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A NNALES DE L ’I. H. P., SECTION A

Erratum : “Drift and diffusion in phase space”

Annales de l’I. H. P., section A, tome 68, n

o

1 (1998), p. 135

<

http://www.numdam.org/item?id=AIHPA_1998__68_1_135_0

>

© Gauthier-Villars, 1998, tous droits réservés.

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(2)

Erratum

For

"Drift

and

diffusion

in

phase space ", by

L. Chierchia and G. Gallavotti,

in Ann. Inst. H.

Poincare, B-60, 1,

1994.

. Statement

c), d)

of theorem 3 on p. 71 and the reference to them in the

following

remark are not correct: this is due to a

computational

error

(claiming

that

811

is

exponentially small)

in the

corresponding proof

in

Appendix

A 13

(first

line after

(A13.23),

page

138)

referred to on p. 76.

. Statement

c)

is never

used;

the statements are commented

in §

11 on p.

81,

82. The discussion about lemma 4 is also invalid

together

with the remark 2 and 4 on p. 84. The parts

of § 10, § 11

unrelated to

c), d)

are

unchanged.

. The

only

role of statement

d)

was that of

making simpler

the discussion

of the

application in § 12

to a

priori

stable

problems

and it does not affect

the results in the sections

preceding §

10. The

application in §

12 is therefore incorrect from

(12.41)

to the final formula

(12.43).

Correcting

the error

in § 10,

i. e.

getting

a lower bound on the

splitting angles

becomes a

nonperturbative problem.

The

techniques

of

appendix

A 13

were not

developed

to deal with such cases because the error made the

nonperturbative analysis

seem unnecessary.

They

have been

developed

in the

subsequent

paper

[G]

and

pushed

to a

nonperturbative analysis

in

[GGM]:

in the latter work

(see §6, 7)

a correction to the theorem 3

in § 10 quoted

above is

proposed. Although

the

splitting

is shown to be

exponentially

small it

might

be

large enough

for the method

in § 12

to

apply;

but this

requires

further

analysis

of the

special

case in

§2,

whose result at the moment remains invalid.

. A further error is in

§8

after

(8.20):

the claims on the

expansion

and contraction rates is correct

only if ~i~

and

~i|

are of the same order

of

magnitude.

This forces

taking

them

equal

in the rest of the section

and therefore the estimated drift time becomes even

longer (wihout

other consequences, as the

point

was to show that the time is

finite).

We are indebted to V. Gelfreich for

pointing

out the first error and to

P. Lochak for

stimulating

and

leading

the detailed discussion that identified it.

[G] G. GALLAVOTTI, Twistless KAM tori, quasi flat homoclinic intersections, and other cancellations in the perturbation series of certain completely integrable hamiltonian systems. A review, Reviews on Mathematical Physics, 6, 343-411, 1994. A substantial part of this paper was developed in collaboration with L. Chierchia:

see the acknowledgements.

[GCM] G. GALLAVOTTI, G. GENTILE and V. MASTROPIETRO, Pendulum: separatrix splitting,

down-loadable at [email protected], #97-472, chao-dyn 9709004, and http://chimera.roma1.infn.it.

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