Atomic and Molecular Physics of Controlled Thermonuclear Fusion 1983
DOI: 10.1007/978-1-4613-3763-8_11
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Atomic Processes in High-Density Plasmas

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Cited by 6 publications
(3 citation statements)
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References 38 publications
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“…An additional data point, Z * = 24, was chosen as an arbitrary value between 19 and 27. When modelling the ionization process self-consistently, the ions were initialized with Z * 0 = 5, in accordance with the widely used Thomas-Fermi model (More 1983). Both field-tunnelling and electron-ion impact ionization were enabled.…”
Section: Simulation Designmentioning
confidence: 99%
“…An additional data point, Z * = 24, was chosen as an arbitrary value between 19 and 27. When modelling the ionization process self-consistently, the ions were initialized with Z * 0 = 5, in accordance with the widely used Thomas-Fermi model (More 1983). Both field-tunnelling and electron-ion impact ionization were enabled.…”
Section: Simulation Designmentioning
confidence: 99%
“…This correlation heating mechanism operates on ion-plasma-frequency time scales , which is much faster than energy exchange due to interspecies Coulomb collisions (More 1980, 1981, 1983).…”
Section: Introductionmentioning
confidence: 99%
“…This mechanism is an example of correlation heating, in which changing the spatial correlations between particles leads to a rapid conversion of potential energy into kinetic energy. This correlation heating mechanism operates on ion-plasma-frequency time scales t ∼ 1/ω pi , which is much faster than energy exchange due to interspecies Coulomb collisions (More 1980(More , 1981(More , 1983.…”
Section: Introductionmentioning
confidence: 99%