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Abstracts Brochure - CERN

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TUPLS — Poster Session 27-Jun-06 16:00 - 18:00<br />

of the thermoelastic displacement potential for the equivalent isothermal two-dimensional stress problem. Finally,<br />

the contribution of dynamic stresses due to longitudinal and bending stress waves is determined by means of the<br />

modal summation method. This method can be effectively applied to any solid having cylindrical shape, made out<br />

of isotropic elastic material.<br />

EURISOL Target Stations Operation and Implications for its Proton Driver Beam<br />

Targets for the next generation radioactive<br />

ion beam (RIB) facilities (RIA, EURISOL) will E. Noah, F. Gerigk, J. Lettry, M. Lindroos, T. Stora (<strong>CERN</strong>)<br />

be subjected to energy deposition levels that<br />

call for a specific design of the target and ion source assembly to dissipate the deposited heat and to extract and<br />

ionize isotopes of interest efficiently. EURISOL, the next generation European RIB facility, plans to operate four target<br />

stations in parallel, three 100 kW direct targets and one 5 MW spallation neutron source with a GeV proton linac<br />

driver. The nature of the beam sharing has yet to be defined because in practice it will have a direct impact on target<br />

design, operation and lifetime. Splitting the beam in time implies that each target would be subjected to a pulsed<br />

beam, whose pulse width and repetition cycle have to be optimized in view of the RIB production. The 100 kW<br />

targets are expected to have a goal lifetime of three weeks. Target operation from the moment it is installed on a target<br />

station until its exhaustion involves several phases during which the incident proton beam intensity will vary. This<br />

paper discusses challenges for high power targetry at EURISOL, with an emphasis on requirements for the proton<br />

linac parameters.<br />

Comparison between Measured and Simulated Beam Loss Patterns in the SPS<br />

A prototype of an LHC collimator has been<br />

tested with proton beams at the <strong>CERN</strong> SPS.<br />

The interaction of the circulating proton<br />

beam with the carbon collimator jaws gen-<br />

S. Redaelli, G. Arduini, R.W. Assmann, G. Robert-Demolaize<br />

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

erated showers that were lost in the downstream SPS aperture. The measured beam loss patterns are compared<br />

in detail with the results of dedicated loss simulations. The simulation package includes (1) a 6D particle tracking<br />

through the SPS lattice; (2) the scattering interaction of protons with the collimator jaw material; (3) the time-dependent<br />

displacement of the collimator jaws with respect to the beam orbit; (4) a detailed aperture model of the full<br />

SPS ring. It is shown that the simulation tools can reliably predict the measured location of losses. This provides an<br />

important assessment of the simulation tools in view of the LHC beam loss studies.<br />

LHC Collimation Efficiency as a Function of Collimator Jaw Flatness<br />

The performance of the LHC collimation system<br />

depends critically on the flatness of the<br />

collimator jaws. Detailed simulation tools<br />

have been setup to study the dependence of<br />

S. Redaelli, R.W. Assmann, C.B. Bracco, G. Robert-Demolaize<br />

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

cleaning efficiency on the jaw flatness. The expected degradation of performance is quantified as a function of jaw<br />

deformation, both for systematic deformation of all jaws and for deformations of single jaws. Production tolerances on<br />

jaw flatness are discussedand secondary collimator locations are classified in terms of sensitivity to jaw deformations.<br />

259<br />

TUPLS129<br />

TUPLS130<br />

TUPLS131

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