Stable top-up operation at SPring-8

Tanaka, H.; Adachi, M.; Aoki, T.; Asaka, T.; Baron, A.; Daté, S.; Fukami, K.; Furukawa, Y.; Hanaki, H.; Hosoda, N.; Ishikawa, T.; Kimura, H.; Kobayashi, K.; Kobayashi, T.; Kohara, S.; Kumagai, N.; Masaki, M.; Masuda, T.; Matsui, S.; Mizuno, A.; Nakamura, T.; Nakatani, T.; Noda, T.; Ohata, T.; Ohkuma, H.; Ohshima, T.; Oishi, M.; Sasaki, S.; Schimizu, J.; Shoji, M.; Soutome, K.; Suzuki, M.; Suzuki, S.; Suzuki, Y.; Takano, S.; Takao, M.; Takashima, T.; Takebe, H.; Takeuchi, A.; Tamura, K.; Tanaka, R.; Tanaka, Y.; Taniuchi, T.; Taniuchi, Y.; Tsumaki, K.; Yamashita, A.; Yanagida, K.; Yoda, Y.; Yonehara, H.; Yorita, T.; Yoshioka, M.; Takata, M.

doi:10.1107/S0909049506022862

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Figure 4
Calculated bump leakage variation as a function of the ratio of two sextupole strengths in the bump orbit. Here the strengths of the bump magnets are adjusted to close the bump orbit at its peak amplitude in consideration of sextupole non-linearity. A pulse width of 3 µs was used in the calculation.

JOURNAL OF
SYNCHROTRON
RADIATION

ISSN: 1600-5775

Volume 13| Part 5| August 2006| Pages 378-391

doi:10.1107/S0909049506022862

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