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Abstracts Brochure - CERN

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

Models to Study Multi-bunch Coupling through Head-on and Long-range Beam-beam Interactions<br />

In the LHC almost 6000 bunches will collide<br />

in four interaction points where they experi- T. Pieloni, W. Herr (<strong>CERN</strong>)<br />

ence head-on as well as clustered long range<br />

interactions. These lead to a coupling between all bunches and coherent beam-beam effects. For two colliding bunches<br />

this is well understood. However, for a large number of bunches colliding with different collision patterns, it results<br />

in a complex spectrum of oscillation frequencies with consequences for beam measurements and Landau damping.<br />

To study the coherent beam-beam modes, three complementary models have been developped and will be described<br />

in this report. Two of these methods rely on self-consistent multi-bunch and multi-particle tracking while the third is<br />

a semi-analytic model based on a complex matrix algorithm. The three methods together provide useful information<br />

about the beam-beam coupling of multi bunch beams and together provide a deeper insight into the underlying<br />

physics.<br />

Measurement and Correction of the 3rd Order Resonance in the Tevatron<br />

At Fermilab Tevatron BPM system has been<br />

recently upgraded resulting much better accuracy<br />

of beam position measurements and<br />

improvements of data acquisition for turn-<br />

F. Schmidt (<strong>CERN</strong>) Y. Alexahin, V.A. Lebedev, D. Still, A. Valishev<br />

(Fermilab)<br />

by-turn measurements. That allows one to record the beam position at each turn for 8000 turns for all BPMs (118<br />

in each plane) with accuracy of about 10 -20 µm. In the last decade a harmonic analysis tool has been developed at<br />

<strong>CERN</strong> that allows relating each FFT line derived from the BPM data with a particular non-linear resonance in the<br />

machine. In fact, one can even detect the longitudinal position of the sources of these resonances. Experiments<br />

have been performed at the Tevatron in which beams have been kicked to various amplitudes to analyze the 3rd<br />

order resonance. It was possible to address this rather large resonance to some purposely powered sextupoles. An<br />

alternative sextupole scheme allowed the suppression of this resonance by a good factor of 2. Lastly, the experimental<br />

data are compared with model calculations.<br />

Beam Dynamics in Compton-ring Gamma Sources<br />

Electron storage rings with a laser cavity<br />

are promising intensive sources of polarized<br />

hard photons to generate polarized positron<br />

beams. The dynamics of electron bunches<br />

circulating in a storage ring and interacting<br />

E.V. Bulyak, P. Gladkikh, V. Skomorokhov (NSC/KIPT) K. Moenig<br />

(DESY Zeuthen) T. Omori, J.U. Urakawa (KEK) F. Zimmermann<br />

(<strong>CERN</strong>)<br />

with high-power laser pulses is studied both analytically and by simulation. Common features and difference in the<br />

bunch behavior interacting with an extremely high power laser pulse (polarized positron source for the ILC project)<br />

and a moderate pulse (source for CLIC) are shown. Also considerations on particular lattice designs for both rings<br />

are presented.<br />

299<br />

WEPCH095<br />

WEPCH096<br />

WEPCH097

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