Applied Mathematics, 2011, 2, 1317-1322
doi:10.4236/am.2011.211184 Published Online November 2011 (http://www.SciRP.org/journal/am)
Copyright © 2011 SciRes. AM
On Generalized φ-Recurrent Sasakian Manifolds
Absos Ali Shaikh, Helaluddin Ahmad
Department of Mathematics, The University of Burdwan, Bur dwan , India
E-mail: aask2003@yahoo.co.in
Received July 22, 2011; revised September 13, 2011; accepted September 20, 2011
Abstract
The object of the present paper is to introduce the notion of generalized φ-recurrent Sasakian manifold and
study its various geometric properties with the existence of such notion. Among others we study generalized
concircularly φ-recurrent Sasakian manifolds. The existence of generalized φ-recurrent Sasakian manifold is
given by a proper example.
Keywords: Locally φ-Symmetric Sasakian Manifold, φ-Recurrent Sasakian Manifold, Generalized
φ-Recurrent Sasakian Manifold, Scalar Curvature
1. Introduction
Let M be an n-dimensional connected Riemannian mani-
fold with Riemannian metric g and Levi-Civita connec-
tion . M is called locally symmetric if its curvature
tensor is parallel with respect to . During the last ve
decades, the notion of locally symmetric manifold has
been weakend many authors in different directions such
as recurrent manifold by Walker [1], semi-symmetric
manifold by Szabό [2], pseudo-symmetric manifold by
Chaki [3], pseudo-symmetric manifold by Deszcz [4],
weakly symmetric manifold by Tamássy and Binh [5],
weakly symmetric manifold by Selberg [6]. However,
the notion of pseudo-symmetry by Chaki and Deszcz are
different and that of weak symmetry by Selberg and Ta-
mássy and Binh are also different. As a weaker version
of local symmetry, in 1977 Takahashi [7] introduced the
notion of local φ-symmetry on a Sasakian manifold. By
extending the notion of local φ-symmetry of Takahashi
[7], De et al. [8] introduced and studied the notion of
φ-recurrent Sasakian manifold. It may be mentioned that
locally φ-symmetric and φ-recurrent LP-Sasakian, (LCS)n
and (k, µ)-contact metric manifolds are respectively stu-
died in [9-13].
Again, in 1979 Dubey [14] introduced the notion of
generalized recurrent manifold and then such a manifold
is studied by De and Guha [15]. The manifold M, n > 2,
is called generalized recurrent [14] if its curvature tensor
R of type (1,3) satises the condition
RARBG , (1)
where A and B are nowhere vanishing unique 1-forms
defined by A(·) = g(·, ρ1), B(·)=g(·, ρ2) and G is a tensor
of type (1,3) given by

,, ,GXYZgYZX gXZY (2)
for all vector fields

,,
X
YZ M
;

M
being the
Lie algebra of all smooth vector fields on M and
is
the Levi-Civita connection. Again M, n > 2, is called
generalized Ricci-recurrent manifold [16] if its Ricci
tensor S of type (0, 2) satises the condition
SASBg
 (3)
where A and B are nowhere vanishing unique 1-forms.
The object of the present paper is to introduce a type
of non-at Sasakian manifolds called generalized φ-re-
current Sasakian manifold, which includes both the no-
tion of local φ-symmetry of Takahashi [7] and also φ-
recurrence of De et al. [8] as particular cases. The paper
is organized as follows. Section 2 deals with some pre-
liminaries of Sasakian manifolds. Section 3 is devoted to
the study of generalized φ-recurrent Sasakian manifolds
and it is shown that such a manifold is generalized
Ricci-recurrent [16]. In Section 4, we study generalized
concircularly φ-recurrent Sasakian manifolds and it is
shown that in a generalized concircularly φ-recurrent
Sasakian manifold the vector field ρ2 associted with the
1-form B and the characterstic vector field ξ are co-di-
rectional. We also introduce the notion of super genera-
lized Ricci-recurrent manifolds and proved that a gener-
alized concircularly φ-recurrent Sasakian manifold is such
one. Also the existence of generalized φ-recurrent Sasa-
kian manifold is ensured by a proper example in the last
Section.
A. A. SHAIKH ET AL.
1318
0
g
2. Sasakian Manifolds
An n= (2m + 1)-dimensional C manifold M is said to be
a contact manifold if it carries a global 1-form η such
that everywhere on the manifold. Given
a contact form η, it is well-known that there exists a
unique vector field ξ, called the characteristic vector field
of η, satisfying and for any
vector field X on M. A Riemannian metric g is said to be
an associated metric if there exists a tensor field φ of
type (1,1) such that

0
m
d



1


,dX

  
2, ,, d,,Ig
 
   (4)
 
0,0, ,,gg
 
 (5)

,,gg
 

. (6)
Then the structure
,,,

on M is called a con-
tact metric stucture and the manifold M equipped with
such a stucture is called a contact metric manifold [17].
Given a contact metric manifold M we dene a (1,1)
tensor field h by 1£
2
h
, where denotes the ope- £
rator of Lie differentiation. Then h is symmetric. The
vector field ξ is a Killing vector field with respect to g if
and only if . A contact metric manifold M for
which ξ is a Killing vector is said to be a K-contact ma-
nifold. A contact structure on M gives rise to an almost
complex structure J on the product
0h
M
defined by
dd
,,(
dd
JXfX fX
tt




 ),
where f is a real valued function, is integrable, then the
structure is said to be normal and the manifold M is a
Sasakian manifold. Equivalently, a contact metric mani-
fold is Sasakian if and only if


,RXYYX XY
 
 (7)
holds for all X, Y where R denotes the curvature tensor of
the manifold.
In an n-dimensional Sasakian manifold M the follow-
ing relations hold [17-19]:

,,
,,
 
 

X
RXYYgXY YX
RX Y (8)


,,
XX
X
YgXY
 
 , (9)


 
,, ,RXYZgYZXgXZY


1,
, (10)

,1,,

 SXnX Sn (11)

 
,,1SXY SXYnXY
 
 , (12)

 
,, 1,
WSYSYWn gYW
 

 

,,
,,




WRXY gWYX
,
g
WXYRXYW (14)

 
,,
,,,



WRXZgXZ W
g
ZWXRXWZ (15)
for all vector fields

,,,
X
YZWM .
Denition 1. [7] A Sasakian manifold is said to be lo-
cally φ-symmetric if

2,
WRXYZ
0
(16)
for all vector fields X, Y, Z, W orthogonal to ξ.
Denition 2. [8] A Sasakian manifold is said to be
φ-recurrent if there exists a nowhere vanishing unique
1-form A such that

2,,
WRXYZ AWRXYZ
 (17)
for all vector fields

,,,
X
YZWM
.
Especially, if the 1-form A vanishes and the vector
fields are horizontal, then the manifold turns to be a lo-
cally φ-symmetric Sasakian manifold [7].
3. Generalized φ-Recurrent Sasakian
Manifolds
Denition 3. An n-dimensional, n 3, Sasakian mani-
fold M is said to be a generalized φ-recurrent if its cur-
vature tensor satisfies the relation


 

22
2
,,
,


WR XYZAWRXYZ
BWG XY Z
(18)
for all
,,,
X
YZWM
, where A and B are nowhere
vanishing unique 1-forms such that

1
,AX gX
,
2
,gXBX
and G(X, Y )Z is defined in (2).
We consider a Sasakian manifold M, n 3, which is
generalized φ-recurrent. Then by virtue of (4), (18)
yields



 

 

,,
,,
,,,



WW
R XYZR XYZ
AWR XYZRXY Z
BW GXYZGXYZ
(19)
from which it follows that



 




 




,, ,
,, ,
,, ,




.


WW
g
RXYZURXYZ U
AWg RXYZUR XYZU
BWgG XY ZUG XY ZU
(20)
Let
:1,2,,
i
ei n be an orthonormal basis of the
tangent space at any point of the manifold. Then putting
, (13)
Copyright © 2011 SciRes. AM
A. A. SHAIKH ET AL.1319
X = U = ei in (20) and taking summation over i, 1 i n,
and using (15), (10), (8) and (2), we get


 

 


,,
2,
.


 

WSYZ AWSYZ
nBWAWgYZ
AW BWYZ
(21)
Setting Z = ξ in (19) and using (7), (2), (14) and (10)
we obtain

 


,
WRXYAW BWYXXY


 
.
(22)
From (14) and (22), we obtain

 


,,,
.
 



 

g
WYXgW XYRXYW
AWBWYXX Y (23)
Taking inner product of (23) with Z and then taking
contraction over X and Z, we get
 

 
,(1),SY WnAWBWYgWY

 

.
(24)
Putting Y
in (24) we get
 
0AW BW for all W. (25)
This leads to the following.
Theorem 1. In a generalized φ-recurrent Sasakian
manifold M, n 3, the associated 1-forms A and B are
related by the relation .
0AB
In view of (25), (21) turns into

    
,,
WSYZAWSYZ bWgYZ ,
, (26)
where . This leads to the follow-
ing.
 
(3)bWn AW
Theorem 2. A generalized φ-recurrent Sasakian mani-
fold M, n 3, is generalized Ricci-recurrent.
4. Generalized Concircularly φ-Reccurent
Sasakian Manifolds
The concircular transformation on a Riemannian mani-
fold is a transformation under which geodesic circles re-
mains invariant [20]. The concircular curvature tensor
of type (1,3) is given by [20]
C
(,) (,)(,)
(1)
r
CXYZ RXYZGXYZ
nn

. (27)
If the concircular curvature tensor
C satises the re-
lation (18), then the manifold is said to be generalized
concircularly φ-recurrent Sasakian manifold. We also note
that since conformal and projective curvature tensors are
trace free, there do not exist any generalized conformally
and projectively φ-reccurent Sasakian manifolds.
Let us consider a generalized concircularly φ-recurrent
Sasakian manifold M, n 3. Hence the dening condi-
tion of a generalized concircularly φ-recurrent Sasakian
manifold, yields by virtue of (27) that


 

 
 
22
2
,,
,
(1)
,,,
WRXYZAWRXYZ
BWG XYZ
rA WdrW
nn
gYZXXgYZgXZYYgXZ

,.
 

 
(28)
This leads to the following.
Theorem 3. A generalized concircularly φ-recurrent
Sasakian manifold M, n 3, is generalized φ-recurrent if
and only if
 
 
,,
(1)
,,0.
rA WdrW
g
YZ XXgYZ
nn
gXZYYgXZ

 
(29)
Now taking inner product of (29) with U we have
 

,, ,
(1)
,, ,
rA WdrW
0.
g
YZgXUX gYZU
nn
gXZgYUYgXZ U



Taking contraction over X and U we get

(2) ,rA WdrWngYZYZ


0


.
Again taking contraction over Y and Z we get
(2)10rA WdrWn n
.
which implies that

1
A
WdrW
r
for all W and 0r
i.e., 1
1
g
radr
r
, where
 
1
,AW gW
.
This leads to the following.
Theorem 4. If a generalized concircularly φ-recurrent
Sasakian manifold M, n 3, is a generalized φ-recurrent
Sasakian manifold, then the associated vector field cor-
responding to the 1-form A is given by 1
1
g
radr
r
, r
being the non-zero and non-constant scalar curvature of
the manifold.
Now by virtue of (4), it follows from (28) that

 

 


 
,,
,,
,,
,,
(1)
,,.
WW
RXYZ RXYZ
AW RXYZRXYZ
BW GXYZGXYZ
rA WdrW
g
YZ XX gYZ
nn
gXZY YgXZ













(30)
Copyright © 2011 SciRes. AM
A. A. SHAIKH ET AL.
1320
Taking inner product of (30) with U and then contra-
cting over X and U, and then using (2), (15), (10) and (8)
we get


 

  

,,
(2) ,
()(2) ,
(1)
(2)
1,
(1) (1)
.
WSYZ AWSYZ
nBWAWgYZ
dr WngYZ YZ
nn
rnr
A
WYZg
nn nn
BW YZ





 






 






YZ
(31)
Again taking contraction over Y and Z in (31), we get
 
2
d(1)(1)rWrnnAWnnBW  . (32)
From (32), we can state the following.
Theorem 5. In a generalized concircularly φ-recurrent
Sasakian manifold M, n 3, the associated 1-forms A
and B are related by the relation (32).
Corollary 1. In a generalized concircularly φ-recurrent
Sasakian manifold M, n 3, with constant scalar curva-
ture, the associated 1-forms A and B are related by

2
(1)(1) 0rnnAnn B .
Now using (32) in (31) we get





,,
(2)(1),
.


 
WSYZ AWSYZ
nnBWnAWg Y Z
nB WYZ
(33)
From (33), it follows that the Ricci tensor S satises
the condition
πSSg

  , (34)
where
,
 
,WAW

(2)Wnn BW
 
(1)nAW


WnBW
and π
.
By extending the notion of generalized Ricci-recurrent
manifold [16], we introduce the notion of super general-
ized Ricci-recurrent manifold defined as follows.
Denition 4. An n-dimensional Riemannian manifold
M, n > 2, is called a super generalized Ricci-recurrent if
its Ricci tensor S of type (0,2) satises the relation
πSSg

  ,
where α, β, γ are nowhere vanishing unique 1-forms and
π
.
From (34), we can state the following:
Theorem 6. A generalized concircularly φ-recurrent
Sasakian manifold M, n 3, is super generalized Ricci-
recurrent manifold.
Now taking contraction of (33) over W and Z, we get
 
 
1
1d,(2)
2
(1)
rY SYnnBY
nAYnYB
.


By virtue of (32), the above relation takes the form
 

 
1
2
(1)(2)
,2
45
.
2
rn n
SY AY
nn n
BYnY B



(35)
From (35), we can state the following.
Theorem 7. In a generalized concircularly φ-recurrent
Sasakian manifold M, n 3, the Ricci tensor in the di-
rection of ρ1 is given by (35).
Now setting Z
in (33) and then using (13) and
(11) we get

,( 1),( 1)SY WngY WnnBWY


. (36)
Replacing Y by φY in (36) and using (12) and (6) we
have

,(1),SYWn gYW
. (37)
Replacing W by φW in (36) and then using (4) we get

,(1),(1)SYWngYWnnB WY

 . (38)
From (37) and (38) we have
0BW
,
which implies that

BWWB
.
This leads to the following.
Theorem 8. In a generalized concircularly φ-recurrent
Sasakian manifold M, n 3, the vector field ρ2 associated
with the 1-form B and the characterstic vector field ξ are
codirectional.
5. Example of Generalized φ-Recurrent
Sasakian Manifold
Example 1. We consider a 3-dimensional manifold

3
,,:0Mxyzy

3
, where (x, y, z) are the stan-
dard coordinates in . Let be a linearly
independent global frame on M given by
123
,,EEE
2
12 3
2,, .EExyE
x
zy z
 
  
 
Let g be the Riemannian metric defined by

1323 12
,,,gEE gEE gEE0
,

112233
,,,gEEgEEgE E1
.
Copyright © 2011 SciRes. AM
A. A. SHAIKH ET AL.1321
Let η be the 1-form defined by for
any . Let φ be the (1,1) tensor field defined
by 1221

3
,UgUE

UM
,EE
EE
 and 30E
. Then using the
linearity of φ and g we have
1
3
E
,
and

3
UE
2UU
 
 
,,
g
UW gUW

()( )UW
for any . Thus for 3

ME,UW
,
(,,, )

denes an almost contact metric structure on
M. Let be the Riemannian connection of g. Then we
have
123 1323
,2, ,0, ,0EEEEEEE 


.
Using Koszul formula for the Riemannian metric g,
we can easily calculate
11 1
1233
0,, ,
EE E
EEEE
2
E
,
0.
222
1323 1
,0,
EEE
EEEE E
33 3
122 13
,,
EE E
EEE EE
From the above it can be easily seen that

,,,
g

3,,,
is
a Sasakian structure on M. Consequently

M
g

is a Sasakian manifold. Using the above relations, we can
easily calculate the components of the curvature tensor
as follows:

12 121221
12 3
,3,, 3
,0,
RE EEERE EEE
RE EE

,
,
 
13 1313213 31
,3,, 0,,REE EEREE EREEEE
 
23 123232332
, 0,,,,RE EERE EEE RE EEE
and the components which can be obtained from these by
the symmetry properties.
Since forms a basis of the Sasakian
manifold, any vector field
123
,,EE E

,,
X
YZ M
can be wri-
tten as
11 1213
,
X
aE bEcE
212 223
,YaEbE cE
31 3233
,
X
aE bEcE
where (the set of all positive real num-
bers), i = 1, 2, 3. Then
,,
iii
abc



312 21312211
31221312 212
31221312 213
,3
3









RXYZc acacb ababE
aab abcbc bc E
aac acbbc bc E
(39)
and



232323 111213
1 31313212223
,
.
 
 
GX YZaabbccaEbEcE
aabbcca EbEc E
(40)
By virtue of (39) we have the following:
 


1312 21312 211
312 212312 213
,=4
44,
ERXYZcab abbacacE
aac acEaab abE


(41)
 



231221 1
31221312212
31221 3
,4
4
4,



ERXYZbbc bcE
cab ababcbcE
bab abE
(42)

3,=
ERXYZ0. (43)
From (39) and (40), we get


2
112 2
2
1122
,
,,


RXYZpE pE
GXYZqEqE
(44)
where
 



13122131221
2312213122
1213131 2323
221313 12323
3
3
.




pbababcacac
paababcbcbc
qabbcc abbcc
qbaacc baacc
1
Also from (41)-(43), we obtain

2
1
,
i
Ei
RXYZuE vE

2i
for i = 1, 2, 3, (45)
where
 




1312213122
131221
231221
23122131221
33
4
4
4
4
0, 0.
 

 


ucababbacac
vaacac
ubbcbc
vabcbccabab
uv
1
Let us now consider the components of the 1-forms as
21
12 21
() i
i
qu qv
AE pq pq
i
for i = 1, 2
0
for i = 3 (46)
and
1i2 i
12 21
-p
()
i
pv u
BE pq pq
for i = 1, 2
0
for i = 3 (47)
where 1221 0pqp q
12
0
ii
pu
, and
21
0
ii
qu qv
pv
for i = 1, 2.
From (18), we have







22
2
,,
,
i
Ei
i
R XYZAERXYZ
BE GXYZ


(48)
Copyright © 2011 SciRes. AM
A. A. SHAIKH ET AL.
Copyright © 2011 SciRes. AM
1322
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