Hindawi Publishing Corporation Geometry Volume 2014, Article ID 616487, 12 pages http://dx.doi.org/10.1155/2014/616487
Research Article Paracomplex Paracontact Pseudo-Riemannian Submersions S. S. Shukla and Uma Shankar Verma Department of Mathematics, University of Allahabad, Allahabad 211002, India Correspondence should be addressed to Uma Shankar Verma;
[email protected] Received 25 February 2014; Accepted 7 April 2014; Published 7 May 2014 Academic Editor: Bennett Palmer Copyright Β© 2014 S. S. Shukla and U. S. Verma. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. We introduce the notion of paracomplex paracontact pseudo-Riemannian submersions from almost para-Hermitian manifolds onto almost paracontact metric manifolds. We discuss the transference of structures on total manifolds and base manifolds and provide some examples. We also obtain the integrability condition of horizontal distribution and investigate curvature properties under such submersions.
1. Introduction The theory of Riemannian submersion was introduced by OβNeill [1, 2] and Gray [3]. It is known that the applications of such Riemannian submersion are extensively used in KaluzaKlein theories [4, 5], Yang-Mill equations [6, 7], the theory of robotics [8], and supergravity and superstring theories [5, 9]. There is detailed literature on the Riemannian submersion with suitable smooth surjective map followed by different conditions applied to total space and on the fibres of surjective map. The Riemannian submersions between almost Hermitian manifolds have been studied by Watson [10]. The Riemannian submersions between almost contact manifolds were studied by Chinea [11]. He also concluded that if π is an almost Hermitian manifold with structure (π½, π) and π is an almost contact metric manifold with structure (π, π, π, π), then there does not exist a Riemannian submersion π : π β π which commutes with the structures on π and π; that is, we cannot have the condition πβ β π½ = π β πβ . Chinea also defined the Riemannian submersion between almost complex manifolds and almost contact manifolds and studied some properties and interrelations between them [12]. In [13], GΒ¨undΒ¨uzalp and Sahin gave the concept of paracontact paracomplex semi-Riemannian submersion between almost paracontact metric manifolds and almost para-Hermitian manifolds submersion giving an example and studied some geometric properties of such submersions.
An almost paracontact structure on a differentiable manifold was introduced by Sato [14], which is an analogue of an almost contact structure and is closely related to almost product structure. An almost contact manifold is always odd dimensional but an almost paracontact manifold could be even dimensional as well. The paracomplex geometry has been studied since the first papers by Rashevskij [15], Libermann [16], and Patterson [17] until now, from several different points of view. The subject has applications to several topics such as negatively curved manifolds, mechanics, elliptic geometry, and pseudoRiemannian space forms. Paracomplex and paracontact geometries are topics with many analogies and also with differences with complex and contact geometries. This motivated us to study the pseudo-Riemannian submersion between pseudo-Riemannian manifolds equipped with paracomplex and paracontact structures. In this paper, we give the notion of paracomplex paracontact pseudo-Riemannian submersion between almost paracomplex manifolds and almost paracontact pseudometric manifolds giving some examples and study the geometric properties and interrelations under such submersions. The composition of the paper is as follows. In Section 2, we collect some basic definitions, formulas, and results on almost paracomplex manifolds, almost paracontact pseudometric manifolds, and pseudo-Riemannian submersion.
2
Geometry
In Section 3, we define paracomplex paracontact pseudoRiemannian submersion giving some relevant examples and investigate transference of structures on the total manifolds and base manifolds under such submersions. In Section 4, curvature relations between total manifolds, base manifolds, and fibres are studied.
If π and π are vector fields on π2π+1 , then we have [18β 20] ππ½ ((π, 0) , (π, 0)) = (ππ (π, π) β 2ππ (π, π) π,
2. Preliminaries 2.1. Almost Paracontact Manifolds. Let π be a (2π + 1)dimensional Riemannian manifold, π a (1,1)-type tensor field, π a vector field, called characteristic vector field, and π a 1form on π. Then, (π, π, π) is called an almost paracontact structure on π if π2 π = π β π (π) π;
π (π) = 1,
(1)
and the tensor field π induces an almost paracomplex structure on the distribution D = ker(π) [18, 19]. π is said to be an almost paracontact manifold, if it is equipped with an almost paracontact structure. Again, π is called an almost paracontact pseudometric manifold if it is endowed with a pseudo-Riemannian metric π of signature +, +, +, . . . , +) such that (β, β, β, . . . , β, βββββββββββββββββββββββ βββββββββββββββββββββββ (π-times)
(π+1)-times)
π (ππ, ππ) = π (π, π) β ππ (π) π (π) ,
βπ, π β Ξ (ππ) , (2)
where π = 1 or β1 according to the characteristic vector field π is spacelike or timelike. It follows that π (π, π) = π,
(3)
π (π, π) = ππ (π) ,
(4)
π (π, ππ) = π (ππ, π) ,
βπ, π β Ξ (ππ) .
(5)
In particular, if πππππ₯(π) = 1, then the manifold (π2π+1 , π, π, π, π, π) is called a Lorentzian almost paracontact manifold. If the metric π is positive definite, then the manifold (π2π+1 , π, π, π, π) is the usual almost paracontact metric manifold [14]. The fundamental 2-form Ξ¦ on π is defined by Ξ¦ (π, π) = π (π, ππ) .
(6)
Let π2π+1 be an almost paracontact manifold with the structure (π, π, π). An almost paracomplex structure π½ on π2π+1 Γ R1 is defined by π½ (π, π
π π ) = (ππ + ππ, π (π) ) , ππ‘ ππ‘ 2π+1
(7) 1
, π‘ is the coordinate on R , and π where π is tangent to π 2π+1 is a smooth function on π . An almost paracontact structure (π, π, π) is said to be normal, if the Nijenhuis tensor ππ½ of almost paracomplex structure π½ defined as ππ½ (π, π) = [π½, π½] (π, π) = [π½π, π½π] + π½2 [π, π] β π½ [π½π, π] β π½ [π, π½π] , for any vector fields π, π β Ξ(ππ), vanishes.
(8)
{(Lππ π) π β (Lππ π) π} ππ½ ((π, 0) , (0,
(9) π ), ππ‘
π π )) = β ((Lπ π) π, ((Lπ π) π) ) , ππ‘ ππ‘ (10)
where ππ is Nijenhuis tensor of π, Lπ is Lie derivative with respect to a vector field π, and π(1) , π(2) , π(3) , and π(4) are defined as ππ (π, π) = [π, π] (π, π)
(11)
= [ππ, ππ] + π2 [π, π] β π [ππ, π] β π [π, ππ] , π(1) (π, π) = ππ (π, π) β 2ππ (π, π) π,
(12)
π(2) (π, π) = (Lππ π) π β (Lππ π) π,
(13)
π(3) (π) = (Lπ π) π,
(14)
π(4) (π) = (Lπ π) π.
(15)
The almost paracontact structure (π, π, π) is normal if and only if the four tensors π(1) , π(2) , π(3) , and π(4) vanish. For an almost paracontact structure (π, π, π), vanishing of π(1) implies the vanishing of π(2) , π(3) , and π(4) . Moreover, π(2) vanishes if and only if π is a killing vector field. An almost paracontact pseudometric manifold (π2π+1 , π, π, π, π, π) is called (i) normal, if ππ β 2ππ β π = 0, (ii) paracontact, if Ξ¦ = ππ, (iii) πΎ-paracontact, if π is paracontact and π is killing, (iv) paracosymplectic, if βΞ¦ = 0, which implies βπ = 0, where β is the Levi-Civita connection on π, (v) almost paracosymplectic, if ππ = 0 and πΞ¦ = 0, (vi) weakly paracosymplectic, if π is almost paracosymplectic and [π
(π, π), π] = π
(π, π)π β ππ
(π, π) = 0, where π
is Riemannian curvature tensor, (vii) para-Sasakian, if Ξ¦ = ππ and π is normal, (viii) quasi-para-Sasakian, if ππ = 0 and π is normal. 2.2. Almost Paracomplex Manifolds. A (1, 1)-type tensor field π½ on 2π-dimensional smooth manifold π is said to be an almost paracomplex structure if π½2 = πΌ and (π2π , π½) is called almost paracomplex manifold.
Geometry
3
An almost paracomplex manifold (π, π½) is such that the two eigenbundles π+ π and πβ π corresponding to respective eigenvalues +1 and β1 of π½ have the same rank [21, 22]. An almost para-Hermitian manifold (π, π½, π) is a smooth manifold endowed with an almost paracomplex structure π½ and a pseudo-Riemannian metric π such that π (π½π, π½π) = βπ (π, π) ,
βπ, π β Ξ (ππ) .
(16)
Here, the metric π is neutral; that is, π has signature (π, π). The fundamental 2-form of the almost para-Hermitian manifold is defined by πΉ (π, π) = π (π, π½π) .
(17)
We have the following properties [21, 22]: π (π½π, π) = βπ (π, π½π) ,
(18)
πΉ (π, π) = βπΉ (π, π) ,
(19)
πΉ (π½π, π½π) = βπΉ (π, π) ,
(20)
(ii) The fibres πβ1 (π) of π over π β π are either pseudo-Riemannian submanifolds of π of dimension (π β π) and index ] or the degenerate submanifolds of π of dimension (π β π) and index ] with degenerate metric π| β1 of type π (π) (0, 0, 0, . . . , 0, βββββββββββββββββββββββ β, β, β, . . . , β, +, +, +, . . . , + ), where βββββββββββββββββββββ βββββββββββββββββββββββ π-times
]-times
(πβπβπβ])-times)
π = dim(Vπ β© Hπ ) and ] = π β π = index of π|
πβ1 (π)
.
(iii) πβ preserves the length of horizontal vectors. We denote the vertical and horizontal projections of a vector field πΈ on π by πΈV (or by VπΈ) and πΈβ (or by βπΈ), respectively. A horizontal vector field π on π is said to be basic if π is π-related to a vector field π on π. Thus, every vector field π on π has a unique horizontal lift π on π. Lemma 1 (see [1, 23]). If π : π β π is a pseudoRiemannian submersion and π, π are basic vector fields on π that are π-related to the vector fields π, π on π, respectively, then one has the following properties: (i) π(π, π) = π(π, π) β π,
3ππΉ (π, π, π) = π (πΉ (π, π)) β π (πΉ (π, π)) + π (πΉ (π, π))
(21)
β πΉ ([π, π] , π) + πΉ ([π, π] , π) β πΉ ([π, π] , π) , (βπ πΉ) (π, π) = π (π, (βπ π½) π) = βπ (π, (βππ½) π) , 3ππΉ (π, π, π) = (βπ πΉ) (π, π) + (βπ πΉ) (π, π) + (βππΉ) (π, π) ,
(22) (23)
2π
the co-differential, (πΏπΉ) (π) = βππ (βππ πΉ) (ππ , π) .
(24)
π=1
(i) para-Hermitian, if ππ½ = 0; equivalently, (βπ½ππ½)π½π + (βπ π½)π = 0, (ii) para-KΒ¨ahler, if, for any π β Ξ(ππ), βπ π½ = 0; that is, βπ½ = 0, (iii) almost para-KΒ¨ahler, if ππΉ = 0, (iv) nearly para-KΒ¨ahler, if (βππ½)π = 0,
(iv) [πΈ, π] β V, for any vector field π β V and for any vector field πΈ β Ξ(ππ). A pseudo-Riemannian submersion π : π β π determines tensor fields T and A of type (1, 2) on π defined by formulas [1, 2, 23]
A (πΈ, πΉ) = AπΈ πΉ = V (ββπΈ βπΉ) + β (ββπΈ VπΉ) , for any πΈ, πΉ β Ξ (ππ) .
π
2.3. Pseudo-Riemannian Submersion. Let (π , π) and (ππ , π) be two connected pseudo-Riemannian manifolds of indices π (0 β€ π β€ π) and π (0 β€ π β€ π), respectively, with π β₯ π . A pseudo-Riemannian submersion is a smooth map π : π π β ππ , which is onto and satisfies the following conditions [2, 3, 23, 24]. β
Tππ = β (βππ) ,
βππ = Tππ + β (βππ) ,
(vi) semi-para-KΒ¨ahler, if πΏπΉ = 0 and ππ½ = 0.
ππ(π) π is
(25) (26)
Let π, π be horizontal vector fields and let π, π be vertical vector fields on π. Then, one has Tππ = V (βππ) ,
(v) almost semi-para-KΒ¨ahler, if πΏπΉ = 0,
surjective at each point π β π.
(iii) β(βπ π) is a basic vector field π-related to βπ π, where β and β are the Levi-Civita connections on π and π, respectively,
T (πΈ, πΉ) = TπΈ πΉ = β (βVπΈ VπΉ) + V (βVπΈ βπΉ) ,
An almost para-Hermitian manifold is called
(i) The derivative map πβπ : ππ π
(ii) β[π, π] is a vector field and β[π, π] = [π, π] β π,
Tπ πΉ = 0,
TπΈ πΉ = TVπΈ πΉ,
βππ = Tππ + V (βππ) , Aπ π = V (βπ π) ,
Aπ π = β (βπ π) ,
βπ π = Aπ π + V (βπ π) , AππΉ = 0,
AπΈ πΉ = AβπΈ πΉ,
βπ π = Aπ π + β (βππ) ,
(27) (28) (29) (30) (31) (32) (33) (34)
4
Geometry 2π
β (βππ) = β (βπ π) = Aπ π,
(35)
1 Aπ π = V [π, π] , 2
(36)
Aπ π = βAπ π,
(37)
Proposition 4. Let π : π β π2π+1 be a paracomplex paracontact pseudo-Riemannian submersion and let the fibres of π be pseudo-Riemannian submanifolds of π. Then, the fibres πβ1 (π), π β π, are semi-π½-invariant submanifolds of π of dimension (2π β 2π β 1).
Tππ = Tππ,
(38)
Proof. Let π β V. Then
for all πΈ, πΉ β Ξ(ππ). Moreover, Tππ coincides with second fundamental form of the submersion of the fibre submanifolds. The distribution H is completely integrable. In view of (37) and (38), A is alternating on the horizontal distribution and T is symmetric on the vertical distribution.
3. Paracomplex Paracontact PseudoRiemannian Submersions
πβ (π½π) = π (πβ (π)) + π (π) π,
β
where πβ π = π. Thus, we have β
π½ (π) β π (π) π = π (π) ,
In this section, we introduce the notion of pseudoRiemannian submersion from almost paracomplex manifolds onto almost paracontact pseudometric manifolds, illustrate examples, and study the transference of structures on total manifolds and base manifolds.
β
πβ β π½ = π β πβ + π β π.
(39)
Since, for each π β π, πβπ is a linear isometry between horizontal spaces Hπ and tangent spaces ππ(π) π, there exists β
β
an induced almost paracontact structure (π , πβ , π , π) on (2π + 1)-dimensional horizontal distribution H such that β π| β behave just like the fundamental collineation of almost D
β
β
β
paracomplex structure π½ on ker πβ = D and π : D β D β
is an endomorphism such that π = π½|
ker πβ
β
β
π = 2π, where dim(D ) = 2π. It follows that, for any π implies that
2 π½|
β
D
β 2
β
β
β
β
β
and the rank of
β
β
(π ) = (π ) (π ) = π , for any π β D
β
β
and H = D β {π } [18].
β
β
πβ (π½ (π )) = 0,
β
that is π½ (π ) β V.
(44)
β
Taking π = π½π in (43), we obtain β
β
β
β
π β π (π½π ) π = π (π½π ) .
(45)
Since fibre πβ1 (π) is an odd dimensional submanifold, there exists an associated 1-form πV which is restriction of π on fibre submanifold πβ1 (π), π β π, and a characteristic vector field V
β
V
V
π = π½π such that π(π ) = 0. So, we have πV (π ) = 1. V Let us put ker πV = D1 and D2 = {π }. Then, ker πβ = D1 β D2 and π½(D1 ) = D1 , π½(D2 ) = V
β
π½{π } = {π } β (ker πβ )β₯ .
Hence, the fibres πβ1 (π) are semi-π½-invariant submanifolds of π.
Corollary 5. Let π : π β π2π+1 be a paracomplex paracontact pseudo-Riemannian submersion and let the fibres of π be pseudo-Riemannian submanifolds of π. Then, the fibres πβ1 (π) are almost paracontact pseudometric manifolds with almost paracontact pseudo-Riemannian structures V
Definition 3 (see [25]). A pseudo-Riemannian submersion π : π β π is called semi-π½-invariant submersion, if there is a distribution D1 β ker πβ such that ker πβ = D1 β D2 , π½ (D1 ) = D1 ,
β
(43)
2π
β
β D , πβ (π ) = 0, which β
for some π (π) β V.
By (19), we get π(π , π½(π )) = 0 = π(π, πβ (π½(π ))) = 0. As π is nondegenerate on π, we have
2π
Definition 2. Let (π , π½, π) be an almost para-Hermitian manifold and let (π2π+1 , π, π, π, π) be an almost paracontact pseudometric manifold. A pseudo-Riemannian submersion π : π β π is called paracomplex paracontact pseudo-Riemannian submersion if there exists a 1-form π on π such that
(42)
β
σ³¨β πβ {π½ (π) β π (π) π } = 0,
(40) β₯
π½ (D2 ) β (ker πβ ) ,
where D2 is orthogonal complementary to D1 in ker πβ .
V
(π , π , πV , πV ), π β π, where π πV = π.
V
β
= π½(π ), πV = π|V , and
Proof. Since πβ1 (π) are semi-π½-invariant submanifolds of π of odd dimension 2π + 1 = 2π β 2π β 1, (39) implies V
β
π½ (π) = π π + πV (π) π ,
(41) for any π β V.
(46)
Geometry
5
On operating π½ on both sides of the above equation, we get
H, and πβπ : Hπ β ππ(π) π is a linear isometry, for any ππ β Hπ , we get
V
V
β
V
V
π = π (π (π)) + πV (π (π)) π + πV (π) π , β
(47)
β
β
πβπ (ππ ) = πππ (ππ , ππ ) = ππ(π) (πβπ ππ , πβπ ππ )
V
where π½(π ) = π . Equating horizontal and vertical components, we have V
V
V
= ππ(π) (ππ(π) , ππ(π) ) = ππ(π) (ππ(π) ) = πββ ππ (ππ ) . (52)
V
π = π (π (π)) + πV (π) π ,
πV β π (π) = 0, (48)
Hence, pullback πββ π = πβ . Results (iii) and (iv) immediately follow from the previous results.
Hence, (π , π , πV , πV ) is almost paracontact pseudometric structure on the fibre πβ1 (π), π β π.
Example 8. Let (R42 , π½, π) be a paracomplex pseudometric manifold and let (R31 , π, π, π, π) be an almost paracontact pseudometric manifold. Define a submersion π : {R42 ; (π₯1 , π₯2 , π¦1 , π¦2 )π‘ } β 3 {R1 ; (π’, V, π€)π‘ } by
V 2
V
V
σ³¨β (π ) (π) = π β π (π) π ; V
V
V
V
π β π = 0; V
πV (π ) = 1.
π (π ) = 0, V
V
2π
Proposition 6. Let π : π β π2π+1 be a paracomplex paracontact pseudo-Riemannian submersion and let the fibres of π be pseudo-Riemannian submanifolds of π. Let π, π be basic vector fields π-related to π, π, respectively. Let π and π be 1-forms on the total manifold π and the base manifold π, respectively. Then, one has the following.
π‘
π ((π₯1 , π₯2 , π¦1 , π¦2 ) ) σ³¨σ³¨β (π₯1 + π₯2 + 3π¦1 + 2π¦2 , 3π₯1 + 2π₯2 + π¦1 + π¦2 , π‘
5π₯1 + 3π₯2 + 5π¦1 + 3π¦2 ) .
β
(i) The characteristic vector field π½π is a vertical vector field. (ii) πββ π = πβ , where πββ π is pullback of π through πβ .
Then, the kernel of πβ is V = ker πβ = Span {π1 =
(iii) πβ (π) = 0, for any vertical vector field π. (iv) πV (π) = 0, for any horizontal vector field π. Remark 7. Results (ii) and (iv) are analogue version of results (i) and (iii) of Proposition 4 of [13]. V
V
β
β
β₯
H = (ker πβ )
= Span {π1 =
β
0 = π (π , π½π ) = π (πβ (π ) , πβ (π½π ))
π3 = 2
= π (π, πβ (π½π )) . Now, β
β
β
β
(50)
π π + }. ππ¦1 ππ¦2
For any real π, the horizontal characteristic vector field π is given by β
π =π
so we have β
β
β
0 = π (π, π (π ) π) = π (π ) π (π, π) = π (π ) .
(51)
β
Thus, πβ (π½π ) = 0. β
π
(55)
β
πβ (π½π ) = π β πβ π + π (π ) π = π (π ) π,
β
π π π π β ,π = +2 , ππ₯1 ππ¦1 2 ππ₯2 ππ¦1
(49)
β
π π π π β2 β +2 }, ππ₯1 ππ₯2 ππ¦1 ππ¦2 (54)
which is the vertical distribution admitting one lightlike vector field; that is, fibre is degenerate submanifold of R42 . The horizontal distribution is
Proof. (i) By Corollary 5, (π , π , πV , πV ) is almost paracontact pseudometric structure on πβ1 (π). We have β
(53)
Hence, π½π is a vertical vector field. 2π (ii) Since π : π β π2π+1 is smooth submersion, = π|H is restriction of π on the horizontal distribution
π π 1 π 5 π β (2π β ) β (π β 1) + (2π β ) , ππ₯1 3 ππ₯2 ππ¦1 3 ππ¦2 (56)
which is π-related to the characteristic vector field π = π/ππ€. Moreover, there exists one form π = 5ππ₯1 + 3ππ₯2 + 5ππ¦1 + 3ππ¦2 on (R42 , π½, π) such that the submersion satisfies (39). Example 9. Let (R63 , π½, π) be an almost paracomplex pseudoRiemannian manifold and let (R31 , π, π, π, π) be an almost
6
Geometry
paracontact pseudo-Riemannian manifold. Consider a submersion π : {R63 ; (π₯1 , π₯2 , π₯3 , π¦1 , π¦2 , π¦3 )π‘ } β {R31 ; (π’, V, π€)π‘ }, defined by
β
β
R42 such that π(π½π ) = 1, π(π ) = 0 and the map π satisfies
π‘
π ((π₯1 , π₯2 , π₯3 , π¦1 , π¦2 , π¦3 ) ) σ³¨σ³¨β (
Thus, the smooth map π is a pseudo-Riemannian submersion. Moreover, we obtain that there exists a 1-form π = ππ₯2 on
(57)
π₯1 + π₯2 π¦1 + π¦2 π¦2 + π¦3 π‘ , , ). β2 β2 β2
Then, there exists one form π = (ππ₯2 + ππ₯3 )/β2 on such that (39) is satisfied. The kernel of πβ is
πβ π½π = ππβ π + π (π) π, (R63 , π½, π)
πβ π½π = ππβ π + π (π) π,
V = ker πβ
β
= Span {π1 =
π }, ππ₯3
Hence, the map π is a paracomplex paracontact pseudo-Riemannian submersion from R42 on to R31 .
which is vertical distribution admitting non-lightlike vector fields; that is, the fibre is nondegenerate submanifold of (R63 , π½, π). The horizontal distribution is H = Span {π1 =
β
πβ π½π = ππβ π + π (π ) π.
π π π π π β ,π = β + , ππ₯1 ππ₯2 2 ππ¦1 ππ¦2 ππ¦3 (58)
π3 =
β
(64)
π π π π + ,π = β + , ππ₯1 ππ₯2 2 ππ¦1 ππ¦3
π π π3 = + }. ππ¦1 ππ¦2
β
π‘
π‘
β
ππ(π, π )π is π-related to ππ. (59)
Example 10. Let (R42 , π½, π) be a paracomplex pseudometric manifold and let (R31 , π, π, π, π) be an almost paracontact pseudometric manifold. Consider a submersion π : {R42 ; (π₯1 , π₯2 , π¦1 , π¦2 )π‘ } β {R31 ; (π’, V, π€)π‘ }, defined by π ((π₯1 , π₯2 , π¦1 , π¦2 ) ) σ³¨σ³¨β (π₯1 , π¦1 , π¦2 ) .
Proposition 11. Let π : π β π be a paracomplex paracontact pseudo-Riemannian submersion and let the fibres of π be pseudo-Riemannian submanifolds of π. Let π, π be basic vector fields π-related to π, π, respectively. Then, π½(π) β
Proof. Since π is π-related to vector field π on π, we have
β
π (π) = {πV + πβ } (π) = 0 + πβ (π) = ππ (π, π ) , σ³¨β πβ (π½ π) = ππ + πβ (π) π, β
(65)
β
(60)
σ³¨β πβ {π½ π β ππ (π, π ) π } = ππ.
(61)
Hence, π½(π) β ππ(π, π )π is π-related to ππ.
Then, the kernel of πβ is V = ker πβ = Span {π1 =
π }, ππ₯2
β
β
which is the vertical distribution and the restriction of π to the fibres of π is nondegenerate. The horizontal distribution is
Proposition 12. Let π : π β π be a paracomplex paracontact pseudo-Riemannian submersion and let the fibres of π be pseudo-Riemannian submanifolds of π. Let V and H be
π π β π ,π = ,π = }. ππ₯1 ππ¦1 ππ¦2 (62)
the vertical and horizontal distributions, respectively. If π is the basic characteristic vector field of horizontal distribution π-related to the characteristic vector field π of base manifold, then
β₯
H = (ker πβ ) = Span {π =
The characteristic vector field π = π/ππ€ on R31 has unique
β
β
horizontal lift π , which is the characteristic vector field on horizontal distribution H of R42 . We also have π (π, π) = π (πβ π, πβ π) = β1, π (π, π) = π (πβ π, πβ π) = 1, β
β
β
β
π (π , π ) = π (πβ π , πβ π ) = π (π, π) = 1.
β
V
β
(i) π½V β D β {π½π } β {π }, β
β
β
(ii) π½H β D β {π } β {π½π }. (63)
Proof. (i) Let π β V. Then, π = ππ| πΆβ (π), as π½π
β
V
D
β
V
+ ππ½π , for π, π β
= π is characteristic vector field on odd
Geometry
7
dimensional fibre submanifold πβ1 (π) of π, π β π. We get 2 β
π½π = ππ½ π|
V
+ ππ½ π
= ππ½ π|
V
+ ππ β V β {π } ,
D
β
D
β
(66)
paracontact pseudo-Riemannian manifold. Consider a submersion π : {R63 ; (π₯1 , π₯2 , π₯3 , π¦1 , π¦2 , π¦3 )π‘ } β {R31 ; (π’, V, π€)π‘ }, defined by π‘
π ((π₯1 , π₯2 , π₯3 , π¦1 , π¦2 , π¦3 ) ) σ³¨σ³¨β (
β
σ³¨β π½V β V β {π } .
Then, the kernel of πβ is
β
Again, let π β V β {π }. Then π = ππ|
D
V
πV (π| V ) = 0, D = ker πV , ππ| D
β
D
πΆ (π). We have π½ π = ππ½ π|
β
D
V
+ ππ + ππ½π
β
β
+ ππ½π + ππ , where
V
= Span {π1 =
β
V
π =
β
β
(67)
β
= (ππ½ π| V + ππ½π ) + ββππ βββββ β V β {π } . D βββββββββββββββββββββββββββββββ β β{π }
βV
V = ker πβ
β
+ ππ½π β V, and π, π, π β
V
Now, by (39), we get
(72)
π } ππ₯3
which is the vertical distribution and the restriction of π to the fibres of π is nondegenerate. The horizontal distribution is β₯
= Span {π1 =
β
= π {π (πβ π ) + π (π) π}
(68) β
π =
= ππ β {π} βΜΈ π½V. We get π½π β V.
β
β
V
β
Hence, π½V β V β {π }; that is, π½V β D β {π½π } β {π }. (ii) Let π = ππ| β
π π π π β ,π = β , ππ₯1 ππ₯2 2 ππ¦1 ππ¦2
H = (ker πβ )
πβ π½ π = π (πβ π) + π (πβ (π)) π
β
π‘ π₯1 + π₯2 π¦1 + π¦2 , , π¦3 ) . β2 β2 (71)
D
+ ππ
β
β
β
β H, where H = D β
{π }, ker πβ = D , and π, π β πΆβ (π). Then π½ π = ππ½ π|
β
D
(69)
β
β
β
β
D
β
2 β
β
+ ππ½π + ππ½ π
= ππ½ π|
β
+ ππ½π + ππ
D
D
β
β
(74)
β
Thus, the smooth map π is a pseudo-Riemannian submersion. Also, we obtain that there exists a 1-form π = ππ₯3 on R63 β
πβ π½ π1 = ππβ π1 + π (π1 ) π, β
(70)
β
β
β
β
β
β
D
π (π2 , π2 ) = π (πβ π2 , πβ π2 ) = 2,
such that π(π½π ) = 1, π(π ) = 0 and the map π satisfies
= π + ππ½π β H β {π½π } , for some π = ππ½ π|
β
horizontal lift π , which is the characteristic vector field on the horizontal distribution H of R63 . We also have
π (π , π ) = π (πβ π , πβ π ) = π (π, π) = 1.
Again, let π β Hβ{π½π }. Then, π = ππ| β +ππ +ππ½π β H,
π½ π = ππ½ π|
π }. ππ¦3
The characteristic vector field π = π/ππ€ on R31 has unique
β
which implies that π½H β H β {π½π }. for π, π, π β πΆβ (π). We have
(73)
π (π1 , π1 ) = π (πβ π1 , πβ π1 ) = β2, β
+ ππ½π β H β {π½π } ,
β
π π π π + ,π = + , ππ₯1 ππ₯2 2 ππ¦1 ππ¦2
+ ππ β H.
We obtain π½ π β H. β β β Hence, π½H β H β {π½(π )}; that is, π½H β D β {π } β β
{π½π }. Example 13. Let (R63 , π½, π) be an almost paracomplex pseudoRiemannian manifold and let (R31 , π, π, π, π) be an almost
πβ π½ π2 = ππβ π2 + π (π2 ) π, β
β
(75)
β
πβ π½π = ππβ π + π (π ) π. Hence, the map π is a paracomplex paracontact pseudoRiemannian submersion from R63 onto R31 . Moreover, we observe that, for this submersion π, we have β
π½V β V β {π } , which verifies Proposition 12.
β
π½H β H β {π½π } ,
(76)
8
Geometry
Proposition 14. Let π : π β π be a paracomplex paracontact pseudo-Riemannian submersion and let the fibres of π be pseudo-Riemannian submanifolds of π. Let π, π be basic vector fields π-related to π, π, respectively. Let πΉ and Ξ¦ be the second fundamental forms and let β and β be the LeviCivita connection on the total manifold π and base manifold π, respectively. Then, one has (i) πβ ((βπ π½)π) = (βπ π)π + ππ(π, βπ π)π + π(π)βππ,
Using Definition 2 and properties of Sections 2.1 and 2.2, we get the following identity: πβ (ππ½ (π, π)) = π(1) (π, π) + 2ππ (ππ, π) π β 2ππ (ππ, π) π + 2π (π) ππ (π, π) π β 2π (π) ππ (π, π) π β π (π) π(3) (π) + π (π) π(3) (π) .
(ii) πΉ = πββ Ξ¦ + ππ β π,
(80)
(iii) πβ ((βπ πΉ)(π, π)) = (βπ Ξ¦)(π, π) + π(π)π(π, βπ π) + π(π)π(π, βπ π). Proof. (i) In view of Definition 2 and Proposition 11, we have
Using (12), (13), (14), and (15), (80) reduces to πβ (ππ½ (π, π)) = π(1) (π, π) + π(2) (π, π) π + π (π) π(4) (π) π
πβ ((βπ π½) π) = πβ (βπ (π½ π) β π½ (βπ π)) = βπ (πβ (π½ π)) β πβ (π½ (βπ π))
β π (π) π(4) (π) π β π (π) π(3) (π)
= βπ (ππ) + βπ (π (π) π) β π (βπ π)
+ π (π) π(3) (π) .
β π (βππ) π = (βπ π) π + βπ (ππ (π, π) π) β π (βππ) π = (βπ π) π + ππ (βπ π, π) π + ππ (π, βπ π) π + ππ (π, π) βπ π β ππ (βπ π, π) π = (βπ π) π + ππ (π, βπ π) π + π (π) βπ π. (77) (ii) Since πββ Ξ¦ is pullback of Ξ¦ through the linear map πβ , we get πββ Ξ¦ (π, π) = Ξ¦ (π, π) β π = π (π, ππ) β π = π (π, π½ π) β ππ (π) π (π)
(78)
= πΉ (π, π) β ππ (π) π (π) ,
= 0, it follows from (81) that Since ππ½ (π, π) (1) (2) (3) tensors π , π , π , and π(4) vanish together. Hence, the almost paracontact structure of base space is normal. Conversely, let the almost paracontact structure of the base space be normal. Then, (81) implies that πβ (ππ½ (π, π)) = 0. Hence, ππ½ (π, π) is vertical. Corollary 16. Let π : π β π be a paracomplex paracontact pseudo-Riemannian submersion and let the fibres of π be pseudo-Riemannian submanifolds of π. Let π, π be basic vector fields π-related to π, π, respectively. Let the total space be para-Hermitian manifold and π(1) vanishes. Then, the base space is paracontact pseudometric manifold if and only if π is killing. Proof. Let the total space be para-Hermitian and π(1) vanishes. Then, from (80), we have
which implies πΉ = πββ Ξ¦ + ππ β π. (iii) By (23), we have πβ ((βπ πΉ) (π, π)) = π (πβ (π) , πβ ((βπ π½) π)) .
(81)
(79)
Now, using (i) in the above equation, we get (iii). Theorem 15. Let π : π β π be a paracomplex paracontact pseudo-Riemannian submersion and let the fibres of π be pseudo-Riemannian submanifolds of π. Let π, π be basic vector fields π-related to π, π, respectively. If the total space is para-Hermitian manifold, then the almost paracontact structure of base space is normal. Moreover, if the almost paracontact structure of base space is normal, then the Nijenhuis tensor of total space is vertical. Proof. The Nijenhuis tensors ππ½ and ππ of almost paracomplex structure π½ and almost paracontact structure π are, respectively, defined by (8) and (11).
0 = 2ππ (ππ, π) π β 2ππ (ππ, π) π + 2π (π) ππ (π, π) π β 2π (π) ππ (π, π) π β π (π) (Lπ π) π + π (π) (Lπ π) π. (82) If π is killing, then we have Lπ π = 0. It immediately follows from (82) that ππ (ππ, π) β π (ππ, π) + π (π) ππ (π, π) β π (π) ππ (π, π) = 0.
(83)
In view of (6) and (7), the above equation gives ππ = Ξ¦. Conversely, let the base space be paracontact. Then, ππ = Ξ¦. Using (6), (7), and (82), we get Lπ π = 0. Hence, the characteristic vector field π is killing.
Geometry
9
Theorem 17. Let π : π β π be a paracomplex paracontact pseudo-Riemannian submersion and let the fibres of π be pseudo-Riemannian submanifolds of π. Let π, π be basic vector fields π-related to π, π, respectively. If the total space is para-KΒ¨ahler, then the base space is paracosymplectic. The converse is true if βπ π½ is vertical. Proof. We have, for any π, π β Ξ(ππ), (βπ π)π = 0, which gives π(π, (βπ π)π) = 0, for any π β Ξ(ππ). From Proposition 14, we have {π (π, (βππ) π) + ππ (π) (βπ π) π + ππ (π) (βπ π) π} β π = π (π, (βπ π½) π) . (84) Let β π½ = 0; that is, the total space is para-KΒ¨ahler. Then, from (84), we obtain βπ = 0 and βπ = 0. Hence, the base space is paracosymplectic. Again, let (βππ)π = 0 and βπ = 0. Then, π(π, (βπ π½)π) = 0, which implies that (βπ π½)π is a vertical vector field.
let the fibres of π be pseudo-Riemannian submanifolds of π. Then, for any horizontal vector fields π, π and for any vertical vector fields π, π on π, one has (i) Aπ (π½ π) = π½(Aπ π), (ii) Aπ½ π (π) = π½(Aπ π), (iii) Tπ(π½ π) = π½(Tππ), (iv) Tπ½ππ = π½(Tππ). Proof. The proof follows using similar steps as in Lemmas 3 and 4 of [13], so we omit it. Lemma 20. Let π : π β π be a paracomplex paracontact pseudo-Riemannian submersion from a para-KΒ¨ahler manifold π onto an almost paracontact pseudometric manifold π and let the fibres of π be pseudo-Riemannian submanifolds of π. Then, for any vector fields πΈ, πΉ on π, one has (i) AπΈ (π½πΉ) = π½(AπΈ πΉ), (ii) TπΈ (π½πΉ) = π½(TπΈ πΉ).
Theorem 18. Let π : π β π be a paracomplex paracontact pseudo-Riemannian submersion and let the fibres of π be pseudo-Riemannian submanifolds of π. Let π, π, and π be basic vector fields π-related to π, π, and π, respectively. If π(π)π(π(π))+π(π)π(π(π))βπ(π)π(π(π)) = 0, then the total space is almost para-KΒ¨ahler if and only if the base space π is an almost paracosymplectic manifold.
Theorem 21. Let π : π β π be a paracomplex paracontact pseudo-Riemannian submersion from a para-KΒ¨ahler manifold π onto an almost paracontact pseudometric manifold π and let the fibres of π be pseudo-Riemannian submanifolds of π. Then, the horizontal distribution is integrable.
Proof. We have the following equation:
Proof. For any vertical vector field π, we have
3ππΉ (π, π, π)
π (π½ (Aπ π) , π) = π (Aπ π½ π, π)
= 3 (πββ πΞ¦) (π, π, π) + 2ππ (π) ππ (π, π)
= βπ (π½ π, Aπ π)
β 2ππ (π) ππ (π, π) + 2ππ (π) ππ (π, π) + 2ππ (π) π (π (π))
Proof. The proof follows from (37) and (38).
(85)
+ 2ππ (π) π (π (π)) β 2ππ (π) π (π (π)) . If ππ = 0, πΞ¦ = 0, and π(π)π(π(π)) + π(π)π(π(π)) β π(π)π(π(π)) = 0, then, from (85), we have ππΉ = 0. Hence, the total space is almost para-KΒ¨ahler. Conversely, let ππΉ = 0 and π(π)π(π(π)) + π(π)π(π(π)) β π(π)π(π(π)) = 0. By using the above equation in (85), we have ππ = 0 and πΞ¦ = 0. Hence, the base space is almost paracosymplectic. Now, we investigate the properties of fundamental tensors T and A of a pseudo-Riemannian submersion. Lemma 19. Let π : π β π be a paracomplex paracontact pseudo-Riemannian submersion from a para-KΒ¨ahler manifold π onto an almost paracontact pseudometric manifold π and
= βπ (π½ π, β (βππ)) = π (π, β (π½ (βππ))) = π (π, β {(ββππ½) π +βπ (π½ π)}) = π (π, β {βπ (π½π)}) = π (π, Aπ½ π π) = βπ (Aπ½ π π, π) = βπ (π½ (Aπ π) , π) . (86) Thus π(π½(Aπ π), π) = 0, which is true for all π and π. So, Aπ π = 0. Hence, the horizontal distribution is integrable. Theorem 22. Let π : π β π be a paracomplex paracontact pseudo-Riemannian submersion from a para-KΒ¨ahler manifold π onto an almost paracontact pseudometric manifold π and let the fibres of π be pseudo-Riemannian submanifolds of π. Then, the submersion is an affine map on H.
10
Geometry
Proof. The second fundamental form of π is defined by π
(βπβ ) (πΈ, πΉ) = (βπΈ πβ (πΉ)) β π β πβ (βπΈ πΉ) ,
(87)
where πΈ, πΉ β Ξ(ππ) and βπ is pullback connection of LeviCivita connection β on π with respect to π. We have, for any π, π β H, π
(βπβ ) (π, π) = (βπ πβ (π)) β π β πβ (βπ π) .
(88)
By using Lemma 1, we have πβ (β(βπ π)) = (βπ π) β π, which implies βπβ = 0. Hence, the submersion π is an affine map on H. Theorem 23. Let π : π β π be a paracomplex paracontact pseudo-Riemannian submersion from a para-Hermitian manifold π onto an almost paracontact pseudometric manifold π and let the fibres of π be pseudo-Riemannian submanifolds of π. Then, the submersion is an affine map on V if and only if the fibres of π are totally geodesic. Proof. We have, for any π, π β V, (βπβ ) (π, π) = βπβ (β (βππ)) ,
(89)
which, in view of (27), gives (βπβ ) (π, π) = βπβ (Tππ) .
Theorem 24. Let π : π β π be a paracomplex paracontact pseudo-Riemannian submersion from a para-Hermitian manifold π onto an almost paracontact pseudometric manifold π and let the fibres of π be pseudo-Riemannian submanifolds of π. Then, the submersion is an affine map if and only if β(βπΈ βπΉ) + AβπΈ VπΉ + TVπΈ VπΉ is π-related to βπ π, for any πΈ, πΉ β Ξ(ππ). Proof. For any πΈ, πΉ β Ξ(ππ) with πβ βπΈ = π β π and πβ VπΉ = π β π, we have (βπβ ) (πΈ, πΉ) = (βπβ βπΈ (πβ βπΉ)) β π β πβ (β (βπΈ πΉ)) = (βπ π) β π β πβ (β (ββπΈ βπΉ + ββπΈ VπΉ +βVπΈ βπΉ + βVπΈ βπΉ)) . (91) By using (27) and (31) in the above equation, we have
+TVπΈ VπΉ) .
4. Curvature Properties In this section, the paraholomorphic bisectional curvatures and paraholomorphic sectional curvatures of total manifold, base manifold, and fibres of paracomplex paracontact pseudo-Riemannian submersion and their curvature properties are studied. Let π : π β π be a paracomplex paracontact pseudoRiemannian submersion from an almost para-Hermitian manifold (π, π½, π) onto an almost paracontact pseudometric manifold (π, π, π, π, π). Suppose that the vector fields πΈ, πΉ span the 2dimensional plane at point π of π and let R be the Riemannian curvature tensor of π. The paraholomorphic bisectional curvature π΅(πΈ, πΉ) of π for any pair of nonzero non-lightlike vector fields πΈ, πΉ on π is defined by the formula
(90)
Let the fibres of π be totally geodesic. Then, T = 0. Consequently, from the above equation, we have βπβ = 0. Thus, the map π is affine on V. Conversely, let the submersion π be an affine map on V. Then, βπβ = 0, which implies T = 0. Hence, the fibres of π are totally geodesic.
(βπβ ) (πΈ, πΉ) = (βπ π) β π β πβ (β (βπΈ βπΉ) + AβπΈ VπΉ
Let the submersion map be affine. Then, for any πΈ, πΉ β Ξ(ππ), (βπβ )(πΈ, πΉ) = 0. Equation (92) implies (βπ π) β π = πβ (β(βπΈ βπΉ) + AβπΈ VπΉ + TVπΈ βπΉ). Conversely, let β(βπΈ πΉ) + AβπΈ VπΉ + TVπΈ βπΉ be π-related to βπ π, for any πΈ, πΉ β Ξ(ππ). Then, from (92), we have (βπβ )(πΈ, πΉ) = 0. Hence, the submersion map π is affine.
π΅ (πΈ, πΉ) =
R (πΈ, π½πΈ, πΉ, π½πΉ) π (πΈ, πΈ) π (πΉ, πΉ)
.
(93)
For a nonzero non-lightlike vector field πΈ, the vector field π½πΈ is also non-lightlike and {πΈ, π½πΈ} span the 2-dimensional plane. Then the paraholomorphic sectional curvature π»(πΈ) is defined as π» (πΈ) = π΅ (πΈ, πΈ) =
R (πΈ, π½πΈ, πΈ, π½πΈ) π (πΈ, πΈ) π (πΈ, πΈ)
.
(94)
The curvature properties of Riemannian submersion and semi-Riemannian submersion have been extensively studied in the work of OβNeill [1] and Gray [3]. β
V
Let π΅ and π΅ be the paraholomorphic bisectional curvatures of horizontal and vertical spaces, respectively. Let β
V
π» and π» be the paraholomorphic sectional curvatures of horizontal and vertical spaces, respectively. Let π΅ and π» be the paraholomorphic bisectional and sectional curvatures of the base manifold, respectively. Proposition 25. Let π : π β π be a paracomplex paracontact pseudo-Riemannian submersion from an almost para-Hermitian manifold onto an almost paracontact pseudometric manifold and let the fibres of π be pseudo-Riemannian submanifolds of π. Let π, π be non-lightlike unit vertical vector fields and let π, π be non-lightlike unit horizontal vector fields on π. Then, one has V
(92)
π΅ (π, π) = π΅ (π, π) + π (Tπ (π½ π) , Tπ½ππ) β π (Tπ½π (π½ π) , Tππ) ,
(95)
Geometry
11
π΅ (π, π) = π ((βπA)π π½ π, π½ π) β π (Aπ π½π, Aπ½ π π) + π (Aπ π, Aπ½ π π½π) β π ((βπ½πA)π π½ π, π)
Proof. Since the fibres are totally geodesic, T = 0; consequently we have V
π» (π) = π» (π) .
+ π (Tπ½ππ, Tπ (π½ π)) β π (Tππ, Tπ½π (π½ π)) , (96) β
π΅ (π, π) = π΅ (π, π) β 2π (Aπ (π½ π) , Aπ (π½ π)) + π (Aπ½ π π, Aπ (π½ π))
(97)
β π (Aπ π, Aπ½ π (π½ π)) . Proof. Using Definitions (93) and (94) of paraholomorphic sectional curvature and fundamental equations of submersion obtained by OβNeill [1], we have (95), (96), and (97). Corollary 26. Let π : π β π be a paracomplex paracontact pseudo-Riemannian submersion from an almost para-Hermitian manifold onto an almost paracontact pseudometric manifold. If the fibres of π are totally geodesic pseudoRiemannian submanifolds of π, then for any non-lightlike unit vertical vector fields π and π, one has V
π΅ (π, π) = π΅ (π, π) .
(98)
Corollary 27. Let π : π β π be a paracomplex paracontact pseudo-Riemannian submersion from an almost paraHermitian manifold onto an almost paracontact pseudometric manifold and let the fibres of π be totally geodesic pseudoRiemannian submanifolds of π. If the horizontal distribution is integrable, then, for any non-lightlike unit horizontal vector fields π and π, one has β
π΅ (π, π) = π΅ (π, π) .
(99)
Proposition 28. Let π : π β π be a paracomplex paracontact pseudo-Riemannian submersion from an almost para-Hermitian manifold onto an almost paracontact pseudometric manifold and let the fibres of π be pseudo-Riemannian submanifolds of π. Let π and π be non-lightlike unit vertical vector field and non-lightlike unit horizontal vector field, respectively. Then, one has V σ΅©2 σ΅© π» (π) = π» (π) + σ΅©σ΅©σ΅©σ΅©Tπ(π½π)σ΅©σ΅©σ΅©σ΅© β π (Tπ½π (π½π) , Tππ) , (100) σ΅© σ΅©2 π» (π) = π» (π) β π β 3σ΅©σ΅©σ΅©σ΅©Aπ (π½ π)σ΅©σ΅©σ΅©σ΅© .
(101)
Proof. The proof is straightforward. If we take π = π in (95) and π = π in (97), we have (98) and (99). Corollary 29. Let π : π β π be a paracomplex paracontact pseudo-Riemannian submersion from an almost para-Hermitian manifold onto an almost paracontact pseudometric manifold. If the fibres of π are totally geodesic pseudoRiemannian submanifolds of π, then the total manifold and fibres of π have the same paraholomorphic sectional curvatures.
(102)
Corollary 30. Let π : π β π be a paracomplex paracontact pseudo-Riemannian submersion from an almost paraHermitian manifold onto an almost paracontact pseudometric manifold and let the fibres of π be totally geodesic pseudoRiemannian submanifolds of π. If the horizontal distribution is integrable, then the base manifold and horizontal distribution have the same paraholomorphic sectional curvatures. Proof. Since the horizontal distribution is integrable, A = 0; consequently, we have π» (π) = π» (π) β π.
(103)
π
Theorem 31. Let π : π β ππ be a paracomplex paracontact pseudo-Riemannian submersion from a paraKΒ¨ahler manifold π onto an almost paracontact pseudometric manifold π and let the fibres of π be pseudo-Riemannian submanifolds of π. If π, π are the non-lightlike unit vertical vector fields and π, π are the non-lightlike unit horizontal vector fields, then one has V
π΅ (π, π) = π΅ (π, π) ,
(104)
σ΅© σ΅©2 π΅ (π, π) = β2σ΅©σ΅©σ΅©σ΅©Tππσ΅©σ΅©σ΅©σ΅© ,
(105)
π΅ (π, π) = π΅ (π, π) β π.
(106)
Proof. Using results of Lemma 19 in (95), we have V
π΅ (π, π) = π΅ (π, π) β π (π½ (Tππ) , π½ (Tππ)) 2
β π (π½ (Tππ) , Tππ) = π΅ (π, π) + π (Tππ, Tππ) β π (Tππ, Tππ) V
= π΅ (π, π) . (107) Applying results of Lemma 19 in (96), we have π΅ (π, π) = π ((βπA)π (π½ π) , π½π) β π ((βπ½πA)π (π½π) , π) σ΅© σ΅©2 σ΅© σ΅©2 + 2σ΅©σ΅©σ΅©Aπ πσ΅©σ΅©σ΅© β 2σ΅©σ΅©σ΅©σ΅©Tππσ΅©σ΅©σ΅©σ΅© .
(108)
Since by Theorem 21 the horizontal distribution is integrable, we have A = 0, which implies σ΅© σ΅©2 π΅ (π, π) = β2σ΅©σ΅©σ΅©σ΅©Tππσ΅©σ΅©σ΅©σ΅© . In view of A = 0, (104) follows from (97).
(109)
12
Geometry π
Theorem 32. Let π : π β ππ be a paracomplex paracontact pseudo-Riemannian submersion from a paraKΒ¨ahler manifold π onto an almost paracontact pseudometric manifold π and let the fibres of π be pseudo-Riemannian submanifolds of π. If π, π are non-lightlike unit vertical and non-lightlike unit horizontal vector fields, respectively, then one has V σ΅©2 σ΅© (110) π» (π) = π» (π) β 2σ΅©σ΅©σ΅©Tππσ΅©σ΅©σ΅© , π» (π) = π» (π) β π.
(111)
Proof. Since π is the paracomplex paracontact pseudoRiemannian submersion from a para-KΒ¨ahler manifold π onto an almost paracontact pseudometric manifold π, by (16) and equations of Lemma 19, we have 2 σ΅© σ΅©2 π (Tπ½π (π½π) , Tππ) = π (π½ (Tππ) , Tππ) = σ΅©σ΅©σ΅©Tππσ΅©σ΅©σ΅© ,
σ΅© σ΅©2 π (Tπ (π½π) , Tπ (π½π)) = βπ (Tππ, Tππ) = βσ΅©σ΅©σ΅©Tππσ΅©σ΅©σ΅© (112) and by using the above results in (100), we have V σ΅©2 σ΅© σ΅©2 σ΅© π» (π) = π» (π) β σ΅©σ΅©σ΅©Tππσ΅©σ΅©σ΅© β σ΅©σ΅©σ΅©Tππσ΅©σ΅©σ΅© V σ΅©2 σ΅© = π» (π) β 2σ΅©σ΅©σ΅©Tππσ΅©σ΅©σ΅© .
(113)
Again, since horizontal distribution is integrable, we have A = 0, and putting it in (101), we obtain (111).
Conflict of Interests The authors declare that there is no conflict of interests regarding the publication of this paper.
Acknowledgment Uma Shankar Verma is thankful to University Grant Commission, New Delhi, India, for financial support.
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