DISCLAIMERThis document wasprepared as an account of workspoxsoredby an agency of the United States Government. Neither the United States Government nor the UniversityofCalifornianoranyof theiremployees,makesanywarranty,express or implied, or assumes any legal liability of responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disdosed, or repmerits that its use would not infringe privately owned rights. Referenceherein toanyspecificcommeraalproduck,process,orserviceby trade name, trademark, manufacturer, or otherwise, does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or the University of California. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or the University of California, and shall not be used for advertising or product endorsement purposes. September 1, 1995 Abstract Chamber transport is an important area of study for heavy ion fusion. Final focus and chamberrtransport are high leverage areas providing opportunities to significantly decreke the cost of electricity from a heavy ion fusion power plant. Chamber transport in two basic regimes is under consideration. In the low chamber density regime ( 5 0.003 torr), ballistic or nearly-ballistic transport is used. Partial beam neutralization has been studied to offset the effects of beam stripping. In the high chamber density regime ( 2 .1 torr), two transport modes (pinched transport and channel transport) are under investigation. Both involve focusing the' beam outside the chamber then transporting it at small radius ( M 2 mm). Both high chamber density modes relax the constraints on the beam quality needed from the accelerator which will reduce the driver cost and the cost of electricity...