• Title/Summary/Keyword: Ar/N_2\

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Properties of the Amorphous Silicon Microbolometer using PECVD (PECVD 이용한 비정질 실리콘형 마이크로 볼로미터 특성)

  • Kang, Tai Young;Kim, Kyung Hwan
    • Journal of the Semiconductor & Display Technology
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    • v.11 no.4
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    • pp.19-23
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    • 2012
  • We report microbolometer characteristic with n-type and p-type amorphous silicon thin film. The n-type and p-type amorphous silicon thin films were made by PECVD. The electrical properties of n-type and p-type a-Si:H thin films were investigated as a function of doping gas flow rate. The doping gas used $B_2H_6/Ar$ (1:9) and $PH_3/Ar$ (1:9). In general, the conductivity of doping a-Si:H thin films increased as doping gas increase but the conductivity of a-Si:H thin films decreased as the doping gas increase because doping gas concentration increase led to dilution gas (Ar) increase as the same time. We fabricated an amorphous silicon microbolometer using surface micromachining technology. The fabricated microbolometer had a negative TCR of 2.3%. The p-type microbolometer had responsivity of $5{\times}10^4V/W$ and high detectivity of $3{\times}10^8cm(Hz)^{1/2}/W$. The p-type microbolometer had more detectivity than n-type for less noise value.

Fabrication of Tantalum Nitride Thin-Film as High-temperature Strain Gauges (고온 스트레인 게이지용 질화탄탈박막의 제작)

  • 최성규;나경일;남효덕;정귀상
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2001.07a
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    • pp.1022-1025
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    • 2001
  • This paper presents the characteristics of TaN thin-film as high-temperature strain gauges, which were deposited on Si substrate by DC reactive magnetron sputtering in an argon-nitrogen atmosphere(Ar-(4∼20%)N$_2$). The electrical and mechanical characteristics of these films investigated with the thickness range 1650∼1870${\AA}$ and room temperature resistivities in the range 178.3 ${\mu}$$\Omega$cm to 3175.7 ${\mu}$$\Omega$cm. The TaN thin-film strain gauge deposited in Ar-(20%)N$_2$atmosphere is obtained a temperature coefficient of resistance(TCR), 0∼-1357 ppm/$^{\circ}C$ in the temperature range 25∼275$^{\circ}C$ and a high temporal stability with a longitudinal gauge factor, 2.92∼3.47. Because of their high resistivity, low TCR and linear gauge factor, these cermet thin-film may allow high-temperature strain gauges miniaturization.

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Surface Modification of Polytetrafluoroethylene by 1 keV Argon and Hydrogen Irradiated in Nitrogen and Ammonia Gas Environment (질소와 암모니아 존재하에서 1 keV 에너지의 알곤과 수소 이온 조사에 의한 PTFE(polytetrafluoroethylene)의 표면형상 변화연구)

  • Yeu, Dae-Hwan;Kim, Ki-Hwan;Kang, Dong-Yeob;Kim, Joong-Soo;Koh, Seok-Keun;Kim, Hyun-Joo
    • Korean Journal of Materials Research
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    • v.16 no.6
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    • pp.367-372
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    • 2006
  • Polytetrafluoroethylene (PTFE) surface was modified for improving hydrophilicity by ion irradiation in environmental gas of $N_2$ and $NH_3$, respectively. The water contact angle onto the PTFE surface increased from $104{\circ}$ to over $140{\circ}$ by Ar ion irradiation in $N_2$ gas. In the case of $NH_3$ as environmental gas, there were a slight increase of contact angle from ion dose of $1{\times}10^{15}\;to\;5{\times}10^{15}\;ions/cm^2$, and its dramatic decrease to the value of 35o at the conditions of ion dose higher than $1{\times}10^{16}\;ions/cm^2$. It was found from SEM results that the surface morphology of PTFE was changed into one with filament structure after Ar ion irradiation in $N_2$ gas environments. On the contrary, Ar ion irradiation in $NH_3$ gas condition induced the PTFE surface with network structure. Hydrogen ion irradiation resulted in a little change of PTFE surface morphology, comparing with the case of Ar ion irradiation. The water contact angle of hydrogen ion irradiated PTFE surface in reactive gas decreased with increment of ion dose. Hydrogen ion irradiation could improve hydrophilicity with little change of surface morphology. It might be considered from FT-IR results that the improvement in wettability of PTFE surface by ion irradiation in $N_2$ and $NH_3$ gases could be due to the hydrophilic groups of NHx bonds.

Ion assisted deposition of $TiO_2$, $ZrO_2$ and $SiO_xN_y$ optical thin films

  • Cho, H.J.;Hwangbo, C.K.
    • Journal of the Korean Vacuum Society
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    • v.6 no.S1
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    • pp.75-79
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    • 1997
  • Optical and mechanical characteristics of $TiO-2, ZrO_2 \;and\; SiO_xN_y$ thin films prepared by ion assisted deposition (IAD) were investigated. IAD films were bombarded by Ar or nitrogen ion beam from a Kaufman ion source while they were grown in as e-beam evaporator. The result shows that the Ae IAD increases the refractive index and packing density of $TiO_2 films close to those of the bulk. For $ZrO_2$ films the Ar IAD increases the average refractive index decreases the negative inhomogeneity of refractive index and reverses to the positive inhomogeneity. The optical properties result from improved packing density and denser outer layer next to air The Ar-ion bombardment also induces the changes in microstructure of $ZrO_2$ films such as the preferred (111) orientation of cubic phase increase in compressive stress and reduction of surface roughness. Inhomogeneous refractive index SiOxNy films were also prepared by nitrogen IAD and variable refractive index of $SiO_xN_y$ film was applied to fabricate a rugate filter.

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Characteristics of Crystalline Silicon Solar Cells with Double Layer Antireflection Coating by PECVD (결정질 실리콘 태양전지의 이중 반사방지막 특성에 대한 연구)

  • Kim, Jin-Kuk;Park, Je-Jun;Hong, Ji-Hwa;Kim, Nam-Soo;Kang, Gi-Hwan;Yu, Gwon-Jong;Song, Hee-Eun
    • 한국태양에너지학회:학술대회논문집
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    • 2012.03a
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    • pp.243-247
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    • 2012
  • The paper focuses on an anti-reflection (AR) coating deposited by PECVD in silicon solar cell fabrication. AR coating is effective to reduce the reflection of the light on the silicon wafer surface and then increase substantially the solar cell conversion efficiency. In this work, we carried out experiments to optimize double AR coating layer with silicon nitride and silicon oxide for the silicon solar cells. The p-type mono crystalline silicon wafers with $156{\times}156mm^2$ area, 0.5-3 ${\Omega}{\cdot}cm$ resistivity, and $200{\mu}m$ thickness were used. All wafers were textured in KOH solution, doped with $POCl_3$ and removed PSG before ARC process. The optimized thickness of each ARC layer was calculated by theoretical equation. For the double layer of AR coating, silicon nitride layer was deposited first using $SiH_4$ and $NH_3$, and then silicon oxide using $SiH_4$ and $N_2O$. As a result, reflectance of $SiO_2/SiN_x$ layer was lower than single $SiN_x$ and then it resulted in increase of short-circuit current and conversion efficiency. It indicates that the double AR coating layer is necessary to obtain the high efficiency solar cell with PECVD already used in commercial line.

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The characterization of AlN thin films grown on GaAs(100) substrate (GaAs(100) 기판위에 성장된 AIN 박막의 특성)

  • 정성훈;김영호;송복식;문동찬;김선태
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 1996.11a
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    • pp.33-36
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    • 1996
  • AIN thin films were prepared using by Rf sputtering method on the GaAs(170) substrate and investigated by X-ray diffractometer, IR spectroscopy, n&k system. The parameters were the substrate temperature, RF power, sputtering duration and the $N_2$/Ar ratio. The AlN thin films of (101) orientation were obtained under the conditions of room temperature and the nitrogen of 60 vol.%. The crystallinity of the films, which were grown respectively under the different conditions, were determined by the comparison of the band width of an E$_1$[TO:680$cm^{-1}$ /] phonon mode. The thicknesses of AlN films were decreased dramatically in the region of the nitrogen of 40~60 vol.% according to the increment of the $N_2$/Ar ratio by which the sputter yield got lower.

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Processing and Characterization of RF Magnetron Sputtered TiN Films on AISI 420 Stainless Steel (AISI 420 stainless steel 기판위에 D.C magnetron sputtering 법으로 제조한 TiN 박막의 특성 평가)

  • Song, Seung-Woo;Choe, Han-Cheol;Kim, Young-Man
    • Journal of the Korean institute of surface engineering
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    • v.39 no.5
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    • pp.199-205
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    • 2006
  • Titanium nitride (TiN) coatings were produced on AISI 420 stainless steel by DC magnetron sputtering of a Ti target changing the processing variables, such as the flow rate of $N_2/Ar$, substrate temperature and the existence of Ti interlayer between TiN coatings and substrates. The hardness and residual stress in the films were investigated using nanoindentation and a laser scanning device, respectively. The stoichiometry and surface morphology were investigated using X-Ray Diffraction and SEM. The corrosion property of the films was also studied using a polarization method in NaCl (0.9%) solution. Mechanical properties including hardness and residual stress were related to the ratio of $N_2/Ar$ flow rate. The corrosion resistance also was related to the processing variables.

Electron Collision Cross Section of Electron Transport Coefficients in Hydrogen-Argon Mixtures ($H_2$ + Ar 혼합기체의 전자수송계수에서의 전자충돌 단면적)

  • Jo, Doo-Yong;Phan, Thi Lan;Jeon, Byung-Hoon
    • Proceedings of the KIEE Conference
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    • 2011.07a
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    • pp.1540-1541
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    • 2011
  • We calculated the electron transport coefficients in $H_2$+Ar gas calculated E/N values 0.01 ~ 1 Td by the Boltzmann equation method. This study gained the values of the electron swarm parameters such as the electron drift velocity and the transverse diffusion coefficients for $H_2$+Ar gas at a range of E/N. The transport coefficient W and Dt/u have been calculated in mixtures of 0.5% and 4% hydrogen in argon. All values were made at 293 K.

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Characteristics of ITO with surface treatment by N2, O2, Ar Plasma and UV (질소, 산소, 아르곤 플라즈마와 자외선에 의하여 표면 처리한 ITO의 특성)

  • Bae, Gyeong-Tae;Jeong, Seon-Yeong;Gang, Seong-Ho;Kim, Hyeon-Gi;Kim, Byeong-Jin;Ju, Seong-Hu
    • Proceedings of the Korean Institute of Surface Engineering Conference
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    • 2018.06a
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    • pp.90-90
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    • 2018
  • 디스플레이는 다수의 가로 전극과 세로 전극으로 구성되고, 전극에 신호를 주어 동작하도록 하는 원리이다. 이 디스플레이에는 전기가 통하고 투명한 전극이 필수적으로 사용되고 있고, 대표적인 투명 전극으로 ITO (Indium Tin Oxide)가 있다. ITO 박막은 $In_2O_3$에 Sn을 첨가하여 $Sn^{4+}$ 이온이 $In^{3+}$ 이온을 치환하고 이 과정에서 잉여 전자가 전기전도에 기여하는 구조이다. ITO 박막은 표면 처리 방법에 따라 표면 상태가 크게 변화한다. 플라즈마를 이용한 표면 처리는 환경오염이 적으며 강도, 탄성률 등과 같은 재료의 기계적 특성을 변화시키지 않으면서 표면 특성만을 변화시킬 수 있는 방법으로 알려져 있다[1]. UV (Ultraviolet)를 조사한 표면처리는 ITO 표면의 탄소를 제거하고, 표면 쌍극자를 형성하며, 표면의 조성을 변화시킬 수 있으며, 페르미 에너지 준위를 이동시킬 수 있어 ITO의 일함수를 증가시킬 수 있다[2]. ITO에 대한 다양한 연구가 수행되었음에도 불구하고 보다 다양한 관점에서의 연구가 지속될 필요가 있다. 따라서 본 연구에서는 다양한 조건으로 표면 처리한 ITO 표면의 일함수, 면저항, 표면 형상, 평탄도, 접촉각 등에 대해 알아보고자 한다. 세정한 ITO, 세정 후 UV 처리한 ITO (UV 처리 시간 2분, 4분 6분, 8분), 세정 후 $N_2$, $O_2$, Ar의 공정 가스를 사용하여 Plasma 처리한 ITO로 표면 처리 조건을 변화하였다. 표면 처리한 ITO의 특성은 Kelvin Probe를 이용한 일함수, 물방울 형상의 각도를 측정한 접촉각, AFM (Atomic Force Microscope)을 이용한 평탄도, 가시광선 (380~780 nm) 파장에 대한 투과도와 면저항을 측정하였다. 접촉각은 세정한 ITO의 경우 $45.5^{\circ}$에서 세정 후 UV를 조사한 ITO의 경우 UV 8분 조사 시 $27.86^{\circ}$로 감소하였고, $N_2$, $O_2$, Ar 가스를 사용하여 Plasma 처리한 ITO는 모두 $10^{\circ}$ 미만을 나타내었다. 플라즈마 처리에 의하여 접촉각이 현저하게 개선되었다. ITO의 면저항은 표면 처리 조건에 따라 $9.620{\sim}9.903{\Omega}/{\square}$로 그 차이가 매우 적어 표면처리에 의하여 면저항의 변화는 없는 것으로 판단된다. 가시광선 영역에서의 투과도는 공정 조건에 따라 87.59 ~ 89.39%로 그 차이가 적어 표면처리에 의한 변화를 나타내지는 않은 것으로 판단된다. 표면 처리 조건에 따른 평탄도 $R_{rms}$는 세정한 ITO의 경우 4.501 nm로부터 UV 2, 4, 6, 8분 처리한 경우 2.797, 2.659, 2.538, 2.584 nm로 평탄도가 개선되었다. $N_2$, $O_2$, Ar 가스를 사용하여 플라즈마 처리한 ITO의 경우 평탄도 $R_{rms}$는 2.49, 4.715, 4.176 nm로 사용한 가스의 종류에 따라 다른 경향을 나타내었다. 표면 처리 조건에 따른 평탄도 Ra는 세정한 ITO의 경우 3.521 nm로부터 UV 2, 4, 6, 8분 처리한 경우 1.858, 1.967, 1.896, 1.942 nm를, $N_2$, $O_2$, Ar 가스를 사용하여 플라즈마 처리한 ITO의 경우는 1.744, 3.206, 3.251 nm로 평탄도 $R_{rms}$와 유사한 경향을 나타내었다.

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A Study on the Orientation and the Roughness with the Deposition Condition of AIN Thin Films Prepared by RF Magnetron Sputtering Method (RF 마그네트론 스퍼터링법에 의해 합성된 AIN 박막의 공정조건에 따른 우선 배향성 및 평탄성에 관한 연구)

  • Lee, Min-Geon;Chang, Dong-Hoon;Kang, Seong-Jun;Yoon, Yung-Sup
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.17 no.10
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    • pp.1023-1028
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    • 2004
  • We fabricated AIN thin film by using RF magnetron sputtering and studied the structural characteristic of AIN thin film with the change of the deposition conditions such as Ar/$N_2$ flow ratio, working pressure, and the distance between substrate and target. The orientation and surface roughness of AIN thin film were studied by using XRD and AFM. We can not identify the orientation of the thin film deposited in Ar, while we obtained the (l00) orientation of the thin film with the addition of $N_2$. Especially, the thin film deposited at 18/2 (seem) of Ar/$N_2$ flow ratio exhibited to be the most (100) oriented. The (100) orientation of thin film becomes weaker as the working pressure becomes higher. The further distance between substrate and target is stronger the (100) orientation of the thin film, but the (100) orientation becomes weaker and (002) orientation started to appear as the distance is shorter. The surface roughness of the thin film deposited at 50$0^{\circ}C$ in Ar only is 1.1 nm, while very smooth thin film of 0.4~0.6 nm is obtained with the addition of $N_2$.