Tune optimization of the third generation light source storage ring based onFrequency Map Analysis

  • Tune optimization is necessary to optimize the nonlinearity of the third generation light source storage ring. In this paper we summarize the common strategies for choosing a tune and discuss tune optimization. Frequency Map Analysis (FMA) is applied as a tune scanning tool to reveal information about nonlinear resonances and guide the tune optimization. The Shanghai Synchrotron Radiation Facility (SSRF) storage ring is taken as a test lattice, and the optimum solutions are presented in this paper. Moreover, the third order regular structural resonances excited by sextupoles are particularly investigated, and it is found that these resonances distort the tune shifts with amplitude and show a stop-band like the linear structural resonances.

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  • [1] . Corbett Je . Rabedeau Thomas. Nucl. Instrum. MethodsA, 2003, 500: 112. Lee Tae-Yeon, Choi Jinhyuk. Nucl. Instrum. Methods A,2003, 515: 4103. Gladkikh P I, Karnaukhov I M, Kononenko S G et al.Nucl.Instrum. Methods A, 2000, 448: 414. Laclare J L. Nucl. Instrum. Methods A, 2001, 467-468: 15. Bengtsson J, Joho W, Marchand P et al. Nucl. Instrum.Methods A, 1998, 404: 2376. Smith S L. Proceedings of the European Particle Acceler-ator Conference. France: Paris, 2002. 44-487. Owen H, Jones J, Smith S. Proceedings of the European Particle Accelerator Conference. France: Paris, 2002. 751-7538. JIAO Y, FANG S X, QIN Q et al. Nucl. Instrum. MethodsA, 2006, 566: 2709. Sacherer F. Proc. of 9th Int. Conf. on High Energy Accel-erators. 1974. 347-34910. LIU Gui-Min, DAI Zhi-Min, LI Hao-Hu et al. HEPNP,2006, 30(Supp..): 144 (in Chinese)11. Robin D. Phys. Rev. ST, 1999, 2: 04400112. Dumas H S, Laskar J. Phys. Rev. Lett., 1993, 70: 297513. Laskar J. Proceedings of the Particle Accelerator Confer-ence. USA: Portland, Oregon, 2003. 378-38214. Sterier C, Robin D, Nadolski L et al. Phys. Rev. E, 2002,65: 05650615. Belgroune M, Baldwin A I, Bartolini R et al. Proceedings ofthe Particle Accelerator Conference. Knoxville, Tennessee,USA: 2005, 1410-141216. Belgroune M, Brunelle P, Laskar J et al. Proceedings of theEuropean Particle Accelerator Conference. Paris, France:2002, 1229-123117. Bengtsson J. Proceedings of the European Particle Accel-erator Conference. Edinburgh, Scotland: 2006, 3478-348018. TIAN Shun-Qiang, LIU Gui-Min, LI Hao-Hu et al. ChinesePhysics C (HEP NP), 2009, 33(2): 12719. FANG Shou-Xian, QIN Qing. HEPNP, 2006, 30(9): 88020. TIAN Shun-Qiang, HOU Jie, CHEN Guang-Ling et al. Chi-nese Physics C, 2008, 32(7): 57621. Terebilo A. Accelerator Toolbox for MATLAB, SLAC-PUB-873222. Arbold V I, Kozlov V V, Neishtadt A I. Mathematical As-pects of Classical and Celestial Mechanics, Dyn. SystemsIII. Arnold V I, ed. Springer, New York: 198823. Bengtsson J. The Sextupole Scheme for the Swiss LightSource, SLS Note 9/97
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TIAN Shun-Qiang, LIU Gui-Min, LI Hao-Hu, HOU Jie and ZHANG Wen-Zhi. Tune optimization of the third generation light source storage ring based onFrequency Map Analysis[J]. Chinese Physics C, 2009, 33(3): 224-231. doi: 10.1088/1674-1137/33/3/012
TIAN Shun-Qiang, LIU Gui-Min, LI Hao-Hu, HOU Jie and ZHANG Wen-Zhi. Tune optimization of the third generation light source storage ring based onFrequency Map Analysis[J]. Chinese Physics C, 2009, 33(3): 224-231.  doi: 10.1088/1674-1137/33/3/012 shu
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Received: 2008-05-09
Revised: 2008-07-23
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Tune optimization of the third generation light source storage ring based onFrequency Map Analysis

    Corresponding author: TIAN Shun-Qiang,

Abstract: 

Tune optimization is necessary to optimize the nonlinearity of the third generation light source storage ring. In this paper we summarize the common strategies for choosing a tune and discuss tune optimization. Frequency Map Analysis (FMA) is applied as a tune scanning tool to reveal information about nonlinear resonances and guide the tune optimization. The Shanghai Synchrotron Radiation Facility (SSRF) storage ring is taken as a test lattice, and the optimum solutions are presented in this paper. Moreover, the third order regular structural resonances excited by sextupoles are particularly investigated, and it is found that these resonances distort the tune shifts with amplitude and show a stop-band like the linear structural resonances.

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