Next Article in Journal
A Note on the Laguerre-Type Appell and Hypergeometric Polynomials
Next Article in Special Issue
Fixed Point Results for Perov–Ćirić–Prešić-Type Θ-Contractions with Applications
Previous Article in Journal
Symmetric Diffeomorphic Image Registration with Multi-Label Segmentation Masks
Previous Article in Special Issue
Self-Adaptive Method and Inertial Modification for Solving the Split Feasibility Problem and Fixed-Point Problem of Quasi-Nonexpansive Mapping
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Ćirić-Type Operators and Common Fixed Point Theorems

by
Claudia Luminiţa Mihiţ
1,*,†,
Ghiocel Moţ
1,† and
Gabriela Petruşel
2,†
1
Department of Mathematics and Computer Science, “Aurel Vlaicu” University of Arad, Elena Drăgoi Street no. 2, 310330 Arad, Romania
2
Department of Business, Babeş-Bolyai University Cluj-Napoca, Horea Street no. 7, 400174 Cluj-Napoca, Romania
*
Author to whom correspondence should be addressed.
These authors contributed equally to this work.
Submission received: 28 March 2022 / Revised: 29 May 2022 / Accepted: 2 June 2022 / Published: 6 June 2022
(This article belongs to the Special Issue Fixed Point, Optimization, and Applications II)

Abstract

:
In the context of a complete metric space, we will consider the common fixed point problem for two self operators. The operators are assumed to satisfy a general contraction type condition inspired by the Ćirić fixed point theorems. Under some appropriate conditions we establish existence, uniqueness and approximation results for the common fixed point. In the same framework, the second problem is to study various stability properties. More precisely, we will obtain sufficient conditions assuring that the common fixed point problem is well-posed and has the Ulam–Hyers stability, as well as the Ostrowski property for the considered problem. Some examples and applications are finally given in order to illustrate the abstract theorems proposed in the first part of the paper. Our results extend and complement some theorems in the recent literature.

1. Introduction and Preliminaries

Let ( X , d ) be a metric space and f : X X be an operator. Throughout this paper we denote by F i x ( f ) : = { x X : x = f ( x ) } the fixed point set of f and by G r a p h ( f ) : = { ( x , f ( x ) ) : x X } the graph of the operator f.
In this context, let f : X X be an α -contraction, in the sense that there exists α ( 0 , 1 ) such that
d ( f ( x ) , f ( y ) ) α d ( x , y ) ,   f o r   a l l   ( x , y ) X × X .
The Banach–Caccioppoli Contraction Principle states that if ( X , d ) is a complete metric space, then any α -contraction f : X X has a unique fixed point, and the sequence { f n ( x ) } n N of Picard iterates starting from any element x X converges to the unique fixed point.
If the operator f : X X satisfies the above condition for every ( x , y ) G r a p h ( f ) , then f is called a graph α -contraction.
It is also known that any graph α -contraction f : X X on a complete metric space ( X , d ) that has a closed graph (i.e., the set G r a p h ( f ) is closed) has at least one fixed point and, for each x X , the sequence { f n ( x ) } n N of Picard iterates converges to a fixed point of f.
The conclusions of the above two fixed point theorems generated the following two important notions.
Let ( X , d ) be a metric space and f : X X be an operator. Then, by definition, f is called a weakly Picard operator if the sequence ( f n ( x ) ) n N of Picard iterates, starting from any point x X , converges to a fixed point x * ( x ) of f. If, in particular, in the above definition f has a unique fixed point, then f is called a Picard operator. By the definition of a weakly Picard operator, the following set retraction is generated f : X F i x ( f ) , f ( x ) = lim n + f n ( x ) .
If f : X X is a weakly Picard operator for which there exists c > 0 such that
d ( x , f ( x ) ) c d ( x , f ( x ) ) ,   f o r   a l l   x X ,
then f is called a weakly c-Picard operator. If a Picard operator satisfies the above condition (with f ( x ) = { x * } , x X ), then f is called a c-Picard operator.
It is easy to see that, in the context of a complete metric space, any self graph α -contraction with a closed graph is a weakly 1 1 k -Picard operator, while any α -contraction is a 1 1 k -Picard operator.
The following general result will be very useful in applications, see [1].
Theorem 1.
Let ( X , d ) be a metric space and f : X X be a c-Picard operator with x * X its unique fixed point. Then:
(a) the fixed point equation x = f ( x ) is well-posed in the sense of Reich and Zaslawski (see [2]), i.e., F i x ( f ) = { x * } and for any sequence ( v n ) n N X with d ( v n , f ( v n ) ) 0 as n + , we have that v n x * as n + ;
(b) the fixed point equation x = f ( x ) is Ulam–Hyers stable, i.e., there exists C > 0 such that for every ε > 0 and for every x ˜ X satisfying d ( x ˜ , f ( x ˜ ) ) ε , we have that d ( x * , x ˜ ) C ε .
Remark 1.
Let ( X , d ) be a metric space and f : X X be a weakly c-Picard operator. Then, the fixed point equation x = f ( x ) is Ulam–Hyers stable.
For our next result, we recall the notion of quasi-contraction. Let ( X , d ) be a metric space and f : X X be an operator such that F i x ( f ) = { x * } . Then, f is said to be a β -quasi-contraction if β ] 0 , 1 [ and
d ( f ( x ) , x * ) β d ( x , x * ) ,   f o r   e v e r y   x X .
The concept was extended by I.A. Rus [3] to the case of weakly Picard operators as follows. Let ( X , d ) be a metric space and f : X X be a weakly Picard operator. Then, f is said to be a γ -quasi-contraction if γ ] 0 , 1 [ and
d ( f ( x ) , f ( x ) ) γ d ( x , f ( x ) ) ,   f o r   e v e r y x X .
Theorem 2.
Let ( X , d ) be a metric space and f : X X be a β-quasi-contraction such that F i x ( f ) = { x * } . Then, f has the Ostrowski stability property, i.e., F i x ( f ) = { x * } and any sequence ( w n ) n N in X with d ( w n + 1 , f ( w n ) ) 0 has the property that w n x * as n + .
For other details on Picard and weakly Picard operator theory, see [4,5,6] and the references therein. For the above concepts and for related notions and results, see [7,8,9,10,11,12].
If ( X , d ) is a metric space and f , g : X X are two operators, then a common fixed point for f and g is an element x * X with the property x * = f ( x * ) = g ( x * ) . The common fixed point set for f and g is denoted by C o m F i x ( f , g ) . Notice that C o m F i x ( f , g ) = F i x ( f ) F i x ( g ) . In the paper [1] (see also [13]), the following open problems are given:
Suppose there exists α ] 0 , 1 [ such that, for every x , y X we have
d ( f ( x ) , g ( y ) ) α max { d ( x , y ) , d ( x , f ( x ) ) , d ( y , g ( y ) ) , 1 2 d ( x , g ( y ) ) + d ( y , f ( x ) ) } .
I. Does the above metric condition of Ćirić (see [14]) on f and g imply all the following conclusions:
  • F i x ( f n ) = F i x ( g n ) = { x * } , for n N * ;
  • for each x 0 X , the sequence ( x n ) n N defined by
    x 2 n + 1 = f ( x 2 n ) , x 2 n + 2 = g ( x 2 n + 1 ) ,
    converges to x * ;
  • for each y 0 X , the sequence ( y n ) n N defined by
    y 2 n + 1 = g ( y 2 n ) , y 2 n + 2 = f ( y 2 n + 1 ) ,
    converges to x * ;
  • for each x 0 X , the sequence ( f n ( x 0 ) ) n N converges to x * ;
  • for each x 0 X , the sequence ( g n ( x 0 ) ) n N converges to x * .
II. Under which additional conditions, some other stability properties can be obtained?
In this work, we establish existence, uniqueness and approximation results for the common fixed point. In the same framework, we will obtain sufficient conditions assuring that the common fixed point problem is well-posed and has the Ulam–Hyers stability, as well as the Ostrowski property for the considered problem. Some examples and applications are finally given in order to illustrate the abstract theorems proposed in the first part of the paper. Our results extend and complement some theorems in the recent literature [1,14,15,16,17,18,19,20].

2. Main Results

Our first main result is the following common fixed point theorem for a pair of Ćirić-type operators.
Theorem 3.
Let ( X , d ) be a complete metric space and f , g : X X be two operators for which there exists α ( 0 , 1 ) such that, for each x , y X , the following condition holds:
d ( f ( x ) , g ( y ) ) α max { d ( x , y ) , d ( x , f ( x ) ) , d ( y , g ( y ) ) , 1 2 d ( x , g ( y ) ) + d ( y , f ( x ) ) } .
Then we have the following conclusions:
(a) C o m F i x ( f , g ) = F i x ( f ) = F i x ( g ) = { x * } ;
(b) for every x 0 X , the sequence ( x n ) n N given by
x 2 n + 1 = f ( x 2 n ) ,     x 2 n + 2 = g ( x 2 n + 1 ) ,     for   all   n N ,
converges to x * as n + ;
(c) for every y 0 X , the sequence ( y n ) n N given by
y 2 n + 1 = g ( y 2 n ) ,     y 2 n + 2 = f ( y 2 n + 1 ) ,     for   all   n N ,
converges to x * as n + ;
(d) if α < 5 2 , then f and g are graph contractions;
(e) if α < 1 3 , then f and g are quasi-contractions;
(f) if α < 5 2 , then f and g are c-Picard operators, with c : = ( 1 α ) 2 1 4 α α 2 ;
(g) if α < 5 2 , then the fixed point equation x = f ( x ) and the fixed point equation x = g ( x ) are well-posed in the sense of Reich and Zaslavski;
(h) if α < 5 2 , then the fixed point equation x = f ( x ) and the fixed point equation x = g ( x ) are Ulam–Hyers stable;
(i) if α < 1 3 , then f and g have the Ostrowski stability property.
Proof. 
(a) Let us prove that F i x ( f ) = F i x ( g ) . Let us consider first x * F i x ( f ) . Then, by (1), we have
d ( x * , g ( x * ) ) = d ( f ( x * ) , g ( x * ) ) α d ( x * , g ( x * ) ) .
Thus x * F i x ( g ) .
We will now prove that f and g have at most one fixed point. Indeed, if we suppose that x * , y * C o m F i x ( f , g ) = F f F g , then: Then, by (1), we have
d ( x * , y * ) = d ( f ( x * ) , g ( y * ) ) α max { d ( x * , y * ) } .
Hence d ( x * , y * ) = 0 .
(b) For arbitrary x 0 X we consider the sequence ( x n ) n N defined in (b). Then
d ( x 1 , x 2 ) = d ( f ( x 0 ) , g ( x 1 ) ) α max { d ( x 0 , x 1 ) , d ( x 0 , f ( x 0 ) ) , d ( x 1 , g ( x 1 ) ) , 1 2 d ( x 0 , g ( x 1 ) ) } = α max { d ( x 0 , x 1 ) , d ( x 1 , x 2 ) , 1 2 d ( x 0 , x 2 ) } α max { d ( x 0 , x 1 ) , d ( x 1 , x 2 ) , 1 2 d ( x 0 , x 1 ) + d ( x 1 , x 2 ) } = α max { d ( x 0 , x 1 ) , d ( x 1 , x 2 ) } .
Since α < 1 , we obtain that
d ( x 1 , x 2 ) α d ( x 0 , x 1 ) .
By induction, we get
d ( x n , x n + 1 ) α n d ( x 0 , x 1 ) ,       for   all   n N .
Using the above expression, we get that ( x n ) n N is a Cauchy sequence. Let x * X be its limit. We have
d ( x * , f ( x * ) ) d ( x * , x 2 n + 2 ) + d ( x 2 n + 2 , f ( x * ) ) d ( x * , x 2 n + 2 ) + d ( g ( x 2 n + 1 ) , f ( x * ) ) d ( x * , x 2 n ) + α max { d ( x * , x 2 n + 1 ) , d ( x * , f ( x * ) ) , d ( x 2 n + 1 , g ( x 2 n + 1 ) ) ,         1 2 d ( x * , g ( x 2 n + 1 ) ) + d ( x 2 n + 1 , f ( x * ) ) } = d ( x * , x 2 n ) + α max { d ( x * , x 2 n + 1 ) , d ( x * , f ( x * ) ) , d ( x 2 n + 1 , x 2 n + 2 ) ,         1 2 d ( x * , x 2 n + 2 ) + d ( x 2 n + 1 , f ( x * ) ) } .
Letting n + , we get d ( x * , f ( x * ) ) α d ( x * , f ( x * ) ) , which yields that x * = f ( x * ) .
Moreover, by (2), we obtain
d ( x n , x n + p ) α n 1 α d ( x 0 , x 1 ) ,       for   all   n N ,   p N * .
Letting p + and taking n = 0 , we obtain:
d ( x 0 , x * ) 1 1 α d ( x 0 , x 1 ) = 1 1 α d ( x 0 , f ( x 0 ) ) ,
which is a retraction-displacement-type condition, see [4].
(c) Consider y 0 X arbitrary chosen and the sequence ( y n ) n N defined as in (c). Thus
d ( y 1 , y 2 ) = d ( g ( y 0 ) , f ( y 1 ) ) α max { d ( y 1 , y 0 ) , d ( y 1 , f ( y 1 ) ) , d ( y 0 , g ( y 0 ) ) , 1 2 d ( y 0 , f ( y 1 ) ) } = α max { d ( y 0 , y 1 ) , d ( y 1 , y 2 ) , 1 2 d ( y 0 , y 2 ) } α max { d ( y 0 , y 1 ) , d ( y 1 , y 2 ) , 1 2 d ( y 0 , y 1 ) + d ( y 1 , y 2 ) } = α max { d ( y 0 , y 1 ) , d ( y 1 , y 2 ) } .
Since α < 1 , we deduce that
d ( y 1 , y 2 ) α d ( y 0 , y 1 ) .
By induction, we obtain
d ( y n , y n + 1 ) α n d ( y 0 , y 1 ) ,       for   all   n N .
By (4), it results that the sequence ( y n ) n N is Cauchy, hence convergent in ( X , d ) . Let y * X be its limit. We have
d ( y * , g ( y * ) ) d ( y * , y 2 n + 2 ) + d ( y 2 n + 2 , g ( y * ) ) d ( y * , y 2 n + 2 ) + d ( f ( y 2 n + 1 ) , g ( y * ) ) d ( y * , y 2 n ) + α max { d ( y * , y 2 n + 1 ) , d ( y * , g ( y * ) ) , d ( y 2 n + 1 , f ( y 2 n + 1 ) ) , 1 2 d ( y * , f ( y 2 n + 1 ) ) + d ( y 2 n + 1 , g ( y * ) ) } = d ( y * , y 2 n ) + α max { d ( y * , y 2 n + 1 ) , d ( y * , g ( y * ) ) , d ( y 2 n + 1 , y 2 n + 2 ) , 1 2 d ( y * , y 2 n + 2 ) + d ( y 2 n + 1 , g ( y * ) ) }
Letting n + , we get d ( y * , g ( y * ) ) α d ( y * , g ( y * ) ) and then y * = g ( y * ) . Since C o m F i x ( f , g ) = F i x ( f ) = F i x ( g ) we get that y * = x * .
On the other hand, by (4), we obtain
d ( y n , y n + p ) α n 1 α d ( y 0 , y 1 ) ,       for   all   n N , p N * .
Letting p + and considering n = 0 , we obtain again a retraction-displacement-type condition:
d ( y 0 , x * ) 1 1 α d ( y 0 , y 1 ) = 1 1 α d ( y 0 , f ( y 0 ) ) .
(d) We will show now that f is a graph contraction. Let x X be arbitrary chosen. We have
d ( f 2 ( x ) , f ( x ) ) d ( f 2 ( x ) , g ( x * ) ) + d ( f ( x ) , g ( x * ) ) α max { d ( f ( x ) , x * ) , d ( f ( x ) , f 2 ( x ) ) , 1 2 ( d ( f ( x ) , g ( x * ) ) + d ( x * , f 2 ( x ) ) ) } + α max { d ( x , x * ) , d ( x , f ( x ) ) , 1 2 ( d ( x , g ( x * ) ) + d ( x * , f ( x ) ) ) } = α max { d ( f ( x ) , x * ) , d ( f ( x ) , f 2 ( x ) ) , 1 2 ( d ( f ( x ) , x * ) + d ( x * , f 2 ( x ) ) ) } + α max { d ( x , x * ) , d ( x , f ( x ) ) , 1 2 ( d ( x , x * ) + d ( x * , f ( x ) ) ) } α max { d ( f ( x ) , x * ) , d ( f ( x ) , f 2 ( x ) ) , 1 2 ( 2 d ( f ( x ) , x * ) + d ( f ( x ) , f 2 ( x ) ) ) } + α max { d ( x , x * ) , d ( x , f ( x ) ) , 1 2 ( 2 d ( x , x * ) + d ( x , f ( x ) ) ) } α d ( f ( x ) , x * ) + d ( f ( x ) , f 2 ( x ) ) + α d ( x , x * ) + d ( x , f ( x ) ) .
Thus,
d ( f 2 ( x ) , f ( x ) ) α 1 α d ( x , x * ) + d ( f ( x ) , x * ) + d ( x , f ( x ) ) .
On the other hand, by the above relations, we have
d ( f ( x ) , x * ) = d ( f ( x ) , g ( x * ) ) α d ( x , x * ) + d ( x , f ( x ) )
and, then we get
d ( x , x * ) d ( x , f ( x ) ) + d ( f ( x ) , x * ) d ( x , f ( x ) ) + α d ( x , x * ) + d ( x , f ( x ) ) .
From the last relation, we deduce
d ( x , x * ) 1 + α 1 α d ( x , f ( x ) ) .
Using (8) in (7) we obtain that
d ( f ( x ) , x * ) α d ( x , x * ) + d ( x , f ( x ) ) α ( 1 + α ) 1 α d ( x , f ( x ) ) + α d ( x , f ( x ) ) = 2 α 1 α d ( x , f ( x ) ) .
Hence
d ( f ( x ) , x * ) 2 α 1 α d ( x , f ( x ) ) .
Now, using (8) and (9) in (6) we conclude that
d ( f 2 ( x ) , f ( x ) ) 2 α ( 1 + α ) ( 1 α ) 2 d ( x , f ( x ) ) .
Since
Γ : = 2 α ( 1 + α ) ( 1 α ) 2 < 1
we get the desired conclusion.
(e) By (a) we know that f and g have a unique fixed point. We prove that f is quasi-contraction. Indeed, we have
d ( f ( x ) , x * ) = d ( f ( x ) , g ( x * ) ) α max { d ( x , x * ) , d ( x , f ( x ) ) , d ( x * , g ( x * ) ) , 1 2 ( d ( x , g ( x * ) ) + d ( x * , f ( x ) ) ) } = α max { d ( x , x * ) , d ( x , f ( x ) ) , 1 2 ( d ( x , x * ) + d ( x * , f ( x ) ) ) } α d ( x , x * ) + d ( x , f ( x ) ) α d ( x , x * ) + α ( d ( x , x * ) + d ( x * , f ( x ) ) ) ,
which implies
d ( f ( x ) , x * ) 2 α 1 α d ( x , x * ) ,     for   all x X .
Thus, f is quasi-contraction. From the symmetry of condition (1), we also get that g is quasi-contraction.
(f) We prove that f and g are Picard operators. Indeed, being graph contractions with a unique fixed point x * , by the Graph Contraction Principle (see Theorem 3 in [21]), we obtain that f and g are c-Picard operators with c : = 1 1 Γ = ( 1 α ) 2 1 4 α α 2 .
(g) and (h) These two conclusions follow (f) via Theorem 1.
(i) The conclusion follows from (e) via Theorem 2. □
In the next example, we show the case of two operators, f and g, for which the main theorem in [1] is not applicable but which satisfies the above condition (1) and hence Theorem 3 applies.
Example 1.
Let f , g : [ 0 , 2 ] [ 0 , 2 ] be given by
f ( x ) = x 9 , x [ 0 , 1 ] x 10 , x ( 1 , 2 ] .
and
g ( y ) = y 10 , y [ 0 , 2 ] .
Choose x = 999 1000 and y = 1001 1000 . Then d ( f ( x ) , g ( y ) ) = 109 10 , 000 , while d ( x , y ) = 20 10 , 000 . If we suppose that there exists α < 1 such that d ( f ( x ) , g ( y ) ) α d ( x , y ) for all x , y [ 0 , 2 ] , then we get the contradiction α > 109 20 . On the other hand, the pair f, g satisfies the condition (1) with α : = 1 4 . Moreover, f and g have a unique common fixed point x * = 0 .
Remark 2.
It could be of real interest to give a common fixed point theory for a pair of Ćirić-type operators in the context of generalized metric spaces (b-metric space, partial metric space, vector-valued metric space, ⋯). See also [7], Chapter 3.

3. An Application

Let us consider the following operatorial problem: find ( x , y ) X × Y satisfying the following relations
x = f ( y ) y = g ( x ) ( x , y ) = h ( x , y ) ,
where f : Y X , g : X Y and h = ( h 1 , h 2 ) : X × Y X × Y are given operators and X , Y are two nonempty and closed subsets of a metric space ( M , d ) . Notice that the problem composed by the first two equations is also called the altering point problem, see [22].
We suppose the following hypotheses:
(i) there exists β ( 0 , 1 ) such that
d ( h 1 ( x 1 , y 1 ) , f ( y 2 ) ) β max { d ( y 1 , y 2 ) , d ( x 1 , h 1 ( x 1 , y 1 ) ) , 1 2 d ( x 1 , f ( y 2 ) ) } ,
for every ( x 1 , y 1 ) X × Y and y 2 Y ;
(ii) there exists γ ( 0 , 1 ) such that
d ( h 2 ( x 1 , y 1 ) , g ( x 2 ) ) γ max { d ( x 1 , x 2 ) , d ( y 1 , h 2 ( x 1 , y 1 ) ) , 1 2 d ( y 1 , g ( x 2 ) ) } ,
for every ( x 1 , y 1 ) X × Y and x 2 X ;
(iii) the space ( M , d ) is complete.
We introduce on X × Y the metric d ˜ defined, for z 1 = ( x 1 , y 1 ) , z 2 = ( x 2 , y 2 ) X × Y , by
d ˜ ( z 1 , z 2 ) : = max { d ( x 1 , x 2 ) , d ( y 1 , y 2 ) } .
We also denote t : X × Y X × Y , t ( x , y ) = ( f ( y ) , g ( x ) ) and α : = max { β , γ } .
Under the above notations, our problem (11) becomes a common fixed point problem of the following form
( x , y ) = t ( x , y ) = h ( x , y ) , ( x , y ) X × Y .
Then, for z 1 = ( x 1 , y 1 ) , z 2 = ( x 2 , y 2 ) X × Y , we have
d ˜ ( h ( z 1 ) , t ( z 2 ) ) = max { d ( h 1 ( x 1 , y 1 ) , f ( y 2 ) ) , d ( h 2 ( x 1 , y 1 ) , g ( x 2 ) ) } max { β max { d ( y 1 , y 2 ) , d ( x 1 , h 1 ( x 1 , y 1 ) ) , 1 2 d ( x 1 , f ( y 2 ) ) } , γ max { d ( x 1 , x 2 ) , d ( x 2 , h 2 ( x 1 , y 1 ) ) , 1 2 d ( y 1 , g ( x 2 ) ) } } α max { max { d ( y 1 , y 2 ) , d ( x 1 , x 2 ) } , max { d ( x 1 , h 1 ( x 1 , y 1 ) ) , d ( x 2 , h 2 ( x 1 , y 1 ) ) } , 1 2 max { d ( x 1 , f ( y 2 ) ) , d ( y 1 , g ( x 2 ) ) } } α max { d ˜ ( z 1 , z 2 ) , d ˜ ( z 1 , h ( z 1 ) ) , 1 2 d ˜ ( z 1 , t ( x 2 ) ) } .
Thus, h and t satisfy the main assumptions of Theorem 3, and we can get the following conclusions for our problem: existence and uniqueness of the solution, convergence results for the corresponding sequences and stability theorems (under additional assumptions on β and γ ).
For example, the above abstract model can be applied in the case of a hierarchical system of nonlinear variational inequality problems, which is defined as follows:
Find ( x * , y * ) F i x ( S ) such that
a T 1 ( y * ) + x * y * , x x * 0 ,           for   all   ( x , y ) F i x ( S ) b T 2 ( x * ) + y * x * , y y * 0 ,
where S : X × Y X × Y is given by S ( x , y ) : = ( S 1 ( x ) , S 2 ( y ) ) , where S 1 : X X , S 2 : Y Y , T 1 : X Y and T 2 : Y X are given operators, a , b > 0 and X , Y are two nonempty closed convex subsets of a real Hilbert space H.
It is known that problem (13) is equivalent to the following problem:
Find ( x * , y * ) X × Y such that
y * = P F i x ( S 2 ) ( I a T 1 ) ( x * ) x * = P F i x ( S 1 ) ( I b T 2 ) ( y * ) ( x * , y * ) F i x ( S ) ,
where, for a nonempty, closed and convex set, C H , the symbol P C denotes the metric projection onto C, i.e., P C ( u ) : = { v C : u v = inf c C u c } , u H .
Notice that (14) is exactly the type of problem modeled by system (11). Thus, imposing adequate assumptions on S , T 1 , T 2 , on the parameters a , b > 0 and on the given sets X , Y we can obtain existence, uniqueness and stability results for the hierarchical system of nonlinear variational inequality problems (13). For other results of this type, see [22,23].

4. Conclusions

In this work, we have considered the common fixed point problem for a pair of operators satisfying a very general metric condition of Ćirić type. Under some mild assumptions, we proved several properties of the common fixed point problem: existence and uniqueness of the common fixed point, approximation of the common fixed point, well-posedness, Ulam–Hyers stability and Ostrowski stability of the common fixed point problem. Our results extend and generalize some recent results in the literature, and an example is given to illustrate the generality of our theorems. Moreover, an application to a system composed by an altering point problem and a fixed point problem is presented. A model for these kinds of applications is the hierarchical system of nonlinear variational inequality problems. As an open problem, we can propose the following one: construct a similar common fixed point theory for a pair of self operators in a complete metric space ( X , d ) satisfying, for every element x , y from the space X, the following condition:
d ( f ( x ) , g ( y ) ) α max { d ( x , y ) , d ( x , f ( x ) ) , d ( y , g ( y ) ) , d ( x , g ( y ) ) , d ( y , f ( x ) ) } .

Author Contributions

Conceptualization, C.L.M., G.M. and G.P.; methodology, C.L.M., G.M. and G.P.; validation, C.L.M., G.M. and G.P.; investigation, C.L.M., G.M. and G.P.; writing—original draft preparation, C.L.M., G.M. and G.P.; writing—review and editing C.L.M., G.M. and G.P. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Acknowledgments

The authors would like to thank the anonymous referees for very useful remarks and suggestions.

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Petruşel, A.; Rus, I.A. The relevance of a metric condition on a pair of operators in common fixed point theory. In Metric Fixed Point Theory and Applications; Cho, Y.J., Jleli, M., Mursaleen, M., Samet, B., Vetro, C., Eds.; Springer: Singapore, 2021; pp. 1–21. [Google Scholar]
  2. Reich, S.; Zaslawski, A.T. Well-posedness of fixed point problems. Far East J. Math. 2011, 46, 393–401. [Google Scholar] [CrossRef]
  3. Rus, I.A. Relevant classes of weakly Picard operators. Anal. Univ. Vest Timişoara Ser. Mat.-Inform. 2016, 54, 131–147. [Google Scholar] [CrossRef] [Green Version]
  4. Berinde, V.; Petruşel, A.; Rus, I.A.; Şerban, M.A. The retraction-displacement condition in the theory of fixed point equation with a convergent iterative algorithm. In Mathematical Analysis, Approximation Theory and Their Applications; Rassias, V.G., Ed.; Springer: Cham, Switzerland, 2016; pp. 75–106. [Google Scholar]
  5. Rus, I.A.; Petruşel, A.; Petruşel, G. Fixed Point Theory; Cluj University Press: Cluj, Napoca, 2008. [Google Scholar]
  6. Rus, I.A.; Şerban, M.A. Basic problems of the metric fixed point theory and the relevance of a metric fixed point theorem. Carpathian J. Math. 2013, 29, 239–258. [Google Scholar] [CrossRef]
  7. Debnath, P.; Konwar, N.; Radenović, S. (Eds.) Metric Fixed Point Theory, Applications in Science, Engineering and Behavioural Sciences; Springer Forum for Interdisciplinary Mathematics; Springer: Berlin, Germany, 2021. [Google Scholar]
  8. Ostrowski, A.M. The round-off stability of iterations. ZAMM 1967, 47, 77–81. [Google Scholar] [CrossRef]
  9. Petru, P.T.; Petruşel, A.; Yao, J.-C. Ulam-Hyers stability for operatorial equations and inclusions via nonself operators. Taiwan. J. Math. 2011, 15, 2195–2212. [Google Scholar] [CrossRef]
  10. Petruşel, A.; Petruşel, G.; Wong, M.M. Fixed point results for orbital contractions in complete gauge spaces with applications. J. Nonlinear Convex Anal. 2020, 21, 791–803. [Google Scholar]
  11. Rus, I.A. Picard operators and applications. Sci. Math. Jpn. 2003, 58, 191–219. [Google Scholar]
  12. Rus, I.A. Some variants of the contraction principle, generalizations and applications. Stud. Univ. Babeş-Bolyai Math. 2016, 61, 343–358. [Google Scholar]
  13. Rus, I.A. On common fixed points. Stud. Univ. Babeş-Bolyai Math. 1973, 18, 31–33. [Google Scholar]
  14. Ćirić, L.B. Generalized contractions and fixed point theorems. Publ. Inst. Math. 1971, 12, 19–26. [Google Scholar]
  15. Ćirić, L. Some Recent Results in Metrical Fixed Point Theory; University of Belgrade: Belgrade, Serbia, 2003. [Google Scholar]
  16. Gopi, R.; Pragadeeswarar, V. Approximating common fixed point via Ishikawa’s iteration. Fixed Point Theory 2021, 22, 645–662. [Google Scholar] [CrossRef]
  17. Moţ, G.; Petruşel, A. Local fixed point theorems for graphic contractions in generalized metric spaces. Theory Appl. Math. Comput. Sci. 2018, 8, 1–5. [Google Scholar]
  18. Petruşel, A. Local fixed point results for graphic contractions. J. Nonlinear Var. Anal. 2019, 3, 141–148. [Google Scholar]
  19. Petruşel, A.; Petruşel, G.; Yao, J.-C. Perov type theorems for orbital contractions. J. Nonlinear Convex Anal. 2020, 21, 759–769. [Google Scholar]
  20. Petruşel, A.; Petruşel, G.; Yao, J.-C. Graph contractions in vector-valued metric spaces and applications. Optimization 2021, 70, 763–775. [Google Scholar] [CrossRef]
  21. Petruşel, A.; Rus, I.A. Graphic contraction principle and applications. In Mathematical Analysis and Applications; Rassias, T.M., Pardalos, P.M., Eds.; Springer: Berlin/Heidelberg, Germany, 2019; pp. 411–432. [Google Scholar]
  22. Sahu, D.R. Altering points and applications. Nonlinear Stud. 2014, 21, 349–365. [Google Scholar]
  23. Sahu, D.R.; Kang, S.M.; Kumar, A. Convergence analysis of parallel S-iteration process for a system of generalized variational inequalities. J. Funct. Spaces 2017, 36, 5847096. [Google Scholar] [CrossRef] [Green Version]
Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations.

Share and Cite

MDPI and ACS Style

Mihiţ, C.L.; Moţ, G.; Petruşel, G. Ćirić-Type Operators and Common Fixed Point Theorems. Mathematics 2022, 10, 1947. https://0-doi-org.brum.beds.ac.uk/10.3390/math10111947

AMA Style

Mihiţ CL, Moţ G, Petruşel G. Ćirić-Type Operators and Common Fixed Point Theorems. Mathematics. 2022; 10(11):1947. https://0-doi-org.brum.beds.ac.uk/10.3390/math10111947

Chicago/Turabian Style

Mihiţ, Claudia Luminiţa, Ghiocel Moţ, and Gabriela Petruşel. 2022. "Ćirić-Type Operators and Common Fixed Point Theorems" Mathematics 10, no. 11: 1947. https://0-doi-org.brum.beds.ac.uk/10.3390/math10111947

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop