Abstract

The wave equation for laser light incident on a static, steep-gradient plasma has been solved numerically, with the inclusion of an intensity-dependent electron-ion collision rate, and incorporating spatial dispersion and wave-breaking effects. At moderate intensities (\ensuremath{\sim}${10}^{14}$ W/${\mathrm{cm}}^{2}$), the nonlinearity has little effect on the calculated reflectivity, but at higher intensities the reflectivity is greater than that predicted by a linear model. The discrepancy is small for a steplike plasma (with a density gradient scale length L\ensuremath{\sim}0.01${\ensuremath{\lambda}}_{0}$), but increases for longer scale lengths (L\ensuremath{\sim}${\ensuremath{\lambda}}_{0}$). In the case of p-polarized light, the angular dependence of reflectivity is sharpened at higher intensities, and resonance effects play an important role even for very short scale lengths.

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