The main object of this article is to present type 2 degenerate poly-Bernoulli polynomials of the second kind and numbers by arising from modified degenerate polyexponential function and investigate some properties of them. Thereafter, we treat the type 2 degenerate unipoly-Bernoulli polynomials of the second kind via modified degenerate polyexponential function and derive several properties of these polynomials. Furthermore, some new identities and explicit expressions for degenerate unipoly polynomials related to special numbers and polynomials are obtained. In addition, certain related beautiful zeros and graphical representations are displayed with the help of Mathematica.
Citation: Waseem A. Khan, Abdulghani Muhyi, Rifaqat Ali, Khaled Ahmad Hassan Alzobydi, Manoj Singh, Praveen Agarwal. A new family of degenerate poly-Bernoulli polynomials of the second kind with its certain related properties[J]. AIMS Mathematics, 2021, 6(11): 12680-12697. doi: 10.3934/math.2021731
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The main object of this article is to present type 2 degenerate poly-Bernoulli polynomials of the second kind and numbers by arising from modified degenerate polyexponential function and investigate some properties of them. Thereafter, we treat the type 2 degenerate unipoly-Bernoulli polynomials of the second kind via modified degenerate polyexponential function and derive several properties of these polynomials. Furthermore, some new identities and explicit expressions for degenerate unipoly polynomials related to special numbers and polynomials are obtained. In addition, certain related beautiful zeros and graphical representations are displayed with the help of Mathematica.
In this paper, we discuss certain discrete fractional boundary value problems in the form
{L+1∇αℓ(ℓ∇α0(v(ℓ)))+ℓ∇α0(L+1∇αℓ(v(ℓ)))+φp(v(ℓ))=λf(ℓ,v(ℓ)),ℓ∈[1,L]N0,v(0)=v(L+1)=0, | (Pfλ) |
where 1<p<∞, α∈(0,1), λ>0, L+1∇αℓ and ℓ∇α0 are the right and left discrete nabla fractional difference operators, f:[1,L]N0×R→R is continuous, and φp stands for the operator that is defined in the usual way by φp(s)=|s|p−2s.
In this paper, we want to utilize a version of Ricceri's variational principle as given in [1]. We build the energy functional and we take some assumptions on the nonlinear term to get a functional that satisfies the conditions in the key theorem. In fact, by first requiring a simple algebraic inequality condition on the nonlinear term for small values of the parameter and requiring an additional asymptotical behavior of the potential at zero if f(ℓ,0)=0, the existence of one nontrivial solution is achieved. Moreover, we deduce the existence of solutions for small positive values of the parameter such that the corresponding solutions have smaller and smaller energies as the parameter goes to zero. Then, under an appropriate oscillating behavior of the nonlinear term, we discuss the existence of an unbounded sequence of solutions. We give exact collections for the parameter for each results, which cannot be found in other works in the literature related to these types of discrete problems.
As is well known, fractional differential equations (FDEs) are valuable tools when modeling many phenomena in various areas of science and engineering. We refer to [2,3,4,5,6,7,8] and the references therein for a range of applications of FDEs in control, electrochemistry, viscoelasticity, electromagneticity, porous media, and other fields. Classical tools that have been employed in the study of nonlinear FDEs (see [9,10,11] and their references) include fixed point theory, monotone iterative methods, coincidence theory, and the upper and lower solutions method.
Thanks to their wide range of applications in many fields such as science, economics, ecology, neural networks, cybernetics, etc., nonlinear difference equations have been studied extensively for the last 50 years. In addition, boundary value problems involving difference equations have received a lot of attention, see, e.g., [12,13,14,15] and references therein. Difference equations subjected to many different kinds of boundary conditions have also been extensively studied by using various techniques. A popular technique has been to use variational methods [16,17,18]. In the last few years, many researchers have investigated nonlinear problems of this type through various approaches. Moreover, such boundary value problems for ordinary differential equations, difference equations, and dynamic equations on time scales have been studied extensively, but there are only a few papers dealing with fractional boundary value problems, besides [19,20,21], especially for discrete fractional boundary value problems involving Caputo fractional difference operators. For example, Lv [22], by using the fixed point theorem of Schaefer, under certain nonlinear growth assumptions, obtained the existence of solutions to a discrete fractional boundary value problem. Furthermore, in [23,24], some existence and multiplicity results for (p,q)-Laplacian problems were considered. For example, in [23], by using suitable variational arguments and Ljusternik–Schnirelmann category theory, the multiplicity and concentration of positive solutions for (p,q)-Laplacian problems were obtained.
In view of the facts presented above, in the current study, we discuss the existence of at least one solution to the boundary value problem (Pfλ), as well as the existence of an infinite number of solutions of (Pfλ). Our primary tool is [1, Theorem 2.1], which is a more precise variant of the famous variational principle of Ricceri [25]. In Theorem 9 below, we show that, subject to certain assumptions, the boundary value problem (Pfλ) possesses at least one nontrivial solution. We also offer Example 17, where all hypotheses of our Theorem 9 are satisfied. We present a series of remarks concerning our results. Moreover, under suitable assumptions of the oscillatory behavior at infinity of the nonlinearity, we investigate the existence of an infinite number of solutions for the boundary value problem (Pfλ). We prove the existence of a definite interval about λ, in which the boundary value problem (Pfλ) admits a sequence of solutions, which is unbounded in the space V, to be introduced later (Theorem 18). We present an example that illustrates Theorem 20 (see Example 21). Moreover, some corollaries of Theorem 18 are offered. Under different assumptions, we ensure the existence of a sequence of pairwise different solutions that strongly converges to zero (see Theorem 26).
The paper is set up as follows. In Section 2, we remind the reader of some basic definitions and our main tool. In Sections 3 and 4, we state and prove our main results.
The key argument in our results is the next version of the variational principle by Ricceri [25, Theorem 2.1], as presented in [1].
Theorem 1. Suppose that X is a reflexive real Banach space. Assume that Φ,Ψ:X→R are Gâteaux-differentiable functionals such that Ψ is sequentially weakly upper semicontinuous, and Φ is strongly continuous, sequentially weakly lower semicontinuous, and coercive. For every r>infXΦ, let us put
φ(r):=infv∈Φ−1(−∞,r)supv∈Φ−1(−∞,r)Ψ(v)−Ψ(v)r−Φ(v) |
and
θ:=lim infr→∞φ(r),δ:=lim infr→(infXΦ)+φ(r). |
One then has the following.
(a) For every r>infXΦ and each λ∈(0,1φ(r)), the restriction of the functional Iλ=Φ−λΨ to Φ−1(]−∞,r[) possesses a global minimum, and this global minimum is a critical point, i.e., a local minimum, of Iλ in X.
(b) If 0<θ<∞, then, for all λ∈(0,1θ), either
(b1) Iλ possesses a global minimum, or
(b2) for all n∈N, Iλ has a critical point un, and
limn→∞Φ(vn)=∞. |
(c) If 0<δ<∞, then, for all λ∈(0,1δ), either
(c1) Φ possesses a global minimum, which is a local minimum of Iλ, or
(c2) a sequence of pairwise different critical points of Iλ exists, and this sequence converges weakly to a global minimum of Φ.
We refer to [9,26,27,28], in which Theorem 1 was applied successfully in order to prove the existence of at least one nontrivial solution for certain boundary value problems, and [29,30,31,32,33], in which Theorem 1 has been successfully employed in order to prove the existence of an infinite number of solutions for certain boundary value problems.
In this section, we present several foundational definitions, notations, and results that are used in the remainder of this paper.
Definition 2 (see [34]). (ⅰ) For m∈N, the m rising factorial of t is defined as
t¯m=m−1∏k=0(t+k),t¯0=1. |
(ⅱ) For t∈R∖{…,−2,−1,0} and α∈R, the α rising function is increasing on N0 and
t¯α=Γ(t+α)Γ(t),0¯α=0. |
Definition 3 (see [34]). For f defined on Na−1∩b+1N, a<b, α∈(0,1), the left Caputo discrete fractional nabla difference operator is given by
(Cℓ∇αa−1f)(ℓ)=1Γ(1−α)ℓ∑s=a∇sf(s)(ℓ−ρ(s))¯−α(ℓ∈Na), | (1) |
the right Caputo discrete fractional nabla difference operator is given by
(Cb+1∇αℓf)(ℓ)=1Γ(1−α)b∑s=ℓ(−Δsf)(s)(s−ρ(ℓ))¯−α(ℓ∈bN), | (2) |
the left Riemann discrete fractional nabla difference operator is given by
(Rℓ∇αa−1f)(ℓ)=1Γ(1−α)∇ℓℓ∑s=af(s)(ℓ−ρ(s))¯−α=1Γ(−α)ℓ∑s=af(s)(ℓ−ρ(s))¯−α−1(ℓ∈Na), |
the right Riemann discrete fractional nabla difference operator is given by
(Rb+1∇αℓf)(ℓ)=1Γ(1−α)(−Δℓ)b∑s=ℓ(f(s))(s−ρ(ℓ))¯−α=1Γ(−α)b∑s=ℓ(f(s))(s−ρ(ℓ))¯−α−1(ℓ∈bN), |
where ρ(ℓ)=ℓ−1 is the backward jump operator.
Example 4. Let us give an example concerning Definition 3. Consider f:Na−1∩b+1N→R defined by f(ℓ)≡1. For this f, from (1) and (2), we have
Cℓ∇αa−11=Cb+1∇αℓ1=0,ℓ∈Na∩bN. | (3) |
The relations among the right and left Riemann and Caputo nabla fractional difference operators are
(Cℓ∇αa−1f)(ℓ)=(Rℓ∇αa−1f)(ℓ)−(ℓ−a+1)¯−αΓ(1−α)f(a−1), | (4) |
(Cb+1∇αℓf)(ℓ)=(Rb+1∇αℓf)(ℓ)−(b+1−ℓ)¯−αΓ(1−α)f(b+1). | (5) |
Thus, by (3)–(5), we have
Rb+1∇αℓ1=(b+1−ℓ)¯−αΓ(1−α),Rℓ∇αa−11=(ℓ−a+1)¯−αΓ(1−α),ℓ∈Na∩bN. |
With respect to the domains of the various fractional-type difference operators, we observe the following:
(ⅰ) The nabla left fractional operator ℓ∇αa−1 maps functions defined on a−1N to functions defined on aN.
(ⅱ) The nabla right fractional operator b+1∇αℓ maps functions defined on b+1N to functions defined on bN.
One can show that for α→0, we have ℓ∇αa−1f(ℓ)→f(ℓ) and for α→1, we have ℓ∇αa−1f(ℓ)→∇f(ℓ). We note that the Caputo and Riemann nabla fractional difference operators for 0<α<1 coincide when f vanishes at the end points, i.e., f(a−1)=0=f(b+1) (see (4), (5), and [2]). So, for convenience, for the remainder of this paper, we use the symbol ℓ∇αa−1 instead of Cℓ∇αa−1 or Rℓ∇αa−1 and b+1∇αℓ instead of Cb+1∇αℓ or Rb+1∇αℓ.
Now we present the discrete fractional summation by parts formula.
Theorem 5. (see [35, Theorem 4.4]). For f,g:Na∩bN→R, a<b, and α∈(0,1), the formulas
b∑ℓ=af(ℓ)(ℓ∇αa−1g)(ℓ)=b∑ℓ=ag(ℓ)(b+1∇αℓf)(ℓ) |
and
b∑ℓ=af(ℓ)(b+1∇αℓg)(ℓ)=b∑ℓ=ag(ℓ)(ℓ∇αa−1f(ℓ) |
hold.
In order to give the variational formulation of the boundary value problem (Pfλ), let us introduce the finite L-dimensional Banach space
V={v:[0,L+1]N0→R:v(0)=v(L+1)=0}, |
which is equipped with the norm
‖v‖=(L∑ℓ=1|v(ℓ)|2)12. |
According to the definition of the norm, the following lemma is obvious.
Lemma 6. For all α∈(0,1) and for all v∈V, we have
‖v‖∞=maxℓ∈[1,L]N0|v(ℓ)|≤‖v‖. | (6) |
For every v∈V, we define the functionals Φ and Ψ as
Φ(v)=12L∑ℓ=1|(ℓ∇α0v)(ℓ)|2+|(L+1∇αℓv)(ℓ)|2+1pL∑ℓ=1|v(ℓ)|p | (7) |
and
Ψ(v)=L∑ℓ=1F(ℓ,v(ℓ)), | (8) |
and we put
Iλ(v)=Φ(v)−λΨ(v). |
Definition 7. A (weak) solution of (Pfλ) is defined to be any function v∈V such that
L∑ℓ=1{(ℓ∇α0v)(ℓ)(ℓ∇α0˜v)(ℓ)+(L+1∇αℓv)(ℓ)(L+1∇αℓ˜v)(ℓ)}+L∑ℓ=1|v(ℓ)|p−2v(ℓ)˜v(ℓ)−λL∑ℓ=1f(ℓ,v(ℓ))˜v(ℓ)=0 | (9) |
for every ˜v∈V.
Note that since V is a finite-dimensional space, every weak solution is a usual solution of the boundary value problem (Pfλ).
Lemma 8. Let v∈V. Then v is a critical point of Iλ in V if and only if v solves (Pfλ).
Proof. First assume that v∈V is a critical point of Iλ. Then, for any ˜v∈V, (9) holds. Bearing in mind that ˜v∈V is arbitrary, we get
L+1∇αℓ(ℓ∇α0(v(ℓ)))+ℓ∇α0(L+1∇αℓ(v(ℓ)))+|v(ℓ)|p−1v(ℓ)−λf(ℓ,v(ℓ))=0 |
for all ℓ∈[1,L]N. Therefore, v solves (Pfλ). Since v was chosen arbitrarily, we deduce that all critical points of the functional Iλ in V solve (Pfλ). Conversely, if v solves (Pfλ), then, by reversing the above steps, the proof is completed.
Put
F(ℓ,ξ)=∫ξ0f(ℓ,x)dxfor all(ℓ,ξ)∈[1,L]N0×R. |
The following is our main result concerning the existence of a solution of (Pfλ).
Theorem 9. Assume that f(ℓ,0)=0 and
supθ>0θpL∑ℓ=1max|x|≤θF(ℓ,x)>p(L+1)p(p−2)4 | (10) |
and there are discrete intervals D=[1,L1]N0⊆[1,L]N0 and B=[1,L2]N0⊂[1,L1]N0 with L1,L2≥2, such that
lim supξ→0+essinfℓ∈BF(ℓ,ξ)|ξ|p=∞ |
and
lim infξ→0+essinfℓ∈DF(ℓ,ξ)|ξ|p>−∞. |
Then, for every
λ∈Λ:=(0,(L+1)p(p−2)4psupθ>0θpL∑ℓ=1max|x|≤θF(ℓ,x)), |
the boundary value problem (Pfλ) admits at least one nontrivial solution vλ∈V.
Proof. Our goal is to apply Theorem 1 to (Pfλ). We utilize the functionals Φ and Ψ as introduced in (7) and (8), respectively. Let us demonstrate that Φ and Ψ meet the required assumptions of Theorem 1. As V is embedded compactly in (C0([1,L]N0),R), we know that Ψ is Gâteaux-differentiable, and its Gâteaux derivative Ψ′(v)∈V∗ at v∈V is given by
Ψ′(v)(v)=L∑ℓ=1f(ℓ,v(ℓ))˜v(ℓ) |
for each ˜v∈V, and Ψ is sequentially weakly upper semicontinuous. Furthermore, Φ is also Gâteaux-differentiable, and its Gâteaux derivative at v∈V is the functional Φ′(v)∈V∗ given by
Φ′(v)(˜v)=L∑ℓ=1{(ℓ∇α0v(ℓ))(ℓ∇α0˜v(ℓ))+(L+1∇αℓv(ℓ))(L+1∇αℓ˜v(ℓ))}+L∑ℓ=1|v(ℓ)|p−2v(ℓ)˜v(ℓ) |
for every ˜v∈V. Furthermore, by the definition of Φ, we observe that it is sequentially weakly lower semicontinuous and strongly continuous. Now, in light of (7), for each v∈V, we obtain
1p(L+1)p(p−2)4‖v‖p≤Φ(v)≤2L(L+1)‖v‖2+1p(L+1)2−p2‖v‖p. | (11) |
By employing the left inequality of (11), we get
lim‖v‖→∞Φ(v)=∞. |
In other words, Φ is coercive. Using (10), there is ˉθ>0 with
ˉθpL∑ℓ=1max|x|≤ˉθF(ℓ,x)>p(L+1)p(p−2)4. |
Put
r:=(L+1)p(p−2)4pˉθp. |
From the way Φ is defined and considering (6), (7), and (11), since r>0, we have
Φ−1(−∞,r)={v∈V:Φ(v)<r}⊆{v∈V:‖v‖p≤pr(L+1)p(p−2)4}⊆{v∈V:‖v‖p∞≤pr(L+1)p(p−2)4}={v∈V:‖v‖p∞≤ˉθp}, |
which implies
supΦ(v)<rΨ(v)=supΦ(v)<rL∑ℓ=1F(ℓ,v(ℓ))≤L∑ℓ=1max|x|≤ˉθF(ℓ,x). |
By considering these computations, as 0∈Φ−1(−∞,r) and Φ(0)=Ψ(0)=0, we get
φ(r)=inf˜v∈Φ−1(−∞,r)(supv∈Φ−1(−∞,r)Ψ(v))−Ψ(˜v)r−Φ(˜v)≤supv∈Φ−1(−∞,r)Ψ(v)r≤p(L+1)p(p−2)4L∑ℓ=1max|x|≤ˉθF(ℓ,x)ˉθp. |
Hence, we put
λ∗=(L+1)p(p−2)4psupθ>0θpL∑ℓ=1max|x|≤θF(ℓ,x). |
At this point, thanks to Theorem 1, for each λ∈(0,λ∗)⊆(0,1φ(r)), Theorem 1 shows that Iλ possesses at least one critical point (local minimum) vλ∈Φ−1(−∞,r). We show that vλ cannot be the trivial function. Let us prove
lim sup‖v‖→0+Ψ(v)Φ(v)=∞. | (12) |
Due to our required conditions at zero, we can find a sequence {ξk}⊂R+ that converges to zero, and ζ>0 and κ with
limk→∞essinfℓ∈BF(ℓ,ξk)|ξk|p=∞ |
and
essinfℓ∈DF(ℓ,ξ)≥κ|ξ|p,ξ∈[0,ζ]. |
Let [1,L3]N0⊂[1,L2]N0, where L3≥2, and let ˜v∈V be such that
(ⅰ) ˜v(ℓ)∈[0,1] for all ℓ∈[1,L]N0,
(ⅱ) ˜v(ℓ)=1∈R for all ℓ∈[1,L3]N0,
(ⅲ) ˜v(ℓ)=0 for all ℓ∈[L1+1,L]N0.
Therefore, we fix an arbitrary Y>0 and η>0 with
Y<ηL3+κL∑ℓ=L3+1|˜v(ℓ)|p1p(L+1)2−p2‖˜v‖p. |
Thus, there is n0∈N with εn<ζ and
essinfℓ∈BF(ℓ,ξn)≥η|ξn|p |
for all n>n0. Next, for all n>n0, using 0≤ξn˜v(ℓ)<ζ for all large enough n, by (11), we get
Ψ(ξn˜v)Φ(ξn˜v)=L3∑ℓ=1F(ℓ,ξn)+L∑ℓ=L3+1F(ℓ,ξn˜v(ℓ))Φ(ξn˜v)>ηL3+κL∑ℓ=L3+1|˜v(ℓ)|p1p(L+1)2−p2‖˜v‖p>Y. |
Since Y can be as large as we desire, we conclude that
limn→∞Ψ(ξn˜v)Φ(ξn˜v)=∞, |
which implies (12). Thus, we have a sequence {υn}⊂V that converges strongly to zero, υn∈Φ−1(−∞,r), and
Iλ(υn)=Φ(υn)−λΨ(υn)<0. |
Since vλ is a global minimum of the restriction of Iλ to Φ−1(−∞,r), we get
Iλ(vλ)<0, | (13) |
and thus vλ is not trivial. The proof is complete.
Some comments are given next.
Remark 10. In Theorem 9, we sought for the critical points of Iλ, a functional that is intrinsically connected to the boundary value problem (Pfλ). We observe that, in a general case, Iλ may not be bounded in V. To see this, consider, for instance, the situation when f(ξ)=1+ξγ−1 for each ξ∈R, where γ>p. Let v∈V∖{0} and μ∈R. We then find
Iλ(μv)=Φ(μv)−λL∑ℓ=1F(μv(ℓ))≤2μ2L(L+1)‖v‖2+μpp(L+1)2−p2‖v‖p+λμL‖v‖−λμγγL‖v‖γ→−∞ |
as μ→∞. Thus, [36, (I2) in Theorem 2.2] is not satisfied. Therefore, we are unable to use direct minimization to find the critical points of Iλ.
Remark 11. Note that Iλ is not coercive. To see this, let s∈(p,∞) and define F by F(ξ)=|ξ|s for each ξ∈R. Let v∈V∖{0} and μ∈R. We then find
Iλ(μv)=Φ(μv)−λL∑ℓ=1F(μv(ℓ))≤2μ2L(L+1)‖v‖2+μpp(L+1)2−p2‖v‖p−λμsL‖v‖s→−∞ |
as μ→−∞.
Remark 12. If, in Theorem 9, f satisfies f(ℓ,x)≥0 for almost every (ℓ,x)∈[1,L]N0×R, then (10) assumes the simpler form
supθ>0θpL∑ℓ=1F(ℓ,θ)>p(L+1)p(p−2)4. | (14) |
Moreover, if the assumption
lim supθ→∞θpL∑ℓ=1F(ℓ,θ)>p(L+1)p(p−2)4 |
is satisfied, then (14) automatically holds.
Remark 13. From (13), we can directly see that
(0,λ∗)∋λ↦Iλ(vλ) | (15) |
is indeed a negative map. Furthermore, we have
limλ→0+‖vλ‖=0. |
Indeed, by considering that Φ is coercive and that for λ∈(0,λ∗), the solution vλ∈Φ−1(−∞,r), we have the existence of L>0 with ‖vλ‖≤L for every λ∈(0,λ∗). Next, it is also easy to see that M>0 exists with
|L∑ℓ=1f(ℓ,vλ(ℓ))vλ(ℓ)|≤M‖vλ‖≤ML | (16) |
for each λ∈(0,λ∗). Since vλ is a critical point of Iλ, I′λ(vλ)(˜v)=0 for any ˜v∈V and each λ∈(0,λ∗). In particular, I′λ(vλ)(vλ)=0, i.e.,
Φ′(vλ)(vλ)=λL∑ℓ=1f(ℓ,vλ(ℓ))vλ(ℓ) | (17) |
for every λ∈(0,λ∗). Then, since
0≤(L+1)p(p−2)4‖v‖p≤Φ′(vλ)(vλ), |
by using (17), it is concluded that
0≤(L+1)p(p−2)4‖v‖p≤Φ′(vλ)(vλ)≤λL∑ℓ=1f(ℓ,vλ(ℓ))vλ(ℓ) |
for all λ∈(0,λ∗). If we now let λ→0+, by (16), then we get limλ→0+‖vλ‖=0. One has
limλ→0+‖vλ‖∞=0. |
Finally, we prove that
λ↦Iλ(vλ) | (18) |
decreases strictly in (0,λ∗). We observe that for all v∈V, we have
Iλ(v)=λ(Φ(v)λ−Ψ(v)). | (19) |
Now, let 0<λ1<λ2<λ∗ and let vλ1, vλ2 be the global minima of the functional Iλi restricted to Φ(−∞,r) for i=1,2. Moreover, let
mλi=(Φ(vλi)λi−Ψ(vλi))=inf˜v∈Φ−1(−∞,r)(Φ(˜v)λi−Ψ(˜v)) |
for i=1,2. Obviously, (15), in connection with (19) and λ>0, yields
mλi<0fori=1,2. |
In addition,
mλ2≤mλ1, | (20) |
because 0<λ1<λ2. Then, by observing (19)–(20) and as 0<λ1<λ2, we get
Iλ2(ˉvλ2)=λ2mλ2≤λ2mλ1<λ1mλ1=Iλ1(ˉvλ1), |
so that (18) decreases strictly for λ∈(0,λ∗). Since λ<λ∗ is arbitrary, we see that (18) indeed decreases strictly in (0,λ∗).
Remark 14. We note that Theorem 9 represents a bifurcation result in the sense that (0,0) belongs to the closure of
{(vλ,λ)∈V×(0,∞):vλ is a nontrivial solution of (Pfλ)} |
in V×R. To observe this, by Remark 13, we get
‖vλ‖→0asλ→0. |
Therefore, there are sequences {vj} in V and {λi} in R+ (here, vj=vλ) with
λi→0+and‖vj‖→0 |
as j→∞. In addition, we want to emphasize that because
(0,λ∗)∋λ↦Iλ(vλ) |
is a strictly decreasing map, for all λ1,λ2∈(0,λ∗) such that λ1≠λ2, the solutions ˉvλ1 and ˉvλ2 ensured by Remark 13 are distinct.
Remark 15. Under the assumption that f≥0, the solution that is ensured by Theorem 9 is nonnegative. To observe this, suppose that v0 is a nontrivial solution of (Pfλ). Assume that
A={ℓ∈[1,L]N0:v0(ℓ)<0}≠∅ |
has positive measure. Put ˉ˜v(ℓ)=min{0,v0(ℓ)} for each ℓ∈[1,L]N0. We obtain ˉ˜v∈V and
L∑ℓ=1{(ℓ∇α0v0(ℓ))(ℓ∇α0ˉ˜v(ℓ))+(L+1∇αℓv0(ℓ))(ℓ∇α0ˉ˜v(ℓ))}+L∑ℓ=1|v0(ℓ)|p−2v0(ℓ)ˉ˜v(ℓ)−λL∑ℓ=1f(ℓ,v0(ℓ))ˉ˜v(ℓ)=0. |
Thus, from our imposed data sign assumptions, we have
0≤(L+1)p(p−2)4‖v‖pA≤∑A{(ℓ∇α0v0(ℓ))2+(L+1∇αℓv0(ℓ))2}+∑A|v0(ℓ)|p=λ∑Af(ℓ,v0(ℓ))v0(ℓ)≤0. |
Hence, v0=0 in A, which is impossible.
The next result concerns a particular case of the previously presented results, in which the function f depends only on the second variable, considering the nonautonomous case of the problem.
Theorem 16. Let f:R→R be nonnegative with f(0)=0. Let F(ξ)=∫ξ0f(x)dx for all x∈R. Assume that
limξ→0+F(ξ)ξp=∞. |
Then, for every
λ∈(0,(L+1)p(p−2)4Lpsupθ>0θpF(θ)), |
the boundary value problem
{L+1∇αℓ(ℓ∇α0(v(ℓ)))+ℓ∇α0(L+1∇αℓ(v(ℓ)))+φp(v(ℓ))=λf(v(ℓ)),ℓ∈[1,L]N0,v(0)=v(L+1)=0, |
possesses at least one nontrivial solution vλ∈V satisfying
limλ→0+‖vλ‖=0, |
and the real function
λ→12L∑ℓ=1{|(ℓ∇α0v)(ℓ)|2+|(L+1∇αℓv)(ℓ)|2}+1pL∑ℓ=1|v(ℓ)|p−λL∑ℓ=1F(v(ℓ)) |
is negative and decreases strictly in (0,(L+1)p(p−2)4Lpsupθ>0θpF(θ)).
Finally, we present the following example to illustrate Theorem 16.
Example 17. Let p=4 and L=2. We consider the problem
{3∇12ℓ(ℓ∇120(v(ℓ)))+ℓ∇120(3∇12ℓ(v(ℓ)))+φ4(v(ℓ))=λf(v(ℓ)),ℓ∈{1,2},v(0)=v(3)=0, | (21) |
where
f(ξ)=34ξ3+2tan(ξ)sec2(ξ)+eξ,ξ∈R. |
By simple computations, we have
F(ξ)=ξ4+sec2(ξ)+eξ−2,ξ∈R. |
We see that all assumptions of Theorem 16 are satisfied, and this implies that the boundary value problem (21), for each λ∈(0,98), admits at least one nontrivial solution vλ∈V such that
limλ→0+‖vλ‖=0, |
and the real function
λ→122∑ℓ=1{|(ℓ∇120v)(ℓ)|2+|(3∇12ℓv)(ℓ)|2}+142∑ℓ=1|v(ℓ)|4−λ2∑ℓ=1F(v(ℓ)) |
is negative and strictly decreasing in (0,98).
Put
B∞=lim supξ→∞L∑ℓ=1F(ℓ,ξ)ξ2(Γ(1−α))2L∑ℓ=1|ℓ¯−α|2+Lξpp. |
Our main result concerning the existence of infinitely many solutions of (Pfλ) is as follows.
Theorem 18. Assume that two sequences {an} and {bn} exist with
limn→∞bn=∞ |
such that
a2n(Γ(1−α))2L∑ℓ=1|ℓ¯−α|2+Lapnp<(L+1)p(p−2)4pbpnfor alln∈N, | (A1) |
A∞=limn→∞L∑ℓ=1max|t|≤bnF(ℓ,t)−L∑ℓ=1F(ℓ,an)(L+1)p(p−2)4pbpn−(a2n(Γ(1−α))2L∑ℓ=1|ℓ¯−α|2+Lapnp)<B∞. | (A2) |
In this case, for all λ∈(1B∞,1A∞), the boundary value problem (Pfλ) possesses an unbounded sequence of solutions.
Proof. Our aim is to employ Theorem 1. We utilize the functionals Φ and Ψ as introduced in (7) and (8), respectively. Therefore, we observe that the regularity assumptions on Φ and Ψ, as required in Theorem 1, are satisfied. Hence v∈V is a solution of (Pfλ) if and only if v is a critical point of the function Iλ. Put
rn=(L+1)p(p−2)4pbpnfor alln∈N. |
We see that rn>0 for all n∈N. From the way Φ is defined and in light of (6), (8), and (11), for each rn>0, we have
Φ−1(−∞,rn)={v∈V:Φ(v)<rn}⊆{v∈V:‖v‖p≤prn(L+1)p(p−2)4}⊆{v∈V:‖v‖p∞≤prn(L+1)p(p−2)4}={v∈V:‖v‖p∞≤bpn}, |
which implies
supΦ(v)<rnΨ(v)=supΦ(v)<rnL∑ℓ=1F(ℓ,v(ℓ))≤L∑ℓ=1max|x|≤bnF(ℓ,x). |
Now, for each n∈N, we define
υ(ℓ)={anifℓ∈[1,L]N0,0ifℓ∈{0,L+1}. |
Clearly, υ∈V. Since υ vanishes at the end points (that is, υ(0)=0=υ(L+1)), its Riemann and Caputo fractional differences coincide. Hence, for any ℓ∈N1∩LN, we have
(L+1∇αℓυ)(ℓ)=(RL+1∇αℓυ)(ℓ)=(CL+1∇αℓυ)(ℓ)=an(L+1−ℓ)¯−αΓ(1−α) |
and
(ℓ∇α0υ)(ℓ)=(Rℓ∇α0υ)(ℓ)=(Cℓ∇α0υ)(ℓ)=an(ℓ)¯−αΓ(1−α). |
Thus,
Φ(υ)=12L∑ℓ=1{|(ℓ∇α0υ)(ℓ)|2+|(L+1∇αℓυ)(ℓ)|2}+1pL∑ℓ=1|υ(ℓ)|p=12L∑ℓ=1{|an(ℓ)¯−αΓ(1−α)|2+|an(L+1−ℓ)¯−αΓ(1−α)|2}+Lapnp=a2n2(Γ(1−α))2L∑ℓ=1|ℓ¯−α|2+|(L+1−ℓ)¯−α|2+Lapnp=a2n(Γ(1−α))2L∑ℓ=1|ℓ¯−α|2+Lapnp. |
We have
Ψ(υ)=L∑ℓ=1F(ℓ,υ(ℓ))=L∑ℓ=1F(ℓ,an). |
In addition, from (A1), we have Φ(υn)<rn. Thus, for all large enough values of n, we obtain
φ(rn)=inf˜v∈Φ−1(−∞,rn)supv∈Φ−1(−∞,rℓ)Ψ(v)−Ψ(˜v)rn−Φ(˜v)≤supv∈Φ−1(−∞,rn)Ψ(v)−L∑ℓ=1F(ℓ,υ(ℓ))rn−Φ(υ)=supv∈Φ−1(−∞,rn)Ψ(v)−L∑ℓ=1F(ℓ,an)(L+1)p(p−2)4pbpn−(a2n(Γ(1−α))2L∑ℓ=1|ℓ¯−α|2+Lapnp)≤L∑ℓ=1max|x|≤bnF(ℓ,x)−L∑ℓ=1F(ℓ,an)(L+1)p(p−2)4pbpn−(a2n(Γ(1−α))2L∑ℓ=1|ℓ¯−α|2+Lapnp). | (22) |
Hence, due to (A2), we get
γ≤limn→∞φ(rn)≤A∞<∞. |
Now, we can verify that Iλ is unbounded from below. First, assume that B∞=∞. Accordingly, fix N such that
N<c2n(Γ(1−α))2L∑ℓ=1|ℓ¯−α|2+Lcpnp |
and let cn>0 for all n∈N such that cn→∞ as n→∞ and
L∑ℓ=1F(ℓ,cn)>Nfor alln∈N. |
For each n∈N, define
yn(ℓ)=cnfor allℓ∈[1,L]N0. |
Thus, yn∈V and
Φ(yn)=c2n(Γ(1−α))2L∑ℓ=1|ℓ¯−α|2+Lcpnp. |
Therefore,
Iλ(yn)=c2n(Γ(1−α))2L∑ℓ=1|ℓ¯−α|2+Lcpnp−λL∑ℓ=1F(ℓ,cn)<c2n(Γ(1−α))2L∑ℓ=1|ℓ¯−α|2+Lcpnp−λN, |
that is, limn→∞Iλ(yn)=−∞. Next, suppose B∞<∞. As λ>1B∞, we can find ε>0 with ε<B∞−1λ. Thus, again letting cn>0 for all n∈N such that cn→∞ as n→∞ and
L∑ℓ=1F(ℓ,cn)>B∞−εfor alln∈N, |
as argued above, and by letting yn∈V as before, we obtain
Iλ(yn)=c2n(Γ(1−α))2L∑ℓ=1|ℓ¯−α|2+Lcpnp−λL∑ℓ=1F(ℓ,cn)<c2n(Γ(1−α))2L∑ℓ=1|ℓ¯−α|2+Lcpnp−λ(B∞−ε). |
Therefore, limn→∞Iλ(yn)=−∞. Hence, in either case, Iλ is not bounded from below. This completes the proof.
Remark 19. If {an} and {bn} are real sequences such that limn→∞bn=∞ and such that (A1) from Theorem 18 is satisfied, then, assuming that A∞=0 and B∞=∞, Theorem 18 ensures that for each λ>0, the boundary value problem (Pfλ) admits an infinite number of solutions.
Theorem 20. Assume that
lim infξ→∞L∑ℓ=1max|x|≤ξF(ℓ,x)(L+1)p(p−2)4pξp<lim supξ→∞L∑ℓ=1F(ℓ,ξ)ξ2(Γ(1−α))2L∑ℓ=1|ℓ¯−α|2+Lξpp. | (\rm A_3 ) |
In this case, for all
\lambda\in\left(\dfrac{\dfrac{\xi^2}{(\Gamma(1-\alpha))^2} \sum\limits_{ \ell = 1}^ L\left|{ \ell^{\overline{-\alpha}}}\right|^2 +\frac{ L\xi^p}{p}}{ \sum\limits^ L_{ \ell = 1}F( \ell,\xi)}, \dfrac{\frac{( L+1)^{\frac{p(p-2)}{4}}}{p}\xi^p} { \sum\limits_{ \ell = 1}^ L\max\limits_{|x|\leq{\xi}}F( \ell,x)}\right), |
the boundary value problem (P^f_\lambda) possesses an unbounded sequence of solutions.
Proof. We pick b_n > 0 for all n\in {\mathbb{N}} with b_n\to\infty as n\to\infty and
\lim\limits_{n\to\infty}\frac{ \sum\limits_{ \ell = 1}^ L \max\limits_{|x|\leq b_n}F( \ell,x)}{\frac{( L+1)^{\frac{p(p-2)}{4}}}{p}b_n^p} = \liminf\limits_{\xi\to\infty}\dfrac{ \sum\limits_{ \ell = 1}^ L \max\limits_{|x|\leq\xi}F( \ell,x)}{\frac{( L+1)^{\frac{p(p-2)}{4}}}{p}\xi^p}. |
Now, as \Phi(0) = \Psi(0) = 0 , we may take a_n = 0 for all n\in {\mathbb{N}} in (22), and then the conclusion follows from Theorem 1.
Now, we present an example that illustrates Theorem 20.
Example 21. Let p = 4 and L = 3 . We consider the boundary value problem
\begin{equation} \begin{cases} {_{4}\nabla^{\frac{1}{2}}_\ell}( {_\ell\nabla^{\frac{1}{2}}_0}( v( \ell))) + {_\ell\nabla^{\frac{1}{2}}_0}( {_{4}\nabla^{\frac{1}{2}}_\ell}( v( \ell)))+\varphi_4( v( \ell)) = \lambda f( v( \ell)),\quad \ell\in\{1,2,3\},\\ v(0) = v(4) = 0, \end{cases} \end{equation} | (23) |
where
f(x) = \begin{cases} 0 &\quad\text{if}\quad x\in(-\infty,0],\\ 4x^3+4x^3\sin(\pi e^x)+\pi x^4e^x\cos(\pi e^x)) &\quad\text{if}\quad x\in(0,\infty). \end{cases} |
Some computation yields
F(x) = \begin{cases} 0 &\quad\text{if}\quad x\in(-\infty,0],\\ x^4(1+\sin(\pi e^x)) &\quad\text{if}\quad x\in(0,\infty). \end{cases} |
Since
\liminf\limits_{\xi\to\infty}\dfrac{ \sum\limits_{ \ell = 1}^3 \max\limits_{|x|\leq\xi}F(x)}{64\xi^4} = 0 |
and
\limsup\limits_{\xi\to\infty}\dfrac{ \sum^3_{ \ell = 1}F(\xi)} {\dfrac{\xi^2}{(\Gamma(1/2))^2} \sum\limits_{ \ell = 1}^3\left|{ \ell^{\overline{-\frac{1}{2}}}}\right|^2 +\frac{3\xi^4}{4}} = 8, |
we clearly see that all assumptions of Theorem 20 are satisfied, and then (23), for every \lambda\in\left(\frac{1}{8}, \infty\right) , has an unbounded sequence of solutions in \left\{ v:[0, 4]_{ {\mathbb{N}}_0}\to {\mathbb{R}}: v(0) = v(4) = 0\right\} .
Here, we point out several simple corollaries of our main results.
Corollary 22. Suppose that there are real sequences \{a_n\} and \{b_n\} with b_n\to\infty as n\to\infty and such that (\rm A_1) from Theorem 18 holds, \mathcal{A}_\infty < 1 , and \mathcal{B}_\infty > 1 . Then, the boundary value problem
\begin{cases} {_{L+1}\nabla^{\alpha}_\ell}( {_\ell\nabla^{\alpha}_0}( v( \ell))) + {_\ell\nabla^{\alpha}_0}( {_{L+1}\nabla^{\alpha}_\ell}( v( \ell)))+\varphi_p( v( \ell)) = f( \ell, v( \ell)),\quad \ell\in[1, L]_{ {\mathbb{N}}_0},\\ v(0) = v( L+1) = 0 \end{cases} | (P^f ) |
possesses an unbounded sequence of solutions.
Corollary 23. Suppose \mathcal{B}_\infty > 1 and
\liminf\limits_{\xi\to\infty}\frac{ \sum\limits_{ \ell = 1}^ L \max\limits_{|x|\leq\xi}F( \ell,x)}{\frac{( L+1)^{\frac{p(p-2)}{4}}}{p}\xi^p} < 1. |
Then the boundary value problem (P^f) possesses an unbounded sequence of solutions.
Corollary 24. Suppose that there are real sequences \{a_n\} and \{b_n\} with b_n\to\infty as n\to\infty and such that (\rm A_1) from Theorem 18 holds, f_1\in\text{C}([1, L]_{ {\mathbb{N}}_0}\times {\mathbb{R}}, {\mathbb{R}}) , and
F_1( \ell,x) = \int_0^xf_1( \ell,\xi){\rm d}\xi \quad\mathit{\text{for all}}\quad ( \ell,x)\in[0, L]_{ {\mathbb{N}}_0}\times {\mathbb{R}}. |
Moreover, assume
\lim\limits_{n\to\infty}\frac{ \sum\limits_{ \ell = 1}^ L \max\limits_{|x|\leq b_n}F_1( \ell,x) - \sum\limits^ L_{ \ell = 1}F_1( \ell,a_n)} {\frac{( L+1)^{\frac{p(p-2)}{4}}}{p}b_n^p -\left({\dfrac{a_n^2}{(\Gamma(1-\alpha))^2} \sum\limits_{ \ell = 1}^ L\left|{ \ell^{\overline{-\alpha}}}\right|^2 +\frac{ L a_n^p}{p}}\right)} < \infty | (\rm A_4 ) |
and
\limsup\limits_{\xi\to\infty}\frac{ \sum\limits^ L_{ \ell = 1}F_1( \ell,\xi)}{\dfrac{\xi^2} {(\Gamma(1-\alpha))^2} \sum\limits_{ \ell = 1}^ L\left|{ \ell^{\overline{-\alpha}}}\right|^2 +\frac{ L\xi^p}{p}} = \infty. | (\rm A_5 ) |
Then, for all f_i\in\text{C}([1, L]_{ {\mathbb{N}}_0}\times {\mathbb{R}}, {\mathbb{R}}) , by writing
F_i( \ell,x) = \int_0^xf_i( \ell,\xi){\rm d}\xi \quad\mathit{\text{for all}}\quad ( \ell,x)\in[1, L]_{ {\mathbb{N}}_0}\times {\mathbb{R}} |
for 2\leq i\leq n , such that
\max\left\{{\sup\limits_{\xi\in {\mathbb{R}}}F_i( \ell,\xi):\; 2\leq i\leq n}\right\}\leq 0 |
and
\min\left\{{\liminf\limits_{\xi\to\infty}\frac{F_i( \ell,\xi)}{\xi^2}:\; 2\leq i\leq n}\right\} > -\infty, |
for all
\lambda\in\left({0,\frac{1}{ \lim\limits_{n\to\infty} \dfrac{ \sum\limits_{ \ell = 1}^ L\max\limits_{|x|\leq b_n}F_1( \ell,x) - \sum\limits^ L_{ \ell = 1}F_1( \ell,a_n)}{\frac{( L+1)^{\frac{p(p-2)}{4}}}{p}b_n^p -\left({\dfrac{a_n^2}{(\Gamma(1-\alpha))^2} \sum\limits_{ \ell = 1}^ L\left|{ \ell^{\overline{-\alpha}}}\right|^2 +\frac{ L a_n^p}{p}}\right)}}}\right), |
the boundary value problem
\begin{equation} \begin{cases} {_{L+1}\nabla^{\alpha}_\ell}( {_\ell\nabla^{\alpha}_0}( v( \ell))) + {_\ell\nabla^{\alpha}_0}( {_{L+1}\nabla^{\alpha}_\ell}( v( \ell)))+\varphi_p( v( \ell)) = \lambda f_i( \ell, v( \ell)),\quad \ell\in[1, L]_{ {\mathbb{N}}_0},\\ v(0) = v( L+1) = 0 \end{cases} \end{equation} | (24) |
has an unbounded sequence of solutions.
Proof. Put F(\ell, \xi) = \sum\limits_{i = 1}^nF_i(\ell, \xi) for (\ell, \xi)\in[1, L]_{ {\mathbb{N}}_0}\times {\mathbb{R}} . (\rm A_4), along with
\min\left\{{\liminf\limits_{\xi\to\infty}\frac{F_i( \ell,\xi)}{\xi^2}:\; 2\leq i\leq n}\right\} > -\infty, |
ensures
\limsup\limits_{\xi\to\infty}\frac{ \sum\limits^ L_{ \ell = 1}F( \ell,\xi)} {\dfrac{\xi^2}{(\Gamma(1-\alpha))^2} \sum\limits_{ \ell = 1}^ L\left|{ \ell^{\overline{-\alpha}}}\right|^2+\frac{ L\xi^p}{p}} = \limsup\limits_{\xi\to\infty}\dfrac{ \sum\limits_{i = 1}^n \sum\limits^ L_{ \ell = 1}F_i( \ell,\xi)}{\dfrac{\xi^2}{(\Gamma(1-\alpha))^2} \sum\limits_{ \ell = 1}^ L\left|{ \ell^{\overline{-\alpha}}}\right|^2 +\frac{ L\xi^p}{p}} = \infty. |
Moreover, Assumption (\rm A_4), together with the condition
\max\left({\sup\limits_{\xi\in {\mathbb{R}}}F_i( \ell,\xi):\; 2\leq i\leq n}\right)\leq 0, |
implies
\begin{array}{l} \lim\limits_{n\to\infty}\frac{ \sum\limits_{ \ell = 1}^ L \max\limits_{|x|\leq b_n}F( \ell,x)- \sum\limits^ L_{ \ell = 1}F( \ell,\sigma_n)} {\frac{( L+1)^{\frac{p(p-2)}{4}}}{p}b_n^p -\left({\dfrac{\sigma_n^2}{(\Gamma(1-\alpha))^2} \sum\limits_{ \ell = 1}^ L\left|{ \ell^{\overline{-\alpha}}}\right|^2 +\frac{ L\sigma_n^p}{p}}\right)}\\ \qquad\qquad\qquad\qquad\qquad\qquad\qquad\qquad \leq\lim\limits_{n\to\infty}\frac{ \sum\limits_{ \ell = 1}^ L \max\limits_{|x|\leq b_n}F_1( \ell,x)- \sum\limits^ L_{ \ell = 1}F_1( \ell,a_n)} {\frac{( L+1)^{\frac{p(p-2)}{4}}}{p}b_n^p -\left({\dfrac{a_n^2}{(\Gamma(1-\alpha))^2} \sum\limits_{ \ell = 1}^ L\left|{ \ell^{\overline{-\alpha}}}\right|^2 +\frac{ L a_n^p}{p}}\right)} < \infty. \end{array} |
Hence, an application of Theorem 18 completes the proof.
Corollary 25. Let f_1\in\text{C}([1, L]_{ {\mathbb{N}}_0}\times {\mathbb{R}}, {\mathbb{R}}) and put
F_1( \ell,x) = \int_0^xf_{1}( \ell,\xi){\rm d}\xi \quad\mathit{\text{for all}}\quad ( \ell,x)\in[1, L]_{ {\mathbb{N}}_0}\times {\mathbb{R}}. |
Assume that
\liminf\limits_{\xi\to\infty}\frac{ \sum\limits_{ \ell = 1}^ L \max\limits_{|x|\leq\sigma(\xi)}F_{1}( \ell,x)} {\frac{( L+1)^{\frac{p(p-2)}{4}}}{p}\xi^p} < \infty |
and
\limsup\limits_{\xi\to\infty}\frac{ \sum\limits^ L_{ \ell = 1}F_1( \ell,\xi)} {\dfrac{\xi^2}{(\Gamma(1-\alpha))^2} \sum\limits_{ \ell = 1}^ L\left|{ \ell^{\overline{-\alpha}}}\right|^2 +\frac{ L\xi^p}{p}} = \infty. |
Then, for all f_i\in\text{C}([1, L]_{ {\mathbb{N}}_0}\times {\mathbb{R}}, {\mathbb{R}}) , by writing
F_i( \ell,x) = \int_0^xf_i( \ell,\xi){\rm d}\xi \quad\mathit{\text{for all}}\quad ( \ell,x)\in[1, L]_{ {\mathbb{N}}_0}\times {\mathbb{R}} |
for 2\leq i\leq n , such that
\max\left\{{\sup\limits_{\xi\in {\mathbb{R}}}F_i( \ell,\xi):\; 2\leq i\leq n}\right\}\leq 0 |
and
\min\left\{{\liminf\limits_{\xi\to\infty}\frac{F_i( \ell,\xi)}{\xi^p}:\; 2\leq i\leq n}\right\} > -\infty, |
for all
\lambda\in\left({0,\dfrac{1}{ \liminf\limits_{\xi\to\infty} \dfrac{ \sum\limits_{ \ell = 1}^ L\max\limits_{|x|\leq\xi}F( \ell,x)} {\frac{( L+1)^{\frac{p(p-2)}{4}}}{p}\xi^p}}}\right), |
the boundary value problem (24) has an unbounded sequence of solutions.
Now put
\mathcal{B}^0 = \limsup\limits_{\xi\to 0} \dfrac{ \sum\limits^ L_{ \ell = 1}F( \ell,\xi)} {\dfrac{\xi^2}{(\Gamma(1-\alpha))^2} \sum\limits_{ \ell = 1}^ L\left|{ \ell^{\overline{-\alpha}}}\right|^2 +\frac{ L\xi^p}{p}}. |
With a proof similar to the proof of Theorem 18, but this time using Theorem 1 (c) instead of Theorem 1 (b), we can establish the next result. The proof is similar to the proof of Theorem 18, but here we have a real sequence \{e_n\} which tends to zero at \infty constructing r , because in Theorem 1 (c) for \delta , it requires r\to(\inf_X\Phi)^+ instead of in Theorem 1 (b) for \theta , it requires r\to\infty .
Theorem 26. Suppose that there are real sequences \{d_n\} and \{e_n\} with \lim_{n\to\infty}e_n = 0 such that
\begin{gather} \frac{d_n^2}{(\Gamma(1-\alpha))^2} \sum\limits_{ \ell = 1}^ L\left|{ \ell^{\overline{-\alpha}}}\right|^2+\frac{ L d_n^p}{p} < \frac{( L+1)^{\frac{p(p-2)}{4}}}{p}e_n^p \quad\mathit{\text{for every}}\quad n\in {\mathbb{N}}, \end{gather} | (\rm A_6 ) |
\begin{gather} \mathcal{A}^0 = \lim\limits_{n\to\infty}\frac{ \sum\limits_{ \ell = 1}^ L \max\limits_{|x|\leq e_n}F( \ell,x)- \sum\limits^ L_{ \ell = 1}F( \ell,d_n)} {\frac{( L+1)^{\frac{p(p-2)}{4}}}{p}e_n^p -\dfrac{d_n^2}{(\Gamma(1-\alpha))^2} \sum\limits_{ \ell = 1}^ L\left|{ \ell^{\overline{-\alpha}}}\right|^2 +\frac{ L d_n^p}{p}} < \mathcal{B}^0. \end{gather} | (\rm A_7 ) |
Then, for each
\lambda\in(\lambda_3,\lambda_4) \quad\mathit{\text{with}}\quad \lambda_3: = \frac{1}{\mathcal{B}^0} \quad\mathit{\text{and}}\quad \lambda_4: = \frac{1}{\mathcal{A}_0}, |
the boundary value problem (P^f_\lambda) possesses a sequence of pairwise different solutions that strongly converges to 0 in {\mathcal{V}} .
Theorem 27. Suppose
\liminf\limits_{\xi\to 0^+}\frac{ \sum\limits_{ \ell = 1}^ L \max\limits_{|x|\leq\xi}F( \ell,x)}{\frac{( L+1)^{\frac{p(p-2)}{4}}}{p}\xi^p} < \limsup\limits_{\xi\to 0}\frac{ \sum\limits^ L_{ \ell = 1}F( \ell,\xi)} {\dfrac{\xi^2}{(\Gamma(1-\alpha))^2} \sum\limits_{ \ell = 1}^ L\left|{ \ell^{\overline{-\alpha}}}\right|^2+\frac{ L\xi^p}{p}}. | (\rm A_8 ) |
Then, for each
\lambda\in\left({\frac{1}{ \limsup\limits_{\xi\to 0} \dfrac{ \sum\limits^ L_{ \ell = 1}F( \ell,\xi)} {\dfrac{\xi^2}{(\Gamma(1-\alpha))^2} \sum\limits_{ \ell = 1}^ L\left|{ \ell^{\overline{-\alpha}}}\right|^2+\frac{ L\xi^p}{p}}}, \frac{1}{ \liminf\limits_{\xi\to 0^+} \dfrac{ \sum\limits_{ \ell = 1}^ L\max\limits_{|x|\leq\xi}F( \ell,x)} {\frac{( L+1)^{\frac{p(p-2)}{4}}}{p}\xi^p}}}\right), |
the boundary value problem (P^f_\lambda) has a sequence of pairwise different solutions that converges strongly to 0 in {\mathcal{V}} .
Remark 28. By employing Theorem 26, we may obtain results that are similar to Remark 19 and Corollaries 22–25.
In this paper, we investigated the existence of one and of infinitely many solutions for a class of discrete fractional boundary value problems. As a matter of fact, by demanding an algebraic condition on the nonlinear term for small values of the parameter and requiring an additional asymptotical behavior of the potential at zero, we obtain the existence of at least one nontrivial solution for the problem. Moreover, under suitable assumptions on the oscillatory behavior at infinity of the nonlinearity, for exact collections of the parameter, we get the existence of a sequence of solutions for the problem. The main results improve and extend recent results from the literature. We also presented some examples that illustrate the applicability of the main results. The main technique of the proofs involves variational methods and critical point theorems for smooth functionals.
There is no conflict of interest.
No AI tools have been used in the preparation of this study.
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