2D Capacitive Plasma Chamber (capacitivelyCoupledPlasma2DT.pre)

Keywords:

capacitively coupled plasma discharge under RF and DC voltage in 2D cylindrical system.

Problem description

The capacitively coupled plasma (CCP) is one of the most common types of industrial plasma sources. These plasma discharges typically take place between metal electrodes in a reaction chamber and are driven by a radio frequency (RF) or direct current (DC) power supply. The plasma is sustained by ohmic heating in the main body and stochastic heating through the capacitive sheath.

This example demonstrates the generation of a capacitively coupled plasma inside an axially symmetric reaction chamber with a 50 mm radius and 50 mm length. The top and side walls are grounded at zero potential. A target located at the bottom of the chamber is connected to a 60 MHz AC voltage source at 200 V. There is a small gap of 5 mm between the target and the grounded wall. The chamber is filled with a background gas of Argon at about 0.005 Torr \(\left(2.0 \times 10^{20} \ \text{m}^{-3}\right)\). An initial electron density at \(10^{12} \ \text{m}^{-3}\) is seeded to start the discharge.

This simulation can be performed with a VSimPD license.

Opening the Simulation

The Capacitively Coupled Plasma 2D example is accessed from within VSimComposer by the following actions:

  • Select the NewFrom Example… menu item in the File menu.
  • In the resulting Examples window expand the VSim for Plasma Discharges option.
  • Expand the Capacitively Coupled Plasmas (text-based setup) option.
  • Select “2D Capacitive Plasma Chamber (text-based setup)” and press the Choose button.
  • In the resulting dialog, create a New Folder if desired, and press the Save button to create a copy of this example.

The basic variables of this problem should now be alterable via the text boxes in the left pane of the Setup Window, as shown in figure Fig. 471.

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Fig. 471 Setup Window for the Capacitively Coupled Plasma 2D example.

Input File Features

The self-consistent electric field is solved from Poisson’s equation by an electrostatic solver in cylindrical coordinates. Time-dependent Dirichlet boundary conditions are used to set up the boundaries of electric fields around the reaction chamber walls.

The plasma is simulated with macroparticles which are moved using the Boris pusher in cylindrical coordinates. Various types of elastic and inelastic collisions of the particles are calculated.

The Setup Window has various parameters available for easy manipulation including the density of the argon background gas (DENSITY_Ar), the voltage (VOLTAGE), and the frequency (FREQ).

Running the simulation

Once finished with the problem setup, continue as follows:

  • Proceed to the Run Window by clicking the Run button in the left column of buttons.
  • Choose your desired parallel computing options under Parallel Run Options.
  • To run the file, click on the Run button in the upper left corner of the Logs and Output Files pane. You will see the output of the run in that pane. The run has completed when you see the output, “Engine completed successfully.” This is shown in Fig. 472.
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Fig. 472 The Run Window at the end of execution.

Visualizing the results

After performing the above actions, continue as follows:

  • Proceed to the Visualize Window by clicking the Visualize button in the left column of buttons.

To plot the potential:

  • In the Variables section of the Visualization Controls pane, expand Scalar Data
  • Select phi
  • Move the dump slider at the bottom of the Visualization Results pane to the right to move forward in time. Once the slider is selected, the left and right arrow keys will control the slider position as well.
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Fig. 473 Visualization of the electric potential in \(r\)-\(z\) coordinates.

Further Experiments

With a time-step of \(10^{-11}\) seconds, running this simulation for the default 200 time-steps will only capture part of the first oscillation. With the frequency set to \(6\times 10^7\) Hz, the oscillation period is \(1.667\times 10^{-8}\) seconds, which corresponds to 1,667 time-steps. To see the approximate steady-state behavior of this example, set the number of time-steps to 10,000 or more and restart or re-run the simulation. When running in parallel on 4 processors, this should take approximately two hours to complete.

After \(5\times 10^{-8}\) seconds, or 500 dumps, the plasma sheath starts to exhibit oscillating steady-state behavior. To view the behavior of the oscillating plasma sheath, take the following steps:

  • In the Variables section of the Visualization Controls pane, expand Scalar Data
  • Select rho
  • At the top of the Visualization Results pane, click Colors to open the Color Options window
  • Select “Fix Minimum” and set the minimum to -0.0005, then select “Fix Maximum” and set the Maximum to 0.0005 (or experiment with minimum and maximum values for best results) and click OK
  • Move the dump slider at the bottom of the Visualization Results pane to dump 250. Once the slider is selected, the left and right arrow keys will control the slider position.

After 250 time-steps, the plasma density should appear as shown in Fig. 474. The green areas at approximately zero charge density denote the quasi-neutral plasma bulk, while the red areas (positive charge density) denote the non-neutral the plasma sheath.

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Fig. 474 Visualization of the plasma sheath via the charge density.

To view the plasma sheath potential profile, take the following steps:

  • In the Variables section of the Visualization Controls pane, select Field Analysis from the Data View drop-down menu
  • In the Field drop-down menu, select phi
  • Under Lineout Settings click on the Horizontal tab, and change the intercept value if desired
  • Click Perform Lineout

The electric potential as well as the axial potential profile should now be visible as shown in Fig. 475. Move the slider to the right to see how the plasma sheath potential oscillates in time.

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Fig. 475 Visualization of the plasma sheath via the charge density.