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arXiv 1111.6725math.DSmath.FA
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$p$ -进$(2,1)$ -有理动力系统

$p$-adic $(2,1)$-rational dynamical systems

S. Albeverio, U. A. Rozikov, I. A. Sattarov

摘要:

研究了任意$(2,1)$ -有理$p$ -进动力系统在复$p$ -进域$\C_p$中的运动轨迹. (i)在不存在不动点的情况下,证明了$p$ -adic动力系统存在2-周期圈$x_1, x_2$ .如果它是吸引的,那么它吸引从半径为$r=|x_1-x_2|_p$且中心在$x_1$或$x_2$的球的元素开始的每个轨迹。如果2-周期循环是一个中性的,那么在每一步中,球会相互转移。所有其他半径为$>r$、圆心为$x_1$和$x_2$的球面都是不变的,与圈的吸引力无关。(ii)在不动点$x_0$是唯一的情况下,我们证明,如果该点吸引,那么存在$δ>0$,这样的吸引盆$x_0$是半径为$δ$的球和中心在$x_0$和任何半径为$\geq δ$的球是不变的。如果$x_0$是一个中性点,那么所有以$x_0$为中心的球面都是不变的。如果$x_0$是排斥点,则存在$δ>0$,使得在半径为$δ$且中心在$x_0$中的球的元素处开始的轨迹离开该球,而半径为$\geq δ$的任何球是不变的。(iii)在存在两个不动点的情况下,我们证明了Siegel圆盘对于动力系统的不同不动点既可以重合也可以不相交。此外,我们还找到了系统吸引子的盆。通过改变参数,证明了存在一个整数$k\geq 2$和一个球面$S_{r_1}(x_i), ..., S_{r_k}(x_i)$,使得极限轨迹周期性地通过球面$S_{r_j}$ .对于某些参数值,有轨迹可以任意远离固定点。

英文摘要:

We investigate the trajectory of an arbitrary $(2,1)$-rational $p$-adic dynamical system in a complex $p$-adic field $\C_p$. (i) In the case where there is no fixed point we show that the $p$-adic dynamical system has a 2-periodic cycle $x_1, x_2$. If it is attracting then it attracts each trajectory which starts from an element of a ball of radius $r=|x_1-x_2|_p$ with the center at $x_1$ or at $x_2$. If the 2-periodic cycle is an indifferent, then in each step the balls transfer to each other. All the other spheres with radius $>r$ and the center at $x_1$ and $x_2$ are invariant independently of the attractiveness of the cycle. (ii) In the case where the fixed point $x_0$ is unique we prove that if the point is attracting then there exists $δ>0$, such that the basin of attraction for $x_0$ is the ball of radius $δ$ and the center at $x_0$ and any sphere with radius $\geq δ$ is invariant. If $x_0$ is an indifferent point then all spheres with the center at $x_0$ are invariant. If $x_0$ is a repelling point then there exits $δ>0$, such that the trajectory which starts at an element of the ball of radius $δ$ with the center in $x_0$ leaves this ball, whereas any sphere with radius $\geq δ$ is invariant. (iii) In case of existence of two fixed points, we show that Siegel disks may either coincide or be disjoint for different fixed points of the dynamical system. Besides, we find the basin of the attractor of the system. Varying the parameters it is proven that there exists an integer $k\geq 2$, and spheres $S_{r_1}(x_i), ..., S_{r_k}(x_i)$ such that the limiting trajectory will be periodically traveling the spheres $S_{r_j}$. For some values of the parameters there are trajectories which go arbitrary far from the fixed points.

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