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ON GLOBAL RIEMANN-CARTAN GEOMETRY

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We know that<br />

5. Vanhecke-Tricerri classification of Riemann-Cartan manifolds<br />

Ň<br />

b<br />

∈ŇĚ<br />

⊗C<br />

∞<br />

2<br />

Λ M<br />

. In turn, the following pointwise O(q)-irreducible decomposition holds<br />

T*M ⊗ Λ 2 M ≅ Ψ 1 (M) ⊕ Ψ 2 (M) ⊕ Ψ 3 (M). In this case, the orthogonal projections on the components of this<br />

decomposition are defined by the following relations:<br />

(1)<br />

Т<br />

Т<br />

b<br />

( )<br />

1 b<br />

b<br />

b<br />

( X ,Y ,Z ) 3 Т ( X ,Y ,Z ) + Т ( Y ,Z, X ) + Т ( Z, X ,Y )<br />

= − ;<br />

( X ,Y ,Z ) = g( X ,Z ) ω( Y ) − g( X ,Y ) ω( Z )<br />

(2) b<br />

;<br />

(3)<br />

Т<br />

b<br />

( )<br />

b<br />

(1) b<br />

(2) b<br />

( X ,Y ,Z ) Т ( X ,Y ,Z ) − Т ( Y ,Z, X ) − Т ( Z, X ,Y )<br />

= ,<br />

b<br />

−1<br />

where Т ( X,<br />

Y,<br />

Z ) = g( T ( X,<br />

Y ),<br />

Z ) and : = ( n −1) trace Т<br />

ω .<br />

[1] Bourguignon J.P. Formules de Weitzenbök en dimension 4. Géométrie Riemannienne en dimension 4: Seminaire<br />

Arthur Besse 1978/79. Paris: Cedic-Fernand Nathan, 1981.<br />

We say that a Riemann-Cartan manifold ( M ,g,∇)<br />

belongs to the class Ψ α or<br />

b<br />

tensor field Т is a section of corresponding tensor bundle Ψ α ( М ) or α ( М ) ⊕Ψβ<br />

( М )<br />

Ψ ⊕Ψ<br />

for , β = 1 , 2,<br />

3<br />

α<br />

Ψ .<br />

β<br />

α and α < β if the<br />

[2] Tricerri F., Vanhecke L. Homogeneous structures. Progress in mathematics (Differential geometry), 32 (1983),<br />

234-246.<br />

The spaces<br />

12<br />

∗<br />

Λ 2 М ⊗Т<br />

М and Т М ⊗Λ М<br />

∗<br />

2<br />

, as well as their irreducible components, are isomorphic. Therefore these<br />

two classifications are equivalent. Moreover, corresponding classes of Riemann-Cartan manifolds from these two<br />

classifications coincide.

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