2021
DOI: 10.1140/epjp/s13360-021-02201-5
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Nonlinear dynamics of proton beams with hollow electron lens in the CERN high-luminosity LHC

Abstract: The design stored beam energy in the CERN high-luminosity large hadron collider (HL-LHC) upgrade is about 700 MJ, with about 36 MJ in the beam tails, according to estimates based on scaling considerations from measurements at the LHC. Such a large amount of stored energy in the beam tails poses serious challenges on its control and safe disposal. In particular, orbit jitters can cause significant losses on primary collimators, which can lead to accidental beam dumps, magnet quenches, or even permanent damage t… Show more

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Cited by 5 publications
(13 citation statements)
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“…The presence of highly populated beam tails risks making the operation very sensitive to small orbit jitters, naturally observed in the beam dynamics or triggered by different sources like earth quakes and power converter ripple [22]. Damage might also be caused in case of fast failure scenarios as potentially expected at the HL-LHC.…”
Section: Motivations and Required Performancementioning
confidence: 99%
See 1 more Smart Citation
“…The presence of highly populated beam tails risks making the operation very sensitive to small orbit jitters, naturally observed in the beam dynamics or triggered by different sources like earth quakes and power converter ripple [22]. Damage might also be caused in case of fast failure scenarios as potentially expected at the HL-LHC.…”
Section: Motivations and Required Performancementioning
confidence: 99%
“…Furthermore, it is planned to bias the electrodes at the entrance of the collector, to reduce the energy deposited to the collector, the secondary electron emission (therefore maximizing the electron efficiency) and the gas induced desorption (to guarantee best vacuum performance). Engineering margins on the design are being finalized, taking into account that the duty factor in operation might be significantly lower than unity for several considered powering schemes [40] and that the possibility to add a bias voltage to decelerate the electron beam before it reaches the collector is planned.…”
Section: Jinst 16 P03042mentioning
confidence: 99%
“…Therefore, ATLAS requested that the luminosity be kept constant for the first few hours of a run (luminosity-levelling) at a luminosity of 1.56 × 10 34 cm −2 s −1 with a pile-up of 60. In 2018, the LHC switched back to the 25 ns BCMS beam for luminosity production, as the problems with beam losses in 16L2 were mitigated [34], and the pile-up interactions were again reduced to about 60. More information about these filling schemes can be found in ref.…”
Section: Lhc Fill Patterns In Runmentioning
confidence: 99%
“…Contributions to this issue represent and attempt to cover a broad domain of topics in beam physics, with a loose classification into three categories of advances, challenges, and applications. References [13][14][15][16][17][18][19][20][21] provide a global overview of the applications of advanced beam dynamics concepts to existing or future machines. The nonlinear beam dynamics combined with the use of electron lenses has been considered in the framework of the High-Luminosity LHC Project and discussed in [21].…”
mentioning
confidence: 99%
“…References [13][14][15][16][17][18][19][20][21] provide a global overview of the applications of advanced beam dynamics concepts to existing or future machines. The nonlinear beam dynamics combined with the use of electron lenses has been considered in the framework of the High-Luminosity LHC Project and discussed in [21]. Various techniques devised to measure the available beam aperture in the LHC, which contributed to the astonishing performance reached during Run 2, are presented in [20].…”
mentioning
confidence: 99%