ImPACT: Innovation in Manufacturing with Palmtop High-power Pulsed Lasers

2020 ◽  
Vol 89 (1) ◽  
pp. 16-20
Author(s):  
Yuji SANO
Keyword(s):  
2013 ◽  
Vol 43 (11) ◽  
pp. 1082-1087
Author(s):  
K F Burdonov ◽  
A A Soloviev ◽  
A S Egorov ◽  
A A Shaikin ◽  
A K Potemkin

1978 ◽  
Vol 9 (2) ◽  
pp. 72-78 ◽  
Author(s):  
A.F Gibson
Keyword(s):  

2020 ◽  
Vol 50 (7) ◽  
pp. 658-661
Author(s):  
A P Pogoda ◽  
A A Sergeev ◽  
I S Khakhalin ◽  
E E Popov ◽  
N L Istomina ◽  
...  

1978 ◽  
Vol 56 (12) ◽  
pp. 1577-1593 ◽  
Author(s):  
E. Pascaud ◽  
G. Poussigue

The development of high power pulsed lasers has permitted the observation of nonlinear light scattering phenomena, in particular the molecular hyper-Raman effect. The wave numbers of hyper-Raman transitions can be predicted simply from the energy differences between known levels. For the intensities, however, it is necessary to devise a well-adapted method of calculation.Hilico, Berger, and Loete have developed a tensor formalism in the (m)O(3) × (F)O(3) group, for the calculation of microwave, infrared, and Raman intensities from XY4 tetrahedral molecules. In this paper, we extend the formalism to a G × (F)O(3) subgroup and make it applicable to the case of hyper-Raman transitions.A general expression for the hyper-Raman intensities of any molecule is given. In the case of XY4 tetrahedral molecules, where a tensor extension to the (m)O(3) × (F)O(3) group is possible, we give the intensity formulas line by line and band by band for the simplest cases.[Journal translation]


2012 ◽  
Vol 42 (4) ◽  
pp. 292-297 ◽  
Author(s):  
G H Kim ◽  
G H Yang ◽  
D S Lee ◽  
Alexander V Kulik ◽  
E G Sall' ◽  
...  

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