I. INTRODUCTION
Creation of high-power sources of x-ray radiation is urgent for a number of applications. Achieved XR energy level is ~1.8, MJ at a power of ~290 TW. Such source is realized at PBFA-Z facility [1] at a liner implosion, which is formed of a multi-wire assembly, with a current having amplitude of ~18 MA and front t~100 ns. Along with that there is an interest to the XR sources having liner implosion times of several hundreds of nanoseconds and up to ~1 µs [2], [3]. One of the reasons of such an interest is relative simplicity of megampere current pulses obtaining having microsecond current rise time and conservation of energy proportionality of generated XR to square of current in the specified implosion time range [4], [5].