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Abstracts Brochure - CERN

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WEPCH092<br />

WEPCH093<br />

WEPCH094<br />

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

for class of piecewise continuous admissible controls and also for case of non-standard control variation, which is<br />

preserving smoothness, are obtained.<br />

Dynamical Aperture Studies for the <strong>CERN</strong> LHC: Comparison between Statistical Assignment<br />

of Magnetic Field Errors and Actual Measured Field Errors<br />

M. Giovannozzi, S.D. Fartoukh, S.S. Gilardoni, J.-B. Jeanneret, A.M.<br />

Lombardi, Y. Papaphilippou, T. Risselada, F. Schmidt (<strong>CERN</strong>)<br />

298<br />

It is customary to evaluate the performance<br />

of a circular particle accelerator by computing<br />

the dynamical aperture, i.e., the domain<br />

in phase space where bounded single-parti-<br />

cle motion occurs. In the case of the LHC the dynamical aperture computation is performed by assuming a statistical<br />

distribution of the magnetic field errors of various magnets’ classes: the numerical computations are repeated for a<br />

given set of realisations of the LHC ring. With the progress in the magnet production and allocation of the available<br />

positions in the ring, the statistical approach has to be replaced by the computation of one single configuration,<br />

namely the actual realisation of the machine. Comparisons between the two approaches are presented and discussed<br />

in details.<br />

Parameter Scans and Accuracy Estimates of the Dynamical Aperture of the <strong>CERN</strong> LHC<br />

Techniques to make use of large distributed<br />

M. Giovannozzi, F. Schmidt (<strong>CERN</strong>)<br />

computing facilities allow for denser parameter<br />

scans of the dynamical aperture, i.e.,<br />

the domain in phase space where bounded single-particle motion prevails. Moreover, one can also increase the<br />

number of ’seeds’ each of which represents a possible realisation of multipolar components around the machine. In<br />

this paper the dependence of the dynamical aperture on the step size of the grid of initial conditions and on the<br />

number of seeds is studied. Estimates on the accuracy of the dynamic aperture are derived and the definition of an<br />

improved protocol for numerical simulations is presented.<br />

An Early Beam Separation Scheme for the LHC<br />

The high nominal luminosity of the LHC re-<br />

J.-P. Koutchouk, G. Sterbini (<strong>CERN</strong>)<br />

quires a large number of bunches spaced by<br />

about 7.5 m. To prevent more than one headon<br />

collision in each interaction region, a crossing angle of 0.285 mrad is necessary. A side effect of this crossing<br />

angle is the increase of the effective transverse beam cross-section, thereby decreasing the luminosity by some 16%.<br />

For the LHC upgrade, depending on the focusing scenarios, this loss significantly increases and largely offsets the<br />

potential gain of a stronger focusing. In this paper we analyze a strategy to circumvent this difficulty, based an early<br />

beam separation using small dipoles placed at a few meters from the interaction point, deep inside the detectors.<br />

This allows quasi co-linear head-on collisions at the crossing point only. From the beam dynamics point of view, the<br />

essential constraint is to control the long-range beam-beam interactions in a scenario where the normalized beam<br />

separation is not constant. In this paper the criteria of the analysis and the performance improvement obtained with<br />

the scheme are discussed. The strength of the dipoles is estimated as well as the impact on the detectors structure.

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