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 n≥3.
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 n≥3.
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)=n∑i=1fi(xi) |
where f1,f2,…,fn are smooth functions. Each function fi depends on the real variable xi and is different from zero for 1≤i≤n. Or else it is a hyperplane.
In [1], Lima gave the parameterization of translation hypersurfaces with zero scalar curvature into Rn+1 for n≥3. Moreover they showed that every translation hypersurface with constant scalar curvature must have zero scalar curvature in the Euclidean space Rn+1 for n≥3 and proved the following theorem.
Theorem 1.1. Let Mn be a translation hypersurface of Rn+1 given by ψ=(x1,…,xn,F) for n≥3. Then Mn has zero scalar curvature iff it is congruent to the graph of the following functions:
1. F(x1,…,xn)=∑n−1i=1aixi+fn(xn)+b, on Rn−1×J, for some interval J and fn:J⊂R→R 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)=n−3∑i=1aixi+√βaln|cos(−aba+b√βxn+c)cos(a√βxn−2+a0)| +√βbln|cos(−aba+b√βxn+c)cos(b√βxn−1+b0)|+d, | (1.1) |
on Rn−3×I1×I2×I3, where a,a1,…,an−3,b,b0,c,d are real constants with a,b,a+b≠0,β=1+∑n−3i=1a2i and I1,I2,I3 are the open intervals defined, respectively, by the conditions |a√βxn−2+a0|<π/2, |b√βxn−1+b0|<π/2 and |−aba+b√βxn+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 n≥3.
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 1≤i,j≤n. The Christoffel symbols or the affine connection of Mn are given by
Γkij=12n∑m=1gkm(∂gjm∂xi+∂gim∂xj−∂gij∂xm), | (2.1) |
for 1≤i,j,k≤n. The Components of the Riemannian curvature tensor R of a semi-Riemannian manifold Mn are given by
Rijkl=∂Γikj∂xl−∂Γilj∂xk+n∑m=1ΓilmΓmkj−n∑m=1ΓikmΓmlj, | (2.2) |
for 1≤i,j,k,l≤n. The Components of the Ricci curvature tensor Ric of a semi-Riemannian manifold Mn are given by
Rij=n∑m=1Rmijm, | (2.3) |
for 1≤i,j≤n. The scalar curvature S of a semi-Riemannian manifold Mn are given by
S=n∑i,j=1gijRij=n∑i,j,k=1gijRkijk. | (2.4) |
Theorem 2.1. Let Mn be a n−dimensional 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)=n∑i=1fi(xi). | (2.5) |
Then the scalar curvature of Mn given by
S=2(εn+1+n∑i=1εif′2i)2∑1≤i<j≤nεiεjf′′if′′j(εn+1+∑1≤k≤nk≠i,jεkf′2k), | (2.6) |
where εi=⟨ei,ei⟩=±1 for 1≤i≤n+1.
Proof. It is easy to check that
gij=⟨ψi,ψj⟩={εi+εn+1f′2i, for i=jεn+1f′if′j, for i≠j | (2.7) |
and their inverse
gij={εi(εn+1+n∑k=1k≠iεkf′2k)Q, for i=j−εiεjf′if′jQ, for i≠j | (2.8) |
with Q=εn+1+n∑k=1εkf′2k 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 n−dimensional translation hypersurface of the semi-Euclidean space Rn+1q for n≥3 determined by the following equations
ψ(x1,…,xn)=(x1,…,xn,F(x1,…,xn)), F(x1,…,xn)=n∑i=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)=n−1∑i=1aixi+fn(xn)+b, | (2.9) |
on Rn−1×I, for some open interval I, where ai,b∈R, 1≤i≤n−1 and fn:I⊂R→R is a smooth function. With a appropiate translation, it is a vertical hypercylinder.
2.
F(x1,…,xn)=n−2∑i=1aixi+fn−1(xn−1)+fn(xn)+b, | (2.10) |
on Rn−2×I1×I2, for some open intervals I1,I2, where ai,b∈R, 1≤i≤n−2 with ∑n−2i=1εia2i=−εn+1 and fn−1:I1⊂R→R, fn:I2⊂R→R are smooth functions.
3. Let a,a0,a1,…,an−3,b,b0,c0,d be real constants with a≠0,b≠0,a+b≠0,b−a≠0, β=εn+1+∑n−3i=1εia2i>0 and I1,I2,I3,I4, I5 be some open intervals defined, respectively, by the conditions |a√βxn−2+a0|<π/2, |b√βxn−1+b0|<π/2, |aba+b√βxn+c0|<π/2,|abb−a√βxn+c0|<π/2 and |−aba+b√βxn+c0|<π/2.
a. If εn−1εn=1 and εn−2εn=1, then
F(x1,…,xn)=n−3∑i=1aixi+1aln|cos(aba+b√βxn+c0)cos(a√βxn−2+a0)| +1bln|cos(aba+b√βxn+c0)cos(b√βxn−1+b0)|+d, | (2.11) |
on Rn−3×I1×I2×I3.
b. If εn−1εn=−1 and εn−2εn=1, then
F(x1,…,xn)=n−3∑i=1aixi+1aln|cos(abb−a√βxn+c0)cos(a√βxn−2+a0)|−1bln|cos(abb−a√βxn+c0)cos(b√βxn−1+b0)|+d, | (2.12) |
on Rn−3×I1×I2×I4.
c. If εn−1εn=1 and εn−2εn=−1, then
F(x1,…,xn)=n−3∑i=1aixi−1aln|cos(abb−a√βxn+c0)cos(a√βxn−2+a0)| +1bln|cos(abb−a√βxn+c0)cos(b√βxn−1+b0)|+d, | (2.13) |
on Rn−3×I1×I2×I4.
d. If εn−1εn=−1 and εn−2εn=−1, then
F(x1,…,xn)=n−3∑i=1aixi−1aln|cos(−aba+b√βxn+c0)cos(a√βxn−2+a0)| −1bln|cos(−aba+b√βxn+c0)cos(b√βxn−1+b0)|+d, | (2.14) |
on Rn−3×I1×I2×I5.
If β=0, then Mn is locally a hyperplane.
Proof. From Theorem 1.1, Mn has zero scalar curvature iff
∑1≤i<j≤nεiεjf′′if′′j(εn+1+∑1≤k≤nk≠i,jεkf′2k)=0. | (2.15) |
We will examine the proof according to the following cases.
Case 1. Let εn+1+∑1≤k≤nk≠i,jεkf′2k=0 for all 1≤i<j≤n, then the functions f′k are constant for all 1≤k≤n. Consequently Mn is locally a hyperplane.
Case 2. Let f′′i(xi)=0 for all i=1,…n−1, then Mn is parameterized by the equation (2.9).
Case 3. Let f′′i(xi)=0 for all i=1,…n−2, then f′i(xi)=ai, ai∈R. Also we can rewrite (2.15) by the following equation
εn−1εnf′′n−1f′′n(εn+1+n−2∑k=1εka2k). |
According to this equation, we have the following cases:
ⅰ. If f′′n−1=0, corresponding to Case 1.
ⅱ. If f′′n=0, corresponding to Case 1.
ⅲ. If εn+1+n−2∑k=1εka2k=0, then Mn is parameterized by the equation (2.10).
Case 4. Let f′′i(xi)=0 for all i=1,…n−3, then f′i(xi)=ai, ai∈R. Also we can rewrite (2.15) by the following equation
εn−2εn−1f′′n−2f′′n−1(β+f′2n)+εn−2εnf′′n−2f′′n(β+f′2n−1)+εn−1εnf′′n−1f′′n(β+f′2n−2)=0, |
where β=εn+1+n−3∑k=1εka2k. If we multiply both sides of the above equation by εn−2εn−1εn, then we obtain
εnf′′n−2f′′n−1(β+f′2n)+εn−1f′′n−2f′′n(β+f′2n−1)+εn−2f′′n−1f′′n(β+f′2n−2)=0. | (2.16) |
According to the assumption, the functions f′′n−2, f′′n−1 and f′′n are different from zero. Also we get β+f′2k≠0 for k=n−2,n−1,n. Hence we rewrite (2.16)
εnf′′n−2f′′n−1(β+f′2n−2)(β+f′2n−1)+εn−1f′′n−2f′′n(β+f′2n−2)(β+f′2n)+εn−2f′′n−1f′′n(β+f′2n−1)(β+f′2n)=0. | (2.17) |
Differentiating the equation with respect to xn−2 and xn−1, we find
(f′′n−2β+f′2n−2)′=0 or (f′′n−1β+f′2n−1)′=0. |
If (f′′n−2β+f′2n−2)′=0, then there is a constant a≠0 such that
f′′n−2=a(β+f′2n−2). | (2.18) |
Substituting this equation into (2.17), we obtain
εnf′′n−1β+f′2n−1a+εn−1f′′nβ+f′2na+εn−2f′′n−1f′′n(β+f′2n−1)(β+f′2n)=0. | (2.19) |
Differentiating the equation with respect to xn−1 and xn, we find
(f′′n−1β+f′2n−1)′=0 or (f′′nβ+f′2n)′=0. |
If (f′′n−1β+f′2n−1)′=0, then there is a constant b≠0 such that
f′′n−1=b(β+f′2n−1). | (2.20) |
Substituting this equation into (2.19), we obtain
εnab+f′′nβ+f′2n(εn−1a+εn−2b)=0. | (2.21) |
Since ab≠0, from (2.21), then εn−1a+εn−2b≠0. If we rearrange the equation, then we get
f′′nβ+f′2n=−εnabεn−1a+εn−2b. | (2.22) |
If we integrate the equations (2.18), (2.20) and (2.22), then we obtain
arctan(f′n−2(xn−2)√β)=a√βxn−2+a0, |
arctan(f′n−1(xn−1)√β)=a√βxn−1+b0, |
arctan(f′n(xn)√β)=−εnab√βεn−1a+εn−2bxn+c0, |
where a0,b0 and c0 are constants. From these equations, we get
fn−2(xn−2)=−1aln|cos(a√βxn−2+a0)|+a1, |
fn−1(xn−1)=−1bln|cos(b√βxn−1+b0)|+b1, |
fn(xn)=εn−1a+εn−2bεnabln|cos(εnab√βεn−1a+εn−2bxn+c0)|+c1, |
where a1,b1 and c1 are constants. Therefore Mn is parameterized by the equation
ψ(x1,…,xn)=(x1,…,xn,n−3∑i=1aixi−1aln|cos(a√βxn−2+a0)| −1bln|cos(b√βxn−1+b0)| +(εn−2εna+εn−1εnb)ln|cos(εnab√βεn−1a+εn−2bxn+c0)|+d) | (2.23) |
where d=a1+b1+c1 is a constant. According to the values of εn−2, εn−1 and εn, if we rearrange the equation (2.23), then we get the following parameterizations.
ⅰ. If εn−1εn=1 and εn−2εn=1, then the translation hypersurface Mn is given by (2.11).
ⅱ. If εn−1εn=−1 and εn−2εn=1, then the translation hypersurface Mn is given by (2.12).
ⅲ. If εn−1εn=1 and εn−2εn=−1, then the translation hypersurface Mn is given by (2.13).
ⅳ. If εn−1εn=−1 and εn−2εn=−1, then the translation hypersurface Mn is given by (2.14).
Case 5. Let f′′i(xi)=0 for 1≤i≤k≤n−4, and f′′j(xj)≠0 for any j>k. We prove that this is not possible. Also we can rewrite (2.15) for any fixed l≥k+1 by the following equation
∑1≤i<j≤nεiεjf′′if′′j(εn+1+∑1≤m≤nm≠i,jεmf′2m)=εlf′′l∑k+1≤j≤nj≠lεjf′′j(εn+1+∑1≤m≤nm≠l,jεmf′2m)+∑k+1≤i<j≤ni,j≠lεiεjf′′if′′j(εn+1+∑1≤m≤nm≠i,jεmf′2m). | (2.24) |
Differentiating the equation (2.24) with respect to xl, we obtain
f′′′l∑k+1≤j≤nj≠lεjf′′j(εn+1+∑1≤m≤nm≠l,jεmf′2m)+2f′lf′′l∑k+1≤i<j≤ni,j≠lεiεjf′′if′′j=0. | (2.25) |
According to the equation (2.25), we define
Al=∑k+1≤j≤nj≠lεjf′′j(εn+1+∑1≤m≤nm≠l,jεmf′2m), Bl=∑k+1≤i<j≤ni,j≠lεiεjf′′if′′j. | (2.26) |
Al and Bl are not dependent on xl. From (2.25) and (2.26), we have
Alf′′′l+2Blf′lf′′l=0. | (2.27) |
Also there are two cases.
ⅰ. Let Al=0 for l≥k+1. From (2.26), we get
∑k+1≤j≤nj≠lεjf′′j(εn+1+∑1≤m≤nm≠l,jεmf′2m)=0. | (2.28) |
Differentiating the equation (2.28) with respect to xp for p≥k+1 and p≠l, we find
f′′′p(εn+1+∑1≤m≤nm≠l,pεmf′2m)+2f′pf′′p∑k+1≤j≤nj≠l,pεjf′′j=0. | (2.29) |
According to this equation, one must have
εn+1+∑1≤m≤nm≠l,pεmf′2m≠0. | (2.30) |
Otherwise the functions f′m are constant and we conclude that f′′m=0 for 1≤m≤n, m≠l,p. This is a contradiction with the assumption in Case 5. Since Al=0, according to (2.25), we get
2εlf′lf′′l∑k+1≤i<j≤ni,j≠lεiεjf′′if′′j=0. | (2.31) |
Since εl≠0 and f′′l≠0, we have
∑k+1≤i<j≤ni,j≠lεiεjf′′if′′j=0. | (2.32) |
Differentiating the equation (2.32) with respect to xp for p≥k+1 and p≠l, we obtain
f′′′p∑k+1≤j≤nj≠l,pεjf′′j=0. | (2.33) |
Differentiating the equation (2.33) with respect to xq for q≥k+1 and q≠l,p, we find f′′′pf′′′q=0. Therefore, at most one of the indexes p≥k+1 and p≠l is nonzero, denoted by p. Also we can get f′′′p≠0 and f′′′q=0 for all q≥k+1 and q≠l,p. From f′′′p≠0 and the equation (2.33), we have
∑k+1≤j≤nj≠l,pεjf′′j=0. | (2.34) |
Substituting this equation into (2.29), since εn+1+∑1≤m≤nm≠l,pεmf′2m≠0, we get f′′′p=0. This is a contradiction with f′′′p≠0. Also we get f′′′p=0 for all p≥k+1 and p≠l. From (2.29), we conclude that
∑k+1≤j≤nj≠l,pεjf′′j=0, | (2.35) |
for all p≥k+1 and p≠l. The above linear system has unique solution such that f′′j=0 for all k+1≤j≤n and j≠l. This is a contradiction with the assumption in Case 5. Consequently, if Al=0, then Case 5 is not possible.
ⅱ. Let Al≠0 for l≥k+1. Since Al≠0, from (2.27), we get
f′′′l+2αlf′lf′′l=0, | (2.36) |
where αl=BlAl is a constant for l≥k+1. Substituting this equation into (2.25), we find
αlf′lf′′l∑k+1≤j≤nj≠lεjf′′j(εn+1+∑1≤m≤nm≠l,jεmf′2m)−f′lf′′l∑k+1≤i<j≤ni,j≠lεiεjf′′if′′j=0. |
Since f′′l(xl)≠0 for l≥k+1, we obtain
αl∑k+1≤j≤nj≠lεjf′′j(εn+1+∑1≤m≤nm≠l,jεmf′2m)−∑k+1≤i<j≤ni,j≠lεiεjf′′if′′j=0. | (2.37) |
Differentiating the equation (2.37) with respect to xs for s≥k+1 and s≠l, we obtain
αlf′′′s(εn+1+∑1≤m≤nm≠l,sεmf′2m)+2αlf′sf′′s∑k+1≤j≤nj≠l,sεjf′′j−f′′′s∑k+1≤j≤nj≠l,sεjf′′j=0. |
From (2.36), f′′′s+2αsf′sf′′s=0 for s≥k+1. Also we can rewrite the above equation
−αlαsf′sf′′s(εn+1+∑1≤m≤nm≠l,sεmf′2m)+αlf′sf′′s∑k+1≤j≤nj≠l,sεjf′′j+αsf′sf′′s∑k+1≤j≤nj≠l,sεjf′′j=0. |
Since f′′s(xs)≠0 for s≥k+1, we get
−αlαs(εn+1+∑1≤m≤nm≠l,sεmf′2m)+αl∑k+1≤j≤nj≠l,sεjf′′j+αs∑k+1≤j≤nj≠l,sεjf′′j=0. | (2.38) |
Differentiating the equation (2.38) with respect to xt for t≥k+1 and t≠l and t≠s, we obtain
−2αlαsf′tf′′t+αlf′′′t+αsf′′′t=0. |
From (2.36), f′′′t+2αtf′tf′′t=0 for t≥k+1. Since f′′t(xt)≠0 for t≥k+1, we obtain the above equation
αlαs+αlαt+αsαt=0, | (2.39) |
with t≠l, t≠s and l≠s. 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 l≥k+1. We assume that αl=0 for k+1≤l≤n−1. From (2.36), f′′′l=0, then f′′l is constant for k+1≤l≤n−1. From (2.37), we obtain
∑k+1≤i<j≤ni,j≠lεiεjf′′if′′j=0 |
for l≠n. Therefore f′′n is constant and so αn=0. Thus, from (2.37), we get
∑k+1≤i<j≤ni,j≠lεiεjf′′if′′j=0. |
According to the equality, at most one of the functions f′′l is nonzero for k+1≤l≤n. This is a contradiction with the assumption in Case 5. Consequently, if Al≠0, then Case 5 is not possible.
Theorem 2.3. Let Mn be a n−dimensional translation hypersurface of the semi-Euclidean space Rn+1q for n≥3 determined by the following equations
ψ(x1,…,xn)=(x1,…,xn,F(x1,…,xn)), F(x1,…,xn)=n∑i=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=2Q2∑1≤i<j≤nεiεjf′′if′′j(εn+1+∑1≤k≤nk≠i,jεkf′2k) | (2.40) |
where Q=εn+1+n∑i=1εif′2i. Differentiating the equation (2.40) with respect to xl, we obtain
0=1Q2[f′′′l∑1≤j≤nj≠lεjf′′j(εn+1+∑1≤k≤nk≠l,jεkf′2k)+2f′lf′′l∑1≤i<j≤ni,j≠lεiεjf′′if′′j]−4f′lf′′lQ3∑1≤i<j≤nεiεjf′′if′′j(εn+1+∑1≤k≤nk≠i,jεkf′2k). |
If we rearrange this equation, then we get
2f′lf′′lS=1Q[f′′′l∑1≤j≤nj≠lεjf′′j(εn+1+∑1≤k≤nk≠l,jεkf′2k)+2f′lf′′l∑1≤i<j≤ni,j≠lεiεjf′′if′′j]. | (2.41) |
Differentiating the equation (2.41) with respect to xs and s≠l, we find
0=1Q[f′′′lf′′′s(εn+1+∑1≤k≤nk≠l,sεkf′2k)+2f′′′lf′sf′′s∑1≤j≤nj≠l,sεjf′′j+2f′lf′′lf′′′s∑1≤j≤nj≠l,sεjf′′j]−2f′sf′′sQ2[f′′′l∑1≤j≤nj≠lεjf′′j(εn+1+∑1≤k≤nk≠l,jεkf′2k)+2f′lf′′l∑1≤i<j≤ni,j≠lεiεjf′′if′′j]. |
From this equation, we get
4f′lf′′lf′sf′′sS=f′′′lf′′′s(εn+1+∑1≤k≤nk≠l,sεkf′2k)+2(f′′′lf′sf′′s+f′lf′′lf′′′s)∑1≤j≤nj≠l,sεjf′′j. | (2.42) |
Differentiating the equation (2.42) with respect to xt, t≠l and t≠s, we have
f′′′lf′′′sf′tf′′t+f′′′lf′′′tf′sf′′s+f′′′sf′′′tf′lf′′l=0. | (2.43) |
We assume that f′′lf′′sf′′t≠0 and f′′′l=0. According to (2.43), we get f′′′s=0 or f′′′t=0. From (2.42), we have 4f′lf′′lf′sf′′sS=0. This contradicts f′′lf′′sf′′t≠0 and S≠0. Also f′′′l≠0 and likewise f′′′s≠0 and f′′′t≠0. From f′′lf′′sf′′t≠0 and (2.43), we find
f′′′lf′lf′′lf′′′sf′sf′′s+f′′′lf′lf′′lf′′′tf′tf′′t+f′′′sf′sf′′sf′′′tf′tf′′t=0. | (2.44) |
From (2.44), we get f′′′l=αlf′lf′′l, with a nonzero constant αl. Substituting this equation into (2.41), we find
2SQ=αl∑1≤j≤nj≠lεjf′′j(εn+1+∑1≤k≤nk≠l,jεkf′2k)+2∑1≤i<j≤ni,j≠lεiεjf′′if′′j. | (2.45) |
Differentiating the equation (2.45) with respect to xl, we have f′lf′′lS=0. This contradicts f′′lf′′sf′′t≠0 and S≠0. Hence, it must be f′′lf′′sf′′t=0. Also, at most two of the functions f′′l are nonzero for 1≤l≤n. Without loss of generality, we assume that f′′n−1≠0, f′′n≠0 and f′′l=0 for 1≤l≤n−2, then f′l=al for 1≤l≤n−2 and we arrange (2.6)
0≠Q2S=f′′n−1f′′nα, | (2.46) |
where α=2εn−1εn(εn+1+n−2∑k=1εka2k) is a nonzero constant. Differentiating the equation (2.46) with respect to xn−1, we have
0≠4εn−1f′n−1f′′n−1QS=f′′′n−1f′′nα. | (2.47) |
Differentiating the equation with respect to xn, we get
0≠8εn−1εnf′n−1f′′n−1f′nf′′nS=f′′′n−1f′′′nα. | (2.48) |
Also, there is a nonzero constant β such that f′′′n−1=βf′n−1f′′n−1≠0 and from (2.47)
0≠4εn−1QS=f′′nαβ. | (2.49) |
Differentiating the equation (2.49) with respect to xn−1, we get
8f′n−1f′′n−1S=0. |
This is a contradiction with f′′n−1≠0. 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)=n∑i=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 n≥3.
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