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Abstracts Brochure - CERN

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MOPCH095<br />

MOPCH096<br />

MOPCH097<br />

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

transverse and longitudinal shaving, are described. In particular, the choice of harmonic number and its consequences<br />

for operation and beam reproducibility are discussed. Finally, the performance achieved for the different beams is<br />

summarized.<br />

Performance of Nominal and Ultimate LHC Beams in the <strong>CERN</strong> PS-booster<br />

The requirements for nominal and ultimate<br />

M. Benedikt, M. Chanel, K. Hanke (<strong>CERN</strong>)<br />

LHC beams in the <strong>CERN</strong> PS-Booster were<br />

specified in 1993 and served as input for the<br />

definition of the "PS conversion for LHC" project. Already during the upgrade project and also after its completion<br />

in 2000, the beam intensities to be provided from the PS Booster were increased in order to compensate for changes<br />

on the LHC machine, the beam production scheme in the PS and for non-anticipated beam losses along the injector<br />

chain. In order to improve the beam brightness, to be compatible with the increased requirements, extensive machine<br />

studies have taken place on the PS-Booster. The working point was changed to reduce the influence of systematic<br />

resonances and the injection line optics was re-matched to improve the injection efficiency. The paper summarizes<br />

briefly the evolution of the performance requirements. The various measures undertaken to improve the LHC beam<br />

quality are outlined and the present performance achieved in the PS-Booster is presented.<br />

LEIR Lattice<br />

The Low Energy Ion Ring (LEIR) is a low<br />

C. Carli, P. Beloshitsky, M. Chanel, J. Pasternak (<strong>CERN</strong>)<br />

energy ion cooling and accumulation ring<br />

and serves to compress long ion pulses from<br />

Linac 3 into high density bunches suitable for LHC ion operation. Issues of the LEIR lattice are to fulfil all constraints<br />

with a small number of quadrupoles and compensations of perturbations due to an electron cooler and gradients seen<br />

by the beam in the bending magnets during the ramp. Furthermore, experimental investigations via orbit reponse<br />

measurements will be reported.<br />

<strong>CERN</strong> Proton Synchrotron Working Point Control Using an Improved Version of the Poleface-windings<br />

and Figure-of-eight Loop Powering<br />

R.R. Steerenberg, J.-P. Burnet, M. Giovannozzi, O. Michels, E. Métral,<br />

B. Vandorpe (<strong>CERN</strong>)<br />

74<br />

The working point of the <strong>CERN</strong> Proton Synchrotron,<br />

which is equipped with combined<br />

function magnets, is controlled using poleface-windings.<br />

Each main magnet consists<br />

of one focusing and one de-focusing half-unit on which four pole-face-winding plates are mounted containing two<br />

separate coils each, called narrow and wide. At present they are connected in series, but can be powered independently.<br />

In addition, a winding called the figure-of-eight loop, contours the pole faces and crosses between the two<br />

half units, generating opposite fields in each half-unit. The four optical parameters, horizontal and vertical tune and<br />

chromaticity, are adjusted by acting on the pole-face-winding currents in both half units and in the figure-of-eight<br />

loop, leaving one physical quantity free. The power supply consolidation project opened the opportunity to use five<br />

independent power supplies, to adjust the four parameters plus an additional degree of freedom. This paper presents<br />

the results of the measurements that have been made in the five-current mode together with the influence of the<br />

magnetic nonlinearities, due to the unbalance in the narrow and wide winding currents, on the beam dynamics.

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