Flat connection: Difference between revisions
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===Symbol-free definition=== | ===Symbol-free definition=== | ||
A [[connection]] on a [[vector bundle]] over a [[differential manifold]] is said to be '''flat''' or '''integrable''' or '''curvature-free''' or '''locally flat''' if the curvature of the connection is zero everywhere. | A [[defining ingredient::connection]] on a [[defining ingredient::vector bundle]] over a [[defining ingredient::differential manifold]] is said to be '''flat''' or '''integrable''' or '''curvature-free''' or '''locally flat''' if the [[defining ingredient::curvature of a connection|curvature of the connection]] is zero everywhere. | ||
===Definition with symbols=== | ===Definition with symbols=== | ||
A [[connection]] <math>\nabla</math> on a [[differential manifold]] <math>M</math> is said to be '''flat''' or '''integrable''' or '''curvature-free''' or '''locally flat''' if the curvature form vanishes identically, viz for any vector fields <math>X</math> and <math>Y</math>: | A [[connection]] <math>\nabla</math> on a [[vector bundle]] <math>E</math> over a [[differential manifold]] <math>M</math> is said to be '''flat''' or '''integrable''' or '''curvature-free''' or '''locally flat''' if the curvature form vanishes identically, viz for any vector fields <math>X</math> and <math>Y</math>: | ||
<math>R(X,Y) = \nabla_X\nabla_Y - \nabla_Y\nabla_X - \nabla_{[X,Y]} = 0</math> | <math>R(X,Y) = \nabla_X\nabla_Y - \nabla_Y\nabla_X - \nabla_{[X,Y]} = 0</math> | ||
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===Definition in local coordinates=== | ===Definition in local coordinates=== | ||
In local coordinates, we require that the [[curvature matrix of a connection|curvature matrix]] should vanish identically; in other words: | In local coordinates, we require that the [[defining ingredient::curvature matrix of a connection|curvature matrix]] should vanish identically; in other words: | ||
<math>\Omega := d\omega + \omega \wedge \omega = 0</math> | <math>\Omega := d\omega + \omega \wedge \omega = 0</math> | ||
where <math>\omega</math> is the [[matrix of connection forms]]. | where <math>\omega</math> is the [[defining ingredient::matrix of connection forms]]. | ||
===Alternative definitions=== | |||
{{further|[[Flat connection equals module structure over differential operators]]}} | |||
Recall that one alternative view of a connection is as giving the space of sections <math>\Gamma(E)</math> the structure of a module over the [[connection algebra]] of <math>M</math>. Equivalently, it is a way of giving the ''sheaf'' of sections <math>\mathcal{E}</math> the structure of a sheaf-theoretic module over the [[sheaf of connection algebras]]. | |||
The connection is flat if and only if this descends to a module structure over the [[sheaf of differential operators]]. In other words, a flat connection is equivalent to a structure of <math>\mathcal{E}</math> as a module over the [[sheaf of differential operators]]. | |||
Latest revision as of 22:01, 24 July 2011
Definition
Symbol-free definition
A connection on a vector bundle over a differential manifold is said to be flat or integrable or curvature-free or locally flat if the curvature of the connection is zero everywhere.
Definition with symbols
A connection on a vector bundle over a differential manifold is said to be flat or integrable or curvature-free or locally flat if the curvature form vanishes identically, viz for any vector fields and :
Definition in local coordinates
In local coordinates, we require that the curvature matrix should vanish identically; in other words:
where is the matrix of connection forms.
Alternative definitions
Further information: Flat connection equals module structure over differential operators
Recall that one alternative view of a connection is as giving the space of sections the structure of a module over the connection algebra of . Equivalently, it is a way of giving the sheaf of sections the structure of a sheaf-theoretic module over the sheaf of connection algebras.
The connection is flat if and only if this descends to a module structure over the sheaf of differential operators. In other words, a flat connection is equivalent to a structure of as a module over the sheaf of differential operators.