2004/01/15 by Garín F. Janampa Añaños, Garin F. J Ananos, Constantino Tsallis · 3 citations
Economics, Econometrics and Finance · Mathematics · Physics and Astronomy · #Advanced Mathematical Theories and Applications #CHAOS (operating system) #Complex Systems and Time Series Analysis #Computer science #Condensed matter physics #Edge of chaos #Enhanced Data Rates for GSM Evolution #Mathematics #Physics #Statistical Mechanics and Entropy #Statistical physics #cond-mat.stat-mech
paper · pdf · doi:10.1103/physrevlett.93.020601
5 pages, 5 figures
arxiv created 2004/01/15 · openalex publication_date 2004/07/07 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
Ensemble averages of the sensitivity to initial conditions \ensuremathξ(t) and the entropy production per unit of time of a new family of one-dimensional dissipative maps, xt+1=1\ensuremath-ae^\ensuremath-1/|xt|z(z>0), and of the known logisticlike maps, xt+1=1\ensuremath-a|xt|z(z>1), are numerically studied, both for strong (Lyapunov exponent \ensuremathλ1>0) and weak (chaos threshold, i.e., \ensuremathλ1=0) chaotic cases. In all cases we verify the following: (i) both \ensuremath⟨lnq\ensuremathξ\ensuremath⟩ [lnqx\ensuremath≡(x^1\ensuremath-q\ensuremath-1)/(1\ensuremath-q); ln1x=lnx] and \ensuremath⟨Sq\ensuremath⟩ [Sq\ensuremath≡\phantom\rule0ex0ex(1\ensuremath-\ensuremath∑ipiq)/(q\ensuremath-1); S1=\ensuremath-\ensuremath∑ipilnpi] linearly increase with time for (and only for) a special value of q, qsenav, and (ii) the slope of \ensuremath⟨lnq\ensuremathξ\ensuremath⟩ and that of \ensuremath⟨Sq\ensuremath⟩ coincide, thus interestingly extending the well known Pesin theorem. For strong chaos, qsenav=1, whereas at the edge of chaos qsenav(z)<1.