• Title/Summary/Keyword: 차폐재료

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CMP Properties of ITO with the deposition temperature (기판온도에 따른 ITO박막의 CMP특성)

  • Choi, Gwon-Woo;Lee, Young-Kyun;Lee, Woo-Sun;Jun, Young-Kil;Ko, Pil-Ju;Seo, Yong-Jin
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2007.11a
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    • pp.165-165
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    • 2007
  • 투명전도박막은 ITO, $SnO_2$, ZnO, 등이 있으나 $SnO_2$는 자외선 영역까지 투과시키는 우수한 광학적 특성을 나타내지만, 상당히 큰 전기저항으로 인해 현재는 현재 ITO가 널리 이용되고 있다. ITO(Indium Tin Oxide)박막은 자외선 영역에서 반사율이 높으며 가시광선영역에서는 80%이상의 뛰어난 투과율을 가지고 있다. 또한 낮은 전기저항과 넓은 광학적 밴드갭 때문에 가장 유용한 투과전도성 재료 중에 하나이다. 이러한 특성 때문에 여러 가지 문자 표시소자의 투명전극, 태양전지의 창재료, 정전차폐를 위한 반도체 포장재료, 열반사막, 면발열체, 광전변환 소자에 응용되고 있다. 일반적으로 박막의 제작에는 저항가열법과 전자선가열법, 스퍼터링법의 물리적 증착과 화학적 증착으로 나뉜다. 본 논문에서는 증착온도를 달리 하여 RF-sputtering에 의해 ITO박막을 증착한 후 온도증가에 따른 박막의 특성을 연구하였으며 또한 광역평탄화를 위한 CMP공정을 적용하여 증착온도가 연마에 미치는 영향을 연구하였다. 본 실험에서 사용된 ITO박막은 $2{\times}2Cm$의 Corning glass위에 증착되었으며 타겟은 $In_2O_3$$SnO_2$가 9:1로 혼합된 Purity 99.99%이상의 직경 2 inch인 ITO타겟을 사용하였다. 박막 증착시 기판온도는 상온에M $200^{\circ}C$까지 변화시켰으며 RF power는 100W로 일정하게 하였으며 증착압력은 $8{\times}10^{-2}$Torr이였다. CMP공정조건은 헤드속도 60rpm, 플레이튼 속도 60rpm, 슬러리 주입 유량 60mml/min, 압력 $300g/cm^2$이였다. 전기적 특성은 four point probe를 이용하여 측정하였으며 광학적 특성은 UV-Visible Spectrometer를 이용하여 200~900nm의 파장범위에서 광투과도를 측정하였다.

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Electric Field Strength and Shielding Effectiveness Comparison According to the Size of Shielding Facility (방호 시설 크기에 따른 전계강도 및 차폐 효과 비교)

  • Kang, Ho-Jae;Huh, Chang-Su;Bang, Jeong-Ju;Choi, Jin-Su;Park, Woo-Chul
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.27 no.4
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    • pp.221-225
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    • 2014
  • In modern times, threat of high power electromagnetic wave is increasing. When the electrical grid and communication network are attacked by these high power electromagnetic wave, the whole infrastructure is paralyzed. To protect the infrastructure from these high power electromagnetic wave threat, the shielding facility that can block high power electromagnetic wave is constructed. Also shielding effectiveness evaluation about the constructed facility is important. But, because of space efficiency and saving of construction cost to construct the actual shielding facility, the shielding room wall is generally adjacent to exterior concrete structures. As space between shielding facility wall and concrete structures is very small, arranging the transmitting antenna exterior shielding facility is realistically difficult. Therefore, in this research, The shielding effectiveness measurement plan in the state of exterior narrow space of HEMP shielding facility is presented. And to apply this plan, The influence of shielding effectiveness according to the size of the shielding facility is analyzed.

A Study on Welding Performance Improvement of $CO_2$ Inverter Arc Welding Machine by Short Circuiting Delay Control and Arc Reignition Detection Control (단락지연제어 및 아크재생검출제어에 의한 $CO_2$ 인버터 아크 용접기의 용접성능향상에 관한 연구)

  • 고재석;김길남;채영민;이승요;이명언;최규하
    • The Transactions of the Korean Institute of Power Electronics
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    • v.7 no.3
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    • pp.272-280
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    • 2002
  • The recent research topics on $CO_2$ arc welding power supplies are focused mainly on the reduction of spatter generation. The method for reducing the spatters can be approached in several ways: finding the new materials fur consumable electrode and shielding gases, researching on the circuit topology and the controller. In this paper, the metal transfer and several control methods for the $CO_2$ GMAW were described. And it was proposed and compared with other schemes that the control method for reducing spatter by controlling the welding current when short-circuit and re-ignition.

The Preparation of Copper Powder Using Solvothermal Process and Its Application as EMI Shielding Agent (솔보써말 방법을 이용한 구리분말 제조 및 전자파 차폐제로의 응용)

  • Lee, Hyo-Won;Kim, Soo-Ryong;Kwon, Woo-Teck;Choi, Duck-Kyun;Kim, Young-Hee
    • Korean Journal of Materials Research
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    • v.16 no.5
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    • pp.285-291
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    • 2006
  • Copper powders have been widely used in electrically conductive coatings, electrode materials et al. and are very prospective since they are cheaper than noble metal powders such as silver or palladium. In this study, copper powders for metal filler of EMI shielding have been prepared using a solvothermal process from $CuSO_4$, NaOH, Glucose, mixed solvent ($H_2O$: Ethanol) and hydrazine which was used as a reducing agent at various reaction conditions. The prepared copper powders showed finely dispersed spherical shape without agglomerate, uniform morphology, narrow size distribution, high purity and were about 400-700 nm in size. The prepared powders were characterized using XRD, SEM, TGA, XPS, particle size measurement and EMI shielding efficiency.

Transparent electrode performance of $TiO_2$/ZnS/Ag/ZnS/$TiO_2$ multi-layer for PDP filter ($TiO_2$/ZnS/Ag/ZnS/$TiO_2$ 다층막의 PDP 필터용 전극 특성)

  • Oh, Won-Seok;Lee, Seo-Hee;Jang, Gun-Eik
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2010.06a
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    • pp.217-217
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    • 2010
  • 산화물유전체/금속/산화물유전체(D/M/D) 구조의 투명전극은 우수한 통전성과 투광성을 갖는 동시에 근적외선 및 전자파 차폐가 가능하여 각종 디스플레이 장치로의 응용을 위해 많은 연구가 진행 중이다. 이러한 구조의 다층막의 경우 금속층과 산화물층간 계면에서의 산소확산으로 인한 광학적, 전기적 특성 저하가 문제가 되고 있다. 본 연구에서는 층간 산소확산방지를 통해 다층막의 전기적 특성을 개선하기 위해 $TiO_2$/Ag/$TiO_2$, $TiO_2$/ZnS/Ag/ZnS/$TiO_2$ 구조의 다층막을 DC/RF 마그네트론 스퍼터를 이용하여 제조하여 ZnS 박막이 다층막의 특성에 미치는 영향을 비교 평가하였다. 제조된 박막의 전기적, 광학적, 계면 특성을 4-point probe, Spctrophotometer, AES을 이용하여 분석하였으며 PDP필터용 전극으로의 적용 가능성을 평가하였다.

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Simultaneous Realization of Electromagnetic Shielding and Antibacterial Effect of Al Doped ZnO Thin Films onto Glass Substrate (유리 기판 위에 증착된 Al Doped ZnO 박막을 이용한 전자파 차폐 및 항균 특성의 동시 구현)

  • Choi, Hyung-Jin;Yoon, Soon-Gil
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.29 no.5
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    • pp.279-283
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    • 2016
  • In this study, we intended to achieve both antibacterial properties and electromagnetic shielding using the Al-doped ZnO (AZO) films. FTS (Facial Target Sputtering) magnetron sputtering was used for the AZO thin films instead of the conventional RF sputtering because the FTS sputtering could avoid the damage for the plasma as well as fabrication of thin films with a high quality. The 300-nm thick AZO thin films grown on glass substrate showed a resistivity of about $7{\times}10^{-4}{\Omega}-cm$ and a transmittance of about 90% at a wavelength of 550 nm. AZO thin films were investigated for the electromagnetic shielding effectiveness measured by 2-port network method at 1.5 ~ 3 GHz. The AZO (300 nm)/glass films showed an EMI shielding effectiveness of approximately 27 dB. An antibacterial effect was measured by the film attachment method (JIS Z 2801). The percent reductions of bacteria by AZO films were 99.99668% and 99.99999% against Staphylococcus aureus and Escherichia coli, respectively.

Analysis on Current Distribution in Multi-layer HTSC Power Cable with Shield Layer (차폐층을 갖는 다층고온초전도 전력케이블의 전류분류 분석)

  • Lee Jong-Hwa;Lim Sung-Hun;Yim Seong-Woo;Du Ho-Ik;Han Byoung-Sung
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.19 no.3
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    • pp.273-279
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    • 2006
  • High-$T_c$ superconducting (HTSC) power cable is one of the interesting parts in power application using HTSC wire. However, its stacked structure makes the current distribution between conducting layers non-uniform due to difference between self inductances of conducting layers and mutual inductances between two conducting layers, which results in lower current transmission capacity of HTSC power cable. In this paper, the transport current distribution between conducting layers was investigated through the numerical analysis for the equivalent circuit of HTSC power cable with a shield layer, and compared with the case of without a shield layer. The transport current distribution due to the increase of the contact resistance in each layer was improved. However, its magnetization loss increased as the contact resistance increased. It was confirmed from the analysis that the shield layer was contributed to the improvement of the current distribution between conducting layers if the winding direction and the pitch length were properly chosen.

A Study on the Electromagnetic shielding Effectiveness Using Conductive Polymers (전도성 고분자를 이용한 전자파 차폐효과의 연구)

  • 하남규;이보현;김태영;김종은;서광석
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.14 no.3
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    • pp.207-214
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    • 2001
  • The conductive polymers, polyaniline (PANI) emeralidin base and 3,4-polyethylene dioxythiophene(PEDOT) were synthesized and coated on the PET film dealt with acryl type primer to study the electromagnetic shielding effectiveness. When both PANI and PEDOT were coated on the PET film dealt with acryl type priemer, their surface properties such as he adhesive increased. For PANI, when blended with the binder such as PMMA, it adhesive and surface hardness increased, too. The visible light transmittance decreased, while the electromagnetic shielding effectiveness increased, when coated thickness of PANI and PEDOT increased. For PANI, the electromagnetic shielding effectiveness increased as its surface resistance decreased. For PANI, when the surface resistance was 140 Ω/$\square$, the shielding effectiveness was found to be 11 dB in the far field, and 13 dB in the near field at 1 GHz. For PEDOT, when the surface resistance was 200 Ω/$\square$, the shielding effectiveness was found to be 3 dB in the far field, and 7dB in the near field.

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Feasibility of the 3D Printing Materials for Radiation Dose Reduction in Interventional Radiology (인터벤션 시술 시 환자의 선량감소를 위한 3D 프린팅 재료의 적용성 평가)

  • Cho, Yong-In
    • Journal of radiological science and technology
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    • v.43 no.3
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    • pp.169-176
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    • 2020
  • Interventional radiology is performed under real-time fluoroscopy, and patients are exposed to a wide range of exposures for a long period of time depending on the examination and procedure. However, studies on radiation protection for patients during an intervention are insufficient. This study aims to evaluate the doses exposed during the intervention and the applicability of 3D printing materials. The organ dose for each intervention site was evaluated using a monte carlo simulatio. Also, the dose reduction effect of the critical organs was calculated when using a shielding device using 3D printing materials. As a result, the organ dose distribution for each intervention site showed a lower dose distribution for organs located far from the x-ray tube. It was analyzed that the influence of scattered rays was higher in the superficial organs of the back of the human body where x-rays were incident. The dose reduction effect on the critical organ using the 3D printing shield showed the highest testis among the gonads, and in the case of other organs, the dose reduction effect gradually decreased in the order of the eye, thyroid, breast, and ovary. Accordingly, it is judged that the 3D printed shield will be sufficiently usable as a shielding device for the radiation protection of critical organs.

White Organic Light-Emitting Diodes Using DCJTB-Doped 24MeSAlq as a New Hole-Blocking Layer (새로운 정공차폐 층 (Hole blocking layer)으로 DCJTB 도핑된 24MeSAlq를 이용한 백색유기발광다이오드)

  • Kim, Mi-Suk;Lim, Jong-Tae;Yeom, Geun-Young
    • Korean Journal of Materials Research
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    • v.16 no.4
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    • pp.231-234
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    • 2006
  • To obtain balanced white-emission and high efficiency of the organic light-emitting diodes (OLEDs), a deep blue emitter made of N,N'-diphenyl-N,N'-bis(1-naphthyl)- (1,1'-biphenyl)-4,4'-diamine (NPB) emitter and a new red emitter made of the Bis(2,4 -dimethyl-8-quinolinolato)(triphenylsilanolato)aluminum(III) (24MeSAlq) doped with red fluorescent 4-(dicyanomethylene)-2-tert-butyl-6-(1,1,7,7-tetramethyljulolidyl-9-enyl)-4H -pyran (DCJTB) were used and the device was tuned by varying the thickness of the DCJTB-doped 24MeSAlq and $Alq_3$. For the white OLED with 10 nm thickness DCJTB (0.5%) doped 24MeSAlq and 45 nm thick $Alq_3$, the maximum luminance of about 29,700 $Cd/m^2$ could be obtained at 14.8 V. Also, Commission Internationale d'Eclairage (CIE) chromaticity coordinates of (0.32, 0.28) at about 100 $Cd/m^2$, which is very close to white light equi-energy point (0.33, 0.33), could be obtained.