• 제목/요약/키워드: Erbium-Doped Fiber

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50 cm of Zirconia, Bismuth and Silica Erbium-doped Fibers for Double-pass Amplification with a Broadband Mirror

  • Markom, Arni Munira;Muhammad, Ahmad Razif;Paul, Mukul Chandra;Harun, Sulaiman Wadi
    • Current Optics and Photonics
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    • v.6 no.1
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    • pp.32-38
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    • 2022
  • Erbium-doped fiber amplifiers (EDFAs) have saturated the technological market but are still widely used in high-speed and long-distance communication systems. To overcome EDFA saturation and limitations, its erbium-doped fiber is co-doped with other materials such as zirconia and bismuth. This article demonstrates and compares the performance using three different fibers as the gain medium for zirconia-erbium-doped fibers (Zr-EDF), bismuth-erbium-doped fibers (Bi-EDF), and commercial silica-erbium-doped fibers (Si- EDF). The optical amplifier was configured with a double-pass amplification system, with a broadband mirror at the end of its configuration to allow double-pass operation in the system. The important parameters in amplifiers such as optical properties, optical amplification and noise values were also examined and discussed. All three fibers were 0.5 m long and entered with different input signals: 30 dBm for low input and 10 dBm for high input. Zr-EDF turned out to be the most relevant optical amplifier as it had the highest optical gain, longest transmission distance, highest average flatness gain with minimal jitter, and relevant noise figures suitable for the latest communication technology.

Investigation of Amplifying Mechanism in an t-Band Erbium-Doped Fiber Amplifier Pumped by a 980 nm Pump

  • Lee, Dong-Han;Lee, Han-Hyub;Oh, Jung-Mi;Kim, Byung-Jun
    • Journal of the Optical Society of Korea
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    • v.7 no.2
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    • pp.67-71
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    • 2003
  • For a more detailed understanding of the mechanism of an L-band erbium-doped fiber amplifier, we investigated 980 nm absorption, signal amplification and forward and backward amplified spontaneous emission along the erbium-doped fiber. In addition, we compared performances of the erbium-doped fiber amplifier with and without a fiber Bragg grating.

Polarization-controlled Interleaved Signal Gating Fiber Device (편광으로 조절되는 인터리빙 신호 게이팅 광섬유 소자)

  • Lee, Yong-Wook
    • The Transactions of The Korean Institute of Electrical Engineers
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    • v.56 no.10
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    • pp.1820-1822
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    • 2007
  • In this paper we fabricated a fiber device composed of cascaded long-period fiber gratings between which a birefringent erbium-doped fiber was inserted and proposed its application as a polarization-controlled interleaved signal gating fiber device. Because the core and cladding modes of the fabricated fiber device have polarization-dependent phase difference due to the birefringence of the erbium-doped fiber, its interference spectrum can be modulated by varying the input polarization.

Regenerative Erbium-Doped Fiber Ring Amplifier with Unidirectional and Bi-directional Feedbacks

  • Shah, N.S.Mohd.;Teyo, T.C.;Poopalan, P.;Ahmad, H.
    • Proceedings of the IEEK Conference
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    • 2002.07a
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    • pp.540-541
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    • 2002
  • In this paper, the performance of upidirectional and hi-directional regenerative erbium-doped fiber amplifier (EDFA) is compared. The systems are operating above laser oscillation threshold. The experimental results show that the unidirectional regenerative EDFA has a better performance than the hi-directional.

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Wideband Gain Flattened Hybrid Erbium-doped Fiber Amplifier/Fiber Raman Amplifier

  • Afkhami, Hossein;Mowla, Alireza;Granpayeh, Nosrat;Hormozi, Azadeh Rastegari
    • Journal of the Optical Society of Korea
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    • v.14 no.4
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    • pp.342-350
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    • 2010
  • An optimal wideband gain flattened hybrid erbium-doped fiber amplifier/fiber Raman amplifier (EDFA/FRA) has been introduced. A new and effective optimization method called particle swarm optimization (PSO) is employed to find the optimized parameters of the EDFA/FRA. Numerous parameters which are the parameters of the erbium-doped fiber amplifier (EDFA) and the fiber Raman amplifier (FRA) define the gain spectrum of a hybrid EDFA/FRA. Here, we optimize the length, $Er^{3+}$ concentration, and pump power and wavelength of the EDFA and also pump powers and wavelengths of the FRA to obtain the flattest operating gain spectrum. Hybrid EDFA/FRA with 6-pumped- and 10-pumped-FRAs have been studied. Gain spectrum variations are 1.392 and 1.043 dB for the 6-pumped- and 10-pumped-FRAs, respectively, in the 108.5 km hybrid EDFA/FRAs, with 1 mW of input signal powers. Dense wavelength division multiplexing (DWDM) system with 60 signal channels in the wavelength range of 1529.2-1627.1 nm, i.e. the wide bandwidth of 98 nm, is studied. In this work, we have added FRA's pump wavelengths to the optimization parameters to obtain better results in comparison with the results presented in our previous works.

Sensitivity improvement of fiber-optic gyroscope with erbium-doped fiber source by source excess noise subtraction (Erbium 첨가 광섬유 광원을 사용하는 자이로스코프에서 광원 과잉잡음 소거에 의한 측정감도 개선)

  • 진영준
    • Proceedings of the Optical Society of Korea Conference
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    • 1999.08a
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    • pp.226-227
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    • 1999
  • In the fiber-optic gyroscope employing the erbium-doped fiber source, the source excess noise was subtracted through a signal processing to improve the gyroscope sensitivity . As the result, we obtained the improvement of 14 dB(electrical) at the proper frequency, which was measured from the noise floor spectrum . In addition the random walk coefficient in the gyro output was reduced by about factor of three.

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All-optical gain control in erbium-doped fiber amplifier using a fiber grating (광섬유격자를 이용한 Erbium 첨가 광섬유 증폭기의 광학적 이득제어)

  • 박희갑
    • Korean Journal of Optics and Photonics
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    • v.8 no.1
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    • pp.58-62
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    • 1997
  • A new, simple lasing loop configuration employing a fiber grating was proposed and demonstrated for all-optical gain control of erbium-doped fiber amplifier. The lasing loop was designed such that the fiber grating acts as a notch filter to cutoff the lasing light as well as selects the lasing wavelength. The operating gain was clamped to the same level as the loop loss and it could be varied with a tunable directional coupler in the loop. It is believed that this type of gain-controlled erbiumdoped fiber amplifier can have several advantages when used in wavelength-division-multiplexed transmission systems.

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Multiple Brillouin Stokes Generation Utilizing a Linear Cavity Erbium-Doped Fiber Laser

  • AL-Mansoori, Mohammed Haydar;Noordin, Nor Kamariah;Saripan, M. Iqbal;Mahdi, Mohd Adzir
    • Journal of Communications and Networks
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    • v.10 no.1
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    • pp.1-4
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    • 2008
  • This paper reports the design of a multiwavelength fiber laser source that utilizes a linear cavity of hybrid Brillouin/Erbium fiber laser (BEFL). The output power, threshold power and free running cavity modes were investigated against the pump powers. The structure exhibited low threshold operation of 4 mW at 2.3 mW injected Brillouin pump power. The optimization of Brillouin pump wavelength, power and Erbium gain led to a maximum possible number of channels generated. Simultaneous and stable operation of 21 channels with 10.88 GHz channels spacing were obtained from this architecture at 1 mW injected Brillouin pump power and 90 m W Erbium doped fiber pump power in the 1555 nm region.

Tunable Channel Spacing of Dual-wavelength Erbium-doped Fiber Ring Laser using a Single Fiber Bragg Grating with Two Coil Heaters

  • Sohn, Kyung-Rak;Kim, Hyung-Pyo
    • Journal of Advanced Marine Engineering and Technology
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    • v.33 no.1
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    • pp.153-158
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    • 2009
  • Stable and tunable dual-wavelength erbium-doped fiber ring laser(EDFL) using a single fiber Bragg grating(FBG) and two coil heaters is proposed and demonstrated. Installing two identical coils into a single FBG, the FBG is symmetrically divided into two different portions. While a current supply to the coil, the refractive index of the FBG under the coil is changed. The FBG can operate as a joint of two different FBGs. Due to the thermo-optic effect of a fiber, the resonance wavelength split into two peaks. The spacing between two adjacent channels was changed as much as the difference of heating power. It was tuned up to 3 nm of wavelength under the electrical power with a 1000 mW. Moreover, the lasing wavelength can be individually tuned without influencing to the adjacent channel.