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@InProceedings{luo:napac2019-tuplo07,
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 = {{Calculation of Action Diffusion With Crabbed Collision in eRHIC}},
booktitle = {Proc. NAPAC'19},
pages = {549--552},
paper = {TUPLO07},
language = {english},
keywords = {proton, cavity, electron, simulation, luminosity},
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-TUPLO07},
url = {http://jacow.org/napac2019/papers/tuplo07.pdf},
note = {https://doi.org/10.18429/JACoW-NAPAC2019-TUPLO07},
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 develop a simulation code to calculate the transverse action diffusion rate as function of the initial proton longitudinal action. The goal of this study is to identify the contributions from various protons to the overall emittance growth. Tune scan is also performed to locate optimum working points which yield less proton emittance growth.},
}