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Abstracts Brochure - CERN

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WEPLS114<br />

WEPLS115<br />

WEPLS116<br />

WEPLS117<br />

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

Progress on the MICE Tracker Solenoid<br />

M.A. Green, S.P. Virostek (LBNL) W. Lau, S.Q. Yang (OXFORDphysics)<br />

366<br />

This report describes the 400 mm warm<br />

bore tracker solenoid for the Muon Ionization<br />

Cooling Experiment (MICE). The 2.923<br />

m long tracker solenoid module includes the<br />

radiation shutter between the end absorber focus coil modules and the tracker as well as the 2.780 meter long magnet<br />

cryostat vacuum vessel. The 2.554 m long tracker solenoid consists of two sections, a three-coil spectrometer magnet<br />

and a two-coil matching section that matches the uniform field 4 T spectrometer solenoid into the MICE cooling<br />

channel. The two tracker magnets are used to provide a uniform magnetic field for the fiber detectors that are used<br />

to measure the muon beam emittance at the two ends of the cooling channel. This paper describes the design for the<br />

tracker magnet coils and the 4.2 K cryogenic coolers that are used to cool the superconducting magnet. Interfaces<br />

between the magnet and the detectors are discussed.<br />

Impedances in Slotted-Pipe Kicker Magnets<br />

Storage ring slotted-pipe kicker magnets<br />

F. Marhauser, O. Dressler, V. Duerr, J. Feikes (BESSY GmbH) based on the DELTA design are foreseen<br />

for the Metrology Light Source (MLS) of the<br />

Physikalisch-Technische Bundesanstalt currently under construction near the BESSY site. Although the slotted pipe<br />

maintains the cross-section of the storage ring vacuum chamber, image currents have to bypass the slots generating<br />

wakefields. Actually modes with substantial impedances have been revealed by simulations and verified by<br />

measurements of a kicker model for the MLS.<br />

Multipole Power Supplies for the Australian Synchrotron<br />

N.J. Meadowcroft, R. Farnsworth (ASP) I. Jensen (Danfysik A/S)<br />

A. Morris (CCLRC/RAL/ISIS)<br />

The Australian Synchrotron storage ring consists<br />

of 28 dipoles, 56 focussing quadrupoles,<br />

28 defocussing quadrupoles, 98 sextupoles,<br />

42 horizontal correctors, 56 vertical correc-<br />

tors and 28 skew quadrupole correctors. Each set of coils on the multipole magnets is supplied by a dedicated power<br />

supply, with the focussing, defocusing, and sextupole magnet coils fed by18-bit unipolar power supplies and the<br />

corrector coils fed by 18-bit bipolar power supplies. This paper will discuss the design, power supply installation<br />

configuration, the testing, commissioning and control interfaces.<br />

The Australian Synchrotron Storage Ring Dipole Power Supply<br />

N.J. Meadowcroft, R. Farnsworth (ASP) P. Bellomo (SLAC) S. Cohen<br />

(LANL) R. Rumrill (Alpha Scientific Electronics)<br />

The Australian Synchrotron storage ring consists<br />

of 28 dipoles, 56 focusing quadrupoles,<br />

28 defocusing quadrupoles, 98 sextupoles, 42<br />

horizontal correctors, 56 vertical correctors<br />

and 28 skew quadrupole correctors. The 28 dipole magnets are series connected and powered by a single 1100V,<br />

850A, 24 pulse power supply with an output stability better than 100ppm. The paper will discuss the design, testing,<br />

commissioning and control interfaces for the storage ring dipole power supply.

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