• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2002년도 하계학술대회 논문집
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• pp.74-77
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• 2002

The channel of the superconducting Flux Flow Transistor has been fabricated with plasma etching method using ICP. The ICP conditions were 700 W of ICP power, 150 W of rf chuck power, 5 mTorr of the pressure in chamber and 1:1 of Ar : Cl$_2$, respectively. The channel etched by plasma gas showed superconducting characteristics of over 77 K and superior surface morphology. The critical current of SFFT was altered by varying the external applied current. As the external applied current increased from 0 to 12 mA, the critical current decreased from 28 to 22 mA. Then the obtained r$\sub$m/ values were smaller than 0.1Ω at a bias current of 40 mA. The current gain was about 0.5. Output resistance was below 0.2 Ω.

• 분석과학
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• 제15권2호
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• pp.127-134
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• 2002

추출한 유기상 속의 희토류 원소를 유도결합 플라스마 질량분석법(inductively coupled plasma mass spectrometry, ICP-MS)으로 정량하는 방법에 대하여 연구하였다. 희토류 원소를 추출한 유기상의 과다한 도입을 방지하기 위하여 탈용매화장치를 장착한 초음파 분무기를 이용하여 ICP-MS에 주입하였다. 에탄올(EtOH)에 MIBK(methyl isobutyl ketone)를 섞은 용매를 도입하였을때, 계수율(count rate)이 증가하였고, 여기에 0.03 M의 추출제 HEH(2-ethylhexyl-2-ethylhexyl phosphonic acid, P507, PC88A)를 섞었을 때는 감소하였다. 탈용매화장치의 냉각장치(condenser)의 최적온도는 -10 $^{\circ}C$이었고, 가열관(heating tube)의 최적온도는 150 $^{\circ}C$이었다. 계수율이 최대이고, 반사파(reflect power)가 최소인 최적 운반기체의 흐름속도는 0.7 L/min이었다. MIBK에 추출제 HEH가 0.03 M이 섞여있는 추출용매로 추출을 행하였을 때, 최적 pH는 4.3이었고, 추출시간은 10 분이었다. 최적조건에서 0.2 ${\sim}$ 20 ng/mL의 표준용액으로 얻은 검정곡선으로부터 구한 검출 한계는 0.02 ${\sim}$ 0.05 ng/mL 이었다.

• 한국결정성장학회지
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• 제21권6호
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• pp.230-234
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• 2011

$CF_4$ Ar 및 $SF_6$/Ar 유도결합 플라즈마을 이용하여 ZnO 박막의 고이온밀도 플라즈마 식각을 수행하였다. $10CF_4$/5Ar, $10SF_6$/5Ar 유도결합 플라즈마에서 최고 ~1950 ${\AA}$/min과 ~1400 ${\AA}$/min의 식각 속도를 확보하였다. 대부분의 조건 하에서 식각된 ZnO 표면은 식각 전보다 더 낮은 표면조도 값들을 나타내었다. $10CF_4$/5Ar 유도결합 플라즈마에서 Ni mask는 ZnO에 대해 최고 11의 높은 식각 선택도를 나타낸 반면에 Al은 이보다 낮은 1.6~4.7 범위의 식각선택도를 나타내었다.

• 열처리공학회지
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• 제22권5호
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• pp.267-274
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• 2009

Titanium Chromium Nitrided (TiCrN) coatings were deposited on stainless steel 316 L and Si (100) wafer by inductively coupled plasma assisted D.C. magnetron sputtering at the various sputtering power on Cr target and $N_2/Ar$ gas ratio. Increasing the sputtering power of Cr target, XRD patterns were changed from TiCrN to nitride $Cr_2Ti$. The maximum hardness was $Hk_{3g}$ 3900 at $0.3\;N_2/Ar$ gas ratio. The thickness of the TiCrN films increased as the Cr target power increased, and it showed over $Hk_{5g}3100$ hardness at 100 W, 150 W. TiCrN films were deposited by the ICP assisted DC magnetron sputtering shown good wear resistance as the $N_2/Ar$ gas ratio was 0.1, 0.3.

• 한국재료학회지
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• 제23권1호
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• pp.47-52
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• 2013

Graphene has been synthesized on 100- and 300-nm-thick Ni/$SiO_2$/Si substrates with $CH_4$ gas (1 SCCM) diluted in mixed gases of 10% $H_2$ and 90% Ar (99 SCCM) at $900^{\circ}C$ by using inductively-coupled plasma chemical vapor deposition (ICP-CVD). The film morphology of 100-nm-thick Ni changed to islands on $SiO_2$/Si substrate after heat treatment at $900^{\circ}C$ for 2 min because of grain growth, whereas 300-nm-thick Ni still maintained a film morphology. Interestingly, suspended graphene was formed among Ni islands on 100-nm-thick Ni/$SiO_2$/Si substrate for the very short growth of 1 sec. In addition, the size of the graphene domains was much larger than that of Ni grains of 300-nm-thick Ni/$SiO_2$/Si substrate. These results suggest that graphene growth is strongly governed by the direct formation of graphene on the Ni surface due to reactive carbon radicals highly activated by ICP, rather than to well-known carbon precipitation from carbon-containing Ni. The D peak intensity of the Raman spectrum of graphene on 300-nm-thick Ni/$SiO_2$/Si was negligible, suggesting that high-quality graphene was formed. The 2D to G peak intensity ratio and the full-width at half maximum of the 2D peak were approximately 2.6 and $47cm^{-1}$, respectively. The several-layer graphene showed a low sheet resistance value of $718{\Omega}/sq$ and a high light transmittance of 87% at 550 nm.

• 반도체디스플레이기술학회지
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• 제21권3호
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• pp.125-129
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• 2022

The current display technology tends to be highly integrated with high resolution, the element size is gradually downsized, and the structure becomes complicated. Inductively coupled plasma (ICP) dry etcher of various types of etching equipment is a structure that places a large multi-divisional antenna source on the top lid, passes current to the Antenna, and generates plasma using the induced magnetic field generated at this time. However, in the case of a device of a large area size, a support that can withstand a load structurally is necessary, and when these support portions are applied, arrangement of antenna becomes difficult, which causes reduction in uniformity. As described above, the development of antenna source of a large area having a uniform plasma density on the whole surface is difficult to restrict hardware (H/W). As a solution to this problem, we confirmed the change in uniformity of plasma by applying two kinds of specific shape faraday shield(FICP) to the lower part of the large area upper lid antenna of 6 and 8th more than that generation size. In this thesis, we verify the faraday shield effect which can improve plasma uniformity control of ICP dry etcher equipment applied to medium and large displays.

• 반도체디스플레이기술학회지
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• 제18권2호
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• pp.98-102
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• 2019

Direct plasma-enhanced atomic layer deposition (PEALD) are widely used for $SiO_2$ and SiON thin film process in current semiconductor industry. However, this exhibits poor step coverage for three-dimensional device structure due directionality of plasma species as well as plasma damage on the substrate. In this study, to overcome this issue, low temperature (< $300^{\circ}C$) $SiO_2$ and SiON thin film processes were studied using inductively coupled plasma (ICP) type remote PEALD with various reactant gases such as $O_2$, $H_2O$, $N_2$ and $NH_3$. It was confirmed that the interfacial properties such as fixed charge density and charge trapping behavior of thin films were considerably improved by hydrogen species in $H_2O$ and $NH_3$ plasma compared to the films grown with $O_2$ and $N_2$ plasma. Furthermore, the leakage current density of the thin films was suppressed for same reason.

• 대한화학회지
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• 제43권2호
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• pp.182-192
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• 1999

글로우 방전(Glow Discharge, GD)과 유도결합플라스마(Inductively Coupled Plasma, ICP)-원자 방출분광법(Atomic Emission Spectrometer, AES)에서 사용되는 새로운 장치를 개발하였다. ICP-AES에서 GDAES로 전환하는 데 불과 15분 정도 소요되기 때문에, 고체 시료 및 액체시료에 포함된 극미량 원소분석을 신속하게 수행할 수 있다. 실험변수 중에서 냉각기체 유속, 시료운반기체 유속, 절단기체 유속, 보조기체 유속, 측정깊이, 이온 통과관 크기, 그리고 rf 전원의 세기 변화에 따른 원자 방출 복사선 변화에 미치는 영향을 조사 연구하였다. Cd(I) 228.8 nm, Mn(II) 257.61 nm, and Fe(II) 259.95 nm에서 측정한 검출한계는 각각 3.86, 1.49, 5.79 ppb로 측정되었으며, 직선성은 1.000으로서 우수하였다.

• 조명전기설비학회논문지
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• 제20권8호
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• pp.6-14
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• 2006

본 논문은 TFT-LCD(Thin Film Transistor Liquid Crystal Display) PECVD(Plasma Enhanced Chemical Vapor Deposition) 장비 공정용 챔버(Chamber) 세정을 위한 새로운 플라즈마 세정방법에 적합한 플라즈마 발생방법과 플라즈마 발생을 위한 고주파 전원장치의 전력회로에 관한 연구이다. 세정에 요구되는 고밀도 플라즈마는 안테나 형태의 기존 ICP(Inductively Coupled Plasma) 방식에 강자성체인 페라이트 코어를 적용하므로 써 $1{\times}10^{11}[EA/cm^3]$이상의 고밀도 플라즈마 발생을 가능하게 하였다. 플라즈마 발생을 위한 400[kHz] 고주파 전력 변환장치의 경우 범용 HB(Half Bridge) 인버터 방식을 적용하여 플라즈마 부하에서도 안정적인 영전압 스위칭 동작을 확인 하였다. 변압기 직렬결합 방식을 사용한 10[kW] 고출력을 통해 $A_r$과 $NF_3$가스 분위기하에서 플라즈마의 밀도와 $NF_3$가스 분해율을 측정하므로서 고주파 전력 변환 장치의 성능을 입증하였다.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2009년도 제36회 동계학술대회 초록집
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• pp.272.2-272.2
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• 2009