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Einstein connection of nonsymmetric pseudo-Riemannian manifold

Vladimir Rovenski, Milan Zlatanović

Abstract

A.~Einstein considered a nonsymmetric (0,2)-tensor $G=g+F$, where $g$ is a pseudo-Riemannian metric and $F\ne0$ is skew-symmetric, and a linear connection $\nabla$ with torsion $T$ such that $(\nabla_X\,G)(Y,Z)=-G(T(X,Y),Z)$. M. Prvanović (1995) obtained the explicit form of the Einstein connection of an almost Hermitian manifold. In this paper, first, we present the result above in coordinate-free form, and then extend it to almost contact metric mani\-folds satisfying the so-called $f^2$-torsion condition. We then derive the Einstein connection of nonsymmetric pseudo-Riemannian, in particular, weak almost Hermitian manifolds $(M,f,g)$, satisfying the $f^2$-torsion condition, where $F(X,Y)=g(X,fY)$, give explicit formulas for the torsion in terms of $\nabla^g F$, $dF$ and a new (1,1)-tensor $\widetilde Q:=-f^2-{\rm Id}$, and show that in the almost Hermitian case, our main result reduces to the coordinate-free form of Prvanović's solution. Finally, we describe special Einstein connections, i.e., the difference tensor has the property~$K_XY=-K_YX$, and indicate the Gray-Hervella classes. Illustrative examples are given, including the construction of a weighted product.

Einstein connection of nonsymmetric pseudo-Riemannian manifold

Abstract

A.~Einstein considered a nonsymmetric (0,2)-tensor , where is a pseudo-Riemannian metric and is skew-symmetric, and a linear connection with torsion such that . M. Prvanović (1995) obtained the explicit form of the Einstein connection of an almost Hermitian manifold. In this paper, first, we present the result above in coordinate-free form, and then extend it to almost contact metric mani\-folds satisfying the so-called -torsion condition. We then derive the Einstein connection of nonsymmetric pseudo-Riemannian, in particular, weak almost Hermitian manifolds , satisfying the -torsion condition, where , give explicit formulas for the torsion in terms of , and a new (1,1)-tensor , and show that in the almost Hermitian case, our main result reduces to the coordinate-free form of Prvanović's solution. Finally, we describe special Einstein connections, i.e., the difference tensor has the property~, and indicate the Gray-Hervella classes. Illustrative examples are given, including the construction of a weighted product.
Paper Structure (6 sections, 16 theorems, 124 equations)

This paper contains 6 sections, 16 theorems, 124 equations.

Key Result

Lemma 2.1

For an Einstein connection $\nabla$, the following conditions are equivalent: (i) $K(X,Y,Z)=-K(X,Z,Y)$, (ii) $\nabla g=0$, (iii) $(\nabla_X F)(Y,Z)=-(\nabla_Y F)(X,Z)$, or $g((\nabla_X f)Z, Y) = -g((\nabla_Y f)Z, X)$.

Theorems & Definitions (39)

  • Lemma 2.1
  • proof
  • Remark 2.2
  • Example 2.3
  • Remark 2.4
  • Lemma 2.5
  • proof
  • Proposition 2.6
  • proof
  • Proposition 2.7: see Proposition 2 of Prvanovic-95
  • ...and 29 more