Next Article in Journal
Impact of Nonlinear Thermal Radiation and the Viscous Dissipation Effect on the Unsteady Three-Dimensional Rotating Flow of Single-Wall Carbon Nanotubes with Aqueous Suspensions
Next Article in Special Issue
β–Hyers–Ulam–Rassias Stability of Semilinear Nonautonomous Impulsive System
Previous Article in Journal
An Analytical Numerical Method for Solving Fuzzy Fractional Volterra Integro-Differential Equations
Previous Article in Special Issue
Optimal Control of Nonsmooth Production Systems with Deteriorating Items, Stock-Dependent Demand, with or without Backorders
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

A New Approach to the Solution of Non-Linear Integral Equations via Various FBe-Contractions

by
Sumati Kumari Panda
1,*,
Asifa Tassaddiq
2,* and
Ravi P Agarwal
3,4
1
Department of Mathematics, Basic Sciences and Humanities, GMR Institute of Technology, Rajam 532127, Andhra Pradesh, India
2
College of Computer and Information Sciences, Majmaah University, Majmaah 11952, Saudi Arabia
3
Department of Mathematics, Texas A&M University-Kingsville, Kingsville, TX 78363, USA
4
Distinguished University Professor of Mathematics, Florida Institute of Technology, Melbourne, FL 32901, USA
*
Authors to whom correspondence should be addressed.
Symmetry 2019, 11(2), 206; https://doi.org/10.3390/sym11020206
Submission received: 8 January 2019 / Revised: 23 January 2019 / Accepted: 28 January 2019 / Published: 12 February 2019
(This article belongs to the Special Issue Nonlinear, Convex, Nonsmooth, Functional Analysis in Symmetry)

Abstract

:
In this article, we introduce and establish various approaches related to the F-contraction using new sorts of contractions, namely the extended F B e -contraction, the extended F B e -expanding contraction, and the extended generalized F B e -contraction. Thereafter, we propose a simple and efficient solution for non-linear integral equations using the fixed point technique in the setting of a B e -metric space. Moreover, to address conceptual depth within this approach, we supply illustrative examples where necessary.

1. Introduction

Widely renowned for the “Fredholm Integral Equation”, Erik Ivar Fredholm [1], a mathematician and researcher par excellence, has provided research contributions on various aspects of integral equation theory.
Inspired by his great work, many fixed point researchers have focused their work on solving the Fredholm integral equation [2,3,4,5].
There was an amazing publication called F-contraction, which was one of the most influential publication in metric fixed point theory. It was introduced by a fellow named Wardkowski in 2012, and he brought this development to mathematical world with his idealistic touch [6]. It contained topological notions such as Cauchy, completeness, converges, and fixed point.
Definition 1.
Let ( X , d ) be a metric space. A mapping H : X X is said to be an F-contraction if there exists τ > 0 such that for all x , y X ,
d ( H x , H y ) > 0 τ + F ( d ( H x , H y ) ) F ( d ( x , y ) ) .
F-expanding mappings were introduced in 2017 by Gornicki [6] as below:
Let ( X , d ) be a metric space. A mapping H : X X is said to be F-expanding if there exists τ > 0 such that for all x , y X ,
d ( x , y ) > 0 F ( d ( H x , H y ) ) + F ( d ( x , y ) ) + τ
where F : R + R is a mapping satisfying:
( F 1 )
F is strictly increasing, i.e., for all α , β R + such that if α < β then F ( α ) < F ( β ) ;
( F 2 )
For each sequence of positive numbers { α n } n N ,
lim n α n = 0 iff lim n F ( α n ) = ;
( F 3 )
There exists k ( 0 , 1 ) such that lim α 0 + α k F ( α ) = 0 .
We represent by F the set of all functions satisfying the conditions ( F 1 ) ( F 3 ) . There is an effort, however, to convert fixed point theorems that are in the theory of topological fixed point theory into non-linear integral equations and differential equations. This effort is spearheaded major developments in related research areas ( see for more info References [6,7,8,9,10,11,12,13]).
Recently, a new kind of generalized metric space was introduced by Kamran et al. [14], as shown below, and named an extended b-metric space (simply, B e -metric space).
Definition 2.
Let X be a non-empty set and s : X × X [ 1 , ) . A function B e : X × X [ 0 , ) is called a B e -metric if, for all x , y , z X , it satisfies:
(i) 
B e ( x , y ) = 0 iff x = y ;
(ii) 
B e ( x , y ) = B e ( y , x ) ;
(iii) 
B e ( x , y ) s ( x , y ) [ B e ( x , z ) + B e ( z , y ) ] .
The pair ( X , B e ) is called a B e -metric space.
Example 1.
Let X = { 1 , 0 , 1 } . Define the function s : X × X R + and B e : X × X R + as s ( x , y ) = 2 + x + y .
B e ( 1 , 1 ) = B e ( 0 , 0 ) = B e ( 1 , 1 ) = 0 ; B e ( 1 , 0 ) = B e ( 0 , 1 ) = 3 ; B e ( 1 , 1 ) = B e ( 1 , 1 ) = 7 ; B e ( 0 , 1 ) = B e ( 1 , 0 ) = 1 .
First, we prove that B e is a B e -metric space. It is clear that (i) and (ii) trivially hold. For (iii), we have
B e ( 1 , 0 ) = 3 ; s ( 1 , 0 ) [ B e ( 1 , 1 ) + B e ( 1 , 0 ) ] = 8 .
Thus,
B e ( 1 , 0 ) s ( 1 , 0 ) [ B e ( 1 , 1 ) + B e ( 1 , 0 ) ] .
B e ( 0 , 1 ) = 1 ; s ( 0 , 1 ) [ B e ( 0 , 1 ) + B e ( 1 , 1 ) ] = 30 .
B e ( 1 , 1 ) = 7 ; s ( 1 , 1 ) [ B e ( 1 , 0 ) + B e ( 0 , 1 ) ] = 8 .
Hence, for all x , y , z X , B e ( x , z ) s ( x , z ) [ B e ( x , y ) + B e ( y , z ) ] .
Hence, ( X , B e ) is a B e -metric space.
Definition 3.
Let ( X , B e ) be a B e -metric space and a sequence { x n } in X is said to
(a) 
Converge to x X iff if for every ϵ > 0 there exists N = N ( ϵ ) N such that B e ( x n , x ) < ϵ , for all n N . For this particular case, we write lim n x n = x .
(b) 
Cauchy iff for every ϵ > 0 there exists N = N ( ϵ ) N such that B e ( x m , x n ) < ϵ , for all m , n N .
Definition 4.
A B e -metric space ( X , B e ) is complete if every Cauchy sequence in X is convergent.
Observe that usually a b-metric is not a continuous functional. Analogously, the functional B e -metric is also not necessarily a continuous function [15,16,17,18,19].
Within the past century, mathematical research has been increasingly drawn towards understanding the link between the Banach contraction principle and non-linear integral equations. The brief and chronological history of these two topics are explored through a developing conceptual model. Since then, many researchers have formulated and developed fixed point approaches of non-linear integral equations in many directions.
Motivated by the above facts, we establish fixed point theorems by using F-contractions in the context of an extended b-metric space since it was very hard to obtain fixed points via the Warkowski [15] approach, which gives a solutions for non-linear integral equations by using the fixed point technique.

2. An Extended F B e -Contraction

Now, we introduce the following definition:
Definition 5.
Let ( X , B e ) be a B e -metric space. A mapping H : X X is said be an extended F B e -contraction if there exists τ > 0 such that for all x , y X ,
B e ( H x , H y ) > 0 τ + F B e ( B e ( H x , H y ) ) F B e ( B e ( x , y ) ) ,
such that for each x 0 X , lim n , m s ( x n , x m ) < 1 k , where k ( 0 , 1 ) , here x n = H n x 0 ; n = 1 , 2 , 3 , and F B e : R + R is a mapping satisfying:
( F 1 )
F B e is strictly increasing, i.e., for all α , β R + such that α < β implies F B e ( α ) < F B e ( β ) ;
( F 2 )
For each sequence { α n } n N of positive numbers lim n α n = 0 iff lim n F B e ( α n ) = ;
( F 3 )
There exists k ( 0 , 1 ) such that lim α 0 + α k F B e ( α ) = 0 .
We denote by F B e the set of all functions satisfying the conditions ( F 1 ) ( F 3 ) .
Theorem 1.
Let ( X , B e ) be a complete B e -metric space such that B e is a continuous functional and let H : X X be an extended F B e -contraction, then H has a fixed point.
Proof. 
In order to show that H has a fixed point, let x 0 X be arbitrary and fixed. We define a sequence { x n } n N X , by
x 0 , H x 0 = x 1 , x 2 = H x 1 = H ( H x 0 ) = H 2 ( x 0 ) x n = H n x 0
Denote γ n = B e ( x n + 1 , x n ) , n = 0 , 1 , 2 , .
If there exists n 0 N for which x n 0 + 1 = x n 0 then H x n 0 = x n 0 and the proof is finished. Suppose now that x n + 1 x n for every n N which yields B e ( x n + 1 , x n ) > 0 , i.e., B e ( H x n , H x n 1 ) > 0 . Thus, by using (3), the following holds for every n N :
F B e ( γ n ) F B e ( γ n 1 ) τ F B e ( γ n 2 ) 2 τ F B e ( γ 0 ) n τ ,
which yields, lim n F B e ( γ n ) = .
By F 2 ,
lim n γ n = 0 .
From F 3 , there exists k ( 0 , 1 ) such that
lim n γ n k F B e ( γ n ) = 0 .
By Equation (4), the following holds for all n N . Thus,
γ n k F B e ( γ n ) γ n k F B e ( γ 0 ) γ n k ( F B e ( γ 0 ) n τ ) γ n k F B e ( γ 0 ) = γ n k n τ 0 .
Letting n in (7) and using (4) and (5), we obtain
lim n n γ n k = 0 .
Now, let us observe that from (8) there exists n 1 N such that n γ n k 1 for all n n 1 .
Consequently, we have
γ n 1 n 1 k for all n n 1 .
In order to prove that { x n } n N is a Cauchy sequence, consider m , n N such that m > n n 1 .
By triangle inequality,
B e ( x n , x m ) s ( x n , x m ) [ B e ( x n , x n + 1 ) + B e ( x n + 1 , x m ) ] s ( x n , x m ) B e ( x n , x n + 1 ) + s ( x n , x m ) s ( x n + 1 , x m ) [ B e ( x n + 1 , x n + 2 ) + B e ( x n + 2 , x m ) ] s ( x n , x m ) B e ( x n , x n + 1 ) + s ( x n , x m ) s ( x n + 1 , x m ) B e ( x n + 1 , x n + 2 ) + + s ( x n , x m ) s ( x n + 1 , x m ) s ( x n + 2 , x m ) s ( x m 2 , x m ) s ( x m 1 , x m ) B e ( x m 1 , x m ) s ( x 1 , x m ) s ( x 2 , x m ) s ( x n , x m ) B e ( x n , x n + 1 ) + s ( x 1 , x m ) s ( x 2 , x m ) s ( x n + 1 , x m ) B e ( x n + 1 , x n + 2 ) + + s ( x 1 , x m ) s ( x 2 , x m ) s ( x m 1 , x m ) B e ( x m 1 , x m ) .
Note that this series
n = 1 B e ( x n , x n + 1 ) i = 1 n s ( x i , x m ) converges .
Since
n = 1 B e ( x n , x n + 1 ) i = 1 n s ( x i , x m ) n = 1 1 n 1 k i = 1 n s ( x i , x m ) < n = 1 1 n 1 k . 1 k = 1 k n = 1 1 n 1 k ; which is convergent .
Let
S = n = 1 B e ( x n , x n + 1 ) i = 1 n s ( x i , x m ) ;
S n = j = 1 n B e ( x j , x j + 1 ) i = 1 j s ( x i , x m ) .
Thus, for m > n , the above inequality implies
B e ( x n , x m ) S m 1 S n 1 .
Letting n , we conclude that { x n } is a Cauchy sequence. Since X is complete, let x n ρ X .
Case 1.
H is continuous, we have
B e ( H ρ , ρ ) = lim n B e ( H x n , x n ) = lim n B e ( x n + 1 , x n ) = 0 .
Thus, H ρ = ρ . Thus ρ is a fixed point of H .
Case 2.
F B e is continuous, in this case, we consider two following subcases:
Case 2.1.
For each n N , there exists i n N such that x i n = H ρ and i n > i n 1 where i = 0 . Then, we have ρ = lim n x i n = lim n H ρ = H ρ , which yields that ρ is a fixed point of H .
Case 2.2.
There exists n 0 N such that x n + 1 H ρ for al n n 0 . That is B e ( H x n , H ρ ) > 0 for all n n 0 .
It follows from (3) that
τ + F B e ( B e ( x n + 1 , H ρ ) ) = τ + F B e ( B e ( H x n , H ρ ) ) F B e ( B e ( x n , ρ ) ) .
Since F B e is continuous, taking the limit as n , then we obtain
τ + F B e ( B e ( ρ , H ρ ) ) F B e ( B e ( ρ , ρ ) )
F B e ( B e ( ρ , ρ ) ) F B e ( B e ( ρ , ρ ) ) τ ,
which is a contradiction due to F 1 . Therefore, B e ( ρ , H ρ ) = 0 . Hence, ρ is a fixed point of H .
Thus, from above two cases, we can conclude that H has a fixed point ρ . Hence, H ρ = ρ .
In order to prove uniqueness, first, let us observe that H has at most one fixed point. Indeed, if x 1 , x 2 X , H x 1 = x 1 x 2 = H x 2 , then B e ( x 1 , x 2 ) > 0 , i.e., B e ( H x 1 , H x 2 ) > 0 . From (3), we get
τ F B e ( B e ( H x 1 , H x 2 ) ) F B e ( B e ( x 1 , x 2 ) ) ,
τ F B e ( B e ( x 1 , x 2 ) ) F B e ( B e ( x 1 , x 2 ) ) = 0 ,
which is a contradiction. Hence, H has a unique fixed point. □
Example 2.
Let X = { 1 5 n 1 ; n N } { 0 } . Define B e : X × X R + by B e ( x , y ) = ( x y ) 2 and s : X × X [ 1 , ) as s ( x , y ) = 1 + x + y . Then, ( X , B e ) is a complete B e -metric space.
Define H : X X by
H ( x ) = { 1 5 2 n } , if x { 1 5 2 n 1 ; n N } 0 , if x = 0 .
Define the function F B e : R + R by F B e ( α ) = ln α for all α R + and τ > 0 .
Case 1.
Let x = 1 5 2 n 1 , y = 1 5 2 m 1 , for m > n 1 .
Consider
F B e ( B e ( H x , H y ) ) = F B e H 1 5 2 n 1 , H 1 5 2 m 1 = F B e B e 1 5 2 n , 1 5 2 m = F B e 1 5 2 n 1 5 2 m 2 = F B e 5 2 m 5 2 n 5 2 n + 2 m 2 = ln 5 2 m 5 2 n 5 2 n + 2 m 2 = 2 ln 5 2 m 5 2 n 5 2 n + 2 m .
F B e ( B e ( x , y ) ) = F B e 1 5 2 n 1 , 1 5 2 m 1 = F B e 1 5 2 n 1 1 5 2 m 1 2 = F B e 5 2 m 1 5 2 n 1 5 2 n + 2 m 2 2 = ln 5 2 m 1 5 2 n 1 5 2 n + 2 m 2 2 = 2 ln 5 2 m 1 5 2 n 1 5 2 n + 2 m 2 .
Consider
F B e ( B e ( H x , H y ) ) F B e ( B e ( x , y ) ) = 2 ln 5 2 m 5 2 n 5 2 n + 2 m ln 5 2 m 1 5 2 n 1 5 2 n + 2 m 2 = 2 ln 5 2 m 5 2 n 5 2 n + 2 m × 5 2 n + 2 m 2 5 2 m 1 5 2 n 1 = 2 ln 5 2 m 5 2 n 5 2 n + 2 m × 5 2 n + 2 m . 5 2 5 1 ( 5 2 m 5 2 n ) = 2 ( ln ( 1 5 ) ) < 3 .
Thus, H is an extended F B e contraction for τ = 3 .
Case 2.
Let x = 1 5 2 n 1 ; y = 0 .
H x = 1 5 2 n ; H y = 0 .
Consider
F B e ( B e ( H x , H y ) ) = F B e B e 1 5 2 n , 0 = F B e 1 5 4 n = ln 1 5 4 n .
Now consider
F B e ( B e ( x , y ) ) = F B e B e 1 5 2 n 1 , 0 = F B e 1 5 4 n 2 = ln 1 5 4 n 2 .
Now take
F B e ( B e ( H x , H y ) ) F B e ( B e ( x , y ) ) = ln 1 5 4 n ln 1 5 4 n 2 = ln 5 4 n 2 5 4 n = ln 1 5 2 = ln 1 25 < 3 .
For τ = 3 , H satisfied all the conditions of the above theorem and 0 is the unique fixed point.
Similarly, for x = 0 and 1 5 2 n 1 , the same proof follows as above. Hence, all the conditions of the above theorem are satisfied for all the cases and 0 is the unique fixed point.
Example 3.
Let X = { 1 , 0 , 1 } . Define the function s : X × X [ 1 , ) by s ( x , y ) = 2 + x + y and B e : X × X R + as:
B e ( 1 , 1 ) = B e ( 0 , 0 ) = B e ( 1 , 1 ) = 0 ;
B e ( 1 , 0 ) = B e ( 0 , 1 ) = 3 ;
B e ( 1 , 1 ) = B e ( 1 , 1 ) = 7 ;
B e ( 0 , 1 ) = B e ( 1 , 0 ) = 1 .
It is clear that ( X , B e ) is a complete B e -metric space.
Let H : X X given by H 0 = 0 = H 1 , H ( 1 ) = 1 . Define F B e : R + R by F B e ( α ) = 1 α + α and τ ( 0 , 2 ] .
Case 1.
Let x = 0 . Now, B e ( H 0 , H 1 ) = B e ( H 0 , H 0 ) = B e ( 0 , 0 ) = 0 . Therefore, we only need to consider y = 1 .
Now, B e ( H 0 , H ( 1 ) ) = B e ( 0 , 1 ) = 1 and B e ( 0 , 1 ) = 3 .
Consider
τ + F B e ( B e ( H 0 , H ( 1 ) ) ) = τ 1 B e ( H 0 , H ( 1 ) ) + ( B e ( H 0 , H ( 1 ) ) = τ 1 + 1 = τ
F B e ( B e ( 0 , 1 ) ) = 1 B e ( 0 , 1 ) + B e ( 0 , 1 ) = 1 3 + 3 = 3 1 3 = 8 3 .
Clearly for τ ( 0 , 1 2 ) ,
τ + F B e ( B e ( H 0 , H ( 1 ) ) ) F B e ( B e ( 0 , 1 ) ) .
Case 2.
Let x = 1 . Now, B e ( H 1 , H 1 ) = B e ( H 1 , H 0 ) = 0 . Therefore, we only need to consider y = 1 .
Now, B e ( H 1 , H ( 1 ) ) = B e ( 0 , 1 ) = 1 and B e ( 1 , 1 ) = 7 .
Consider
τ + F B e ( B e ( H 1 , H ( 1 ) ) ) = τ 1 B e ( H 1 , H ( 1 ) ) + ( B e ( H 1 , H ( 1 ) ) = τ 1 + 1 = τ .
F B e ( B e ( 1 , 1 ) ) = 1 B e ( 1 , 1 ) + B e ( 1 , 1 ) = 1 7 + 7 = 7 1 7 = 48 7 .
Clearly for τ ( 0 , 1 2 ) ,
τ + F B e ( B e ( H 1 , H ( 1 ) ) ) F B e ( B e ( 1 , 1 ) ) .
For x = 1 , the proof is similar as above cases. Hence, all the conditions of the Theorem 1 are satisfied and 0 is the unique fixed point. Thus, the above examples illustrate the above theorem.

3. An Extended F B e -Expanding Contraction

We start this section by introducing following definition:
Definition 6.
Let ( X , B e ) be a B e -metric space. A mapping H : X X is said to be an extended expanding if
x , y X B e ( H x , H y ) κ B e ( x , y ) ; w h e r e κ > 1 .
Theorem 2.
Let ( X , B e ) be a complete B e -metric space such that B e is a continuous functional. Let H : X X be surjective and extended expanding. Then, H is bijective and has a unique fixed point.
Proof. 
First, we will prove that H is bijective. For this, we need to prove H is injective.
Let x , y X with x y . From the definition of extended expanding,
B e ( H x , H y ) κ B e ( x , y ) > 0 .
which yields H x H y . Hence, H is bijective.
Since H is bijective, H has an inverse on its range. Note that H 1 is a Banach contraction in the setting of an B e -metric space. In addition, since 1 κ < 1 , we can conclude that H 1 has a unique fixed point by using Theorem 3 of Kamran et al. [13]. This completes the proof of the theorem. □
Theorem 3.
Let ( X , B e ) be a complete B e -metric space such that B e is a continuous functional. If H : X X is surjective then there exists a mapping H * : X X such that H H * is the identity map on X.
The proof is omitted as it is easy to prove.
Now, we define a new definition.
Definition 7.
Let ( X , B e ) be a complete B e -metric space. A mapping H is said to be extended F-expanding if there exists F F * and τ > 0 such that for all x , y X ,
B e ( x , y ) > 0 F B e ( B e ( H x , H y ) ) F B e ( B e ( x , y ) ) + τ
where F B e : ( 0 , + ) R is a mapping satisfying:
( F 1 )
F B e is strictly increasing, i.e., for all α , β R + such that if α < β then F B e ( α ) < F B e ( β ) ;
( F 2 )
For each sequence { α n } ( 0 , + ) , then
lim n α n = 0 lim n F B e ( α n ) = ;
( F 3 )
There exists k ( 0 , 1 ) such that lim α 0 + α k F B e ( α ) = 0 .
We represent by F * the set of all functions satisfying the conditions ( F 1 ) ( F 3 ) .
Theorem 4.
Let ( X , B e ) be a complete B e -metric space such that B e is a continuous functional. Let H : X X be surjective and extended F-expanding. Then, H has a unique fixed point.
Proof. 
From Theorem 3, there exists a mapping H * : X X such that H H * is the identity mapping on X.
Let x , y X be arbitrary points such that x y , and let η = H * x and ξ = H * y (obviously η ξ ) which yields B e ( η , ξ ) > 0 .
From the definition of extended F-expanding, we get
F B e ( B e ( H η , H ξ ) ) F B e ( B e ( η , ξ ) ) + τ .
Since H η = H ( H * x ) = x and H ξ = H ( H * y ) = y , then
F B e ( B e ( x , y ) ) F B e ( B e ( H * x , H * y ) ) + τ .
Therefore, H * : X X is an extended F-contraction. By Theorem 1, H * has a unique fixed point δ X .
Now consider
H δ = H ( H * δ ) = δ
Hence, δ is also a fixed point of H .
In order to get uniqueness, let us suppose that H has at most two fixed points. If δ 1 , δ 2 X and H δ 1 = δ 1 δ 2 = H δ 2 , then B e ( δ 1 , δ 2 ) > 0 which yields
F B e ( B e ( H δ 1 , H δ 2 ) ) F B e ( B e ( δ 1 δ 2 ) ) + τ
0 = F B e ( B e ( H δ 1 , H δ 2 ) ) F B e ( B e ( δ 1 δ 2 ) ) τ > 0 ,
which is a contradiction. Thus, δ 1 = δ 2 . Therefore, the fixed point of H is unique. □
Remark 1.
If H is not surjective, the above theorem is false.
For example, let X = [ 0 , 1 ] . Define B e ( x , y ) : X × X R + and s : X × X [ 1 , ) as B e ( x , y ) = ( x y ) 2 , s ( x , y ) = x + y + 1 .
Then, B e is a complete B e -metric space on X . Define H : X X by H x = 2 x + 1 for all x X . Then,
B e ( H x , H y ) = B e ( 2 x + 1 , 2 y + 1 ) = ( 2 x 2 y ) 2 = 4 ( x y ) 2 > B e ( x , y ) .
Thus, H satisfies all the conditions of the theorem but H has no fixed point.
If s ( x , y ) = 1 , then the above theorem will reduce to Theorem 2.1 of Jaroslaw Gornicki [7]. Thus, we can conclude that our theorem is a standard generalization of Theorem 2.1 of Jaroslaw Gornicki [7].

4. An Extended Generalized F B e -Contraction

Definition 8.
Let ( X , B e ) be a B e -metric space. A map H : X X is said to be an extended generalized F B e -contraction on ( X , B e ) if there exists F F * and τ > 0 such that for all x , y X satisfying B e ( H x , H y ) > 0 , the following holds:
τ + F B e ( B e ( H x , H y ) ) F B e max B e ( x , y ) , B e ( x , H x ) 1 + B e ( x , H x ) , B e ( y , H y ) 1 + B e ( y , H y ) , B e ( x , H x ) + B e ( y , H y ) 2 ,
and for each x 0 X , lim n , m s ( x n , x m ) < 1 k , where k ( 0 , 1 ) . Here x n = H n x 0 ; n = 1 , 2 , 3 , .
Remark 2.
1.
Every F -contraction is an extended generalized F B e -contraction.
2.
Let H be an extended generalized F B e -contraction and from the definition of extended generalized F B e -contractions we have for all x , y X , H x H y , which gives B e ( H x , H y ) > 0 . Thus,
F B e ( B e ( H x , H y ) ) < τ + F B e ( B e ( H x , H y ) ) F B e max B e ( x , y ) , B e ( x , H x ) 1 + B e ( x , H x ) , B e ( y , H y ) 1 + B e ( y , H y ) , B e ( x , H x ) + B e ( y , H y ) 2 .
Then, by ( F 1 ) , we get
B e ( H x , H y ) max B e ( x , y ) , B e ( x , H x ) 1 + B e ( x , H x ) , B e ( y , H y ) 1 + B e ( y , H y ) , B e ( x , H x ) + B e ( y , H y ) 2 ;
x , y X , H x H y .
Counter example for Remark: The following example shows that the inverse implication of the remark does not hold. Let X = [ 0 , ) define B e : X × X R by B e ( x , y ) = ( x y ) 2 and s : X × X [ 1 , ) by s ( x , y ) = x + y + 1 . Then, B e is an B e -metric. Define H : X X as
H x = 0 , if 0 x < 1 1 4 , if x 1 .
Clearly H is not continuous.
Thus, H is not an F -contraction. For x [ 0 , 1 ) and y = 1 we have B e ( H x , H 1 ) = B e ( 0 , 1 4 ) = 1 16 > 0 and
max B e ( x , 1 ) , B e ( x , H x ) 1 + B e ( x , H x ) , B e ( 1 , H 1 ) 1 + B e ( 1 , H 1 ) , B e ( x , H x ) + B e ( 1 , H 1 ) 2 B e ( 1 , H 1 ) = B e ( 1 , 1 4 ) = 9 16 > 1 16 = B e ( H x , H 1 ) .
Define the function F B e : R + R by F B e ( α ) = ln α , α R + & τ > 0 . Then consider
F B e ( B e ( H x , H 1 ) ) F B e ( B e ( 1 , H 1 ) ) = F B e ( 1 16 ) F B e ( 9 16 ) = ln ( 1 16 ) ln ( 9 16 ) = ln ( 1 16 ) × ( 16 9 ) = ln 1 9 < 2 .
Thus, H is an extended generalized F B e -contraction for τ = 2 .
Theorem 5.
Let ( X , B e ) be a B e -metric space such that B e is a continuous functional and H : X X be an extended generalized F B e -contraction. Then, H has a unique fixed point.
Proof. 
Let x X be arbitrary and fixed. We define x n + 1 = H x n ; n N { 0 } , where x 0 = x . If there exists n 0 N { 0 } such that x n 0 + 1 = x n 0 , then H x n 0 = x n 0 . This concludes that x n 0 is a fixed point of H .
Let us suppose that x n + 1 x n for all n N { 0 } . Which gives B e ( x n + 1 , x n ) > 0 . It follows from extended generalized F B e -contraction that for each n N .
F B e ( B e ( x n + 1 , x n ) ) = F B e ( B e ( H x n , H x n 1 ) ) F B e ( max { B e ( x n , x n 1 ) , B e ( x n , x n + 1 ) 1 + B e ( x n , x n + 1 ) , B e ( x n 1 , x n ) 1 + B e ( x n 1 , x n ) , B e ( x n , x n + 1 ) + B e ( x n 1 , x n ) 2 } ) τ F B e ( max { B e ( x n , x n 1 ) , B e ( x n , x n + 1 ) , B e ( x n 1 , x n ) , B e ( x n , x n + 1 ) + B e ( x n 1 , x n ) 2 } ) τ F B e max B e ( x n , x n 1 ) , B e ( x n , x n + 1 ) τ .
If B e ( x n + 1 , x n ) = B e ( x n , x n + 1 ) then F B e ( B e ( x n + 1 , x n ) ) F B e ( B e ( x n , x n + 1 ) ) τ , which is a contradiction due to F 1 .
Thus,
F B e ( B e ( x n + 1 , x n ) ) F B e ( B e ( x n , x n 1 ) ) τ ; n N { 0 } .
Similarly,
F B e ( B e ( x n , x n 1 ) ) F B e ( B e ( x n 1 , x n 2 ) ) τ ; n N { 0 } .
By using (20)&(21), we have
F B e ( B e ( x n + 1 , x n ) ) F B e ( B e ( x n 1 , x n 2 ) ) 2 τ .
By repeating same scenario, we get
F B e ( B e ( x n + 1 , x n ) ) F B e ( B e ( x 1 , x 0 ) ) n τ ; n N { 0 } .
Taking the limit as n in (23), we get
lim n F B e ( B e ( x n + 1 , x n ) ) = .
By using ( F 2 ) , we get
lim n B e ( x n + 1 , x n ) = 0 .
From ( F 3 ) , there exists k ( 0 , 1 ) such that
lim n ( B e ( x n + 1 , x n ) ) k F B e ( B e ( x n + 1 , x n ) ) = 0 .
Now consider
( B e ( x n + 1 , x n ) ) k ( F B e ( B e ( x n + 1 , x n ) ) F B e ( B e ( x 1 , x 0 ) ) ) ( B e ( x n + 1 , x n ) ) k n τ 0 ; n N .
By using (25)&(26) and taking the limit as n in (27), we get
lim n n ( B e ( x n + 1 , x n ) ) k = 0 .
Then, there exists n 1 N such that n ( B e ( x n + 1 , x n ) ) k 1 ; n n 1 , which yields
B e ( x n + 1 , x n ) 1 n 1 k ; n n 1 .
In order to prove that { x n } is a Cauchy sequence, consider m , n N such that m > n n 1 . By using (29) and the triangle inequality, we get
B e ( x n , x m ) s ( x n , x m ) [ B e ( x n , x n + 1 ) + B e ( x n + 1 , x m ) ] s ( x n , x m ) B e ( x n , x n + 1 ) + s ( x n , x m ) s ( x n + 1 , x m ) [ B e ( x n + 1 , x n + 2 ) + B e ( x n + 2 , x m ) ] s ( x n , x m ) B e ( x n , x n + 1 ) + s ( x n , x m ) s ( x n + 1 , x m ) B e ( x n + 1 , x n + 2 ) + + s ( x n , x m ) s ( x n + 1 , x m ) s ( x n + 2 , x m ) s ( x m 2 , x m ) s ( x m 1 , x m ) B e ( x m 1 , x m ) s ( x 1 , x m ) s ( x 2 , x m ) s ( x n , x m ) B e ( x n , x n + 1 ) + s ( x 1 , x m ) s ( x 2 , x m ) s ( x n + 1 , x m ) B e ( x n + 1 , x n + 2 ) + + s ( x 1 , x m ) s ( x 2 , x m ) s ( x m 1 , x m ) B e ( x m 1 , x m ) .
Note that this series
n = 1 B e ( x n , x n + 1 ) i = 1 n s ( x i , x m ) converges .
Since
n = 1 B e ( x n , x n + 1 ) i = 1 n s ( x i , x m ) n = 1 1 n 1 k i = 1 n s ( x i , x m ) < n = 1 1 n 1 k . 1 k = 1 k n = 1 1 n 1 k ; which is convergent .
Let
S = n = 1 B e ( x n , x n + 1 ) i = 1 n s ( x i , x m ) ;
S n = j = 1 n B e ( x j , x j + 1 ) i = 1 j s ( x i , x m ) .
Thus, for m > n above inequality implies
B e ( x n , x m ) S m 1 S n 1 .
Letting n , we conclude that { x n } is a Cauchy sequence. Hence, there exists κ X such that { x n } κ .
We shall prove that κ is a fixed point of H by two following cases:
Case 1.
H is continuous, we have
B e ( κ , H κ ) = lim n B e ( x n , H x n ) = lim n B e ( x n , x n + 1 ) = 0 .
This proves that κ is a fixed point of H .
Case 2.
F B e is continuous. In this case, we consider two following sub-cases:
Case 2.1.
For each n N , there exists i n N such that x i n + 1 = H κ and i n > i n 1 where i 0 = 1 . Then, we have
κ = lim n x i n + 1 = lim n H κ = H κ .
This proves that κ is a fixed point of H .
Case 2.2.
There exists n 0 N such that x n + 1 H κ ; n n 0 .
i . e , B e ( H x n , H κ ) > 0 ; n n 0 .
It follows from extended generalized F B e -contraction and F 1 ,
τ + F B e ( B e ( x n + 1 , H κ ) ) = τ + F B e ( B e ( H x n , H κ ) ) F B e ( max { B e ( x n , κ ) , B e ( x n , H x n ) 1 + B e ( x n , H x n ) , B e ( κ , H κ ) 1 + B e ( κ , H κ ) , B e ( x n , H x n ) + B e ( κ , H κ ) 2 } ) F B e ( max { B e ( x n , κ ) , B e ( x n , x n + 1 ) , B e ( κ , H κ ) , B e ( x n , H x n ) + B e ( κ , H κ ) 2 } ) F B e ( max { B e ( x n , κ ) , B e ( x n , x n + 1 ) , B e ( κ , H κ ) , B e ( x n , x n + 1 ) + B e ( κ , H κ ) 2 } ) .
If B e ( κ , H κ ) > 0 then lim n B e ( x n , κ ) = lim n B e ( κ , x n + 1 ) = 0 .
Then, there exists n 1 N such that for all n n 1 , we have
max B e ( x n , κ ) , B e ( x n , x n + 1 ) , B e ( κ , H κ ) , B e ( x n , x n + 1 ) + B e ( κ , H κ ) 2 = B e ( κ , H κ ) .
From (33), we get
τ + F B e ( B e ( x n + 1 , H κ ) ) F B e ( B e ( κ , H κ ) ) ; n max { n 0 , n 1 } .
Since F B e is continuous, taking the limit as n in ( 34 ) , we obtain
τ + F B e ( B e ( κ , H κ ) ) F B e ( B e ( κ , H κ ) ) ,
which is a contradiction. Hence, B e ( κ , H κ ) = 0 . Therefore, κ is a fixed point of H .
By the above two cases, H has a fixed point κ.
To prove uniqueness, let κ , κ * be two fixed points of H , such that κ κ * .
Thus, B e ( κ , κ * ) > 0 which implies B e ( H κ , H κ * ) > 0 .
From extended generalized F-contraction,
τ + F B e ( B e ( κ , κ * ) ) = τ + F B e ( B e ( H κ , H κ * ) ) F B e ( max { B e ( κ , κ * ) , B e ( κ , H κ ) 1 + B e ( κ , H κ ) , B e ( κ * , H κ * ) 1 + B e ( κ * , H κ * ) , B e ( κ , H κ ) + B e ( κ * , H κ * ) 2 } ) = F B e max B e ( κ , κ * ) , B e ( κ , κ ) 1 + B e ( κ , κ ) , B e ( κ * , κ * ) 1 + B e ( κ * , κ * ) = F B e ( B e ( κ , κ * ) ) .
which implies, τ F B e ( B e ( κ , κ * ) ) F B e ( B e ( κ , κ * ) ) = 0 . This is a contradiction.
Thus, B e ( κ , κ * ) = 0 , which yields κ = κ * . Hence, the fixed point of H is unique. □
Example 4.
Let X = 1 2 n 1 ; n N { 0 } . Define B e : X × X R + by B e ( x , y ) = ( x y ) 2 and s : X × X [ 1 , ) as s ( x , y ) = x + y + 1 . Then, B e is a complete B e -metric on X.
Define H : X X by
H ( x ) = 1 2 n , if x 1 2 n 1 ; n N ; 0 , if x X .
Define the function F B e : R + R by F B e ( α ) = ln α for all α R + and τ > 0 .
Case 1.
For m > n 1 . Let x = 1 2 n 1 and y = 1 2 m 1 .
Now take n = 1 and m = 2 .
Consider
F B e ( B e ( H x , H y ) ) = F B e ( B e ( H 1 , H 1 2 ) ) = F B e ( B e ( 1 2 , 1 4 ) ) = F B e ( 1 16 ) = ln 1 16 = 2.7725 .
Additionally,
F B e max B e ( x , y ) , B e ( x , H x ) 1 + B e ( x , H x ) , B e ( y , H y ) 1 + B e ( y , H y ) , B e ( x , H x ) + B e ( y , H y ) 2 = F B e max B e ( 1 , 1 2 ) , B e ( 1 , 1 2 ) 1 + B e ( 1 , 1 2 ) , B e ( 1 2 , 1 2 ) 1 + B e ( 1 2 , 1 2 ) , B e ( 1 , 1 2 ) + B e ( 1 2 , 1 4 ) 2 = F B e max 1 4 , 1 5 , 1 17 , 5 16 = F B e ( 5 16 ) = ln 5 16 = 1.1631 .
Consider
F B e ( B e ( H x , H y ) ) F max B e ( x , y ) , B e ( x , H x ) 1 + B e ( x , H x ) , B e ( y , H y ) 1 + B e ( y , H y ) , B e ( x , H x ) + B e ( y , H y ) 2 = 2.7725 + 1.1631 = 1.6094 < 1 .
Thus, H is an extended generalized F B e -contraction for τ = 1 .
Case 2.
Let x = 1 2 and y = 0 .
Consider F B e ( B e ( H x , H y ) ) = F B e ( B e ( 1 4 , 0 ) ) = F B e ( 1 16 ) = ln 1 16 = 2 . 77 .
Now,
F B e max B e ( x , y ) , B e ( x , H x ) 1 + B e ( x , H x ) , B e ( y , H y ) 1 + B e ( y , H y ) , B e ( x , H y ) + B e ( y , H x ) 2 = F B e max B e ( 1 2 , 0 ) , B e ( 1 2 , 1 4 ) 1 + B e ( 1 2 , 1 4 ) , B e ( 0 , 0 ) 1 + B e ( 0 , 0 ) , B e ( 1 2 , 1 4 ) + B e ( 0 , 0 ) 2 = F B e max 1 4 , 1 17 , 0 , 1 32 = F B e ( 1 4 ) = ln 1 4 = 1.38 .
Now consider
F B e ( B e ( H x , H y ) ) F max B e ( x , y ) , B e ( x , H x ) 1 + B e ( x , H x ) , B e ( y , H y ) 1 + B e ( y , H y ) , B e ( x , H x ) + B e ( y , H y ) 2 = 2.77 + 1.38 = 1.39 < 1 .
Thus, H is an extended generalized F B e -contraction for τ = 1 .
Hence, we can conclude that all the conditions of above theorem are satisfied in all cases and 0 is the unique fixed point.

5. Applications to Existence of Solutions of Non-linear Integral Equation

As applications, we use Theorem 1 and Theorem 5 to study the existence problem of unique solutions of non-linear integral equations.
Theorem 6.
Let X be the set of all continuous real valued functions defined on [ a , b ] . i . e . , X = C ( [ a , b ] , R ) .
Define B e : X × X R by B e ( U , V ) = s u p | U ( t ) V ( t ) | 2 , t [ a , b ] with s ( U , V ) = | U ( t ) | + | V ( t ) | + 1 , where s : X × X [ 1 , ) .
Note that ( X , B e ) is a complete B e -metric space.
Consider the Fredholm integral equation as
U ( t ) = a b H ( t , p , U ( p ) ) d p + F B e ( t ) t , p [ a , b ] ,
where F B e : [ a , b ] R and H : [ a , b ] × [ a , b ] × R R are continuous functions.
Define H : A B A B by H ( U ( t ) ) = a b H ( t , p , U ( p ) ) d p + F B e ( t ) t , p [ a , b ] ; where F B e : [ a , b ] R and H : [ a , b ] × [ a , b ] × R R are continuous functions.
Further assume that the following condition holds:
| H ( t , p , U ( p ) ) H ( t , p , V ( p ) ) | e τ 2 | U ( p ) V ( p ) |
for each t , p [ a , b ] , U , V X and τ > 0 . Then, the integral Equation (35) has a solution. We will prove that the operator H satisfies the conditions of Theorem 1.
For any U ( t ) , V ( t ) X . Consider
| H U ( t ) H V ( t ) | 2 = a b | H ( t , p , U ( p ) ) H ( t , p , V ( p ) ) | 2 d p a b e τ 2 | U ( p ) V ( p ) | 2 d p e τ a b | U ( p ) V ( p ) | 2 d p e τ B e ( U ( t ) , V ( t ) ) ,
which implies B e ( H U ( t ) , H V ( t ) ) e τ B e ( U ( t ) , V ( t ) ) .
Applying logarithms on both sides, we get
ln ( B e ( H U ( t ) , H V ( t ) ) ) ln ( e τ B e ( U ( t ) , V ( t ) ) ) ;
ln ( B e ( H U ( t ) , H V ( t ) ) ) ln ( e τ ) + ln ( B e ( U ( t ) , V ( t ) ) ) ;
ln ( B e ( H U ( t ) , H V ( t ) ) ) τ + ln ( B e ( U ( t ) , V ( t ) ) ) .
Thus,
τ + ln ( B e ( H U ( t ) , H V ( t ) ) ) ln ( B e ( U ( t ) , V ( t ) ) ) .
Let us define F B e : R + R by F B e ( α ) = ln ( α ) , α > 0 . Then, from (36), we get
τ + F B e ( B e ( H U ( t ) , H V ( t ) ) ) F ( B e ( U ( t ) , V ( t ) ) ) .
Thus all the conditions of the Theorem 1 are satisfied. Thus, the operator H has a unique fixed point. Hence, the Fredholm integral equation has a solution.
Theorem 7.
Let us consider the non-linear integral equation.
U ( t ) = F B e ( t ) + 0 t k ( t , p ) g ( p , U ( p ) ) d p ,
where the unknown function U ( t ) takes real values.
Let X = C ( [ 0 , β ] ) be the space of all real continuous functions defined on [ 0 , β ] .
Define B e : X × X R by B e ( U , V ) = max t [ 0 , β ] | U ( t ) V ( t ) | 2 and s : X × X [ 1 , ) by s ( U , V ) = | U ( t ) | + | V ( t ) | + 1 .
Clearly, ( X , B e ) is a complete B e -metric space.
Define a mapping H : X X by H U ( t ) = F B e ( t ) + 0 t k ( t , p ) g ( p , U ( p ) ) d p ; t [ 0 , β ] .
Furthermore, we assume the following conditions:
  • g C ( [ 0 , β ] × ( , ) ) and k C ( [ 0 , β ] × [ 0 , β ] ) such that k ( t , p ) 0 .
  • g ( t , . ) : ( , + ) ( , + ) is increasing for all t [ 0 , β ] .
  • There exists τ [ 1 , + ) such that for all U , V X , t [ 0 , β ] , | g ( t , U ) g ( t , V ) | 2 τ e τ M ( U , V ) ,
    where, M ( U , V ) = max | U V | 2 , | U H U | 2 1 + | U H U | 2 , | V H V | 2 1 + | V H V | 2 , | U H U | 2 + | V H V | 2 2 .
  • max t , p [ 0 , β ] | k ( t , s ) | 2 1 ; For U X , we define a norm | | U | | τ = max t [ 0 , β ] | U ( t ) | e τ t , where t 1 is chosen arbitrarily.
It is easy to check that . τ is equivalent to the maximum norm . in X, and X be endowed with the B e τ defined by
B e τ ( U , V ) = | | U V | | τ = max t [ 0 , β ] { | U ( t ) V ( t ) | 2 e τ t } ; U , V X and e t τ 1 .
Then, ( X , B e τ ) is a complete B e -metric space.
Now, we will prove that the non-linear integral Equation (37) has a unique solution. For any U , V C ( [ 0 , β ] ) , t [ 0 , β ] we have
| H U ( t ) H V ( t ) | 2 = | 0 t k ( t , p ) [ g ( p , U ( p ) ) g ( p , V ( p ) ) ] d p | 2 0 t | k ( t , p ) | 2 | | g ( p , U ( p ) ) g ( p , V ( p ) ) | 2 d p 0 t | | g ( p , U ( p ) ) g ( p , V ( p ) ) | 2 d p 0 t τ e τ M ( U ( p ) , V ( p ) ) d p = τ e τ 0 t e p τ max { | U ( p ) V ( p ) | 2 e p τ , | U ( p ) H U ( p ) | 2 e 2 p τ 1 + | U ( p ) H U ( p ) | 2 e p τ , | V ( p ) H V ( p ) | 2 e 2 p τ 1 + | V ( p ) H V ( p ) | 2 e p τ , | U ( p ) H U ( p ) | 2 + | V ( p ) H V ( p ) | 2 2 e p τ } d p τ e τ 0 t e s τ max { B e τ ( U , V ) , B e τ ( U , H U ) 1 + B e τ ( U , H U ) , B e τ ( V , H V ) 1 + B e τ ( V , H V ) , B e τ ( U , H U ) + B e τ ( V , H V ) 2 } d p = τ e τ M ( U , V ) 0 t e s τ d p τ e τ M ( U , V ) e t τ τ e τ M ( U , V ) e t τ e ( 1 t ) τ M ( U , V )
which implies
| H U ( t ) H V ( t ) | 2 e t τ e τ M ( U , V ) ,
which yields
B e τ ( H U , H V ) = max t [ 0 , β ] { | H U ( t ) H V ( t ) | 2 e t τ } e τ M ( U , V ) .
Applying logarithms on both sides, we get
τ + ln B e τ ( H U , H V ) ln M ( U , V ) ; U , V X .
Define F B e : R + R by F B e ( α ) = ln α , α > 0 . Then, from ( 41 ) we get
τ + F B e ( B e τ ( H U , H V ) ) F B e ( M ( U , V ) ) ;
where M ( U , V ) = max B e τ ( U , V ) , B e τ ( U , H U ) 1 + B e τ ( U , H U ) , B e τ ( V , H V ) 1 + B e τ ( V , H V ) , B e τ ( U , H U ) + B e τ ( V , H V ) 2 .
Thus, H is an extended generalized F-contraction. By Theorem 5, H has a unique fixed point. Hence, it is the unique solution of the non-linear integral equation.

6. Conclusions

The research topic of fixed point theory and applications, with an extended approach being the latest, has continued for decades.
An extended b-metric space was introduced in 2017 by Kamran et al. [14]. Since then, very few researchers established fixed point theorems using F-contractions in an extended b-metric space since it was very hard to obtain fixed points via the Warkowski [15] approach. In this article, we first introduce various topics called the extended F B e -contraction, the extended F B e -expanding contraction, and the extended generalized F B e -contraction. Thereafter, we presented various fixed point theorems related to F-contractions, which gives a solutions for a non-linear integral equation by using the fixed point technique. Our results are important as they open new research avenues for non-linear analysis and its applications.

Author Contributions

All authors contributed equally and significantly in writing this article. All authors read and approved the final manuscript.

Funding

This research received no external funding.

Acknowledgments

The authors would like to thank the editor and referees for careful reading the original manuscript and giving comments which were useful for improving the manuscript.

Conflicts of Interest

The authors declare that they have no competing interests.

References

  1. Fredholm, E.I. Sur une classe d’equations fonctionnelles. Acta Math. 1903, 27, 365–390. [Google Scholar] [CrossRef]
  2. Rus, M.D. A note on the existaence of positive solution of Fredholm integral equations. Fixed Point Theory 2004, 5, 369–377. [Google Scholar]
  3. Berenguer, M.I.; Munoz, M.V.F.; Guillem, A.I.G.; Galan, M.R. Numerical Treatment of Fixed Point Applied to the Nonlinear Fredholm Integral Equation. Fixed Point Theory Appl. 2009, 2009, 735638. [Google Scholar] [CrossRef] [Green Version]
  4. Shahi, P.; Kaur, J.; Bhatia, S.S. Fixed point theorems for (α,ϕ) -contractive mappings of rational type in complex valued metric spaces with applications. Results Fixed Point Theory Appl. 2018, 2018, 20187. [Google Scholar] [CrossRef]
  5. Rasham, T.; Shoaib, A.; Hussain, N.; Arshad, M.; Khan, S.U. Common fixed point results for new Ciric-type rational multivalued F-contraction with an application. J. Fixed Point Theory Appl. 2018, 20, 45. [Google Scholar] [CrossRef]
  6. Wardowski, D. Fixed point theory of a new type of contractive mappings in complete metric spaces. Fixed Point Theory Appl. 2012, 2012, 94. [Google Scholar] [CrossRef]
  7. Gornicki, J. Fixed points theorems for F-expanding mappings. Fixed Point Theory Appl. 2017, 2017, 10. [Google Scholar] [CrossRef]
  8. Piri, H.; Kumam, P. Some fixed point theorems concerning F-contraction in complete metric spaces. Fixed Point Theory Appl. 2014, 2014, 210. [Google Scholar] [CrossRef] [Green Version]
  9. Singh, D.; Chauhan, V.; Kumam, P.; Joshi, V. Some applications of fixed point results for generalized two classes of Boyd–Wong’s F-contraction in partial b-metric spaces. Math. Sci. 2018, 12, 111–127. [Google Scholar] [CrossRef] [Green Version]
  10. Kumari, P.S.; Zoto, K.; Panthi, D. d-Neighborhood system and generalized F-contraction in dislocated metric space. SpringerPlus 2015, 4, 368. [Google Scholar] [CrossRef] [PubMed]
  11. Kumari, P.S.; Panthi, D. Connecting various types of cyclic contractions and contractive self-mappings with Hardy-Rogers self-mappings. Fixed Point Theory Appl. 2016, 2016, 15. [Google Scholar] [CrossRef]
  12. Kumari, P.S.; Panthi, D. Cyclic compatible contraction and related fixed point theorems. Fixed Point Theory Appl. 2016, 2016, 28. [Google Scholar] [CrossRef]
  13. Sumati Kumari, P.; Alqahtani, O.; Karapınar, E. Some Fixed-Point Theorems in b-Dislocated Metric Space and Applications. Symmetry 2018, 10, 691. [Google Scholar] [CrossRef]
  14. Kamran, T.; Samreen, M.; Ain, Q.U. A generalization of b-metric space and some fixed point Theorems. Mathematics 2017, 5, 19. [Google Scholar] [CrossRef]
  15. Alqahtani, B.; Karapinar, E.; Ozturk, A. On (α,ψ)-K-contractions in the extended b-metric space. Filomat 2018, 32, 15. [Google Scholar]
  16. Alqahtani, B.; Fulga, A.; Karapinar, E. Non-Unique Fixed Point Results in Extended B-Metric Space. Mathematics 2018, 6, 68. [Google Scholar] [CrossRef]
  17. Alqahtani, B.; Fulga, A.; Karapinar, E. Common fixed point results on extended b-metric space. J. Inequal. Appl. 2018, 2018, 158. [Google Scholar] [CrossRef] [PubMed]
  18. Karapınar, E.; Kumari, P.S.; Lateef, D. A New Approach to the Solution of the Fredholm Integral Equation via a Fixed Point on Extended b-Metric Spaces. Symmetry 2018, 10, 512. [Google Scholar] [CrossRef]
  19. Kumari, P.S.; Ampadu, C.B.; Nantadilok, J. On New Fixed Point Results in Eb-Metric Spaces. Thai J. Math. 2018, 16, 2018. [Google Scholar]

Share and Cite

MDPI and ACS Style

Panda, S.K.; Tassaddiq, A.; Agarwal, R.P. A New Approach to the Solution of Non-Linear Integral Equations via Various FBe-Contractions. Symmetry 2019, 11, 206. https://doi.org/10.3390/sym11020206

AMA Style

Panda SK, Tassaddiq A, Agarwal RP. A New Approach to the Solution of Non-Linear Integral Equations via Various FBe-Contractions. Symmetry. 2019; 11(2):206. https://doi.org/10.3390/sym11020206

Chicago/Turabian Style

Panda, Sumati Kumari, Asifa Tassaddiq, and Ravi P Agarwal. 2019. "A New Approach to the Solution of Non-Linear Integral Equations via Various FBe-Contractions" Symmetry 11, no. 2: 206. https://doi.org/10.3390/sym11020206

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