摘要
解析地讨论一个冲击振子模型中的边界激变特征 ,证明了这类分段光滑二维映象中激变的生存时间标度律为τ ε-γ,而γ =ln|β2 |ln|β1β2 |(β1,β2 分别是混沌吸引子吸引域边界上鞍点的不稳定和稳定本征值 ) ,这与处处光滑二维映象中相应的规律完全不同 .
This paper analytically discusses the characteristics of boundary crisis in a model of impact oscillator,and proves that the scaling behavior of the life time after crisis follows the rule τ ε\+\{-γ\} and γ=ln|β 2|ln|β 1β\-2|.Here β 1 and β 2 are the unstable and stable eigenvalues,respectively,of a saddle node on the basin boundary of a chaotic attractor.This rule is completely different from that in everywhere\|smooth maps.
出处
《物理学报》
SCIE
EI
CAS
CSCD
北大核心
2000年第9期1679-1682,共4页
Acta Physica Sinica
基金
国家自然科学基金!(批准号 :19975 0 3 9)&&