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ON GLOBAL RIEMANN-CARTAN GEOMETRY

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9. Scalar and complete scalar curvature<br />

of Riemann-Cartan manifolds<br />

It is well known that the curvature tensor R of the linear non-symmetric connection ∇ of a Riemann-Cartan<br />

manifold ( ,g,∇)<br />

2<br />

2<br />

M is a section of the tensor bundle Λ M ⊗ Λ M . Therefore the scalar curvature of the Riemann-<br />

Cartan manifold ( ,g,∇)<br />

a Riemannian manifold (M, g).<br />

n<br />

M we can define by the formula s ∑ R( e ,e ,e ,e )<br />

_<br />

= as an analogy to the scalar curvature s of<br />

The dependence between the scalar curvatures s and s is described in the following formula<br />

i = 1<br />

( 1) b<br />

2<br />

( ) ( 2 ) b<br />

2 ( 3 ) b<br />

2<br />

b<br />

= s − S −2<br />

n −2<br />

S + 2 S − div ( trace S ). (9.1)<br />

s 4<br />

In particular, for the Weitzenböck connection ∇ we have the identity s = 0. Then the formula (9.1) can be rewritten in<br />

the following form<br />

( 1) b<br />

2<br />

( ) ( 2 ) b<br />

2 ( 3 ) b<br />

2<br />

b<br />

S + 2 n −2<br />

S −2<br />

S 4div ( traceS )<br />

s = +<br />

.<br />

i<br />

j<br />

i<br />

j<br />

[1] Yano K., Bochner S. Curvature and Betti number. Princeton: Princeton University Press, 1953.<br />

[2] Stepanov S.E., Gordeeva I.A. Pseudo-Killing and pseudo harmonic vector field on a Riemann-Cartan manifold.<br />

Mathematical Notes, 87: 2 (2010), 238-247.<br />

19

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