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
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Let a, b∈R with b−a∈N1. Consider the homogeneous nabla fractional boundary value problem with general boundary conditions:
{−(∇ν−1a(∇u))(t)=0,t∈Nba+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=(β−α)γ+αγHν−1(b,a)+αδHν−2(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),t≤s−1,v(t,s),t≥s, | (1.3) |
where
u(t,s)=1ξ[αγHν−1(t,a)Hν−1(b,ρ(s))+αδHν−1(t,a)Hν−2(b,ρ(s))+(β−α)γHν−1(b,ρ(s))+(β−α)δHν−2(b,ρ(s))], | (1.4) |
and
v(t,s)=u(t,s)−Hν−1(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
{(∇ν−1a(∇u))(t)+q(t)u(t)=0,t∈Nba+2,αu(a+1)−β(∇u)(a+1)=0,γu(b)+δ(∇u)(b)=0, | (1.6) |
where q:Nba+1→R.
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, b∈R such that b−a∈N1.
Definition 2.1(See [4]). The backward jump operator ρ:Na→Na is defined by
ρ(t):={a,t=a,t−1,t∈Na+1. |
Definition 2.2 (See [14,15]). The Euler gamma function is defined by
Γ(z):=∫∞0tz−1e−tdt,ℜ(z)>0. |
Using its well-known reduction formula, the Euler gamma function can be extended to the half-plane ℜ(z)≤0 except for z∈{…,−2,−1,0}.
Definition 2.3 (See [7]). For t∈R∖{…,−2,−1,0} and r∈R 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 r∈R such that (t+r)∈R∖{…,−2,−1,0}, then we use the convention that t¯r:=0.
Definition 2.4 (See [7]). Let μ∈R∖{…,−2,−1}. Define the μth-order nabla fractional Taylor monomial by
Hμ(t,a):=(t−a)¯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 t∈Na.
Definition 2.5 (See [4]). Let u:Na→R and N∈N1. The first order backward (nabla) difference of u is defined by
(∇u)(t):=u(t)−u(t−1),t∈Na+1, |
and the Nth-order nabla difference of u is defined recursively by
(∇Nu)(t):=(∇(∇N−1u))(t),t∈Na+N. |
Definition 2.6 (See [7]). Let u:Na+1→R and N∈N1. The Nth-order nabla sum of u based at a is given by
(∇−Nau)(t):=t∑s=a+1HN−1(t,ρ(s))u(s),t∈Na, |
where by convention (∇−Nau)(a)=0. We define (∇−0au)(t):=u(t) for all t∈Na+1.
Definition 2.7 (See [7]). Let u:Na+1→R and ν>0. The νth-order nabla sum of u based at a is given by
(∇−νau)(t):=t∑s=a+1Hν−1(t,ρ(s))u(s),t∈Na, |
where by convention (∇−νau)(a)=0.
Definition 2.8 (See [7]). Let u:Na+1→R, ν>0 and choose N∈N1 such that N−1<ν≤N. The νth-order nabla difference of u is given by
(∇νau)(t):=(∇N(∇−(N−ν)au))(t),t∈Na+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)¯μ−1.
4. ∇(ν−t)¯μ=−μ(ν−ρ(t))¯μ−1.
5. ∇Hμ(t,a)=Hμ−1(t,a).
6. Hμ(t,a)−Hμ−1(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 ν∈R+ and μ∈R such that μ, μ+ν and μ−ν are nonnegative integers. Then, for all t∈Na,
(i) ∇−νa(t−a)¯μ=Γ(μ+1)Γ(μ+ν+1)(t−a)¯μ+ν.
(ii) ∇νa(t−a)¯μ=Γ(μ+1)Γ(μ−ν+1)(t−a)¯μ−ν.
(iii) ∇−νaHμ(t,a)=Hμ+ν(t,a).
(iv) ∇νaHμ(t,a)=Hμ−ν(t,a).
Proposition 3 (See [8]). Let μ>−1 and s∈Na. Then, the following hold:
(a) If t∈Nρ(s), then Hμ(t,ρ(s))≥0, and if t∈Ns, then Hμ(t,ρ(s))>0.
(b) If t∈Nρ(s) and μ>0, then Hμ(t,ρ(s)) is a decreasing function of s.
(c) If t∈Ns and −1<μ<0, then Hμ(t,ρ(s)) is an increasing function of s.
(d) If t∈Nρ(s) and μ≥0, then Hμ(t,ρ(s)) is a nondecreasing function of t.
(e) If t∈Ns and μ>0, then Hμ(t,ρ(s)) is an increasing function of t.
(f) If t∈Ns+1 and −1<μ<0, then Hμ(t,ρ(s)) is a decreasing function of t.
Proposition 4 (See [8]). If 0<ν≤μ, then Hν(t,a)≤Hμ(t,a), for each fixed t∈Na.
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 t∈S,
|f(t)−g(t)|≤max{f(t),g(t)}≤max{maxt∈Sf(t),maxt∈Sg(t)}. |
Proposition 6. Let μ>−1, s∈Na+1, and t∈Ns. 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)=(t−ρ(s))¯μ(t−a)¯μ=Γ(t−s+μ+1)Γ(t−a)Γ(t−s+1)Γ(t−a+μ). | (2.1) |
Since Γ(t−a), Γ(t−a+μ), Γ(t−s+1), Γ(t−s+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)=∇[(t−ρ(s))¯μ(t−a)¯μ]=(t−s+1)¯μ(t−a)¯μ−(t−s)¯μ(t−a−1)¯μ=Γ(t−s+μ+1)Γ(t−a)Γ(t−s+1)Γ(t−a+μ)−Γ(t−s+μ)Γ(t−a−1)Γ(t−s)Γ(t−a+μ−1)=Γ(t−s+μ)Γ(t−a−1)Γ(t−s)Γ(t−a+μ−1)[(t−s+μ)(t−a−1)(t−s)(t−a+μ−1)−1]=μ(s−a−1)[Γ(t−s+μ)Γ(t−a−1)Γ(t−s+1)Γ(t−a+μ)]. | (2.2) |
Since Γ(t−a−1), Γ(t−a+μ), Γ(t−s+μ), Γ(t−s+1)>0, and (s−a−1)≥0, it follows from (2.2) that ∇hμ(t,s)≥0, implying that (Ⅲ) holds.
(Ⅳ) Clearly, from (2.2), we have
∇h−μ(t,s)=−μ(s−a−1)[Γ(t−s−μ)Γ(t−a−1)Γ(t−s+1)Γ(t−a−μ)]. | (2.3) |
Since Γ(t−a−1), Γ(t−a−μ), Γ(t−s−μ), Γ(t−s+1)>0, (s−a−1)≥0, it follows from (2.3) that ∇h−μ(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, δ≥0 and β≥α such that (1.2) holds. Then,
1. ξ>0 for all t∈Nba.
2. u(t,s)≥0 for all (t,s)∈Nba×Nba+1 such that t≤s−1.
3. v(t,s)≥0 for all (t,s)∈Nba×Nba+1 such that t≥s.
Proof. (1) From Proposition 3, we have Hν−1(b,a), Hν−2(b,a)>0 implying that
ξ=(β−α)γ+αγHν−1(b,a)+αδHν−2(b,a)>0. |
(2) From Proposition 3, we have Hν−1(b,ρ(s)), Hν−2(b,ρ(s))>0 for all s∈Nba+1, and Hν−1(t,a)≥0 for all t∈Nba. Also, from (1), we have ξ>0 for all t∈Nba. Thus, we obtain
u(t,s)=1ξ[αγHν−1(t,a)Hν−1(b,ρ(s))+αδHν−1(t,a)Hν−2(b,ρ(s))+(β−α)γHν−1(b,ρ(s))+(β−α)δHν−2(b,ρ(s))]≥0, |
for all (t,s)∈Nba×Nba+1 such that t≤s−1.
(3) Consider
v(t,s)=u(t,s)−Hν−1(t,ρ(s))=1ξ[αγHν−1(t,a)Hν−1(b,ρ(s))+αδHν−1(t,a)Hν−2(b,ρ(s))+(β−α)γHν−1(b,ρ(s))+(β−α)δHν−2(b,ρ(s))−ξHν−1(t,ρ(s))] (3.1)=1ξ[(β−α)δHν−2(b,ρ(s))+(β−α)γ(Hν−1(b,ρ(s))−Hν−1(t,ρ(s)))+αδ(Hν−1(t,a)Hν−2(b,ρ(s))−Hν−1(t,ρ(s))Hν−2(b,a))+αγ(Hν−1(t,a)Hν−1(b,ρ(s))−Hν−1(b,a)Hν−1(t,ρ(s)))] (3.2)=1ξ[E1+E2+E3+E4], |
where
E1=(β−α)δHν−2(b,ρ(s)),E2=(β−α)γ(Hν−1(b,ρ(s))−Hν−1(t,ρ(s))),E3=αδ(Hν−1(t,a)Hν−2(b,ρ(s))−Hν−1(t,ρ(s))Hν−2(b,a)),E4=αγ(Hν−1(t,a)Hν−1(b,ρ(s))−Hν−1(b,a)Hν−1(t,ρ(s))). |
We already know that ξ>0 for all t∈Nba. Now, we show that
Ei≥0,i=1,2,3,4. |
From Proposition 3, we have Hν−2(b,ρ(s))>0 for all s∈Nba+1. So, we obtain
E1≥0. |
Again, from Proposition 3, we have Hν−1(t,ρ(s))≤Hν−1(b,ρ(s)) for all (t,s)∈Nba×Nba+1 such that t≥s, implying that
E2≥0. |
From Proposition 3, we have Hν−1(t,ρ(s))≤Hν−1(t,a), Hν−2(b,a)≤Hν−2(b,ρ(s)) for all (t,s)∈Nba×Nba+1 such that t≥s, implying that
E3≥0. |
Now, consider
Hν−1(t,a)Hν−1(b,ρ(s))−Hν−1(b,a)Hν−1(t,ρ(s))=Hν−1(b,a)Hν−1(t,ρ(s))[Hν−1(b,ρ(s))Hν−1(b,a)⋅Hν−1(t,a)Hν−1(t,ρ(s))−1]=Hν−1(b,a)Hν−1(t,ρ(s))[hν−1(b,s)hν−1(t,s)−1]. |
From Proposition 3, we have Hν−1(b,a), Hν−1(t,ρ(s))>0, and hν−1(b,s)≥hν−1(t,s) for all (t,s)∈Nba×Nba+1 such that t≥s, implying that
E4≥0. |
Therefore, we obtain v(t,s)≥0 for all (t,s)∈Nba×Nba+1 such that t≥s. The proof is complete.
Theorem 3.1. Assume α, β, γ, δ≥0 and β≥α 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, δ≥0 and β≥α 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 t≤s−1.
2. v(t,s) is a decreasing function of t for all (t,s)∈Nba×Nba+1 such that t≥s.
Proof. (1) Consider
∇tu(t,s)=1ξ[αγHν−2(t,a)Hν−1(b,ρ(s))+αδHν−2(t,a)Hν−2(b,ρ(s))]. |
From Proposition 3, we have Hν−1(b,ρ(s)), Hν−2(b,ρ(s))>0 for all s∈Nba+1, and Hν−2(t,a)>0 for all t∈Nba+1. Also, from (1), we have ξ>0 for all t∈Nba+1. Thus, we obtain ∇tu(t,s)>0, implying that (1) holds.
(2) From (3.2), we obtain
∇tv(t,s)=1ξ[−(β−α)γHν−2(t,ρ(s))+αδ(Hν−2(t,a)Hν−2(b,ρ(s))−Hν−2(t,ρ(s))Hν−2(b,a))+αγ(Hν−2(t,a)Hν−1(b,ρ(s))−Hν−1(b,a)Hν−2(t,ρ(s)))]=1ξ[E5+E6+E7], |
where
E5=−(β−α)γHν−2(t,ρ(s)),E6=αδ(Hν−2(t,a)Hν−2(b,ρ(s))−Hν−2(t,ρ(s))Hν−2(b,a)),E7=αγ(Hν−2(t,a)Hν−1(b,ρ(s))−Hν−1(b,a)Hν−2(t,ρ(s))). |
Clearly, ξ>0 for all t∈Nba+1. Now, we show that
Ei≤0,i=5,6,7. |
From Proposition 3, we have Hν−2(t,ρ(s))>0 for all (t,s)∈Nba×Nba+1 such that t≥s, implying that
E5≤0. |
From Proposition 3, we have Hν−2(t,ρ(s))≥Hν−2(t,a), Hν−1(b,a)≥Hν−1(b,ρ(s)) for all (t,s)∈Nba×Nba+1 such that t≥s, implying that
E7≤0. |
Now, consider
Hν−2(t,a)Hν−2(b,ρ(s))−Hν−2(t,ρ(s))Hν−2(b,a)=Hν−2(t,ρ(s))Hν−2(b,a)[Hν−2(b,ρ(s))Hν−2(b,a)⋅Hν−2(t,a)Hν−2(t,ρ(s))−1]=Hν−2(t,ρ(s))Hν−2(b,a)[hν−2(b,s)hν−2(t,s)−1]. |
From Proposition 3, we have Hν−2(b,a), Hν−2(t,ρ(s))>0, and hν−2(t,s)≥hν−2(b,s) for all (t,s)∈Nba×Nba+1 such that t≥s, implying that
E6≤0. |
Therefore, (2) holds. The proof is complete.
Theorem 3.2. Assume α, β, γ, δ≥0 and β≥α 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[αγHν−1(b,a)Hν−1(b,a)+αδHν−1(b,a)+(β−α)γHν−1(b,a)+(β−α)δ]. | (3.4) |
Proof. From Lemma 2, we have
max(t,s)∈Nba×Nba+1G(t,s)=maxs∈Nba+1{u(ρ(s),s),v(s,s)}. |
Consider
u(ρ(s),s)=1ξ[αγHν−1(ρ(s),a)Hν−1(b,ρ(s))+αδHν−1(ρ(s),a)Hν−2(b,ρ(s))+(β−α)γHν−1(b,ρ(s))+(β−α)δHν−2(b,ρ(s))],s∈Nba+1. |
Denote by
f(s)=1ξ[αγHν−1(s,a)Hν−1(b,ρ(s))+αδHν−1(s,a)Hν−2(b,ρ(s))+(β−α)γHν−1(b,ρ(s))+(β−α)δHν−2(b,ρ(s))],s∈Nba+1. |
Then, by Lemma 1 and Proposition 3, we have
0≤u(ρ(s),s)<f(s),s∈Nba+1. | (3.5) |
Now, consider
v(s,s)=1ξ[αγHν−1(s,a)Hν−1(b,ρ(s))+αδHν−1(s,a)Hν−2(b,ρ(s))+(β−α)γHν−1(b,ρ(s))+(β−α)δHν−2(b,ρ(s))]−1=f(s)−1,s∈Nba+1. | (3.6) |
It follows from Lemma 1 that
0≤v(s,s)<f(s),s∈Nba+1. | (3.7) |
Since
maxs∈Nba+1Hν−1(s,a)=Hν−1(b,a),maxs∈Nba+1Hν−1(b,ρ(s))=Hν−1(b,a),maxs∈Nba+1Hν−2(b,ρ(s))=1, |
we have
f(s)<Ω,s∈Nba+1. | (3.8) |
Thus, by Proposition 3, (3.5), (3.7) and (3.8), we obtain
max(t,s)∈Nba×Nba+1G(t,s)=maxs∈Nba+1{u(ρ(s),s),v(s,s)}≤{maxs∈Nba+1u(ρ(s),s),maxs∈Nba+1v(s,s)}<maxs∈Nba+1f(s)<Ω. |
The proof is complete.
Theorem 3.3. Assume α, β, γ, δ≥0 and β≥α such that (1.2) holds. The following inequality holds for the Green's function G(t,s):
b∑s=a+1G(t,s)<Λ, | (3.9) |
for all (t,s)∈Nba×Nba+1, where
Λ=1ξ[αγHν−1(b,a)Hν(b,a)+αδHν−1(b,a)Hν−1(b,a)+(β−α)γHν(b,a)+(β−α)δHν−1(b,a)]. | (3.10) |
Proof. Consider
b∑s=a+1G(t,s)=t∑s=a+1v(t,s)+b∑s=t+1u(t,s)=b∑s=a+1u(t,s)−t∑s=a+1Hν−1(t,ρ(s))=1ξ[αγHν−1(t,a)b∑s=a+1Hν−1(b,ρ(s))+αδHν−1(t,a)b∑s=a+1Hν−2(b,ρ(s))+(β−α)γb∑s=a+1Hν−1(b,ρ(s))+(β−α)δb∑s=a+1Hν−2(b,ρ(s))]−t∑s=a+1Hν−1(t,ρ(s))=1ξ[αγHν−1(t,a)Hν(b,a)+αδHν−1(t,a)Hν−1(b,a)+(β−α)γHν(b,a)+(β−α)δHν−1(b,a)]−Hν(t,a)=1ξ[αγ(Hν−1(t,a)Hν(b,a)−Hν−1(b,a)Hν(t,a))+αδ(Hν−1(t,a)Hν−1(b,a)−Hν(t,a)Hν−2(b,a))+(β−α)γ(Hν(b,a)−Hν(t,a))+(β−α)δHν−1(b,a)]. |
Since Hν(t,a)≥0 for all t∈Nba and
maxt∈NbaHν(t,a)=Hν(b,a),maxt∈NbaHν−1(t,a)=Hν−1(b,a), |
we obtain (3.9). The proof is complete.
Theorem 3.4 (See [5]). Let h:Nba+1→R. If (1.1) has only the trivial solution, then the nonhomogeneous boundary value problem
{−(∇ν−1a(∇u))(t)=h(t),t∈Nba+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)=b∑s=a+1G(t,s)h(s),t∈Nba. | (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, δ≥0 and β≥α such that (1.2) holds. If the nabla fractional boundary value problem (1.6) has a nontrivial solution, then
b∑s=a+1|q(s)|>1Ω. | (3.13) |
Proof. Let B be the Banach space of functions endowed with norm
‖u‖:=maxt∈Nba|u(t)|. |
It follows from the above Theorem that a solution to (1.6) satisfies the equation
u(t)=b∑s=a+1G(t,s)q(s)u(s),t∈Nba. |
Hence
‖u‖=maxt∈Nba|u(t)|=maxt∈Nba|b∑s=a+1G(t,s)q(s)u(s)|≤maxt∈Nba[b∑s=a+1G(t,s)|q(s)||u(s)|]≤‖u‖maxt∈Nba[b∑s=a+1G(t,s)|q(s)|]<Ω‖u‖b∑s=a+1|q(s)|,(using Theorem 3.2) |
or, equivalently,
b∑s=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
{(∇ν−1a(∇u))(t)+λu(t)=0,t∈Nba+2,αu(a+1)−β(∇u)(a+1)=0,γu(b)+δ(∇u)(b)=0, | (4.1) |
where u(t)≠0 for each t∈Nb−1a+1. Then,
|λ|>1(b−a)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. |
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