1549055384-Symplectic_Geometry_and_Topology__Eliashberg_

(jair2018) #1
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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).



  1. 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.
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