2001
DOI: 10.1007/s002200100456
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Bryuno Function and the Standard Map

Abstract: For the standard map the homotopically non-trivial invariant curves of rotation number ω satisfying the Bryuno condition are shown to be analytic in the perturbative parameter ε, provided |ε| is small enough. The radius of convergence ρ(ω) of the Lindstedt series -sometimes called critical function of the standard map -is studied and the relation with the Bryuno function B(ω) is derived: the quantity | log ρ(ω) + 2B(ω)| is proved to be bounded uniformily in ω. cleare, Sez. Tor Vergata

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Cited by 44 publications
(49 citation statements)
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“…Davie's result implies the upper bound Q 2 (ω) < C The results stated in proposition (9.2.1) were first conjectured in [BM94], supported by numerical results, and a proof was given for the resonances p/q = 0/1 and p/q = 1/2. Validity of Bryuno's interpolation formula |Q 2 (ω)| < C was recently proved in [BG01], where a bound Q 2 (ω) > C was found via a refinement of the techniques discussed in the present section. §9.4 Scaling laws for the standard map…”
mentioning
confidence: 64%
“…Davie's result implies the upper bound Q 2 (ω) < C The results stated in proposition (9.2.1) were first conjectured in [BM94], supported by numerical results, and a proof was given for the resonances p/q = 0/1 and p/q = 1/2. Validity of Bryuno's interpolation formula |Q 2 (ω)| < C was recently proved in [BG01], where a bound Q 2 (ω) > C was found via a refinement of the techniques discussed in the present section. §9.4 Scaling laws for the standard map…”
mentioning
confidence: 64%
“…for suitable universal constants C 1 and C 2 ; see [27,9] for a proof of the last statement. The proof of the lower bound in (12.3) relies on deeper cancellations than those discussed in Section 7; see [9] for details.…”
Section: Weaker Diophantine Conditionsmentioning
confidence: 99%
“…All the results of the previous sections can be extended to rotation vectors satisfying the Bryuno condition: see [39] for maximal and lower-dimensional tori, [9] for the standard map, and [40] for dissipative systems. For d = 2 one can write ω = (ω 1 , ω 2 ) = (1, α)ω 1 , where α = ω 2 /ω 1 is the rotation number.…”
Section: Weaker Diophantine Conditionsmentioning
confidence: 99%
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