Difference between revisions of "Hermitian connection"
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− | + | An [[Affine connection|affine connection]] on a Hermitian manifold $ M $ | |
+ | relative to which the tensor $ \phi $ | ||
+ | defined by the complex structure and the fundamental $ 2 $- | ||
+ | form $ \Omega = ( 1 / 2 ) g _ {\alpha \beta } \omega ^ \beta \wedge \overline \omega \; {} ^ \alpha $ | ||
+ | are parallel, implying the same property for the Hermitian form $ ds ^ {2} = g _ {\alpha \beta } \overline \omega \; {} ^ \alpha \omega ^ \beta $. | ||
+ | If the affine connection on $ M $ | ||
+ | is given by local connection forms $ \omega _ \beta ^ \alpha = \Gamma _ {\beta \gamma } ^ \alpha \omega ^ \gamma + \Gamma _ {\beta {\overline \gamma \; } } ^ \alpha \overline \omega \; {} ^ \gamma $, | ||
+ | then these conditions can be expressed as | ||
− | + | $$ | |
+ | \omega _ {down - 3 {\overline \beta \; } } ^ \alpha = \omega _ {down - 3 {\overline \beta \; } } ^ {\overline \alpha \; } = 0,\ \ | ||
+ | \omega _ {down - 3 {\overline \beta \; } } ^ {\overline \alpha \; } = \ | ||
+ | \overline \omega \; {} _ \beta ^ \alpha , | ||
+ | $$ | ||
− | A generalization is an almost-Hermitian connection, which is defined by similar conditions on the tensors | + | $$ |
+ | d g _ {\alpha \beta } = \overline \omega \; {} _ \alpha ^ \gamma g _ {\gamma \beta } + g _ {\alpha \gamma } \omega _ \beta ^ \gamma . | ||
+ | $$ | ||
+ | |||
+ | On a given Hermitian manifold $ M $ | ||
+ | there is one and only one Hermitian connection for which $ \Gamma _ {\beta \overline \gamma \; } ^ \alpha = 0 $. | ||
+ | |||
+ | A generalization is an almost-Hermitian connection, which is defined by similar conditions on the tensors $ \phi _ {j} ^ {i} $ | ||
+ | and $ g _ {ij} $ | ||
+ | with $ g _ {kl} \phi _ {i} ^ {k} \phi _ {l} ^ {l} = g _ {ij} $ | ||
+ | on an almost-Hermitian manifold $ \widetilde{M} $. | ||
+ | An almost-Hermitian connection on a given $ \widetilde{M} $ | ||
+ | exists. It is uniquely defined by its torsion tensor: If the torsion tensors of two almost-Hermitian connections are the same, then so are the connections. For example, there is one and only one almost-Hermitian connection for which the torsion forms are sums of "pure" forms (that is, forms of type $ ( 2 , 0 ) $ | ||
+ | and $ ( 0 , 2 ) $), | ||
+ | namely, the second canonical Lichnerowicz connection. | ||
====References==== | ====References==== | ||
<table><TR><TD valign="top">[1]</TD> <TD valign="top"> A. Lichnerowicz, "Global theory of connections and holonomy groups" , Noordhoff (1976) (Translated from French)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> K. Yano, "Differential geometry on complex and almost complex spaces" , Pergamon (1965)</TD></TR></table> | <table><TR><TD valign="top">[1]</TD> <TD valign="top"> A. Lichnerowicz, "Global theory of connections and holonomy groups" , Noordhoff (1976) (Translated from French)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> K. Yano, "Differential geometry on complex and almost complex spaces" , Pergamon (1965)</TD></TR></table> | ||
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====Comments==== | ====Comments==== |
Revision as of 22:10, 5 June 2020
An affine connection on a Hermitian manifold $ M $
relative to which the tensor $ \phi $
defined by the complex structure and the fundamental $ 2 $-
form $ \Omega = ( 1 / 2 ) g _ {\alpha \beta } \omega ^ \beta \wedge \overline \omega \; {} ^ \alpha $
are parallel, implying the same property for the Hermitian form $ ds ^ {2} = g _ {\alpha \beta } \overline \omega \; {} ^ \alpha \omega ^ \beta $.
If the affine connection on $ M $
is given by local connection forms $ \omega _ \beta ^ \alpha = \Gamma _ {\beta \gamma } ^ \alpha \omega ^ \gamma + \Gamma _ {\beta {\overline \gamma \; } } ^ \alpha \overline \omega \; {} ^ \gamma $,
then these conditions can be expressed as
$$ \omega _ {down - 3 {\overline \beta \; } } ^ \alpha = \omega _ {down - 3 {\overline \beta \; } } ^ {\overline \alpha \; } = 0,\ \ \omega _ {down - 3 {\overline \beta \; } } ^ {\overline \alpha \; } = \ \overline \omega \; {} _ \beta ^ \alpha , $$
$$ d g _ {\alpha \beta } = \overline \omega \; {} _ \alpha ^ \gamma g _ {\gamma \beta } + g _ {\alpha \gamma } \omega _ \beta ^ \gamma . $$
On a given Hermitian manifold $ M $ there is one and only one Hermitian connection for which $ \Gamma _ {\beta \overline \gamma \; } ^ \alpha = 0 $.
A generalization is an almost-Hermitian connection, which is defined by similar conditions on the tensors $ \phi _ {j} ^ {i} $ and $ g _ {ij} $ with $ g _ {kl} \phi _ {i} ^ {k} \phi _ {l} ^ {l} = g _ {ij} $ on an almost-Hermitian manifold $ \widetilde{M} $. An almost-Hermitian connection on a given $ \widetilde{M} $ exists. It is uniquely defined by its torsion tensor: If the torsion tensors of two almost-Hermitian connections are the same, then so are the connections. For example, there is one and only one almost-Hermitian connection for which the torsion forms are sums of "pure" forms (that is, forms of type $ ( 2 , 0 ) $ and $ ( 0 , 2 ) $), namely, the second canonical Lichnerowicz connection.
References
[1] | A. Lichnerowicz, "Global theory of connections and holonomy groups" , Noordhoff (1976) (Translated from French) |
[2] | K. Yano, "Differential geometry on complex and almost complex spaces" , Pergamon (1965) |
Comments
The first and second canonical connections on an almost-Hermitian manifold are described in [1], p. 192 and pp. 194-195, respectively.
References
[a1] | S. Kobayashi, K. Nomizu, "Foundations of differential geometry" , 2 , Interscience (1969) |
[a2] | R.O. Wells jr., "Differential analysis on complex manifolds" , Springer (1980) |
Hermitian connection. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Hermitian_connection&oldid=13208