International Journal of Engineering and Applied Sciences (IJEAS) ISSN: 2394-3661, Volume-2, Issue-10, October 2015
On CR-Structure And F-Structure Satisfying Fp1p2 + F = 0 Lakhan Singh, Shailendra Kumar Gautam
II. NIJENHUIS TENSOR:
Abstract— In this paper, we have studied a relationship
Fpp
1 2 between CR-structure and F-structure satisfying + F=0, where p1 and p2 are twin primes. Nijenhuis tensor and integrability conditions have also been discussed.
Index Terms— Projection operators, distributions, Nijenhuis tensor, integrability conditions and CR-structure.
(2.1)
(2.2) N X ,Y FX , FY F FX ,Y F X , FY F 2 X ,Y
I. INTRODUCTION
Theorem (2.1) A necessary and sufficient condition for the F-structure to be integrable is
Let M be an n-dimensional differentiable manifold of class
1.1
N X ,Y 0
C . Let F be a non-zero tensor of type (1, 1) and class C defined on M, such that F p1 p2 F 0 where p1 and p2 are twin primes. Let
F r
rank
1.2
l F p1 p2 1 , m F p1 p2 1 I
(1.3)
where I is the identity operator on M. Theorem (1.1) Let M be an F- structure satisfying (1.1) Then (a) lmI
F
Dm
be
the
(2.5)
complementary
2
F
p1 p2 2
on both the sides of
F p1 p2 1 l l ,
Proof: Operating m on both the sides of (2.2) and using (1.4) (a) we get (2.5) (a). Replacing X by
m
Proof: From (1.1), (1.2), (1.3)(a), (b), we get the results.
m N F p1 p2 2 X ,Y m F p1 p2 1 X , FY
D n r F p1 p2 1m 0
m N X , Y m FX , FY
(a) (b)
Theorem (1.2) Let M be an F-structure satisfying (1.1). Then (a) lF Fl F , mF Fm 0
F p1 p2 2 X
(2.6)
F 1 2 acts on Dl as an almost complex structure and on Dm as a null operator. From (1.4) (b), it is clear that
FX , FY F X ,Y l FX ,Y X , FY .
(2.4) and using (1.2), we get the result. Theorem (2.3) On the F-structure satisfying (1.1)
dim Dl r , dim
(b)
p1 p2 2
FX , FY F 2 X ,Y F FX ,Y X , FY
distributions corresponding to the operators l and m respectively. then
(1.4)
vector
& Y on M.
Operating by
Proof: From (1.1) and (1.2), we get the results. and
two
Proof: using theorem (2.1) in (2.2), we get
m m lm ml 0
Dl
any
(2.4)
2
(d)
for
Theorem (2.2) Let the F-structure satisfying (1.1) be integrable, then
l2 l
(c)
Let
fields X
,
(2.3)
, which is constant
everywhere. We define the operators on M as
(b)
Definifion (2.1) Let X and Y be any two vector fields on M, then their Lie bracket [X, Y] is defined by [X, Y] = XY- YX, and Nijenhuis tensor N(X,Y) of F is defined as
p p 1 / 2
in (2.5) (a), we get (2.5) (b). Theorem (2.4): On the F-structure satisfying (1.1), the following conditions are all equivalent (a) m N X ,Y 0 (b) m FX , FY 0
0
(c)
m N F p1 p2 2 X , Y
(d)
m F
(e)
m F p1 p2 1 lX , FY 0
p1 p2 1
X , FY 0
Proof: Using (1.4) (a), (b) in (2.5) (a), (b), we get the results.
Lakhan Singh, Department of Mathematics, D.J. College, Baraut, Baghpat (U.P.) Shailendra Kumar Gautam, Eshan College of Engineering, Mathura(UP)
1
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