Instability dynamics of nonlinear normal modes in the Fermi-Pasta-Ulam-Tsingou chains

Nonlinear normal modes are periodic orbits that survive in nonlinear chains, whose instability plays a crucial role in the dynamics of many-body Hamiltonian systems toward thermalization. Here we focus on how the stability of nonlinear modes depends on the perturbation strength and the system size to observe whether they have the same behavior in different models. To this end, as illustrating examples, the instability dynamics of the N/2 mode in both the Fermi-Pasta-Ulam-Tsingou-alpha and -beta chains under fixed boundary conditions are studied systematically. Applying the Floquet theory, we show that for both models the stability time T as a function of the perturbation strength lambda follows the same behavior; i.e., T proportional to (lambda - lambda(c))(-1/2), where lambda(c) is the instability threshold. The dependence of lambda(c) on N is also obtained. The results of T and lambda(c) agree well with those obtained by the direct molecular dynamics simulations. Finally, the effect of instability dynamics on the thermalization properties of a system is briefly discussed.

Automated summary

This study investigates how the stability of nonlinear modes depends on the perturbation strength and system size, and verifies the same behavior in two different models. The results show that the stability time is inversely proportional to the perturbation strength, and the instability threshold is related to the system size.