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Abstracts Brochure - CERN

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

particle loss process and finally cause significant beam loss within a very short time (a few turns). A program package<br />

has been developed, which links the described beam loss mechanisms to the residual gas status and determines the<br />

vacuum dynamics. Core of the program is an ion optics tracking routine, in which the atomic physics and vacuum<br />

effects are embedded.<br />

Ion Optical Design of the Planned Heavy Ion Synchrotron SIS100<br />

The ion optical design of SIS100, which is the<br />

main synchrotron of the FAIR project, will be<br />

presented. The main purpose of SIS100 is the<br />

acceleration of high intensity heavy ion and<br />

J. Stadlmann, K. Blasche, B. Franczak, C. Omet, N. Pyka, P.J. Spiller<br />

(GSI) A.D. Kovalenko (JINR)<br />

proton beams and the generation of short compressed single bunches for the production of secondary beams. Since<br />

ionization in the residual gas is the main loss mechanism, a new lattice design concept had to be developed, especially<br />

for the operation with intermediate charge state, heavy ions. The lattice was optimized to generate a peaked loss<br />

distribution in charge separator like lattice cells. Thereby it enables the control of generated desorbtion gases in<br />

special catchers. For bunch compression the lattice provides dispersion free straight sections and a low dispersion<br />

in the arcs. A special difficulty is the optical design for fast and slow extraction, and the emergency dumping of the<br />

high rigidity ions that would make it possible to install necessary equipment within one and the same short straight<br />

section.<br />

Design of the NESR Storage Ring for Operation with Ions and Antiprotons<br />

The New Experimental Storage Ring (NESR)<br />

of the FAIR project has two major modes of<br />

operation. These are storage of heavy ion<br />

beams for internal experiments and deceler-<br />

M. Steck, K. Beckert, P. Beller, C. Dimopoulou, A. Dolinskii, F.<br />

Nolden, J. Yang (GSI)<br />

ation of highly charged ions and antiprotons before transfer into a low energy experimental area. The heavy ion<br />

beams can be either stable highly charged ions or rare isotope beams at an energy of 740 MeV/u selected in a magnetic<br />

separator. The antiprotons come with an energy of 3 GeV from the production target, they are pre-cooled and<br />

accumulated in a storage ring complex. The magnetic structure of the NESR has been optimized for large transverse<br />

and longitudinal acceptance by detailed dynamic aperture calculations. This will allow storage of multi-component<br />

beams with a large spread of charge to mass ratio, corresponding to a large spread in magnetic rigidity. Highest phase<br />

space density of the stored beams is provided by an electron cooling system, which for ions covers the full energy<br />

range and for antiprotons allows intermediate cooling during the deceleration process. For experiments with shortlived<br />

isotopes the cooling time and the time of deceleration will be optimized to a few seconds.<br />

FLAIR: a Facility for Low-energy Antiproton and Ion Research<br />

To exploit the unique possibilities that will<br />

become available at the Facility for Antipro- C.P. Welsch, C.P. Welsch (<strong>CERN</strong>) H. Danared (MSL)<br />

ton and Ion Research (FAIR), a collaboration<br />

of about 50 institutes from 15 countries was formed to efficiently enable an innovative research program towards<br />

low-energy antimatter-physics. In the Facility for Low-energy Antiproton and Ion Research (FLAIR) antiprotons and<br />

heavy ions are slowed down from 30 MeV to energies as low as 20 keV by a magnetic and an electrostatic storage ring.<br />

In this contribution, the facility and the research program covered are described with an emphasis on the accelerator<br />

69<br />

MOPCH079<br />

MOPCH080<br />

MOPCH081

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