2018
DOI: 10.1016/j.nima.2018.04.014
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Space charge compensation with pulsed electron lenses for intense ion beams in synchrotrons

Abstract: For booster synchrotrons, like the SIS at GSI, space charge is one of the main intensity limitations. At injection energy the space charge induced tune spreads in booster synchrotrons are large, reaching up to 0.5 and the ramping times are typically short. We study the effect of several localized electron lenses distributed equally around the circumference in order to compensate for the transverse space charge force.

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Cited by 11 publications
(14 citation statements)
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“…2 and Eqs. (9,16). In contrast, for a transverse detuning there is no effective impedance modification and only Landau damping is affected.…”
Section: Discussionmentioning
confidence: 98%
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“…2 and Eqs. (9,16). In contrast, for a transverse detuning there is no effective impedance modification and only Landau damping is affected.…”
Section: Discussionmentioning
confidence: 98%
“…2. This is the regime foreseen for a PEL in the SIS100 as a space-charge compensation device [16]. Due to the large mode spectrum modification by PEL, expressions of Eq.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…4. pulsed electron lenses: for the existing SIS18 pulsed electron lenses for partial compensation of the space charge tune spread are under consideration [21]. Studies for the SIS100 are ongoing.…”
Section: Beta Beat Correctionmentioning
confidence: 99%
“…However, the SIS18 will serve as testbed to demonstrate the space charge compensation scheme and the electron lens with an interaction length of 3.36 m will be installed in one of the available drift sections [1]. The SIS18 ion beam has an elliptical cross section over the length of the interaction region and has to be transversally embedded into a homogeneous electron beam while the pulse needs to be exactly matched to the bunch form in order to avoid over-compensation of the bunch head and tail as presented in [2]. During acceleration of the ion beam the SC tune spread reaches its maximum.…”
Section: Introductionmentioning
confidence: 99%