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@inproceedings{blednykh:ipac2021-thpab239,
author = {A. Blednykh and E.C. Aschenauer and M. Blaskiewicz and C. Hetzel and M.P. Sangroula and G. Wang and H. Witte},
% author = {A. Blednykh and E.C. Aschenauer and M. Blaskiewicz and C. Hetzel and M.P. Sangroula and G. Wang and others},
% author = {A. Blednykh and others},
title = {{Impedance Optimization of the EIC Interaction Region Vacuum Chamber}},
booktitle = {Proc. IPAC'21},
pages = {4270--4273},
eid = {THPAB239},
language = {english},
keywords = {electron, vacuum, impedance, detector, wakefield},
venue = {Campinas, SP, Brazil},
series = {International Particle Accelerator Conference},
number = {12},
publisher = {JACoW Publishing, Geneva, Switzerland},
month = {08},
year = {2021},
issn = {2673-5490},
isbn = {978-3-95450-214-1},
doi = {10.18429/JACoW-IPAC2021-THPAB239},
url = {https://jacow.org/ipac2021/papers/thpab239.pdf},
note = {https://doi.org/10.18429/JACoW-IPAC2021-THPAB239},
abstract = {{The interaction region chamber has a complex geometry at the crossing location of electron and proton beam pipes. In the direction of the electron beam, the pipe is designed in a way to avoid joints with cavity characteristics. The horizontal slot on the upstream side and the tapered transition on the downstream side are applied to minimize the IR chamber contribution to the total impedance of the electron ring and to avoid generating Higher Order Modes and heating-related issues. The synchrotron radiation mask is included to protect the IR chamber from synchrotron radiation without significant aperture reduction. In the direction of the proton beam, the main area for optimization is the transition area right after the detector.}},
}