Generalized Sasakian-space-forms Admitting 𝑾 𝟐 -curvature Tensor
Abhishek Kushwaha
1*and Dhruwa Narain
21&2
Department of Mathematics and Statistics,
D. D. U. Gorakhpur University, Gorakhpur (U.P.) – 273009, INDIA.
email:
1[email protected] and
2[email protected].
(Received on: June 8, 2019)
ABSTRACT
The aim of present paper is to study 𝜉−𝑊2 flat, 𝜙 − 𝑊2 flat, pseudo-𝑊2
flat and quasi−𝑊2 flat generalized Sasakian-space-forms. Further we study 𝜙 − 𝑊2 semi-symmetric generalized Sasakian-space-forms.
AMS Subject Classification No. 53C25, 53D15.
Keywords: Generalized Sasakian-space-forms, 𝜉 − 𝑊2 flat, 𝜙 − 𝑊2 flat, pseudo-𝑊2
flat, quasi−𝑊2 flat and 𝜙 − 𝑊2 semi-symmetric.
1. INTRODUCTION
In differential geometry of contact metric manifolds the nature of Riemannian manifolds depends on the curvature tensor 𝑅 of the manifolds. It is well known that the sectional curvatures of a manifold determine the curvature tensor 𝑅 completely. A Riemannian manifold with constant sectional curvature c is known as real-space-form and it’s curvature tensor 𝑅 satisfied the condition
𝑅(𝑋, 𝑌)𝑍 = 𝑐{𝑔(𝑌, 𝑍)𝑋 − 𝑔(𝑋, 𝑍)𝑌}. (1.1) Representation of these spaces are hyperbolic spaces (𝑐 < 0), the Euclidean spaces (𝑐 = 0) and the spheres (c > 0).
In contact geometry, a Sasakian manifold with constant 𝜙-sectional curvature is called Sasakian-space-forms and it has a specific form of curvature tensor. In (2004) P. Alegre, D.
Blair and A. Carriazo
10introduced the notation of generalized Sasakian-space-forms. An
almost contact metric manifold (𝑀
2𝑛+1, 𝜙, 𝜉, 𝜂, 𝑔) is said to be generalized Sasakian-space-
forms if there exist three differentiable functions 𝑓
1, 𝑓
2and 𝑓
3on 𝑀
2𝑛+1such that the curvature
tensor 𝑅 is given by
𝑅(𝑋, 𝑌)𝑍 = 𝑓
1{𝑔(𝑌, 𝑍)𝑋 − 𝑔(𝑋, 𝑍)𝑌}
+𝑓
2{𝑔(𝑋, 𝜙𝑍)𝜙𝑌 − 𝑔(𝑌, 𝜙𝑍)𝜙𝑋 + 2𝑔(𝑋, 𝜙𝑌)𝜙𝑍}
+𝑓
3{𝜂(𝑋)𝜂(𝑍)𝑌 − 𝜂(𝑌)𝜂(𝑍)𝑋 + 𝑔(𝑋, 𝑍)𝜂(𝑌)𝜉 − 𝑔(𝑌, 𝑍)𝜂(𝑋)𝜉}, (1.2) for any vector fields 𝑋, 𝑌, 𝑍 on 𝑀
2𝑛+1. In such case we denote the manifold as 𝑀
2𝑛+1(𝑓
1, 𝑓
2, 𝑓
3). In
10the authors give several examples of generalized Sasakian-space-forms.
If 𝑓
1=
𝑐+34, 𝑓
2=
𝑐−14and 𝑓
3=
𝑐−14, where c denotes 𝜙-sectional curvature, then a generalized Sasakian-space-forms with Sasakian structure becomes a Sasakian-space-forms.
A Riemannian manifold (𝑀
2𝑛+1, 𝑔) is called locally symmetric if its curvature tensor 𝑅 is parallel, i.e., ∇𝑅 = 0, where ∇ is the Levi-Civita connection. The notation of semi-symmetric, a proper generalization of locally symmetric manifold, is defined by 𝑅(𝑋, 𝑌). 𝑅 = 0, where 𝑅(𝑋, 𝑌) acts on 𝑅 as derivation. A complete intrinsic classification of these manifolds was given by Z. I. Szabo
20. Kushwaha and Narain
2studied some curvature properties on Sasakian manifold. Also Kushwaha and Narain
3studied projective and conformal curvature tensor in 𝐾-contact 𝜂-Einstein manifolds. In a Sasakian manifolds the Ricci operator 𝑄 commutes with 𝜙 i.e., 𝜙𝑄 = 𝑄𝜙. In
16it has been shown that there exist 𝐾-contact manifold with 𝜙𝑄 = 𝑄𝜙, which is not Sasakian. It is to be noted that a 𝐾-contact manifold being intermediate between a contact metric manifold and a Sasakian manifold.
In 1970 Mishra and Pokhariyal
9defined the 𝑊
2-curvature tensor, given by
𝑊
2(𝑋, 𝑌)𝑍 = 𝑅(𝑋, 𝑌)𝑍 +
2𝑛1{𝑔(𝑋, 𝑍)𝑄𝑌 − 𝑔(𝑌, 𝑍)𝑄𝑋}, (1.3) where 𝑅 is the curvature tensor and 𝑄 is the Ricci-operator, i.e.,
𝑔(𝑄𝑋, 𝑌) = 𝑆(𝑋, 𝑌)for all 𝑋, 𝑌.
The generalized Sasakian-space-forms have been studied by several authors
1,10,11, D.
Narain, S. Yadav and Dwivedi
7, De and Sarkar
17,18, Alegre and Carriazo
12and many other authors. Many geometers studied the 𝑊
2-curvature tensor on different manifolds such as De and Sarkar
19, A. A. Shaikh, S. K. Jana and S. Eyasmin
4, Yilidiz and De
5, A. Taleshian and A.
A. Husseinzadeh
6and many others.
Motivated by above studies, the object of present paper is to study the properties of 𝑊
2-curvature tensor in a generalized Sasakian-space-forms. The present paper is organized as follows. Section 2 is concerned with preliminaries. In section 3 we study 𝜉 − 𝑊
2flat generalized Sasakian-space-forms. Section 4 is devoted to study of 𝜙 − 𝑊
2flat generalized Sasakian-space-forms. Further section 5 deals with pseudo-𝑊
2flat generalized Sasakian- space-forms and it is shown that pseudo-𝑊
2flat generalized Sasakian-space-forms is a special type of 𝜂-Einstein manifolds. In section 6 we study quasi−𝑊
2flat generalized Sasakian-space- forms and finally in last section, we study 𝜙 − 𝑊
2semi-symmetric generalized Sasakian- space forms.
2. PRELIMINARIES
A (2𝑛 + 1)-dimensional Riemannian manifold 𝑀
2𝑛+1(𝜙, 𝜉, 𝜂, 𝑔), where 𝜙 is a
tensor field, ξ is a contravariant vector field, 𝜂 is a 1-form and 𝑔 is a Riemannian metric, is
called an almost contact metric manifold if the following results holds
8,13,14:
𝜙
2𝑋 = −𝑋 + 𝜂(𝑋)𝜉, 𝜙𝜉 = 0, (2.1) 𝜂(𝜉) = 1, 𝑔(𝑋, 𝜉) = 𝜂(𝑋), 𝜂(𝜙𝑋) = 0, (2.2) 𝑔(𝜙𝑋, 𝜙𝑌) = 𝑔(𝑋, 𝑌) − 𝜂(𝑋)𝜂(𝑌), (2.3) 𝑔(𝜙𝑋, 𝑌) = −𝑔(𝑋, 𝜙𝑌), 𝑔(𝜙𝑋, 𝑋) = 0, (2.4) (∇
𝑋𝜂)(𝑌) = 𝑔(∇
𝑋𝜉, 𝑌). (2.5) For a (2𝑛 + 1)-dimensional generalized Sasakian-space-forms
10, the curvature tensor 𝑅, the Ricci tensor 𝑆 and Ricci operator 𝑄 satisfy
𝑅(𝑋, 𝑌)𝜉 = (𝑓
1− 𝑓
3){𝜂(𝑌)𝑋 − 𝜂(𝑋)𝑌}, (2.6) 𝑅(𝜉, 𝑋)𝑌 = (𝑓
1− 𝑓
3){𝑔(𝑋, 𝑌)𝜉 − 𝜂(𝑌)𝑋}, (2.7) 𝑅(𝜉, 𝑋)𝜉 = (𝑓
1− 𝑓
3){𝜂(𝑋)𝜉 − 𝑋}, (2.8) 𝑆(𝑋, 𝑌) = (2𝑛𝑓
1+ 3𝑓
2− 𝑓
3)𝑔(𝑋, 𝑌) − (3𝑓
2+ (2𝑛 − 1)𝑓
3)𝜂(𝑋)𝜂(𝑌), (2.9) 𝑆(𝑋, 𝜉) = 2𝑛(𝑓
1− 𝑓
3)𝜂(𝑋), (2.10) 𝑄𝑋 = (2𝑛𝑓
1+ 3𝑓
2− 𝑓
3)𝑋 − (3𝑓
2+ (2𝑛 − 1)𝑓
3)𝜂(𝑋)𝜉, (2.11) 𝑟 = 2𝑛(2𝑛 + 1)𝑓
1+ 6𝑛𝑓
2− 4𝑛𝑓
3, (2.12) 𝜂(𝑅(𝑋, 𝑌)𝑍) = (𝑓
1− 𝑓
3){𝑔(𝑌, 𝑍)𝜂(𝑋) − 𝑔(𝑋, 𝑍)𝜂(𝑌)}, (2.13) 𝜂(𝑅(𝑋, 𝑌)𝜉) = 0, (2.14) 𝜂(𝑅(𝜉, 𝑋)𝑌) = (𝑓
1− 𝑓
3){𝑔(𝑋, 𝑌) − 𝜂(𝑋)𝜂(𝑌)}, (2.15) 𝑆(𝜙𝑋, 𝜙𝑌) = 𝑆(𝑋, 𝑌) − 2𝑛(𝑓
1− 𝑓
3)𝜂(𝑋)𝜂(𝑌). (2.16) An almost contact manifold 𝑀
2𝑛+1is said to be 𝜂-Einstein if it’s Ricci tensor 𝑆 is of the form 𝑆 = 𝐴𝑔 + 𝐵𝜂 ⊗ 𝜂, (2.17) where A and B are smooth function on the manifold, 𝜂 is called the associated 1-form and vector field 𝜉 defined by
𝑔(𝑋, 𝜉) = 𝜂(𝑋), (2.18) is called the generator. If 𝐵 = 0 then the manifold is Einstein and if 𝐴 = 0 then the manifold is special type of 𝜂-Einstein.
3. 𝝃 − 𝑾
𝟐FLAT GENERALIZED SASAKIAN SPACE FORMS
Definition 3.1. An almost contact metric manifold (𝑀
2𝑛+1, 𝑔), 𝑛 > 1, is said to be 𝜉 − 𝑊
2flat if it satisfies the condition 𝑊
2(𝑋, 𝑌)𝜉 = 0 on M, for all 𝑋, 𝑌 ∈ 𝜒(𝑀).
Let M be a (2𝑛 + 1)-dimensional 𝜉 − 𝑊
2flat generalized Sasakian-space-forms then from (1.3), we have
𝑅(𝑋, 𝑌)𝜉 +
2𝑛1{𝑔(𝑋, 𝜉)𝑄𝑌 − 𝑔(𝑌, 𝜉)𝑄𝑋} = 0. (3.1) Using (2.6) and (2.11) in (3.1), we have
(3𝑓
2+ (2𝑛 − 1)𝑓
3){𝜂(𝑌)𝑋 − 𝜂(𝑋)𝑌} = 0. (3.2) Since {𝜂(𝑌)𝑋 − 𝜂(𝑋)𝑌} ≠ 0, therefore (3.2) yields
𝑓
3=
(1−2𝑛)3𝑓2. (3.3) Thus we can state the following theorem:
Theorem 3.1. If a (2𝑛 + 1)-dimensional generalized Sasakian-space-forms is 𝜉 − 𝑊
2flat
then 𝑓
3=
(1−2𝑛)3𝑓2.
Conversely, we assume that (3.3) holds.
Now in view of (1.3), we have
𝑊
2(𝑋, 𝑌)𝜉 = 𝑅(𝑋, 𝑌)𝜉 +
2𝑛1{𝑔(𝑋, 𝜉)𝑄𝑌 − 𝑔(𝑌, 𝜉)𝑄𝑋}. (3.4) Using (2.6) and (2.11) in (3.1), we have
𝑊
2(𝑋, 𝑌)𝜉 = [(𝑓
1− 𝑓
3) −
2𝑛1(2𝑛𝑓
1+ 3𝑓
2− 𝑓
3)] {𝜂(𝑌)𝑋 − 𝜂(𝑋)𝑌}. (3.5) In view of (3.3) and (3.5), we obtain
𝑊
2(𝑋, 𝑌)𝜉 = 0.
Hence we can state the following theorem:
Theorem 3.2. A (2𝑛 + 1)-dimensional generalized Sasakian-space-forms is 𝜉 − 𝑊
2flat if and only if 𝑓
3=
(1−2𝑛)3𝑓2.
S. K. Hui and A. Sarkar
15proved that a (2𝑛 + 1)-dimensional generalized Sasakian-space- forms is 𝑊
2-flat if and only if 𝑓
3=
(1−2𝑛)3𝑓2.
Thus, in view of above statement and by virtue of theorem 3.2 we can state the following theorem:
Theorem 3.3. In a (2𝑛 + 1)-dimensional generalized Sasakian-space-forms following statements are equivalent:
(i) 𝑊
2−flat (ii) 𝑓
3=
(1−2𝑛)3𝑓2(iii) 𝜉 − 𝑊
2flat.
4. 𝝓 − 𝑾
𝟐FLAT GENERALIZED SASAKIAN-SPACE-FORMS
Definition 4.1. An almost contact metric manifold (𝑀
2𝑛+1, 𝑔), 𝑛 > 1, is said to be 𝜙 − 𝑊
2flat if it satisfies the condition
𝑔(𝑊2(𝜙𝑋, 𝜙𝑌)𝜙𝑍, 𝜙𝑊) = 0on
𝑀2𝑛+1, for all
𝑋, 𝑌, 𝑍, 𝑊 ∈ 𝜒(𝑀). Let M be a (2𝑛 + 1)-dimensional 𝜙 − 𝑊
2flat generalized Sasakian-space-forms then from (1.3), we have
𝑔{𝑅((𝜙𝑋, 𝜙𝑌)𝜙𝑍, 𝜙𝑊)} +
2𝑛1{𝑔(𝜙𝑋, 𝜙𝑍)𝑆(𝜙𝑌, 𝜙𝑊) − 𝑔(𝜙𝑌, 𝜙𝑍)𝑆(𝜙𝑋, 𝜙𝑊)} = 0. (4.1) Using (1.2) and (2.9) in (4.1), we obtain
{𝑓
1− (2𝑛𝑓
1+ 3𝑓
2− 𝑓
3)
2𝑛 } {𝑔(𝜙𝑌, 𝜙𝑍)𝑔(𝜙𝑋, 𝜙𝑊) − 𝑔(𝜙𝑋, 𝜙𝑍)𝑔(𝜙𝑌, 𝜙𝑊)}
+𝑓
2{𝑔(𝜙𝑋, 𝑍)𝑔(𝑌, 𝜙𝑊) − 𝑔(𝜙𝑌, 𝑍)𝑔(𝑋, 𝜙𝑊) + 2𝑔(𝜙𝑋, 𝑌)𝑔(𝑍, 𝜙𝑊)} = 0. (4.2) Contracting 𝑌 and 𝑍 in (4.2), we get
{𝑓
1−
(2𝑛𝑓1+3𝑓2−𝑓3)2𝑛
} {2𝑛𝑔(𝜙𝑋, 𝜙𝑊) − 𝑔(𝜙
2𝑋, 𝜙
2𝑊)} + 3𝑓
2𝑔(𝜙𝑋, 𝜙𝑊) = 0. (4.3) Using (2.1) and (2.3) in (4.3), we obtain
[(2𝑛 − 1) {𝑓
1−
(2𝑛𝑓1+3𝑓2−𝑓3)2𝑛
} + 3𝑓
2] 𝑔(𝜙𝑋, 𝜙𝑊) = 0. (4.4)
Since 𝑔(𝜙𝑋, 𝜙𝑊) ≠ 0, therefore (4.4) yields 𝑓
3= 3𝑓
2(1 − 2𝑛) .
Thus we can state the following theorem:
Theorem 4.1. If a (2𝑛 + 1)-dimensional generalized Sasakian-space-forms is 𝜙 − 𝑊
2flat then 𝑓
3=
(1−2𝑛)3𝑓2.
5. PSEUDO - 𝑾
𝟐FLAT GENERALIZED SASAKIAN-SPACE-FORMS
Definition 5.1. An almost contact metric manifold (𝑀
2𝑛+1, 𝑔), 𝑛 > 1, is said to be pseudo-𝑊
2flat if it satisfies the condition 𝑔(𝑊
2(𝜙𝑋, 𝑌)𝑍, 𝜙𝑊) = 0 on 𝑀
2𝑛+1, for all 𝑋, 𝑌, 𝑍, 𝑊 ∈ 𝜒(𝑀).
Let us consider a (2𝑛 + 1)-dimensional pseudo-𝑊
2flat generalized Sasakian-space- forms then from (1.3) we have
𝑔(𝑅(𝜙𝑋, 𝑌)𝑍, 𝜙𝑊) =
2𝑛1[𝑔(𝑌, 𝑍)𝑆(𝜙𝑋, 𝜙𝑊) − 𝑔(𝜙𝑋, 𝑍)𝑆(𝑌, 𝜙𝑊)]. (5.1) Let us take an orthonormal basis {𝑒
1, 𝑒
2, ……..,𝑒
2𝑛, 𝜉} in
𝑀2𝑛+1.Putting
𝑌 = 𝑍 = 𝑒𝑖in (5.1), we get
∑2𝑛𝑖=1𝑔(𝑅(𝜙𝑋,𝑒𝑖, 𝑒𝑖, 𝜙𝑊)) = 2𝑛1 {∑2𝑛 𝑔(𝑒𝑖, 𝑒𝑖
𝑖=1 )𝑆(𝜙𝑋, 𝜙𝑊) − ∑2𝑛𝑖=1𝑔(𝜙𝑋, 𝑒𝑖)𝑆(𝑒𝑖, 𝜙𝑊)}
(5.2) In a (2𝑛 + 1)-dimensional almost contact metric manifold if {𝑒
1, 𝑒
2, ……..,𝑒
2𝑛, 𝜉} is a local orthonormal basis of vector fields in 𝑀
2𝑛+1then {𝜙𝑒
1, 𝜙𝑒
2, ……..,𝜙𝑒
2𝑛, 𝜉} is also a local orthonormal basis. It is easy to verify that
∑
2𝑛𝑖=1𝑔(𝑒
𝑖, 𝑒
𝑖) = ∑
2𝑛𝑖=1𝑔(𝜙𝑒
𝑖, 𝜙𝑒
𝑖) = 2𝑛, (5.3)
∑
2𝑛𝑖=0𝑔(𝜙𝑋, 𝑒
𝑖)𝑔(𝑒
𝑖, 𝜙𝑊) = ∑
2𝑛𝑖=0𝑔(𝜙𝑋, 𝜙𝑒
𝑖)𝑔(𝜙𝑒
𝑖, 𝜙𝑊) = 𝑔(𝜙𝑋, 𝜙𝑊), (5.4)
∑
2𝑛𝑖=0𝑔(𝑋, 𝑒
𝑖)𝑔(𝑒
𝑖, 𝜙𝑊) = ∑
2𝑛𝑖=0𝑔(𝑋, 𝜙𝑒
𝑖)𝑔(𝜙𝑒
𝑖, 𝜙𝑊) = 𝑔(𝑋, 𝜙𝑊), (5.5)
∑
2𝑛𝑖=1𝑔(𝜙𝑋, 𝑒
𝑖)𝑆(𝑒
𝑖, 𝜙𝑊) = 𝑆(𝜙𝑋, 𝜙𝑊). (5.6)
∑
2𝑛𝑖=1𝑔(𝑋, 𝑒
𝑖)𝑆(𝑒
𝑖, 𝜙𝑊) = 𝑆(𝑋, 𝜙𝑊). (5.7) Using (1.2), (5.3), (5.4) and (5.6) in (5.2), we obtain
[(2𝑛 − 1)𝑓
1+ 3𝑓
2]𝑔(𝜙𝑋, 𝜙𝑊) = (1 −
2𝑛1) 𝑆(𝜙𝑋, 𝜙𝑊). (5.8) In view of (2.3), (2.16) and (5.8), we have
𝑆(𝑋, 𝑊) = 𝐴𝑔(𝑋, 𝑊) + 𝐵𝜂(𝑋)𝜂(𝑊), where 𝐴 = [2𝑛𝑓
1+
6𝑛𝑓2(2𝑛−1)
] and 𝐵 = [−2𝑛𝑓
3−
6𝑛𝑓2(2𝑛−1)
] . Thus we can state the following theorem:
Theorem 5.1. A (2𝑛 + 1)-dimensional pseudo−𝑊
2flat generalized Sasakian-space-forms is a 𝜂-Einstein manifold.
6. QUASI - 𝑾
𝟐FLAT GENERALIZED SASAKIAN-SPACE-FORMS
Definition 6.1. An almost contact metric manifold (𝑀
2𝑛+1, 𝑔), 𝑛 > 1, is said to be quasi-𝑊
2flat if it satisfies the condition 𝑔(𝑊
2(𝑋, 𝑌)𝑍, 𝜙𝑊) = 0 on 𝑀
2𝑛+1, for all X,Y, 𝑍, 𝑊 ∈ 𝜒(𝑀).
Let us consider a (2𝑛 + 1)-dimensional quasi-𝑊
2flat generalized Sasakian-space-forms then from (1.3), we have
𝑔(𝑅(𝑋, 𝑌)𝑍, 𝜙𝑊) =
2𝑛1[𝑔(𝑌, 𝑍)𝑆(𝑋, 𝜙𝑊) − 𝑔(𝑋, 𝑍)𝑆(𝑌, 𝜙𝑊)]. (6.1) Let us take an orthonormal basis {𝑒
1, 𝑒
2, ……..,𝑒
2𝑛, 𝜉} in 𝑀
2𝑛+1. Putting 𝑌 = 𝑍 = 𝑒
𝑖in (6.1), we get
∑
2𝑛𝑖=1𝑔(𝑅(𝑋, 𝑒
𝑖, 𝑒
𝑖, 𝜙𝑊)) =
2𝑛1{∑
2𝑛𝑖=1𝑔(𝑒
𝑖, 𝑒
𝑖)𝑆(𝑋, 𝜙𝑊) − ∑
2𝑛𝑖=1𝑔(𝑋, 𝑒
𝑖)𝑆(𝑒
𝑖, 𝜙𝑊) }. (6.2) Using (1.2), (5.3), (5.5) and (5.7) in (6.2), we obtain
[(2𝑛 − 1)𝑓
1+ 3𝑓
2]𝑔(𝑋, 𝜙𝑊) = (1 −
2𝑛1) 𝑆(𝑋, 𝜙𝑊). (6.3) Replacing 𝑊 by 𝜙𝑊 in (6.3) and then using (2.1), we get
𝑆(𝑋, 𝑊) = 𝐴𝑔(𝑋, 𝑊) + 𝐵𝜂(𝑋)𝜂(𝑊), where 𝐴 = [2𝑛𝑓
1+
6𝑛𝑓2(2𝑛−1)
] and 𝐵 = [−2𝑛𝑓
3−
6𝑛𝑓2(2𝑛−1)
] . Thus we can state the following theorem:
Theorem 6.1. A (2𝑛 + 1)-dimensional quasi−𝑊
2flat generalized Sasakian-space-forms is a 𝜂-Einstein manifold.
7. 𝜙- 𝑾
𝟐SEMI-SYMMETRIC FLAT GENERALIZED SASAKIAN-SPACE-FORMS Definition 7.1: An almost contact metric manifold (𝑀
2𝑛+1, 𝑔), 𝑛 > 1, is said to be 𝜙-𝑊
2semi-symmetric if it satisfies the condition 𝑊
2(𝑋, 𝑌). 𝜙 = 0 on 𝑀
2𝑛+1, for all 𝑋, 𝑌 ∈ 𝜒(𝑀).
Let us consider a (2𝑛 + 1)-dimensional 𝜙- 𝑊
2semi-symmetric generalized Sasakian-space- forms then 𝑊
2(𝑋, 𝑌). 𝜙 = 0 reduces in to
(𝑊
2(𝑋, 𝑌). 𝜙)𝑍 = 𝑊
2(𝑋, 𝑌)𝜙𝑍 − 𝜙𝑊
2(𝑋, 𝑌)𝑍 = 0, (7.1) for any vector fields 𝑋, 𝑌 and 𝑍 ∈ 𝜒(𝑀).
Now by virtue of (1.3) and (7.1), we have
𝑅(𝑋, 𝑌)𝜙𝑍 − 𝜙𝑅(𝑋, 𝑌)𝑍 +
2𝑛1{𝑔(𝑋, 𝜙𝑍)𝑄𝑌 − 𝑔(𝑌, 𝜙𝑍)𝑄𝑋
−𝑔(𝑋, 𝑍)𝜙𝑄𝑌 + 𝑔(𝑌, 𝑍)𝜙𝑄𝑋} = 0. (7.2) Using (1.2), (2.1), (2.2) and (2.11) in (7.2), we have
𝑓
1[𝑔(𝑌, 𝜙𝑍)𝑋 − 𝑔(𝑋, 𝜙𝑍)𝑌 − 𝑔(𝑌, 𝑍)𝜙𝑋 + 𝑔(𝑋, 𝑍)𝜙𝑌]
+ 𝑓
2[−𝑔(𝑋, 𝑍)𝜙𝑌 + 𝜂(𝑋)𝜂(𝑍)𝜙𝑌 + 𝑔(𝑌, 𝑍)𝜙𝑋 − 𝜂(𝑌)𝜂(𝑍)𝜙𝑋 +𝑔(𝑋, 𝜙𝑍)𝑌 − 𝜂(𝑌)𝑔(𝑋, 𝜙𝑍)𝜉 − 𝑔(𝑌, 𝜙𝑍)𝑋 + 𝜂(𝑋)𝑔(𝑌, 𝜙𝑍)𝜉]
+𝑓
3[𝑔(𝑋, 𝜙𝑍)𝜂(𝑌)𝜉 − 𝑔(𝑌, 𝜙𝑍)𝜂(𝑋)𝜉 − 𝜂(𝑋)𝜂(𝑍)𝜙𝑌 + 𝜂(𝑌)𝜂(𝑍)𝜙𝑋]
+
12𝑛