1
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Wicks JK, Singh S, Millot M, Fratanduono DE, Coppari F, Gorman MG, Ye Z, Rygg JR, Hari A, Eggert JH, Duffy TS, Smith RF. B1-B2 transition in shock-compressed MgO. SCIENCE ADVANCES 2024; 10:eadk0306. [PMID: 38848357 PMCID: PMC11160462 DOI: 10.1126/sciadv.adk0306] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 07/29/2023] [Accepted: 05/02/2024] [Indexed: 06/09/2024]
Abstract
Magnesium oxide (MgO) is a major component of the Earth's mantle and is expected to play a similar role in the mantles of large rocky exoplanets. At extreme pressures, MgO transitions from the NaCl B1 crystal structure to a CsCl B2 structure, which may have implications for exoplanetary deep mantle dynamics. In this study, we constrain the phase diagram of MgO with laser-compression along the shock Hugoniot, with simultaneous measurements of crystal structure, density, pressure, and temperature. We identify the B1 to B2 phase transition between 397 and 425 gigapascal (around 9700 kelvin), in agreement with recent theory that accounts for phonon anharmonicity. From 425 to 493 gigapascal, we observe a mixed-phase region of B1 and B2 coexistence. The transformation follows the Watanabe-Tokonami-Morimoto mechanism. Our data are consistent with B2-liquid coexistence above 500 gigapascal and complete melting at 634 gigapascal. This study bridges the gap between previous theoretical and experimental studies, providing insights into the timescale of this phase transition.
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Affiliation(s)
- June K. Wicks
- Dept. of Earth & Planetary Sciences, Johns Hopkins University, Baltimore, MD 21218, USA
| | - Saransh Singh
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - Marius Millot
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | | | - Federica Coppari
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - Martin G. Gorman
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - Zixuan Ye
- Dept. of Earth & Planetary Sciences Div. of Mechanical Engineering, Johns Hopkins University, Baltimore, MD 21218, USA
| | - J. Ryan Rygg
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY 14623, USA
- Dept. of Mechanical Engineering and Dept. of Physics and Astronomy, University of Rochester, Rochester, NY 14623, USA
| | - Anirudh Hari
- Dept. of Earth & Planetary Sciences Div. of Mechanical Engineering, Johns Hopkins University, Baltimore, MD 21218, USA
- Dept. of Materials Science and Engineering and PULSE Institute, Stanford University, Stanford, CA 94305, USA
- SLAC National Accelerator Laboratory, Menlo Park, CA 94025, USA
| | - Jon H. Eggert
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - Thomas S. Duffy
- Dept. of Geosciences, Princeton University, Princeton, NJ 08544, USA
| | - Raymond F. Smith
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
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2
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Werellapatha K, Palmer NE, Gorman MG, Bernier JV, Bhandarkar NS, Bradley DK, Braun DG, Bruhn M, Carpenter A, Celliers PM, Coppari F, Dayton M, Durand C, Eggert JH, Ferguson B, Heidl B, Heinbockel C, Heredia R, Huckins J, Hurd E, Hsing W, Krauland CM, Lazicki AE, Kalantar D, Kehl J, Killebrew K, Masters N, Millot M, Nagel SR, Petre RB, Ping Y, Polsin DN, Singh S, Stan CV, Swift D, Tabimina J, Thomas A, Zobrist T, Benedetti LR. Time-resolved X-ray diffraction diagnostic development for the National Ignition Facility. THE REVIEW OF SCIENTIFIC INSTRUMENTS 2024; 95:013903. [PMID: 38236087 DOI: 10.1063/5.0161343] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/09/2023] [Accepted: 11/23/2023] [Indexed: 01/19/2024]
Abstract
We present the development of an experimental platform that can collect four frames of x-ray diffraction data along a single line of sight during laser-driven, dynamic-compression experiments at the National Ignition Facility. The platform is comprised of a diagnostic imager built around ultrafast sensors with a 2-ns integration time, a custom target assembly that serves also to shield the imager, and a 10-ns duration, quasi-monochromatic x-ray source produced by laser-generated plasma. We demonstrate the performance with diffraction data for Pb ramp compressed to 150 GPa and illuminated by a Ge x-ray source that produces ∼7 × 1011, 10.25-keV photons/ns at the 400 μm diameter sample.
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Affiliation(s)
- K Werellapatha
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - N E Palmer
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - M G Gorman
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J V Bernier
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - N S Bhandarkar
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D K Bradley
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D G Braun
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - M Bruhn
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - A Carpenter
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - P M Celliers
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - F Coppari
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - M Dayton
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - C Durand
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J H Eggert
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - B Ferguson
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - B Heidl
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - C Heinbockel
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - R Heredia
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J Huckins
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - E Hurd
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - W Hsing
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - C M Krauland
- General Atomics, San Diego, California 92121, USA
| | - A E Lazicki
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D Kalantar
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J Kehl
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - K Killebrew
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - N Masters
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - M Millot
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - S R Nagel
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - R B Petre
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - Y Ping
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D N Polsin
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - S Singh
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - C V Stan
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D Swift
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J Tabimina
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - A Thomas
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - T Zobrist
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - L R Benedetti
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
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3
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Sio H, Krygier A, Braun DG, Rudd RE, Bonev SA, Coppari F, Millot M, Fratanduono DE, Bhandarkar N, Bitter M, Bradley DK, Efthimion PC, Eggert JH, Gao L, Hill KW, Hood R, Hsing W, Izumi N, Kemp G, Kozioziemski B, Landen OL, Le Galloudec K, Lockard TE, Mackinnon A, McNaney JM, Ose N, Park HS, Remington BA, Schneider MB, Stoupin S, Thorn DB, Vonhof S, Wu CJ, Ping Y. Extended X-ray absorption fine structure of dynamically-compressed copper up to 1 terapascal. Nat Commun 2023; 14:7046. [PMID: 37949859 PMCID: PMC10638371 DOI: 10.1038/s41467-023-42684-7] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 05/17/2023] [Accepted: 10/18/2023] [Indexed: 11/12/2023] Open
Abstract
Large laser facilities have recently enabled material characterization at the pressures of Earth and Super-Earth cores. However, the temperature of the compressed materials has been largely unknown, or solely relied on models and simulations, due to lack of diagnostics under these challenging conditions. Here, we report on temperature, density, pressure, and local structure of copper determined from extended x-ray absorption fine structure and velocimetry up to 1 Terapascal. These results nearly double the highest pressure at which extended x-ray absorption fine structure has been reported in any material. In this work, the copper temperature is unexpectedly found to be much higher than predicted when adjacent to diamond layer(s), demonstrating the important influence of the sample environment on the thermal state of materials; this effect may introduce additional temperature uncertainties in some previous experiments using diamond and provides new guidance for future experimental design.
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Affiliation(s)
- H Sio
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA.
| | - A Krygier
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - D G Braun
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - R E Rudd
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - S A Bonev
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - F Coppari
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - M Millot
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - D E Fratanduono
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - N Bhandarkar
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - M Bitter
- Princeton Plasma Physics Laboratory, Princeton University, 100 Stellarator Rd, Princeton, NJ, 08540, USA
| | - D K Bradley
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - P C Efthimion
- Princeton Plasma Physics Laboratory, Princeton University, 100 Stellarator Rd, Princeton, NJ, 08540, USA
| | - J H Eggert
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - L Gao
- Princeton Plasma Physics Laboratory, Princeton University, 100 Stellarator Rd, Princeton, NJ, 08540, USA
| | - K W Hill
- Princeton Plasma Physics Laboratory, Princeton University, 100 Stellarator Rd, Princeton, NJ, 08540, USA
| | - R Hood
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - W Hsing
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - N Izumi
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - G Kemp
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - B Kozioziemski
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - O L Landen
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - K Le Galloudec
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - T E Lockard
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - A Mackinnon
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - J M McNaney
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - N Ose
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - H-S Park
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - B A Remington
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - M B Schneider
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - S Stoupin
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - D B Thorn
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - S Vonhof
- General Atomics, 3550 General Atomics Court, San Diego, CA, 92121, USA
| | - C J Wu
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
| | - Y Ping
- Lawrence Livermore National Laboratory, 7000 East Ave, Livermore, CA, 94550, USA
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4
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Liu C, Errea I, Ding C, Pickard C, Conway LJ, Monserrat B, Fang YW, Lu Q, Sun J, Boronat J, Cazorla C. Excitonic insulator to superconductor phase transition in ultra-compressed helium. Nat Commun 2023; 14:4458. [PMID: 37491484 PMCID: PMC10368699 DOI: 10.1038/s41467-023-40240-x] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 01/31/2023] [Accepted: 07/13/2023] [Indexed: 07/27/2023] Open
Abstract
Helium, the second most abundant element in the universe, exhibits an extremely large electronic band gap of about 20 eV at ambient pressures. While the metallization pressure of helium has been accurately determined, thus far little attention has been paid to the specific mechanisms driving the band-gap closure and electronic properties of this quantum crystal in the terapascal regime (1 TPa = 10 Mbar). Here, we employ density functional theory and many-body perturbation calculations to fill up this knowledge gap. It is found that prior to reaching metallicity helium becomes an excitonic insulator (EI), an exotic state of matter in which electrostatically bound electron-hole pairs may form spontaneously. Furthermore, we predict metallic helium to be a superconductor with a critical temperature of ≈ 20 K just above its metallization pressure and of ≈ 70 K at 100 TPa. These unforeseen phenomena may be critical for improving our fundamental understanding and modeling of celestial bodies.
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Affiliation(s)
- Cong Liu
- Departament de Física, Universitat Politècnica de Catalunya, Campus Nord B4-B5, Barcelona, 08034, Spain
| | - Ion Errea
- Fisika Aplikatua Saila, Gipuzkoako Ingeniaritza Eskola, University of the Basque Country (UPV/EHU), Europa Plaza 1, 20018, Donostia/San Sebastián, Spain
- Centro de Física de Materiales (CSIC-UPV/EHU), Manuel de Lardizabal pasealekua 5, 20018, Donostia/San Sebastián, Spain
- Donostia International Physics Center (DIPC), Manuel de Lardizabal pasealekua 4, 20018, Donostia/San Sebastián, Spain
| | - Chi Ding
- National Laboratory of Solid State Microstructures, School of Physics and Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing, 210093, China
| | - Chris Pickard
- Department of Materials Science and Metallurgy, University of Cambridge, Cambridge, CB30FS, UK
- Advanced Institute for Materials Research, Tohoku University, Sendai, 980-8577, Japan
| | - Lewis J Conway
- Department of Materials Science and Metallurgy, University of Cambridge, Cambridge, CB30FS, UK
- Advanced Institute for Materials Research, Tohoku University, Sendai, 980-8577, Japan
| | - Bartomeu Monserrat
- Department of Materials Science and Metallurgy, University of Cambridge, Cambridge, CB30FS, UK
- Cavendish Laboratory, University of Cambridge, Cambridge, CB30HE, UK
| | - Yue-Wen Fang
- Fisika Aplikatua Saila, Gipuzkoako Ingeniaritza Eskola, University of the Basque Country (UPV/EHU), Europa Plaza 1, 20018, Donostia/San Sebastián, Spain
- Centro de Física de Materiales (CSIC-UPV/EHU), Manuel de Lardizabal pasealekua 5, 20018, Donostia/San Sebastián, Spain
| | - Qing Lu
- National Laboratory of Solid State Microstructures, School of Physics and Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing, 210093, China
| | - Jian Sun
- National Laboratory of Solid State Microstructures, School of Physics and Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing, 210093, China.
| | - Jordi Boronat
- Departament de Física, Universitat Politècnica de Catalunya, Campus Nord B4-B5, Barcelona, 08034, Spain
| | - Claudio Cazorla
- Departament de Física, Universitat Politècnica de Catalunya, Campus Nord B4-B5, Barcelona, 08034, Spain.
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5
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Gong X, Polsin DN, Paul R, Henderson BJ, Eggert JH, Coppari F, Smith RF, Rygg JR, Collins GW. X-Ray Diffraction of Ramp-Compressed Silicon to 390 GPa. PHYSICAL REVIEW LETTERS 2023; 130:076101. [PMID: 36867795 DOI: 10.1103/physrevlett.130.076101] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/10/2022] [Revised: 11/15/2022] [Accepted: 01/19/2023] [Indexed: 06/18/2023]
Abstract
Silicon (Si) exhibits a rich collection of phase transitions under ambient-temperature isothermal and shock compression. This report describes in situ diffraction measurements of ramp-compressed Si between 40 and 389 GPa. Angle-dispersive x-ray scattering reveals that Si assumes an hexagonal close-packed (hcp) structure between 40 and 93 GPa and, at higher pressure, a face-centered cubic structure that persists to at least 389 GPa, the highest pressure for which the crystal structure of Si has been investigated. The range of hcp stability extends to higher pressures and temperatures than predicted by theory.
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Affiliation(s)
- X Gong
- University of Rochester Laboratory for Laser Energetics, Rochester, New York 14623-1299, USA
- Department of Mechanical Engineering, University of Rochester, Rochester, New York 14627-0132, USA
| | - D N Polsin
- University of Rochester Laboratory for Laser Energetics, Rochester, New York 14623-1299, USA
- Department of Mechanical Engineering, University of Rochester, Rochester, New York 14627-0132, USA
| | - R Paul
- University of Rochester Laboratory for Laser Energetics, Rochester, New York 14623-1299, USA
- Department of Mechanical Engineering, University of Rochester, Rochester, New York 14627-0132, USA
| | - B J Henderson
- University of Rochester Laboratory for Laser Energetics, Rochester, New York 14623-1299, USA
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627-0171, USA
| | - J H Eggert
- Lawrence Livermore National Laboratory, Livermore, California 94550-9234, USA
| | - F Coppari
- Lawrence Livermore National Laboratory, Livermore, California 94550-9234, USA
| | - R F Smith
- Lawrence Livermore National Laboratory, Livermore, California 94550-9234, USA
| | - J R Rygg
- University of Rochester Laboratory for Laser Energetics, Rochester, New York 14623-1299, USA
- Department of Mechanical Engineering, University of Rochester, Rochester, New York 14627-0132, USA
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627-0171, USA
| | - G W Collins
- University of Rochester Laboratory for Laser Energetics, Rochester, New York 14623-1299, USA
- Department of Mechanical Engineering, University of Rochester, Rochester, New York 14627-0132, USA
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627-0171, USA
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6
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Celliers PM, Millot M. Imaging velocity interferometer system for any reflector (VISAR) diagnostics for high energy density sciences. THE REVIEW OF SCIENTIFIC INSTRUMENTS 2023; 94:011101. [PMID: 36725591 DOI: 10.1063/5.0123439] [Citation(s) in RCA: 4] [Impact Index Per Article: 4.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/30/2022] [Accepted: 11/28/2022] [Indexed: 06/18/2023]
Abstract
Two variants of optical imaging velocimetry, specifically the one-dimensional streaked line-imaging and the two-dimensional time-resolved area-imaging versions of the Velocity Interferometer System for Any Reflector (VISAR), have become important diagnostics in high energy density sciences, including inertial confinement fusion and dynamic compression of condensed matter. Here, we give a brief review of the historical development of these techniques, then describe the current implementations at major high energy density (HED) facilities worldwide, including the OMEGA Laser Facility and the National Ignition Facility. We illustrate the versatility and power of these techniques by reviewing diverse applications of imaging VISARs for gas-gun and laser-driven dynamic compression experiments for materials science, shock physics, condensed matter physics, chemical physics, plasma physics, planetary science and astronomy, as well as a broad range of HED experiments and laser-driven inertial confinement fusion research.
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Affiliation(s)
- Peter M Celliers
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - Marius Millot
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
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7
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Chin DA, Nilson PM, Mastrosimone D, Guy D, Ruby JJ, Bishel DT, Seely JF, Coppari F, Ping Y, Rygg JR, Collins GW. High-resolution x-ray spectrometer for x-ray absorption fine structure spectroscopy. THE REVIEW OF SCIENTIFIC INSTRUMENTS 2023; 94:013101. [PMID: 36725595 DOI: 10.1063/5.0125712] [Citation(s) in RCA: 1] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/13/2022] [Accepted: 12/04/2022] [Indexed: 05/26/2023]
Abstract
Two extended x-ray absorption fine structure flat crystal x-ray spectrometers (EFX's) were designed and built for high-resolution x-ray spectroscopy over a large energy range with flexible, on-shot energy dispersion calibration capabilities. The EFX uses a flat silicon [111] crystal in the reflection geometry as the energy dispersive optic covering the energy range of 6.3-11.4 keV and achieving a spectral resolution of 4.5 eV with a source size of 50 μm at 7.2 keV. A shot-to-shot configurable calibration filter pack and Bayesian inference routine were used to constrain the energy dispersion relation to within ±3 eV. The EFX was primarily designed for x-ray absorption fine structure (XAFS) spectroscopy and provides significant improvement to the Laboratory for Laser Energetics' OMEGA-60 XAFS experimental platform. The EFX is capable of performing extended XAFS measurements of multiple absorption edges simultaneously on metal alloys and x-ray absorption near-edge spectroscopy to measure the electron structure of compressed 3d transition metals.
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Affiliation(s)
- D A Chin
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA
| | - P M Nilson
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - D Mastrosimone
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - D Guy
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623-1299, USA
| | - J J Ruby
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D T Bishel
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA
| | - J F Seely
- Syntek Technologies, Fairfax, Virginia 22031, USA
| | - F Coppari
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - Y Ping
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J R Rygg
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA
| | - G W Collins
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA
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8
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Werellapatha K, Hall GN, Krauland C, Krygier A, Bhandarkar N, Bradley DK, Coppari F, Gorman MG, Heinbockel C, Kemp GE, Khan SF, Lazicki A, Masters N, May MJ, Nagel SR, Palmer NE, Eggert JH, Benedetti LR. Optimized x-ray emission from 10 ns long germanium x-ray sources at the National Ignition Facility. THE REVIEW OF SCIENTIFIC INSTRUMENTS 2022; 93:123902. [PMID: 36586918 DOI: 10.1063/5.0106696] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/29/2022] [Accepted: 11/13/2022] [Indexed: 06/17/2023]
Abstract
This study investigates methods to optimize quasi-monochromatic, ∼10 ns long x-ray sources (XRS) for time-resolved x-ray diffraction measurements of phase transitions during dynamic laser compression measurements at the National Ignition Facility (NIF). To support this, we produce continuous and pulsed XRS by irradiating a Ge foil with NIF lasers to achieve an intensity of 2 × 1015 W/cm2, optimizing the laser-to-x-ray conversion efficiency. Our x-ray source is dominated by Ge He-α line emission. We discuss methods to optimize the source to maintain a uniform XRS for ∼10 ns, mitigating cold plasma and higher energy x-ray emission lines.
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Affiliation(s)
- K Werellapatha
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - G N Hall
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - C Krauland
- General Atomics, San Diego, California 92121, USA
| | - A Krygier
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - N Bhandarkar
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D K Bradley
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - F Coppari
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - M G Gorman
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - C Heinbockel
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - G E Kemp
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - S F Khan
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - A Lazicki
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - N Masters
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - M J May
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - S R Nagel
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - N E Palmer
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J H Eggert
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - L R Benedetti
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
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9
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Structural complexity in ramp-compressed sodium to 480 GPa. Nat Commun 2022; 13:2534. [PMID: 35534461 PMCID: PMC9085792 DOI: 10.1038/s41467-022-29813-4] [Citation(s) in RCA: 4] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 06/29/2021] [Accepted: 03/30/2022] [Indexed: 11/09/2022] Open
Abstract
AbstractThe properties of all materials at one atmosphere of pressure are controlled by the configurations of their valence electrons. At extreme pressures, neighboring atoms approach so close that core-electron orbitals overlap, and theory predicts the emergence of unusual quantum behavior. We ramp-compress monovalent elemental sodium, a prototypical metal at ambient conditions, to nearly 500 GPa (5 million atmospheres). The 7-fold increase of density brings the interatomic distance to 1.74 Å well within the initial 2.03 Å of the Na+ ionic diameter, and squeezes the valence electrons into the interstitial voids suggesting the formation of an electride phase. The laser-driven compression results in pressure-driven melting and recrystallization in a billionth of a second. In situ x-ray diffraction reveals a series of unexpected phase transitions upon recrystallization, and optical reflectivity measurements show a precipitous decrease throughout the liquid and solid phases, where the liquid is predicted to have electronic localization. These data reveal the presence of a rich, temperature-driven polymorphism where core electron overlap is thought to stabilize the formation of peculiar electride states.
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10
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Kim D, Smith RF, Ocampo IK, Coppari F, Marshall MC, Ginnane MK, Wicks JK, Tracy SJ, Millot M, Lazicki A, Rygg JR, Eggert JH, Duffy TS. Structure and density of silicon carbide to 1.5 TPa and implications for extrasolar planets. Nat Commun 2022; 13:2260. [PMID: 35477934 PMCID: PMC9046200 DOI: 10.1038/s41467-022-29762-y] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 07/09/2021] [Accepted: 03/16/2022] [Indexed: 11/10/2022] Open
Abstract
There has been considerable recent interest in the high-pressure behavior of silicon carbide, a potential major constituent of carbon-rich exoplanets. In this work, the atomic-level structure of SiC was determined through in situ X-ray diffraction under laser-driven ramp compression up to 1.5 TPa; stresses more than seven times greater than previous static and shock data. Here we show that the B1-type structure persists over this stress range and we have constrained its equation of state (EOS). Using this data we have determined the first experimentally based mass-radius curves for a hypothetical pure SiC planet. Interior structure models are constructed for planets consisting of a SiC-rich mantle and iron-rich core. Carbide planets are found to be ~10% less dense than corresponding terrestrial planets.
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Affiliation(s)
- D Kim
- Department of Geosciences, Princeton University, Princeton, NJ, USA.
| | - R F Smith
- Lawrence Livermore National Laboratory, Livermore, CA, USA
| | - I K Ocampo
- Department of Geosciences, Princeton University, Princeton, NJ, USA
| | - F Coppari
- Lawrence Livermore National Laboratory, Livermore, CA, USA
| | - M C Marshall
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - M K Ginnane
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - J K Wicks
- Department of Earth & Planetary Sciences, Johns Hopkins University, Baltimore, MD, USA
| | - S J Tracy
- Earth and Planets Laboratory, Carnegie Institution for Science, Washington, DC, USA
| | - M Millot
- Lawrence Livermore National Laboratory, Livermore, CA, USA
| | - A Lazicki
- Lawrence Livermore National Laboratory, Livermore, CA, USA
| | - J R Rygg
- Laboratory for Laser Energetics, University of Rochester, Rochester, NY, USA
| | - J H Eggert
- Lawrence Livermore National Laboratory, Livermore, CA, USA
| | - T S Duffy
- Department of Geosciences, Princeton University, Princeton, NJ, USA
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11
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Kraus RG, Hemley RJ, Ali SJ, Belof JL, Benedict LX, Bernier J, Braun D, Cohen RE, Collins GW, Coppari F, Desjarlais MP, Fratanduono D, Hamel S, Krygier A, Lazicki A, Mcnaney J, Millot M, Myint PC, Newman MG, Rygg JR, Sterbentz DM, Stewart ST, Stixrude L, Swift DC, Wehrenberg C, Eggert JH. Measuring the melting curve of iron at super-Earth core conditions. Science 2022; 375:202-205. [PMID: 35025665 DOI: 10.1126/science.abm1472] [Citation(s) in RCA: 6] [Impact Index Per Article: 3.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/03/2022]
Abstract
The discovery of more than 4500 extrasolar planets has created a need for modeling their interior structure and dynamics. Given the prominence of iron in planetary interiors, we require accurate and precise physical properties at extreme pressure and temperature. A first-order property of iron is its melting point, which is still debated for the conditions of Earth’s interior. We used high-energy lasers at the National Ignition Facility and in situ x-ray diffraction to determine the melting point of iron up to 1000 gigapascals, three times the pressure of Earth’s inner core. We used this melting curve to determine the length of dynamo action during core solidification to the hexagonal close-packed (hcp) structure. We find that terrestrial exoplanets with four to six times Earth’s mass have the longest dynamos, which provide important shielding against cosmic radiation.
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Affiliation(s)
- Richard G Kraus
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - Russell J Hemley
- Departments of Physics, Chemistry, and Earth and Environmental Sciences, University of Illinois at Chicago, Chicago, IL 60607, USA
| | - Suzanne J Ali
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - Jonathan L Belof
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - Lorin X Benedict
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - Joel Bernier
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - Dave Braun
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - R E Cohen
- Earth and Planets Laboratory, Carnegie Institution for Science, Washington, DC 20015, USA
| | - Gilbert W Collins
- Department of Mechanical Engineering, Department of Physics and Astronomy, and Laboratory for Laser Energetics, University of Rochester, Rochester, NY 14627, USA
| | - Federica Coppari
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | | | | | - Sebastien Hamel
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - Andy Krygier
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - Amy Lazicki
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - James Mcnaney
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - Marius Millot
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - Philip C Myint
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - Matthew G Newman
- Division of Engineering and Applied Science, California Institute of Technology, Pasadena, CA 91125, USA
| | - James R Rygg
- Department of Mechanical Engineering, Department of Physics and Astronomy, and Laboratory for Laser Energetics, University of Rochester, Rochester, NY 14627, USA
| | - Dane M Sterbentz
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - Sarah T Stewart
- Department of Earth and Planetary Sciences, University of California Davis, Davis, CA 95616, USA
| | - Lars Stixrude
- Department of Earth, Planetary, and Space Sciences, University of California Los Angeles, Los Angeles, CA 90095, USA
| | - Damian C Swift
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - Chris Wehrenberg
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - Jon H Eggert
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
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12
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McMahon MI. Probing extreme states of matter using ultra-intense x-ray radiation. JOURNAL OF PHYSICS. CONDENSED MATTER : AN INSTITUTE OF PHYSICS JOURNAL 2021; 34:043001. [PMID: 33725673 DOI: 10.1088/1361-648x/abef26] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/29/2020] [Accepted: 03/16/2021] [Indexed: 06/12/2023]
Abstract
Extreme states of matter, that is, matter at extremes of density (pressure) and temperature, can be created in the laboratory either statically or dynamically. In the former, the pressure-temperature state can be maintained for relatively long periods of time, but the sample volume is necessarily extremely small. When the extreme states are generated dynamically, the sample volumes can be larger, but the pressure-temperature conditions are maintained for only short periods of time (ps toμs). In either case, structural information can be obtained from the extreme states by the use of x-ray scattering techniques, but the x-ray beam must be extremely intense in order to obtain sufficient signal from the extremely-small or short-lived sample. In this article I describe the use of x-ray diffraction at synchrotrons and XFELs to investigate how crystal structures evolve as a function of density and temperature. After a brief historical introduction, I describe the developments made at the Synchrotron Radiation Source in the 1990s which enabled the almost routine determination of crystal structure at high pressures, while also revealing that the structural behaviour of materials was much more complex than previously believed. I will then describe how these techniques are used at the current generation of synchrotron and XFEL sources, and then discuss how they might develop further in the future at the next generation of x-ray lightsources.
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Affiliation(s)
- M I McMahon
- SUPA, School of Physics and Astronomy, and Centre for Science at Extreme Conditions, The University of Edinburgh, Peter Guthrie Tait Road, Edinburgh, EH9 3FD, United Kingdom
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13
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Chen XH, Xue T, Tan BZ, Li XY, Li J. Iterative diffraction pattern retrieval from a single focal construct geometry image. J Appl Crystallogr 2021. [DOI: 10.1107/s1600576721009626] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/10/2022] Open
Abstract
Understanding the crystal structure of materials under extreme conditions of pressure and temperature has been revolutionized by major advances in laser-driven dynamic compression and in situ X-ray diffraction (XRD) technology. Instead of the well known Debye–Scherrer configuration, the focal construct geometry (FCG) was introduced to produce high-intensity diffraction data from laser-based in situ XRD experiments without increasing the amount of laser energy, but the resulting reflections suffered from profoundly asymmetrical broadening, leading to inaccuracy in determination of the crystal structure. Inspired by fast-neutron energy spectrum measurements, proposed here is an iterative retrieval method for recovering diffraction data from a single FCG image. This iterative algorithm restores both the peak shape and relative intensity with rapid convergence and requires no prior knowledge about the expected diffraction pattern, allowing the FCG to increase the in situ XRD intensity while simultaneously preserving the angular resolution. The feasibility and validity of the method are shown by successful recovery of the diffraction pattern from both a single simulated FCG image and a single laser-based nanosecond XRD measurement.
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14
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Kraus RG, Coppari F, Fratanduono DE, Smith RF, Lazicki A, Wehrenberg C, Eggert JH, Rygg JR, Collins GW. Melting of Tantalum at Multimegabar Pressures on the Nanosecond Timescale. PHYSICAL REVIEW LETTERS 2021; 126:255701. [PMID: 34241515 DOI: 10.1103/physrevlett.126.255701] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 02/12/2021] [Accepted: 05/05/2021] [Indexed: 06/13/2023]
Abstract
Tantalum was once thought to be the canonical bcc metal, but is now predicted to transition to the Pnma phase at the high pressures and temperatures expected along the principal Hugoniot. Furthermore, there remains a significant discrepancy between a number of static diamond anvil cell experiments and gas gun experiments in the measured melt temperatures at high pressures. Our in situ x-ray diffraction experiments on shock compressed tantalum show that it does not transition to the Pnma phase or other candidate phases at high pressure. We observe incipient melting at approximately 254±15 GPa and complete melting by 317±10 GPa. These transition pressures from the nanosecond experiments presented here are consistent with what can be inferred from microsecond gas gun sound velocity measurements. Furthermore, the observation of a coexistence region on the Hugoniot implies the lack of significant kinetically controlled deviation from equilibrium behavior. Consequently, we find that kinetics of phase transitions cannot be used to explain the discrepancy between static and dynamic measurements of the tantalum melt curve. Using available high pressure thermodynamic data for tantalum and our measurements of the incipient and complete melting transition pressures, we are able to infer a melting temperature 8070_{-750}^{+1250} K at 254±15 GPa, which is consistent with ambient and a recent static high pressure melt curve measurement.
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Affiliation(s)
- R G Kraus
- Physics Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - F Coppari
- Physics Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D E Fratanduono
- Physics Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - R F Smith
- Physics Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - A Lazicki
- Physics Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - C Wehrenberg
- Physics Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J H Eggert
- Physics Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J R Rygg
- Laboratory for Laser Energetics, and Departments of Mechanical Engineering and Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA
| | - G W Collins
- Laboratory for Laser Energetics, and Departments of Mechanical Engineering and Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA
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15
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Fratanduono DE, Millot M, Braun DG, Ali SJ, Fernandez-Pañella A, Seagle CT, Davis JP, Brown JL, Akahama Y, Kraus RG, Marshall MC, Smith RF, O’Bannon EF, McNaney JM, Eggert JH. Establishing gold and platinum standards to 1 terapascal using shockless compression. Science 2021; 372:1063-1068. [DOI: 10.1126/science.abh0364] [Citation(s) in RCA: 24] [Impact Index Per Article: 8.0] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 02/11/2021] [Accepted: 04/14/2021] [Indexed: 11/02/2022]
Affiliation(s)
| | - M. Millot
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - D. G. Braun
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - S. J. Ali
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | | | - C. T. Seagle
- Sandia National Laboratories, Albuquerque, NM 87185-1195, USA
| | - J.-P. Davis
- Sandia National Laboratories, Albuquerque, NM 87185-1195, USA
| | - J. L. Brown
- Sandia National Laboratories, Albuquerque, NM 87185-1195, USA
| | - Y. Akahama
- Graduate School of Material Science, University of Hyogo, 3-2-1 Kouto, Kamigohri 678-1297, Japan
| | - R. G. Kraus
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - M. C. Marshall
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - R. F. Smith
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - E. F. O’Bannon
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - J. M. McNaney
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
| | - J. H. Eggert
- Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
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16
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Werellapatha K, Hall GN, Coppari F, Kemp GE, Palmer NE, Krauland C, Khan SF, Lazicki A, Gorman MG, Nagel SR, Heinbockel C, Bhandarkar N, Masters N, Bradley DK, Eggert JH, Benedetti LR. Long duration x-ray source development for x-ray diffraction at the National Ignition Facility. THE REVIEW OF SCIENTIFIC INSTRUMENTS 2021; 92:053904. [PMID: 34243269 DOI: 10.1063/5.0043677] [Citation(s) in RCA: 3] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/10/2021] [Accepted: 04/16/2021] [Indexed: 06/13/2023]
Abstract
We present the results of experiments to produce a 10 ns-long, quasi-monochromatic x-ray source. This effort is needed to support time-resolved x-ray diffraction (XRDt) measurements of phase transitions during laser-driven dynamic compression experiments at the National Ignition Facility. To record XRDt of phase transitions as they occur, we use high-speed (∼1 ns) gated hybrid CMOS detectors, which record multiple frames of data over a timescale of a few to tens of ns. Consequently, to make effective use of these imagers, XRDt needs the x-ray source to be narrow in energy and uniform in time as long as the sensors are active. The x-ray source is produced by a laser irradiated Ge foil. Our results indicate that the x-ray source lasts during the whole duration of the main laser pulse. Both time-resolved and time-integrated spectral data indicate that the line emission is dominated by the He-α complex over higher energy emission lines. Time-integrated spectra agree well with a one-dimensional Cartesian simulation using HYDRA that predicts a conversion efficiency of 0.56% when the incident intensity is 2 × 1015 W/cm2 on a Ge backlighter.
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Affiliation(s)
- K Werellapatha
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - G N Hall
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - F Coppari
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - G E Kemp
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - N E Palmer
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - C Krauland
- General Atomics, San Diego, California 92121, USA
| | - S F Khan
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - A Lazicki
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - M G Gorman
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - S R Nagel
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - C Heinbockel
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - N Bhandarkar
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - N Masters
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D K Bradley
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J H Eggert
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - L R Benedetti
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
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17
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Huang JW, Zhang YY, Hu SC, Cai Y, Luo SN. DATAD: a Python-based X-ray diffraction simulation code for arbitrary texture and arbitrary deformation. J Appl Crystallogr 2021. [DOI: 10.1107/s1600576721000364] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/10/2022] Open
Abstract
DATAD, a Python-based X-ray diffraction simulation code, has been developed for simulating one- and two-dimensional diffraction patterns of a polycrystalline specimen with an arbitrary texture under an arbitrary deformation state and an arbitrary detection geometry. Pixelated planar and cylindrical detectors can be used. The basic principles and key components of the code are presented along with the usage of DATAD. As validation and application cases, X-ray diffraction patterns of single-crystal and polycrystalline specimens with or without texture, or applied strain, on a planar or cylindrical detector are simulated.
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18
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Metastability of diamond ramp-compressed to 2 terapascals. Nature 2021; 589:532-535. [PMID: 33505034 DOI: 10.1038/s41586-020-03140-4] [Citation(s) in RCA: 27] [Impact Index Per Article: 9.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 06/01/2020] [Accepted: 10/26/2020] [Indexed: 11/08/2022]
Abstract
Carbon is the fourth-most prevalent element in the Universe and essential for all known life. In the elemental form it is found in multiple allotropes, including graphite, diamond and fullerenes, and it has long been predicted that even more structures can exist at pressures greater than those at Earth's core1-3. Several phases have been predicted to exist in the multi-terapascal regime, which is important for accurate modelling of the interiors of carbon-rich exoplanets4,5. By compressing solid carbon to 2 terapascals (20 million atmospheres; more than five times the pressure at Earth's core) using ramp-shaped laser pulses and simultaneously measuring nanosecond-duration time-resolved X-ray diffraction, we found that solid carbon retains the diamond structure far beyond its regime of predicted stability. The results confirm predictions that the strength of the tetrahedral molecular orbital bonds in diamond persists under enormous pressure, resulting in large energy barriers that hinder conversion to more-stable high-pressure allotropes1,2, just as graphite formation from metastable diamond is kinetically hindered at atmospheric pressure. This work nearly doubles the highest pressure at which X-ray diffraction has been recorded on any material.
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Denoeud A, Hernandez JA, Vinci T, Benuzzi-Mounaix A, Brygoo S, Berlioux A, Lefevre F, Sollier A, Videau L, Ravasio A, Guarguaglini M, Duthoit L, Loison D, Brambrink E. X-ray powder diffraction in reflection geometry on multi-beam kJ-type laser facilities. THE REVIEW OF SCIENTIFIC INSTRUMENTS 2021; 92:013902. [PMID: 33514214 DOI: 10.1063/5.0020261] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/29/2020] [Accepted: 12/16/2020] [Indexed: 06/12/2023]
Abstract
An ultrafast x-ray powder diffraction setup for laser-driven dynamic compression has been developed at the LULI2000 laser facility. X-ray diffraction is performed in reflection geometry from a quasi-monochromatic laser-generated plasma x-ray source. In comparison to a transmission geometry setup, this configuration allows us to probe only a small portion of the compressed sample, as well as to shield the detectors against the x-rays generated by the laser-plasma interaction on the front side of the target. Thus, this new platform facilitates probing of spatially and temporarily uniform thermodynamic conditions and enables us to study samples of a large range of atomic numbers, thicknesses, and compression dynamics. As a proof-of-concept, we report direct structural measurements of the bcc-hcp transition both in shock and ramp-compressed polycrystalline iron with diffraction signals recorded between 2θ ∼ 30° and ∼150°. In parallel, the pressure and temperature history of probed samples is measured by rear-side visible diagnostics (velocimetry and pyrometry).
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Affiliation(s)
- A Denoeud
- CEA, DAM, DIF, F-91297 Arpajon, France
| | - J-A Hernandez
- LULI, CNRS, CEA, Sorbonne Université, École Polytechnique, Institut Polytechnique de Paris, F-91128 Palaiseau, France
| | - T Vinci
- LULI, CNRS, CEA, Sorbonne Université, École Polytechnique, Institut Polytechnique de Paris, F-91128 Palaiseau, France
| | - A Benuzzi-Mounaix
- LULI, CNRS, CEA, Sorbonne Université, École Polytechnique, Institut Polytechnique de Paris, F-91128 Palaiseau, France
| | - S Brygoo
- CEA, DAM, DIF, F-91297 Arpajon, France
| | - A Berlioux
- LULI, CNRS, CEA, Sorbonne Université, École Polytechnique, Institut Polytechnique de Paris, F-91128 Palaiseau, France
| | - F Lefevre
- LULI, CNRS, CEA, Sorbonne Université, École Polytechnique, Institut Polytechnique de Paris, F-91128 Palaiseau, France
| | - A Sollier
- CEA, DAM, DIF, F-91297 Arpajon, France
| | - L Videau
- CEA, DAM, DIF, F-91297 Arpajon, France
| | - A Ravasio
- LULI, CNRS, CEA, Sorbonne Université, École Polytechnique, Institut Polytechnique de Paris, F-91128 Palaiseau, France
| | - M Guarguaglini
- LULI, CNRS, CEA, Sorbonne Université, École Polytechnique, Institut Polytechnique de Paris, F-91128 Palaiseau, France
| | - L Duthoit
- CEA, DAM, DIF, F-91297 Arpajon, France
| | - D Loison
- Univ Rennes, CNRS, IPR (Institut de Physique de Rennes)-UMR 6251, F-35000 Rennes, France
| | - E Brambrink
- LULI, CNRS, CEA, Sorbonne Université, École Polytechnique, Institut Polytechnique de Paris, F-91128 Palaiseau, France
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