Research article

Fixed point results for a new contraction mapping with integral and fractional applications

  • Received: 18 February 2022 Revised: 17 May 2022 Accepted: 18 May 2022 Published: 24 May 2022
  • MSC : 47H10, 47H09, 54E50, 55M20

  • The purpose of this manuscript is to present some fixed point results for a Λ-Ćirić mapping in the setting of non-triangular metric spaces. Also, two numerical examples are given to support the theoretical study. Finally, under suitable conditions, the existence and uniqueness of a solution to a general Fredholm integral equation, a Riemann-Liouville fractional differential equation and a Caputo non-linear fractional differential equation are discussed as applications.

    Citation: Hasanen A. Hammad, Hassen Aydi, Choonkil Park. Fixed point results for a new contraction mapping with integral and fractional applications[J]. AIMS Mathematics, 2022, 7(8): 13856-13873. doi: 10.3934/math.2022765

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  • The purpose of this manuscript is to present some fixed point results for a Λ-Ćirić mapping in the setting of non-triangular metric spaces. Also, two numerical examples are given to support the theoretical study. Finally, under suitable conditions, the existence and uniqueness of a solution to a general Fredholm integral equation, a Riemann-Liouville fractional differential equation and a Caputo non-linear fractional differential equation are discussed as applications.



    Fixed point theory is an active field of research with wide range of applications in numerous directions. It is interested with the results about stating that due to some conditions a self mapping T on a set Λ possesses one or more fixed points. Fixed point theory began almost immediately after the classical analysis started its quick development. The main next growth was investigated by the need to establish existence results for problems dealing with integral and differential equations. Hence, the fixed point theory began a pure analytical theory.

    The Banach contraction principle [1] is one of the most nice theorems in fixed point theory. Due to its application in variant fields such as biology, physics, computer science, chemistry and several branches of mathematics, this classical famous theorem has been improved, extended and generalized in nonlinear analysis.

    In mathematics, the Fredholm integral equation is an integral equation whose solution is due to Fredholm operators and the study of Fredholm kernels. Several types of numerical and analytical methods and numerical methods were used to solve this problem. One of useful techniques to solve such equations is the usage of fixed point method, see [2,3,4,5,6]. Fractional differential equations appear in many fields such as physics, mechanics, chemistry, economics, engineering and biological sciences, etc.; see for example [7,8,9,10,11,12]. The theory of fractional differential (evolution) equations is a useful branch of mathematics by which variant physical phenomena in several fields of engineering and science can be studied. In the recent years, there has been a remarkable development in partial and ordinary differential equations using fractional derivatives. Many authors studied the existence and uniqueness of positive solutions for (nonlinear) fractional differential equation boundary value problems, see [13,14]. Among them, new existence results in Banach spaces by using the fractional derivatives and fixed point theorems have been presented, see [15,16].

    In last years, many generalizations of standard metric spaces related to generalizing the Banach contraction theorem have been investigated. Most of known fixed point achievements in literature are given by taking into account the triangle inequality or other its generalizations (b-metric [17], partial metric [18], dislocated metric [19], G-metric [20], extended b-metric [21], controlled metric [22], double controlled metric [23], etc). Many works appeared in order to make weaker the triangle inequality. Amon them, Jleli and Samet [24] introduced a new metric setting, called as a JS-metric involving the power of sequences, covering some generalized metrics, as the b-metric, the dislocated metric and the modular metric. Recently, Khojasteh and Khandani [25] initiated the notion of non-triangular metric spaces in order to weaken the condition suggested in [24]. Their concept is based on the fact that if the limit of a convergent sequence exists, it is unique. Some fixed point results using manageable functions are presented in [26].

    When the triangle inequality is omitted, the results becomes more difficult to establish. However, several real applications suffer from the lack of the triangle inequality, and so the related results will be more interesting and nice. Our paper goes with this point of view. In particular, we deal with a non-triangulat metric space. We will prove some related fixed point results involving Ćirić [27] and Wardowski [28] contraction mappings. Some concrete examples are provided. At the end, by applying our obtained results we ensure the existence of solutions of a Fredholm integral equation, a Riemann-Liouville fractional differential equation and a Caputo non-linear fractional differential equation.

    This part is devoted to present the initial characteristics of contraction mappings and some previously defined ideas with references.

    Definition 2.1. [25] Let be a non-empty set and :2[0,) be a mapping satisfying, for all ϑ,θ,ς,

    (n1) (ϑ,ϑ)=0;

    (n2) (ϑ,θ)=(θ,ϑ);

    (n3) for a sequence {ϑi}iN with limi(ϑi,ϑ)=0 and limi(ϑi,θ)=0, we have ϑ=θ.

    Then is called a non-triangular metric and the pair (,) is called a non-triangular metric space (NTMS, for short).

    The definition of a Ćirić contraction mapping is stated as follows:

    Definition 2.2. [27] A self mapping ζ on a metric space (,) is called a Ćirić contraction if there exists (0,12) so that the inequality below holds:

    (ζϑ,ζθ)((ϑ,ζϑ)+(θ,ζθ)), ϑ,θ.

    In 2012, Wardowski [28] generalized the Banach contraction mapping [1] and introduced some different forms for contraction mappings. His definition is stated as follows:

    Definition 2.3. Assume that Λ:R+R is a function justifying

    (Λi) Λ is strictly increasing;

    (Λii) for each sequence {ϑi}iN of positive numbers with limiϑi=0limiΛ(ϑi)=;

    (Λiii) there is a constant μ(0,1) so that limi0+(ϑi)μΛ(ϑi)=0.

    Let Σ be the family of all functions Λ:R+R fulfilling (ⅰ)-(ⅲ). A function ζ: is called a Λcontraction if the following inequality

    (ζϑ,ζθ)>0α+Λ((ζϑ,ζθ))Λ((ϑ,θ)). (2.1)

    holds for all ϑ,θ and ΛΣ.

    Based on the inequality (2.1), the same author presented some various contractions as follows: For all ϑ,θΛ with ζϑζθ,

    (i) Λ1(ϑ)=ln(ϑ),(ζϑ,ζθ)(ϑ,θ)eα,(ii) Λ2(ϑ)=ln(ϑ)+ϑ,(ζϑ,ζθ)e(ζϑ,ζθ)(ϑ,θ)e(ϑ,θ)α,(iii) Λ3(ϑ)=1ϑ,(ζϑ,ζθ)(1+(ϑ,θ))2(ϑ,θ),(iv) Λ4(ϑ)=ln(ϑ2+ϑ),(ζϑ,ζθ)(1+(ζϑ,ζθ)))eα(ϑ,θ)(1+(ϑ,θ)),

    where {Λi:i=1,2,3,4}Σ.

    It should be noted that, the inequality (2.1) yields that the mapping is contractive. Hence, every Λcontraction is continuous.

    Rashwan and Hasanen [29] added a new function to the family Σ but the shape of the contraction under this function is not known until now. This function takes the form Λ(ϑ)=1rϑ, where r>1 and ϑ>0.

    Now, we merge the results of Ćirić and Wardowski to obtain the following contraction mapping in the context of NTMSs.

    Definition 2.4. Let (,) be an NTMS. We say that ζ: is a ΛĆirić mapping if there exists (0,1) such that for each ϑ,θ with ϱ>0, we have

    ϱ+Λ((ζϑ,ζθ))Λ([(ϑ,ζϑ)+(θ,ζθ)]). (2.2)

    Clearly, the inequality (2.2) reduces to (2.1), if we take Λ(ϑ)=ln(ϑ).

    Definition 2.5. [25] Let (,) be an NTMS. A mapping ζ: is called asymptotically regular if for all {ϑi}, limi(ζϑi,ζϑi+1)=0.

    Definition 2.6. [25] Let (,) be an NTMS. A sequence {ϑi} is said to be

    ● convergent to the point ϑ if limi(ϑi,ϑ)=0,

    ● a Cauchy sequence if limi,j(ϑi,ϑj)=0.

    If every Cauchy sequence in converges to some element ϑ, then the NTMS (,) is called complete.

    This part is devoted to discuss the existence and uniqueness of an FP for the ΛĆirić mapping under asymptotic regularity in the setting of an NTMS.

    Theorem 3.1. Let (,) be a complete NTMS. Then a ΛĆirić mapping ζ: owns aunique FP.

    Proof. Let ϑ0 be an arbitrary point in and define a sequence {ϑi}i1 by ϑi+1=ζϑi and ϑi=ζiϑ0 for all iN.

    Based on the definition of ζ, we get

    ϱ+Λ((ζϑ,ζθ))Λ([(ϑ,ζϑ)+(θ,ζθ)]), for some ϱ>0.

    It follows that, for some (0,12),

    Λ((ζϑ,ζθ))<Λ([(ϑ,ζϑ)+(θ,ζθ)]).

    From (Λi), we can write

    (ζϑ,ζθ)<ϖ[(ϑ,ζϑ)+(θ,ζθ)], ϑ,θ. (3.1)

    Putting ϑ=ϑi1 and θ=ϑi in (3.1), we have

    (ϑi,ϑi+1)=(ζϑi1,ζϑi)<ϖ[(ϑi1,ζϑi1)+(ϑi,ζϑi)]=ϖ[(ϑi1,ϑi)+(ϑi,ϑi+1)],

    which implies that

    (ϑi,ϑi+1)<ρ(ϑi1,ϑi), for all iN, (3.2)

    where ρ=ϖ1ϖ<1. Effecting the function Λ on both sides of (3.1), we obtain

    Λ((ϑi,ϑi+1))<Λ(ρ(ϑi1,ϑi)).

    Hence,

    Λ((ϑi,ϑi+1))Λ(ρ(ϑi1,ϑi))ϱ, for some ϱ>0.

    Similarly, one can write

    Λ((ϑi1,ϑi))Λ(ρ2(ϑi2,ϑi1))2ϱ, for some ϱ>0.

    Following the same scenario, for some ϱ>0, we find that

    Λ((ζϑi1,ζϑi))=Λ((ϑi,ϑi+1))Λ(ρi(ϑ0,ϑ1))iϱ. (3.3)

    Letting i in (3.3), we conclude that

    limiΛ((ζϑi1,ζϑi))=.

    Using (Λii), we have

    limi(ζϑi1,ζϑi)=0. (3.4)

    This shows that the sequence {ζϑi} is asymptotically regular and hence the sequence {ϑi+1} or {ϑi}.

    Now, we prove that {ζϑi} is a Cauchy sequence. Indeed, for i,jN with ji, putting ϑ=ϑi and θ=ϑj in (2.2), we have

    (ζϑi,ζϑj)<ϖ[(ϑi,ζϑi)+(ϑj,ζϑj)]=ϖ[(ζϑi1,ζϑi)+(ζϑj1,ζϑj)]. (3.5)

    Taking the limit as i in (3.5) and using (3.4), we have

    (ζϑi,ζϑj)0 as i.

    This proves that the sequence {ζϑi} is Cauchy in . Since (,) is complete, there is a point ϑ such that

    limiζϑi=ϑ. (3.6)

    In order to obtain an FP of ζ, choosing ϑ=ϑi and θ=ϑ in (2.2), we get

    ϱ+Λ((ζϑi,ζϑ))Λ([(ϑi,ζϑi)+(ϑ,ζϑ)]), for some ϱ>0.

    Hence,

    (ζϑi,ζϑ)[(ϑi,ζϑi)+(ϑ,ζϑ)].

    As i in the above inequality and using (3.6), we can write

    (1)(ϑ,ζϑ)0,

    since <1. Then the above inequality holds only if (ϑ,ζϑ)=0, that is, ϑ=ζϑ. Hence, ϑ is an FP of ζ. For the uniqueness, let ˆϑ be another distinct FP of ζ, i.e.,

    ϑ=ζϑ and ˆϑ=ζˆϑ.

    Selecting ϑ=ϑ and θ=ˆϑ in (2.2), we have

    ϱ+Λ((ζϑ,ζˆϑ))Λ([(ϑ,ζϑ)+(ˆϑ,ζˆϑ)]), for some ϱ>0.

    Hence,

    (ϑ,ˆϑ)=(ζϑ,ζˆϑ)[(ϑ,ζϑ)+(ˆϑ,ζˆϑ)]=0.

    This implies that ϑ=ˆϑ. This completes the proof.

    The following results follow immediately from Theorem 3.1.

    Corollary 3.2. Let (,) be a complete NTMS and ζ be a self-mapping such that

    (ζϑ,ζθ)<min{(ϑ,ζϑ),(θ,ζθ)},

    for all ϑ,θ, where (0,12). Then ζ owns a unique FP in .

    Proof. For each ϑ,θ, it's easy to see that

    (ζϑ,ζθ)<min{(ϑ,ζϑ),(θ,ζθ)}[(ϑ,ζϑ)+(θ,ζθ)].

    Since Λ is monotonically increasing, we obtain

    Λ((ζϑ,ζθ))<Λ([(ϑ,ζϑ)+(θ,ζθ)]).

    For some constant ϱ>0, we can write

    ϱ+Λ((ζϑ,ζθ))Λ([(ϑ,ζϑ)+(θ,ζθ)]).

    This implies that ζ is a ΛĆirić mapping. Applying Theorem 3.1, we can find a unique FP of ζ.

    Corollary 3.3. Let (,) be a complete NTMS and ζ be a self-mapping such that

    (ζϑ,ζθ)((ϑ,ζϑ)+(θ,ζθ)1+(ϑ,ζϑ)+(θ,ζθ)),

    for all ϑ,θ, where (0,12). Then ζ owns a unique FP in .

    Proof. Consider

    (ζϑ,ζθ)((ϑ,ζϑ)+(θ,ζθ)1+(ϑ,ζϑ)+(θ,ζθ))((ϑ,ζϑ)+(θ,ζθ)).

    Then ζ is a ΛĆirić mapping. Hence, the desired result is obtained.

    To support our studies, we present the examples below.

    Example 3.4. Let =[0,) and :2[0,) be a metric described as

    (ϑ,θ)={ϑ+θϑ+θ+1, if ϑθ,ϑ0,θ0,0, if ϑ=θ,ϑ2, if θ=0,θ2, if ϑ=0.

    Clearly, (,) is an NTMS [25]. It is not a metric space. Define a self-mapping ζ by ζϑ=117ϑ. Consider for all ϑ,θ,

    Λ((ζϑ,ζθ))=Λ((ϑ17,θ17))=Λ(ϑ+θϑ+θ+17).

    Also,

    Λ([(ϑ,ζϑ)+(θ,ζθ)])=Λ(13[(ϑ,ϑ17)+(θ,θ17)])=Λ(6[ϑ18ϑ+17+θ18θ+17])Λ(3(ϑ+θϑ+θ+17)),

    where =13. Let ΛΣ be a function defined by Λ(ϑ)=ln(ϑ), for ϑ>0. Then

    Λ((ζϑ,ζθ))Λ([(ϑ,ζϑ)+(θ,ζθ)])ln(ϑ+θϑ+θ+17)ln(3(ϑ+θϑ+θ+17))=ln((ϑ+θϑ+θ+17)3(ϑ+θϑ+θ+17))=ln(13)=ln(3).

    Therefore, ζ a ΛĆirić mapping with ϱ=ln(3)>0. According to Theorem 3.1, ζ has 0 as a unique FP.

    Example 3.5. Let ={12j4:jN}{0} under the metric defined in Example 3.4. Then the pair (,) is an NTMS. Define a nonlinear mapping ζ: by

    ζϑ={{122j}, if ϑ{122j4;jN},0, if ϑ=0.

    To prove that ζ is a ΛĆirić mapping, we discuss the following cases:

    (i) If ϑ=122j4 and θ=122m4, for m>j1, then one can write

    Λ((ζϑ,ζθ))=Λ((ζ(122j4),ζ(122m4)))=Λ((122j,122m))=Λ(122j+122m1+122j+122m)=Λ(22m+22j22m+22j+22m+2j). (3.7)

    Also,

    Λ([(ϑ,ζϑ)+(θ,ζθ)])=Λ(13[(122j4,ζ(122j4))+(122m4,ζ(122m4))])=Λ(13[(122j4,122j)+(122m4,122m)])=Λ(13[1616+22j+1616+22m])=Λ(163[32+22m+22j256+16(22m+22j)+22m+2j])Λ(32[22m+22j22m+22j+22m+2j]). (3.8)

    It follows from (3.7) and (3.8) that

    Λ((ζϑ,ζθ))Λ([(ϑ,ζϑ)+(θ,ζθ)])Λ(22m+22j22m+22j+22m+2j)Λ(32[22m+22j22m+22j+22m+2j])=ln(22m+22j22m+22j+22m+2j)ln(32[22m+22j22m+22j+22m+2j])=ln((22m+22j22m+22j+22m+2j)32(22m+22j22m+22j+22m+2j))=ln(23)=ln(32)0.4055.

    (ii) If ϑ=122j4 and θ=0, then we have

    Λ((ζϑ,ζθ))=Λ((ζ(122j4),ζ(0)))=Λ((122j,0))=Λ(122j1+122j)=Λ(11+22j).

    Also,

    Λ([(ϑ,ζϑ)+(θ,ζθ)])=Λ(13[(122j4,ζ(122j4))+(0,ζ0)])=Λ(13[(122j4,122j)])=Λ(13[1616+22j])=Λ(163[116+22j])Λ(32[11+22j]).

    Hence,

    Λ((ζϑ,ζθ))Λ([(ϑ,ζϑ)+(θ,ζθ)])Λ(11+22j)Λ(32[11+22j])=ln(11+22j)ln(32[11+22j])=ln((11+22j)32[11+22j])=ln(23)=ln(32)0.4055.

    (iii) If ϑ=0 and θ=122m4, then the proof follows immediately from Cases (ⅰ) and (ⅱ).

    Based on the above cases, we conclude that ζ is a ΛĆirić mapping with ϱ=0.4055 and Λ(ϑ)=ln(ϑ) for ϑ>0. So by Theorem 3.1, 0 is the unique FP of ζ.

    In this part, we apply Theorem 3.1 to discuss the existence and uniqueness of a unique solution to a general Fredholm integral equation. This solution is equivalent to find a unique fixed point of the mapping ζ.

    Consider the following problem:

    ϑ(τ)φ(τ)=eϱν(τ)+eϱδ1δ0ϖ(τ,s)φ(s)ds, τ,s[δ0,δ1], ϱ>0, (4.1)

    where φ(τ)C[δ0,δ1] is a continuous function, ϖ:[δ0,δ1]×[δ1,δ0]R is a square integrable function and ν:[δ0,δ1]R is a known function.

    Assume that =(C[δ0,δ1],R) is the set of real continuous functions on [δ0,δ1] endowed with

    (ϑ,θ)=maxτ[δ1,δ0]{|ϑ(τ)θ(τ)|}, for each ϑ,θ. (4.2)

    Problem (4.1) will be considered under the following assumptions:

    (p1) there exist functions ϑ1(τ) and ϑ2(τ) in C[δ0,δ1] so that ϑ2(τ)ϑ1(τ) for each ϑ1(τ),ϑ2(τ)>0;

    (p2) for some φ1(τ),φ2(τ) and for all τ[δ0,δ1], we have

    ν2(τ)+δ1δ0ϖ2(τ,s)φ2(s)ds=(φ1(τ)φ2(τ))eϱϑ2(τ),

    for any function ν2(τ)R and ϱ>0.

    Now, we can state and prove our main theorem in this section.

    Theorem 4.1. Under the hypotheses (p1) and (p3), Eq (4.1) has a unique solution in .

    Proof. Define the mapping ζ: by

    ζ(φ1)(τ)=ν1(τ)+δ1δ0ϖ1(τ,s)φ1(s)dseϱϑ1(τ), (4.3)

    for all φ1(τ) and τ[δ0,δ1]. Using (4.3), we get

    |ζ(φ2)(τ)ζ(φ1)(τ)|=|ν2(τ)+δ1δ0ϖ2(τ,s)φ2(s)dseϱϑ2(τ)ν1(τ)+δ1δ0ϖ1(τ,s)φ1(s)dseϱϑ1(τ)|.

    From assumption (p1), ϑ2(τ)ϑ1(τ), i.e., 1ϑ1(τ)1ϑ2(τ), we obtain 1ϑ1(τ)>12ϑ2(τ). Applying this fact in the above equation, we can write

    |ζ(φ2)(τ)ζ(φ1)(τ)||ν2(τ)+δ1δ0ϖ2(τ,s)φ2(s)dseϱϑ2(τ)ν1(τ)+δ1δ0ϖ1(τ,s)φ1(s)ds2eϱϑ2(τ)|=12|2ν2(τ)+2δ1δ0ϖ2(τ,s)φ2(s)dseϱϑ2(τ)ν1(τ)+δ1δ0ϖ1(τ,s)φ1(s)dseϱϑ2(τ)|=12|ν2(τ)+δ1δ0ϖ2(τ,s)φ2(s)dseϱϑ2(τ)+ν2(τ)+δ1δ0ϖ2(τ,s)φ2(s)dseϱϑ2(τ)ν1(τ)+δ1δ0ϖ1(τ,s)φ1(s)dseϱϑ2(τ)|. (4.4)

    Applying the assumption (p2) in (4.5), one can write

    |ζ(φ2)(τ)ζ(φ1)(τ)|12|ν2(τ)+δ1δ0ϖ2(τ,s)φ2(s)dseϱϑ2(τ)+(φ1(τ)φ2(τ))e2ϱϑ2(τ)eϱϑ2(τ)ν1(τ)+δ1δ0ϖ1(τ,s)φ1(s)dseϱϑ2(τ)|=12|(eϱ(ν2(τ)+δ1δ0ϖ2(τ,s)φ2(s)ds)ϑ2(τ)φ2(τ)eϱ)(eϱ(ν1(τ)+δ1δ0ϖ1(τ,s)φ1(s)ds)ϑ2(τ)φ1(τ)eϱ)|12|(eϱ(ν2(τ)+δ1δ0ϖ2(τ,s)φ2(s)ds)ϑ2(τ)φ2(τ)eϱ)(eϱ(ν1(τ)+δ1δ0ϖ1(τ,s)φ1(s)ds)ϑ2(τ)φ1(τ)eϱ)|eϱ2[|(ν2(τ)+δ1δ0ϖ2(τ,s)φ2(s)dsϑ2(τ)φ2(τ))|+|(ν1(τ)+δ1δ0ϖ1(τ,s)φ1(s)dsϑ2(τ)φ1(τ))|].

    Since 1ϑ1(τ)1ϑ2(τ), we have

    |ζ(φ2)(τ)ζ(φ1)(τ)|eϱ2(|ν1(τ)+δ1δ0ϖ1(τ,s)φ1(s)dsϑ1(τ)φ1(τ)|+|ν2(τ)+δ1δ0ϖ2(τ,s)φ2(s)dsϑ2(τ)φ2(τ)|)=eϱ2(|ζ(φ1)(τ)φ1(τ)|+|ζ(φ2)(τ)φ2(τ)|).

    Using (4.2), we obtain

    eϱ(ζ(φ2),ζ(φ1))12[(ζ(φ1),φ1)+(ζ(φ1),φ1)].

    Taking =12 and applying ln to both sides, we get

    ϱ+ln[(ζ(φ2),ζ(φ1))]ln[((ζ(φ1),φ1)+(ζ(φ1),φ1))], for some ϱ>0.

    This implies that ζ is a ΛĆirić mapping with Λ(ϑ)=ln(ϑ)Σ. By Theorem 3.1, there exists a unique FP of a mapping ζ, that is, the unique solution of the integral equation (4.1).

    In this part, we discuss the existence and uniqueness solution of a Riemann-Liouville fractional order operator by Theorem 3.1. This operator is defined as follows: Assume that φ(τ) is a class of functions, which have c+1 continuous derivatives for all τ[0,δ], then the Riemann-Liouville fractional derivative of the function φ(τ) with the order ε is described as

    δDετφ(τ)=1Γ(ε+c+1)dd(τ)cτδ(τϑ)cεφ(ϑ)dϑ=ck=0φ(k)(δ)(τδ)kεΓ(kε+1)+1Γ(ε+c+1)τδ(τϑ)cεφ(c+1)(ϑ)dϑ, (5.1)

    where c<εc+1 and τ[0,δ].

    Assume that =(C[0,δ],R) is the set of real continuous functions on [0,δ] equipped with

    (ϑ,θ)=maxτ[0,δ]|ϑ(τ)θ(τ)|, for all ϑ,θ.

    The existence solution of the integral operator (5.1) will be discussed under the postulate below:

    (IO) there exist functions φ1(τ) and φ2(τ) in so that for each τ[0,δ], we have φ1(τ)φ2(τ) and

    φ(s)1(τ)φ(s)2(τ)eϱ(φ(s)1(τ)+φ(s)2(τ)3),

    for all s(0,) and for some ϱ>0. Here φ(s)1(τ) refers to the sth-order derivative of the function φ1.

    Theorem 5.1. Riemann-Liouville fractional derivative operator (5.1) has a unique solution in provided that the postulate (IO) holds.

    Proof. Define an operator ζ: by

    ζφ(τ)=ck=0φ(k)(δ)(τδ)kεΓ(kε+1)+1Γ(cε+1)τδ(τϑ)cεφ(c+1)(ϑ)dϑ, (5.2)

    for all φ(τ) and τ[0,δ]. Then the unique solution of the integral operator (5.1) is equivalent to find a unique FP of the operator (5.2). For each τ[0,δ] and c<εc+1, we have

    |ζφ1(τ)φ1(τ)|+|ζφ2(τ)φ2(τ)|=|ck=0φ(k)1(δ)(τδ)kεΓ(kε+1)+1Γ(ε+c+1)τδ(τϑ)cεφ(c+1)1(ϑ)dϑφ1(ϑ)|+|ck=0φ(k)2(δ)(τδ)kεΓ(kε+1)+1Γ(ε+c+1)τδ(τϑ)cεφ(c+1)2(ϑ)dϑφ2(ϑ)|. (5.3)

    Consider

    |ζφ1(τ)ζφ2(τ)|=|ck=0φ(k)1(δ)(τδ)kεΓ(kε+1)+1Γ(ε+c+1)τδ(τϑ)cεφ(c+1)1(ϑ)dϑck=0φ(k)2(δ)(τδ)kεΓ(kε+1)1Γ(ε+c+1)τδ(τϑ)cεφ(c+1)2(ϑ)dϑ|=|ck=0(τδ)kεΓ(kε+1)[φ(k)1(δ)φ(k)2(δ)]+1Γ(ε+c+1)τδ(τϑ)cε[φ(c+1)1(ϑ)φ(c+1)2(ϑ)]dϑ|.

    Applying the condition (IO) and using (5.3), one can write

    |ζφ1(τ)ζφ2(τ)||ck=0(τδ)kεΓ(kε+1)[φ(k)1(δ)φ(k)2(δ)]+1Γ(ε+c+1)τδ(τϑ)cε[φ(c+1)1(ϑ)φ(c+1)2(ϑ)]dϑ+φ2(ϑ)φ1(ϑ)|=|ck=0(τδ)kεΓ(kε+1)[φ(k)1(δ)φ(k)2(δ)]+1Γ(ε+c+1)τδ(τϑ)cε[φ(c+1)1(ϑ)φ(c+1)2(ϑ)]dϑ[φ1(ϑ)φ2(ϑ)]|eϱ3|ck=0(τδ)kεΓ(kε+1)[φ(k)1(δ)+φ(k)2(δ)]+1Γ(ε+c+1)τδ(τϑ)cε[φ(c+1)1(ϑ)+φ(c+1)2(ϑ)]dϑ[φ1(ϑ)+φ2(ϑ)]|=eϱ3(|ck=0φ(k)1(δ)(τδ)kεΓ(kε+1)+1Γ(ε+c+1)τδ(τϑ)cεφ(c+1)1(ϑ)dϑφ1(ϑ)+ck=0φ(k)2(δ)(τδ)kεΓ(kε+1)+1Γ(ε+c+1)τδ(τϑ)cεφ(c+1)2(ϑ)dϑφ2(ϑ)|)=eϱ3(|ζφ1(τ)φ1(τ)|+|ζφ2(τ)φ2(τ)|).

    By (4.2), we have

    eϱ(ζ(φ2),ζ(φ1))13[(ζ(φ1),φ1)+(ζ(φ1),φ1)].

    Putting =13 and applying ln to both sides, we get

    ϱ+ln[(ζ(φ2),ζ(φ1))]ln[((ζ(φ1),φ1)+(ζ(φ1),φ1))], for some ϱ>0,

    or equivalently

    ϱ+Λ((ζ(φ2),ζ(φ1)))Λ(((ζ(φ1),φ1)+(ζ(φ1),φ1))).

    This implies that ζ is a ΛĆirić mapping with Λ(ϑ)=ln(ϑ)Σ. Based on Theorem 3.1, the mapping ζ has a unique FP, which is the unique solution of the integral operator (5.1).

    There is no doubt that non-linear fractional differential equations play a great role in many applications such as mathematical modeling, engineering, physics, and many real-world problems. So, the goal of this part is to study the existence of a solution to non-linear fractional differential equation of Caputo type by Theorem 3.1. El-Hady and Agrekci [30] studied the stability problem of some fractional differential equations with Caputo derivatve in the sense of Hyers-Ulam and Hyers-Ulam-Rassias based on some fixed point techniques.

    Caputo's formula for derivatives is presented as follows:

    CDεφ(τ)=Ξ(τ,φ(τ)), (6.1)

    with boundary conditions

    φ(0)=0, φ(1)=δ0φ(ϑ)dϑ, δ(0,1),

    where CDε represents the Caputo fractional derivative with order ε. Moreover, for a continuous function φ:[0,)R, the Caputo fractional derivative with order ε is described as

    CDεφ(τ)=1Γ(cε)δ10(δ1ϑ)cε1φ(c)(ϑ)dϑ, c1<εc.

    Let =C[0,1] be the set of all real-valued continuous functions on [0,1]. Define :2[0,) by

    (ϑ,θ)=maxτ[0,1]|ϑ(τ)θ(τ)|, for each ϑ,θ. (6.2)

    Now, we consider the following hypotheses:

    (h1) there exist continuous functions Ξ1,Ξ2:[0,1]×RR+ satisfying

    Ξ(τ,φ2(τ))Ξ(τ,φ1(τ))Ξ(τ,φ2(τ))+Ξ(τ,φ1(τ))4eϱ,

    for all τ[0,1] and φ1,φ2;

    (h2) there are φ1(τ),φ2(τ)0 with φ1(τ)φ2(τ) such that

    φ2(τ)φ1(τ)φ2(τ)+φ1(τ)4eϱ,

    for all φ1(τ),φ2(τ).

    We are ready to state and prove the main theorem in this section.

    Theorem 6.1. Under hypotheses (h1) and (h2), the boundary valueproblem (6.1) has a unique solution in .

    Proof. Let ζ: be a mapping defined by

    ζφ(τ)=1Γ(ε)τ0(τϑ)ε1Ξ(ϑ,φ(ϑ))dϑ2τ(2δ2)Γ(ε)10(1ϑ)ε1Ξ(ϑ,φ(ϑ))dϑ+2τ(2δ2)Γ(ε)δ0ϑ0(ϑϕ)ε1Ξ(ϕ,φ(ϕ))dϕdϑ, (6.3)

    for τ[0,1]. The function φ is a unique solution of the problem (6.1) if and only if φ=ζφ, i.e., φ is a unique FP of ζ. To achieve that, we shall prove that the ζ is a ΛĆirić mapping. Consider,

    |ζφ1(τ)φ1(τ)|+|ζφ2(τ)φ2(τ)|=|1Γ(ε)τ0(τϑ)ε1Ξ(ϑ,φ1(ϑ))dϑ2τ(2δ2)Γ(ε)10(1ϑ)ε1Ξ(ϑ,φ1(ϑ))dϑ+2τ(2δ2)Γ(ε)δ0ϑ0(ϑϕ)ε1Ξ(ϕ,φ1(ϕ))dϕdϑφ1(τ)|+|1Γ(ε)τ0(τϑ)ε1Ξ(ϑ,φ2(ϑ))dϑ2τ(2δ2)Γ(ε)10(1ϑ)ε1Ξ(ϑ,φ2(ϑ))dϑ+2τ(2δ2)Γ(ε)δ0ϑ0(ϑϕ)ε1Ξ(ϕ,φ2(ϕ))dϕdϑφ1(τ)|=|1Γ(ε)τ0(τϑ)ε1[Ξ(ϑ,φ1(ϑ))+Ξ(ϑ,φ2(ϑ))]dϑ2τ(2δ2)Γ(ε)10(1ϑ)ε1[Ξ(ϑ,φ1(ϑ))+Ξ(ϑ,φ2(ϑ))]dϑ[φ1(τ)+φ2(ϑ)]|. (6.4)

    Also, we obtain

    |ζφ2(τ)ζφ1(τ)|=|1Γ(ε)τ0(τϑ)ε1Ξ(ϑ,φ2(ϑ))dϑ2τ(2δ2)Γ(ε)10(1ϑ)ε1Ξ(ϑ,φ2(ϑ))dϑ+2τ(2δ2)Γ(ε)δ0ϑ0(ϑϕ)ε1Ξ(ϕ,φ2(ϕ))dϕdϑ1Γ(ε)τ0(τϑ)ε1Ξ(ϑ,φ1(ϑ))dϑ+2τ(2δ2)Γ(ε)10(1ϑ)ε1Ξ(ϑ,φ1(ϑ))dϑ2τ(2δ2)Γ(ε)δ0ϑ0(ϑϕ)ε1Ξ(ϕ,φ1(ϕ))dϕdϑ||1Γ(ε)τ0(τϑ)ε1[Ξ(ϑ,φ2(ϑ))Ξ(ϑ,φ1(ϑ))]dϑ2τ(2δ2)Γ(ε)10(1ϑ)ε1[Ξ(ϑ,φ2(ϑ))Ξ(ϑ,φ1(ϑ))]dϑ[φ2(ϑ)φ1(ϑ)]+2τ(2δ2)Γ(ε)δ0ϑ0(ϑϕ)ε1[Ξ(ϕ,φ2(ϕ))Ξ(ϕ,φ1(ϕ))]dϕdϑ|.

    Applying the assumptions (h1), (h2) and using (6.3), we get

    |ζφ2(τ)ζφ1(τ)|eϱ4(|1Γ(ε)τ0(τϑ)ε1[Ξ(ϑ,φ2(ϑ))+Ξ(ϑ,φ1(ϑ))]dϑ2τ(2δ2)Γ(ε)10(1ϑ)ε1[Ξ(ϑ,φ2(ϑ))+Ξ(ϑ,φ1(ϑ))]dϑ[φ2(ϑ)+φ1(ϑ)]+2τ(2δ2)Γ(ε)δ0ϑ0(ϑϕ)ε1[Ξ(ϕ,φ2(ϕ))+Ξ(ϕ,φ1(ϕ))]dϕdϑ|)=eϱ4(|ζφ1(τ)φ1(τ)|+|ζφ2(τ)φ2(τ)|).

    Using (6.2), we can write

    eϱ(ζ(φ2),ζ(φ1))14[(ζ(φ1),φ1)+(ζ(φ1),φ1)].

    Letting =14 and applying ln to both sides, we obtain

    ϱ+ln[(ζ(φ2),ζ(φ1))]ln[((ζ(φ1),φ1)+(ζ(φ1),φ1))], for some ϱ>0,

    or equivalently

    ϱ+Λ((ζ(φ2),ζ(φ1)))Λ(((ζ(φ1),φ1)+(ζ(φ1),φ1))).

    Thus, the mapping ζ is a ΛĆirić mapping with Λ(ϑ)=ln(ϑ)Σ. According to Theorem 3.1, ζ has a unique FP. This completes the proof.

    Open Question: It is clear that the space of interest lacks many assumptions and situations through which we can address many applications. Among these situations, how can we study Hyers-Ulam-Rassias and Hyers-Ulam stability (see [31,32,33]) of some fractional differential equation with Caputo derivative?

    In this work, we presented some fixed point results involving ΛĆirić mappings in the setting of non-triangular metric spaces. We illustrated the obtained results by some concrete examples and some applications. We solved a general Fredholm integral equation, a Riemann-Liouville fractional differential equation and a Caputo non-linear fractional differential equation. As perspectives, it would be interesting to extend the paper and give related applications to non classical metric spaces, like fuzzy bipolar metric spaces [34].

    The authors declare that they have no conflict of interest.



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