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@inproceedings{witte:ipac2021-wepab002,
author = {H. Witte and J. Adam and M. Anerella and E.C. Aschenauer and J.S. Berg and M. Blaskiewicz and A. Blednykh and W. Christie and J.P. Cozzolino and K.A. Drees and B.R. Gamage and D.M. Gassner and K. Hamdi and C. Hetzel and H.M. Hocker and D. Holmes and A. Jentsch and A. Kiselev and P. Kovach and H. Lovelace III and Y. Luo and G.J. Mahler and A. Marone and G.T. McIntyre and T.J. Michalski and C. Montag and V.S. Morozov and R.B. Palmer and B. Parker and S. Peggs and S.R. Plate and V. Ptitsyn and G. Robert-Demolaize and C.E. Runyan and J. Schmalzle and K.S. Smith and M.L. Stutzman and M.K. Sullivan and S. Tepikian and P. Thieberger and J.E. Tuozzolo and F.J. Willeke and W. Wittmer and Q. Wu and Z. Zhang},
% author = {H. Witte and J. Adam and M. Anerella and E.C. Aschenauer and J.S. Berg and M. Blaskiewicz and others},
% author = {H. Witte and others},
title = {{The Interaction Region of the Electron-Ion Collider EIC}},
booktitle = {Proc. IPAC'21},
pages = {2574--2577},
eid = {WEPAB002},
language = {english},
keywords = {electron, radiation, synchrotron-radiation, synchrotron, detector},
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-WEPAB002},
url = {https://jacow.org/ipac2021/papers/wepab002.pdf},
note = {https://doi.org/10.18429/JACoW-IPAC2021-WEPAB002},
abstract = {{This paper presents an overview of the Interaction Region (IR) design for the planned Electron-Ion Collider (EIC) at Brookhaven National Laboratory. The IR is designed to meet the requirements of the nuclear physics community *. The IR design features a ±4.5 m free space for the detector; a forward spectrometer magnet is used for the detection of hadrons scattered under small angles. The hadrons are separated from the neutrons allowing detection of neutrons up to ±4 mrad. On the rear side, the electrons are separated from photons using a weak dipole magnet for the luminosity monitor and to detect scattered electrons (e-tagger). To avoid synchrotron radiation backgrounds in the detector no strong electron bending magnet is placed within 40 m upstream of the IP. The magnet apertures on the rear side are large enough to allow synchrotron radiation to pass through the magnets. The beam pipe has been optimized to reduce the impedance; the total power loss in the central vacuum chamber is expected to be less than 90 W. To reduce risk and cost the IR is designed to employ standard NbTi superconducting magnets, which are described in a separate paper.}},
}