Interaction of deuterium plasma of streams and shock-waves (velocities up to 5 × 10 7 cm s −1 ) and fast ion beams (50-150 keV) generated in a dense plasma focus (DPF) device with low-activated austenitic steel, 25Cr12Mn20W, and ferritic steel, 10Cr9W, specimens positioned in the cathode part of DPF chamber has been investigated. If the power flux density of both types of irradiation is about q = 10 5 -10 7 W cm −2 , then ion implantation into a surface layer of the materials was observed. An increase of this parameter till q = 10 7 -10 8 W cm −2 results in the so-called 'detachment' effect (screening of the specimen surface by a cold plasma cloud). When the power flux density is increased up to q = 10 9 -10 10 W cm −2 , the evaporated plasma cloud becomes of the same temperature as the plasma of the shock-wave, and melting and evaporation of material from the specimen surface appears to be very strong, thus the so-called 'broken-implantation' takes place.

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This paper reports on experiments undertaken to compare the radiation resistance of two types of ceramics, boron nitride (BN) and pure alumina (Al 2 O 3 ), which are used in a TAEA antenna coil installed in the MAST spherical tokamak. Samples of the investigated materials (bulk BN and a 20 µm film of Al 2 O 3 on Al substrate) were exposed on the axis of the plasma-focus PF-1000 device, which can emit intense streams of hot plasma (v ≈ 10 7 cm s −1 and N pl ≈ 10 18 cm −3 ) and fast deuteron beams (E i ≈ 100 keV). The most powerful plasma-ion pulse lasted 0.2-1.0 µs and its intensity decayed in about 100 µs. The irradiation process was diagnosed using fast optical cameras, laser interferometry and optical spectrometry. Experiments were performed at power flux densities equal to 10 9 -10 10 W cm −2 or 10 8 -10 9 W cm −2 during the most powerful stage of the interaction process. The irradiated specimens were investigated by means of optical microscopy and x-ray structure analysis (XRSA). It was shown that at 10 10 W cm −2 pulses the Al 2 O 3 coating was completely evaporated, whereas a surface of the BN sample became smoother than in the virgin one. A direct comparison of both samples after the action of 10 8 W cm −2 pulses demonstrated a wave-like structure (more distinct on Al 2 O 3 ). Weighing of these samples showed, however, that the evaporation of BN was about two times stronger than that of Al 2 O 3 in spite of the lower irradiation flux; the XRSA showed no evidence of cracking of Al 2 O 3 after these pulses. The insulation properties of Al 2 O 3 did not decline, and the Al 2 O 3 coating may be potentially more beneficial, provided that it is kept below its melting point. Characteristic features of damages of a material based on the carbon-fiber composite with additions of silicium carbide (SiC; 8-40% volumetric) were also investigated. It was found that at q = 10 9 W cm −2 , the surface erosion is associated with sputtering and evaporation. The degree of this erosion depends on the fibers' orientation in relation to the direction of the plasma-ion streams, and on the percentage of the SiC admixture.

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