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Abstracts Brochure - CERN

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MOPCH — Poster Session 26-Jun-06 16:00 - 18:00<br />

Study of the Electron Beam Dynamics in the FERMI @ ELETTRA Linac<br />

A study of the electron beam dynamics in<br />

the linac is made within the framework of<br />

the design of a free electron laser (FEL) at the<br />

Syncrotrone Trieste*. A scope of the work includes<br />

analysis of two operational scenarios,<br />

M. Cornacchia, P. Craievich, S. Di Mitri (ELETTRA) I.V. Pogorelov,<br />

J. Qiang, M. Venturini, A. Zholents (LBNL) D. Wang (MIT) R.L.<br />

Warnock (SLAC)<br />

one with relatively long electron bunches of the order of 1.5 ps and a moderate peak current of 500 A and one with<br />

shorter bunches of the order of 0.7 ps and higher peak current of the order of 800 A. In both cases, care has been<br />

taken to preserve the slice and projected emittances formed in the photocathode gun injector and to minimize the<br />

slice energy spread. The latter goal is accomplished by balancing the onset of the microbunching instability driven<br />

by the longitudinal space charge forces and the emission of coherent synchrotron radiation using Landau damping<br />

produced by a so-called laser heater. Various analytical techniques and tracking codes have been employed to obtain<br />

the reported results.<br />

*C. Bocchetta, et al., this conference.<br />

Linac Coherent Light Source Electron Beam Collimation<br />

This paper describes the design and preliminary<br />

simulations of the electron beam colli- J. Wu, P. Emma (SLAC)<br />

mation system in the Linac Coherent Light<br />

Source (LCLS) linac. Dark current is expected from the gun and some of the accelerating cavities. Particle tracking<br />

of the expected dark current through the entire LCLS linac, from L0-linac exit to FEL undulator entrance, is used to<br />

estimate final particle extent in the undulator as well as expected beam loss at each collimator or aperture restriction.<br />

A table of collimators and aperture restrictions is listed along with halo particle loss results, which includes an<br />

estimate of average continuous beam power lost on each individual collimator. In addition, the transverse wakefield<br />

alignment tolerances are calculated for each collimator.<br />

Trajectory Stability Modeling and Tolerances in the Linac Coherent Light Source<br />

To maintain stable performance of the Linac<br />

Coherent Light Source X-ray Free-electron J. Wu, P. Emma (SLAC)<br />

laser, one has to control undulator trajectory<br />

stability to a small fraction of the rms beam size. BPM based feedback loops running at 120 Hz will be effective<br />

in controlling jitter at low frequencies less than a few Hz. On the other hand, linac and injector stability tolerances<br />

must control jitter at higher frequencies. In this paper, we study the possible sources of such high frequency jitter,<br />

including: 1) steering coil current regulation; 2) quadrupole (and solenoid) transverse vibrations; 3) quadrupole (and<br />

solenoid) current regulation in presence of typical 200-micron misalignments; 4) charge jitter coupling to RF cavity<br />

transverse wakefield due to alignment errors; and 5) bunch length jitter coupling to Coherent Synchrotron Radiation<br />

in Chicane. Based on this study, we then set tolerances on each item.<br />

59<br />

MOPCH047<br />

MOPCH048<br />

MOPCH049

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