Simulation of the Radiation Reaction Orbits of a Classical Relativistic Charged Particle with Generalized Off-Shell Lorentz Force
Figure 6
(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 cycles, the mass fluctuation amplitude significantly grows towards the cycle’s end. One should also observe the relatively low value of the effective mass around the iteration value of 2500 (the climax of the cycle). (e) Again, the Lyapunov exponent fluctuates during the cycle and returns to decay afterwards.
