• Title/Summary/Keyword: Microwave Plasma

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A Study of the Properties of Optically Induced Layers in Semiconductors Aided by the Reflection of Optically Controlled Microwave Pulses

  • Wang, Xue;Choi, Yue-Soon;Park, Jong-Goo;Kim, Yong-K.
    • Transactions on Electrical and Electronic Materials
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    • v.10 no.4
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    • pp.111-115
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    • 2009
  • We present a study on the reflection of optically controlled microwave pulses from non uniform plasma layers in semiconductors. The transient response of the microwave pulses in different plasma layers has been evaluated by means of the reflection function of dielectric microstrip lines. The lines were used with an open-ended termination containing an optically induced plasma region, which was illuminated by a light source. The reflection characteristics impedance resulting from the presence of plasma is evaluated by means of the equivalent transmission line model. We have analyzed the variation of the transient response in a 0.01 cm layer with a surface frequency in the region of 128 GHz. In the reflection the variation of the diffusion length $L_D$ is large compared with the absorption depth $1/{\alpha}_l$. The variation of the characteristic response of the plasma layer with differentially localized pulses has been evaluated analytically. The change of the reflection amplitude has been observed at depths of 0.1 cm, 0.01 cm and $0.1{\times}10^{-5}$ cm respectively.

Electron Density and Electron Temperature in Atmospheric Pressure Microplasma

  • Tran, T.H.;Kim, J.H.;Seong, D.J.;Jeong, J.R.;You, S.J.
    • Proceedings of the Korean Vacuum Society Conference
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    • 2012.08a
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    • pp.152-152
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    • 2012
  • In this work we measured electron temperature and electron density of a microplasma by optical emission spectroscopy. The plasma is generated from a small discharge gap of a microwave parallel stripline resonator (MPSR) in Helium at atmospheric pressure. The microwave power supplied for this plasma source from 0.5 to 5 watts at a frequency close to 800 MHz. The electron temperature and electron density were estimated through Collisional-radiative model combined with Corona-equilibrium model. The results show that the electron density and temperature of this plasma in the case small discharge gap width are higher than that in larger gap width. The diagnostic techniques and associated challenges will be presented and discussed.

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Development of Direct Analysis of Metal and Non-metal Ions in Aqueous Samples with the Moderate Power Helium Microwave Induced Plasma (중급 출력 마이크로파 유도 플라즈마를 이용한 금속 및 비금속 수용액시료의 직접 분석법의 개발)

  • Park, Yong-Nam
    • Journal of the Korean Chemical Society
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    • v.35 no.6
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    • pp.699-706
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    • 1991
  • The moderate power (500 W) Microwave Induced Plasma was generated with helium gas and was used for the direct analysis of aqueous samples. Usually, the helium plasma obtained with a modified Beenakker type cavity forms a cylindrical one. Though, by the careful controls of gas flows, a "toroidal" shape plasma could be made but its analytical performances were found to be worse. Using the glass frit nebuliser, the detection limits for metal ions obtained were around 10~100 ppb and that for chloride was about 50ppm.

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Characteristics on the Breakdown and Frequency Spectrum of High Power Microwave Pulse Propagating through the Atmosphere (고출력 마이크로파 펄스의 대기권 전파시 방전 및 주파수 스펙트럼에 관한 특성)

  • Kim, Yeong-Ju
    • The Transactions of the Korean Institute of Electrical Engineers C
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    • v.48 no.8
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    • pp.591-597
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    • 1999
  • The propagation characteristics of high power microwave pulse in an air-breakdown environment are examined. The maximum electron density produced by microwave air-breakdown is limited to $10^6cm^{-3}$ by the tail-erosion effect. Inorder to increase the electron density, the scheme using two pulses intersecting at a desired height is considered. Increasing the carrier frequency, it is shown that microwave pulse can be transferred without the serious erosion in the numerical simulation. This result is useful for the above scheme. Also, an experiment is conducted to show the tail-erosion effect and confirm that a rapidly generated lossy plasma can cause spectral breaking and frequency shift of a high-power microwave pulse. The experimental results are presented by comparing the frequency spectrum of an incident pulse with that of the pulse transmitted through a self-induced air-breakdown environment. The experimental results show that the amount of frequency upshift is co-related with the ionization rate, whereas that of frequency downshift is correlated with the energy losses from the pulse in the self-generated plasma.

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Design of compact klystron amplifier using Field-emitter-arrays (FEA)-based cathode

  • Jin, Jeong-Gu;Ha, Hyun-Jun;Park, Gun-Sik
    • Journal of Korean Vacuum Science & Technology
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    • v.3 no.1
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    • pp.59-65
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    • 1999
  • There has been an interest to develop an efficient, compact microwave device using field-emitter-arrays (FEA)-based cathode. Toe valuate the optimum device-efficiency in a compact size, the propagation properties of the premodulated electron beam for the FEA-based cathode is studied in detail by the computer simulation using a PIC code, MAGIC. For the premodulated electron beam whose phase of the energy leads the phase of the current by $\pi$/2, the amplitude of the downstream current modulation can be kept as high as the initial modulation level. Using the beam parameters with the beam voltage of 6kV and the current of 2.0A, 30% of efficiency is predicted when the quality factor of 800 is chosen. the device length is reduced about twice compared with that of the conventional device. The design of practical planar cathode is carried out to meet the minimum diameter of the electron beam as 0.5 mm.

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Design and Characterization of a Microwave Plasma Source Using a Rectangular Resonant Cavity (마이크로웨이브 공진 공동을 이용한 플라즈마 원의 설계 및 특성)

  • Kim, H.T.;Park, Y.S.;Sung, C.K.;Yi, J.R.;Hwang, Y.S.
    • Journal of the Korean Vacuum Society
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    • v.17 no.5
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    • pp.408-418
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    • 2008
  • The rectangular resonant cavity was designed and characterized as a microwave plasma source for focused ion beam. The optimum cavity was calculated analytically and analyzed in detail by using HFSS(High Frequency Structure Simulator). Since the resonant cavity can be affected by the permittivity of quartz chamber and plasma, the cavity is designed to be changeable in one direction. By observing the microwave input power at which the breakdown begins, the optimum cavity length for breakdown is measured and compared with the calculated one, showing in good agreement with the optimum length reduced by 10cm according to the permittivity change in the presence of quartz chamber. The shape of breakdown power curve as a function of pressure appears to be similar to Paschen-curve. After breakdown, plasma densities increase with microwave power and the reduced effective permittivity in the cavity with plasma results in larger optimum length. However, it is not possible to optimize the cavity condition for high density plasmas with increased input power, because too high input power causes expansion of density cutoff region where microwave cannot penetrate. For more accurate microwave cavity design to generate high density plasma, plasma column inside and outside the density cutoff region needs to be treated as a conductor or dielectric.

Cutoff Probe Analysis and Improvement

  • Kim, Dae-Ung;Yu, Sin-Jae;Yu, Gwang-Ho;Park, Min;Kim, Jeong-Hyeong;Seong, Dae-Jin;Jang, Hong-Yeong
    • Proceedings of the Korean Vacuum Society Conference
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    • 2011.08a
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    • pp.142-142
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    • 2011
  • Microwave diagnostics method for plasma science and engineering is vigorous research area for its good characteristics such as high sensitivity, reliability, and broad measurement spectrum from low density plasma to high density. We investigate mechanism of microwave probes (hairpin, impedance and absorbtionf probe) and apply it for interpretation of full transmitted spectrum of cutoff probe. Mechanism of the spectrum having same key roles of I-V curve of Langmuir probe is not exactly revealed yet in spite of its importance. This study elucidates physics behind it using a circuit model and E/M wave simulation. Circuit model reveals exact cut-off peak frequency taking account of a collision frequency and a plasma frequency and it enable precise diagnostics of plasma densty from low pressure to high pressre. Cut-off like peaks have been obstacle for choosing cut-off peak is analyzed by E/M simulation and one of cutoff like peaks made by probe holder used for acquire plasma density with cutoff peak applying the hairpin relation. Furthermore, phase difference method for plasma density is conducted. This method uses a single microwave frequency source and it is low-priced.

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The Properties of Microwave Propagation in Discharging Plasma (방전에 의한 프라즈마에서의 마이크로파 전파특성)

  • Yang, In-Eung;No, Bang-Hyeon;Kim, Bong-Yeol
    • Journal of the Korean Institute of Telematics and Electronics
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    • v.5 no.3
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    • pp.31-39
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    • 1968
  • In this paper microwave power propagated through the cold plasma was analyzed and measured with respect to the external magenetic flux density. The d. c discharge plasma was in the rectangular waveguide in which two electrode was inserted, and also the glass diseharge tube inserted in the ractangular wavegside. The direction of microwave pro-pagation, the axis of the discharge tube and external magnetic flux were perpendicular to each other. It showed that the attenuation and absorption of micro wave power propagated in the plasma was increased as the magnetic flux density, the discharge current and the pressure of the gas were increased.

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LOW TEMPERATURE DIAMOND GROWTH USING MICROWAVE PLASMA CVD

  • Sakamoto, Yukihiro;Takaya, Matsufumi;Shinohara, Kibatsu
    • Journal of the Korean institute of surface engineering
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    • v.29 no.5
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    • pp.487-493
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    • 1996
  • Diamond films were grown at lower temperatures (630-813K) on Si, Al (1100P), and Al-Si(8A, 8B, BC) alloy substrates using improved microwave plasma CVD apparatus in a mixed methane and hydrogen plasma. Improved microwave plasma CVD apparatus equipped water cooled substrate holder and the substrates were set up lower position than bottom line of the applicator waveguide. When the methane concentration was high and growth was conducted at lower pressures the diamond films were synthesized. Moreover the deposits on the scratched substrates formed flat surfaces consisting of fine grains. XRD results, the deposits were identified to cubic diamond. An analysis using Raman spectroscopy, further confirmed that diamond films deposited on the Si substrates were high quality. The deposits on the Al substrates, in contrast, contained amorphous carbon. While the quality of the deposits on the Al-Si substrates were differed with the substrate alloys.

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Chemical Vapor Deposition of Diamond Film from Methane-Hydrogen Gas in Microwave Plasma (마이크로웨이브 플라즈마에서 메탄-수소가스로부터 다이아몬드박막의 화학증착)

  • 이길용;제정호
    • Journal of the Korean Ceramic Society
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    • v.26 no.3
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    • pp.331-340
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    • 1989
  • In this study, it was tried to deposit diamond films from a mixture of CH4 and H2 by the microwave plasma chemical vapor deposition(MWCVD). The MWCVD process was designed and set up from the 2.45GHz microwave generator. And the diamond film was successfully deposited on silicon wafers from the mixture of methane and hydrogen. The microstructures of the deposited diamond films were studied by using the following deposition variables : (a) methane concentration(0.6-10%), (b) reaction pressure(10-100torr), and (c) the substrate temperature(450-76$0^{\circ}C$).

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