• Title/Summary/Keyword: 파장가변 레이저

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Implementation and modeling of wavelength tunable all-optical clok recovery using a semiconductor-fiber ring laser (고리형 반도체-광섬유 레이저를 이용한 파장 가변형 전광 동기 신호 재생 구현과 모델링)

  • 유봉안;김동환;이병호
    • Korean Journal of Optics and Photonics
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    • v.11 no.3
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    • pp.166-170
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    • 2000
  • A wavelength tunable all-optical clock recovery using a semiconductor optical amplifier in a fiber ring cavity is proposed and demonstrated at the wavelength of 1530 nm to 1570 nm. A synchronized optical pulse train is recovered from 10 Gbps and 30 Gbps randomly generated optical pulse streams with injection locking technique. Also, the system responses to the perturbation and the input average power variation are analyzed by a large-signal model based on time-domain travelling wave equation. ation.

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Walk-off Output Characteristics of OPO Pumpedby SHG of Nd:YAG Laser (Nd:YAG 레이저의 SHG로 펌핑된 OPO의 Walk-off 출력특성)

  • 이용우
    • Proceedings of the Korean Institute of Information and Commucation Sciences Conference
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    • 2003.05a
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    • pp.419-423
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    • 2003
  • In this paper, we have constructed singly resonant KTP OPO system pumped by 532 nm to obtain broadly frequency tunable pulses. Also we have mathematically simulated frequency tuning range, phase matching angle for 900 nm output and threshold energy, and we calculated output intensity using wave propagation equations for optical parametric oscillator which include walk-off, pump depletion.

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Near Infrared Laser Based on Polymer Waveguide Bragg Grating (폴리머 광도파로 브래그 격자 기반의 근적외선 레이저)

  • Kim, Kyung-Jo;Son, Nam-Seon;Kim, Jun-Whee;Oh, Min-Cheol
    • Korean Journal of Optics and Photonics
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    • v.22 no.4
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    • pp.179-183
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    • 2011
  • An external cavity laser operating at near infrared wavelength is demonstrated by incorporating polymer waveguide Bragg reflectors. 3rd order Bragg grating and oversized rip waveguide structure were designed by using the effective index method and the transmission matrix method. The polymer waveguide was fabricated using polymer materials with refractive indices of 1.462 and 1.435 for the core and the cladding layers, respectively. The external feedback laser with 875-nm Bragg grating exhibits single mode lasing located at 850-nm wavelength with an output power of 0 dBm, a 20-dB bandwidth of 0.2 nm and a side mode suppression ratio of 40 dB.

Implementation of tunable laser source for WDM-PON using an self seeded F-P LD (Self Seeded F-P LD를 이용한 WDM-PON에서의 파장 가변 레이저 소스 구현)

  • Oh, Yeong-guk;Hwang, Ji-hong;Lee, Hyuek-jae;Lee, Chang-hee
    • Proceedings of the Korean Institute of Information and Commucation Sciences Conference
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    • 2012.10a
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    • pp.439-441
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    • 2012
  • A new wavelength tunable laser source based on a self-seeded F-P LD for a WDM-PON system has been proposed in this paper. The proposed laser source has a merit of the wavelength tunable range of approximately 20 nm with very simple setup. The measured minimum relative intensity noise(RIN) was approximately -124 dB/Hz and the possibility of 10 Gb/s external modulation was showed.

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Construction and operational characteristics of a Ultra-Short pulse Cr4+:YAG laser (극초단 펄스 Cr4+:YAG 레이저의 제작 및 동작 특성)

  • Lee Bong Yeon;Lee Dong Han;Lee Chi Weon;Yoon Seok Beom;Choo Han Tae
    • Korean Journal of Optics and Photonics
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    • v.15 no.5
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    • pp.455-460
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    • 2004
  • We have developed a mode-locked ultra-short pulse C $r^{4+}$:YAG laser, as well as a continuous wave C $r^{4+}$:YAG laser. The laser was pumped by a Nd:YAG laser and its characteristics were investigated. In continuous wave mode, we obtained as much as 600 mW at 1.436 ${\mu}{\textrm}{m}$ with pumping power of 6 W, by using an output coupler with a reflectivity of 98%. The power slope efficiency was 10%, when the gain medium was cooled to 19$^{\circ}C$. The tuning range was varied from 1.39 ${\mu}{\textrm}{m}$ to 1.55 ${\mu}{\textrm}{m}$ and the maximum power was 400 mW at 1.492 ${\mu}{\textrm}{m}$ with a 3-plate birefringent filter. The C $r^{4+}$:YAG laser was mode-locked by a Kerr lens mode locking method. Mode locking at 1.436 ${\mu}{\textrm}{m}$was initiated by slightly rocking a mirror mount. But the pulses were very unstable because of the strong water absorption at this region. So we shifted the lasing wavelength to 1.492 ${\mu}{\textrm}{m}$ by using a 3-plate birefringent filter. Then we obtained stable state mode-locking with the maximum average power of 280 mW for a pumping power of 6 W. The pulse width of 43 fs was measured using an autocorrelator and the repetition rate was 104.5 MHz.

Double-pass Second Harmonics Generation of Tunable CW Infrared Laser Beam of DOFA System in Periodically Poled LiNbO3 (PPLN 비선형 결정과 이중통과법을 이용한 DOFA 시스템에서 증폭된 연속발진형 파장가변 적외선 레이저광의 제 2고조파 발생)

  • Yoo, Kil-Sang;Jo, Jae-Heung;Ko, Kwang-Hoon;Lim, Gwon;Jeong, Do-Young
    • Korean Journal of Optics and Photonics
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    • v.19 no.3
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    • pp.229-236
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    • 2008
  • The optimum conditions of second harmonic generation (SHG) can be successfully achieved experimentally using single pass and double pass methods of a pumping beam. The beam has a power of several Watts radiated by a DOFA (Diode Laser Oscillator & Fiber Amplifier) system, which is a high power CW wavelength tunable infrared laser system, in a PPLN (Periodically Poled MgO doped Lithium Niobate) nonlinear crystal. In the case of a single pass method, the parameters are the wavelength of 535 nm for SHG and the output power of 245 mW generated from the pumping input beam with wavelength of 1070 nm and the power of 2.45 W at phase matching temperature of $108.9^{\circ}C$. The conversion efficiency of SHG was 10%. In order to enhance the output of SHG, the double pass method of the SHG system of a PPLN using a concave mirror for the retroreflection and a pair of wedged flat windows for phase compensation was also presented. In this double pass system, we obtained the SHG output beam with the wavelength of 535 nm and the maximum power of 383 mW at optimum phase matching temperature of $108.5^{\circ}C$ by using an incident pumping beam with wavelength of 1070 nm and the power of 2.45 W. The maximum conversion efficiency is 15.6%, which is more than that of the single pass method.

An optical channel-switching transmission filter using the segmented chirped fiber Bragg grating (영역이 분리된 첩 광섬유 격자를 이용한 광 채널 스위칭용 투과 필터의 설계)

  • 박세강;박진우;구현덕;이상배
    • Korean Journal of Optics and Photonics
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    • v.12 no.5
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    • pp.401-405
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    • 2001
  • We propose a novel channel-switching transmission filter using segmented chirped fiber Bragg gratings (CFBG's) each of which has separate transmission bands in the reflection spectrum of the CFBG. The segmented CFBG's are made by using specially designed slits. The separated reflection spectral bands of the segmented CFBG's are controlled by the attached fiber stretchers, and the controlled reflection bands are used to choose the channels independently. Tunability of the transmission spectra is experimentally demonstrated in WDM transmission experiments.

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유연 전자소자 구현을 위한 폴리이미드 기판 제작

  • Lee, Jun-Gi;Kim, Sang-Seop;Choe, Byeong-Deok
    • Proceedings of the Korean Vacuum Society Conference
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    • 2011.08a
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    • pp.258-258
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    • 2011
  • 최근 유연 기판을 이용한 태양전지 및 TFT 등 전자소자 개발에 관한 연구가 주목받고 있다. 본 연구에서는 공정 시 유리한 유리기판상 전자소자 제작 후 폴리이미드막 박리를 통한 유연전자 소자 구현을 목적으로 한다. 폴리이미드막 박리를 목적으로 희생층으로서 a-Si:H을 사용하였다. 유리기판상에 60 nm 두께의 a-Si : H을 ICP (Induced coupled plasma) 공정으로 증착한 후 a-Si : H층 상부에 30 ${\mu}m$ 두께로 폴리이미드를 코팅하여 Hot plate와 furnace에서 열처리를 거쳤다. 이후 각기 다른 파장을 갖는 레이저의 파워를 가변하며 유리 기판 후면에 조사하였다. 실험 결과 355 nm UV 레이저로 가공한 경우 희생층으로 사용 된 a-Si : H층 내에 존재하는 수소가 레이저 빛 에너지에 의해 결합이 끊어지면서 유리기판과 폴리이미드막이 분리됨을 확인하였다.

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A study on the implementation of a tunable laser system for holebuning optical memory (Holeburning 광메모리용 가변파장 레이저 시스템의 구현에 관한연구)

  • 김민지
    • Proceedings of the Optical Society of Korea Conference
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    • 1998.08a
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    • pp.170-171
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    • 1998
  • Here are proposed the tunable laser for optical memory which uses the acousto-optic deflector. This laser includes the acousto-optic deflector in the Littrow mount configuration so that we may control the beam deflection by means of the induced RF. Consequently, we can achieve the higher speed and accuracy to compare with the Littrow monut configuration only.

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