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Chinese Science Bulletin

Multiphoton process and optical amplification in Er3+-Yb3+-doped fiber pumped by Ti:Al2O3 tunable laser at 980-nm band

Hai Ming, XiaoYan SUN, Y. Liu, Xiaopeng Dong, Bingchao Yang, Jin Xie, Yiqiao Zhang, Ying Geng, 董小鹏

Published Jan 1, 1995• 0 citations
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Simultaneous 853 nm + 1533 nm amplification and wavelength conversion between 1533 nm and 853 nm in Er3+-doped fluoride fiber

Guanshi Qin, Takenobu Suzuki, Yasutake Ohishi

In this paper, we investigate simultaneous 853 nm + 1533 nm amplification, and wavelength conversion between 1533 nm and 853 nm in Er3+-doped fluoride fiber. Based on our simulation results, simultaneous 853 nm (4S3/2→4I13/2 transition) + 1533 nm (4I13/2→4I15/2 transition) amplification, and wavelength conversion between 1533 nm and 853 nm can be realized in Er3+-doped fluoride fibers with the excitation of a 974 nm laser diode, respectively. Furthermore, we investigate the interactions between 853 nm and 1533 nm amplifications, and discuss their effects on simultaneously 853 nm + 1533 nm amplifier. The crosstalk between 853 nm and 1533 nm signals is very weak because of relatively long lifetime (~10 ms) of the 4I13/2 level. By introducing a cavity for 853 nm or 1533 nm lasing into the system, the possibility of wavelength conversion from 1533 nm to 853 nm or from 853 nm to 1533 nm in Er3+-doped fluoride fiber excited at 974 nm is clarified, which can be used as the wavelength converter or optical switch between public (the third window: ~1533 nm) and local (the first window: ~853 nm) networks in future networks.

Proceedings of SPIE, the International Society for Optical Engineering/Proceedings of SPIE•Jan 30, 2008•0 citations
In this paper, we propose a new pumping scheme—a dual-frequency laser-pumped cascade structure of Er3+-doped optical fiber based on the theory of coherent population oscillation. While realizing slow light transmission, the loss of output signal light power is reduced. Using numerical simulation, we compare the effects of a single fiber without pumping, a 980 nm single pumping single fiber, and a dual-frequency laser-pumped cascade structure of Er3+-doped optical fiber on signal light intensity loss coefficient τ and maximum time delay with the increase of input signal light power. The results show that the signal light intensity loss coefficient τ of the three structures decreases gradually with the increase of input signal light power. However, the transmission of lower signal light intensity loss coefficient τ=0.0823 and a larger time delay of 0.15 ms can be obtained under the dual-frequency laser-pumped cascade structure of Er3+-doped optical fiber. On the basis of the dual-frequency laser-pumped cascade structure of Er3+-doped optical fiber, the signal light intensity loss coefficient τ decreases gradually with the increase of pump ratio M (M=P1480∶P980) and the decrease of length ratio N (N=L2∶L1; L1 and L2 represent the length of the first and second cascaded optical fibers, respectively). Moreover, we compare the effects of ion density of the Er3+-doped optical fiber on the time delay of three structures. The dual-frequency laser-pumped cascade structure of Er3+-doped optical fiber can provide a larger time delay and smaller signal light intensity loss coefficient τ at low ion density of the Er3+-doped optical fiber.
In this paper, we investigate simultaneous 853 nm + 1533 nm amplification, and wavelength conversion between 1533 nm and 853 nm in Er3+-doped fluoride fiber. Based on our simulation results, simultaneous 853 nm (4S3/2→4I13/2 transition) + 1533 nm (4I13/2→4I15/2 transition) amplification, and wavelength conversion between 1533 nm and 853 nm can be realized in Er3+-doped fluoride fibers with the excitation of a 974 nm laser diode, respectively. Furthermore, we investigate the interactions between 853 nm and 1533 nm amplifications, and discuss their effects on simultaneously 853 nm + 1533 nm amplifier. The crosstalk between 853 nm and 1533 nm signals is very weak because of relatively long lifetime (~10 ms) of the 4I13/2 level. By introducing a cavity for 853 nm or 1533 nm lasing into the system, the possibility of wavelength conversion from 1533 nm to 853 nm or from 853 nm to 1533 nm in Er3+-doped fluoride fiber excited at 974 nm is clarified, which can be used as the wavelength converter or optical switch between public (the third window: ~1533 nm) and local (the first window: ~853 nm) networks in future networks.