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Analysis of Multi-Turn ERLs for X-ray Sources

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Presentation on theme: "Analysis of Multi-Turn ERLs for X-ray Sources"— Presentation transcript:

1 Analysis of Multi-Turn ERLs for X-ray Sources
Georg Hoffstaetter Cornell Physics Dept. / CLASSE Progress report on a paper with I. Bazarov, S. Belomestnyk, J. Crittenden, M. Ehrlichman, M. Liepe, C. Mayes, S. Peck, M. Tigner Georg H. Hoffstaetter, October 5, 2004

2 BBU: Collective Instabilities
Higher Order Modes Georg H. Hoffstaetter, October 5, 2004

3 BBU: Collective Instabilities
Higher Order Modes Georg H. Hoffstaetter, October 5, 2004

4 BBU: Collective Instabilities
Higher Order Modes Georg H. Hoffstaetter, October 5, 2004

5 HOM with BBU: Starting from Noise
Georg H. Hoffstaetter, October 5, 2004

6 Main Linac Cavity Optimization
Optimize shape of cavity (>70 parameter…) to minimize cryogenic losses and maximize limits to beam current Understand sensitivity of optimized design to fabrication errors; find “sloppy” parameter! Higher-Order-modes Red: Optimized cavity; blue: perturbed cavities

7 Cavities with misalignments
R/Q and Q in cavities with misalignments can be significantly worse then expected, but orders of magnitude. (Here for 1/16mm construction error) A very good safety margin for BBU is therefore needed. Georg H. Hoffstaetter, October 5, 2004

8 Reason for high sensitivity of HOMs
Trapped TTF HOMs: Construction errors in cells change the individual cell’s HOM frequencies and hinder good coupling between cells, leading to trapped modes with much larger Q. Georg H. Hoffstaetter, October 5, 2004

9 +-1/16 mm perturbations, 400 cavities
Perturbatio: Baseline Center Cell (minimize cryo-load) and optimized end cells (HOM damping) +-1/16 mm perturbations, 400 cavities

10 +-1/16 mm perturbations, 400 cavities
Center Cell (optimized HOM passband widths), optimized end cells (HOM damping) +-1/16 mm perturbations, 400 cavities

11 +-1/8 mm perturbations, 400 cavities
Center Cell (optimized HOM passband widths), optimized end cells (HOM damping) +-1/8 mm perturbations, 400 cavities

12 One turn BBU Threshold current
Improved center cell with increased width passbands Preliminary optimized end-cells, no perturbations, 10 MHz HOM frequency spread One turn BBU Threshold current 1000 simulations

13 Improved center cell with increased width passbands, and deformations
+- 1/16 mm perturbations, no additional HOM frequency spread One turn BBU Threshold current

14 Detuning from deformations
+- 1/16 mm perturbations, no additional HOM frequency spread  1 MHz only!

15 Need for BBU investigation
Is an ERL test loop needed and why? For BBU studies? Trapped modes above the beam pipe cutoff are hard to measure without a return loop. Are there beam based measurements without return loop? Excite by beam of 1MHz rep rate as function of x offset to get R/Q*Q. From the width of the resonances one can get Q. Needs a linac cryomodule with beam, possibly a shortened model. Important to measure Q of HOMs in vertical test as quality test. Study is needed on keeping production tolerances. Conclusion: BBU effects are well understood and mitigations have been well understood in experiments with existing return loops. Georg H. Hoffstaetter, October 5, 2004


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