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Abstracts Brochure - CERN

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

Experience of Operation of Short Period Undulator for E-166<br />

We represent results of operation of 2.54 mm<br />

period, K=0.2, up to 30 Hz undulator used A.A. Mikhailichenko (Cornell University, Department of Physics)<br />

in E-166 experiment for polarized positron<br />

production. One peculiarity is in usage of Ferrofluid for cooling.<br />

ILC Linac R&D at SLAC<br />

Since the ITRP recommendation in 2004 to<br />

use superconducting rf technology for a next C. Adolphsen (SLAC)<br />

generation linear collider, the former NLC<br />

group at SLAC has been actively pursuing a broad range of R&D for this collider (the ILC). In this paper, we review<br />

the progress of those programs relating to linac technology. These include the development of a Marx-style modulator<br />

(120 kV, 120 A, 1.5 ms, 5 Hz) and a 10 MW sheet-beam klystron, construction of an L-band (1.3 GHz) rf source using<br />

a SNS HVCM modulator and commercial klystrons, fabrication and testing of a five-cell L-band cavity prototype for<br />

the ILC positron capture accelerator, high power tests of cavity coupler components, beam tests of prototype S-band<br />

linac beam position monitors and measurements of the magnetic center stability of an ILC prototype superconducting<br />

quadrupole magnet built by the CIEMAT group in Spain.<br />

Commissioning of the ALTO 50 MeV Electron Linac<br />

The ALTO 50 MeV electron linac is dedicated<br />

to the production of neutron-rich radioactive<br />

nuclei using the photo-fission process and<br />

the optimisation of the target-ion source system<br />

for SPIRAL 2 and Eurisol projects. A<br />

description of the accelerator consisting in 3<br />

J. Lesrel, J. Arianer, O. Bajeat, J-M. Buhour, H. Bzyl, M. Chabot,<br />

J.-L. Coacolo, T. Corbin, H. Croiset, M. Ducourtieux, S. Essabaa,<br />

H. Lefort, M. Raynaud (IPN) G. Bienvenu, J-N. Cayla, M. Desmons<br />

(LAL)<br />

Mev injector (old test station of LAL), LIL accelerating structure, RF power plant, beam line, control system and<br />

diagnostics will be given. Specified and measured beam parameters will be compared to show the performance for<br />

the photo-fission and eventually other applications.<br />

Construction of the Probe Beam Photo-injector of CTF3<br />

The paper describes the HF and dynamic<br />

beam modelling performed onto the 3 GHz J. Brossard, M. Desmons, B.M. Mercier, C.P. Prevost, R. Roux (LAL)<br />

/ 2,5 cells photo-injector of the future CTF3<br />

(CLIC Test Facility 3) probe beam linac, whose goal is to demonstrate the feasibility of the 30 GHz accelerating sections<br />

in the framework of the CLIC project. The Probe Beam Photo-Injector (PBPI) conception is inspired from the drive<br />

beam photo-injector already designed by LAL (Orsay, France) and actually tested in our laboratory. However, the<br />

design of PBPI has been simplified with respect to the previous because the charge per bunch is 4 times lower and the<br />

number of bunches several orders of magnitude smaller. The internal geometry and the coupling system of the PBPI<br />

have been designed with 2D (SUPERFISH) and 3D (HFSS, ANSYS) codes. A detailed analysis of the dissymmetry<br />

(induced by the coupling system) of the accelerating field component has been performed. Based on the modified<br />

139<br />

MOPLS109<br />

MOPLS110<br />

MOPLS113<br />

MOPLS114

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