Hans Schamel
Hans Schamel



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Hans Schamel > Publications > Plasma Expansion into Vacuum - the spiky fast ion front

Plasma Expansion into Vacuum - the spiky fast ion front

Plasma Expansion into Vacuum and the Spiky Fast Ion Front

APPLICATIONS:
  ~ intense laser irradiation of matter and atomic clusters[1-3]
  ~ plasma based acceleration of  ions [1-3]
  ~ matter generation in the early phase of our expanding universe [3]

REVIEW ARTICLES:
  [1] Ch.Sack and H.Schamel,  Sunion - an algorithm for one-dimensional
  laser-plasma interaction, J. Comp. Phys. 53(1984)395-428
  [2] Ch.Sack and H.Schamel, Plasma expansion into vacuum -
  a hydrodynamic approach, Phys. Reports 156(1987)311-395
  [3] H.Schamel, Lagrangian fluid description with simple applications in
  compressible plasma and gas dynamics,
  Phys.Reports 392(2004)279 - 319  and references therein

BASIC EQUATIONS:
  ~ cold ion fluid equations without and with Navier-Stokes viscosity term
  ~ polytropic electron equation of state
  ~ Poisson's equation
  at t=0: semi-infinite plasma with a step-like, but continuous ion density

NEW RESULTS:
  a) inviscid case
  ~ discovery of ion density collapse in the laser-plasma interaction [1]
  ~ explanation of density collapse during plasma expansion as an ion
  wave breaking phenomenon resulting from wave steepening  [2,3] 
  Keywords: simple wave analysis, derivation and solution of  nonlinear
  scalar wave equation in Lagrangian fluid description-> Sack-Schamel equation:
  (see also https://en.wikipedia.org/wiki/ Sack-Schamel equation)
 
 
  V = 1 / n , the specific volume.
 
  b) viscid case
  to allow long term simulations:  inclusion of an ion viscosity term
 accounting for anomalous plasma transport
 (keywords: plasma turbulence due to multiple ion streaming after the
  collapse event, coarse-grained  ion Vlasov distribution function)
  ~ supersonic propagation of a peaked ion density front, the peak
 being a remnant of  the density collapse [2,3]
 
  ~ essentially 3 phases of evolution can be distinguished :
  i) initial phase up to ion density bunching
  ii) a stable peaked ion density front propagating with constant
  velocity supersonically towards vacuum
  iii) decay of the leading density hump due to debunching and
  further acceleration of the resultant tiny ion front up to a
  value determined by self-similar theory [2,3] 

NUMERICAL SUBTLETIES :  
  ~ exact numerical treatment of ion dynamics by a Lagrangian code [1,2]
  ~ need for a Poisson solver of high resolution and fast convergence of
  the iteration procedure [1,2]
  ~ tri-diagonal coefficient matrix for the discretized evolution equations
  with open (i.e. differential) boundary conditions [1,2]


© Hans Schamel Last update: April 25. 2023 10:22:36