Figure 1.

Time-dependent charge carrier concentration for electrons and holes as a function of normalised position ${\mathrm{x}}^{\prime }$ with varying magnetic fields of (a) $B_z^{\prime }=0$ (b) $B_z^{\prime }=0.3$ (c) $B_z^{\prime }=0.6$ (d) $B_z^{\prime }=1$ for Langevin system with $\frac{\beta }{{\beta }_L}=1$.