Mishra Seemant, Ryabov Artem, Maass Philipp
Universität Osnabrück, Fachbereich Mathematik/Informatik/Physik, Barbarastraße 7, D-49076 Osnabrück, Germany.
Charles University, Faculty of Mathematics and Physics, Department of Macromolecular Physics, V Holešovičkách 2, CZ-18000 Praha 8, Czech Republic.
Phys Rev Lett. 2025 Mar 14;134(10):107102. doi: 10.1103/PhysRevLett.134.107102.
In driven nonlinear systems, phase locking is an intriguing effect leading to robust stationary states that are stable over extended ranges of control parameters. Recent experiments allow for exploring microscopic mechanisms underlying such phenomena in collective dynamics of micro- and nanoparticles. Here, we show that phase-locked dynamics of hardcore-interacting microparticles in a densely populated periodic potential under time-periodic driving arises from running solitary cluster waves. We explain how values of phase-locked currents are related to soliton velocities and why collective particle dynamics synchronize with the driving for certain particle diameters only. Our analysis is based on an effective potential for the solitary wave propagation and a unit displacement law, which states that the total average shift of all particle positions per soliton period equals one wavelength of the periodic potential.
在受驱动的非线性系统中,锁相是一种引人入胜的效应,它会导致在扩展的控制参数范围内稳定的稳健稳态。最近的实验使得探索微观和纳米粒子集体动力学中此类现象背后的微观机制成为可能。在此,我们表明,在时间周期驱动下,处于密集填充的周期势中的硬核相互作用微粒的锁相动力学源于运行的孤立簇波。我们解释了锁相电流的值如何与孤子速度相关,以及为什么仅对于某些粒径,集体粒子动力学才会与驱动同步。我们的分析基于孤立波传播的有效势和单位位移定律,该定律指出每个孤子周期内所有粒子位置的总平均位移等于周期势的一个波长。