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Abstracts Brochure - CERN

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WEPCH — Poster Session 28-Jun-06 16:00 - 18:00<br />

Study of the Effect of Multipolar Components in the SPARC Emittance Compensation<br />

Gun Solenoid<br />

The SPARC photoinjector rf gun requires a<br />

solenoid immediately downstream for emittance<br />

compensation. The analysis of the measured<br />

solenoid magnetic maps shows the existence<br />

of multipolar components added to<br />

the pure solenoid field. The effect of these<br />

C. Ronsivalle, G. Dattoli, L. Picardi, M. Quattromini (ENEA C.R.<br />

Frascati) G. Bazzano (CNAO Foundation) M. Ferrario, M. Migliorati,<br />

L. Palumbo, M.A. Preger, C. Sanelli (INFN/LNF) P. Musumeci<br />

(INFN-Roma) J.B. Rosenzweig (UCLA)<br />

added fields on beam dynamics and possible correction schemes have been studied from the theoretical point of view<br />

and by numerical calculations based on PARMELA/TREDI codes. An accurate 3D numerical modelization by using<br />

CST EM Studio has been done, in order to investigate the source of these multipolar components and to suggest some<br />

design modifications aimed to reduce their magnitude. The results of this study are presented here.<br />

Longitudinal Coherent Oscillation Induced in Quasi-isochronous Ring<br />

Noise sources, which excite longitudinal coherent<br />

oscillation is discussed. Especially in<br />

a quasi-isochronous electron storage ring an<br />

identification of the noise sources is impor-<br />

Y. Shoji, Y. Hisaoka, T. Mitsui (NewSUBARU/SPring-8, Laboratory<br />

of Advanced Science and Technology for Industry (LASTI))<br />

tant to obtain an extremely short bunch. One possible source is a well-known rf noise in the acceleration field. The<br />

other is a magnetic field ripple, which changes a path-length for a revolution. The analytical formula for the longitudinal<br />

coherent oscillation is explained. It contains the path-length oscillation, which had never been considered. The<br />

third is a beam itself, probably be a coherent radiation loss. The driving term is not symmetric along the energy axis,<br />

then the oscillation amplitude depends on the higher order momentum compaction factor.<br />

Matrix Formulation for Hamilton Perturbation Theory of Linearly Coupled Betatron Motion<br />

Linear coupled motion in a circular accelerator<br />

was successfully parametrized through M. Takao (JASRI/SPring-8)<br />

the transfer matrix approach, where normal<br />

mode Twiss and coupling parameters are defined as an extension of Courand and Snyder formulation. However it is<br />

not straightforward to assign analytical expressions to the coupling parameters. On the other hand the coupled motion<br />

was analytically solved by the Hamilton perturbation theory, which ingeniously describes the resonance phenomena.<br />

In the perturbation theory, however, the symplectic structure of the coupled motion is obscure in turn. Hence, for the<br />

purpose of combining both the theories with each other with keeping the respective virtues, we develop the matrix<br />

formulation based on the Hamilton perturbation theory. Since we have already known the solution of equation of<br />

motion, we can construct the transfer matrix in terms of the solution. Thus we formulate the betatron motion with<br />

linear coupling resonance in analytic and symplectic manner. As an application of the formulation, we investigate<br />

the two-dimensional beam ellipse in an electron storage ring.<br />

279<br />

WEPCH022<br />

WEPCH023<br />

WEPCH024

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