Bulletin of the American Physical Society
66th Annual Meeting of the APS Division of Plasma Physics
Monday–Friday, October 7–11, 2024; Atlanta, Georgia
Session FR01: Review: Advanced plasma modeling tools that can simulate plasmas used for semiconductor processing
8:00 AM–9:00 AM,
Tuesday, October 8, 2024
Hyatt Regency
Room: Centennial Ballroom I-III
Abstract: FR01.00001 : Advanced plasma modeling tools that can simulate plasmas used for semiconductor processing*
8:00 AM–9:00 AM
Presenter:
Igor D Kaganovich
(Princeton Plasma Physics Laboratory)
Authors:
Igor D Kaganovich
(Princeton Plasma Physics Laboratory)
Dmytro Sydorenko
(Department of Physics, University of Alberta, AB, Canada)
Andrew Tasman Powis
(Princeton Plasma Physics Laboratory, Princeton, USA)
Alexander V. Khrabrov
(Princeton Plasma Physics Laboratory)
Sierra E Jubin
(Princeton University)
Willca Villafana
(Princeton Plasma Physics Laboratory)
Yuri Barsukov
(Princeton Plasma Physics Laboratory)
Stephane Ethier
(Princeton Plasma Physics Laboratory, Princeton, USA)
Haomin Sun
(École polytechnique fédérale de Lausanne)
Sarveshwar Sharma
(Institute for Plasma Research)
Jian Chen
(Sun Yat-sen University, Zhuhai, China)
Shahid Rauf
(Applied Materials)
Sathya Swaroop Ganta
(Applied Materials Inc)
Abhishek Verma
(Applied Materials)
Kallol Bera
(Applied Materials)
Liang Xu
(Soochow University, China)
For plasma processing, there is a need to simulate large plasma devices via kinetic means, because the Electron Velocity Distribution Function in these devices is non-Maxwellian and therefore a fluid treatment is insufficient to accurately capture the physics. The method of choice for many fully kinetic simulations has been the particle-in-cell (PIC) technique due to relatively ease of implementation of the method and that it can be parallelized effectively over many processors and accelerated on GPUs. However, PIC codes that use standard explicit schemes are constrained by the requirement to resolve the short length and time scales associated with the plasma Debye radius and plasma frequency respectively [1]. This makes it extremely challenging to perform long time 2D PIC simulations for large plasma devices. For this reason, many 2D kinetic simulations of plasmas have been limited to small or artificially scaled systems. Energy conserving [2] or implicit methods [3] must be used to remove these limitations. Effects of numerical noise in simulations using PIC code need to be analyzed and taken into account [1]. The PIC codes have been applied to study plasma processing applications, such as capacitively coupled plasmas, electron beam produced plasmas, inductively coupled, hollow cathodes [4-9]. To model surface processes we used a combination of quantum chemistry methods and molecular dynamics [10-13]. For analysis of chemical reaction pathways, we employed direct sensitivity analysis and an uncertainty-aware strategy for plasma mechanism reduction with directed weighted graphs [14].
*Supported by the US Department of Fusion Energy Science.
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