Abstract
In this article, we present new methods for constructing uninorms on bounded lattices under the additional constraints and prove that some of these constraints are sufficient and necessary for the uninorms. Moreover, some illustrative examples for the construction of uninorms are provided. At last, we show that the additional constraints on t-norms (t-conorms) and t-subnorms (t-subconorms) of some uninorms in the literature are exactly sufficient and necessary.
Keywords
Introduction
In [5], as a function from [0, 1] × [0, 1] to [0, 1], the aggregative operator is for the theory of evaluation, which “sheds new fight on such well-known concepts as membership, conjunction and disjunction and seems to be a very promising tool to handle representation problems as they grow from the fields of theory of fuzzy set and its many applications of human decision making and of multi-criteria analysis” [5].
Triangular norms (t-norms for short) and triangular conorms (t-conorms for short) on the unit interval [0, 1], introduced by Menger [26], Schweizer and Sklar [30, 32], play an important role in many fields, such as fuzzy set theory, fuzzy logic and so on (see, e.g., [4, 18, 25, 31, 34, 40]). Uninorms on [0, 1], as an important aggregative operator generalizing the notions of t-norms and t-conorms, are introduced by Yager and Rybalov [37] and then applied to various fields [14–16, 28, 29], such as fuzzy logic, fuzzy set theory, expert systems, neural networks and so on.
Recently, on one hand, because of “For general systems, where we cannot always expect real (or comparable) data, this extension of the underlying career together with its structure is significant...” [9], the researchers widely study uninorms on the bounded lattices instead of [0, 1]. On the other hand, In [17], fuzzy sets are extended to L-fuzzy sets, where L is a lattice. Then many fuzzy theories are generalized to L-fuzzy theories, such as L-fuzzy topology. From the point of view of generalization, it is necessary to study uninorms on the bounded lattices. This generalization may makes uninorms on lattices to be applied in L-fuzzy theory, lattice-valued logic and so on.
About the methods for the construction of uninorms, they mainly focus on t-norms (t-conorms) [1, 3, 6–8, 10, 11, 13, 23, 35], t-subnorms (t-subconorms) [19, 22, 38], closure operators (interior operators) [9, 20, 27, 39], additive generators [21] and uninorms [36].
For the extension, as shown in many existing results, yielding uninorms on the bounded lattice always needs some additional constraints on the lattice, t-norms (resp. t-conorms), t-subnorms (resp. t-subconorms) or closure operators (resp. interior operators) to guarantee that the methods work well. However, we may ask the following question: are these additional constraints necessary?
In this paper, we present new methods for constructing uninorms on the bounded lattices under some additional constraints and show that some constraints are necessary, that is, these constraints are sufficient and necessary for the uninorms. Moreover, some sufficient conditions of some uninorms are modified to be sufficient and necessary.
Preliminaries
In this section, we recall some preliminary details concerning bounded lattice and results related to aggregation functions on bounded lattices.
Throughout this article, unless stated otherwise, we denote L as a bounded lattice with the top and bottom elements 1 and 0, respectively.
(i) An operation T : L2 → L is called a t-norm on L if it is commutative, associative, and increasing with respect to both variables, and it has the neutral element 1 ∈ L, that is, T (1, x) = x for all x ∈ L. The greatest t-norm T∧ on L is given as T∧ (x, y) = x ∧ y;
(ii) An operation S : L2 → L is called a t-conorm on L if it is commutative, associative, and increasing with respect to both variables, and it has the neutral element 0 ∈ L, that is, S (0, x) = x for all x ∈ L. The smallest t-conorm S∨ on L is given as S∨ (x, y) = x ∨ y.
(i) T e = U ∣ [0, e] 2 : [0, e] 2 → [0, e] is a t-norm on [0, e];
(ii) S e = U ∣ [e, 1] 2 : [e, 1] 2 → [e, 1] is a t-conorm on [e, 1].
T e and S e given in proposition 2.5 are called the underlying t-norm and t-conorm of a uninorm U on a bounded lattice L with the neutral element e, respectively. Throughout this study, we denote T e as the underlying t-norm and S e as the underlying t-conorm of a given uninorm U on L.
(i) An operation F : L2 → L is called a t-subnorm on L if it is commutative, associative, increasing with respect to both variables, and F (x, y) ≤ x ∧ y for all x, y ∈ L.
(ii) An operation R : L2 → L is called a t-subconorm on L if it is commutative, associative, increasing with respect to both variables, and R (x, y) ≥ x ∨ y for all x, y ∈ L.
(i)If x ∥ y for all x ∈ I e and y ∈ [e, 1 [, then R (x, y) ∈ I e or R (x, y) =1 for all x, y ∈ I e .
(ii)If x ∥ y for all x ∈ I e and y ∈]0, e], then F (x, y) ∈ I e or F (x, y) =0 for all x, y ∈ I e .
New construction of uninorms on bounded lattices
In this section, we present new construction of uninorms on some appropriate bounded lattices L, which are constructed by means of t-conorms (t-norms) and t-subconorms (t-subnorms). Moreover, the sufficient and necessary conditions are provided for these uninorms.
is a uninorm on L with e ∈ L \ {0, 1} iff S e (x, y) <1 for all x, y < 1.
Necessity. Let U1 be a uninorm on L with the identity e. Then we prove that S e (x, y) <1 for all x, y < 1. Assume that there are some elements x ∈] e, 1 [ and y ∈] e, 1 [ such that S e (x, y) =1. Then U1 (x, U1 (y, 0)) = U1 (x, 0) =0 and U1 (U1 (x, y) , 0) = U1 (S e (x, y) , 0) = U1 (1, 0) =1. Since 0 ≠ 1, the associativity property of U1 is violated. Then U1 is not a uninorm on L, which is a contradiction. Hence, S e (x, y) <1 for all x, y < 1.
Sufficiency. To prove the sufficiency, we compare U1 with
I. Monotonicity: We prove that if x ≤ y, then for all z ∈ L, U1 (x, z) ≤ U1 (y, z).
If one of x, y, z is equal to 1, then it is clear that U1 (x, z) ≤ U1 (y, z). There is no 1 in any of the following cases.
1. Let x ∈ [0, e [.
1.1. y ∈ [0, e [,
1.1.1. z ∈ I e ,
U1 (x, z) = z = U1 (y, z)
1.2. y ∈ [e, 1 [,
1.2.1. z ∈ I e ,
U1 (x, z) = z = U1 (y, z)
1.3. y ∈ I e ,
1.3.1. z ∈ [0, e [,
U1 (x, z) = T e (x, z) ≤ y = U1 (y, z)
1.3.2. z ∈ [e, 1 [,
U1 (x, z) = x ≤ y = U1 (y, z)
1.3.3. z ∈ I e ,
U1 (x, z) = z ≤ y ∨ z = U1 (y, z)
2. Let x ∈ I e .
2.1. y ∈ I e ,
2.1.1. z ∈ [0, e [,
U1 (x, z) = x ≤ y = U1 (y, z)
II. Associativity: We prove that U1 (x, U1 (y, z)) = U1 (U1 (x, y) , z) for all x, y, z ∈ L.
If one of x, y, z is equal to 1, then it is clear that U1 (x, U1 (y, z)) =1 = U1 (U1 (x, y) , z). So there is no 1 in any of the following cases.
1. Let x ∈ [0, e [.
1.1. y ∈ [0, e [,
1.1.1. z ∈ I e ,
U1 (x, U1 (y, z)) = U1 (x, z) = z = U1 (T e (x, y) , z) = U1 (U1 (x, y) , z)
1.2. y ∈ [e, 1 [,
1.2.1. z ∈ I e ,
U1 (x, U1 (y, z)) = U1 (x, z) = z = U1 (x, z) U1 (U1 (x, y) , z)
1.3. y ∈ I e ,
1.3.1. z ∈ [0, e [,
U1 (x, U1 (y, z)) = U1 (x, y) = y = U1 (y, z) = U1 (U1 (x, y) , z)
1.3.2. z ∈ [e, 1 [,
U1 (x, U1 (y, z)) = U1 (x, y) = y = U1 (y, z) = U1 (U1 (x, y) , z)
1.3.3. z ∈ I e ,
1.3.3.1. y ∨ z ∈ I e ,
U1 (x, U1 (y, z)) = U1 (x, y ∨ z) = y ∨ z = U1 (y, z) = U1 (U1 (x, y) , z)
1.3.3.2. y ∨ z = 1,
U1 (x, U1 (y, z)) = U1 (x, y ∨ z) =1 = y ∨ z = U1 (y, z) = U1 (U1 (x, y) , z)
2. Let x ∈ [e, 1 [.
2.1. y ∈ [0, e [,
2.1.1. z ∈ I e ,
U1 (x, U1 (y, z)) = U1 (x, z) = z = U1 (y, z) = U1 (U1 (x, y) , z)
2.2. y ∈ I e ,
2.2.1. z ∈ [0, e [,
U1 (x, U1 (y, z)) = U1 (x, y) = y = U1 (y, z) = U1 (U1 (x, y) , z)
3. Let x ∈ I e .
3.1. y ∈ [0, e [,
3.1.1. z ∈ [0, e [,
U1 (x, U1 (y, z)) = U1 (x, T e (y, z)) = x = U1 (x, z) = U1 (U1 (x, y) , z)
3.1.2. z ∈ [e, 1 [,
U1 (x, U1 (y, z)) = U1 (x, y) = x = U1 (x, z) = U1 (U1 (x, y) , z)
3.1.3. z ∈ I e ,
U1 (x, U1 (y, z)) = U1 (x, z) = x ∨ z = U1 (x, z) = U1 (U1 (x, y) , z)
3.2. y ∈ [e, 1 [,
3.2.1. z ∈ [0, e [,
U1 (x, U1 (y, z)) = U1 (x, z) = x = U1 (x, z) = U1 (U1 (x, y) , z)
3.3. y ∈ I e ,
3.3.1. z ∈ [0, e [,
3.3.1.1. x ∨ y ∈ I e ,
U1 (x, U1 (y, z)) = U1 (x, y) = x ∨ y = U1 (x ∨ y, z) = U1 (U1 (x, y) , z)
3.3.1.2. x ∨ y = 1,
U1 (x, U1 (y, z)) = U1 (x, y) = x ∨ y = 1 = U1 (x ∨ y, z) = U1 (U1 (x, y) , z)
Hence, U1 is a uninorm on L with a neutral element e.
It is worth pointing out that if the condition that x ∥ y for all x ∈ I e and y ∈ [e, 1 [ in Theorem 3.1 is not satisfied, then U1 may not be a uninorm on L1. Similarly, if the condition that x ∥ y for all x ∈ I e and y ∈]0, e] in Theorem 3.1 is not satisfied, then U2 may not be a uninorm on L1. The following example will show the above facts.

The lattice L
The function U1 on L1 given in Fig. 1
The function U2 on L1 given in Fig. 1
(1) If x ∥ y for all x ∈ I e and y ∈ [e, 1 [ and R (x, y) <1 for all x, y < 1, then U3 is a uninorm on L with e ∈ L \ {0, 1} iff T e (x, y) >0 for all x, y > 0.
(2) If x ∥ y for all x ∈ I e and y ∈ [e, 1 [ and I e ∪]0, e [≠ ∅, then U3 is a uninorm on L with e ∈ L \ {0, 1} iff T e (x, y) >0 for all x, y > 0 and R (x, y) <1 for all x, y < 1.
Necessity. Let the function U3 be a uninorm on L with the identity e. Then we will prove that T e (x, y) >0 for all x, y > 0. Assume that there are some elements x ∈]0, e [ and y ∈]0, e [ such that T e (x, y) =0. Then U3 (x, U3 (y, 1)) = U3 (x, 1) =1 and U3 (U3 (x, y) , 1) = U3 (T e (x, y) , 1) = U3 (0, 1) =0. Since 0 ≠ 1, the associativity property is violated. Hence, U3 is not a uninorm on L which is a contradiction. Therefore, the condition that T e (x, y) >0 for all x, y > 0 is necessary.
Sufficiency. To prove the sufficiency, we compare U3 with
The commutativity of U3 and the fact that e is a neutral element are evident. Hence, we prove only the monotonicity and the associativity of U3.
I. Monotonicity: We prove that if x ≤ y, then for all z ∈ L, U3 (x, z) ≤ U3 (y, z).
1.x = 0 or y = 0 or z = 0
U3 (x, z) =0 ≤ U3 (y, z)
II. Associativity: We prove that U3 (x, U3 (y, z)) = U3 (U3 (x, y) , z) for all x, y, z ∈ L.
If one of x, y, z is equal to 0, then it is clear that U3 (x, U3 (y, z)) = U3 (U3 (x, y) , z).
Hence, U3 is a uninorm on L with a neutral element e.
(2) Next we just prove that if x ∥ y for all x ∈ I e and y ∈ [e, 1 [ and I e ∪]0, e [≠ ∅, then the condition R (x, y) <1 for all x, y < 1 is necessary.
Let the function U3 be a uninorm on L with the identity e. Then we will prove that R (x, y) <1 for all x, y < 1. Assume that there are some elements x ∈] e, 1 [ and y ∈] e, 1 [ such that R (x, y) =1. If z ∈ I e ∪]0, e [, then we obtain U3 (x, U3 (y, z)) = U3 (x, z) = z and U3 (U3 (x, y) , z) = U3 (R (x, y) , z) = U3 (1, z) =1. Since z ≠ 1, the associativity property is violated. Hence, U3 is not a uninorm on L which is a contradiction. Therefore, the condition that R (x, y) <1 for all x, y < 1 is necessary.
(1) If x ∥ y for all x ∈ I e and y ∈]0, e] and F (x, y) >0 for all x, y > 0, then U4 is a uninorm on L with e ∈ L \ {0, 1} iff S e (x, y) <1 for all x, y < 1.
(2) If x ∥ y for all x ∈ I e and y ∈]0, e] and I e ∪] e, 1 [≠ ∅, then U4 is a uninorm on L with e ∈ L \ {0, 1} iff F (x, y) >0 for all x, y > 0 and S e (x, y) <1 for all x, y < 1.
It is worth pointing out that if the condition that x ∥ y for all x ∈ I e and y ∈ [e, 1 [ in Theorem 3.4 is not satisfied, then U3 may not be a uninorm on L1. Similarly, if the condition that x ∥ y for all x ∈ I e and y ∈]0, e] in Theorem 3.5 is not satisfied, then U4 may not be a uninorm on L1.
The function U3 on L1 given in Fig. 1
(2) If we take S e (x, y) = S∨ (x, y) on [e, 1] and F (x, y) = x ∧ y, then the function U4 on L1, shown in Table 4, is not a uninorm on L1 with the neutral element e. In fact, the associativity is not satisfied, since U4 (g, U4 (c, f)) = U4 (g, a) = g and U4 (U4 (g, c) , f) = U4 (c, f) = a.
The function U4 on L1 given in Fig. 1
is a uninorm on L with the neutral element e iff x > y for all x ∈ I e and y ∈ [0, e [.
Necessity. Let the function U5 be a uninorm on L with the identity e. Then we will prove that x > y for all x ∈ I e and y ∈ [0, e [. Assume that there are some elements x ∈ I e and y ∈ [0, e [ such that x ∥ y. Then U5 (y, U5 (x, 1)) = U5 (y, 1) = y and U5 (U5 (y, x) , 1) = U5 (x ∧ y, 1) = x ∧ y. Since y ≠ x ∧ y, the associativity property is violated. Then U5 is not a uninorm on L which is a contradiction. Hence, x > y for all x ∈ I e and y ∈ [0, e [.
Sufficiency. Let x > y for all x ∈ I e and y ∈ [0, e [, with x ∥ y for all x ∈ I e and y ∈ [e, 1 [. The commutativity of U5 and the fact that e is a neutral element are evident. Hence, we prove only the monotonicity and the associativity of U5.
I. Monotonicity: We prove that if x ≤ y, then for all z ∈ L, U5 (x, z) ≤ U5 (y, z). The proof is split into all possible cases. If one of x, y, z is equal to e, then it is clear that U5 (x, z) = z = U5 (y, z)
1. Let z = e.
U5 (x, z) = x ≤ y = U5 (y, z)
2. Let x = e.
2.1. y = e,
U5 (x, z) = z = U5 (y, z)
2.2. y ∈] e, 1],
2.2.1. z ∈ [0, e [,
U5 (x, z) = z = U5 (y, z)
2.2.2. z ∈] e, 1],
U5 (x, z) = z ≤ 1 = U5 (y, z)
2.2.3. z ∈ I e ,
U5 (x, z) = z ≤ 1 = U5 (y, z)
3. Let y = e.
3.1. x ∈ [0, e [,
3.1.1. z ∈ [0, e [,
U5 (x, z) = T e (x, z) ≤ z = U5 (y, z)
3.1.2. z ∈] e, 1],
U5 (x, z) = x ≤ z = U5 (y, z)
3.1.3. z ∈ I e ,
U5 (x, z) = x ∧ z = x ≤ z = U5 (y, z)
There is no e in any of the following cases.
1. Let x ∈ [0, e [.
1.1. y ∈ [0, e [,
1.1.1. z ∈ [0, e [,
U5 (x, z) = T e (x, z) ≤ T e (y, z) = U5 (y, z)
1.1.2. z ∈] e, 1],
U5 (x, z) = x ∧ z = x ≤ y = y ∧ z = U5 (y, z)
1.1.3. z ∈ I e ,
U5 (x, z) = x ∧ z = x ≤ y = y ∧ z = U5 (y, z)
1.2. y ∈] e, 1],
1.2.1. z ∈ [0, e [,
U5 (x, z) = T e (x, z) ≤ z = y ∧ z = U5 (y, z)
1.2.2. z ∈] e, 1],
U5 (x, z) = x ∧ z = x ≤ 1 = U5 (y, z)
1.2.3. z ∈ I e ,
U5 (x, z) = x ∧ z = x ≤ 1 = U5 (y, z)
1.3. y ∈ I e ,
1.3.1. z ∈ [0, e [,
U5 (x, z) = T e (x, z) ≤ z = y ∧ z = U5 (y, z)
1.3.2. z ∈] e, 1],
U5 (x, z) = x ∧ z = x ≤ 1 = U5 (y, z)
1.3.3. z ∈ I e ,
U5 (x, z) = x ∧ z = x ≤ R (y, z) = U5 (y, z)
2. Let x ∈] e, 1].
2.1. y ∈] e, 1],
2.1.1. z ∈ [0, e [,
U5 (x, z) = x ∧ z = z = y ∧ z = U5 (y, z)
2.1.2. z ∈] e, 1],
U5 (x, z) =1 = U5 (y, z)
2.1.3. z ∈ I e ,
U5 (x, z) =1 = U5 (y, z)
3. Let x ∈ I e .
3.1. y ∈ I e ,
3.1.1. z ∈ [0, e [,
U5 (x, z) = x ∧ z = z = y ∧ z = U5 (y, z)
3.1.2. z ∈] e, 1],
U5 (x, z) =1 = U5 (y, z)
3.1.3. z ∈ I e ,
U5 (x, z) = R (x, z) ≤ R (y, z) = U5 (y, z)
II. Associativity: We need to prove that U5 (x, U5 (y, z))
= U5 (U5 (x, y) , z) for all x, y, z ∈ L. The proof is split into all possible cases. If one of x, y, z is equal to e, then it is clear that U5 (x, U5 (y, z)) = U5 (U5 (x, y) , z). So there is no e in any of the following cases. By Theorem 3.12 of [19], we only need to consider the following cases:
1. Let x ∈ [0, e [.
1.1. y ∈ [0, e [,
1.1.1. z ∈ [0, e [,
U5 (x, U5 (y, z)) = T e (x, T e (y, z)) = T e (T e (x, y) , z) = U5 (U5 (x, y) , z)
1.1.2. z ∈] e, 1],
U5 (x, U5 (y, z)) = U5 (x, y ∧ z) = T e (x, y) = U5 (T e (x, y) , z) =
U5 (U5 (x, y) , z)
1.1.3. z ∈ I e ,
U5 (x, U5 (y, z)) = U5 (x, y ∧ z) = T e (x, y) = U5 (T e (x, y) , z) =
U5 (U5 (x, y) , z)
1.2. y ∈] e, 1],
1.2.1. z ∈] e, 1],
U5 (x, U5 (y, z)) = U5 (x, 1) = x = U5 (x, z) = U5 (U5 (x, y) , z)
1.2.2. z ∈ I e ,
U5 (x, U5 (y, z)) = U5 (x, 1) = x, U5 (U5 (x, y) , z) = U5 (x, z) = x
and U5 (y, U5 (x, z)) = U5 (y, x) = x
1.3. y ∈ I e ,
1.3.1. z ∈ I e ,
U5 (x, U5 (y, z)) = U5 (x, R (y, z)) = x = U5 (x, z) = U5 (U5 (x, y) , z)
2. Let x ∈] e, 1].
2.1. y ∈] e, 1],
2.1.1. z ∈] e, 1],
U5 (x, U5 (y, z)) = U5 (x, 1) =1 = U5 (1, z) = U5 (U5 (x, y) , z)
2.1.2. z ∈ I e ,
U5 (x, U5 (y, z)) = U5 (x, 1) =1 = U5 (1, z) = U5 (U5 (x, y) , z)
2.2. y ∈ I e ,
2.2.1. z ∈ I e ,
U5 (x, U5 (y, z)) = U5 (x, R (y, z)) =1 = U5 (1, z) = U5 (U5 (x, y) , z)
3. Let x ∈ I e .
3.1. y ∈ I e ,
3.1.1. z ∈ I e ,
3.1.1.1. R (x, y) =1, R (y, z) =1,
U5 (x, U5 (y, z)) = U5 (x, R (y, z)) =1 = U5 (R (x, y) , z) = U5 (U5 (x, y) , z)
3.1.1.2. R (x, y) =1, R (y, z) ∈ I
e
,
3.1.1.3. R (x, y) ∈ I
e
, R (y, z) =1,
3.1.1.4. R (x, y) ∈ I e , R (y, z) ∈ I e ,
U5 (x, U5 (y, z)) = R (x, R (y, z)) = R (R (x, y) , z) = U5 (U5 (x, y) , z)
Hence, by Theorem 3.12 of [19], U5 (x, U5 (y, z)) = U5 (U5 (x, y) , z) for all x, y, z ∈ L. Therefore, U5 is a uninorm on L with the neutral element e.
It is worth pointing out that if the condition that x ∥ y for all x ∈ I e and y ∈ [e, 1 [ in Theorem 3.7 is not satisfied, then U5 may not be a uninorm on L2 with the neutral element e. Similarly, if the condition that x ∥ y for all x ∈ I e and y ∈]0, e] in Theorem 3.8 is not satisfied, then U6 may not be a uninorm on L2 with the neutral element e. The following example will show the above facts.

The lattice L2
The function U5 on L2 given in Fig. 2
The function U6 on L2 given in Fig. 2
In this section, we mainly modify some uninorms, in which some constraints are actually necessary and sufficient.
(1) If x ∥ y for all x ∈ I
e and y ∈ [e, 1 [ and Se (x, y) <1 for all x, y < 1, then
(2) If x ∥ y for all x ∈ Ie and y ∈ [e, 1 [ and I
e
∪]0, e [≠ ∅, then
Necessity. Let
Sufficiency. This proof is the same as Theorem 5 of [7].
(2) Next we just prove that if x ∥ y for all x ∈ I e and y ∈ [e, 1 [ and I e ∪]0, e [≠ ∅, then the condition S e (x, y) <1 for all x, y < 1 is necessary.
Assume that there exist x ∈] e, 1 [ and y ∈] e, 1 [ such that S
e
(x, y) =1. Take z ∈ I
e
∪]0, e [. Then
(1) If x ∥ y for all x ∈ I
e
and y ∈]0, e] and T
e
(x, y) >0 for all x, y > 0, then
(2) If x ∥ y for all x ∈ I
e
and y ∈]0, e] and I
e
∪] e, 1 [≠ ∅, then
(1) It is easy to see that the values of U1 and
(2) The additional constraints of U1 and
According to (1) and (2), by changing the values of
Similarly, the relationship between U2 and
is a uninorm on L with e ∈ L \ {0, 1} iff R (x, y) <1 for all x, y < 1.
Necessity. Let
Sufficiency. This proof is the same as Theorem 3.1 of [7]. □
(1) It is easy to see that the values of U3 and
(2) The additional constraints of U3 and
According to (1) and (2), by changing the values of
Similarly, the relationship between U4 and
Conclusion
In this article, we investigate the constructions of uninorms on some appropriate bounded lattices with e ∈ L \ {0, 1}, based on some additional constraints. In this progress, we mainly focus on the rationality of these constraints and then show that some of these constraints are sufficient and necessary for the construction of uninorms. Meanwhile, we study the constraints of some existing uninorms and find that some constraints are also necessary. In the future research, when considering the new construction of uninorms, if the constraints are needed, we expect they are sufficient and necessary. Moreover, as we can see, the constructions of uninorms on bounded lattices had been investigated widely. Then it may be an interesting work that how to apply uninorms on bounded lattices to L-fuzzy theory, lattice-valued logic and so on.
