Experimental determination of the absolute intensities of Raman-scattering lines and calculation of thresholds and amplifications for the stimulated Raman lines of phenylacetylene and styrene

1971 ◽  
Vol 14 (3) ◽  
pp. 409-412
Author(s):  
N. D. Shvedova ◽  
S. M. Kats ◽  
L. M. Sverdlov
1975 ◽  
Vol 53 (5) ◽  
pp. 455-458 ◽  
Author(s):  
J. A. Kernahan ◽  
P. H-L. Pang

We have obtained the transition probabilities of the 5577 Å, and 6300 Å lines of [OI] by simultaneously measuring the absolute intensity and the population of the upper state of each line in an inert gas–oxygen discharge. Further, we have obtained A values for the 2972 Å and 6364 Å lines by measuring relative intensities of lines from the 1S0 and 1D2 levels.


Author(s):  
Yao Zhao ◽  
Zhengming Sheng ◽  
Suming Weng ◽  
Shengzhe Ji ◽  
Jianqiang Zhu

Absolute instability modes due to secondary scattering of stimulated Raman scattering (SRS) in a large nonuniform plasma are studied theoretically and numerically. The backscattered light of convective SRS can be considered as a pump light with a finite bandwidth. The different frequency components of the backscattered light can be coupled to develop absolute SRS instability near their quarter-critical densities via rescattering process. The absolute SRS mode develops a Langmuir wave with a high phase velocity of about $c/\sqrt{3}$ with $c$ the light speed in vacuum. Given that most electrons are at low velocities in the linear stage, the absolute SRS mode grows with very weak Landau damping. When the interaction evolves into the nonlinear regime, the Langmuir wave can heat abundant electrons up to a few hundred keV via the SRS rescattering. Our theoretical model is validated by particle-in-cell simulations. The absolute instabilities may play a considerable role in the experiments of inertial confinement fusion.


2017 ◽  
Vol 89 (13) ◽  
pp. 6931-6935 ◽  
Author(s):  
Michael O. McAnally ◽  
Brian T. Phelan ◽  
Ryan M. Young ◽  
Michael R. Wasielewski ◽  
George C. Schatz ◽  
...  

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