Femtosecond electronic response of atoms to ultra-intense X-rays

An era of exploring the interactions of high-intensity, hard X-rays with matter has begun with the start-up of a hard-X-ray free-electron laser, the Linac Coherent Light Source (LCLS). Understanding how electrons in matter respond to ultra-intense X-ray radiation is essential for all applications. H...

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Veröffentlicht in:Nature 2010-07, Vol.466 (7302), p.56-61
Hauptverfasser: Young, L., Kanter, E. P., Krässig, B., Li, Y., March, A. M., Pratt, S. T., Santra, R., Southworth, S. H., Rohringer, N., DiMauro, L. F., Doumy, G., Roedig, C. A., Berrah, N., Fang, L., Hoener, M., Bucksbaum, P. H., Cryan, J. P., Ghimire, S., Glownia, J. M., Reis, D. A., Bozek, J. D., Bostedt, C., Messerschmidt, M.
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container_end_page 61
container_issue 7302
container_start_page 56
container_title Nature
container_volume 466
creator Young, L.
Kanter, E. P.
Krässig, B.
Li, Y.
March, A. M.
Pratt, S. T.
Santra, R.
Southworth, S. H.
Rohringer, N.
DiMauro, L. F.
Doumy, G.
Roedig, C. A.
Berrah, N.
Fang, L.
Hoener, M.
Bucksbaum, P. H.
Cryan, J. P.
Ghimire, S.
Glownia, J. M.
Reis, D. A.
Bozek, J. D.
Bostedt, C.
Messerschmidt, M.
description An era of exploring the interactions of high-intensity, hard X-rays with matter has begun with the start-up of a hard-X-ray free-electron laser, the Linac Coherent Light Source (LCLS). Understanding how electrons in matter respond to ultra-intense X-ray radiation is essential for all applications. Here we reveal the nature of the electronic response in a free atom to unprecedented high-intensity, short-wavelength, high-fluence radiation (respectively 10 18  W cm −2 , 1.5–0.6 nm, ∼10 5  X-ray photons per Å 2 ). At this fluence, the neon target inevitably changes during the course of a single femtosecond-duration X-ray pulse—by sequentially ejecting electrons—to produce fully-stripped neon through absorption of six photons. Rapid photoejection of inner-shell electrons produces ‘hollow’ atoms and an intensity-induced X-ray transparency. Such transparency, due to the presence of inner-shell vacancies, can be induced in all atomic, molecular and condensed matter systems at high intensity. Quantitative comparison with theory allows us to extract LCLS fluence and pulse duration. Our successful modelling of X-ray/atom interactions using a straightforward rate equation approach augurs favourably for extension to complex systems. First strike from the LCLS The world's first X-ray free-electron laser — the Linac Coherent Light Source (LCLS) at SLAC National Accelerator Laboratory in Menlo Park, California — came online last year. It opened a new era for studies at the atomic level, including the prospect of single-shot imaging of complex nano-objects such as biological molecules. The results of one of the first user experiments carried out at the LCLS are presented in this issue. The new facility produces ultrashort (femtosecond) pulses of high-intensity X-rays at a wavelength of less than 1.5 nm. The experiment examined the electronic response of free neon atoms to such radiation. During a single X-ray pulse, the atoms sequentially ejected all their ten electrons to produce fully stripped neon — 'hollow' atoms that are X-ray transparent. The authors explain the observations and underlying mechanisms of electron stripping using a straightforward model, which bodes well for further studies of interactions of the X-rays with more complex systems. With the start-up of the first X-ray free-electron laser, a new era has begun in dynamical studies of atoms. Here the facility is used to study the fundamental nature of the electronic response in free neon atoms. During a sin
doi_str_mv 10.1038/nature09177
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P. ; Krässig, B. ; Li, Y. ; March, A. M. ; Pratt, S. T. ; Santra, R. ; Southworth, S. H. ; Rohringer, N. ; DiMauro, L. F. ; Doumy, G. ; Roedig, C. A. ; Berrah, N. ; Fang, L. ; Hoener, M. ; Bucksbaum, P. H. ; Cryan, J. P. ; Ghimire, S. ; Glownia, J. M. ; Reis, D. A. ; Bozek, J. D. ; Bostedt, C. ; Messerschmidt, M.</creator><creatorcontrib>Young, L. ; Kanter, E. P. ; Krässig, B. ; Li, Y. ; March, A. M. ; Pratt, S. T. ; Santra, R. ; Southworth, S. H. ; Rohringer, N. ; DiMauro, L. F. ; Doumy, G. ; Roedig, C. A. ; Berrah, N. ; Fang, L. ; Hoener, M. ; Bucksbaum, P. H. ; Cryan, J. P. ; Ghimire, S. ; Glownia, J. M. ; Reis, D. A. ; Bozek, J. D. ; Bostedt, C. ; Messerschmidt, M. ; Argonne National Lab. (ANL), Argonne, IL (United States)</creatorcontrib><description>An era of exploring the interactions of high-intensity, hard X-rays with matter has begun with the start-up of a hard-X-ray free-electron laser, the Linac Coherent Light Source (LCLS). Understanding how electrons in matter respond to ultra-intense X-ray radiation is essential for all applications. Here we reveal the nature of the electronic response in a free atom to unprecedented high-intensity, short-wavelength, high-fluence radiation (respectively 10 18  W cm −2 , 1.5–0.6 nm, ∼10 5  X-ray photons per Å 2 ). At this fluence, the neon target inevitably changes during the course of a single femtosecond-duration X-ray pulse—by sequentially ejecting electrons—to produce fully-stripped neon through absorption of six photons. Rapid photoejection of inner-shell electrons produces ‘hollow’ atoms and an intensity-induced X-ray transparency. Such transparency, due to the presence of inner-shell vacancies, can be induced in all atomic, molecular and condensed matter systems at high intensity. Quantitative comparison with theory allows us to extract LCLS fluence and pulse duration. Our successful modelling of X-ray/atom interactions using a straightforward rate equation approach augurs favourably for extension to complex systems. First strike from the LCLS The world's first X-ray free-electron laser — the Linac Coherent Light Source (LCLS) at SLAC National Accelerator Laboratory in Menlo Park, California — came online last year. It opened a new era for studies at the atomic level, including the prospect of single-shot imaging of complex nano-objects such as biological molecules. The results of one of the first user experiments carried out at the LCLS are presented in this issue. The new facility produces ultrashort (femtosecond) pulses of high-intensity X-rays at a wavelength of less than 1.5 nm. The experiment examined the electronic response of free neon atoms to such radiation. During a single X-ray pulse, the atoms sequentially ejected all their ten electrons to produce fully stripped neon — 'hollow' atoms that are X-ray transparent. The authors explain the observations and underlying mechanisms of electron stripping using a straightforward model, which bodes well for further studies of interactions of the X-rays with more complex systems. With the start-up of the first X-ray free-electron laser, a new era has begun in dynamical studies of atoms. Here the facility is used to study the fundamental nature of the electronic response in free neon atoms. During a single X-ray pulse, they sequentially eject all their ten electrons to produce fully stripped neon. 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(ANL), Argonne, IL (United States)</creatorcontrib><title>Femtosecond electronic response of atoms to ultra-intense X-rays</title><title>Nature</title><addtitle>Nature</addtitle><addtitle>Nature</addtitle><description>An era of exploring the interactions of high-intensity, hard X-rays with matter has begun with the start-up of a hard-X-ray free-electron laser, the Linac Coherent Light Source (LCLS). Understanding how electrons in matter respond to ultra-intense X-ray radiation is essential for all applications. Here we reveal the nature of the electronic response in a free atom to unprecedented high-intensity, short-wavelength, high-fluence radiation (respectively 10 18  W cm −2 , 1.5–0.6 nm, ∼10 5  X-ray photons per Å 2 ). At this fluence, the neon target inevitably changes during the course of a single femtosecond-duration X-ray pulse—by sequentially ejecting electrons—to produce fully-stripped neon through absorption of six photons. Rapid photoejection of inner-shell electrons produces ‘hollow’ atoms and an intensity-induced X-ray transparency. Such transparency, due to the presence of inner-shell vacancies, can be induced in all atomic, molecular and condensed matter systems at high intensity. Quantitative comparison with theory allows us to extract LCLS fluence and pulse duration. Our successful modelling of X-ray/atom interactions using a straightforward rate equation approach augurs favourably for extension to complex systems. First strike from the LCLS The world's first X-ray free-electron laser — the Linac Coherent Light Source (LCLS) at SLAC National Accelerator Laboratory in Menlo Park, California — came online last year. It opened a new era for studies at the atomic level, including the prospect of single-shot imaging of complex nano-objects such as biological molecules. The results of one of the first user experiments carried out at the LCLS are presented in this issue. The new facility produces ultrashort (femtosecond) pulses of high-intensity X-rays at a wavelength of less than 1.5 nm. The experiment examined the electronic response of free neon atoms to such radiation. During a single X-ray pulse, the atoms sequentially ejected all their ten electrons to produce fully stripped neon — 'hollow' atoms that are X-ray transparent. The authors explain the observations and underlying mechanisms of electron stripping using a straightforward model, which bodes well for further studies of interactions of the X-rays with more complex systems. With the start-up of the first X-ray free-electron laser, a new era has begun in dynamical studies of atoms. Here the facility is used to study the fundamental nature of the electronic response in free neon atoms. During a single X-ray pulse, they sequentially eject all their ten electrons to produce fully stripped neon. 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D. ; Bostedt, C. ; Messerschmidt, M.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c675t-af32f34038b61d161e23e20a22c2564c1c343a0dd1591122a2982274054abaea3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2010</creationdate><topic>639/766/119/1001</topic><topic>639/766/25</topic><topic>639/766/36</topic><topic>639/766/400/1106</topic><topic>ABSORPTION</topic><topic>Atomic and molecular physics</topic><topic>Atomic properties and interactions with photons</topic><topic>ATOMS</topic><topic>Auger effect and inner-shell excitation or ionization</topic><topic>Coherent light</topic><topic>Condensed matter</topic><topic>Electromagnetism; electron and ion optics</topic><topic>Electronics</topic><topic>ELECTRONS</topic><topic>Exact sciences and technology</topic><topic>Femtosecond</topic><topic>Fluence</topic><topic>FREE ELECTRON LASERS</topic><topic>Fundamental areas of phenomenology (including applications)</topic><topic>Humanities and Social Sciences</topic><topic>Infrared radiation</topic><topic>LIGHT SOURCES</topic><topic>LINEAR ACCELERATORS</topic><topic>Monte Carlo simulation</topic><topic>multidisciplinary</topic><topic>NEON</topic><topic>Nonlinear optics</topic><topic>Optics</topic><topic>PARTICLE ACCELERATORS</topic><topic>Photon interactions with atoms</topic><topic>PHOTONS</topic><topic>Physics</topic><topic>Properties</topic><topic>RADIATIONS</topic><topic>Science</topic><topic>Science (multidisciplinary)</topic><topic>START-UP</topic><topic>Studies</topic><topic>TARGETS</topic><topic>Ultrafast processes; optical pulse generation and pulse compression</topic><topic>VACANCIES</topic><topic>X-ray beams and x-ray optics</topic><topic>X-rays</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Young, L.</creatorcontrib><creatorcontrib>Kanter, E. P.</creatorcontrib><creatorcontrib>Krässig, B.</creatorcontrib><creatorcontrib>Li, Y.</creatorcontrib><creatorcontrib>March, A. M.</creatorcontrib><creatorcontrib>Pratt, S. T.</creatorcontrib><creatorcontrib>Santra, R.</creatorcontrib><creatorcontrib>Southworth, S. H.</creatorcontrib><creatorcontrib>Rohringer, N.</creatorcontrib><creatorcontrib>DiMauro, L. F.</creatorcontrib><creatorcontrib>Doumy, G.</creatorcontrib><creatorcontrib>Roedig, C. A.</creatorcontrib><creatorcontrib>Berrah, N.</creatorcontrib><creatorcontrib>Fang, L.</creatorcontrib><creatorcontrib>Hoener, M.</creatorcontrib><creatorcontrib>Bucksbaum, P. H.</creatorcontrib><creatorcontrib>Cryan, J. P.</creatorcontrib><creatorcontrib>Ghimire, S.</creatorcontrib><creatorcontrib>Glownia, J. M.</creatorcontrib><creatorcontrib>Reis, D. A.</creatorcontrib><creatorcontrib>Bozek, J. D.</creatorcontrib><creatorcontrib>Bostedt, C.</creatorcontrib><creatorcontrib>Messerschmidt, M.</creatorcontrib><creatorcontrib>Argonne National Lab. (ANL), Argonne, IL (United States)</creatorcontrib><collection>Pascal-Francis</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>Gale In Context: Middle School</collection><collection>ProQuest Central (Corporate)</collection><collection>Animal Behavior Abstracts</collection><collection>Bacteriology Abstracts (Microbiology B)</collection><collection>Calcium &amp; Calcified Tissue Abstracts</collection><collection>Chemoreception Abstracts</collection><collection>Nursing &amp; Allied Health Database</collection><collection>Ecology Abstracts</collection><collection>Entomology Abstracts (Full archive)</collection><collection>Environment Abstracts</collection><collection>Immunology Abstracts</collection><collection>Meteorological &amp; Geoastrophysical Abstracts</collection><collection>Neurosciences Abstracts</collection><collection>Nucleic Acids Abstracts</collection><collection>Oncogenes and Growth Factors Abstracts</collection><collection>Virology and AIDS Abstracts</collection><collection>Agricultural Science Collection</collection><collection>Health &amp; 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Aerospace Collection</collection><collection>Biotechnology and BioEngineering Abstracts</collection><collection>Environmental Science Database</collection><collection>Earth, Atmospheric &amp; Aquatic Science Database</collection><collection>Materials Science Collection</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest One Psychology</collection><collection>Engineering Collection</collection><collection>Environmental Science Collection</collection><collection>ProQuest Central Basic</collection><collection>University of Michigan</collection><collection>Genetics Abstracts</collection><collection>SIRS Editorial</collection><collection>Environment Abstracts</collection><collection>Computer and Information Systems Abstracts</collection><collection>Electronics &amp; Communications Abstracts</collection><collection>Engineered Materials Abstracts</collection><collection>Mechanical &amp; Transportation Engineering Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>ANTE: Abstracts in New Technology &amp; Engineering</collection><collection>Materials Research Database</collection><collection>ProQuest Computer Science Collection</collection><collection>Civil Engineering Abstracts</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Computer and Information Systems Abstracts – Academic</collection><collection>Computer and Information Systems Abstracts Professional</collection><collection>MEDLINE - Academic</collection><collection>OSTI.GOV</collection><jtitle>Nature</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Young, L.</au><au>Kanter, E. P.</au><au>Krässig, B.</au><au>Li, Y.</au><au>March, A. M.</au><au>Pratt, S. T.</au><au>Santra, R.</au><au>Southworth, S. H.</au><au>Rohringer, N.</au><au>DiMauro, L. F.</au><au>Doumy, G.</au><au>Roedig, C. A.</au><au>Berrah, N.</au><au>Fang, L.</au><au>Hoener, M.</au><au>Bucksbaum, P. H.</au><au>Cryan, J. P.</au><au>Ghimire, S.</au><au>Glownia, J. M.</au><au>Reis, D. A.</au><au>Bozek, J. D.</au><au>Bostedt, C.</au><au>Messerschmidt, M.</au><aucorp>Argonne National Lab. (ANL), Argonne, IL (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Femtosecond electronic response of atoms to ultra-intense X-rays</atitle><jtitle>Nature</jtitle><stitle>Nature</stitle><addtitle>Nature</addtitle><date>2010-07-01</date><risdate>2010</risdate><volume>466</volume><issue>7302</issue><spage>56</spage><epage>61</epage><pages>56-61</pages><issn>0028-0836</issn><eissn>1476-4687</eissn><coden>NATUAS</coden><abstract>An era of exploring the interactions of high-intensity, hard X-rays with matter has begun with the start-up of a hard-X-ray free-electron laser, the Linac Coherent Light Source (LCLS). Understanding how electrons in matter respond to ultra-intense X-ray radiation is essential for all applications. Here we reveal the nature of the electronic response in a free atom to unprecedented high-intensity, short-wavelength, high-fluence radiation (respectively 10 18  W cm −2 , 1.5–0.6 nm, ∼10 5  X-ray photons per Å 2 ). At this fluence, the neon target inevitably changes during the course of a single femtosecond-duration X-ray pulse—by sequentially ejecting electrons—to produce fully-stripped neon through absorption of six photons. Rapid photoejection of inner-shell electrons produces ‘hollow’ atoms and an intensity-induced X-ray transparency. Such transparency, due to the presence of inner-shell vacancies, can be induced in all atomic, molecular and condensed matter systems at high intensity. Quantitative comparison with theory allows us to extract LCLS fluence and pulse duration. Our successful modelling of X-ray/atom interactions using a straightforward rate equation approach augurs favourably for extension to complex systems. First strike from the LCLS The world's first X-ray free-electron laser — the Linac Coherent Light Source (LCLS) at SLAC National Accelerator Laboratory in Menlo Park, California — came online last year. It opened a new era for studies at the atomic level, including the prospect of single-shot imaging of complex nano-objects such as biological molecules. The results of one of the first user experiments carried out at the LCLS are presented in this issue. The new facility produces ultrashort (femtosecond) pulses of high-intensity X-rays at a wavelength of less than 1.5 nm. The experiment examined the electronic response of free neon atoms to such radiation. During a single X-ray pulse, the atoms sequentially ejected all their ten electrons to produce fully stripped neon — 'hollow' atoms that are X-ray transparent. The authors explain the observations and underlying mechanisms of electron stripping using a straightforward model, which bodes well for further studies of interactions of the X-rays with more complex systems. With the start-up of the first X-ray free-electron laser, a new era has begun in dynamical studies of atoms. Here the facility is used to study the fundamental nature of the electronic response in free neon atoms. During a single X-ray pulse, they sequentially eject all their ten electrons to produce fully stripped neon. The authors explain this electron-stripping in a straightforward model, auguring favourably for further studies of interactions of X-rays with more complex systems.</abstract><cop>London</cop><pub>Nature Publishing Group UK</pub><pmid>20596013</pmid><doi>10.1038/nature09177</doi><tpages>6</tpages></addata></record>
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subjects 639/766/119/1001
639/766/25
639/766/36
639/766/400/1106
ABSORPTION
Atomic and molecular physics
Atomic properties and interactions with photons
ATOMS
Auger effect and inner-shell excitation or ionization
Coherent light
Condensed matter
Electromagnetism
electron and ion optics
Electronics
ELECTRONS
Exact sciences and technology
Femtosecond
Fluence
FREE ELECTRON LASERS
Fundamental areas of phenomenology (including applications)
Humanities and Social Sciences
Infrared radiation
LIGHT SOURCES
LINEAR ACCELERATORS
Monte Carlo simulation
multidisciplinary
NEON
Nonlinear optics
Optics
PARTICLE ACCELERATORS
Photon interactions with atoms
PHOTONS
Physics
Properties
RADIATIONS
Science
Science (multidisciplinary)
START-UP
Studies
TARGETS
Ultrafast processes
optical pulse generation and pulse compression
VACANCIES
X-ray beams and x-ray optics
X-rays
title Femtosecond electronic response of atoms to ultra-intense X-rays
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