• Title/Summary/Keyword: Fabry-Perot cavity

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Highly Sensitive Optical-fiber Humidity Sensor Based on Nafion-PVA Sol-gel

  • Ning, Wang;Yuhao, Li;Xiaolei, Yin;Wenting, Liu;Shiqi, Liu; Xuwei, Zhao; Yanxi, Zhong;Liang, Xu
    • Current Optics and Photonics
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    • v.7 no.1
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    • pp.21-27
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    • 2023
  • A highly sensitive optical-fiber humidity sensor is demonstrated in this paper. By using Nafion-PVA sol-gel and single-mode optical fibers, the Fabry-Perot humidity sensor is easily fabricated. In the humidity range of 29%-72%, humidity-response experiments are carried out with a cycle of rising and falling humidity to investigate humidity-response characteristics. The experimental results show 2.25 nm/%RH sensitivity and a 0.9997 linear correlation coefficient, with good consistency. The changes in optical-path difference (OPD) and free spectral range (FSR) with humidity are also discussed. The humidity sensitivities of a typical sensor are 80.3 nm/%RH (OPD) and 0.03 nm/%RH (FSR). Furthermore, many humidity sensors with different Nafion-PVA sol-gel concentration and initial cavity length are experimentally investigated for humidity response. The results show that the sensitivity increases with higher Nafion ratio of the Nafion-PVA sol-gel. The influence of changing cavity length on sensitivity is not obvious. These results are helpful to research on optical-fiber humidity sensors with good performance, easy fabrication, and low cost.

Measurement of Birefringence with Brillouin Spectroscopy

  • Lee, Suk-Mock;Hwangbo, Chang-Kwon
    • Journal of the Optical Society of Korea
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    • v.5 no.3
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    • pp.67-69
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    • 2001
  • An alternative way to determine the birefringence for uniaxial crystals with Brillouin scattering experiments equipped with a Fabry-Perot interferometer is presented. The value of the minimum cavity spacing of the interferometer to observe the birefringence was found, and it is shown that the experimental error of the birefringence could be reduced by increasing the cavity spacing. For a single crystal of $\alpha$-LiIO$_3$, the birefringence was found to be 0.14814$\pm$0.0007 at 514.5 nm.

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.

Linear interrogation of fiber Bragg grating sensor array using time-delayed quadrature sampling technique (시간지연 샘플링을 이용한 광섬유 격자 센서어레이의 선형 복조)

  • 김종섭;송민호
    • Korean Journal of Optics and Photonics
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    • v.15 no.1
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    • pp.34-38
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    • 2004
  • A fiber laser of which wavelength was scanned by an intra-cavity FP (Fabry-Perot) filter was used to interrogate a fiber Bragg grating strain sensor array. We calculated the wavelength variation of the fiber laser using quadrature signal processing with an unbalanced M/Z (Mach-Zehnder) interferometer and time-delayed sampling technique. The calculated wavelengths are mapped to corresponding temporal reflection peaks from the sensor array, which enables more accurate and stable interrogation without the problems caused by the FP filter's nonlinear characteristics. Wavelength resolution of ∼20 pm was obtained in our experimental setup, which could have been greatly enhanced with faster phase modulation.

Coherent optical transmission experiment using FSK modulation and heterodyne detection scheme (FSK/Heterodyne 변복조 방식에 의한 코히런트 광송수신 실험)

  • 박희갑
    • Proceedings of the Optical Society of Korea Conference
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    • 1991.06a
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    • pp.121-125
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    • 1991
  • A basic coherent optical transmission was demonstrated using FSK modulation and heterodyne detection scheme. Optical frequency of DFB LD light source at the transmitter side was stabilized with Fabry Perot etalon and bias feedback circuit. A tunable external cavity LD was used as a local oscillator at the receiver. Heterodyned output signal at IF frequency of 2GHz was measured and discussed.

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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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Design of 850 nm Vertical-Cavity Surface-Emitting Lasers by Using a Transfer Matrix Method (전달 행렬 방법을 이용한 850 nm수직 공진기 레이저 구조의 최적설계)

  • Kim Tae-Yong;Kim Sang-Bae
    • Journal of the Institute of Electronics Engineers of Korea SD
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    • v.41 no.1
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    • pp.35-46
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    • 2004
  • In comparison with edge-emitting lasers(EELs), predicting the output power and slope efficiency of Vertical-Cavity Surface-Emitting Lasers(VCSELs) is very difficult due to the absorption loss in DBR layers. However, by using transfer matrix method(TMM), we've made possible to calculate such parameters of multi-layer structures like VCSELs. In this paper, we've calculated the threshold gain, threshold current and slope efficiency through the methodology based on TMM. Also TMM is the way of customizing the VCSEL structure for the desired threshold current and slope efficiency by changing the number of DBR mirror layers.

Long-term stabilization of optical feedback of a resonant external cavity coupled semiconductor laser (공진형 외부 캐비티 부착 반도체 레이저의 광피드백 장기 안정화)

  • 신철호
    • Korean Journal of Optics and Photonics
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    • v.9 no.2
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    • pp.96-99
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    • 1998
  • In this study, a novel long term stabilization method of optical feedback for the resonant cavity coupled semiconductor lasers is proposed, and its utility was shown experimentally. The proposed method is realized by using the pahse discriminator of optical feedback with high gain. The phase discriminating signal was obtained by the polarization spectroscopic technique using reflection light from the external reflector, which is a confocal Fabry-Perot cavity. Experimental result shows that stable control state can be maintained up to 20 hours. The period can be increased by reducing size of the system and/or fixing position stably of optical parts used, which were arranged on an optical table by using magnetic bases in this experiment. The proposed long-term stabilization method of optical feedack of a resonant external cavity coupled semiconductor laser is very useful for the field of high sensitivity measurement, and for the use in the laboratory level in particular.

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High Performance $2{\times}4$ S-SEED Array with Extremely Shallow Quantum Well and Asymmetric Fabry-Peort Cavity Structure (저장벽 양자우물고조와 비대칠 패브리-페로 공명기 구조에 의한 고성능 $2{\times}4$ S-SEED Array 구현)

  • 권오균;최영완;김광준;이일항;이상훈;원용협;유형모
    • Korean Journal of Optics and Photonics
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    • v.5 no.1
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    • pp.144-151
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    • 1994
  • We designed and fabricated a $2{\times}4$ symmetric self electro-optic effect device array using GaAs/ AIo.04 G$\DeltaR$), and optical bistability loop width ($\Delta$). The average values of the elements of the $2{\times}4$ S-SEED array were CR~13.1, R~24%, and $\Delta$~91%. It was found that the AFP cavity structure enhances the self-biased optical bistability in ESQW-SEED under no external bias. That is due to the decreased intrisic region thickness in AFP-SEED structures, and which increases the built-in electric fields. The zero-biased S-SEED showed CR of ~4.7, R~9%, and $\Delta$~22%.X>~22%.

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Development of FBG sensor System for Measuring the High Frequent Vibration of Structures and the Natural Frequency of Composites (고주파 진동 측정을 위한 FBG 센서 시스템 개발 및 복합재 시편의 고유진동수 측정)

  • Kim, Dae-Hyun;Koo, Bon-Yong;Kim, Chun-Gon;Hong, Chang-Sun;Lee, In
    • Proceedings of the Korean Society For Composite Materials Conference
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    • 2002.05a
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    • pp.159-162
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    • 2002
  • We introduce a simple optically passive detection scheme for Bragg grating sensors. This detection scheme is based on two cavity lengths in Fabry-Perot read-out interferometers to produce two quadrature phase shifted signals from the Bragg grating sensor. The passive detection technique is demonstrated by the use of Bragg grating sensors in measuring the dynamic vibrations of the composites.

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