Graduate Defining a Contact Structure Globally -- Obstructions?

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SUMMARY

This discussion focuses on the obstructions to defining a contact structure on a 3-manifold ##M^3## embedded in ##\mathbb R^3## as a global 1-form. Key points include the necessity of the tangent bundle splitting as ##TM=V⊕ξ##, where ##V## is a smooth distribution of 2-planes and ##ξ## is a trivial line bundle. The conversation highlights that while every oriented 3-manifold has a trivial tangent bundle, the presence of curvature can obstruct the horizontal distribution from being a contact structure. The condition ##\theta \wedge d\theta \neq 0## is essential for a distribution to be contact.

PREREQUISITES
  • Understanding of 3-manifolds and their embeddings in ##\mathbb R^3##
  • Familiarity with contact geometry and the definition of contact structures
  • Knowledge of tangent bundles and their properties
  • Basic concepts of Riemannian metrics and curvature forms
NEXT STEPS
  • Explore the properties of contact structures in differential geometry
  • Study the implications of the Frobenius theorem in relation to contact distributions
  • Investigate the role of curvature in the context of Riemannian manifolds
  • Learn about the classification of 3-manifolds and their tangent bundles
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Mathematicians, particularly those specializing in differential geometry, topology, and contact geometry, will benefit from this discussion. It is also relevant for researchers exploring the properties of manifolds and their geometric structures.

WWGD
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Hi,
Let ##M^3## be a 3-manifold embedded in ##\mathbb R^3## and consider a 2-plane field ( i.e. a Contact Structure) assigned at each tangent space ##T_p##. I am trying to understand obstructions to defining the plane field as a 1-form ( Whose kernel is the plane field/ Contact Structure) Given a specific point we can define a local form w as a linear map ##\mathbb R^3 \rightarrow \mathbb R ## whose kernel is the contact plane. I am curious about the obstructions to defining the contact structure through a global 1-form. I suspect it may have to see with the triviality of either the global (tangent) bundle or the 2-subbundle of the tangent bundle . Is this correct? Can anyone add anything and/or give examples?
Thanks. This seems like @lavinia could know the answer.
 
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Hi WWGD

I don't know anything about contact geometry but it seems if there is a smooth distribution of 2 planes ##V## on a 3 manifold that is the kernel of a global 1 form ,then the tangent bundle splits as ##TM=V⊕ξ## where ##ξ## is a trivial line bundle.

Conversely if with respect to some Riemannian metric ##<,>## , one can choose a globally non-zero vector field ##s## that is orthogonal to ##V##, then the 1 form ##ω= <s,>## is a global 1 form whose kernel is ##V##.

Notes:

- Every oriented 3 manifold has trivial tangent bundle.
- If the 3 manifold is orientable and the 2 plane distribution is the kernel of a global 1 form. then the 2 plane distribution is also orientable.
- I think a contact distribution is automatically a sub-bundle since locally it is the kernel of a 1 form. Yes?
- It is possible in a oriented 3 manifold to have an unorientable 2 dimensional sub-bundle with non-trivial normal line bundle. It would be interesting to find one that is a contact structure.

Sorry not to be of more help.
 
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lavinia said:
Hi WWGD

I don't know anything about contact geometry but it seems if there is a smooth distribution of 2 planes ##V## on a 3 manifold that is the kernel of a global 1 form ,then the tangent bundle splits as ##TM=V⊕ξ## where ##ξ## is a trivial line bundle.

Conversely if with respect to some Riemannian metric ##<,>## , one can choose a globally non-zero vector field ##s## that is orthogonal to ##V##, then the 1 form ##ω= <s,>## is a global 1 form whose kernel is ##V##.

Notes:

- Every oriented 3 manifold has trivial tangent bundle.
- If the 3 manifold is orientable. then the 2 plane distribution is also orientable.
- I think a contact distribution is automatically a sub-bundle since locally it is the kernel of a 1 form. Yes?
- It is possible in a oriented 3 manifold to have an unorientable 2 dimensional sub-bundle with non-trivial normal line bundle. It would be interesting to find one that is a contact structure.

Sorry not to be of more help.
Actually pretty helpful, Lavinia, thanks, and sorry to put you on the spot :).
 
It was fun to learn a little about it.

Here is a different idea of obstruction in a special case. This time there will be a global 1 form whose kernel is a distribution of 2 planes but there will be an nice obstruction to this being a contact structure.

For a closed orientable Riemannian 2 manifold such as the sphere, the tangent unit circle bundle is a closed 3 manifold and is also a principal ##SO(2)## bundle. ##SO(2)## acts on a fiber circle by rotation. A connection 1 form is dual to the line bundle along the fiber circles - this is a trivial line bundle - and its kernel is a distribution of 2 planes that is called the horizontal space of the connection. In general this horizontal space not a contact structure. The obstruction is the curvature. The curvature form must be everywhere non-zero in order for the horizontal distribution to be a contact structure. So for instance, the horizontal distribution on the tangent circle bundle to the unit sphere in ##R^3## is a contact structure.
 
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Just to add a few things in the unlikely case you don't know them yet: Contact structures are nowhere-integrable , meaning there is no open set the restriction of whch is the tangent bundle of a manifold. The condition ## \theta \wedge d \theta \neq 0## follows from Frobenius theorem, as the needed condition for a distribution to be somewhere-involutive.
 
WWGD said:
Just to add a few things in the unlikely case you don't know them yet: Contact structures are nowhere-integrable , meaning there is no open set the restriction of whch is the tangent bundle of a manifold. The condition ## \theta \wedge d \theta \neq 0## follows from Frobenius theorem, as the needed condition for a distribution to be somewhere-involutive.

Right. Thank you. I read the proof. It is a nice way to characterize it.

In the curvature case, if ##ω## is the connection 1 form then ##dω## is the curvature 2 form and is equal to ##π^{*}-KdV## where ##K## is the Gauss curvature so ##ω∧dω## is zero at a point only if ##K \circ π## is zero at that point. So if ##K## is never zero, ##ω∧dω## is never zero.
 
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