M2 of MOPA CuBr Laser Radiation
| Autor: | Nikola V. Sabotinov, Lyubomir I. Stoychev, Dimo N. Astadjov |
|---|---|
| Rok vydání: | 2007 |
| Předmět: |
Copper vapor laser
Materials science business.industry Linear polarization Near and far field Optical polarization Radiation Laser Atomic and Molecular Physics and Optics Electronic Optical and Magnetic Materials law.invention Optics law Optoelectronics Electrical and Electronic Engineering Absorption (electromagnetic radiation) business Beam (structure) |
| Zdroj: | Optical and Quantum Electronics. 39:603-610 |
| ISSN: | 1572-817X 0306-8919 |
| DOI: | 10.1007/s11082-007-9113-5 |
| Popis: | The beam propagation factor, M2 of the master-oscillator power-amplifier (MOPA) CuBr laser emission compliant with ISO 11146 is studied methodically. Statistical parameters of 2D intensity profile of the near and far fields of MOPA laser radiation are measured by a beam analyzing technique as functions of timing delay between MO and PA. For first time the influence of the gas buffer (causing the radiation profile to change from annular to top-hat and Gaussian-like) and light polarization on CuBr laser beam focusability (M2) was under investigation. The MOPA gain curve is found and the influence of gain on the input signal (from MO into PA) due to the absorption/amplification in PA on the field profiles is shown. For annular radiation M2 range is from 13–14 (small delays) to 5–6 (large delays) and for filled-center radiation M2 is 6–7 (small delays) and at the end of gain curve is as much as 4. With polarized light, M2 drops to 3 at the end of gain curve. The brightness of laser emission with hydrogen goes up 3–5 times and the linearly-polarized beam is at least 40% brighter than that of partial or non-polarized beams. |
| Databáze: | OpenAIRE |
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