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Volumn 13, Issue 2, 2006, Pages

Harmonic decomposition to describe the nonlinear evolution of stimulated Brillouin scattering

Author keywords

[No Author keywords available]

Indexed keywords

ACOUSTIC WAVES; CHAOS THEORY; DECOMPOSITION; HYDRODYNAMICS; ION ACOUSTIC WAVES; NUMERICAL ANALYSIS; PLASMA DEVICES;

EID: 33644594663     PISSN: 1070664X     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.2168403     Document Type: Article
Times cited : (53)

References (47)
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    • Two different hydrodynamic schemes were checked: (1) CLAWPACK solver, by R. J. Le Vecque [see http://www.amath.washington.edu/claw/; R. J. Le Vecque, J. Comp. Phys. 0021-9991 131, 327 (1997); R. J. Le Vecque Numerical Methods for Conservation Laws, Birkhäuser, Basel, 1992)]; (2) the "leap frog" method cited in M. Kozlov and C. J. McKinstrie, Phys. Plasmas 9, 3783 (2002).
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    • Two different hydrodynamic schemes were checked: (1) CLAWPACK solver, by R. J. Le Vecque [see http://www.amath.washington.edu/claw/; R. J. Le Vecque, J. Comp. Phys. 0021-9991 131, 327 (1997); R. J. Le Vecque Numerical Methods for Conservation Laws, Birkhäuser, Basel, 1992)]; (2) the "leap frog" method cited in M. Kozlov and C. J. McKinstrie, Phys. Plasmas 9, 3783 (2002).
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    • Two different hydrodynamic schemes were checked: (1) CLAWPACK solver, by R. J. Le Vecque [see http://www.amath.washington.edu/claw/; R. J. Le Vecque, J. Comp. Phys. 0021-9991 131, 327 (1997); R. J. Le Vecque Numerical Methods for Conservation Laws, Birkhäuser, Basel, 1992)]; (2) the "leap frog" method cited in M. Kozlov and C. J. McKinstrie, Phys. Plasmas 9, 3783 (2002).
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    • In the averaging procedure, we disregard the early instability transient growth.
    • In the averaging procedure, we disregard the early instability transient growth.
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    • note
    • To do so, we modified the electrostatic potential φ (z,t) ∝ c se 2 ln N0 (z,t) by subtracting its value φ (z,t=0) ∝ c se 2 ln N0 (z,t=0), corresponding to the initial density profile at t=0, so that the electron pressure term c se 2 ∇ N0 (z,t) of Eq. has to be replaced by c se 2 ∇ [N0 (z,t) - N0 (z,t=0)].


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