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Research article Special Issues

A new family of degenerate poly-Bernoulli polynomials of the second kind with its certain related properties

  • Received: 19 July 2021 Accepted: 18 August 2021 Published: 06 September 2021
  • MSC : 05A19, 11B73, 11B83

  • 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+1α(α0(v()))+α0(L+1α(v()))+φp(v())=λf(,v()),[1,L]N0,v(0)=v(L+1)=0, (Pfλ)

    where 1<p<, α(0,1), λ>0, L+1α and α0 are the right and left discrete nabla fractional difference operators, f:[1,L]N0×RR is continuous, and φp stands for the operator that is defined in the usual way by φp(s)=|s|p2s.

    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(,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:XR 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):=infvΦ1(,r)supvΦ1(,r)Ψ(v)Ψ(v)rΦ(v)

    and

    θ:=lim infrφ(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=ΦλΨ to Φ1(],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 nN, Iλ has a critical point un, and

    limnΦ(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 mN, the m rising factorial of t is defined as

    t¯m=m1k=0(t+k),t¯0=1.

    (ⅱ) For tR{,2,1,0} and αR, 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 Na1b+1N, a<b, α(0,1), the left Caputo discrete fractional nabla difference operator is given by

    (Cαa1f)()=1Γ(1α)s=asf(s)(ρ(s))¯α(Na), (1)

    the right Caputo discrete fractional nabla difference operator is given by

    (Cb+1αf)()=1Γ(1α)bs=(Δsf)(s)(sρ())¯α(bN), (2)

    the left Riemann discrete fractional nabla difference operator is given by

    (Rαa1f)()=1Γ(1α)s=af(s)(ρ(s))¯α=1Γ(α)s=af(s)(ρ(s))¯α1(Na),

    the right Riemann discrete fractional nabla difference operator is given by

    (Rb+1αf)()=1Γ(1α)(Δ)bs=(f(s))(sρ())¯α=1Γ(α)bs=(f(s))(sρ())¯α1(bN),

    where ρ()=1 is the backward jump operator.

    Example 4. Let us give an example concerning Definition 3. Consider f:Na1b+1NR defined by f()1. For this f, from (1) and (2), we have

    Cαa11=Cb+1α1=0,NabN. (3)

    The relations among the right and left Riemann and Caputo nabla fractional difference operators are

    (Cαa1f)()=(Rαa1f)()(a+1)¯αΓ(1α)f(a1), (4)
    (Cb+1αf)()=(Rb+1αf)()(b+1)¯αΓ(1α)f(b+1). (5)

    Thus, by (3)–(5), we have

    Rb+1α1=(b+1)¯αΓ(1α),Rαa11=(a+1)¯αΓ(1α),NabN.

    With respect to the domains of the various fractional-type difference operators, we observe the following:

    (ⅰ) The nabla left fractional operator αa1 maps functions defined on a1N to functions defined on aN.

    (ⅱ) The nabla right fractional operator b+1α maps functions defined on b+1N to functions defined on bN.

    One can show that for α0, we have αa1f()f() and for α1, we have αa1f()f(). 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(a1)=0=f(b+1) (see (4), (5), and [2]). So, for convenience, for the remainder of this paper, we use the symbol αa1 instead of Cαa1 or Rαa1 and b+1α instead of Cb+1α or Rb+1α.

    Now we present the discrete fractional summation by parts formula.

    Theorem 5. (see [35, Theorem 4.4]). For f,g:NabNR, a<b, and α(0,1), the formulas

    b=af()(αa1g)()=b=ag()(b+1αf)()

    and

    b=af()(b+1αg)()=b=ag()(αa1f()

    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]N0R:v(0)=v(L+1)=0},

    which is equipped with the norm

    v=(L=1|v()|2)12.

    According to the definition of the norm, the following lemma is obvious.

    Lemma 6. For all α(0,1) and for all vV, we have

    v=max[1,L]N0|v()|v. (6)

    For every vV, we define the functionals Φ and Ψ as

    Φ(v)=12L=1|(α0v)()|2+|(L+1αv)()|2+1pL=1|v()|p (7)

    and

    Ψ(v)=L=1F(,v()), (8)

    and we put

    Iλ(v)=Φ(v)λΨ(v).

    Definition 7. A (weak) solution of (Pfλ) is defined to be any function vV such that

    L=1{(α0v)()(α0˜v)()+(L+1αv)()(L+1α˜v)()}+L=1|v()|p2v()˜v()λL=1f(,v())˜v()=0 (9)

    for every ˜vV.

    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 vV. Then v is a critical point of Iλ in V if and only if v solves (Pfλ).

    Proof. First assume that vV is a critical point of Iλ. Then, for any ˜vV, (9) holds. Bearing in mind that ˜vV is arbitrary, we get

    L+1α(α0(v()))+α0(L+1α(v()))+|v()|p1v()λf(,v())=0

    for all [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(,ξ)=ξ0f(,x)dxfor all(,ξ)[1,L]N0×R.

    The following is our main result concerning the existence of a solution of (Pfλ).

    Theorem 9. Assume that f(,0)=0 and

    supθ>0θpL=1max|x|θF(,x)>p(L+1)p(p2)4 (10)

    and there are discrete intervals D=[1,L1]N0[1,L]N0 and B=[1,L2]N0[1,L1]N0 with L1,L22, such that

    lim supξ0+essinfBF(,ξ)|ξ|p=

    and

    lim infξ0+essinfDF(,ξ)|ξ|p>.

    Then, for every

    λΛ:=(0,(L+1)p(p2)4psupθ>0θpL=1max|x|θF(,x)),

    the boundary value problem (Pfλ) admits at least one nontrivial solution vλV.

    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 vV is given by

    Ψ(v)(v)=L=1f(,v())˜v()

    for each ˜vV, and Ψ is sequentially weakly upper semicontinuous. Furthermore, Φ is also Gâteaux-differentiable, and its Gâteaux derivative at vV is the functional Φ(v)V given by

    Φ(v)(˜v)=L=1{(α0v())(α0˜v())+(L+1αv())(L+1α˜v())}+L=1|v()|p2v()˜v()

    for every ˜vV. 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 vV, we obtain

    1p(L+1)p(p2)4vpΦ(v)2L(L+1)v2+1p(L+1)2p2vp. (11)

    By employing the left inequality of (11), we get

    limvΦ(v)=.

    In other words, Φ is coercive. Using (10), there is ˉθ>0 with

    ˉθpL=1max|x|ˉθF(,x)>p(L+1)p(p2)4.

    Put

    r:=(L+1)p(p2)4pˉθp.

    From the way Φ is defined and considering (6), (7), and (11), since r>0, we have

    Φ1(,r)={vV:Φ(v)<r}{vV:vppr(L+1)p(p2)4}{vV:vppr(L+1)p(p2)4}={vV:vpˉθp},

    which implies

    supΦ(v)<rΨ(v)=supΦ(v)<rL=1F(,v())L=1max|x|ˉθF(,x).

    By considering these computations, as 0Φ1(,r) and Φ(0)=Ψ(0)=0, we get

    φ(r)=inf˜vΦ1(,r)(supvΦ1(,r)Ψ(v))Ψ(˜v)rΦ(˜v)supvΦ1(,r)Ψ(v)rp(L+1)p(p2)4L=1max|x|ˉθF(,x)ˉθp.

    Hence, we put

    λ=(L+1)p(p2)4psupθ>0θpL=1max|x|θF(,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) vλΦ1(,r). We show that vλ cannot be the trivial function. Let us prove

    lim supv0+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

    limkessinfBF(,ξk)|ξk|p=

    and

    essinfDF(,ξ)κ|ξ|p,ξ[0,ζ].

    Let [1,L3]N0[1,L2]N0, where L32, and let ˜vV be such that

    (ⅰ) ˜v()[0,1] for all [1,L]N0,

    (ⅱ) ˜v()=1R for all [1,L3]N0,

    (ⅲ) ˜v()=0 for all [L1+1,L]N0.

    Therefore, we fix an arbitrary Y>0 and η>0 with

    Y<ηL3+κL=L3+1|˜v()|p1p(L+1)2p2˜vp.

    Thus, there is n0N with εn<ζ and

    essinfBF(,ξn)η|ξn|p

    for all n>n0. Next, for all n>n0, using 0ξn˜v()<ζ for all large enough n, by (11), we get

    Ψ(ξn˜v)Φ(ξn˜v)=L3=1F(,ξn)+L=L3+1F(,ξn˜v())Φ(ξn˜v)>ηL3+κL=L3+1|˜v()|p1p(L+1)2p2˜vp>Y.

    Since Y can be as large as we desire, we conclude that

    limnΨ(ξn˜v)Φ(ξn˜v)=,

    which implies (12). Thus, we have a sequence {υn}V that converges strongly to zero, υnΦ1(,r), and

    Iλ(υn)=Φ(υn)λΨ(υn)<0.

    Since vλ is a global minimum of the restriction of Iλ to Φ1(,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+ξγ1 for each ξR, where γ>p. Let vV{0} and μR. We then find

    Iλ(μv)=Φ(μv)λL=1F(μv())2μ2L(L+1)v2+μpp(L+1)2p2vp+λμLvλμγγLvγ

    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 ξR. Let vV{0} and μR. We then find

    Iλ(μv)=Φ(μv)λL=1F(μv())2μ2L(L+1)v2+μpp(L+1)2p2vpλμsLvs

    as μ.

    Remark 12. If, in Theorem 9, f satisfies f(,x)0 for almost every (,x)[1,L]N0×R, then (10) assumes the simpler form

    supθ>0θpL=1F(,θ)>p(L+1)p(p2)4. (14)

    Moreover, if the assumption

    lim supθθpL=1F(,θ)>p(L+1)p(p2)4

    is satisfied, then (14) automatically holds.

    Remark 13. From (13), we can directly see that

    (0,λ)λIλ(vλ) (15)

    is indeed a negative map. Furthermore, we have

    limλ0+vλ=0.

    Indeed, by considering that Φ is coercive and that for λ(0,λ), the solution vλΦ1(,r), we have the existence of L>0 with vλL for every λ(0,λ). Next, it is also easy to see that M>0 exists with

    |L=1f(,vλ())vλ()|MvλML (16)

    for each λ(0,λ). Since vλ is a critical point of Iλ, Iλ(vλ)(˜v)=0 for any ˜vV and each λ(0,λ). In particular, Iλ(vλ)(vλ)=0, i.e.,

    Φ(vλ)(vλ)=λL=1f(,vλ())vλ() (17)

    for every λ(0,λ). Then, since

    0(L+1)p(p2)4vpΦ(vλ)(vλ),

    by using (17), it is concluded that

    0(L+1)p(p2)4vpΦ(vλ)(vλ)λL=1f(,vλ())vλ()

    for all λ(0,λ). If we now let λ0+, by (16), then we get limλ0+vλ=0. One has

    limλ0+vλ=0.

    Finally, we prove that

    λIλ(vλ) (18)

    decreases strictly in (0,λ). We observe that for all vV, we have

    Iλ(v)=λ(Φ(v)λΨ(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)λiΨ(vλi))=inf˜vΦ1(,r)(Φ(˜v)λiΨ(˜v))

    for i=1,2. Obviously, (15), in connection with (19) and λ>0, yields

    mλi<0fori=1,2.

    In addition,

    mλ2mλ1, (20)

    because 0<λ1<λ2. Then, by observing (19)–(20) and as 0<λ1<λ2, we get

    Iλ2(ˉvλ2)=λ2mλ2λ2mλ1<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

    vλ0asλ0.

    Therefore, there are sequences {vj} in V and {λi} in R+ (here, vj=vλ) with

    λi0+andvj0

    as j. In addition, we want to emphasize that because

    (0,λ)λIλ(vλ)

    is a strictly decreasing map, for all λ1,λ2(0,λ) such that λ1λ2, the solutions ˉvλ1 and ˉvλ2 ensured by Remark 13 are distinct.

    Remark 15. Under the assumption that f0, 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={[1,L]N0:v0()<0}

    has positive measure. Put ˉ˜v()=min{0,v0()} for each [1,L]N0. We obtain ˉ˜vV and

    L=1{(α0v0())(α0ˉ˜v())+(L+1αv0())(α0ˉ˜v())}+L=1|v0()|p2v0()ˉ˜v()λL=1f(,v0())ˉ˜v()=0.

    Thus, from our imposed data sign assumptions, we have

    0(L+1)p(p2)4vpAA{(α0v0())2+(L+1αv0())2}+A|v0()|p=λAf(,v0())v0()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:RR be nonnegative with f(0)=0. Let F(ξ)=ξ0f(x)dx for all xR. Assume that

    limξ0+F(ξ)ξp=.

    Then, for every

    λ(0,(L+1)p(p2)4Lpsupθ>0θpF(θ)),

    the boundary value problem

    {L+1α(α0(v()))+α0(L+1α(v()))+φp(v())=λf(v()),[1,L]N0,v(0)=v(L+1)=0,

    possesses at least one nontrivial solution vλV satisfying

    limλ0+vλ=0,

    and the real function

    λ12L=1{|(α0v)()|2+|(L+1αv)()|2}+1pL=1|v()|pλL=1F(v())

    is negative and decreases strictly in (0,(L+1)p(p2)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

    {312(120(v()))+120(312(v()))+φ4(v())=λf(v()),{1,2},v(0)=v(3)=0, (21)

    where

    f(ξ)=34ξ3+2tan(ξ)sec2(ξ)+eξ,ξR.

    By simple computations, we have

    F(ξ)=ξ4+sec2(ξ)+eξ2,ξR.

    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 vλV such that

    limλ0+vλ=0,

    and the real function

    λ122=1{|(120v)()|2+|(312v)()|2}+142=1|v()|4λ2=1F(v())

    is negative and strictly decreasing in (0,98).

    Put

    B=lim supξL=1F(,ξ)ξ2(Γ(1α))2L=1|¯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

    limnbn=

    such that

    a2n(Γ(1α))2L=1|¯α|2+Lapnp<(L+1)p(p2)4pbpnfor allnN, (A1)
    A=limnL=1max|t|bnF(,t)L=1F(,an)(L+1)p(p2)4pbpn(a2n(Γ(1α))2L=1|¯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 vV is a solution of (Pfλ) if and only if v is a critical point of the function Iλ. Put

    rn=(L+1)p(p2)4pbpnfor allnN.

    We see that rn>0 for all nN. From the way Φ is defined and in light of (6), (8), and (11), for each rn>0, we have

    Φ1(,rn)={vV:Φ(v)<rn}{vV:vpprn(L+1)p(p2)4}{vV:vpprn(L+1)p(p2)4}={vV:vpbpn},

    which implies

    supΦ(v)<rnΨ(v)=supΦ(v)<rnL=1F(,v())L=1max|x|bnF(,x).

    Now, for each nN, we define

    υ()={anif[1,L]N0,0if{0,L+1}.

    Clearly, υV. 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 N1LN, we have

    (L+1αυ)()=(RL+1αυ)()=(CL+1αυ)()=an(L+1)¯αΓ(1α)

    and

    (α0υ)()=(Rα0υ)()=(Cα0υ)()=an()¯αΓ(1α).

    Thus,

    Φ(υ)=12L=1{|(α0υ)()|2+|(L+1αυ)()|2}+1pL=1|υ()|p=12L=1{|an()¯αΓ(1α)|2+|an(L+1)¯αΓ(1α)|2}+Lapnp=a2n2(Γ(1α))2L=1|¯α|2+|(L+1)¯α|2+Lapnp=a2n(Γ(1α))2L=1|¯α|2+Lapnp.

    We have

    Ψ(υ)=L=1F(,υ())=L=1F(,an).

    In addition, from (A1), we have Φ(υn)<rn. Thus, for all large enough values of n, we obtain

    φ(rn)=inf˜vΦ1(,rn)supvΦ1(,r)Ψ(v)Ψ(˜v)rnΦ(˜v)supvΦ1(,rn)Ψ(v)L=1F(,υ())rnΦ(υ)=supvΦ1(,rn)Ψ(v)L=1F(,an)(L+1)p(p2)4pbpn(a2n(Γ(1α))2L=1|¯α|2+Lapnp)L=1max|x|bnF(,x)L=1F(,an)(L+1)p(p2)4pbpn(a2n(Γ(1α))2L=1|¯α|2+Lapnp). (22)

    Hence, due to (A2), we get

    γlimnφ(rn)A<.

    Now, we can verify that Iλ is unbounded from below. First, assume that B=. Accordingly, fix N such that

    N<c2n(Γ(1α))2L=1|¯α|2+Lcpnp

    and let cn>0 for all nN such that cn as n and

    L=1F(,cn)>Nfor allnN.

    For each nN, define

    yn()=cnfor all[1,L]N0.

    Thus, ynV and

    Φ(yn)=c2n(Γ(1α))2L=1|¯α|2+Lcpnp.

    Therefore,

    Iλ(yn)=c2n(Γ(1α))2L=1|¯α|2+LcpnpλL=1F(,cn)<c2n(Γ(1α))2L=1|¯α|2+LcpnpλN,

    that is, limnIλ(yn)=. Next, suppose B<. As λ>1B, we can find ε>0 with ε<B1λ. Thus, again letting cn>0 for all nN such that cn as n and

    L=1F(,cn)>Bεfor allnN,

    as argued above, and by letting ynV as before, we obtain

    Iλ(yn)=c2n(Γ(1α))2L=1|¯α|2+LcpnpλL=1F(,cn)<c2n(Γ(1α))2L=1|¯α|2+Lcpnpλ(Bε).

    Therefore, limnIλ(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 limnbn= 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 infξL=1max|x|ξF(,x)(L+1)p(p2)4pξp<lim supξL=1F(,ξ)ξ2(Γ(1α))2L=1|¯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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