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Phys. Rev. ST Accel. Beams 11, 103501 (2008) [19 pages]

Tevatron electron lenses: Design and operation

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Vladimir Shiltsev1,*, Kip Bishofberger2, Vsevolod Kamerdzhiev1, Sergei Kozub3, Matthew Kufer1, Gennady Kuznetsov1, Alexander Martinez1, Marvin Olson1, Howard Pfeffer1, Greg Saewert1, Vic Scarpine1, Andrey Seryi4, Nikolai Solyak1, Veniamin Sytnik3, Mikhail Tiunov5, Leonid Tkachenko3, David Wildman1, Daniel Wolff1, and Xiao-Long Zhang1
1Fermi National Accelerator Laboratory, P.O. Box 500, Batavia, Illinois 60510, USA
2Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
3Institute of High Energy Physics, Protvino, 142284, Russia
4Stanford Linear Accelerator Center, Stanford, California 94025, USA
5Budker Institute of Nuclear Physics, Novosibirsk, 630090, Russia

Received 11 August 2008; published 9 October 2008

The beam-beam effects have been the dominating sources of beam loss and lifetime limitations in the Tevatron proton-antiproton collider [ V. Shiltsev et al. Phys. Rev. ST Accel. Beams 8 101001 (2005)]. Electron lenses were originally proposed for compensation of electromagnetic long-range and head-on beam-beam interactions of proton and antiproton beams [ V. Shiltsev et al. Phys. Rev. ST Accel. Beams 2 071001 (1999)]. Results of successful employment of two electron lenses built and installed in the Tevatron are reported by Shiltsev et al. [ Phys. Rev. Lett. 99 244801 (2007); New J. Phys. 10 043042 (2008)] and by Zhang et al. [ X.-L. Zhang et al. Phys. Rev. ST Accel. Beams 11 051002 (2008)]. In this paper we present design features of the Tevatron electron lenses (TELs), discuss the generation of electron beams, describe different modes of operation, and outline the technical parameters of various subsystems.

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© 2008 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevSTAB.11.103501
DOI:
10.1103/PhysRevSTAB.11.103501
PACS:
29.27.Eg, 29.25.Bx, 29.27.Bd, 29.27.Fh

*shiltsev@fnal.gov