• Title/Summary/Keyword: fabry-perot

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Optical frequency domain reflectometry based on Wavelength swept mode locked fiber laser (Wavelength Swept 모드 록킹된 광섬유 레이저를 이용한 광주파수 영역에서 반사계)

  • 오명숙;박희수;김병윤
    • Proceedings of the Optical Society of Korea Conference
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    • 2003.07a
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    • pp.204-205
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    • 2003
  • We demonstrate a novel OFDR system with compactness and short measurement time based on the use of a wavelength-swept mode-locked fiber laser. The optical source uses an intra-cavity tunable Fabry-Perot filter as a tuning element. The fiber laser sweeps 20 nm in less than 10 ms. Spatial resolution of 100 fm and total measurement range of several centimeters are demonstrate

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A Low Noise Broadband Light Source and its Application on WDM-PON (저잡음 특성의 광대역 비간섭성 광원과 파장 분할 다중방식 수동형 광가입자망에의 응용)

  • Choi Ki-Man;Moon Jung-Hyung;Lee Chang-Hee
    • Journal of the Institute of Electronics Engineers of Korea TC
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    • v.43 no.5 s.347
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    • pp.68-76
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    • 2006
  • We propose a low noise broadband light source (BLS) and investigate a cost-effective wavelength division multiplexing-passive optical network (WDM-PON) for the convergence of broadcasting and data service. The proposed BLS is used for an injection light of wavelength-locked Fabry-Perot laser diodes (F-P LD) and helps the color-free operation of dense WDM-PON (DWDM-PON). In addition, we apply this BLS to a optical source for overlay of digital broadcasting channel on the WDM-PON.

Implementation of the Wavelength-Swept-Source and Signal Processing for the Frequency Domain Optical Coherence Tomography (주파수영역 광 간섭 단층촬영 시스템을 위한 파장가변 광원 및 신호처리계의 구현)

  • Lee, Eung-Je;Kim, Yong-Pyung
    • Korean Journal of Optics and Photonics
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    • v.18 no.5
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    • pp.309-316
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    • 2007
  • We demonstrate the wavelength swept source and signal processing for the frequency domain optical coherence tomography. The laser output performance is improved by using a semiconductor optical amplifier with a booster amplifier. The laser generates 14 mW of average power of which wavelength shift in the lasing spectral shape is compensated. Adopting a Fabry-Perot etalon and digital signal processing, the broadening of the beat frequency due to the variance of wavelength-sweep-velocity is calibrated. The optical coherence tomography system shows 154.4 kHz of axial scanning speed, 0.95mm of depth range, and $12{\pm}0.37{\mu}m$ of axial resolution.

Fabrication and Measurement of Optical Waveguide using Multi Quantum Well Intermixing (다중양자우물구조의 상호섞임을 이용한 광도파로의 제작 및 측정)

  • Yeo, Deok-Ho;Yoon, Kyung-Hun;Kim, Sung-June
    • Journal of the Korean Institute of Telematics and Electronics D
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    • v.36D no.7
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    • pp.50-55
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    • 1999
  • We have fabricated optical waveguide which utilizes intermixing of InGaAs/InGaAsP multi quantum well separate confinement heterostructure. The waveguide was fabricated by reactive ion etching technique using $CH_4/H_2$ gas mixture, and the width and depth of the waveguide ware $5{\mu}m$ and $1.2{\mu}m$, respectively. The propagation loss of the waveguide was measured by Fabry-Perot interference phenomena using tunable laser. For the waveguide after $800^{\circ}C$, 30s heat treatment, the measured loss was 3.76dB/cm and 3.95dB/cm for TE and TM mode, respectively. This value is very small compared to other waveguide made by IFVD technique. Hence, this technique can applied to integration of waveguide and electronic devices.

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Chaos Characteristics of Laser Diodes with External Optical Feedback (외부 광귀환이 있는 레이저 다이오드의 혼돈특성)

  • 양동석;한영진;김창민
    • Korean Journal of Optics and Photonics
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    • v.5 no.3
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    • pp.394-403
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    • 1994
  • Chaos characteristics of laser diodes with external optical feedback is investigated. For a FabryPerot resonator laser, optical feedback by external mirror is assumed. The simulation is performed in such a way that a current of $1.3J_{th}$ is injected into the $1.3{\mu}m$wavelength "InGaAsP" buried hetero structure laser. With the increment of K, the system shows the evolution of four steps as follows: i) When the optical feedback coefficient K is very small, the relaxation oscillation is damped and the system reaches the steady state showing the stable operation characteristics. ii) As K increases a little bit, the relaxation oscillation is not damped any more and the system begins to maintain the periodic oscillation. iii) When K is increased further, the oscillation shows the larger amplitude and the long periodic length. iv) When K is increased very large, the system gets unstable and enters into the coherejlce collapse state. state.

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Resonance Fiber Bragg Grating Sensor system based on Fourier Domain Mode-locking Laser (분광 영역 모드록킹 레이저를 이용한 공진형 광섬유 격자 센서)

  • Choi, Byeong Kwon;Jeon, Min Yong
    • Korean Journal of Optics and Photonics
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    • v.23 no.5
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    • pp.211-216
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    • 2012
  • We report a resonance fiber Bragg sensor interrogation based on a Fourier domain mode-locking (FDML) laser. The FDML laser is constructed based on a conventional ring laser cavity configuration with fiber Fabry-Perot tunable filter (FFP-TF). There are two sensor parts which are composed with two FBGs inside the laser cavity. Each sensor part provides a separate laser cavity for the FDML laser. The resonance frequencies of the laser cavities are 46.687 kHz and 44.340 kHz, respectively. We applied a static and a dynamic strain on the FBG sensor system. The slope coefficients of the measured relative wavelength shift and relative time interval from the static strain are found to be $0.61pm/{\mu}{\epsilon}$ and $0.8ns/{\mu}{\epsilon}$, respectively.

Effect of spectral drift to coherent optical fiber sensor (가간섭성 광섬유 센서에 대한 주파수 천이도의 영향)

  • Choi, Kyoo-Nam
    • The Journal of the Korea institute of electronic communication sciences
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    • v.11 no.3
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    • pp.277-282
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    • 2016
  • Effect of spectral drift in coherent fiber laser was investigated by injecting optical feedback to Fabry-Perot resonance loop. Er+3 doped fiber laser having unilateral optical feedback loop in Fabry-Perot configuration using two FBGs was fabricated. The optical feedback was found to be effective in linewidth reduction of fiber laser compared to the case without any optical feedback. The linewidth of three fiber lasers using above configuration were measured to be within 3kHz which is resolution-limited performance of self-heterodyne linewidth measurement set-up. The frequency drift measurement using Mach-Zehnder measurement set-up having 200m optical delay-line in one arm showed that the frequency drift rate of optical feedback fiber laser was measured as 300kHz/sec which was better than the case without optical feedback.

Study of Optical Fiber Sensor Systems for the Simultaneous Monitoring of Fracture and Strain in Composite Laminates (복합적층판의 변형파손 동시감지를 위한 광섬유 센서 시스템에 관한 연구)

  • 방형준;강현규;홍창선;김천곤
    • Composites Research
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    • v.16 no.3
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    • pp.58-67
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    • 2003
  • To perform the realtime strain and fracture monitoring of the smart composite structures, two optical fiber sensor systems are proposed. The two types of the coherent sources were used for fracture signal detection - EDFA with FBG and EDFA with Fabry-Perot filter. These sources were coupled to EFPI sensors imbedded in composite specimens. To understand the characteristics of matrix crack signals, at first, we performed tensile tests using surface attached PZT sensors by changing the thickness and width of the specimens. This paper describes the implementation of time-frequency analysis such as short time Fourier transform (STFT) and wavelet transform (WT) for the quantitative evaluation of fracture signals. The experimental result shows the distinctive signal features in frequency domain due to the different specimen shapes. And, from the test of tensile load monitoring using optical fiber sensor systems, measured strain agreed with the value of electric strain gage and the fracture detection system could detect the moment of damage with high sensitivity to recognize the onset of micro-crack fracture signal.

Analysis and assessment of the gain of optically pumped surface-normal optical amplifiers (광여기 면형 광증폭기의 이득해석 및 제작)

  • 김운하;정기태;조용환
    • The Journal of Korean Institute of Communications and Information Sciences
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    • v.25 no.1B
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    • pp.8-14
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    • 2000
  • This paper analyzes and accesses the gain of optically pumped surface-normal MQW optical amplifiers. The proposed amplifiers have the advantage of polarization independence, high coupling efficiency to and from optical fibers, and flexibility of operating wavelength. We analyzed the gain characteristics of 100 - 200-period MQWs and verified the dependence of a strained lattice and selective doping. Theoretical analysis of such MQWs showsa single-pass gain of 3 dB with broad operation bandwidth. A single-pass gain of 2.6 dB is obtained experimentally in an InGaAs/InGaAlAs MQW amplifier, which is compared with calculations. The use of Fabry-Perot interferometer (FPI) structure in an optical amplifier is a useful way to increase the gain, but causes a problem of narrow operation bandwidth when the single-pass gain is low. Therefore, a single-pass gain above 2to 3 dB is a prerequisite to achieve both a high gain and moderate operation bandwidth in FPI-structured opticalamplifiers. We have designed an FPI-structured surface-normal optical amplifier both with a high gain of broad operation bandwidth of 4.6mm, when a single-pass gain is 3 dB.

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Low Stratospheric Wind Measurement Using Mobile Rayleigh Doppler Wind LIDAR

  • Shu, Zhi-Feng;Dou, Xian-Kang;Xia, Hai-Yun;Sun, Dong-Song;Han, Yan;Cha, Hyunki;Kim, Dukhyeon;Wang, Guo-Cheng;Baik, Sunghoon;Hu, Dong-Dong
    • Journal of the Optical Society of Korea
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    • v.16 no.2
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    • pp.141-144
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    • 2012
  • A mobile Rayleigh Doppler wind LIDAR at an eye-safe wavelength of 355 nm incorporating double-edge technique with triple-channel Fabry-Perot etalon is developed for wind measurement from 5 to 40km. The structure of this LIDAR system is described. An intercomparsion experiment with rawinsonde is made, showing good agreement with expected measurement accuracy. A continuous observation of stratosphere wind field for several days with temporal resolution of 15 min and spatial resolution of 200 m from 5 to 40 km is presented, demonstrating the stability and robustness of the LIDAR. A stratospheric quasi-zero wind layer can be found at around 20 km with a direction change from east to west evident in the continuous observation.