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TUP079 |
Status of the Hard X-Ray Self-Seeding Setup at the European XFEL |
242 |
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- G. Geloni, S. Karabekyan, D. La Civita, L. Samoylova, S. Serkez, R. Shayduk, H. Sinn, V. Sleziona, M. Vannoni, M. Yakopov
EuXFEL, Schenefeld, Germany
- J.W.J. Anton, S.P. Kearney, D. Shu
ANL, Lemont, Illinois, USA
- V.D. Blank, S. Terentiev
TISNCM, Troitsk, Russia
- W. Decking, V. Kocharyan, S. Liu, E. Negodin, E. Saldin, T. Wohlenberg
DESY, Hamburg, Germany
- X. Dong
European X-Ray Free-Electron Laser Facility GmbH, Schelefeld, Germany
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A Hard X-Ray Self-Seeding (HXRSS) setup will be soon commissioned at the European XFEL. It relies on a two-chicanes scheme to deal, in particular, with the high pulse repetition rate of the facility. In this contribution we review the physics choices made at the design stage and the expected performance of the setup. We will also focus on the description of the hardware installations made at the SASE2 line of the European XFEL.
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-FEL2019-TUP079
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About • |
paper received ※ 27 August 2019 paper accepted ※ 28 August 2019 issue date ※ 05 November 2019 |
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TUD04 |
Cavity-Based Free-Electron Laser Research and Development: A Joint Argonne National Laboratory and SLAC National Laboratory Collaboration |
282 |
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- G. Marcus, F.-J. Decker, G.L. Gassner, A. Halavanau, J.B. Hastings, Z. Huang, Y. Liu, J.P. MacArthur, R.A. Margraf, T.O. Raubenheimer, A. Sakdinawat, T.-F. Tan, D. Zhu
SLAC, Menlo Park, California, USA
- J.W.J. Anton, L. Assoufid, K. Goetze, W.G. Jansma, S.P. Kearney, K. Kim, R.R. Lindberg, A. Miceli, X. Shi, D. Shu, Yu. Shvyd’ko, J.P. Sullivan, M. White
ANL, Lemont, Illinois, USA
- B. Lantz
Stanford University, Stanford, California, USA
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One solution for producing longitudinally coherent FEL pulses is to store and recirculate the output of an amplifier in an X-ray cavity so that the X-ray pulse can interact with following fresh electron bunches over many passes. The X-ray FEL oscillator (XFELO) and the X-ray regenerative amplifier FEL (XRAFEL) concepts use this technique and rely on the same fundamental ingredients to realize their full capability. Both schemes require a high repetition rate electron beam, an undulator to provide FEL gain, and an X-ray cavity to recirculate and monochromatize the radiation. The shared infrastructure, complementary performance characteristics, and potentially transformative FEL properties of the XFELO and XRAFEL have brought together a joint Argonne National Laboratory (ANL) and SLAC National Laboratory (SLAC) collaboration aimed at enabling these schemes at LCLS-II. We present plans to install a rectangular X-ray cavity in the LCLS-II undulator hall and perform experiments employing 2-bunch copper RF linac accelerated electron beams. This includes performing cavity ring-down measurements and 2-pass gain measurements for both the low-gain XFELO and the high-gain RAFEL schemes.
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Slides TUD04 [12.425 MB]
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-FEL2019-TUD04
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About • |
paper received ※ 25 August 2019 paper accepted ※ 29 August 2019 issue date ※ 05 November 2019 |
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WEP079 |
Effect of Heat Load on Cryo-Cooled Monochromators at the European X-Ray Free-Electron Laser: Simulations and First Experimental Observations |
502 |
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- I. Petrov, U. Boesenberg, M. Dommach, J. Eidam, J. Hallmann, K. Kazarian, C. Kim, W. Lu, A. Madsen, J. Möller, M. Reiser, L. Samoylova, R. Shayduk, H. Sinn, V. Sleziona, A. Zozulya
EuXFEL, Schenefeld, Germany
- J.W.J. Anton, S.P. Kearney, D. Shu
ANL, Lemont, Illinois, USA
- X. Dong
SINAP, Shanghai, People’s Republic of China
- X. Dong
SARI-CAS, Pudong, Shanghai, People’s Republic of China
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European XFEL (EuXFEL) generates high-intensity ultra-short pulses at MHz repetition rate. At hard X-ray instruments, cryo-cooled silicon monochromators are used to reduce pulse bandwidth. Here, first experimental observations during commissioning of a cryo-cooled monochromator at Materials Imaging and Dynamics (MID) instrument are presented and compared with heat flow simulations. A thermal relaxation time is estimated and compared with arrival time interval between pulses. This provides the repetition rate tolerable for stable operation of monochromator.
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DOI • |
reference for this paper
※ https://doi.org/10.18429/JACoW-FEL2019-WEP079
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About • |
paper received ※ 19 August 2019 paper accepted ※ 25 August 2019 issue date ※ 05 November 2019 |
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