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"FDTD"

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"FDTD"

PLC Optical Sensor for Contamination Monitoring on the Flow-Cell in the Water Quality Measurement System
Seung Heon Han, Tae Un Kim, Haeng Yun Jung, Hyun Chul Ki, Doo Gun Kim, Seon Hoon Kim
J Electr Electron Mater 2019;32(6):472-476.   Published online November 1, 2019
We have proposed a novel planar lightwave circuit (PLC) optical sensor to monitor the contamination in a flow-cell where water is continuously supplied through a water quality measurement system. We designed a PLC chip with a V-shape waveguide and the simulated its function as a sensor for monitoring contamination in a flow-cell using a numerical the FDTD (finite-difference time-domain) analysis. A novel cross type of waveguide was introduced to make the PLC chip of the V-shaped waveguide. The fabricated PLC was cut into the cross waveguide. A change in the optical propagation loss of the PLC sensor was observed after immersing the PLC sensor into city water. It was determined that the propagation loss of the PLC sensor was 3 dB at a wavelength of 1.55 μm in the city water for 15 days.
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Regular Paper : Optical Characteristics of Plasmonic Nano-structure Using Polystyrene Nano-beads
Doo Gun Kim, Byung Gue Jung, Hong Seung Kim, Tae Ryong Kim, Seon Hoon Kim, Hyun Chul Ki, Tae Un Kim, Jae Cheol Shin, Young Wan Choi
J Electr Electron Mater 2015;28(4):244-248.   Published online April 1, 2015
We proposed and demonstrated the double layered metallic nano-hole structure using polystyrene beads process to enhance the sensitivity of surface plasmon resonance (SPR). The double layered SPR structures are calculated using the finite-difference time-domain (FDTD) method for the width, thickness, and period of the metallic nano-hole structures. The thickness of the metal film and the metallic nano-hole is 30 and 20 nm in the 214 nm wide nano-hole size, respectively. The double layered SPR structures are fabricated with monolayer polystyrene beads of 420 nm wide. The sensitivities of the conventional SPR sensor and the double layered SPR sensor are obtained to 42.2 and 52.1 degree/RIU, respectively.
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Display and Optical Devices : Optical Characteristics of Plamonic Waveguide Using Tapered Structure
Doo Gun Kim, Hong Seung Kim, Geum Yoon Oh, Seon Hoon Kim, Hyun Chul Ki, Tae Un Kim, Hwe Jong Kim, Ping Ma, Christian Hafner, Young Wan Choi
J Electr Electron Mater 2014;27(3):156-161.   Published online March 1, 2014
We have investigated the optical properties of plamonic waveguide with tapered structure based on InP material for photonic integrated circuit(PIC). The proposed plasmonic waveguide is covered with the Ag thin film to generate the plasmonic wave on metallic interface. The optical characteristics of plasmonic waveguide were calculated using the three-dimensional finite-difference time-domain method. The plasmonic waveguide was fabricated with the lengths of 2 to 10 μm and the widths of 400 to 700 nm, respectively. The plasmonic mode and optical loss were measured. The optimum plasmonic length is 10 μm and widths are 600 and 700 nm in the fabricated waveguide. This plasmonic waveguide can be directly integrated with other conventional optical devices and can be essential building blocks of PIC.
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Effects of Light Incident Mode on Optical Scattering of Au Nanoparticle by Localized Surface Plasmon Resonance
Taek Sung Lee, Kyeong Seok Lee, Won Mok Kim, Jang Kyo Lee, Seok Joo Byun
J Electr Electron Mater 2009;22(4):307-313.   Published online April 1, 2009
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Characteristics of the Photonic Bandgaps in Two-dimensional Photonic Crystals with a Square Lattice by FDTD Simulation
Jong Bin Yeo, Hoe Young Yang, Hyun Yong Lee
J Electr Electron Mater 2009;22(1):61-66.   Published online January 1, 2009
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A Studying on the Crosstalk Characteristic of mm-wave Coplanar-waveguide
J Electr Electron Mater 2006;19(2):158-161.   Published online February 1, 2006
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Optimum Design of EHF CPW using FDTD
J Electr Electron Mater 2005;18(12):1129-1132.   Published online December 1, 2005
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