Spectral photoconductivity of tellurium in the CO2 laser wavelength range

1973 ◽  
Vol 13 (7) ◽  
pp. 789-791 ◽  
Author(s):  
K.J. Siemsen ◽  
H.D. Riccius
1967 ◽  
Vol 38 (6) ◽  
pp. 2692-2693 ◽  
Author(s):  
G. B. Jacobs ◽  
H. C. Bowers

1985 ◽  
Vol 17 (2) ◽  
pp. 96-98 ◽  
Author(s):  
D. Ignjatijevic ◽  
P. Vujkovic Cvijin ◽  
M. Sreckovic ◽  
I. Pippi

Author(s):  
Lan Jiang ◽  
Hai-Lung Tsai

Lasers especially multiple laser beams demonstrate unique advantages as energy sources in diamond synthesis. However, the fundamental mechanisms involved in the laser-assisted processes are not Well understood. In a reported amazingly-fast multiple laser coating technique, CO2 gas is claimed as the sole precursor or secondary precursor, which remains poorly understood and unverified. The absorption coefficient changes under the irradiation of the multiple lasers are one of the keys to resolve the mysteries of multiple laser beam coating processes. This study investigates the optical absorption in CO2 gas at the CO2 laser wavelength. This resonance absorption process is modeled as an inverse process of the lasing transitions of CO2 lasers. The well-established CO2 vibrational-rotational energy structures are used as the basis for the calculations with the Boltzmann distribution for equilibrium states and the three-temperature model for non-equilibrium states. Based on the population distribution, our predictions of CO2 absorption coefficient changes as the function of temperature are in agreement with the published data.


2009 ◽  
Vol 97 (1) ◽  
pp. 199-206 ◽  
Author(s):  
L. Jiang ◽  
L. Li ◽  
H.-L. Tsai

1986 ◽  
Vol 6 (6) ◽  
pp. 361-371 ◽  
Author(s):  
Susan M. Grenci ◽  
George R. Bird ◽  
Brian W. Keelan ◽  
Ahmed H. Zewail

We have operated a dye laser over a broad wavelength range (593.8–667.0 nm) by shifting the dye emission profile with incremental changes of solvent composition. This was accomplished with the laser operating continuously, and only minor adjustment of the laser optics was required. Solvent tuning was facilitated by the critical dependence of the optimum laser wavelength on concentration of the second solvent. Using the known solvent-sensitive laser dye 9-diethylaminobenzo[a]phenoxaz-5-one (DBP), 87% of the tuning range from pure xylenes to pure methanol was covered by cumulative addition of 24 vol. % methanol to the starting xylenes solution. The optimum dye concentration was found to be independent of solvent composition, so that maximum laser power could be maintained by mixing equimolar dye solutions in the two solvents. These results establish the practicality of solvent-tuning as a method of conducting laser experiments over a broad wavelength range.


1979 ◽  
Vol 57 (10) ◽  
pp. 1779-1783 ◽  
Author(s):  
V. E. Merchant

The energy per unit urea necessary for the occurrence of visible fluorescence from dissociation products of laser irradiated SiF4 has been measured for several values of CO2 laser wavelength and gas pressure. Fluorescence was observed at a lower irradiance when the laser was tuned far from the ν3 absorption band of SiF4 than when the laser was coincident with the absorption band. In the latter case the irradiance required for dissociation decreased as gas pressure was increased from 2 to 10 Torr. However, for nonresonant excitation the irradiance required increased with increasing pressure in the same pressure range. In addition the temporal response of the fluorescence to the exciting radiation was found to depend upon the laser wavelength.


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