Author/Authors :
Ponce، نويسنده , , D.M. and Niemann، نويسنده , , C. and Yu، نويسنده , , S.S. and Leemans، نويسنده , , W.P. and Fessenden، نويسنده , , T.J. and Dahlbacka، نويسنده , , G. and Sharp، نويسنده , , W.M. and Taushwitz، نويسنده , , A.، نويسنده ,
Abstract :
An alternate technique for heavy ion final transport, from the driver to the target, is by the use of the self-standing Z-pinched plasma channel. Experiments conducted at the Lawrence Berkeley National Laboratory have produced 40 cm long stable plasma channels with a peak discharge current of 55 kA in a 7 Torr nitrogen gas fill. These channels are produced using a double pulse discharge scheme, namely, a pre-pulse discharge and a main capacitor bank discharge. It is postulated that the channelʹs insensitivity to MHD instabilities within the time scale relevant to beam transport is due to the wall effect the pre-pulse discharge creates. This is accomplished by leaving a gas density depression on the channelʹs axis after hydrodynamic expansion. Since the pre-pulse discharge creates the initial conditions for the main bank Z-pinch, it is critical to understand how to control and engineer the pre-pulse. Here we present some of the results of ongoing experiments geared to understand the underlying physics of the LBNL Z-pinch plasma channel. Schlieren and phase contrast measurements show the radial propagation of a shock wave during the pre-pulse discharge and suggest indirectly the evidence of the on axis gas density depression, that is believed to be <110 of the original gas fill pressure. For the main bank Z-pinch, interferometry show an integrated electron line density of 1.6×1017 cm−2 for a 15 kV discharge on axis. These measurements coupled with Faraday rotation measurements will indicate ultimately the current density distribution in the channel. This data will be used to benchmark simulation codes.