Research article

Lyapunov-type inequalities for Hadamard type fractional boundary value problems

  • Received: 03 November 2019 Accepted: 29 December 2019 Published: 14 January 2020
  • MSC : Primary: 34A08, 34A40; Secondary: 26D10, 33E12, 34C10

  • In this paper, we present few Lyapunov-type inequalities for Hadamard fractional boundary value problems associated with different sets of boundary conditions. Further, we discuss two applications of the established results.

    Citation: Jaganmohan Jonnalagadda, Basua Debananda. Lyapunov-type inequalities for Hadamard type fractional boundary value problems[J]. AIMS Mathematics, 2020, 5(2): 1127-1146. doi: 10.3934/math.2020078

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  • In this paper, we present few Lyapunov-type inequalities for Hadamard fractional boundary value problems associated with different sets of boundary conditions. Further, we discuss two applications of the established results.


    In the last few decades, fractional differential equations have gained more importance due to its applications in various sciences such as physics, mechanics, chemistry, engineering, etc. For a detailed introduction on this topic, we refer the monographs of Podlubny [23], Miller & Ross [16], Kibas et al. [12] and the references therein. Many mathematicians and scientists have contributed to the development of the theory of fractional differential equations. In this process, several types of fractional derivatives were introduced including the Hadamard fractional derivative, which is the focus of this article.

    There has been a rigorous development in the theory and applications of fractional boundary value problems. However, most of the results are concerned with the Riemann-Liouville or the Caputo fractional derivatives. Recently, much attention has been paid to the study of two-point boundary value problems for fractional differential equations involving Hadamard fractional derivatives. In [2], Ahmad and Ntouyas studied a coupled system of Hadamard fractional differential equations together with integral boundary conditions. Also, they developed Hadamard fractional integro-differential boundary value problems in [3]. Wang et al. [26] investigated a non-local Hadamard fractional boundary value problem with Hadamard integral and discrete boundary condition on half line. Recently, Mao et al. [19] and Ardjouni [1] established sufficient conditions on positive solutions for Hadamard fractional boundary value problems. More recently, Wang et al. [27,28] analysed the stability properties of nonlinear Hadamard fractional differential system.

    On the other hand, Lyapunov [14] proved a necessary condition for the existence of a nontrivial solution of Hill's equation associated with Dirichlet boundary conditions.

    Theorem 1.1. [14] If the boundary value problem

    {y(t)+q(t)y(t)=0,a<t<b,y(a)=y(b)=0, (1.1)

    has a nontrivial solution, where q:[a,b]R is a continuous function, then

    ba|q(s)|ds>4ba. (1.2)

    The Lyapunov inequality (1.2) has several applications in various problems related to differential equations. Due to its importance, it has been generalized in many forms. Many researchers have derived Lyapunov-type inequalities for various classes of fractional boundary value problems in the recent years. For the first time, in 2013, Ferreira [8] generalized Theorem 1.1 to the case where the classical second-order derivative in (1.1) is replaced by the αth-order (1<α2) Riemann–Liouville fractional derivative. Further, in 2014, Ferreira [9] developed a Lyapunov-type inequality for the Caputo fractional derivative. In 2018, Ntouyas et al. [21] presented a survey of results on Lyapunov-type inequalities for fractional differential equations associated with a variety of boundary conditions. For more details on Lyapunov-type inequalities and their applications, we refer [4,6,10,11,22,24,25,29,30] and the references therein.

    In particular, Ma et al. [17] developed a Lyapunov-type inequality for the Hadamard fractional boundary value problem in 2017.

    Theorem 1.2. If the Hadamard fractional boundary value problem

    {HDαy(t)q(t)y(t)=0,1<t<e,1<α2,y(1)=y(e)=0, (1.3)

    has a non-trivial solution, where q:[1,e]R is a continuous function, then

    e1|q(s)|ds>Γ(α)(1λ)1αλ1αeλ. (1.4)

    Here λ=2α1(2α2)2+12 and HDα denotes the αth-order Hadamard fractional differential operator with 1<α2.

    Recently, Dhar [7] and Laadjal et al. [15] generalized the Lyapunov-type inequality in Theorem 1.2 by replacing the interval [1,e] with [a,b].

    Theorem 1.3. If the Hadamard fractional boundary value problem

    {HDαy(t)+q(t)y(t)=0,0<a<t<b,1<α2,y(a)=y(b)=0, (1.5)

    has a non-trivial solution and y(t)0 on (a,b), where q:[a,b]R is a continuous function, then

    baq+(s)ds>4α1Γ(α)(logba)α1. (1.6)

    Here q+(t)=max{q(t),0}.

    Theorem 1.4. If the Hadamard fractional boundary value problem

    {HDαy(t)+q(t)y(t)=0,1a<t<b,1<α2,y(a)=y(b)=0, (1.7)

    has a non-trivial solution, where q:[a,b]R is a continuous function, then

    ba|q(s)|ds>Γ(α)ξ1(logξ1alogbξ1logba)1α. (1.8)

    where

    ξ1=exp(12[[(2α2)+logba](2α2)2+log2ba]).

    Motivated by the works in [7,15,17], in this article, we establish a few Lyapunov-type inequalities for Hadamard fractional boundary value problems associated with a variety of boundary conditions.

    Throughout, we shall use the following notations, definitions and some lemmas from the theory of fractional calculus in the sense of Hadamard. These results can be found in the monographs [6,12]. Denote the set of all real numbers and complex numbers by R and C, respectively.

    Definition 2.1. [12] Let α>0 and aR. The αth-order Hadamard fractional integral of a function y:[a,b]R is defined by

    (HIαy)(t)=1Γ(α)ta(logts)α1y(s)dss,a<t<b, (2.1)

    provided the right-hand side exists. Here Γ(.) denotes the Euler's Gamma function.

    Definition 2.2. [12] The αth-order Hadamard fractional derivative of a function y:[a,b]R is defined by

    (HDαy)(t)=1Γ(nα)(tddt)nta(logts)nα1y(s)dss,a<t<b, (2.2)

    where n=[α]+1.

    Definition 2.3. [12] C[a,b] be the space of all continuous functions y:[a,b]R with the norm

    yC=maxt[a,b]|y(t)|.

    Definition 2.4. [12] Let 0γ<1, y:(a,b]R and define

    yγ,log(t)=(logta)γy(t),t[a,b].

    Cγ,log[a,b] be the weighted space of functions y such that yγ,logC[a,b], and

    yCγ,log=maxt[a,b]|(logta)γy(t)|.

    Lemma 2.1. [12] If α>0, β>0 and 0<a<b<, then

    (HIα(logta)β1)(x)=Γ(β)Γ(β+α)(logxa)β+α1,(HDα(logta)β1)(x)=Γ(β)Γ(βα)(logxa)βα1.

    Lemma 2.2. [6] Let α>0, n=[α]+1, and 0<a<b<. Assume yC(a,b). The equality

    (HDαy)(t)=0

    is valid if, and only if,

    y(t)=C1(logta)α1+C2(logta)α2++Cn(logta)αn,

    where C1, C2, , Cn are arbitrary constants.

    Lemma 2.3. [6] Let α>0, n=[α]+1, and 0<a<b<. Assume yC(a,b). Then,

    (HDα(HIαy))(t)=y(t),

    and

    (HIα(HDαy))(t)=y(t)+ni=1Ci(logta)αi,

    where C1, C2, , Cn are arbitrary constants.

    In this section, we obtain Lyapunov-type inequalities for Hadamard fractional boundary value problems associated with mixed, Sturm-Liouville, Robin and general boundary conditions, using the properties of the corresponding Green's functions.

    Theorem 3.1. Let 1<α2 and h:[a,b]R. The fractional boundary value problem

    {(HDαay)(t)+h(t)=0,a<t<b,l(HI2αay)(a)m(HDα1ay)(a)=0,ny(b)+p(HDα1ay)(b)=0, (3.1)

    has the unique solution

    y(t)=baG(t,s)h(s)ds, (3.2)

    where G(t,s) is given by

    G(t,s)={G1(t,s),a<stb,G2(t,s),a<tsb, (3.3)
    G1(t,s)=G2(t,s)(logts)α1sΓ(α), (3.4)

    and

    G2(t,s)=[l(logta)α1+m(α1)(logta)α2sA][n(logbs)α1Γ(α)+p]. (3.5)

    Here l, p0; m, n>0 and

    A=ln(logba)α1+mn(α1)(logba)α2+lpΓ(α)>0.

    Proof. Applying HIαa (the αth-order Hadamard fractional integral operator) on both sides of (3.1) and using Lemma 2.2, we have

    y(t)=(HIαah)(t)+C1(logta)α1+C2(logta)α2, (3.6)

    for some C1, C2R. Applying HI2αa on both sides of (3.6) and using Lemmas 2.1, we get

    (HI2αay)(t)=(HI2ah)(t)+C1Γ(α)(logta)+C2Γ(α1). (3.7)

    Applying HDα1a (the (α1)th-order Hadamard fractional differential operator) on both sides of (3.6) and using Lemmas 2.1, we obtain

    (HDα1ay)(t)=(HI1ah)(t)+C1Γ(α). (3.8)

    From the first boundary condition, we have

    mC1(α1)+lC2=0. (3.9)

    The second boundary condition yields

    C1[n(logba)α1+pΓ(α)]+nC2(logba)α2=n(HIαah)(b)+p(HI1ah)(b). (3.10)

    Solving (3.9) and (3.10) for C1 and C2, we have

    C1=lAba(n(logbs)α1Γ(α)+p)h(s)dss,

    and

    C2=m(α1)Aba(n(logbs)α1Γ(α)+p)h(s)dss.

    Substituting C1 and C2 in (3.6), it follows that

    y(t)=l(logta)α1Aba(n(logbs)α1Γ(α)+p)h(s)dss+m(α1)(logta)α2Aba(n(logbs)α1Γ(α)+p)h(s)dss1Γ(α)ta(logta)α1h(s)dss=baG(t,s)h(s)ds.

    The proof is complete.

    Corollary 1. Let 1<α2 and h:[a,b]R. The fractional boundary value problem

    {(HDαay)(t)+h(t)=0,a<t<b,y(a)=0,ny(b)+p(HDα1ay)(b)=0, (3.11)

    has the unique solution

    y(t)=baˉG(t,s)h(s)ds, (3.12)

    where ˉG(t,s) is given by

    ˉG(t,s)={ˉG1(t,s),astb,ˉG2(t,s),atsb, (3.13)
    ˉG1(t,s)=ˉG2(t,s)(logts)α1sΓ(α), (3.14)

    and

    ˉG2(t,s)=(logta)α1sˉA(n(logbs)α1Γ(α)+p). (3.15)

    Here n0, p>0 and ˉA=n(logba)α1+pΓ(α)>0.

    Proof. The proof is similar to Theorem 3.1.

    We define H(t,s)=sG(t,s) and ˉH(t,s)=sˉG(t,s). Now, we prove that these Green's functions are positive and obtain upper bounds for both the Green's functions and their integrals.

    Theorem 3.2. The Green's function H(t,s) for (3.1) satisfies H(t,s)>0 for (t,s)(a,b]×(a,b].

    Proof. Clearly, for a<tsb,

    H(t,s)=[l(logta)α1+m(α1)(logta)α2A][n(logbs)α1Γ(α)+p]>0.

    Now, suppose a<stb. Consider

    H(t,s)=[l(logta)α1+m(α1)(logta)α2A][n(logbs)α1Γ(α)+p](logts)α1Γ(α)=lnAΓ(α){(logta)α1(logbs)α1(logba)α1(logts)α1}+mn(α1)AΓ(α){(logta)α2(logbs)α1(logba)α2(logts)α1}+lpA{(logta)α1(logts)α1}+mp(α1)A(logta)α2=1AΓ(α)[X1+X2+X3+X4]. (3.16)

    Clearly, AΓ(α)>0. Consider

    (logta)(logbs)(logba)(logts)=(logtloga)(logblogs)(logbloga)(logtlogs)=(logsloga)(logblogt)0,

    implying that

    X1=ln{(logta)α1(logbs)α1(logba)α1(logts)α1}0. (3.17)

    Since

    a<stb,

    we have

    (logta)α2(logba)α2,(logbs)α1(logts)α1

    and

    (logta)α1>(logts)α1,

    implying that

    X2=mn(α1){(logta)α2(logbs)α1(logba)α2(logts)α1}mn(α1)(logba)α2{(logbs)α1(logts)α1}0, (3.18)

    and

    X3=lpΓ(α)[(logta)α1(logts)α1]>0. (3.19)

    Clearly,

    X4=mp(α1)Γ(α)(logta)α2>0. (3.20)

    Using (3.17) - (3.20) in (3.16), we have H(t,s)>0. The proof is complete.

    Corollary 2. The Green's function ˉH(t,s) for (3.11) satisfies ˉH(t,s)0 for (t,s)[a,b]×[a,b].

    Proof. The proof is similar to Theorem 3.2.

    Theorem 3.3. For the Green's function H(t,s) defined in (3.3),

    maxs(a,b]H(t,s)=H(t,t),t(a,b],

    and

    (logta)2αH(t,t)<[l(logba)+m(α1)A][n(logba)α1Γ(α)+p],t[a,b].

    Proof. For the first part, we show that for any fixed t(a,b], H(t,s) increases with respect to s from a to t, and then decreases with respect s from t to b. Let a<tsb. Consider

    sH(t,s)=[n(α1)(logbs)α2sΓ(α)][l(logta)α1+m(α1)(logta)α2A]<0,

    implying that H(t,s) is a decreasing function of s. Now, suppose a<stb. Consider

    sH(t,s)=[n(α1)(logbs)α2sΓ(α)][l(logta)α1+m(α1)(logta)α2A]+(α1)(logts)α2sΓ(α)=ln(α1)AΓ(α){(logta)α1(logbs)α2+(logba)α1(logts)α2}+mn(α1)2AΓ(α){(logta)α2(logbs)α2+(logba)α2(logts)α2}+lp(α1)A(logts)α2=(α1)AΓ(α)[X5+X6+X7]. (3.21)

    Clearly, (α1)AΓ(α)>0. Since a<s<tb, we have

    (logts)α2(logbs)α2and(logba)α1(logta)α1,

    implying that

    X5=ln[(logta)α1(logbs)α2+(logba)α1(logts)α2]ln(logts)α2[(logta)α1+(logba)α1]0. (3.22)

    Since

    (logta)(logbs)(logba)(logts)=(logtloga)(logblogs)(logbloga)(logtlogs)=(logsloga)(logblogt)0,

    we have that

    X6=mn(α1)2{(logta)α2(logbs)α2+(logba)α2(logts)α2}0. (3.23)

    Clearly,

    X7=lpΓ(α)(logts)α2>0. (3.24)

    Using (3.22) - (3.24) in (3.21), we have sH(t,s)>0, implying that H(t,s) is an increasing function of s. Then, it follows that

    maxs(a,b]H(t,s)=H(t,t),t(a,b].

    To prove the second part, for t[a,b], consider

    (logta)2αH(t,t)=[l(logta)+m(α1)A][n(logbt)α1Γ(α)+p]<[l(logba)+m(α1)A][n(logba)α1Γ(α)+p].

    The proof is complete.

    Corollary 3. For the Green's function ˉH(t,s) defined in (3.13),

    maxs[a,b]ˉH(t,s)=ˉH(t,t),t[a,b],

    and

    ˉH(t,t)<[(logba)α1ˉA][n(logba)α1Γ(α)+p],t[a,b].

    Proof. The first part of the proof is similar to the proof of Theorem 3.3. To prove the second part, for t[a,b], consider

    ˉH(t,t)=[(logta)α1ˉA][n(logbt)α1Γ(α)+p]<[(logba)α1ˉA][n(logba)α1Γ(α)+p].

    The proof is complete.

    We are now able to formulate Lyapunov-type inequalities for the fractional boundary value problems (3.1) and (3.11).

    Theorem 3.4. If the following fractional boundary value problem

    {(HDαy)(t)+p(t)y(t)=0,0<a<t<b,l(HI2αy)(a)m(HDα1y)(a)=0,ny(b)+p(HDα1y)(b)=0, (3.25)

    has a nontrivial solution, then

    ba(logsa)α2|p(s)|ds>AΓ(α)[n(logba)α1+pΓ(α)][l(logba)+m(α1)]. (3.26)

    Proof. Let B=Cγ,log[a,b] be the Banach space of functions y endowed with norm

    yCγ,log=maxt[a,b]|(logta)γy(t)|.

    It follows from Theorem 3.1 that a solution to (3.25) satisfies the equation

    y(t)=baH(t,s)p(s)y(s)ds=basG(t,s)p(s)y(s)ds.

    Hence,

    yC2α,log=maxt[a,b]|(logta)2αbasG(t,s)p(s)y(s)ds|maxt[a,b][ba|(logta)2αsG(t,s)||p(s)||y(s)|ds]yC2α,log[maxt[a,b]ba|(logta)2αH(t,s)|(logsa)α2|p(s)|ds]yC2α,log[maxt[a,b]|(logta)2αH(t,s)|]ba(logsa)α2|p(s)|ds,

    or, equivalently,

    1<[|(logta)2αH(t,t)|]ba(logsa)α2|p(s)|ds.

    An application of Theorem 3.3 yields the result.

    Corollary 4. If the following fractional boundary value problem

    {(HDαay)(t)+q(t)y(t)=0,a<t<b,y(a)=0,ny(b)+p(HDα1ay)(b)=0, (3.27)

    has a nontrivial solution, then

    ba|q(s)|ds>ˉAΓ(α)[n(logba)2α2+p(logba)α1Γ(α)]. (3.28)

    Proof. Let B=C[a,b] be the Banach space of functions y endowed with norm

    y=maxt[a,b]|y(t)|.

    It follows from Corollary 1 that a solution to (3.27) satisfies the equation

    y(t)=baˉH(t,s)q(s)y(s)ds=basˉH(t,s)q(s)y(s)ds.

    Hence,

    y=maxt[a,b]|baˉH(t,s)q(s)y(s)ds|maxt[a,b][baˉH(t,s)|q(s)||y(s)|ds]y[maxt[a,b]baˉH(t,s)|q(s)|ds]y[maxt[a,b]ˉH(t,t)]ba|q(s)|ds,

    or, equivalently,

    1<[maxt[a,b]ˉH(t,t)]ba|q(s)|ds.

    An application of Corollary 3 yields the result.

    Take l=p=0 in Theorem 3.4. Then, we obtain the following Lyapunov-type inequality for the left-focal fractional boundary value problem.

    Corollary 5. If the following fractional boundary value problem

    {(HDαay)(t)+q(t)y(t)=0,a<t<b,(HDα1ay)(a)=0,y(b)=0, (3.29)

    has a nontrivial solution, then

    ba(logsa)α2|q(s)|ds>Γ(α)(logba). (3.30)

    Take n=0 in Corollary 4. Then, we obtain the following Lyapunov-type inequality for the right-focal fractional boundary value problem.

    Corollary 6. If the following fractional boundary value problem

    {(HDαay)(t)+q(t)y(t)=0,a<t<b,y(a)=0,(HDα1ay)(b)=0, (3.31)

    has a nontrivial solution, then

    ba|q(s)|ds>Γ(α)(logba)α1. (3.32)

    Take l=m=n=p=1 in Theorem 3.4. Then, we obtain the following Lyapunov-type inequality for the fractional boundary value problem with Robin boundary conditions.

    Corollary 7. If the following fractional boundary value problem

    {(HDαay)(t)+q(t)y(t)=0,a<t<b,(HI2αay)(a)(HDα1ay)(a)=0,y(b)+(HDα1ay)(b)=0, (3.33)

    has a nontrivial solution, then

    ba(logsa)α2|q(s)|ds>Γ(α)[(logba)α1+(α1)(logba)α2+Γ(α)][(logba)α1+Γ(α)][logba+α1]. (3.34)

    Take l>0 and p=0 in Theorem 3.4. Then, we obtain the following Lyapunov-type inequality for the fractional boundary value problem with Sturm-Liouville boundary conditions.

    Corollary 8. If the following fractional boundary value problem

    {(HDαay)(t)+q(t)y(t)=0,a<t<b,l(HI2αay)(a)m(HDα1ay)(a)=0,y(b)=0, (3.35)

    has a nontrivial solution, then

    ba(logsa)α2|q(s)|ds>Γ(α)logba. (3.36)

    In this section, we obtain a Lyapunov-type inequality for an anti-periodic fractional boundary value problem using the properties of the corresponding Green's function.

    Theorem 4.1. Let 1<α2 and h:[1,T]R. The fractional boundary value problem

    {HDαy(t)+h(t)=0,1<t<T,(HI2αy)(1)+(HI2αy)(T)=0,(HDα1y)(1)+(HDα1y)(T)=0, (4.1)

    has the unique solution

    y(t)=T1˜G(t,s)h(s)ds,1<tT, (4.2)

    where

    ˜G(t,s)={(logt)α12sΓ(α)+(logt)α2(logT2logs)4sΓ(α1)(logts)α1sΓ(α),1stT,(logt)α12sΓ(α)+(logt)α2(logT2logs)4sΓ(α1),1tsT. (4.3)

    Proof. Applying HIα on both sides of (4.1) and using Lemma 2.2, we have

    y(t)=C1(logt)α1+C2(logt)α2t1(logtlogs)α1h(s)dss, (4.4)

    for some C1, C2R. Applying HI2α on both sides of (4.4) and using Lemma (2.1), we get

    (HI2αy)(t)=t1h(s)dss+C1Γ(α)(logt)+C2Γ(α1). (4.5)

    Applying HDα1 on both sides of (4.4) and using Lemma (2.1), we obtain

    (HDα1y)(t)=t1h(s)dss+C1Γ(α). (4.6)

    From the first boundary condition, we get

    C1Γ(α)(logT)+2C2Γ(α1)=T1(logTs)h(s)dss. (4.7)

    The second boundary condition yields

    T1h(s)dss=2C1Γ(α). (4.8)

    Solving (4.7) and (4.8) for C1 and C2, we have

    C1=12Γ(α)T1h(s)dss,

    and

    C2=14Γ(α1)T1(logT2logs)h(s)dss.

    Substituting C1 and C2 in (3.6), we obtain the unique solution of (4.1) as

    y(t)=(logt)α12Γ(α)T1h(s)dss+(logt)α24Γ(α1)T1(logT2logs)h(s)dss1Γ(α)t1(logtlogs)α1h(s)dss=t1[(logt)α12sΓ(α)+(logt)α2(logT2logs)4sΓ(α1)(logts)α1sΓ(α)]h(s)ds+Tt[(logt)α12sΓ(α)+(logt)α2(logT2logs)4sΓ(α1)]h(s)ds=T1˜G(t,s)h(s)ds.

    The proof is complete.

    Let us define ˜H(t,s)=s(logt)2α˜G(t,s) Now, we obtain an upper bound for the Green's function ˜H(t,s).

    Theorem 4.2. For the Green's function ˜H(t,s) defined in (4.3), we observe that

    |˜H(t,s)|<(3α)logT4Γ(α),(t,s)[1,T]×[1,T].

    Proof. Consider

    ˜H(t,s)={logt2Γ(α)+(logT2logs)4Γ(α1)(logt)2α(logtlogs)α1Γ(α),1stT,logt2Γ(α)+(logT2logs)4Γ(α1),1tsT. (4.9)

    Denote by

    ~H1(t,s)=logt2Γ(α)+(logT2logs)4Γ(α1)(logt)2α(logtlogs)α1Γ(α)

    and

    ~H2(t,s)=logt2Γ(α)+(logT2logs)4Γ(α1).

    For a fixed t[1,T],

    dds~H1(t,s)=(α1)(logtlogs)α2(logt)2αsΓ(α)24sΓ(α1)=(logtlogs)2α+(logt)2α2sΓ(α1)(logtlogs)2α0,

    for all s[1,t]. So, ~H1(t,s) is an increasing function of s. Thus,

    maxs[1,t]|~H1(t,s)|=max{|~H1(t,1)|,|~H1(t,t)|}.

    We observe that ~H1(t,t) is an increasing function of s, since

    ddt~H1(t,t)=2α2tΓ(α)>0.

    Therefore, we have

    maxs[1,T]~H1(t,t)=max{|~H1(1,1)|,|~H1(T,T)|}=max{logT4Γ(α1),(3α)logT4Γ(α)}=(3α)logT4Γ(α).

    Now, consider

    ddt~H1(t,1)=12tΓ(α)<0,

    implying that H1(t,1) is a decreasing function of t. So, we have

    maxt[1,T]|~H1(t,1)|=max{|~H1(1,1)|,|~H1(T,1)|}=max{logT4Γ(α1),(3α)logT4Γ(α)}=(3α)logT4Γ(α).

    Therefore,

    maxs[1,t],t[1,T]|~H1(t,s)|=(3α)logT4Γ(α). (4.10)

    For a fixed s[1,T],

    ddt~H2(t,s)=12tΓ(α)>0,

    implying that ~H2(t,s) is an increasing function of t. So,

    maxt[1,s]|~H2(t,s)|=max{|~H2(1,s)|,|~H2(s,s)|}.

    Since |~H2(s,s)|=|~H1(s,s)| for s[1,T], we only consider ~H2(1,s). Since

    dds~H2(1,s)=12sΓ(α1)<0,

    ~H2(1,s) is a decreasing function of s. Thus, we have

    maxs[1,T]|~H2(1,s)|=max{|~H2(1,1)|,|~H2(1,T)|}=max{logT4Γ(α1),logT4Γ(α1)}=logT4Γ(α1).

    Hence, we have

    maxt[1,s],s[1,T]|~H2(t,s)|=(3α)logT4Γ(α). (4.11)

    The final result follows from (4.10) and (4.11).

    We are now able to formulate a Lyapunov-type inequality for the Hadamard type fractional boundary value problem with anti-periodic boundary condition.

    Theorem 4.3. If the following fractional boundary value problem

    {(HDαy))(t)+p(t)y(t)=0,1<t<T,(HI2αy)(0)+(HI2αy)(T)=0,(HDα1y)(0)+(HDα1y)(T)=0, (4.12)

    has a nontrivial solution, then

    T1(logs)α2|p(s)|ds>4Γ(α)(3α)logT. (4.13)

    Proof. Let B=Cγ,log[1,T] be the Banach space of functions y endowed with norm

    yCγ,log=maxt[1,T]|(logt)γy(t)|.

    It follows from Theorem 4.1 that a solution to (4.12) satisfies the equation

    y(t)=T1˜H(t,s)p(s)y(s)ds=T1(logt)2αs˜G(t,s)p(s)y(s)ds.

    Hence,

    yC2α,log=maxt[1,T]|(logt)2αT1s˜G(t,s)p(s)y(s)ds|maxt[1,T][T1|(logt)2αs˜G(t,s)||p(s)||y(s)|ds]yC2α,log[maxt[1,T]T1|(logt)2αs˜G(t,s)|(logs)α2|p(s)|ds]yC2α,log[maxt[1,T]|(logt)2αs˜G(t,s)|]T1(logs)α2|p(s)|ds,

    or, equivalently,

    1<[maxt[1,T]|˜H(t,s)|]T1(logs)α2|p(s)|ds.

    An application of Theorem 4.2 yields the result.

    In this section, we discuss two applications of the results established in previous sections. First, we estimate lower bounds on the smallest eigenvalues of the eigenvalue problems corresponding to (3.25), (3.27) and (3.25).

    Theorem 5.1. Assume y is a nontrivial solution of the Hadamard fractional eigenvalue problem

    {(HDαay)(t)+p(t)y(t)=0,a<t<b,l(HI2αay)(a)m(HDα1ay)(a)=0,ny(b)+p(HDα1ay)(b)=0,

    where y(t)0 for each t(a,b). Then,

    |λ|>(1)αAΓ(α)[Γ(α1)Γ(α1,logba)]1a[n(logba)α1+pΓ(α)][l(logba)+m(α1)].

    Corollary 9. Assume y is a nontrivial solution of the Hadamard fractional eigenvalue problem

    {(HDαay)(t)+p(t)y(t)=0,a<t<b,y(a)=0,ny(b)+p(HDα1ay)(b)=0,

    where y(t)0 for each t(a,b). Then,

    |λ|>ˉAΓ(α)(logba)α[n(logba)α1+pΓ(α)].

    Theorem 5.2. Assume y is a nontrivial solution of the Hadamard fractional eigenvalue problem

    {(HDαy)(t)+λy(t)=0,1<t<T,(HI2αy)(0)+(HI2αy)(T)=0,(HDα1y)(0)+(HDα1y)(T)=0, (5.1)

    where y(t)0 for each t(1,T). Then,

    |λ|>4Γ(α)(α1)[Γ(α1)Γ(α1,logT)]logT(3α).

    Proof. From (4.13), we obtain

    T1(logs)α2|λ|ds>4Γ(α)(3α)logT,

    or, equivalently,

    |λ|>4Γ(α)[Γ(α1)Γ(α1,logT)]logT(3α).

    This proves the result (5.2).

    The proof is complete. Now we will discuss the disconjugacy and disfocality for Hadamard fractional boundary value problems (1.5), (3.29) and (3.31).

    Definition 5.1. The Hadamard fractional boundary value problem (1.5) is disconjugate on [a,b] if and only if each nontrivial solution has less than [α]+1 zeros on [a,b].

    Definition 5.2. The Hadamard fractional boundary value problem (3.29) is left disfocal on [a,b] if and only if each nontrivial solution has less than [α] zeros on [a,b].

    Definition 5.3. The Hadamard fractional boundary value problem (3.31) is right disfocal on [a,b] if and only if each nontrivial solution has less than [α] zeros on [a,b].

    Using these definitions, we introduce non-existence criteria for non-trivial solutions as follows:

    Theorem 5.3. The Hadamard fractional boundary value problem (1.5) is disconjugate if

    ba|q(s)|dsΓ(α)(4)α1(logba)α1. (5.2)

    Theorem 5.4. Assume that the assumptions of Theorem 5.3 are satisfied. Then, the Hadamard fractional boundary value problem (1.5) has no non-trivial solution on [a,b].

    Theorem 5.5. The Hadamard fractional boundary value problem (3.29) is left disfocal if

    ba(logsa)α2|q(s)|dsΓ(α)logba. (5.3)

    Theorem 5.6. Assume that the assumptions of Theorem 5.5 are satisfied. Then, the Hadamard fractional boundary value problem (3.29) has no non-trivial solution on [a,b].

    Theorem 5.7. The Hadamard fractional boundary value problem (3.31) is right disfocal if

    ba|q(s)|dsΓ(α)(logba)α1. (5.4)

    Theorem 5.8. Assume that the assumptions of Theorem 5.7 are satisfied. Then, the Hadamard fractional boundary value problem (3.31) has no non-trivia l solution on [a,b].

    In this article, we considered Hadamard fractional boundary value problems associated with two different types of boundary conditions-general and anti-periodic, and established Lyapunov-type inequalities for the same. In this process, we derived a few important properties of the corresponding Green's functions. In the later part of the article, we illustrated the applicability of established results through two applications. As the first application, we obtained lower bounds on the smallest eigenvalues for the corresponding Hadamard fractional eigenvalue problems. For the second application, we introduced the concepts of disconjugacy and disfocality and using which we obtained non-existence criteria for non-trivial solutions of Hadamard fractional boundary value problems.

    All the authors declare no conflicts of interest.



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