• Title/Summary/Keyword: optical losses

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Fabrication and Packaging of Planar Waveguide Brags Grating (평판도파로 브래그격자 제조 및 접속)

  • 한준모;최준석;문형명;임기건;이형종;최두선
    • Proceedings of the Korean Society of Precision Engineering Conference
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    • 2002.10a
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    • pp.141-144
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    • 2002
  • Computer code was developed to design waveguide gratings based on coupled-mode equations and the transfer matrix formalism. The experimental set-up has been constructed for inscribing Bragg gratings in planar waveguides with a phase mask and uv laser beam, which enables alignment and packaging of grating devices as well as in-situ performance measurements. Bragg grating has been fabricated on silica planar waveguides with 0.75% Germanium concentration and its transmittance spectrum was measured to have 95% reflectance at the peak wavelength. Optical losses as the function of the misalignment were measured and their usage is described.

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A multiplexed fiber-optic sensor for measuring large displacement (대변위 측정을 위한 다중화된 광섬유 센서)

  • Yoo, Jung-Ae;Kwon, Il-Bum;Jo, Jae-Heung;Seo, Dae-Cheol
    • Journal of Sensor Science and Technology
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    • v.14 no.3
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    • pp.169-179
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    • 2005
  • A multiplexed bend loss type single-mode fiber-optic sensor system was prepared to measure the displacement of several cm of the civil engineering structures such as many bridges, tunnels and various buildings. This bend loss type fiber-optic sensor used the signal difference between two reflection signals due to various bend losses generating at a pair of optical connectors by using OTDR (optical time domain reflectometer) for measuring displacements. And the experiments were conducted for showing the measurement feasibility on the range of 10 cm, and the multiplexing experiments were also performed to measure the displacements of 5 measuring positions of an object by setting these 5 fiber-optic sensors on a single mode fiber simultaneously.

Effects of system imperfections on optical interaction-free measurements (시스템 결함이 광학적 무작용 검출에 미치는 영향)

    • Korean Journal of Optics and Photonics
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    • v.10 no.2
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    • pp.114-119
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    • 1999
  • In an interation-free measurement system with the polarization-based Mach-Zehnder interferometer structure, effects of two system imperfections, i.e., the system loss and the low quantum efficiency of photon detectors, on the system perfomance are analyzed, Although both the two system imperfections limit the maximal defection efficiency that can be achievable, we show that the quantum efficiency of photon detectors is less important when the system loss becomes small. In addition, for given system losses and quantum efficiencies, we derive the maximal detection efficiencies that can be achievable.

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Ultrathin Metamaterial for Polarization Independent Perfect Absorption and Band-pass Filter

  • Zhang, Xu;Gong, Zhijie
    • Journal of the Optical Society of Korea
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    • v.19 no.6
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    • pp.665-672
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    • 2015
  • We demonstrate an ultrathin metamaterial for polarization independent perfect absorption as well as a band-pass filter (BPF) which works at a higher frequency band compared to the perfect absorption band. The planar metamaterial is comprised of three layers, symmetric split ring resonators (SSRRs) at the front and structured ground plane (SGP) at the back separated by a dielectric layer. The perfect metamaterial absorber (MA) can realize near 100% absorption due to high electromagnetic losses from the electric and/or magnetic resonances within a certain frequency band. The thickness of the structure is only 1/28 of the maximum absorption wavelength.

Gold Stripe Optical Waveguides Fabricated by a Novel Double-Layered Liftoff Process

  • Kim, Jin-Tae;Park, Sun-Tak;Park, Seung-Koo;Kim, Min-Su;Lee, Myung-Hyun;Ju, Jung-Jin
    • ETRI Journal
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    • v.31 no.6
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    • pp.778-783
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    • 2009
  • To fabricate uniform and reliable thin gold stripes that provide low-loss optical waveguides, we developed a novel liftoff process placing an additional $SiN_x$ layer under conventional photoresists. By patterning a photoresist and over-etching the $SiN_x$, the photoresist patterns become free-standing structures on a lower-cladding. This leads to uniform metal stripes with good reproducibility and effectively removes parasitic structures on the edge of the metal stripe in the image reversal photolithography process. By applying the newly developed process to polymer-based gold stripe waveguide fabrication, we improved the propagation losses about two times compared with that incurred by the conventional image-reversal process.

A Study on the Ultrashort Optical Pulse Generation of the Gain Switched V-Groove Quantum Wire Laser (이득 스위칭 방법을 이용한 V-자형 양자선 레이저의 초단 광펄스 생성에 관한 연구)

  • 최영철;김주연;김태근
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.16 no.9
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    • pp.833-837
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    • 2003
  • The spectral and temporal characteristics of a V-groove AIGaAs-GaAs quantum wire (QWR) laser were investigated with varying the cavity length. At cavity lengths shorter than 300 ${\mu}{\textrm}{m}$, a discrete shift in tile wavelength occurred from the n=1 to the n=2 subband due to the increased cavity losses. Utilizing this characteristic, ultrafast lasing characteristics at each subband were investigated by tile gain switching method.

In-line Variable Attenuator Based on the Evanescent Wave Coupling Between a Side-polished Single-mode Fiber and an Index Matched Dielectric Plate

  • Kim, Kwang-Taek;Kim, Hyo-Kyeom
    • Journal of the Optical Society of Korea
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    • v.8 no.1
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    • pp.17-20
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    • 2004
  • An in-line variable attenuator has been proposed and demonstrated exploiting a side-polished single-mode (SM) fiber evanescently coupled with an index matched dielectric plate. The attenuation can be controlled by fine mechanical sliding of the index matched dielectric plate. We have achieved 49 ㏈ dynamic range and very low excess loss of 0.2 ㏈ at 1550 nm wavelength. The measured polarization dependent losses (PDL) were 0.1, 0.2, and 0.4 ㏈ at 10, 20, and 30 ㏈ attenuation, respectively. Wavelength sensitivity was measured to be -0.017/nm ㏈ at 20 ㏈ attenuation.

Dependence of Round type electrodeless lamp according to Ferrite shape (페라이트 형상에 따른 둥근형 무전극 램프의 의존성)

  • Kim, Nam-Goon;Yang, Jong-Kyung;Lee, Joo-Ho;Park, Dae-Hee
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2007.11a
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    • pp.465-466
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    • 2007
  • In electrode-less lamp, The key point in creating an efficient light source based on RF discharge is to minimize the RF power loss in the RF coupler which for Anderson's type of RF lamp is due to losses in the ferrite core. This loss depends on the particular ferrite material, its size, geometry, frequency in this kind of inductive lamp shows that the correct choice of discharge current has a crucial effect on the core loss. In this study, we measured Ferrite temperature in normal state, then analyzed electrical and optical characteristics according to ferrite shape. We were able to know that was ferrite of the antenna had relate closely with temperature and luminous of the lamp. Also we appraised temperature and electrical, optical properties during turn on the lamp.

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A Study on the Fabrication of Polarimetric Fiber Optic Current Sensor (편광측정법에 의한 광섬유 전류 센서 제작에 관한 연구)

  • Jang, Nam-Young;Chio, Pyung-Suk;Eun, Jae-Jeong;Park, Hae-Soo
    • Journal of the Institute of Electronics Engineers of Korea SD
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    • v.41 no.6
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    • pp.33-41
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    • 2004
  • In this paper, a polarimetric fiber optic current sensor(P-FOCS) is experimented and fabricated, and then a possibility to the commercial utilization of the P-FOCS is also investigated. The P-FOCS measures an applied current by a Faraday rotation linearly proportional to a magnetic field generated by the applied current. The bending-induced linear birefringence in the sensing fiber is minimized by using the low birefringent fiber. Also, all fiber-optic components are used to avoid optical losses coming from the use of bulk components. A signal processing circuit is constructed and used to eliminate the effects of intensity variations in the output signal due to losses coming from misalignments of components such as fiber connectors. Using the optical source of 632.8nm wavelength, Faraday rotation is measured by passing through the sensing fiber within the solenoid of about 1500 turns which is equivalent to a current source of about 7500A. In the range of 1000A to 7500A, the measurement error for linearity is within about 1.5%.

Near IR Luminescence Properties of Er-doped Sol-Gel Films (Er이 도핑된 졸-겔 코팅막의 발광특성)

  • Lim, Mi-Ae;Seok, Sang-Il;Kim, Ju-Hyeun;Ahn, Bok-Yeop;Kwon, Jeong-Oh
    • Proceedings of the Materials Research Society of Korea Conference
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    • 2003.11a
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    • pp.136-136
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    • 2003
  • In fiber optic networks, system size and cost can be significantly reduced by development of optical components through planar optical waveguides. One important step to realize the compact optical devices is to develop planar optical amplifier to compensate the losses in splitter or other components. Planar amplifier provides optical gain in devices less than tens of centimeters long, as opposed to fiber amplifiers with lengths of typically tens of meters. To achieve the same amount of gain between the planar and fiber optical amplifier, much higher Er doping levels responsible for the gain than in the fiber amplifier are required due to the reduced path length. These doping must be done without the loss of homogeniety to minimize Er ion-ion interactions which reduce gain by co-operative upconversion. Sol-gel process has become a feasible method to allow the incorporation of Er ion concentrations higher than conventional glass melting methods. In this work, Er-doped $SiO_2$-A1$_2$ $O_3$ films were prepared by two different method via sol -Eel process. Tetraethylorthosilicate(TEOS)/aluminum secondary butoxide [Al (OC$_4$ $H_{9}$)$_3$], methacryloxypropylcnethoxysaane(MPTS)/aluminum secondary butofde [Al(OC$_4$ $H_{9}$)$_3$] systems were used as starting materials for hosting Er ions. Er-doped $SiO_2$-A1$_2$ $O_3$ films obtahed after heat-treating, coatings on Si substrate were characterized by X-ray din action, FT-IR, and N-IR fluorescence spectroscopy. The luminescence properties for two different processing procedure will be compared and discussed from peak intensity and life time.

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