Abstract
In this paper, extension of relative co-annihilator in residuated lattices is introduced for subsets T and Y of residuated lattice L and is denoted by (T, Y). In this extension, T has a more important role than Y, as expected. It is proved if T is a filter, then co-annihilator of T relative to Y is a filter and is the same as the co-annihilator of T relative to the filter generated by Y. Also some theorems are stated and proved which determine the relationship between this special subset and the other types of filters. Finally, we give some conditions for subsets T and Y of residuated lattices L, for which (T, Y) is a special subset of L.
Keywords
Introduction
The concept of a commutative residuated lattice was firstly introduced by M. Ward and R.P. Dilworth [13] as generalization of ideal lattices of rings. H. Ono considered residuated lattices as an algebraic structure of substructural logics in [10]. P. Hájek introduced the notion of BL-algebra as a residuated lattice with two more conditions, namely divisibility and prelinearity to prove the completeness of Łukasiewicz logic as a many valued logic [4]. He showed that these algebras are the best algebraic counterparts of fuzzy logics generated by continuous t-norms [4]. Leuştean introduced the concept of co-annihilator of an element a relative to a filter F in a BL-algebra L as (F, a) = {x ∈ L|x ∨ a ∈ F} [8].
Here, we extend this notion to a residuated lattice L and arbitrary subsets T and Y of L.
This paper is organized as follows: in the next section we give some preliminaries including the basic definition and theorems that are needed in the sequel. In Section 3, we extend co-annihilators to arbitrary subsets T and Y of residuated lattices called co-annihilator of T relative to Y and denoted by (T, Y). We show that if T is a filter, then (T, Y) is a filter but it does not depend on Y, as expected. So we show that (T, Y) = (T, [Y)), where [Y) is the filter generated by subset Y. Also we investigate many properties of (T, Y) corresponding to constraints on T or Y. Examples are given for showing that some properties hold under some necessary condition. In Section 4, we prove some theorems which determine the relationship between this special subset and the other types of filters. Finally, we give conditions on subsets T and Y of residuated lattices L containing elements such as atoms and molecules, for which (T, Y) is a special subset of L.
Preliminaries
(i) (L, ∧ , ∨ , 0, 1) is a bounded lattice,
(ii) (L, ∗ , 1) is a commutative monoid,and
(iii) the operation ∗ and → form an adjoint pair,i.e.,
From now on by (L, ∨ , ∧ , ∗ , → , 0, 1) or simply L we mean a residuated lattice, unless otherwise specified.
(1)x ∨ y = 1 implies x ∗ y = x ∧ y,
(2)x ∨ (y ∗ z) ≥ (x ∨ y) ∗ (x ∨ z).
for all x, y in L: if x ∈ F and x ≤ y, then y ∈ F. for all x, y in F: x ∗ y ∈ F (i.e. F is closed under ∗).
Boolean filter (BF) iff for all x ∈ L, x ∨ ¬ x ∈ F. Prime filter (PF) iff for all x and y in L, x → y ∈ F or y → x ∈ F. Obstinate filter (OF) iff for all x and y in L, if x, y ∉ F, then x → y ∈ F and y → x ∈ F. Prime filter of the second kind (PF2) iff for all x and y in L, if x ∨ y ∈ F, then x ∈ F or y ∈ F. Boolean filter of the second kind (BF2) iff for all x ∈ L, x ∈ F or ¬x ∈ F. Fantastic filter (FF) iff for all x and y in L, y → x ∈ F imply ((x → y) → y) → x ∈ F. Involution filter (VF) iff for all x ∈ L, ¬¬ x → x ∈ F. Implicative filter (IF) iff for all x, y and z in L, x → (y → z) ∈ F and x → y ∈ F imply x → z ∈ F. Positive implicative filter (PIF) iff for all x, y and z in L, x → ((y → z) → y) ∈ F and x ∈ F imply y ∈ F. Pseudocomplementation filter (PSF) iff for all x ∈ L, ¬ (x ∧ ¬ x) ∈ F.
A proper filter F of L is said to be a maximal filter (MF) iff it is not included in any other proper filter of L.
We collect and summarize the connections between the above filters from [1, 6] into Fig. 1. In Fig. 1, by A ⟶ B we mean a filter of type A is a filter of type B and A/B means that filters of type A and B are equivalent.
M. Kondo claimed that fantastic filters and involution filters are equivalent [7]. In the following example we show that it is not true.
It is clear that F = {1} is an involution filter of L but it is not a fantastic filter of L. Since for m and n, we have n → m = 1 ∈ F, but ((m → n) → n) → m = m ∉ F.
Relative co-annihilators
In this section, we give definition of relative co-annihilators in a residuated lattice L and investigate some basic properties of these co-annihilators.
If Y = {a}, then we denote (T, {a}) by (T, a). For example, by choosing T = {f, m, 1} and Y = {0, a, 1} in Example 2, we have (T, Y) = {f, m, 1}.
In the following proposition, we consider (T, Y) for some special cases of T and Y.
(i) If Y =∅, then (T, Y) = L.
(ii) If T =∅ , Y ≠ ∅, then (T, Y) =∅.
(iii) (T, {0}) = T, (T, {1}) = L::iff::1 ∈ T.
(iv) ({0} , Y) = {0} ::iff::Y = {0}, ({1} , Y) ⊆ {x ∈ L| (∀ y ∈ Y) :x ∗ y = x ∧ y}.
(v) ({1} , {0}) = {1} , (L, {1}) = L, ({0} , {0}) = {0} , ({1} , {1}) = L.
(vi) (L, {0}) = L.
(vii) 1∉ T iff (T, L) = ∅.
(viii) (T, L) ⊆ T.
(i) We write (T, Y) in a more logical form as {x ∈ L| (∀ y) (y ∈ Y ⇒ x ∨ y ∈ T)}. So (T, ∅) = {x ∈ L| (∀ y) (y ∈ ∅ ⇒ x ∨ y ∈ T)} = L, since the formula (∀ y) (y ∈ ∅ ⇒ x ∨ y ∈ T) is always true for all x ∈ L.
(iv) We know ({1} , Y) = {x ∈ L| (∀ y ∈ Y) :x ∨ y = 1}, by Theorem 2.2, (1), we have ({1} , Y) ⊆ {x ∈ L| (∀ y ∈ Y) :x ∗ y = x ∧ y}. Also if ({0} , Y) = {x ∈ L| (∀ y ∈ Y) :x ∨ y = 0} = {0}, then we have x = y = 0, for all y ∈ Y, so Y = {0}. The converse is obvious.
(vii) By contrary, assume that (T, L)≠ ∅. So there exist x ∈ L such that x ∨ a ∈ T, for all a ∈ L. Since 1 ∈ L, therefore x ∨ 1 =1 ∈ T, which is a contradiction. Converse is easy to see.□
Since one of our main goals is to extend the notion of co-annihilator to filters, from now on we assume that all subsets under consideration are non-empty.
(i) T1 ⊆ T2 implies (T1, Y) ⊆ (T2, Y).
(ii) Y1 ⊆ Y2 implies (T, Y2) ⊆ (T, Y1).
(iii) (T1, Y) ∩ (T2, Z) ⊆ (T1 ∩ T2, Y ∩ Z).
(iv) (T, (T, Y ∩ Z)) ⊆ (T, (T, Y)) ∩ (T, (T, Z)).
(v) (T, ⋃ i∈IY i ) = ⋂ i∈I (T, Y i ) ⊆ ⋃ i∈I (T, Y i ) ⊆ (T, ⋂ i∈IY i ).
(vi) ⋂i∈I (T i , Y) = ( ⋂ i∈IT i , Y) and ⋃i∈I (T i , Y)⊆ ( ⋃ i∈IT i , Y).
(vii) ((T, Y) , Z) = ((T, Z) , Y) = ⋂ z∈Z,y∈Y (T, z∨y).
(viii) Y ⊆ (T, (T, Y)).
(ix) Y ∩ (T, Y) ⊆ T.
(x) (T, (T, (T, Y)) = (T, Y).
(xi) (T, Y) = ⋂ y∈Y (T, y).
(ii) Let x ∈ (T, Y2). Then x ∨ z ∈ T, for all z ∈ Y2. We have Y1 ⊆ Y2, so x ∈ (T, Y1).
(iii) Let x ∈ (T1, Y) ∩ (T2, Z). Then x ∨ y ∈ T1 and x ∨ z ∈ T2, for all y ∈ Y and z ∈ Z. Since Y ∩ Z ⊆ Y, Z, we have x ∨ u ∈ T1 ∩ T2, for all u ∈ Y ∩ Z, hence x ∈ (T1 ∩ T2, Y ∩ Z).
(iv) We have Y ∩ Z ⊆ Y, Z, by (ii), (T, Y) , (T, Z) ⊆ (T, Y ∩ Z) and so (T, (T, Y ∩ Z)) ⊆ (T, (T, Y)) , (T, (T, Z)). Hence (T, (T, Y ∩ Z)) is a lower bound for (T, (T, Y)) , (T, (T, Z)), therefore (T, (T, Y ∩ Z)) ⊆ (T, (T, Y)) ∩ (T, (T, Z)).
(v) By (ii), we have (T, ⋃ i∈IY i ) ⊆ (T, Y i ), for every i ∈ I. So (T, ⋃ i∈IY i ) is an lower bound for (T, Y i ), for every i ∈ I, therefore (T, ⋃ i∈IY i ) ⊆ ⋂ i∈I (T, Y i ).
Conversely, let x ∈ ⋂ i∈I (T, Y i ). Then x ∨ y i ∈ T, for all y i ∈ Y i . Now let z be an arbitrary element in ⋃i∈IY i . So there is i ∈ I such that z ∈ Y i . Hence the result holds due to the assumption.
Once again by (ii), we have (T, Y i ) ⊆ (T, ⋂ i∈IY i ), for every i ∈ I. So (T, ⋂ i∈IY i ) is an upper bound for (T, Y i ) for every i ∈ I, hence ⋃i∈I (T, Y i ) ⊆ (T, ⋂ i∈IY i ).
(vi) We have ⋂i∈IT i ⊆ T i , for every i ∈ I. By (i), ( ⋂ i∈IT i , Y) ⊆ (T i , Y), for every i ∈ I. So ( ⋂ i∈IT i , Y) ⊆ ⋂ i∈I (T i , Y).
Conversely, let x ∈ ⋂ i∈I (T i , Y). Then x ∨ y ∈ T i , for every i ∈ I, y ∈ Y, hence x ∨ y ∈ ⋂ i∈IT i , for all y∈Y. Thus x ∈ (⋂ i∈IT i , Y). The other part is similar.
(vii) We have that x ∈ ((T, Y) , Z) iff x ∨ z ∈ (T, Y), for all z ∈ Z iff (x ∨ z) ∨ y ∈ T, for all z ∈ Z, y ∈ Y iff x ∨ (z ∨ y) ∈ T, for all z ∈ Z, y ∈ Y iff x ∈ ⋂ z∈Z,y∈Y (T, z ∨ y).
(viii) Let x be an arbitrary element in Y. We must show that x ∨ z ∈ T, for all z ∈ (T, Y) that is, y ∨ z ∈ T, for all y ∈ Y, so x ∨ z ∈ T.
(ix) Let x ∈ Y ∩ (T, Y). Then x ∈ Y and x ∨ y ∈ T, for all y ∈ Y, hence x = x ∨ x ∈ T. Thus Y ∩ (T, Y) ⊆ T.
(x) By (viii), we have (T, Y) ⊆ (T, (T, (T, Y)) ). Let x ∈ (T, (T, (T, Y)) ). Then z ∨ x ∈ T, for all z ∈ (T, (T, Y)). Since Y ⊆ (T, (T, Y)), we conclude that x ∨ z ∈ T, for all z ∈ Y. Hence x ∈ (T, Y).
(xi) x ∈ (T, Y) ⇔ (∀ y ∈ Y) :x ∨ y ∈ T ⇔ (∀ y∈Y) :x ∈ (T, y) ⇔ x ∈ ⋂ y∈Y (T, y).□
By an upset U of L, we mean a subset U of L with the property that, if x ∈ U, y ∈ L and x ≤ y, then y ∈ U.
(i) T ⊆ (T, Y).
(ii) (T, Y) = L iff Y ⊆ T, (So (L, Y) = L).
(iii) (T, L) = T and (T, T) = L.
(iv) (T, (T, T)) = T and ((T, T) , T) = L.
(v) T ⊆ Y implies (T, Y) ∩ Y = T.
(vi) Y ∩ (T, Y) = Y ∩ T.
(vii) (T, (T, Y)) ∩ (T, Y) = T.
(ii) If (T, Y) = L, then 0 ∈ (T, Y), hence y = 0 ∨ y ∈ T, for all y ∈ Y. Let y be an arbitrary element in Y. Then for any x ∈ L, y ≤ x ∨ y, hence x ∨ y ∈ T. That is, for any x ∈ L, we have that x ∈ (T, Y).
(iii) By (i) and Proposition 3.2 (viii), (T, L) = T. Now, Let x be an arbitrary element in L. We have t ≤ x ∨ t, for all t ∈ T, so by the definition of an upset x ∨ t ∈ T, for all t ∈ T. Hence x ∈ (T, T).
(iv) It is a straight conclusion from (ii) and (iii).
(v) An immediate consequence of (i) and Proposition 3.3 (ix).
(vi) By (i), we have T ⊆ (T, Y). So Y ∩ T ⊆ Y ∩ (T, Y). We have Y ∩ (T, Y) ⊆ Y, also by Proposition 3 (ix), Y ∩ (T, Y) ⊆ T which means Y ∩ (T, Y) is a lower bound for Y and T. Hence Y ∩ (T, Y) ⊆ Y ∩ T.
(vii) It follows when we put (T, Y) instead of Y in (vi).
From Proposition 3.4 (ii) and (iii), we can conclude that:
Let T1 and T2 be filters of L. We recall from [3] that T1 ⟶ T2 = {x ∈ L ∣ T1 ∩ [x) ⊆ T2}, where [x) = {a ∈ L ∣ a ≥ x n for some n ≥ 1}.
(i) (T, Y) is a filter of L.
(ii) (T, ⋁ i∈IY i ) = ⋂ i∈I (T, Y i ).
(iii) (T1, Y) ∩ (T2, Y) ⊆ (T1 ⟶ T2, Y).
By ⋁i∈IY i , we mean the filter generated by ⋃i∈IY i and denoted by [⋃ i∈IY i ). If A is a non-empty subset of L, then [A) = {x ∈ L ∣ x ≥ a1 ∗ . . . ∗ a n , for some n ≥ 1 and a1, . . . , a n ∈ A}.
(ii) We know Y i ⊆ ⋁ i∈IY i = [⋃ i∈IY i ), for all i ∈ I, so by Proposition 3.3 (ii), (T, ⋁ i∈IY i ) ⊆ (T, Y i ), for all i ∈ I. So (T, ⋁ i∈IY i ) ⊆ ⋂ i∈I (T, Y i ). Let x be an arbitrary element in ⋂i∈I (T, Y i ) which means x ∈ (T, Y i ), for all i ∈ I. We must show that x ∨ z ∈ T, for all z ∈ ⋁ i∈IY i = [⋃ i∈IY i ). Let z be an arbitrary element in ⋁i∈IY i . Hence there exist i1, i2, . . . , i m in I, y i j ∈ Y j (1 ≤ j ≤ m) such that z ≥ y i 1 ∗ y i 2 ∗ . . . ∗ y i m . By Theorem 2.2 (2), we obtain x ∨ z ≥ x ∨ (y i 1 ∗ y i 2 ∗ . . . ∗ y i m ) ≥ (x ∨ y i 1 ) ∗ (x ∨ y i 2 ) ∗ . . . ∗ (x ∨ y i m ). Since x ∨ y i j ∈ T, for every 1 ≤ j ≤ m, by Definition 2.3, we get x ∨ z ∈ T.
(iii) Let x ∈ (T1, Y) ∩ (T2, Y). Then x ∨ y ∈ T1, T2, for all y ∈ Y. It is sufficient to show that T1 ∩ [x ∨ y) ⊆ T2, for all y ∈ Y. We have x ∨ y ∈ T2 for all y ∈ Y, so [x ∨ y) ⊆ T2, for all y ∈ Y and therefore T1 ∩ [x ∨ y) ⊆ T2, for all y ∈ Y, which means x ∈ (T1 ⟶ T2, Y).
In the following we give examples to show that some of the statements in Proposition 3.3, 3.4 and Theorem 3.6 are true only under necessary conditions such as upset, filter, etc, and just one side of some of them holds.
Put T1 = {b, c, 1}, T2 = {a, c, 1} which are not filters, Y = {c, a, b} and Z = {c, 1}, then (T1, Y) = {b, c, 1} and (T2, Z) = {0, a, b, c, 1}, hence (T1 ∩ T2, Y ∩ Z) = ({c, 1} , {c}) = {0, a, b, c, 1} ⊈ (T1, Y) ∩ (T2, Z) = {b, c, 1}. This shows that the other side of Proposition 3.3 (iii) fails.
By setting Y1 = {b, 2}, Y2 = {a, 2} and T = {0, c, 2}, then (T, Y1) = {a, c, 2}, (T, Y2) = {b, c, 2} and (T, Y1 ∩ Y2) = {0, a, b, c, 1, 2}, so (T, Y1 ∩ Y2) ⊈ (T, Y1) ∪ (T, Y2). This shows that converse of Proposition 3.3 (v) fails.
If we choose T = {c, 1}, Y = {c, 1, 2} and Z = {c, b}, then (T, Y) =∅ and (T, Z) = {a, c, 1}, so (T, (T, Y)) ∩ (T, (T, Z)) = L ∩ {b, c, 1} ⊈ (T, (T, Y∩Z)) = {c, 1}. This shows that the other side of Proposition 3.3 (iv) fails.
If we choose T1 = {b, c, 1}, T2 = {a, c, 1} and Y = {c, a, b}, then (T1, Y) = {b, c, 1} and (T2, Y)= {a, c, 1}, hence (T1 ∪ T2, Y) = {0, a, b, c, 1} ⊈ (T1, Y) ∪ (T2, Y). This shows that the other side of Proposition 3.3 (vi) fails.
By choosing T = {b, c, 1} and Y = {c, a, b}, we have (T, Y) = {b, c, 1} and (T, (T, Y)) = {0, a, b, c, 1}. Hence (T, (T, Y)) ⊈ Y and T ⊈ Y ∩ (T, Y) = {b, c}. This shows that converse of Proposition 3.3 (viii) , (ix) fails.
Also if we choose T1 = {c, 1, 2, 3}, T2 ={b, c, 1, 2, 3} and Y = {0, a}, then (T1, Y) = {c, 1, 2, 3}, (T2, Y) = {b, c, 1, 2, 3} and T1 ⟶ T2 = L, hence (T1 ⟶ T2, Y) = L ⊈ (T1, Y) ∩ (T2, Y). This shows that the other side of Theorem 3.6 (iii) fails.
Then L = (L, ∨ , ∧ , ∗ , ⟶ , 0, 1) is a residuated lattice to the operation defined in Table 3, also the lattice structure of L is shown in Fig. 3. Put T = {1, b, c, d, e} and Y = L. We see that Y is a filter and T is not a filter. We have (T, Y) = {1, b, c, d, e}, that is not a filter. This shows that T being filter is a necessary condition for Theorem 3.6 (i). Once again, put T = {0, a, e, 1} and Y = {0, c, d, e, 1}. We see that T is not an upset. We have (T, Y) = {a, 1} and T ⊈ (T, Y). This shows that T being upset is a necessary condition for Proposition 3.4 (i).
Also if we choose T1 = {1, b, c, d, e}, T2 = {0, a, e, 1} and Y = {0, c, d, e, 1}, then (T1, Y) = {1, b, c, d, e} and (T2, Y) = {a, 1}, hence (T1, Y) ⊈ (T2, Y). This shows that Proposition 3.3 (i) fails without the condition T1 ⊆ T2.
By choosing Y1 = {1, b, c, d, e}, Y2 = {0, a, e, 1} and T = {0, c, e, 1}, then (T, Y1) = {1, e} and (T, Y2) = {c, e, 1}, so (T, Y2) ⊈ (T, Y1). This shows that Proposition 3.3 (ii) fails without the condition Y1 ⊆ Y2.
In Theorem 3.6 (i), we showed that if T is a filter, then (T, Y) is a filter but it does not important on the set Y, to be a filter or not. In the other words, it doesn’t need filter restriction on the set Y. It is interesting to know that if Y is replaced by [Y), we get the same co-annihilator.
Recall from [12] that an element a ∈ L is called a node, if and only if for every x ∈ L either x ≤ a or a ≤ x.
Now we can extend previous Proposition to all elements of L, specifically we assume that L is a linear residuated lattice.
We recall that in an MTL-algebra L (a residuated lattice with the condition (x → y) ∨ (y → x) =1) we have B (L) = Rg (L) ∩ Id (L) [2]. So it is worth to note that (B (L) , Y) = (Rg (L) , Y) ∩ (Id (L) , Y), for any Y ⊆ L, where Rg (L) = {x ∈ L|: ¬¬ x = x} and B (L) = {x ∈ L|:x ∨ ¬ x = 1}.
Relationship between relative co-annihilator and filters
Now, we investigate the relationship between the notions of various types of filters and their relative co-annihilators in a residuated lattice L.
(i) If T is a Boolean filter of the second kind (BF2), then (T, Y) is so. (ii) If T is a pseudocomplementation filter (PSF), of L, then (T, Y) is so. (iii) If T is an implicative filter (IF), of L, then (T, Y) is so.
(i) (T, Y) is a prime filter of the second kind of L.
(ii) (T, Y) = T.
(iii) (T, (T, Y)) = L.
(ii) By Proposition 3.4 (i), we have T ⊆ (T, Y). It is sufficient to show that (T, Y) ⊆ T. By contrary, we assume that a ∈ (T, Y) and a ∉ T, so a ∨ y ∈ T, for all y ∈ Y. By assumption, we have y ∈ T, for all y ∈ Y, hence Y ⊆ T, which is a contradiction.
(iii) An immediate consequence of (ii) and Proposition 3.4 (iii).
Finally, we give conditions on subsets T and Y of residuated lattices L containing elements such as atoms and molecules, for which (T, Y) is a special subset of L.
Recall that an element of L is an atom, if there aren’t any element between that element and bottom element and is a molecule, if there aren’t any element between that element and top element in a residuated lattice.
(i) If L contains only one molecule c, 1 ∈ T, c ∉ T and c ∈ Y, then (T, Y) = {1}.
(ii) If L contains at least one molecule c, c ∈ T, 1 ∈ T and Y only contains the molecule c, then (T, Y) = L.
(iii) If L contains at least one atom, T = AT (L) ∪ {1} and Y = AT (L), where AT (L) is the set of all atoms of L, then (T, Y) is a subset of AT (L) ∪ {0, 1}.
In particular, if L consists of at least two atoms and one molecule, then (T, Y) = {0, 1}, and if L consists of one atom b, then (T, Y) = {0, b, 1}.
(iv) If L contains only one atom b and at least two molecules, T = {1, b}, Y consists of at least one molecule, m, and 1 ∈ Y, then M = {x ∈ L| x is a molecule of L and x ∉ Y} ⊆ (T, Y) ⊆ ({1} , m). In particular, if Y = {1, m}, then (T, Y) = ({1} , m).
(ii) Let c be the molecule of L. For all a ∈ L, a ∨ c = c ∈ T or a ∨ c = 1 ∈ T, hence (T, Y) = L.
(iii) It is obvious that 0, 1 ∈ (T, Y). Let AT (L) = {a i } i∈I and x be an element of L other than 0, 1 and {a i }, for all i ∈ I. Then either x ∧ a j = 0 or x ∧ a j = a j , for some j ∈ I. The first case does not happen, since otherwise x ∈ AT (L) that is not true. In the latter case x is comparable with some a j (j ∈ I), thus x ∨ a j = x which is not in T. Therefore x ∉ (T, Y).
(iv) Let x be an element of M. Then x ∨ y = 1 ∈ T, for all y ∈ Y, so x ∈ (T, Y). Now let x ∈ (T, Y). Then either x ∨ m = m or x ∨ m = 1. The first case does not happen, since otherwise x ∉ (T, Y). Hence x ∈ ({1} , m). □
Conclusion and future research
We introduced the extension of co-annihilator in residuated lattices and investigated its properties. It is extended to two subsets of L such as T, Y and denoted by (T, Y). In this extension, T has a more important role than Y, as expected. It is proved if T is a filter, then (T, Y) is a filter but it is not important that Y be a filter or not. In the other words, it doesn’t need filter restriction on the set Y for being filter. So we showed that (T, Y) = (T, [Y)). Examples are given for better understanding the results. In addition, we showed that if T is a Boolean filter of the second kind, then (T, Y) is so. In other words, (T, Y) is an obstinate filter and therefore it is (MF), (BF), (PF), (PF2), (FF), (VF) and (PIF). We proved that if T is (PF2) and Y ⊈ T, then (T, Y) is so and (T, Y) = T. We also showed that if T is an upset of L and Y ⊆ T, then (T, (T, Y)) = T. and other results obtained. Finally we have given one of our main theorems consisting of statements concerning some constraints on subsets T and Y as well as on L (e.g. containing special elements such as atoms or molecules) and found co-annihilators as special subsets.
In our future work, we will continue our study of algebraic properties of this extension, especially singleton subsets, Y, of L. We will use these filters to define congruence relations on L. It seems that the residuated lattice can be partitioned in a very “nice" way.
Footnotes
Acknowledgments
We wish to thank the reviewers for excellent suggestions that have been incorporated into the paper.
