Defining a Contact Structure Globally -- Obstructions?

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Discussion Overview

The discussion revolves around the obstructions to defining a contact structure globally on a 3-manifold embedded in \(\mathbb{R}^3\). Participants explore the relationship between local definitions of contact structures and their global counterparts, particularly through the lens of 1-forms and tangent bundles. The conversation touches on theoretical aspects of contact geometry, including conditions under which a distribution of 2-planes can be represented as a global 1-form.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions the obstructions to defining a contact structure through a global 1-form, suggesting it may relate to the triviality of the global tangent bundle or the 2-subbundle of the tangent bundle.
  • Another participant proposes that if there is a smooth distribution of 2-planes that is the kernel of a global 1-form, then the tangent bundle splits as \(TM = V \oplus \xi\), where \(\xi\) is a trivial line bundle.
  • It is noted that every oriented 3-manifold has a trivial tangent bundle, and if the manifold is orientable, the 2-plane distribution is also orientable.
  • One participant introduces a specific case involving a closed orientable Riemannian 2-manifold, discussing how the curvature must be non-zero for a horizontal distribution to qualify as a contact structure.
  • Contact structures are described as nowhere-integrable, with a reference to Frobenius' theorem regarding the condition \(\theta \wedge d\theta \neq 0\).
  • Another participant elaborates on the relationship between the connection 1-form and curvature, indicating that if the Gauss curvature is never zero, then certain conditions regarding the contact structure hold true.

Areas of Agreement / Disagreement

Participants express various viewpoints regarding the conditions and definitions surrounding contact structures, with no clear consensus reached on the obstructions or specific examples. The discussion remains open-ended, with multiple competing ideas presented.

Contextual Notes

Some limitations include the dependence on definitions of orientability and triviality of bundles, as well as unresolved mathematical steps regarding the curvature and its implications for contact 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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