Numerical Calculations of Plasma Heating by Means of Subnanosecond Laser Pulses

Author(s):  
J. W. Shearer ◽  
W. S. Barnes
1979 ◽  
Vol 34 (9) ◽  
pp. 1059-1062 ◽  
Author(s):  
P. Mulser ◽  
G. Spindler

Abstract The influence of light pressure on plane and spherical plasma flows is treated. Numerical calculations show that smooth laser pulses lead to formation of an overdense plateau if thermal transport is non-negligible there, and that an originally supersonic flow becomes subsonic in this region. The results are consistent with analytical considerations. Density humps, as reported in the literature, are found in conjunction with spiking pulses or prepulses only.


2013 ◽  
Vol 12 (03) ◽  
pp. 1350006 ◽  
Author(s):  
YONG LIU ◽  
JIAN LI ◽  
JIE YU ◽  
SHU-LIN CONG

We present a theoretical scheme for achieving the field-free molecular orientation in dissipative media by a combination of femtosecond and THz laser pulses. Numerical calculations are performed by solving the quantum Liouville equation based on multilevel Bloch model. The molecular orientation degree is sensitive to the carrier-envelope phase of the THz pulse and the delay time between the two pulses. The orientation and the rotational population of CO molecules in dissipative environment are computed at different pressures and temperatures. The influence of pure decoherence on the molecular orientation is also discussed.


1991 ◽  
Vol 9 (2) ◽  
pp. 465-475 ◽  
Author(s):  
F. Cornolti ◽  
P. Mulser ◽  
M. Hahn

Femtosecond laser pulses are capable of producing very high light intensities at moderate pulse energies. We study the laser light absorption at flux densities of 1017 W/cm2 and higher during the plasma formation and the plasma heating process. In the first stage multiphoton and collisional ionization dominate. Modification of the inverse bremsstrahlung absorption occur owing to ionization dephasing. In the second stage beam energy conversion is mainly by collisional absorption at normal incidence, and by resonance absorption at oblique illumination. Simultaneously strong electron heat conduction provides for plasma formation and heating in deeper layers of the solid not accessible to the laser light. The penetration depth of the laser beam is modified by the anomalous skin effect. The electron-ion collision frequency at the high laser intensities under consideration is determined by the oscillation energy of the electrons rather than by their thermal motion. Although it reaches high values (1014-1016 S-1), all kinds of solid targets become strongly reflecting (>60%) owing to the formation of electron densities largely exceeding those of solid-state plasmas. Effects modifying the degree of absorption are briefly discussed.


1988 ◽  
Vol 6 (3) ◽  
pp. 621-624 ◽  
Author(s):  
W. Brunner ◽  
R. John ◽  
Th. Schlegel

Plasma heating by short laser pulses is investigated theoretically. Gain coefficients of 3… 4 cm−1 at the Balmer α transition in carbon could be obtained. The theoretical results agree with the corresponding experimental findings.


2003 ◽  
Author(s):  
Konstantin N. Makarov ◽  
Dmitri D. Maluta ◽  
Vitali C. Roerich ◽  
Yuri A. Satov ◽  
Yuri B. Smakovskii ◽  
...  

1972 ◽  
Vol 38 (5) ◽  
pp. 303-304
Author(s):  
B.A. Demidov ◽  
S.D. Fanchenko ◽  
G.V. Sholin ◽  
S.D. Zakharov ◽  
P.G. Kriukov

Photonics ◽  
2020 ◽  
Vol 7 (2) ◽  
pp. 38
Author(s):  
Ivan Laryushin

The dependence of the terahertz energy generated by two-color femtosecond ionizing pulses on intensities of both one-color components is studied. The numerical calculations are supported with analytical formulas which help to reveal the nature of these dependences. The optimal intensity ratios in the cases when the frequency ratios in two-color pulse are equal to 2, 3/2 and 4 are found.


2004 ◽  
Vol 164 (1-3) ◽  
pp. 67-72 ◽  
Author(s):  
A.V. Brantov ◽  
V.Yu. Bychenkov ◽  
O.V. Batishchev ◽  
W. Rozmus

2002 ◽  
Vol 12 (3) ◽  
pp. 201-206 ◽  
Author(s):  
Janina Marciak-Kozłowska ◽  
Mirosław Kozłowski
Keyword(s):  

2001 ◽  
Vol 11 (PR2) ◽  
pp. Pr2-39-Pr2-42 ◽  
Author(s):  
M. Kado ◽  
T. Kawachi ◽  
N. Hasegawa ◽  
M. Tanaka ◽  
K. Sukegawa ◽  
...  

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