- Open Access
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- Authors : Dr. M. Jeyalakshmi
- Paper ID : IJERTV2IS1270
- Volume & Issue : Volume 02, Issue 01 (January 2013)
- Published (First Online): 30-01-2013
- ISSN (Online) : 2278-0181
- Publisher Name : IJERT
- License: This work is licensed under a Creative Commons Attribution 4.0 International License
Extension of a Drl – Group
Dr. M. Jeyalakshmi
Assistant Professor in Mathematics Alagappa Govt. Arts College, Karaikudi 630 003
Abstract: In this paper we introduce the idea of a DR – group is a direct product of a Brouwerian Algebra and a commutative – group.
Key words: commutative – group, Brouwerian Algebra, DR – group.
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Preliminaries Definition 1.1 [4]
A non empty set G is called a commutative group if and only if
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(G, +) is an abelian group
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(G, ) is a lattice
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If x y, then a + x + b a + y + b, for all a, b, x, y in G.
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(or)
(a + x + b) (a + y + b) = (a + x y + b)
(a + x + b) (a + y + b) = (a + x y + b), for all a, b, x, y in G.
Definition 1.2 [1], [4]
A non empty set B is called a Brouwerian Algebra if and only if
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(B, ) is a lattice
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B has a least element
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To each a, b in B, there is a least x = a b in B such that b x a
Definition 1.3 [4], [5]
A lattice L is called a residuated lattice if
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(L, .) is an group.
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Given a, b in L, there exist the largest x, y such that bx a and yb a.
Definition 1.3 [4]
A system A = (A, +, ) is called dually residuated lattice ordered group (simply DR group) if and only if
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(A, +) is an abelian group.
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(A, ) is a lattice.
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b c a + b a + c, for all a, b, c in A
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Given a, b in A, there exist a least element x = a – b in A such that b + x a.
Definition 1.4 [4]
A system A = (A, +, , ) is called a DR group if and only if
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(A, +) is an abelian group.
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(A, , ,) is a lattice.
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a + (b c) = (a + b) (a + c),
a + (b c) = (a + b) (a + c), for all a, b, c in A.
-
x + (y x) y,
x y (x z) y,
(x + y) y x, for all x, y, z in A.
Remark [4]
Two definitions for DR group are equivalent.
Examples 1.1 [4]
Commutative – group, Brouwerian Algebra and Boolean ring are DR – groups.
Extension of a DR – group Theorem : 1.1
Any DR – group A is the direct product of a Brouwerian Algebra B and a commutative – group G if and only if
i) (a + b) (c + c) (a c) + (b c) and
ii) (ma + nb) (a + b) (ma a) + (nb b),
for all a, b, c in A and any pair of positive integers m, n.
Proof :
Assume that
(a + b) (c + c) (a – c) + (b – c) (1)
(ma + nb) (a + b) (ma a) + (nb b) (2) To prove A = B x G
Let a, b, c in A be arbitrary
(a + b) c (a c) + b, by property 11 [4]
[(a + b) c] c [(a c) + b] c
= (a c) + (b c)
(a + b) (c – c) (a c) + (b c) (3)
From (1) and (3), we get
(a + b) (c + c) = (a c) + (b c) (4) Also, (ma + nb) a (ma a) + nb, by property 11 [4]
[(ma + nb) a] b [(ma a) + nb] b
(ma + nb) (a + b) (ma a) + (nb b) (5)
Form (2) and (5), we have
(ma + nb) (a + b) = (ma a) +( nb b) (6) Let B = {a / a + a a = 0}
G = {a / a+ a a = a}
Claim (1): B is a Brouwerian Algebra
-
Closed with respect to and
Let a in B be arbitrary
(a + a ) – a = 0 0
(a + a ) – a 0
[(a + a ) a ] + a 0 + aa + a a
Now 0 = ( a + a ) a ( a – a ) + a , by property 11 [4]
0 a
0 + a a + a
a a + a
Thus a + a = a (7)
Hence B is closed under + Let a, b in B be arbitrary
Then (a b) + (a b) = (a + a) (b + b), by (4)
a b in B
= a – b, by (7)
(a b) + b in B
a b in B, by property 7 [4]
Also, (a + b) – (a b) = (a + b) – [( a b) + (a b)], since a b in B
= [ a (a b)] + [ b (a b)], by (4)
= [(a a) (a b)] + [(b a) (b b)], by property 4 [4]
= [ 0 (a b)] + [(b a) 0]
= 0 + 0
(a + b) – (a b) = 0
a + b = a b Let a, b in B a + b , a b in B
(a + b) – (a b) in B
a b in B
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( B, , ) is a lattice Idempotent law
Let a in B be arbitrary Then a a = a + a
= a
a a = (a + a) (a a)
= a + a a
= a
Thus a a = a; a a = a, for all a in B.
Commutative law:
Let a, b in B be arbitrary Then a b = a+ b
= b + a
= b a
a b = (a + b) (a b), by property 8 [4]
= ( b + a) (b a)
= b a
Thus a b = b a ; a b = b a, for all a, b, in B
Associative Law :
Let a, b, c in B be arbitrary.
Then a (b c) = a + (b + c)
= (a + b) + c
= (a b) c
a (b c) = [a + (b c)] [a (b c)], by property 8 [4]
= [a + (b c)] [a + (b c)]
= 0
(a b) c = [(a b) + c] [(a b) c]
= [(a b) + c] [(a b) + c]
= 0
Thus a (b c) = (a b) c; a (b c) = (a b) c, for all a, b, c in B
Absorption law :
Let a, b in B be arbitrary
Then a (a b ) = a + (a b)
= a + [(a + b) (a b)]
= a + [(a + b) (a + b)]
= a
a (a b) = [a + (a b)] – [a (a b)]
= [a + (a b)] – [(a a) b]
= a + (a b) ( a b)
= a
Thus a (a b ) = a; a (a b ) = a , for all a, b in B Hence ( B, , ) is a lattice.
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B has a least element :
Let a in B be arbitrary
Then 0 = (a + a ) – a (a a ) + a
0 a, for all a in B Hence B has a least element.
-
To each a, b in B , there exist a least element x = a b in B such that b x a :
Let a, b in B be arbitrary
there exist a least element x = a b in B Now b x = b + x
= b + (a b)
= a a
Thus to each a, b in B, there exist a least element x = a b in B such that b x a Hence B is a Brouwerian Algebra
Claim (2) : G is a commutative – group
-
(G, +) is an abelian group Closure law :
Let a, b in G be arbitrary
Then [(a + b) + (a + b)] – (a + b) = (2a + 2b) (a + b)
= (2a – a) + (2b – b), by (6)
a + b in G
= a + b
Thus a, b in G a + b in G
Clearly, + is both associative and commutative in G, since G is a subset of A.
Existence of Identity:
Let a in G be arbitrary.
Clearly 0 in G, since 0 = 0 + 0 0 Then a + 0 = 0 + a = a , for all a in G.
Existence of Inverse :
Let a in G be arbitrary
Then (-a) + (-a) (-a) = a a + a
= -a
-a in G Now, a + (-a) = (-a) + a = 0
Hence (G, +) is an abelian group
-
(G , ) is a lattice :
Let a, b in G be arbitrary.
a, -b, b in G
a b, b in G
(a b) + b in G
a b in G, by property 7 [4] Also a, b in G a + b , a b in G
(a + b) (a b) in G
a b in G
Idempotent law:
Let a in G be arbitrary
Then a a = ( a a ) + a
= a
a a = ( a + a ) ( a a)
= ( a+ a) a
= a
Thus a a = a ; a a = a, for all a in G
Commutative law:
Let a, b in G be arbitrary
Then a b = (a+ b) (a b)
= [(a + b) – a] [(a + b) – b]
= b a
a b = (a + b) (a b)
= (b + a) (b a)
= b a
Thus a b = b a ; a b = b a, for all a, b in G
Associatve law :
Let a, b, c in G be arbitrary
Then a ( b c) = [ a (b c)] + (b c)
= a
(a b) c = [(a b) c] + c
= a b
= (a b) + b
= a
Therefore, a (b c) = (a b) c, for all a, b, c in G.
Also, a (b c) = [ a + (b c)] [ a (b c)]
= [ a + ( b c) ([a (b c)] + (b c))
= a + ( b c) a
= b c
= (b + c) (b c)
= (b + c) [(b – c) + c ]
= b + c b
= c
(a b) c = [(a b) + c] – [(a b) c]
= [(a b) + c] ([(a b) c] + c)
= (a b) + c (a b) = c Therefore, a (b c) = (a b) c, for all a, b, c in G.
Absorption Law :
Let a, b in G be arbitrary
Then a (a b) = [ a – (a b)] + (a b)
= a
a (a b) = [ a – (a b)] [a (a b)]
= [a + (a b)] [(a a) b]
= a + (a b) (a b) = a
Thus a (a b) = a, a (a b) = a, for all a, b in G Therefore, (G, , ) is a lattice
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a + (b c) = ( a + b) ( a + c),
a + (b c) = ( a + b) ( a + c), for all a, b , c in G :
Let a, b, c in G be arbitrary
Then a + (b c) = a + [(b – c) +c]
= a + b
( a + b) ( a + c) = [( a + b) – ( a + c)] + ( a + c)
= a + b
Therefore, a + (b c) = (a + b) (a + c) , for all a, b, c in G Also, a + (b c) = a + [( b + c) – (b c)]
= a + (( b + c) [(b- c) + c])
= a + [( b + c) b]
= a + c
(a + b) (a + c) = [(a + b) + (a + c)] [(a + b) (a + c)], by property 8 [4]
= (a + b) + (a + c) (a + b), by previous result
= ( a + c)
Therefore, a + (b c) = (a + b) (a + c), for all a, b, c in G Hence G is a commutative – group.
Claim (3): A = B x G
For any a in A, y = (a + a) a, x = a – [(a + a) a] implies y in G, x in B Now (y + y) y = [(2a – a) + (2a – a)] (2a a)
= [(2a + 2a) (a + a)] (2a a), by (6)
= ( 4a 2a) (2a a)
4a 2a a , since 2a a a
= a
(y + y) y y
Also, (y + y) y (y y) + y, by property 11 [4]
= y
(y + y) y y Therefore , (y + y) y y
y in G
y = (a + a) a
y a
x 0
x + x 0 + x
x + x x
Now, (a y) + (a y) = (a + a) (y + y), by (4)
= 2a 2y
= 2a 2 ( 2a a)
x + x = 2a ( 4a 2a)
We have
( 4a 2a) + [a (2a a)] = (2a a) + (2a a) + [a (2a a)]
(2a a) + a
= 2a
( 4a 2a) + [a (2a a)] 2a
2a ( 4a 2a) a (2a a) = x
x + x x
x + x = x
x in B
Thus if a in A, then a = x + y , where x in B, y in G Now, let a = x' + y', where x' in B, y' in G Then a + a = (x' + y' ) + (x' + y' )
= (x' + x' ) + (y' + y' )
= x' + 2 y', since x' in B
= (x' + y') + y'
a + a = a + y'
(a + a) a = (a + y' ) a
(a + y' ) a in G
[(a + y' ) a] y' = (a + y' ) (a + y' )= 0
a + y' = a + y'
a + y' a = y'
(a + a) a = y'
Now, a = x' + y'
a y' = x' x'
a y' x'
Also, x' ( a y') (x' a) + y'
= [x' (x' + y')] + y'
= ( 0 y') + y' = 0
x' (a y' ) 0
x' a y'
Hence x' = a y'
Hence follows that A is the direct product of a Brouwerian Algebra B and a commutative – group G.
Conversely, assume that A = B x G, where B is a Brouwerian Algebra and G is a commutative group.
To prove
(i) (a + b) (c + c) (a c) + (b c),
(ii) (ma + nb) (a + b) (ma a) + (nb b),
for all a, b, c in A and any pair of positive integers m, n. Let a, b, c in A be arbitrary
(i). To each [(a c) + (b c)], (a + b) in B, there exist a least ( c + c ) in B such that (a + b) (c + c) (a c) + (b c),
(ii). To each [(ma a) + (nb b)], (ma + nb) in B, there exist a least element (a + b) in B such that (ma +nb) (a + b) (ma a) + (nb b),
since B is a Brouwerian Algebra
(i) (a + b) (c + c) (a c) + (b c),
(ii) (ma + nb) (a + b) (ma a) + (nb b), for all a, b, c in A and any pair of positive integers m, n.
References:
[1]. E. A. Nordhaus and Leo Lapidus, Brouwerian Geometry, Canad. J. Math.,6 (1954). [2]. G. Birkhoff, Lattice Theory, American Mathematical Society, Colloguium Publications, Volume 25, Providence R. I., 3rd Edition, 3rd Printing, (1979). [3]. K.L.N. Swamy, Dually Residuated Lattice Ordered Semigroup, Math. Ann. 159, 105 114, (1965). [4]. M. Jeyalakshmi and R. Natarajan, DR group, Acta Cienca Indica, Vol. XXIX. M, No.4, 823 830 (2003). [5]. M. Ward and R. P. Dilworth, Residuated Lattice, Trans, Am. Math., Soc. 45, (1939).