• Title/Summary/Keyword: Silica Waveguide

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Thermo-optic Effects of Bragg Grating Optical Temperature Sensor

  • Ahn, Kook-Chan;Lee, Sang-Mae;Lee, Gwang-Seok;Park, Seung-Bum
    • International Journal of Aeronautical and Space Sciences
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    • v.3 no.2
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    • pp.24-30
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    • 2002
  • This paper demonstrates a comparison of linear and nonlinear analyses for thermo-optic effects of optical temperature sensor based on the etched silica-based planar waveguide Bragg grating. Topics include theoretical analyses and experiment of the etched planar waveguide Bragg grating optical temperature sensor. Theoretical models with nonlinear than linear temperature effect for the grating response based on waveguide and plate deformation theories agree with experiments to within acceptable tolerance.

Thermo-optic Effects of Optical Temperature Sensor (광 온도센서의 열전.광 효과)

  • Lee, Kwang-Seok;Kim, Hyun-Deok
    • Journal of the Korea Institute of Information and Communication Engineering
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    • v.10 no.11
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    • pp.2049-2054
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    • 2006
  • This paper demonstrates a comparison of linear and nonlinear analyses for thermo-optic effects of optical temperature sensor based on the etched silica-based planar waveguide Bragg grating. Topics include theoretical analyses and experiment of the etched planar waveguide Bragg grating optical temperature sensor, Theoretical models with nonlinear than linear temperature effect for the grating response based on waveguide and plate deformation theories agree with experiments to within acceptable tolerance.

The Study of Silica Surface Reaction with Fluorocarbon Plasma Using Inductively Coupled Plasma (Inductively Coupled Plasma에 의한 fluorocarbon 가스 플라즈마의 실리카 표면 반응 연구)

  • Park, Sang-Ho;Shin, Jang-Uk;Jung, Myung-Young;Choy, Tae-Goo;Kwon, Kwang-Ho
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.11 no.6
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    • pp.472-476
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    • 1998
  • The surface reactions of silica film($SiO_2-P_2O_5-B_2O_3-GeO_2$) with fluorocarbon plasma has been studied by using angle -resolved x-ray photoelectron spectroscopy(XPS). It has been confirmed that residual carbon consists of C-C and C-CFx bonds and fluorine mainly binds silicon in the case of etched silica by using $CF_4$ gas plasma. The surface reaction of silica with various fluorocarbon gases, such as $CF_4,C_2F_6 and CHF_3$ were investigated. XPS results showed that though the etching gases were changed, the elements and binding states of the residual layers on the etched silica by using various fluorocarbon gas plasma were nearly the same . This seems to be due to the high volatility of byproducts, that is, $SiF_4 and CO_2$ etc..

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Laser microstructuring of trench and its application to optical waveguide (레이저를 이용한 트렌치 제작 및 응용 연구)

  • Choi, Hun-Kook;Yoo, Dongyoon;Sohn, Ik-Bu;Noh, Young-Chul;Kim, Young-Sic;Kim, Su-yong;Kim, Wan-Chun;Kim, Jin-Bong
    • Laser Solutions
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    • v.18 no.1
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    • pp.7-11
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    • 2015
  • In this paper, micro trench structure is fabricated by femtosecond laser for inserting optical reflecting wavelength filter in planar waveguide. The width and depth of the trench is controlled by femtosecond laser machining condition. Also, large scale of single channel with 500um and 1000um on silica plate is fabricated by femtosecond laser, and roughness of the channel surface is polished by $CO_2$ laser for the insertion of the filter. Then, the characteristic of the planar waveguide inserted the filter is verified.

Refractive Index Control of Silicon Oxynitride Thick Films on Core Layer of Silica Optical Waveguide (실리카 광도파로의 Core층인 Silicon Oxynitride후박의 굴절률 제어)

  • 김용탁;조성민;윤석규;서용곤;임영민;윤대호
    • Journal of the Korean Ceramic Society
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    • v.39 no.6
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    • pp.594-597
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    • 2002
  • Silicon Oxynitride(SiON) thick films on p-type silicon(100) wafers have obtained by using plasma-enhanced chemical vapor deposition from SiH$_4$ , N$_2$O and N$_2$. Prism coupler measurements show that the refractive indices of SiON layers range from 1.4620 to 1.5312. A high deposition power of 180 W leads to deposition rates of up to 5.92${\mu}$m/h. The influence of the deposition condition on the chemical composition was investigated using X-ray photoelectron spectroscopy. After deposition of the SiON thick films, the films were annealed at 1050$^{\circ}C$ in a nitrogen atmosphere for 2 h to remove absorption band near 1.5${\mu}$m.

Cost Effective Silica-Based 100 G DP-QPSK Coherent Receiver

  • Lee, Seo-Young;Han, Young-Tak;Kim, Jong-Hoi;Joung, Hyun-Do;Choe, Joong-Seon;Youn, Chun-Ju;Ko, Young-Ho;Kwon, Yong-Hwan
    • ETRI Journal
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    • v.38 no.5
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    • pp.981-987
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    • 2016
  • We present a cost-effective dual polarization quadrature phase-shift coherent receiver module using a silica planar lightwave circuit (PLC) hybrid assembly. Two polarization beam splitters and two $90^{\circ}$ optical hybrids are monolithically integrated in one silica PLC chip with an index contrast of $2%-{\Delta}$. Two four-channel spot-size converter integrated waveguide-photodetector (PD) arrays are bonded on PD carriers for transverse-electric/transverse-magnetic polarization, and butt-coupled to a polished facet of the PLC using a simple chip-to-chip bonding method. Instead of a ceramic sub-mount, a low-cost printed circuit board is applied in the module. A stepped CuW block is used to dissipate the heat generated from trans-impedance amplifiers and to vertically align RF transmission lines. The fabricated coherent receiver shows a 3-dB bandwidth of 26 GHz and a common mode rejection ratio of 16 dB at 22 GHz for a local oscillator optical input. A bit error rate of $8.3{\times}10^{-11}$ is achieved at a 112-Gbps back-to-back transmission with off-line digital signal processing.

Optimization of a Birefringence-Enhanced-Waveguide-Based Polarization Beam Splitter

  • Kim, Jong-Hoi;Choe, Joong-Seon;Youn, Chun-Ju;Kim, Duk-Jun;Kwon, Yong-Hwan;Nam, Eun-Soo
    • ETRI Journal
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    • v.34 no.6
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    • pp.946-949
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    • 2012
  • We present the optimization of a birefringence-enhanced-waveguide (BWG)-based polarization beam splitter (PBS) in a Mach-Zehnder interferometer (MZI) configuration and analyze the structure-dependent or polarization-dependent phase difference, using a delay-line MZI (DL-MZI). We fabricate the DL-MZI using silica-based planar lightwave circuit technology and, using the DL-MZI, demonstrate the ability to optimize a PBS by measuring the birefringence of the BWG and structure-dependent phase offset.

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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Femtosecond Laser Application to PLC Optical Devices and Packaging

  • Sohn, Ik-Bu;Lee, Man-Seop;Lee, Sang-Man
    • ETRI Journal
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    • v.27 no.4
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    • pp.446-448
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    • 2005
  • Using tightly focused femtosecond laser pulses, we produce an optical waveguide and devices in transparent materials. This technique has the potential to generate not only channel waveguides, but also three-dimensional optical devices. In this paper, an optical splitter and U-grooves, which are used for fiber alignment, are simultaneously fabricated in a fused silica glass using near-IR femtosecond laser pulses. The fiber- aligned optical splitter has a low insertion loss, less than 4 dB, including an intrinsic splitting loss of 3 dB and excess loss due to the passive alignment of a single-mode fiber. Finally, we present an output field pattern, demonstrating that the splitting ratio of the optical splitter becomes approximately 1:1.

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