# Note on the Choquet Integral as an Interval-Valued Aggregation Operators and Their Applications

Authors: Lee-Chae Jang
Journal: Journal of Applied Mathematics
 (2012)

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## Abstract

The concept of an interval-valued capacity is motivated by the goal to generalize a capacity, and it can be used for representing an uncertain capacity. In this paper, we define the discrete interval-valued capacities, a measure of the entropy of a discrete interval-valued capacity, and, Choquet integral with respect to a discrete interval-valued capacity. In particular, we discuss the Choquet integral as an interval-valued aggregation operator and discuss an application of them.


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## Body

## 1. Introduction

Let(X,Ω) be a measurable space. A capacity (or a fuzzy measure) on X is a nonnegative monotone set function μ:Ω→ℝ¯+=[0,∞] with μ(∅)=0. Many researchers have been studying a discrete capacity in many topics such as capacity functionals of random sets (see [1–5]) and entropy-like measures (see [6–9]).The Choquet integral with respect to a capacity of a nonnegative measurable functionf is given by(1.1)Cμ(f)=(C)∫fdμ=∫0∞μf(α)dα,
where μf(α)=μ({x∈X∣f(x)>α}) and the integral on the right-hand side is an ordinary one. If we take N={1,2,…,n} and f:N→ℝ+ by f(i)=xi for all i∈N, then we have(1.2)Cμ(f)=∑i=1nxπ(i)[μ(Aπ(i))-μ(Aπ(i+1))],
where π is a permutation on {1,2,…,n} such that xπ(1)≤xπ(2)≤⋯≤xπ(n) and Aπ(i)={π(i),…,π(n)} and Aπ(n+1)=∅(see [1–4, 6, 9, 10]). Note that if we put xπ(0)=0 and Aπ(n+1)=∅, then we obtain the following formula:(1.3)Cμ(f)=∑i=0n-1(xπ(i+1)-xπ(i))μ(Aπ(i+1)).By using interval-valued functions to express uncertain functions, we have studied the Choquet integral with respect to a capacity of an interval-valued function which is able to better handle the representation of decision making and information theory (see [10–16]). During the last decade, it has been suggested to use intervals in order to represent uncertainty in the area of decision theory and information theory, for example, calculation of economic uncertainty [8], theory of interval probability as a unifying concept for uncertainty [17], and the Choquet integral of uncertain functions [3, 12–16, 18]. Recently, Xu et al. [19–24] have been studying the application of the Choquet integral with uncertain and fuzzy information.The main idea of this paper is to use the concept of an interval-valued capacity in the entropy-like measure which is an aggregation defined by the discrete interval-valued capacities. In Section2, we introduce the Choquet integral with respect to an interval-valued capacity and discuss some of its properties. In Section 3, we investigate the interval-valued weighted arithmetic mean, the interval-valued Shannon entropy, the interval-valued weighted averaging operator, and an interval-valued measure of the entropy of an interval-valued capacity. In Section 4, we give the problem of evaluating students as an example where interval-valued weights and some suitable interval-valued capacity are used in practical situation. In Section 5, we give a brief summary results and some conclusions.


## 2. The Choquet Integral with Respect to a Discrete  Interval-Valued Capacity

Throughout this paper,I(ℝ+) is the set of all closed intervals in ℝ+=[0,∞), that is, (2.1)I(R+)={[a1,a2]∣a1,a2∈R+,a1≤a2}.
For any a∈ℝ+, we define a=[a,a]. Obviously, a∈I(ℝ+)(see [13–15]).Definition 2.1.
Ifa¯=[a1,a2],b¯=[b1,b2]∈I(ℝ+), and k∈ℝ+, then one defines arithmetic, minimum, order, and inclusion operations as follows:(1)
a¯+b¯=[a1+b1,a2+b2],(2)
ka¯=[ka1,ka2],(3)
a¯b¯=[a1b1,a2b2],(4)
a¯∧b¯=[a1∧b1,a2∧b2],(5)
a¯∨b¯=[a1∨b1,a2∨b2],(6)
a¯≤b¯ if and only if a1≤b1 and a2≤b2,(7)
a¯<b¯ if and only if a¯≤b¯ and a¯≠b¯,(8)
a¯⊂b¯ if and only if b1≤a1 and a2≤b2.LetU be a countably infinite set as the universe of discourse and 𝒫(U) the power set of U. We propose an interval-valued capacity and discuss some of its properties.Definition 2.2.
(1) An interval-valued set functionμ¯=[μl,μr]:𝒫(U)→I(ℝ¯+) is said to be a discrete interval-valued capacity on U if it satisfies the following conditions:(i)
μ¯(∅)=0¯,(ii)
μ¯(S)≤μ¯(T), whenever S,T∈𝒫(U) and S⊂T.
(2) A setD(∈𝒫(U)) is said to be a carrier (or support) of an interval-valued capacity μ¯ if μ¯(S)=μ¯(D∩S) for all S∈𝒫(U).
(3) An interval-valued capacityμ¯ with nonempty finite carrier D(∈𝒫(U)) is said to be normalized if μ¯(D)=1¯.For any integerk≥1, the set {1,…,k} will simply be denoted by [k] and I([0,1])={[a1,a2]∣a1,a2∈[0,1]anda1≤a2}. For the sake of convenience, we will henceforth assume that D=N is the n-element set [n]. We denote by IVC the set of interval-valued capacities with a nonempty finite carrier on U and by IVCN the set of normalized interval-valued capacities having N⊂U as a nonempty finite carrier.Definition 2.3.
(1) An interval-valued capacityμ¯∈IVCN is said to be additive if μ¯(S∪T)=μ¯(S)+μ¯(T) for all disjoint subsets S,T⊂N.
(2)μ¯∈IVCN is said to be cardinality based if for all T⊂N, μ¯(T) depends only on the cardinality of T; that is, there exists μ¯0,μ¯1,…,μ¯n∈I([0,1]) such that μ¯(T)=μ¯t=[μlt,μrt] for all T⊂N such that |T|=t, where |T| is the cardinality of T.In [6, p. 135], there is only one normalized capacity μN* with a nonempty finite carrier N which is both additive and cardinality based, and in this case, μN* is given by μN*(T)=t/n for all T⊂N such that |T|=t. Thus we can obtain the following theorem.Theorem 2.4.
Ifμ¯∈IVCN is both additive and cardinality based, then μ¯(T)=[t/n,t/n], for all T⊂N with |T|=t.Theorem2.4 implies that if a discrete interval-valued normalized capacity μ¯ is both additive and cardinality based, then it is a discrete real-valued capacity (or a real-valued monotone set function). By Definition 2.3, we can easily obtain the following theorem.Theorem 2.5.
(1) An interval-valued set functionμ¯=[μl,μr] is a discrete interval-valued capacity if and only if μl and μr are discrete capacities.(2)
A setN(⊂U) is a carrier of μ¯=[μl,μr] if and only if N is a carrier of both μl and μr.(3)
μ¯=[μl,μr] is normalized if and only if μl and μr are normalized.(4)
μ¯=[μl,μr] is additive if and only if μl and μr are additive.(5)
μ¯=[μl,μr] is cardinality based if and only if μl and μr are cardinality based.By using formula (1.3) of the Choquet integral and a discrete interval-valued capacity with a nonempty finite carrier N, we will define the Choquet integral with respect to a discrete interval-valued capacity.Definition 2.6.
Letx:N→ℝ+ be a function such that x(i)=xi for all i∈N and μ¯ a discrete interval-valued capacity with a nonempty finite carrier N. The Choquet integral with respect to μ¯ of x is defined by
(2.2)Cμ¯(f)=∑i=0n-1(xπ(i+1)-xπ(i))μ¯(Aπ(i+1)),
where π is a permutation on N such that xπ(0)=0≤xπ(1)≤xπ(2)≤⋯≤xπ(n) and Aπ(i)={π(i),…,π(n)} and Aπ(n+1)=∅.By (2.2), we can easily obtain the following basic property of 𝒞μ¯.Theorem 2.7.
Ifμ¯∈IVCN, then one has
(2.3)Cμ¯(x)=[Cμl(x),Cμr(x)],
where a function x:N→ℝ+ by x(i)=xi for all i∈N.From the right-hand side of (2.2), we note that (2.4)∑i=0n(xπ(i+1)-xπ(i))μ¯(Aπ(i+1))≠∑i=1nxπ(i)(μ¯(Aπ(i+1))-μ¯(Aπ(i))),
in general. Because of this note, we consider a new difference operation ⊖ defined by(2.5)[a,b]⊖[c,d]={[a-c,b-d]if0≤a-c≤b-d,0¯ifotherwise,
where a,b,c,d∈ℝ+. From this difference operation, we can easily see that [ka,kb]⊖[kc,kd]=k([a,b]⊖[c,d]) for all k,a,b,c,d∈ℝ+. We denote byIVCN1(x) the set of normalized interval-valued capacities μ¯=[μl,μr] with a nonempty finite carrier N satisfying the following condition: (2.6)μl(Aπ(i))-μl(Aπ(i+1))≤μr(Aπ(i))-μr(Aπ(i+1)),
for all i∈N and where π is a permutation on {1,2,…,n} such that xπ(1)≤xπ(2)≤⋯≤xπ(n) and Aπ(i)={π(i),…,π(n)} and Aπ(n+1)=∅. We remark that IVCN1(x)⊂IVCN and that if μ¯∈IVCN1(x), then we have(2.7)μ¯(Aπ(i))⊖μ¯(Aπ(i+1))=[μl(Aπ(i))-μl(Aπ(i+1)),μr(Aπ(i))-μr(Aπ(i+1))].
By Theorem 2.7 and (1.2), (2.5), and (2.7), we derive the following theorem.Theorem 2.8.
If there exists functionx:N→ℝ+ by x(i)=xi for all i∈N and μ¯∈IVCN1(x), then one has
(2.8)Cμ¯(x)=∑i=1nxπ(i)(μ¯(Aπ(i))⊖μ¯(Aπ(i+1))),
where π is a permutation on N such that xπ(1)≤xπ(2)≤⋯≤xπ(n) and Aπ(i)={π(i),…,π(n)} and Aπ(n+1)=∅.Proof.
By Theorem2.7 and the definition (1.2) and the difference (2.5) operation, we have
(2.9)Cμ¯(x)=[Cμl(x),Cμr(x)]=[∑i=1nxπ(i)(μl(Aπ(i))-μl(Aπ(i+1))),∑i=1nxπ(i)(μr(Aπ(i))-μr(Aπ(i+1)))]=∑i=1nxπ(i)[μl(Aπ(i))-μl(Aπ(i+1)),μr(Aπ(i))-μr(Aπ(i+1))]=∑i=1nxπ(i)[μl(Aπ(i)),μr(Aπ(i))]⊖[μl(Aπ(i+1)),μr(Aπ(i+1))]=∑i=1nxπ(i)(μ¯(Aπ(i))⊖μ¯(Aπ(i+1))).


## 3. The Choquet Integral as an Interval-Valued Aggregation Operator

In this section, we define the interval-valued weighted arithmetic mean (IWAM), which is the concept of a generalized aggregation (or an uncertain aggregation), as follows:(3.1)IWAMw¯(x)=∑i=1nw¯ixi,
where w¯i=[wli,wri], 0≤wli≤wri≤1 for all i∈N, ∑i=1nwli≤∑i=1nwri=1, and x:N→ℝ+ by x(i)=xi for all i∈N is a function such that x1,…,xn represent the arguments. We denote by x=(x1,…,xn) an n-dimensional vector in (ℝ+)n.Note that the argumentsx1,…,xn that are used in such an interval-valued aggregation process strongly depend upon the interval-valued (or uncertain) weight vector w¯=(w¯1,…,w¯n)∈(I([0,1]))n. Then the interval-valued Shannon-entropy H¯S of w¯ defined on N is given by(3.2)H¯S(w¯)=∑i=1nh¯(w¯i),
where h¯(w¯i)=[h(wli),h(wri)] for 0≤wli≤wri≤1 for all i∈N, and(3.3)h(w)={-wln⁡wif0<w≤1,0¯ifw=0,
for all w∈[0,1]. Then it means a measure of dispersion associated to the interval-valued weight vector of the interval-valued weighted arithmetic mean IWAMw¯. We also easily see that(3.4)H¯S(w¯)=[HS(wl),HS(wr)],
where w¯=[wl,wr].Now, we define the following interval-valued (or uncertain) ordered weight averaging (IOWA) operator.Definition 3.1.
Letw¯=(w¯1,…,w¯n)∈(I([0,1]))n be an interval-valued weight vector such that w¯i=[wli,wri], 0≤wli≤wri≤1 for all i∈N, and ∑i=1nwli≤∑i=1nwri=1. The interval-valued ordered weighted averaging (IOWA) operator on (ℝ+)n is defined by
(3.5)IOWAw¯(x)=∑i=1nw¯ixπ(i),
where x=(x1,…,xn)∈(ℝ+)n and π is a permutation on N such that 0≤xπ(1)≤xπ(2)≤⋯≤xπ(n).From Definition3.1, we have(3.6)IOWAw¯(x)=[∑i=1nwlixπ(i),∑i=1nwrixπ(i)].
By (3.5) and (3.6), we obtain that if s∈{l,r} and we write ws=(ws1,…,wsn), then OWAws is an ordered weighted averaging operator associated to a weight vector ws, proposed by Yager [18]. Remark that if wli=wri=wi for all i∈N and we write w=(w1,…,wn), then IWAMw¯(x)=∑i=1nwixi is the weight arithmetic mean (WAM), H¯S(w¯)=∑i=1nh(wi) is the Shannon entropy of w, and IOWAw¯(x)=∑i=1nwixπ(i) is the ordered weighted averaging (OWA) operator (see [3, 5]).Theorem 3.2.
(1) If one takeswl=wr=(1/n,…,1/n), then H¯S(w¯)=ln¯n is maximum.
(2) If one takeswli=1 and wrj=1 for some i,j∈N, then H¯(w¯)=0¯ is minimum.Proof.
(1)H¯S(w¯)=[∑i=1n(-wl1lnwli),∑i=1n(-wrilnwri)]=[lnn,lnn]=ln¯n.
(2)H¯S(w¯)=[∑k=1nh(wlk),∑k=1nh(wrk)]=[h(wli),h(wrj)]=[0,0]=0¯.From Theorem3.2, the interval-valued measure of dispersion can be normalized into(3.7)1ln⁡nH¯S(w¯)=1ln⁡n∑i=1nh¯(w¯i),
so that it ranges in I([0,1]). Finally, we will define the interval-valued entropy of an interval-valued capacity which is the generalization of the entropy proposed by Marichal [3] as follows:(3.8)HM(μ)=∑i∈N∑T⊂N∖{i}pth(μ(T∪{i})-μ(T)),
where μ is a capacity on N, |T|=t is the cardinality of T, the coefficients pt(|T|=t) are nonnegative, and ∑T⊂N∖{i}pt=1.Definition 3.3.
The interval-valued entropy of an interval-valued capacityμ¯ is defined by
(3.9)H¯M(μ¯)=∑i∈N∑T⊂N∖{i}pth¯(μ¯(T∪{i})⊖μ¯(T)),
where ⊖ is the same operation in (2.5), the coefficients pt(|T|=t) are nonnegative, ∑T⊂N∖{i}pt=1, and h¯ is the same function in (3.3).From Definition3.3, if we take μl=μr=μ, then H¯M(μ¯)=HM(μ). We consider the following assumption of μ¯=[μl,μr]:(3.10)∑T⊂N∖{i}pth(μl(T∪{i})-μl(T))≤∑T⊂N∖{i}pth(μr(T∪{i})-μr(T)),∀i∈N,
and let IVCN2={μ¯∈IVCN∣μ¯satisfyassumption(3.10)}.Theorem 3.4.
Ifμ¯=[μl,μr]∈IVCN2, then one has
(3.11)H¯M(μ¯)=[HM(μl),HM(μr)].Proof.
By Definition3.3, we can directly calculate H¯M(μ¯) as follows:
(3.12)H¯M(μ¯)=∑i∈N∑T⊂N∖{i}pth¯(μ¯(T∪{i})⊖μ¯(T))=∑i∈N∑T⊂N∖{i}pth¯([μl(T∪{i})-μl(T),μr(T∪{i})-μr(T)])=∑i∈N∑T⊂N∖{i}pt[h(μl(T∪{i})-μl(T)),h(μr(T∪{i})-μr(T))]=[∑i∈N∑T⊂N∖{i}pth(μl(T∪{i})-μl(T)),∑i∈N∑T⊂N∖{i}pth(μr(T∪{i})-μr(T))]=[HM(μl),HM(μr)].From Theorem3.4, we can see that if we take μ¯=[μl,μr]∈IVCN such that HM(μr)<HM(μl), then H¯M(μ¯) is not defined. Thus, the Assumption (3.10) of μ¯ is a sufficient condition for defining the interval-valued entropy H¯M(μ¯) of an interval-valued capacity μ¯. We also suggest that that H¯M(μ¯) is interpreted as an interval-valued measure of dispersion for 𝒞μ¯ a sum over i∈N of an average value of h¯(μ¯(T∪{i})⊖μ¯(T))(T⊂N∖{i}) as follows: for all i∈N,(3.13)(μ¯(Aπ(i))⊖μ¯(Aπ(i+1)))=∑T⊂N∖{i}pth¯(μ¯(T∪{i})⊖μ¯(T)).Theorem 3.5.
Ifx=(x1,…,xn) and μ¯∈IVCN1(x), then μ¯∈IVCN2.Proof.
Letx=(x1,…,xn)∈(ℝ+)n and π be a permutation on N such that 0≤xπ(1)≤xπ(2)≤⋯≤xπ(n). Since μ¯∈IVCN1(x), we get μl(Aπ(i))-μl(Aπ(i+1))≤μr(Aπ(i))-μr(Aπ(i+1)) for all i∈N. Thus, by (3.13),
(3.14)∑T⊂N∖{i}pth(μl(T∪{i})-μl(T))=μl(Aπ(i))-μl(Aπ(i+1))≤μr(Aπ(i))-μr(Aπ(i+1))=∑T⊂N∖{i}pth(μr(T∪{i})-μr(T)).
This implies HM(μl)≤HM(μr). Therefore μ¯∈IVCN2.Theorem 3.6.
Ifx=(x1,…,xn), μ¯∈IVCN1(x), and 𝒞μ¯=IOWAw¯, then one has H¯M(μ¯)=H¯S(w¯), that is,
(3.15)H¯M(μ¯)=∑i=1nh¯(μ¯(Aπ(i))⊖μ¯(Aπ(i+1))),
where ⊖ is the same operation in (2.3), h¯ is the same function in (2.8), and x=(x1,…,xn)∈(ℝ+)n, and π is a permutation on N such that 0≤xπ(1)≤xπ(2)≤⋯≤xπ(n)Proof.
Since𝒞μ¯=IOWAw¯, w¯i=μ¯(Aπ(i))⊖μ¯(Aπ(i+1)). By (3.13), we get
(3.16)H¯M(μ¯)=∑i∈N∑T⊂N∖{i}pth¯(μ¯(T∪{i})⊖μ¯(T))=∑i=1nh¯(μ¯(Aπ(i))⊖μ¯(Aπ(i+1)))=∑i=1nh¯(w¯)=H¯S(w¯).


## 4. Applications

In this section, we consider the problem of evaluating students in a high school with respect to three subjects: mathematics (M), physics (P), and literature (L), proposed by Marichal [3]. Suppose that the school is more scientifically than literary from somewhat oriented to extremely oriented, so that interval-valued weights could be, for example, w¯M=[1/4,1/2], w¯P=[1/4,3/8], and w¯L=[1/8,1/8], respectively. We note that w¯=(w¯M,w¯P,w¯L) and IWAMw¯(x)=[WAMwl(x),WAMwr(x)] for all x∈{a,b,c}.If we takew¯=[wl,wr], then wl=(1/4,1/4,1/8) and wr=(1/2,3/8,1/8). Then the interval-valued weighted arithmetic mean will give the results for three students a,b, and c (marks are given on a scale from 0 to 20) (see Table 1).Table 1StudentMathematics (M)Physics (P)Literature (L)IWAMw¯a181610[9.75, 16.25]b101218[7.75, 11.75]c141515[9.13, 14.50]We note thatIWAMw¯(a)>IWAMw¯(c)>IWAMw¯(b). The total interval-valued weight is from rather well distributed to quite well distributed over three subjects since we have (4.1)1ln⁡nH¯S(w¯)=[0.868,0.887].We consider theα-mean evaluation Eα of IWAMw¯l as follows:(4.2)Eα(x)=αWAMwl(x)+(1-α)WAMwr(x)
for all α∈[0,1] and x∈{a,b,c}. The α-mean evaluation Eα implies that we can interpret the difference of the degree of favor for students. Indeed, if α=0, that is, if the school is more scientifically than literary extremely oriented, then the school wants to favor more student c as E0(a)-E0(c)=1.75; if α=1, that is, if the school is more scientifically than literary somewhat oriented, then the school wants to favor more student c as E1(a)-E1(c)=0.575.Now, if the school wants to favor somewhat well-equilibrated over extremely well equilibrated students without weak points, then studentc should be considered better than student a, who has a severe weakness in literature. Unfortunately, no interval-valued vector (w¯M,w¯P,w¯L) satisfying w¯M>w¯P>w¯L is able to favor student c. Indeed, it is possible that (4.3)IWAMw¯(14,15,15)>IWAMw¯(18,16,10)⟺w¯L>w¯M.The reason of this problem is that much importance is given to mathematics and physics, which present some overlap effect since, usually, students from little good to rather good at mathematics are also from little good to rather good at physics (and vice versa), so that the interval-valued evaluation is overestimated (resp., underestimated) for students from little good to rather good (resp., from little bad to rather bad) at mathematics and/or physics.This problem can be overcome by using a suitable interval-valued capacityμ¯ and the Choquet integral 𝒞μ¯ as follows.(i) Since scientific subjects are more important than literature, the following interval-valued weights can be put on subjects taken individually:μ¯({M})=[0.25,0.5], μ¯({P})=[0.25,0.375] and μ¯({L})=[0.125,0.125]. Note that the initial interval-valued ratio of interval-valued weight ([2,4],[2,3],[1,1]) is kept unchanged.(ii) Since mathematics and physics overlap, the interval-valued weight attributed to the pair{M,P} should be less than the sum of the interval-valued weight of mathematics and physics: μ¯({M,P})=[0.3,0.6].(iii) Since students equally good at scientific subjects and literature must be favored, the interval-valued weight attributed to the pair{L,M} should be greater than the sum of individual interval-valued weights (the same for physics and literature): μ¯({M,L})=[0.45,0.75]=μ¯({P,L}).(iv)μ¯(∅)=0¯ and μ¯({M,P,L})=[0.55,1].If we takeμ¯=[μl,μr], and μl({L,P,M})=0.55, μr({L,P,M})=1, μl({P,M})=0.3, μr({P,M})=0.6, μl({M,L})=0.45, μr({M,L})=0.75, μl({P,L})=0.45, μr({P,L})=0.75, μl({P})=0.25, μr({P})=0.375, μl({M})=0.25, μr({M})=0.5, μl({L})=0.125, and μr({L})=0.125, then HM(μl)=0.8802<0.9974=HM(μr) and hence μ¯∈IVCN2.Applying the Choquet integral with respect to the above interval-valued capacity leads to the Choquet integrals see Table2.Table 2StudentMathematics (M)Physics (P)Literature (L)𝒞μ¯(student)a181610[7.80, 14.60]b101218[6.85, 12.25]c141515[8.15, 14.75]SinceIWAMw¯(a)>IWAMw¯(c)>IWAMw¯(b) and 𝒞μ¯(c)>𝒞μ¯(a)>𝒞μ¯(b), we can see that if we use IWAMw¯, then student a has the best rank, but if we use 𝒞μ¯, then student c has the best rank. We also consider the α-mean Choquet evaluation Eαc of 𝒞μ¯ as follows:(4.4)Eαc(x)=αCμl(x)+(1-α)Cμr(x)
for all α∈[0,1] and x∈{a,b,c}.Theα-mean Choquet evaluation Eαc implies that we can interpret the difference of the degree of favor for student a and student c. Indeed, if α=1, that is, if the school wants to favor extremely well-equilibrated students, then the school wants to favor student c than student a as E1c(c)-E1c(a)=0.35; if α=0, that is, if the school wants to favor somewhat more well-equilibrated students, then the school wants to favor student c more than student a as E0c(c)-E0c(a)=0.15.Finally, we have the normalized entropy of interval-valued capacity inIVCN2 as follows: (4.5)1ln⁡nH¯M(μ¯)=[1ln⁡nHM(μl),1ln⁡nHM(μr)],HM(μl)=∑T⊂N∖{P}(3-t-1)!t!3!h(μl(T∪{P})-μl(T))+∑T⊂N∖{M}(3-t-1)!t!3!h(μl(T∪{M})-μl(T))+∑T⊂N∖{L}(3-t-1)!t!3!h(μl(T∪{L})-μl(T)),HM(μl)=∑T⊂N∖{P}(3-t-1)!t!3!h(μr(T∪{P})-μr(T))+∑T⊂N∖{M}(3-t-1)!t!3!h(μr(T∪{M})-μr(T))+∑T⊂N∖{L}(3-t-1)!t!3!h(μr(T∪{L})-μr(T)),
where N={P,M,L}. Thus, we have (4.6)1ln⁡nH¯M(μ¯)=[0.8012,0.9079],
which shows that the total interval-valued weight is from still rather well distributed to very quite well distributed.


## 5. Conclusions

In this paper we consider the new interval-valued measure of the entropy of an interval-valued capacity which generalizes a measure of the entropy proposed by Marichal's [3]. From (3.1), (3.5), and (3.9) and Theorems 3.4, 3.5, 3.6, we investigate the interval-valued weighted arithmetic mean and interval-valued ordered weighted averaging operator for representing uncertain weight vectors which are used in the concept of an uncertain aggregations.From an example in Section4, it is possible that we use from somewhat oriented to extremely oriented instead of oriented, from rather well distributed to quite well distributed instead of well distributed, and from somewhat well equilibrated to extremely well equilibrated instead of well equilibrated in the problem of evaluating students.In the future, by using these results of this paper, we can develop various problems and models for representing uncertain weights related to interacting criteria.



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