Titlebook: Dynamical Systems and Chaos; Proceedings of the S Luis Garrido Conference proceedings 1983 Springer-Verlag Berlin Heidelberg 1983 Chaos.Cha

MAXIM

書目名稱Dynamical Systems and Chaos影響因子(影響力)




書目名稱Dynamical Systems and Chaos影響因子(影響力)學(xué)科排名




書目名稱Dynamical Systems and Chaos網(wǎng)絡(luò)公開(kāi)度




書目名稱Dynamical Systems and Chaos網(wǎng)絡(luò)公開(kāi)度學(xué)科排名




書目名稱Dynamical Systems and Chaos被引頻次




書目名稱Dynamical Systems and Chaos被引頻次學(xué)科排名




書目名稱Dynamical Systems and Chaos年度引用




書目名稱Dynamical Systems and Chaos年度引用學(xué)科排名




書目名稱Dynamical Systems and Chaos讀者反饋




書目名稱Dynamical Systems and Chaos讀者反饋學(xué)科排名

OGLE

https://doi.org/10.1007/978-3-662-44268-5ternal forces. The onset of diffusion has strong analogies with a phase-transition. The diffusion coefficient is the order parameter and has a universal critical exponent. The dependence on random external fluctuations is also universal and can be expressed in terms of a universal scaling function which is calculated analytically.

capillaries

Macroscopic behavior in a simple chaotic Hamiltonian system,ich too (like the main regime) is the same for both time directions. One of the two particles hereby shows a statistical directional preference. This preference is the same as when the system is run as an open system (‘temporarily open regime’). The simple nature of the system encourages further quantitative and qualitative investigations.

彎彎曲曲

Self-generated diffusion and universal critical properties in chaotic systems,ternal forces. The onset of diffusion has strong analogies with a phase-transition. The diffusion coefficient is the order parameter and has a universal critical exponent. The dependence on random external fluctuations is also universal and can be expressed in terms of a universal scaling function which is calculated analytically.

激怒某人

過(guò)分自信

Imbedding of a one-dimensional endomorphism into a two-dimensional diffeomorphism. Implications,μ, such that μ = o gives a one unit decrease of the dimension. The method of sections of Poincaré gives a generalization of T., x. = f(x., a) + y. h(x., y.), y. b g(x., y.) ., b = 0(μ.), a > o, f, g, h being functions such that this mapping T is a difformorphism .. Then Tb can be considered as a first approach to the study of T.

過(guò)分自信

Chaotic dynamics in Hamiltonian systems with divided phase space,

ironic

CRUMB

,A universal transition from quasi-periodicity to Chaos — Abstract,

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