Observation of Raman Gain in Reduced Length of Bismuth Erbium Doped Fiber
محورهای موضوعی : فصلنامه نانوساختارهای اپتوالکترونیکیشریفه شاهی 1 , PARVANE MARNANI 2 , mohsen ranjbaran 3 , sulaiman harun 4
1 - Laser and Biophotonics in Biotechnologies Research Center, Isfahan (Khorasgan) Branch, Islamic Azad University, Isfahan, Iran
2 - Laser and Biophotonics in Biotechnologies Research Center, Isfahan (Khorasgan) Branch, Islamic Azad University, Isfahan, Iran
3 - Laser and Biophotonics in Biotechnologies Research Center, Isfahan (Khorasgan) Branch, Islamic Azad University, Isfahan, Iran
4 - Department of Electrical Engineering, Faculty of Engineering, University of Malaya, 50630 Kuala lumpur, Malaysia
کلید واژه: Bi-EDF, Compact gain medium, C-band, Dual wavelength source, Raman gain,
چکیده مقاله :
Raman amplification of a 49 cm Bismuth oxide (Bi2O3) as a nonlinear gain
medium based erbium doped fiber amplifier (EDFA) is reported in new and compact
design in near infrared spectral regions. The bismuth glass host provides the
opportunity to be doped heavily with erbium ions to allow a compact optical gain fiber
amplifier design by using reduced fiber length and the 1480 nm low pump power
around 150 mW. A extended Raman amplification bandwidth of 45 nm, from 1520-
1565 nm (C-band window) wavelengths is empirically proposed in a backward and
dualwavelength pumped Bi-EDF by employing 350 mW Raman pump in 1440 nm.
Because of the short length gain medium as a nonlinear Bi-EDF, amplification of 3 dB
is achieved over a C-band wavelength range. This simple C-band Raman amplifier
based Brillouin and ASE backscattering was constructed to test the forward, backward
and dual-wavelength pump laser and on-off gain. A peak gain of 1.53 dB was obtained
with a 3-dB bandwidth of 45 nm that the varieties of gain is 2.02 dB around 1545 nm in
backward pumping design. It array will be employ for sensing, spectroscopy and
telecommunication systems.
[1] S. Aozasa, T. Sakamoto, H. Ono, A. Mori, M. Yamada, Wideband Rare-earth-doped Fiber Amplification Tech-nologies—O-band and S-band Amplification Technologies transition, (2004),1(3F4), 3F3.
[2] Y. S. Seo, Y. Fujimoto, and M. Nakatsuka. Optical Amplification in Bi-doped Silica Fiber. Journal of the American Ceramic Society 266(1) (2006) 169-171.
[3] N.Tamchek, Characterisation of bismuth-based erbium-doped fibre and its application in wide-band optical amplifiers. Diss. University Malaya, (2009).
[4] A. Markom, M. C. Paul, A. Dhar, S. Das, M. Pal, S.K. Bhadra, et al.Performance comparison of enhanced Erbium–Zirconia–Yttria–Aluminum co-doped conventional erbium-doped fiber amplifiers. Optik-Int J Light Electron Opt, 132 (2017), 75-79.
[5] Y. Kuroiwa. Fusion Spliceable and High Efficient Bi2O3-based EDF for Short-length and Broadband Application Pumped at 1480 nm. Presented at Optical Fiber Communication Conference. Optical Society of America. (2001).
[6] N. Sugimoto, Ultrafast optical switches and wavelength division multiplexing (WDM) amplifiers based on bismuth oxide glasses. Journal of the American Ceramic Society. 85 (5) (2002 ,may) 1083-1088.
[7] T. Kenji. Dispersion and pulse amplification characteristics of Bismuth oxide-based Erbium doped fiber amplifiers. Optcal Amplifiers and their Applications. (2002) 1-3.
[8] A. Al-Azzawi, A. Almukhtar, P. H.Reddy D. Dutta, H. Ahmad and S.W. Harun, Compact and flat-gain fiber optical amplifier with Hafnia-Bismuth-Erbium co-doped fibe. Optik. (170) (2018, October) 56-60.
[9] F. Mohammadi, S. Shahi, M. Haffaatifar, M. Kanani and H. Normohammadi, Novelty Design in Gain Flattening Filter of ASE Source Based on Fat Ultra-Long Period Fiber Grating, Photonic Sensors. 6 (2016)243–248.
[10] L. Sirleto, and M. Antonietta Ferrara. Fiber Amplifiers and Fiber Lasers Based on Stimulated Raman Scattering: A Review. Micromachines.11(3) (2020, February) 247.
80 * Journal of Optoelectronical Nanostructures Summer 2020 / Vol. 5, No. 3
[11] M. R. Shirazi, and M. Biglary. Multiple wavelength generation using a compacted hybrid Raman / Bi-EDF amplifier. Published by EDP Sciences. (48) (2013, May) 00022.
[12] S. W. Harun, N. Tamchek, S. Shahi, and H. Ahmad. L-band amplification and multi-wavelength lasing with bismuth-based erbium doped fiber. Progress In Electromagnetics Research. 6 (2009) 1-12
[13] D. A. Chestnut, C. J. S. De Matos, P. C. Reeves-Hall, and J. R. Taylor. High efficiency, dual-wavelength fibre Raman pump laser for U-band fibre Raman amplifiers. Optical and quantum electronics. 34 (10) (2002, October) 1025-1030.
[14] G. P. Agrawal. Non-linear Fibre Optics Academic Press INC. (1989).
[15] G.Felinskyi and M.Y.Dyrin. Noise gain features of fiber Raman amplifier. Advances in OptoElectronics. (2016, Jun) 7.
[16] Q. MENG, H. WU, B. HAN, J. LI AND Z. WANG. LD-PUMPED RANDOM FIBER LASER BASED ON ERBIUM-YTTERBIUM CO-DOPED FIBER. PHOTONIC SENSORS , 10 (2020) 181–185.
[17] Y. Dong, P. Xu, H. Zhang ,Z. Lu, L. Chen, and X. Bao. Characterization of evolution of mode coupling in a graded-index polymer optical fiber by using Brillouin optical time-domain analysis. Optics express, 22 (22) (2014) 26510-26516.
[18] A. Schreier, S. Liehr, A. Wosniok., and K. Krebber. Investigation on the influence of humidity on stimulated Brillouin backscattering in perfluorinated polymer optical fibers. Sensors. 18 (11) (2018, November) 3952.
[19] S. Darwish, A.Samra and M. Aly. ASE noise in Raman amplifiers pump depletion impact. Radio engineering. 27(1) (2018) 22-28.
[20] Mohammad Reza Mohebbifar, Mehdi Zohrabi. Influence of Grating Parameters on the Field Enhancement of an Optical Antenna under Laser Irradiation. Journal of Optoelectronical Nanostructures.4 (4) (2019).
[21] A. Ghadimi, and M. Ahmadzadeh, Effect of variation of specification o quantum well and contact length on performance of InP-based Vertical Cavity Surface Emitting Laser (VCSEL), Journal of Optoelectronical Nanostructures,5(1),(2020.),19- 34.
[22] M. Riahinasab, and E. Darabi, Analytical Investigation of Frequency Behavior in Tunnel Injection Quantum Dot VCSEL, Journal of Optoelectronical Nanostructures, 3(2), (2020.), 65-86.