Copyright © IFAC Fuzzy Infonnation MalYille, France, 1983
ON THE FUZZY MEASURES AND THE MEASURES OF FUZZINESS FOR L-FUZZY SETS Zi-Xiao Wang Department of Mathematics, Northeast Normal University, Changchun, jilin, People's Republic of China
Abstract.
This paper is based
o~
the results of De Luca and Termini(1.2)
and Wang (6,7.8) . It includes the following three parts. (1) We extend the
fuzz~'
integrals taking value in the unit inteval (0, 1) to a fuzzy
integrals taking value in a lattice. When the lattice is total order. it is given that one group equivalent conditions such that the L-fuzzy measure can be represented as a L-fuzzy integral. (2) We extend the measure of
fu~ziness
for general fuzzy sets to the measure of fuzziness
for L-fuzzy sets , where L is a complement lattice. (3)
We investigate
the L-ruzzy inteeral representation for the measure of fuzziness on the L-fuzzy sets. Keywords
1
L-Fuzzy Measure
L-Fuzzy Integrals
L-Measure of Fuzziness.
TNTHOlJUCT10N
In 1968, Zadeh (11) first suggested the fuzzy
probability. In 1?72. De Luca :>.nd Termini
probability on fuzzy events and peoneared G.c\v e three princirles as a measure of fuzzi ·
the consideration of fuzzy measu re. Klement
ne~s.
et a1. (4) Harked important 1'e3u1 t ~; at this
This paper has itself generated a
direction. 'f heir work's characteristic is
number of papers in this arAa
that their tool i s the classical Lebesgqe
sugg ested an intuitive definition of the
integral. In 1974, Sugeno (5) suggested a
fuzzille"'" anci Yagor (10) and Dc Luc:>. a1,d
complete theory of fuzzy integral which is
Terlliini (2) investigated the measure o~
indepenJent of Lebesgue meas ure and integral.
These authors cOLsidor
L-fuzzy sets on the universal space is a
dation of Lebesgue i ntegral. Therefore, in
lattice. Thus their rather conSider the
(6. 7 ). we supplemented the fuzzy addi tivi ty r.
on lattice
the fuzziness of a la ttice because of the
Generally, Sugeno's fuzzy integral is exten-
for the fuzzy
~uzzine~~
YBEAr (g)
fuzziness of a lattice with the betweenness
easure such tha t the measure
of elements of a lattice than investigate
].s really a ex tenda tion of a " similarity" At the samel tillJe, vie g8-ve a new definition
the fuzziness on L-fuzzy sets.
which is eCiuivahnn wl ti; Sugeno' s fuzzy
In this paper, first of all. we conSider
integral ano. is !JlOre c:Ol.vellie,1t. This is
the fuzzy integral taking value in a lattice
anathel' deriction on the investigation of
~nd
fuzz; measure, it is more intuitive than
we investigate immed1atly the fuzziness of
the first deriction on fuzzy measure.
L-fuzzy sets. Here, we require the lattice
By a measure of
L is a metric lattice. At the Same time. an
fUt;.;ll1e~$,
we ,Lean a measur·
.e call it as L-fuzzy integral, Next,
axiomatic definition of the measure (If fuzzi-
men t of the fuzz:i grade for a fuzzy set. J t
ness for L-fuzzy sets is given, Finally, 341
342
Zi-Xiao Wang
we prove an integral representation of the htx)
measure of fuzziness. 2
=V'~l ~-
Coi.~
j\
.p
Ei (\ Ej =
'x. E i (x»)
( i /:. j)
L-FUZZY INTEGRAL then
In (5) . Sugeno first suggested complete theory of fuzzy integral. In (6,7) , we gave a new definition of the fuzzy integral
i E hlx)
dm
V
=
n
1.= 1
(0(1"
m(E.(I ~
El)
is called L-!u.zzy in tegral of h( x) on E ~ Il.
which is equivalent with Sugeno's integral.
(it) hex) is a general function. we take a
Now. we shall consider the fuzzy integral
monotone incroasing sequence of simple
taking value in a lattice.
functions such that hn(x)~h(X) (uniformly)
Throughout this paper . we suppose that L
then
denotes a complete distributive metric lattice with the maximum element I and the minimum element () . The universll l space is a measurable space ( X.$). where $ is ordinary Eorel field on X.
~ --..L.
1E h n( x)
dm
is called L-fuzzy integral of h( x) on E" ~. PropoSition 2.1
The L-fuzzy integral
defined in the Def. 2.2 e quivalent with the ~o is the
Borel field of the unit inteval (0, ))
By a L-fuzzy measure m(.):
Definition 2.1
h( x) dm = lim
fuzzy integral defined by Sugeno,
L-fuzzy measure
I
'1 E
Proof.
Sugeno's fuzz y integral is defined
we mean that m(· ) satisfies the (s)
following conditions
•
~ E h( x) dm = suplo<. /\ m(l>~"E»)
wh.e re Fo< = {x : h( x ) ~ 0( } , 0 '- 01. ~ 1 . If hex) is a simple function, say, (2 ) I f
A.bEt>. then m(AU
.lJ)~.I1(A)V
m(.tJ)
is a monotone sequence. (3) If {A n I.J n9 1c:.f> ;:>
h( x) =Vi:1 (oI. i "
oil n
RE'ma.rk. (i)
=
lirr m(.'" )
~I.).
i.e. t:f' Ac.B.
A () P
1>
~
jB
wnere Fi =
0(2
~
A.FE~
Uk~l
and
(i
1>
f j)
~ o(n .
V i~1
Coli A m( F / ' E)j
Ek · It folluws that dm
=V~:1
(oIi":;:(E () El)
f E h( x ~
rr: 1 A U B) = :Ti( A ) V m( E)
t h,.,n
•..
h( x) dm =
\::;d E hex)
The condit i on (2) is equivalent to
following condition that H
i
1m
If h( x) is a g eneral fur:ctior:, the pro pOSi-
L - fuzz:' integral
11
( s)
th l'"
m( A) ~ m( A) V m( B) = m( B) • ( i ')
Ei () E j =
So that
n
Th,., COTId i t i on (2) i t:! )'lUE'S tl1,.,
::0noi;Ol"icitv of
~
No lest generality, we assume that
then m( lim A )
1 E~x)J
tion is imrr.cdiate re suI t of the monctonici ty In this section . we suppose that D(· ). L ~
(0, MJ is a distance on L
where M is a
firit p pOSitive real number t'1f'olo£,." ami ~
D
"
is the metric is the Borel field on 1-_
of "lueeno' s fuzzy in tesral ·qr.d L-fuzz/ intebra1s. Now l der.ote the set of all measurable fuz zy sets, and define that
~_
function h( x) is called measurable iff
h-1(c)E~ for all CE~ .
for all A E ~
o
PropOSition 2.1
Tt is c] par' t hqt m(. ) is a fuzzy mE'asurc on
If hex) is measurable. then
there exists a sequence {hn(x)}n~ 1
of
simple functions SUCh that lim h (x) = hex) ( unif
Defini tion 2.2
Let (X,1> .m) b" a fuzzy
n.
If L is also total ord'lr lattice, then we have
Theorem?l measure on
Let iii(.) ,b-+L he a I,-fuzzy
E'
then the following statements
are equivalent.
measure space, h(x) a measurable function ( i)
h( x) is a simple function
\ 1)
m(.) is represented as a L-fuzzy
343
On the Fuzzy Measures and the Measures of Fuzziness integral, i.e. there exists a L-fuzzy
intuitive definition of fuzziness, he asso-
measure m(· ): ~-L such that
ciates fuzziness with the lack of distintion
( i i)
A( x»
m( ( 0<. t\
V
between a proposition and its negation. In
for all A E ~
meA) = -) A( x) dm
(f3 /\ B( x) »)
(lOJ , Yager devoloped his concept to L-
=
fuzzy sets.
= (o<.i\m(A(x») V (j3Am(B(x»)
In ('7, 8 ) , we have pointed out th'l.t
for all o(.'{3 ELand A.B E ~ , (iii) and A e( i v)
ilrto<.AA(x»
=oI.i\m(A\x)
forallotEL
t>, For all 0<. , a ELand A E; D( m(
0<.
m(f3 /\
A (a /\ A) ),
SO:r:8
faults of De Luca and Termini's conditions of fuzziness measurement and have retieved it.
f, . (a /\ A) ) )
lim
In this section, first of al]. we sh'1.Jl give an axiomatic definition for measure
-° a ,. ° me a m(
K( ( a /\ A ), o() { :
/I A ) ~ 0(
11 A)
> 0(
Proof. The procedure of the proof is the
of fuzzlness on ordinary fuzzy sets that t he grades of menbership lie the unit inteval lO, 1) , then we shall extend this aefinition to L-fuzzy sets.
following ti1.at (i)~( ii)~( iii)~(
iv)==>( iii)~ i)
The conditions for measure of fuzziness which De Luca and Terrr.tni suggested in (lJ
i")==}(iii). T,ot 0(. !l.€L and AE$. 1) 01. ;>m(A). By the condition (iv) "nil
I
the connecti vi tv of the inteval (m( a 1\ A( x) )
. 1) it follows that
m(o(/\ (a/\ A( x») is a
constant function on the inteval(m( a /\ A( x» , nand m( '" 1\ (a /\ A( x» = m( a " A( x». thUS. ITi(m(a/\Alx))/\(aAA(x))) =m(aAA(x». (?)o«m(.A). I f a
Indeed. if m(ai\A(x»
= m(b/\A(x». then
m( a J\ A( x » = m( 0( /\ A( x» = m( h J\ A( x ) ) . :"la that KtA, 0<. ) = ° for'1.1J o(.~ (a b) m(o\ A(x»
m( 0< /I A( x» =
< 0(
me 0(, A Al x »
'"
0(
~
!ll(' ):
~-L
(D ) 3
is a fuzzy mea>lure
AE
33
AXIOMATIC DEFINITION OF
In (1) . De Luca and Termini first suggested the measure of fuzziness and they gave three conditions what the measure of fUZ2iness ~atisfy
0
for all A E:
P( X) ,
~
d( A) 11 d(B) if
AeX)
when
A( x) ~ ~
iJ(x) '" A( x)
when
A( xl", X
x)
In (2J ,
iUZZINESS
should
=
~
De
Luca and Termini suggested
further the following definition,
m( A)
for all 3
:j( A)
( D ) d( A) is maximum of d(·) if A(x) 2 for all x E: X ,
at least, His intial paper
introduce in the inteval I = (0, 1)
~s
Let
the partial order relation '", defineo. for all x ,Y E I, as
such that
m( A)
11 , then d(·)
that
x) )
i\
p( X) the pOvler
satisfies at least tne following conditions
B(
( iii) ==* ( i). For any A c ~. define m(A) = on
ma pping dC,): r(x) __ (o,
then
this is impossible. Thus, we have
X,
set of X. A
mlm(o(AA(x»td",I\A(x»)
< m( 0( /\ A(
m( A), then
Let X be an universa l set, :rlX) the set of all ord inary fuzzy sets on
(D ) l
< rn' b i\ At x) ) .
Therefore, if
are the following that
X I~
.Y
So tllat A .. ' B ~ .A. ( x) ",' B( x )
for all XEX
for all A,BE f(X) and a real value mapping d( .) is called a meaSUJ'e of fuzziness, if
, lD ) l
d( A) = 0
(D~)
d(A)
has ge nerated a lot of papers un this area.
A = A',
In particular, in (9) • Yager suggested the
(D )
, 3
ift A i.s a crisp set,
reaches its maximum value iff
d( A) ~ d( B)
if
A '~ B •
Zi-Xiao Wang
344
It is obverous that (D ) l includes (Di), (D2 ) includes (D arid (D ) 3 includes lD we think that the condition
sequence, tnen
( Dl ), (D2 ) and (D ) are more reasonable than 3 the conditions (Di), (D;2.l and (D are.
cept to L-fuzzy sets, let us to
Remark.
(1)
2)
3).
3)
d(·) satisfying the condition (D ), l (D 2 ) and (D ) may be not a voluation on 3 (X).
Defini tiOD 3.2
13n (~,
A mapping
cC·) : L ---I' L is
L --+ L satisfies the following conditions
~n(o, X) =
= { An [0, ~l : AE~}' $2 =
r3 J
called a complementory operation, if cl· ):
Counterexample. Let X = (0, IJ , ~ is the
=
that the lattice 1 is complementary, Here, Dubois in
r
j31
su~pose
the complementary operatinn is defined by
( 2)
Borel field of X.
d( lim A ) = lim d( A ). n n
In order to extend the abovo mentioned con-
1J
AfM,
( 1)
c( 0) = I,
(?)
C fR
( "")
c is involutive ( co c = identify)
strictly decreasing,
tnen$lana 13 2 are Borel fields on [0, ~) and l~, 1) respE'cti.-.
Proposition 3.1
vely.
mentory metric lattice. Any element x and
1et m and m2 are fuzzy measures on ~l and l $2 respectively, so that a mapping
its complementory element x' is comparable.
=
{An
0;,
1) :
Ill(') : mlA) = m_,(A)V m lA) for all A.:!3
2 The following mapping
$ .
is a measure on
d( A) = 2-}1 A( x) where A.
{x:
=
A(
x)
and (x, e', x') ( see
f; .
But d(' )
~
A( x) Bl
B
x)
B( x)
f." '
X,
when
xf (
when
x r: (0, ~)
when
x E ( ~, 1) ,
11
of I"
and
b~
as tne following that
of all
$ -
'$
rn),
ji
°
i f A~
deAl
( F2 )
d( A) ~ d( B)
iff
(F J 3 lF 4 )
dlA) If
=
lA n \
n~
sothata~a'
~
( x' )' ~
X
I
=*
1
x'
E
12
L , then x' E: L , Thus, 2 l b and a' E 12~ b ~ a' ==> b
E
and b E: Ll =+ b"
b, and a
= b
a"'" a
a' b'
Since a< b is
prove that tne condi t~on is necessary,
we assume that any element x such that x< x' , if
if
~A')
~ x
2
impossi ble.
13 A(X)
>
B( x) )
B( x) ~ A( x)
Ll ' then
"'* a' b ~ a' "'* b' ~ a
'1'0
if
B( x) ~ A( x) V A '( x)
Eo
a ) b'
d(·) satisfios tne following conditions (}'r)
2
similarly, if x
A mapping d(·) :~~(o, I)
is called a measure of fuzziness on
l
x ---+ x'
denote the set
measurable fuzzy sets on X.
Definition 3.1
E 11 and b E: L , thus, a' a' 2 b'. It is sufficient to show a = b.
Indeed, if x
Assume tnat tne universal set is a fuzzy
X,D ,
1
By the definitions of 11 and 1 2 , we have x-x' : L ---+ L ; x---+ x' : 1 - 1
,we suggested the concept of
'lleasure space l
x E 1 } and
easily to prove a
$" .
fu~ziness
V {x :
x E L2 \ exist in L and they are denoted by a and b respectively. It is
and ~A) = d(B) = 1, this is to say d(·) is
mea sure 01'
it follows that
V {x:
d(AUB) = 1, d(AOB) = u,
In (8)
{x: x ~ x'}
Ll and 12 are non-empty. By the completeness
that
not a valuation on
)
{x:x~x'~
11 L2
x E (0, ~)
when
°0
(10)
Proof. Put
not a valuation on ~ • lndeed, let A : A( x)
So
di tions that if x < x', then there exist an
} ,
is a measure of fuzziness on 4S
To exist uniquely an element a sucn that a = a' it is necessary and sufficient conelement e f x and x' such that (x, e, x')
M x) I dm
~ ~
1et 1 be a complete comple-
~ ~
B( x) ~ ~~
for all H~ ,
l e i is a monotone
or
then the element a is an element satisfyinC the condition. Assume that 1 denote the lattice satisfying the condition of tiLe pro posi tion 3.1, then ;
By a meaSure of fuzziness
345
On the Fuzzy Measures and the Measures of Fuzziness d( -) :
're X)---+L
we mean that d( -) satisfies
dlA)
=0
d(A)
~
Proof. By h(O)
if A is a crisp set,
heAl xl>
d(B) i f
B( x) VB' ( x) "> A( x) V A•( x)
i f A( x) > a
orB(x»a
At
B( x) ~
x)
if
At x) <; a
and
for all A E:
j ( X) ,
If {An} n~ le 1(X) is a monotone
A )
n
= lim
By A and B satisfy the condition (1 2 ), therefore, h( A( x» "9 h( B( x» , so that deAl "9 d(B). Other conditions are clearly The measure of fuzziness defined in the proposition 4.i possesses the following If d(-) satisfies fuzzy adctitivity. i.e.
d(A ). n
d( ( 0( /\ A( x) ) V (~/\ B( x) ) )
To illustrate the above mentioned definition is reasonable, we have ~roposition
3.2
= for all
The element a is comparable
in the lattice 1 , in
~ ELand A and B Eo
For all E E $ and If
In order to com pare the fuzziness grades element ~
d( cl 1\ A( x) ) V d( ~ 1\ Et x) ) 01. ,
wi th any element x ~ 1. between two
therefore, it is
property.
sequence of 1-fuzzy sets, then d( iim
= h(I) = 0,
for all AEi·
= 0
satisfied.
B(x)(,a d( A) = d( A ')
The mapping d(') is a
measure of fuzziness.
the following conditions (1 ) 1 (12 )
PrOpoSition 4.1
(ii)
0(
~
0(
~
f;,
then
L
a. then d( 0( 1\ E( x » = d(
Ifo«a, then there
exist~
0(' /\
Et x ) )
an
element A( E) such that
(10) , Yager suggested the following
concept. Definition 3.5
when h(e() <
Given two elements x and y
in a lattice, we shall say t hat element x
where A ( .) : $-+L and ,\IAUB)
i s at least as fuzzy a s y. denoted xfy, if
for all
the following two conditions hold. (1)
(y,
( 2 )
(
,B E1J , =
h(O
y, x~, y*)
,;here x" anO y" are the nega tions of x and y respectively. Proposition 3 .3
A
X(A)UA(B)
h(') satisfies that
y*)
Y.,
A(E)
Assume that A and Bare
h(~)
V h(~)
for allo(.~~ a. Conversely, we have Theorem 4.1
Let d(·) be a mea sure of
two 1-fuzzy sets on X. 'l'hen AfB iff A and B
fuzziness satisfying thp fuzzy additivity
satisfy the condition (L ). where A" is the
and the condition
complement of A.
fuzzy measure m(·) : f,-L such that
2
THE MEaSURE OF FUZZINESS FOR L-FUZZY SETS
for all A E Proof.
In th1s section, we shail consider the
dm :
First of all, we define the
following mapping m(·) :
(ii)
L--+L
(iii)
h( 0) = 0
h( u)
=
for all u E L
h(') is strictly monotone increa-
sing on (0, a).
.
tJ
dlA) = ~h(A(X» i)
A = rf.../\ E( x) lA =
h( u·)
that
Now, we shall show that
satisfies the following conditions ( i)
$ __ L
for all A E $ meaSure on
:t ---,>L.
.where the continuous function h(x)
")
It is clear that the mapping ~-) is a fuzzy
}'or all A Et, we define that d( A) = ~ h( A( x»
(
i.
relation between the fuzzy integ ral and the measure of fuzziness.
there exists a
~ h( A) dm
d( A)
4 THE INTEGRAL REPRESENTATION OF
(1~),then
dm
for all AE:j •
where
lh(A(x»
EE$, dm
S
h( 0(.,) /\ m( E)
t
h( o() t\ m( E)
Therefore, it is obverously that
'" ~ a 0(
<
~A)
a
= lA
Zi-xiao Wang
346
by the condition (L ) ii)
VoIi "
A( x) =
and E.Sanchez (Editors), North-
5
Holland Publishing Company, 1982.
Ei\ x) is a simple
71-78
function. 'I'he formula \ *) holds s ince d(' ) possesses the fuzzy additivity. iii)
A(x} is
a sequence taat
{An}
A) x) __ h(
An \
X») ---+
~ h( A( x)
measures of fuzziness, Presented at
of simple func"tions such.
" Procedings of the Second World
a( x; \ uniformly). By the
continuity of the function n(· ) , i t tha t
h(
X)
Conference on Mathematics at Severce th th of Man", June 28 to Jlily 3 ,
follow~
1982, Canary Islands, Spain.
and
lim ~ h( A (x)
dm
n
dm
( 9)
R.R.Yager, On the measure of fuzziness and negation part I : Membership
lim d( A } n
in the uni t in tevB1, In t. J. Gen eral
d( A) •
Remark.
, Fuzzy measures and
(8)
a general function. We take
Systems 5, 221-229.
The function h(' ) may be regarded
as a subjective principle of the measurement
. On the measure of fuzziness
(10)
of fuzzincss, thus, it is very intereflting
and negation
pr oblem how h(') i '; determined .
Information and Control, 44(1980)
~rt
JJ : T,l'tttice.
236-260
REl-'ERl!:NCES (1)
(ID
A. De Luca and 'l'ermini, It d efini tion of a n on -probabilistic entropy in tne setting of fuzzy se ts tneory, Inform. awl Contr ., 20 (1972) 301--312.
( 2)
, On some ale ebrai c as pects of the measure of fuzzine s s, " Fuzzy Information ani' Decision Pro cesses " M.tvl.Gupta and l!:. Sanchez \ Editors ) Nortn-·Hulland
(3)
Publishin~
Company , l':;ltlc .
D. DuboiS, Uncertainty in tran sportation network design: some new techniques, Presented at the IV Euro pean congress on
(4)
0
t il
pera tion re s each.
B.P.Klement et al., E'uzzy probability measures, J. Int.
Sets and
~ uzzy
Sys tems 5(1981) 21-30. (5)
M. Sugeno, '2heory of fnzzy integrals and its applications , Ph.D.Dissertati on, Tokyo Institute of Tech. , 1'::J74.
(6 )
Zi-Xiao Wang,
Note on the fuzzy
mea s ure, It Monthly J. of SCience, Vol. 26, No. 11 \Beijing, Cnina) 961- 964.
(7 )
The structure of fuzzy Lebesgue measures, " Fuzzy Information and Decision
Proc ess e~
", M.M.Gupta
L.A.Zadeh, Probability measure on fuzzy events. J. Math.Anal.Appl. (1968) .