• Title/Summary/Keyword: RF Plasma

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Application of Si3N4 Thin Film as a Humidity Protection Layer for Organic Light Emitting Diode (Si3N4 박막의 유기발광소자 수분침투 방지막으로의 응용)

  • Kim, Chang-Jo;Shin, Paik-Kyun
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.23 no.5
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    • pp.397-402
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    • 2010
  • In this paper, we studied WVTR(water vapor transmission rate) properties of $Si_3N_4$ thin film that was deposited using TCP-CVD (transformer coupled plasma chemical vapor deposition) method for the possibility of OLED(organic light emitting diode) encapsulation. Considering the conventional OLED processing temperature limit of below $80^{\circ}C$, the $Si_3N_4$ thin films were deposited at room temperature. The $Si_3N_4$ thin films were prepared with the process conditions: $SiH_4$ and $N_2$, as reactive gases; working pressure below 15 mTorr; RF power for TCP below 500 W. Through MOCON test for WVTR, we analyzed water vapor permeation per day. We obtained that WVTR property below 6~0.05 gm/$m^2$/day at process conditions. The best preparation condition for $Si_3N_4$ thin film to get the best WVTR property of 0.05 gm/$m^2$/day were $SiH_4:N_2$ gas flow rate of 10:200 sccm, working pressure of 10 mTorr, working distance of 70 mm, TCP power of 500 W and film thickness of 200 nm. respectively. The proposed results indicates that the $Si_3N_4$ thin film could replace metal or glass as encapsulation for flexible OLED.

Effects of Carbon Nitride Surface Layers and Thermal Treatment on Field-Emission and Long-Term Stability of Carbon Nanotube Micro-Tips (질화탄소 표면층 및 열처리가 탄소 나노튜브 미세팁의 전계방출 및 장시간 안정성에 미치는 영향)

  • Noh, Young-Rok;Kim, Jong-Pil;Park, Jin-Seok
    • Journal of the Semiconductor & Display Technology
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    • v.9 no.1
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    • pp.41-47
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    • 2010
  • The effects of thermal treatment on CNTs, which were coated with a-$CN_x$ thin film, were investigated and related to variations of chemical bonding and morphologies of CNTs and also properties of field emission induced by thermal treatment. CNTs were directly grown on nano-sized conical-type tungsten tips via the inductively coupled plasma-chemical vapor deposition (ICP-CVD) system, and a-$CN_x$ films were coated on the CNTs using an RF magnetron sputtering system. Thermal treatment on a-$CN_x$ coated CNT-emitters was performed using a rapid thermal annealing (RTA) system by varying temperature ($300-700^{\circ}C$). Morphologies and microstructures of a-$CN_x$/CNTs hetero-structured emitters were analyzed by FESEM and HRTEM. Chemical composition and atomic bonding structures were analyzed by EDX, Raman spectroscopy, and XPS. The field emission properties of the a-$CN_x$/CNTs hetero-structured emitters were measured using a high vacuum (below $10^{-7}$ Torr) field-emission measurement system. For characterization of emission stability, the fluctuation and degradation of the emission current were monitored in terms of operation time. The results were compared with a-$CN_x$ coated CNT-emitters that were not thermally heated as well as with the conventional non-coated CNT-emitters.

Laser patterning process for a-Si:H single junction module fabrication (레이저 가공에 의한 비정질 실리콘 박막 태양전지 모듈 제조)

  • Lee, Hae-Seok;Eo, Young-Joo;Lee, Heon-Min;Lee, Don-Hee
    • 한국신재생에너지학회:학술대회논문집
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    • 2007.11a
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    • pp.281-284
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    • 2007
  • Recently, we have developed p-i-n a-Si:H single junction thin film solar cells with RF (13.56MHz) plasma enhanced chemical vapor deposition (PECVD) system, and also successfully fabricated the mini modules ($>300cm^2$), using the laser patterning technique to form an integrated series connection. The efficiency of a mini module was 7.4% ($Area=305cm^2$, Isc=0.25A, Voc=14.74V, FF=62%). To fabricate large area modules, it is important to optimise the integrated series connection, without damaging the cell. We have newly installed the laser patterning equipment that consists of two different lasers, $SHG-YVO_4$ (${\lambda}=0.532{\mu}m$) and YAG (${\lambda}=1.064{\mu}m$). The mini-modules are formed through several scribed lines such as pattern-l (front TCO), pattern-2 (PV layers) and pattern-3 (BR/back contact). However, in the case of pattern-3, a high-energy part of laser shot damaged the textured surface of the front TCO, so that the resistance between the each cells decreases due to an incomplete isolation. In this study, the re-deposition of SnOx from the front TCO, Zn (BR layer) and Al (back contact) on the sidewalls of pattern-3 scribed lines was observed. Moreover, re-crystallization of a-Si:H layers due to thermal damage by laser patterning was evaluated. These cause an increase of a leakage current, result in a low efficiency of module. To optimize a-Si:H single junction thin film modules, a laser beam profile was changed, and its effect on isolation of scribed lines is discussed in this paper.

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Microfabrication of Submicron-size Hole on the Silicon Substrate using ICP etching

  • Lee, J.W.;Kim, J.W.;Jung, M.Y.;Kim, D.W.;Park, S.S.
    • Proceedings of the Korean Vacuum Society Conference
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    • 1999.07a
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    • pp.79-79
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    • 1999
  • The varous techniques for fabrication of si or metal tip as a field emission electron source have been reported due to great potential capabilities of flat panel display application. In this report, 240nm thermal oxide was initially grown at the p-type (100) (5-25 ohm-cm) 4 inch Si wafer and 310nm Si3N4 thin layer was deposited using low pressure chemical vapor deposition technique(LPCVD). The 2 micron size dot array was photolithographically patterned. The KOH anisotropic etching of the silicon substrate was utilized to provide V-groove formation. After formation of the V-groove shape, dry oxidation at 100$0^{\circ}C$ for 600 minutes was followed. In this procedure, the orientation dependent oxide growth was performed to have a etch-mask for dry etching. The thicknesses of the grown oxides on the (111) surface and on the (100) etch stop surface were found to be ~330nm and ~90nm, respectively. The reactive ion etching by 100 watt, 9 mtorr, 40 sccm Cl2 feed gas using inductively coupled plasma (ICP) system was performed in order to etch ~90nm SiO layer on the bottom of the etch stop and to etch the Si layer on the bottom. The 300 watt RF power was connected to the substrate in order to supply ~(-500)eV. The negative ion energy would enhance the directional anisotropic etching of the Cl2 RIE. After etching, remaining thickness of the oxide on the (111) was measured to be ~130nm by scanning electron microscopy.

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Thermoelectric properties of individual PbTe nanowires grown by a vapor transport method

  • Lee, Seung-Hyun;Jang, So-Young;Lee, Jun-Min;Roh, Jong-Wook;Park, Jeung-Hee;Lee, Woo-Young
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2009.04b
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    • pp.7-7
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    • 2009
  • Lead telluride (PbTe) is a very promising thermoelectric material due to its narrow band gap (0.31 eV at 300 K), face-centered cubic structure and large average excitonic Bohr radius (46 nm) allowing for strong quantum confinement within a large range of size. In this work, we present the thermoelectric properties of individual single-crystalline PbTe nanowires grown by a vapor transport method. A combination of electron beam lithography and a lift-off process was utilized to fabricate inner micron-scaled Cr (5 nm)/Au (130 nm) electrodes of Rn (resistance of a near electrode), Rf (resistance of a far electrode) and a microheater connecting a PbTe nanowire on the grid of points. A plasma etching system was used to remove an oxide layer from the outer surface of the nanowires before the deposition of inner electrodes. The carrier concentration of the nanowire was estimated to be as high as $3.5{\times}10^{19}\;cm^{-3}$. The Seebeck coefficient of an individual PbTe nanowire with a radius of 68 nm was measured to be $S=-72{\mu}V/K$ at room temperature, which is about three times that of bulk PbTe at the same carrier concentration. Our results suggest that PbTe nanowires can be used for high-efficiency thermoelectric devices.

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Effect of Si3N4 Buffer Layer on Transmittance of TiO2/Si3N4/Ag/Si3N4/TiO2 Multi Layered Structure (TiO2/Si3N4/Ag/Si3N4/TiO2 다층구조에서 Si3N4 버퍼층이 투과율에 미치는 영향)

  • Lee, Seo-Hee;Jang, Gun-Eik
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.25 no.1
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    • pp.44-47
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    • 2012
  • The $TiO_2/Si_3N_4/Ag/Si_3N_4/TiO_2$ multi layered structure was designed for the possible application of transparent electrodes in PDP (Plasma Display Panel). Multi layered film was deposited on a glass substrate at room temperature by DC/RF magnetron sputtering system and EMP (Essential Macleod Program) was adopted to optimize the optical characteristics of film. During the deposition process, the Ag layer in $TiO_2/Ag/TiO_2$ became heavily oxidized and the filter characteristic was degraded easily. In thus study, Si3N4 layer was used as a diffusion buffer layer between $TiO_2$ and Ag. in order to prevent the oxidation of Ag layer in $TiO_2/Si_3N_4/Ag/Si_3N_4/TiO_2$ structure. It was confirmed that $Si_3N_4$ layer is one of candidate materials acting as diffusin barrier between $TiO_2/Ag/TiO_2$.

Physical properties and electrical characteristic analysis of silicon nitride deposited by PECVD using $N_2$ and $SiH_4$ gases ($N_2$$SiH_4$ 가스를 사용하여 PECVD로 증착된 Silicon Nitride의 물성적 특성과 전기적 특성에 관한 연구)

  • Ko, Jae-Kyung;Kim, Do-Young;Park, Joong-Hyun;Park, Sung-Hyun;Kim, Kyung-Hae;Yi, Jun-Sin
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2002.05c
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    • pp.83-87
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    • 2002
  • Plasma enhanced chemical vapor deposited (PECVD) silicon nitride ($SiN_X$) is widely used as a gate dielectric material for the hydrogenated amorphous silicon(a-Si:H) thin film transistors (TFT's). We investigated $SiN_X$ films were deposited PECVD at low temperature ($300^{\circ}C$). The reaction gases were used pure nitrogen and a helium diluted of silane gas(20% $SiH_4$, 80% He). Experimental investigations were carried out with the variation of $N_2/SiH_4$ flow ratios from 3 to 50 and the rf power of 200 W. This article presents the $SiN_X$ gate dielectric studies in terms of deposition rate, hydrogen content, etch rate and C-V, leakage current density characteristics for the gate dielectric layer of thin film transistor applications. Electrical properties were analyzed through high frequency (1MHz) C-V and current-voltage (I-V) measurements. The thickness and the refractive index on the films were measured by ellipsometry and chemical bonds were determined by using an FT-IR equipment.

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The Characteristics of (Ba,Sr)$TiO_3$ Thin Films Etched With The high Density $BCl_3/Cl_2$/Ar Plasma ($BCl_3/Cl_2$/Ar 고밀도 플라즈마에서 (Ba,Sr)$TiO_3$ 박막의 식각 특성에 관한 연구)

  • Kim, Seung-Bum;Kim, Chang-Il
    • Proceedings of the KIEE Conference
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    • 1999.11d
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    • pp.863-866
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    • 1999
  • (Ba,Sr)$TiO_3$ thin films have attracted groat interest as new dielectric materials of capacitors for ultra-large-scale integrated dynamic random access memories (ULSI-DRAMs) such as 1 Gbit or 4 Gbit. In this study, inductively coupled $BCl_3/Cl_2$/Ar plasmas was used to etch (Ba,Sr)$TiO_3$ thin films. RF power/dc bias voltage = 600 W/-250 V and chamber pressure was 10 mTorr. The $Cl_2/(Cl_2+Ar)$ was fixed at 0.2, the (Ba,Sr)$TiO_3$ thin films were etched adding $BCl_3$. The highest (Ba,Sr)$TiO_3$ etch rate is 480$\AA/min$ at 10 % $BCl_3$ adding to $Cl_2$/Ar. The characteristics of the plasmas were estimated using optical emission spectroscopy (OES). The change of Cl, B radical density measured by OES as a function of $BCl_3$ percentage in $Cl_2$/Ar. The highest Cl radical density was shown at the addition of 10% $BCl_3$ to $Cl_2$/Ar. To study on the surface reaction of (Ba,Sr)$TiO_3$ thin films was investigated by XPS analysis. Ion enhancement etching is necessary to break Ba-O bond and to remove $BaCl_2$. There is a little chemical reaction between Sr and Cl, but Sr is removed by physical sputtering. There is a chemical reaction between Ti and Cl, and Tic14 is removed with ease. The cross-sectional of (Ba,Sr)$TiO_3$ thin film was investigated by scanning electron microscopy (SEM), the etch slope is about $65\;{\sim}\;70$.

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Characteristics of InGaN/GaN Quantum Well Structure Grown by MBE

  • 윤갑수;김채옥;박승호;원상현;정관수;엄기석
    • Proceedings of the Korean Vacuum Society Conference
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    • 1998.02a
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    • pp.110-110
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    • 1998
  • GaN는 직접천이형 에너지 캡을 가지며 In과 화합물을 형성할 경우 1.geV-3.4eV까지 다양한 에너지 캡을 가지므로 청색 발광소자 고출력소자 고온 전자소자둥 웅용성이 많 은 물절로서 각광을 받고 있다. 그러나 G랴‘에 적합한 기판이 없다는 문제점으로 인하여 F FET, LD와 같은 다양한 구조의 웅용에 제 약이 따랐다. 이에 본 연구에서는 RF(radio frequency) Plasma-Assisted MBE( molecular beam e epitaxy )를 이용하여 InxGaj xN/G암J 양자우물 구조를 성장하였다. 이렇게 성장된 I InxGaj xN 박막과 InxGaj xN/GaN 양자우물구조의 특성의 분석은 광학적 특성올 PL( p photoluminescence ) , 결 정 성 의 분석 은 XRD ( x-ray diffraction ), 표면 과 단변 의 계 변 특성은 SEM(scanning electron microscopy)을 이용하여 분석하였다. 저온 PL의 측정결 과 기판온도를 680$^{\circ}$C로 고정한 후 In cell의 온도를 650$^{\circ}$C에서 775$^{\circ}$C까지 증가함에 따라 I InxGaj xN에 관계된 피크위치가 약3이neV정도 red shift 함을 관찰할 수 있었다. 한편 I InxGaj xN/GaN 양자우물구조의 경우 PL피크가 3.2없eV로써 InxGaj- xN의 PL 피크에 비 해 에서 약 25me V 고에너지 이동이 관측되었으며 이것은 우불 내에서 에너지레벨의 c confinement효과에 의해 에너지의 변화에 의한 것엄올 확인하였으며, 양자우물 구조에서 우물의 두께를 줄임에 따라 변화 폭은 1이neV정도 고에너지 이동을 관찰할 수 있었다. X XRD 측정의 결과 In의 mole fraction에 따라 격자상수의 변화를 관찰하였으며, 결정 성의 변화를 피크의 세기로 관찰하였다 .. XRD로 판단한 In의 mole fraction은 0.2임을 알 았다 .. SEM 측정은 표변과 단면의 측정으로서 표연특성과 단면의 특성을 InxGaj xN, I InxGaj xN/GaN 양자우물 구조 모두 알아보았다. 측정 결과 InxGaj-xN의 성 장조건으로 기판온도가 낮아지면서 표면의 거칠기 정도가 증가하였으며,680$^{\circ}$C의 기판온도에서 성장 한 양자우물 구조에 있어서 매끄라운 표면올 얻올 수 있었다.

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Effect of N2 flow rate on growth and photoluminescence properties of GaN nanorods grown by using molecular beam epitaxy (분자선 에피택시를 이용하여 GaN 나노로드를 성장시 구조 및 광학적인 특성에 미치는 N2의 양의 효과)

  • Park, Y.S.
    • Journal of the Korean Vacuum Society
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    • v.16 no.4
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    • pp.298-304
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    • 2007
  • We have studied the effect of $N_2$ flow rate on the structural and optical properties of GaN nanorods grown on (111) Si substrates by radio-frequency plasma-assisted molecular-beam epitaxy. The hexagonal shape nanorods with lateral diameters from 80 to 190 nm with increasing $N_2$ flow rate from 1.1 to 2.0 sccm are obtained. However, the ratio of length (thickness) and compact region increases with increasing $N_2$ flow rate up to 1.7 sccm and then saturate. From the photoluminescence, free exciton transition is clearly observed for GaN nanorods with low $N_2$ flow rate. And the PL peak energies are blue-shifted with decreasing diameter of the GaN nanorods due to size effect. Temperature-dependent photoluminescence spectra for the nanorods with $N_2$ flow rate of 1.7 sccm show an abnormal behavior like "S-shape" with increasing temperature.