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@InProceedings{luo:napac2019-tuplo06,
author = {Y. Luo and G. Bassi and M. Blaskiewicz and W. Fischer and Y. Hao and C. Montag and V. Ptitsyn and J. Qiang and F.J. Willeke and D. Xu},
% author = {Y. Luo and G. Bassi and M. Blaskiewicz and W. Fischer and Y. Hao and C. Montag and others},
% author = {Y. Luo and others},
title = {{Weak-Strong Beam-Beam Simulation for eRHIC}},
booktitle = {Proc. NAPAC'19},
pages = {545--548},
paper = {TUPLO06},
language = {english},
keywords = {proton, cavity, simulation, luminosity, electron},
venue = {Lansing, MI, USA},
series = {North American Particle Accelerator Conference},
number = {4},
publisher = {JACoW Publishing, Geneva, Switzerland},
month = {10},
year = {2019},
issn = {2673-7000},
isbn = {978-3-95450-223-3},
doi = {10.18429/JACoW-NAPAC2019-TUPLO06},
url = {http://jacow.org/napac2019/papers/tuplo06.pdf},
note = {https://doi.org/10.18429/JACoW-NAPAC2019-TUPLO06},
abstract = {In the eRHIC, to compensate the geometric luminosity loss due to the crossing angle, crab cavities are to be installed on both sides of the interaction point. When the proton bunch length is comparable to the wavelength of its crab cavities, protons will not be perfectly tilted in the x-z plane. In the article, we employ weak-strong beam-beam interaction model to calculate the proton beam size growth rates and luminosity degradation rate with various machine and time parameters. The goal of these studies is to optimize the the beam-beam related machine and beam parameters of eRHIC.},
}