Abstract: In this paper, we study a system of Hadamard fractional multi-point boundary value problems. We first obtain triple positive solutions when the nonlinearities satisfy some bounded conditions. Next, we also obtain a nontrivial solution when the nonlinearities can be asymptotically linear growth. Furthermore, we provide two examples to illustrate our main results.
Keywords: Hadamard fractional differential equations, multi-point boundary value problems, multiple solutions, asymptotically linear growth.
Article
Solvability for a system of Hadamard fractionalmulti-point boundary value problems

Recepción: 28 Febrero 2020
Revisado: 02 Septiembre 2020
Publicación: 01 Mayo 2021
In this paper, we use some fixed point theorems to study the existence of solutions for the system of Hadamard fractional multi-point boundary value problems
(1)where . (2,3] is a real number, D. is the .-order Hadamard fractional derivatives, and . means the delta derivative, i.e., δu(1) = (. du/d.) .=1, δv(1) = (. dv/d.) .=1. The constants a., b., ξ., η. (. = 1, 2, . . . , m 1, . = 1, 2, . . . , n ., m, n ≥ 2) and .., .. satisfy the conditions:

Fractional-order equations, as a generalization of the case of integer order, can accu- rately characterize some complex phenomena in nature. It has been proved that there are many special advantages in some fields, such as physics, chemistry, aerodynam- ics, electrodynamics of complex medium, polymer rheology, economics, control theory, signal and image processing, biophysics, blood flow phenomena, which has become a hot research topic of common concern in the world. For example, in [5], the authors investigated the following fractional-order advection–diffusion–reaction boundary value problem:

where 1 < α ≤ 2, 0 < ε ≤ 1, . R, .D. is the fractional derivative of Caputo sense, and .(.) is a spatially dependent source term.
It has been observed that most of papers in the literature on the fractional-order equations involves either Riemann–Liouville- or Caputo-type fractional derivative. Apart from the two derivatives, Hadamard derivative is another kind of fractional derivative that was introduced by Hadamard [9]. This fractional derivative differs from the other ones in the sense that the kernel of the integral contains logarithmic function of arbitrary exponent. For detailed materials of Hadamard fractional derivative and integral, we refer to the papers [1–4, 8, 10, 11, 13–23, 25–29] and references therein. In [14], the authors studied the Riemann–Liouville fractional differential inclusion with Hadamard fractional integral boundary conditions

where 1 < q ≤ 2, RLD. is the Riemann–Liouville fractional derivative, .I.i is the Hadamard fractional integral, η. ∈ (0, T ) with Σn α.η.−1.(. − 1).i /= T.−1. In [29], Zhang et al. utilized the Guo–Krasnosel’skii fixed point theorem to obtain the multiple positive solutions for the Hadamard fractional integral boundary value problems

where . (2, 3], . (1, 2], . [0, β], ϕ. is the .-Laplacian, and the nonlinearity . grows (. 1)-superlinearly and (. 1)-sublinearly.
On the other hand, we note that coupled systems of fractional-order equations have also been investigated by many authors, we refer to [2, 4, 8, 11, 13, 17–21, 23, 25–27]. Ah- mad and Ntouyas in [2] investigated some results for the system of Hadamard fractional differential equations

where I. is the Hadamard fractional integral with γ > 0. By using Leray–Schauder’s alternative and Banach’s contraction principle the authors obtained the existence and uniqueness of solutions, respectively. In [11], Jiang et al. adopted the fixed point index to study the existence of positive solutions for the system of nonlinear Hadamard fractional differential equations involving coupled integral boundary conditions

where the nonlinearities f. (. = 1, 2) can grow superlinearly and sublinearly.
Inspired by the works above, in this paper, we use some fixed point methods to study the existence of solutions for (1). We first obtain triple positive solutions when the nonlinearities satisfy some bounded conditions. Next, we also obtain a nontrivial solution when the nonlinearities can be asymptotically linear growth. Finally, we offer two examples to illustrate our main results.
The outline of the paper is organized as follows. In Section 2, we give revelent defini- tions and lemmas, and some important properties of the corresponding Green’s function are also obtained. In Section 3, we give the detailed proofs for the existence theorems. In Section 4, we present two examples to illustrate our main results.
In this section, we only provide the definition of the Hadamard fractional derivative, for more details we refer the reader to [1].
(See [1].) The Hadamard derivative of fractional order . for a function . : [1, ∞) → R is defined as

where . = [.] + 1, [.] denotes the integer part of the real number ., and log(·) = loge(·).
Let y C[1, e]. Then the Hadamard fractional multi-point boundary value problems

has a solution, which can take the form u(.) = ∫ e . (t, s).(.)(ds/s., where

Proof. Using Lemmas 2–3 of [27], we have

where c. R (. = 1, 2, 3). Note that from .(1) = δu(1) = 0 we have .. = .. = 0. Consequently, we obtain
(2)From .(e) = Σ.−1 a.u.ξ.) we obtain

This, together with (H0), implies that

Therefore, by (2) we have

This completes the proof.
(See [24].) The function G. has the following inequalities:


Proof. From Lemma 2(i) we have

and

This completes the proof.
Let . := .[1,e], ǁ.ǁ = max.∈[1,e] |.(.)|, and . := {. ∈ .: .(.) ≥ 0 ∀. ∈ [1, e]}. Then (E, ǁ·ǁ) becomes a real Banach space, and . is a cone on .. Moreover, . × . is a Banach space with the norm ǁ(u, v)ǁ = ǁ.ǁ + ǁ.ǁ, and . × . is a cone on . × .. Let

Then from Lemma 1 we obtain that (1) is equivalent to the following system of Hammersteintype integral equations:

Therefore, we can define an operator . : . × . → . × . as follows:

Note that G. and f. (. = 1, 2) are nonnegative continuous functions, so the operators A.. P P P (. = 1, 2) and .: P P P P are three completely continuous operators. Moreover, if (u, v) (P P ) . is a fixed point of ., then (u, v) is a positive solution for (1). Therefore, in what follows, we turn to study the existence of
fixed points of the operator ..
Let η = min.∈[5.4,3e.4] .(.). Then A..P, P ) ⊂ .. (. = 1, 2), where

Proof. From Lemma 3 we have

This implies that

Consequently, if . ∈ [5.4, 3e.4], we obtain

and then

On the other hand, using the method of Lemma 3, we also have ..(t, s) ≥ .(.)..(τ, s) for t, s, τ ∈ [1, e], and thus ..(P, P ) ⊂ ... This completes the proof.
Let γ, β, θ be nonnegative continuous convex functionals on . , and let α, ψ be nonnegative continuous concave functionals on . ; then for nonnegative numbers .., .., .., .. and .., convex sets are defined:

(See [6].) Let P be a cone in the real Banach space E. Suppose that α and ψ are nonnegative continuous concave functionals on P and γ, β, θ are nonnegative continuous convex functionals on P such that, for some positive numbers c. and e., ...) ≤ .(.) and y ≤ e..(.) for all y P .γ, c′). Suppose further that T : . (γ, c′) . (γ, c′) is completely continuous and there exist constants h., d., a., and b. ≥ 0 with . < d. < a. such that each of the following is satisfied:

Then T has at least three fixed points y., y., y. . (y, c′) such that β(..) < d., a. < α(..) and d. < β(..) with α(..) < a..
(See [12].) Let E be a Banach space, and A: .→ E be a completely continuous operator. Assume that T : . → E is a bounded linear operator such that . is not an eigenvalue of T and lim..ǁ→∞ ǁAu . Tuǁ.ǁ.ǁ = 0. Then A has a fixed point
(i) If we use t, s to replace log ., log . in .. of Lemma 1, respectively, we can obtain a function

This function happens to be the Green’s function for the Riemann–Liouville fractional boundary value problem

where . ∈ (2, 3], and D. is the Riemann–Liouville fractional derivative, . ∈ .[0, 1].
For details, please refer to Lemma 3.1 in [24].
(ii) Note that for multi-point boundary value problems, the Green’s functions may be complicated. For example, in [7], Bai studied the fractional three-point boundary value problem
(3)where . ∈ (1, 2], βη.−1, . ∈ (0, 1). The Green’s function is
(4)Note that if . = 0, then (3) reduces to the problema.
(5)The Green’s function is
(6)Now, if the three-point problem (3) is considered as a perturbation of the two-point problem (5), we can use (6) to obtain (4), i.e.,

This simple idea motivates our study in Lemma 1.
Combining the above, we do not need to construct new Green’s functions to obtain the equivalent Hammerstein-type integral equations for our problem (1).
Now, we state our main theorems, and provide their proofs.
Let . < a. < b. < b./η < c., (H0).(H1) and the following conditions hold

Where

And

Then (1) has at least triple positive solutions.
Proof. From Lemma 4 we have

Therefore, for our conclusions, we need to define the nonnegative continuous concave functionals α, ψ and the nonnegative continuous convex functionals β, θ, γ on .. by

where . = [5.4, 3e.4], .. = [3.2, 2]. For any (u, v) ∈ .., we have

We show that .: . (γ, c′) → . (γ, c′ . Indeed, if (u, v) ∈ . (γ, c′), then we have 0 ≤ .(.) + .(.) ≤ .. for . ∈ [1, e]. Consequently, (H4) is used to obtain

Now, (B1) and (B2) of Lemma 5 are to be verified. Note that

Therefore, if (u, v) .(γ, θ, α, b., b./η, c.), then .. ≤ .(.) + .(.) ≤ ../η for t I; if (u, v) .(γ, β, ψ, ηa., a., c.), then ηa. ≤ .(.) + .(.) ≤ .. for t I.. As a result, (H3) enables us to find

Moreover, (H2) implies that

Next, (B3) of Lemma 5 is satisfied. Let (u, v) ∈ . (γ, α, b., c.) with .(.(u, v))(.) > b./η. Therefore, for all . ∈ [1, e], we have

Note that the last line of the above is independent of the variable ., and thus we obtain

Finally, we prove that (B4) holds. Let (u, v) ∈ .(γ, β, a., c.) with .(.(u, v))(.) < ηa.. Note that min... G..t, s) ≥ ηG..τ, s) for τ, s ∈ [1, e], and thus min... G..t, s) ≥ . max.∈[1,e]G..τ, s) for . ∈ [1, e], . = 1, 2. Therefore, we have

Up to now, we have proved that all the assumptions of Lemma 5 are satisfied. There- fore, (1) has at least triple positive solutions, (.., x.), (.., y.), and (.., z.) such that .(.., x.) < a., .. < α(y., y.), and .. < β(.., z.) with .(.., z.) < b.. This completes the proof.
Suppose that (H0) and the following conditions hold: (H1.) f. ∈ .([1, e] × R × R, R), i = 1, 2;

Then (1) has at least one nontrivial solution.
Proof. Define operators T. : . × . → . as follows:

Now, we prove that 1 is not an eigenvalue of T. (. = 1, 2), and we only need to consider the case . = 1 (the case . = 2 can be dealt with a similar method). Argument by contrary. If let . + . = ., then we have
(7)and by Lemma 1 we obtain

where q, δ, a., ξ. (. = 1, 2, . . . , m − 1) satisfy (H0). We distinguish two cases.
Case 1. .. = 0. From (8) and Lemma 1 of [23] we have

where c. R (. = 1, 2, 3). By the boundary conditions in (8) we have .. = .. = 0. Therefore, we find

and (H0) indicates that .. = 0. Consequently, we have .(.) 0 for . [1, e]. This contradicts to the definition of eigenvalue and eigenfunction.
Case 2. .. =/ 0. From (7) we have

This has a contradiction.
Above all, 1 is not an eigenvalue of T. (. = 1, 2) as required. Hence, if we let the operator . : . × . → . × . as follows:

we know . := (1, 1) is not an eigenvalue of . .
From (H5), for all ε > 0, there exist M. > 0 (. = 1, 2) such that

Consequently, there are .. > ., ζ. > 0 such that

As a result, we have

For the arbitrariness of ., we have limǁ(u,v)ǁ→∞ .(u, v) .(u, v) . (u, v) = 0. Note from (H6) that . = (0,0) is not a fixed point of .. Hence, from Lemma 6 we have that . has a fixed point in ., and this fixed point is nontrivial, i.e., (1) has at least one nontrivial solution. This completes the proof.
In (1), let . = 2.5, . = .= 2, .. = .. = 2, .. = .. = 1.5, and then we obtain the system of Hadamard fractional three-point boundary value problems
[91]

By direct calculation we obtain

Therefore, we obtain

Example 1. If we choose .. = 1, .. = 10, .. = 900, then 0 < a. < b. < b./η < c.. Moreover, let

and

Then we obtain

Then all the assumptions of Theorem 1 are satisfied. So, (9) has at least triple positive
solutions.
Example 2. Let

where σ. < 1.51, µ. = 0, ν. = 0 for u, v R, . [1, e], . = 1, 2. Then all the conditions of Theorem 2 hold. Hence, (9) has at least one nontrivial solution.
The authors would like to thank the referee for his/her valuable comments and suggestions.