• Title/Summary/Keyword: polarized

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Structure of Dual Polarized System for Wireless Communication (무선 통신을 위한 이중 편파 시스템 구조)

  • Kim, Jaekil;Gwak, Gye Seok;Ahn, Jae Min
    • The Journal of Korean Institute of Communications and Information Sciences
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    • v.39C no.8
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    • pp.746-755
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    • 2014
  • In this paper, we propose the structure of a dual polarized system for a wireless communication. The proposed dual polarized antenna is formed by one vertical antenna and two horizontal antennas that are orthogonal to each other. Vertical and horizontal polarized antennas transmit different signals, but two orthogonal horizontal polarized antennas transmit the same data signals. So, the signals of the proposed dual polarized system construct two dual-polarization planes. And, only one dual-polarization plane with a large signal power is selected at the side of a receiver. The simulation results show that the proposed dual polarized system could obtain a higher capacity compared to an ordinary $2{\times}2$ MIMO (Multi-input Multi-output) system.

Land Use and Land Cover Mapping from Kompsat-5 X-band Co-polarized Data Using Conditional Generative Adversarial Network

  • Jang, Jae-Cheol;Park, Kyung-Ae
    • Korean Journal of Remote Sensing
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    • v.38 no.1
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    • pp.111-126
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    • 2022
  • Land use and land cover (LULC) mapping is an important factor in geospatial analysis. Although highly precise ground-based LULC monitoring is possible, it is time consuming and costly. Conversely, because the synthetic aperture radar (SAR) sensor is an all-weather sensor with high resolution, it could replace field-based LULC monitoring systems with low cost and less time requirement. Thus, LULC is one of the major areas in SAR applications. We developed a LULC model using only KOMPSAT-5 single co-polarized data and digital elevation model (DEM) data. Twelve HH-polarized images and 18 VV-polarized images were collected, and two HH-polarized images and four VV-polarized images were selected for the model testing. To train the LULC model, we applied the conditional generative adversarial network (cGAN) method. We used U-Net combined with the residual unit (ResUNet) model to generate the cGAN method. When analyzing the training history at 1732 epochs, the ResUNet model showed a maximum overall accuracy (OA) of 93.89 and a Kappa coefficient of 0.91. The model exhibited high performance in the test datasets with an OA greater than 90. The model accurately distinguished water body areas and showed lower accuracy in wetlands than in the other LULC types. The effect of the DEM on the accuracy of LULC was analyzed. When assessing the accuracy with respect to the incidence angle, owing to the radar shadow caused by the side-looking system of the SAR sensor, the OA tended to decrease as the incidence angle increased. This study is the first to use only KOMPSAT-5 single co-polarized data and deep learning methods to demonstrate the possibility of high-performance LULC monitoring. This study contributes to Earth surface monitoring and the development of deep learning approaches using the KOMPSAT-5 data.

Relationship between the pretilt angle generation and the polarization component with linearily polarized UV light irradiation on polymer surface. (직선편광된 UV광을 폴리이미드막에 조사한 경우의 프리틸트각의 발생과 편광성분의 상호관계)

  • Seo, Dae-Shik;Park, Doo-Seok;Han, Jeong-Min
    • Proceedings of the KIEE Conference
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    • 1998.07d
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    • pp.1391-1394
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    • 1998
  • In this paper, we investigated the generation of pretilt for nematic liquid crystal (NLC) in a cell with linearly polarized ultraviolet (UV) light irradiation on polyimide (PI) surface. The pretilt angle of the NLC increases with increasing the incident angle in the cells with S-wave polarized UV light irradiation on PI surface. It is considered that the pretilt angle of the NLC increased due to decreasing the UV light intencity. We suggest that the pretilt angle of the NLC is attributed to asymmetry triangular of the polymer surface with S-wave polarized UV light irradiation on PI surface. Also, we consider that the asymmetry triangular of the Polymer not formed with P-wave polarized UV light irradiation on PI surface. Therefore, the pretilt angle of the NLC is attributed to asymmetry triangular of the polymer surface with UV light irradiation on PI surface.

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Generation of High Pretilt Angle in Liquid Crystal Cell with Slanted Non-Polarized Ultraviolet Light Irradiation on Polyimide Film as for Non-Rubbing Techniques (경사진 자외선을 폴리이미드막 표면에 조사한 넌러방법에 의한 액정소자의 고 프리틸트각의 발생)

  • Seo, Dae-Shik;Hwang, Lyul-Yeon;Lee, Bo-Ho
    • Proceedings of the KIEE Conference
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    • 1997.07d
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    • pp.1585-1587
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    • 1997
  • We investigated the generation of high pretilt angle for nematic liquid crystal (NLC) in the cell with slanted non-polarized ultraviolet (UV) light irradiation on two kinds of the polyimide (PI) film. It was shown that the monodomain alignment in NLC is obtained in the cell with slanted non-polarized UV light irradiation on PI surface. The pretilt angle of NLC is generated about 3 degrees in the cell with slanted non-polarized UV light irradiation with 70 degrees on PI surface without side chain. But, the pretilt angle of NLC is generated about 1 degree in the cell with slanted non-polarized UV light irradiation with 80 degrees on PI surface with side chain. We consider that the pretilt angle generation in NLC is attributted to anisotropic dispersion force between the LC molecular and the PI surface.

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Thermal Stability of Polarized UV Exposed Polyimide Films for Liquid Crystal Display (편광 자외선이 조사된 액정 디스플레이용 폴리이미드 필름의 열 안정성)

  • 김일형;김욱수;하기룡
    • Polymer(Korea)
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    • v.26 no.4
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    • pp.431-438
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    • 2002
  • We studied the orientation behavior and thermal stability of polyimide (PI) molecules under irradiation of polarized UV (PUV) using polarized fourier transform infrared (FTIR) spectroscopy. In the case of PUV-exposed PI films, the remaining PI molecules after photo-degradation showed molecular orientation perpendicular to the irradiated PUV polarization direction predominantly, due to the preferential degradation of PI molecules parallel to the irradiated PUV Polarization direction. On the other hand, the rubbing of PI films induced reorientation of the PI molecules parallel to the rubbing direction. We also investigated the thermal stability of the alignment layers furled by rubbing and PUV irradiation on the PI films using Polarized FTIR. The thermal stability of the PUV irradiated PI alignment layer is lower than that of the rubbed PI layer due to the fragmentation reaction of the PI by PUV.

Generation of valley polarized current in graphene using quantum adiabatic pumping

  • Wang, Jing;Chan, K.S.
    • Advances in nano research
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    • v.3 no.1
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    • pp.39-47
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    • 2015
  • We study a device structure which can be used to generate pure valley current and valley polarized current using quantum adiabatic pumping. The design of the structure allows the flexibility of changing the structure from one for pure valley current generation to one for valley polarized current generation by changing the applied electric potentials through changing the symmetry of the structure. The device is useful for the development of valleytronic devices.

Optical Anisotropy of Polyimide and Polymethacrylate Containing Photocrosslinkable Chalcone Group in the Side Chain under Irradiation of a Linearly Polarized UV Light

  • Choi, Dong-Hoon;Cha, Young-Kwan
    • Bulletin of the Korean Chemical Society
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    • v.23 no.3
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    • pp.469-476
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    • 2002
  • Photocrosslinkable soluble polyimide and polymethacrylate compound were synthesized for studying the optically induced anisotropy of the thin films. Chalcone group was introduced into the side chain unit of two polymers. We observed a photodimerization behavior between the double bonds in the chalcone group and an optical anisotropy of these materials by irradiation of a linearly polarized UV light (LPL). Optical anisotropy of the thin film was also investigated by using polarized UV absorption spectroscopy. The dynamic property of optical anisotropy in photoreactive polyimide was compared to that in polymethacrylate containing chalcone group in the side chain.

Polarized Raman Spectroscopy of Graphene

  • Cheong, Hyeon-Sik
    • Proceedings of the Korean Vacuum Society Conference
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    • 2011.02a
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    • pp.5-5
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    • 2011
  • Raman spectroscopy has become one of the most widely used tools in graphene research. The resonant Raman scattering process that gives rise to the observed strong Raman signal carries information regarding the electronic structure as well as the structural properties. When polarization of the incident excitation laser light or the scattered signal is carefully controlled, more information on the electronic and structural properties becomes available. In this tutorial, the basics of polarized Raman scattering experiments will be introduced first. Then several examples from real research will be highlighted to illustrate the application of polarized Raman spectroscopy in graphene research.

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Modeling Polarized Dust Emission from Aligned Grains by Radiative Torques

  • Lee, Hyeseung;Lazarian, A.;Chepurnov, A.
    • The Bulletin of The Korean Astronomical Society
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    • v.39 no.1
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    • pp.58.1-58.1
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    • 2014
  • We model the polarized dust emission from aligned grains by radiative torques in molecular clouds. We consider various models of molecular clouds and calculate the polarization spectrum from aligned grains by both internal and external radiation fields. We show that some polarization spectrum exhibits the bump at wavelengths ${\lambda}$ < $100{\mu}m$, which can be explained due to the polarized emission from a population of small grains aligned by internal radiation fields. Our polarization spectra can explain the anomalous spectra observed by Hildebrand et al, with the rising polarization toward short wavelengths

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Polarized OLED on a flexible optical anisotropic substrate for mobile display

  • Park, Byoung-Choo;Park, Chan-Hyuk;Kim, Mi-Na;Han, Mi-Young
    • 한국정보디스플레이학회:학술대회논문집
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    • 2009.10a
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    • pp.1523-1526
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    • 2009
  • We present highly polarized light emissions from an OLED on a flexible photonic anisotropic substrate. It was found that the polarization direction of emitted electroluminescent light corresponded to the ordinaryaxis of the photonic anisotropic substrate. Furthermore, it was also found that luminous polarized electroluminescence over 4,500 cd/$m^2$ was produced with high peak efficiency of 6 cd/A and high polarization ratio over 25.

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