Open AccessEnergy density distribution of a modulated electron beam in a source with a plasma cathode based on a low pressure arc
Author(s) -
V. I. Shin,
P. V. Moskvin,
M. S. Vorobyov,
V. N. Devyatkov,
N. N. Koval
Publication year - 2021
Publication title -
journal of physics. conference series
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.21
H-Index - 85
eISSN - 1742-6596
pISSN - 1742-6588
DOI - 10.1088/1742-6596/2064/1/012066
Subject(s) - atomic physics , beam (structure) , cathode ray , pulse duration , plasma , arc (geometry) , amplitude , cathode , pulse (music) , current density , electron , current (fluid) , electron density , m squared , laser beam quality , optics , chemistry , physics , laser , laser beams , geometry , mathematics , quantum mechanics , detector , thermodynamics
The article presents the results of studies devoted to the study of the energy density distribution in the amplitude-modulated regime of electron beam generation. It is shown that in the first ≈ 50 μs of the duration of the beam current pulse, its spatial rearrangement occurs, due to the development of the arc discharge current. Thus, the rearrangement of the arc current, which develops from the axis of the system, leads to an axial diving of the emission current density and the beam current density on the target. With the development of the arc current, the energy density on the target on the axis of the system decreases and after ≈ 50 μs takes on a steady-state value, which can change only as a result of a change in the conditions for generating an electron beam or the transition to a modulated regime of electron beam generation. It has been experimentally shown using calorimetric measurements that the shape of the electron beam current pulse with its amplitude modulation with a pulse duration of more than 100 μs has little effect on the distribution of the beam energy density in the target region.