JACoW is a publisher in Geneva, Switzerland that publishes the proceedings of accelerator conferences held around the world by an international collaboration of editors.
@inproceedings{jebramcik:ipac2022-tupoms019,
author = {M.A. Jebramcik and I.V. Agapov and S.A. Antipov and R. Bartolini and R. Brinkmann and D. Einfeld and T. Hellert and J. Keil},
% author = {M.A. Jebramcik and I.V. Agapov and S.A. Antipov and R. Bartolini and R. Brinkmann and D. Einfeld and others},
% author = {M.A. Jebramcik and others},
title = {{Collimation Strategy for the Low-Emittance PETRA IV Storage Ring}},
booktitle = {Proc. IPAC'22},
% booktitle = {Proc. 13th International Particle Accelerator Conference (IPAC'22)},
pages = {1445--1448},
eid = {TUPOMS019},
language = {english},
keywords = {kicker, collimation, injection, undulator, emittance},
venue = {Bangkok, Thailand},
series = {International Particle Accelerator Conference},
number = {13},
publisher = {JACoW Publishing, Geneva, Switzerland},
month = {07},
year = {2022},
issn = {2673-5490},
isbn = {978-3-95450-227-1},
doi = {10.18429/JACoW-IPAC2022-TUPOMS019},
url = {https://jacow.org/ipac2022/papers/tupoms019.pdf},
abstract = {{The beam-intensity losses in the proposed PETRA IV electron storage ring that will replace DESY’s synchrotron light source PETRA III will be dominated by the Touschek effect due to the high bunch density. The beam lifetime will only be in the range of 5 h in the timing mode (80 high-intensity bunches) leading to a maximum power loss of ~170 mW along the storage ring (excluding injection losses). To avoid the demagnetization of the permanent-magnet undulators and combined-function magnets, this radiation-sensitive hardware has to be shielded against losses as well as possible. Such shielding elongates the lifetime of the hardware and consequently reduces the time and the resources that are spent on maintenance once PETRA IV is operational. This contribution presents options for collimator locations, e.g., at the dispersion bump in the achromat cell, to reduce the exposure to losses from the Touschek effect and the injection process. This contribution also quantifies the risk of damaging the installed collimation system in case of hardware failure, e.g., RF cavity or quadrupole failure, since the beam with an emittance of 20 pm could damage collimators if there is no emittance blow-up.}},
}