Generation of coherent radiation continuously tunable in 515-650-nm range by efficient second harmonic conversion of LiF:F/sub 2//sup -/ laser radiation

Author(s):  
A.Yu. Dergachev ◽  
S.B. Mirov
1972 ◽  
Vol 2 (2) ◽  
pp. 175-176
Author(s):  
V D Volosov ◽  
A M Dykhovnyi ◽  
V N Krylov ◽  
T V Sokolova

2013 ◽  
Vol 40 (7) ◽  
pp. 205-209 ◽  
Author(s):  
B. L. Vasin ◽  
Yu. V. Korobkin ◽  
M. V. Osipov ◽  
V. N. Puzyrev ◽  
A. T. Sahakyan ◽  
...  

2011 ◽  
Vol 38 (11) ◽  
pp. 317-322
Author(s):  
B. L. Vasin ◽  
M. V. Osipov ◽  
V. N. Puzyrev ◽  
A. T. Saakyan ◽  
A. N. Starodub

1995 ◽  
Vol 413 ◽  
Author(s):  
G. I. Stegeman ◽  
M. JÄger ◽  
A. Otomo ◽  
W. Brinker ◽  
S. Yilmaz ◽  
...  

ABSTRACTThe phenomenon of second harmonic generation has been studied from the earliest days of nonlinear optics.[l] To date the most impressive results in terms of conversion efficiency for as low an input power as possible have been obtained in channel waveguides made from inorganic materials.[2] However, when their second order nonlinearities (10s of pm/V) are compared with those of organic materials (10s → 100s pmn/V), it is clear that organic materials should eventually produce much better harmonic conversion efficiencies. [3]


1997 ◽  
Vol 58 (4) ◽  
pp. 613-621 ◽  
Author(s):  
JETENDRA PARASHAR ◽  
H. D. PANDEY ◽  
A. K. SHARMA ◽  
V. K. TRIPATHI

An intense short laser pulse or a millimetre wave propagating through a plasma channel may act as a wiggler for the generation of shorter wavelengths. When a relativistic electron beam is launched into the channel from the opposite direction, the laser radiation is Compton/Raman backscattered to produce coherent radiation at shorter wavelengths. The scheme, however, requires a superior beam quality with energy spread less than 1% in the Raman regime.


1987 ◽  
Vol 7 (2-4) ◽  
pp. 129-139 ◽  
Author(s):  
Toshiaki Munakata ◽  
Tadahiko Mizukuki ◽  
Akira Misu ◽  
Motowo Tsukakoshi ◽  
Takahiro Kasuya

The photoionization spectrum of HBr around the first ionization limit was measured at resolution of up to 5 x 10−4 nm. The ionizing vacuum ultraviolet radiation was generated by frequency tripling of the second harmonic output of a dye laser. Three sets of Rydberg series, each converging to the ground state (2Π3/2) of HBr+, were observed on the longer wavelength side of the ionization limit. By extrapolation of the Rydberg series, the ionization potential of HBr was determined to be 11.666 ± 0.001 eV.


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