Suetani Hiromichi, Horita Takehiko, Mizutani Shin
NTT Communication Science Laboratories, NTT Corporation, 2-4 Hikaridai, Seika-cho, Soraku-gun, Kyoto 619-0237, Japan.
Phys Rev E Stat Nonlin Soft Matter Phys. 2004 Jan;69(1 Pt 2):016219. doi: 10.1103/PhysRevE.69.016219. Epub 2004 Jan 30.
We study the dynamics of a pair of two uncoupled identical type-I intermittent chaotic systems driven by common random forcing. We first observe that the degree of the fluctuation of the local expansion rate of orbits to perturbations of a single system as a function of the noise intensity shows a convex curve and takes its maximum value at a certain noise intensity, whereas the Liapunov exponent itself monotonically increases in this range. Furthermore, it is numerically demonstrated that this nontrivial enhancement of fluctuation causes that two orbits with different initial conditions may synchronize each other after a finite interval of time. As pointed out by Pikovsky [Phys. Lett. A 165, 33 (1992)], since the Liapunov exponent of the present system is positive, the synchronization that we observed is a numerical artifact due to the finite precision of calculations. The spurious noise-induced synchronization in an ensemble of uncoupled type-I intermittent chaotic systems are numerically characterized and the relations between these features and the fluctuation properties of the local expansion rate are also discussed.
我们研究了由共同随机强迫驱动的一对两个未耦合的相同I型间歇混沌系统的动力学。我们首先观察到,单个系统轨道对扰动的局部膨胀率的波动程度作为噪声强度的函数呈现出一条凸曲线,并在一定噪声强度下取最大值,而李雅普诺夫指数本身在此范围内单调增加。此外,数值结果表明,这种波动的非平凡增强导致具有不同初始条件的两条轨道在有限时间间隔后可能相互同步。正如皮科夫斯基所指出的[《物理快报A》165, 33 (1992)],由于当前系统的李雅普诺夫指数为正,我们观察到的同步是由于计算的有限精度导致的数值假象。对未耦合I型间歇混沌系统集合中的虚假噪声诱导同步进行了数值表征,并讨论了这些特征与局部膨胀率波动特性之间的关系。