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@inproceedings{dhital:ipac2021-tuxa07,
author = {B. Dhital and Y.S. Derbenev and D. Douglas and A. Hutton and G.A. Krafft and F. Lin and V.S. Morozov and Y. Zhang},
% author = {B. Dhital and Y.S. Derbenev and D. Douglas and A. Hutton and G.A. Krafft and F. Lin and others},
% author = {B. Dhital and others},
title = {{Beam Dynamics Study in a Dual Energy Storage Ring for Ion Beam Cooling*}},
booktitle = {Proc. IPAC'21},
pages = {1290--1293},
eid = {TUXA07},
language = {english},
keywords = {storage-ring, cavity, electron, focusing, emittance},
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-TUXA07},
url = {https://jacow.org/ipac2021/papers/tuxa07.pdf},
note = {https://doi.org/10.18429/JACoW-IPAC2021-TUXA07},
abstract = {{A dual energy storage ring designed for beam cooling consists of two closed rings with significantly different energies: the cooling and damping rings. These two rings are connected by an energy recovering superconducting RF structure that provides the necessary energy difference. In our design, the RF acceleration has a main linac and harmonic cavities both running at crest that at first accelerates the beam from low energy E_{L} to high energy E_{H} and then decelerates the beam from E_{H} to E_{L} in the next pass. The purpose of the harmonic cavities is to extend the bunch length in a dual energy storage ring as such a longer bunch length may be very useful in a cooling application. Besides these cavities, a bunching cavity running on zero-crossing phase is used outside of the common beamline to provide the necessary longitudinal focusing for the system. In this paper, we present a preliminary lattice design along with the fundamental beam dynamics study in such a dual energy storage ring.}},
}