I. Introduction
Since the terrorist attacks of 9-11 the needs of the EOD community continue to evolve and the desire for higher-energy operation and even more compact pulsed-power radiation generating units has arisen [1]. Simply stated, the need to radiograph ever-smaller objects through ever-thicker shielded containers is a challenging problem. To resolve small features in a thick object, one needs to carefully match both the x-ray flux and the x-ray energy to obtain optimal statistical information [2]).