1
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Lima FA, Otte F, Vakili M, Ardana-Lamas F, Biednov M, Dall’Antonia F, Frankenberger P, Gawelda W, Gelisio L, Han H, Huang X, Jiang Y, Kloos M, Kluyver T, Knoll M, Kubicek K, Bermudez Macias IJ, Schulz J, Turkot O, Uemura Y, Valerio J, Wang H, Yousef H, Zalden P, Khakhulin D, Bressler C, Milne C. Experimental capabilities for liquid jet samples at sub-MHz rates at the FXE Instrument at European XFEL. JOURNAL OF SYNCHROTRON RADIATION 2023; 30:1168-1182. [PMID: 37860937 PMCID: PMC10624029 DOI: 10.1107/s1600577523008159] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 07/14/2023] [Accepted: 09/18/2023] [Indexed: 10/21/2023]
Abstract
The Femtosecond X-ray Experiments (FXE) instrument at the European X-ray Free-Electron Laser (EuXFEL) provides an optimized platform for investigations of ultrafast physical, chemical and biological processes. It operates in the energy range 4.7-20 keV accommodating flexible and versatile environments for a wide range of samples using diverse ultrafast X-ray spectroscopic, scattering and diffraction techniques. FXE is particularly suitable for experiments taking advantage of the sub-MHz repetition rates provided by the EuXFEL. In this paper a dedicated setup for studies on ultrafast biological and chemical dynamics in solution phase at sub-MHz rates at FXE is presented. Particular emphasis on the different liquid jet sample delivery options and their performance is given. Our portfolio of high-speed jets compatible with sub-MHz experiments includes cylindrical jets, gas dynamic virtual nozzles and flat jets. The capability to perform multi-color X-ray emission spectroscopy (XES) experiments is illustrated by a set of measurements using the dispersive X-ray spectrometer in von Hamos geometry. Static XES data collected using a multi-crystal scanning Johann-type spectrometer are also presented. A few examples of experimental results on ultrafast time-resolved X-ray emission spectroscopy and wide-angle X-ray scattering at sub-MHz pulse repetition rates are given.
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Affiliation(s)
- F. A. Lima
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - F. Otte
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
- Fakultät für Physik, Technical University Dortmund, Dortmund, Germany
| | - M. Vakili
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
- Center for Free-Electron Laser Science CFEL, Deutsches Elektronen-Synchrotron DESY, Notkestr. 85, 22607 Hamburg, Germany
| | | | - M. Biednov
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | | | | | - W. Gawelda
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
- Faculty of Physics, Adam Mickiewicz University, 61-614 Poznań, Poland
| | - L. Gelisio
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - H. Han
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - X. Huang
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Y. Jiang
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - M. Kloos
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - T. Kluyver
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - M. Knoll
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - K. Kubicek
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
- The Hamburg Centre for Ultrafast Imaging, 22761 Hamburg, Germany
- Institut für Experimentalphysik, Universität Hamburg, 22607 Hamburg, Germany
| | | | - J. Schulz
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - O. Turkot
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Y. Uemura
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - J. Valerio
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - H. Wang
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - H. Yousef
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - P. Zalden
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - D. Khakhulin
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - C. Bressler
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
- The Hamburg Centre for Ultrafast Imaging, 22761 Hamburg, Germany
- Institut für Experimentalphysik, Universität Hamburg, 22607 Hamburg, Germany
| | - C. Milne
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
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2
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Diez M, Kirchberg H, Galler A, Schulz S, Biednov M, Bömer C, Choi TK, Rodriguez-Fernandez A, Gawelda W, Khakhulin D, Kubicek K, Lima F, Otte F, Zalden P, Coffee R, Thorwart M, Bressler C. A sensitive high repetition rate arrival time monitor for X-ray free electron lasers. Nat Commun 2023; 14:2495. [PMID: 37120432 PMCID: PMC10148857 DOI: 10.1038/s41467-023-38143-y] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 09/20/2022] [Accepted: 04/17/2023] [Indexed: 05/01/2023] Open
Abstract
X-ray free-electron laser sources enable time-resolved X-ray studies with unmatched temporal resolution. To fully exploit ultrashort X-ray pulses, timing tools are essential. However, new high repetition rate X-ray facilities present challenges for currently used timing tool schemes. Here we address this issue by demonstrating a sensitive timing tool scheme to enhance experimental time resolution in pump-probe experiments at very high pulse repetition rates. Our method employs a self-referenced detection scheme using a time-sheared chirped optical pulse traversing an X-ray stimulated diamond plate. By formulating an effective medium theory, we confirm subtle refractive index changes, induced by sub-milli-Joule intense X-ray pulses, that are measured in our experiment. The system utilizes a Common-Path-Interferometer to detect X-ray-induced phase shifts of the optical probe pulse transmitted through the diamond sample. Owing to the thermal stability of diamond, our approach is well-suited for MHz pulse repetition rates in superconducting linear accelerator-based free-electron lasers.
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Affiliation(s)
- Michael Diez
- European XFEL GmbH, Holzkoppel 4, 22869, Schenefeld, Germany.
- The Hamburg Centre for Ultrafast Imaging, Luruper Chaussee 149, 22761, Hamburg, Germany.
| | - Henning Kirchberg
- I. Institut für Theoretische Physik, Universität Hamburg, Notkestr. 9, 22607, Hamburg, Germany
- Department of Chemistry, University of Pennsylvania, Philadelphia, Pennsylvania, 19104, USA
| | - Andreas Galler
- European XFEL GmbH, Holzkoppel 4, 22869, Schenefeld, Germany.
| | - Sebastian Schulz
- Deutsches Elektronen-Synchrotron DESY, Notkestraße 85, 22607, Hamburg, Germany
| | - Mykola Biednov
- European XFEL GmbH, Holzkoppel 4, 22869, Schenefeld, Germany
| | - Christina Bömer
- European XFEL GmbH, Holzkoppel 4, 22869, Schenefeld, Germany
- Deutsches Elektronen-Synchrotron DESY, Notkestraße 85, 22607, Hamburg, Germany
| | - Tae-Kyu Choi
- European XFEL GmbH, Holzkoppel 4, 22869, Schenefeld, Germany
- XFEL division, Pohang Accelerator Laboratory, Jigok-ro 127-80, 37673, Pohang, Republic of Korea
| | | | - Wojciech Gawelda
- European XFEL GmbH, Holzkoppel 4, 22869, Schenefeld, Germany
- Faculty of Physics, Adam Mickiewicz University, ul. Uniwersytetu Poznańskiego 2, 61-614, Poznań, Poland
- Department of Chemistry, Faculty of Sciences, Universidad Autónoma de Madrid, 28049, Madrid, Spain
- IMDEA-Nanociencia, Calle Faraday 9, 28049, Madrid, Spain
| | | | - Katharina Kubicek
- European XFEL GmbH, Holzkoppel 4, 22869, Schenefeld, Germany
- The Hamburg Centre for Ultrafast Imaging, Luruper Chaussee 149, 22761, Hamburg, Germany
- Fachbereich Physik, Universität Hamburg, Notkestraße 9-11, 22607, Hamburg, Germany
| | - Frederico Lima
- European XFEL GmbH, Holzkoppel 4, 22869, Schenefeld, Germany
| | - Florian Otte
- European XFEL GmbH, Holzkoppel 4, 22869, Schenefeld, Germany
| | - Peter Zalden
- European XFEL GmbH, Holzkoppel 4, 22869, Schenefeld, Germany
| | - Ryan Coffee
- SLAC National Accelerator Laboratory, 2575 Sand Hill Rd., Menlo Park, CA, 94025, USA
- The Pulse Institute, SLAC National Accelerator Laboratory, Menlo Park, CA, 94028, USA
| | - Michael Thorwart
- The Hamburg Centre for Ultrafast Imaging, Luruper Chaussee 149, 22761, Hamburg, Germany
- I. Institut für Theoretische Physik, Universität Hamburg, Notkestr. 9, 22607, Hamburg, Germany
| | - Christian Bressler
- European XFEL GmbH, Holzkoppel 4, 22869, Schenefeld, Germany.
- The Hamburg Centre for Ultrafast Imaging, Luruper Chaussee 149, 22761, Hamburg, Germany.
- Fachbereich Physik, Universität Hamburg, Notkestraße 9-11, 22607, Hamburg, Germany.
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3
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Kim J, Kim JS, Kim J, Chae B, Kim JH, Lim J. Surface figure correction with roughness reduction using carbon-doped platinum film for high-precision X-ray mirror fabrication. OPTICS EXPRESS 2023; 31:7579-7588. [PMID: 36859887 DOI: 10.1364/oe.480993] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/15/2022] [Accepted: 01/25/2023] [Indexed: 06/18/2023]
Abstract
To obtain the surface shape of an X-ray mirror with high precision, a differential deposition method was used instead of a direct removal method. To modify the mirror surface shape using the differential deposition method, it is necessary to coat it with a thick film, and the co-deposition method is used to suppress the increase in surface roughness. The addition of C to the Pt thin film, which is often used as an X-ray optical thin film, resulted in lower surface roughness compared with that with the Pt coating alone, and the stress change according to the thin film thickness was evaluated. Differential deposition controls the speed of the substrate during coating based on continuous motion. The stage was controlled by calculating the dwell time through deconvolution calculations based on the accurate measurement of the unit coating distribution and target shape. We successfully fabricated an X-ray mirror with high precision. This study indicated that an X-ray mirror surface could be manufactured by modifying the surface shape at a micrometer level through the coating. Changing the shape of existing mirrors can not only result in the manufacture of high-precision X-ray mirrors but also improve their performance.
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4
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Zastrau U, Appel K, Baehtz C, Baehr O, Batchelor L, Berghäuser A, Banjafar M, Brambrink E, Cerantola V, Cowan TE, Damker H, Dietrich S, Di Dio Cafiso S, Dreyer J, Engel HO, Feldmann T, Findeisen S, Foese M, Fulla-Marsa D, Göde S, Hassan M, Hauser J, Herrmannsdörfer T, Höppner H, Kaa J, Kaever P, Knöfel K, Konôpková Z, Laso García A, Liermann HP, Mainberger J, Makita M, Martens EC, McBride EE, Möller D, Nakatsutsumi M, Pelka A, Plueckthun C, Prescher C, Preston TR, Röper M, Schmidt A, Seidel W, Schwinkendorf JP, Schoelmerich MO, Schramm U, Schropp A, Strohm C, Sukharnikov K, Talkovski P, Thorpe I, Toncian M, Toncian T, Wollenweber L, Yamamoto S, Tschentscher T. The High Energy Density Scientific Instrument at the European XFEL. JOURNAL OF SYNCHROTRON RADIATION 2021; 28:1393-1416. [PMID: 34475288 PMCID: PMC8415338 DOI: 10.1107/s1600577521007335] [Citation(s) in RCA: 8] [Impact Index Per Article: 2.7] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 03/06/2021] [Accepted: 07/15/2021] [Indexed: 06/13/2023]
Abstract
The European XFEL delivers up to 27000 intense (>1012 photons) pulses per second, of ultrashort (≤50 fs) and transversely coherent X-ray radiation, at a maximum repetition rate of 4.5 MHz. Its unique X-ray beam parameters enable groundbreaking experiments in matter at extreme conditions at the High Energy Density (HED) scientific instrument. The performance of the HED instrument during its first two years of operation, its scientific remit, as well as ongoing installations towards full operation are presented. Scientific goals of HED include the investigation of extreme states of matter created by intense laser pulses, diamond anvil cells, or pulsed magnets, and ultrafast X-ray methods that allow their diagnosis using self-amplified spontaneous emission between 5 and 25 keV, coupled with X-ray monochromators and optional seeded beam operation. The HED instrument provides two target chambers, X-ray spectrometers for emission and scattering, X-ray detectors, and a timing tool to correct for residual timing jitter between laser and X-ray pulses.
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Affiliation(s)
- Ulf Zastrau
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Karen Appel
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Carsten Baehtz
- Helmholtz-Zentrum Dresden-Rossendorf eV, 01328 Dresden, Germany
| | - Oliver Baehr
- Helmholtz-Zentrum Dresden-Rossendorf eV, 01328 Dresden, Germany
| | | | | | - Mohammadreza Banjafar
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
- Helmholtz-Zentrum Dresden-Rossendorf eV, 01328 Dresden, Germany
| | | | | | - Thomas E. Cowan
- Helmholtz-Zentrum Dresden-Rossendorf eV, 01328 Dresden, Germany
| | - Horst Damker
- Deutsches Elektronen-Synchrotron DESY, 22607 Hamburg, Germany
| | | | | | - Jörn Dreyer
- Helmholtz-Zentrum Dresden-Rossendorf eV, 01328 Dresden, Germany
| | - Hans-Olaf Engel
- Helmholtz-Zentrum Dresden-Rossendorf eV, 01328 Dresden, Germany
| | | | | | - Manon Foese
- Deutsches Elektronen-Synchrotron DESY, 22607 Hamburg, Germany
| | | | | | - Mohammed Hassan
- Helmholtz-Zentrum Dresden-Rossendorf eV, 01328 Dresden, Germany
| | - Jens Hauser
- Helmholtz-Zentrum Dresden-Rossendorf eV, 01328 Dresden, Germany
| | | | - Hauke Höppner
- Helmholtz-Zentrum Dresden-Rossendorf eV, 01328 Dresden, Germany
| | - Johannes Kaa
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
- Technische Universität Dortmund, 44227 Dortmund, Germany
| | - Peter Kaever
- Helmholtz-Zentrum Dresden-Rossendorf eV, 01328 Dresden, Germany
| | - Klaus Knöfel
- Helmholtz-Zentrum Dresden-Rossendorf eV, 01328 Dresden, Germany
| | | | | | | | - Jona Mainberger
- Deutsches Elektronen-Synchrotron DESY, 22607 Hamburg, Germany
| | - Mikako Makita
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | | | - Emma E. McBride
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
- SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA
| | - Dominik Möller
- Helmholtz-Zentrum Dresden-Rossendorf eV, 01328 Dresden, Germany
| | | | - Alexander Pelka
- Helmholtz-Zentrum Dresden-Rossendorf eV, 01328 Dresden, Germany
| | | | | | | | - Michael Röper
- Deutsches Elektronen-Synchrotron DESY, 22607 Hamburg, Germany
| | | | - Wolfgang Seidel
- Helmholtz-Zentrum Dresden-Rossendorf eV, 01328 Dresden, Germany
| | | | | | - Ulrich Schramm
- Helmholtz-Zentrum Dresden-Rossendorf eV, 01328 Dresden, Germany
| | - Andreas Schropp
- Deutsches Elektronen-Synchrotron DESY, 22607 Hamburg, Germany
| | | | | | - Peter Talkovski
- Deutsches Elektronen-Synchrotron DESY, 22607 Hamburg, Germany
| | - Ian Thorpe
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Monika Toncian
- Helmholtz-Zentrum Dresden-Rossendorf eV, 01328 Dresden, Germany
| | - Toma Toncian
- Helmholtz-Zentrum Dresden-Rossendorf eV, 01328 Dresden, Germany
| | | | - Shingo Yamamoto
- Helmholtz-Zentrum Dresden-Rossendorf eV, 01328 Dresden, Germany
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5
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Dommach M, Di Felice M, Dickert B, Finze D, Eidam J, Kohlstrunk N, Neumann M, Meyn F, Petrich M, Rio B, Sinn H, Villanueva R. The photon beamline vacuum system of the European XFEL. JOURNAL OF SYNCHROTRON RADIATION 2021; 28:1229-1236. [PMID: 34212888 PMCID: PMC8284404 DOI: 10.1107/s1600577521005154] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 02/18/2021] [Accepted: 05/13/2021] [Indexed: 06/13/2023]
Abstract
The photon beamline vacuum system of the European X-ray Free-Electron Laser Facility (European XFEL) is described. The ultra-large, in total more than 3 km-long, fan-like vacuum system, consisting of three photon beamlines is an essential part of the photon beam transport. It is located between the accelerator vacuum system and the scientific instruments. The main focus of the design was on the efficiency, reliability and robustness of the entire system to ensure the retention of beam properties and the operation of the X-ray optics and X-ray photon diagnostics components. Installation started in late 2014, the first of the three beamline vacuum systems was commissioned in spring 2017, and the last one was operational in mid-2018. The present state and experience from the first years of operation are outlined.
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Affiliation(s)
| | | | | | - Denis Finze
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Janni Eidam
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | | | - Maik Neumann
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Frederik Meyn
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | | | - Benoit Rio
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Harald Sinn
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
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6
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Madsen A, Hallmann J, Ansaldi G, Roth T, Lu W, Kim C, Boesenberg U, Zozulya A, Möller J, Shayduk R, Scholz M, Bartmann A, Schmidt A, Lobato I, Sukharnikov K, Reiser M, Kazarian K, Petrov I. Materials Imaging and Dynamics (MID) instrument at the European X-ray Free-Electron Laser Facility. JOURNAL OF SYNCHROTRON RADIATION 2021; 28:637-649. [PMID: 33650576 PMCID: PMC7941285 DOI: 10.1107/s1600577521001302] [Citation(s) in RCA: 22] [Impact Index Per Article: 7.3] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/19/2020] [Accepted: 02/04/2021] [Indexed: 05/27/2023]
Abstract
The Materials Imaging and Dynamics (MID) instrument at the European X-ray Free-Electron Laser (EuXFEL) facility is described. EuXFEL is the first hard X-ray free-electron laser operating in the MHz repetition range which provides novel science opportunities. The aim of MID is to enable studies of nano-structured materials, liquids, and soft- and hard-condensed matter using the bright X-ray beams generated by EuXFEL. Particular emphasis is on studies of structure and dynamics in materials by coherent scattering and imaging using hard X-rays. Commission of MID started at the end of 2018 and first experiments were performed in 2019.
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Affiliation(s)
- A. Madsen
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - J. Hallmann
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - G. Ansaldi
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - T. Roth
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - W. Lu
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - C. Kim
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - U. Boesenberg
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - A. Zozulya
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - J. Möller
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - R. Shayduk
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - M. Scholz
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - A. Bartmann
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - A. Schmidt
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - I. Lobato
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - K. Sukharnikov
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - M. Reiser
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - K. Kazarian
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - I. Petrov
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
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7
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Wollenweber L, Preston TR, Descamps A, Cerantola V, Comley A, Eggert JH, Fletcher LB, Geloni G, Gericke DO, Glenzer SH, Göde S, Hastings J, Humphries OS, Jenei A, Karnbach O, Konopkova Z, Loetzsch R, Marx-Glowna B, McBride EE, McGonegle D, Monaco G, Ofori-Okai BK, Palmer CAJ, Plückthun C, Redmer R, Strohm C, Thorpe I, Tschentscher T, Uschmann I, Wark JS, White TG, Appel K, Gregori G, Zastrau U. High-resolution inelastic x-ray scattering at the high energy density scientific instrument at the European X-Ray Free-Electron Laser. THE REVIEW OF SCIENTIFIC INSTRUMENTS 2021; 92:013101. [PMID: 33514249 DOI: 10.1063/5.0022886] [Citation(s) in RCA: 7] [Impact Index Per Article: 2.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 07/24/2020] [Accepted: 12/12/2020] [Indexed: 06/12/2023]
Abstract
We introduce a setup to measure high-resolution inelastic x-ray scattering at the High Energy Density scientific instrument at the European X-Ray Free-Electron Laser (XFEL). The setup uses the Si (533) reflection in a channel-cut monochromator and three spherical diced analyzer crystals in near-backscattering geometry to reach a high spectral resolution. An energy resolution of 44 meV is demonstrated for the experimental setup, close to the theoretically achievable minimum resolution. The analyzer crystals and detector are mounted on a curved-rail system, allowing quick and reliable changes in scattering angle without breaking vacuum. The entire setup is designed for operation at 10 Hz, the same repetition rate as the high-power lasers available at the instrument and the fundamental repetition rate of the European XFEL. Among other measurements, it is envisioned that this setup will allow studies of the dynamics of highly transient laser generated states of matter.
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Affiliation(s)
- L Wollenweber
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - T R Preston
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - A Descamps
- SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA
| | - V Cerantola
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - A Comley
- Atomic Weapons Establishment, Aldermaston, Reading, Berkshire RG7 4PR, United Kingdom
| | - J H Eggert
- Lawrence Livermore National Laboratory, 7000 East Avenue, Livermore, California 94550, USA
| | - L B Fletcher
- SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA
| | - G Geloni
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - D O Gericke
- Centre for Fusion, Space & Astrophysics, Department of Physics, University of Warwick, Coventry CV4 7AL, United Kingdom
| | - S H Glenzer
- SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA
| | - S Göde
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - J Hastings
- SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA
| | - O S Humphries
- Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom
| | - A Jenei
- Lawrence Livermore National Laboratory, 7000 East Avenue, Livermore, California 94550, USA
| | - O Karnbach
- Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom
| | - Z Konopkova
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - R Loetzsch
- Institut für Optik und Quantenelektronik, Friedrich-Schiller-Universität Jena, Max-Wien-Platz 1, 07743 Jena, Germany
| | - B Marx-Glowna
- Institut für Optik und Quantenelektronik, Friedrich-Schiller-Universität Jena, Max-Wien-Platz 1, 07743 Jena, Germany
| | - E E McBride
- SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA
| | - D McGonegle
- Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom
| | - G Monaco
- Dipartimento di Fisica, Universita di Trento, via Sommarive 14, Povo 38123, TN, Italy
| | - B K Ofori-Okai
- SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA
| | - C A J Palmer
- School of Mathematics and Physics, Queen's University Belfast, University Road, BT7 1NN Belfast, United Kingdom
| | - C Plückthun
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - R Redmer
- Universität Rostock, Institut für Physik, Albert-Einstein-Straße 23-24, 18051 Rostock, Germany
| | - C Strohm
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - I Thorpe
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | | | - I Uschmann
- Institut für Optik und Quantenelektronik, Friedrich-Schiller-Universität Jena, Max-Wien-Platz 1, 07743 Jena, Germany
| | - J S Wark
- Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom
| | - T G White
- Physics Department, University of Nevada at Reno, Reno, Nevada 89506, USA
| | - K Appel
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - G Gregori
- Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom
| | - U Zastrau
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
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8
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Descamps A, Ofori-Okai BK, Appel K, Cerantola V, Comley A, Eggert JH, Fletcher LB, Gericke DO, Göde S, Humphries O, Karnbach O, Lazicki A, Loetzsch R, McGonegle D, Palmer CAJ, Plueckthun C, Preston TR, Redmer R, Senesky DG, Strohm C, Uschmann I, White TG, Wollenweber L, Monaco G, Wark JS, Hastings JB, Zastrau U, Gregori G, Glenzer SH, McBride EE. An approach for the measurement of the bulk temperature of single crystal diamond using an X-ray free electron laser. Sci Rep 2020; 10:14564. [PMID: 32884061 PMCID: PMC7471281 DOI: 10.1038/s41598-020-71350-x] [Citation(s) in RCA: 8] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 05/20/2020] [Accepted: 08/06/2020] [Indexed: 11/25/2022] Open
Abstract
We present a method to determine the bulk temperature of a single crystal diamond sample at an X-Ray free electron laser using inelastic X-ray scattering. The experiment was performed at the high energy density instrument at the European XFEL GmbH, Germany. The technique, based on inelastic X-ray scattering and the principle of detailed balance, was demonstrated to give accurate temperature measurements, within [Formula: see text] for both room temperature diamond and heated diamond to 500 K. Here, the temperature was increased in a controlled way using a resistive heater to test theoretical predictions of the scaling of the signal with temperature. The method was tested by validating the energy of the phonon modes with previous measurements made at room temperature using inelastic X-ray scattering and neutron scattering techniques. This technique could be used to determine the bulk temperature in transient systems with a temporal resolution of 50 fs and for which accurate measurements of thermodynamic properties are vital to build accurate equation of state and transport models.
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Affiliation(s)
- A Descamps
- SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA.
- Aeronautics and Astronautics Department, Stanford University, Stanford, CA, 94305, USA.
| | - B K Ofori-Okai
- SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA
| | - K Appel
- European X-Ray Free-Electron Laser Facility GmbH, Holzkoppel 4, 22869, Schenefeld, Germany
| | - V Cerantola
- European X-Ray Free-Electron Laser Facility GmbH, Holzkoppel 4, 22869, Schenefeld, Germany
| | - A Comley
- Atomic Weapons Establishment, Aldermaston, Reading, RG7 4PR, UK
| | - J H Eggert
- Lawrence Livermore National Laboratory, Livermore, CA, 94550, USA
| | - L B Fletcher
- SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA
| | - D O Gericke
- Centre for Fusion, Space and Astrophysics, Department of Physics, University of Warwick, Coventry, CV4 7AL, UK
| | - S Göde
- European X-Ray Free-Electron Laser Facility GmbH, Holzkoppel 4, 22869, Schenefeld, Germany
| | - O Humphries
- Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford, OX1 3PU, UK
| | - O Karnbach
- Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford, OX1 3PU, UK
| | - A Lazicki
- Lawrence Livermore National Laboratory, Livermore, CA, 94550, USA
| | - R Loetzsch
- Institut für Optik und Quantenelektronik, Friedrich-Schiller-Universität Jena, Max-Wien-Platz 1, 07743, Jena, Germany
- Helmholtz-Institut Jena, Fröbelstieg 3, 07743, Jena, Germany
| | - D McGonegle
- Atomic Weapons Establishment, Aldermaston, Reading, RG7 4PR, UK
- Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford, OX1 3PU, UK
| | - C A J Palmer
- School of Mathematics and Physics, Queen's University, University Road BT7 1NN, Belfast, UK
| | - C Plueckthun
- European X-Ray Free-Electron Laser Facility GmbH, Holzkoppel 4, 22869, Schenefeld, Germany
| | - T R Preston
- European X-Ray Free-Electron Laser Facility GmbH, Holzkoppel 4, 22869, Schenefeld, Germany
| | - R Redmer
- Institut für Physik, Universität Rostock, A.-Einstein-Str. 23-24, 18059, Rostock, Germany
| | - D G Senesky
- Aeronautics and Astronautics Department, Stanford University, Stanford, CA, 94305, USA
| | - C Strohm
- European X-Ray Free-Electron Laser Facility GmbH, Holzkoppel 4, 22869, Schenefeld, Germany
- Deutsches Elektronen Synchrotron, Notkestrasse 85, 22607, Hamburg, Germany
| | - I Uschmann
- Institut für Optik und Quantenelektronik, Friedrich-Schiller-Universität Jena, Max-Wien-Platz 1, 07743, Jena, Germany
- Helmholtz-Institut Jena, Fröbelstieg 3, 07743, Jena, Germany
| | - T G White
- University of Nevada, Reno, NV, 89557, USA
| | - L Wollenweber
- European X-Ray Free-Electron Laser Facility GmbH, Holzkoppel 4, 22869, Schenefeld, Germany
| | - G Monaco
- Dipartimento di Fisica, Università di Trento, Via Sommarive 14, 38123, Povo, TN, Italy
| | - J S Wark
- Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford, OX1 3PU, UK
| | - J B Hastings
- SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA
| | - U Zastrau
- European X-Ray Free-Electron Laser Facility GmbH, Holzkoppel 4, 22869, Schenefeld, Germany
| | - G Gregori
- Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford, OX1 3PU, UK
| | - S H Glenzer
- SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA
| | - E E McBride
- SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA
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9
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Galler A, Gawelda W, Biednov M, Bomer C, Britz A, Brockhauser S, Choi TK, Diez M, Frankenberger P, French M, Görries D, Hart M, Hauf S, Khakhulin D, Knoll M, Korsch T, Kubicek K, Kuster M, Lang P, Alves Lima F, Otte F, Schulz S, Zalden P, Bressler C. Scientific instrument Femtosecond X-ray Experiments (FXE): instrumentation and baseline experimental capabilities. JOURNAL OF SYNCHROTRON RADIATION 2019; 26:1432-1447. [PMID: 31490131 PMCID: PMC6730617 DOI: 10.1107/s1600577519006647] [Citation(s) in RCA: 6] [Impact Index Per Article: 1.2] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/16/2018] [Accepted: 05/08/2019] [Indexed: 05/15/2023]
Abstract
The European X-ray Free-Electron Laser (EuXFEL) delivers extremely intense (>1012 photons pulse-1 and up to 27000 pulses s-1), ultrashort (<100 fs) and transversely coherent X-ray radiation, at a repetition rate of up to 4.5 MHz. Its unique X-ray beam parameters enable novel and groundbreaking experiments in ultrafast photochemistry and material sciences at the Femtosecond X-ray Experiments (FXE) scientific instrument. This paper provides an overview of the currently implemented experimental baseline instrumentation and its performance during the commissioning phase, and a preview of planned improvements. FXE's versatile instrumentation combines the simultaneous application of forward X-ray scattering and X-ray spectroscopy techniques with femtosecond time resolution. These methods will eventually permit exploitation of wide-angle X-ray scattering studies and X-ray emission spectroscopy, along with X-ray absorption spectroscopy, including resonant inelastic X-ray scattering and X-ray Raman scattering. A suite of ultrafast optical lasers throughout the UV-visible and near-IR ranges (extending up to mid-IR in the near future) with pulse length down to 15 fs, synchronized to the X-ray source, serve to initiate dynamic changes in the sample. Time-delayed hard X-ray pulses in the 5-20 keV range are used to probe the ensuing dynamic processes using the suite of X-ray probe tools. FXE is equipped with a primary monochromator, a primary and secondary single-shot spectrometer, and a timing tool to correct the residual timing jitter between laser and X-ray pulses.
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Affiliation(s)
- Andreas Galler
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Wojciech Gawelda
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
- Faculty of Physics, Adam Mickiewicz University, Umultowska 85, 61-614 Poznań, Poland
| | - Mykola Biednov
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Christina Bomer
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
- The Hamburg Centre for Ultrafast Imaging, Universität Hamburg, 22607 Hamburg, Germany
| | - Alexander Britz
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Sandor Brockhauser
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
- Biological Research Centre (BRC), Hungarian Academy of Sciences, Temesvári krt 62, H-6726 Szeged, Hungary
| | - Tae-Kyu Choi
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Michael Diez
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
- The Hamburg Centre for Ultrafast Imaging, Universität Hamburg, 22607 Hamburg, Germany
| | - Paul Frankenberger
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Marcus French
- STFC Technology, Rutherford Appleton Laboratory, Didcot, Oxfordshire OX11 0QX, UK
| | - Dennis Görries
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Matthiew Hart
- STFC Technology, Rutherford Appleton Laboratory, Didcot, Oxfordshire OX11 0QX, UK
| | - Steffen Hauf
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Dmitry Khakhulin
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Martin Knoll
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Timo Korsch
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Katharina Kubicek
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Markus Kuster
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Philipp Lang
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Frederico Alves Lima
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Florian Otte
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
- The Hamburg Centre for Ultrafast Imaging, Universität Hamburg, 22607 Hamburg, Germany
- Fakultät Physik, Technische Universität Dortmund, 44227 Dortmund, Germany
| | - Sebastian Schulz
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Peter Zalden
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Christian Bressler
- Femtosecond X-ray Experiments Group, European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
- The Hamburg Centre for Ultrafast Imaging, Universität Hamburg, 22607 Hamburg, Germany
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10
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Mancuso AP, Aquila A, Batchelor L, Bean RJ, Bielecki J, Borchers G, Doerner K, Giewekemeyer K, Graceffa R, Kelsey OD, Kim Y, Kirkwood HJ, Legrand A, Letrun R, Manning B, Lopez Morillo L, Messerschmidt M, Mills G, Raabe S, Reimers N, Round A, Sato T, Schulz J, Signe Takem C, Sikorski M, Stern S, Thute P, Vagovič P, Weinhausen B, Tschentscher T. The Single Particles, Clusters and Biomolecules and Serial Femtosecond Crystallography instrument of the European XFEL: initial installation. JOURNAL OF SYNCHROTRON RADIATION 2019; 26:660-676. [PMID: 31074429 PMCID: PMC6510195 DOI: 10.1107/s1600577519003308] [Citation(s) in RCA: 50] [Impact Index Per Article: 10.0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/04/2018] [Accepted: 03/07/2019] [Indexed: 05/22/2023]
Abstract
The European X-ray Free-Electron Laser (FEL) became the first operational high-repetition-rate hard X-ray FEL with first lasing in May 2017. Biological structure determination has already benefitted from the unique properties and capabilities of X-ray FELs, predominantly through the development and application of serial crystallography. The possibility of now performing such experiments at data rates more than an order of magnitude greater than previous X-ray FELs enables not only a higher rate of discovery but also new classes of experiments previously not feasible at lower data rates. One example is time-resolved experiments requiring a higher number of time steps for interpretation, or structure determination from samples with low hit rates in conventional X-ray FEL serial crystallography. Following first lasing at the European XFEL, initial commissioning and operation occurred at two scientific instruments, one of which is the Single Particles, Clusters and Biomolecules and Serial Femtosecond Crystallography (SPB/SFX) instrument. This instrument provides a photon energy range, focal spot sizes and diagnostic tools necessary for structure determination of biological specimens. The instrumentation explicitly addresses serial crystallography and the developing single particle imaging method as well as other forward-scattering and diffraction techniques. This paper describes the major science cases of SPB/SFX and its initial instrumentation - in particular its optical systems, available sample delivery methods, 2D detectors, supporting optical laser systems and key diagnostic components. The present capabilities of the instrument will be reviewed and a brief outlook of its future capabilities is also described.
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Affiliation(s)
- Adrian P. Mancuso
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
- Department of Chemistry and Physics, La Trobe Institute for Molecular Science, La Trobe University, Melbourne, Victoria 3086, Australia
| | - Andrew Aquila
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | | | | | | | | | | | | | - Rita Graceffa
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | | | - Yoonhee Kim
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | | | | | - Romain Letrun
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | | | | | | | - Grant Mills
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Steffen Raabe
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
- Center for Free Electron Laser Science, Deutsches Elektronen-Synchrotron, Notkestraße 85, 22607 Hamburg, Germany
| | - Nadja Reimers
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Adam Round
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Tokushi Sato
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
- Center for Free Electron Laser Science, Deutsches Elektronen-Synchrotron, Notkestraße 85, 22607 Hamburg, Germany
| | | | | | | | - Stephan Stern
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Prasad Thute
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Patrik Vagovič
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
- Center for Free Electron Laser Science, Deutsches Elektronen-Synchrotron, Notkestraße 85, 22607 Hamburg, Germany
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