Processing math: 100%
Research article Special Issues

On a nabla fractional boundary value problem with general boundary conditions

  • In this article, we consider a nabla fractional boundary value problem with general boundary conditions. Brackins & Peterson [5] gave an explicit expression for the corresponding Green's function. Here, we show that this Green's function is nonnegative and obtain an upper bound for its maximum value. Since the expression for the Green's function is complicated, derivation of its properties may not be straightforward. For this purpose, we use a few properties of fractional nabla Taylor monomials. Using the Green's function, we will then develop a Lyapunov-type inequality for the nabla fractional boundary value problem.

    Citation: Jagan Mohan Jonnalagadda. On a nabla fractional boundary value problem with general boundary conditions[J]. AIMS Mathematics, 2020, 5(1): 204-215. doi: 10.3934/math.2020012

    Related Papers:

    [1] Lakhdar Ragoub, J. F. Gómez-Aguilar, Eduardo Pérez-Careta, Dumitru Baleanu . On a class of Lyapunov's inequality involving $ \lambda $-Hilfer Hadamard fractional derivative. AIMS Mathematics, 2024, 9(2): 4907-4924. doi: 10.3934/math.2024239
    [2] Jaganmohan Jonnalagadda, Basua Debananda . Lyapunov-type inequalities for Hadamard type fractional boundary value problems. AIMS Mathematics, 2020, 5(2): 1127-1146. doi: 10.3934/math.2020078
    [3] Amna Kalsoom, Sehar Afsheen, Akbar Azam, Faryad Ali . Existence and compatibility of positive solutions for boundary value fractional differential equation with modified analytic kernel. AIMS Mathematics, 2023, 8(4): 7766-7786. doi: 10.3934/math.2023390
    [4] Shuqin Zhang, Lei Hu . The existence of solutions and generalized Lyapunov-type inequalities to boundary value problems of differential equations of variable order. AIMS Mathematics, 2020, 5(4): 2923-2943. doi: 10.3934/math.2020189
    [5] Rabah Khaldi, Assia Guezane-Lakoud . On a generalized Lyapunov inequality for a mixed fractional boundary value problem. AIMS Mathematics, 2019, 4(3): 506-515. doi: 10.3934/math.2019.3.506
    [6] Limin Guo, Lishan Liu, Ying Wang . Maximal and minimal iterative positive solutions for $ p $-Laplacian Hadamard fractional differential equations with the derivative term contained in the nonlinear term. AIMS Mathematics, 2021, 6(11): 12583-12598. doi: 10.3934/math.2021725
    [7] Wei Zhang, Jifeng Zhang, Jinbo Ni . New Lyapunov-type inequalities for fractional multi-point boundary value problems involving Hilfer-Katugampola fractional derivative. AIMS Mathematics, 2022, 7(1): 1074-1094. doi: 10.3934/math.2022064
    [8] Yitao Yang, Dehong Ji . Properties of positive solutions for a fractional boundary value problem involving fractional derivative with respect to another function. AIMS Mathematics, 2020, 5(6): 7359-7371. doi: 10.3934/math.2020471
    [9] Hasanen A. Hammad, Hassen Aydi, Manuel De la Sen . The existence and stability results of multi-order boundary value problems involving Riemann-Liouville fractional operators. AIMS Mathematics, 2023, 8(5): 11325-11349. doi: 10.3934/math.2023574
    [10] Varaporn Wattanakejorn, Sotiris K. Ntouyas, Thanin Sitthiwirattham . On a boundary value problem for fractional Hahn integro-difference equations with four-point fractional integral boundary conditions. AIMS Mathematics, 2022, 7(1): 632-650. doi: 10.3934/math.2022040
  • In this article, we consider a nabla fractional boundary value problem with general boundary conditions. Brackins & Peterson [5] gave an explicit expression for the corresponding Green's function. Here, we show that this Green's function is nonnegative and obtain an upper bound for its maximum value. Since the expression for the Green's function is complicated, derivation of its properties may not be straightforward. For this purpose, we use a few properties of fractional nabla Taylor monomials. Using the Green's function, we will then develop a Lyapunov-type inequality for the nabla fractional boundary value problem.


    Let a, bR with baN1. Consider the homogeneous nabla fractional boundary value problem with general boundary conditions:

    {(ν1a(u))(t)=0,tNba+2,αu(a+1)β(u)(a+1)=0,γu(b)+δ(u)(b)=0, (1.1)

    where 1<ν<2, α2+β2>0 and γ2+δ2>0. Brackins & Peterson [5] proved that the boundary value problem (1.1) has only the trivial solution if, and only if

    ξ=(βα)γ+αγHν1(b,a)+αδHν2(b,a)0. (1.2)

    In the following theorem, Brackins & Peterson [5] gave an explicit expression for its Green's function.

    Theorem 1.1 (See [5]). Assume (1.2) holds. The Green's function for the boundary value problem (1.1) is given by

    G(t,s)={u(t,s),ts1,v(t,s),ts, (1.3)

    where

    u(t,s)=1ξ[αγHν1(t,a)Hν1(b,ρ(s))+αδHν1(t,a)Hν2(b,ρ(s))+(βα)γHν1(b,ρ(s))+(βα)δHν2(b,ρ(s))], (1.4)

    and

    v(t,s)=u(t,s)Hν1(t,ρ(s)). (1.5)

    We show that this Green's function is nonnegative and obtain an upper bound for its maximum value. Using the Green's function, we will then develop a Lyapunov-type inequality for the nabla fractional boundary value problem

    {(ν1a(u))(t)+q(t)u(t)=0,tNba+2,αu(a+1)β(u)(a+1)=0,γu(b)+δ(u)(b)=0, (1.6)

    where q:Nba+1R.

    We shall use the following notations, definitions and known results of nabla fractional calculus throughout the article [1,2,3,6,9,10,11,12,13]. Denote by Na:={a,a+1,a+2,} and Nba:={a,a+1,a+2,,b} for any a, bR such that baN1.

    Definition 2.1(See [4]). The backward jump operator ρ:NaNa is defined by

    ρ(t):={a,t=a,t1,tNa+1.

    Definition 2.2 (See [14,15]). The Euler gamma function is defined by

    Γ(z):=0tz1etdt,(z)>0.

    Using its well-known reduction formula, the Euler gamma function can be extended to the half-plane (z)0 except for z{,2,1,0}.

    Definition 2.3 (See [7]). For tR{,2,1,0} and rR such that (t+r)R{,2,1,0}, the generalized rising function is defined by

    t¯r:=Γ(t+r)Γ(t).

    Also, if t{,2,1,0} and rR such that (t+r)R{,2,1,0}, then we use the convention that t¯r:=0.

    Definition 2.4 (See [7]). Let μR{,2,1}. Define the μth-order nabla fractional Taylor monomial by

    Hμ(t,a):=(ta)¯μΓ(μ+1),

    provided the right-hand side exists. Observe that Hμ(a,a)=0 and Hμ(t,a):=0 for all μ{,2,1} and tNa.

    Definition 2.5 (See [4]). Let u:NaR and NN1. The first order backward (nabla) difference of u is defined by

    (u)(t):=u(t)u(t1),tNa+1,

    and the Nth-order nabla difference of u is defined recursively by

    (Nu)(t):=((N1u))(t),tNa+N.

    Definition 2.6 (See [7]). Let u:Na+1R and NN1. The Nth-order nabla sum of u based at a is given by

    (Nau)(t):=ts=a+1HN1(t,ρ(s))u(s),tNa,

    where by convention (Nau)(a)=0. We define (0au)(t):=u(t) for all tNa+1.

    Definition 2.7 (See [7]). Let u:Na+1R and ν>0. The νth-order nabla sum of u based at a is given by

    (νau)(t):=ts=a+1Hν1(t,ρ(s))u(s),tNa,

    where by convention (νau)(a)=0.

    Definition 2.8 (See [7]). Let u:Na+1R, ν>0 and choose NN1 such that N1<νN. The νth-order nabla difference of u is given by

    (νau)(t):=(N((Nν)au))(t),tNa+N.

    The following properties of gamma function, generalized rising function, and fractional nabla Taylor monomial will be used in Section 3.

    Proposition 1 (See [7]). Assume the following generalized rising functions and fractional nabla Taylor monomials are well defined.

    1. Γ(t)>0 for t>0, and Γ(t)<0 for 1<t<0.

    2. t¯ν(t+ν)¯μ=t¯ν+μ.

    3. (ν+t)¯μ=μ(ν+t)¯μ1.

    4. (νt)¯μ=μ(νρ(t))¯μ1.

    5. Hμ(t,a)=Hμ1(t,a).

    6. Hμ(t,a)Hμ1(t,a)=Hμ(t,a+1).

    7. ts=a+1Hμ(s,a)=Hμ+1(t,a).

    8. ts=a+1Hμ(t,ρ(s))=Hμ+1(t,a).

    Proposition 2 (See [7]). Let νR+ and μR such that μ, μ+ν and μν are nonnegative integers. Then, for all tNa,

    (i) νa(ta)¯μ=Γ(μ+1)Γ(μ+ν+1)(ta)¯μ+ν.

    (ii) νa(ta)¯μ=Γ(μ+1)Γ(μν+1)(ta)¯μν.

    (iii) νaHμ(t,a)=Hμ+ν(t,a).

    (iv) νaHμ(t,a)=Hμν(t,a).

    Proposition 3 (See [8]). Let μ>1 and sNa. Then, the following hold:

    (a) If tNρ(s), then Hμ(t,ρ(s))0, and if tNs, then Hμ(t,ρ(s))>0.

    (b) If tNρ(s) and μ>0, then Hμ(t,ρ(s)) is a decreasing function of s.

    (c) If tNs and 1<μ<0, then Hμ(t,ρ(s)) is an increasing function of s.

    (d) If tNρ(s) and μ0, then Hμ(t,ρ(s)) is a nondecreasing function of t.

    (e) If tNs and μ>0, then Hμ(t,ρ(s)) is an increasing function of t.

    (f) If tNs+1 and 1<μ<0, then Hμ(t,ρ(s)) is a decreasing function of t.

    Proposition 4 (See [8]). If 0<νμ, then Hν(t,a)Hμ(t,a), for each fixed tNa.

    Proposition 5 (See [8]). Let f, g be nonnegative real-valued functions on a set S. Moreover, assume f and g attain their maximum in S. Then, for each fixed tS,

    |f(t)g(t)|max{f(t),g(t)}max{maxtSf(t),maxtSg(t)}.

    Proposition 6. Let μ>1, sNa+1, and tNs. Denote by

    hμ(t,s)=Hμ(t,ρ(s))Hμ(t,a).

    Then, the following hold:

    (I) 0<hμ(t,s).

    (II) If μ>0, then hμ(t,s)1, and if 1<μ<0, then hμ(t,s)1. In particular, h0(t,s)=1.

    (III) If μ>0, then hμ(t,s) is a nondecreasing function of t.

    (IV) If 1<μ<0, then hμ(t,s) is a nonincreasing function of t.

    Proof. (Ⅰ) First, consider

    hμ(t,s)=(tρ(s))¯μ(ta)¯μ=Γ(ts+μ+1)Γ(ta)Γ(ts+1)Γ(ta+μ). (2.1)

    Since Γ(ta), Γ(ta+μ), Γ(ts+1), Γ(ts+μ+1)>0, it follows from (2.1) that hμ(t,s)>0.

    (Ⅱ) The proof of (Ⅱ) follows from the monotonicity of Hμ(t,ρ(s)) with respect to s.

    (Ⅲ) Next, consider

    hμ(t,s)=[(tρ(s))¯μ(ta)¯μ]=(ts+1)¯μ(ta)¯μ(ts)¯μ(ta1)¯μ=Γ(ts+μ+1)Γ(ta)Γ(ts+1)Γ(ta+μ)Γ(ts+μ)Γ(ta1)Γ(ts)Γ(ta+μ1)=Γ(ts+μ)Γ(ta1)Γ(ts)Γ(ta+μ1)[(ts+μ)(ta1)(ts)(ta+μ1)1]=μ(sa1)[Γ(ts+μ)Γ(ta1)Γ(ts+1)Γ(ta+μ)]. (2.2)

    Since Γ(ta1), Γ(ta+μ), Γ(ts+μ), Γ(ts+1)>0, and (sa1)0, it follows from (2.2) that hμ(t,s)0, implying that (Ⅲ) holds.

    (Ⅳ) Clearly, from (2.2), we have

    hμ(t,s)=μ(sa1)[Γ(tsμ)Γ(ta1)Γ(ts+1)Γ(taμ)]. (2.3)

    Since Γ(ta1), Γ(taμ), Γ(tsμ), Γ(ts+1)>0, (sa1)0, it follows from (2.3) that hμ(t,s)0, implying that (IV) holds.

    In this section, we obtain a few properties of G(t,s) which we use in the later part of the article.

    Lemma 1. Assume α, β, γ, δ0 and βα such that (1.2) holds. Then,

    1. ξ>0 for all tNba.

    2. u(t,s)0 for all (t,s)Nba×Nba+1 such that ts1.

    3. v(t,s)0 for all (t,s)Nba×Nba+1 such that ts.

    Proof. (1) From Proposition 3, we have Hν1(b,a), Hν2(b,a)>0 implying that

    ξ=(βα)γ+αγHν1(b,a)+αδHν2(b,a)>0.

    (2) From Proposition 3, we have Hν1(b,ρ(s)), Hν2(b,ρ(s))>0 for all sNba+1, and Hν1(t,a)0 for all tNba. Also, from (1), we have ξ>0 for all tNba. Thus, we obtain

    u(t,s)=1ξ[αγHν1(t,a)Hν1(b,ρ(s))+αδHν1(t,a)Hν2(b,ρ(s))+(βα)γHν1(b,ρ(s))+(βα)δHν2(b,ρ(s))]0,

    for all (t,s)Nba×Nba+1 such that ts1.

    (3) Consider

    v(t,s)=u(t,s)Hν1(t,ρ(s))=1ξ[αγHν1(t,a)Hν1(b,ρ(s))+αδHν1(t,a)Hν2(b,ρ(s))+(βα)γHν1(b,ρ(s))+(βα)δHν2(b,ρ(s))ξHν1(t,ρ(s))]              (3.1)=1ξ[(βα)δHν2(b,ρ(s))+(βα)γ(Hν1(b,ρ(s))Hν1(t,ρ(s)))+αδ(Hν1(t,a)Hν2(b,ρ(s))Hν1(t,ρ(s))Hν2(b,a))+αγ(Hν1(t,a)Hν1(b,ρ(s))Hν1(b,a)Hν1(t,ρ(s)))]                            (3.2)=1ξ[E1+E2+E3+E4],

    where

    E1=(βα)δHν2(b,ρ(s)),E2=(βα)γ(Hν1(b,ρ(s))Hν1(t,ρ(s))),E3=αδ(Hν1(t,a)Hν2(b,ρ(s))Hν1(t,ρ(s))Hν2(b,a)),E4=αγ(Hν1(t,a)Hν1(b,ρ(s))Hν1(b,a)Hν1(t,ρ(s))).

    We already know that ξ>0 for all tNba. Now, we show that

    Ei0,i=1,2,3,4.

    From Proposition 3, we have Hν2(b,ρ(s))>0 for all sNba+1. So, we obtain

    E10.

    Again, from Proposition 3, we have Hν1(t,ρ(s))Hν1(b,ρ(s)) for all (t,s)Nba×Nba+1 such that ts, implying that

    E20.

    From Proposition 3, we have Hν1(t,ρ(s))Hν1(t,a), Hν2(b,a)Hν2(b,ρ(s)) for all (t,s)Nba×Nba+1 such that ts, implying that

    E30.

    Now, consider

    Hν1(t,a)Hν1(b,ρ(s))Hν1(b,a)Hν1(t,ρ(s))=Hν1(b,a)Hν1(t,ρ(s))[Hν1(b,ρ(s))Hν1(b,a)Hν1(t,a)Hν1(t,ρ(s))1]=Hν1(b,a)Hν1(t,ρ(s))[hν1(b,s)hν1(t,s)1].

    From Proposition 3, we have Hν1(b,a), Hν1(t,ρ(s))>0, and hν1(b,s)hν1(t,s) for all (t,s)Nba×Nba+1 such that ts, implying that

    E40.

    Therefore, we obtain v(t,s)0 for all (t,s)Nba×Nba+1 such that ts. The proof is complete.

    Theorem 3.1. Assume α, β, γ, δ0 and βα such that (1.2) holds. Then, G(t,s)0 for all (t,s)Nba×Nba+1.

    Proof. The proof follows from the preceding lemma.

    Lemma 2. Assume α, β, γ, δ0 and βα such that (1.2) holds. Then,

    1. u(t,s) is an increasing function of t for all (t,s)Nba×Nba+1 such that ts1.

    2. v(t,s) is a decreasing function of t for all (t,s)Nba×Nba+1 such that ts.

    Proof. (1) Consider

    tu(t,s)=1ξ[αγHν2(t,a)Hν1(b,ρ(s))+αδHν2(t,a)Hν2(b,ρ(s))].

    From Proposition 3, we have Hν1(b,ρ(s)), Hν2(b,ρ(s))>0 for all sNba+1, and Hν2(t,a)>0 for all tNba+1. Also, from (1), we have ξ>0 for all tNba+1. Thus, we obtain tu(t,s)>0, implying that (1) holds.

    (2) From (3.2), we obtain

    tv(t,s)=1ξ[(βα)γHν2(t,ρ(s))+αδ(Hν2(t,a)Hν2(b,ρ(s))Hν2(t,ρ(s))Hν2(b,a))+αγ(Hν2(t,a)Hν1(b,ρ(s))Hν1(b,a)Hν2(t,ρ(s)))]=1ξ[E5+E6+E7],

    where

    E5=(βα)γHν2(t,ρ(s)),E6=αδ(Hν2(t,a)Hν2(b,ρ(s))Hν2(t,ρ(s))Hν2(b,a)),E7=αγ(Hν2(t,a)Hν1(b,ρ(s))Hν1(b,a)Hν2(t,ρ(s))).

    Clearly, ξ>0 for all tNba+1. Now, we show that

    Ei0,i=5,6,7.

    From Proposition 3, we have Hν2(t,ρ(s))>0 for all (t,s)Nba×Nba+1 such that ts, implying that

    E50.

    From Proposition 3, we have Hν2(t,ρ(s))Hν2(t,a), Hν1(b,a)Hν1(b,ρ(s)) for all (t,s)Nba×Nba+1 such that ts, implying that

    E70.

    Now, consider

    Hν2(t,a)Hν2(b,ρ(s))Hν2(t,ρ(s))Hν2(b,a)=Hν2(t,ρ(s))Hν2(b,a)[Hν2(b,ρ(s))Hν2(b,a)Hν2(t,a)Hν2(t,ρ(s))1]=Hν2(t,ρ(s))Hν2(b,a)[hν2(b,s)hν2(t,s)1].

    From Proposition 3, we have Hν2(b,a), Hν2(t,ρ(s))>0, and hν2(t,s)hν2(b,s) for all (t,s)Nba×Nba+1 such that ts, implying that

    E60.

    Therefore, (2) holds. The proof is complete.

    Theorem 3.2. Assume α, β, γ, δ0 and βα such that (1.2) holds. The following inequality holds for the Green's function G(t,s):

    max(t,s)Nba×Nba+1G(t,s)<Ω, (3.3)

    where

    Ω=1ξ[αγHν1(b,a)Hν1(b,a)+αδHν1(b,a)+(βα)γHν1(b,a)+(βα)δ]. (3.4)

    Proof. From Lemma 2, we have

    max(t,s)Nba×Nba+1G(t,s)=maxsNba+1{u(ρ(s),s),v(s,s)}.

    Consider

    u(ρ(s),s)=1ξ[αγHν1(ρ(s),a)Hν1(b,ρ(s))+αδHν1(ρ(s),a)Hν2(b,ρ(s))+(βα)γHν1(b,ρ(s))+(βα)δHν2(b,ρ(s))],sNba+1.

    Denote by

    f(s)=1ξ[αγHν1(s,a)Hν1(b,ρ(s))+αδHν1(s,a)Hν2(b,ρ(s))+(βα)γHν1(b,ρ(s))+(βα)δHν2(b,ρ(s))],sNba+1.

    Then, by Lemma 1 and Proposition 3, we have

    0u(ρ(s),s)<f(s),sNba+1. (3.5)

    Now, consider

    v(s,s)=1ξ[αγHν1(s,a)Hν1(b,ρ(s))+αδHν1(s,a)Hν2(b,ρ(s))+(βα)γHν1(b,ρ(s))+(βα)δHν2(b,ρ(s))]1=f(s)1,sNba+1. (3.6)

    It follows from Lemma 1 that

    0v(s,s)<f(s),sNba+1. (3.7)

    Since

    maxsNba+1Hν1(s,a)=Hν1(b,a),maxsNba+1Hν1(b,ρ(s))=Hν1(b,a),maxsNba+1Hν2(b,ρ(s))=1,

    we have

    f(s)<Ω,sNba+1. (3.8)

    Thus, by Proposition 3, (3.5), (3.7) and (3.8), we obtain

    max(t,s)Nba×Nba+1G(t,s)=maxsNba+1{u(ρ(s),s),v(s,s)}{maxsNba+1u(ρ(s),s),maxsNba+1v(s,s)}<maxsNba+1f(s)<Ω.

    The proof is complete.

    Theorem 3.3. Assume α, β, γ, δ0 and βα such that (1.2) holds. The following inequality holds for the Green's function G(t,s):

    bs=a+1G(t,s)<Λ, (3.9)

    for all (t,s)Nba×Nba+1, where

    Λ=1ξ[αγHν1(b,a)Hν(b,a)+αδHν1(b,a)Hν1(b,a)+(βα)γHν(b,a)+(βα)δHν1(b,a)]. (3.10)

    Proof. Consider

    bs=a+1G(t,s)=ts=a+1v(t,s)+bs=t+1u(t,s)=bs=a+1u(t,s)ts=a+1Hν1(t,ρ(s))=1ξ[αγHν1(t,a)bs=a+1Hν1(b,ρ(s))+αδHν1(t,a)bs=a+1Hν2(b,ρ(s))+(βα)γbs=a+1Hν1(b,ρ(s))+(βα)δbs=a+1Hν2(b,ρ(s))]ts=a+1Hν1(t,ρ(s))=1ξ[αγHν1(t,a)Hν(b,a)+αδHν1(t,a)Hν1(b,a)+(βα)γHν(b,a)+(βα)δHν1(b,a)]Hν(t,a)=1ξ[αγ(Hν1(t,a)Hν(b,a)Hν1(b,a)Hν(t,a))+αδ(Hν1(t,a)Hν1(b,a)Hν(t,a)Hν2(b,a))+(βα)γ(Hν(b,a)Hν(t,a))+(βα)δHν1(b,a)].

    Since Hν(t,a)0 for all tNba and

    maxtNbaHν(t,a)=Hν(b,a),maxtNbaHν1(t,a)=Hν1(b,a),

    we obtain (3.9). The proof is complete.

    Theorem 3.4 (See [5]). Let h:Nba+1R. If (1.1) has only the trivial solution, then the nonhomogeneous boundary value problem

    {(ν1a(u))(t)=h(t),tNba+2,αu(a+1)β(u)(a+1)=0,γu(b)+δ(u)(b)=0, (3.11)

    has a unique solution given by

    u(t)=bs=a+1G(t,s)h(s),tNba. (3.12)

    Now, we are able to establish a Lyapunov-type inequality for the nabla fractional boundary value problem (1.6).

    Theorem 3.5. Assume α, β, γ, δ0 and βα such that (1.2) holds. If the nabla fractional boundary value problem (1.6) has a nontrivial solution, then

    bs=a+1|q(s)|>1Ω. (3.13)

    Proof. Let B be the Banach space of functions endowed with norm

    u:=maxtNba|u(t)|.

    It follows from the above Theorem that a solution to (1.6) satisfies the equation

    u(t)=bs=a+1G(t,s)q(s)u(s),tNba.

    Hence

    u=maxtNba|u(t)|=maxtNba|bs=a+1G(t,s)q(s)u(s)|maxtNba[bs=a+1G(t,s)|q(s)||u(s)|]umaxtNba[bs=a+1G(t,s)|q(s)|]<Ωubs=a+1|q(s)|,(using Theorem 3.2)

    or, equivalently,

    bs=a+1|q(s)|>1Ω.

    The proof is complete.

    Here, we estimate a lower bound for the eigenvalues of the nabla fractional eigenvalue problem corresponding to the nabla fractional boundary value problem (1.6).

    Theorem 4.1. Assume that 1<ν<2 and u is a nontrivial solution of the nabla fractional eigenvalue problem

    {(ν1a(u))(t)+λu(t)=0,tNba+2,αu(a+1)β(u)(a+1)=0,γu(b)+δ(u)(b)=0, (4.1)

    where u(t)0 for each tNb1a+1. Then,

    |λ|>1(ba)Ω. (4.2)

    We thank referees for helpful comments and suggestions on our article.

    The author declares no conflicts of interest in this paper.



    [1] T. Abdeljawad, F. M. Atici, On the definitions of nabla fractional operators, Abstr. Appl. Anal., 2012 (2012), 406757.
    [2] K. Ahrendt, L. Castle, M. Holm, et al. Laplace transforms for the nabla-difference operator and a fractional variation of parameters formula, Commun. Appl. Anal., 16 (2012), 317-347.
    [3] F. M. Atici, P. W. Eloe, Discrete fractional calculus with the nabla operator, Electron. J. Qual. Theory Differ. Eq., 2009 (2009), 1-12.
    [4] M. Bohner, A. C. Peterson, Dynamic Equations on Time Scales: An Introduction with Applications, Boston: Birkhäuser Boston, Inc., 2001.
    [5] A. Brackins, Boundary value problems of nabla fractional difference equations, Thesis (Ph.D.)-The University of Nebraska-Lincoln, 2014.
    [6] Y. Gholami, K. Ghanbari, Coupled systems of fractional -difference boundary value problems, Differ. Eq. Appl., 8 (2016), 459-470.
    [7] C. Goodrich, A. C. Peterson, Discrete Fractional Calculus, Cham: Springer, 2015.
    [8] A. Ikram, Lyapunov inequalities for nabla Caputo boundary value problems, J. Differ. Eq. Appl., 25 (2019), 757-775. doi: 10.1080/10236198.2018.1560433
    [9] J. M. Jonnalagadda, An ordering on Green's function and a Lyapunov-type inequality for a family of nabla fractional boundary value problems, Fract. Differ. Calc., 9 (2019), 109-124.
    [10] J. M. Jonnalagadda, Analysis of a system of nonlinear fractional nabla difference equations, Int. J. Dyn. Syst. Differ. Eq., 5 (2015), 149-174.
    [11] J. M. Jonnalagadda, Lyapunov-type inequalities for discrete Riemann-Liouville fractional boundary value problems, Int. J. Differ. Eq., 13 (2018), 85-103.
    [12] J. M. Jonnalagadda, On two-point Riemann-Liouville type nabla fractional boundary value problems, Adv. Dyn. Syst. Appl., 13 (2018), 141-166.
    [13] W. G. Kelley, A. C. Peterson, Theory and Applications of Fractional Differential Equations, 2 Eds., San Diego: Harcourt/Academic Press, 2001.
    [14] A. A. Kilbas, H. M. Srivastava, J. J. Trujillo, Difference Equations: An Introduction with Applications, Amsterdam: Elsevier Science B.V., 2006.
    [15] I. Podlubny, Fractional Differential Equations: An Introduction to Fractional Derivatives, Fractional Differential Equations, to Methods of Their Solution and Some of Their Applications, San Diego: Academic Press, Inc., 1999.
  • This article has been cited by:

    1. Nandhihalli Srinivas Gopal, Jagan Mohan Jonnalagadda, Existence and Uniqueness of Solutions to a Nabla Fractional Difference Equation with Dual Nonlocal Boundary Conditions, 2022, 2, 2673-9321, 151, 10.3390/foundations2010009
    2. Alberto Cabada, Nikolay D. Dimitrov, Jagan Mohan Jonnalagadda, Non-Trivial Solutions of Non-Autonomous Nabla Fractional Difference Boundary Value Problems, 2021, 13, 2073-8994, 1101, 10.3390/sym13061101
    3. Jagan Mohan Jonnalagadda, A Comparison Result for the Nabla Fractional Difference Operator, 2023, 3, 2673-9321, 181, 10.3390/foundations3020016
    4. Nikolay D. Dimitrov, Jagan Mohan Jonnalagadda, Existence, Uniqueness, and Stability of Solutions for Nabla Fractional Difference Equations, 2024, 8, 2504-3110, 591, 10.3390/fractalfract8100591
    5. Sangeeta Dhawan, Jagan Mohan Jonnalagadda, Discrete relaxation equations of arbitrary order with periodic boundary conditions, 2024, 12, 2195-268X, 115, 10.1007/s40435-023-01225-2
    6. Sangeeta Dhawan, Jagan Mohan Jonnalagadda, Nontrivial solutions for arbitrary order discrete relaxation equations with periodic boundary conditions, 2024, 32, 0971-3611, 2113, 10.1007/s41478-023-00631-1
    7. Jagan Mohan Jonnalagadda, Anita Tomar, POSITIVE SOLUTIONS OF DISCRETE FRACTIONAL STURM–LIOUVILLE PROBLEMS, 2025, 1072-3374, 10.1007/s10958-025-07720-5
  • Reader Comments
  • © 2020 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Metrics

Article views(4341) PDF downloads(471) Cited by(7)

Other Articles By Authors

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog