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Printed version ISSN 0001-3765 / Online version ISSN 1678-2690 http://dx.doi.org/10.1590/0001-3765201620150326

www.scielo.br/aabc

Translation Hypersurfaces with ConstantSSSrrr Curvature in the Euclidean Space

BARNABÉ P. LIMA1, NEWTON L. SANTOS1, JUSCELINO P. SILVA2and PAULO A.A. SOUSA1

1Universidade Federal do Piauí, Campus Ininga, Centro de Ciências da Natureza, Departamento de Matemática, Bairro Ininga,

64049-550 Teresina, PI, Brazil

2Universidade Federal do Cariri, Campus Juazeiro do Norte, Centro de Ciências e Tecnologia, Bairro Cidade Universitária,

63048-080 Juazeiro do Norte, CE, Brazil

Manuscript received on May 12, 2015; accepted for publication on October 20, 2015

ABSTRACT

The main goal of this paper is to present a complete description of all translation hypersurfaces with constant r-curvatureSr, in the Euclidean spaceR

n+1, where3

≤r≤n−1.

Key words:Euclidean space, Scherk’s surface, Translation hypersurfaces,r-Curvature.

INTRODUCTION

It is well known that translation hypersurfaces are very important in Differential Geometry, providing an interesting class of constant mean curvature hypersurfaces and minimal hypersurfaces in a number of spaces endowed with good symmetries and even in certain applications in Microeconomics. There are many results about them, for instance, Chen et al. (2003), Dillen et al. (1991), Inoguchi et al. (2012), Lima et al. (2014), Liu (1999), López (2011), López and Moruz (2015), López and Munteanu (2012), Seo (2013) and Chen (2011), for an interesting application in Microeconomics.

Scherk (1835) obtained the following classical theorem: LetM :={(x, y, z) : z=f(x) +g(y)}be a

translation surface inR3, if is minimal then it must be a plane or the Scherk surface defined by

z(x, y) = 1 aln

cos

(ay)

cos(ax)

,

wherea is a nonzero constant. In a different aspect, Liu (1999) considered the translation surfaces with

constant mean curvature in 3-dimensional Euclidean space and Lorentz-Minkowski space and Inoguchi

et al. (2012) characterized the minimal translation surfaces in the Heisenberg groupN il3, and López and

Munteanu, the minimal translation surfaces inSol3.

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The concept of translation surfaces was also generalized to hypersurfaces of Rn+1 by Dillen et al.

(1991), who obtained a classification of minimal translation hypersurfaces of the (n + 1)-dimensional

Euclidean space. A classification of the translation hypersurfaces with constant mean curvature in (n+ 1)-dimensional Euclidean space was made by Chen et al. (2003).

The absence of an affine structure in hyperbolic space does not permit to give an intrinsic concept of translation surface as in the Euclidean setting. Considering the half-space model of hyperbolic space, López (2011), introduced the concept of translation surface and presented a classification of the minimal translation surfaces. Seo (2013) has generalized the results obtained by Lopez to the case of translation hypersurfaces of the(n+ 1)-dimensional hyperbolic space.

Definition 1. We say that a hypersurfaceMnof the Euclidean spaceRn+1is a translation hypersurface if it is the graph of a function given by

F(x1, . . . , xn) =f1(x1) +. . .+fn(xn)

where (x1, . . . , xn) are cartesian coordinates and each fi is a smooth function of one real variable for

i= 1, . . . , n.

Now, letMn Rn+1 be an oriented hypersurface and

λ1, . . . , λn denote the principal curvatures of

Mn. For each r = 1, . . . , n, we can consider similar problems to the above ones, related with the r-th

elementary symmetric polynomials,Sr, given by

Sr =

X

1≤i1<···<ir≤n

λi1· · ·λir

In particular,S1is the mean curvature,S2the scalar curvature andSnthe Gauss-Kronecker curvature, up to normalization factors. A very useful relationship involving the variousSris given in the [Proposition 1, Caminha (2006)]. This result will play a central role along this paper.

Recently, some authors have studied the geometry of translational hypersurfaces under a condition in theSrcurvature, wherer >1. Namely, Leite (1991) gave a new example of a translation hypersurface ofR4 with zero scalar curvature. Lima et al. 2014 presented a complete description of all translation hypersurfaces with zero scalar curvature in the Euclidean space Rn+1 and Seo 2013 proved that if

M is a translation

hypersurface with constant Gauss-Kronecker curvature GK inRn+1, thenM is congruent to a cylinder,

and henceGK = 0.

In this paper, we obtain a complete classification of translation hypersurfaces ofRn+1withS

r= 0. We prove the following

Theorem 1. LetMn(n3)be a translation hypersurface inRn+1. Then, for

2< r < n,Mnhas zeroSr

curvature if, and only if, it is congruent to the graph of the following functions

• F(x1, . . . , xn) = n−Xr+1

i=1

aixi+ n X

j=n−r+2

fj(xj) +b,

on Rn−r+1

×Jn−r+2 × · · · × Jn, for certain intervals Jn−r+2, . . . , Jn, and arbitrary smooth functions

(3)

A generalized periodic Enneper hypersurface given by

F(x1, . . . , xn) =

n−r−1

X

i=1 aixi

+

n−1

X

k=n−r

β ak ln

cos−σ an−r. . . an−1

r−1(an−r, . . . , an−1)

βxn+bn

cos(ak√βxk+bk)

+c

on Rn−r−1

× In−r × · · · × In, with a1, . . . , an−r, . . . , an−1, bn−r, . . . , bn and c are real constants

where an−r, . . . , an−1 and σr−1(an−r, . . . , an−1) nonzero, β = 1 +

n−r−1

X

i=1

a2i, Ik(n − r ≤ k ≤

n 1) are open intervals defined by the conditions |ak√βxk + bk| < π/2 while In is defined by

an−r. . . an−1 σr−1(an−r, . . . , an−1)

βxn+bn

< π/2.

Theorem 2. Any translation hypersurface inRn+1

(n 3)withSr constant, for2 < r < n, must have

Sr= 0.

Finally, we observe that, when one considers the upper half-space model of the(n+ 1)-dimensional

hyperbolic spaceHn+1, that is, Rn+1

+ ={(x1, . . . , xn, xn+1)∈Rn+1 :xn+1 >0}

endowed with the hyperbolic metricds2 = 1

x2

n+1 dx2

1+. . .+dx 2

n+1

then, unlike in the Euclidean setting, the coordinatesx1, . . . , xnare interchangeable, but the same does not happen with the coordinatexn+1and,

due to this observation, López 2011 and Seo 2013 considered two classes of translation hypersurfaces in

Hn+1:

A hypersurfaceM Hn+1is called a translation hypersurface oftype I(respectively,type II)if it is given by an immersionX:U RnHn+1 satisfying

X(x1, . . . , xn) = (x1, . . . , xn, f1(x1) +. . .+fn(xn))

where eachfi is a smooth function of a single variable. Respectively, in case oftype II,

X(x1, . . . , xn) = (x1, . . . , xn−1, f1(x1) +. . .+fn(xn), xn) Seo proved

Theorem 3(Theorem 3.2, Seo 2013). There is no minimal translation hypersurface oftype IinHn+1.

and with respect totype IIsurfaces he proved

Theorem 4(Theorem 3.3, Seo 2013). LetM H3 be a minimal translation surface oftype IIgiven by the parametrizationX(x, z) = (x, f(x) +g(z), z). Then the functionsf andgare as follows:

f(x) = ax+b,

g(z) = p1 +a2

Z cz2

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wherea,b, andcare constants.

We emphasize that the result proved by Seo, Theorem 3.2 of Seo 2013, implies that our result (Theorem 2) is not valid in the hyperbolic space context.

PRELIMINARIES AND BASIC RESULTS

LetMn+1be a connected Riemannian manifold. In the remainder of this paper, we will be concerned with

isometric immersions,Ψ : Mn Mn+1, from a connected,n-dimensional orientable Riemannian

man-ifold, Mn, into Mn+1. We fix an orientation of Mn, by choosing a globally defined unit normal vector

field,ξ, onM. Denote byA, the corresponding shape operator. At eachpM,Arestricts to a self-adjoint

linear mapAp : TpM → TpM. For each1 ≤r ≤n, letSr : Mn → Rbe the smooth function such that

Sr(p)denotes ther-th elementary symmetric function on the eigenvalues ofAp, which can be defined by the identity

det(Ap−λI) = n X

k=0

(1)n−kSk(p)λn−k. (1)

where S0 = 1by definition. If p ∈ Mn and{el} is a basis ofTpM, given by eigenvectors of Ap, with corresponding eigenvalues{λl}, one immediately sees that

Sr =σr(λ1, . . . , λn),

whereσr∈R[X1, . . . , Xn]is ther-th elementary symmetric polynomial onX1, . . . , Xn. Consequently,

Sr=

X

1≤i1<···<ir≤n

λi1· · ·λir, where r = 1, . . . , n.

In the next result we present an expression for the curvatureSr of a translation hypersurface in the Euclidean space. This expression will play an essential role in this paper.

Proposition 1. LetF : Ω Rn Rbe a smooth function, defined asF(x

1, . . . , xn) = Pni=1fi(xi), where eachfi is a smooth function of one real variable. LetMnbe the graphic ofF, given in coordinates

by

ϕ(x1, . . . , xn) = n X

i=1

xiei+F(x1, . . . , xn)en+1. (2) TheSrcurvature ofMnis given by

Sr =

1 Wr+2 ·

n X

1≤i1<...<ir≤n

¨

fi1. . .f¨ir(1 + X

1≤m≤n m6=i1...ir

˙

fm2), (3)

where the dot represents derivative with respect to the corresponding variable, that is, for eachj= 1, . . . , n, one hasf˙j = dfj

dxj

(xj) =

∂F ∂xj

(x1, . . . , xn)andW2 = 1 +|∇F|2

Proof. LetF be as stated in the Proposition, denote byF = Pni=1 ∂F

∂xi ei the Euclidean gradient ofF andh,ithe standard Euclidean inner product. Then, we have

∇F =

n X

(5)

and the coordinate vector fields associated to the parametrization given in (2) have the following form

∂ϕ ∂xm

=em+ ˙fmen+1, m= 1, . . . , n.

Hence, the elementsGij of the metric ofMnare given by

Gij = ∂ϕ

∂xi,

∂ϕ ∂xj

=δij + ˙fif˙j,

implying that the matrix of the metricGhas the following form

G=In+ (∇F)t ∇F,

whereInis the identity matrix of ordern. Note that thei-th column ofG, which will be denoted byGi, has the expression given by the column vector

Gi=ei+ ˙fi∇F. (4)

An easy calculation shows that the unitary normal vector fieldξofMnsatisfies

W ξ=en+1− ∇F,

whereW2= 1 +|∇F|2. Thus, the second fundamental formBij ofMnsatisfies

W Bij =

W ξ, ∂ 2ϕ

∂xi∂xj

=Den+1− ∇F, δijf¨ien+1

E

=δijf¨i,

implying that the matrix ofBis diagonal

B = 1

W ·diag( ¨f1, . . . ,f¨n),

withi-th column given by the column vector

Bi= f¨i

W ei. (5)

IfAdenotes the matrix of the Weingarten mapping, thenA=G−1B. In (1), changingλbyλ−1gives

det(λAI) =

n X

i=1

(1)n−iSiλi.

Thus, we conclude that the expression for curvatureSrcan be found by the following calculation

(1)n−rSr=

1 r!

dr

dλrλ=0det(λA−I). Note that

(1)n−rdetG·Sr=

1

r!detG· dr

dλrλ=0det(λA−I) =

1 r!

dr

(6)

Due to the multilinearity of function det, on itsncolumn vectors, it follows immediately that

d

dλλ=0det[

λB1G1,· · ·, λBnGn] =

n X

i=1

(1)n−1det[G1,· · · , Bi

|{z} i-th term

,· · · , Gn],

leading to the conclusion

dr

dλrλ=0det(λB−G) =r! n X

1≤i1<...<ir≤n

(1)n−rdet[G1,· · ·, Bi1,

· · · , Bir,· · · , Gn]

and thus

Sr=

1

detG

n X

1≤i1<···<ir≤n

det[G1,· · ·, Bi1,· · ·, Bir,· · · , Gn]. (6)

Now, applying the expressions (4) and (5) in (6) we reach to the expression

Sr =

1

detG·Wr

n X

1≤i1<...<ir≤n

¨

fi1. . .f¨irdet[e1+ ˙f1∇F, . . . , ei1, . . . , eir, . . . , en+ ˙fn∇F]. (7)

Calculating the determinant on the right in the equality above, we get det[e1+ ˙f1∇F, . . . , ei1, . . . , eir, . . . , en+ ˙fn∇F] =

= 1 + X

i6=i1,...,ir

˙

fidet[e1, . . . , ei1, . . . , |{z}∇F i-th term

, . . . , eir, . . . , en]

= 1 + X

1≤i≤n i6=i1,...,ir

˙ fi2.

Consequently, the expression forSrin (7) assumes the following form

Sr=

1

detG·Wr

n X

1≤i1<...<ir≤n

¨

fi1. . .f¨ir(1 + X

1≤i≤n i6=i1,...,ir

˙ fi2).

Finally, using that detG=W2we obtain the desired expression

Sr =

1 Wr+2

n X

1≤i1<...<ir≤n

¨

fi1. . .f¨ir(1 + X

1≤i≤n i6=i1,...,ir

˙ fi2).

RESULTS

In order to prove Theorem 1 we need the following lemma.

Lemma 1. Letf1, . . . , frbe smooth functions of one real variable satisfying the differential equation r

X

k=1 ¨

f1(x1). . .f\¨k(xk). . .f¨r(xr)(β+ ˙fk

2

(7)

whereβis a positive real constant and the big hat means an omitted term. Iff¨i 6= 0, for eachi = 1, . . . r

then

r X

k=1

fk(xk) = r−1

X k=1 √ β ak ln

cos−σ a1. . . ar−1

r−2(a1, . . . , ar−1)

βxr+br

cos(ak√βxk+bk)

+c

whereai, bi, c,i= 1, . . . rare real constants withai, σr−2(a1, . . . , ar−1)6= 0.

Proof. Since the derivativesf¨i6= 0it follows thatf¨1(x1). . .f¨r(xn)6= 0. Thus dividing (8) by this product

we get the equivalent equation:

r X

k=1 β+ ˙fk

2 (xk)

¨ fk(xk)

= 0,

which implies, after taking derivative with respect toxlfor each l = 1, . . . r, that

β+ ˙fl

2 (xl)

¨ fl(xl)

!′ = 0,

thus β+ ˙fl

2 (xl)

¨ fl(xl)

= ˜alfor some non null constant˜al. Thus, settingal=

1 ˜ al

¨ fl(xl)

β+ ˙fl

2 (xl)

=al for eachl= 1, . . . , r

which can be easily solved to give:

arctan f˙l(xl)

β

!

=al p

βx+bl for some constantbl

and consequently

fl(xl) =−

1 al

p

βln|cos(al p

βxl+bl)|+cl, l= 1, . . . , r. (9)

Now, sincePr k=1

1 ak

= 0it implies that 1 ar

=σr−2(a1, . . . , ar−1)

a1. . . ar−1 , from (9) it follows that

fr(xr) =

σr−2(a1, . . . , ar−1) a1. . . ar−1

p

βln|cos(ar p

βxr+br)|+cr.

Consequently

r X

k=1

fk(xk) = r−1

X k=1 1 ak p βln

cos−σ a1. . . ar−1

r−2(a1, . . . , ar−1)

βxr+br

cos(ak√βxk+bk)

+c,

wherec=c1+. . .+cr.

(8)

Proof of the Theorem 1. From Proposition 1, we have thatMnhas zeroSrcurvature if, and only if,

X

1≤i1<...<ir≤n

¨ fi1. . .f¨ir

1 + X

1≤k≤n k∈{/ i1,...ir}

˙

fk2= 0. (10)

In order to ease the analysis, we divide the proof in four cases.

Case 1:Supposef¨i(xi) = 0,i= 1, . . . , nr+ 1. In this case, we have no restrictions on the functions fn−r+2, . . . , fn. Thus

Ψ(x1, . . . , xn) = (x1, . . . , xn, n−r+1

X

i=1

aixi+ n X

j=n−r+2

fj(xj) +b)

whereai, b∈Rand forl=n−r+ 2, . . . , n, the functionsfl:Il⊂R→Rare arbitrary smooth functions of one real variable. Note that the parametrization obtained comprise hyperplanes.

Case 2: Suppose f¨i(xi) = 0, i = 1, . . . , n r, then, there are constants αi such that f˙i = αi, for i= 1, . . . , nr. From (10) we have

¨

fn−r+1. . .f¨n(1 +α21+· · ·+α 2

n−r) = 0,

from which we conclude thatf¨k= 0for somek∈ {nr+ 1, . . . n}and thus, this case is contained in the

Case1.

Case 3:Now supposef¨i(xi) = 0,i = 1, . . . , nr 1andf¨k(xk) 6= 0, for everyk = nr, . . . , n.

Observe that if we hadf¨k(xk) = 0for somek=nr, . . . , nthe analysis would reduce to the Cases 1 and

2. In this case, there are constantsαisuch thatf˙i=αifor any1≤i≤n−r−1. From (10) we have

n X

k=n−r

¨

fn−r. . .f¨bk. . .f¨n(β+ ˙fk2) = 0

whereβ = 1 +

n−r−1

X

k=1

α2kand the hat means an omitted term. Then, from Lemma 1 we have that

n X

k=n−r

fk(xk) = n−1

X

k=n−r

β ak

ln

cos−σ an−r. . . an−1

r−1(an−r, . . . , an−1)

βxn+bn

cos(ak√βxk+bk)

+c

(9)

Case 4:Finally, supposef¨i(xi) = 0, where1ikandnk r+ 2, andf¨i(xi)6= 0for anyi > k.

We will show that this case cannot occur. In fact, note that for any fixedlk+ 1

X

k+1≤i1<...<ir≤n

¨ fi1. . .f¨ir

1 + X

1≤m≤n m6=i1,...ir

˙ fm2

= f¨l

X

k+1≤i1<...<ir−1≤n i1,...,ir−16=l

¨

fi1. . .f¨ir−1

1 + X

1≤m≤n m6=l,i1,...,ir−1

˙ fm2

+ X

k+1≤i1<...ir≤n i1,...,ir6=l

¨ fi1. . .f¨ir

1 + X

1≤m≤n m6=i1,...ir

˙ fm2

Derivative with respect to the variablexl(l≥k+ 1), in the above equality, gives ...

fl X

k+1≤i1<...<ir−1≤n i1,...,ir−16=l

¨

fi1. . .f¨ir−1

1 + X

1≤m≤n m6=l,i1,...,ir−1

˙ fm2

+ 2 ˙flf¨l

X

k+1≤i1<...<ir≤n i1,...,ir6=l

¨

fi1. . .f¨ir = 0. (11)

That is, if we set

Al =

X

k+1≤i1<...<ir−1≤n i1,...,ir−16=l

¨

fi1. . .f¨ir−1

1 + X

1≤m≤n m6=l,i1,...,ir−1

˙

fm2 and

Bl =

X

k+1≤i1<...<ir≤n i1,...,ir6=l

¨ fi1. . .f¨ir

then, it follows thatAl, Bldo not depend on the variablexland we can write

Al ...

fl+ 2Blf˙lf¨l= 0. (12) We have two possible situations to take into account:Case I.Al 6= 0,∀l≥k+ 1, andCase II.there is an

lk+ 1such thatAl= 0.

Case I. Al 6= 0:Under this assumption, there are constantsαl(l =k+ 1, . . . , n)such that equation (12) becomes...fl+ 2αlf˙lf¨l= 0. Furthermore, it can be shown that for{l1, . . . , lr+1} ⊂ {k+ 1, . . . , n}

∂r+1G

r(f1, . . . , fn)

∂xl1· · ·∂xlr+1

= 2

r+1

X

k=1

  f˙lkf¨lk

r+1

Y

m=1

m6=k ...

flm

 

 (13)

where

Gr(fk+1, . . . , fn) :=Wr+2Sr =

n X

k+1≤i1<...<ir≤n

¨

fi1. . .f¨ir(1 + X

1≤i≤n i6=i1,...,ir

(10)

SinceSr= 0it follows thatGr= 0, and using that r+1

Y

k=1 ˙

flkf¨lk 6= 0we obtain

r+1

X

k=1

  

rY+1

m=1

m6=k ...

flm ˙ flmf¨lm

 

 =

r+1

X

s=1

  f˙lsf¨ls

r+1

Y

m=1

m6=s ...

flm

  

r+1

Y

k=1 ˙ flkf¨lk

= 0. (14)

Now, forl=l1, . . . lr+1, substitute

...

fl+ 2αlf˙lf¨l= 0in (14) to obtain the identity

σr(αl1, . . . , αlr, αlr+1) = 0 (15) for anyl1, . . . , lr, lr+1∈ {k+ 1, . . . , n}. Hence we conclude that,

σr(αk+1, . . . , αn) = 0

σr+1(αk+1, . . . , αn) = 0.

These equalities, from [Proposition 1, Caminha (2006)], imply that at mostr1of the constantsαl(l ≥

k+ 1) are nonzero. Ifαl1 6= 0, . . . , αlm 6= 0withm ≤ r−1, in the expression obtained forBl, making

l6=l1, . . . , lm and taking derivatives with respect to the variablesxl1, . . . , xlmwe get lm

Y

j=l1 ...

fj ·σr−m( ¨fk+1, . . . ,f¨bl, . . . ,fb¨l1, . . . ,

flm, . . . ,f¨n) = 0

for alll∈ {k+ 1, . . . , n}r{l1, . . . , lm}. As...f

j 6= 0for allj∈ {l1. . . , lm}, we obtain that

σr−m( ¨fk+1, . . . ,fb¨l, . . . ,fb¨l1, . . . ,fb¨lm, . . . ,f¨n) = 0 for alll∈ {k+ 1, . . . , n}r{l1, . . . , lm}. Consequently,

σr−m( ¨fk+1, , . . . ,fb¨l1, . . . ,fb¨lm, . . . , ,f¨n) = 0

σr−m+1( ¨fk+1, , . . . ,fb¨l1, . . . ,fb¨lm, . . . , ,f¨n) = 0.

Since(nkm)(rm) =nkr 2, at mostrm1of the functionsf¨lare nonzero, for

k+ 1l nandl6=l1, . . . , lm, leading to a contradiction. So,αj = 0for allj ∈ {l1. . . , lr−1}, which

implies thatf¨lis constant for alll∈ {k+ 1, . . . , n}. Now, again from equation (11) we get

X

k+1≤i1<...<ir≤n i1,...,ir6=l

¨

fi1. . .f¨ir = 0, for anyl∈ {k+ 1, . . . , n}.

From which, we conclude that

σr( ¨fk+1, . . . ,f¨n) = 0

(11)

Therefore, at mostr1of the functionsf¨l (k+ 1≤l≤n)are nonzero, leading to a contradiction. Thus, it follows that Case 4 cannot occur, ifAl6= 0for everyl.

Case Al = 0:In this case, we haveBlf˙lf¨l= 0implying

Al =

X

k+1≤i1<...<ir−1≤n i1,...,ir−16=l

¨

fi1. . .f¨ir−1

1 + X

1≤m≤n m6=l,i1,...,ir−1

˙

fm2= 0 and

Bl =

X

k+1≤i1<...<ir≤n i1,...,ir6=l

¨

fi1. . .f¨ir = 0.

Derivative ofAlwith respect to variablexs, fors=k+ 1, . . . , nands6=l, gives

...

fs X

k+1≤i1<...<ir−2≤n i1,...,ir−26=l,s

¨

fi1. . .f¨ir−2

1 + X

k+1≤m≤n m6=l,s,i1,...,ir−2

˙ fm2

+2 ˙fsf¨s

X

k+1≤i1<...<ir−1≤n i1,...,ir−16=l,s

¨

fi1. . .f¨ir−1 = 0. (16)

Now, fori1, . . . , ir ∈ {k+ 1, . . . , n}with i1, . . . , ir, l distinct indices, taking the derivatives of Bl with respect toxi1, . . . , xir gives

...

fi1. . ....fir = 0.

Consequently, for at mostr1indices, sayi1, . . . , ir−1, we can have

...

fim 6= 0,(m = 1, . . . , r1), and

...

fj = 0for everyj = k+ 1, . . . , n, withj 6= l, i1, . . . , ir−1. Thus

...

fim 6= 0, withim 6= l, together with equation ∂Bl

∂xim = 0implies that the sum X

k+1≤i1<...<ir−1≤n i1,...,ir−16=l,im

¨

fi1. . .f¨ir−1 = 0.

Now, if...fj = 0we have by equation (16) that

X

k+1≤i1<...<ir−1≤n i1,...,ir−16=l,j

¨

fi1. . .f¨ir−1 = 0.

Therefore, X

k+1≤i1<...<ir−1≤n i1,...,ir−16=l,j

¨

fi1. . .f¨ir−1 = 0, j=k+ 1, . . . , n andj 6=l

From which, we conclude that

σr−1( ¨fk+1, . . . ,fb¨l, . . . ,f¨n) = 0

σr( ¨fk+1, . . . ,fb¨l, . . . ,f¨n) = 0.

(12)

Proof of the Theorem 2. LetMn Rn+1 be a translation hypersurface with constant

Srcurvature. First, note that

∂mWr+2 ∂xi1· · ·∂xim

=

m Y

j=1

(r+ 42j)·

m Y

k=1 ˙

fikf¨ik·W

r+2−2m. (17)

We have as a consequence of the proof of Theorem 1, see (13), the identity

∂r+1G

r(f1, . . . , fn)

∂xl1· · ·∂xlr+1

= 2 r+1 X k=1   f˙lkf¨lk

r+1

Y

m=1

m6=k ...

flm

  

whereGr(f1, . . . , fn) =

n X

1≤i1<...<ir≤n

¨

fi1. . .f¨ir(1 + X

1≤i≤n i6=i1,...,ir

˙

fi2). With this we conclude, by Proposition 1,

that

r+1

Y

j=1

(r+ 42j)·

r+1

Y

k=1 ˙

flkf¨lk·W

−rS

r =

∂r+1(Wr+2S

r)

∂xl1· · ·∂xlr+1

= 2 r+1 X k=1   f˙lkf¨lk

r+1

Y

m=1

m6=k ...

flm

 

. (18)

Now, we have two cases to consider:rodd andreven.

Case rodd:Suppose that there arel1, . . . , lr+1such that

r+1

Y

k=1 ˙

flkf¨lk 6= 0. Then,

Qr := r+1

Y

j=1

(r+ 42j)·W−rSr = 2 r+1

X

s=1

  f˙lsf¨ls

r+1

Y

m=1

m6=s ...

flm

  

rY+1

k=1 ˙ flkf¨lk

= 2 r+1 X k=1    r+1 Y m=1

m6=k ...

flm ˙ flmf¨lm

  .

Therefore,

∂r+1Qr

∂xl1· · ·∂xlr+1

= 0.

On the other hand, using (17) we obtain

∂r+1Q

r

∂xl1· · ·∂xlr+1

=

r+1

Y

j=1

(r+ 42j)

r+1

Y

i=1

(r+ 22i)

r+1

Y

k=1 ˙ flkf¨lkW

(13)

Sinceris odd, we conclude thatr+ 42j6= 0andr+ 22j6= 0, for anyj Nand, therefore,Sr = 0.

Now, if for at mostrindices we havef¨j 6= 0for examplej=l1, . . . , lrthen

Wr+2Sr = ¨fl1· · ·f¨lrα, for some constantα6= 0. Thus,

(r+ 2)Wrf˙l1f¨l1Sr = ...

fl1f¨l2· · ·f¨lrα. If...fl1 = 0, thenSr= 0. Otherwise,

(r+ 2)Wr+2f˙l1f¨l1Sr= ...

fl1f¨l2· · ·f¨lrW

2

α (r+ 2) ˙fl1( ¨fl1)

2

=...fl1W2.

Asr >1implies thatW does not depend on the variablesxl2, . . . , xln, it follows thatf¨l2 =· · ·= ¨fln= 0 leading to a contradiction.

Case reven:In this case, there is a naturalq2such thatr= 2q. Thenr+ 1q+ 2and consequently

r+1

Y

k=1

(r+ 42k) = 0.

Therefore, by (18) we get

r+1

X

k=1

  f˙lkf¨lk

r+1

Y

m=1

m6=k ...

flm

  = 0.

Suppose that there arel1, . . . , lr+1such that

r+1

Y

k=1 ¨

flk 6= 0. In this case,

r+1

X

k=1

  

r+1

Y

m=1

m6=k ...

flm ˙ flmf¨lm

  = 0.

We conclude that for eachlithere is a constantαli such that ...

fli =αlif˙lif¨li. Now, it is easy to verify (see (11)) that

(r+ 2) ˙flr+1f¨lr+1W rS

r =

∂ Gr(f1, . . . , fn)

∂xlr+1

= ...flr+1Gr−1(f1, . . . ,fbl, . . . , fn)

+ 2 ˙flr+1f¨lr+1

X

1≤i1<...<ir≤n i1,...,ir6=lr+1

¨

fi1. . .f¨ir.

Therefore,

(r+ 2)WrSr=αlr+1Gr−1(f1, . . . ,fblr+1, . . . , fn) + 2

X

1≤i1<...<ir≤n i1,...,ir6=lr+1

¨

(14)

Differentiating this identity with respect to the variablexlr+1, gives

(r+ 2)rf˙lr+1f¨lr+1W r−2

Sr= 0 implying that Sr= 0.

Finally, suppose that for any(r+ 1)-tuple of indices, sayl1, . . . , lr+1it holds that

r+1

Y

k=1 ¨

flk = 0. Then,

σr+1( ¨f1, . . . ,f¨n) = 0

σr+2( ¨f1, . . . ,f¨n) = 0.

Implying that at leastnr derivativesf¨l vanish, i.e., there are at mostr functions such thatf¨j 6= 0for examplej=l1, . . . , lr. Thus, by Proposition 1

Wr+2Sr= ¨fl1· · ·f¨lrα

for some constantα 6= 0. We conclude thatSr = 0analogously to the way it was presented for the caser odd.

ACKNOWLEDGMENTS

The authors would like to express their gratitude to referee for valuable suggestions on the improvement of the paper. The first, second and third author are partially supported by Coordenação de Aperfeiçoamento de Pessoal de Nível Superior (CAPES). The fourth author is partially supported by CAPES and Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq).

REFERENCES

CAMINHA A. 2006. On spacelike hypersurfaces of constant sectional curvature lorentz manifolds. J Geom Phys 56: 1144-1174. CHEN BY. 2011. On some geometric properties ofh-homogeneous production functions in microeconomics. Kragujevac J Math

35(3): 343-357.

CHEN C, SUN H AND TANG L. 2003. On translation Hypersurfaces with Constant Mean Curvature in(n+ 1)-Dimensional

Spaces. J Beijing Inst Tech 12: 322-325.

DILLEN F, VERSTRAELEN L AND ZAFINDRATAFA G. 1991. A generalization of the translational surfaces of Scherk. In Differential Geometry in honor of Radu Rosca, Belgium: Catholic University of Leuven, p. 107-109.

INOGUCHI JI, LÓPEZ R AND MUNTEANU MI. 2012. Minimal translation surfaces in the Heisenberg groupN il3. Geometriae

Dedicata 161(1): 221-231.

LEITE ML. 1991. An example of a triply periodic complete embedded scalar-flat hypersurface ofR4. An Acad Bras Cienc 63:

383-385.

LIMA BP, SANTOS NL AND SOUZA PA. 2014. Translation Hypersurfaces with Constant Scalar Curvature into the Euclidean Space. Israel J Math 201: 797-811.

LIU H. 1999. Translation Surfaces with Constant Mean Curvature in 3-Dimensional Spaces. J Geom 64: 141-149. LÓPEZ R. 2011. Minimal translation surfaces in hyperbolic space. Beitr Algebra Geom 52: 105-112.

LÓPEZ R AND MORUZ M. 2015. Translation and homothetical surfaces in Euclidean space with constant curvature. J Korean Math Soc 52(3): 523-535.

LÓPEZ R AND MUNTEANU MI. 2012. Minimal translation surfaces inSol3. J Math Soc Japan 64(3): 985-1003.

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