• Aucun résultat trouvé

Note rectificative : “Asymptotic winding of the geodesic flow on modular surfaces and continuous fractions”

N/A
N/A
Protected

Academic year: 2022

Partager "Note rectificative : “Asymptotic winding of the geodesic flow on modular surfaces and continuous fractions”"

Copied!
5
0
0

Texte intégral

(1)

A NNALES SCIENTIFIQUES DE L ’É.N.S.

Y. G UIVARCH Y. L E J AN

Note rectificative : “Asymptotic winding of the geodesic flow on modular surfaces and continuous fractions”

Annales scientifiques de l’É.N.S. 4e série, tome 29, no6 (1996), p. 811-814

<http://www.numdam.org/item?id=ASENS_1996_4_29_6_811_0>

© Gauthier-Villars (Éditions scientifiques et médicales Elsevier), 1996, tous droits réservés.

L’accès aux archives de la revue « Annales scientifiques de l’É.N.S. » (http://www.

elsevier.com/locate/ansens) implique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/conditions). Toute utilisation commerciale ou impression systé- matique est constitutive d’une infraction pénale. Toute copie ou impression de ce fi- chier doit contenir la présente mention de copyright.

Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques

http://www.numdam.org/

(2)

4° serie, t. 29, 1996, p. 811 a 814.

NOTE RECTIFICATIVE D'Y. GUIVARCH ET Y. LE JAN CONCERNANT L'ARTICLE

ASYMPTOTIC WINDING OF THE GEODESIC FLOW ON MODULAR SURFACES

AND CONTINUOUS FRACTIONS

(paru dans le tome 26, fascicule 1, 1993, pp. 23-50)

The object of this note is to complete the proof of theorem 2.1 in [G-L]. The main steps of the proof are valid, but the replacement of the discrete coding time used in Proposition 4-3 by the time of the flow should have been done more carefully. We use the notations of [G-L].

We recall that the geodesic flow Ut on Y / G has been presented as a special flow over S = [0, 1] x Z/2Z x Fo/r. The transformation 0 on S is an extension of the continuous fraction transformation and the height function ^ is explicit. We denote by g the projection of g C G on F / G and by tmk (9) = ^mk (9) ^e sequence of return times to the section

S. The following points are essential in the proof.

a) Set Ni{g) = Inf{fc e N; t^(g) > t}, A(g) = f^ ^ a;.

Nf[g}-l

One has ;^ ^ - E ^^ p(g)} = A(g) - A(gUi).

Because the Liouville measure is Ut -invariant, the laws of A (g) and A (g Ut) are the same; hence —^gl and A{g^ut) converge to zero in probability. The case of UJC can be treated in the same way.

b) To reduce Theorem 2.1 to Proposition 4-3, we will use, in addition to Lemma 4.1 (Lemma 4.2 is incorrect) the tightness of Nt ^-^/6LO^ ^ ^s ^ f oo.

To show this result, set i = ^/GLog 2 and note that:

and that:

Nt^-^^^AVt iff r^^^(g)^T(g)<t

Nt {g) - [r11] < -AVt iff T^ ^_^ (g) + T (g) > t.

ANNALES SCIENTIPIQUES DE L'ECOLE NORMALE SUPERIEURE. - 0012-9593/96/06/$ 7.00/© Gauthier-Villars

(3)

812 Y. GUIVARCH AND Y. LE JAN

Hence the result will follow from the tightness of the sequence :r2]-^. Set (^v , — X ' ) =

6n 0<_, ^+) (N.B. 0 (^-, ^+) = (O^tx;1])"1, X+1- [X+1])^ a parenthesis was dropped in [G-L].) From the expression of <&, it is enough to prove a central limit theorem for the

n . . n , .

sequences ^ Log^' ) and ^ Log ( ; ( ; ' ) under ZA i i

The law of { ^v , m G N} is the law of the stationary Markov chain Xn studied in §5. The law of ( : \ - , . . . , X + , ^+) given that ^( / = re coincides with the law of (^_, ^(1), . . . , x^) given that ^_ = re.

n

Henceforth, it is sufficient to prove the central limit theorem for ^ Log (xm)- This can be done easily by following the steps given in §5, using the perturbed transfer operatori

00

Q^ defined by Q^u(x) = ^ p ( x , k) e^0^'^ u(k ' x) if we take into account the i

following remarks (see also [G-H]):

The function Logx on [0, 1] is not Lipchitz as in [G-H] but the key properties of the operators are the same, namely.

1) Q\ acts on the space of Lipchitz functions on [0, 1] and satisfies the basic inequality

110^11 < J |M| +c|^

for some constant C > 0.

2) Q^ is an analytic family of operators (|A| < 1). In particular, if we set

00

Dfu(x)=Y^p (;r, k) e^0^'^ u ( k - x ) i

there exist a constant C ' > 0 such that \\Q^ - Q' - i\D'\\ < C'\\\2.

In order to get the required inequality for ||0^|| one needs to control the Lipchitz coefficient. One has:

lO^C.) - Q^CzQI < ^ p^ k)\———^ - I ^

1 1 i (k-\-x) (fc+rc')

00 00

^ \p(x^ k) — p(x^ k)\ \u(k • x)\ + V^ p [ x ^ k)\u[h • x) — u[

+ V^ \p(x^ k) — p(x^ k)\ \u(k • x)\ + V^ p(x^ k)\u{k • x) — u{k ' x') i i

Clearly | . 1 .^ — x ^ < [A| \x — x'\ ^ hence the first term is bounded by

00

|A| \x - x'\ \u\oQ ^ p(x, k) ^ < C7i|A| \u oo\x - x'\.

i

The other terms are bounded by [Gsl^loo + j IMI]!^ — x'\.

The analyticity of the family Q^ follows from the Cauchy formula on a loop i in the unit disk:

r [ °° i

\ Q^udz = / V^ p(x^ k) -———^ u(k • x) dz.

Ji h ~^ (x + k)

4s SERIE - TOME 29 - 1996 - N° 6

(4)

If \z\ < 1 - £, one has \p (x, k) ^^y \ < p (x, k) (k + l)1"^.

Hence, summation and integration can be exchanged and the result follows form the

relation h ^W dz = °-

Nt , [^t]

c) To show that ^ (^ -0 o 071 - ^ -0 o ^n) converges to zero in probability, it is i i

[AVn\

enough to show the convergence to 0 in probability of ^ ^ |^ o ^l as n f oo. From i

the expressions of ^ and z>, it is clear that f H1"6 di> is finite for any e in ]0, 1[. Moreover

k k

the inequality (^ \ai\Y < ^ [a^ (0 < e < 1) implies:

i i

[Ay/n] x 1-e A^/n

n-1 ^ |^ o r1! ) < n'-1 ^, |^ o <

~^ ^ i

/ L^V'^J \ i—e' ^V "•

(n-1 ^ l ^ o ^ l ) ^ n ^1 ^ l ^ o ^ l1- ^

^ i ^ i

Hence, for any p such that 1 < p < (1- e)~1, from the triangular inequality in LP

/ [AVn\ x 1-e / . \ 1/p

(n-1 V l ^ o ^ l ) ^ [A^n]^-1 / l^l^-^^

\ 1 / LP(I>} ^ )

< i / HLP(I>)

n-

2^

l r o

'

l

- L^v^j^

which converges to zero as n \ oo for e < j.

This completes the proof of 2.1 a) (A different approach was also given in [LJ], and developed in [E] for a) and b) using Brownian motion instead of the coding.)

Ni , [^t]

d) To show that — (^ T] o ^ - ^ T] o 071) converges to zero in probability, it is

Vt ^ ^

n ^

enough to show the convergence to 0 in probability of -^ S^^ with Sn = Y, T] o 0^, S^ = sup|5fc|.

k<n

Since rj is bounded and of integral zero, an extension of the classical Kolmogorov inequality is required here, in the case of the Markov chain on [0, 1] x 1/21 x Fo/F

n

defined by Q, and the functional Sn = S T] o 6^: there exists a constant C > 0 such that:

i

m{S:>b}<C^.

This implies m {— 5r* ,-\ > b} < C ^%. hence the convergence to zero in probability

Of — — — 5 r * -..

Vn [A^/n\

Such an inequality is proved in [G] p. 451 Cor. 1, on the basis of the Berry-Essen estimate for Sn. In turn, this estimate is obtained in [G-H] p. 80 Th. 2. The operator Q which occurs here satisfies the properties required in [G-H] as follows from Prop. 5.2, p. 36.

Such estimates are studied in full detail in [Br] in the context of expanding transformations

of the interval, a situation close to the situation considered here.

The proof of 2.1 b) and c) is now completed.

ANNALES SCIENTIFIQUES DE L'ECOLE NORMALE SUPERIEURE

(5)

814 Y. GUIVARCH AND Y. LE JAN

REFERENCES

[Br] A. BROISE, Asterisque, n° 238, 1996.

[E] N. ENRIQUEZ, These de FUniversite Paris-Sud, 1995.

[G] Y. GUIVARC'H, Ergod. Th & Dynam. Sys., 9, 1989, pp. 433-453.

[G-H] Y. GUIVARC'H and G. HARDY, Ann. I.H.P., Vol. 24, 1988, pp. 73-93.

[G-L] Y. GUIVARC'H and Y. LE JAN, Ann. Sci. E.N.S., T. 26, 1993, pp. 23-50.

[L-J] Y. LE JAN, C. R. Acad. Sci. Paris, 314, Series I, 1992, pp. 763-765.

4e SERIE - TOME 29 - 1996 - N° 6

Références

Documents relatifs

In this note, we prove that the density of the free additive convolution of two Borel probability measures supported on R whose Cauchy transforms behave well at innity can be

The heuristic is as follows: the boundary causes the average height function of a tiling (see definition in w to deviate slightly from its

Wang, Error analysis of the semi-discrete local discontinuous Galerkin method for compressible miscible displacement problem in porous media, Applied Mathematics and Computation,

An estimation of the length of closed geodesics combined with the curvature evaluation of §1 allows to compute the injectivity radius of the metric restricted to S 2 and to devise

Roughly speaking, his result says that at the first singular time of the mean curvature flow, the product of the mean curvature and the norm of the second fundamental form blows

We consider a continuous time Markov chain on a countable state space and prove a joint large deviation principle for the empirical measure and the empirical flow, which accounts

In our proof, an important idea is to reduce the problem to the study of harmonic forms integrated along the geodesic and change the contour of integration along the lines of the

Before going straight to the point, we want to add some words about the fact that the observation function h depends on u. This situation is not common in automatic control theory,