a | |||||||
b | |||||||
c | a | ||||||
d | b | a | |||||
e | b | a | |||||
f | a | b | |||||
g |
The next theorem characterizes weakly complete hypergroups, in that it yields a necessary and sufficient condition for a given hypergroup to be weakly complete, based on the structure of its quotient group.
Let be a hypergroup, and let be the canonical projection. Consider the following relation :
The following conditions are equivalent:
-
1.
J is product free;
-
2.
is a weakly complete hypergroup.
Suppose that J is product free. For every , let , and note that . For every introduce the function such that . It is not difficult to see that is a bi-covering. Indeed, for any fixed we have by construction
The identity can be derived analogously, so is a bi-covering. It remains to observe that , and we have the first part of the claim.
Conversely, suppose that is a weakly complete hypergroup, . Identifying G with modulo an isomorphism, we have . Indeed, let . By hypotesis, there exist such that , and . Hence, by (4). This conclusion follows immediately from the fact that a subset of a -relation is a -relation. □
5. Completeness Degree of Finite Hypergroups
In this section, we introduce the notion of completeness degree of finite hypergroups and analyze the completeness degree of finite weakly complete hypergroups.
Let be a finite hypergroup. Define the set ,
The rational number
is the completeness degree of .Thus, the completeness degree of a hypergroup is the probability that the hyperproduct of two randomly chosen elements is a -class. Clearly, and if and only if is complete. In the next lemma, we deduce an explicit formula for the completeness degree of finite weakly complete hypergroups. For this purpose, we make use of the following auxiliary notation. Let . For every , let
Let . Then,
(6)
Moreover, if is uniform, then
(7)
Firstly, note that . From the definition of the hyperproduct ∘ in (4), we deduce the alternative formula
hence,Recalling that the sets of the family are pairwise disjoint, we obtain
and Equation (6) follows. Moreover, if is n-uniform, then and and we also obtain (7). □Our next result provides two lower bounds on that depend only on the size of the -classes of H.
Let be a finite weakly complete hypergroup. Then,
where is the heart of H. Moreover, if is uniform, then .
Let be the family of disjoint sets in the representation of . Then,
Recalling that and using (6), we obtain the first inequality. Moreover, from (7) we have ; hence, the second part of the claim is an immediate consequence of Theorem 1. □
The next example shows that the inequalities in Theorem 6 can hold as equalities.
Let be an even number, and let G and I be the same as in Example 3. Let be any uniform weakly complete hypergroup such that for all ; i.e., all bi-coverings are proper. A straightforward application of Lemma 2 proves that . Moreover, if , then and . Thus, also the first inequality in Theorem 6 holds as an equality.
In the forthcoming example, we construct uniform weakly complete hypergroups where all bi-coverings are proper, that is, , for all . According to Lemma 2, these hypergroups achieve the smallest possible for a given -relation.
Let G be a group and . Let be a family of finite, pairwise disjoint sets such that for all . We assume , with , nonempty disjoint sets. For every , let be defined as follows:
It is not difficult to verify that is a proper bi-covering. Moreover, the hypergroup is n-uniform. Owing to (7) and the finiteness of G, the completeness degree of is
i.e., the smallest possible value for the given relation I.
6. Commutativity Degree of Weakly Complete Hypergroups
In a nonabelian group and, more generally, in any nonabelian algebraic structure, it makes sense to compute the probability that two randomly chosen elements commute. This problem was popularized by Gustafson in [14], who defined the commutativity degree of a group G as the probability that two arbitrary elements commute,
(8)
and proved that if then G is abelian. Moreover, we have if and only if , where is the center of G. The basic technique adopted for the proof relies on the relationship between and the number of conjugacy classes of G, and can be traced back to a paper by Erdős and Turán [17]. Later on, there has been considerable interest in the use of probabilistic techniques in group theory, and this concept has had significant developments.Recently, the concept of commutativity degree has been introduced also in hypergroup theory [13,18]. In particular, in [13] the authors defined the commutativity degree of a finite hypergroup as
(9)
and characterized this index when is complete by considering a partitioning of H into suitably defined conjugacy classes. In this section, we study the commutativity degree of weakly complete hypergroups. Our main tool is the partitioning of H into -classes. To begin with, we point out an important observation. For any and for any and , a necessary condition for the identity to be valid is , because , and if . Hence, we can restrict our attention to pairs belonging to the setThis set is directly related to the commutativity degree of G, since .
We say that a relation isG-symmetric if its restriction to is symmetric; that is, for every , if then .
Equivalently, is G-symmetric if and only if . It can be observed that if G is abelian then a relation in is G-symmetric if and only if it is symmetric. The relevance of the previous definition lies in the fact that every weakly complete hypergroup admits a representation with a G-symmetric relation, as shown in the following lemma.
Let be a weakly complete hypergroup. Then, there exists a representation where I is G-symmetric.
Let be any representation of . If is G-symmetric, then it is complete. Otherwise, and we define the relation
We have , so I is G-symmetric, and I properly extends . Moreover, from Lemma 1 we can deduce that , because both the support and the span of I coincide with those of .
For every let be the trivial bi-covering, and define . To conclude the proof, it suffices to show that the hypergroup coincides with . Indeed, for arbitrary and , if , then
Otherwise, if either or then the identity follows trivially from the construction (4). We can conclude that . □
In what follows, we obtain different characterizations of the commutativity degree of a weakly complete hypergroup in terms of the parameters of its representation. By virtue of Lemma 3, we can safely assume that I is G-symmetric. In this case, for every pair the sets
(10)
(11)
are well defined.Let where I is G-symmetric. Then,
(12)
Moreover, if is uniform then
(13)
(14)
Let , and . Two cases are possible:
(a). . In this case, ; hence
(b). . Owing to the G-symmetry of I, we have both and . By (10),
The first claim follows from the fact that the set is the disjoint union of and . Moreover, if for all , then
Since , we also have
and (13) follows. Finally, using (11) we obtain which yields (14), and the proof is complete. □The previous theorem yields a few notable consequences. For example, taking we conclude that if is complete and
In particular, if is also uniform, then . More generally, for any uniform weakly complete hypergroup, and the equality holds if and only if for every .
Finally, the similarity between formulas (6) and (12) suggests that we should study the relationship between the degrees of commutativity and completeness, at least in the commutative case. We propose our result below. Before doing so, we recall that if G is abelian, then G-symmetric relations are symmetric. Hence, by Lemma 3, every weakly complete hypergroup built from an abelian group admits a representation whose -relation is symmetric.
Let G be abelian and let , where I is symmetric. Then,
(15)
Moreover, if is uniform then .
Since G is abelian, we have and the condition reduces to . Therefore, subtracting (13) from (6) we obtain (15). Furthermore, for every we have . If H is n-uniform, then and . Hence,
Thus, . The rightmost inequality in the claim comes from Theorem 1. □
7. Conclusions
The class of complete hypergroups is among the best known in hypergroup theory. Complete hypergroups have a variety of group-like properties and are characterized by the fact that the composition of two elements is a -class [9,10,11,12]. In this paper, we introduce a class of hypergroups that includes complete hypergroups as a particular case. The construction of these hypergroups, called weakly complete, is crucially based on particular binary relations defined on the quotient group . We call these relations product free because no group element is in relation with the product of two elements that are related to each other. Product-free relations are interesting by themselves, and we show a number of their main properties on generic groups in Section 2. For example, we prove an attainable upper bound on the cardinality of product-free relations in finite groups.
The main motivation of introducing weakly complete hypergroups lies in the possibility of measuring their “closeness” to complete hypergroups. Indeed, to every finite hypergroup, we can associate a completeness degree, which quantifies how close to completion the hypergroup is. We introduce and analyze this concept in Section 5. More precisely, the completeness degree of a hypergroup is the probability that the composition of two randomly chosen elements is a -class. For a weakly complete hypergroup whose -classes have the same cardinality, this probability is bounded from below by . Indeed, the completeness degree of weakly complete hypergroups admits simple closed formulas. Furthermore, it can be related to the commutativity degree, which has been recently brought into hypercompositional algebra from group theory [13,18].
Completeness concepts and probabilistic methods are relevant topics nowadays not only in classical algebra but also in hypercompositional algebra, and this discipline is continually expanding with the introduction of structures with distinctive properties [19]. It would be interesting to discover more hypergroup classes, and more general hypercompositional structures, for which useful results can be found along these directions.
Conceptualization and investigation: D.F. (Dario Fasino), D.F. (Domenico Freni), and G.L.F.; writing—original draft: D.F. (Domenico Freni); writing—review and editing: M.D.S. and D.F. (Dario Fasino). All authors have read and agreed to the published version of the manuscript.
The research work of Mario De Salvo was funded by Università di Messina, Italy, grant FFABR Unime 2019. Giovanni Lo Faro was supported by INdAM-GNSAGA, Italy, and by Università di Messina, Italy, grant FFABR Unime 2020. The work of Dario Fasino was partially supported by INdAM-GNCS, Italy.
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The authors declare no conflict of interest.
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Abstract
We introduce a family of hypergroups, called weakly complete, generalizing the construction of complete hypergroups. Starting from a given group G, our construction prescribes the
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1 Dipartimento di Scienze Matematiche e Informatiche, Scienze Fisiche e Scienze della Terra, Università di Messina, 98122 Messina, Italy;
2 Dipartimento di Scienze Matematiche, Informatiche e Fisiche, Università di Udine, 33100 Udine, Italy;