62
and
H. HOFER, HOLOMORPHIC CURVES AND DYNAMICS
Vs+ lvt = 0
E(v) < oo
{ v(O,-)*>-=m
Js,
{ v*d>-=O.
lbs'
We leave it as an easy exercise to show that
v(s, t) =(ms+ d, x(tm))
for some orbit x of x = X(x).
Summing up now our construction we see that
lim u(sk, t) = lim vk(O, t) = v(O, t) = x(tm).
k->w k->oo
D
There are some arguments in the previous proof which have to be completed.
Exercise 2.10. 1. For cp E I: with cp' ( s) > 0 for some s E IR we have
[ 1P'(a)da /\ df = oo
(8)
if a+ if is a non-constant holomorphic map.
2. Assume that v : IR x 81 --> IR x M satisfies
Then v has the form
Vs+ lvt = 0
E(v) < oo
f 3 , v(O, ·)* >. = m
fRxS 1 v*d). = 0.
v(s,t) = (ms+d,x(tm))
for some orbit x of x = X(x).
- Assume we are given a sequence ue: D --> IR x M of smooth maps satisfying
(ue)s + l(ue)t = 0
E(ue)::::; c
IV'ue(ze)I--> oo
ze --> 0,
where the energy is as defined before. Show that the following inequalities
hold.
(9) / :S liminfk_,oo { u'kd>-:S limsupk_, 00 { u'kd>-:S c
}De JD
for every c E (0, 1], where/> 0 is the infimum of all periods of contractible
periodic orbits for X>. in M.