Abstract

Metallic mirrors are to be used extensively within ITER for diagnostics and real time control. Erosion of the first wall within ITER will cause particles to be redeposited around the machine, including on these first mirrors, which will cause a reduction in reflectivity and a degradation in quality of signal received by the detectors. Powering these mirrors to form capacitively-coupled plasmas (CCPs) with an induced self bias, and using the ions within the plasmas to bombard and remove the deposits, has shown some experimental success in recovering mirror reflectivity. In this work the ion energy distribution functions (IEDFs) from an Ar CCP formed on a 5 cm radius metallic mirror are modelled and investigated using the hybrid plasma equipment model. Initially a geometry variation is done showing that a simple increase in reactor volume can significantly impact the spatial distribution of the ion flux to the mirror surface leading to non-uniform etch rates across the surface, even after the maximum bias has been achieved. The ion energies need to be sufficient to remove depositions (focussing on the first wall material of Be which forms a surface oxide BeO) but not subsequently damage the underlying mirror. In order to achieve this both the voltage (50–1000 V) and the frequency (13.56–60 MHz) have been varied within the model showing trends that may lead towards IEDF optimisation. The increase in voltage increases the self bias linearly and the plasma density super-linearly, whereas increasing the frequency barely effects the self bias while increasing the plasma density sub-linearly. Both increases cause an increase in ion flux for these reasons but both also decrease the homogeneity of the ion flux across the mirror surface which will be required should the energies be above the threshold for the mirror. These results are also unique to the geometry being investigated and thus the conclusion is that it would be prudent to model individual mirror geometries to find optimal parameters. This becomes especially clear with the introduction of a perpendicular magnetic field into the simulation that significantly reduces electron transport within the plasma.

Highlights

  • Erosion of the first wall within ITER will cause particles to be redeposited around the machine, including on these first mirrors, which will cause a reduction in reflectivity and a degradation in quality of signal received by the detectors

  • In this work the ion energy distribution functions (IEDFs) from an Ar capacitively-coupled plasmas (CCPs) formed on a 5 cm radius metallic mirror are modelled and investigated using the hybrid plasma equipment model

  • The increase in voltage increases the self bias linearly and the plasma density super-linearly, whereas increasing the frequency barely effects the self bias while increasing the plasma density sub-linearly. Both increases cause an increase in ion flux for these reasons but both decrease the homogeneity of the ion flux across the mirror surface which will be required should the energies be above the threshold for the mirror

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Summary

Author to whom any correspondence should be addressed

The ions created within this plasma can be attracted to the surface with sufficient energy to sputter the deposited material using a self-bias voltage [8] This is physical etching and is a well understood process that is used extensively in the manufacturing of microprocessors [9, 10]. This is compounded through the use of a blocking capacitor between the electrode and the AC supply which stops the electrons, that have reached the surface during the RF cycle, from flowing to ground [12] This imparts a DC component which further increases the sheath width such that ions may accelerate to an energy that is a combination of the plasma potential and the self bias voltage. This is half of that of Al2O3 [20, 21]

Methods
Geometry variation
Voltage variation
Frequency variation
Influence of a magnetic field
Conclusion
Full Text
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