Uphill anomalous transport in a deterministic system with speed-dependent friction coefficient
Guo Wei1, †, Du Lu-Chun2, Liu Zhen-Zhen2, Yang Hai1, Mei Dong-Cheng2
       

Bifurcation diagram as a function of β for the two curves in Fig. 1, f = 0 (a) and f = 0.1 (b), obtained by stroboscopically sampling trajectories after each period of the driving, discarding a considerably long transient. The initial condition (uniformly distributed position and vanished velocity [21]) is reset whenever β changes.[46]