Dipartimento di Fisica e Astronomia and CSDC, Università degli Studi di Firenze, via G. Sansone 1, 50019 Sesto Fiorentino, Italy.
INFN Sezione di Firenze, via G. Sansone 1, 50019 Sesto Fiorentino, Italy.
Phys Rev E. 2019 Jan;99(1-1):012303. doi: 10.1103/PhysRevE.99.012303.
We consider a one-dimensional directional array of diffusively coupled oscillators. They are perturbed by the injection of small additive noise, typically orders of magnitude smaller than the oscillation amplitude, and the system is studied in a region of the parameters that would yield deterministic synchronization. Non-normal directed couplings seed a coherent amplification of the perturbation: this latter manifests as a modulation, transversal to the limit cycle, which gains in potency node after node. If the lattice extends long enough, the initial synchrony gets eventually lost, and the system moves toward a nontrivial attractor, which can be analytically characterized as an asymptotic splay state. The noise assisted instability, ultimately vehiculated and amplified by the non-normal nature of the imposed couplings, eventually destabilizes also this second attractor. This phenomenon yields spatiotemporal patterns, which cannot be anticipated by a conventional linear stability analysis.
我们考虑一维定向耦合振荡器的方向数组。它们受到小的附加噪声的注入的干扰,通常比振荡幅度小几个数量级,并且在参数区域中研究系统,该区域将产生确定性同步。非正态定向耦合会引发对扰动的相干放大:后者表现为横向于极限环的调制,其在每个节点上都增强。如果晶格足够长,初始同步最终会丢失,系统会朝着一个非平凡的吸引子移动,这个吸引子可以通过渐近 splay 状态进行分析。噪声辅助不稳定性最终通过施加的非正态耦合的性质得到传递和放大,最终也会破坏第二个吸引子。这种现象产生了时空模式,这是传统线性稳定性分析无法预测的。