Cavity dumping by the second harmonic generation

  • Alexander S. Gorbatsevich Belarusian State University, 4 Niezaliežnasci Avenue, Minsk 220030, Belarus
  • Roza I. Navitskaya Belarusian State University, 4 Niezaliežnasci Avenue, Minsk 220030, Belarus
  • Ihar V. Stashkevich Belarusian State University, 4 Niezaliežnasci Avenue, Minsk 220030, Belarus

Abstract

In this paper we propose a method of cavity dumping by the second harmonic generation. Theoretical modeling of laser operation in this mode has been performed, the main characteristics of the output pulse have been calculated, and the effect exerted by the characteristics of the setup elements on the pulse duration and intensity has been examined. It is shown that a minimum length of the output pulse is equal to the time required for double-passing the cavity. The peak intensity of the pulse nonlinearly decreases with the increased ratio of inactive loss within the cavity. This affords an opportunity to generate stable duration nanosecond pulses of the second harmonic, the peak intensity being increased with the pump power and decreased with increasing operation time of the electrooptic crystal. The pulse duration can be controlled by changing the polarizer transmittance, and also the electrooptic crystal response time that at best is about 1 ns. The method is implemented experimentally.

Author Biographies

Alexander S. Gorbatsevich, Belarusian State University, 4 Niezaliežnasci Avenue, Minsk 220030, Belarus

PhD (physics and mathematics); associate professor at the department of general physics, faculty of physics

Roza I. Navitskaya, Belarusian State University, 4 Niezaliežnasci Avenue, Minsk 220030, Belarus

student at the faculty of physics

Ihar V. Stashkevich, Belarusian State University, 4 Niezaliežnasci Avenue, Minsk 220030, Belarus

PhD (physics and mathematics), docent; associate professor at the department of laser physics and spectroscopy, faculty of physics

References

  1. Ma Y. F., Zhang J. W., Li H., et al. High stable electro-optical cavity-dumped Nd : YAG laser. Laser Phys. Lett. 2012. Vol. 9, No. 8. P. 561–563.
  2. Yu X., Wang C., Ma Y. F., et al. Performance improvement of high repetition rate electro-optical cavity-dumped Nd : GdVO4laser. Appl. Phys. B. 2012. Vol. 106, issue 2. P. 309–313. DOI: 10.1007/s00340-011-4786-7.
  3. Hitotsuya H., Shimojo N., Matsubara S., et al. High efficiency laser-diode-pumped cavity-dumped ytterbium-doped Y3Al5O12 laser. Int. J. Latest Res. Sci. Technol. 2013. Vol. 2, issue 1. P. 450–453.
  4. Kalisky Y. Y. The physics and engineering of solid state lasers. 2006.
  5. Khramov V. Y. [Calculation of elements of laser systems for information and technological complexes]. Saint Petersburg, 2008 (in Russ.).
  6. Stashkevich I. V., Karanouskaya Y. V. Temperature dependence generation of quasi-three-level Nd laser. Vestnik BGU. Ser. 1, Fiz. Mat. Inform. 2016. No. 1. P. 68–74 (in Russ.).
Published
2017-05-30
Keywords: neodymium laser, cavity dumping, second harmonic, electrooptic crystal, rate equations
How to Cite
Gorbatsevich, A. S., Navitskaya, R. I., & Stashkevich, I. V. (2017). Cavity dumping by the second harmonic generation. Journal of the Belarusian State University. Physics, 2, 57-62. Retrieved from https://journals.bsu.by/index.php/physics/article/view/440