Abstract

The experimental work presented in this paper focuses on the consequences of both nonlocal heat transport and rapid time variation in atomic physics as a function of the initial gradient scale length of a plasma. We look at the time history of K-shell emission when an intense 0.53-{mu}m high-contrast pulse heats aluminum plasmas having a chosen gradient scale length. We compare our experimental results to hydrodynamics and atomic physics calculations and we study three different plasma regimes. When the laser pulse interacts with an ultrashort density gradient scale length, the plasma is at local thermodynamic equilibrium and the calculations are in very good agreement with the experimental results. These calculations also agree with the observed spectra in the case of a long gradient scale length (nonstationary Maxwellian regime). However, in the intermediate regime, the observed time history of the Li-like satellite lines is strongly affected by transient atomic physics and nonlocal thermal transport. In this particular regime, the calculated spectra are strongly dependent on the thermal transport model used in the simulations. Simulations in the intermediate regime can therefore be benchmarked and tested against our experimental spectra. {copyright} {ital 1997} {ital The American Physical Society}

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