1989
DOI: 10.1016/0168-9002(89)90853-x
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Beam emittance forming line of the CW race-track microtron of the institute of nuclear physics of Moscow State University (INP MSU)

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“…AS with cell length increasing in proportion to velocity of the particles has low capture efficiency; that is when continuous beam is injected into the structure, only about 30% of the particles are captured, whereas the remaining particles leave the structure with the energy close to the energy of injection, or are absorbed by the beam channel walls. To get beams with high monochromaticity and small losses of current, a chopper and a buncher are used [20,21]. At that, the buncher is adjusted to achieve minimum length of the bunch in the first accelerating cell.…”
Section: B Beam Dynamicsmentioning
confidence: 99%
“…AS with cell length increasing in proportion to velocity of the particles has low capture efficiency; that is when continuous beam is injected into the structure, only about 30% of the particles are captured, whereas the remaining particles leave the structure with the energy close to the energy of injection, or are absorbed by the beam channel walls. To get beams with high monochromaticity and small losses of current, a chopper and a buncher are used [20,21]. At that, the buncher is adjusted to achieve minimum length of the bunch in the first accelerating cell.…”
Section: B Beam Dynamicsmentioning
confidence: 99%