DocumentCode
409112
Title
Energy dispersion compensation and beam loading in X-band linacs for the JLC/NLC
Author
Jones, R.M. ; Dolgashev, V.A. ; Miller, R.H. ; Adolphsen, C. ; Wang, J.W.
Author_Institution
SLAC, Stanford, CA, USA
Volume
4
fYear
2003
fDate
12-16 May 2003
Firstpage
2763
Abstract
The shape of an RF pulse is distorted upon propagating through an X-band accelerator structure due to dispersive effects. This distortion together with beam loading introduce energy spread between 192 bunches. In order to minimize this energy spread we modify the input RF pulse shape. The pulse propagation, energy gain, and beam loading are modelled with a mode-matching computer code and a circuit model. A 2D model and a circuit model of a complete 60 cm structure, consisting of 55 cells and input and output couplers is analyzed. This structure operates with a 5π/6 phase advance per cell. Dispersive effects for this structure are more significant than for previously studied 2π/3 phase advance accelerating structures. Experimental results are compared with the theoretical model and excellent agreement is obtained for the propagation of an RF pulse through the structure.
Keywords
accelerator RF systems; beam handling techniques; electron accelerators; linear colliders; particle beam bunching; 2D model; 5pi/6 phase advance; 60 cm; JLC/NLC; Next Linear Collider/Japanese Linear Collider; RF pulse propagation; X-band accelerator structure; X-band linacs; beam loading; circuit model; distorted RF pulse shape; electron bunches; energy dispersion compensation; energy gain; energy spread; input coupler; mode-matching computer code; output coupler; Acceleration; Circuit simulation; Dispersion; Linear accelerators; Optical reflection; Pulse circuits; Pulse measurements; Pulse shaping methods; Radio frequency; Shape measurement;
fLanguage
English
Publisher
ieee
Conference_Titel
Particle Accelerator Conference, 2003. PAC 2003. Proceedings of the
ISSN
1063-3928
Print_ISBN
0-7803-7738-9
Type
conf
DOI
10.1109/PAC.2003.1289260
Filename
1289260
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