scholarly journals Vlasov–Maxwell simulations of backward Raman amplification of seed pulses in plasmas

2016 ◽  
Vol 34 (4) ◽  
pp. 576-600
Author(s):  
Magdi Shoucri ◽  
Bedros Afeyan

AbstractWe study the problem of the amplification of an ultra-short seed pulse via stimulated Raman backscattering (SRB) from a long pump pulse (assumed to have an envelope with a constant amplitude), in an underdense plasma. The SRB interaction couples the pump light wave to a daughter light seed wave propagating in the opposite direction, scattered off an electron plasma wave. In recent numerical simulations, it has been observed that besides stimulated Raman backward scattering (SRBS) and stimulated Raman forward scattering, other high-frequency kinetic instabilities can occur when modified distribution functions exist during the evolution of the system. In particular, we showed the prominent role played by kinetic electrostatic electron nonlinear (KEEN) waves (Afeyan et al., 2004). We continue this work by applying a relativistic Vlasov–Maxwell code to study stimulated KEEN wave scattering (SKEENS) and its role in the SRBS short pulse amplification processes. An analysis of the full spectrum of waves participating in the amplification processes is presented. The absence of spurious noise in grid-based Vlasov codes allows us to follow the evolution of the system with a kinetic (collisionless) description. This affords us a glimpse at the intricate phase-space structures such as trapped particle orbits, which coexist and interact nonlinearly in the electron distribution function.

2016 ◽  
Vol 688 ◽  
pp. 012112 ◽  
Author(s):  
Miloš M. Škorić ◽  
Ljubomir Nikolić ◽  
Ljupčo Hadžievski ◽  
Dimitri Batani ◽  
Seiji Ishiguro ◽  
...  

1996 ◽  
Vol 3 (5) ◽  
pp. 1682-1688 ◽  
Author(s):  
V. Malka ◽  
E. De Wispelaere ◽  
J. R. Marquès ◽  
R. Bonadio ◽  
F. Amiranoff ◽  
...  

1996 ◽  
Vol 34 (1) ◽  
pp. 19-24 ◽  
Author(s):  
M. M Škorić ◽  
M. S Jovanović ◽  
M. R Rajković

2010 ◽  
Vol 35 (14) ◽  
pp. 2397 ◽  
Author(s):  
Shian Zhou ◽  
Tetsuji Takamido ◽  
Shinji Imai ◽  
Frank Wise

2021 ◽  
Vol 2056 (1) ◽  
pp. 012022
Author(s):  
A M Bishaev ◽  
M V Abgaryan

Abstract A problem related to the rarefied plasma plume of the stationary plasma thruster (SPT) is considered in the paper. The consideration is conducted fully in terms of kinetics, namely, distribution functions are introduced to describe motion of every plasma component. The system of kinetics equations for the distribution functions should be solved in combination with the Maxwell’s equations. The paper discusses methods for solving the stated problem.


Author(s):  
E. Guillaume ◽  
K. Humphrey ◽  
H. Nakamura ◽  
R. M. G. M. Trines ◽  
R. Heathcote ◽  
...  

Abstract The energy transfer by stimulated Brillouin backscatter from a long pump pulse (15 ps) to a short seed pulse (1 ps) has been investigated in a proof-of-principle demonstration experiment. The two pulses were both amplified in different beamlines of a Nd:glass laser system, had a central wavelength of 1054 nm and a spectral bandwidth of 2 nm, and crossed each other in an underdense plasma in a counter-propagating geometry, off-set by $\def \xmlpi #1{}\def \mathsfbi #1{\boldsymbol {\mathsf {#1}}}\let \le =\leqslant \let \leq =\leqslant \let \ge =\geqslant \let \geq =\geqslant \def \Pr {\mathit {Pr}}\def \Fr {\mathit {Fr}}\def \Rey {\mathit {Re}}10^\circ $ . It is shown that the energy transfer and the wavelength of the generated Brillouin peak depend on the plasma density, the intensity of the laser pulses, and the competition between two-plasmon decay and stimulated Raman scatter instabilities. The highest obtained energy transfer from pump to probe pulse is 2.5%, at a plasma density of $0.17 n_{cr}$ , and this energy transfer increases significantly with plasma density. Therefore, our results suggest that much higher efficiencies can be obtained when higher densities (above $0.25 n_{cr}$ ) are used.


1995 ◽  
Vol 2 (1) ◽  
pp. 274-279 ◽  
Author(s):  
S. C. Wilks ◽  
W. L. Kruer ◽  
E. A. Williams ◽  
P. Amendt ◽  
D. C. Eder

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