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Li X, Inhester L, Robatjazi SJ, Erk B, Boll R, Hanasaki K, Toyota K, Hao Y, Bomme C, Rudek B, Foucar L, Southworth SH, Lehmann CS, Kraessig B, Marchenko T, Simon M, Ueda K, Ferguson KR, Bucher M, Gorkhover T, Carron S, Alonso-Mori R, Koglin JE, Correa J, Williams GJ, Boutet S, Young L, Bostedt C, Son SK, Santra R, Rolles D, Rudenko A. Pulse Energy and Pulse Duration Effects in the Ionization and Fragmentation of Iodomethane by Ultraintense Hard X Rays. Phys Rev Lett 2021; 127:093202. [PMID: 34506178 DOI: 10.1103/physrevlett.127.093202] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/20/2019] [Revised: 01/24/2021] [Accepted: 07/02/2021] [Indexed: 06/13/2023]
Abstract
The interaction of intense femtosecond x-ray pulses with molecules sensitively depends on the interplay between multiple photoabsorptions, Auger decay, charge rearrangement, and nuclear motion. Here, we report on a combined experimental and theoretical study of the ionization and fragmentation of iodomethane (CH_{3}I) by ultraintense (∼10^{19} W/cm^{2}) x-ray pulses at 8.3 keV, demonstrating how these dynamics depend on the x-ray pulse energy and duration. We show that the timing of multiple ionization steps leading to a particular reaction product and, thus, the product's final kinetic energy, is determined by the pulse duration rather than the pulse energy or intensity. While the overall degree of ionization is mainly defined by the pulse energy, our measurement reveals that the yield of the fragments with the highest charge states is enhanced for short pulse durations, in contrast to earlier observations for atoms and small molecules in the soft x-ray domain. We attribute this effect to a decreased charge transfer efficiency at larger internuclear separations, which are reached during longer pulses.
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Affiliation(s)
- X Li
- J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, Kansas, USA
| | - L Inhester
- Center for Free-Electron Laser Science, DESY, Hamburg, Germany
- The Hamburg Centre for Ultrafast Imaging, Hamburg, Germany
| | - S J Robatjazi
- J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, Kansas, USA
| | - B Erk
- Deutsches Elektronen-Synchrotron (DESY), Hamburg, Germany
| | - R Boll
- Max Planck Institute for Nuclear Physics, Heidelberg, Germany
- European XFEL, Schenefeld, Germany
| | - K Hanasaki
- Center for Free-Electron Laser Science, DESY, Hamburg, Germany
- The Hamburg Centre for Ultrafast Imaging, Hamburg, Germany
| | - K Toyota
- Center for Free-Electron Laser Science, DESY, Hamburg, Germany
- The Hamburg Centre for Ultrafast Imaging, Hamburg, Germany
| | - Y Hao
- Center for Free-Electron Laser Science, DESY, Hamburg, Germany
- The Hamburg Centre for Ultrafast Imaging, Hamburg, Germany
- Institute of Theoretical Physics and Department of Physics, University of Science and Technology Beijing, Beijing, People's Republic of China
| | - C Bomme
- Deutsches Elektronen-Synchrotron (DESY), Hamburg, Germany
| | - B Rudek
- Physikalisch-Technische Bundesanstalt (PTB), Braunschweig, Germany
| | - L Foucar
- Max Planck Institute for Medical Research, Heidelberg, Germany
| | - S H Southworth
- Chemical Sciences and Engineering Division, Argonne National Laboratory, Lemont, Illinois, USA
| | - C S Lehmann
- Chemical Sciences and Engineering Division, Argonne National Laboratory, Lemont, Illinois, USA
- Fachbereich Chemie, Philipps-Universität Marburg, Marburg, Germany
| | - B Kraessig
- Chemical Sciences and Engineering Division, Argonne National Laboratory, Lemont, Illinois, USA
| | - T Marchenko
- Sorbonne Université, CNRS, Laboratoire de Chimie Physique-Matière et Rayonnement, LCPMR, Paris, France
| | - M Simon
- Sorbonne Université, CNRS, Laboratoire de Chimie Physique-Matière et Rayonnement, LCPMR, Paris, France
| | - K Ueda
- Institute of Multidisciplinary Research for Advanced Materials, Tohoku University, Sendai, Japan
| | - K R Ferguson
- LCLS, SLAC National Accelerator Laboratory, Menlo Park, California, USA
| | - M Bucher
- Chemical Sciences and Engineering Division, Argonne National Laboratory, Lemont, Illinois, USA
- LCLS, SLAC National Accelerator Laboratory, Menlo Park, California, USA
| | - T Gorkhover
- LCLS, SLAC National Accelerator Laboratory, Menlo Park, California, USA
- Institut für Optik und Atomare Physik, Technische Universität Berlin, Berlin, Germany
| | - S Carron
- LCLS, SLAC National Accelerator Laboratory, Menlo Park, California, USA
| | - R Alonso-Mori
- LCLS, SLAC National Accelerator Laboratory, Menlo Park, California, USA
| | - J E Koglin
- LCLS, SLAC National Accelerator Laboratory, Menlo Park, California, USA
| | - J Correa
- Center for Free-Electron Laser Science, DESY, Hamburg, Germany
- Deutsches Elektronen-Synchrotron (DESY), Hamburg, Germany
| | - G J Williams
- LCLS, SLAC National Accelerator Laboratory, Menlo Park, California, USA
- NSLS-II, Brookhaven National Laboratory, Upton New York, USA
| | - S Boutet
- LCLS, SLAC National Accelerator Laboratory, Menlo Park, California, USA
| | - L Young
- Chemical Sciences and Engineering Division, Argonne National Laboratory, Lemont, Illinois, USA
- Department of Physics and James Franck Institute, The University of Chicago, Chicago, Illinois, USA
| | - C Bostedt
- Chemical Sciences and Engineering Division, Argonne National Laboratory, Lemont, Illinois, USA
- Paul Scherrer Institut, Villigen-PSI, Villigen, Switzerland
- Institute of Chemical Sciences and Engineering, Ecole Polytechnique Fédérale de Lausanne, Lausanne, Switzerland
| | - S-K Son
- Center for Free-Electron Laser Science, DESY, Hamburg, Germany
- The Hamburg Centre for Ultrafast Imaging, Hamburg, Germany
| | - R Santra
- Center for Free-Electron Laser Science, DESY, Hamburg, Germany
- The Hamburg Centre for Ultrafast Imaging, Hamburg, Germany
- Department of Physics, Universität Hamburg, Hamburg, Germany
| | - D Rolles
- J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, Kansas, USA
- Deutsches Elektronen-Synchrotron (DESY), Hamburg, Germany
| | - A Rudenko
- J. R. Macdonald Laboratory, Department of Physics, Kansas State University, Manhattan, Kansas, USA
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2
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Galli L, Son SK, Klinge M, Bajt S, Barty A, Bean R, Betzel C, Beyerlein KR, Caleman C, Doak RB, Duszenko M, Fleckenstein H, Gati C, Hunt B, Kirian RA, Liang M, Nanao MH, Nass K, Oberthür D, Redecke L, Shoeman R, Stellato F, Yoon CH, White TA, Yefanov O, Spence J, Chapman HN. Electronic damage in S atoms in a native protein crystal induced by an intense X-ray free-electron laser pulse. Struct Dyn 2015; 2:041703. [PMID: 26798803 PMCID: PMC4711609 DOI: 10.1063/1.4919398] [Citation(s) in RCA: 5] [Impact Index Per Article: 0.6] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/12/2015] [Accepted: 04/17/2015] [Indexed: 05/07/2023]
Abstract
Current hard X-ray free-electron laser (XFEL) sources can deliver doses to biological macromolecules well exceeding 1 GGy, in timescales of a few tens of femtoseconds. During the pulse, photoionization can reach the point of saturation in which certain atomic species in the sample lose most of their electrons. This electronic radiation damage causes the atomic scattering factors to change, affecting, in particular, the heavy atoms, due to their higher photoabsorption cross sections. Here, it is shown that experimental serial femtosecond crystallography data collected with an extremely bright XFEL source exhibit a reduction of the effective scattering power of the sulfur atoms in a native protein. Quantitative methods are developed to retrieve information on the effective ionization of the damaged atomic species from experimental data, and the implications of utilizing new phasing methods which can take advantage of this localized radiation damage are discussed.
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Affiliation(s)
| | | | - M Klinge
- Joint Laboratory for Structural Biology of Infection and Inflammation, Institute of Biochemistry and Molecular Biology, University of Hamburg and Institute of Biochemistry, University of Luebeck at DESY, 22607 Hamburg, Germany
| | - S Bajt
- Photon Science, Deutsches Elektronen-Synchrotron DESY , Notkestrasse 85, 22607 Hamburg, Germany
| | - A Barty
- Center for Free-Electron Laser Science, Deutsches Elektronen-Synchrotron DESY , Notkestrasse 85, 22607 Hamburg, Germany
| | - R Bean
- Center for Free-Electron Laser Science, Deutsches Elektronen-Synchrotron DESY , Notkestrasse 85, 22607 Hamburg, Germany
| | - C Betzel
- Department of Chemistry, Institute of Biochemistry and Molecular Biology, University of Hamburg at DESY, 22607 Hamburg, Germany
| | - K R Beyerlein
- Center for Free-Electron Laser Science, Deutsches Elektronen-Synchrotron DESY , Notkestrasse 85, 22607 Hamburg, Germany
| | | | - R B Doak
- Department of Biomolecular Mechanisms, Max Planck-Institute for Medical Research , Jahnstrasse 29, 69120 Heidelberg, Germany
| | - M Duszenko
- Interfaculty Institute of Biochemistry, University of Tübingen , 72076 Tübingen, Germany
| | - H Fleckenstein
- Center for Free-Electron Laser Science, Deutsches Elektronen-Synchrotron DESY , Notkestrasse 85, 22607 Hamburg, Germany
| | - C Gati
- Center for Free-Electron Laser Science, Deutsches Elektronen-Synchrotron DESY , Notkestrasse 85, 22607 Hamburg, Germany
| | - B Hunt
- Department of Physics and Astronomy, Brigham Young University , Provo, Utah 84602, USA
| | - R A Kirian
- Center for Free-Electron Laser Science, Deutsches Elektronen-Synchrotron DESY , Notkestrasse 85, 22607 Hamburg, Germany
| | - M Liang
- Center for Free-Electron Laser Science, Deutsches Elektronen-Synchrotron DESY , Notkestrasse 85, 22607 Hamburg, Germany
| | - M H Nanao
- EMBL , Grenoble Outstation, Rue Jules Horowitz 6, Grenoble 38042, France
| | - K Nass
- Department of Biomolecular Mechanisms, Max Planck-Institute for Medical Research , Jahnstrasse 29, 69120 Heidelberg, Germany
| | - D Oberthür
- Center for Free-Electron Laser Science, Deutsches Elektronen-Synchrotron DESY , Notkestrasse 85, 22607 Hamburg, Germany
| | - L Redecke
- Joint Laboratory for Structural Biology of Infection and Inflammation, Institute of Biochemistry and Molecular Biology, University of Hamburg and Institute of Biochemistry, University of Luebeck at DESY, 22607 Hamburg, Germany
| | - R Shoeman
- Department of Biomolecular Mechanisms, Max Planck-Institute for Medical Research , Jahnstrasse 29, 69120 Heidelberg, Germany
| | - F Stellato
- Center for Free-Electron Laser Science, Deutsches Elektronen-Synchrotron DESY , Notkestrasse 85, 22607 Hamburg, Germany
| | | | - T A White
- Center for Free-Electron Laser Science, Deutsches Elektronen-Synchrotron DESY , Notkestrasse 85, 22607 Hamburg, Germany
| | - O Yefanov
- Center for Free-Electron Laser Science, Deutsches Elektronen-Synchrotron DESY , Notkestrasse 85, 22607 Hamburg, Germany
| | - J Spence
- Department of Physics, Arizona State University , Tempe, Arizona 85287-1504, USA
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3
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Murphy BF, Osipov T, Jurek Z, Fang L, Son SK, Mucke M, Eland JHD, Zhaunerchyk V, Feifel R, Avaldi L, Bolognesi P, Bostedt C, Bozek JD, Grilj J, Guehr M, Frasinski LJ, Glownia J, Ha DT, Hoffmann K, Kukk E, McFarland BK, Miron C, Sistrunk E, Squibb RJ, Ueda K, Santra R, Berrah N. Femtosecond X-ray-induced explosion of C60 at extreme intensity. Nat Commun 2014; 5:4281. [PMID: 24969734 DOI: 10.1038/ncomms5281] [Citation(s) in RCA: 108] [Impact Index Per Article: 10.8] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 01/21/2014] [Accepted: 06/02/2014] [Indexed: 11/09/2022] Open
Abstract
Understanding molecular femtosecond dynamics under intense X-ray exposure is critical to progress in biomolecular imaging and matter under extreme conditions. Imaging viruses and proteins at an atomic spatial scale and on the time scale of atomic motion requires rigorous, quantitative understanding of dynamical effects of intense X-ray exposure. Here we present an experimental and theoretical study of C60 molecules interacting with intense X-ray pulses from a free-electron laser, revealing the influence of processes not previously reported. Our work illustrates the successful use of classical mechanics to describe all moving particles in C60, an approach that scales well to larger systems, for example, biomolecules. Comparisons of the model with experimental data on C60 ion fragmentation show excellent agreement under a variety of laser conditions. The results indicate that this modelling is applicable for X-ray interactions with any extended system, even at higher X-ray dose rates expected with future light sources.
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Affiliation(s)
- B F Murphy
- 1] Department of Physics, Western Michigan University, Kalamazoo, Michigan 49008, USA [2]
| | - T Osipov
- 1] Department of Physics, Western Michigan University, Kalamazoo, Michigan 49008, USA [2]
| | - Z Jurek
- 1] Center for Free-Electron Laser Science, DESY, 22607 Hamburg, Germany [2] The Hamburg Centre for Ultrafast Imaging, 22761 Hamburg, Germany [3]
| | - L Fang
- Department of Physics, Western Michigan University, Kalamazoo, Michigan 49008, USA
| | - S-K Son
- 1] Center for Free-Electron Laser Science, DESY, 22607 Hamburg, Germany [2] The Hamburg Centre for Ultrafast Imaging, 22761 Hamburg, Germany
| | - M Mucke
- Gothenburg University, Department of Physics Origovägen 6, SE-412 96 Gothenburg, Sweden
| | - J H D Eland
- 1] Gothenburg University, Department of Physics Origovägen 6, SE-412 96 Gothenburg, Sweden [2] Department of Chemistry, Oxford University, Oxford OX1 3QZ, UK
| | - V Zhaunerchyk
- Gothenburg University, Department of Physics Origovägen 6, SE-412 96 Gothenburg, Sweden
| | - R Feifel
- Gothenburg University, Department of Physics Origovägen 6, SE-412 96 Gothenburg, Sweden
| | - L Avaldi
- Instituto di Metodologie Inorganiche e dei Plasmi, C.N.R., Rome 00133, Italy
| | - P Bolognesi
- Instituto di Metodologie Inorganiche e dei Plasmi, C.N.R., Rome 00133, Italy
| | - C Bostedt
- SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - J D Bozek
- SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - J Grilj
- PULSE, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - M Guehr
- PULSE, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - L J Frasinski
- Blackett Laboratory, Imperial College London, London SW7 2AZ, UK
| | - J Glownia
- SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - D T Ha
- Department of Physics, University of Turku, FIN-20014 Turku, Finland
| | - K Hoffmann
- Department of Physics, University of Texas at Austin, Austin, Texas 78712, USA
| | - E Kukk
- Department of Physics, University of Turku, FIN-20014 Turku, Finland
| | - B K McFarland
- PULSE, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - C Miron
- Synchrotron SOLEIL, l'Orme des Merisiers, Saint-Aubin, BP 48, 91192 Gif-sur-Yvette, France
| | - E Sistrunk
- PULSE, SLAC National Accelerator Laboratory, Menlo Park, California 94025, USA
| | - R J Squibb
- 1] Gothenburg University, Department of Physics Origovägen 6, SE-412 96 Gothenburg, Sweden [2] Blackett Laboratory, Imperial College London, London SW7 2AZ, UK
| | - K Ueda
- Department of Physics, Tohoku University, Sendai 980-8577, Japan
| | - R Santra
- 1] Center for Free-Electron Laser Science, DESY, 22607 Hamburg, Germany [2] The Hamburg Centre for Ultrafast Imaging, 22761 Hamburg, Germany [3] Department of Physics, University of Hamburg, 20355 Hamburg, Germany
| | - N Berrah
- Department of Physics, University of Connecticut, Storrs, Connecticut 06269, USA
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4
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Müller L, Gutt C, Pfau B, Schaffert S, Geilhufe J, Büttner F, Mohanty J, Flewett S, Treusch R, Düsterer S, Redlin H, Al-Shemmary A, Hille M, Kobs A, Frömter R, Oepen HP, Ziaja B, Medvedev N, Son SK, Thiele R, Santra R, Vodungbo B, Lüning J, Eisebitt S, Grübel G. Breakdown of the x-ray resonant magnetic scattering signal during intense pulses of extreme ultraviolet free-electron-laser radiation. Phys Rev Lett 2013; 110:234801. [PMID: 25167501 DOI: 10.1103/physrevlett.110.234801] [Citation(s) in RCA: 9] [Impact Index Per Article: 0.8] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 10/11/2012] [Indexed: 05/23/2023]
Abstract
We present results of single-shot resonant magnetic scattering experiments of Co/Pt multilayer systems using 100 fs long ultraintense pulses from an extreme ultraviolet (XUV) free-electron laser. An x-ray-induced breakdown of the resonant magnetic scattering channel during the pulse duration is observed at fluences of 5 J/cm(2). Simultaneously, the speckle contrast of the high-fluence scattering pattern is significantly reduced. We performed simulations of the nonequilibrium evolution of the Co/Pt multilayer system during the XUV pulse duration. We find that the electronic state of the sample is strongly perturbed during the first few femtoseconds of exposure leading to an ultrafast quenching of the resonant magnetic scattering mechanism.
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Affiliation(s)
- L Müller
- Deutsches Elektronen-Synchrotron (DESY), Notkestraße 85, 22607 Hamburg, Germany
| | - C Gutt
- Deutsches Elektronen-Synchrotron (DESY), Notkestraße 85, 22607 Hamburg, Germany and The Hamburg Centre for Ultrafast Imaging, Luruper Chaussee 149, 22761 Hamburg, Germany
| | - B Pfau
- Institut für Optik und Atomare Physik, TU Berlin, 10623 Berlin, Germany
| | - S Schaffert
- Institut für Optik und Atomare Physik, TU Berlin, 10623 Berlin, Germany
| | - J Geilhufe
- Helmholtz-Zentrum Berlin für Materialien und Energie GmbH, 14109 Berlin, Germany
| | - F Büttner
- Institut für Optik und Atomare Physik, TU Berlin, 10623 Berlin, Germany
| | - J Mohanty
- Institut für Optik und Atomare Physik, TU Berlin, 10623 Berlin, Germany
| | - S Flewett
- Institut für Optik und Atomare Physik, TU Berlin, 10623 Berlin, Germany
| | - R Treusch
- Deutsches Elektronen-Synchrotron (DESY), Notkestraße 85, 22607 Hamburg, Germany
| | - S Düsterer
- Deutsches Elektronen-Synchrotron (DESY), Notkestraße 85, 22607 Hamburg, Germany
| | - H Redlin
- Deutsches Elektronen-Synchrotron (DESY), Notkestraße 85, 22607 Hamburg, Germany
| | - A Al-Shemmary
- Deutsches Elektronen-Synchrotron (DESY), Notkestraße 85, 22607 Hamburg, Germany
| | - M Hille
- Institut für Angewandte Physik, Universität Hamburg, 20355 Hamburg, Germany
| | - A Kobs
- Institut für Angewandte Physik, Universität Hamburg, 20355 Hamburg, Germany
| | - R Frömter
- Institut für Angewandte Physik, Universität Hamburg, 20355 Hamburg, Germany
| | - H P Oepen
- Institut für Angewandte Physik, Universität Hamburg, 20355 Hamburg, Germany
| | - B Ziaja
- Deutsches Elektronen-Synchrotron (DESY), Notkestraße 85, 22607 Hamburg, Germany and The Hamburg Centre for Ultrafast Imaging, Luruper Chaussee 149, 22761 Hamburg, Germany and Center for Free-Electron Laser Science, DESY, 22607 Hamburg, Germany and Institute of Nuclear Physics, Polish Academy of Sciences, Radzikowskiego 152, 31-342 Krakow, Poland
| | - N Medvedev
- Deutsches Elektronen-Synchrotron (DESY), Notkestraße 85, 22607 Hamburg, Germany and Center for Free-Electron Laser Science, DESY, 22607 Hamburg, Germany
| | - S-K Son
- Deutsches Elektronen-Synchrotron (DESY), Notkestraße 85, 22607 Hamburg, Germany and Center for Free-Electron Laser Science, DESY, 22607 Hamburg, Germany
| | - R Thiele
- Deutsches Elektronen-Synchrotron (DESY), Notkestraße 85, 22607 Hamburg, Germany and Center for Free-Electron Laser Science, DESY, 22607 Hamburg, Germany
| | - R Santra
- Deutsches Elektronen-Synchrotron (DESY), Notkestraße 85, 22607 Hamburg, Germany and The Hamburg Centre for Ultrafast Imaging, Luruper Chaussee 149, 22761 Hamburg, Germany and Center for Free-Electron Laser Science, DESY, 22607 Hamburg, Germany and I. Institut für Theoretische Physik, Universität Hamburg, 20355 Hamburg, Germany
| | - B Vodungbo
- Laboratoire de Chimie Physique Matière et Rayonnement-CNRS UMR 7614, Université Pierre et Marie Curie, 75005 Paris, France
| | - J Lüning
- Laboratoire de Chimie Physique Matière et Rayonnement-CNRS UMR 7614, Université Pierre et Marie Curie, 75005 Paris, France
| | - S Eisebitt
- Institut für Optik und Atomare Physik, TU Berlin, 10623 Berlin, Germany and Helmholtz-Zentrum Berlin für Materialien und Energie GmbH, 14109 Berlin, Germany
| | - G Grübel
- Deutsches Elektronen-Synchrotron (DESY), Notkestraße 85, 22607 Hamburg, Germany and The Hamburg Centre for Ultrafast Imaging, Luruper Chaussee 149, 22761 Hamburg, Germany
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5
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Fukuzawa H, Son SK, Motomura K, Mondal S, Nagaya K, Wada S, Liu XJ, Feifel R, Tachibana T, Ito Y, Kimura M, Sakai T, Matsunami K, Hayashita H, Kajikawa J, Johnsson P, Siano M, Kukk E, Rudek B, Erk B, Foucar L, Robert E, Miron C, Tono K, Inubushi Y, Hatsui T, Yabashi M, Yao M, Santra R, Ueda K. Deep inner-shell multiphoton ionization by intense x-ray free-electron laser pulses. Phys Rev Lett 2013; 110:173005. [PMID: 23679721 DOI: 10.1103/physrevlett.110.173005] [Citation(s) in RCA: 27] [Impact Index Per Article: 2.5] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/23/2012] [Revised: 02/04/2013] [Indexed: 05/11/2023]
Abstract
We have investigated multiphoton multiple ionization dynamics of xenon atoms using a new x-ray free-electron laser facility, SPring-8 Angstrom Compact free electron LAser (SACLA) in Japan, and identified that Xe(n+) with n up to 26 is produced at a photon energy of 5.5 keV. The observed high charge states (n≥24) are produced via five-photon absorption, evidencing the occurrence of multiphoton absorption involving deep inner shells. A newly developed theoretical model, which shows good agreement with the experiment, elucidates the complex pathways of sequential electronic decay cascades accessible in heavy atoms. The present study of heavy-atom ionization dynamics in high-intensity hard-x-ray pulses makes a step forward towards molecular structure determination with x-ray free-electron lasers.
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Affiliation(s)
- H Fukuzawa
- Institute of Multidisciplinary Research for Advanced Materials, Tohoku University, Sendai 980-8577, Japan
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6
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Doumy G, Roedig C, Son SK, Blaga CI, DiChiara AD, Santra R, Berrah N, Bostedt C, Bozek JD, Bucksbaum PH, Cryan JP, Fang L, Ghimire S, Glownia JM, Hoener M, Kanter EP, Krässig B, Kuebel M, Messerschmidt M, Paulus GG, Reis DA, Rohringer N, Young L, Agostini P, DiMauro LF. Nonlinear atomic response to intense ultrashort x rays. Phys Rev Lett 2011; 106:083002. [PMID: 21405568 DOI: 10.1103/physrevlett.106.083002] [Citation(s) in RCA: 73] [Impact Index Per Article: 5.6] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 12/13/2010] [Indexed: 05/11/2023]
Abstract
The nonlinear absorption mechanisms of neon atoms to intense, femtosecond kilovolt x rays are investigated. The production of Ne(9+) is observed at x-ray frequencies below the Ne(8+), 1s(2) absorption edge and demonstrates a clear quadratic dependence on fluence. Theoretical analysis shows that the production is a combination of the two-photon ionization of Ne(8+) ground state and a high-order sequential process involving single-photon production and ionization of transient excited states on a time scale faster than the Auger decay. We find that the nonlinear direct two-photon ionization cross section is orders of magnitude higher than expected from previous calculations.
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Affiliation(s)
- G Doumy
- The Ohio State University, Columbus, Ohio 43210, USA
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7
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Abstract
Two new one-dimensional single azide-bridged metal(II) compounds [[M(5-methylpyrazole)4(N3)]n](ClO4)n(H2O)n [M = Co (1a), Ni (2a)] were prepared by treating an M(II) ion with stoichiometric amount of sodium azide in the presence of four equivalents of the 3(5)-methylpyrazole ligand. The isostructural compounds 1a and 2a crystallize in the monoclinic space group P2(1)/n. The azide bridging ligands have a unique end-to-end coordination mode that brings two neighboring metal centers into a cis-position with respect to the azide unit to form single end-to-end azide-bridged cobalt(II) and nickel(II) chains. The two neighboring metal atoms at inversion centers adopt octahedral environments with four equatorial 3(5)-methylpyrazole ligands and two axial azide bridges. Two adjacent equatorial least-squares planes form dihedral angles of 60.5 degrees and 60.6 degrees for Co and Ni, respectively. In addition, the metal-azide-metal units form large M-N3-M torsion angles, which are magnetically important geometrical parameters, of 71.6 degrees for M=Co and 75.7 degrees for M=Ni. It should also be noted that the M-N-N angles associated with end-to-end azide group, another magnetically important structural parameter, fall into the experimentally observed range of 120-140 degrees as 128.3(3) and 147.8(3) degrees for cobalt species and 128.4(2) and 146.1(3) degrees for nickel species; these values deviate from the theoretical value of around 164 degrees at which the incidental orthogonality is achieved under the torsion angle of 0 degrees. The compounds 1a and 2a have unique magnetic properties of ferromagnetism, zero-field splitting, and spin canting. The MO calculations indicate that the quasiorthogonality between the magnetic orbitals of metal ions and the p atomic orbitals of the bridging azide is possible in the observed structures and leads to the ferromagnetism. The spin canting related to the perturbation of ferromagnetism arises from the magnetic anisotropy and antisymmetric interactions judged by the structural parameters of the zero-field splitting and the tilted MN4 planes in a chain. The enhancement of magnetic interactions was accomplished by dehydrating the chain compounds to afford two soft magnets with critical temperature T(C) and coercive field of 2 K and 35 G for 1b and 2.3 K and 20 G for 2b, respectively.
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Affiliation(s)
- C S Hong
- Department of Chemistry, School of Molecular Science and Center for Molecular Design and Synthesis, Korea Advanced Institute of Science and Technology, Daejeon
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