2007 IEEE Particle Accelerator Conference (PAC) 2007
DOI: 10.1109/pac.2007.4439921
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Efficient accelerating structures for low-energy light IONS

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Cited by 4 publications
(10 citation statements)
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“…At the high-energy end of our deuteron linac, at 0.065 β = , the differences in efficiency and size between H-structures and DTL become somewhat smaller but still are very significant, see [10] for details. One should mention that the accelerating structures presented in Tab.…”
Section: H-mode Accelerating Structures H-mode Structures Versus Dtlmentioning
confidence: 99%
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“…At the high-energy end of our deuteron linac, at 0.065 β = , the differences in efficiency and size between H-structures and DTL become somewhat smaller but still are very significant, see [10] for details. One should mention that the accelerating structures presented in Tab.…”
Section: H-mode Accelerating Structures H-mode Structures Versus Dtlmentioning
confidence: 99%
“…The venerable LANSCE DTL has been in service for $40 years. In view of recent plans to upgrade the linac front end [33], we have explored [34] a potential option of replacing the aging DTL (or some parts of it) by more efficient H-PMQ accelerating structures. The LANSCE DTL consists of four DTL tanks; the parameters of the first three tanks are listed in Table VII [13].…”
Section: Ch-pmq Linac As a Dtl Replacementmentioning
confidence: 99%
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“…Moreover, if this short 1.8-m RFQ were connected to a short 1.3-m drift tube linac (DTL), a beam of 4-MeV deuterons could be obtained in a much shorter length than an equivalent single RFQ, which would be roughly 8 m long. This combination also consumes less than 90 kW of rf power because of the high accelerating gradient of the DTL [8]. Thus, it would be a very efficient injector for compact neutron sources.…”
Section: Introductionmentioning
confidence: 99%