Paper |
Title |
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TUA01 |
Parallel Operation of SASE1 and SASE3 at the European XFEL |
25 |
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- S. Liu, F. Brinker, W. Decking, L. Fröhlich, R. Kammering, D. Nölle, F. Obier, E. Schneidmiller, M. Scholz, T. Wilksen, M.V. Yurkov
DESY, Hamburg, Germany
- R. Boll, N. Gerasimova, T. Mazza, M. Meyer, A. Scherz, H. Sinn
EuXFEL, Schenefeld, Germany
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At the European XFEL a hard X-Ray SASE FEL (SA-SE1) and a soft X-Ray SASE FEL (SASE3) share in series the same electron beamline. This configuration couples the operation conditions for both undulators and their subsequent user experiments in terms of SASE in-tensity and background. We report on our experience in parallel operation and discuss the solutions that enable the operation of both undulators as independently as possible.
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Slides TUA01 [13.809 MB]
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-FEL2019-TUA01
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About • |
paper received ※ 26 August 2019 paper accepted ※ 17 October 2019 issue date ※ 05 November 2019 |
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WEP008 |
Multi-Beamline Operation at the European XFEL |
335 |
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- L. Fröhlich, A. Aghababyan, V. Balandin, B. Beutner, F. Brinker, W. Decking, N. Golubeva, O. Hensler, Y. Janik, R. Kammering, H. Kay, T. Limberg, S. Liu, D. Nölle, F. Obier, M. Omet, M. Scholz, T. Wamsat, T. Wilksen, J. Wortmann
DESY, Hamburg, Germany
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The European XFEL uses a unique beam distribution scheme to direct electron bunches to its three undulator lines. The accelerator delivers up to 600 microsecond long bunch trains, out of which parts or individual bunches can be selected for photon production in any of the FELs. This contribution gives a brief overview of the kicker-septum scheme facilitating this and highlights how even complex bunch patterns can easily be configured via the timing system.
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-FEL2019-WEP008
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About • |
paper received ※ 19 August 2019 paper accepted ※ 29 August 2019 issue date ※ 05 November 2019 |
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WEP013 |
Fast Kicker System for European XFEL Beam Distribution |
353 |
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- F. Obier, W. Decking, M. Hüning, J. Wortmann
DESY, Hamburg, Germany
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A special feature of the European XFEL X-ray laser is the possibility to distribute the electron bunches of one beam pulse to different free-electron laser (FEL) beam-lines. This is achieved through a combination of kickers and a Lambertson DC septum. The integration of a beam abort dump allows a flexible selection of the bunch pattern at the FEL experiment, while the superconducting linear accelerator operates with constant beam loading. The driver linac of the FEL can deliver up to 600 µs long bunch trains with a repetition rate of 10 Hz and a maximum energy of 17.5 GeV. The FEL process poses very strict requirements on the stability of the beam position and hence on all upstream magnets. It was therefore decided to split the beam distribution system into two kicker systems, long pulse kickers with very stable amplitude (flat-top) and relatively slow pulses and fast stripline kickers with moderate stability but very fast pulses. This contribution gives a brief overview of the fast kicker system.
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-FEL2019-WEP013
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About • |
paper received ※ 20 August 2019 paper accepted ※ 27 August 2019 issue date ※ 05 November 2019 |
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WEP014 |
Long Pulse Kicker for European XFEL Beam Distribution |
357 |
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- F. Obier, W. Decking, M. Hüning, J. Wortmann
DESY, Hamburg, Germany
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A special feature of the European XFEL X-ray laser is the possibility to distribute the electron bunches of one beam pulse to different free-electron laser (FEL) beam-lines. This is achieved through a combination of kickers and a Lambertson DC septum. The integration of a beam abort dump allows a flexible selection of the bunch pattern at the FEL experiment, while the superconducting linear accelerator operates with constant beam loading. The driver linac of the FEL can deliver up to 600 µs long bunch trains with a repetition rate of 10 Hz and a maximum energy of 17.5 GeV. The FEL process poses very strict requirements on the stability of the beam position and hence on all upstream magnets. It was therefore decided to split the beam distribution system into two kicker systems, long pulse kickers with very stable amplitude (flat-top) and relatively slow pulses and fast stripline kickers with moderate stability but very fast pulses. This contribution gives a brief overview of the long pulse kicker system.
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-FEL2019-WEP014
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|
About • |
paper received ※ 20 August 2019 paper accepted ※ 27 August 2019 issue date ※ 05 November 2019 |
|
Export • |
reference for this paper using
※ BibTeX,
※ LaTeX,
※ Text/Word,
※ RIS,
※ EndNote (xml)
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