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Accelerator design at SuperKEKB

delete2013-03-26
delete165
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OA
AI
Y
Y. Ohnishi *
A
Abe, Tetsuo
T
Toshikazu Adachi
K
K. Akai
Y
Y. Arimoto
E
Ebihara, Kiyokazu
K
K. Egawa
J
J. Flanagan
H
H. Fukuma
Y
Y. Funakoshi
K
K. Furukawa
T
T. Furuya
N
N. Iida
H
H. Iinuma
H
H. Ikeda
T
Takuya Ishibashi
M
M. Iwasaki
T
T. Kageyama
S
S. Kamada
T
T. Kamitani
K
K. Kanazawa
M
M. Kikuchi
H
H. Koiso
M
M. Masuzawa
T
T. Mimashi
T
Takako Miura
T
T. Mori
A
A. Morita
T
T. Nakamura
N
Nakanishi, Kota
H
Hiroyuki Nakayama
M
Michiru Nishiwaki
Y
Y. Ogawa
K
K. Ohmi
N
N. Ohuchi
K
K. Oide
T
T. Oki
M
Masaaki Ono
M
M. Satoh
S
Shibata, Kyo
M
M. Suetake
Y
Y. Suetsugu
R
R. Sugahara
H
H. Sugimoto
T
T. Suwada
M
M. Tawada
M
M. Tobiyama
N
N. Tokuda
K
K. Tsuchiya
H
H. Yamaoka
Y
Y. Yano
M
M. Yoshida
S
S. Yoshimoto
D
Demin Zhou
Z
Zhanguo Zong
DOI:10.1093/ptep/pts083delete
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摘要

摘要

En 中文
The SuperKEKB project requires a positron and electron collider with a peak luminosity of 8 x 10(35) cm(-2) s(-1). This luminosity is 40 times that of the KEKB B-factory, which operated for 11 years up to 2010. SuperKEKB is an asymmetry-energy and double-ring collider; the beam energy of the positron (LER) is 4 GeV and that of the electron (HER) is 7 GeV. An extremely small beta function at the interaction point (IP) and a low emittance are necessary. In addition, in order to achieve the target luminosity, a large horizontal crossing angle between two colliding beams is adopted, as is a bunch length much longer than the beta function at the IP. This method is called the nano-beam scheme. The beam-beam parameter is assumed to be similar to KEKB, the beta function at the IP is 1/20, and the beam currents are twice those of KEKB in the nano-beam scheme. Consequently, the luminosity gain of 40 with respect to KEKB can be obtained.
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Progress of Theoretical and Experimental Physics 封面图
Progress of Theoretical and Experimental Physics
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high energy accelerator research organization (kek)
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