Kinetics of HgX(B‐X) formation due to collisions of Ar+2ions with CH3HgX(X=Cl, Br, I) molecules related to blue‐green laser emission

1990 ◽  
Vol 56 (13) ◽  
pp. 1216-1218
Author(s):  
M. F. Mahmood
1975 ◽  
Vol 4 (8) ◽  
pp. 947-951 ◽  
Author(s):  
N A Borisevich ◽  
V V Gruzinskii ◽  
S V Davydov

Author(s):  
Zhe Liu ◽  
Jean-Louis Doualan ◽  
Western Bolaños ◽  
Bin Xu ◽  
Florent Starecki ◽  
...  
Keyword(s):  

1993 ◽  
Vol 63 (6) ◽  
pp. 729-730 ◽  
Author(s):  
R. Brede ◽  
T. Danger ◽  
E. Heumann ◽  
G. Huber ◽  
B. Chai

2018 ◽  
Vol 6 (1) ◽  
pp. 1801455 ◽  
Author(s):  
Qi Zhang ◽  
Qi Wei ◽  
Xiangru Guo ◽  
Gang Hai ◽  
Huizhi Sun ◽  
...  

2006 ◽  
Vol 8 (2) ◽  
pp. 172-174 ◽  
Author(s):  
F J Duarte ◽  
L S Liao ◽  
K M Vaeth ◽  
A M Miller

2011 ◽  
Vol 8 (10) ◽  
pp. 715-718 ◽  
Author(s):  
Y. Shao ◽  
H.J. Jin ◽  
J. Lin ◽  
D. Zhang ◽  
Z.H. Tao ◽  
...  

1972 ◽  
Vol 50 (20) ◽  
pp. 2523-2535 ◽  
Author(s):  
J. Gilbert ◽  
J. L. Lachambre ◽  
F. Rheault ◽  
R. Fortin

The dynamical processes responsible for laser emission in the pulsed pumping of a transversely excited atmospheric (TEA) CO2 laser are investigated. An explanation for the formation of the giant pulse is proposed on the basis of a gain-switching mechanism in which it is assumed that with short strong-current pulses a high population inversion can be achieved prior to the onset of laser action. The kinetics of the mechanism are described by means of a set of nonlinear rate equations idealized to a four-energy-state system. With suitable initial conditions on the populations, the transient solution of these equations for the mixtures CO2–He and CO–N2–He appears to be consistent with the major features of experimental observation.


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