Pulsed rf Discharges


Chemically reactive plasmas are widely used in modification of the surface properties of materials. It is important for these technological applications to have good control over the plasma behaviour, in particular the flux of ions and radical species to the substrate; the ion impact energy and angular distribution; and the electron temperature. Improved control over some of these parameters has been obtained in low pressure rf plasmas by turning the source voltage on and off, with pulse lengths of the order of micro to milliseconds, which is much longer than rf period. Pulsed rf plasmas have been used to achieve improved conditions for processing in both etching of semiconductors and deposition of thin films [1-3]. However, at the present time, the mechanisms behind this improvement are still not well understood. In particular the temporal behaviour of the plasma during the breakdown phase, including sheath creation and the development of ion and electron distributions, require more detailed study.

Pulsed plasmas are also important for studying the fundamental physical processes taking place during non-equilibrium discharge conditions, such as breakdown. At SP3 studies have been made of plasma breakdown, using experimental measurements of a pulsed plasma together with simulation results, to shed light on the evolution of the bias voltage in asymmetric reactor geometry (see "Charging of the blocking capacitor in an asymmetric discharge" ). The effect of applying multiple pulses is discussed in the paper "Pulsing a low pressure rf plasma" . Simulations have also been used to study processes such as breakdown ("Simulation of plasma breakdown in a low pressure rf plasma" ) and the multipactor effect, which up until now have only recieved theoretical treatment [4].


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References

  1. R.W. Boswell, and D. Henry, Appl. Phys. Lett. 47,1095 (1985)
  2. L. J. Overzet, J. T. Verdeyen, and J. Beberman, J. Appl. Phys. 66, 1622 (1989).
  3. Y. Watanabe, M. Shiratani, Y. Kubo, I. Ogowa, and S. Ogi, Appl. Phys. Lett. 53, 1263 (1988).
  4. D. Vender, H.B. Smith, and R.W. Boswell, J. Appl. 80,4292 (1996).