• Title/Summary/Keyword: nonlinear loop mirror

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Passive Mode Locking of Figure '8' Type Erbium-doped Fiber Ring Laser Using Nonlinear Loop Mirror (비선형 Loop Mirror 방식을 이용한 '8'자 고리형 Erbium 광섬유 레이저의 수동형 모드 록킹)

  • 박희갑
    • Korean Journal of Optics and Photonics
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    • v.4 no.3
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    • pp.330-337
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    • 1993
  • Figure '8' type, passively-mode-locked erbium-doped-fiber ring laser was developed, incorporating a nonlinear loop mirror. Transmittance of the loop mirror was found to be dependent on the incident light intensity due to the non-reciprocal nonlinear phase shift, which enables the passive mode locking of the laser. Self-starting of stable mode locking was possible with only controlling the polarization controllers inside the cavity without any help of external perturbation or modulation. The mode-locked output pulse shape was discussed in relation with the transmission characteristics of nonlinear loop mirror.

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Solitin Pulse Generation with Mode-Locked Erbium-Doped Fiber Laser Using Nonlinear Amplifying Loop Mirror (Nonlinear Amplifying Loop Mirror를 사용하여 모우드 록킹된 Erbium 첨가 광섬유 레이저에서 발생하는 솔리톤 펄스)

  • 박희갑;임경아
    • Korean Journal of Optics and Photonics
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    • v.6 no.2
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    • pp.142-147
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    • 1995
  • Soliton pulse outputs are generated with figure '8' type erbium-doped fiber laser mode-locked by using a fiber loop mirror. The fiber loop mirror consists of an erbium-doped fiber amplifier at the one end of the loop, and 504 m-long dispersion-shifted fiber as a nonlinear medium. By pumping with a $1.48{\mu}m$ wavelength laser diode and adjusting the polarization controllers inside the loop, soliton pulses are generated with 1574 nm center wavelength and 1.2 nm linewidth. The soliton pulses are found randomly spaced within the fundamental period corresponding to cavity round trip time. The autocorrelation trace shows that the pulse width is 2.4 ps, which is in good agreement with the theoretical prediction. The pulsewidth- bandwidth product is found to be 0.348 which means that the pulses are nearly transform-limited.imited.

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New wavelength converter for optical NRZ data signal using SOA-loop-mirror (반도체 광 증폭기가 삽입된 광섬유 루프 미러를 이용한 NRZ 데이터에 대한 새로운 파장 변환기)

  • Lee, Hyuek-Jae
    • Korean Journal of Optics and Photonics
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    • v.16 no.1
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    • pp.27-33
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    • 2005
  • In this paper, a new wavelength converter using an SOA(Semiconductor Optical Amplifier)-loop-mirror for NRZ(NonReturn to Zero) optical data has been proposed and experimentally demonstrated. Conventional nonlinear fiber-loop-mirror methods can perform RZ-to-RZ, NRZ-to-RZ, and RZ-to-NRZ data format conversion, but NRZ-to-NRZ conversion has not been demonstrated until now. The experiment for the conversion from a 1300 nm NRZ data signal at 1.5 Gbps to a 1550 nm NRZ data one is successfully performed using a fiber-loop-mirror with 1300 nm-SOA.

Stability of average soliton propagation in a nonlinear amplifying loop mirror (비선형 증폭 루프에서의 평균 솔리톤의 안정성)

  • 심숙이;이성서;김광훈;김기옥
    • Korean Journal of Optics and Photonics
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    • v.12 no.6
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    • pp.507-510
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    • 2001
  • A numerical analysis based on the nonlinear Schroedinger equation is presented to analyze the propagation stability of the average soliton in a simple nonlinear amplifying loop mirror. The ratio of amplification period to soliton period and the length fraction of the erbium-doped fiber in the loop are varied to investigate their effects on the soliton stability. It is observed that stable soliton propagation is obtained even when the amplification period is only slightly shorter than the soliton period when the length fraction of the erbium-doped fiber in the loop is small, which is different from the previously published condition for stable average soliton propagation.

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Numerical Study of 40Gbit/s Optical Soliton Transmission System Using In-Line All-Optically Regenerative Repeater Constructed by Nonlinear Optical Loop Mirror

  • Kaewplung, Pasu;Thipchatchawanwong, Puttarak
    • Proceedings of the IEEK Conference
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    • 2002.07a
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    • pp.12-13
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    • 2002
  • The performance improvement of 40Gbit/s soliton transmission system employing nonlinear optical loop mirror (NOLM) as all-optical regenerative repeater is investigated. The switching characteristic of NOLM is optimized using our design strategies. By inserting the optical repeater where the eye-penalty of the transmitted signal becomes 1 ㏈, we achieve the improvement of 0.3㏈ eye-penalty resulting in further 480km transmission distance.

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Passive Mode Locking of Linear Cavity Fiber Laser with a Sagnac Loop (선형 공진기 구조 광섬유 레이저에서 Sagnac loop를 이용한 수동형 모우드록킹)

  • 박희갑;이경화;오왕열;이해웅;김병윤
    • Korean Journal of Optics and Photonics
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    • v.5 no.1
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    • pp.125-130
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    • 1994
  • A new cavity configuration for passive mode locking of fiber laser is proposed and demonstrated. It consists of a dichroic mirror at one end of the cavity, and a nonlinear loop mirror, which is a Sagnac loop, at the other end. The experimental observations are described for both Er-doped fiber laser and Nd-doped fiber laser. laser.

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Ultralow Intensity Noise Pulse Train from an All-fiber Nonlinear Amplifying Loop Mirror-based Femtosecond Laser

  • Dohyeon Kwon;Dohyun Kim
    • Current Optics and Photonics
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    • v.7 no.6
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    • pp.708-713
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    • 2023
  • A robust all-fiber nonlinear amplifying loop-mirror-based mode-locked femtosecond laser is demonstrated. Power-dependent nonlinear phase shift in a Sagnac loop enables stable and power-efficient mode-locking working as an artificial saturable absorber. The pump power is adjusted to achieve the lowest intensity noise for stable long-term operation. The minimum pump power for mode-locking is 180 mW, and the optimal pump power is 300 mW. The lowest integrated root-mean-square relative intensity noise of a free-running mode-locked laser is 0.009% [integration bandwidth: 1 Hz-10 MHz]. The long-term repetition-rate instability of a free-running mode-locked laser is 10-7 over 1,000 s averaging time. The repetition-rate phase noise scaled at 10-GHz carrier is -122 dBc/Hz at 10 kHz Fourier frequency. The demonstrated method can be applied as a seed source in high-precision real-time mid-infrared molecular spectroscopy.

Improvement of extinction ratio of amplified pulses by incorporating a nonlinear optical loop mirror (EDFA로 증폭된 고출력 펄스 신호의 소광비 향상)

  • Kim, Byung-Jun;Choi, Hyun-Beom;Lee, Han-Hyub;Lee, Dong-Han;Kim, Dae-Yun;Kwon, Il-Bum
    • Korean Journal of Optics and Photonics
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    • v.14 no.2
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    • pp.189-193
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    • 2003
  • A two-stage erbium-doped fiber amplifier (EDFA) with a band pass filter is used to get optical pulses of high peak value. The pulse signal has a 32 ㏈ extinction ratio, 125 W peak power and 79 ㎽ pulse off power. A nonlinear optical loop mirror (NOLM) is used to lower the pulse off power so as to increase the extinction ratio. The pulse signal after the NOLM has a 50.4 ㏈ extinction ratio, 35 W peak power and 0.3 ㎽ pulse off power.

Effects of Wavelength Dependent Birefringence inside a Fiber Cavity on the Fiber Laser Output Characteristics with a Nonlinear Amplifying Loop Mirror

  • Kim, Ho-Young;Kim, Kyong-Hon;Lee, El-Hang
    • Journal of the Optical Society of Korea
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    • v.2 no.2
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    • pp.64-73
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    • 1998
  • We have theoretically analyzed and experimentally observed the effects of wavelength dependent birefringence inside a laser cavity on the output characteristics of fiber lasers with a figure eight geometry. The spectral and polarization characteristics of fiber lasers are found to be very susceptible to the resultant birefringence composed of the intrinsically existing wavelength dependent birefringence and the externally induced birefringences inside the fiber. For the variation of twist-induced birefringence inside the nonlinear amplifying loop mirror, the laser output power and center wave-length of continuous wave lasers change periodically, but the polarization characteristics remains nearly unchanged. The changes of the birefringence inside the linear loop has little effect on the spectral characteristics but changes the polarization properties such as the polarization direction.

2.5 Gb/s transmission of a spectrum-sliced incoherent hight source with 0.92 nm bandwidth over 80 km of dispersion-shifted fiber

  • Shin, Sang-Yung;Han, Jung-Hee;Lee, Jae-Seung
    • Journal of the Optical Society of Korea
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    • v.2 no.1
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    • pp.22-25
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    • 1998
  • We present a spectrum broadening technique to improve the signal-to-noise ratio of spectrum sliced incoherent light sources using the fiber four-wave mixing effect which occurs in a nonlinear loop mirror located at the receiver. The initial transmission channel bandwidth of 0.92 nm was increased to 1.62 nm in the nonlinear loop mirror at the optical receiver, which enhances the signal-to-noise ratio to a desired value. Using this technique, we have demonstrated the transmission of a 2.5 Gb/s NRZ signal with the 0.92 nm bandwidth through a 80 km dispersion-shifted fiber. The measured transmission penalty was less than 0.2 dB at $1{\imes}10^{-10}$ BER.