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FRANCISCO GALLEGO LUPI ´A ˜NEZ

Received 22 September 2004 and in revised form 29 March 2005

The introduction of intuitionistic fuzzy sets is due to K. T. Atanassov, who also proposed some problems about this subject. D. C¸oker defined the intuitionistic fuzzy topological spaces and, with some coworkers, studied these spaces. In this paper, we define and study the notion of quasicoincidence for intuitionistic fuzzy points and obtain a characteriza- tion of continuity for maps between intuitionistic fuzzy topological spaces

The introduction of “intuitionistic fuzzy sets” is due to Atanassov [1], and this theory has been developed in many papers [2,3,4]. This author proposed as an open prob- lem “to investigate the topological and geometric properties of the IFSs” remarking that

“some first steps in this direction are made” [4].

In this paper, we define for intuitionistic fuzzy sets the notion of quasicoincidence and the corresponding neighborhood structure (see [9]). These concepts allow us to obtain a characterization of continuity for maps between two intuitionistic fuzzy topological spaces.

(For notions on ordinary fuzzy topology used in this paper, see [7,8].) First, we list some previous definitions.

Definition 1[1]. LetXbe a nonempty set. An intuitionistic fuzzy set (IFS)AofXis an object having the form

A=

x,µAA

| xX, (1)

where the functions µA:XI andγA:XI denote the degree of membership and the degree of nonmembership of each elementxX to an ordinary subset ofX, and 0µA(x) +γA(x)1 for eachxX.

Notation 2. 0= x, 0, 1and 1= x, 1, 0.

Definition 3[2]. LetXbe a nonempty set, and letAandBbe two IFSs ofX. Then, (a)ABifµA(x)µB(x) andγA(x)γB(x);

(b)A=BifABandBA;

Copyright©2005 Hindawi Publishing Corporation

International Journal of Mathematics and Mathematical Sciences 2005:10 (2005) 1539–1542 DOI:10.1155/IJMMS.2005.1539

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1540 Quasicoincidence for intuitionistic fuzzy points (c)AB= {x,µAµBAγB |xX};

(d)AB= {x,µAµB,γAγB |xX}.

Definition 4[5]. Let{Aj|jJ}be an arbitrary family of IFSs ofX. Then, (a)Aj= {x,µAj,γAj |xX};

(b)Aj= {x,µAj,γAj |xX}.

(For other definitions concerning IFSs used in this paper, see [5,6].)

Definition 5. LetA= {x,µA,γA |xX}andB= {x,µB,γB |xX}be two IFSs. Say thatAquasicoincides withB, denoted byAqBifµAquasicoincides withµBandγAquasi- coincides withγB.

Remark 6. If AqB, we have that AB=0. (µAB implies that µAµB=0, then AB=0).

Remark 7. IfAandBverify thatγA=µAandγB=µB, thenAqBif, and only if,µAB. Proposition 8. Let A and B be two IFSs of X, let f :XY be a map between two nonempty setsXandY, then ifAqB, f(A)q f(B).

Proof. AqB if and only if µAB and γAB. Then, we have that fA)q f(µB) and fA)q f(γB), that is, (1fA))q(1fB)). Thus f(A)q f(B).

Proposition9. LetXandYbe two nonempty sets, let f :XYbe a map, letAbe an IFS ofX, and letCbe an IFS ofY. If f(A)qC,Aq f1(C).

Proof. f(A)qC if and only if fA)qµC and fA)qγC. Then, µAq f1C) and γAq f1(γC), that is,γAq(f1(γC))(because f1(γC)=f1(γC)).

Remark 10. IfA,B, andCare IFSs ofX, such thatAqB, andBC, thenAqC.

Definition 11. Let (X,τ) be an IFTS, and letpbe an IFP ofX. Say that an IFSNofXis a Q-neighborhood ofpif there exists an IFOSAof (X,τ) such thatpqAandAN.

Theorem12. Let(X,τ)be anIFTS, letpbe anIFPofX, and letQ(p)be the family of all theQ-neighborhoods ofpin(X,τ), then,

(1)NQ(p)implies thatpqN,

(2)N1,N2Q(p)imply thatN1N2Q(p), (3)ifNQ(p)andNM, thenMQ(p),

(4)ifNQ(p), there exists MQ(p),MN, such that, for everyIFPe which quasicoincides withM,MQ(e).

Proof. (1)NQ(p) if and only if there exists an IFOSAsuch that pqAandAN, thenpqN (byRemark 10).

(2)N1,N2areQ-neighborhoods ofpif and only if there exist two IFOSsAisuch that pqAi,AiNi(i=1, 2), then, ifp=c(α,β), we have thatcαAi,µAiµNi,c1βAi,γAi γNi(i=1, 2), thencαA1A2,µA1A2µN1N2,c1βA1A2,γA1A2γN1N2, andpq(A1 A2),A1A2N1N2, withA1A2an IFOS.

(3) It is obvious.

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(4)NQ(p) if and only if there exists an IFOSAsuch thatpqAandAN, thenA is also aQ-neighborhood ofp, and for each IFPesuch thateqA,Ais aQ-neighborhood

ofe.

Proposition13. LetXbe a nonempty set, for eachIFPpofX, letQ(p)be a family of IFSsverifying (1), (2), and (3) of the theorem, thenτ= {UIFS|UQ(p)ifpqU}is an IFTinX. If also the family verifies (4), thenQ(p)is the system ofQ-neighborhoods ofpin (X,τ).

Proof. 1τby (3).

Uiτ(i=1, 2), andpq(U1U2), thenUiQ(p) andU1U2Q(p) by (2).

{Uj}jJ τ,pqUj with p=c(α,β) if and only ifcαUj andc1βUj and it is equivalent tocαUj0 (for somej0ofJ) andc1βUj (for all jofJ). Then pqUj0 for some j0J,Uj0Q(p) for some j0J, andUjQ(p) by (3).

Finally, ifNQ(p), there existsMQ(p),MN, such that for every IFPewhich quasicoincides withM, we have thatMQ(e), thenMτ,pqM,MN, andN is a Q-neighborhood of pin (X,τ). Conversely, for everyQ-neighborhoodNofpin (X,τ), there is anAτsuch thatpqA,AN, then for every IFPewhich quasicoincides with A, we have thatAQ(e), thusNQ(p).

Proposition14. LetX,Y be two nonempty sets, let f :XY be a map, letτbe anIFT inX, and letsbe anIFTinY. Then, f : (X,τ)(Y,s)is continuous if, and only if, for each IFPpofX, and for eachQ-neighborhoodVof f(p), there exists aQ-neighborhoodUofp such that f(U)V.

Proof. IfV is aQ-neighborhood of f(p), there exists an IFOSGsuch that f(p)qGand GV, then pq f1(G) (byProposition 9), and f1(G) is an IFOS such that f1(G)

f1(V). Thus,f1(V) is aQ-neighborhood ofpand f(f1(V))V.

Conversely, for each Gs, we have that, for every IFP p such that pq f1(G) is f(p)q f(f1(G)) (byProposition 8), then f(p)qG, andGis aQ-neighborhood of f(p).

By the hypothesis, there exists aQ-neighborhoodUofpsuch that f(U)G, thenU f1(G) and f1(G)Q(p). FromProposition 13, it follows that f1(G)τ.

References

[1] K. T. Atanassov,Intuitionistic fuzzy sets, VII ITKR’s Session, Sofia, 1983 (Central Sci. Tech.

Library, Bulg. Acad. Sci, 1984).

[2] ,Intuitionistic fuzzy sets, Fuzzy Sets and Systems20(1986), no. 1, 87–96.

[3] ,More on intuitionistic fuzzy sets, Fuzzy Sets and Systems33(1989), no. 1, 37–45.

[4] ,Intuitionistic Fuzzy Sets. Theory and Applications, Studies in Fuzziness and Soft Com- puting, vol. 35, Physica-Verlag, Heidelberg, 1999.

[5] D. C¸oker,An introduction to intuitionistic fuzzy topological spaces, Fuzzy Sets and Systems88 (1997), no. 1, 81–89.

[6] D. C¸oker and M. Demirci,On intuitionistic fuzzy points, Notes IFS1(1995), no. 2, 79–84.

[7] Y.-M. Liu and M.-K. Luo,Fuzzy Topology, Advances in Fuzzy Systems—Applications and The- ory, vol. 9, World Scientific, New Jersey, 1997.

[8] N. Palaniappan,Fuzzy Topology, CRC Press, Florida, 2002.

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1542 Quasicoincidence for intuitionistic fuzzy points

[9] P. M. Pu and Y.-M. Liu,Fuzzy topology. I. Neighborhood structure of a fuzzy point and Moore- Smith convergence, J. Math. Anal. Appl.76(1980), no. 2, 571–599.

Francisco Gallego Lupi´a˜nez: Departamento de Geometr´ıa y Topolog´ıa, Facultad de Ciencias Matem´aticas, Universidad Complutense de Madrid, 28040 Madrid, Spain

E-mail address:fg [email protected]

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Special Issue on

Time-Dependent Billiards

Call for Papers

This subject has been extensively studied in the past years for one-, two-, and three-dimensional space. Additionally, such dynamical systems can exhibit a very important and still unexplained phenomenon, called as the Fermi acceleration phenomenon. Basically, the phenomenon of Fermi accelera- tion (FA) is a process in which a classical particle can acquire unbounded energy from collisions with a heavy moving wall.

This phenomenon was originally proposed by Enrico Fermi in 1949 as a possible explanation of the origin of the large energies of the cosmic particles. His original model was then modified and considered under different approaches and using many versions. Moreover, applications of FA have been of a large broad interest in many different fields of science including plasma physics, astrophysics, atomic physics, optics, and time-dependent billiard problems and they are useful for controlling chaos in Engineering and dynamical systems exhibiting chaos (both conservative and dissipative chaos).

We intend to publish in this special issue papers reporting research on time-dependent billiards. The topic includes both conservative and dissipative dynamics. Papers dis- cussing dynamical properties, statistical and mathematical results, stability investigation of the phase space structure, the phenomenon of Fermi acceleration, conditions for having suppression of Fermi acceleration, and computational and numerical methods for exploring these structures and applications are welcome.

To be acceptable for publication in the special issue of Mathematical Problems in Engineering, papers must make significant, original, and correct contributions to one or more of the topics above mentioned. Mathematical papers regarding the topics above are also welcome.

Authors should follow the Mathematical Problems in Engineering manuscript format described at http://www .hindawi.com/journals/mpe/. Prospective authors should submit an electronic copy of their complete manuscript through the journal Manuscript Tracking System athttp://

mts.hindawi.com/according to the following timetable:

Manuscript Due December 1, 2008 First Round of Reviews March 1, 2009 Publication Date June 1, 2009

Guest Editors

Edson Denis Leonel,Departamento de Estatística, Matemática Aplicada e Computação, Instituto de Geociências e Ciências Exatas, Universidade Estadual Paulista, Avenida 24A, 1515 Bela Vista, 13506-700 Rio Claro, SP, Brazil ; [email protected]

Alexander Loskutov,Physics Faculty, Moscow State University, Vorob’evy Gory, Moscow 119992, Russia;

[email protected]

Hindawi Publishing Corporation http://www.hindawi.com

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