Fig. 6: The robustness of the magnetized plasma rotator.

a–d The Stokes parameters, the eccentricity \({E}_{z}/{E}_{y}\), and e–h the beam parameters and the efficiency of the generated mid-IR pulse with different plasma density \({n}_{0}\), converter length \({L}_{{\rm{c}}}\), output length \({L}_{{\rm{o}}}\), and the initial laser intensity \({a}_{{\rm{L}}}\). In all cases, \(B=1000\) T