scholarly journals Effects of energy chirp on bunch length measurement in linear accelerator beams

2017 ◽  
Vol 28 (8) ◽  
pp. 084002 ◽  
Author(s):  
L Sabato ◽  
P Arpaia ◽  
A Giribono ◽  
A Liccardo ◽  
A Mostacci ◽  
...  
Author(s):  
Philipp Heil ◽  
Kurt Aulenbacher ◽  
Christoph Matejcek ◽  
Simon Friederich ◽  
Max Bruker ◽  
...  

2017 ◽  
Vol 12 (09) ◽  
pp. T09001-T09001
Author(s):  
H.K. Pandey ◽  
S. Dechoudhury ◽  
T.K. Bhattacharyya ◽  
A. Chakrabarti

Author(s):  
V.E. Kaljuzhny ◽  
D.V. Kostin ◽  
N.P. Sobenin ◽  
S.N. Yarigin ◽  
A.A. Zavadtsev ◽  
...  

Author(s):  
B. Y. Wang ◽  
B. G. Sun ◽  
J. G. Wang ◽  
P. Lu ◽  
H. L. Xu ◽  
...  

2011 ◽  
Vol 35 (5) ◽  
pp. 505-508
Author(s):  
Ying-Chao Du ◽  
Jian-Fei Hua ◽  
Li-Xin Yan ◽  
Qiang Du ◽  
Wen-Hui Huang ◽  
...  

2020 ◽  
Vol 10 (1) ◽  
Author(s):  
Ji-Gwang Hwang ◽  
Tsukasa Miyajima ◽  
Yosuke Honda ◽  
Eun-San Kim

Abstract We demonstrate an experimental methodology for measuring the temporal distribution of pico-second level electron bunch with low energy using radial electric and azimuthal magnetic fields of an accelerating ($$\hbox {TM}_{01}$$ TM 01 mode) radio frequency (RF) cavity that is used for accelerating electron beams in a linear accelerator. In this new technique, an accelerating RF cavity provides a phase-dependent transverse kick to the electrons, resulting in the linear coupling of the trajectory angle with the longitudinal position inside the bunch. This method does not require additional devices on the beamline since it uses an existing accelerating cavity for the projection of the temporal distribution to the transverse direction. We present the theoretical basis of the proposed method and validate it experimentally in the compact-energy recovery linac accelerator at KEK. Measurements were demonstrated using a 2-cell superconducting booster cavity with a peak on-axis accelerating field ($$E_0$$ E 0 ) of 7.21 MV/m.


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