Kinetic simulation of a plasma collision experiment

The ionic Fokker–Planck code which was written for describing plasma shock wave fronts [M. Casanova et al. Phys. Rev. Lett. 67, 2143 (1991)] is applied to model the collision of two plasmas in plane geometry. Improvements brought to the code for that purpose are described. The initial phase of the experiment during which the plasmas interpenetrate is accounted for by a simple fluid model, which yields qualitative insight into the phenomena at play as well as an initial condition to start the kinetic simulation. The kinetic results obtained in the stagnation and thermalization phases are discussed with respect to a specific laser‐produced plasma collision experiment, as well as to existing fluid and kinetic (‘‘particle‐in‐cell’’) simulations.

[1]  W. Yu,et al.  Temporal evolution of X-ray spectra from laser microtube targets , 1988 .

[2]  J. Luciani,et al.  Collisional effects and dispersion relation of magnetic field structures , 1987 .

[3]  R. Berger,et al.  Effect of counterstreaming ion flow on ion acoustic modes and stimulated Brillouin scattered light , 1988 .

[4]  Casanova,et al.  Kinetic simulation of a collisional shock wave in a plasma. , 1991, Physical review letters.

[5]  Lyman Spitzer,et al.  THE ELECTRICAL CONDUCTIVITY OF AN IONIZED GAS , 1950 .

[6]  H. E. Dalhed,et al.  Plasma‐implosion‐driven, photoionization‐pumped, soft x‐ray laser targets , 1989 .

[7]  M. Marconi,et al.  Proposal for soft-x-ray and XUV lasers in capillary discharges. , 1988, Optics letters.

[8]  J. Allen,et al.  The expansion of a plasma into a vacuum , 1975, Journal of Plasma Physics.

[9]  H. Kunze,et al.  Observation of gain at 18.22 nm in the carbon plasma of a capillary discharge , 1990 .

[10]  Richard L. Berger,et al.  Collision and interpenetration of plasmas created by laser-illuminated disks , 1992 .

[11]  J. Gillis,et al.  Methods in Computational Physics , 1964 .

[12]  A. B. Langdon,et al.  Stopping and thermalization of interpenetrating plasma streams , 1991 .

[13]  J. Scofield,et al.  A gas puff soft x‐ray laser target design , 1985 .

[14]  J. Denavit,et al.  Time-implicit fluid simulation of collisional plasmas , 1992 .

[15]  I. S. Gradshteyn,et al.  Table of Integrals, Series, and Products , 1976 .

[16]  R. S. Craxton,et al.  X-ray laser experiments using double foil nickel targets , 1990 .

[17]  N. A. Krall,et al.  Principles of Plasma Physics , 1973 .

[18]  Deeney,et al.  Role of the implosion kinetic energy in determining the kilovolt x-ray emission from aluminum-wire-array implosions. , 1991, Physical review. A, Atomic, molecular, and optical physics.

[19]  G. Tsakiris,et al.  Experiments with laser-irradiated cylindrical targets , 1991 .

[20]  G. Marchuk Methods of Numerical Mathematics , 1982 .

[21]  William M. MacDonald,et al.  Fokker-Planck Equation for an Inverse-Square Force , 1957 .

[22]  H. Daido,et al.  Simulation of recombination-pumped soft-x-ray lasers in wall-confined laser-produced plasmas , 1990 .

[23]  Remy Fabbro,et al.  Planar laser-driven ablation: Effect of inhibited electron thermal conduction , 1985 .

[24]  Epstein,et al.  Multibeam, laser-imploded cylindrical plasmas. , 1986, Physical review. A, General physics.