TY - JOUR
T1 - Effects of amplitude modulated capacitively coupled discharge Ar plasma on kinetic energy and angular distribution function of ions impinging on electrodes
T2 - Particle-in-cell/Monte Carlo collision model simulation
AU - Abe, Kohei
AU - Kamataki, Kunihiro
AU - Yamamoto, Akihiro
AU - Nagao, Iori
AU - Otaka, Michihiro
AU - Yamashita, Daisuke
AU - Okumura, Takamasa
AU - Yamashita, Naoto
AU - Itagaki, Naho
AU - Koga, Kazunori
AU - Shiratani, Masaharu
N1 - Funding Information:
This work was partly supported by JSPS KAKENHI (Grant No. JP19K03809 and JP20H00142) and JSPS Core-to-Core Program (Grant No. JSPSCCA2019002).
Publisher Copyright:
© 2022 The Japan Society of Applied Physics.
PY - 2022/10/1
Y1 - 2022/10/1
N2 - We investigated the effects of amplitude modulated (AM) capacitively coupled Ar discharge plasma on the ion energy distribution function (IEDF) and the ion angular distribution function (IADF) incident on electrodes using the particle-in-cell/Monte Carlo collision model. For AM discharge, the electron density and electron temperature and the kinetic energy and angle of ions incident on the ground electrode change periodically with AM frequency, whereas ones for continuous wave discharge are almost constant. For AM discharge, the plasma had hysteresis characteristics. The peak energy of IEDF varies from 53 to 135 eV and the FWHM of IADF varies from 1.82 to 3.34 degrees for gas pressure 10mTorr, the peak-to-peak input voltage 400 V and AM level of 50%. The variation width of the peak energy of IEDF and FWHM of IADF increases with the AM level. These effects of AM method discharge are more noticeable at lower pressures. Thus, the AM discharge offers a way to control simultaneously IEDF and IADF, which opens a new avenue for plasma processes such as an ALD-like PECVD.
AB - We investigated the effects of amplitude modulated (AM) capacitively coupled Ar discharge plasma on the ion energy distribution function (IEDF) and the ion angular distribution function (IADF) incident on electrodes using the particle-in-cell/Monte Carlo collision model. For AM discharge, the electron density and electron temperature and the kinetic energy and angle of ions incident on the ground electrode change periodically with AM frequency, whereas ones for continuous wave discharge are almost constant. For AM discharge, the plasma had hysteresis characteristics. The peak energy of IEDF varies from 53 to 135 eV and the FWHM of IADF varies from 1.82 to 3.34 degrees for gas pressure 10mTorr, the peak-to-peak input voltage 400 V and AM level of 50%. The variation width of the peak energy of IEDF and FWHM of IADF increases with the AM level. These effects of AM method discharge are more noticeable at lower pressures. Thus, the AM discharge offers a way to control simultaneously IEDF and IADF, which opens a new avenue for plasma processes such as an ALD-like PECVD.
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U2 - 10.35848/1347-4065/ac7626
DO - 10.35848/1347-4065/ac7626
M3 - Article
AN - SCOPUS:85138181153
SN - 0021-4922
VL - 61
JO - Japanese journal of applied physics
JF - Japanese journal of applied physics
IS - 10
M1 - 106003
ER -