51
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Kurta RP, Wiegart L, Fluerasu A, Madsen A. Fluctuation X-ray scattering from nanorods in solution reveals weak temperature-dependent orientational ordering. IUCRJ 2019; 6:635-648. [PMID: 31316808 PMCID: PMC6608627 DOI: 10.1107/s2052252519005499] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 12/20/2018] [Accepted: 04/23/2019] [Indexed: 06/10/2023]
Abstract
Higher-order statistical analysis of X-ray scattering from dilute solutions of polydisperse goethite nanorods was performed and revealed structural information which is inaccessible by conventional small-angle scattering. For instance, a pronounced temperature dependence of the correlated scattering from suspension was observed. The higher-order scattering terms deviate from those expected for a perfectly isotropic distribution of particle orientations, demonstrating that the method can reveal faint orientational order in apparently disordered systems. The observation of correlated scattering from polydisperse particle solutions is also encouraging for future free-electron laser experiments aimed at extracting high-resolution structural information from systems with low particle heterogeneity.
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Affiliation(s)
| | - Lutz Wiegart
- Brookhaven National Laboratory, Photon Sciences Directorate, Upton, NY 11973, USA
| | - Andrei Fluerasu
- Brookhaven National Laboratory, Photon Sciences Directorate, Upton, NY 11973, USA
| | - Anders Madsen
- European XFEL, Holzkoppel 4, 22869 Schenefeld, Germany
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52
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Abstract
X-ray free-electron lasers provide femtosecond-duration pulses of hard X-rays with a peak brightness approximately one billion times greater than is available at synchrotron radiation facilities. One motivation for the development of such X-ray sources was the proposal to obtain structures of macromolecules, macromolecular complexes, and virus particles, without the need for crystallization, through diffraction measurements of single noncrystalline objects. Initial explorations of this idea and of outrunning radiation damage with femtosecond pulses led to the development of serial crystallography and the ability to obtain high-resolution structures of small crystals without the need for cryogenic cooling. This technique allows the understanding of conformational dynamics and enzymatics and the resolution of intermediate states in reactions over timescales of 100 fs to minutes. The promise of more photons per atom recorded in a diffraction pattern than electrons per atom contributing to an electron micrograph may enable diffraction measurements of single molecules, although challenges remain.
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Affiliation(s)
- Henry N. Chapman
- Center for Free-Electron Laser Science, DESY, 22607 Hamburg, Germany
- Department of Physics, University of Hamburg, 22761 Hamburg, Germany
- Centre for Ultrafast Imaging, University of Hamburg, 22761 Hamburg, Germany
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53
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Bielecki J, Hantke MF, Daurer BJ, Reddy HKN, Hasse D, Larsson DSD, Gunn LH, Svenda M, Munke A, Sellberg JA, Flueckiger L, Pietrini A, Nettelblad C, Lundholm I, Carlsson G, Okamoto K, Timneanu N, Westphal D, Kulyk O, Higashiura A, van der Schot G, Loh NTD, Wysong TE, Bostedt C, Gorkhover T, Iwan B, Seibert MM, Osipov T, Walter P, Hart P, Bucher M, Ulmer A, Ray D, Carini G, Ferguson KR, Andersson I, Andreasson J, Hajdu J, Maia FRNC. Electrospray sample injection for single-particle imaging with x-ray lasers. SCIENCE ADVANCES 2019; 5:eaav8801. [PMID: 31058226 PMCID: PMC6499549 DOI: 10.1126/sciadv.aav8801] [Citation(s) in RCA: 34] [Impact Index Per Article: 5.7] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/30/2018] [Accepted: 03/19/2019] [Indexed: 05/11/2023]
Abstract
The possibility of imaging single proteins constitutes an exciting challenge for x-ray lasers. Despite encouraging results on large particles, imaging small particles has proven to be difficult for two reasons: not quite high enough pulse intensity from currently available x-ray lasers and, as we demonstrate here, contamination of the aerosolized molecules by nonvolatile contaminants in the solution. The amount of contamination on the sample depends on the initial droplet size during aerosolization. Here, we show that, with our electrospray injector, we can decrease the size of aerosol droplets and demonstrate virtually contaminant-free sample delivery of organelles, small virions, and proteins. The results presented here, together with the increased performance of next-generation x-ray lasers, constitute an important stepping stone toward the ultimate goal of protein structure determination from imaging at room temperature and high temporal resolution.
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Affiliation(s)
- Johan Bielecki
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
- European XFEL GmbH, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Max F. Hantke
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
- Chemistry Research Laboratory, Department of Chemistry, Oxford University, 12 Mansfield Rd, Oxford OX1 3TA, UK
| | - Benedikt J. Daurer
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
- Centre for BioImaging Sciences, Department of Biological Sciences, National University of Singapore, 14 Science Drive 4, Singapore 117557, Singapore
| | - Hemanth K. N. Reddy
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
| | - Dirk Hasse
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
| | - Daniel S. D. Larsson
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
| | - Laura H. Gunn
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
| | - Martin Svenda
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
- Biomedical and X-ray Physics, Department of Applied Physics, AlbaNova University Center, KTH Royal Institute of Technology, SE-10691 Stockholm, Sweden
| | - Anna Munke
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
| | - Jonas A. Sellberg
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
- Biomedical and X-ray Physics, Department of Applied Physics, AlbaNova University Center, KTH Royal Institute of Technology, SE-10691 Stockholm, Sweden
| | - Leonie Flueckiger
- ARC Centre of Advanced Molecular Imaging, Department of Chemistry and Physics, La Trobe University, Melbourne, Victoria 3086, Australia
| | - Alberto Pietrini
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
| | - Carl Nettelblad
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
- Division of Scientific Computing, Department of Information Technology, Science for Life Laboratory, Uppsala University, Lägerhyddsvägen 2 (Box 337), SE-751 05 Uppsala, Sweden
| | - Ida Lundholm
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
| | - Gunilla Carlsson
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
| | - Kenta Okamoto
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
| | - Nicusor Timneanu
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
- Department of Physics and Astronomy, Uppsala University, Box 516, SE-75120 Uppsala, Sweden
| | - Daniel Westphal
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
| | - Olena Kulyk
- Institute of Physics, ELI Beamlines, Academy of Sciences of the Czech Republic, Na Slovance 2, CZ-18221 Prague, Czech Republic
| | - Akifumi Higashiura
- Institute for Protein Research, Osaka University, Suita, Osaka 565-0871, Japan
- Department of Virology, Graduate School of Biomedical and Health Sciences, Hiroshima University, Hiroshima 734-8551, Japan
| | - Gijs van der Schot
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
- Cryo-Electron Microscopy, Bijvoet Center for Biomolecular Research, Utrecht University, 3584 CH Utrecht, Netherlands
| | - Ne-Te Duane Loh
- Centre for BioImaging Sciences, Department of Biological Sciences, National University of Singapore, 14 Science Drive 4, Singapore 117557, Singapore
- Department of Physics, National University of Singapore, Singapore, Singapore
| | - Taylor E. Wysong
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA
| | - Christoph Bostedt
- Chemical Sciences and Engineering Division, Argonne National Laboratory, Argonne, IL 60439, USA
- Department of Physics and Astronomy, Northwestern University, Evanston, IL 60208, USA
| | - Tais Gorkhover
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA
| | - Bianca Iwan
- Stanford PULSE Institute, SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA
- Institut für Quantenoptik, Leibniz Universität Hannover, Welfengarten 1, 30167 Hannover, Germany
| | - M. Marvin Seibert
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
| | - Timur Osipov
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA
| | - Peter Walter
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA
| | - Philip Hart
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA
| | - Maximilian Bucher
- Chemical Sciences and Engineering Division, Argonne National Laboratory, Argonne, IL 60439, USA
| | - Anatoli Ulmer
- Institut für Optik und Atomare Physik, Technische Universität Berlin, 10623 Berlin, Germany
| | - Dipanwita Ray
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA
| | - Gabriella Carini
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA
| | - Ken R. Ferguson
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA
| | - Inger Andersson
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
| | - Jakob Andreasson
- Institute of Physics, ELI Beamlines, Academy of Sciences of the Czech Republic, Na Slovance 2, CZ-18221 Prague, Czech Republic
- Condensed Matter Physics, Department of Physics, Chalmers University of Technology, Gothenburg, Sweden
| | - Janos Hajdu
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
- Institute of Physics, ELI Beamlines, Academy of Sciences of the Czech Republic, Na Slovance 2, CZ-18221 Prague, Czech Republic
| | - Filipe R. N. C. Maia
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-75124 Uppsala, Sweden
- NERSC, Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA
- Corresponding author.
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54
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Uetrecht C, Lorenzen K, Kitel M, Heidemann J, Robinson Spencer JH, Schlüter H, Schulz J. Native mass spectrometry provides sufficient ion flux for XFEL single-particle imaging. JOURNAL OF SYNCHROTRON RADIATION 2019; 26:653-659. [PMID: 31074428 PMCID: PMC6510201 DOI: 10.1107/s1600577519002686] [Citation(s) in RCA: 5] [Impact Index Per Article: 0.8] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/04/2018] [Accepted: 02/21/2019] [Indexed: 05/11/2023]
Abstract
The SPB/SFX instrument at the European XFEL provides unique conditions for single-particle imaging (SPI) experiments due to its high brilliance, nano-focus and unique pulse structure. Promising initial results provided by the international LCLS (Linac Coherent Light Source) SPI initiative highlight the potential of SPI. Current available injection methods generally have high sample consumption and do not provide any options for pulsing, selection or orientation of particles, which poses a problem for data evaluation. Aerosol-injector-based sample delivery is the current method of choice for SPI experiments, although, to a lesser extent, electrospray and electrospinning are used. Single particles scatter only a limited number of photons providing a single orientation for data evaluation, hence large datasets are required from particles in multiple orientations in order to reconstruct a structure. Here, a feasibility study demonstrates that nano-electrospray ionization, usually employed in biomolecular mass spectrometry, provides enough ion flux for SPI experiments. A novel instrument setup at the SPB/SFX instrument is proposed, which has the benefit of extremely low background while delivering mass over charge and conformation-selected ions for SPI.
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Affiliation(s)
- Charlotte Uetrecht
- Heinrich Pette Institute, Leibniz Institute for Experimental Virology, Martinistrasse 52, Hamburg 20251, Germany
- European XFEL GmbH, Holzkoppel 4, Schenefeld 22869, Germany
| | | | - Matthäus Kitel
- European XFEL GmbH, Holzkoppel 4, Schenefeld 22869, Germany
| | - Johannes Heidemann
- Heinrich Pette Institute, Leibniz Institute for Experimental Virology, Martinistrasse 52, Hamburg 20251, Germany
| | - Jesse Huron Robinson Spencer
- European XFEL GmbH, Holzkoppel 4, Schenefeld 22869, Germany
- Institute for Clinical Chemistry, University Medical Centre Hamburg-Eppendorf, Martinistrasse 52, Hamburg 20246, Germany
| | - Hartmut Schlüter
- Institute for Clinical Chemistry, University Medical Centre Hamburg-Eppendorf, Martinistrasse 52, Hamburg 20246, Germany
| | - Joachim Schulz
- European XFEL GmbH, Holzkoppel 4, Schenefeld 22869, Germany
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55
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Giewekemeyer K, Aquila A, Loh NTD, Chushkin Y, Shanks KS, Weiss J, Tate MW, Philipp HT, Stern S, Vagovic P, Mehrjoo M, Teo C, Barthelmess M, Zontone F, Chang C, Tiberio RC, Sakdinawat A, Williams GJ, Gruner SM, Mancuso AP. Experimental 3D coherent diffractive imaging from photon-sparse random projections. IUCRJ 2019; 6:357-365. [PMID: 31098017 PMCID: PMC6503918 DOI: 10.1107/s2052252519002781] [Citation(s) in RCA: 12] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/09/2018] [Accepted: 02/24/2019] [Indexed: 05/19/2023]
Abstract
The routine atomic resolution structure determination of single particles is expected to have profound implications for probing structure-function relationships in systems ranging from energy-storage materials to biological molecules. Extremely bright ultrashort-pulse X-ray sources - X-ray free-electron lasers (XFELs) - provide X-rays that can be used to probe ensembles of nearly identical nanoscale particles. When combined with coherent diffractive imaging, these objects can be imaged; however, as the resolution of the images approaches the atomic scale, the measured data are increasingly difficult to obtain and, during an X-ray pulse, the number of photons incident on the 2D detector is much smaller than the number of pixels. This latter concern, the signal 'sparsity', materially impedes the application of the method. An experimental analog using a conventional X-ray source is demonstrated and yields signal levels comparable with those expected from single biomolecules illuminated by focused XFEL pulses. The analog experiment provides an invaluable cross check on the fidelity of the reconstructed data that is not available during XFEL experiments. Using these experimental data, it is established that a sparsity of order 1.3 × 10-3 photons per pixel per frame can be overcome, lending vital insight to the solution of the atomic resolution XFEL single-particle imaging problem by experimentally demonstrating 3D coherent diffractive imaging from photon-sparse random projections.
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Affiliation(s)
| | - A. Aquila
- European XFEL GmbH, Holzkoppel 4, 22869 Schenefeld, Germany
| | - N.-T. D. Loh
- Centre for Bio-imaging Sciences, National University of Singapore, 14 Science Drive 4, 117557 Singapore
- Department of Physics, National University of Singapore, 2 Science Drive 3, 117551 Singapore
- Department of Biological Sciences, National University of Singapore, 14 Science Drive 4, 117557 Singapore
| | - Y. Chushkin
- ESRF – The European Synchrotron, 71 avenue des Martyrs, 38000 Grenoble, France
| | - K. S. Shanks
- Laboratory for Atomic and Solid State Physics, Cornell University, Ithaca, NY 14853, USA
| | - J.T. Weiss
- Laboratory for Atomic and Solid State Physics, Cornell University, Ithaca, NY 14853, USA
| | - M. W. Tate
- Laboratory for Atomic and Solid State Physics, Cornell University, Ithaca, NY 14853, USA
| | - H. T. Philipp
- Laboratory for Atomic and Solid State Physics, Cornell University, Ithaca, NY 14853, USA
| | - S. Stern
- European XFEL GmbH, Holzkoppel 4, 22869 Schenefeld, Germany
- Center for Free-Electron Laser Science, Deutsches Elektronen-Synchrotron, 22607 Hamburg, Germany
| | - P. Vagovic
- European XFEL GmbH, Holzkoppel 4, 22869 Schenefeld, Germany
- Center for Free-Electron Laser Science, Deutsches Elektronen-Synchrotron, 22607 Hamburg, Germany
| | - M. Mehrjoo
- European XFEL GmbH, Holzkoppel 4, 22869 Schenefeld, Germany
| | - C. Teo
- Centre for Bio-imaging Sciences, National University of Singapore, 14 Science Drive 4, 117557 Singapore
- Department of Biological Sciences, National University of Singapore, 14 Science Drive 4, 117557 Singapore
| | - M. Barthelmess
- Center for Free-Electron Laser Science, Deutsches Elektronen-Synchrotron, 22607 Hamburg, Germany
| | - F. Zontone
- ESRF – The European Synchrotron, 71 avenue des Martyrs, 38000 Grenoble, France
| | - C. Chang
- SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025, USA
| | - R. C. Tiberio
- Stanford Nano Shared Facilities, Stanford University, 348 Via Pueblo, Stanford, CA 94305, USA
| | - A. Sakdinawat
- SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025, USA
| | - G. J. Williams
- SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025, USA
| | - S. M. Gruner
- Laboratory for Atomic and Solid State Physics, Cornell University, Ithaca, NY 14853, USA
- Cornell High Energy Synchrotron Source (CHESS), Cornell University, Ithaca, NY 14853, USA
- Kavli Institute at Cornell for Nanoscale Science, Cornell University, Ithaca, NY 14853, USA
| | - A. P. Mancuso
- European XFEL GmbH, Holzkoppel 4, 22869 Schenefeld, Germany
- Department of Chemistry and Physics, La Trobe Institute for Molecular Science, La Trobe University, Melbourne, Victoria 3086, Australia
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56
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Kirkwood HJ, Letrun R, Tanikawa T, Liu J, Nakatsutsumi M, Emons M, Jezynski T, Palmer G, Lederer M, Bean R, Buck J, Di Dio Cafisio S, Graceffa R, Grünert J, Göde S, Höppner H, Kim Y, Konopkova Z, Mills G, Makita M, Pelka A, Preston TR, Sikorski M, Takem CMS, Giewekemeyer K, Chollet M, Vagovic P, Chapman HN, Mancuso AP, Sato T. Initial observations of the femtosecond timing jitter at the European XFEL. OPTICS LETTERS 2019; 44:1650-1653. [PMID: 30933113 DOI: 10.1364/ol.44.001650] [Citation(s) in RCA: 6] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/30/2019] [Accepted: 02/14/2019] [Indexed: 06/09/2023]
Abstract
Intense, ultrashort, and high-repetition-rate X-ray pulses, combined with a femtosecond optical laser, allow pump-probe experiments with fast data acquisition and femtosecond time resolution. However, the relative timing of the X-ray pulses and the optical laser pulses can be controlled only to a level of the intrinsic error of the instrument which, without characterization, limits the time resolution of experiments. This limitation inevitably calls for a precise determination of the relative arrival time, which can be used after measurement for sorting and tagging the experimental data to a much finer resolution than it can be controlled to. The observed root-mean-square timing jitter between the X-ray and the optical laser at the SPB/SFX instrument at European XFEL was 308 fs. This first measurement of timing jitter at the European XFEL provides an important step in realizing ultrafast experiments at this novel X-ray source. A method for determining the change in the complex refractive index of samples is also presented.
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57
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Shi Y, Yin K, Tai X, DeMirci H, Hosseinizadeh A, Hogue BG, Li H, Ourmazd A, Schwander P, Vartanyants IA, Yoon CH, Aquila A, Liu H. Evaluation of the performance of classification algorithms for XFEL single-particle imaging data. IUCRJ 2019; 6:331-340. [PMID: 30867930 PMCID: PMC6400180 DOI: 10.1107/s2052252519001854] [Citation(s) in RCA: 11] [Impact Index Per Article: 1.8] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/18/2018] [Accepted: 01/31/2019] [Indexed: 05/22/2023]
Abstract
Using X-ray free-electron lasers (XFELs), it is possible to determine three-dimensional structures of nanoscale particles using single-particle imaging methods. Classification algorithms are needed to sort out the single-particle diffraction patterns from the large amount of XFEL experimental data. However, different methods often yield inconsistent results. This study compared the performance of three classification algorithms: convolutional neural network, graph cut and diffusion map manifold embedding methods. The identified single-particle diffraction data of the PR772 virus particles were assembled in the three-dimensional Fourier space for real-space model reconstruction. The comparison showed that these three classification methods lead to different datasets and subsequently result in different electron density maps of the reconstructed models. Interestingly, the common dataset selected by these three methods improved the quality of the merged diffraction volume, as well as the resolutions of the reconstructed maps.
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Affiliation(s)
- Yingchen Shi
- Department of Engineering Physics, Tsinghua University, 30 Shuangqing Rd, Haidian, Beijing 100084, People’s Republic of China
- Complex Systems Division, Beijing Computational Science Research Centre, 8 E Xibeiwang Rd, Haidian, Beijing 100193, People’s Republic of China
| | - Ke Yin
- Center for Mathematical Sciences, Huazhong University of Science and Technology, Wuhan, Hubei 430074, People’s Republic of China
| | - Xuecheng Tai
- Department of Mathematics, University of Bergen, PO Box 7800, Bergen, 5020, Norway
| | - Hasan DeMirci
- Biosciences Division, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025, USA
- Stanford PULSE Institute, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025, USA
| | - Ahmad Hosseinizadeh
- Department of Physics, University of Wisconsin–Milwaukee, Milwaukee, Wisconsin USA
| | - Brenda G. Hogue
- Biodesign Center for Immunotherapy, Vaccines, and Virotherapy, Biodesign Institute at Arizona State University, Tempe, 85287, USA
| | - Haoyuan Li
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025, USA
- Department of Physics, Stanford University, 450 Serra Mall, Stanford, CA 94305, USA
| | - Abbas Ourmazd
- Department of Physics, University of Wisconsin–Milwaukee, Milwaukee, Wisconsin USA
| | - Peter Schwander
- Department of Physics, University of Wisconsin–Milwaukee, Milwaukee, Wisconsin USA
| | - Ivan A. Vartanyants
- Deutsches Elektronen-Synchrotron DESY, Notkestrasse 85, Hamburg, D-22607, Germany
- National Research Nuclear University MEPhI (Moscow Engineering Physics Institute), Kashirskoe shosse 31, Moscow, 115409, Russian Federation
| | - Chun Hong Yoon
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025, USA
| | - Andrew Aquila
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025, USA
| | - Haiguang Liu
- Complex Systems Division, Beijing Computational Science Research Centre, 8 E Xibeiwang Rd, Haidian, Beijing 100193, People’s Republic of China
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58
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Coherence and pulse duration characterization of the PAL-XFEL in the hard X-ray regime. Sci Rep 2019; 9:3300. [PMID: 30824784 PMCID: PMC6397240 DOI: 10.1038/s41598-019-39765-3] [Citation(s) in RCA: 10] [Impact Index Per Article: 1.7] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 11/19/2018] [Accepted: 01/28/2019] [Indexed: 11/08/2022] Open
Abstract
We characterize the spatial and temporal coherence properties of hard X-ray pulses from the Pohang Accelerator Laboratory X-ray Free Electron Laser (PAL-XFEL, Pohang, Korea). The measurement of the single-shot speckle contrast, together with the introduction of corrections considering experimental conditions, allows obtaining an intrinsic degree of transverse coherence of 0.85 ± 0.06. In the Self-Amplified Spontaneous Emission regime, the analysis of the intensity distribution of X-ray pulses also provides an estimate for the number of longitudinal modes. For monochromatic and pink (i.e. natural bandwidth provided by the first harmonic of the undulator) beams, we observe that the number of temporal modes is 6.0 ± 0.4 and 90.0 ± 7.2, respectively. Assuming a coherence time of 2.06 fs and 0.14 fs for the monochromatic and pink beam respectively, we estimate an average X-ray pulse duration of 12.6 ± 1.0 fs.
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59
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Mancini GF, Pennacchio F, Latychevskaia T, Reguera J, Stellacci F, Carbone F. Local photo-mechanical stiffness revealed in gold nanoparticles supracrystals by ultrafast small-angle electron diffraction. STRUCTURAL DYNAMICS (MELVILLE, N.Y.) 2019; 6:024304. [PMID: 31041361 PMCID: PMC6461555 DOI: 10.1063/1.5091858] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 02/06/2019] [Accepted: 03/27/2019] [Indexed: 05/03/2023]
Abstract
We demonstrate that highly ordered two-dimensional crystals of ligand-capped gold nanoparticles display a local photo-mechanical stiffness as high as that of solids such as graphite. In out-of-equilibrium electron diffraction experiments, a strong temperature jump is induced in a thin film with a femtosecond laser pulse. The initial electronic excitation transfers energy to the underlying structural degrees of freedom, with a rate generally proportional to the stiffness of the material. Using femtosecond small-angle electron diffraction, we observe the temporal evolution of the diffraction feature associated with the nearest-neighbor nanoparticle distance. The Debye-Waller decay for the octanethiol-capped nanoparticle supracrystal, in particular, is found to be unexpectedly fast, almost as fast as the stiffest solid known and observed by the same technique, i.e., graphite. Our observations unravel that local stiffness in a dense supramolecular assembly can be created by van der Waals interactions up to a level comparable to crystalline systems characterized by covalent bonding.
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Affiliation(s)
| | - Francesco Pennacchio
- Laboratory for Ultrafast Microscopy and Electron Scattering, Lausanne Center for Ultrafast Science (LACUS), École Polytechnique Fédérale de Lausanne, CH-1015 Lausanne, Switzerland
| | - Tatiana Latychevskaia
- Physics Institute, University of Zurich, Winterthurerstrasse 190, 8057 Zurich, Switzerland
| | - Javier Reguera
- CIC biomaGUNE, Paseo de Miramón 182C, 20014 Donostia-San Sebastian, Spain and Ikerbasque, Basque Foundation for Science, 48011 Bilbao, Spain
| | - Francesco Stellacci
- Supramolecular Nanomaterials and Interfaces Laboratory, Institute of Materials, École Polytechnique Fédérale de Lausanne, CH-1015 Lausanne, Switzerland
| | - Fabrizio Carbone
- Laboratory for Ultrafast Microscopy and Electron Scattering, Lausanne Center for Ultrafast Science (LACUS), École Polytechnique Fédérale de Lausanne, CH-1015 Lausanne, Switzerland
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60
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Liu J, van der Schot G, Engblom S. Supervised classification methods for flash X-ray single particle diffraction imaging. OPTICS EXPRESS 2019; 27:3884-3899. [PMID: 30876013 DOI: 10.1364/oe.27.003884] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/29/2018] [Accepted: 12/19/2018] [Indexed: 06/09/2023]
Abstract
Current Flash X-ray single-particle diffraction Imaging (FXI) experiments, which operate on modern X-ray Free Electron Lasers (XFELs), can record millions of interpretable diffraction patterns from individual biomolecules per day. Due to the practical limitations with the FXI technology, those patterns will to a varying degree include scatterings from contaminated samples. Also, the heterogeneity of the sample biomolecules is unavoidable and complicates data processing. Reducing the data volumes and selecting high-quality single-molecule patterns are therefore critical steps in the experimental setup. In this paper, we present two supervised template-based learning methods for classifying FXI patterns. Our Eigen-Image and Log-Likelihood classifier can find the best-matched template for a single-molecule pattern within a few milliseconds. It is also straightforward to parallelize them so as to match the XFEL repetition rate fully, thereby enabling processing at site. The methods perform in a stable way on various kinds of synthetic data. As a practical example we tested our methods on a real mimivirus dataset, obtaining a convincing classification accuracy of 0.9.
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61
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Three-dimensional optical trapping and orientation of microparticles for coherent X-ray diffraction imaging. Proc Natl Acad Sci U S A 2019; 116:4018-4024. [PMID: 30765527 DOI: 10.1073/pnas.1720785116] [Citation(s) in RCA: 11] [Impact Index Per Article: 1.8] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/12/2023] Open
Abstract
Optical trapping has been implemented in many areas of physics and biology as a noncontact sample manipulation technique to study the structure and dynamics of nano- and mesoscale objects. It provides a unique approach for manipulating microscopic objects without inducing undesired changes in structure. Combining optical trapping with hard X-ray microscopy techniques, such as coherent diffraction imaging and crystallography, provides a nonperturbing environment where electronic and structural dynamics of an individual particle in solution can be followed in situ. It was previously shown that optical trapping allows the manipulation of micrometer-sized objects for X-ray fluorescence imaging. However, questions remain over the ability of optical trapping to position objects for X-ray diffraction measurements, which have stringent requirements for angular stability. Our work demonstrates that dynamic holographic optical tweezers are capable of manipulating single micrometer-scale anisotropic particles in a microfluidic environment with the precision and stability required for X-ray Bragg diffraction experiments-thus functioning as an "optical goniometer." The methodology can be extended to a variety of X-ray experiments and the Bragg coherent diffractive imaging of individual particles in solution, as demonstrated here, will be markedly enhanced with the advent of brighter, coherent X-ray sources.
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63
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Rose M, Bobkov S, Ayyer K, Kurta RP, Dzhigaev D, Kim YY, Morgan AJ, Yoon CH, Westphal D, Bielecki J, Sellberg JA, Williams G, Maia FR, Yefanov OM, Ilyin V, Mancuso AP, Chapman HN, Hogue BG, Aquila A, Barty A, Vartanyants IA. Single-particle imaging without symmetry constraints at an X-ray free-electron laser. IUCRJ 2018; 5:727-736. [PMID: 30443357 PMCID: PMC6211532 DOI: 10.1107/s205225251801120x] [Citation(s) in RCA: 50] [Impact Index Per Article: 7.1] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Received: 05/04/2018] [Accepted: 08/06/2018] [Indexed: 05/19/2023]
Abstract
The analysis of a single-particle imaging (SPI) experiment performed at the AMO beamline at LCLS as part of the SPI initiative is presented here. A workflow for the three-dimensional virus reconstruction of the PR772 bacteriophage from measured single-particle data is developed. It consists of several well defined steps including single-hit diffraction data classification, refined filtering of the classified data, reconstruction of three-dimensional scattered intensity from the experimental diffraction patterns by orientation determination and a final three-dimensional reconstruction of the virus electron density without symmetry constraints. The analysis developed here revealed and quantified nanoscale features of the PR772 virus measured in this experiment, with the obtained resolution better than 10 nm, with a clear indication that the structure was compressed in one direction and, as such, deviates from ideal icosahedral symmetry.
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Affiliation(s)
- Max Rose
- Deutsches Elektronen-Synchrotron DESY, Notkestrasse 85, Hamburg D-22607, Germany
| | - Sergey Bobkov
- National Research Centre ’Kurchatov Institute’, Akademika Kurchatova pl. 1, Moscow 123182, Russia
| | - Kartik Ayyer
- Center for Free Electron Laser Science (CFEL), Notkestrasse 85, Hamburg 22607, Germany
| | | | - Dmitry Dzhigaev
- Deutsches Elektronen-Synchrotron DESY, Notkestrasse 85, Hamburg D-22607, Germany
| | - Young Yong Kim
- Deutsches Elektronen-Synchrotron DESY, Notkestrasse 85, Hamburg D-22607, Germany
| | - Andrew J. Morgan
- Center for Free Electron Laser Science (CFEL), Notkestrasse 85, Hamburg 22607, Germany
| | - Chun Hong Yoon
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025, USA
| | - Daniel Westphal
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Sweden
| | - Johan Bielecki
- European XFEL GmbH, Holzkoppel 4, Schenefeld 22869, Germany
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Sweden
| | - Jonas A. Sellberg
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Sweden
- Biomedical and X-Ray Physics, Department of Applied Physics, AlbaNova University Center, KTH Royal Institute of Technology, Stockholm SE-106 91, Sweden
| | - Garth Williams
- Brookhaven National Laboratory, 98 Rochester St, Shirley, NY 11967, USA
| | - Filipe R.N.C. Maia
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Sweden
- NERSC, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
| | - Olexander M. Yefanov
- Center for Free Electron Laser Science (CFEL), Notkestrasse 85, Hamburg 22607, Germany
| | - Vyacheslav Ilyin
- National Research Centre ’Kurchatov Institute’, Akademika Kurchatova pl. 1, Moscow 123182, Russia
| | | | - Henry N. Chapman
- Center for Free Electron Laser Science (CFEL), Notkestrasse 85, Hamburg 22607, Germany
| | - Brenda G. Hogue
- Biodesign Center for Immunotherapy, Vaccines, and Virotherapy, Biodesign Institute at Arizona State University, Tempe 85287, USA
- Biodesign Center for Applied Structural Discovery, Biodesign Institute at Arizona State University, Tempe, AZ 85287, USA
- Arizona State University, School of Life Sciences (SOLS), Tempe, AZ 85287, USA
| | - Andrew Aquila
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025, USA
| | - Anton Barty
- Center for Free Electron Laser Science (CFEL), Notkestrasse 85, Hamburg 22607, Germany
| | - Ivan A. Vartanyants
- Deutsches Elektronen-Synchrotron DESY, Notkestrasse 85, Hamburg D-22607, Germany
- National Research Nuclear University MEPhI (Moscow Engineering Physics Institute), Kashirskoe shosse 31, Moscow 115409, Russia
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64
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Oberthür D. Biological single-particle imaging using XFELs - towards the next resolution revolution. IUCRJ 2018; 5:663-666. [PMID: 30443350 PMCID: PMC6211524 DOI: 10.1107/s2052252518015129] [Citation(s) in RCA: 6] [Impact Index Per Article: 0.9] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Indexed: 06/09/2023]
Abstract
Better injectors resulting from careful iterative optimization used at high repetition XFELs in combination with better detectors and further developed algorithms might, in the not so distant future, result in a 'resolution revolution' in SPI, enabling the molecular and atomic imaging of the dynamics of biological macromolecules without the need to freeze or crystallize the sample.
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Affiliation(s)
- Dominik Oberthür
- Center for Free-Electron Laser Science, Deutsches Elektronen-Synchrotron DESY, Notkestrasse 85, 22607 Hamburg, Germany
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65
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Ab initio structure determination from experimental fluctuation X-ray scattering data. Proc Natl Acad Sci U S A 2018; 115:11772-11777. [PMID: 30373827 PMCID: PMC6243272 DOI: 10.1073/pnas.1812064115] [Citation(s) in RCA: 23] [Impact Index Per Article: 3.3] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/24/2023] Open
Abstract
Fluctuation X-ray scattering is a biophysical structural characterization technique that overcomes low data-to-parameter ratios encountered in traditional X-ray methods used for studying noncrystalline samples. By collecting a series of ultrashort X-ray exposures on an ensemble of particles at a free-electron laser, information-dense experimental data can be extracted that ultimately result in structures with a greater level of detail than can be obtained using traditional X-ray scattering methods. In this article we demonstrate the practical feasibility of this technique by introducing data-processing techniques and advanced noise-filtering methods that reduce the required data collection time to less than a few minutes. This will ultimately allow one to visualize details of structural dynamics that may be inaccessible through traditional methods. Fluctuation X-ray scattering (FXS) is an emerging experimental technique in which X-ray solution scattering data are collected from particles in solution using ultrashort X-ray exposures generated by a free-electron laser (FEL). FXS experiments overcome the low data-to-parameter ratios associated with traditional solution scattering measurements by providing several orders of magnitude more information in the final processed data. Here we demonstrate the practical feasibility of FEL-based FXS on a biological multiple-particle system and describe data-processing techniques required to extract robust FXS data and significantly reduce the required number of snapshots needed by introducing an iterative noise-filtering technique. We showcase a successful ab initio electron density reconstruction from such an experiment, studying the Paramecium bursaria Chlorella virus (PBCV-1).
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66
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Pande K, Donatelli JJ, Malmerberg E, Foucar L, Poon BK, Sutter M, Botha S, Basu S, Bruce Doak R, Dörner K, Epp SW, Englert L, Fromme R, Hartmann E, Hartmann R, Hauser G, Hattne J, Hosseinizadeh A, Kassemeyer S, Lomb L, Montero SFC, Menzel A, Rolles D, Rudenko A, Seibert MM, Sierra RG, Schwander P, Ourmazd A, Fromme P, Sauter NK, Bogan M, Bozek J, Bostedt C, Schlichting I, Kerfeld CA, Zwart PH. Free-electron laser data for multiple-particle fluctuation scattering analysis. Sci Data 2018; 5:180201. [PMID: 30277481 PMCID: PMC6167951 DOI: 10.1038/sdata.2018.201] [Citation(s) in RCA: 5] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Grants] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 05/24/2018] [Accepted: 07/09/2018] [Indexed: 01/26/2023] Open
Abstract
Fluctuation X-ray scattering (FXS) is an emerging experimental technique in which solution scattering data are collected using X-ray exposures below rotational diffusion times, resulting in angularly anisotropic X-ray snapshots that provide several orders of magnitude more information than traditional solution scattering data. Such experiments can be performed using the ultrashort X-ray pulses provided by a free-electron laser source, allowing one to collect a large number of diffraction patterns in a relatively short time. Here, we describe a test data set for FXS, obtained at the Linac Coherent Light Source, consisting of close to 100 000 multi-particle diffraction patterns originating from approximately 50 to 200 Paramecium Bursaria Chlorella virus particles per snapshot. In addition to the raw data, a selection of high-quality pre-processed diffraction patterns and a reference SAXS profile are provided.
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Affiliation(s)
- Kanupriya Pande
- Center for Advanced Mathematics in Energy Research Applications, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
- Molecular Biophysics and Integrated Bio-imaging, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
| | - Jeffrey J. Donatelli
- Center for Advanced Mathematics in Energy Research Applications, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
- Computational Research Division, Dept. of Mathematics, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
| | - Erik Malmerberg
- Center for Advanced Mathematics in Energy Research Applications, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
- Molecular Biophysics and Integrated Bio-imaging, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
- Hit Discovery, Discovery Sciences, IMED Biotech Unit, AstraZeneca, Gothenburg, Sweden
| | - Lutz Foucar
- Max-Planck-Institut für medizinische Forschung, Jahnstr. 29, 69120 Heidelberg, Germany
- Max Planck Advanced Study Group, Center for Free Electron Laser Science (CFEL), Notkestrasse 85, 22607 Hamburg, Germany
| | - Billy K. Poon
- Molecular Biophysics and Integrated Bio-imaging, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
| | - Markus Sutter
- Molecular Biophysics and Integrated Bio-imaging, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
| | - Sabine Botha
- Max-Planck-Institut für medizinische Forschung, Jahnstr. 29, 69120 Heidelberg, Germany
- University of Hamburg, Hamburg Germany
| | - Shibom Basu
- Arizona State University, Tempe, AZ, USA
- Macromolecular Crystallography Group, Paul Scherrer Institute, 5232 Villigen – PSI, Switzerland
| | - R. Bruce Doak
- Max-Planck-Institut für medizinische Forschung, Jahnstr. 29, 69120 Heidelberg, Germany
- Arizona State University, Tempe, AZ, USA
| | - Katerina Dörner
- Arizona State University, Tempe, AZ, USA
- European XFEL GmbH, Schenefeld, Germany
| | - Sascha W. Epp
- Max Planck Advanced Study Group, Center for Free Electron Laser Science (CFEL), Notkestrasse 85, 22607 Hamburg, Germany
- Max-Planck-Institut für Kernphysik, Saupfercheckweg 1, 69117 Heidelberg, Germany
- Max Planck Institute for the Structure and Dynamics of Matter, Center for Free Electron Laser Science, Hamburg, Germany
| | - Lars Englert
- Max-Planck-Institut für extraterrestrische Physik, Giessenbachstrasse, 85741 Garching, Germany
- Carl von Ossietzky Universität Oldenburg, Department of Physics, Oldenburg, Germany
| | | | - Elisabeth Hartmann
- Max-Planck-Institut für medizinische Forschung, Jahnstr. 29, 69120 Heidelberg, Germany
| | | | - Guenter Hauser
- Max-Planck-Institut für extraterrestrische Physik, Giessenbachstrasse, 85741 Garching, Germany
| | - Johan Hattne
- Molecular Biophysics and Integrated Bio-imaging, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
- University of California, Los Angeles, Los Angeles, CA, USA
| | - Ahmad Hosseinizadeh
- Department of Physics, University of Wisconsin-Milwaukee, 3135N. Maryland Ave, Milwaukee, WI 53211, USA
| | - Stephan Kassemeyer
- Max-Planck-Institut für medizinische Forschung, Jahnstr. 29, 69120 Heidelberg, Germany
| | - Lukas Lomb
- Max-Planck-Institut für medizinische Forschung, Jahnstr. 29, 69120 Heidelberg, Germany
| | - Sebastian F. Carron Montero
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Stanford, CA, USA
- Department of Physics, California Lutheran University, Thousand Oaks, CA, USA
| | - Andreas Menzel
- Laboratory for Macromolecules and Bioimaging, Paul Scherrer Institute, 5232 Villigen – PSI, Switzerland
| | - Daniel Rolles
- Max-Planck-Institut für medizinische Forschung, Jahnstr. 29, 69120 Heidelberg, Germany
- Max Planck Advanced Study Group, Center for Free Electron Laser Science (CFEL), Notkestrasse 85, 22607 Hamburg, Germany
- James R Macdonald Laboratory, Kansas State University, Manhattan, KS, USA
| | - Artem Rudenko
- Max Planck Advanced Study Group, Center for Free Electron Laser Science (CFEL), Notkestrasse 85, 22607 Hamburg, Germany
- Max-Planck-Institut für Kernphysik, Saupfercheckweg 1, 69117 Heidelberg, Germany
- James R Macdonald Laboratory, Kansas State University, Manhattan, KS, USA
| | - Marvin M. Seibert
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Stanford, CA, USA
| | - Raymond George Sierra
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Stanford, CA, USA
| | - Peter Schwander
- Department of Physics, University of Wisconsin-Milwaukee, 3135N. Maryland Ave, Milwaukee, WI 53211, USA
| | - Abbas Ourmazd
- Department of Physics, University of Wisconsin-Milwaukee, 3135N. Maryland Ave, Milwaukee, WI 53211, USA
| | - Petra Fromme
- Max-Planck-Institut für Kernphysik, Saupfercheckweg 1, 69117 Heidelberg, Germany
| | - Nicholas K. Sauter
- Molecular Biophysics and Integrated Bio-imaging, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
| | - Michael Bogan
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Stanford, CA, USA
- Traction on Demand, Burnaby, BC, Canada
| | - John Bozek
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Stanford, CA, USA
- Synchrotron SOLEIL, L’Orme des Merisiers, Saint-Aubin, BP 48, F-91192 Gif-sur-Yvette Cedex, France
| | - Christoph Bostedt
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Stanford, CA, USA
- Department of Physics and Astronomy, Northwestern University, Evanston, IL, USA
- Atomic, Molecular and Optical Physics, Advanced Photon Source, Argonne National Laboratory, Argonne, IL, USA
| | - Ilme Schlichting
- Max-Planck-Institut für medizinische Forschung, Jahnstr. 29, 69120 Heidelberg, Germany
- Max Planck Advanced Study Group, Center for Free Electron Laser Science (CFEL), Notkestrasse 85, 22607 Hamburg, Germany
| | - Cheryl A. Kerfeld
- Molecular Biophysics and Integrated Bio-imaging, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
- DOE Plant Research Laboratory, Department of Biochemistry and Molecular Biology, Michigan State University, East Lansing, MI, USA
| | - Petrus H. Zwart
- Center for Advanced Mathematics in Energy Research Applications, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
- Molecular Biophysics and Integrated Bio-imaging, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
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67
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Pietrini A, Nettelblad C. Using convex optimization of autocorrelation with constrained support and windowing for improved phase retrieval accuracy. OPTICS EXPRESS 2018; 26:24422-24443. [PMID: 30469561 DOI: 10.1364/oe.26.024422] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/20/2018] [Accepted: 08/08/2018] [Indexed: 06/09/2023]
Abstract
In imaging modalities recording diffraction data, such as the imaging of viruses at X-ray free electron laser facilities, the original image can be reconstructed assuming known phases. When phases are unknown, oversampling and a constraint on the support region in the original object can be used to solve a non-convex optimization problem using iterative alternating-projection methods. Such schemes are ill-suited for finding the optimum solution for sparse data, since the recorded pattern does not correspond exactly to the original wave function. Different iteration starting points can give rise to different solutions. We construct a convex optimization problem, where the only local optimum is also the global optimum. This is achieved using a modified support constraint and a maximum-likelihood treatment of the recorded data as a sample from the underlying wave function. This relaxed problem is solved in order to provide a new set of most probable "healed" signal intensities, without sparseness and missing data. For these new intensities, it should be possible to satisfy the support constraint and intensity constraint exactly, without conflicts between them. By making both constraints satisfiable, traditional phase retrieval with superior results is made possible. On simulated data, we demonstrate the benefits of our approach visually, and quantify the improvement in terms of the crystallographic R factor for the recovered scalar amplitudes relative to true simulations from .405 to .097, as well as the mean-squared error in the reconstructed image from .233 to .139. We also compare our approach, with regards to theory and simulation results, to other approaches for healing as well as noise-tolerant phase retrieval. These tests indicate that the COACS pre-processing allows for best-in-class results.
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68
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Abstract
Progress in single-particle three-dimensional imaging is discussed, with advances in both data-collection and data-handling techniques described.
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Affiliation(s)
- Changyong Song
- Department of Physics, Pohang University of Science and Technology, Pohang 37673, Republic of Korea
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69
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Lundholm IV, Sellberg JA, Ekeberg T, Hantke MF, Okamoto K, van der Schot G, Andreasson J, Barty A, Bielecki J, Bruza P, Bucher M, Carron S, Daurer BJ, Ferguson K, Hasse D, Krzywinski J, Larsson DSD, Morgan A, Mühlig K, Müller M, Nettelblad C, Pietrini A, Reddy HKN, Rupp D, Sauppe M, Seibert M, Svenda M, Swiggers M, Timneanu N, Ulmer A, Westphal D, Williams G, Zani A, Faigel G, Chapman HN, Möller T, Bostedt C, Hajdu J, Gorkhover T, Maia FRNC. Considerations for three-dimensional image reconstruction from experimental data in coherent diffractive imaging. IUCRJ 2018; 5:531-541. [PMID: 30224956 PMCID: PMC6126651 DOI: 10.1107/s2052252518010047] [Citation(s) in RCA: 32] [Impact Index Per Article: 4.6] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/08/2018] [Accepted: 07/11/2018] [Indexed: 05/19/2023]
Abstract
Diffraction before destruction using X-ray free-electron lasers (XFELs) has the potential to determine radiation-damage-free structures without the need for crystallization. This article presents the three-dimensional reconstruction of the Melbournevirus from single-particle X-ray diffraction patterns collected at the LINAC Coherent Light Source (LCLS) as well as reconstructions from simulated data exploring the consequences of different kinds of experimental sources of noise. The reconstruction from experimental data suffers from a strong artifact in the center of the particle. This could be reproduced with simulated data by adding experimental background to the diffraction patterns. In those simulations, the relative density of the artifact increases linearly with background strength. This suggests that the artifact originates from the Fourier transform of the relatively flat background, concentrating all power in a central feature of limited extent. We support these findings by significantly reducing the artifact through background removal before the phase-retrieval step. Large amounts of blurring in the diffraction patterns were also found to introduce diffuse artifacts, which could easily be mistaken as biologically relevant features. Other sources of noise such as sample heterogeneity and variation of pulse energy did not significantly degrade the quality of the reconstructions. Larger data volumes, made possible by the recent inauguration of high repetition-rate XFELs, allow for increased signal-to-background ratio and provide a way to minimize these artifacts. The anticipated development of three-dimensional Fourier-volume-assembly algorithms which are background aware is an alternative and complementary solution, which maximizes the use of data.
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Affiliation(s)
- Ida V. Lundholm
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
| | - Jonas A. Sellberg
- Biomedical and X-ray Physics, Department of Applied Physics, AlbaNova University Center, KTH Royal Institute of Technology, SE-106 91 Stockholm, Sweden
| | - Tomas Ekeberg
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
| | | | - Kenta Okamoto
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
| | - Gijs van der Schot
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
| | - Jakob Andreasson
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
- ELI Beamlines, Institute of Physics, Czech Academy of Science, Na Slovance 2, CZ-182 21 Prague, Czech Republic
- Condensed Matter Physics, Department of Physics, Chalmers University of Technology, Gothenburg, Sweden
| | - Anton Barty
- Center for Free-Electron Laser Science, DESY, Notkestrasse 85, 22607 Hamburg, Germany
| | - Johan Bielecki
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
- European XFEL GmbH, Holzkoppel 4, 22869 Schenefeld, Germany
| | - Petr Bruza
- Condensed Matter Physics, Department of Physics, Chalmers University of Technology, Gothenburg, Sweden
| | - Max Bucher
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Stanford, California 94309, USA
- Institut für Optik und Atomare Physik, Technische Universität Berlin, Hardenbergstr. 36, 10623 Berlin, Germany
- Chemical Sciences and Engineering Division, Argonne National Laboratory, 9700 South Cass Avenue, Lemont, IL 60439, USA
| | - Sebastian Carron
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Stanford, California 94309, USA
| | - Benedikt J. Daurer
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
| | - Ken Ferguson
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Stanford, California 94309, USA
- PULSE Institute and SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025, USA
| | - Dirk Hasse
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
| | - Jacek Krzywinski
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Stanford, California 94309, USA
| | - Daniel S. D. Larsson
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
| | - Andrew Morgan
- Center for Free-Electron Laser Science, DESY, Notkestrasse 85, 22607 Hamburg, Germany
| | - Kerstin Mühlig
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
| | - Maria Müller
- Institut für Optik und Atomare Physik, Technische Universität Berlin, Hardenbergstr. 36, 10623 Berlin, Germany
| | - Carl Nettelblad
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
- Division of Scientific Computing, Department of Information Technology, Science for Life Laboratory, Uppsala University, Lagerhyddsvägen 2 (Box 337), SE-751 05 Uppsala, Sweden
| | - Alberto Pietrini
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
| | - Hemanth K. N. Reddy
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
| | - Daniela Rupp
- Institut für Optik und Atomare Physik, Technische Universität Berlin, Hardenbergstr. 36, 10623 Berlin, Germany
| | - Mario Sauppe
- Institut für Optik und Atomare Physik, Technische Universität Berlin, Hardenbergstr. 36, 10623 Berlin, Germany
| | - Marvin Seibert
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
| | - Martin Svenda
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
| | - Michelle Swiggers
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Stanford, California 94309, USA
| | - Nicusor Timneanu
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
- Department of Physics and Astronomy, Uppsala University, Box 516, SE-751 20 Uppsala, Sweden
| | - Anatoli Ulmer
- Institut für Optik und Atomare Physik, Technische Universität Berlin, Hardenbergstr. 36, 10623 Berlin, Germany
| | - Daniel Westphal
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
| | - Garth Williams
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Stanford, California 94309, USA
- NSLS-II, Brookhaven National Laboratory, PO Box 5000, Upton, NY 11973, USA
| | - Alessandro Zani
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
| | - Gyula Faigel
- Research Institute for Solid State Physics and Optics, 1525 Budapest, Hungary
| | - Henry N. Chapman
- Center for Free-Electron Laser Science, DESY, Notkestrasse 85, 22607 Hamburg, Germany
| | - Thomas Möller
- Institut für Optik und Atomare Physik, Technische Universität Berlin, Hardenbergstr. 36, 10623 Berlin, Germany
| | - Christoph Bostedt
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Stanford, California 94309, USA
- Chemical Sciences and Engineering Division, Argonne National Laboratory, 9700 South Cass Avenue, Lemont, IL 60439, USA
- PULSE Institute and SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025, USA
- Department of Physics, Northwestern University, 2145 Sheridan Road, Evanston, IL 60208, USA
| | - Janos Hajdu
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
- ELI Beamlines, Institute of Physics, Czech Academy of Science, Na Slovance 2, CZ-182 21 Prague, Czech Republic
| | - Tais Gorkhover
- Linac Coherent Light Source, SLAC National Accelerator Laboratory, Stanford, California 94309, USA
- Institut für Optik und Atomare Physik, Technische Universität Berlin, Hardenbergstr. 36, 10623 Berlin, Germany
- PULSE Institute and SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, CA 94025, USA
| | - Filipe R. N. C. Maia
- Laboratory of Molecular Biophysics, Department of Cell and Molecular Biology, Uppsala University, Husargatan 3 (Box 596), SE-751 24 Uppsala, Sweden
- NERSC, Lawrence Berkeley National Laboratory, 1 Cyclotron Rd, Berkeley, CA 94720, USA
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70
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Sun Z, Fan J, Li H, Liu H, Nam D, Kim C, Kim Y, Han Y, Zhang J, Yao S, Park J, Kim S, Tono K, Yabashi M, Ishikawa T, Song C, Fan C, Jiang H. Necessary Experimental Conditions for Single-Shot Diffraction Imaging of DNA-Based Structures with X-ray Free-Electron Lasers. ACS NANO 2018; 12:7509-7518. [PMID: 29986128 DOI: 10.1021/acsnano.8b01838] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/08/2023]
Abstract
It has been proposed that the radiation damage to biological particles and soft condensed matter can be overcome by ultrafast and ultraintense X-ray free-electron lasers (FELs) with short pulse durations. The successful demonstration of the "diffraction-before-destruction" concept has made single-shot diffraction imaging a promising tool to achieve high resolutions under the native states of samples. However, the resolution is still limited because of the low signal-to-noise ratio, especially for biological specimens such as cells, viruses, and macromolecular particles. Here, we present a demonstration single-shot diffraction imaging experiment of DNA-based structures at SPring-8 Angstrom Compact Free Electron Laser (SACLA), Japan. Through quantitative analysis of the reconstructed images, the scattering abilities of gold and DNA were demonstrated. Suggestions for extracting valid DNA signals from noisy diffraction patterns were also explained and outlined. To sketch out the necessary experimental conditions for the 3D imaging of DNA origami or DNA macromolecular particles, we carried out numerical simulations with practical detector noise and experimental geometry using the Linac Coherent Light Source (LCLS) at the SLAC National Accelerator Laboratory, USA. The simulated results demonstrate that it is possible to capture images of DNA-based structures at high resolutions with the technique development of current and next-generation X-ray FEL facilities.
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Affiliation(s)
- Zhibin Sun
- State Key Laboratory of Crystal Materials , Shandong University , Jinan 250100 , China
- Linac Coherent Light Source , SLAC National Accelerator Laboratory , 2575 Sand Hill Road , Menlo Park , California 94025 , United States
- School of Physical Science and Technology , ShanghaiTech University , Shanghai 201210 , China
| | - Jiadong Fan
- School of Physical Science and Technology , ShanghaiTech University , Shanghai 201210 , China
| | - Haoyuan Li
- Linac Coherent Light Source , SLAC National Accelerator Laboratory , 2575 Sand Hill Road , Menlo Park , California 94025 , United States
- Department of Physics , Stanford University , Stanford , California 94305 , United States
| | - Huajie Liu
- Laboratory of Physical Biology , Shanghai Institute of Applied Physics, Chinese Academy of Sciences , Shanghai 201800 , China
| | - Daewoong Nam
- Pohang Accelerator Laboratory , Pohang University of Science and Technology , Pohang 37673 , Korea
- Department of Physics , Pohang University of Science and Technology , Pohang 37673 , Korea
| | - Chan Kim
- European XFEL GmbH , Holzkoppel 4 , Schenefeld 22869 , Germany
- Department of Physics and Photon Science & School of Materials Science and Engineering , Gwangju Institute of Science and Technology , Gwangju 61005 , Korea
| | - Yoonhee Kim
- European XFEL GmbH , Holzkoppel 4 , Schenefeld 22869 , Germany
- Department of Physics and Photon Science & School of Materials Science and Engineering , Gwangju Institute of Science and Technology , Gwangju 61005 , Korea
| | - Yubo Han
- Institute of High Energy Physics, Chinese Academy of Sciences , Beijing 100049 , China
- SLAC National Accelerator Laboratory , 2575 Sand Hill Road , Menlo Park , California 94025 , United States
| | - Jianhua Zhang
- State Key Laboratory of Crystal Materials , Shandong University , Jinan 250100 , China
- School of Physical Science and Technology , ShanghaiTech University , Shanghai 201210 , China
| | - Shengkun Yao
- School of Physical Science and Technology , ShanghaiTech University , Shanghai 201210 , China
| | - Jaehyun Park
- Pohang Accelerator Laboratory , Pohang University of Science and Technology , Pohang 37673 , Korea
| | - Sunam Kim
- Pohang Accelerator Laboratory , Pohang University of Science and Technology , Pohang 37673 , Korea
| | - Kensuke Tono
- Japan Synchrotron Radiation Research Institute , Kouto, Sayo-cho, Sayo-gun , Hyogo 679-5198 , Japan
| | - Makina Yabashi
- RIKEN SPring-8 Center , Kouto, Sayo-cho, Sayo-gun , Hyogo 679-5148 , Japan
| | - Tetsuya Ishikawa
- RIKEN SPring-8 Center , Kouto, Sayo-cho, Sayo-gun , Hyogo 679-5148 , Japan
| | - Changyong Song
- Department of Physics , Pohang University of Science and Technology , Pohang 37673 , Korea
| | - Chunhai Fan
- Laboratory of Physical Biology , Shanghai Institute of Applied Physics, Chinese Academy of Sciences , Shanghai 201800 , China
| | - Huaidong Jiang
- School of Physical Science and Technology , ShanghaiTech University , Shanghai 201210 , China
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71
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Lehmkühler F, Schulz F, Schroer MA, Frenzel L, Lange H, Grübel G. Heterogeneous local order in self-assembled nanoparticle films revealed by X-ray cross-correlations. IUCRJ 2018; 5:354-360. [PMID: 29755751 PMCID: PMC5929381 DOI: 10.1107/s2052252518005407] [Citation(s) in RCA: 4] [Impact Index Per Article: 0.6] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/12/2018] [Accepted: 04/06/2018] [Indexed: 05/04/2023]
Abstract
We report on the self-assembly of gold nanoparticles coated with a soft poly(ethylene glycol) shell studied by X-ray cross-correlation analysis. Depending on the initial concentration of gold nanoparticles used, structurally heterogeneous films were formed. The films feature hot spots of dominating four- and sixfold local order with patch sizes of a few micrometres, containing 104-105 particles. The amplitude of the order parameters suggested that a minimum sample amount was necessary to form well ordered local structures. Furthermore, the increasing variation in order parameters with sample thickness demonstrated a high degree of structural heterogeneity. This wealth of information cannot be obtained by the conventional microscopy techniques that are commonly used to study nanocrystal superstructures, as illustrated by complementary scanning electron microscopy measurements.
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Affiliation(s)
- Felix Lehmkühler
- Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, 22607 Hamburg, Germany
- The Hamburg Centre for Ultrafast Imaging, Luruper Chaussee 149, 22761 Hamburg, Germany
| | - Florian Schulz
- The Hamburg Centre for Ultrafast Imaging, Luruper Chaussee 149, 22761 Hamburg, Germany
- Institute of Physical Chemistry, University of Hamburg, Grindelallee 117, 20146 Hamburg, Germany
| | - Martin A. Schroer
- European Molecular Biology Laboratory EMBL c/o DESY, Notkestrasse 85, 22607 Hamburg, Germany
| | - Lara Frenzel
- Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, 22607 Hamburg, Germany
- The Hamburg Centre for Ultrafast Imaging, Luruper Chaussee 149, 22761 Hamburg, Germany
| | - Holger Lange
- The Hamburg Centre for Ultrafast Imaging, Luruper Chaussee 149, 22761 Hamburg, Germany
- Institute of Physical Chemistry, University of Hamburg, Grindelallee 117, 20146 Hamburg, Germany
| | - Gerhard Grübel
- Deutsches Elektronen-Synchrotron (DESY), Notkestrasse 85, 22607 Hamburg, Germany
- The Hamburg Centre for Ultrafast Imaging, Luruper Chaussee 149, 22761 Hamburg, Germany
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72
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Mancini GF, Karl RM, Shanblatt ER, Bevis CS, Gardner DF, Tanksalvala MD, Russell JL, Adams DE, Kapteyn HC, Badding JV, Mallouk TE, Murnane MM. Colloidal crystal order and structure revealed by tabletop extreme ultraviolet scattering and coherent diffractive imaging. OPTICS EXPRESS 2018; 26:11393-11406. [PMID: 29716059 DOI: 10.1364/oe.26.011393] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 02/06/2018] [Accepted: 04/03/2018] [Indexed: 06/08/2023]
Abstract
Colloidal crystals with specific electronic, optical, magnetic, vibrational properties, can be rationally designed by controlling fundamental parameters such as chemical composition, scale, periodicity and lattice symmetry. In particular, silica nanospheres -which assemble to form colloidal crystals- are ideal for this purpose, because of the ability to infiltrate their templates with semiconductors or metals. However characterization of these crystals is often limited to techniques such as grazing incidence small-angle scattering that provide only global structural information and also often require synchrotron sources. Here we demonstrate small-angle Bragg scattering from nanostructured materials using a tabletop-scale setup based on high-harmonic generation, to reveal important information about the local order of nanosphere grains, separated by grain boundaries and discontinuities. We also apply full-field quantitative ptychographic imaging to visualize the extended structure of a silica close-packed nanosphere multilayer, with thickness information encoded in the phase. These combined techniques allow us to simultaneously characterize the silica nanospheres size, their symmetry and distribution within single colloidal crystal grains, the local arrangement of nearest-neighbor grains, as well as to quantitatively determine the number of layers within the sample. Key to this advance is the good match between the high harmonic wavelength used (13.5nm) and the high transmission, high scattering efficiency, and low sample damage of the silica colloidal crystal at this wavelength. As a result, the relevant distances in the sample - namely, the interparticle distance (≈124nm) and the colloidal grains local arrangement (≈1μm) - can be investigated with Bragg coherent EUV scatterometry and ptychographic imaging within the same experiment simply by tuning the EUV spot size at the sample plane (5μm and 15μm respectively). In addition, the high spatial coherence of high harmonics light, combined with advances in imaging techniques, makes it possible to image near-periodic structures quantitatively and nondestructively, and enables the observation of the extended order of quasi-periodic colloidal crystals, with a spatial resolution better than 20nm. In the future, by harnessing the high time-resolution of tabletop high harmonics, this technique can be extended to dynamically image the three-dimensional electronic, magnetic, and transport properties of functional nanosystems.
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73
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Recent developments in small-angle X-ray scattering and hybrid method approaches for biomacromolecular solutions. Emerg Top Life Sci 2018; 2:69-79. [PMID: 33525782 DOI: 10.1042/etls20170138] [Citation(s) in RCA: 23] [Impact Index Per Article: 3.3] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 12/17/2017] [Revised: 02/01/2018] [Accepted: 02/05/2018] [Indexed: 01/05/2023]
Abstract
Small-angle X-ray scattering (SAXS) has become a streamline method to characterize biological macromolecules, from small peptides to supramolecular complexes, in near-native solutions. Modern SAXS requires limited amounts of purified material, without the need for labelling, crystallization, or freezing. Dedicated beamlines at modern synchrotron sources yield high-quality data within or below several milliseconds of exposure time and are highly automated, allowing for rapid structural screening under different solutions and ambient conditions but also for time-resolved studies of biological processes. The advanced data analysis methods allow one to meaningfully interpret the scattering data from monodisperse systems, from transient complexes as well as flexible and heterogeneous systems in terms of structural models. Especially powerful are hybrid approaches utilizing SAXS with high-resolution structural techniques, but also with biochemical, biophysical, and computational methods. Here, we review the recent developments in the experimental SAXS practice and in analysis methods with a specific focus on the joint use of SAXS with complementary methods.
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74
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Xavier PL, Chandrasekaran AR. DNA-based construction at the nanoscale: emerging trends and applications. NANOTECHNOLOGY 2018; 29:062001. [PMID: 29232197 DOI: 10.1088/1361-6528/aaa120] [Citation(s) in RCA: 38] [Impact Index Per Article: 5.4] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/19/2023]
Abstract
The field of structural DNA nanotechnology has evolved remarkably-from the creation of artificial immobile junctions to the recent DNA-protein hybrid nanoscale shapes-in a span of about 35 years. It is now possible to create complex DNA-based nanoscale shapes and large hierarchical assemblies with greater stability and predictability, thanks to the development of computational tools and advances in experimental techniques. Although it started with the original goal of DNA-assisted structure determination of difficult-to-crystallize molecules, DNA nanotechnology has found its applications in a myriad of fields. In this review, we cover some of the basic and emerging assembly principles: hybridization, base stacking/shape complementarity, and protein-mediated formation of nanoscale structures. We also review various applications of DNA nanostructures, with special emphasis on some of the biophysical applications that have been reported in recent years. In the outlook, we discuss further improvements in the assembly of such structures, and explore possible future applications involving super-resolved fluorescence, single-particle cryo-electron (cryo-EM) and x-ray free electron laser (XFEL) nanoscopic imaging techniques, and in creating new synergistic designer materials.
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Affiliation(s)
- P Lourdu Xavier
- Center for Free Electron Laser Science, Deutsches Elektronen-Synchrotron (DESY) and Department of Physics, University of Hamburg, D-22607 Hamburg, Germany. Max-Planck Institute for the Structure and Dynamics of Matter, Luruper Chaussee 149, D-22761 Hamburg, Germany
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75
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Current Status of Single Particle Imaging with X-ray Lasers. APPLIED SCIENCES-BASEL 2018. [DOI: 10.3390/app8010132] [Citation(s) in RCA: 21] [Impact Index Per Article: 3.0] [Reference Citation Analysis] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 12/11/2022]
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