Advances in Pure Mathematics, 2012, 2, 220-225
http://dx.doi.org/10.4236/apm.2012.24032 Published Online July 2012 (http://www.SciRP.org/journal/apm)
Minimal Surfaces and Gauss Curvature of Conoid in
Finsler Spaces with (α, β)-Metrics*
Dinghe Xie, Qun He
Department of Mathematics, Tongji University, Shanghai, China
Email: x_dinghe8707@126.com
Received December 26, 2011; received March 18, 2012; accepted March 26, 2012
ABSTRACT
In this paper, minimal submanifolds in Finsler spaces with (α, β)-metrics are studied. Especially, helicoids are also
minimal in (α, β)-Minkowski spaces. Then the minimal surfaces of conoid in Finsler spaces with (α, β)-metrics are
given. Last, the Gauss curvature of the conoid in the 3-dimension Randers-Minkowski space is studied.
Keywords: Isometrical Immersion; Minimal Submanifold; (α, β)-Metric; Conoid Surface; Gauss Curvature
1. Introduction
In recent decades, geometry of submanifolds in Finsler
geometry has been rapidly developed. By using the
Busemann-Hausdorff volume form, Z. Shen [1] intro-
duced the notions of mean curvature and normal curva-
ture for Finsler submanifolds. Being based on it, Bern-
stein type theorem of minimal rotated surfaces in Rand-
ers-Minkowski space was considered in [2]. Later, Q. He
and Y. B. Shen used another important volume form, i.e.,
Holmes-Thompson volume form, to introduce notions of
another mean curvature and the second fundamental form
[3]. Thus, Q. He and Y. B. Shen constructed the corre-
sponding Bernstein type theorem in a general Minkowski
space [4].
The theory of minimal surfaces in Euclidean space has
developed into a rich branch of differential geometry. A
lot of minimal surfaces have been found in Euclidean
space. Minkowski space is an analogue of Euclidean
space in Finsler geometry. A natural problem is to study
minimal surfaces with Busemann-Hausdorff or Holmes-
Thompson volume forms. M. Souza and K. Tenenblat
first studied the minimal surfaces of rotation in Randers-
Minkowski spaces, and used an ODE to characterize the
BH-minimal rotated surfaces in [5]. Later, the nontrivial
HT-minimal rotated hypersurfaces in quadratic (α, β)-
Minkowski space are studied [6]. N. Cui and Y. B. Shen
used another method to give minimal rotational hyper-
surface in quadratic Minkowski (α, β)-space [7]. How-
ever, these examples only consider the special (α, β)-
metrics either Randers or quadratic. Therefore, what is
the case with the general (α, β)-metric?
The main purpose of this paper is to study the conoid
in (α, β)-space. It includes minimal submanifolds in
Finsler spaces with general (α, β)-metric (F




)
and the Causs curvature in Randers-Minkowski 3-space.
We present the equations that characterize the minimal
hypersurfaces in general (α, β)-Minkowski space. We
prove that the conoid in Minkowski 3-space with metric
F




:0,FTM
is minimal if and only if it is a helicoid or
a plane under some conditions. Finally, similar to [7], we
give the Gauss curvature of conoid in Randers-Min-
kowski 3-space and point out that the Gauss curvature is
not always nonpositive on minimal surfaces.
2. Preliminaries
Let M be an n-dimensional smooth manifold. A Finsler
metric on M is a function satisfying
the following properties: 1) F is smooth on
\0TM ; 2)
,,
F
xy Fxy

0 for all
; 3) The induced
quadratic form g is positively definite, where
2
:,dd,
1
:.
2ij
ij
ij
ij yy
g
gxyx x
gF



(1)
Here and from now on,
i
F
,
ij
y
y
F mean
F
,
i
y
2
ij
F
yy

1,,;1 ,,.ijnm n

 
, and we shall use the following convention of
index ranges unless otherwise stated:
*Project supported by NNSFC (no. 10971239, no. 10771160) and the
N
atural Science Foundation of Shanghai (no. 09ZR1433000).
C
opyright © 2012 SciRes. APM
D. H. XIE, Q. HE 221
The projection gives rise to the pull-
back bundle and its dual , which sits
over . We shall work on and rigidly
use only objects that are invariant under positive re-
scaling in y, so that one may view them as objects on the
projective sphere bundle SM using homogeneous coor-
dinates.
π:TM M
**
πTM

\0TM
**
πTM
*
πTM

\0TM
In there is a global section
d
i
i
y
F
x
,
called the Hilbert form, whose dual is ,
i
i
ll
x
ii
lyF
dV
ˆ
, called the distinguished field.The volume
element SM of SM with respect to the Riemannian
metric
, the pull-back of the Sasaki metric on
, can be expressed as

\0TM
ddd,Vx
SM
  (2)
where
1
dd,
n
:det, d
ij
g
x
xx 
d d
i
n
y y
F



 (3)

11
1
d:1 d
nii
i
yy
 
.
(4)
The volume form of a Finsler n-manifold (M, F) is
defined by
 
1
1d,
x
SM
n
c
d: d,:
M
Vxxx


1n
c

(5)
where denotes the volume of the unit Euclidean
(n 1)-sphere ,
1n
S
xx
y yTM=SM
,
.
Let (M, F) and
M
F

be Finsler manifolds, and
:
f
MM

,
be an immersion. If


,d
F
xyF fxf

y for all
,\0TM

,,
i j
xy ,
then f is called an isometric immersion. It is clear that

,
ij
g
xygxy ff


,

(6)
for the isometric immersion
:,
f
MF MF
, where

x
fx

, i
i
y
fy

, ii
f
f
x
. Let

*
πTM
be the orthogonal complement of in
*
πTM
*1
π
f
TM
with respect to
, and set
2
,
,,
k
k
fGG
h
h
ij
ij
hfyy
hgh
F
x




(7)
where
2
ij
ij
f
f
x
x

k
G G, and
are the geodesic
coefficients of F and
F

*
πhT
respectively. We can see that
(see (1.14) in [3]), which is called the
normal curvature. Recall that for an isometric immersion
M
:, ,
f
MF MF
, we have (see formulae (2.14) and
(3.14) of Chapter V in [8])
,
kk ij
ij
GfyyG


.
klk
l
(8)
gg
f
where

From (2.7), it follows that
,
ij
ij
hpfyyG


:.
i
i
pf

(9)
where

 Set
2
1
1dd,
SM
x
n
h
x
cF





(10)
which is called the mean curvature form of f. An isomet-
ric immersion

:, ,
f
MF MF
0
is called a minimal
immersion if any compact domain of M is the critical
point of its volume functional with respect to any varia-
tion vector field. Then f is minimal if and only if
.
3. Minimal Hypersurfaces of (α, β)-Spaces
Here and from now on, we consider general (α, β)-metric.
Let

s
s
C is a positive
F
s

, , where
function on
00
,bb

,

,,
ij i
ij i
axyy bxy



0
0.
ij
ij
abbbb b

1
If
s
s
, then F is a Randers metric. If
is
an Euclidean metric and
is parallel with respect to
, F is a locally Minkowski metric and (M, F) is called
an (α, β)-Minkowski metric. By [9], F is a Finsler metric
if and only if
s
satisfies

22
0
() 0,
s
.ss bsssbb
 

 
 
(11)
Let
det ,det,.
ijij n
g
Aag g
F

 
,
n
(12)
It have been proved ([9]) that
g
sHsA
 

222 .
n
Hsssb s
(13)
where
 


In the following part, we will discuss minimal hyper-
surfaces in Minkowski space with (α, β)-metric. Let
:, ,MFMF
be an isometric immersion,

f
Fs
 





, where
Copyright © 2012 SciRes. APM
D. H. XIE, Q. HE
222
,
,.yy bya

 
 
tric immer

Since f is an isomesion, we get
*
Ff ,F





where
,,
,.
j
i
iii
ayyaa f f
bybbf
ij
ijij i



hat (M, F) is a hype of

,
Note trsurface
M
F

, let
nne
be the unit normeld of al vector fi
f
M with
respect to
and nne
 it nmal vector
fiel ect to
be the unor
d of M with resp
ely. That is , respectiv
0, 0,
ii
nfg nf
 




,1,1.nnangnngn n
 
 


,n
There exist a function

,
x
y
on SM , sch that
,
u
g
nan



1
,,ann



where gnn


. Then
ga.n n


14)
From above, we know that f is minial if and only if
 (
m
2d0.
h
F
 (15)
ca
G
x
SM
n
From (3.3) and (3.4), a
nd in a similar way as in [5], we
n get
ij
ij
ij
hghg fyy
gnn

2.
ij
fy
yG an an
 







 






1
2.
n1
22
n
A
AHA
gg HA
AA

 

Then (3.5) is equivalent to



d0.
ij
ij
fy
y G

122
2
x
n
n
SM
ssbs
na

 

 


(16)

If F




is an (α, β)-Minkowski metric,
0. In Minkowski-(α, β) space, f is minimal if and
only if
then
G


122
n
ssbs


 


2
xn
d0.
ij
ij SM
yy
fn
em 1 Let (M, F) be a hypersurface of
(17)
Theor
M
F

,
and
F




be an (α, β)-Minkowski metric. Then
:, ,
f
MF MF
is a minimal immersion if and
only if




22
()
ij
ij Sx
fn yy
b

  


1n
()
 
d 0,


 
(18)
x
S is a sphere such that 1
where
.
Now, we consider the conoid in 3-dimensional (α, β)-
Minkowski space paralleling to x3-axis. Set



,
F
where
  
222
123 3
,,
y
yy by

 
 
and b
is a constant. Let
sin ,
cos ,
f
uvu,
vhv
where
hv is a unknown function. Then

23
cossin0 ,
sin cos
i
vv
fuvu vh




1
12122
cossin 0
s
cossin sincos.
vv
vh
yvuyvyvuy vyh

23 12
sin co
yy yyyuvu

 
Assume that

 
12
2
2
1
cos ,sinyy
uh

,
0, 2π,
then
  




222
123
22
2
12 2
1.
yy y
yuhy

 
 
Note thatal vector of the surface is

the norm
 
22 2
22 2
sin cos
,, ,
hvh vu
n
hu huhu






 
 

and

 



11 13
12 21
13 13
22 13
000,
sincos0 ,
=cos sin.
f
ff vv
fuvuvh





Set

 


22 d,
ijij
Sx
Wyy
b





 


 
(19)
Copyright © 2012 SciRes. APM
D. H. XIE, Q. HE 223
Then (3.8) is equivalent to

22
22
20.nW


(20)
Since
312
12
1
fnW f

x
S is symmetric with resp 1
ect to
y
and
ision onlyding on a funct depen 2
y
,


 

121 2
22
Sx
Wyy
b



 

 

d
 


22 0, .W u
ver, 22 0W is impossible. Recall th
0,
Therefore, (3.10) becomes to
uh
Howe at

 
2
2
22 2
2d, 0
xn
S
g
Wys
s


,
and 2
y
is not identically vanishing, we can obtain
W. Then 0h ,
,hcvd
wThe Let

3,VF
be an (α, β)-Minkowski
22 0
here c, d are arbitrary constants.
orem 2
space, 3
,
F
by


, and





sin,cos ,
f
uv
if and only if f i
uvhv be a conoid. Then f imal
s a helicoid or a plane.
ma
helicoid al nt
in (α, β)ski swhere 3
by
. This is an
interesting result for minisurf
ition 3
by
is we co
tion:
s mini
Rerk 3.1 From theorem 2, we can affirm that a
is minim o only in Euclidean space but also
Minkowpace,
mal aces.
But whether the result hold if the cond
not satisfied? Nownsider the following condi-
123
12 3
cossin
byb yby
bvbv





12
12 21
cossin ,ybvbvy

 

where 123
,,bbb
 
are not all zeros. To simplify the com-
putation, we only discuss quadratic (α, β)-metric:
2
Fk
 . Set 112
cos sinBb vbv

,


3
3
0
0,
Cvu
uCv


(21)
where
22 1
cos sinBbvb v

. Then (3.8) becomes an equation
respect to u:
 
 
54
54
2
21
Cv
u Cvu
Cvu Cv
4
52
15 ,
8
CBh



2
22
133 2
,
2B
bbhB


4
15
C hh

23
12
32224222
23321
2222 2
11
15 4539 π
2484
π
π21,
2
B
Bb hbBkB hkB B
kBkbB kbh
2 322
3 121212
3342CkBkBBkBBkbBBh
1 2




 



5
3222
22313223
15 9
9,
22
CBbhhkBbBhkBbhh
 






4
4
13
3
23222 2
211 13
242222
111
2
22 2
31
15
8
342 2
3ππ
8
921 ,
4
Cbhh
BkBkBkbBkbh
kBkBk bB
kbBkbh h








4
22
0311
31 .CkbBBh
 
Since (3.11) is valid for any u, we can obtain
00,,5,.
i
Ci v

If 10b
or 20b
, then 10B or 20B
, such
that . Therefore, when 12
,bb

are not all zeros,
0hv
hv const. That is to say a minimal conoid hypersur-
face is a plane with respect to the given metric above.
Theorem 3 Let
3,VF
be an (α, β)-Minkowski
space, where
2
Fk

b
satisfying
123
byb yby
 
 

(,bb

are not all zeros). Then a
mne.
4. Gauss Curvature of Conoid in Randers
all kn
m
dy the Gauss curvatun Min-
kowski-Randers 3-space around x
3-axis in the direction
#
12 312
inimal conoid hypersurface in

3,VF
is a pla
3-Space
As we own, the Gauss curvature of a minimal sur-
face is nonpositive everywhere in Euclidean space. Then,
a fact honatural problem arises: whether this lds for
inimal surfaces in Minkowski-Randers 3-space? In this
section, we sture of conoid i
, that is #3
by
. Consider the conoid
,cos,sin,
f
uvuvuvh v, w0 and vShere u1
.
Let 1def
u



, 2def
v



. Then 12
ye e

es a natur
gival coordinates

,,,uv
on its tangent
bundle. In this section we shall use the convention that
1, 2ij
and 1, 3
. Besides, the notations
12
:, :uv

and 12
:, :yy
are also used.
Note that the induced 1-form *
f
on the surface
is closed. Then the Ricci curvature tensor of *
F
fF
is given by ([10], Page 118)
Copyright © 2012 SciRes. APM
D. H. XIE, Q. HE
224
23
4
Ric Ricr
F

where
2
00 00|0
12 ,Fr (22)
Ric

denotes the Ricci curvature tensor of the
ced Riemindu*
annian metric
f
, 00
r
efficients of the covarie
|
ij
ij
byy and
b denote the cnt derivatives
|ij
of
o
with respect to .
Thuss curvature of
the surface is given by

en the Ga


2
2
132,
4
F
KrFr
00 00|0
4
Ricy
K,xy
F
 
(23)
where

,,
x
fuv
K
denotes the Gau
to
ss curvature
with respect
.
te Denoii
f
z
and
2
.
ij ij
f
z

Then


23
cossin0 ,
sin cos
i
vv
zu vhv




000,

cos0 ,vv


ature is computed in Euclid-
ean space as follows:
v
u

11 13
z
 
12 21
1313 sinzz



cos sizuv

22 13
e Gauss curv
n .uvh

Noting that th
2
2,
LN M
EG F
wher
22
,,,LznMznNz n
K
e
11 12


22
.Gzz
11 12
,,Ezz Fzz

 


n obtain By direct computation, we ca

2
2
22
.
h
(24)
cients of *
K
i
uh
Meanwhile, the coeff
f
are given by

2
10
,
uh






ij 2
0
a


1
0
kl
kl
aa

where iji j
azz
2
2
10
1,
uh





. It is easy to verify that
kkl
ijl ij
azz

 . By a direct computation, we have
100
,


0
ij u

2
 
2
2
22
22
0
.
ij
u
uh
uhh
uh uh











Since 3
ii
bbz,
22
0
.
s
s ij
hu
uh
b b



|,
22 22
j
ij i
bb uh
h
uh uh

h







From
||| |
|, k
s
s
ijkisjksj ik
ij
bb bb
 , we have

2
1|1| 22
22
2,
bu h
b
uh

2
2|1|12|12
22
,
buh
bb
uh


1|

22
1| 2| 22|1| 22
22
,
buh
bb hu
uh

 

3
2|2|1 2
22
2,
buh
b
uh


2
2
2|2|2 2222
21
.
bh u
bh
uhuh


 




Besides,

22
12 2
00 |22 22
2,
ij
ij
buhu h
rbyyyyy
uh uh

 







22
12
00|0| |2
22
2
2212
2
22
23
22
2222
4
22
21
ijk
ijk
bu h
rbyyyyy
uh
buh huyy
uh
bh uhy
uh uh










(4.2) and (4.3), we obtain the following
theorem.
Theorem 4 Let
Then, from
3,VF
be an Randers-Minkow
space with 3
by
, the Gauss curvature of the conoid
ski
,cos,sin,uvuvuvhv at

,
f
x
fuv in direc-
tion of 12
yee
is given by

0212222
4
334253 64
1
,128
4
12443,
Kxyb bF
F
bbbF
 
 
 
 


where
Copyright © 2012 SciRes. APM
D. H. XIE, Q. HE
APM
225
Copyright © 2012 SciRes.
 



222
01
22
22 22
3
34
2
2
2
22
2
22
22 22
24
526
2222 2
22
,,,
,2,
1,.
huhuh
uh uhuh
uhhuh hu
uh uh
uh uh
h
uhuh uh

  



 





 




to (α, 3
2
Note that a helicoid is minimal if and only if it is a
conoid with respectβ)-metrics (where by
).
Let
hvcv d
(c is a constant), then the Gauss cur-
vate y
ur of this surface is given b

222
4
12,y bF
F
 
 

(25
where
02122
,3Kx b

 
)
 
222 2
12
22 2
22 2222
,, .
ccucu
uc ucuc
 

However, for

,
0

a given point
x
fuv, in which
directions of
x
TS,

,0?y

,0Kxy,

,0Kxy,
1)
Kx
If 0
, then

,<0Kxy for any 0c;
2) If 0
, Since
22ij i
ij i
F
ayy byu ccb


,
Equation (4.4) becomes


2
3
3
cbu
Kxy c
uc uc cb




0, let 0
2
2
22 22
12
,.
If c
, then


2
3
22
.
cbu
u c

we ca
2
2
22
12
,Kxy c
uc cb


an also mke
2
u
2
3
22
20
cb
c
cbu c


, then

,0Kxyrwise, let 0; Othe
, then


2
2
23
22 22
12
,.
cbu
Kxy c
uc cbuc


we can make
2
2
3
2
20
cbu
cb c
2
c
u
, then

,0Kxy. In sum, the Gauss curvature is not nonposi-
tive anywhere.
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