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Influence of strong magnetic fields on laser pulse propagation in underdense plasma

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Figure

Figure 2: The calculated relationship between γ and afor RCP light in the whistler mode
Figure 3: Calculated group velocity for light of varyingintensity in a plasma of constant densityquite different from those calculated due to the finitenature of real pulses
Figure 4: The adjustment to the critical power for self-focusing as induced by an applied magnetic field
Figure 6: Simulation results for a RCP pulse with Bcolumn shows the longitudinal amplitude profile, the right column shows the transverse amplitude profile at thelongitudinal peak amplitude
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