New Zealand Institute for Advanced Study, Centre for Theoretical Chemistry & Physics, Massey University, Auckland 0745, New Zealand.
Center for Theoretical Physics of Complex Systems, Institute for Basic Science, Daejeon 34051, Korea.
Phys Rev E. 2017 Jun;95(6-1):060202. doi: 10.1103/PhysRevE.95.060202. Epub 2017 Jun 2.
The equilibrium value of an observable defines a manifold in the phase space of an ergodic and equipartitioned many-body system. A typical trajectory pierces that manifold infinitely often as time goes to infinity. We use these piercings to measure both the relaxation time of the lowest frequency eigenmode of the Fermi-Pasta-Ulam chain, as well as the fluctuations of the subsequent dynamics in equilibrium. The dynamics in equilibrium is characterized by a power-law distribution of excursion times far off equilibrium, with diverging variance. Long excursions arise from sticky dynamics close to q-breathers localized in normal mode space. Measuring the exponent allows one to predict the transition into nonergodic dynamics. We generalize our method to Klein-Gordon lattices where the sticky dynamics is due to discrete breathers localized in real space.
可观测的平衡值在遍历的、等分配的多体系统的相空间中定义了一个流形。随着时间的推移,一个典型的轨迹会无限次地穿过这个流形。我们利用这些穿透来测量费米-玻色-乌伦贝克链的最低频率本征模的弛豫时间,以及平衡后动力学的涨落。平衡后的动力学特征是在远离平衡时的跃迁时间的幂律分布,具有发散的方差。长的跃迁来自于在正常模空间中局部化的 q 声子附近的粘性动力学。测量指数可以预测进入非遍历动力学的转变。我们将我们的方法推广到克菜因-戈尔登格点,其中粘性动力学是由于在实空间中局部化的离散声子引起的。