research article regularity in terms of hyperidealsand studied the notion of a partial -ary...
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Hindawi Publishing CorporationChinese Journal of MathematicsVolume 2013, Article ID 167037, 4 pageshttp://dx.doi.org/10.1155/2013/167037
Research ArticleRegularity in terms of Hyperideals
Kostaq Hila,1 Bijan Davvaz,2 Krisanthi Naka,1 and Jani Dine1
1 Department of Mathematics and Computer Science, Faculty of Natural Sciences, University of Gjirokastra,Gjirokastra 6001, Albania
2Department of Mathematics, Yazd University, Yazd, Iran
Correspondence should be addressed to Bijan Davvaz; [email protected]
Received 9 August 2013; Accepted 9 October 2013
Academic Editors: L. Denis and G. Toth
Copyright Β© 2013 Kostaq Hila et al. This is an open access article distributed under the Creative Commons Attribution License,which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
This paper deals with the algebraic hypersystems.The notion of regularity of different type of algebraic systems has been introducedand characterized by different authors such as Iseki, Kovacs, and Lajos. We generalize this notion to algebraic hypersystems givinga unified generalization of the characterizations of Kovacs, Iseki, and Lajos. We generalize also the concept of ideal introducingthe notion of π-hyperideal and hyperideal of an algebraic hypersystem. It turns out that the description of regularity in terms ofhyperideals is intrinsic to associative hyperoperations in general. The main theorem generalizes to algebraic hypersystems someresults on regular semigroups and regular rings and expresses a necessary and sufficient condition bymeans of principal hyperideals.Furthermore, two more theorems are obtained: one is concerned with a necessary and sufficient condition for an associative,commutative algebraic hypersystem to be regular and the other is concerned with nilpotent elements in the algebraic hypersystem.
1. Introduction
Algebraic structures play a prominent role in mathematicswith wide ranging applications in many disciplines such astheoretical physics, computer sciences, control engineering,information sciences, and coding theory.
Hyperstructure theory was introduced in 1934, whenMarty [1] defined hypergroups based on the notion of hyper-operation, began to analyze their properties, and appliedthem to groups. In the following decades and nowadays, anumber of different hyperstructures are widely studied fromthe theoretical point of view and for their applications tomany subjects of pure and applied mathematics by manymathematicians. In a classical algebraic structure, the com-position of two elements is an element, while in an algebraichyperstructure, the composition of two elements is a set.Several books have been written on hyperstructure theory;see [2β5]. A recent book on hyperstructures [3] points outtheir applications in rough set theory, cryptography, codes,automata, probability, geometry, lattices, binary relations,graphs, and hypergraphs. Another book [4] is devoted espe-cially to the study of hyperring theory. Several kinds of hyper-rings are introduced and analyzed. The volume ends with an
outline of applications in chemistry and physics, analyzingseveral special kinds of hyperstructures: π-hyperstructuresand transposition hypergroups. The theory of suitable modi-fied hyperstructures can serve as a mathematical backgroundin the field of quantum communication systems.π-ary generalizations of algebraic structures are the most
natural way for further development and deeper understand-ing of their fundamental properties [6, 7]. In [8], Davvaz andVougiouklis introduced the concept of π-ary hypergroups asa generalization of hypergroups in the sense of Marty. Also,we can consider π-ary hypergroups as a nice generalization ofπ-ary groups. Leoreanu-Fotea and Davvaz in [9] introducedand studied the notion of a partial π-ary hypergroupoid,associated with a binary relation. Some important results,concerning Rosenberg partial hypergroupoids, induced byrelations, are generalized to the case of π-ary hypergroupoids.Davvaz et al. in [10, 11] considered a class of algebraic hyper-systems which represent a generalization of semigroups,hypersemigroups, and π-ary semigroups. In this paper wedeal with the algebraic hypersystems.The notion of regularityof different type of algebraic systems has been introduced andcharacterized by different authors such as Iseki [12], Kovacs[13], and Lajos [14]. We generalize this notion to algebraic
2 Chinese Journal of Mathematics
hypersystems giving a unified generalization of the charac-terizations of Kovacs, Iseki, and Lajos. We generalize alsothe concept of ideal introducing the notion of π-hyperidealand hyperideal of an algebraic hypersystem. It turns outthat the description of regularity in terms of hyperidealsis intrinsic to associative hyperoperations in general. Themain theorem generalizes to algebraic hypersystems someresults on regular semigroups and regular rings and expressesa necessary and sufficient condition by means of principalhyperideals. Furthermore, two more theorems are obtained:one is concerned with a necessary and sufficient conditionfor an associative, commutative algebraic hypersystem to beregular; another is concerned with nilpotent elements in thealgebraic hypersystem.
2. Algebraic Hypersystems andπ-Ary Hyperstructures
In this section we recall some known notions on what ismeant by an algebraic hypersystem and π-ary hyperstruc-ture.
Letπ» be a nonempty set and π a mapping π : π» Γπ» β
Pβ(π»), wherePβ(π») denotes the set of all nonempty subsetsof π». Then π is called a binary (algebraic) hyperoperationon π». In general, a mapping π : π» Γ π» Γ β β β Γ π» β
Pβ(π»), where π» appears π times, is called an π-ary(algebraic) hyperoperation, and π is called the arity of thishyperoperation. An algebraic system (π», π), where π is anπ-ary hyperoperation defined on π», is called an π-aryhypergroupoid or anπ-ary hypersystem. Since we identify theset {π₯} with the element π₯, anyπ-ary (binary) groupoid is anπ-ary (binary) hypergroupoid.
Let π anπ-ary hyperoperation onπ» andπ΄1, π΄2, . . . , π΄
π
nonempty subsets ofπ». We define
π (π΄1, π΄2, . . . , π΄
π)
= {π (π₯1, π₯2, . . . , π₯
π) | π₯πβ π΄π, π = 1, 2, . . . , π} .
(1)
We will use the following abbreviated notation: thesequence π₯
π, π₯π+1, . . . , π₯
πwill be denoted by π₯π
π. For π < π, π₯π
π
is the empty symbol. In this convention,
π (π₯1, . . . , π₯
π, π¦π+1, . . . , π¦
π, π§π+1, . . . , π§
π) (2)
will be written as π(π₯π1, π¦π
π+1, π§ππ+1). In the case when π¦
π+1=
β β β = π¦π= π¦, the last expression will be written in the form
π(π₯π1,(πβπ)
π¦ , π§ππ+1).
Similarly, for subsets π΄1, π΄2, . . . , π΄
πofπ» we define
π (π΄π
1) = π (π΄
1, π΄2, . . . , π΄
π)
= {π (π₯π
1) | π₯πβ π΄π, π = 1, . . . , π} .
(3)
Anπ-ary hyperoperation π is called (π, π)-associative if
π (π₯πβ1
1, π (π₯π+πβ1
π) , π₯2πβ1
π+π) = π (π₯
πβ1
1, π (π₯π+πβ1
π) , π₯2πβ1
π+π)
(4)
holds for fixed 1 β€ π < π β€ π and all π₯1, π₯2, . . . , π₯
2πβ1β π».
Note that (π, π)-associativity follows from (π, π)- and (π, π)-associativity.
If the above condition is satisfied for all π, π β {1, 2, . . . , π},then we say that π is associative.
The π-ary hyperoperation π is called commutative ifand only if for all π₯
1, . . . , π₯
πβ π» and for all π β S
π,
π(π₯1, π₯2, . . . , π₯
π) = π(π₯
π(1), π₯π(2), . . . , π₯
π(π)).
By an algebraic hypersystem (π», π1, π2, . . . , π
π) or simply
π» is meant a set π» closed under a collection of ππ-ary
hyperoperation ππand often also satisfying a fixed set of laws,
for instance, the associative law.
3. Regular Algebraic Hypersystems
Letπ»be an algebraic hypersystem.π» is said to be regularwithrespect to the hyperoperation π if and only if for each π β π»there existπ₯
2, π₯3, . . . , π₯
π; π¦1, π¦3, . . . , π¦
π; . . . ; π§
1, π§2, . . . , π§
πβ1β
π» such that
π β π (π (π, π₯2, . . . , π₯
π) , π (π¦
1, π, π¦3, . . . , π¦
π) , . . . ,
π (π§1, π§2, . . . , π§
πβ1, π)) .
(5)
A subset π ofπ» constitutes a subhypersystem if and only ifπ is closed under the same hyperoperations and satisfies thesame fixed laws inπ».
Let π» be an algebraic hypersystem. A π-hyperideal π =1, 2, . . . , π relative to the π-ary hyperoperation is defined tobe a subhypersystem πΌ
πsuch that, for any π₯
1, π₯2, . . . , π₯
πβ π»,
if π₯πβ πΌπ, then π(π₯
1, π₯2, . . . , π₯
π) β πΌ
π. The π-hyperideal
relative to π generated by an element π β π» (usually called aprincipal π-hyperideal) is denoted by
(π)π= π(π»,π», . . . ,
π
π, . . . , π») βͺ {π} . (6)
A subhypersystem πΌ which is a π-hyperideal for each π =1, . . . , π is simply called a hyperideal.
Theorem 1. Let π» be an algebraic hypersystem which isassociative relative to an π-ary hyperoperation π. Then thefollowing conditions are equivalent.
(1) π» is regular relative to the hyperoperation π.
(2) π(πΌ1, πΌ2, . . . , πΌ
π) = β
π
π=1πΌπfor any set of π-hyperideals
πΌπrelative to the hyperoperation.
(3) π((π1)1, (π2)2, . . . , (π
π)π) = β
π
π=1(ππ)πfor any set of
elements π1, π2, . . . , π
πβ π».
(4) π((π)1, (π)2, . . . , (π)
π) = β
π
π=1(π)πfor each element
π β π».
Chinese Journal of Mathematics 3
Proof. β(1) β (2).β Let π» be regular relative to the π-aryhyperoperation π and let π β βπ
π=1πΌπfor any set of π π-
hyperideals πΌπrelative to the hyperoperation.Thenby regular-
ity there exists π₯2, . . . , π₯
π; π¦1, π¦3, . . . , π¦
π, . . . ; π§
1, . . . , π§
πβ1β
π» such that
π β π (π (π, π₯2, . . . , π₯
π) , π (π¦
1, π, . . . , π¦
π) , . . . ,
π (π§1, . . . , π§
πβ1, π)) .
(7)
With πΌπbeing a π-hyperideal for each π = 1, . . . , π, we
thus obtain π(π, π₯2, . . . , π₯
π) β πΌ1, π(π¦1, π, . . . , π¦
π) β πΌ2, . . .,
and π(π§1, π§2, . . . , π§
πβ1, π) β πΌ
πand hence βπ
π=1πΌπβ
π(πΌ1, πΌ2, . . . , πΌ
π).
Conversely, if π β π(πΌ1, πΌ2, . . . , πΌ
π), then π β
π(π1, π2, . . . , π
π) for π
πβ πΌπ, π = 1, . . . , π, and therefore π β πΌ
π
for each π = 1, . . . , π. Hence, (2) is proved.β(2) β (3) β (4)β are obvious.β(4) β (1).β Let π((π)
1, (π)2, . . . , (π)
π) = β
π
π=1(π)πfor
each π β π». Since for each π β π», π β βππ=1(π)π, then π β
π(π1, π2, . . . , π
π), where either π
π= π or π
πβ π(π1, π2, . . . , π
π)
with ππ= π. Thus, we have in any case the following:
π β π (π1, π2, . . . , π
π)
= π (π (π, π₯2, . . . , π₯
π) , π (π¦
1, π, . . . , π¦
π) , . . . ,
π (π§1, π§2, . . . , π§
πβ1, π))
(8)
for some π₯2, . . . , π₯
π; π¦1, π¦3, . . . , π¦
π; . . . ; π§
1, . . . π§πβ1
β π». Thisshows that π» is regular with respect to the hyperoperation.
Theorem 2. An algebraic hypersystem π» which is associativeand commutative relative to an π-ary hyperoperation π isregular with respect to the same hyperoperation if and only ifevery hyperideal πΌ ofπ» is idempotent; that is,π(πΌ, πΌ, . . . , πΌ) = πΌ.
Proof. If π» is commutative relative to π, then π(π,π», . . . , π») = π(π», π, . . . , π») = β β β = π(π»,π», . . . , π)and hence every π-hyperideal is also a π-hyperideal for allπ, π = 1, . . . , π. Hence, by regularity
π (πΌ, πΌ, . . . , πΌ) = πΌ β© πΌ β© πΌ β© β β β β© πΌ = πΌ
β hyperideal πΌ in π».(9)
Conversely, suppose that every hyperideal in π» is idem-potent. If πΌ
1, πΌ2, . . . , πΌ
πare hyperideals of π», then βπ
π=1πΌπis
also an hyperideal and therefore
π
βπ=1
πΌπ= π(
π
βπ=1
πΌπ,π
βπ=1
πΌπ, . . . ,π
βπ=1
πΌπ) β π (πΌ
1, πΌ2, . . . , πΌ
π) (10)
inasmuch as πΌπcontains the intersection for each π. Further-
more, since each πΌπ, π = 1, . . . , π is also a π-hyperideal, then
π(πΌ1, πΌ2, . . . , πΌ
π) β β
π
π=1πΌπ. Hence, the conclusion follows.
By what we mentioned in the beginning of the section,note that in case theπ-ary hyperoperationπ is an associativeπ-ary hyperoperation inπ» one may conveniently abbreviate
π (π, π, . . . , π) = π (ππ
) ,
π (π (ππ
) , π, . . . , π) = π (π2πβ1
) ,
π (π (ππ
) , π (ππ
) , . . . , π) = π (π3πβ2
) ,
...
π (π (ππ
) , π (ππ
) , . . . , π (ππ
)) = π (ππ2
) = π (π(π+1)πβπ
) .
(11)
Thus, the admissible exponents of compositions of rank atmost 2 are each of the form ππ β π + 1 for some integer.Proceeding inductively, suppose that π
1π β π
1+ 1, π
2π β
π2+ 1, . . . , π
ππ β π
π+ 1 are previously known admissible
exponents; then the exponent
π
βπ=1
(πππ β π
π+ 1) = (
π
βπ=1
ππβ 1)π β
π
βπ=1
ππ
(12)
of π(π(ππ1πβπ1+1), π(ππ2πβπ2+1), . . . , π(ππππβππ+1)) is evi-dently also of the same form. Hence, every admissibleexponent of an π-ary hyperoperation is of the formππ β π + 1.
An element π β π» such that
π (π, π₯1, . . . , π₯
πβ1) = π (π₯
1, π, . . . , π₯
πβ1)
= π (π₯1, . . . , π₯
πβ1, π) = {π} ,
(13)
for all π₯1, π₯2, . . . , π₯
πβ1β π», is called zero element. The zero
element is denoted by 0. A nilpotent element π β π» is onewhich satisfies π(πππβπ+1) = {0} for some integer π greaterthan 0.
Theorem 3. An algebraic hypersystem π» which is commuta-tive, associative, regular, and has a 0 with respect to an π-aryhyperoperation π possesses no nilpotent element other than 0.
Proof. For all 0 ΜΈ= π β π», let [π] denote the subhypersystemof π» generated by π, which may be inductively defined asfollows:
(1) π β [π](2) π(ππ) β [π](3) whenever π(ππ1), . . . , π(πππ) β [π], then alsoπ(ππ1+β β β +ππ) β [π].
In order to prove the theorem it suffices to show that π β [π].We proceed inductively as follows.
(1) π ΜΈ= 0 by assumption.(2) Consider π(ππ) ΜΈ= {0}. For, if π(ππ) = {0}, then
by virtue of the associativity, commutativity, andregularity of the given hyperoperation, there exist
4 Chinese Journal of Mathematics
π₯1, . . . , π₯
πβ1β π» such that π β π(π, π₯
1, π, . . . ,
π(. . . , π₯πβ1, π)) = π(π(π, π, . . . , π), π₯
1, . . . , π₯
πβ1) =
π(π(ππ), π₯1, . . . , π₯
πβ1) = π(0, π₯
1, . . . , π₯
πβ1) = {0}
contrary to (1).(3) We now show that if π(ππ1), . . . , π(πππ) are
all nonzero elements of [π] , then π(π(ππ1),π(ππ2), . . . , π(πππ)) = π(ππ1+π2+β β β +ππ) ΜΈ= {0}. Supposeπ(ππ1+π2+β β β +ππ) = {0}. Then by the above remark, wehave
ππ= πππ β π
π+ 1 for π = 1, 2, . . . , π. (14)
Since π is commutative, it may be assumed without loss ofgenerality that π
1= max
πππ. Then
πππ=π
βπ=1
ππ+ (ππ
1βπ
βπ=1
ππ) =π
βπ=1
ππ+π
βπ=1
(ππβ ππ)
=π
βπ=1
ππ+π
βπ=1
[(π1β ππ)π β (π
1β ππ)]
=π
βπ=1
ππ+ (π
βπ=1
(π1β ππ)π
βπ
βπ=1
(π1β ππ) β π + 2) + (π β 2)
=π
βπ=1
ππ+ {[
π
βπ=1
(π1β ππ) β 1]π
β[π
βπ=1
(π1β ππ) β 2]} + (π + 2)
=π
βπ=1
ππ+ π + (π β 2) ,
(15)
where π is an admissible exponent. Hence, by associativity,commutativity, and regularity of the hyperoperation π, thereexist π₯
1, π₯2, . . . , π₯
πβ1β π» such that
{0} ΜΈ= π (ππ1)
= π (π (ππ1) , π₯1, π (ππ1) , . . . , π (. . . , π₯
πβ1, π (ππ1)))
= π (π (πππ1) , π₯1, . . . , π₯
πβ1)
= π (π (ππ1+π2+β β β +π
π+π+(πβ2)
) , π₯1, . . . , π₯
πβ1)
= π (π (ππ1+π2+β β β +π
π) ,
π (π (ππ
) , π, π, . . . , π, π₯1) , π₯2, . . . , π₯
πβ1)
= π (0, π (π (ππ
) , π, π, . . . , π, π₯1) , π₯2, . . . , π₯
πβ1) = {0} ,
(16)
a contradiction.Thus, every element of [π] is nonzero and theconclusion follows.
Acknowledgments
KostaqHilawishes to express his warmest thanks to ProfessorApostolos Thoma and the Department of Mathematics,University of Ioannina (Greece) for their hospitality duringthe authorβs postdoctoral scholarship supported by the StateScholarships Foundation of Hellenic Republic.
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