A problem with integral boundary conditions (IBVP) involving conformable fractional derivatives is considered in this article. The upper and lower solutions technique is used to discuss the existence and uniqueness of positive solutions. The fixed point Theorem of Schauder proves the existence of positive solutions, and the fixed point Theorem of Banach proves the uniqueness of solutions. Our results are illustrated by an example.
Citation: Mouataz Billah Mesmouli, Taher S. Hassan. On the positive solutions for IBVP of conformable differential equations[J]. AIMS Mathematics, 2023, 8(10): 24740-24750. doi: 10.3934/math.20231261
[1] | Tingting Guan, Guotao Wang, Haiyong Xu . Initial boundary value problems for space-time fractional conformable differential equation. AIMS Mathematics, 2021, 6(5): 5275-5291. doi: 10.3934/math.2021312 |
[2] | Changlong Yu, Jufang Wang, Huode Han, Jing Li . Positive solutions of IBVPs for $ q $-difference equations with $ p $-Laplacian on infinite interval. AIMS Mathematics, 2021, 6(8): 8404-8414. doi: 10.3934/math.2021487 |
[3] | Youness Chatibi, El Hassan El Kinani, Abdelaziz Ouhadan . Lie symmetry analysis of conformable differential equations. AIMS Mathematics, 2019, 4(4): 1133-1144. doi: 10.3934/math.2019.4.1133 |
[4] | Jan Nordström, Fredrik Laurén, Oskar Ålund . An explicit Jacobian for Newton's method applied to nonlinear initial boundary value problems in summation-by-parts form. AIMS Mathematics, 2024, 9(9): 23291-23312. doi: 10.3934/math.20241132 |
[5] | Mahmoud Abul-Ez, Mohra Zayed, Ali Youssef . Further study on the conformable fractional Gauss hypergeometric function. AIMS Mathematics, 2021, 6(9): 10130-10163. doi: 10.3934/math.2021588 |
[6] | Abdelouaheb Ardjouni . Positive solutions for nonlinear Hadamard fractional differential equations with integral boundary conditions. AIMS Mathematics, 2019, 4(4): 1101-1113. doi: 10.3934/math.2019.4.1101 |
[7] | Rabha W. Ibrahim, Jay M. Jahangiri . Conformable differential operator generalizes the Briot-Bouquet differential equation in a complex domain. AIMS Mathematics, 2019, 4(6): 1582-1595. doi: 10.3934/math.2019.6.1582 |
[8] | Xiulin Hu, Lei Wang . Positive solutions to integral boundary value problems for singular delay fractional differential equations. AIMS Mathematics, 2023, 8(11): 25550-25563. doi: 10.3934/math.20231304 |
[9] | Mustafa Inc, Hadi Rezazadeh, Javad Vahidi, Mostafa Eslami, Mehmet Ali Akinlar, Muhammad Nasir Ali, Yu-Ming Chu . New solitary wave solutions for the conformable Klein-Gordon equation with quantic nonlinearity. AIMS Mathematics, 2020, 5(6): 6972-6984. doi: 10.3934/math.2020447 |
[10] | Yun Xin, Hao Wang . Positive periodic solution for third-order singular neutral differential equation with time-dependent delay. AIMS Mathematics, 2020, 5(6): 7234-7251. doi: 10.3934/math.2020462 |
A problem with integral boundary conditions (IBVP) involving conformable fractional derivatives is considered in this article. The upper and lower solutions technique is used to discuss the existence and uniqueness of positive solutions. The fixed point Theorem of Schauder proves the existence of positive solutions, and the fixed point Theorem of Banach proves the uniqueness of solutions. Our results are illustrated by an example.
Since the inception of the fractional derivatives by the scientist Leibniz in the year 1695, this type of derivative has known development in all branches of mathematics and even included applications in engineering and science (see [3,10,16,18,19,20,21]).
Recently, a new definition has drawn much interest from many researchers, namely conformable fractional derivative introduced in [14] by Khalil et al. Since that time, several equations and applications have been studied and several articles have been published regarding this type of derivative (see [1,4,5,6,7,9,12,17,23,24,25]). Many researchers study existence and positivity problems using the upper and lower solutions technique due to its effectiveness and good results (see [2,8,11,13,15,22]). The upper and lower solutions method is associated with the use of fixed point theory to prove the existence and uniqueness of the solution.
Xu and Sun [22] proved the existence of positive solutions for the IBVP of the fractional differential equations
{Dsy(r)+p(r,y(r))=Ds−1q(r,y(r)), r∈(0,1),y(0)=0, y(1)=∫10q(r,y(r))dr, | (1.1) |
where Ds is the standard Riemann-Liouville derivative and s∈(1,2].
Zhong and Wang [25] used the fixed point theorem in a cone to show the existence of positive solutions of the BVP
{Tsy(r)+p(r,y(r))=0, r∈[0,1],y(0)=0, y(1)=λ∫10y(r)dr, | (1.2) |
where s∈(1,2], Ts denotes the conformable derivative of order s and λ is positive number.
The purpose of this paper is to examine an integral boundary value problem of conformable differential equations defined as follows
{Tsy(r)+p(r,y(r))=Ts−1q(r,y(r)), r∈(0,1),y(0)=0, y(1)=∫10q(r,y(r))dr, | (1.3) |
where s∈(1,2], the functions p,q:[0,1]×[0,∞)→[0,∞) are continuous such that q(r,y) is non-decreasing on y.
In this context, the main contributions of this paper is to apply the conformable derivative introduced in [14] to an integral boundary value problem which is the generalization of the problem (1.2). So, our study is organized as follow. After recalling some definitions and results of the conformable derivative in Section 2, and we give, in Section 3, the proof of our results concerning the existence and uniqueness of positive solutions. In Section 4, we write the conclusion in which we explain the contribution of this research.
The purpose of this section is to provide the most important materials and preliminaries results for understanding conformable derivatives, (See [1,14,25]).
Definition 2.1. [1,14] Let s∈(1,2]. The conformable fractional derivative of a function p:[0,∞)→R of order s is defined by
Tsp(r)=limε→0p(r+εr1−s)−p(r)ε. |
If Tsp(r) exists on (0,∞), then Tsp(0)=limr→0+Tsp(r).
Definition 2.2. [1,14] Let s∈(m,m+1], m∈N0 and function p:[0,∞)→R.
(a) The conformable fractional derivative of a function p of order s is defined by
Tsp(r)=Tβp(m)(r) with β=s−m. |
(b) The fractional integral of a function p of order s is defined by
Isp(r)=1m!∫r0(r−ζ)mζs−m−1p(ζ)dζ. |
Lemma 2.1. [1,25] Let s be in (m,m+1].
(a) If p is a continuous function on [0,∞), then, for all r>0, TsIsp(r)=p(r).
(b) Tsrk=0 for r in [0,1] and k=0,1,2,...,m.
(c) If Tsp(r) is continuous on [0,∞), then
IsTsp(r)=p(r)+c0+c1r+c2r2+...+cmrm, |
for some real numbers ck,k=0,1,2,...,m.
Lemma 2.2. Let y∈C([0,1],R). Then y is a solution of (1.3) if and only if
y(r)=∫r0q(ζ,y(ζ))dζ+∫10Q(r,ζ)p(ζ,y(ζ))dζ, |
where
Q(r,ζ)={(1−r)ζs−1, 0≤ζ≤r≤1,r(1−ζ)ζs−2, 0<r≤ζ≤1. | (2.1) |
Proof. Note that
Ts∫r0q(ζ,y(ζ))dζ=Ts−1q(r,y(r)). |
So
Ts(y(r)−∫r0q(ζ,y(ζ))dζ)+p(r,y(r))=0, r∈(0,1). |
Then, by Lemma 2.1 we have
y(r)−∫r0q(ζ,y(ζ))dζ+c0+c1r=−Isp(r,y(r)), |
the boundary conditions y(0)=0, implies c0=0 and
y(1)−∫10q(ζ,y(ζ))dζ+c1=−∫10(1−ζ)ζs−2p(ζ,y(ζ))dζ, |
c1=−∫10(1−ζ)ζs−2p(ζ,y(ζ))dζ. |
Hence
y(r)=∫r0q(r,y(r))dr+∫10r(1−ζ)ζs−2p(ζ,y(ζ))dζ−∫r0(r−ζ)ζs−2p(ζ,y(ζ))dζ=∫r0q(r,y(r))dr+∫r0r(1−ζ)ζs−2p(ζ,y(ζ))dζ+∫1rr(1−ζ)ζs−2p(ζ,y(ζ))dζ−∫r0(r−ζ)ζs−2p(ζ,y(ζ))dζ=∫r0q(r,y(r))dr+∫r0ζs−1p(ζ,y(ζ))dζ−∫r0rζs−1p(ζ,y(ζ))dζ+∫1rr(1−ζ)ζs−2p(ζ,y(ζ))dζ=∫r0q(r,y(r))dr+∫r0(1−r)ζs−1p(ζ,y(ζ))dζ+∫1rr(1−ζ)ζs−2p(ζ,y(ζ))dζ. |
So,
y(r)=∫r0q(ζ,y(ζ))dζ+∫10Q(r,ζ)p(ζ,y(ζ))dζ. |
Lemma 2.3 ([25]). For any (r,ζ) in (0,1]×(0,1],
0≤ω(r)Q(ζ,ζ)≤Q(r,ζ)≤Q(ζ,ζ), |
where ω(r)=r(1−r).
Let the norm
‖y‖=maxr∈[0,1]|y(r)|, |
of the Banach space X=C([0,1]). Denote Ω:={y∈X:y(r)≥0,r∈[0,1]}.
Let a,b∈R+ with a<b. For any y∈[a,b], we define the upper control function with
U(r,y)=sup{p(r,λ):a≤λ≤y}, |
and the lower control function with
L(r,y)=inf{p(r,λ):y≤λ≤b}. |
Clearly, U(r,y) and L(r,y) are monotonous non-decreasing on y and
L(r,y)≤p(r,y)≤U(r,y). |
We need the following hypothesis:
(A) Let y_(r),¯y(r)∈Ω with a≤y_(r)≤¯y(r)≤b and
y_(r)≤∫r0q(ζ,y_(ζ))dζ+∫10Q(r,ζ)L(ζ,y_(ζ))dζ, |
¯y(r)≥∫r0q(ζ,¯y(ζ))dζ+∫10Q(r,ζ)U(ζ,¯y(ζ))dζ, |
for all r∈[0,1].
The function y_(r) called the lower solution and the function ¯y(r) is the upper solution of (1.3).
We need the following Lemma in the proof of the Theorem below
Lemma 3.1. For each r1,r2∈[0,1], r1<r2, the function Q defined by (2.1) satisfies
∫10|Q(r1,ζ)−Q(r2,ζ)|dζ≤maxs∈(1,2]{1s,1s(s−1),2s−1s(s−1)}|r1−r2|. |
Proof. Let ζ∈[0,1], for each r1,r2∈[0,1], such that r1<r2 we have three cases:
Case 1. For 0≤ζ≤r1<r2≤1, we have
∫10|Q(r1,ζ)−Q(r2,ζ)|dζ=∫10|(1−r1)ζs−1−(1−r2)ζs−1|dζ=|r1−r2|∫10ζs−1dζ=1s|r1−r2|. |
Case 2. For 0≤r1<r2≤ζ≤1, we have
∫10|Q(r1,ζ)−Q(r2,ζ)|dζ=∫10|r1(1−ζ)ζs−2−r2(1−ζ)ζs−2|dζ=|r1−r2|∫10(1−ζ)ζs−2dζ=1s(s−1)|r1−r2|. |
Case 3. For 0≤r1<ζ≤r2≤1
∫10|Q(r1,ζ)−Q(r2,ζ)|dζ=∫10|r1(1−ζ)ζs−2−(1−r2)ζs−1|dζ=∫10|r1ζs−2−r1ζs−1−ζs−1+r2ζs−1|dζ≤∫10(ζs−1|r1ζ−1|+ζs−1|r2−r1|)dζ≤∫10(ζs−1|r1ζ−r2ζ|+ζs−1|r2−r1|)dζ=|r2−r1|∫10(ζs−2+ζs−1)dζ=2s−1s(s−1)|r2−r1|. |
Theorem 3.1. The problem (1.3) has at least one positive solution y∈Ω if (A) holds. Furthermore,
y_(r)≤y(r)≤¯y(r), for all r∈[0,1]. |
Proof. Let
Σ:={y∈Ω:y_(r)≤y(r)≤¯y(r),r∈[0,1]}. |
It is easy to see that ‖y‖≤b, so Σ⊂X is closed, convex and bounded. If y∈Σ, ∃Rp,Rq>0 two constants such that
maxr∈[0,1]p(r,y(r))<Rp, |
and
maxr∈[0,1]q(r,y(r))<Rq. |
From Lemma 2.2 we define the operator ϝ as
ϝy(r)=∫r0q(ζ,y(ζ))dζ+∫10Q(r,ζ)p(ζ,y(ζ))dζ. |
The continuity of p and q give the continuity of the operator ϝ on Σ. Then, for y∈Σ we have
ϝy(r)=∫r0q(ζ,y(ζ))dζ+∫10Q(r,ζ)p(ζ,y(ζ))dζ≤Rq+Rp∫10Q(ζ,ζ)dζ=Rq+Rps(s+1). |
Hence ϝ(Σ) is uniformly bounded.
Now, for each y∈Σ, r1,r2∈[0,1], r1<r2, we get
|(ϝy)(r1)−(ϝy)(r2)|≤|∫r10q(ζ,y(ζ))dζ−∫r20q(ζ,y(ζ))dζ|+∫10|Q(r1,ζ)−Q(r2,ζ)|p(ζ,y(ζ))dζ=Rq|r1−r2|+∫10|Q(r1,ζ)−Q(r2,ζ)|p(ζ,y(ζ))dζ≤(Rq+Rpmaxs∈(1,2]{1s,1s(s−1),2s−1s(s−1)})|r1−r2|. |
Therefore, ϝ(Σ) is equicontinuous. By Ascoli-Arzele Theorem, ϝ:Σ→X is compact.
Next we will show that ϝ(Σ)⊂Σ. Let y∈Σ, then from the hypothesis (A) we get
(ϝy)(r)=∫r0q(ζ,y(ζ))dζ+∫10Q(r,ζ)p(ζ,y(ζ))dζ≤∫r0q(ζ,y(ζ))dζ+∫10Q(r,ζ)U(ζ,y(ζ))dζ≤∫r0q(ζ,¯y(ζ))dζ+∫10Q(r,ζ)U(ζ,¯y(ζ))dζ≤¯y(r). |
Similarly, (ϝy)(r)≥y_(r).
As a conclusion, by the Schauder fixed point theorem, ϝ has at least one fixed point, y∈Σ. So, the Eq (1.3) has at least one positive solution for all y∈X and y_(r)≤y(r)≤¯y(r), for all r∈[0,1].
Corollary 3.1. Assume that there exist continuous functions h1, h2, h3 and h4 such that
0≤h1(r)≤p(r,z)≤h2(r)<∞,(r,z)∈[0,1]×[0,+∞), | (3.1) |
0≤h3(r)≤q(r,z)≤h4(r)<∞,(r,z)∈[0,1]×[0,+∞), | (3.2) |
and at least one of h1(r) and h3(r) is not identically equal to 0. Then (1.3) has at least one positive solution y∈X and
∫r0h3(ζ)dζ+∫10Q(r,ζ)h1(ζ)dζ≤y(r)≤∫r0h4(ζ)dζ+∫10Q(r,ζ)h2(ζ)dζ. | (3.3) |
Proof. Consider the problem
{Tsx(r)+h2(r)=Ts−1h4(r), r∈(0,1),x(0)=0, x(1)=∫10h4(r)dr, | (3.4) |
which is equivalent to
x(r)=∫r0h4(ζ)dζ+∫10Q(r,ζ)h2(ζ)dζ. | (3.5) |
By the definitions of control function, we have
h1(r)≤L(r,x)≤U(r,x)≤h2(r), (r,x)∈[0,1]×[a,b], |
where a,b are minimal and maximal of x(r) on [0,1]. Therefore we have
x(r)≥∫r0q(ζ,x(ζ))dζ+∫10Q(r,ζ)U(ζ,x(ζ))dζ. |
Thus (3.5) is an upper solution of (1.3). On the other hand, we can prove
∫r0h1(ζ)dζ+∫10Q(r,ζ)h3(ζ)dζ, |
is a lower solution of (1.3). According to Theorem 3.1, (1.3) has at least one positive solution y∈X and we obtain (3.3).
Corollary 3.2. Suppose that
(i) (3.2) and 0≤h1(r)≤p(r,z),r∈[0,1] hold,
(ii) p(r,z) uniformly converges to h(r) on [0,1] as z→∞,
(iii) at least one of h1(r) and h3(r) is not identically equal to 0.
Then (1.3) has at least one positive solution y∈X.
Proof. From (ⅱ), there exist η, K>0 such that
|p(r,z)−h(r)|<η,(r,z)∈[0,1]×[K,+∞), |
hence
p(r,z)<h(r)+η,(r,z)∈[0,1]×[K,+∞). |
Let v=max(r,z)∈[0,1]×[0,K]p(r,z), hence
h1(r)≤p(r,z)≤h(r)+η+v,(r,z)∈[0,1]×[0,∞). |
From Corollary 3.1, the IBVP (1.3) has at least one solution, y∈X, satisfies
∫r0h3(ζ)dζ+∫10Q(r,ζ)h1(ζ)dζ≤y(r)≤∫r0h4(ζ)dζ+∫10Q(r,ζ)h(ζ)dζ+η+vs(s+1). |
Theorem 3.2. Let (A) holds and assume that for any r∈[0,1], z,z∗∈Σ,
|p(r,z)−p(r,z∗)|≤Lp‖z−z∗‖, |
|q(r,z)−q(r,z∗)|≤Lq‖z−z∗‖, |
where Lp,Lq>0 are constants satisfie
Lq+Lps(s+1)<1. | (3.6) |
Then the IBVP (1.3) has a unique positive solution on Σ.
Proof. We show in Theorem 3.1 that ϝ:Σ→Σ. So, for any r∈[0,1], z,z∗∈Σ, we have
|(ϝz)(r)−(ϝz∗)(r)|≤∫r0|q(ζ,z(ζ))−q(ζ,z∗(ζ))|dζ+∫10Q(r,ζ)|p(ζ,z(ζ))−p(ζ,z∗(ζ))|dζ≤Lq‖z−z∗‖+Lps(s+1)‖z−z∗‖=(Lq+Lps(s+1))‖z−z∗‖. |
Since (3.6) is hold, then ϝ is a contraction mapping that has unique fixed point y∈Σ. Therefore, the IBVP (1.3) has a unique positive solution on Σ.
In order to illustrate our results, we provide an example.
Example 3.1. Consider the IBVP
{T74y(r)+r3+ry(r)4+y(r)=T34(π2+r+12tan−1y(r)), r∈(0,1),y(0)=0, y(1)=∫10(π2+ζ+12tan−1y(ζ))dζ, | (3.7) |
where q(r,y)=π2+r+tan−1y(r), p(r,y)=r3+ry(r)4+y(r). We can find q is non-decreasing on y, and
π2+r≤q(r,y)≤3π4+r, |
r3≤p(r,y)≤r3+1≤2, |
for (r,y)∈[0,1]×[0,∞).
So, the IBVP (3.7) has at least one solution according to the above Corollaries. In addition, we have
|p(r,z)−p(r,z∗)|≤14‖z−z∗‖, |
|q(r,z)−q(r,z∗)|≤12‖z−z∗‖, |
this implies Lq+Lps(s+1)=12+1474(74+1)<1, so the IBVP(3.7) has a unique positive solution due to Theorem 3.2.
In this paper, we study an integral boundary problem with a conformable fractional derivative, such that our problem is more general than the problem studied in [25], so if q(r,y(r))≡0 or constant then we obtain results for the problem (1.2). Especially, the uniqueness has not been studied in the work [25].
The method of upper and lower solutions is more applicable and easily used for more general problems. Also, the fixed point theorems play an important role to show the existence and the uniquenes.
The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.
The authors declare that they have no competing interests
[1] |
T. Abdeljawad, On conformable fractional calculus, J. Comput. Appl. Math., 279 (2015), 57–66. https://doi.org/10.1016/j.cam.2014.10.016 doi: 10.1016/j.cam.2014.10.016
![]() |
[2] |
S. Ailing, Z. Shuqin, Upper and lower solutions method and a fractional differential equation boundary value problem, Electron. J. Qual. Theory Differ. Equ., 30 (2009), 1–13. https://doi.org/10.14232/ejqtde.2009.1.30 doi: 10.14232/ejqtde.2009.1.30
![]() |
[3] |
F. M. Al-Askar, W. W. Mohammed, S. K. Samura, M. El-Morshedy, The exact solutions for fractional-stochastic Drinfel'd-Sokolov-Wilson equations using a conformable operator, J. Funct. Space., 2022 (2022), 7133824. https://doi.org/10.1155/2022/7133824 doi: 10.1155/2022/7133824
![]() |
[4] | D. R. Anderson, D. J. Ulness, Newly defined conformable derivatives, Adv. Dyn. Syst. Appl., 10 (2015), 109–137. |
[5] |
S. Asawasamrit, S. K. Ntouyas, P. Thiramanus, J. Tariboon, Periodic boundary value problems for impulsive conformable fractional integrodifferential equations, Bound. Value Probl., 2016 (2016), 122. https://doi.org/10.1186/s13661-016-0629-0 doi: 10.1186/s13661-016-0629-0
![]() |
[6] |
I. Bachar, H. Eltayeb, Positive solutions for a class of conformable fractional boundary value problems, Math. Method. Appl. Sci., 2020 (2020). https://doi.org/10.1002/mma.6637 doi: 10.1002/mma.6637
![]() |
[7] |
H. Batarfi, J. Losada, J. J. Nieto, W. Shammakh, Three-point boundary value problems for conformable fractional differential equations, J. Funct. Space., 2015 (2015), 706383. https://doi.org/10.1155/2015/706383 doi: 10.1155/2015/706383
![]() |
[8] |
A. Batool, I. Talib, M. B. Riaz, C. Tunç, Extension of lower and upper solutions approach for generalized nonlinear fractional boundary value problems, Arab J. Basic Appl. Sci., 29 (2022), 249–256. https://doi.org/10.1080/25765299.2022.2112646 doi: 10.1080/25765299.2022.2112646
![]() |
[9] |
Y. Cenesiz, D. Baleanu, A. Kurt, O. Tasbozan, New exact solutions of Burgers' type equations with conformable derivative, Wave. Random Complex, 27 (2017), 103–116. https://doi.org/10.1080/17455030.2016.1205237 doi: 10.1080/17455030.2016.1205237
![]() |
[10] | K. Diethelm, Multi-Term Caputo fractional differential equations, In: The analysis of fractional differential equations, Berlin: Springer, 2010. https://doi.org/10.1007/978-3-642-14574-2_8 |
[11] |
K. Diethelm, H. T. Tuan, Upper and lower estimates for the separation of solutions to fractional differential equations, Fract. Calc. Appl. Anal., 25 (2022), 166–180. https://doi.org/10.1007/s13540-021-00007-x doi: 10.1007/s13540-021-00007-x
![]() |
[12] |
X. Han, H. Gao, Positive solutions of nonlinear eigenvalue problems for a nonlocal fractional differential equation, Math. Probl. Eng., 2011 (2011), 725494. https://doi.org/10.1155/2011/725494 doi: 10.1155/2011/725494
![]() |
[13] |
R. Khaldi, A. Guezane-Lakoud, Upper and lower solutions method for higher order boundary value problems, Progr. Fract. Differ. Appl., 3 (2017), 53–57. http://dx.doi.org/10.18576/pfda/030105 doi: 10.18576/pfda/030105
![]() |
[14] |
R. Khalil, M. A. Horani, A. Yousef, M. Sababheh, A new definition of fractional derivative, J. Comput. Appl. Math., 264 (2014), 65–70. https://doi.org/10.1016/j.cam.2014.01.002 doi: 10.1016/j.cam.2014.01.002
![]() |
[15] |
N. Khodabakhshi, S. Vaezpour, J. Trujillo, Method of upper and lower solutions for coupled system of nonlinear fractional integro-differential equations with advanced arguments, Math. Slovaca, 67 (2017), 89–98. https://doi.org/10.1515/ms-2016-0250 doi: 10.1515/ms-2016-0250
![]() |
[16] | A. A. Kilbas, H. M. Srivastava, J. J. Trujillo, Theory and applications of fractional differential equations, Elsevier, 2006. |
[17] |
A. Korkmaz, Explicit exact solutions to some one-dimensional conformable time fractional equations, Wave. Random Complex., 29 (2017), 124–137. https://doi.org/10.1080/17455030.2017.1416702 doi: 10.1080/17455030.2017.1416702
![]() |
[18] |
W. W. Mohammed, N. Iqbal, A. M. Albalahi, A. E. Abouelregal, D. Atta, H. Ahmad, et al., Brownian motion effects on analytical solutions of a fractional-space long-short-wave interaction with conformable derivative, Results Phys., 35 (2022), 105371. https://doi.org/10.1016/j.rinp.2022.105371 doi: 10.1016/j.rinp.2022.105371
![]() |
[19] | K. B. Oldham, J. Spanier, Theory and applications of differentiation and integration to arbitrary order, New York: Academic Press, 1974. |
[20] | I. Podlubny, Fractional differential equations, 1999. |
[21] | A. A. Kilbas, O. I. Marichev, S. G. Samko, Fractional integral and derivatives: Theory and applications, 1993. |
[22] |
M. Xu, S. Sun, Positivity for integral boundary value problems of fractional differential equations with two nonlinear terms, J. Appl. Math. Comput., 59 (2019), 271–283. https://doi.org/10.1007/s12190-018-1179-7 doi: 10.1007/s12190-018-1179-7
![]() |
[23] |
S. Yang, L. Wang, S. Zhang, Conformable derivative: Application to non-Darcian flow in low-permeability porous media, Appl. Math. Lett., 79 (2018), 105–110. https://doi.org/10.1016/j.aml.2017.12.006 doi: 10.1016/j.aml.2017.12.006
![]() |
[24] |
D. Zhao, M. Luo, General conformable fractional derivative and its physical interpretation, Calcolo, 54 (2017), 903–917. https://doi.org/10.1007/s10092-017-0213-8 doi: 10.1007/s10092-017-0213-8
![]() |
[25] |
W. Zhong, L. Wang, Positive solutions of conformable fractional differential equations with integral boundary conditions, Bound. Value Probl., 2018 (2018), 137. https://doi.org/10.1186/s13661-018-1056-1 doi: 10.1186/s13661-018-1056-1
![]() |
1. | Taher S. Hassan, Clemente Cesarano, Mouataz Billah Mesmouli, Hasan Nihal Zaidi, Ismoil Odinaev, Iterative Hille‐type oscillation criteria of half‐linear advanced dynamic equations of second order, 2024, 47, 0170-4214, 5651, 10.1002/mma.9883 | |
2. | Mouataz Billah Mesmouli, Nahed Mustafa Dahshan, Wael W. Mohammed, Existence results for IBVP of $ \left(p, q\right) $-fractional difference equations in Banach space, 2024, 9, 2473-6988, 15748, 10.3934/math.2024760 |