Simulation of the Radiation Reaction Orbits of a Classical Relativistic Charged Particle with Generalized Off-Shell Lorentz Force
Figure 5
(a) and (b) The and the phase space graphs, respectively. (c) and (d) and the (universal time) effective mass as functions of the number of iterations. As in the previous cycle, the mass fluctuation amplitude grows. (e) Again, the Lyapunov exponent fluctuates during the cycle and returns to decay as it ends.
