Frobenius' Theorem: Characterization & Proof Difficulty

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The discussion centers on the characterization of Frobenius' Theorem, specifically the relationship between the equations \nabla_{[a}\xi_{b]}=\xi_{[a}v_{b]} and \xi_{[a}\nabla_{b}\xi_{c]}=0. Participants express that while the proof is not inherently difficult, it can be lengthy and tedious, typical of geometric proofs. The converse condition, \xi_{[a}\nabla_{b}\xi_{c]}=0, is identified as the integrability condition that ensures the solvability of the differential equation for the dual vector field v. Understanding this relationship is crucial for grasping the theorem's implications in differential geometry. The conversation emphasizes the need for clarity in proving these connections.
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I need to understand a certain characterization of Frobenius' Theorem, part of which contains the following statement:

\nabla_{[a}\xi_{b]}=\xi_{[a}v_{b]} for some dual vector field v_{b} if and only if \xi_{[a}\nabla_{b}\xi_{c]}=0, where \xi^a\xi_a\neq 0.

Is it obvious, or difficult to prove? I do not see the converse ...
 
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toogood said:
I need to understand a certain characterization of Frobenius' Theorem, part of which contains the following statement:

\nabla_{[a}\xi_{b]}=\xi_{[a}v_{b]} for some dual vector field v_{b} if and only if \xi_{[a}\nabla_{b}\xi_{c]}=0, where \xi^a\xi_a\neq 0.

Is it obvious, or difficult to prove? I do not see the converse ...

Ι wouldn't say it is hard, it is just -as many proofs in geometry- rather long and tedious. For the converse part, the condition \xi_{[a}\nabla_{b}\xi_{c]}=0 is the integrability condition that guarantees us that the partial differential equation \nabla_{[a}\xi_{b]}=\xi_{[a}v_{b]} is solvable for v.
 

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