2008
DOI: 10.1088/1367-2630/10/4/043042
|View full text |Cite
|
Sign up to set email alerts
|

Experimental studies of compensation of beam–beam effects with Tevatron electron lenses

Abstract: Applying the space-charge forces of a low-energy electron beam can lead to a significant improvement of the beam-particle lifetime limit arising from the beam-beam interaction in a highenergy collider [1]. In this article we present the results of various beam experiments with "electron lenses," novel instruments developed for the beam-beam compensation at the Tevatron, which collides 980-GeV proton and antiproton beams. We study the dependencies of the particle betatron tunes on the electron beam current, ene… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
36
0
3

Year Published

2009
2009
2015
2015

Publication Types

Select...
5
3
1

Relationship

0
9

Authors

Journals

citations
Cited by 37 publications
(39 citation statements)
references
References 9 publications
0
36
0
3
Order By: Relevance
“…On the other hand such an implementation is beyond what has been achieved so far: Assuming an effective length of 6 m on both sides of the IP an electron beam current of about 30 A would be needed in order to produce the field equivalent to a 1 m long wire powered at 177 A. This is about an order of magnitude larger than what has been achieved for the Tevatron Electron Lens [27,34] and with the electron lenses at RHIC [35]. A factor of 2 could be gained by placing a second electron beam wire on the other side of the IP, resulting in a total of eight installations.…”
Section: Discussionmentioning
confidence: 99%
“…On the other hand such an implementation is beyond what has been achieved so far: Assuming an effective length of 6 m on both sides of the IP an electron beam current of about 30 A would be needed in order to produce the field equivalent to a 1 m long wire powered at 177 A. This is about an order of magnitude larger than what has been achieved for the Tevatron Electron Lens [27,34] and with the electron lenses at RHIC [35]. A factor of 2 could be gained by placing a second electron beam wire on the other side of the IP, resulting in a total of eight installations.…”
Section: Discussionmentioning
confidence: 99%
“…The collision with the electron beam can cancel part of the head-on tune spread (and possibly of the resonance excitation) induced in the same main beam by primary collisions with a positively charged (proton) beam. A first set of electron lenses was implemented and operated at the Tevatron [49]. Instead of compensating head-on beam-beam effects, the Tevatron electron lenses were successfully used as pulsed quadrupoles to equalize the tunes along a bunch train.…”
Section: Beam-beam Compensationmentioning
confidence: 99%
“…collisions with a large Piwinski angle [62] -including "superbunch" schemes in hadron colliders [3,39]; "nanobeam schemes" proposed for the former SuperB (together with crab waist collisions [60]) and adopted for SuperKEKB, in which the short length of the beambeam overlap enables the implementation of an extremely low  y * [63];; colliding hadron bunches with longitudinally flat profile [64,65]; or compensating the beam-beam tune shift with electron(-beam) lenses [48] as implemented at the Tevatron [49] and at RHIC [50], and proposed for the HL-LHC.…”
Section: Collision Schemesmentioning
confidence: 99%
“…They are described in great detail in [7,8]. The TELs employ strong solenoids and have electrostatic electrodes which can be used to arrange the configuration similar to what is depicted in Fig.1.…”
Section: First Tests Of Electron Columns In the Tevatronmentioning
confidence: 99%