• 제목/요약/키워드: Optical Pulses

검색결과 262건 처리시간 0.025초

반도체 광증폭기 루프 거울을 포함한 8자형 레이저를 이용한 10Gb/s RZ 신호의 전광 클럭 추출 (All optical clock recovery from 10 Gb/s RZ signal using an actively mode-locked figure eight laser incorporating a SLALOM)

  • 정희상;주무정;김광준;이종현
    • 한국광학회지
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    • 제11권6호
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    • pp.400-404
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    • 2000
  • 능동 모드 잠김 8자형 레이저를 이용하여 10Gb/s RZ 신호로부터 클럭을 추출하고 이 클럭 성분의 품질을 평가하였다. 10ps의 펄스폭을 갖는 광원을 $2^{23}-1$ PRBS로 외부 변조하였으며 이를 클럭 추출회로에 인가함으로써 12ps의 펄스폭을 갖는 클럭을 얻었다. 이렇게 얻어진 펄스를 다시 같은 외부 변조기에 입력하여 BER을 측정한 결과 $10_{11}$의 BER에서 패널티가 거의 나타나지 않았다.

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Wideband Flat Optical Frequency Comb Generated from a Semiconductor Based 10 GHz Mode-Locked Laser with Intra-cavity Fabry-Perot Etalon

  • Leaird, Daniel E.;Weiner, Andrew M.;Seo, Dongsun
    • 전기전자학회논문지
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    • 제18권1호
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    • pp.19-24
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    • 2014
  • We report stable, wideband, flat-topped, 10 GHz optical frequency comb generation from a semiconductor-based mode-locked ring laser with an intra-cavity high finesse Fabry-Perot etalon. We demonstrate a stable 10 GHz comb with greater than 200 lines within a spectral power variation below 1 dB, which is the largest value obtained from a similar mode-locked laser in our knowledge. Greater than 20 dB of the spectral peak to deep ratio at 0.02 nm resolution, ~92 femtosecond timing jitter over 1 kHz to 1 MHz range, and non-averaged time traces of pulses confirm very stable optical frequency comb lines.

Structural Analysis of a Cavitary Region Created by Femtosecond Laser Process

  • Fujii, Takaaki;Goya, Kenji;Watanabe, Kazuhiro
    • 동력기계공학회지
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    • 제19권3호
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    • pp.5-10
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    • 2015
  • Femtosecond laser machining has been applied for creating a sensor function in silica glass optical fibers. Femtosecond laser pulses make it possible to fabricate micro structures in processed regions of a very thin glass fiber line because femtosecond laser pulses can extremely minimize thermal effects. With the laser machining to optical fiber using a single shot of 210-fs laser at a wavelength of 800 nm, it was observed that a processed region surrounded a thin layer which seemed to be a hollow cavity monitored by scanning electron microscopy (SEM). This study aims at a theoretical investigation for the processed region by using a numerical analysis in order to embed sensing function to optical fibers. Numerical methods based finite element method (FEM) has been used for an optical waveguide modeling. This report suggests two types modeling and describes a comparative study on optical losses obtained by the experiment and the numerical analysis.

광전궤환을 이용한 짧은 광펄스 생성 (Generation of Optical Short Pulses with Optoelectronic Feedback)

  • 이창희;조건호;이성호;신상영
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 1988년도 전기.전자공학 학술대회 논문집
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    • pp.477-479
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    • 1988
  • A new method of optical short pulse generation using stable diode lasers with negative optoelectronic feedback is demonstrated experimentally. About 1 nanosecond pulses with 300 MHz repetition rate are generated.

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Wavelength-Tunable, Passively Mode-Locked Erbium-Doped Fiber Master-Oscillator Incorporating a Semiconductor Saturable Absorber Mirror

  • Vazquez-Zuniga, Luis A.;Jeong, Yoonchan
    • Journal of the Optical Society of Korea
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    • 제17권2호
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    • pp.117-129
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    • 2013
  • We briefly review the recent progress in passively mode-locked fiber lasers (PMLFLs) based on semiconductor saturable absorber mirrors (SESAMs) and discuss the detailed characterization of a SESAM-based, passively mode-locked erbium-doped fiber (EDF) laser operating in the 1.5-${\mu}m$ spectral range for various configurations. A simple and compact design of the laser cavity enables the PMLFL to generate either femtosecond or wavelength-tunable picosecond pulses with high stability as the intra-cavity filtering method is altered. All the cavities investigated in our experiments present self-starting, continuous-wave mode-locking with no Q-switching instabilities. The excellent stability of the source eventually enables the wavelength-tunable PMLFL to be used as a master oscillator for a power-amplifier source based on a large-core EDF, generating picosecond pulses of >10-kW peak power and >100-nJ pulse energy.