• Title/Summary/Keyword: 건식플라즈마

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Capacitively Coupled Dry Etching of GaAs in BCl3/N2 Discharges at Low Vacuum Pressure (저진공 축전 결합형 BCl3/N2 플라즈마를 이용한 GaAs의 건식 식각)

  • Kim, Jae-Kwon;Park, Ju-Hong;Lee, Sung-Hyun;Noh, Ho-Seob;Joo, Young-Woo;Park, Yeon-Hyun;Kim, Tae-Jin;Lee, Je-Won
    • Korean Journal of Materials Research
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    • v.19 no.3
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    • pp.132-136
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    • 2009
  • This study investigates GaAs dry etching in capacitively coupled $BCl_3/N_2$ plasma at a low vacuum pressure (>100 mTorr). The applied etch process parameters were a RIE chuck power ranging from $100{\sim}200W$ on the electrodes and a $N_2$ composition ranging from $0{\sim}100%$ in $BCl_3/N_2$ plasma mixtures. After the etch process, the etch rates, RMS roughness and etch selectivity of the GaAs over a photoresist was investigated. Surface profilometry and field emission-scanning electron microscopy were used to analyze the etch characteristics of the GaAs substrate. It was found that the highest etch rate of GaAs was $0.4{\mu}m/min$ at a 20 % $N_2$ composition in $BCl_3/N_2$ (i.e., 16 sccm $BCl_3/4$ sccm $N_2$). It was also noted that the etch rate of GaAs was $0.22{\mu}m/min$ at 20 sccm $BCl_3$ (100 % $BCl_3$). Therefore, there was a clear catalytic effect of $N_2$ during the $BCl_3/N_2$ plasma etching process. The RMS roughness of GaAs after etching was very low (${\sim}3nm$) when the percentage of $N_2$ was 20 %. However, the surface roughness became rougher with higher percentages of $N_2$.

Dry Etching of PMMA and Polycarbonate in a Diffusion Pump-based Capacitively Coupled O2 Plasma (확산펌프 기반의 O2 축전결합 플라즈마를 이용한 PMMA와 폴리카보네이트의 건식 식각)

  • Park, Ju-Hong;Lee, Seong-Hyun;Choi, Jyoung-Hoon;Noh, Ho-Sub;Lee, Je-Won
    • Korean Journal of Materials Research
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    • v.19 no.8
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    • pp.421-426
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    • 2009
  • We report on the capacitively coupled O2 plasma etching of PMMA and polycarbonate (PC) with a diffusion pump. Plasma process variables were process pressure and CCP power at 5 sccm $O_2$ gas flow rate. Characterization was done in order to analyze etch rate, etch selectivity, surface roughness, and morphology using stylus surface profilometry and scanning electron microscopy. Self bias decreased with increase of process pressure in the range of 25$\sim$180 mTorr. We found an important result for optimum pressure for the highest etch rate of PMMA and PC, which was 60 mTorr. PMMA and PC had etch rates of 0.46 and 0.28 ${\mu}m$/min under pressure conditions, respectively. More specifically, etch rates of the materials increased when the pressure changed from 25 mTorr to 60 mTorr. However, they reduced when the pressure increased further after 60 mTorr. RMS roughnesses of the etched surfaces were in the range of 2.2$\sim$2.9 nm. Etch selectivity of PMMA to a photoresist was $\sim$1.5:1 and that of PC was $\sim$0.9:1. Etch rate constant was about 0.04 ${\mu}m$/minW and 0.02 ${\mu}m$/minW for PMMA and PC, respectively, with the CCP power change at 5 sccm $O_2$ and 40 mTorr process pressure. PC had more erosion on the etched sidewall than PMMA did. The OES data showed that the intensity of the oxygen atomic peak (777.196 nm) proportionally increased with the CCP power.

Steam Reforming of Ethylene Glycol over Ni/Al2O3 Catalysts: Effect of the Preparation Method and Reduction Temperature (Ni/Al2O3 촉매를 사용한 에틸렌글리콜의 수증기 개질 반응: 촉매 제조 방법과 환원온도의 영향)

  • Choi, Dong Hyuck;Park, Jung Eun;Park, Eun Duck
    • Korean Chemical Engineering Research
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    • v.53 no.3
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    • pp.372-381
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    • 2015
  • The effect of preparation method on the catalytic activities of the $Ni/Al_2O_3$ catalysts on steam reforming of ethylene glycol was investigated. The catalysts were prepared with various preparation methods such as an incipient wetness impregnation, wet impregnation, and coprecipitation method. In the case of coprecipitation method, various precipitants such as KOH, $K_2CO_3$, and $NH_4OH$ were compared. The prepared catalysts were characterized by using $N_2$ physisorption, inductively coupled plasma-atomic emission spectroscopy, X-ray diffraction, temperatureprogrammed reduction, pulsed $H_2$ chemisorption, temperature-programmed oxidation, scanning electron microscopy, and thermogravimetric analysis. Among the catalysts reduced at 773 K, the $Ni/Al_2O_3$ catalyst prepared by a coprecipitation with KOH or $K_2CO_3$ as precipitants showed the best catalytic performance. The preparation method affected the particle size of Ni, reducibility of nickel oxides, catalytic performance (activity and stability), and types of coke formed during the reaction. The $Ni/Al_2O_3$ catalyst prepared by a coprecipitation with KOH showed the increasing catalytic activity with an increase in the reduction temperature from 773 to 1173 K because of an increase in the reduction degree of Ni oxide species even though the particle size of Ni increased with increasing reduction temperature.

Characteristic of Pd-Cu-Ni Alloy Hydrogen Membrane using the Cu Reflow (Cu Reflow를 이용한 Pd-Cu-Ni 합금 수소분리막 특성)

  • Kim, Dong-Won;Kim, Heung-Gu;Um, Ki-Youn;Kim, Sang-Ho;Lee, In-Seon;Park, Jong-Su;Ryi, Shin-Kun
    • Korean Chemical Engineering Research
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    • v.44 no.2
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    • pp.160-165
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    • 2006
  • A Pd-Cu-Ni alloyed hydrogen membrane has fabricated on porous nickel support formed by nickel powder. Porous nickel support made by sintering shows a strong resistance to hydrogen embrittlement and thermal fatigue. Plasma surface modification treatment is introduced as pre-treatment process instead of conventional HCl wet activation. Nickel was electroplated to a thickness of $2{\mu}m$ in order in to fill micropores at the nickel support surface. Palladium and copper were deposited at thicknesses of $4{\mu}m$ and $0.5{\mu}m$, respectively, on the nickel coated support by DC sputtering process. Subsequently, copper reflow at $700^{\circ}C$ was performed for an hour in $H_2$ ambient. And, as a result PdCu-Ni composite membrane has a pinhole-free and extremely dense microstructure, having a good adhesion to the porous nickel support and infinite hydrogen selectivity in $H_2/N_2$ mixtures.

MEDICI와 SUPREM4를 이용한 폴리 실리콘 게이트의 벽면 기울기에 따른 NMOS 소자의 전기적 특성 분석

  • No, Ho-Seop;Kim, Jin-Su;Sin, Ju-Yong;Song, Han-Jeong;Lee, Je-Won
    • Proceedings of the Materials Research Society of Korea Conference
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    • 2009.05a
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    • pp.20.1-20.1
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    • 2009
  • 반도체 소자 제조 공정 프로그램인 T-suprem4와 MEDICI를 이용하여 NMOS구조를 설계 하였다. MOS 소자 시뮬레이션을 통해 식각 공정에서 생기는 언더컷에 의한 전기적 특성을 I-V 곡선으로 비교하여 분석하였다. NMOS 구조는 반도체 소자 제조 공정 프로그램 T-suprem4를 이용하여 기본 소자 구조를 설계하였다. 실험의 변수로는 첫째, 소자 공정 중 폴리 실리콘의 언더컷 식각의 각도를 $70^{\circ}C$부터 $110^{\circ}C$까지 $10^{\circ}C$의 차이로 설계하였다. 또한, 언더컷에 의한 드레인-소스사이의 전류($I_{DS}$) 손실이 없는 유효한 각도를 확인하기 위해 $80^{\circ}C$부터 $100^{\circ}C$까지는 $2^{\circ}C$ 크기로 설계 하였다. 둘째, 게이트 크기를 축소하고 역시 언더컷 식각의 각도를 다양하게 설계하였다. 설계된 소자를 반도체 소자 특성 분석 프로그램 MEDICI를 이용하여 소자의 전기적 특성을 측정하였다. 우선 NMOS소자 게이트에 2V의 전압을 인가하였다. 그리고 드레인 부분에 전압을 인가하여 그에 따른 드레인의 전류를 측정 하였다. 드레인 전압은 0V 부터 변화시키며 인가하였다. 측정된 전류 값으로 I-V 곡선을 나타내었다. I-V 곡선의 분석을 통해 식각 후 언더컷의 각도가 $70^{\circ}C$, $80^{\circ}C$, $110^{\circ}C$ 일 때 $4\times10^{-8}A/{\mu}$의 전류가 흐르고, $90^{\circ}C$, $100^{\circ}C$ 일 때는 $1.8\times10^{-7}A/{\mu}$의 전류가 흐르는 것을 확인 하였다. $80^{\circ}C$에서 $100^{\circ}C$까지는 $2^{\circ}C$ 크기로 측정한 결과 $88^{\circ}C$에서 $100^{\circ}C$ 사이 일 때 $90^{\circ}C$ 각도의 경우와 같이 $1.8\times10^{-7}A/{\mu}$의 전류가 측정 되었다. 즉, 식각 중 수직 측벽 도에 언더컷이 $10^{\circ}C$이상 발생하면 $I_{DS}$ 전류 값이 약 22%로 감소하였다. 또한 일반적으로 $90^{\circ}C$의 수직측벽을 가지는 공정이 중요하다고만 생각 되었지만, 이번 연구를 통하여 식각 후 측벽의 각도가 $88^{\circ}C$에서 $92^{\circ}C$ 사이에 있을 때 $I_{DS}$ 값이 가장 최대가 되는 것을 확인 할 수 있었다.

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패턴 사파이어 기판 위에 AlN 중간층을 이용한 GaN 에피성장

  • Kim, Nam-Hyeok;Lee, Geon-Hun;Park, Seong-Hyeon;Kim, Jong-Hak;Kim, Min-Hwa;Yu, Deok-Jae;Mun, Dae-Yeong;Yun, Ui-Jun;Yeo, Hwan-Guk;Mun, Yeong-Bu;Si, Sang-Gi
    • Proceedings of the Korean Vacuum Society Conference
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    • 2010.02a
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    • pp.123-123
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    • 2010
  • 3족 질화물계 물질은 발광다이오드와 같은 광전자소자적용에 있어서 매우 우수한물 질이다.일반적으로, GaN 에피 성장에 있어서 저온 중간층을 삽입한 2 단계 성장 방법은 낮은 결함밀도와 균일한 표면을 얻기 위해 도입된 기술이다. 특히 AlN 중간층은 GaN 중간층과 비교하였을 때 결정성뿐만 아니라 높은 온도에서의 열적안정성, GaN 기반의 자외선 검출기서의빛 흡수 감소 등의 장점을 가지고 있다. 또한 패턴 사파이어 기판위 GaN 에피 성장은 측면성장 효과를 통해 결함 밀도 감소와 광 추출 효율을 향상시키는 것으로 알려져 있다.또한 열응력으로 인한 기판의 휨 현상은 박막성장중 기판의 온도 분포를 불균일하게 만드는 원인이 되며 이는 결국 박막 조성 및 결정성의 열화를 유도하게 되고 최종적으로 소자특성을 떨어 뜨리는 원인이 되는데 AlN 중간층의 도입으로 이것을 완화시킬 수 있는 효과가 있다. 하지만, AlN 중간층이 패턴된 기판 위에 성장시킨 GaN 에피층에 미치는 영향은 명확하지 않다. 본 연구팀은 일반적인 c-plane 사파이어 기판과 플라즈마 건식 에칭을 통한 렌즈 모양의 패턴된 사파이어 기판을 이용해서 AlN 중간층과 GaN 에피층을 유기금속 화학기상증착법으로 성장하였다. 특히, 렌즈 모양의 패턴된 사파이어 기판은 패턴 모양과 패턴 밀도가 성장에 미치는 영향을 연구하기 위해 두가지 패턴의 사파이어 기판을 이용하였다. AlN 중간층 두께를 조절함으로써 최적화된 GaN 에피층을 90분까지 4단계로 시간 변화를 주어 성장 양상을 관찰한 결과, GaN 에피박막의 성장은 패턴 기판의 trench 부분에서 시작하여 기판의 패턴부분을 덮는 측면 성장을 보이고있다. 또한 TEM과 CL을 통해 GaN 에피박막의 관통 전위를 분석해 본 결과 측면 성장과정에서 성장 방향을 따라 옆으로 휘게 됨으로 표면까지 도달하는 결정결함의 수가 획기적으로 줄어드는 것을 확인함으로써 고품질의 GaN 에피층을 성장시킬 수 있었다. 그리고 패턴밀도가 높고 모양이 볼록할수록 측면 성장 효과로 인한 결정성 향상과 난반사 증가를 통한 임계각 증가로 광추출 효율이 향상 되는 것을 확인할 수 있었다. 이러한 결과를 바탕으로 최적화된 AlN 중간층을 이용하여 패턴 기판위에서 고품질의 GaN 에피층을 성장시킬 수 있었다.

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Study of Coherent High-Power Electromagnetic Wave Generation Based on Cherenkov Radiation Using Plasma Wakefield Accelerator with Relativistic Electron Beam in Vacuum (진공 내 상대론적인 영역의 전자빔을 이용한 플라즈마 항적장 가속기 기반 체렌코프 방사를 통한 결맞는 고출력 전자파 발생 기술 연구)

  • Min, Sun-Hong;Kwon, Ohjoon;Sattorov, Matlabjon;Baek, In-Keun;Kim, Seontae;Hong, Dongpyo;Jang, Jungmin;Bhattacharya, Ranajoy;Cho, Ilsung;Kim, Byungsu;Park, Chawon;Jung, Wongyun;Park, Seunghyuk;Park, Gun-Sik
    • The Journal of Korean Institute of Electromagnetic Engineering and Science
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    • v.29 no.6
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    • pp.407-410
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    • 2018
  • As the operating frequency of an electromagnetic wave increases, the maximum output and wavelength of the wave decreases, so that the size of the circuit cannot be reduced. As a result, the fabrication of a circuit with high power (of the order of or greater than kW range) and terahertz wave frequency band is limited, due to the problem of circuit size, to the order of ${\mu}m$ to mm. In order to overcome these limitations, we propose a source design technique for 0.1 THz~0.3 GW level with cylindrical shape (diameter ~2.4 cm). Modeling and computational simulations were performed to optimize the design of the high-power electromagnetic sources based on Cherenkov radiation generation technology using the principle of plasma wakefield acceleration with ponderomotive force and artificial dielectrics. An effective design guideline has been proposed to facilitate the fabrication of high-power terahertz wave vacuum devices of large diameter that are less restricted in circuit size through objective verification.

The characteristic of InGaN/GaN MQW LED by different diameter in selective area growth method (선택성장영역 크기에 따른 InGaN/GaN 다중양자우물 청색 MOCVD-발광다이오드 소자의 특성)

  • Bae, Seon-Min;Jeon, Hun-Soo;Lee, Gang-Seok;Jung, Se-Gyo;Yoon, Wi-Il;Kim, Kyoung-Hwa;Yang, Min;Yi, Sam-Nyung;Ahn, Hyung-Soo;Kim, Suck-Whan;Yu, Young-Moon;Ha, Hong-Ju
    • Journal of the Korean Crystal Growth and Crystal Technology
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    • v.22 no.1
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    • pp.5-10
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    • 2012
  • In general, the fabrications of the LEDs with mesa structure are performed grown by MOCVD method. In order to etch and separate each chips, the LEDs are passed the RIE and scribing processes. The RIE process using plasma dry etching occur some problems such as defects, dislocations and the formation of dangling bond in surface result in decline of device characteristic. The SAG method has attracted considerable interest for the growth of high quality GaN epi layer on the sapphire substrate. In this paper, the SAG method was introduced for simplification and fabrication of the high quality epi layer. And we report that the size of selective area do not affect the characteristics of original LED. The diameter of SAG circle patterns were choose as 2500, 1000, 350, and 200 ${\mu}m$. The SAG-LEDs were measured to obtain the device characteristics using by SEM, EL and I-V. The main emission peaks of 2500, 1000, 350, and 200 ${\mu}m$ were 485, 480, 450, and 445 nm respectively. The chips of 350, 200 ${\mu}m$ diameter were observed non-uniform surface and resistance was higher than original LED, however, the chips of 2500, 1000 ${\mu}m$ diameter had uniform surface and current-voltage characteristics were better than small sizes. Therefore, we suggest that the suitable diameter which do not affect the characteristic of original LED is more than 1000 ${\mu}m$.