Transversality of a Vector Field in terms of Forms (Open Books)

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SUMMARY

This discussion focuses on the transversality of a Reeb field, denoted as Rω, in relation to a contact form ω and its implications for open book decompositions in contact 3-manifolds. The key argument presented is the equivalence between the contact manifold (M, ζ) being supported by the open book (B, π) and the conditions that Rω is positively-tangent to the binding B and positively-transverse to the pages of the open book. The proof leverages properties of differential forms, specifically the relationship between the Reeb field and the area form dω on the pages of the open book.

PREREQUISITES
  • Understanding of Reeb fields and contact forms in differential geometry.
  • Familiarity with open book decompositions in contact 3-manifolds.
  • Knowledge of differential forms and their properties, particularly the exterior derivative.
  • Concept of transversality in the context of vector fields and manifolds.
NEXT STEPS
  • Study the properties of Reeb fields in contact geometry.
  • Learn about open book decompositions and their applications in topology.
  • Explore the concept of transversality and its implications in differential topology.
  • Investigate the role of differential forms in defining area forms on manifolds.
USEFUL FOR

Mathematicians, particularly those specializing in differential geometry, topology, and contact geometry, will benefit from this discussion. It is also valuable for graduate students and researchers exploring the interplay between vector fields and differential forms in manifold theory.

WWGD
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Hi, All:
Sorry for the length of the post, but I think it is necessary to set things up so that the post is understandable:

I'm going through an argument in which we intend to show that a given vector field [ itex]R_ω [/ itex]
(actually a Reeb field associated with a contact form ω) is positively-tangent to a
link ( as in a space whose connected components are S^1 -knots. This means the Reeb field
lives in the tangent space to the Link, along the positive direction) , and R_{\omega} is positively-
transverse to a surface S ( so that R_{\omega} intersects S positively at points).
The argument is made using properties of differential forms, in the context of open book decompositions of contact 3-manifolds.
A needed definition is this: A contact structure ζ is _supported by an open book decomposition (B, π )_ if ζ can be isotope thru contact structures so that there is a contact 1-form ω for ζ satisfying:

1)dω is a positive area form on each page ∑_{\theta} of the open book, and:

2)ω>0 on the binding B ; both B and the pages are oriented.

End of setup.

------------------------------------------------------------------------------
Actual Question:

To be more specific, I'm trying to understand the following arguments purporting to show
the equivalence between these two conditions:

(1) The contact manifold (M,ζ ) is supported by the open book (B,π)

(3) There is a Reeb field R_ω for a contact structure isotopic to ω , so that [ itex]R_ω[/itex] is positively-tangent to the binding B, and positively-transverse to the pages of the open book.

Proof:
(3)->(1) : Since R_ω is assumed positively -tangent to the binding B , we have ω>0 on oriented tangent vectors to B. Since the Reeb field R_ω is positively-transverse to the pages of the OB (open book) , we have that dω=i_{R_ω}(ω /\ dω) >0 on the pages of the OB (where i is --I am? -- the interior product , or contraction of the form ω /\ dω by the vector field
R_ω

Questions:
i)How does R_{ω} being positively-tangent to the ( knots in the ) binding imply ω >0 ?
I know this means the vector field being positively-tangent to the binding means that R_{ω} lies along the tangent space ; a 1-d tangent space, to each of the knots, along the chosen positive direction orientation.

ii)Why is dω equal to the contraction of ω /\ dω ? , and how does the positive transversality imply that dω>0?

(1)->(3): Assume (1), and let ω be the form with the given conditions, and let R_{ω} be the Reeb field associated with ω. Then "It is clear that R_{ω} is positively-transverse to the pages of the OB, since dω is an area form on the pages of the open book"

I have no clue about the connection between the Reeb field being positively-transverse to the pages, and dω being an area form on the pages. I know if dw is a positive area form on the pages, then dω (X,Y)>0 at any pair of positively-oriented tangent vectors. And I know a Reeb field associated to a contact structure is transverse to the planes in the contact structure .But I can't see how this relates to $dω being an area form for the pages of the open book.

Thanks for any suggestions, ideas.
 
Last edited:

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