• Title/Summary/Keyword: Polarization grating

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Fiber-optic Ccurrent Sensor Using a Long-period Fiber Grating Inscribed on a High Birefringent Fiber (복굴절이 큰 광섬유에 제작된 장주기 광섬유 격자를 이용한 광섬유 전류 센서)

  • Lee, Yong-Wook
    • The Transactions of The Korean Institute of Electrical Engineers
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    • v.56 no.10
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    • pp.1823-1825
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    • 2007
  • Based on Faraday effect, the variation of current flowing through the conductor can be encoded as that of azimuth angle of light polarization propagating through the fiber coil wound onto the conductor. The amount of current can be obtained by measuring the variation of the light intensity transformed from that of the azimuth angle through a polarization analyzer. In this paper we propose a fiber-optic current sensor system that employs a fiber polarization analyzer as a sensor interrogation device. The fiber polarization analyzer was prepared by inscribing a long-period fiber grating on a high birefringent fiber. At the fixed wavelength of 1522.5 nm, the fabricated fiber device has the polarization extinction ratio of more than 25 dB. The measurement of large current up to 600 Arms was accomplished based on a simple fiber interrogation device and the measurement output of the sensor system showed a good linearity.

The recording of surface relief grating on the chalcogenide thin film (비정질 칼코게나이드 박막에 Surface Relief 격자 형성)

  • 박종화;장선주;박정일;여철호;이영종;정홍배
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2000.07a
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    • pp.299-302
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    • 2000
  • In this study, we have made the large holographic surface relief gratings on amorphous chalcogenide $As_{40}$$Ge_{10}$$Se_{15}$$S_{35}$ films by two beam interference using a He-Ne laser(632.8nm) light. The film thickness was about 0.6$\mu\textrm{m}$, we could magnify beam size by using beam expander. We made use $90^{\circ}$ holder which was made of reflection mirror and sample. Formed the surface relief structures were investigated using optical microscope. The diffraction efficiency was obtained by measuring +lst order intensity. In addition we investigated grating formation and diffraction efficiency as a function of polarization states which is linear or circular polarization. The results indicate that the grating was formed by linear polarized beam is better clear than that by circular polarized beam.

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Polarization-Diversity-Loop-Configuration-Based Fiber Filter Realizing Inline Conversion Between Transmission and Reflection Spectra of Fiber Bragg Grating (광섬유 브래그 격자의 투과 및 반사 스펙트럼간 동일 선로상 변환이 가능한 편광상이 배치구조 기반 광섬유 필터)

  • Jang, Wook;Lee, Yong-Wook
    • Journal of the Korean Institute of Illuminating and Electrical Installation Engineers
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    • v.25 no.5
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    • pp.1-6
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    • 2011
  • By incorporating a polarization-diversity loop configuration (PDLC), we have demonstrated inline conversion between transmission and reflection spectra of a fiber Bragg grating (FBG) without reconfiguration of the fiber filter structure. The proposed apparatus consists of a polarization beam splitter, an FBG, and two quarter-wave plates (QWP's). The inline conversion operation between transmission and reflection spectra of the FBG was performed by proper adjustment of QWP's within the proposed filter. The band rejection ratio and side-mode suppression ratio in transmission and reflection modes of the fabricated filter were measured as ~17.0[dB] and ~16.4[dB], respectively.

Polarization recording and reconstruction in the chalcogenide As-Ge-Se-S thin films (비정길 칼코게나이드 As-Ge-Se-S 박막에서 편광기록 재생)

  • 장선주;박종화;손철호;정홍배
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.13 no.9
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    • pp.781-785
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    • 2000
  • Chalcogenide glasses are suggested as a candidate for optical recording. In this study, we have investigated the holography recording and reconstruction of the polarization state in chalcogenide As$_{40}$ Ge$_{10}$Se$_{15}$ S$_{35}$ thin films. We have used a He-Ne laser light(633nm) to probe and record of the grating. Also the polarization state of object beam was modulated with a λ/4 wave plate. The polarization state of the +1st order diffracted beam was generated by readout of the grating with a linearly polarized reference beam. It was the same-handed polarization state as the polarization state of the recording beam. The result is shown that the diffraction efficiency of circularly polarized recording represents higher than other polarization state.ate.e.

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Polarization recording and reconstruction in the chalcogenide As-Ge-Se-S thin films (비정질 칼코게나이드 As-Ge-Se-S 박막에서 편광기록 및 재생)

  • 장선주;손철호;여철호;박정일;이영종;정홍배
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2000.07a
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    • pp.312-315
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    • 2000
  • In this study, we have investigated the holography recording and reconstruction of the polarization state in chalcogenide $A_{s40}Ge_{10}Se_{15}S_{35}4 thin films using a He-Ne laser light(633nm). The thickness of thin films is a 8677${\AA}$ and 9093${\AA}$. A He-Ne laser used to probe and record of the grating. Also the polarization state of object beam modulated with a $\lambda/4$ wave plate. The polarization state of the +lst order diffracted beam generated by readout of the grating with a linearly polarized reference beam. It was the same-handed polarization state as the polarization state of the recording beam. The diffraction efficiency of circularly polarized recording represented higher than other polarization state.

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Polarization recording and reconstruction in the chalcogenide As-Ge-Se-S thin films. (비정질 칼코게나이드 As-Ge-Se-5 박막에서 편광기록 및 재생)

  • 장선주;손철호;여철호;박정일;이영종;정흥배
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2000.07a
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    • pp.820-823
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    • 2000
  • In this study, we have investigated the holography recording and reconstruction of the polarization state in chalcogenide $As_{40}$$Ge_{10}$$Se_{15}$$S_{35}$ thin films using a He-Ne laser light(633nm). The thickness of thin films is a 8677${\AA}$ and 9093${\AA}$. A He-Ne laser used to probe and record of the grating. Also the, polarization state of object beam modulated with a $\lambda/4$ wave plate. The polarization state of the +1st order diffracted beam generated by readout of the grating with a linearly polarized reference beam. It was the same-handed polarization state as the polarization state of the recording beam. The diffraction efficiency of circularly polarized recording represented higher than other polarization state.

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Diffraction-efficiency Correction of Polarization-independent Multilayer Dielectric Gratings (무편광 유전체 다층박막 회절격자의 효율 보정)

  • Cho, Hyun-Ju;Kim, Gwan-Ha;Kim, Dong Hwan;Lee, Yong-Soo;Kim, Sang-In;Cho, Joonyoung;Kim, Hyun Tae
    • Korean Journal of Optics and Photonics
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    • v.33 no.1
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    • pp.22-27
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    • 2022
  • We fabricate a polarization-independent dielectric multilayer thin-film diffraction grating for a spectral-beam-combining (SBC) system with a simple grating structure and low aspect ratio. Due to the refractive index and thickness error of the manufactured thin films, the diffraction efficiency of the fabricated diffraction grating was lower than that of the design. The causes of the errors were analyzed, and it was confirmed through simulation that diffraction efficiency could be compensated through an additional coating on the manufactured diffraction grating. As a result of sputtering an additional Ta2O5 layer on a fabricated diffraction grating, the diffraction efficiency was corrected and a maximum 91.7% of polarization-independent diffraction efficiency was obtained.

Polarization Holographic Grating Formation and Diffraction Efficiency Measurement in Amorphous Chalcogenide Thin Films (비정질 칼코게나이드 박막에서의 편광 홀로그라피 격자 형성 및 회절효율 측정)

  • 전진영;여철호;이현용;정홍배
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 1998.11a
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    • pp.89-92
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    • 1998
  • Amorphous chalcogenide thin films, especially a-(Se, S) based films, exhibit a number of photoinduced phenomena not observed in other types of amorphous thin films. The polarization holographic grating has been formed in amorphous As-Ge-Se-S thin films using two linearly polarized He-Ne laser light. In addition, dffraction efficiency has been measured by the same laser of a relative lower intensity at the same time.

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Wavelength-Switchable Fiber Ring Laser Employing a Long-Period Fiber Grating Inscribed on a High Birefringent Fiber (복굴절이 큰 광섬유에 형성된 장주기 광섬유 격자를 이용한 파장 스위칭 가능한 광섬유 고리형 레이저)

  • Lee, Yong-Wook
    • The Transactions of The Korean Institute of Electrical Engineers
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    • v.56 no.11
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    • pp.1995-1997
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    • 2007
  • In this paper we propose a wavelength-switchable fiber ring laser that employs a polarization-dependent fiber band stop filter. The fiber filter was fabricated by inscribing a long-period fiber grating on a high birefringent fiber. Dual-wavelength switching operation was accomplished by controlling the rotatable linear polarizer which rotated the polarization plane of the light circulating through the fiber laser cavity. The amplitude variation of both laser lines was measured to be less than 0.5 dB and the signal-to-amplified spontaneous emission ratio was more than 55 dB.

Polarization-Controlled Waveband Switching in a Multiwavelength Fiber Bragg Grating Laser (다파장 광섬유 격자 레이저의 편광 제어 파장밴드 스위칭)

  • Lee, Yong-Wook
    • The Transactions of The Korean Institute of Electrical Engineers
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    • v.56 no.12
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    • pp.2214-2216
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    • 2007
  • Based on a semiconductor optical amplifier and sampled fiber Bragg gratings, polarization-controlled waveband switching in multiwavelength fiber laser is successfully demonstrated at room temperature by using high polarization selectivity of a polarization beam splitter. A multiwavelength-switching operation between eight and six laser lines with signal to noise ratio over 35 dB and wavelength spacing of ${\sim}0.8nm$ has been successfully demonstrated. The switching displacement of the proposed laser was ${\sim}7.1nm$. The intensity unevenness between different laser lines was measured to be less than 6.5 dB. The switching displacement between wavebands (groups of contiguous wavelengths), wavelength channels, and their spacings can be flexibly designed by the selected comb filters.