Abstract
From (1.12) at a fixed location s we can write \(x = \sqrt {2{I_x}{\beta _x}} \cos {\phi _x},\)where φx includes the initial phase φ0 We then have
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References
R. Assmann, A. Chao: Dispersion in the Presence of Strong Transverse Wake- fields. In: Proc. PAC 97, Vancouver, 1997 (IEEE, Piscataway 1998) P. 1523
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Minty, M.G., Zimmermann, F. (2003). Solutions to Exercises. In: Measurement and Control of Charged Particle Beams. Particle Acceleration and Detection. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-662-08581-3_12
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DOI: https://doi.org/10.1007/978-3-662-08581-3_12
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