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Frequency Map Calculation for the Advanced Light Source David Robin Advanced Light Source

Frequency Map Calculation for the Advanced Light Source David Robin Advanced Light Source work done in collaboration with

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Frequency Map Calculation for the Advanced Light Source David Robin Advanced Light Source

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  1. Frequency Map Calculation for the Advanced Light Source David Robin Advanced Light Source work done in collaboration with Christoph Steier (ALS), Ying Wu (Duke), Weishi Wan (ALS), Winfried Decking (DESY), James Safranek (SLAC/SSRL), Jacques Laskar (BdL), Laurent Nadolski (SOLEIL), Scott Dumas (U. Cinc.) with help from Alan Jackson (LBNL), Greg Portmann (SLAC/SSRL), Etienne Forest (KEK), Amor Nadji (SOLEIL), Andrei Terebilo (SLAC/SSRL) FMAP_Workshop - April 1, 2004

  2. Outline Motivation • Beam Lifetime • Injection Efficiency Single Particle Beam Dynamics in the ALS • Importance of Periodicity • Example of Frequency Map with Lattice Errors Frequency Map and Particle Loss Injection • Superbend Example Summary FMAP_Workshop - April 1, 2004

  3. Motivation Performance of the Advanced Light Source (ALS) is limited by the single particle electron beam dynamics • Injection efficiency • Beam lifetime Continue to strive for better understanding of the beam dynamics in order to • Improve the performance of the ALS • Accurately predict what will happen when the ALS is upgraded to include • Superbends, narrow gap insertion devices, elliptically polarizing undulators, femtoslicing modifications, … FMAP_Workshop - April 1, 2004

  4. Dynamics of the ALS The ALS is an interesting machine for studying the particle beam dynamics: • Simple  Simple Magnetic Lattice • Very Nonlinear In terms of single particle beam dynamics, the ALS is one of the most extensively studied storage rings • Theoretical investigations of the ALS began in the mid 1980s (Nishimura, Forest, Ruth, Bengtsson, …) • The ALS was used as the first example of frequency map analysis applied to accelerators (Laskar and Dumas in 1993) FMAP_Workshop - April 1, 2004

  5. Dynamics in the ALS: Lattice QFA 2 QFA 1 B 2 SF 1 SF 2 SD 1 SD 2 B 1 B 3 QD 2 QD 1 QF 1 QF 2 Typical ALS Sector ALS consists of 12 sectors • 12-fold periodicity Suppression of resonances mnx + nny = 12 x q where m, n, and q, are integers FMAP_Workshop - April 1, 2004

  6. Resonance Excitation • Resonances can lead to irregular and chaotic behavior for the orbits of particles which eventually will get lost by diffusion in the outer parts of the beam. • Rule of thumb  Avoid low order resonances FMAP_Workshop - April 1, 2004

  7. Benefits of Periodicity Tune plane - resonances up to 5th order Allowed resonances All resonances working point Unfortunately there is no simple way to forecast the real strength of a resonances without a realistic model of the ring and a tracking code. FMAP_Workshop - April 1, 2004

  8. ALS : Ideal Lattice versus Calibrated Model FMAP_Workshop - April 1, 2004

  9. Ideal versus Calibrated Model • Introducing linear errors fundamentally changes the beam dynamics • Ideal ring • The dynamic aperture is large • Small chaotic zone at large amplitudes • Particle loss is fast • Particle loss is due to high order resonances • Ring with calibrated linear errors • Dynamic aperture is smaller • Large chaotic zone at large amplitudes • Particle loss is slow • Particle loss is due to lower order unallowed resonances FMAP_Workshop - April 1, 2004

  10. Ideal versus Calibrated Model • Introducing linear errors fundamentally changes the beam dynamics • Ideal ring • The dynamic aperture is large • Small chaotic zone at large amplitudes • Particle loss is fast • Particle loss is due to high order resonances • Ring with calibrated linear errors • Dynamic aperture is smaller • Large chaotic zone at large amplitudes • Particle loss is slow • Particle loss is due to lower order unallowed resonances FMAP_Workshop - April 1, 2004

  11. Vertical orbit diffusion – On-energy example Particle are lost in the vertical plane • via nonlinear coupling and diffusion of the trajectory. Example : Particle launched at 12 mm horizontally and 1 mm vertically and tracked with damping and synchrotron oscillations. FMAP_Workshop - April 1, 2004

  12. Frequency Map Analysis Vertical Tune Vertical Amplitude [mm] Horizontal Tune Horizontal Amplitude [mm] Frequency Space Amplitude Space 4 8.2 8.0 0 0 14.0 14.25 15 FMAP_Workshop - April 1, 2004

  13. Frequency Map Analysis Vertical Tune Vertical Amplitude [mm] Horizontal Tune Horizontal Amplitude [mm] Frequency Space Amplitude Space working point 4 8.2 8.0 0 0 14.0 14.25 15 FMAP_Workshop - April 1, 2004

  14. Tools and Techniques FMAP_Workshop - April 1, 2004

  15. Tools and Techniques FMAP_Workshop - April 1, 2004

  16. Frequency Map Analysis Frequency Space Amplitude Space 4 8.25 Vertical Tune Vertical Amplitude [mm] 8.0 0 0 14.0 15 14.25 Horizontal Tune Horizontal Amplitude [mm] FMAP_Workshop - April 1, 2004

  17. On-energy dynamic aperture - frequency map (left) versus induced amplitude (right) Frequency Map Induced Amplitude FMAP_Workshop - April 1, 2004

  18. Injection efficiency • Like to have a good injection efficiency • Minimize fill times • Minimize radiation levels • Top-off • Insertion devices • At the ALS the injected beam is horizontally offset by ~10mm from the stored beam when it enters the ring. • The injected beam oscillates about the stored beam and slowly damps down. • If particles in the injected beam encounter regions of high diffusion they can be lost. Goal is to ensure that the particle motion is stable in the region where injected particles may travel FMAP_Workshop - April 1, 2004

  19. Example : Superbend Upgrade Normal ALS Sector QDA 1 QDA 2 Modified ALS Sector • In three of the twelve ALS Sectors • Replaced the central combined functiondipole with a Superbend and two quadrupoles FMAP_Workshop - April 1, 2004

  20. Frequency Maps without Superbends (Top) versus with Superbends (Bottom) Amplitude Space Frequency Space 4 8.25 Vertical Tune Vertical Amplitude [mm] 0 8.0 4 8.25 Vertical Amplitude [mm] Vertical Tune 0 8.0 0 15 14.0 14.25 Horizontal Tune Horizontal Amplitude [mm] FMAP_Workshop - April 1, 2004

  21. Momentum Aperture and Lifetime Frequency Map Analysis has been extended to study the momentum aperture and the effect on lifetime In the case of the Superbends the predictions agreed with the result to within 5% The off energy frequency maps will be discussed in the next talk. FMAP_Workshop - April 1, 2004

  22. Other Results Frequency Map Analysis has been an important technique for optimizing and predicting the performance of future upgrades In addition to the Superbend Upgrade we have used FMA for studying • Effect of Insertion Devices with Complicated Field Profiles • Smaller Gap Insertion Devices • Femtosecond Slicing Upgrade • Higher Tune Lattice • … FMAP_Workshop - April 1, 2004

  23. Some References • H. Dumas and J. Laskar, Phys. Rev. Lett. 70, 2975-2979 • J. Laskar and D. Robin, “Application of Frequency Map Analysis to the ALS”, Particle Accelerators, 1996, Vol 54 pp. 183-192 • D. Robin and J. Laskar, “Understanding the Nonlinear Beam Dynamics of the Advanced Light Source”, Proceedings of the 1997 Computational Particle Accelerator Conference • D. Robin, J. Safranek, and W. Decking, “Realizing the benefits of restored periodicity in the advanced light source”, PRST, Vol 2, 044001 (1999) • D. Robin, C. Steier, J. Laskar, and L. Nadolski, “Global Dynamics of the Advanced Light Source Revealed through Experimental Frequency Map Analysis”, Phys. Rev. Lett. Vol. 85, No. 3 (2000) • C. Steier, et. al.,”Measuring and optimizing the momentum aperture in a particle accelerator”,Phys. Rev. E. Vol. 65, 056506 • D. Robin and C. Steier, W. Wan, and A. Wolski, “Impact of Narrow Gap Undulators on the Advanced Light Source”, Proceedings of the 2003 Particle Accelerator Conference • D. Robin, “Superbend Upgrade of the Advanced Light Source”, Proceedings of the 2003 Particle Accelerator Conference • Y. Wu, E. Forest, and D. Robin, “Explicit symplectic integrator for s-dependent static magnetic field”, Phys Rev. E. Vol 68 046502 (2003) FMAP_Workshop - April 1, 2004

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