HITRAP – Heavy , Highly-Charged Ions at Rest

F. Herfurth, W. Barth, G. Clemente, L. A. Dahl, P. Gerhard, M. Kaiser,O. K. Kester,H.-J. Kluge, N. Kotovskiy, C. Kozhuharov, M. Maier, J. Pfister, W. Quint, U. Ratzinger,A. Schempp, A. Sokolov,Th. Stöhlker, H. Vormann, G. Vorobjev, S. Yaramishev

semanticscholar(2011)

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Abstract
At the GSI accelerator complex, using the universal linear accelerator UNILAC and the synchrotron SIS, highly-charged ions up to U 92+ are produced by passing a 400 MeV/u beam through a gold foil stripping off al l or nearly all electrons. The HITRAP facility is built to decelerate those ions to almost rest and to provide t hem to the experiments [1]. First, the ions are decelerate d in the experimental storage ring ESR from 400 to 4 MeV/u a ccompanied with stochastic and electron cooling to k eep the emittance small. Then, in the HITRAP linear dec elerator the deceleration is performed in two additio nal steps. An interdigital H-type (IH) structure and a radiofrequency quadrupole (RFQ) structure are operated i n inverse mode to decelerate first from 4 MeV/u to 0. 5 MeV/u and then further to 6 keV/u. For final coolin g below one meV the ions are captured in a Penning trap .
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