The electron velocity distribution function in the plasma, formed by gas ionization by a microwave pulse of sub-nanosecond timescale width and hundreds of megawatts power, is studied by a theoretical model and by 3D numerical simulations which confirm quite well the model. It is shown that the distribution function is defined by the field amplitude variation during the entire pulse. After the pulse's passage through the gas, the remaining plasma distribution function follows a decreasing power-law function. Experiments performed in a waveguide filled with helium gas confirm that energetic (from several keV to several tens of keV) electrons remain in plasma long after the pulse has crossed the experimental volume. These electrons continue the gas ionization over extended times up to tens of nanoseconds.
Read full abstract