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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.}}, }