Abstract
This paper presents an x-ray laser mechanism that uses radiation trapping of the strongest 3${\mathit{d}}^{1}$${\mathit{P}}_{1}$\ensuremath{\rightarrow}2${\mathit{p}}^{1}$${\mathit{S}}_{0}$ neonlike resonance line in an optically thick plasma to create an intense radiation field that radiatively drives population from the neonlike ground state to the 3${\mathit{d}}^{1}$${\mathit{P}}_{1}$ state, which then lases to the 3${\mathit{p}}^{1}$${\mathit{P}}_{1}$ and 3${\mathit{p}}^{3}$${\mathit{P}}_{1}$ states. Collisional mixing of the 3p states with nearby 3s and 3d states depopulates the lower laser states. Modeling is presented for this mechanism in neonlike argon. Strong gain is predicted on the two 3d\ensuremath{\rightarrow}3p transitions at 451 and 465 \AA{}, the first of which has been observed in recent x-ray laser experiments using an argon gas puff. This pumping mechanism also enhances the population of the 3${\mathit{p}}^{1}$${\mathit{S}}_{0}$ state and the gain of the two 3p\ensuremath{\rightarrow}3s, J=0\ensuremath{\rightarrow}1 transitions, which are at 431 and 469 \AA{} in argon. \textcopyright{} 1996 The American Physical Society.
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