1
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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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2
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Jiang J, Sun W, Luo N. Shock-Induced Microstructural Evolution, Phase Transformation, Sintering of Al-Ni Dissimilar Nanoparticles: A Molecular Dynamics Study. Chemphyschem 2023:e202300419. [PMID: 37794826 DOI: 10.1002/cphc.202300419] [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: 06/15/2023] [Revised: 10/04/2023] [Accepted: 10/04/2023] [Indexed: 10/06/2023]
Abstract
Molecular dynamic simulations have been performed to explore contact behavior, microstructure evolution and sintering mechanism of Al-Ni dissimilar nanoparticles under high-velocity impact. We confirmed that the simulated contact stress, contact radius, and contact force under low-velocity impact are in good agreement with the predicted results of the Hertz model. However, with increasing the impact velocity, the simulated results gradually deviate from the predicted results of the Hertz model due to the elastic-plastic transition and atomic discrete structure. The normalized contact radius versus strain exhibits a weak dependence on nanosphere diameter. Below a critical velocity, there are very few HCP atoms in the nanospheres after thermal equilibrium. There are two different sintering mechanisms: under low-velocity impact, the sintering process relies mainly on the dislocation slip of Al nanospheres, while the dislocation slip of Ni nanospheres and the atomic diffusion of Al nanospheres predominate under high-velocity impact.
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Affiliation(s)
- Jun Jiang
- State Key Laboratory of Explosion Science and Technology, Beijing Institute of Technology, Beijing, 100081, China
- Beijing Institute of Technology Chongqing Innovation Center, Chongqing, 401120, China
- Explosion Protection and Emergency Disposal Technology Engineering Research Center of the Ministry of Education, Beijing, 10081, China
| | - Weifu Sun
- State Key Laboratory of Explosion Science and Technology, Beijing Institute of Technology, Beijing, 100081, China
- Beijing Institute of Technology Chongqing Innovation Center, Chongqing, 401120, China
- Explosion Protection and Emergency Disposal Technology Engineering Research Center of the Ministry of Education, Beijing, 10081, China
| | - Ning Luo
- School of Mechanics and Civil Engineering, China University of Mining and Technology, Xuzhou, 221116, China
- State Key Laboratory for Geomechanics & Deep Underground Engineering, Xuzhou, 221116, China
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3
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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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4
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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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5
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Phase transformation path in Aluminum under ramp compression; simulation and experimental study. Sci Rep 2022; 12:18954. [DOI: 10.1038/s41598-022-23785-7] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 08/17/2022] [Accepted: 11/04/2022] [Indexed: 11/09/2022] Open
Abstract
AbstractWe present a framework based on non-equilibrium molecular dynamics (NEMD) to reproduce the phase transformation event of Aluminum under ramp compression loading. The simulated stress-density response, virtual x-ray diffraction patterns, and structure analysis are compared against the previously observed experimental laser-driven ramp compression in-situ x-ray diffraction data. The NEMD simulations show the solid–solid phase transitions are consistent to experimental observations with a close-packed face-centered cubic (fcc) (111), hexagonal close-packed (hcp) structure (002), and body-centered cubic bcc (110) planes remaining parallel. The atomic-level analysis of NEMD simulations identifiy the exact phase transformation pathway happening via Bain transformation while the previous in situ x-ray diffraction data did not provide sufficient information for deducing the exact phase transformation path.
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6
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Li C, Li W, Zhang X, Du L, Sheng HW. Predicted Stable Electrides in Mg-Al System under High Pressure. Phys Chem Chem Phys 2022; 24:12260-12266. [DOI: 10.1039/d2cp00981a] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/21/2022]
Abstract
Magnesium and aluminum, as the adjacent light metal elements, are difficult to form the stable stoichiometries compounds under ambient conditions. In this work, using evolutionary ab initio structural prediction approaches,...
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7
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Huang T, Liu C, Wang J, Pan S, Han Y, Pickard CJ, Helled R, Wang HT, Xing D, Sun J. Metallic Aluminum Suboxides with Ultrahigh Electrical Conductivity at High Pressure. RESEARCH (WASHINGTON, D.C.) 2022; 2022:9798758. [PMID: 36111317 PMCID: PMC9448442 DOI: 10.34133/2022/9798758] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 06/09/2022] [Accepted: 07/29/2022] [Indexed: 11/25/2022]
Abstract
Aluminum, as the most abundant metallic elemental content in the Earth's crust, usually exists in the form of alumina (Al2O3). However, the oxidation state of aluminum and the crystal structures of aluminum oxides in the pressure range of planetary interiors are not well established. Here, we predicted two aluminum suboxides (Al2O, AlO) and two superoxides (Al4O7, AlO3) with uncommon stoichiometries at high pressures using first-principle calculations and crystal structure prediction methods. We find that the P4/nmm Al2O becomes stable above ~765 GPa and may survive in the deep mantles or cores of giant planets such as Neptune. Interestingly, the Al2O and AlO are metallic and have electride features, in which some electrons are localized in the interstitials between atoms. We find that Al2O has an electrical conductivity one order of magnitude higher than that of iron under the same pressure-temperature conditions, which may influence the total conductivity of giant planets. Our findings enrich the high-pressure phase diagram of aluminum oxides and improve our understanding of the interior structure of giant planets.
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Affiliation(s)
- Tianheng Huang
- National Laboratory of Solid State Microstructures, School of Physics, And Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China
| | - Cong Liu
- National Laboratory of Solid State Microstructures, School of Physics, And Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China
| | - Junjie Wang
- National Laboratory of Solid State Microstructures, School of Physics, And Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China
| | - Shuning Pan
- National Laboratory of Solid State Microstructures, School of Physics, And Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China
| | - Yu Han
- National Laboratory of Solid State Microstructures, School of Physics, And Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China
| | - Chris J. Pickard
- Department of Materials Science & Metallurgy, University of Cambridge, 27 Charles Babbage Road, Cambridge CB3 0FS, UK
- Advanced Institute for Materials Research, Tohoku University, 2-1-1 Katahira, Aoba, Sendai 980-8577, Japan
| | - Ravit Helled
- Institute for Computational Science, Center for Theoretical Astrophysics & Cosmology, University of Zurich, Switzerland
| | - Hui-Tian Wang
- National Laboratory of Solid State Microstructures, School of Physics, And Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China
| | - Dingyu Xing
- 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
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8
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Ruby JJ, Rygg JR, Chin DA, Gaffney JA, Adrian PJ, Forrest CJ, Glebov VY, Kabadi NV, Nilson PM, Ping Y, Stoeckl C, Collins GW. Energy Flow in Thin Shell Implosions and Explosions. PHYSICAL REVIEW LETTERS 2020; 125:215001. [PMID: 33274978 DOI: 10.1103/physrevlett.125.215001] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 08/26/2020] [Accepted: 10/30/2020] [Indexed: 06/12/2023]
Abstract
Energy flow and balance in convergent systems beyond petapascal energy densities controls the fate of late-stage stars and the potential for controlling thermonuclear inertial fusion ignition. Time-resolved x-ray self-emission imaging combined with a Bayesian inference analysis is used to describe the energy flow and the potential information stored in the rebounding spherical shock at 0.22 PPa (2.2 Gbar or billions of atmospheres pressure). This analysis, together with a simple mechanical model, describes the trajectory of the shell and the time history of the pressure at the fuel-shell interface, ablation pressure, and energy partitioning including kinetic energy of the shell and internal energy of the fuel. The techniques used here provide a fully self-consistent uncertainty analysis of integrated implosion data, a thermodynamic-path independent measurement of pressure in the petapascal range, and can be used to deduce the energy flow in a wide variety of implosion systems to petapascal energy densities.
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Affiliation(s)
- J J Ruby
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
| | - J R Rygg
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
- Department of Mechanical Engineering, University of Rochester, Rochester, New York 14627, USA
| | - D A Chin
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
| | - J A Gaffney
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - P J Adrian
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - C J Forrest
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
| | - V Yu Glebov
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
| | - N V Kabadi
- Plasma Science and Fusion Center, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA
| | - P M Nilson
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
| | - Y Ping
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - C Stoeckl
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
| | - G W Collins
- Department of Physics and Astronomy, University of Rochester, Rochester, New York 14627, USA
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14627, USA
- Department of Mechanical Engineering, University of Rochester, Rochester, New York 14627, USA
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9
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Rygg JR, Smith RF, Lazicki AE, Braun DG, Fratanduono DE, Kraus RG, McNaney JM, Swift DC, Wehrenberg CE, Coppari F, Ahmed MF, Barrios MA, Blobaum KJM, Collins GW, Cook AL, Di Nicola P, Dzenitis EG, Gonzales S, Heidl BF, Hohenberger M, House A, Izumi N, Kalantar DH, Khan SF, Kohut TR, Kumar C, Masters ND, Polsin DN, Regan SP, Smith CA, Vignes RM, Wall MA, Ward J, Wark JS, Zobrist TL, Arsenlis A, Eggert JH. X-ray diffraction at the National Ignition Facility. THE REVIEW OF SCIENTIFIC INSTRUMENTS 2020; 91:043902. [PMID: 32357733 DOI: 10.1063/1.5129698] [Citation(s) in RCA: 18] [Impact Index Per Article: 4.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/30/2019] [Accepted: 03/20/2020] [Indexed: 06/11/2023]
Abstract
We report details of an experimental platform implemented at the National Ignition Facility to obtain in situ powder diffraction data from solids dynamically compressed to extreme pressures. Thin samples are sandwiched between tamper layers and ramp compressed using a gradual increase in the drive-laser irradiance. Pressure history in the sample is determined using high-precision velocimetry measurements. Up to two independently timed pulses of x rays are produced at or near the time of peak pressure by laser illumination of thin metal foils. The quasi-monochromatic x-ray pulses have a mean wavelength selectable between 0.6 Å and 1.9 Å depending on the foil material. The diffracted signal is recorded on image plates with a typical 2θ x-ray scattering angle uncertainty of about 0.2° and resolution of about 1°. Analytic expressions are reported for systematic corrections to 2θ due to finite pinhole size and sample offset. A new variant of a nonlinear background subtraction algorithm is described, which has been used to observe diffraction lines at signal-to-background ratios as low as a few percent. Variations in system response over the detector area are compensated in order to obtain accurate line intensities; this system response calculation includes a new analytic approximation for image-plate sensitivity as a function of photon energy and incident angle. This experimental platform has been used up to 2 TPa (20 Mbar) to determine the crystal structure, measure the density, and evaluate the strain-induced texturing of a variety of compressed samples spanning periods 2-7 on the periodic table.
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Affiliation(s)
- J R Rygg
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - R F Smith
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - A E Lazicki
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - D G Braun
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - D E Fratanduono
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - R G Kraus
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - J M McNaney
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - D C Swift
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - C E Wehrenberg
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - F Coppari
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - M F Ahmed
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - M A Barrios
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - K J M Blobaum
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - G W Collins
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - A L Cook
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - P Di Nicola
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - E G Dzenitis
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - S Gonzales
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - B F Heidl
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - M Hohenberger
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - A House
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - N Izumi
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - D H Kalantar
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - S F Khan
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - T R Kohut
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - C Kumar
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - N D Masters
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - D N Polsin
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - S P Regan
- Laboratory for Laser Energetics, University of Rochester, Rochester, New York 14623, USA
| | - C A Smith
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - R M Vignes
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - M A Wall
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - J Ward
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - J S Wark
- Department of Physics, Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom
| | - T L Zobrist
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - A Arsenlis
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
| | - J H Eggert
- Lawrence Livermore National Laboratory, Livermore, California 94551, USA
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10
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Eidelstein E, Barzilai S, Curtarolo S, Levy O. First Principles Investigation of Cold Curves of Metals. Isr J Chem 2020. [DOI: 10.1002/ijch.201900096] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/06/2022]
Affiliation(s)
- Eitan Eidelstein
- Department of Physics NRCN P.O. Box 9001 Beer-Sheva 84190 Israel
- Department of Chemistry Tel-Aviv University Tel Aviv 69978 Israel
| | - Shmuel Barzilai
- Department of Chemistry NRCN P.O. Box 9001 Beer-Sheva 84190 Israel
| | - Stefano Curtarolo
- Department of Mechanical Engineering and Materials Science Duke University Durham, NC 27708 USA
| | - Ohad Levy
- Department of Physics NRCN P.O. Box 9001 Beer-Sheva 84190 Israel
- Department of Mechanical Engineering and Materials Science Duke University Durham, NC 27708 USA
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11
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Coppari F, Smith RF, Thorn DB, Rygg JR, Liedahl DA, Kraus RG, Lazicki A, Millot M, Eggert JH. Optimized x-ray sources for x-ray diffraction measurements at the Omega Laser Facility. THE REVIEW OF SCIENTIFIC INSTRUMENTS 2019; 90:125113. [PMID: 31893795 DOI: 10.1063/1.5111878] [Citation(s) in RCA: 12] [Impact Index Per Article: 2.4] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 05/30/2019] [Accepted: 11/20/2019] [Indexed: 06/10/2023]
Abstract
The use of x-ray diffraction (XRD) measurements in laser-driven dynamic compression experiments at high-power laser facilities is becoming increasingly common. Diffraction allows one to probe in situ the transformations occurring at the atomic level at extreme conditions of pressure, temperature, and time scale. In these measurements, the x-ray source is generated by irradiation of a solid foil. Under certain laser drive conditions, quasimonochromatic He-α radiation is generated. Careful analysis of the x-ray source plasma spectra reveals that this radiation is not a single line emission and that monochromaticity is highly dependent on the laser irradiance. In this work, we analyze how the spectra emitted by laser-irradiated copper, germanium, and iron foils at the Omega Laser vary depending on different laser drive conditions and discuss the implications for XRD experiments.
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Affiliation(s)
- F Coppari
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - R F Smith
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D B Thorn
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J R Rygg
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - D A Liedahl
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - R G Kraus
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - A Lazicki
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - M Millot
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
| | - J H Eggert
- Lawrence Livermore National Laboratory, Livermore, California 94550, USA
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Xiong Y, Li X, Xiao S, Deng H, Huang B, Zhu W, Hu W. Effect of particle packing and density on shock response in ordered arrays of Ni + Al nanoparticles. Phys Chem Chem Phys 2019; 21:7272-7280. [PMID: 30624453 DOI: 10.1039/c8cp06497k] [Citation(s) in RCA: 8] [Impact Index Per Article: 1.6] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/16/2023]
Abstract
We investigate the shock response of Ni + Al reactive nanoparticle systems through molecular dynamics simulations. The powder configurations with varying arrangements and densities are constructed by stacking equal-sized Ni and Al particles based on five typical crystal structures, i.e., zinc-blende, NaCl, CsCl, AuCu and the close-packed. The effects of configuration and shock strength on mechanochemical and diffusion processes in the shock-induced chemical reactions are characterized. A reaction kinetic model is developed to describe these behaviors, assess the extent of mechanochemical effect, and explain the occurrence of ultra-fast reaction. Significant dependence of shock wave velocity, plastic deformation, temperature response, chemistry and microstructure change on particle packing and density is observed under shock loading at the same piston velocity, but we see a relatively weak dependency on the stacking mode with the same density. Our results indicate the important role of particle coordination number and density in shock response of energetic powder materials.
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Affiliation(s)
- Yongnan Xiong
- College of Materials Science and Engineering, Hunan University, Changsha 410082, China.
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13
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Toroidal diamond anvil cell for detailed measurements under extreme static pressures. Nat Commun 2018; 9:2913. [PMID: 30046093 PMCID: PMC6060175 DOI: 10.1038/s41467-018-05294-2] [Citation(s) in RCA: 95] [Impact Index Per Article: 15.8] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 03/20/2018] [Accepted: 06/22/2018] [Indexed: 11/25/2022] Open
Abstract
Over the past 60 years, the diamond anvil cell (DAC) has been developed into a widespread high static pressure device. The adaptation of laboratory and synchrotron analytical techniques to DAC enables a detailed exploration in the 100 GPa range. The strain of the anvils under high load explains the 400 GPa limit of the conventional DAC. Here we show a toroidal shape for a diamond anvil tip that enables to extend the DAC use toward the terapascal pressure range. The toroidal-DAC keeps the assets for a complete, reproducible, and accurate characterization of materials, from solids to gases. Raman signal from the diamond anvil or X-ray signal from the rhenium gasket allow measurement of pressure. Here, the equations of state of gold, aluminum, and argon are measured with X-ray diffraction. The data are compared with recent measurements under similar conditions by two other approaches, the double-stage DAC and the dynamic ramp compression. Extreme static pressures exceeding a million atmospheres exist in a variety of natural environments, but obtaining such pressures in a laboratory is still a challenge. Here, the authors develop a toroidal diamond anvil design that allows for the generation of 600 GPa (6 million atmospheres) in routinely used diamond anvil cells.
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