• Title/Summary/Keyword: L-band erbium doped fiber amplifier

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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.

An Extended L-band Erbium-doped Fiber Amplifier to Amplify 1625 nm OTDR Signal for a Long Distance Monitoring System (장거리 광선로 감시용 1625 nm OTDR 신호 증폭을 위한 효율적인 Extended L-band Erbium-doped Fiber Amplifier)

  • Lee, Han-Hyub;Seo, Dae-Dong;Lee, Dong-Han;Choi, Hyun-Beom;Jeon, Jeon-Gu
    • Korean Journal of Optics and Photonics
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    • v.16 no.5
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    • pp.411-416
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    • 2005
  • We have designed an extended L-band Erbium-doped fiber amplifier to amplify 1625 nm optical time domain reflectometry signal for a long distance monitoring system. The proposed amplifier has a dual-stage structure without an isolator. Gain improvement of 5.1 dB has been achieved by adding a fiber Bragg grating and a narrow band pass filter. As a result, the 16.3 dB gain and 7.1 dB noise figure has been successfully accomplished.

Structure optimization of a L-band erbium-doped fiber amplifier for 64 optical signal channels of 50 GHz channel spacing (50 GHz 채널 간격의 64 채널 광신호 전송을 위한 L-band EDFA의 구조 최적화)

  • Choi, Bo-Hun
    • Journal of the Korea Institute of Information and Communication Engineering
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    • v.26 no.11
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    • pp.1666-1671
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    • 2022
  • The structure of a high-power gain-flattened long wavelength band (L-band) optical amplifier was optimized, which was implemented for 64-channel wavelength division multiplexed optical signals with a channel spacing of 50 GHz. The output characteristics of this L-band amplifier were measured and analyzed. The amplifier of the optimized two-stage amplification configuration had a flattened gain of 20 dB within 1 dB deviation between 1570 and 1600 nm for -2 dBm input power condition. The noise figure under this condition was minimized to within 6 dB in the amplification bandwidth. The gain flattening was realized by considering only the characteristics of gain medium in the amplifier without using additional optical or electrical devices. The proposed amplifier consisted of two stages of amplification stages, each of which was based on the erbium-doped fiber amplifier (EDFA) structure. The erbium-doped fiber length and pumping structures in each stage of the amplifier were optimized through experiments.

Design of Hybrid Optical Amplifiers for High Capacity Optical Transmission

  • Kim, Seung-Kwan;Chang, Sun-Hyok;Han, Jin-Soo;Chu, Moo-Jung
    • ETRI Journal
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    • v.24 no.2
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    • pp.81-96
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    • 2002
  • This paper describes our design of a hybrid amplifier composed of a distributed Raman amplifier and erbium-doped fiber amplifiers for C- and L-bands. We characterize the distributed Raman amplifier by numerical simulation based on the experimentally measured Raman gain coefficient of an ordinary single mode fiber transmission line. In single channel amplification, the crosstalk caused by double Rayleigh scattering was independent of signal input power and simply given as a function of the Raman gain. The double Rayleigh scattering induced power penalty was less than 0.1 dB after 1000 km if the on-off Raman gain was below 21 dB. For multiple channel amplification, using commercially available pump laser diodes and fiber components, we determined and optimized the conditions of three-wavelength Raman pumping for an amplification bandwidth of 32 nm for C-band and 34 nm for L-band. After analyzing the conventional erbium-doped fiber amplifier analysis in C-band, we estimated the performance of the hybrid amplifier for long haul optical transmission. Compared with erbium-doped fiber amplifiers, the optical signal-to-noise ratio was calculated to be higher by more than 3 dB in the optical link using the designed hybrid amplifier.

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Investigation of Pump Wavelength Dependence of Long-Wavelength-Band Erbium-Doped Fiber Amplifier using 1530nm-Band Pump (L 대역 EDFA 특성의 펌프 파장 의존성에 관한 연구)

  • Choi, Bo-Hun
    • Journal of the Korea Institute of Information and Communication Engineering
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    • v.12 no.7
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    • pp.1249-1255
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    • 2008
  • 1530nm band has been studied as pump wavelength for long-wavelength-band erbium-doped fiber amplifier (L-band EDFA). The pump source is built using a tunable light source and cascaded conventional-band (C-band) EDFA. The L-band EDFA uses a forward pumping scheme. Within the 1530nm band, 1545nm pump demonstrates 0.45dB/mW gain coefficient, which is twice better than that of conventional 1480nm pumped EDFA. The noise figure of 1530nm pump is at worst 6.36dB, which is 0.75dB higher than that of 1480nm pumped EDFA. Such high gain coefficient indicates that the L-band EDFA consumes low power.

Performances of Erbium-Doped Fiber Amplifier Using 1530nm-Band Pump for Long Wavelength Multichannel Amplification

  • Choi, Bo-Hun;Chu, Moo-Jung;Park, Hyo-Hoon;Lee, Jong-Hyun
    • ETRI Journal
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    • v.23 no.1
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    • pp.1-8
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    • 2001
  • The performance of a long wavelength-band erbium-doped fiber amplifier (L-band EDFA) using 1530nm-band pumping has been studied. A 1530nm-band pump source is built using a tunable light source and two C-band EDFAs in cascaded configuration, which is able to deliver a maximum output power of 23dBm. Gain coefficient and noise figure (NF) of the L-band EDFA are measured for pump wavelengths between 1530nm and 1560nm. The gain coefficient with a 1545nm pump is more than twice as large as with a 1480nm pump. It indicates that the L-band EDFA consumes low power. The noise figure of 1530nm pump is 6.36dB at worst, which is 0.75dB higher than that of 1480nm pumped EDFA. The optimum pump wavelength range to obtain high gain and low NF in the 1530nm band appears to be between 1530nm and 1540nm. Gain spectra as a function of a pump wavelength have bandwidth of more than 10nm so that a broadband pump source can be used as 1530nm-band pump. The L-band EDFA is also tested for WDM signals. Flat Gain bandwidth is 32nm from 1571.5 to 1603.5nm within 1dB excursion at input signal of -10dBm/ch. These results demonstrate that 1530nm-band pump can be used as a new efficient pump source for L-band EDFAs.

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A compensation method for a temperature-dependent gain tilt in L-band EDFA using a voltage-controlled attenuator (L-band EDFA 에서의 온도에 따른 이득 변화와 가변 감쇄기를 이용한 온도 보상)

  • 이원경;정희상;주무정
    • Korean Journal of Optics and Photonics
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    • v.14 no.1
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    • pp.12-16
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    • 2003
  • This paper presents a compensation method for a temperature-dependent gain tilt in L-band erbium-doped fiber amplifier using a voltage-controlled attenuator. The gain tilts in the L-band of 1570-1605 nm due to a temperature change have negative slopes, whereas they have positive slopes for the increasing optical input powers in a saturation region. The proposed method utilizes these opposite gain variations to compensate for the gain tilt over a wide range of temperature. While applying forty channels with a channel spacing of 100 GHz in the L-band and changing the ambient temperature from 0 to $50^{\circ}C$, the compensation method maintained the gain deviation within 1 dB.

Simulation and Experimental Validation of Gain-Control Parallel Hybrid Fiber Amplifier

  • Ali, Mudhafar Hussein;Abdullah, Fairuz;Jamaludin, Md. Zaini;Al-Mansoori, Mohammed Hayder;Al-Mashhadani, Thamer Fahad;Abass, Abdulla Khudiar
    • Journal of the Optical Society of Korea
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    • v.18 no.6
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    • pp.657-662
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    • 2014
  • We demonstrate a simulation of a parallel hybrid fiber amplifier in the C+L-band with a gain controlling technique. A variable optical coupler is used to control the input signal power for both EDFA and RFA branches. The gain spectra of the C+L-band are flattened by optimizing the coupling ratio of the input signal power. In order to enhance the pump conversion efficiency, the EDFA branch was pumped by the residual Raman pump power. A gain bandwidth of 60 nm from 1530 nm to 1590 nm is obtained with large input signal power less than -5 dBm. The gain variation is about 1.06 dB at a small input signal power of -30 dBm, and it is reduced to 0.77 dB at the large input signal power of -5 dBm. The experimental results show close agreement with the simulation results.

320km Optical Transmission using EDFA and Raman amplifier for 10Gbit/s 128 Channel DWDM Signals (10 Gbit/s 128 채널 고밀도 파장다중화 신호를 위해 EDFA와 라만 증폭기를 이용한 320km 광전송 실험)

  • Choi, Bo-Hun
    • The Journal of Korean Institute of Communications and Information Sciences
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    • v.34 no.6B
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    • pp.568-574
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    • 2009
  • 320km optical transmission link for 128 channel DWDM (dense wavelength-division-multiplexing) signals is simulated and fabricated. An optical fiber amplifier for the link is composed of a distributed Raman amplifier and dual C/L-band EDFAs which are optimized for the performances of an optical amplifier obtained from the simulation. Gain and NF of the optimized EDFAs are above 19dB and below 7.5dB, respectively. The resultant OSNRs (optical signal to noise ratios) of the link are average 25dB on each band.

1.6 Tb/s (160x10 Gb/s) WDM Transmission over 2,000 km of Single Mode Fiber (1.6 Tb/s (160x10 Gb/s) WDM 신호의 단일 모드 광섬유 2,000 km 전송)

  • 한진수;장순혁;이현재
    • The Journal of Korean Institute of Communications and Information Sciences
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    • v.29 no.7A
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    • pp.712-718
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    • 2004
  • We report 1.6 Tb/s (160${\times}$10 Gb/s) WDM transmission over 2,000 km of single mode fiber using distributed hybrid(distributed Raman amplifier+Erbium-doped fiber amplifier) optical amplifiers. After transmission over 2,000 km of single mode fiber, average optical signal to noise ratios of C/L-band were 20.5 dB, 21.9 dB, respectively. The minimum Q-factors of each band were 14.65 dB (BER=5.8e-8) in C-band, 13.75 dB (BER=5.0e-7) in L-band without forward error correction. We performed 1.6 Tb/s error-free transmission over 2,000 km of single mode fiber using Reed-Solomon (255, 239) forward error correction code.