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Low-impedance diodes with hollow tapered cathodes produce strong self-pinching in intense relativistic electron beams. Early in the pulse a thin hollow beam is formed, based on evidence of electrons striking the anode. This hollow beam collapses, accelerating toward the diode axis with velocities (1 to 5 mm/nsec) which depend locally on the anode material. An efficient and stable pinch, less than 3 mm in diameter, is formed at the anode. In the center 0.1 cm², the power rises to 10¹¹ W in less than 3 nsec. About 50% of the total diode energy ({~} 9 kJ) is dissipated within the pinch region.
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Blaugrund et al. (1975) studied this question.
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