LECTURE 1. PROBLEMS, BASIC CONCEPTS AND OVERVIEW 47
Given J and (x, T) this interval only depends on the homotopy class [u] of u with
boundary fixed. Hence we shall write I(x, T, [u], J). Sometimes it is independent
even of the choice of [u]. Namely in the following case. Define a group homomor-
phism 'PC. by
'PC. : 7r2 ( M) ---7 z: u ---7 ( u. C1 ( ~' J)) [ S^2 ].
If 'PC. = 0 then I(x, T, [u], J) = I(x, T, J).
Exercise 1.28. Show that 'PE. is a well-defined group homorphism.
The winding interval I(x, T, [u], J) in fact depends on J. But certain informa-
tion does not depend on J.
Some properties of the winding interval are easily established, see [41]. For
example its length is smaller than ~:
1
[I(x, T, [u], J)[ <
2
.
Exercise 1.29. Prove the bound on the length of the winding interval.
We define the Conley Zehnder index of the contractible periodic orbit (x, T)
with respect to [u] by
{
2k+ 1
μ( x, T, [u]) =
2
k
if I(x, T , [u], J) C (k, k + 1)
if k E J(x, T, [u], J)
Exercise 1.30. Show that the definition of μ is independent of the choice of an
admissable J.
Definition 1.31. A contact form ,\ on the closed three manifold M is called dy-
namically convex if
- 'PC.= 0
- For every contractible periodic orbit (x, T) of the associated Reeb vector
field X we have μ(x, T) 2: 3.
The following exercise is not difficult.
Exercise 1.32. The standard contact form Ao on S^3 is dynamically convex.
The above exercise is only a very particular case of a more general fact.
Proposition 1.33. Let M be a closed hypersurface in JR^4 = C^2 enclosing a strictly
convex domain G containing 0. Let,\ be the restriction of the 1-form ~[q·dp-p·dq]
to M. Then ,\ is a dynamically convex contact farm.
The proof of this proposition is not trivial and can be found in [49]. Neverthe-
less the reader might enjoy to try to prove it!
For dynamically convex contact forms on S^3 much more can be said about the
dynamics; see [51, 48]:
Theorem 1.34. Let ,\ be a dynamically convex contact form on S^3. Then there
exists an embedded disk V c S^3 such that av is a periodic orbit for X and iJ is
transversal to X. Moreover, every orbit for X other than av hits iJ in forward and
backward time. Further there are precisely two periodic orbits or infinitely many.