• DOI:10.1063/1.5090803
• Corpus ID: 125950461

Atomic modeling of photoionization fronts in nitrogen gas

@article{Gray2018AtomicMO,
  title={Atomic modeling of photoionization fronts in nitrogen gas},
  author={William Gray and Paul Arthur Keiter and H. J. LeFevre and C. R. Patterson and J. Steve Davis and Kenneth G. Powell and Carolyn C. Kuranz and R. Paul Drake},
  journal={Physics of Plasmas},
  year={2018}
}

• W. Gray, P. Keiter, +5 authors R. P. Drake
• Published 5 November 2018
• Physics
• Physics of Plasmas

Photoionization fronts play a dominant role in many astrophysical environments, but remain difficult to achieve in a laboratory experiment. Recent papers have suggested that experiments using a nitrogen medium held at ten atmospheres of pressure that is irradiated by a source with a radiation temperature of T$_{\rm R}\sim$ 100 eV can produce viable photoionization fronts. We present a suite of one-dimensional numerical simulations using the \helios\ multi-material radiation hydrodynamics code that models these conditions and the formation of a photoionization front. We study the effects of varying the atomic kinetics and radiative transfer model on the hydrodynamics and ionization state of the nitrogen gas, finding that more sophisticated physics, in particular a multi-angle long characteristic radiative transfer model and a collisional-radiative atomics model, dramatically changes the atomic kinetic evolution of the gas. A photoionization front is identified by computing the ratios between the photoionization rate, the electron impact ionization rate, and the total recombination rate. We find that due to the increased electron temperatures found using more advanced physics that photoionization fronts are likely to form in our nominal model. We report results of several parameter studies. In one of these, the nitrogen pressure is fixed at ten atmospheres and varies the source radiation temperature while another fixes the temperature at 100 eV and varied the nitrogen pressure. Lower nitrogen pressures increase the likelihood of generating a photoionization front while varying the peak source temperature has little effect.