Research article

The number of solutions of cubic diagonal equations over finite fields

  • Received: 17 October 2022 Revised: 16 December 2022 Accepted: 19 December 2022 Published: 03 January 2023
  • MSC : 11T06, 11T24

  • Let p be a prime, k be a positive integer, q=pk, and Fq be the finite field with q elements. Let Fq be the multiplicative group of Fq, that is Fq=Fq{0}. In this paper, explicit formulae for the numbers of solutions of cubic diagonal equations a1x31+a2x32=c and b1x31+b2x32+b3x33=c over Fq are given, with ai,bjFq (1i2,1j3), cFq and p1(mod 3). Furthermore, by using the reduction formula for Jacobi sums, the number of solutions of the cubic diagonal equations a1x31+a2x32++asx3s=c of s4 variables with aiFq (1is), cFq and p1(mod 3), can also be deduced.

    Citation: Shuangnian Hu, Rongquan Feng. The number of solutions of cubic diagonal equations over finite fields[J]. AIMS Mathematics, 2023, 8(3): 6375-6388. doi: 10.3934/math.2023322

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  • Let p be a prime, k be a positive integer, q=pk, and Fq be the finite field with q elements. Let Fq be the multiplicative group of Fq, that is Fq=Fq{0}. In this paper, explicit formulae for the numbers of solutions of cubic diagonal equations a1x31+a2x32=c and b1x31+b2x32+b3x33=c over Fq are given, with ai,bjFq (1i2,1j3), cFq and p1(mod 3). Furthermore, by using the reduction formula for Jacobi sums, the number of solutions of the cubic diagonal equations a1x31+a2x32++asx3s=c of s4 variables with aiFq (1is), cFq and p1(mod 3), can also be deduced.



    One of the most important components of Riemannian geometry is determining the bound of the eigenvalue for the Laplacian on a particular manifold. The eigenvalue that occurs as a solutions of the Dirichlet or Neumann boundary value problems for the curvature functions is one of the main goals. Because different boundary conditions exist on a manifold, one can adopt a theoretical perspective to the Dirichlet boundary condition, using the upper bound for the eigenvalue as a technique of analysis for the Laplacians on a given manifold by using appropriate bound. Estimating the eigenvalue for the Laplacian and α-Laplacian operators has been increasingly popular over the years [18,19,21,25,26,27,31]. The generalization of the usual Laplacian operator, which is anisotropic mean curvature, was studied in [15]. Let K denotes a complete non compact Riemannian manifold, and B denotes the compact domain within K. Let λ1(B)>0 be a first eigenvalue of the Dirichlet boundary value problem:

    Δα+λα=0,inBandαonB,

    where Δ represents the Laplacian operator on the Riemannian manifold Km. The Reilly formula is dedicated entirely with the fundamental geometry of a given manifold. This can be generally acknowledged with the following phrase.

    Let (Km,g) be a compact m-dimensional Riemannian manifold, and λ1 denotes the first nonzero eigenvalue of the Neumann problem:

    Δα+λα=0,onKmandαν=0onKm,

    where ν is the outward normal on Km.

    Reilly [25] established the following inequality for a manifold Km isometrically immersed in the Euclidean space Rk with Km=0:

    λ11Vol(Km)KmH2dV, (1.1)

    where H is the mean curvature vector of immersion Km into Rn, λ1 denotes the first non-zero eigenvalue of the Laplacian on Km and dV denotes the volume element of Km.

    The upper bounds for α-Laplace operator in the sense of first eigenvalue for Finsler submanifold in the setting of Minkowski space was computed by Zeng and He [32]. Seto and Wei [28] presented the first eigenvalue of the Laplace operator for a closed manifold. However, F. Du et al. [13] derived the generalized Reilly inequality (1.3) and the first nonzero eigenvalue of the α-Laplace operator. Having followed the very similar approach, Blacker and Seto [4] demonstrated a Lichnerowicz type lower limit for the first nonzero eigenvalue of the α-Laplacian for Neumann and Dirichlet boundary conditions. Further, Papageorgiou et al. [24] studied p-Laplacian for concave-convex problems. Recently, p(x)-Laplacian are studied in the papers [14,17].

    The first non-null eigenvalue of the Laplacian is demonstrated in [10,12], which is deemed a generalization of work of Reilly [29]. The results of the distinct classes of Riemannian submanifolds for diverse ambient spaces show that the results of both first nonzero eigenvalues portray similar inequality and have same upper bounds [9,10]. In the case of the ambient manifold, it is clear from the previous studies that Laplace operators on Riemannian manifolds played a significant role in achieving various advances in Riemannian geometry (see [3,6,8,11,15,22,23,29,32]).

    The α-Laplacian on a m-dimensional Riemannian manifold Km is defined as

    Δα=div(|h|α2h), (1.2)

    where α>1, if α=2, then the above formula becomes usual Laplacian operator.

    The eigenvalue of Δh, from the other hand is Laplacian like. If a function h0 meets the following equation with dirichlet boundary condition or Neumann boundary condition as discussed earlier:

    Δαh=λ|h|α2h,

    where λ is a real number called Dirichlet eigenvalue. In the same way, the previous requirements apply to the Neumann boundary condition.

    If we look at Riemannian manifold without boundary, the Reilly type inequality for first nonzero eigenvalue λ1,α for α-Laplacian was computed in [30]:

    λ1,α=inf{K|h|qK|h|q:hW1,α(K1){0},K|h|α2h=0}. (1.3)

    However, Chen [7] pioneered the geometry of slant immersions as a natural extension of both holomorphic and totally real immersions. Further, Lotta [20] introduced the notion of slant submanifolds in the frame of almost contact metric manifolds, these submanifolds further explored by Cabrerizo et al. [5]. More precisely, Cabririzo et al. explored slant submanifolds in the setting of Sasakian manifolds. Another generalization of slant and contact CR-submanifolds was given by V. A. Khan and M. A. Khan [16], basically they proposed the notion of pseudo-slant submanifolds in the almost contact metric manifolds and provide an example of these submanifolds.

    After reviewing the literature, a natural question emerges: Is it possible to obtain the Reilly type inequalities for submanifolds of spheres via almost contact metric manifolds, which were studied in [2,10,12]? To answer this question, we explore the Reilly type inequalities for pseudo-slant submanifolds isometrically immersed in a generalized Sasakian space form. To this end our aim is to compute the bound for first non zero eigenvalues via α-Laplacian. The present study is leaded by the application of Gauss equation and studies done in [9,10,13].

    A (2n+1)-dimensional C-manifold ˉK is said to have an almost contact structure, if on ˉK there exist a tensor field ϕ of type (1,1), a vector field ξ and a 1-form η satisfying the following properties:

    ϕ2=I+ηξ,ϕξ=0,ηϕ=0,η(ξ)=1. (2.1)

    The manifold ˉK with the structure (ϕ,ξ,η) is called almost contact metric manifold. There exists a Riemannian metric g on an almost contact metric manifold ˉK, satisfying the following:

    η(e1)=g(e1,ξ),g(ϕe1,ϕe2)=g(e1,e2)η(e1)η(e2), (2.2)

    for all e1,e2TˉK, where TˉK is the tangent bundle of ˉK.

    In [1], Alegre et al. introduced the notion of generalized Sasakian space form as that an almost contact metric manifold (ˉK,ϕ,ξ,η,g) whose curvature tensor ˉR satisfies

    ˉR(e1,e2)e3=f1{g(e2,e3)e1g(e1,e3)e2}+f2{g(e1,ϕe3)ϕe2g(e2,ϕe3)ϕe1+2g(e1,ϕe2)ϕe3}+f3{η(e1)η(e3)e2η(e2)η(e3)e1+g(e1,e3)η(e2)ξg(e2,e3)η(e1)ξ}, (2.3)

    for all vector fields e1e3 and certain differentiable functions f1f3 on ˉK.

    A generalized Sasakian space form with functions f1f3 is denoted by ˉK(f1,f2,f3). If f1=c+34, f2=f3=c14, then ˉM(f1,f2,f3) becomes a Sasakian space form ˉM(c) [1]. If f1=c34, f2=f3=c+14, then ˉM(f1,f2,f3) becomes a Kenmotsu space form ˉM(c) [1], and if f1=f2=f3=c4, then ˉK(f1,f2,f3) becomes a cosymplectic space form ˉK(c) [1].

    Let K be a submanifold of an almost contact metric manifold ˉK with induced metric g. The Riemannian connection ˉ of ˉK induces canonically the connections and on the tangent bundle TK and the normal bundle TK of K respectively, then the Gauss and Weingarten formulae are governed by

    ˉe1e2=e1e2+σ(e1,e2), (2.4)
    ˉe1v=Ave1+e1v, (2.5)

    for each e1,e2TK and vTK, where σ and Av are the second fundamental form and the shape operator respectively for the immersion of K into ˉK, they are related as

    g(σ(e1,e2),v)=g(Ave1,e2), (2.6)

    where g is the Riemannian metric on ˉK as well as the induced metric on K.

    If Te1 and Ne1 represent the tangential and normal part of ϕe1 respectively, for any e1TK, one can write

    ϕe1=Te1+Ne1. (2.7)

    Similarly, for any vTK, we write

    ϕv=tv+nv, (2.8)

    where tv and nv are the tangential and normal parts of ϕv, respectively. Thus, T (resp. n) is 1-1 tensor field on TK (resp. TK) and t (resp. n) is a tangential (resp. normal) valued 1-form on TK (resp. TK).

    The notion of slant submanifolds in contact geometry was first defined by Lotta [20]. Later, these submanifolds were studied by Cabrerizo et al. [5]. Now, we have following definition of slant submanifolds.

    Definition 2.1. A submanifold K of an almost contact metric manifold ˉK is said to be slant submanifold if for any xK and XTxKξ, the angle between X and ϕX is constant. The constant angle θ[0,π/2] is then called slant angle of K in ˉK. If θ=0, the submanifold is invariant submanifold, and if θ=π/2, then it is anti-invariant submanifold. If θ0,π/2, it is proper slant submanifold.

    Moreover, Cabrerizo et al. [5] proved the characterizing equation for slant submanifold. More precisely, they proved that a submanifold Nm is said to be a slant submanifold if and only if a constant τ[0,π/2] and a (1,1) tensor field T which satisfies the following relation:

    T2=τ(Iηξ), (2.9)

    where τ=cos2θ.

    From (2.9), it is easy to conclude the following:

    g(Te1,Te2)=cos2θ{g(e1,e2)η(e1)η(e2)}, (2.10)

    e1,e2K.

    Now, we define the pseudo-slant submanifold, which was introduced by V. A. Khan and M. A. Khan [16].

    A submanifold K of an almost contact metric manifold ˉK is said to be pseudo-slant submanifold if there exist two orthogonal complementary distributions Sθ and S such that

    (1) TK=SSθξ.

    (2) The distribution S is anti-invariant, i.e., ϕSTK.

    (3) The distribution Sθ is slant with slant angle θπ/2.

    If θ=0, then the pseudo-slant submanifold is a semi-invariant submanifold. Now, we have the following example of pseudo-slant submanifold.

    Example 2.1. [16] Consider the 5-dimensional submanifold R9 with usual Sasakian structure, such that

    x(u,v,w,s,t)=2(u,0,w,0,0,v,scosθ,ssinθ,t),

    for any θ(0,π/2). Then it is easy to see that this is an example of pseudo-slant submanifold. Moreover, it can be observed

    e1=2(x1+y1z),e2=2y2e3=2(x3+y3z),
    e4=2cosθy3+2sinθy4,e5=2z=ξ,

    form a local orthonormal frame of TM. In which S=e1,e2 and Sθ=e3,e4, where D is anti-invariant and Sθ is slant distribution with slant angle θ.

    Suppose Km=p+2q+1 be a pseudo-slant submanifold of dimension m, in which p and 2q are the dimensions of the anti-invariant and slant distributions respectively. Moreover, let {u1,u2,,up,up+1=v1,up+2=v2,,um1=v2q,um=v2q+1=ξ} is an orthonormal frame of vectors which form a basis for the submanifold Kp+2q+1, such that {u1,,up} is tangential to the distribution D and the set {v1,v2=secθTv1,v3,v4=secθTv3,v2q=secθTv2q1} is tangential to Dθ. By the Eq (2.3), the curvature tensor ˉR for pseudo-slant submanifold Np+2q+1 is given by

    ˉR(ui,uj,ui,uj)=f1(m2m)+f2(3mi,j=1g2(ϕui,uj)2(m1)). (2.11)

    The dimension of the pseudo-slant submanifold Km can be decomposed as m=p+2q+1, then using the formula (2.9) for slant and anti-invariant distributions, we have

    g2(ϕui,ui+1)=0,fori{1,,p1},

    and

    g2(ϕui,ui+1)=cos2θ,fori{p+1,,2q1}.

    Then

    mi,j=1g2(ϕui,uj)=2qcos2θ.

    The relation (2.11) implies that

    ˉR(ui,uj,ui,uj)=f1(m2m)+f2(6qcos2θ2(m1)). (2.12)

    From the relation (2.12) and Gauss equation, one has

    f1m(m1)+f2(6qcos2θ2(m1))=2τn2H2+σ2

    or

    2τ=n2H2σ2+f1m(m1)+f2(6qcos2θ2(m1)). (2.13)

    In the paper [2], one of the present author Ali H. Alkhaldi with others studied the effect of the conformal transformation on the curvature and second fundamental form. More precisely, assume that ˉK2n+1 consists a conformal metric g=e2ρˉg, where ρC(ˉK). Then ˉΓa=eρΓa stands for the dual coframe of (ˉK,ˉg), ˉea==eρea represents the orthogonal frame of (ˉK,ˉg). Moreover, we have

    ˉΓab=Γab+ρaΓbρbΓa, (2.14)

    where ρa is the covariant derivative of ρ along the vector ea, i.e., dρ=aρaea.

    e2ρˉRpqrs=Rpqrs(ρprδqs+ρqsδprρpsδqrρqrδps)+(ρpρrδqs+ρqρsδprρqρtδpsρpρsδqr)|α|2(δprδqsδilδqr). (2.15)

    Applying pullback property in (2.14) to Km via point x, we get

    ˉσαpq=eρ(σαpqραδqp), (2.16)
    ˉHα=eα(Hαρα). (2.17)

    The following significant relation was proved in [1]:

    e2ρ(ˉσ2mˉH2)+mH2=σ2. (2.18)

    Initially, some basic results and formulas will be discussed which are compatible with the papers [2,22]. Now, we have the following result.

    Lemma 3.1. [2] Let Km be a slant submanifold of a Sasakian space form ˉK2t+1(c) which is closed and oriented with dimension 2. If f:KmˉK2t+1(c) is embedding from Km to ˉK2t+1(c). Then there is a standard conformal map x:ˉK2t+1(c)S2t+1(1)R2t+2 such that the embedding Γ=xf=(Γ1,,Γ2t+2) satisfies that

    Km|Γa|α2ΓadVK=0,a=1,,2(t+1),

    for α>1.

    In the next result, we obtain a result which is analogous to Lemma 2.7 of [22]. Indeed, in Lemma 3.1, by the application of test function, we obtain the higher bound for λ1,α in terms of conformal function.

    Proposition 3.1. Let Km be a m-dimensional pseudo slant submanifold, which is closed orientable isometrically immersed in a generalized Sasakian space form ˉK2t+1(f1,f2,f3), then we have

    λ1,αVol(Km)2|1α2|(t+1)|1α2|mα2Km(e2ρ)α2dV, (3.1)

    where x is the conformal map used in Lemma 3.1, and α>1. The standard metric is identified by Lc and consider xL1=e2pLc.

    Proof. Consider Γa as a test function along with Lemma 3.1, we have

    λ1,αKm|Γa|α|Γa|αdV,1a2(t+1), (3.2)

    observing that 2t+2a=1|Γa|2=1, then |Γa|1, we get

    2t+2a=1|Γa|2=mi=1|eiΓ|2=me2ρ. (3.3)

    On using 1<α2, we conclude

    |Γa|2|Γa|α. (3.4)

    By the application of Hölder's inequality, together with (3.2)–(3.4), we get

    λ1,αVol(Km)=λ1,α2t+2a=1Km|Γa|2dVλ1,α2t+2a=1Km|Γa|αdVλ1,αKm2t+2a=1|Γa|αdV(2t+2)1α/2Km(2t+1a=1|Γa|2)α/2dV=21α2(t+1)1α2Km(me2ρ)α2dV, (3.5)

    which is (3.1). On the other hand, if we assume α2, then, by Hölder inequality,

    I=2t+2a=1|Γa|2(2t+2)12α(2t+2a=1|Γa|α)2α. (3.6)

    As a result, we get

    λ1,αVol(Nm)(2t+2)α21(2t+2a=1λ1,αNm|Γa|αdV). (3.7)

    The Minkowski inequality provides

    2t+2a=1|Γa|α(2t+2a=1|Γa|2)α2=(me2ρ)α2. (3.8)

    By the application of (3.2), (3.7) and (3.8), it is easy to get (3.1).

    In the next theorem, we are going to provide a sharp estimate for the first eigenvalue of the α-Laplace operator on the pseudo-slant submanifold of a generalized Sasakian space form ˉK2t+1(f1,f2,f3).

    Theorem 3.1. Let Km be a m-dimensional pseudo-slant submanifold of a generalized Sasakian space form ˉK2t+1(f1,f2,f3), then

    (1)The first non-null eigenvalue λ1,α of the α-Laplacian satisfies

    λ1,α2(1α2)(t+1)(1α2)mα2(Vol(K))α/2×{Km(f1+f2(6qcos2θm(m1)2m)+H2)dV}α/2 (3.9)

    for 1<α2, and

    λ1,α2(1α2)(t+1)(1α2)mα2(Vol(K))α/2×{Km(f1+f2(6qcos2θm(m1)2m)+H2)dV}α/2 (3.10)

    for 2<αm2+1, where p and 2q are the dimensions of the anti-invariant and slant distributions.

    (2) The equality satisfies in (3.9) and (3.10) if and only if α=2 and Km is minimally immersed in a geodesic sphere of radius rc of ˉK2t+1(f1,f2,f3) with the following relations:

    r0=(mλΔ1)1/2,r1=sin1r0,r1=sinh1r0.

    Proof. 1<α2 α21. Proposition 3.1 together with Hölder inequality provides

    λ1,αVol(Km)21α2(t+1)1α2mα2Km(e2ρ)α2dV21α2(t+1)|1α2|mα2(Vol(Km))1α2(Kme2ρdV)α2. (3.11)

    We can calculate e2ρ with the help of conformal relations and Gauss equation. Let ˉK2k+1=ˉK2k+1(f1,f2,f3), and ˉg=e2ρLc, ˉg=cL1. From (2.13), the Gauss equation for the embedding f and the pseudo slant embedding Γ=xf, we have

    R=(f1)m(m1)+(f2)(m1){6qcos2θ2(m1)}+m(m1)H2+mH2Sσ|2, (3.12)
    ˉRm(m1)=m(m1)ˉH2+(mˉH2ˉσ|2). (3.13)

    On tracing (2.15), we have

    e2ρˉR=R(m2)(m1)|ρ|22(m1)Δρ. (3.14)

    Using (3.12) and (3.13) in (3.14), we get

    e2ρ(m(m1)+m(m1)ˉH2+(mˉH2ˉσ|2))=(f1)m(m1)+(f2){6qcos2θ2(m1)}+m(m1)H2+(mH2σ|2)(m2)(m1)ρ22(m1)Δρ. (3.15)

    The above relation implies

    e2ρˉσ|2(m2)(m1)|ρ|22(m1)Δρ=m(m1)[{e2ρf1(f2)(6qcos2θm(m1)2m)}(e2ρˉH2H2)]+m(e2ρˉH2H2). (3.16)

    From (2.17) and (2.18), we derive

    m(m1){e2ρ(f1)(f2)(6qcos2θm(m1)2m)}+m(m1)α(Hαρα)2=m(m1)H2(m2)(m1)|ρ|22(m1)Δρ. (3.17)

    Further, on simplification we get

    e2ρ={(f1)+(f2)(6qcos2θm(m1)2m)+H2}2mΔρm2m|Δρ|2(ρ)H2. (3.18)

    On integrating along dV, it is easy to see that

    λ1,αVol(Km)2|1α2|(t+1)|1α2|mα2(Vol(Km))1α2(Kme2ρdV)α2.2|1α2|(t+1)|1α2|mα2(Vol(Km))α21{Km{f1+f2(6qcos2θm(m1)2m)+H2}dV}α/2, (3.19)

    which is equivalent to (3.9). If α>2, then it is not possible to apply Hölder inequality to govern Km(e2ρdV)α2 by using Km(e2ρ). Now, multiply both sides of (3.18) by e(α2)ρ and integrating on Km,

    KmeαρdVKm{f1+f2(6qcos2θm(m1)2m)+H2}e(α2)ρdV(m22α+4m)Kme(α2)|Δρ|2dVKm{f1+f2(6qcos2θm(m1)2m)+H2}e(α2)ρdV. (3.20)

    From the assumption, it is evident that m2α2. On applying Young's inequality, we arrive

    Km{f1+f2(6qcos2θm(m1)2m)+H2}e(α2)ρdV2αKm{|f1+f2(6qcos2θm(m1)2m)+H2|}α/2dV+α2αKmeαρdV. (3.21)

    From (3.20) and (3.21), we conclude the following:

    KmeαρdVKm{|f1+f2(6qcos2θm(m1)2m)+H2|}α/2dV. (3.22)

    Substituting (3.22) in (3.1), we obtain (3.10). For the pseudo slant submanifolds, the equality case holds in (3.9), the equality cases of (3.2) and (3.4) imply that

    |Γa|2=|Γa|α,ΔαΓa=λ1,α|Γa|α2Γa,

    for a=1,,2t+2. For 1<α<2, we have |Γa|=0 or 1. Therefore, there exists only one a for which |Γa|=1 and λi,α=0, and it can not be possible since eigenvalue λi,α0. This leads to use the value of α equal to 2, therefore, we can apply Theorem 1.5 of [15].

    For α>2, the equality in (3.10) still holds, this indicates that equalities in (3.7) and (3.8) satisfy, and this leads to

    |Γ1|α==|Γ2t+2|α,

    and there exists a such that |Γa|=0. It shows that Γa is a constant and λ1,α=0, this again contradicts with the fact that λ1,α0, this completes the proof.

    Note 3.1. If α=2, then the α-Laplacian operator becomes the Laplacian operator. Therefore, we have the following corollary.

    Corollary 3.1. Let Km be a m-dimensional pseudo-slant submanifold of a generalized Sasakian space form ˉK2t+1(f1,f2,f3), then the first non-null eigenvalue λΔ1 of the Laplacian satisfies

    λΔ1m(Vol(K))Km{f1+f2(6qcos2θ2m)+H2)}dV. (3.23)

    By the application of Theorem 3.1 for 1<α2, we have the following result.

    Theorem 3.2. Let Km be a m-dimensional pseudo-slant submanifold of a generalized Sasakian space form ˉK2t+1(f1,f2,f3), then the first non-null eigenvalue λ1,α of the α-Laplacian satisfies

    λ1,α2(1α2)(t+1)(1α2)mα2(Vol(K))α/2×[Km(f1+f2(6qcos2θ2m)+H2)α2(α1)]α1dV (3.24)

    for 1<α2, and

    λ1,α2(1α2)(t+1)(1α2)mα2(Vol(K))α/2×[Km(f1+f2(6qcos2θ2m)+H2)α2(α1)]α1dV (3.25)

    for 2<αm2+1.

    Proof. Suppose 1<α2, we have α2(α1)1, then the Hölder inequality provides

    Km{(f1)+(f2)(3cos2θ2m)+H2}dV((Vol(Km))12(α1)α)×[Km(f1+f2(6qcos2θm(m1)2m)+H2)α2(α1)]2(α1)α. (3.26)

    On combining (3.9) and (3.26), we get the required inequality, this completes the proof.

    Note 3.2. If θ=0, then the pseudo-slant submanifolds become the semi-invariant submanifolds.

    By the application of above findings, we can deduce the following results for semi-invariant submanifolds in the setting of Sasakian manifolds.

    Corollary 3.2. Let Km be a m-dimensional semi-invariant submanifold of a generalized Sasakian space form ˉK2t+1(f1,f2,f3), then

    (1) The first non-null eigenvalue λ1,α of the α-Laplacian satisfies

    λ1,α2(1α2)(t+1)(1α2)mα2(Vol(K))α/2×{Km(f1+f2(6q2)m+H2)}α/2dV (3.27)

    for 1<α2, and

    λ1,α2(1α2)(t+1)(1α2)mα2(Vol(K))α/2×{Km(f1+f2(6q2)m+H2)}α/2dV (3.28)

    for 2<αm2+1, where p and 2q are the dimensions of the anti-invariant and slant distributions.

    (2) The equality satisfies in (3.27) and (3.28) if and only if α=2, and Km is minimally immersed in a geodesic sphere of radius rc of ˉK2t+1(f1,f2,f3) with the following relations:

    r0=(mλΔ1)1/2,r1=sin1r0,r1=sinh1r0.

    Further, by Corollary 3.4 and Note 3.1, we deduce the following.

    Corollary 3.3. Let Km be a m-dimensional semi-invariant submanifold of a generalized Sasakian space form ˉK2t+1(f1,f2,f3), then the first non-null eigenvalue λΔ1 of the Laplacian satisfies

    λΔ1m(Vol(K))Km{f1+f2(6q2)m+H2)}dV. (3.29)

    In addition, we also have the following corollary, which can be derived by Theorem 3.2.

    Corollary 3.4. Let Km be a m-dimensional semi-invariant submanifold of a generalized Sasakian space form ˉK2t+1(f1,f2,f3), then the first non-null eigenvalue λ1,α of the α-Laplacian satisfies

    λ1,α2(1α2)(t+1)(1α2)mα2(Vol(K))α/2×[Km(f1+f2(6q2)4+H2)α2(α1)]α1dV (3.30)

    for 1<α2.

    In this paper, we established the upper bounds for the first eigenvalues of the α-Laplacian operator for the pseudo-slant submanifolds in the setting of generalized Sasakian space forms. The class of pseudo-slant submanifold includes the class of semi-invariant, invariant, anti-invariant, and slant submanifolds. Therefore, the results obtained in this paper generalize the results for the first eigenvalues for these particular submanifolds.

    The second author extends his appreciation to the Deanship of Scientific Research at King Khalid University for funding this work (No. R.G.P.2/199/43).

    The authors state that there is no conflict of interest.



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