Properties of cooled, uncoated ruby laser oscillators

1964 ◽  
Vol 52 (10) ◽  
pp. 1255-1256 ◽  
Author(s):  
F.A. Brand ◽  
H. Jacobs ◽  
C. LoCascio ◽  
G. Novick ◽  
D. Schick
Keyword(s):  
1966 ◽  
Vol 37 (10) ◽  
pp. 3750-3753 ◽  
Author(s):  
David W. Gregg ◽  
Scott J. Thomas

1964 ◽  
Vol 35 (7) ◽  
pp. 2267-2269 ◽  
Author(s):  
D. P. Bortfeld ◽  
R. S. Congleton ◽  
M. Geller ◽  
R. S. McComas ◽  
L. D. Riley ◽  
...  

1995 ◽  
Vol 131 (5) ◽  
pp. 621-623 ◽  
Author(s):  
D. J. Goldberg
Keyword(s):  

2007 ◽  
Vol 69 (5) ◽  
pp. 511-514 ◽  
Author(s):  
Takako KURIHARA ◽  
Yoshihide HONDA
Keyword(s):  

Optik ◽  
2020 ◽  
Vol 214 ◽  
pp. 164583
Author(s):  
Qihao Hu ◽  
Pengrui Wang ◽  
Meng Wang ◽  
Zefeng Wang

1993 ◽  
Vol 164-166 ◽  
pp. 235-238 ◽  
Author(s):  
O. Klíma ◽  
O. Štika ◽  
Ho Tha Ha ◽  
S. Fouad Abdel Hamied ◽  
J. Stuchlík ◽  
...  

1970 ◽  
Vol 25 (12) ◽  
pp. 1374-1381 ◽  
Author(s):  
W. Kiefer ◽  
H. W. Schrötter

The Raman spectra of four molecules absorbing in the visible region (SnJ4, GeJ4, TiBr4, and TiJ4) are presented. They were excited with a quasi-continuous ruby laser and recorded with a special electronic detection system. Except for TiJ4, complete Raman spectra of crystal powder pellets could be obtained for the first time. The assignment reported by previous authors was confirmed by accurate polarization studies of solutions or pure liquid. The assignment is also in the solid state possible on the basis of Td point group symmetry. The fundamental vibrations of TiJ4 in solutions are: ν1 (A1) =162, ν2 (E) =51, ν3 (F2) =319 and ν4 (F2) Y = 67 cm-1


Sign in / Sign up

Export Citation Format

Share Document