Frequency dependence of the amplifying parameters of a CuBr laser
Source abstract
Abstract
A pair of copper bromide lasers in an oscillator–amplifier configuration was used to investigate the small-signal gain and saturation intensity as amplifying parameters in terms of pulse repetition frequency. Some fluctuations in the laser output power were recorded by varying the excitation frequency from 13 to 29 kHz as well as the amplifying parameters. The effect arises from the laser tube, which performs as both an optical resonator and an acoustic resonator. At some frequencies, which were matched by tube acoustic resonance, the acoustic energy overcomes the optical energy. The relation between frequencies that give maximum and minimum laser output powers was obtained so that the frequency that corresponds to a minimum laser output power is the average of two adjacent frequencies that correspond to a maximum output power. An empirical formula was obtained to calculate the optimum operational frequency in terms of tube diameter, which gives a maximum laser output power. The efficiency of the laser is highest at the lowest pulse repetition frequency, which gives considerable output power.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Laser Design and Applications · Spectroscopy and Laser Applications · Analytical Chemistry and Sensors
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Plasma Physics Research Center, Sciences and Research Branch, Islamic Azad University 1 , 1477893855 Tehran, Iran
Photonics and Quantum Technologies Research School, Nuclear Science and Technology Research School 2 , P.O. Box 14399511-13, 1439951113 Tehran, Iran
References (20)
Show source-provided references
1. Characteristics of a copper bromide laser with flowing Ne-HBr buffer gas10.1007/BF01234281 ↗
2. High-power gas lasers10.1117/12.18498 ↗
3. Study of scalability of capacitive excited CuBr lasers10.1134/S1024856013030081 ↗
4. Bul. Tomsk Polytechnic-Univ. · 2009 · 305 · 141
5. Active optical systems with a copper bromide vapor amplifier10.1070/QE1988v018n04ABEH011761 ↗
6. Prametric study of CuBr laser with hydrogen additives10.1109/3.7136 ↗
7. Gain characteristics of large volume CuBr laser active media10.1016/j.optcom.2011.01.047 ↗
8. Acoustic effects of metal vapor lasers10.1364/AO.48.003460 ↗
9. Frequency dependence of the output power of metal vapor lasers10.1016/j.optcom.2008.03.059 ↗
10. Influence of acoustic waves on the output power of pulsed gas discharge lasers10.1070/QE1982v012n02ABEH005463 ↗
11. A CuBr laser with 1.4W/cm3 average output power10.1109/3.299456 ↗
12. Influence on operating characteristics of scaling sealed-off CuBr lasers in active length10.1016/S0030-4018(96)00638-4 ↗
13. Pressure dependence of the small-signal gain and saturation intensity of a copper vapor laser10.1364/AO.42.001013 ↗
14. Temperature dependence of the amplifying parameters of a copper vapor laser
15. Pressure dependence of the small-signal gain and saturation intensity of a gold-vapor laser using various buffer gases in gain medium10.1016/j.optcom.2009.11.052 ↗
16. Dependence of small-signal gain and saturation intensity on laser active length, buffer gas type, and pressure variations in gold-vapor laser10.1007/s10946-008-9026-1 ↗
17. Frequency dependence of amplifying parameters of a copper vapor laser using air as a buffer gas10.1007/s10946-011-9241-z ↗
18. Gain measurement of a CuBr laser by means of modified amplified spontaneous emission10.1063/1.345002 ↗
19. Time dependence of the gain of a CuBr laser10.1016/0030-4018(92)90224-F ↗
20. The operating regime of longitudinal discharge copper vapor lasers10.1007/BF00619645 ↗