Time-resolved evolution of plasma parameters in a plasma immersion ion implantation source

The origin and nature of perturbations induced by a high-voltage pulse on plasma parameters and their relationship to operating conditions (power and pressure) in an argon inductively coupled radio frequency plasma device is explored. The plasma parameters are measured with two radio frequency compensated Langmuir probes positioned either vertically above the pulsing target or horizontally along the diameter of the chamber, in the same axial plane as the target and same distance from the RF antenna. Fluctuations are observed in electron density n(e), temperature T-e, and plasma potential V-pl following negative polarity high voltage pulses and propagate deep in the plasma and well after the end of the pulse. Time-resolved data results indicate that the perturbations are significantly dampened at higher power as well as when closer to the plasma RF coil. The perturbation amplitudes depart significantly from steady state values when the pulse amplitude exceeds 2.0 kV and increase with the increasing pulse amplitude. Perturbation amplitudes are also higher for target materials having larger secondary electron yield. Our experimental results suggest that the underlying mechanism of this perturbation could be plasma heating driven by damping of a beam-plasma instability as a result of a beam of secondary electrons emitted by the target streaming into the plasma.

Automated summary

The study investigates the perturbations induced by high-voltage pulses on plasma parameters in an argon inductively coupled radio frequency plasma device, where fluctuations in electron density, temperature, and plasma potential are observed following negative polarity pulses. The perturbations are significantly dampened at higher power and closer to the plasma RF coil, with amplitudes increasing with pulse amplitude and secondary electron yield from the target material. The underlying mechanism of the perturbation is suggested to be plasma heating driven by damping of a beam-plasma instability due to a beam of secondary electrons emitted by the target.