{ "id": "0802.3433", "version": "v2", "published": "2008-02-23T09:09:27.000Z", "updated": "2008-04-23T16:40:34.000Z", "title": "On Khintchine exponents and Lyapunov exponents of continued fractions", "authors": [ "Ai-Hua Fan", "Ling-Min Liao", "Bao-Wei Wang", "Jun Wu" ], "comment": "37 pages, 5 figures, accepted by Ergodic Theory and Dyanmical Systems", "categories": [ "math.DS" ], "abstract": "Assume that $x\\in [0,1) $ admits its continued fraction expansion $x=[a_1(x), a_2(x),...]$. The Khintchine exponent $\\gamma(x)$ of $x$ is defined by $\\gamma(x):=\\lim\\limits_{n\\to \\infty}\\frac{1}{n}\\sum_{j=1}^n \\log a_j(x)$ when the limit exists. Khintchine spectrum $\\dim E_\\xi$ is fully studied, where $ E_{\\xi}:=\\{x\\in [0,1):\\gamma(x)=\\xi\\} (\\xi \\geq 0)$ and $\\dim$ denotes the Hausdorff dimension. In particular, we prove the remarkable fact that the Khintchine spectrum $\\dim E_{\\xi}$, as function of $\\xi \\in [0, +\\infty)$, is neither concave nor convex. This is a new phenomenon from the usual point of view of multifractal analysis. Fast Khintchine exponents defined by $\\gamma^{\\phi}(x):=\\lim\\limits_{n\\to\\infty}\\frac{1}{\\phi(n)} \\sum_{j=1}^n \\log a_j(x)$ are also studied, where $\\phi (n)$ tends to the infinity faster than $n$ does. Under some regular conditions on $\\phi$, it is proved that the fast Khintchine spectrum $\\dim (\\{x\\in [0,1]: \\gamma^{\\phi}(x)= \\xi \\}) $ is a constant function. Our method also works for other spectra like the Lyapunov spectrum and the fast Lyapunov spectrum.", "revisions": [ { "version": "v2", "updated": "2008-04-23T16:40:34.000Z" } ], "analyses": { "subjects": [ "11K55", "28A78", "28A80" ], "keywords": [ "lyapunov exponents", "fast lyapunov spectrum", "fast khintchine spectrum", "continued fraction expansion", "usual point" ], "note": { "typesetting": "TeX", "pages": 37, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2008arXiv0802.3433F" } } }