Dual-Frequency RF Impedance Matching Circuits for Semiconductor Plasma Etch Equipment
The change in electrode impedance of semiconductor equipment due to repetitive processes is a major issue that creates process drift. In the current plasma etch chamber with a dual-frequency power system, the high-powered radio frequency (RF) source contributes to the enhancement of the plasma densi...
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Online Access: | https://www.mdpi.com/2079-9292/10/17/2074 |
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doaj-ec2cdd413f8f46f0afdb73c99493f9e82021-09-09T13:41:59ZengMDPI AGElectronics2079-92922021-08-01102074207410.3390/electronics10172074Dual-Frequency RF Impedance Matching Circuits for Semiconductor Plasma Etch EquipmentJeongsu Lee0Sangjeen Hong1Department of Electronic Engineering, Myongji University, Seoul 17058, KoreaDepartment of Electronic Engineering, Myongji University, Seoul 17058, KoreaThe change in electrode impedance of semiconductor equipment due to repetitive processes is a major issue that creates process drift. In the current plasma etch chamber with a dual-frequency power system, the high-powered radio frequency (RF) source contributes to the enhancement of the plasma density, and the low-frequency bias power at the bottom electrode is adopted to enhance the injected ion energy in the plasma. The impedance control of the top electrode in dual-frequency capacity coupled plasma limits the impedance matching capability of the RF matching system because it only considers the high-frequency RF source. To control the precise impedance in dual-frequency semiconductor equipment, independent impedance control is required for each frequency. In this study, the impedance corresponding to a specific frequency was independently controlled using L (inductor) and C (capacitor). A 60 MHz stop filter and VVC were used to control 2 MHz impedance at a specific point, and a 2 MHz stop filter and VVC were used to control 60 MHz impedance. In the case of 2 MHz impedance control, the 2 MHz impedance changed from 10.9−<i>j</i>893 to 0.3−<i>j</i>62 and the 60 MHz impedance did not change. When controlling the 60 MHz impedance, the 60 MHz impedance changed from 0.33 + <i>j</i>26.53 to 0.2 + <i>j</i>190 and the 2 MHz impedance did not change. The designed LC circuits cover the impedance of 60 and 2 MHz separately and are verified by the change in the capacitance of the vacuum variable capacitors implemented in the RF impedance matching system.https://www.mdpi.com/2079-9292/10/17/2074dual-frequency capacitively coupled plasmaprocess driftimpedance matching |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Jeongsu Lee Sangjeen Hong |
spellingShingle |
Jeongsu Lee Sangjeen Hong Dual-Frequency RF Impedance Matching Circuits for Semiconductor Plasma Etch Equipment Electronics dual-frequency capacitively coupled plasma process drift impedance matching |
author_facet |
Jeongsu Lee Sangjeen Hong |
author_sort |
Jeongsu Lee |
title |
Dual-Frequency RF Impedance Matching Circuits for Semiconductor Plasma Etch Equipment |
title_short |
Dual-Frequency RF Impedance Matching Circuits for Semiconductor Plasma Etch Equipment |
title_full |
Dual-Frequency RF Impedance Matching Circuits for Semiconductor Plasma Etch Equipment |
title_fullStr |
Dual-Frequency RF Impedance Matching Circuits for Semiconductor Plasma Etch Equipment |
title_full_unstemmed |
Dual-Frequency RF Impedance Matching Circuits for Semiconductor Plasma Etch Equipment |
title_sort |
dual-frequency rf impedance matching circuits for semiconductor plasma etch equipment |
publisher |
MDPI AG |
series |
Electronics |
issn |
2079-9292 |
publishDate |
2021-08-01 |
description |
The change in electrode impedance of semiconductor equipment due to repetitive processes is a major issue that creates process drift. In the current plasma etch chamber with a dual-frequency power system, the high-powered radio frequency (RF) source contributes to the enhancement of the plasma density, and the low-frequency bias power at the bottom electrode is adopted to enhance the injected ion energy in the plasma. The impedance control of the top electrode in dual-frequency capacity coupled plasma limits the impedance matching capability of the RF matching system because it only considers the high-frequency RF source. To control the precise impedance in dual-frequency semiconductor equipment, independent impedance control is required for each frequency. In this study, the impedance corresponding to a specific frequency was independently controlled using L (inductor) and C (capacitor). A 60 MHz stop filter and VVC were used to control 2 MHz impedance at a specific point, and a 2 MHz stop filter and VVC were used to control 60 MHz impedance. In the case of 2 MHz impedance control, the 2 MHz impedance changed from 10.9−<i>j</i>893 to 0.3−<i>j</i>62 and the 60 MHz impedance did not change. When controlling the 60 MHz impedance, the 60 MHz impedance changed from 0.33 + <i>j</i>26.53 to 0.2 + <i>j</i>190 and the 2 MHz impedance did not change. The designed LC circuits cover the impedance of 60 and 2 MHz separately and are verified by the change in the capacitance of the vacuum variable capacitors implemented in the RF impedance matching system. |
topic |
dual-frequency capacitively coupled plasma process drift impedance matching |
url |
https://www.mdpi.com/2079-9292/10/17/2074 |
work_keys_str_mv |
AT jeongsulee dualfrequencyrfimpedancematchingcircuitsforsemiconductorplasmaetchequipment AT sangjeenhong dualfrequencyrfimpedancematchingcircuitsforsemiconductorplasmaetchequipment |
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