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Hierarchically guided in situ nanolaminography for the visualisation of damage nucleation in alloy sheets. Sci Rep 2023; 13:1055. [PMID: 36658141 PMCID: PMC9852562 DOI: 10.1038/s41598-022-27035-8] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 09/30/2022] [Accepted: 12/23/2022] [Indexed: 01/20/2023] Open
Abstract
Hierarchical guidance is developed for three-dimensional (3D) nanoscale X-ray imaging, enabling identification, refinement, and tracking of regions of interest (ROIs) within specimens considerably exceeding the field of view. This opens up new possibilities for in situ investigations. Experimentally, the approach takes advantage of rapid multiscale measurements based on magnified projection microscopy featuring continuous zoom capabilities. Immediate and continuous feedback on the subsequent experimental progress is enabled by suitable on-the-fly data processing. For this, by theoretical justification and experimental validation, so-called quasi-particle phase-retrieval is generalised to conical-beam conditions, being key for sufficiently fast computation without significant loss of imaging quality and resolution compared to common approaches for holographic microscopy. Exploiting 3D laminography, particularly suited for imaging of ROIs in laterally extended plate-like samples, the potential of hierarchical guidance is demonstrated by the in situ investigation of damage nucleation inside alloy sheets under engineering-relevant boundary conditions, providing novel insight into the nanoscale morphological development of void and particle clusters under mechanical load. Combined with digital volume correlation, we study deformation kinematics with unprecedented spatial resolution. Correlation of mesoscale (i.e. strain fields) and nanoscale (i.e. particle cracking) evolution opens new routes for the understanding of damage nucleation within sheet materials with application-relevant dimensions.
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Hagemann J, Vassholz M, Hoeppe H, Osterhoff M, Rosselló JM, Mettin R, Seiboth F, Schropp A, Möller J, Hallmann J, Kim C, Scholz M, Boesenberg U, Schaffer R, Zozulya A, Lu W, Shayduk R, Madsen A, Schroer CG, Salditt T. Single-pulse phase-contrast imaging at free-electron lasers in the hard X-ray regime. JOURNAL OF SYNCHROTRON RADIATION 2021; 28:52-63. [PMID: 33399552 PMCID: PMC7842230 DOI: 10.1107/s160057752001557x] [Citation(s) in RCA: 22] [Impact Index Per Article: 5.5] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/04/2020] [Accepted: 11/24/2020] [Indexed: 05/31/2023]
Abstract
X-ray free-electron lasers (XFELs) have opened up unprecedented opportunities for time-resolved nano-scale imaging with X-rays. Near-field propagation-based imaging, and in particular near-field holography (NFH) in its high-resolution implementation in cone-beam geometry, can offer full-field views of a specimen's dynamics captured by single XFEL pulses. To exploit this capability, for example in optical-pump/X-ray-probe imaging schemes, the stochastic nature of the self-amplified spontaneous emission pulses, i.e. the dynamics of the beam itself, presents a major challenge. In this work, a concept is presented to address the fluctuating illumination wavefronts by sampling the configuration space of SASE pulses before an actual recording, followed by a principal component analysis. This scheme is implemented at the MID (Materials Imaging and Dynamics) instrument of the European XFEL and time-resolved NFH is performed using aberration-corrected nano-focusing compound refractive lenses. Specifically, the dynamics of a micro-fluidic water-jet, which is commonly used as sample delivery system at XFELs, is imaged. The jet exhibits rich dynamics of droplet formation in the break-up regime. Moreover, pump-probe imaging is demonstrated using an infrared pulsed laser to induce cavitation and explosion of the jet.
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Affiliation(s)
- Johannes Hagemann
- Deutsches Elektronen Synchrotron – DESY, Notkestraße 85, 22607 Hamburg, Germany
| | - Malte Vassholz
- Institute for X-ray Physics, University of Göttingen, Friedrich-Hund-Platz 1, 37077 Göttingen, Germany
| | - Hannes Hoeppe
- Institute for X-ray Physics, University of Göttingen, Friedrich-Hund-Platz 1, 37077 Göttingen, Germany
| | - Markus Osterhoff
- Institute for X-ray Physics, University of Göttingen, Friedrich-Hund-Platz 1, 37077 Göttingen, Germany
| | - Juan M. Rosselló
- Third Institute of Physics, University of Göttingen, Friedrich-Hund-Platz 1, 37077 Göttingen, Germany
| | - Robert Mettin
- Third Institute of Physics, University of Göttingen, Friedrich-Hund-Platz 1, 37077 Göttingen, Germany
| | - Frank Seiboth
- Deutsches Elektronen Synchrotron – DESY, Notkestraße 85, 22607 Hamburg, Germany
| | - Andreas Schropp
- Deutsches Elektronen Synchrotron – DESY, Notkestraße 85, 22607 Hamburg, Germany
| | - Johannes Möller
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Jörg Hallmann
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Chan Kim
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Markus Scholz
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Ulrike Boesenberg
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Robert Schaffer
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Alexey Zozulya
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Wei Lu
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Roman Shayduk
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Anders Madsen
- European X-ray Free-Electron Laser Facility, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Christian G. Schroer
- Deutsches Elektronen Synchrotron – DESY, Notkestraße 85, 22607 Hamburg, Germany
- Department Physik, Universität Hamburg, Luruper Chaussee 149, 22761 Hamburg, Germany
| | - Tim Salditt
- Institute for X-ray Physics, University of Göttingen, Friedrich-Hund-Platz 1, 37077 Göttingen, Germany
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Seifert M, Weule M, Cipiccia S, Flenner S, Hagemann J, Ludwig V, Michel T, Neumayer P, Schuster M, Wolf A, Anton G, Funk S, Akstaller B. Evaluation of the Weighted Mean X-ray Energy for an Imaging System Via Propagation-Based Phase-Contrast Imaging. J Imaging 2020; 6:63. [PMID: 34460656 PMCID: PMC8321046 DOI: 10.3390/jimaging6070063] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.6] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 05/13/2020] [Revised: 06/13/2020] [Accepted: 07/01/2020] [Indexed: 11/17/2022] Open
Abstract
For imaging events of extremely short duration, like shock waves or explosions, it is necessary to be able to image the object with a single-shot exposure. A suitable setup is given by a laser-induced X-ray source such as the one that can be found at GSI (Helmholtzzentrum für Schwerionenforschung GmbH) in Darmstadt (Society for Heavy Ion Research), Germany. There, it is possible to direct a pulse from the high-energy laser Petawatt High Energy Laser for Heavy Ion eXperiments (PHELIX) on a tungsten wire to generate a picosecond polychromatic X-ray pulse, called backlighter. For grating-based single-shot phase-contrast imaging of shock waves or exploding wires, it is important to know the weighted mean energy of the X-ray spectrum for choosing a suitable setup. In propagation-based phase-contrast imaging the knowledge of the weighted mean energy is necessary to be able to reconstruct quantitative phase images of unknown objects. Hence, we developed a method to evaluate the weighted mean energy of the X-ray backlighter spectrum using propagation-based phase-contrast images. In a first step wave-field simulations are performed to verify the results. Furthermore, our evaluation is cross-checked with monochromatic synchrotron measurements with known energy at Diamond Light Source (DLS, Didcot, UK) for proof of concepts.
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Affiliation(s)
- Maria Seifert
- ECAP, Friedrich-Alexander-Universität Erlangen-Nürnberg, Erwin-Rommel-Str. 1, 91058 Erlangen, Germany; (M.S.); (M.W.); (V.L.); (T.M.); (M.S.); (A.W.); (G.A.); (S.F.)
| | - Mareike Weule
- ECAP, Friedrich-Alexander-Universität Erlangen-Nürnberg, Erwin-Rommel-Str. 1, 91058 Erlangen, Germany; (M.S.); (M.W.); (V.L.); (T.M.); (M.S.); (A.W.); (G.A.); (S.F.)
| | - Silvia Cipiccia
- Diamond Light Source Ltd., Diamond House, Harwell Science and Innovation Campus, Didcot, Oxfordshire OX11 0DE, UK;
| | - Silja Flenner
- Helmholtz-Zentrum Geesthacht, Max-Planck-Straße 1, 21502 Geesthacht, Germany;
| | | | - Veronika Ludwig
- ECAP, Friedrich-Alexander-Universität Erlangen-Nürnberg, Erwin-Rommel-Str. 1, 91058 Erlangen, Germany; (M.S.); (M.W.); (V.L.); (T.M.); (M.S.); (A.W.); (G.A.); (S.F.)
| | - Thilo Michel
- ECAP, Friedrich-Alexander-Universität Erlangen-Nürnberg, Erwin-Rommel-Str. 1, 91058 Erlangen, Germany; (M.S.); (M.W.); (V.L.); (T.M.); (M.S.); (A.W.); (G.A.); (S.F.)
| | - Paul Neumayer
- GSI Helmholtzzentrum für Schwerionenforschung GmbH, Planckstr. 1, 64291 Darmstadt, Germany;
| | - Max Schuster
- ECAP, Friedrich-Alexander-Universität Erlangen-Nürnberg, Erwin-Rommel-Str. 1, 91058 Erlangen, Germany; (M.S.); (M.W.); (V.L.); (T.M.); (M.S.); (A.W.); (G.A.); (S.F.)
| | - Andreas Wolf
- ECAP, Friedrich-Alexander-Universität Erlangen-Nürnberg, Erwin-Rommel-Str. 1, 91058 Erlangen, Germany; (M.S.); (M.W.); (V.L.); (T.M.); (M.S.); (A.W.); (G.A.); (S.F.)
| | - Gisela Anton
- ECAP, Friedrich-Alexander-Universität Erlangen-Nürnberg, Erwin-Rommel-Str. 1, 91058 Erlangen, Germany; (M.S.); (M.W.); (V.L.); (T.M.); (M.S.); (A.W.); (G.A.); (S.F.)
| | - Stefan Funk
- ECAP, Friedrich-Alexander-Universität Erlangen-Nürnberg, Erwin-Rommel-Str. 1, 91058 Erlangen, Germany; (M.S.); (M.W.); (V.L.); (T.M.); (M.S.); (A.W.); (G.A.); (S.F.)
| | - Bernhard Akstaller
- ECAP, Friedrich-Alexander-Universität Erlangen-Nürnberg, Erwin-Rommel-Str. 1, 91058 Erlangen, Germany; (M.S.); (M.W.); (V.L.); (T.M.); (M.S.); (A.W.); (G.A.); (S.F.)
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Robisch AL, Eckermann M, Töpperwien M, van der Meer F, Stadelmann C, Salditt T. Nanoscale x-ray holotomography of human brain tissue with phase retrieval based on multienergy recordings. J Med Imaging (Bellingham) 2020; 7:013501. [PMID: 32016134 PMCID: PMC6975131 DOI: 10.1117/1.jmi.7.1.013501] [Citation(s) in RCA: 5] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 08/05/2019] [Accepted: 12/24/2019] [Indexed: 11/14/2022] Open
Abstract
X-ray cone-beam holotomography of unstained tissue from the human central nervous system reveals details down to subcellular length scales. This visualization of variations in the electron density of the sample is based on phase-contrast techniques using intensities formed by self-interference of the beam between object and detector. Phase retrieval inverts diffraction and overcomes the phase problem by constraints such as several measurements at different Fresnel numbers for a single projection. Therefore, the object-to-detector distance (defocus) can be varied. However, for cone-beam geometry, changing defocus changes magnification, which can be problematic in view of image processing and resolution. Alternatively, the photon energy can be altered (multi-E). Far from absorption edges, multi-E data yield the wavelength-independent electron density. We present the multi-E holotomography at the Göttingen Instrument for Nano-Imaging with X-Rays (GINIX) setup of the P10 beamline at Deutsches Elektronen-Synchrotron. The instrument is based on a combined optics of elliptical mirrors and an x-ray waveguide positioned in the focal plane for further coherence, spatial filtering, and high numerical aperture. Previous results showed the suitability of this instrument for nanoscale tomography of unstained brain tissue. We demonstrate that upon energy variation, the focal spot is stable enough for imaging. To this end, a double-crystal monochromator and automated alignment routines are required. Three tomograms of human brain tissue were recorded and jointly analyzed using phase retrieval based on the contrast transfer function formalism generalized to multiple photon energies. Variations of the electron density of the sample are successfully reconstructed.
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Affiliation(s)
- Anna-Lena Robisch
- Georg-August-Universität Göttingen, Institut für Röntgenphysik, Göttingen, Germany
| | - Marina Eckermann
- Georg-August-Universität Göttingen, Institut für Röntgenphysik, Göttingen, Germany.,University of Göttingen, Cluster of Excellence "Multiscale Bioimaging: from Molecular Machines to Networks of Excitable Cells," Göttingen, Germany
| | - Mareike Töpperwien
- Georg-August-Universität Göttingen, Institut für Röntgenphysik, Göttingen, Germany
| | - Franziska van der Meer
- Universitätsmedizin Göttingen, Institut für Neuropathologie, Klinik für Neurologie, Göttingen, Germany
| | - Christine Stadelmann
- Universitätsmedizin Göttingen, Institut für Neuropathologie, Klinik für Neurologie, Göttingen, Germany
| | - Tim Salditt
- Georg-August-Universität Göttingen, Institut für Röntgenphysik, Göttingen, Germany.,University of Göttingen, Cluster of Excellence "Multiscale Bioimaging: from Molecular Machines to Networks of Excitable Cells," Göttingen, Germany
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