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3D-printed sheet jet for stable megahertz liquid sample delivery at X-ray free-electron lasers.
Konold, Patrick E; You, Tong; Bielecki, Johan; Valerio, Joana; Kloos, Marco; Westphal, Daniel; Bellisario, Alfredo; Varma Yenupuri, Tej; Wollter, August; Koliyadu, Jayanath C P; Koua, Faisal H M; Letrun, Romain; Round, Adam; Sato, Tokushi; Mészáros, Petra; Monrroy, Leonardo; Mutisya, Jennifer; Bódizs, Szabolcs; Larkiala, Taru; Nimmrich, Amke; Alvarez, Roberto; Adams, Patrick; Bean, Richard; Ekeberg, Tomas; Kirian, Richard A; Martin, Andrew V; Westenhoff, Sebastian; Maia, Filipe R N C.
Affiliation
  • Konold PE; Laboratory of Molecular Biophysics, Institute for Cell and Molecular Biology, Uppsala University, Box 596, 75124 Uppsala, Sweden.
  • You T; Laboratory of Molecular Biophysics, Institute for Cell and Molecular Biology, Uppsala University, Box 596, 75124 Uppsala, Sweden.
  • Bielecki J; European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany.
  • Valerio J; European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany.
  • Kloos M; European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany.
  • Westphal D; Laboratory of Molecular Biophysics, Institute for Cell and Molecular Biology, Uppsala University, Box 596, 75124 Uppsala, Sweden.
  • Bellisario A; Laboratory of Molecular Biophysics, Institute for Cell and Molecular Biology, Uppsala University, Box 596, 75124 Uppsala, Sweden.
  • Varma Yenupuri T; Laboratory of Molecular Biophysics, Institute for Cell and Molecular Biology, Uppsala University, Box 596, 75124 Uppsala, Sweden.
  • Wollter A; Laboratory of Molecular Biophysics, Institute for Cell and Molecular Biology, Uppsala University, Box 596, 75124 Uppsala, Sweden.
  • Koliyadu JCP; European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany.
  • Koua FHM; European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany.
  • Letrun R; European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany.
  • Round A; European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany.
  • Sato T; European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany.
  • Mészáros P; Department of Chemistry - BMC, Uppsala University, Box 576, 75123 Uppsala, Sweden.
  • Monrroy L; Department of Chemistry - BMC, Uppsala University, Box 576, 75123 Uppsala, Sweden.
  • Mutisya J; Department of Chemistry - BMC, Uppsala University, Box 576, 75123 Uppsala, Sweden.
  • Bódizs S; Department of Chemistry and Molecular Biology, University of Gothenburg, Gothenburg, Sweden.
  • Larkiala T; Department of Chemistry and Molecular Biology, University of Gothenburg, Gothenburg, Sweden.
  • Nimmrich A; Department of Chemistry and Molecular Biology, University of Gothenburg, Gothenburg, Sweden.
  • Alvarez R; Department of Physics, Arizona State University, 550 E. Tyler Drive, Tempe, AZ 85287, USA.
  • Adams P; School of Science, STEM College, RMIT University, Melbourne, Victoria 3000, Australia.
  • Bean R; European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany.
  • Ekeberg T; Laboratory of Molecular Biophysics, Institute for Cell and Molecular Biology, Uppsala University, Box 596, 75124 Uppsala, Sweden.
  • Kirian RA; Department of Physics, Arizona State University, 550 E. Tyler Drive, Tempe, AZ 85287, USA.
  • Martin AV; School of Science, STEM College, RMIT University, Melbourne, Victoria 3000, Australia.
  • Westenhoff S; Department of Chemistry - BMC, Uppsala University, Box 576, 75123 Uppsala, Sweden.
  • Maia FRNC; Laboratory of Molecular Biophysics, Institute for Cell and Molecular Biology, Uppsala University, Box 596, 75124 Uppsala, Sweden.
IUCrJ ; 10(Pt 6): 662-670, 2023 Nov 01.
Article de En | MEDLINE | ID: mdl-37721770
ABSTRACT
X-ray free-electron lasers (XFELs) can probe chemical and biological reactions as they unfold with unprecedented spatial and temporal resolution. A principal challenge in this pursuit involves the delivery of samples to the X-ray interaction point in such a way that produces data of the highest possible quality and with maximal efficiency. This is hampered by intrinsic constraints posed by the light source and operation within a beamline environment. For liquid samples, the solution typically involves some form of high-speed liquid jet, capable of keeping up with the rate of X-ray pulses. However, conventional jets are not ideal because of radiation-induced explosions of the jet, as well as their cylindrical geometry combined with the X-ray pointing instability of many beamlines which causes the interaction volume to differ for every pulse. This complicates data analysis and contributes to measurement errors. An alternative geometry is a liquid sheet jet which, with its constant thickness over large areas, eliminates the problems related to X-ray pointing. Since liquid sheets can be made very thin, the radiation-induced explosion is reduced, boosting their stability. These are especially attractive for experiments which benefit from small interaction volumes such as fluctuation X-ray scattering and several types of spectroscopy. Although their use has increased for soft X-ray applications in recent years, there has not yet been wide-scale adoption at XFELs. Here, gas-accelerated liquid sheet jet sample injection is demonstrated at the European XFEL SPB/SFX nano focus beamline. Its performance relative to a conventional liquid jet is evaluated and superior performance across several key factors has been found. This includes a thickness profile ranging from hundreds of nanometres to 60 nm, a fourfold increase in background stability and favorable radiation-induced explosion dynamics at high repetition rates up to 1.13 MHz. Its minute thickness also suggests that ultrafast single-particle solution scattering is a possibility.
Mots clés

Texte intégral: 1 Collection: 01-internacional Base de données: MEDLINE Langue: En Journal: IUCrJ Année: 2023 Type de document: Article Pays d'affiliation: Suède

Texte intégral: 1 Collection: 01-internacional Base de données: MEDLINE Langue: En Journal: IUCrJ Année: 2023 Type de document: Article Pays d'affiliation: Suède
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