Semiconductor Optical Amplifier (SOA)-Fiber Ring Laser and Its Application to Stress Sensing
Yoshitaka Takahashi, Shinji Sekiya, Tatsuro Suemune
.
DOI: 10.4236/opj.2011.14027   PDF    HTML     6,747 Downloads   12,701 Views   Citations

Abstract

We have developed a novel optical fiber ring laser using a semiconductor optical amplifier (SOA) as the gain medium, and taking advantage of polarization anisotropy of its gain. The frequency difference of the bi-directional laser is controlled by birefringence which is introduced in the ring laser cavity. The beat frequency generated by combining two counter-propagating oscillations is proportional to the birefringence, the fiber ring laser of the present study is, therefore, applicable to the fiber sensor. The sensing signal is obtained in a frequency domain with the material which causes the retardation change by a physical phenomenon to be measured. For the application to stress sensing, the present laser was investigated with a photoelastic material.

Share and Cite:

Y. Takahashi, S. Sekiya and T. Suemune, "Semiconductor Optical Amplifier (SOA)-Fiber Ring Laser and Its Application to Stress Sensing," Optics and Photonics Journal, Vol. 1 No. 4, 2011, pp. 167-171. doi: 10.4236/opj.2011.14027.

Conflicts of Interest

The authors declare no conflicts of interest.

References

[1] Y. Takahashi, S. Sekiya and N. Iwai, “Semiconductor Optical Amplifier(SOA)-Fiber Ring Laser for Sensor Application,” Optical Review, Vol. 10, No. 4, 2003, pp. 315-317. doi:10.1007/s10043-003-0315-1
[2] Y. Takahashi, H. Kuroda and T. Suemune, “Semiconductor Optical Amplifier-Fiber Laser and Its Application for Temperature Sensing,” The Review of Laser Engineering, Vol. 33, No. 5, 2005, pp. 329-332.
[3] T. Suemune and Y. Takahashi, “SOA-fiber ring laser and its application to electric field sensing in frequency domain,” Optics and Lasers in Engineering, Vol. 45, No. 7, 2007, pp. 789-794. doi:10.1016/j.optlaseng.2006.12.002
[4] R. K. Kadiwar and I. P. Giles, “Optical Fibre Brillouin Ring Laser Gyroscope,” Electronics Letters, Vol. 25, No. 25, 1989, pp. 1729-1731. doi:10.1049/el:19891157
[5] S. K. Kim, H. K. Kim and B. Y. Kim, “Er3+-Doped Fiber Ring Laser for Gyroscope Applications,” Optical Letters, Vol. 19, No. 22, 1994, pp. 1810-1812. doi:10.1364/OL.19.001810
[6] A. Kung, P.-A. Nicati and P. A. Robert, “Reciprocal and Quasi-Reciprocal Brillouin Fiber-Optic Current Sensors,” IEEE Photonics Technology Letters, Vol. 8, No. 12, 1996, pp. 1680-1682. doi:10.1109/68.544717
[7] Y. Takahashi and T. Yoshino, “Fiber Ring Laser with Flint Glass Fiber and Its Sensor Applications,” Journal of Lightwave Technology, Vol. 17, No. 4, 1999, pp. 591-597. doi:10.1109/50.754788
[8] D. E. Gray, “American Institute of Physics Handbook,” 3rd Edition, McGraw-Hill, New York, 1972, pp. 233-236.

Copyright © 2024 by authors and Scientific Research Publishing Inc.

Creative Commons License

This work and the related PDF file are licensed under a Creative Commons Attribution 4.0 International License.