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  6. [Case Study] Plasma Analysis of "Particle-PLUS" Dual Frequency CCP

[Case Study] Plasma Analysis of "Particle-PLUS" Dual Frequency CCP

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Particle-PLUS

last updated:Jan 20, 2022

ウェーブフロント 本社
ウェーブフロント 本社
  • Official site

Introduction to Particle-PLUS Analysis Case: "Plasma Analysis of Dual Frequency CCP" Simulation Case

This is a case study on plasma analysis of CCP (Capacitively Coupled Plasma) devices. Particle-PLUS specializes in plasma analysis within vacuum chambers and can perform high-speed simulations even when multiple electrodes are present or when applying overlapping frequencies. ◇ Features of 'Particle-PLUS' - Excels in low-pressure plasma analysis. - By combining axisymmetric models with mirror-symmetric boundary conditions, it can quickly obtain results without the need for full device simulations. - Specializes in plasma simulations for low-pressure gases, where calculations using fluid models are challenging. - Supports 2D (two-dimensional) and 3D (three-dimensional) analyses, efficiently handling complex models. - As a strength of our in-house developed software, customization to fit the customer's device is also possible. ◆ Various calculation results can be output ◆ - Potential distribution - Density distribution/temperature distribution/generation distribution of electrons and ions - Particle flux and energy flux to the wall - Energy spectrum of electrons and ions at the wall - Density distribution/temperature distribution/velocity distribution of neutral gas and more. *For more details, please feel free to contact us.

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スライド1.JPG

[Case Study] Plasma Analysis of "Particle-PLUS" Dual Frequency CCP

スライド1.JPG
スライド1.JPG
  • Related Link - http://www.wavefront.co.jp/CAE/particle-plus/

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basic information

**Features** - The time scheme uses an implicit method, allowing for stable time evolution calculations over a large time step Δt compared to conventional methods. - The collision reaction model between neutral gas and electrons and ions employs the Monte Carlo Scattering method, enabling accurate and rapid calculations of complex reaction processes. - The neutral gas module determines the initial neutral gas distribution used in the plasma module above, allowing for quick evaluation of gas flow using the DSMC method. - The sputtered particle module calculates the behavior of atoms sputtered from the target in devices such as magnetron sputtering systems, enabling quick evaluation of flux distribution on opposing substrates. *For other functions and details, please feel free to contact us.*

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Applications/Examples of results

【Dual Frequency Capacitive Coupled Plasma】 - Optimization of voltage and other parameters to obtain high-density plasma - Damage to chamber walls - Optimization of power using external circuit models - It is possible to apply voltages to the electrode plates that align with real devices - The waveform of the applied voltage can be simulated smoothly and with relatively realistic voltages - Calculations are relatively stable to avoid applying excessive voltages 【DC Magnetron Sputtering】 - Uniformity of erosion dependent on magnetic field distribution - Adsorption distribution of sputtered materials on the substrate 【Pulsed Voltage Magnetron Sputtering】 - Optimization of the application time of pulsed voltage for efficient material sputtering 【Ion Implantation】 - Influence of the substrate on erosion distribution 【Time Evolution of Applied Voltage on Electrode Plates】 - Enables observation of physical quantities that are difficult to measure experimentally, such as electron density and ion velocity distribution - By investigating electron density and ion velocity distribution, it is possible to examine the uniformity of the film and damage to the chamber walls - Changing calculation conditions allows for optimization of high-density plasma generation at low power

Detailed information

  • スライド1.JPG

    This is a case study on plasma analysis of CCP (Capacitively Coupled Plasma) devices. Particle-PLUS specializes in plasma analysis within vacuum chambers and can perform high-speed simulations even in cases with multiple electrodes or when applying overlapping frequencies.

  • スライド2.JPG

    ◇Model Overview Conducted plasma analysis of 2-frequency CCP using an axisymmetric model.

  • スライド3.JPG

    Electric potential - Since the electron speed is considerably faster than the ion speed, ions are left behind in the plasma, resulting in a slight positive charge in the plasma. - Due to the self-bias effect, the electrodes are negatively charged. The high-frequency side has a self-bias of about -20 V, while the low-frequency side has a self-bias of about -150 V.

  • スライド4.JPG

    Transition of Particles - Change in particle number over time: It reaches a steady state in about 1×10^(−5) seconds, achieving a balance between the generation and annihilation of plasma particles. - Time variation of accumulated charge: It can be inferred that ions are left behind in the chamber, causing the plasma charge to be positively biased.

  • スライド5.JPG

    Particle number density Electron number density (periodic average) Ar ion number density (periodic average)

  • スライド6.JPG

    Ar ion flux Ar ion number flux (time-averaged) Ar ion energy flux (time-averaged) In Particle-PLUS, these flux distributions can be used to calculate the sputtering phenomenon.

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