2003
DOI: 10.1063/1.1583860
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Development of movable mask system to cope with high beam current

Abstract: Application of a sawtooth surface to accelerator beam chambers with low electron emission rate

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Cited by 6 publications
(11 citation statements)
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“…If the length of the mask head is 90 mm, the ratio of that to the radiation length is about 1.2, which is almost the same as that used in KEKB (40 mm Ti head, where the radiation length of Ti is 36 mm [25]). On the other hand, when an intense highenergy beam hits the mask head directly, the deposited energy is likely to cause a groove on the head [6,7]. Al 2 O 3 has a melting point of over 2000 C, and is said to be available up to about 1700 C. The melting point is higher than that of the titanium (1670 C).…”
Section: Basic Conceptmentioning
confidence: 96%
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“…If the length of the mask head is 90 mm, the ratio of that to the radiation length is about 1.2, which is almost the same as that used in KEKB (40 mm Ti head, where the radiation length of Ti is 36 mm [25]). On the other hand, when an intense highenergy beam hits the mask head directly, the deposited energy is likely to cause a groove on the head [6,7]. Al 2 O 3 has a melting point of over 2000 C, and is said to be available up to about 1700 C. The melting point is higher than that of the titanium (1670 C).…”
Section: Basic Conceptmentioning
confidence: 96%
“…The trapped mode could be a source of discharge near the mask head, heating of the mask head and the support, and also excitation of any beam instability [1,3,[5][6][7]11]. The HOM absorber, however, can be a HOM source, itself, and so the quantity of the absorber should be as small as possible.…”
Section: Basic Conceptmentioning
confidence: 99%
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