Research article Special Issues

Translation hypersurfaces of semi-Euclidean spaces with constant scalar curvature

  • In this paper, we present translation hypersurfaces of semi-Euclidean spaces with zero scalar curvature. In addition, we prove that translation hypersurfaces with constant scalar curvature must have zero scalar curvature in the semi-Euclidean space Rn+1q for n3.

    Citation: Derya Sağlam, Cumali Sunar. Translation hypersurfaces of semi-Euclidean spaces with constant scalar curvature[J]. AIMS Mathematics, 2023, 8(2): 5036-5048. doi: 10.3934/math.2023252

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  • In this paper, we present translation hypersurfaces of semi-Euclidean spaces with zero scalar curvature. In addition, we prove that translation hypersurfaces with constant scalar curvature must have zero scalar curvature in the semi-Euclidean space Rn+1q for n3.



    Translation hypersurfaces are special Monge hypersurfaces. Many studies have been carried out with these hypersurfaces until today [1,2,3,4,5,6,7,8,9,10,11].

    In [1], Lima presented a complete description of all translation hypersurfaces with constant scalar curvature in the Euclidean space. In [2], they showed that every minimal translation and homothetical lightlike hypersurface is locally a hyperplane. In [3], the minimal translation hypersurfaces of E4 were studied. Yang, Zhang and Fu obtained a characterization of a class of minimal translation graphs which are the generalization of minimal translation hypersurfaces in the Euclidean space [4]. In [5], the authors studied a characterization of minimal translation graphs in the semi-Euclidean space. Recently, homothetical and translation lightlike graphs, which are generalizations of homothetical and translation lightlike hypersurfaces were investigated in the semi-Euclidean space Rn+2q [6]. Moreover Sağlam proved that all homothetical and all translation lightlike graphs are locally hyperplanes and according to this fact, both of these graphs are minimal. In [7], Seo gave a classification of the translation hypersurfaces with constant mean curvature or constant Gauss–Kronecker curvature in the Euclidean space and the Lorentz– Minkowski space. Moreover the author characterized the minimal translation hypersurfaces in the upper half-space model of the hyperbolic space. In 2019, Aydın and Ogrenmis studied translation hypersurfaces generated by translating planar curves and classified the translation hypersurfaces with constant Gauss-Kronecker curvature and constant mean curvature in the 4-dimensional isotropic space [8]. In [9], Ruiz-Hernandez investigated translation hypersurfaces in the (n+1)-dimensional Euclidean space whose Gauss-Kronecker curvature depends on its variables. In [10], Sousa, Lima and Vieira studied the geometry of generalized translation hypersurfaces immersed in Euclidean space equipped with a metric conformal to Euclidean metric and obtained results that characterize such hypersurfaces. In [11], Lima, Santos and Sousa gave a classification of the generalized translation graphs with constant mean curvature or constant Gauss–Kronecker curvature in the Euclidean space.

    In the semi-Euclidean space Rn+1q, a translation hypersurface Mn is a semi-Riemannian manifold with codimension 1 given by

    ψ(x1,,xn)=(x1,,xn,F(x1,,xn)), F(x1,,xn)=ni=1fi(xi)

    where f1,f2,,fn are smooth functions. Each function fi depends on the real variable xi and is different from zero for 1in. Or else it is a hyperplane.

    In [1], Lima gave the parameterization of translation hypersurfaces with zero scalar curvature into Rn+1 for n3. Moreover they showed that every translation hypersurface with constant scalar curvature must have zero scalar curvature in the Euclidean space Rn+1 for n3 and proved the following theorem.

    Theorem 1.1. Let Mn be a translation hypersurface of Rn+1 given by ψ=(x1,,xn,F) for n3. Then Mn has zero scalar curvature iff it is congruent to the graph of the following functions:

    1. F(x1,,xn)=n1i=1aixi+fn(xn)+b, on Rn1×J, for some interval J and fn:JRR is a smooth function, which defines, after a suitable linear change of variables, a vertical cylinder.

    2. A generalized periodic Enneper hypersurface given by

    F(x1,,xn)=n3i=1aixi+βaln|cos(aba+bβxn+c)cos(aβxn2+a0)|         +βbln|cos(aba+bβxn+c)cos(bβxn1+b0)|+d, (1.1)

    on Rn3×I1×I2×I3, where a,a1,,an3,b,b0,c,d are real constants with a,b,a+b0,β=1+n3i=1a2i and I1,I2,I3 are the open intervals defined, respectively, by the conditions |aβxn2+a0|<π/2, |bβxn1+b0|<π/2 and |aba+bβxn+c|<π/2.

    In this paper, we obtain the parameterization of translation hypersurfaces with zero scalar curvature into Rn+1q. In addition we prove that translation hypersurfaces with constant scalar curvature must have zero scalar curvature in the semi-Euclidean space Rn+1q for n3.

    Let Mn be a semi-Riemannian manifold and gij be the components of the metric tensor of Mn and gij be inverse of the functions gij for 1i,jn. The Christoffel symbols or the affine connection of Mn are given by

    Γkij=12nm=1gkm(gjmxi+gimxjgijxm), (2.1)

    for 1i,j,kn. The Components of the Riemannian curvature tensor R of a semi-Riemannian manifold Mn are given by

    Rijkl=ΓikjxlΓiljxk+nm=1ΓilmΓmkjnm=1ΓikmΓmlj, (2.2)

    for 1i,j,k,ln. The Components of the Ricci curvature tensor Ric of a semi-Riemannian manifold Mn are given by

    Rij=nm=1Rmijm, (2.3)

    for 1i,jn. The scalar curvature S of a semi-Riemannian manifold Mn are given by

    S=ni,j=1gijRij=ni,j,k=1gijRkijk. (2.4)

    Theorem 2.1. Let Mn be a ndimensional translation hypersurface of the semi-Euclidean space Rn+1q with a natural orthonormal basis {e1,en+1} determined by the following equations

    ψ(x1,,xn)=(x1,,xn,F(x1,,xn)), F(x1,,xn)=ni=1fi(xi). (2.5)

    Then the scalar curvature of Mn given by

    S=2(εn+1+ni=1εif2i)21i<jnεiεjfifj(εn+1+1knki,jεkf2k), (2.6)

    where εi=ei,ei=±1 for 1in+1.

    Proof. It is easy to check that

    gij=ψi,ψj={εi+εn+1f2i, for i=jεn+1fifj, for ij (2.7)

    and their inverse

    gij={εi(εn+1+nk=1kiεkf2k)Q, for i=jεiεjfifjQ, for ij (2.8)

    with Q=εn+1+nk=1εkf2k and i,j=1,...,n. By the direct calculation from the equations (2.1)–(2.4), we get (2.6).

    Theorem 2.2. Let Mn be a ndimensional translation hypersurface of the semi-Euclidean space Rn+1q for n3 determined by the following equations

    ψ(x1,,xn)=(x1,,xn,F(x1,,xn)), F(x1,,xn)=ni=1fi(xi).

    Then Mn has zero scalar curvature iff it is locally a hyperplane or it is parameterized by one of the following functions.

    1.

    F(x1,,xn)=n1i=1aixi+fn(xn)+b, (2.9)

    on Rn1×I, for some open interval I, where ai,bR, 1in1 and fn:IRR is a smooth function. With a appropiate translation, it is a vertical hypercylinder.

    2.

    F(x1,,xn)=n2i=1aixi+fn1(xn1)+fn(xn)+b, (2.10)

    on Rn2×I1×I2, for some open intervals I1,I2, where ai,bR, 1in2 with n2i=1εia2i=εn+1 and fn1:I1RR, fn:I2RR are smooth functions.

    3. Let a,a0,a1,,an3,b,b0,c0,d be real constants with a0,b0,a+b0,ba0, β=εn+1+n3i=1εia2i>0 and I1,I2,I3,I4, I5 be some open intervals defined, respectively, by the conditions |aβxn2+a0|<π/2, |bβxn1+b0|<π/2, |aba+bβxn+c0|<π/2,|abbaβxn+c0|<π/2 and |aba+bβxn+c0|<π/2.

    a. If εn1εn=1 and εn2εn=1, then

    F(x1,,xn)=n3i=1aixi+1aln|cos(aba+bβxn+c0)cos(aβxn2+a0)|         +1bln|cos(aba+bβxn+c0)cos(bβxn1+b0)|+d, (2.11)

    on Rn3×I1×I2×I3.

    b. If εn1εn=1 and εn2εn=1, then

    F(x1,,xn)=n3i=1aixi+1aln|cos(abbaβxn+c0)cos(aβxn2+a0)|1bln|cos(abbaβxn+c0)cos(bβxn1+b0)|+d, (2.12)

    on Rn3×I1×I2×I4.

    c. If εn1εn=1 and εn2εn=1, then

    F(x1,,xn)=n3i=1aixi1aln|cos(abbaβxn+c0)cos(aβxn2+a0)|         +1bln|cos(abbaβxn+c0)cos(bβxn1+b0)|+d, (2.13)

    on Rn3×I1×I2×I4.

    d. If εn1εn=1 and εn2εn=1, then

    F(x1,,xn)=n3i=1aixi1aln|cos(aba+bβxn+c0)cos(aβxn2+a0)|         1bln|cos(aba+bβxn+c0)cos(bβxn1+b0)|+d, (2.14)

    on Rn3×I1×I2×I5.

    If β=0, then Mn is locally a hyperplane.

    Proof. From Theorem 1.1, Mn has zero scalar curvature iff

    1i<jnεiεjfifj(εn+1+1knki,jεkf2k)=0. (2.15)

    We will examine the proof according to the following cases.

    Case 1. Let εn+1+1knki,jεkf2k=0 for all 1i<jn, then the functions fk are constant for all 1kn. Consequently Mn is locally a hyperplane.

    Case 2. Let fi(xi)=0 for all i=1,n1, then Mn is parameterized by the equation (2.9).

    Case 3. Let fi(xi)=0 for all i=1,n2, then fi(xi)=ai, aiR. Also we can rewrite (2.15) by the following equation

    εn1εnfn1fn(εn+1+n2k=1εka2k).

    According to this equation, we have the following cases:

    ⅰ. If fn1=0, corresponding to Case 1.

    ⅱ. If fn=0, corresponding to Case 1.

    ⅲ. If εn+1+n2k=1εka2k=0, then Mn is parameterized by the equation (2.10).

    Case 4. Let fi(xi)=0 for all i=1,n3, then fi(xi)=ai, aiR. Also we can rewrite (2.15) by the following equation

    εn2εn1fn2fn1(β+f2n)+εn2εnfn2fn(β+f2n1)+εn1εnfn1fn(β+f2n2)=0,

    where β=εn+1+n3k=1εka2k. If we multiply both sides of the above equation by εn2εn1εn, then we obtain

    εnfn2fn1(β+f2n)+εn1fn2fn(β+f2n1)+εn2fn1fn(β+f2n2)=0. (2.16)

    According to the assumption, the functions fn2, fn1 and fn are different from zero. Also we get β+f2k0 for k=n2,n1,n. Hence we rewrite (2.16)

    εnfn2fn1(β+f2n2)(β+f2n1)+εn1fn2fn(β+f2n2)(β+f2n)+εn2fn1fn(β+f2n1)(β+f2n)=0. (2.17)

    Differentiating the equation with respect to xn2 and xn1, we find

    (fn2β+f2n2)=0   or   (fn1β+f2n1)=0.

    If (fn2β+f2n2)=0, then there is a constant a0 such that

    fn2=a(β+f2n2). (2.18)

    Substituting this equation into (2.17), we obtain

    εnfn1β+f2n1a+εn1fnβ+f2na+εn2fn1fn(β+f2n1)(β+f2n)=0. (2.19)

    Differentiating the equation with respect to xn1 and xn, we find

    (fn1β+f2n1)=0   or   (fnβ+f2n)=0.

    If (fn1β+f2n1)=0, then there is a constant b0 such that

    fn1=b(β+f2n1). (2.20)

    Substituting this equation into (2.19), we obtain

    εnab+fnβ+f2n(εn1a+εn2b)=0. (2.21)

    Since ab0, from (2.21), then εn1a+εn2b0. If we rearrange the equation, then we get

    fnβ+f2n=εnabεn1a+εn2b. (2.22)

    If we integrate the equations (2.18), (2.20) and (2.22), then we obtain

    arctan(fn2(xn2)β)=aβxn2+a0,
    arctan(fn1(xn1)β)=aβxn1+b0,
    arctan(fn(xn)β)=εnabβεn1a+εn2bxn+c0,

    where a0,b0 and c0 are constants. From these equations, we get

    fn2(xn2)=1aln|cos(aβxn2+a0)|+a1,
    fn1(xn1)=1bln|cos(bβxn1+b0)|+b1,
    fn(xn)=εn1a+εn2bεnabln|cos(εnabβεn1a+εn2bxn+c0)|+c1,

    where a1,b1 and c1 are constants. Therefore Mn is parameterized by the equation

    ψ(x1,,xn)=(x1,,xn,n3i=1aixi1aln|cos(aβxn2+a0)|   1bln|cos(bβxn1+b0)|    +(εn2εna+εn1εnb)ln|cos(εnabβεn1a+εn2bxn+c0)|+d) (2.23)

    where d=a1+b1+c1 is a constant. According to the values of εn2, εn1 and εn, if we rearrange the equation (2.23), then we get the following parameterizations.

    ⅰ. If εn1εn=1 and εn2εn=1, then the translation hypersurface Mn is given by (2.11).

    ⅱ. If εn1εn=1 and εn2εn=1, then the translation hypersurface Mn is given by (2.12).

    ⅲ. If εn1εn=1 and εn2εn=1, then the translation hypersurface Mn is given by (2.13).

    ⅳ. If εn1εn=1 and εn2εn=1, then the translation hypersurface Mn is given by (2.14).

    Case 5. Let fi(xi)=0 for 1ikn4, and fj(xj)0 for any j>k. We prove that this is not possible. Also we can rewrite (2.15) for any fixed lk+1 by the following equation

    1i<jnεiεjfifj(εn+1+1mnmi,jεmf2m)=εlflk+1jnjlεjfj(εn+1+1mnml,jεmf2m)+k+1i<jni,jlεiεjfifj(εn+1+1mnmi,jεmf2m). (2.24)

    Differentiating the equation (2.24) with respect to xl, we obtain

    flk+1jnjlεjfj(εn+1+1mnml,jεmf2m)+2flflk+1i<jni,jlεiεjfifj=0. (2.25)

    According to the equation (2.25), we define

    Al=k+1jnjlεjfj(εn+1+1mnml,jεmf2m), Bl=k+1i<jni,jlεiεjfifj. (2.26)

    Al and Bl are not dependent on xl. From (2.25) and (2.26), we have

    Alfl+2Blflfl=0. (2.27)

    Also there are two cases.

    ⅰ. Let Al=0 for lk+1. From (2.26), we get

    k+1jnjlεjfj(εn+1+1mnml,jεmf2m)=0. (2.28)

    Differentiating the equation (2.28) with respect to xp for pk+1 and pl, we find

    fp(εn+1+1mnml,pεmf2m)+2fpfpk+1jnjl,pεjfj=0. (2.29)

    According to this equation, one must have

    εn+1+1mnml,pεmf2m0. (2.30)

    Otherwise the functions fm are constant and we conclude that fm=0 for 1mn, ml,p. This is a contradiction with the assumption in Case 5. Since Al=0, according to (2.25), we get

    2εlflflk+1i<jni,jlεiεjfifj=0. (2.31)

    Since εl0 and fl0, we have

    k+1i<jni,jlεiεjfifj=0. (2.32)

    Differentiating the equation (2.32) with respect to xp for pk+1 and pl, we obtain

    fpk+1jnjl,pεjfj=0. (2.33)

    Differentiating the equation (2.33) with respect to xq for qk+1 and ql,p, we find fpfq=0. Therefore, at most one of the indexes pk+1 and pl is nonzero, denoted by p. Also we can get fp0 and fq=0 for all qk+1 and ql,p. From fp0 and the equation (2.33), we have

    k+1jnjl,pεjfj=0. (2.34)

    Substituting this equation into (2.29), since εn+1+1mnml,pεmf2m0, we get fp=0. This is a contradiction with fp0. Also we get fp=0 for all pk+1 and pl. From (2.29), we conclude that

    k+1jnjl,pεjfj=0, (2.35)

    for all pk+1 and pl. The above linear system has unique solution such that fj=0 for all k+1jn and jl. This is a contradiction with the assumption in Case 5. Consequently, if Al=0, then Case 5 is not possible.

    ⅱ. Let Al0 for lk+1. Since Al0, from (2.27), we get

    fl+2αlflfl=0, (2.36)

    where αl=BlAl is a constant for lk+1. Substituting this equation into (2.25), we find

    αlflflk+1jnjlεjfj(εn+1+1mnml,jεmf2m)flflk+1i<jni,jlεiεjfifj=0.

    Since fl(xl)0 for lk+1, we obtain

    αlk+1jnjlεjfj(εn+1+1mnml,jεmf2m)k+1i<jni,jlεiεjfifj=0. (2.37)

    Differentiating the equation (2.37) with respect to xs for sk+1 and sl, we obtain

    αlfs(εn+1+1mnml,sεmf2m)+2αlfsfsk+1jnjl,sεjfjfsk+1jnjl,sεjfj=0.

    From (2.36), fs+2αsfsfs=0 for sk+1. Also we can rewrite the above equation

    αlαsfsfs(εn+1+1mnml,sεmf2m)+αlfsfsk+1jnjl,sεjfj+αsfsfsk+1jnjl,sεjfj=0.

    Since fs(xs)0 for sk+1, we get

    αlαs(εn+1+1mnml,sεmf2m)+αlk+1jnjl,sεjfj+αsk+1jnjl,sεjfj=0. (2.38)

    Differentiating the equation (2.38) with respect to xt for tk+1 and tl and ts, we obtain

    2αlαsftft+αlft+αsft=0.

    From (2.36), ft+2αtftft=0 for tk+1. Since ft(xt)0 for tk+1, we obtain the above equation

    αlαs+αlαt+αsαt=0, (2.39)

    with tl, ts and ls. From [1], in a similar way to the proof of Theorem 1.2, this equality imply that at most one of the constants αl is nonzero for lk+1. We assume that αl=0 for k+1ln1. From (2.36), fl=0, then fl is constant for k+1ln1. From (2.37), we obtain

    k+1i<jni,jlεiεjfifj=0

    for ln. Therefore fn is constant and so αn=0. Thus, from (2.37), we get

    k+1i<jni,jlεiεjfifj=0.

    According to the equality, at most one of the functions fl is nonzero for k+1ln. This is a contradiction with the assumption in Case 5. Consequently, if Al0, then Case 5 is not possible.

    Theorem 2.3. Let Mn be a ndimensional translation hypersurface of the semi-Euclidean space Rn+1q for n3 determined by the following equations

    ψ(x1,,xn)=(x1,,xn,F(x1,,xn)), F(x1,,xn)=ni=1fi(xi).

    Assume further that Mn has constant scalar curvature. Then its constant scalar curvature must be zero.

    Proof. We assume that a translation hypersurface Mn has nonzero constant scalar curvature S. From (2.6) the scalar curvature of Mn is given by

    S=2Q21i<jnεiεjfifj(εn+1+1knki,jεkf2k) (2.40)

    where Q=εn+1+ni=1εif2i. Differentiating the equation (2.40) with respect to xl, we obtain

    0=1Q2[fl1jnjlεjfj(εn+1+1knkl,jεkf2k)+2flfl1i<jni,jlεiεjfifj]4flflQ31i<jnεiεjfifj(εn+1+1knki,jεkf2k).

    If we rearrange this equation, then we get

    2flflS=1Q[fl1jnjlεjfj(εn+1+1knkl,jεkf2k)+2flfl1i<jni,jlεiεjfifj]. (2.41)

    Differentiating the equation (2.41) with respect to xs and sl, we find

    0=1Q[flfs(εn+1+1knkl,sεkf2k)+2flfsfs1jnjl,sεjfj+2flflfs1jnjl,sεjfj]2fsfsQ2[fl1jnjlεjfj(εn+1+1knkl,jεkf2k)+2flfl1i<jni,jlεiεjfifj].

    From this equation, we get

    4flflfsfsS=flfs(εn+1+1knkl,sεkf2k)+2(flfsfs+flflfs)1jnjl,sεjfj. (2.42)

    Differentiating the equation (2.42) with respect to xt, tl and ts, we have

    flfsftft+flftfsfs+fsftflfl=0. (2.43)

    We assume that flfsft0 and fl=0. According to (2.43), we get fs=0 or ft=0. From (2.42), we have 4flflfsfsS=0. This contradicts flfsft0 and S0. Also fl0 and likewise fs0 and ft0. From flfsft0 and (2.43), we find

    flflflfsfsfs+flflflftftft+fsfsfsftftft=0. (2.44)

    From (2.44), we get fl=αlflfl, with a nonzero constant αl. Substituting this equation into (2.41), we find

    2SQ=αl1jnjlεjfj(εn+1+1knkl,jεkf2k)+21i<jni,jlεiεjfifj. (2.45)

    Differentiating the equation (2.45) with respect to xl, we have flflS=0. This contradicts flfsft0 and S0. Hence, it must be flfsft=0. Also, at most two of the functions fl are nonzero for 1ln. Without loss of generality, we assume that fn10, fn0 and fl=0 for 1ln2, then fl=al for 1ln2 and we arrange (2.6)

    0Q2S=fn1fnα, (2.46)

    where α=2εn1εn(εn+1+n2k=1εka2k) is a nonzero constant. Differentiating the equation (2.46) with respect to xn1, we have

    04εn1fn1fn1QS=fn1fnα. (2.47)

    Differentiating the equation with respect to xn, we get

    08εn1εnfn1fn1fnfnS=fn1fnα. (2.48)

    Also, there is a nonzero constant β such that fn1=βfn1fn10 and from (2.47)

    04εn1QS=fnαβ. (2.49)

    Differentiating the equation (2.49) with respect to xn1, we get

    8fn1fn1S=0.

    This is a contradiction with fn10. Thus the constant scalar curvature must be zero.

    Translation hypersurfaces are special Monge hypersurfaces defined by the following equations

    ψ(x1,,xn)=(x1,,xn,F(x1,,xn)), F(x1,,xn)=ni=1fi(xi).

    In this paper, we obtain the parameterization of translation hypersurfaces with zero scalar curvature into Rn+1q. Moreover we prove that translation hypersurfaces with constant scalar curvature must have zero scalar curvature in the semi-Euclidean space Rn+1q for n3.



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