Experimental Analysis of a Pulsed Inductively Coupled Linear Plasma Source
碩士 === 國立清華大學 === 工程與系統科學系 === 101 === The purpose of this study is to develop a pulsed inductively coupled linear plasma source, and analyze the temporal and spatial behavior of plasma characteristic parameters. In this research, we has successfully developed a pulsed inductively coupled linear...
Main Author: | |
---|---|
Other Authors: | |
Format: | Others |
Language: | zh-TW |
Published: |
2013
|
Online Access: | http://ndltd.ncl.edu.tw/handle/40639363625242533241 |
id |
ndltd-TW-101NTHU5593073 |
---|---|
record_format |
oai_dc |
spelling |
ndltd-TW-101NTHU55930732015-10-13T22:29:57Z http://ndltd.ncl.edu.tw/handle/40639363625242533241 Experimental Analysis of a Pulsed Inductively Coupled Linear Plasma Source 脈衝線性電感式耦合電漿源研製與實驗量測分析 蕭偉銘 碩士 國立清華大學 工程與系統科學系 101 The purpose of this study is to develop a pulsed inductively coupled linear plasma source, and analyze the temporal and spatial behavior of plasma characteristic parameters. In this research, we has successfully developed a pulsed inductively coupled linear plasma source. We modify and use measurement systems for a pulsed plasma source. We measure the temporal and spatial behavior of plasma parameters by using Langmuir probe and measure the rf parameters by using rf impedance meter (VI probe). In the results of rf impedance meter measurement, the magnitude of rf voltage didn't change significantly as the duty cycle or pulsed frequency increases, rf voltage decreases as the pressure increases. The magnitude of rf current didn't change significantly as pulsed frequency increases, rf current decreases as the duty cycle or pressure increases. A spike of the real part rf impedance due to the transition from capacitive to inductive coupling is observed in the beginning of the modulation pulse. In the results of Langmuir probe measurement, plasma density first increases and then decreases if the probe is moved away from the antenna, because there are more diffusion loss near the linear antenna. In the results, the plasma density at pulse mode is higher than that at continuous wave mode when they are operated at the same average power. In pulse mode, the highest average plasma density is 7.87 × 1010 cm-3 (10 mtorr, 70%, 10 kHz ). A spike of electron temperature due to the power increases substantially in the beginning of the modulation pulse. The magnitude of electron temperature has maximum, the electron temperature decreases if the probe is moved away from the antenna. Because there are interference of rf fieid in rf plasma, it make more error in electron temperature. 柳克強 2013 學位論文 ; thesis 92 zh-TW |
collection |
NDLTD |
language |
zh-TW |
format |
Others
|
sources |
NDLTD |
description |
碩士 === 國立清華大學 === 工程與系統科學系 === 101 === The purpose of this study is to develop a pulsed inductively coupled linear plasma source, and analyze the temporal and spatial behavior of plasma characteristic parameters. In this research, we has successfully developed a pulsed inductively coupled linear plasma source. We modify and use measurement systems for a pulsed plasma source. We measure the temporal and spatial behavior of plasma parameters by using Langmuir probe and measure the rf parameters by using rf impedance meter (VI probe).
In the results of rf impedance meter measurement, the magnitude of rf voltage didn't change significantly as the duty cycle or pulsed frequency increases, rf voltage decreases as the pressure increases. The magnitude of rf current didn't change significantly as pulsed frequency increases, rf current decreases as the duty cycle or pressure increases. A spike of the real part rf impedance due to the transition from capacitive to inductive coupling is observed in the beginning of the modulation pulse.
In the results of Langmuir probe measurement, plasma density first increases and then decreases if the probe is moved away from the antenna, because there are more diffusion loss near the linear antenna. In the results, the plasma density at pulse mode is higher than that at continuous wave mode when they are operated at the same average power. In pulse mode, the highest average plasma density is 7.87 × 1010 cm-3 (10 mtorr, 70%, 10 kHz ). A spike of electron temperature due to the power increases substantially in the beginning of the modulation pulse. The magnitude of electron temperature has maximum, the electron temperature decreases if the probe is moved away from the antenna. Because there are interference of rf fieid in rf plasma, it make more error in electron temperature.
|
author2 |
柳克強 |
author_facet |
柳克強 蕭偉銘 |
author |
蕭偉銘 |
spellingShingle |
蕭偉銘 Experimental Analysis of a Pulsed Inductively Coupled Linear Plasma Source |
author_sort |
蕭偉銘 |
title |
Experimental Analysis of a Pulsed Inductively Coupled Linear Plasma Source |
title_short |
Experimental Analysis of a Pulsed Inductively Coupled Linear Plasma Source |
title_full |
Experimental Analysis of a Pulsed Inductively Coupled Linear Plasma Source |
title_fullStr |
Experimental Analysis of a Pulsed Inductively Coupled Linear Plasma Source |
title_full_unstemmed |
Experimental Analysis of a Pulsed Inductively Coupled Linear Plasma Source |
title_sort |
experimental analysis of a pulsed inductively coupled linear plasma source |
publishDate |
2013 |
url |
http://ndltd.ncl.edu.tw/handle/40639363625242533241 |
work_keys_str_mv |
AT xiāowěimíng experimentalanalysisofapulsedinductivelycoupledlinearplasmasource AT xiāowěimíng màichōngxiànxìngdiàngǎnshìǒuhédiànjiāngyuányánzhìyǔshíyànliàngcèfēnxī |
_version_ |
1718077552055025664 |