The subject of this work is the existence and Mittag-Leffler-Ulam (MLU) stability of solutions for fractional pantograph equations with three sequential fractional derivatives. Sufficient conditions for the existence and uniqueness of solutions are constructed by utilizing well-known classical fixed point theorems such as the Banach contraction principle, and Leray-Schauder nonlinear alternative. The generalized singular Gronwall's inequality is used to show the MLU stability results. An illustrated example is provided to support the main findings.
Citation: Mohamed Houas, Kirti Kaushik, Anoop Kumar, Aziz Khan, Thabet Abdeljawad. Existence and stability results of pantograph equation with three sequential fractional derivatives[J]. AIMS Mathematics, 2023, 8(3): 5216-5232. doi: 10.3934/math.2023262
[1] | Wedad Albalawi, Muhammad Imran Liaqat, Fahim Ud Din, Kottakkaran Sooppy Nisar, Abdel-Haleem Abdel-Aty . Well-posedness and Ulam-Hyers stability results of solutions to pantograph fractional stochastic differential equations in the sense of conformable derivatives. AIMS Mathematics, 2024, 9(5): 12375-12398. doi: 10.3934/math.2024605 |
[2] | Saeed M. Ali, Mohammed S. Abdo, Bhausaheb Sontakke, Kamal Shah, Thabet Abdeljawad . New results on a coupled system for second-order pantograph equations with $ \mathcal{ABC} $ fractional derivatives. AIMS Mathematics, 2022, 7(10): 19520-19538. doi: 10.3934/math.20221071 |
[3] | Songkran Pleumpreedaporn, Chanidaporn Pleumpreedaporn, Weerawat Sudsutad, Jutarat Kongson, Chatthai Thaiprayoon, Jehad Alzabut . On a novel impulsive boundary value pantograph problem under Caputo proportional fractional derivative operator with respect to another function. AIMS Mathematics, 2022, 7(5): 7817-7846. doi: 10.3934/math.2022438 |
[4] | Souad Ayadi, Ozgur Ege, Manuel De la Sen . On a coupled system of generalized hybrid pantograph equations involving fractional deformable derivatives. AIMS Mathematics, 2023, 8(5): 10978-10996. doi: 10.3934/math.2023556 |
[5] | Abdelkader Moumen, Ramsha Shafqat, Zakia Hammouch, Azmat Ullah Khan Niazi, Mdi Begum Jeelani . Stability results for fractional integral pantograph differential equations involving two Caputo operators. AIMS Mathematics, 2023, 8(3): 6009-6025. doi: 10.3934/math.2023303 |
[6] | Ahmed M. A. El-Sayed, Wagdy G. El-Sayed, Kheria M. O. Msaik, Hanaa R. Ebead . Riemann-Liouville fractional-order pantograph differential equation constrained by nonlocal and weighted pantograph integral equations. AIMS Mathematics, 2025, 10(3): 4970-4991. doi: 10.3934/math.2025228 |
[7] | Sabri T. M. Thabet, Miguel Vivas-Cortez, Imed Kedim . Analytical study of $ \mathcal{ABC} $-fractional pantograph implicit differential equation with respect to another function. AIMS Mathematics, 2023, 8(10): 23635-23654. doi: 10.3934/math.20231202 |
[8] | Anumanthappa Ganesh, Swaminathan Deepa, Dumitru Baleanu, Shyam Sundar Santra, Osama Moaaz, Vediyappan Govindan, Rifaqat Ali . Hyers-Ulam-Mittag-Leffler stability of fractional differential equations with two caputo derivative using fractional fourier transform. AIMS Mathematics, 2022, 7(2): 1791-1810. doi: 10.3934/math.2022103 |
[9] | A. M. A. El-Sayed, H. H. G. Hashem, Sh. M. Al-Issa . A comprehensive view of the solvability of non-local fractional orders pantograph equation with a fractal-fractional feedback control. AIMS Mathematics, 2024, 9(7): 19276-19298. doi: 10.3934/math.2024939 |
[10] | Sabri T. M. Thabet, Sa'ud Al-Sa'di, Imed Kedim, Ava Sh. Rafeeq, Shahram Rezapour . Analysis study on multi-order $ \varrho $-Hilfer fractional pantograph implicit differential equation on unbounded domains. AIMS Mathematics, 2023, 8(8): 18455-18473. doi: 10.3934/math.2023938 |
The subject of this work is the existence and Mittag-Leffler-Ulam (MLU) stability of solutions for fractional pantograph equations with three sequential fractional derivatives. Sufficient conditions for the existence and uniqueness of solutions are constructed by utilizing well-known classical fixed point theorems such as the Banach contraction principle, and Leray-Schauder nonlinear alternative. The generalized singular Gronwall's inequality is used to show the MLU stability results. An illustrated example is provided to support the main findings.
Differential equations (DEs) involving fractional operators of different orders have recently been studied by a number of scientific researchers because of the fact that they are valuable tools in the modeling of numerous problems in sciences and engineering such as biology, chemistry, physics, economics, signal and control theory, etc. The readers might refer to [13,14,18] for more information and the references therein. By utilizing diverse nonlinear analysis techniques, many researchers have identified the uniqueness and existence of solutions for numerous classes of DEs of fractional order. For more details, see [3,6,8,9,12,16,17,19]. Stability analysis, on the other hand, is usually one of the most popular essential concerns in the concept and utilization of fractional differential equations (FDEs). Several authors have recently become interested in the Ulam and MLU-stability concerns, we refer to the papers [1,2,7,8,21,22,23,24] and the references therein. Following the concerns raised in this work, we will focus on a significant area of differential problems widely used in engineering and other scientific fields. The equation is referred to as the pantograph equation. For additional details and uses of the pantograph equation, we recommend reading works [10,11,20,25,26,27,28,29,30,31,32,33]. It's worth mentioning that the standard expression of the pantograph equation is
{w′(τ)=Aw(τ)+Bw(ωτ),w(0)=w0,0≤τ≤T, 0<ω<1. |
Some scholars have studied several versions of the above pantograph equation. For example, the researchers examined the following multi-pantograph equation in [20,25]
w′(τ)=Aw(τ)+n∑i=1νi(τ)w(ωiτ)+e(τ), τ≥0. |
In [20], the authors investigated the non-linear neutral pantograph equation
{w′(τ)=ψ(τ,w(τ),w(ωτ),w′(ωτ)),w(0)=w0,0≤τ≤T, 0<ω<1. |
Recently, in [4] the author evaluated the pantograph type's following difficulty
{CDqw(τ)=ψ(τ,w(τ),z(ωτ)),w(0)=w0,0≤τ≤T, 0<q<1,0<ω<1, |
where CDq denote Caputo fractional derivative. The following sequential fractional pantograph equation is the subject of the current work, which examines the uniqueness, existence, and MLU-stability of solutions.
{RLDδ(CDϑ(CDθw(t)))=Aψ(τ,w(τ),w(ωτ))+BIα[ϕ(τ,w(τ),w(ϖτ))],w(0)=0,λ1w(1)−λ2w(η)=φ(w),CDθw(0)=0,0<η<1,β,λ1,λ2∈R,τ∈[0,1],0<δ,ϑ,θ≤1,α≥0,0<ω,ϖ<1,A,B∈R,λ1≠λ2ηδ+ϑ+θ−1, | (1.1) |
where RLDδ,CDq,q∈{ϑ,θ} stand for the fractional derivatives of Riemann-Liouville (RL) and Caputo, ϕ,ψ:[0,1]×R×R→R and φ:C([0,1],R)→R are continuous functions. RLDδ [15,18], is defined by
RLDδy(τ)=1Γ(n−δ)(ddτ)n∫τ0(τ−s)n−δ−1y(s)ds,n=[δ]+1, |
where Γ(.) represents Euler gamma function. The operator, CDq[15,18], is defined by
CDqy(τ)=1Γ(n−q)∫τ0(τ−s)n−q−1y(n)(s)ds,n=[q]+1, |
and the RL fractional integral [15,18] of order α>0, stated as
Iϑy(τ)=1Γ(ϑ)∫τ0(τ−s)ϑ−1y(s)ds, τ>0. |
Following are several lemmas that we notice [13,18].
Lemma 1. Let q,p>0 and y∈L1([0,1]). Then IqIpy(τ)=Iq+py(τ) and DqIqy(τ)=y(τ).
Lemma 2. Let q>p>0 and y∈L1([0,1]). Then DpIqy(τ)=Iq−py(τ).
Also, we recall the observing lemmas.
Lemma 3. [13] Let δ>0. Then for w∈C(0,1)∩L1(0,1) and RLDδw∈C(0,1)∩L1(0,1), we have
Iδ[RLDδw(τ)]=w(τ)+n∑i=1ciτδ−i, |
where ci∈R, i=1,2,...,n,n=[δ]+1.
Lemma 4. [13] Let q>0. Then
Iq[CDqw(τ)]=w(τ)+n−1∑i=0ciτi, |
for some ci∈R, i=0,1,2,...,n−1,n=[q]+1.
In what follow, we require an important singular type Gronwall inequality.
Theorem 5. [15] For each τ∈[0,1). If
u(τ)≤p(τ)+n∑i=1ki(τ)∫τ0(τ−s)εi−1u(s)ds, |
where all of the functions are continuous and non-negative. The costants εi>0, ki (i=1,2,...,n) are monotonic increasing and bounded functions on [0,1), then
u(τ)≤p(τ)+∞∑j=1(n∑1′,2′,...,j′=1j∏i=1[ki′(τ)Γ(εi′)]Γ(j∑i=1εi′)∫τ0(τ−s)j∑i=1εi′−1p(s)ds). |
Remark 6. For n=2, if ε1,ε2>0,k1,k2≥0,p(τ) is locally integrable and non-negative on [0,1) and u(τ) is locally integrable and non-negative on [0,1) with
u(τ)≤p(τ)+k1∫τ0(τ−s)ε1−1u(s)ds+k2∫τ0(τ−s)ε2−1u(s)ds, |
then
u(τ)≤p(τ)+∞∑j=1((k1Γ(ε1))jΓ(jε1)∫τ0(τ−s)jε1−1p(s)ds+(k2Γ(ε2))jΓ(jε2)∫τ0(τ−s)jε2−1p(s)ds). |
Remark 7. Let p(τ) be a non-decreasing function on [0,1) under the criteria of Remark 6. Then we have
u(τ)≤p(τ)(Eε1[k1Γ(ε1)τε1]+Eε2[k2Γ(ε2)τε2]), |
where the Mittag-Leffler function, Eε[24] defined by: Eε[x]=∑∞j=1xεΓ(jε+1),x∈C.
The subsequent auxiliary result is also necessary.
Lemma 8. Suppose that y(τ)∈C([0,1],R) and let's examine the fractional problem
RLDδ(CDϑ(CDθ)w(τ))=y(τ), τ∈[0,1], 0<δ,ϑ,θ≤1, | (1.2) |
with the condition
w(0)=0,λ1w(1)−λ2w(η)=φ(w),CDθw(0)=0. | (1.3) |
Then, we have
w(τ)=1Γ(δ+ϑ+θ)∫τ0(τ−s)δ+ϑ+θ−1y(s)ds+τδ+ϑ+θ−1λ1−λ2ηδ+ϑ+θ−1[λ2Γ(δ+ϑ+θ)∫η0(η−s)δ+ϑ+θ−1y(s)ds−λ1Γ(δ+ϑ+θ)∫10(1−s)δ+ϑ+θ−1y(s)ds]+tδ+ϑ+θ−1λ1−λ2ηδ+ϑ+θ−1φ(w). | (1.4) |
Proof. Utilizing Lemma 3 and the RL fractional integral of order δ on both sides of Eq (1.2), we obtain
CDϑ(CDθ)w(τ)=Iδy(τ)+c1τδ−1 | (1.5) |
where c1∈R. Next, using Lemma 4 and the RL fractional integral of order ϑ on both sides of Eq (1.5), we obtain
CDθw(τ)=Iδ+ϑy(τ)+Γ(δ)c1Γ(δ+ϑ)τδ+ϑ−1+c2, | (1.6) |
where c2∈R. When both sides of Eq (1.6) are solved using the RL fractional integral of order θ, we obtain
w(τ)=Iδ+ϑ+θy(τ)+Γ(δ)c1Γ(δ+ϑ+θ)τδ+ϑ+θ−1+c2Γ(θ+1)τθ+c3,c3∈R. | (1.7) |
Using (1.3), we obtain
c1=Γ(δ+ϑ+θ)(λ1−λ2ηδ+ϑ+θ−1)Γ(δ)[φ(w)+λ2Iδ+ϑ+θy(η)−λ1Iδ+ϑ+θy(1)], |
and
c2=c3=0, |
inserting the values of c0,c1 and c2 in (1.7) provides the solution (1.4).
Under this section, let's look at the sequential fractional pantograph problem using fixed point theory.
So, we need to introduce the following space.
Let Z=C([0,1],R), the space of continuous Banach functions from [0,1] into R with the norm, ‖w‖ where ‖w‖=sup{|w(τ)|:τ∈[0,1]}. We construct operator O:Z→Z in the context of Lemma 8 by
Ow(τ)=AΓ(δ+ϑ+θ)∫τ0(τ−s)δ+ϑ+θ−1ψ(s,w(s),w(ωs))ds+BΓ(δ+ϑ+θ+α)∫τ0(τ−s)δ+ϑ+θ+α−1ϕ(s,w(s),w(ϖs))ds+τδ+ϑ+θ−1λ1−λ2ηδ+ϑ+θ−1[λ2AΓ(δ+ϑ+θ)∫η0(η−s)δ+ϑ+θ−1ψ(s,w(s),w(ωs))ds+λ2BΓ(δ+ϑ+θ+α)∫η0(η−s)δ+ϑ+θ+α−1ϕ(s,w(s),w(ϖs))ds−λ1AΓ(δ+ϑ+θ)∫10(1−s)δ+ϑ+θ−1ψ(s,w(s),w(ωs))ds−λ1BΓ(δ+ϑ+θ+α)∫10(1−s)δ+ϑ+θ+α−1ϕ(s,w(s),w(ϖs))ds]+τδ+ϑ+θ−1λ1−λ2ηδ+ϑ+θ−1φ(w). | (2.1) |
For convenience, we consider the following hypotheses:
(H1) Continuous functions: ψ,ϕ:[0,1]×R×R→R and ∃ constants μi>0,i=1,2 such that for each τ∈[0,1] and zj,wj∈R,j=1,2
|ψ(τ,z1,z2)−ψ(τ,w1,w2)|≤μ1(|z1−w1|+|z2−w2|),|ϕ(τ,z1,z2)−ϕ(τ,w1,w2)|≤μ2(|z1−w1|+|z2−w2|). |
(H2) φ:C([0,1],R)→R is continuous function with φ(0)=0 and ∃ a constant σ>0 such that
|φ(z)−φ(w)|≤σ|z−w|, z,w∈C([0,1],R). |
We also introduce the notations shown below:
Δ1:=|A|Γ(δ+ϑ+θ+1)[1+1|λ1−λ2ηδ+ϑ+θ−1|(|λ2|ηδ+ϑ+θ+|λ1|)],Δ2:=|B|Γ(δ+ϑ+θ+α+1)[1+1|λ1−λ2ηδ+ϑ+θ−1|(|λ2|ηδ+ϑ+θ+α+|λ1|)]. | (2.2) |
The first result of our existence is based on Banach's principle of contraction.
Theorem 9. If (Hi),i=1,2, are satisfied and also
2μ(Δ1+Δ2)<1−σ|λ1−λ2ηϑ+θ|, | (2.3) |
where μ=max{μi,i=1,2} and Δi,i=1,2, are given by (2.2), then problem (1.1) has a unique solution on [0,1].
Proof. Let's define Λ=max{Λi:i=1,2}, where Λi are finite numbers given by
Λ1=supτ∈[0,1]|ψ(τ,0,0)|and Λ2=supτ∈[0,1]|ϕ(τ,0,0)|. |
Setting
r≥ΛΔ1+ΛΔ21−(2μ(Δ1+Δ2)+σ|λ1−λ2ηδ+ϑ+θ−1|), |
we demonstrate that OBr⊂Br, where Br={w∈Z:‖w‖≤r}.
For w∈Br and for each τ∈[0,1], by using the hypothesis (Hi),i=1,2, we can write
|ψ(τ,w(τ),w(λτ))|≤|ψ(τ,w(τ),w(ωτ))−ψ(τ,0,0)|+|ψ(τ,0,0)|≤2μ1‖w‖+Λ1≤2μ1r+Λ1,|ϕ(τ,w(τ),w(ϖτ))|≤|ϕ(τ,w(τ),w(μτ))−φ(τ,0,0)|+|φ(τ,0,0)|≤2μ2‖w‖+Λ2≤2μ2r+Λ2, |
and
|φ(w)|≤σ‖w‖≤σr. |
Using these estimates, we obtain
‖O(w)‖≤supτ∈[0,1]{|A|Γ(δ+ϑ+θ)∫τ0(τ−s)δ+ϑ+θ−1|ψ(s,w(s),w(ωs))|ds+|B|Γ(δ+ϑ+θ+α)∫τ0(τ−s)δ+ϑ+θ+α−1|ϕ(s,w(s),w(ϖs))|ds+τδ+ϑ+θ−1|λ1−λ2ηδ+ϑ+θ−1|[|λ2||A|Γ(δ+ϑ+θ)∫η0(η−s)δ+ϑ+θ−1|ψ(s,w(s),w(ωs))|ds+|λ2||B|Γ(δ+ϑ+θ+α)∫η0(η−s)δ+ϑ+θ+α−1|ϕ(s,w(s),w(ϖs))|ds+|λ1||A|Γ(δ+ϑ+θ)∫10(1−s)δ+ϑ+θ−1|ψ(s,w(s),w(ωs))|ds+|λ1||B|Γ(δ+ϑ+θ+α)∫10(1−s)δ+ϑ+θ+α−1|ϕ(s,w(s),w(ϖs))|ds]+τδ+ϑ+θ−1|λ1−λ2ηδ+ϑ+θ−1||φ(w)|}≤(2μr+Λ)|A|Γ(δ+ϑ+θ+1)[1+1|λ1−λ2ηδ+ϑ+θ−1|(|λ2|ηδ+ϑ+θ+|λ1|)]+(2μr+Λ)|B|Γ(δ+ϑ+θ+α+1)[1+1|λ1−λ2ηδ+ϑ+θ−1|(|λ2|ηδ+ϑ+θ+|λ1|)]+σr|λ1−λ2ηδ+ϑ+θ−1|=(2μ(Δ1+Δ2)+σ|λ1−λ2ηδ+ϑ+θ−1|)r+Λ(Δ1+Δ2)≤r |
⇒ OBr⊂Br. Now, for w,z∈Br, we obtain
‖O(w)−O(z)‖≤supτ∈[0,1]{|A|Γ(δ+ϑ+θ)∫τ0(τ−s)δ+ϑ+θ−1|ψ(s,w(s),w(ωs))−ψ(s,z(s),z(ωs))|ds+|B|Γ(δ+ϑ+θ+α)∫τ0(τ−s)δ+ϑ+θ+α−1|ϕ(s,w(s),w(ϖs))−ϕ(s,z(s),z(ϖs))|ds+τδ+ϑ+θ−1|λ1−λ2ηδ+ϑ+θ−1|[+|λ2||A|Γ(δ+ϑ+θ)∫η0(η−s)δ+ϑ+θ−1|ψ(s,w(s),w(ωs))−ψ(s,z(s),z(ϖs))|ds+|λ2||B|Γ(δ+ϑ+θ+α)∫η0(η−s)δ+ϑ+θ+α−1|ϕ(s,w(s),w(ϖs))−ϕ(s,z(s),z(ϖs))|ds+|λ1||A|Γ(δ+ϑ+θ)∫10(1−s)δ+ϑ+θ−1|ψ(s,w(s),w(ωs))−ψ(s,z(s),z(ωs))|ds+|λ1||B|Γ(δ+ϑ+θ+α)∫10(1−s)δ+ϑ+θ+α−1|ϕ(s,w(s),w(ϖs))−ϕ(s,z(s),z(ϖs))|ds]+τδ+ϑ+θ−1|λ1−λ2ηδ+ϑ+θ−1||φ(w)−φ(z)|}≤(2μ(Δ1+Δ2)+σ|λ1−λ2ηδ+ϑ+θ−1|)‖w−z‖, |
in context of condition 2μ(Δ1+Δ2)+σ|λ1−λ2ηδ+ϑ+θ−1|<1, this demonstrates that O is a contraction. The operator O possesses an unique fixed point that corresponds to an unique solution to the problem according to Banach's fixed point theorem (1.1). The Leray-Schauder alternative yielded the second main result.
Lemma 10. [5] Let Q:X→X be a completely continuous operator. Let G(Q)={u∈X:u=ρQ(u) for some 0<ρ<1}. Then either the set G(Q) is unbounded, or Q has at least one fixed point (Leray-Schauder alternative).
For the forthcoming result, we suppose that
(H3) ψ,ϕ:[0,1]×R×R→R are continuous and ∃ real constants πi,γi≥0,i=1,2 and π0>0,γ0>0 such that for any wi∈R,i=1,2, we have
|φ(τ,w1,w2)|≤π0+π1|w1|+π2|w2|, |
and
|ϕ(τ,w1,w2)|≤γ0+γ1|w1|+γ2|w2|. |
(H4) φ:C([0,1],R)⟶R is continuous function with φ(0)=0 and ∃ constant ϵ>0 such that
|φ(w)|≤ϵ‖w‖ for all w∈C([0,1],R). |
Theorem 11. If (Hi),i=3,4, are satisfied and also
(π1+π2)Δ1+(γ1+γ2)Δ2+ϵ|λ1−λ2ηδ+ϑ+θ−1|<1, | (2.4) |
then on [0,1] the problem (1.1) has at least one solution.
Proof. We demonstrate that the operator O:Z⟶Z is completely continuous in the first step. Since the functions ψ,ϕ and φ are continuous, the operator O is also continuous.
Let Θ⊂W be bounded. Then ∃ positive constants Mi,(i=1,2) such that
|φ(τ,w,z)|≤M1,|ϕ(τ,w,z)|≤M2, |
for each w,z∈Θ and constants N such that |ψ(w)|≤N for all z∈C([0,1],R). Then for any w∈Θ and by (Hi),i=3,4, we have
‖Ow‖≤M1|A|Γ(δ+ϑ+θ+1)[1+1|λ1−λ2ηδ+ϑ+θ−1|(|λ2|ηδ+ϑ+θ+|λ1|)]+M2|B|Γ(δ+ϑ+θ+α+1)[1+1|λ1−λ2ηδ+ϑ+θ−1|(|λ2|ηδ+ϑ+θ+α+|λ1|)]+N|λ1−λ2ηδ+ϑ+θ−1|, |
which implies that
‖O(z)‖≤M1Δ1+M2Δ2+N|λ1−λ2ηδ+ϑ+θ−1|. |
The operator O is uniformly bounded, as shown in the above Eq (2.1).
As a follow-up, we demonstrate that O is equicontinuous sets of Z. Let τ1,τ2∈[0,1] with τ1<τ2. Next, we obtain
|Ow(τ2)−Ow(τ1)|≤M1|A|Γ(δ+ϑ+θ+1)[(τ2−τ1)δ+ϑ+θ+|τδ+ϑ+θ2−τδ+ϑ+θ1|]+M2|B|Γ(δ+ϑ+θ+α+1)[(τ2−τ1)δ+ϑ+θ+α+|τδ+ϑ+θ+α2−τδ+ϑ+θ+α1|]+|τδ+ϑ+θ−12−τδ+ϑ+θ−11||λ1−λ2ηδ+ϑ+θ−1|(|λ2||A|ηδ+ϑ+θΓ(δ+ϑ+θ+1)+|λ2||B|ηδ+ϑ+θ+αΓ(δ+ϑ+θ+α+1)+|λ1||A|Γ(δ+ϑ+θ+1)+|λ1||B|Γ(δ+ϑ+θ+α+1)+N), |
which does not depend on w and tends to 0 as τ2−τ1→0. Thus, O is equicontinuous. Thus, by using the Arzelá-Ascoli theorem, O:Z→Z is completely continuous.
Finally, we demonstrate that the set, χ={w∈Z:w=ϱO(w), 0<ϱ<1}, is bounded. Let w∈χ, then w=ϱO(w).For each τ∈[0,1], we have
w(τ)=ϱOw(τ). |
Then,
|w(τ)|≤[π0+(π1+π2)‖w‖]|A|Γ(δ+ϑ+θ+1)[1+1|λ1−λ2ηδ+ϑ+θ−1|(|λ2|ηδ+ϑ+θ+|λ1|)]+[γ0+(γ1+γ2)‖w‖]|B|Γ(δ+ϑ+θ+α+1)[1+1|λ1−λ2ηδ+ϑ+θ−1|(|λ2|ηδ+ϑ+θ+α+|λ1|)]+ϵ|λ1−λ2ηδ+ϑ+θ−1|‖w‖ |
which implies
‖w‖≤[π0+(π1+π2)‖w‖]Δ1+[γ0+(γ1+γ2)‖w‖]Δ2+ϵ|λ1−λ2ηδ+ϑ+θ−1|‖w‖=[(π1+π2)Δ1+(γ1+γ2)Δ2+ϵ|λ1−λ2ηδ+ϑ+θ−1|]‖w‖+π0Δ1+γ0Δ2. |
Consequently,
‖w‖≤π0Δ1+γ0Δ21−[(π1+π2)Δ1+(γ1+γ2)Δ2+ϵ|λ1−λ2ηδ+ϑ+θ−1|]. |
This implies that χ is bounded. According to Lemma 10, this indicates that the operator O contains at least one fixed point. The problem (1.1) on [0,1] has hence at least one solution in this case. Hence, the proof is completed.
The MLUS of the sequential fractional problem (1.1) will be defined and studied in this section. For τ∈[0,1], we provide the following fractional inequalities:
|RLDδ(CDϑ(CDθz(τ)))−Aψ(τ,z(τ),z(ωτ))−BIα[ϕ(τ,z(τ),z(ϖτ))]|≤κ, | (3.1) |
and
|RLDδ(CDϑ(CDθz(τ)))−Aψ(τ,z(τ),z(ωτ))−BIα[ϕ(τ,z(τ),z(ϖτ))]|≤κm(τ), | (3.2) |
where κ∈R+ and m:[0,1]→R+ is continuous function.
Definition 12. The problem (1.1) is MLU-Hyers stable, with respect to Eδ+ϑ+θ if ∃ a real number υ such that for each κ>0 and for each solution z∈Z of the inequality (3.1), ∃ a solution w∈Z of the problem (1.1) with
|z(τ)−w(τ)|≤υκEδ+ϑ+θ[τ], τ∈[0,1]. |
Definition 13. The problem (1.1) is MLU-Hyers-Rassias stable, with respect to mEδ+ϑ+θ if ∃ a real number υm>0 such that for each κ>0 and for each solution z∈Z of the inequality (3.2), ∃ a solution w∈Z of problem (1.1) with
|z(τ)−w(τ)|≤υmκm(τ)Eδ+ϑ+θ[τ], τ∈[0,1]. |
Remark 14. A function z∈Z is a solution of the inequality (3.1) if and only if ∃ a function f∈C([0,1],R) (which depend on z) such that
|f(τ)|≤κ, τ∈[0,1], |
and
CDδ(CDϑ(CDθz(τ)))−Aψ(τ,z(τ),z(ωτ))+BIα[ϕ(τ,z(τ),z(ϖτ))]=f(τ), τ∈[0,1]. |
Theorem 15. If hypotheses (Hi),i=1,2, are satisfied, then the problem (1.1) is MLU-Hyers stable.
Proof. Let z∈Z represent the inequality's (3.1) solution and let w∈Z represents the unique solution of the problem
{RLDδ(CDϑ(CDθw(τ)))=Aψ(τ,w(τ),w(ωτ))+BIα[ϕ(τ,w(τ),w(ϖτ))],w(0)=0,λ1w(1)−λ2w(η)=φ(w),CDθw(0)=0,0<η<1,β,λ1,λ2∈R,τ∈[0,1],0<δ,ϑ,θ≤1,α≥0,0<ω,ϖ<1,A,B∈R,λ1≠λ2ηδ+ϑ+θ−1. |
According to Lemma 8, we have
w(τ)=Iδ+ϑ+θy(τ)+Γ(δ)c1τδ+ϑ+θ−1Γ(δ+ϑ+θ)+c2τθΓ(θ+1)+c3,ci∈R,i=1,2,3. |
By integrating the inequality (3.1), we obtain
|z(τ)−Iδ+ϑ+θyz(τ)−Γ(δ)a1τδ+ϑ+θ−1Γ(δ+ϑ+θ)−a2τθΓ(θ+1)−a3|≤κτδ+ϑ+θΓ(δ+ϑ+θ+1)≤κΓ(δ+ϑ+θ+1), | (3.3) |
where
yz(τ)=Aψ(τ,z(τ),z(ωτ))+BIα[ϕ(τ,z(τ),z(ϖτ))]. |
Latter, if w(0)=z(0),w(ω)=z(ω) and CDθw(0)= CDθz(0), then c1=a1,c2=a2 and c3=a3.
For each τ∈[0,1], we have
|z(τ)−w(τ)|=|z(τ)−Iδ+ϑ+θyz(τ)−Γ(δ)a1τδ+ϑ+θ−1Γ(δ+ϑ+θ)−a2τθΓ(θ+1)−a3+Iδ+ϑ+θ[yz(τ)−yw(τ)]|≤|z(τ)−Iδ+ϑ+θyz(τ)−Γ(δ)a1τδ+ϑ+θ−1Γ(δ+ϑ+θ)−a2τθΓ(θ+1)−a3|+|Iδ+ϑ+θ[yz(τ)−yw(τ)]|, |
then
|Iδ+ϑ+θ[yz(τ)−yw(τ)]|≤|A|Γ(δ+ϑ+θ)∫τ0(τ−s)δ+ϑ+θ−1|ψ(τ,z(τ),z(ωτ))−ψ(τ,w(τ),w(ωτ))|ds+|B|Γ(δ+ϑ+θ+α)∫τ0(τ−s)δ+ϑ+θ+α−1|ϕ(s,z(s),z(ϖs))−ϕ(s,w(s),w(ϖs))|ds. |
Using (H1), we get
|Iδ+ϑ+θ[yz(τ)−yw(τ)]|≤2|A|μ1Γ(δ+ϑ+θ)∫τ0(τ−s)δ+ϑ+θ−1|z(τ)−w(τ)|ds+2|B|μ2Γ(δ+ϑ+θ+α)∫τ0(τ−s)δ+ϑ+θ+α−1|z(τ)−w(τ)|ds. | (3.4) |
By using (3.3) and (3.4), we have got
|z(τ)−w(τ)|≤κΓ(δ+ϑ+θ+1)+2|A|μ1Γ(δ+ϑ+θ)∫τ0(τ−s)δ+ϑ+θ−1|z(τ)−w(τ)|ds+2|B|μ2Γ(δ+ϑ+θ+α)∫τ0(τ−s)δ+ϑ+θ+α−1|z(τ)−w(τ)|ds. |
According to Remarks 6 and 7, we have got
|z(τ)−w(τ)|≤κΓ(δ+ϑ+θ+1)(Eδ+ϑ+θ[2|A|μ1τδ+ϑ+θ]+Eδ+ϑ+θ+α[2|B|μ2τδ+ϑ+θ+α])=υκ(Eδ+ϑ+θ[2|A|μ1τδ+ϑ+θ]+Eδ+ϑ+θ+α[2|B|μ2τδ+ϑ+θ+α]). |
As a result, the problem (1.1) is MLU-Hyers stable.
Theorem 16. If hypotheses (Hi),i=1,2, are satisfied. Suppose there exists υm>0 such that
1Γ(δ+ϑ+θ)∫t0(t−s)δ+ϑ+θ−1m(s)ds≤υmm(t),t∈[0,1], | (3.5) |
where m∈C([0,1],R+) is increasing. Then the problem (1.1) is Mittag-Leffler-Ulam-Hyers-Rassias stable with respect to mEδ+ϑ+θ.
Proof. By integrating the inequality (3.2), we have
|z(τ)−Iδ+ϑ+θyz(τ)−Γ(δ)a1tδ+ϑ+θ−1Γ(δ+ϑ+θ)−a2τθΓ(θ+1)−a3|≤κΓ(δ+ϑ+θ)∫τ0(τ−s)δ+ϑ+θ−1m(s)ds, |
where the inequality (3.2) has z∈Z as a solution. Let's call the unique solution to the problem w∈Z
{CDδ(CDϑ(CDθw(τ)))=Aψ(τ,w(τ),w(ωτ))+BIα[ϕ(τ,w(τ),w(ϖτ))],τ∈[0,1]w(1)=z(1),w(0)=z(0),w(η)=z(η),CDθw(0)=CDθz(0),0<η<1. |
We have
w(τ)=Iδ+ϑ+θyw(τ)+Γ(δ)c1τδ+ϑ+θ−1Γ(δ+ϑ+θ)+c2τθΓ(θ+1)+c3. |
Then
|z(τ)−w(τ)|≤κΓ(δ+ϑ+θ)∫τ0(τ−s)δ+ϑ+θ−1m(s)ds+2|A|μ1Γ(δ+ϑ+θ)∫τ0(τ−s)δ+ϑ+θ−1|z(τ)−w(τ)|ds+2|B|μ2Γ(δ+ϑ+θ+α)∫τ0(τ−s)δ+ϑ+θ+α−1|z(τ)−w(τ)|ds. |
From (3.5), as it can be observed,
|z(τ)−w(τ)|≤κυmm(τ)+2|A|μ1Γ(δ+ϑ+θ)∫τ0(τ−s)δ+ϑ+θ−1|z(τ)−w(τ)|ds+2|B|μ2Γ(δ+ϑ+θ+α)∫τ0(τ−s)δ+ϑ+θ+α−1|z(τ)−w(τ)|ds. |
Now, by Remarks 6 and 7, we have got
|z(τ)−w(τ)|≤κυmm(τ)(Eδ+ϑ+θ[2|A|μ1τδ+ϑ+θ]+Eδ+ϑ+θ+α[2|B|μ2τδ+ϑ+θ+α]). |
The problem (1.1) is therefore MLU-Hyers-Rassias stable.
Take the fractional pantograph problem below into consideration:
{RLD45 C(CD12(CD23w(τ)))=e−237π2(15+e−2τ45πe2sinw(τ)+e−2τ45πe2cosw(1011τ))+147e3I√52[1113+1√402+τ2w(τ)+e−τ40+τ2sinw(1312τ)],τ∈[0,1],w(0)=0,43w(1)−32w(56)=145w(τ),CDθw(0)=√34, | (4.1) |
and the following fractional inequalities
|RLD45(CD12(CD23z(τ)))−e−237π2ψ(τ,z(τ),z(ωτ)) |
−147e3I√52[ϕ(τ,z(τ),z(ϖτ))]|≤κ, |
and
|RLD45(CD12(CD23z(τ)))−e−237π2ψ(τ,z(τ),z(ωτ)) |
−147e3I√52[ϕ(τ,z(τ),z(ϖτ))]|≤κm(τ), |
where
ψ(τ,z(τ),z(ωτ))=15+e−2τ45πe2sinz(τ)+e−2τ45πe2cosz(ωτ),ϕ(τ,z(τ),z(ϖτ))=1113+1√(40e2)2+τ2z(τ)+e−τ40e2+τ2sinz(ϖτ), |
and
δ=45,ϑ=12,θ=23,α=√52, |
A=e−237π2,φ(w)=145w(τ),B=147e3, |
λ1=43,λ2=32,ω=1011,ϖ=1312, |
η=56,β=√34,λ1≠λ2ηδ+ϑ+θ−1. |
For each τ∈[0,1] and wj,zj∈R,j=1,2, we have
|ψ(τ,w1(τ),w2(λτ))−ψ(τ,z1(τ),z2(λτ))|≤145πe2(|w1−z1|+|w2−z2|),|ϕ(τ,w1(τ),w2(λτ))−ϕ(τ,z1(τ),z2(λτ))|≤140e2(|w1−z1|+|w2−z2|), |
and
|φ(w1)−φ(z1)|≤145|w1−z1|, |
hence conditions (H1) and (H2) hold with μ1=145πe2,μ2=140e2 and σ=145 respectively.
With the given data, it is found that
μ=max{μi,i=1,2}=140e2, λ1−λ2ηδ+ϑ+θ−1=7.5713×10−2,Δ1=6.200×10−3, Δ2=4.7412×10−3. |
Thus condition
2μ(Δ1+Δ2)=7.4037×10−5<1−σ|λ1−λ2ηδ+ϑ+θ−1|=0.70649, |
is satisfied. Therefore, the problem (4.1) has a unique solution on [0,1], according to Theorem 9, and is MLU-Hyers stable with
|z(τ)−w(τ)|≤κΓ(8930)(E5930[2e−21665π3e2τ5930]+E118+30√560[1940e5τ118+30√560]),τ∈[0,1]. |
Let m(τ)=τ2, then
I45+12+23m(τ)=I45+12+23(τ2)=2Γ(14930)τ2+45+12+23≤2Γ(14930)τ2=υmm(τ). |
Thus condition (3.4) is satisfied with m(τ)=τ2 and υm=2Γ(14930). Thus, Theorem 16 demonstrates that problem (4.1) is MLU-Hyers-Rassias stable with
|z(τ)−w(τ)|≤κτ2Γ(17930)(E5930[2e−21665π3e2τ5930]+E118+30√560[1940e5τ118+30√560]),τ∈[0,1]. |
In this work, we considered pantograph equations with three sequential fractional derivatives. The existence and Mittag-Leffler-Ulam stability of solutions have been discussed. The existence results of the solutions for the mentioned problem were investigated by the contraction mapping principle and Leray-Schauder's alternative. The Mittag-Leffler-Ulam-Hyers stability and Mittag-Leffler-Ulam-Hyers-Rassias stability results have been proved by applying generalized singular Gronwall's inequality. The main results were illustrated with the aid of an example.
Authors would like to express gratitude to Central university of Punjab, India-151401 to encourage us for the research work. The authors Aziz Khan and Thabet Abdeljawad would like to thanks Prince Sultan University for paying the APC and the support through TAS research lab.
The publication of this paper, according to the author, is free from any conflicts of interest.
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