ON GLOBAL RIEMANN-CARTAN GEOMETRY
ON GLOBAL RIEMANN-CARTAN GEOMETRY
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 />
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