In this paper, we studied a Hadamard-type fractional Riemann-Stieltjes integral boundary value problem. The existence of nontrivial solutions was obtained by using the fixed-point method when the nonlinearities can be superlinear, suberlinear, and have asymptotic linear growth. Our results improved and generalized some results of the existing literature.
Citation: Keyu Zhang, Qian Sun, Jiafa Xu. Nontrivial solutions for a Hadamard fractional integral boundary value problem[J]. Electronic Research Archive, 2024, 32(3): 2120-2136. doi: 10.3934/era.2024096
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In this paper, we studied a Hadamard-type fractional Riemann-Stieltjes integral boundary value problem. The existence of nontrivial solutions was obtained by using the fixed-point method when the nonlinearities can be superlinear, suberlinear, and have asymptotic linear growth. Our results improved and generalized some results of the existing literature.
In this work, we are devoted to studying the existence of nontrivial solutions for the Hadamard-type fractional Riemann-Stieltjes integral boundary value problem
{−Dβz(x)=f(x,z(x)),x∈(1,e),z(1)=δz(1)=0,δz(e)=∫e1g(x,z(x))dη(x)x, | (1.1) |
where Dβ is the Hadamard-type fractional derivative with β∈(2,3], δz(x)=xdzdx, and the functions f,g,η satisfy the following conditions:
(H1) f,g∈C([1,e]×R,R).
(H2) There exist γi,σi∈C([1,e],R+) and Mi∈C(R,R+)(i=1,2) such that
f(x,z)≥−γ1(x)−γ2(x)M1(z),g(x,z)≥−σ1(x)−σ2(x)M2(z), x∈[1,e],z∈R. |
(H3) lim|z|→+∞Mi(z)|z|=0, i=1,2.
(H4) η is a nondecreasing function in [1,e] with η(1)=0.
As an important branch of mathematical analysis, fractional calculus can more accurately describe some dynamic processes with memory and heredity characteristics. In view of outstanding advantages of fractional calculus, it has attracted the great attention of many researchers and developed rapidly; we refer the reader to [1,2,3,4,5,6,7,8,9,10]. Moreover, we note that originating from the work of Hadamard in 1892, Hadamard fractional calculus is now successfully applied to describe ultra-slow phenomena in the objective world, such as fracture of materials, creep of rocks, etc. Therefore, it is of great significance to study Hadamard-type fractional problems, see [11,12,13,14,15,16,17,18,19] and the references therein. For example, in [11], the authors used the Guo-Krasnosel'skii fixed point theorem to study the existence and nonexistence of positive solutions for the system of Hadamard fractional differential equations
{Dα1φp1(Dβ1x(s))=μf1(s,x(s),y(s)),s∈(1,e),Dα2φp2(Dβ2y(s))=vf2(s,x(s),y(s)),s∈(1,e),δx(1)=δ2x(1)=⋯=δn1−2x(1)=0, Dγ0x(e)=q2∑i=1∫θi1hi(s)Dηiy(s)dHi(s)s,δy(1)=δ2y(1)=⋯=δn2−2y(1)=0, Dη0y(e)=q1∑j=1∫ϑj1kj(s)Dγjx(s)dKj(s)s,Dβ1x(1)=Dβ1x(e)=δ(φp1(Dβ1x(1)))=0, Dβ2y(1)=Dβ2y(e)=δ(φp2(Dβ2y(1)))=0, |
where fi(i=1,2) are nonnegative continuous functions on [1,e]×R+×R+ and satisfy some (pi−1)−superlinear and (pi−1)−suberlinear growth conditions.
In [12], the authors studied the following system of Hadamard fractional differential equations with multipoint Hadamard fractional derivative boundary conditions
{Dpu(t)+w1(t)f(t,v(t),Dq−1v(t))=0,n−1<p≤n,t∈(1,+∞),Dqv(t)+w2(t)g(t,u(t),Dp−1u(t))=0,m−1<q≤m,t∈(1,+∞),u(1)=u′(1)=⋯=u(n−2)(1)=0,Dp−1u(∞)=k1∑i=1aiDr1u(ni),v(1)=v′(1)=⋯=v(m−2)(1)=0,Dq−1v(∞)=k2∑j=1bjDr2v(mj), |
where Dϑ are Hadamard-type fractional derivatives of order ϑ∈{p,q,r1,r2},r1∈[0,p−1],r2∈[0,q−1]. Using the monotone iterative method, they obtained the existence of monotone positive solutions for their considered problems. In [13], the authors used the fixed-point techniques to study the existence and uniqueness results for the following Riemann-Stieltjes integral boundary value problem involving a Hadamard-type fractional differential equation
{Dνy(x)=f(x,y(x),Dνy(x)),t∈[1,T],y(1)=0, ∫T1y(x)dZ(x)=μΓ(δ)∫η1(lnηx)δ−1y(x)dxx,η∈(1,T), |
where f∈([1,T]×R×R→R) satisfies the Lipschitz condition.
Inspired by the aforesaid works, we use the fixed-point methods to study the nontrivial solutions for the Hadamard-type fractional Riemann-Stieltjes integral boundary value problem (1.1). We consider the two-folds: When the nonlinearities f,g are superlinear and suberlinear, we use some conditions concerning the spectral radius of a new linear operator to obtain our existence theorems. When the nonlinearities f,g are asymptotic linear, we use a fixed-point theorem to obtain a nontrivial solution.
We first briefly provide the definition of the Hadamard-type fractional derivative, which can be founded in [11,14,15].
Definition 2.1. Let g:[1,∞)→R, then the Hadamard-type fractional q-order derivative is defined as
Dqg(x)=1Γ(n−q)(xddx)n∫x1(lnx−lny)n−q−1g(y)dyy,n−1<q<n, |
where n=[q]+1,[q] means the integer part of q, and ln(⋅)=loge(⋅).
Now, we calculate the Green's function for (1.1).
Lemma 2.2. Let h,V be functions on [1,e], then
{−Dβz(x)=h(x),x∈(1,e),z(1)=δz(1)=0,δz(e)=∫e1V(x)dη(x)x |
has a solution
z(x)=∫e1Gβ(x,y)h(y)dyy+(lnx)β−1β−1∫e1V(x)dη(x)x, |
where
Gβ(x,y)=1Γ(β){(lnx)β−1(1−lny)β−2−(lnx−lny)β−1,1≤y≤x≤e,(lnx)β−1(1−lny)β−2,1≤x≤y≤e. |
Proof. We first consider the problem
{−Dβz(x)=h(x),x∈(1,e),z(1)=δz(1)=δz(e)=0. | (2.1) |
By the methods of [15], we can obtain
z(x)=c1(lnx)β−1+c2(lnx)β−2+c3(lnx)β−3−1Γ(β)∫x1(lnx−lny)β−1h(y)dyy, |
where ci∈R,i=1,2,3. The condition z(1)=δz(1)=0 implies that c2=c3=0. Furthermore, from δz(e)=0, we find
z(e)=c1−1Γ(β)∫e1(1−lns)β−2h(s)dss=0, |
then
z(x)=1Γ(β)∫e1(lnx)β−1(1−lny)β−2h(y)dyy−1Γ(β)∫x1(lnx−lny)β−1h(y)dyy=∫e1Gβ(x,y)h(y)dyy. | (2.2) |
Next, we consider the problem
{−Dβz(x)=0,x∈(1,e),z(1)=δz(1)=0,δz(e)=∫e1V(x)dη(x)x, | (2.3) |
which yields that
z(x)=˜c1(lnx)β−1+˜c2(lnx)β−2+˜c3(lnx)β−3, |
where ˜ci∈R, i=1,2,3. Similarly, ˜c2=˜c3=0. Consequently, we get
δz(e)=(β−1)˜c1=∫e1V(x)dη(x)x, |
and
z(x)=(lnx)β−1β−1∫e1V(x)dη(x)x. | (2.4) |
Combining (2.1)–(2.4), we can obtain the conclusion of this lemma. This completes the proof.
Lemma 2.3 (see [1]). The function Gβ satisfies the following properties:
(I1) Gβ(x,y)≥0 for x,y∈[1,e];
(I2) (lnx)β−1Gβ(e,y)≤Gβ(x,y)≤Gβ(e,y) for x,y∈[1,e].
Let E:=C[1,e],‖z‖:=maxx∈[1,e]|z(x)|,P:={z∈E:z(x)≥0,∀x∈[1,e]}, then (E,‖⋅‖) is a real Banach space and P a cone on E. By Lemma 2.2, we can define an operator as follows:
(Tz)(x)=∫e1Gβ(x,y)f(y,z(y))dyy+(lnx)β−1β−1∫e1g(x,z(x))dη(x)x, x∈[1,e], z∈E. |
Moreover, it is easy to find that if there is a z∗∈E∖{0} such that Tz∗=z∗, then this z∗ is a nontrivial solution for (1.1). Hence, we only need to study the existence of nontrivial fixed points of T. For ξi>0(i=1,2), let Lξ1,ξ2:E→E be defined as
(Lξ1,ξ2z)(x)=ξ1∫e1Gβ(x,y)z(y)dyy+ξ2(lnx)β−1β−1∫e1z(x)dη(x)x,x∈[1,e],z∈E. | (2.5) |
We then see that Lξ1,ξ2 is a linear operator, and we also obtain the following lemma.
Lemma 2.4. Let P0={z∈E:z(x)≥(lnx)β−1‖z‖,x∈[1,e]}, then Lξ1,ξ2(P)⊂P0.
This can be easily obtained from Lemma 2.3 (I2), so we don't need to offer its proof.
Lemma 2.5. r(Lξ1,ξ2)>0, where r(Lξ1,ξ2) stands for the spectral radius of Lξ1,ξ2.
Proof. Let (Lξ1z)(x)=ξ1∫e1Gβ(x,y)z(y)dyy,x∈[1,e],z∈E, then for all n∈N+, we have
(Lnξ1z)(x)=ξn1∫e1⋯∫e1⏟nGβ(x,y1)Gβ(y1,y2)⋯Gβ(yn−1,yn)z(yn)dy1y1dy2y2⋯dynyn. |
By Lemma 2.3 (I2), we have
‖Lnξ1‖≥maxx∈[1,e](Lnξ11)(x)≥ξn1maxx∈[1,e](lnx)β−1[∫e1(lny)β−1Gβ(e,y)dyy]n−1∫e1Gβ(e,y)dyy, |
where 1(x)≡1,x∈[1,e]. Consequently, the Gelfand's theorem implies that
r(Lξ1)=lim infn→∞n√‖Lnξ1‖≥ξ1∫e1(logy)β−1Gβ(e,y)dyy=ξ1Γ(β−1)Γ(2β−1)>0 for ξ1>0. |
Note that r(Lξ1,ξ2)≥r(Lξ1)>0. This completes the proof.
Lemma 2.5 and the Krein-Rutman theorem [20] imply that there exists ζξ1,ξ2∈P∖{0} such that
Lξ1,ξ2ζξ1,ξ2=r(Lξ1,ξ2)ζξ1,ξ2. | (2.6) |
Moreover, by Lemma 2.4, we have
ζξ1,ξ2∈P0. | (2.7) |
Lemma 2.6 (see [21]). Let E be a Banach space, W⊂E a bounded open set, and T:W→E a continuous compact operator. If there exists z0∈E∖{0} such that
z−Tz≠μz0,∀z∈∂W,μ≥0, |
then the topological degree deg(I−T,W,0)=0.
Lemma 2.7 (see [21]). Let E be a Banach space, W⊂E a bounded open set with 0∈W, and T:W→E a continuous compact operator. If
Tz≠μz,∀z∈∂W,μ≥1, |
then the topological degree deg(I−T,W,0)=1.
Lemma 2.8 (see [22]). Let T:E→E be a completely continuous operator, and L:E→E a bounded linear operator. Suppose that 1 isn't an eigenvalue of L and
lim‖z‖→∞‖Tz−Lz‖‖z‖=0, |
then there exists z∗∗∈E such that Tz∗∗=z∗∗.
Now, we list some assumptions on f and g, which we need in this section.
(H5) There exist ξ1,ξ2>0 with r(Lξ1,ξ2)≥1 such that
lim inf|z|→+∞f(x,z)|z|>ξ1,lim inf|z|→+∞g(x,z)|z|>ξ2, uniformly for x∈[1,e]. |
(H6) There exist ξ3,ξ4>0 with r(Lξ3,ξ4)<1 such that
lim sup|z|→0|f(x,z)||z|<ξ3,lim sup|z|→0|g(x,z)||z|<ξ4, uniformly for x∈[1,e]. |
(H7) There exist ξ5,ξ6>0 with r(Lξ5,ξ6)>1 such that
lim inf|z|→0+f(x,z)|z|>ξ5,lim inf|z|→0+g(x,z)|z|>ξ6, uniformly for x∈[1,e]. |
(H8) There exist ξ7,ξ8>0 with r(Lξ7,ξ8)<1 such that
lim sup|z|→+∞|f(x,z)||z|<ξ7,lim sup|z|→+∞|g(x,z)||z|<ξ8, uniformly for x∈[1,e]. |
(H9) f,g(x,0)≢0,x∈[1,e], and there exist ξ9,ξ10 with |ξ9|β(β−1)Γ(β)+|ξ10|∫e1dη(t)tβ−1<1 such that
limz→∞f(x,z)z=ξ9, limz→∞g(x,z)z=ξ10, uniformly for ∈x∈[1,e]. |
Theorem 3.1. Let (H1)–(H6) hold, then (1.1) has a nontrivial solution.
Proof. From (H5), there exist ϵi>0(i=1,2) and Z0>0 such that
f(x,z)≥(ξ1+ϵ1)|z|, g(x,z)≥(ξ2+ϵ2)|z|, for |z|>Z0,x∈[1,e]. |
From (H3), for any εi>0(i=1,2), there exists Z1>Z0 such that
M1(z)≤ε1|z|, M2(z)≤ε2|z|, for |z|>Z1. |
Let M∗1=max|z|≤Z1M1(z),M∗2=max|z|≤Z1M2(z), then we have
M1(z)≤ε1|z|+M∗1, M2(z)≤ε2|z|+M∗2,z∈R. | (3.1) |
Note that by (H2), for |z|>Z1,x∈[1,e], and we obtain
f(x,z)≥(ξ1+ϵ1)|z|−γ1(x)−γ2(x)M1(z)≥(ξ1+ϵ1−ε1‖γ2‖)|z|−γ1(x),g(x,z)≥(ξ2+ϵ2)|z|−σ1(x)−σ2(x)M2(z)≥(ξ2+ϵ2−ε2‖σ2‖)|z|−σ1(x). |
Note that f,g(x,z) are bounded on [1,e]×[−Z1,Z1], then let Cf=(ξ1+ϵ1−ε1‖γ2‖)Z1+maxx∈[1,e],|z|≤Z0|f(x,z)|, Cg=(ξ2+ϵ2−ε2‖σ2‖)Z1+maxx∈[1,e],|z|≤Z0|g(x,z)|, so we have
f(x,z)≥(ξ1+ϵ1−ε1‖γ2‖)|z|−γ1(x)−Cf, g(x,z)≥(ξ2+ϵ2−ε2‖σ2‖)|z|−σ1(x)−Cg, z∈R,x∈[1,e]. | (3.2) |
Note that εi(i=1,2) can be chosen arbitrarily small, and let a sufficiently large R1 satisfy:
R1>β−1βN1+(β−1)N2β−1−ε1‖γ2‖βΓ(β)−ε2‖σ2‖∫e1dη(x)x,R1>(ϵ1−ε1‖γ2‖)(N1β+N2)+(ξ1+ϵ1−ε1‖γ2‖)(N1+N2)(ϵ1−ε1‖γ2‖)[1−ε1‖γ2‖β(β−1)Γ(β)−ε2‖σ2‖∫e1dη(x)xβ−1]−(ξ1+ϵ1−ε1‖γ2‖)[ε1‖γ2‖(β−1)Γ(β)+ε2‖σ2‖∫e1dη(x)xβ−1],and R1>(ϵ2−ε2‖σ2‖)(N1β+N2)+(ξ2+ϵ2−ε2‖σ2‖)(N1+N2)(ϵ2−ε2‖σ2‖)[1−ε1‖γ2‖β(β−1)Γ(β)−ε2‖σ2‖∫e1dη(x)xβ−1]−(ξ2+ϵ2−ε2‖σ2‖)[ε1‖γ2‖(β−1)Γ(β)+ε2‖σ2‖∫e1dη(x)xβ−1], | (3.3) |
where
N1=‖γ1‖+‖γ2‖M∗1+Cf(β−1)Γ(β), N2=∫e1dη(x)xβ−1[‖σ1‖+‖σ2‖M∗2+Cg]. |
In the following, we shall prove
z−Tz≠μζξ1,ξ2, z∈∂BR1,μ≥0, | (3.4) |
where ζξ1,ξ2 is defined by (2.6) and BR1 is an open ball: {z∈E:‖z‖<R1}. If the claim (3.4) isn't satisfied, then there exist z1∈∂BR1 and μ1≥0 such that
z1−Tz1=μ1ζξ1,ξ2. | (3.5) |
Note that μ1≠0. If not, z1 is a fixed point of T and the theorem is proved. In order to prove (3.5), let
˜z1(x)=∫e1Gβ(x,y)[γ1(y)+γ2(y)M1(z1(y))+Cf]dyy+(lnx)β−1β−1∫e1[σ1(x)+σ2(x)M2(z1(x))+Cg]dη(x)x,x∈[1,e]. | (3.6) |
By γ1+γ2M1(z1)+Cf∈P and σ1+σ2M2(z1)+Cg∈P, Lemma 2.4 implies that
˜z1∈P0. |
Moreover, we calculate z1+˜z1 as follows:
z1(x)+˜z1(x)=(Tz1)(x)+˜z1(x)+μ1ζξ1,ξ2(x)=∫e1Gβ(x,y)[f(y,z1(y))+γ1(y)+γ2(y)M1(z1(y))+Cf]dyy +(lnx)β−1β−1∫e1[g(x,z1(x))+σ1(x)+σ2(x)M2(z1(x))+Cg]dη(x)x+μ1ζξ1,ξ2(x),x∈[1,e]. |
From (H2), (2.7), and Lemma 2.4 we know
z1+˜z1∈P0. | (3.7) |
By (3.1), (3.3) and (3.6), note that ‖z1‖=R1, and we have
˜z1(x)≤∫e1Gβ(x,y)[γ1(y)+γ2(y)(ε1|z1(y)|+M∗1)+Cf]dyy +(lnx)β−1β−1∫e1[σ1(x)+σ2(x)(ε2|z1(x)|+M∗2)+Cg]dη(x)x≤∫e1Gβ(e,y)[‖γ1‖+‖γ2‖(ε1‖z1‖+M∗1)+Cf]dyy +1β−1∫e1[‖σ1‖+‖σ2‖(ε2‖z1‖+M∗2)+Cg]dη(x)x=‖γ1‖+‖γ2‖(ε1R1+M∗1)+Cfβ(β−1)Γ(β)+∫e1dη(x)xβ−1[‖σ1‖+‖σ2‖(ε2R1+M∗2)+Cg]<R1. |
Note that ˜z1,z1+˜z1∈P0. From (3.2) and (H2), we have
(Tz1)(x)+˜z1(x)≥∫e1Gβ(x,y)[(ξ1+ϵ1−ε1‖γ2‖)|z1(y)|−γ1(y)−Cf+γ1(y)+γ2(y)M1(z1(y))+Cf]dyy +(lnx)β−1β−1∫e1[(ξ2+ϵ2−ε2‖σ2‖)|z1(x)|−σ1(x)−Cg+σ1(x)+σ2(x)M2(z1(x))+Cg]dη(x)x≥∫e1Gβ(x,y)(ξ1+ϵ1−ε1‖γ2‖)z1(y)dyy+(lnx)β−1β−1∫e1(ξ2+ϵ2−ε2‖σ2‖)z1(x)dη(x)x=∫e1Gβ(x,y)(ξ1+ϵ1−ε1‖γ2‖)[z1(y)+˜z1(y)]dyy+(lnx)β−1β−1∫e1(ξ2+ϵ2−ε2‖σ2‖)[z1(x)+˜z1(x)]dη(x)x −∫e1Gβ(x,y)(ξ1+ϵ1−ε1‖γ2‖)˜z1(y)dyy−(lnx)β−1β−1∫e1(ξ2+ϵ2−ε2‖σ2‖)˜z1(x)dη(x)x≥ξ1∫e1Gβ(x,y)[z1(y)+˜z1(y)]dyy+ξ2(lnx)β−1β−1∫e1[z1(x)+˜z1(x)]dη(x)x | (3.8) |
using the fact that
∫e1Gβ(x,y)(ϵ1−ε1‖γ2‖)[z1(y)+˜z1(y)]dyy+(lnx)β−1β−1∫e1(ϵ2−ε2‖σ2‖)[z1(x)+˜z1(x)]dη(x)x −∫e1Gβ(x,y)(ξ1+ϵ1−ε1‖γ2‖)˜z1(y)dyy−(lnx)β−1β−1∫e1(ξ2+ϵ2−ε2‖σ2‖)˜z1(x)dη(x)x≥0,x∈[1,e]. | (3.9) |
In what follows, we prove that (3.9) holds. Note that ‖z1‖=R1, and by (3.7), we have
z1(x)+˜z1(x)≥(lnx)β−1‖z1+˜z1‖≥(lnx)β−1(R1−‖˜z1‖). |
Consequently, note that Gβ(x,y)≤(lnx)β−1(1−logy)β−2Γ(β),x,y∈[1,e], and (3.9) is greater than
∫e1Gβ(x,y)(ϵ1−ε1‖γ2‖)(lny)β−1(R1−‖˜z1‖)dyy+(lnx)β−1β−1∫e1(ϵ2−ε2‖σ2‖)(lnx)β−1(R1−‖˜z1‖)dη(x)x −∫e1Gβ(x,y)(ξ1+ϵ1−ε1‖γ2‖)∫e1(lny)β−1(1−lnτ)β−2Γ(β)[γ1(τ)+γ2(τ)M1(z1(τ))+Cf]dττdyy −∫e1Gβ(x,y)(ξ1+ϵ1−ε1‖γ2‖)(lny)β−1β−1∫e1[σ1(τ)+σ2(τ)M2(z1(τ))+Cg]dη(τ)τdyy −(lnx)β−1(β−1)Γ(β)∫e1(ξ2+ϵ2−ε2‖σ2‖)∫e1(lnx)β−1(1−lny)β−2[γ1(y)+γ2(y)M1(z1(y))+Cf]dyydη(x)x −(lnx)β−1β−1∫e1(ξ2+ϵ2−ε2‖σ2‖)(lnx)β−1β−1∫e1[σ1(y)+σ2(y)M2(z1(y))+Cg]dη(y)ydη(x)x. |
(3.3) enables us to obtain
(ϵ1−ε1‖γ2‖)(R1−‖˜z1‖) −(ξ1+ϵ1−ε1‖γ2‖)∫e1(1−lnτ)β−2Γ(β)[γ1(τ)+γ2(τ)M1(z1(τ))+Cf]dττ −ξ1+ϵ1−ε1‖γ2‖β−1∫e1[σ1(τ)+σ2(τ)M2(z1(τ))+Cg]dη(τ)τ≥(ϵ1−ε1‖γ2‖)(R1−‖˜z1‖) −ξ1+ϵ1−ε1‖γ2‖(β−1)Γ(β)[‖γ1‖+‖γ2‖(ε1R1+M∗1)+Cf] −ξ1+ϵ1−ε1‖γ2‖β−1∫e1dη(τ)τ[‖σ1‖+‖σ2‖(ε2R1+M∗2)+Cg]≥0 |
and
(ϵ2−ε2‖σ2‖)(R1−‖˜z1‖) −ξ2+ϵ2−ε2‖σ2‖Γ(β)∫e1(1−lny)β−2[γ1(y)+γ2(y)M1(z1(y))+Cf]dyy −ξ2+ϵ2−ε2‖σ2‖β−1∫e1[σ1(y)+σ2(y)M2(z1(y))+Cg]dη(y)y≥(ϵ2−ε2‖σ2‖)(R1−‖˜z1‖) −ξ2+ϵ2−ε2‖σ2‖(β−1)Γ(β)[‖γ1‖+‖γ2‖(ε1R1+M∗1)+Cf] −ξ2+ϵ2−ε2‖σ2‖β−1∫e1dη(y)y[‖σ1‖+‖σ2‖(ε2R1+M∗2)+Cg]≥0. |
As a result, (3.9) holds, as required. From (3.5) and (3.8), we have
z1(x)+˜z1(x)=(Tz1)(x)+˜z1(x)+μ1ζξ1,ξ2(x)≥(Lξ1,ξ2(z1+˜z1))(x)+μ1ζξ1,ξ2(x),x∈[1,e]. |
Define a set W={μ:z1+˜z1≥μζξ1,ξ2} and μ∗=supW, then μ1∈W and μ∗≥μ1. Hence, note that Lξ1,ξ2:P→P, and we have
z1(x)+˜z1(x)≥μ1ζξ1,ξ2(x)+(Lξ1,ξ2(z1+˜z1))(x)≥μ1ζξ1,ξ2(x)+(Lξ1,ξ2μ∗ζξ1,ξ2)(x)=μ1ζξ1,ξ2(x)+μ∗r(Lξ1,ξ2)ζξ1,ξ2(x)≥(μ∗+μ1)ζξ1,ξ2(x), |
which contradicts the definition of μ∗. As a result, (3.4) holds, and Lemma 2.6 implies that
deg(I−T,BR1,0)=0. | (3.10) |
By (H6), there exists r1∈(0,R1) such that
|f(x,z)|≤ξ3|z|, |g(x,z)|≤ξ4|z|, for |z|∈[0,r1],x∈[1,e]. | (3.11) |
In what follows, we prove that
Tz≠μz,z∈∂Br1,μ≥1, | (3.12) |
where Br1={z∈E:‖z‖<r1}. If (3.12) doesn't hold, and there exist z2∈∂Br1,μ2≥1, such that
Tz2=μ2z2, |
then this, along with (3.11), implies that
|z2(x)|=1μ2|(Tz2)(x)|≤|∫e1Gβ(x,y)f(y,z2(y))dyy+(lnx)β−1β−1∫e1g(x,z2(x))dη(x)x|≤∫e1Gβ(x,y)|f(y,z2(y))|dyy+(lnx)β−1β−1∫e1|g(x,z2(x))|dη(x)x≤ξ3∫e1Gβ(x,y)|z2(y)|dyy+ξ4(lnx)β−1β−1∫e1|z2(x)|dη(x)x=(Lξ3,ξ4|z2|)(x),x∈[1,e]. |
Note that r(Lξ3,ξ4)<1. This means that (I−Lξ3,ξ4)−1 exists and
(I−Lξ3,ξ4)−1=I+Lξ3,ξ4+L2ξ3,ξ4+⋯+Lnξ3,ξ4+⋯. |
Consequently, note that (I−Lξ3,ξ4)−1:P→P, and we have
((I−Lξ3,ξ4)|z2|)(x)≤0⇒|z2(x)|≤(I−Lξ3,ξ4)−10=0, |
which implies that z2(x)≡0,x∈[1,e] and contradicts z2∈∂Br1. Therefore, Lemma 2.7 implies that
deg(I−T,Br1,0)=1. |
Using this with (3.10), we have
deg(I−T,BR1∖¯Br1,0)=deg(I−T,BR1,0)−deg(I−T,Br1,0)=−1. |
Hence, T has at least one fixed point in BR1∖¯Br1, i.e., (1.1) has at least one nontrivial solution. This completes the proof.
Now, we consider the case that our nonlinearities are suberlinear. From [8], we know that E's conjugate space E∗:={ρ:ρ has bounded variation on [1,e]}. Moreover, the dual cone of P and the bounded linear functional on E are
P∗:={ρ∈E∗:ρ is non-decreasing on [1,e]} and ⟨ρ,z⟩=∫e1z(x)dρ(x),z∈E,ρ∈E∗. |
Note that r(Lξ5,ξ6)>1 in (H7), and from the similar method in [23], there exists ψξ5,ξ6∈P∗∖{0} such that
L∗ξ5,ξ6ψξ5,ξ6=r(Lξ5,ξ6)ψξ5,ξ6, | (3.13) |
where L∗ξ5,ξ6:E∗→E∗ is the conjugate operator of Lξ5,ξ6, denoted by
(L∗ξ5,ξ6ρ)(y):=ξ5∫y1dτ∫e1Gβ(x,τ)dρ(x)x+ξ6η(y)∫e1(lnx)β−1β−1dρ(x)x,ρ∈P∗. |
Theorem 3.2. Let (H1)–(H4), (H7), and (H8) hold, then (1.1) has a nontrivial solution.
Proof. From (H7), there exists r2>0 such that
f(x,z)≥ξ5|z|, g(x,z)≥ξ6|z|, for x∈[1,e],|z|≤r2. | (3.14) |
For this r2, we prove that
z−Tz≠μω0, z∈∂Br2,μ≥0, | (3.15) |
where ω0∈P is a fixed element and Br2={z∈E:‖z‖<r2}. We use an argument by indirection, then there exist z3∈∂Br2,μ3≥0 such that
z3−Tz3=μ3ω0. |
Note that by (3.14), we have
(Tz3)(x)=∫e1Gβ(x,y)f(y,z3(y))dyy+(lnx)β−1β−1∫e1g(x,z3(x))dη(x)x≥0,z3∈∂Br2,x∈[1,e]. |
Hence, μ3≥0,ω0∈P enable us to find
z3=Tz3+μ3ω0≥0, |
and
z3(x)≥(Tz3)(x)≥ξ5∫e1Gβ(x,y)z3(y)dyy+ξ6(lnx)β−1β−1∫e1z3(x)dη(x)x. |
Multiplying dψξ5,ξ6(x)x on both sides of the above inequalities and integrating over [1,e], from (3.13), we obtain
∫e1z3(x)dψξ5,ξ6(x)x≥∫e1dψξ5,ξ6(x)x(ξ5∫e1Gβ(x,y)z3(y)dyy+ξ6(lnx)β−1β−1∫e1z3(x)dη(x)x)=∫e1z3(y)yd(ξ5∫y1dτ∫e1Gβ(x,τ)dψξ5,ξ6(x)x+ξ6η(y)∫e1(lnx)β−1β−1dψξ5,ξ6(x)x)=∫e1z3(y)yd(L∗ξ5,ξ6ψξ5,ξ6)(y)=r(Lξ5,ξ6)∫e1z3(y)ydψξ5,ξ6(y). | (3.16) |
Note that ψξ5,ξ6∈P∗∖{0}, then from the definition of the Riemann-Stieltjes integral, we have
∫e1z3(x)dψξ5,ξ6(x)x=limλ→0n∑i=1z3(ξi)ξi[ψξ5,ξ6(xi)−ψξ5,ξ6(xi−1)]≥0, | (3.17) |
where 0=x0<x1<⋯<xn−1<xn<xn+1=1,λ=max1≤i≤n(xi−xi−1),∀ξi∈[xi−1,xi],i= 1,2,⋯,n. Therefore, r(Lξ5,ξ6)>1 and (3.16) enable us to obtain
∫e1z3(x)dψξ5,ξ6(x)x=0. | (3.18) |
Note that for all divisions xi, (3.18) holds, and we only obtain z3(x)≡0,x∈[1,e]. Therefore, this contradicts z3∈∂Br2 and (3.15) holds. Lemma 2.6 implies that
deg(I−T,Br2,0)=0. | (3.19) |
By (H8), there exist d1,d2>0 such that
|f(x,z)|≤ξ7|z|+d1, |g(x,z)|≤ξ8|z|+d2, for |z|∈R,x∈[1,e]. | (3.20) |
In what follows, we prove that S={z∈E:Tz=μz,μ≥1} is a bounded set. If there exist z4∈S,μ4≥1 such that
Tz4=μ4z4, |
then (3.20) implies that
|z4(x)|=1μ4|(Tz4)(x)|≤∫e1Gβ(x,y)|f(y,z4(y))|dyy+(lnx)β−1β−1∫e1|g(x,z4(x))|dη(x)x≤∫e1Gβ(x,y)(ξ7|z4(y)|+d1)dyy+(lnx)β−1β−1∫e1(ξ8|z4(x)|+d2)dη(x)x≤(Lξ7,ξ8|z4|)(x)+d1∫e1Gβ(e,y)dyy+d2∫e1dη(x)xβ−1, x∈[1,e]. |
Note that r(Lξ7,ξ8)<1. Thus (I−Lξ7,ξ8)−1 exists, and
(I−Lξ7,ξ8)−1=I+Lξ7,ξ8+L2ξ7,ξ8+⋯+Lnξ7,ξ8+⋯. |
Consequently, note that (I−Lξ7,ξ8)−1:P→P, and we have
((I−Lξ7,ξ8)|z4|)(x)≤(d1β(β−1)Γ(β)+d2∫e1dη(x)xβ−1) |
and, thus,
|z4(x)|≤(I−Lξ7,ξ8)−1(d1β(β−1)Γ(β)+d2∫e1dη(x)xβ−1), x∈[1,e], |
which implies that S is a bounded set, as required. Let R2>supS and R2>r2, then we have
Tz≠μz, z∈∂BR2,μ≥1. |
Therefore, Lemma 2.7 implies that
deg(I−T,BR2,0)=1. |
Using this with (3.19), we have
deg(I−T,BR2∖¯Br2,0)=deg(I−T,BR2,0)−deg(I−T,Br2,0)=−1. |
Hence, T has at least one fixed point in BR2∖¯Br2, i.e., (1.1) has at least one nontrivial solution. This completes the proof.
Theorem 3.3. Let (H1), (H4), and (H9) hold, then (1.1) has a nontrivial solution.
Proof. Define a linear operator Lξ9,ξ10:E→E as follows:
(Lξ9,ξ10z)(x)=ξ9∫e1Gβ(x,y)z(y)dyy+ξ10(lnx)β−1β−1∫e1z(x)dη(x)x, x∈[1,e], z∈E. |
Now, we prove that 1 isn't an eigenvalue for Lξ9,ξ10. On the contrary, then there exists z∗∈E∖{0} such that
Lξ9,ξ10z∗=z∗. | (3.21) |
By Lemma 2.2, we obtain
{−Dβz∗(x)=ξ9z∗(x), x∈(1,e),z∗(1)=δz∗(1)=0,δz∗(e)=ξ10∫e1z∗(x)dη(x)x. |
Next, we will consider the following two cases.
Case 1. ξ29+ξ210=0. By Lemma 2.2, we have
z∗(x)=˜d1(lnx)β−1+˜d2(lnx)β−2+˜d3(lnx)β−3, |
where ˜di∈R, i=1,2,3. Note that β∈(2,3], the boundary condition z∗(1)=δz∗(1)=δz∗(e)=0 implies that ˜di=0, and z∗(x)≡0, x∈[1,e]. This contradicts z∗∈E∖{0}.
Case 2. ξ29+ξ210≠0. From (3.21), we have
z∗(x)=ξ9∫e1Gβ(x,y)z∗(y)dyy+ξ10(lnx)β−1β−1∫e1z∗(x)dη(x)x≤‖z∗‖(|ξ9|∫e1Gβ(e,y)dyy+|ξ10|∫e1dη(x)xβ−1), x∈[1,e]. |
By (H9), we obtain that
‖z∗‖≤‖z∗‖(|ξ9|β(β−1)Γ(β)+|ξ10|∫e1dη(x)xβ−1)<‖z∗‖. |
This is impossible.
As a result, we claim that 1 isn't an eigenvalue for Lξ9,ξ10, as required.
By (H9), for all ε>0, there exists Λ>0 such that
|f(x,z)−ξ9z|≤ε|z|, |g(x,z)−ξ10z|≤ε|z|, for |z|>Λ, x∈[1,e]. |
Note that when |z|≤Λ and x∈[1,e], |f(x,z)−ξ9z| and |g(x,z)−ξ10z| are bounded. Therefore, there exist ϱi>0(i=1,2) such that
|f(x,z)−ξ9z|≤ε|z|+ϱ1, |g(x,z)−ξ10z|≤ε|z|+ϱ2, z∈R, x∈[1,e]. | (3.22) |
Hence, (3.22) enables us to obtain
‖Tz−Lξ9,ξ10z‖=maxx∈[1,e]|∫e1Gβ(x,y)[f(y,z(y))−ξ9z(y)]dyy+(lnx)β−1β−1∫e1[g(x,z(x))−ξ10z(x)]dη(x)x|≤∫e1Gβ(e,y)|f(y,z(y))−ξ9z(y)|dyy+1β−1∫e1|g(x,z(x))−ξ10z(x)|dη(x)x≤ε‖z‖+ϱ1β(β−1)Γ(β)+∫e1dη(x)xβ−1(ε‖z‖+ϱ2). |
This implies that
lim‖z‖→∞‖Tz−Lξ9,ξ10z‖‖z‖≤ε(1β(β−1)Γ(β)+∫e1dη(x)xβ−1). |
Note that from the arbitrariness of ε, we know that
lim‖z‖→∞‖Tz−Lξ9,ξ10z‖‖z‖=0. |
Lemma 2.8 indicates that T has at least one fixed point, and note that T0≠0 by f,g(t,0)≢0,t∈[1,e]. Therefore, (1.1) has at least one nontrivial solution. This completes the proof.
We note that the spectral theory of linear operators can be used to study differential equations, see for example, [2,6,9,10]. In [9], the authors studied the following fractional boundary value problem
{Dα0+z(t)+q(t)f(t,z(t))=0,0<t<1,n−1<α≤n,z(0)=z′(0)=⋯=z(n−2)(0)=0,z(1)=∫10z(s)dA(s), |
where α≥2,Dα0+ is the Riemann-Liouville derivative and f∈C([0,1]×(0,+∞),R+). They obtained two existence theorems of positive solutions for their problem when the nonlinearity f satisfies one of the following growth conditions
sublinear condition: lim supz→+∞supt∈[0,1]f(t,z)z<λ1, and lim infz→0+inft∈[0,1]f(t,z)z>λ1;
superlinear condition: lim supz→0+supt∈[0,1]f(t,z)z<λ1, and lim infz→+∞inft∈[0,1]f(t,z)z>λ1, where λ1=(r(L))−1, r(L) is the spectral radius of the linear operator (Lz)(t)=∫10GWang(t,s)q(s)z(s)ds, GWang is their Green's function.
Compared with our problem, we don't incorporate the integral boundary conditions into the Green's function, and consider a new linear operator (2.5). Moreover, we obtain several existence theorems of nontrivial solutions under some conditions regarding the spectral radius of the linear operator. On the other hand, our nonlinearities f,g can be sign-changing, in contrast to the nonlinearities in [1,2,3,4,5,6,7,8,9,10], which are assumed to be nonnegative. These imply that our main results generalize and improve the corresponding ones in the works cited above.
The authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.
This research was supported by Talent Introduction Project of Ludong University (Grant No. LY2015004). The authors would like to express their heartfelt gratitude to the editors and reviewers for their constructive comments.
The authors declare there is no conflict of interest.
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