• 제목/요약/키워드: Plasma emission

검색결과 1,183건 처리시간 0.032초

Field emission from hydrogen-free DLC

  • Suk Jae chung;Han, Eun-Jung;Lim, Sung-Hoon;Jin Jang
    • Journal of Korean Vacuum Science & Technology
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    • 제3권1호
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    • pp.49-53
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    • 1999
  • We have studied the field emission characteristics of diamond-like-carbon (DLC) films deposited by a layer-by-layer technique using plasma enhanced chemical vapor deposition, in which the deposition of a thin layer of DLC and a CH4 plasma exposure on its surface were carried out alternatively. The hydrogen-free DLC can be deposited by CH4 plasma exposure for 140 sec on a 5 nm DLC layer. N2 gas-phase doping in the CH4 plasma was also carried out to reduce the work function of the DLC. The optimum [N2]/[CH4] flow rate ratio was found to be 9% for the efficient electron emission, at which the onset-field was 7.2 V/$\mu\textrm{m}$. It was found that the hydrogen-free DLC has a stable electron emitting property.

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레이저 용접시 용접결함의 실시간 모니터링법 개발에 관한 연구 (Fundamental Study on the Weld Defects and Its Real-time Monitoring Method)

  • 김종도
    • Journal of Welding and Joining
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    • 제20권1호
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    • pp.26-33
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    • 2002
  • This study was undertaken to obtain the fundamental knowledges on the weld deflects and it's realtime monitoring method. The paper describes the results of high speed photography, acoustic emission (AE) detection and plasma light emission (LE) measurements during $CO_2$ laser welding of STS 304 stainless steel and A5083 aluminum alloy in different welding condition. The characteristic frequencies of plasma and keyhole fluctuations at different welding speed and shield gases were measured and compared with the results of Fourier analyses of temporal AE and LE spectra, and they had considerably good agreement with keyhole and plasma fluctuation. Namely, the low frequency peaks of AE and LE shifted to higher frequency range with the welding speed increase, and leer the argon shield gas it was higher than that in helium and nitrogen gases. The low frequencies dominating in fluctuation spectra of LE probably reflect keyhole opening instability. It is possible to monitor the weld bead deflects by analyzing the acoustic and/or plasma light emission signals.

대기압 아르곤 플라즈마 토치의 진동 및 회전온도 측정 연구 (A Study on the Measurement of Vibrational and Rotational Temperature Using the Atmospheric Ar Plasma Torch)

  • 최광주;장문국;한상보;박재윤
    • 전기학회논문지
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    • 제60권10호
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    • pp.1895-1902
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    • 2011
  • This work was carried out for the measurement of vibration and rotation temperature using the optical emission spectroscopy of nitrogen second positive system in the small plasma torch. Among emissions $N_2$ SP systems, the emission of $N_2$ SP(0-0) was so strong. Emission peaks of SP system increased until the position of 12.5[mm] from the end of plasma torch, after that it decreased. However, vibration temperature decreased from 1540[K] to 1000[K] at the position of 12.5[mm]. In addition, rotational temperature was about 400[K] at the position of 10[mm] and it increased a little as much of 420[K] at 12.5[mm]. Consequently, the plasma torch discussed in this work is possible to apply in the surface treatment process under the low temperature.

RF 플라즈마에 의해 생성된 산소 플라즈마의 발광 스펙트럼 (Optical Emission Spectra of Oxygen Plasma Produced by Radio-Frequency Plasma)

  • 김도엽;김민수;김태훈;김군식;최현영;조민영;전수민;박성동;김진하;김은도;황도원;임재영
    • 한국진공학회지
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    • 제18권2호
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    • pp.102-107
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    • 2009
  • 본 연구에서는 ZnO 박막을 성장하기 위한 plasma-assisted molecular beam epitaxy (PAMBE)에 장착된 플라즈마건에 13.56 MHz의 rf 전력을 인가하였을 때 발생되는 산소 플라즈마의 발광 스펙트럼을 광발광 분광기(optical emission spectroscopy: OES)를 이용하여 조사하였다. 실험은 산소 가스 유량을 1 sccm에서 20 sccm, rf 전력을 25W에서 250 W 범위에서 플라즈마건의 오리피스의 직경을 각각 3 mm 와 5 mm로 달리하여 행해졌다. 산소 플라즈마를 발생시켰을 때 오리피스의 직경에 상관없이 전형적인 산소 플라즈마의 발광 스펙트럼이 관측되었다. 특히 776.8 nm와 843.9 nm에서 $3p^{5}P-3s^{5}S^{0}$, $3p^{3}P-3s^{3}S^{0}$ 천이에 기인하는 강한 산소 원자 발광선이 관측되었다. 산소 유량과 rf 파워가 증가함에 따라 776.8 nm와 843.9 nm의 발광 세기는 증가하였고, 776.8 nm의 스펙트럼 발광 세기의 증가율이 843.9 nm의 스펙트럼 발광 세기 증가율보다 컸다. 또한 오리피스 직경이 3 mm일 때가 5 mm일 때보다 산소 플라즈마가 더 안정적으로 발생하였다.

The influence of Ne-Xe gas mixture ratio on vacuum Ultraviolet and infrared line in AC-PDP

  • Oh, Phil-Y.;Cho, I.R.;Jung, Y.;Park, K.D.;Ahn, J.C.;Choi, E.H.
    • 한국정보디스플레이학회:학술대회논문집
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    • 한국정보디스플레이학회 2003년도 International Meeting on Information Display
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    • pp.743-747
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    • 2003
  • The improvement of luminance and luminous efficiency is the one of the most important part in AC-PDPs. To achieve high luminance and luminous efficiency, high VUV emission efficiency is needed. We measured the emission spectra of vacuum ultraviolet(VUV) and infrared(IR) rays in surface discharge AC-PDP with Ne-Xe mixture gas. The influence of Ne-Xe gas-mixture ratio on resonance state $Xe^{\ast}(3P_{1})$ and exited state $Xe^{\ast}(3P_{2})$ has been investigated. It is found that the intensity of VUV 147nm emission is proportional to that of the IR 828 nm emission, and the VUV 173nm emission is roughly proportional to that of the IR 823nm emission. The electron temperature and plasma density have been experimentally measured from the center of sustaining electrode gap by a micro Langmuir probe in AC-PDPs. The plasma density from the center of sustaining electrode gap are shown to be maximum value of $9{\times}10^{11}cm^{-3}$, where the electron temperature is about 1.6 eV in this experiment

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Ion-induced secondary electron emission coefficient and work function for MgO thin film with $O_2$ plasma treatment

  • Jung, J.C.;Jeong, H.S.;Lee, J.H.;Oh, J.S.;Park, W.B.;Lim, J.Y.;Cho, J.W.;Choi, E.H.
    • 한국정보디스플레이학회:학술대회논문집
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    • 한국정보디스플레이학회 2004년도 Asia Display / IMID 04
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    • pp.525-528
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    • 2004
  • The ion-induced secondary electron emission coefficient ${\gamma}$ and work function for MgO thin film with $O_2$ plasma treatment has been investigated by ${\gamma}$ -FIB (focused ion beam) system. The MgO thin film deposited from sintered material with $O_2$ plasma treatment is found to have higher ${\gamma}$ and lower work function than those without $O_2$ plasma treatment. The energy of various ions used has been ranged from 100eV to 200eV throughout this experiment. It is found that the highest secondary electron emission coefficient ${\gamma}$ has been achieved for 10 minutes of $O_2$ plasma treatment under RF power of 50W.

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Quantitative Analysis for Plasma Etch Modeling Using Optical Emission Spectroscopy: Prediction of Plasma Etch Responses

  • Jeong, Young-Seon;Hwang, Sangheum;Ko, Young-Don
    • Industrial Engineering and Management Systems
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    • 제14권4호
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    • pp.392-400
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    • 2015
  • Monitoring of plasma etch processes for fault detection is one of the hallmark procedures in semiconductor manufacturing. Optical emission spectroscopy (OES) has been considered as a gold standard for modeling plasma etching processes for on-line diagnosis and monitoring. However, statistical quantitative methods for processing the OES data are still lacking. There is an urgent need for a statistical quantitative method to deal with high-dimensional OES data for improving the quality of etched wafers. Therefore, we propose a robust relevance vector machine (RRVM) for regression with statistical quantitative features for modeling etch rate and uniformity in plasma etch processes by using OES data. For effectively dealing with the OES data complexity, we identify seven statistical features for extraction from raw OES data by reducing the data dimensionality. The experimental results demonstrate that the proposed approach is more suitable for high-accuracy monitoring of plasma etch responses obtained from OES.

Secondary Electron Emission Characteristics of Functional Layer in AC-PDP

  • Son, Chang-Gil;Han, Young-Gyu;Kim, Yong-Hee;Cho, Byeong-Seong;Hong, Young-Jun;Song, Ki-Baek;Bae, Young-Joo;Kim, In-Tae;Choi, Eun-Ha
    • 한국정보디스플레이학회:학술대회논문집
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    • 한국정보디스플레이학회 2009년도 9th International Meeting on Information Display
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    • pp.736-739
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    • 2009
  • We have studied that the secondary electron emission characteristics of functional layers which have different kinds of MgO sub-micrometer size powder in AC-PDP. We used cathodoluminescence(CL) and gamma focused ion beam (${\gamma}$-FIB) system for measurement of secondary electron emission characteristics. Also we made 6 inch test panel which applied functional layers for evaluation of discharge characteristics.

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XPS Investigation and Field Emission Property of the Ar Plasma Processed Carbon Nanotube Films

  • Lee, Sun-Woo;Lee, Boong-Joo;Oda, Tetsuji
    • Transactions on Electrical and Electronic Materials
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    • 제9권2호
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    • pp.52-56
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    • 2008
  • Carbon nanotube films were fabricated by the catalytic CVD method. Plasma processed time effects on the field emission property were studied. The atomic structure was observed by using X-ray photoelectron spectroscopy (XPS). The surface composition changes were observed on the plasma processed CNT films. The O1s/C1s signal ratio and the Fls/Cls signal ratio changed from 1.1 % to 24.65 % and from 0 % to 3.1 % with plasma process time, respectively. We could guess it from these results that the Ar plasma process could change the surface composition effectively. In the case of the original-CNT film, no carbon shift was observed. In the case of the Ar plasma processed CNT films, however the oxygen related carbon shifts were observed. This oxygen related carbon shift at higher binding energy implies the increment of amount of the oxygen. It's possible that the increment of these bonds between carbon and oxygen results in the improvement of field emission performance.

Influence of Ne-Xe Gas Mixture Ratio on the Extreme Ultraviolet (EUV) Emission Measurement from the Coaxially Focused Plasma

  • Lee, Sung-Hee;Hong, Young-June;Choi, Duk-In;Uhm, Han-Sup;Choi, Eun-Ha
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2011년도 제40회 동계학술대회 초록집
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    • pp.220-220
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    • 2011
  • The Ne-Xe plasmas in dense plasma-focus device with coaxial electrodes were generated for extreme ultraviolet (EUV) lithography. The influence of gas mixture ratio, Ne-Xe (1, 10, 15, 20, 25, 30, 50%) mixture gas, on EUV emission measurement, EUV intensity and electron temperature in the coaxially focused plasma were investigated. An input voltage of 4.5 kV was applied to the capacitor bank of 1.53mF and the diode chamber was filled with Ne-Xe mixture gas at a prescribed pressure. The inner surface of the cylindrical cathode was lined by an acetal insulator. The anode was made of tin metal. The EUV emission signal of the wavelength in the range of 6~16 nm has been detected by a photo-detector (AXUV-100 Zr/C, IRD). The visible emission line was also detected by the composite-grating spectrometer of the working wavelength range of 200~1100 nm (HR 4000CG). The electron temperature is obtained by the optical emission spectroscopy (OES) and measured by the Boltzmann plot with the assumption of local thermodynamic equilibrium (LTE).

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