2021
DOI: 10.1140/epjp/s13360-021-01312-3
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Electron bunchers for industrial RF linear accelerators: theory and design guide

Abstract: The acceleration of electrons in resonant linear accelerators (linacs) typically consists of three main stages: (1) emission of the electrons from the cathode and their pre-acceleration with a DC field to the energy of tens of keV; (2) grouping the DC electron beam into bunches and their synchronization with the correct phase of high-frequency electromagnetic fields, and (3) accelerating the bunches of relativistic electrons to the required energies. Although many books describe the theoretical and practical a… Show more

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Cited by 20 publications
(11 citation statements)
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“…A conceptual design for the typical high-current linac is presented in Figure 2. While this design differs from those of standard medical linacs, the design is characteristic of those found in high-current industrial settings and scientific laboratories (Adolphsen et al, 2014;Kutsaev, 2021a) The thermionic electron gun with a DC Pierce geometry gun and gridded cathode can provide 1.5-3 A continuous beam, accelerated to 100-150 keV energies, so that losses in the injection system yield at least 25% of the initial current after the acceleration.…”
Section: Accelerator Designmentioning
confidence: 99%
“…A conceptual design for the typical high-current linac is presented in Figure 2. While this design differs from those of standard medical linacs, the design is characteristic of those found in high-current industrial settings and scientific laboratories (Adolphsen et al, 2014;Kutsaev, 2021a) The thermionic electron gun with a DC Pierce geometry gun and gridded cathode can provide 1.5-3 A continuous beam, accelerated to 100-150 keV energies, so that losses in the injection system yield at least 25% of the initial current after the acceleration.…”
Section: Accelerator Designmentioning
confidence: 99%
“…In this section, we have summarized the techniques used to simulate the geometry of a medical linear accelerator by two codes based on the Geant4 toolkit: G4Linac_MT [8] and GATE [14]. The efficiency of the Monte Carlo calculation depends on the simulated events, the correct initiation of the initial parameters, the correct modeling of the LINAC geometry.…”
Section: Monte Carlo Simulationmentioning
confidence: 99%
“…accelerated to create collisions on the target. The energy of the electrons accelerated by the 6MV voltage is generally between 0 and 9 MeV [8,25]. In the Monte Carlo simulation of the dose delivered by LINACs, only the treatment head is modeled from the x-ray target.…”
Section: Initial Parametersmentioning
confidence: 99%
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“…The split structure has higher efficiency (shunt impedance and Q-factor) due to the thinner iris, and also higher peak electric and magnetic fields for the same gradient due to the gap between halves. It is worth noting that some parameters (peak-to-accelerating-field ratio, filling time and pulse heating) are higher than they will be in a traveling wave structure of the same iris shape [34].…”
Section: Design and Simulationsmentioning
confidence: 99%