Abstract
Uninorms are an important generalization of triangular norms and triangular conorms, having a neutral element lying anywhere in the unit interval. Many different classes of uninorms have been discussed in literature. In this paper, a construction method for a class of left-continuous uninorms is proposed based on the representable uninorm. The idea stems from the rotation method. Some illustrative examples of such uninorms are provided.
Introduction
Uninorms were introduced in 1996 by Yager and Rybalov [28] and generalize the notions of both triangular norms and triangular conorms [2, 19] by allowing the neutral element to lie anywhere in the unit interval rather than at one or zero as in the case of triangular norms (t-norms for short) and triangular conorms (t-conorms for short). The first deep study by Fodor et al. [13] revealed the structure of uninorms. Later on it was shown that uninorms are useful in many fields like expert systems [6, 29], fuzzy decision making [30], fuzzy integrals [20] and fuzzy morphology [3]. On the other hand, the theoretical study of uninorms has been even more extensive. Many different classes of uninorms [24] have been discussed in the literature, including
Preliminaries
It is assumed that the reader is familiar with the theory of t-norms, t-conorms and fuzzy negations (see for instance [2, 19]). We recall here only some basic facts and necessary notations on uninorms which will be used in this paper.
A negation N on [0, 1] is a decreasing unary function on [0, 1] satisfying N (0) =1, N (1) =0. A negation is called strong if it is involutive, i.e. if N (N (x)) = x for any x ∈ [0, 1].
A uninorm is a commutative, associative, increasing function U : [0, 1] 2 → [0, 1] such that U (e, x) = x for all x ∈ [0, 1], where e ∈ [0, 1] is called the neutral element. Note that uninorm can be defined on any interval I ⊆ [0,1] by an isomorphic transformation from I to [0, 1].
We summarize some fundamental results from [13]. It is clear that uninorm U becomes a t-norm when e = 1 and a t-conorm when e = 0. For any uninorm we have U (0, 1) ∈ {0, 1}. A uninorm U such that U (0, 1) =0 is called conjunctive and if U (0, 1) =1 then it is called disjunctive.
Throughout this paper, we exclusively consider uninorms with a neutral element e ∈]0, 1 [.
With any uninorm U with neutral element e ∈]0, 1 [, we can associate two binary operations T
U
, S
U
: [0, 1] 2 → [0, 1] defined by
It is easy to see that T
U
is a t-norm and that S
U
is a t-conorm. In other words, on [0, e] 2 any uninorm U is determined by a t-norm T
U
, and on [e, 1] 2 any uninorm U is determined by a t-conorm S
U
; T
U
is called the underlying t-norm, and S
U
is called the underlying t-conorm. Let us denote the remaining part of the unit square by A (e), i.e.,
On the set
The residual implication I
U
[5] corresponding to conjunctive, left-continuous U is the binary function on [0, 1] defined by
Note that the residual implication corresponding to left-continuous t-norm can be defined similarly. For any x, y, z ∈ [0, 1] the following equivalence (called residuation property) holds:
Some class of left-continuous uninorms and the corresponding residual implications have been characterized in [1]. Their applications in fuzzy logic, fuzzy control were discussed in [27].
It is well known that there exist many construction methods of left-continuous t-norms which are summarized in [17], for example, rotation construction, rotation-annihilation construction and so on. In [16], Jenei and De Baets generalized these methods to construct the left-continuous uninorms. First, we recall the main results in [16] about the rotation of uninorms.
Note that the uninorm M constructed in Theorem 1 satisfies the rotation invariance property with respect to the strong negation N, i.e., for any x, y, z ∈ [0, 1],
Some illustrated examples about the uninorm M were presented in [16] (see Example 3 and Example 4 in [16]).
In this section, we will focus on the condition (C1) in Theorem 1.
If the left-continuous underlying t-norm T U of uninorm U satisfies condition (C1) in Theorem 1, then T U (x, y) >0 for all (x, y) ∈]0, 1] 2. It is obvious that the representable uninorm U satisfies condition (C1). The first result of this type is due to Klement et al. [18] (compare also the paper of Dombi [10]). Moreover, in papers [5, 14], many properties of the representable uninorm were also discussed. In the following proposition, some related results used in this section are presented.
(i) There exists a strictly increasing continuous function h : [0, 1] → [- ∞, + ∞] with h (0) = -∞, h (e) =0, h (1) = + ∞ such that, for all x, y ∈ [0, 1] 2 \ {(0, 1), (1, 0)},
(ii) U (x, 1) = U (1, x) =1 for all x ∈]0, 1].
(iii) U (x, y) = U (y, x) >0 for all (x, y) ∈]0, 1] 2.
(iv) U is strictly increasing and continuous on ] 0, 1 [2;
(v) The underlying operators T U , S U of U are strict, i.e. continuous and strictly increasing in the region ] 0, 1] 2;
(vi) There exists an strong negation with fixpoint e,i.e. N (e) = e, such that
Note that the statement (v) in Proposition 1 is from Theorem 5 in [14] (compare also Theorem 2 in [18]), the other statements are from Theorem 3 in [13] and Proposition 6 in [5], moreover, the statement about the residual implication is from Theorem 7 in [5]. By Proposition 1, it is known that for fixed x0 ∈ [0, t [, N (I
U
1
(y, N (x0))) in Theorem 1 is a strictly increasing function about y ∈] t, 1] and for fixed y0 ∈] t, 1], N (I
U
1
(y0, N (x))) in Theorem 1 is a strictly increasing function about x ∈ [0, t]. A problem emerges: Can these strictly increasing functions be replaced with arbitrary functions? So, we want to offer a construction method of left-continuous uninorm based on the representable uninorm, i.e. our aim is to construct a conjunctive left-continuous uninorm such that
Standing assumption: throughout this section, notation U will denote the conjunctive left-continuous uninorm with form (3) when no explicit statement is mentioned.
For arbitrary x ∈]0, t [, we denote by U x : [t, 1] → [0, 1] the partial function U x (y) = U (x, y). For arbitrary y ∈] t, 1], we denote by U y : [0, t] → [0, t] the partial function U y (x) = U (x, y).
First, we discuss some properties about the partial function U y : [0, t] → [0, t]. Let us denote the range of U y by Ran (U y ).
So,
Now, we prove that U (x1, y0) ∈ [0, t]. On the contrary, suppose that U (x1, y0) > t. Then by Proposition 1 and the associativity of uninorm U,
So, by the associativity of U, we have
By Proposition 4, we know that the partial function U y : [0, t] → [0, t] is strict increasing.
By the associativity of U, we have U (x0, y1) = x0. By the monotonicity of U, U (x0, y) = x0 for the interval I = [min(y0, y1), max(y0, y1)].
If U (x0, 1) = x0, then for arbitrary positive number ɛ ∈]0, 1 - t],
By the associativity of U, we have U (x0, t + ɛ) = x0. So, by the monotonicity of U, U (x0, y) = x0 for all y ∈] t, 1].□
From Proposition 6, we know that the uninorm U (x, y) = min(x, y), (x, y) ∈]0, t [×] t, 1 [ whenever U (x, 1) = min(x, 1) for all x ∈]0, t [.
Now, one result of Clifford [7] is introduced in the following theorem.
Then G = (X, ∗) is a semigroup. The semigroup G is commutative if and only if for each α ∈ A the semigroup G α is commutative.
It is a representable uninorm with neutral element
It is obvious that U is a left-continuous uninorm with neutral element
For arbitrary x ∈]0, t [, we discuss the partial function U x : [t, 1] → [0, 1].
Since U (y1, y) ≥ t, U x 2 (y) = U x 1 (U (y1, y)).□
(i) If e > y for arbitrary y ∈ I, then I ⊆]0, e [. Assume that U
x
1
(y) = c < x1 for all y ∈ I. Since x2 ∈ Ran (U
x
1
), x2 ≤ x1, there exists y1 ∈] t, e] such that U (x1, y1) = x2. Hence, for arbitrary y ∈ I,
So, the result holds.
(ii) and (iii) The proof is similar to (i).□
Without loss of generality, suppose that x ≤ y ≤ z. Only several cases need to be considered.
and
(iii) The other cases. Then
The left-continuity of U can be obtained by the continuity of f, h, h-1 and Proposition 1.□
(ii) By taking the underlying t-norm T U of uninorm U in Theorem 4, this procedure results in a class of left-continuous t-norms which are different from those of Theorem 5 in [8].
It is a representable uninorm with neutral element
It is obvious that U
r
is a representable uninorm defined on
Then, we can construct the left-continuous uninorm
The result of Theorem 4 can be generalized.
(ii) By taking the underlying t-norm T U of uninorm U in Theorem 5, this procedure results in another class of left-continuous t-norms which are different from those of Theorem 5 in [8].
Then, we can construct the left-continuous uninorm
At last of this section, we focus on the (generalized) Modus Ponens which comes from approximate reasoning. In fuzzy rules based systems, any fuzzy conditional: p → q is often represented by a residual implication. If the residual implications are used in inference processes, where a concrete conjunction (usually a left-continuous t-norm) is selected, then it is essential that such residual implications satisfy the Modus Ponens with respect to the selected t-norm.
Let I
U
be an residual implication from the conjunctive left-continuous uninorm U and T a t-norm. It is said that I
U
satisfies the Modus Ponens property with respect to T or that I
U
is a T-conditional if
A well known general result on T-conditionality was proved in [25].
Consider the conjunctive representable uninorm U r defined on [t, 1] 2 with neutral element e ∈] t, 1 [ and the additive generator h : [t, 1] → [- ∞, + ∞]. Let denote the corresponding uninorms in Theorem 3 by U3.
So,
Hence, by the monotonicity of T and T (x, y) ≤ min(x, y), t-norm T must satisfy the following conditions:
By Proposition 10, the result holds.□
(ii) Consider the t-norm T defined by
By Theorem 5 in [8], T is left-continuous t-norm. T satisfies the condition in Proposition 10. Hence, I U 3 is a T-conditional.
In this paper, one construction method of left-continuous uninorm has been proposed based on the representable uninorm. The full characterization of residual implications corresponding to them is our future work.
Footnotes
Acknowledgements
The authors were supported by the National Natural Science Foundation of China (Grant No. 61403220, 61573211).
