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Integration of Vlasov equation by quantum mechanical formalism

โœ Scribed by V.T. Nguyen; P. Bertrand; B. Izrar; E. Fijalkow; M.R. Feix


Publisher
Elsevier Science
Year
1985
Tongue
English
Weight
360 KB
Volume
34
Category
Article
ISSN
0010-4655

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โœฆ Synopsis


Title ofprogram: SHRD Method of solution The Vlasov-Poisson system governing collisionless plasma be-Catalogue number.ACCY haviour is replaced by the Schrodinger-Poisson system of equations. To integrate this system numerically, the potential Program available from: CPC Program Library, Queen's Uni-ct'(x, I) is approximated by a series of Dirac time functions and versity of Belfast, N. Ireland (see application form in this issue) takes the form: Computer: NAS 9080 or CRAY 1; Installation: CIRCE, Campus ~( x, t ) ATh (z -(2p + 1) ~T/2). du CNRS, Orsay, France (NAS), CCVR (CRAY 1) p 1 Operating system: (MVS + JES 3) NAS or CRAY OS With this approximation for every time step LIT the Schrbdinger equation splits into two parts, the free particle term Programming language used: Fortran IV or Fortran 77 -h 2/2 m )8 2ip/8x2 and the acceleration term e~( xt)i~(x, I), which are treated separately but exactly. The first term is


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