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Electron cooling system for ITEP ion storage ring

Published online by Cambridge University Press:  12 February 2003

P.R. ZENKEVICH
Affiliation:
Institute for Theoretical and Experimental Physics, Moscow, Russia
N.N. ALEXEEV
Affiliation:
Institute for Theoretical and Experimental Physics, Moscow, Russia
A.V. BARKHUDARYAN
Affiliation:
Institute for Theoretical and Experimental Physics, Moscow, Russia
A.Ye. BOLSHAKOV
Affiliation:
Institute for Theoretical and Experimental Physics, Moscow, Russia
D.G. KOSHKAREV
Affiliation:
Institute for Theoretical and Experimental Physics, Moscow, Russia
Yu.V. SHARKOV
Affiliation:
Institute for Theoretical and Experimental Physics, Moscow, Russia
V.F. BYKOVSKY
Affiliation:
Joint Institute of Nuclear Research, Dubna, Russia
Yu.V. KOROTAEV
Affiliation:
Joint Institute of Nuclear Research, Dubna, Russia
I.N. MESHKOV
Affiliation:
Joint Institute of Nuclear Research, Dubna, Russia
A.O. SIDORIN
Affiliation:
Joint Institute of Nuclear Research, Dubna, Russia
A.V. SMIRNOV
Affiliation:
Joint Institute of Nuclear Research, Dubna, Russia
Ye.M. SYRESIN
Affiliation:
Joint Institute of Nuclear Research, Dubna, Russia
I.V. TITKOVA
Affiliation:
Joint Institute of Nuclear Research, Dubna, Russia

Abstract

The main goal of the Tera Watt A Cumulator project (Institute for Theoretical and Experimental Physics, Moscow) is accumulation in the storage ring of an intense ion beam, its longitudinal compression and the use of the extracted beam for plasma experiments. However, beam parameters at the target are decreased because of extreme transverse heating and growth of the beam momentum spread due to intrabeam scattering. These effects can be suppressed by application of the electron cooling system (ECS). Design study of ECS has been performed in the Joint Institute for Nuclear Research. The design project and characteristics of the system are described, as well as analysis of the accumulation kinetics in the presence of the cooling system. Design work has shown that because of the small length of the straight section (2.35 m), the effective length of the cooling system is small (about 55–60 cm). Nevertheless, for long accumulation times (>100 s), the system allows us to significantly improve the beam parameters at the target (specific energy, specific power, and so on) and to suppress the beam losses by an order of magnitude.

Type
Research Article
Copyright
© 2002 Cambridge University Press

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