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Stacking faults in shock-compressed copper

Shock-induced stacking faults in dynamically compressed copper modelled using large-scale molecular dynamics simulations

Patrick Heighway

Postdoctoral Research Assistant in High Energy Density Science

Research theme

  • Lasers and high energy density science

Sub department

  • Atomic and Laser Physics

Research groups

  • Oxford Centre for High Energy Density Science (OxCHEDS)
patrick.heighway@physics.ox.ac.uk
Clarendon Laboratory, room Simon
  • About
  • Publications

Featured Work

Molecular dynamics simulation of double-slip in a bcc crystal
Giving the slip to a metal deformation mystery

A kinematic model uses X-ray diffraction patterns to identify active slip systems during the dynamic compression of metals

Link to Scilight

Diffuse scattering from dynamically compressed single-crystal zirconium following the pressure-induced $\alpha\to\omega$ phase transition

(2024)

Authors:

PG Heighway, S Singh, MG Gorman, D McGonegle, JH Eggert, RF Smith
More details from the publisher
Details from ArXiV

Slip competition and rotation suppression in tantalum and copper during dynamic uniaxial compression

(2022)

Authors:

Patrick G Heighway, Justin S Wark
More details from the publisher
Details from ArXiV

Kinematics of slip-induced rotation for uniaxial shock or ramp compression

Journal of Applied Physics AIP Publishing 129:8 (2021) 085109

Authors:

Patrick Heighway, Justin Wark

Abstract:

When a metallic specimen is plastically deformed, its underlying crystal structure must often rotate in order to comply with its macroscopic boundary conditions. There is growing interest within the dynamic compression community in exploiting x-ray diffraction measurements of lattice rotation to infer which combinations of plasticity mechanisms are operative in uniaxially shock- or ramp-compressed crystals, thus informing materials science at the greatest extremes of pressure and strain rate. However, it is not widely appreciated that several of the existing models linking rotation to slip activity are fundamentally inapplicable to a planar compression scenario. We present molecular dynamics simulations of single crystals suffering true uniaxial strain, and show that the Schmid and Taylor analyses used in traditional materials science fail to predict the ensuing lattice rotation. We propose a simple alternative framework based on the elastoplastic decomposition that successfully recovers the observed rotation for these single crystals, and can further be used to identify the operative slip systems and the amount of activity upon them in the idealized cases of single and double slip.
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Non-isentropic release of a shocked solid

Physical Review Letters American Physical Society 123:24 (2019) 245501

Authors:

PG Heighway, M Sliwa, D McGonegle, C Wehrenberg, CA Bolme, J Eggert, A Higginbotham, A Lazicki, HJ Lee, B Nagler, H-S Park, RE Rudd, RF Smith, MJ Suggit, D Swift, F Tavella, BA Remington, Justin Wark

Abstract:

We present molecular dynamics simulations of shock and release in micron-scale tantalum crystals that exhibit postbreakout temperatures far exceeding those expected under the standard assumption of isentropic release. We show via an energy-budget analysis that this is due to plastic-work heating from material strength that largely counters thermoelastic cooling. The simulations are corroborated by experiments where the release temperatures of laser-shocked tantalum foils are deduced from their thermal strains via in situ x-ray diffraction and are found to be close to those behind the shock.
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X-ray thermal diffuse scattering as a texture-robust temperature diagnostic for dynamically compressed solids

Journal of Applied Physics AIP Publishing 138:15 (2025) 155903

Authors:

PG Heighway, DJ Peake, T Stevens, JS Wark, B Albertazzi, SJ Ali, L Antonelli, MR Armstrong, C Baehtz, OB Ball, S Banerjee, AB Belonoshko, CA Bolme, V Bouffetier, R Briggs, K Buakor, T Butcher, S Di Dio Cafiso, V Cerantola, J Chantel, A Di Cicco, AL Coleman, J Collier, G Collins, AJ Comley, F Coppari, TE Cowan, G Cristoforetti, H Cynn, A Descamps, F Dorchies, MJ Duff, A Dwivedi, C Edwards, JH Eggert, D Errandonea, G Fiquet, E Galtier, A Laso Garcia, H Ginestet, L Gizzi, A Gleason, S Goede, JM Gonzalez, MG Gorman, M Harmand, NJ Hartley, C Hernandez-Gomez, A Higginbotham, H Höppner, OS Humphries, RJ Husband, TM Hutchinson, H Hwang, DA Keen, J Kim, P Koester, Z Konopkova, D Kraus, A Krygier, L Labate, AE Lazicki, Y Lee, H-P Liermann, P Mason, M Masruri, B Massani, EE McBride, C McGuire, JD McHardy, D McGonegle, RS McWilliams, S Merkel, G Morard, B Nagler, M Nakatsutsumi, K Nguyen-Cong, A-M Norton, II Oleynik, C Otzen, N Ozaki, S Pandolfi, A Pelka, KA Pereira, JP Phillips, C Prescher, T Preston, L Randolph, D Ranjan, A Ravasio, J Rips, D Santamaria-Perez, DJ Savage, M Schoelmerich, J-P Schwinkendorf, S Singh, J Smith, RF Smith, A Sollier, J Spear, C Spindloe, M Stevenson, C Strohm, T-A Suer, M Tang, M Toncian, T Toncian, SJ Tracy, A Trapananti, T Tschentscher, M Tyldesley, CE Vennari, T Vinci, SC Vogel, TJ Volz, J Vorberger, JT Willman, L Wollenweber, U Zastrau, E Brambrink, K Appel, MI McMahon

Abstract:

We present a model of x-ray thermal diffuse scattering (TDS) from a cubic polycrystal with an arbitrary crystallographic texture, based on the classic approach of Warren [B. E. Warren, Acta Crystallogr. 6, 803 (1953)]. We compare the predictions of our model with femtosecond x-ray diffraction patterns gathered from ambient and dynamically compressed rolled copper foils obtained at the High Energy Density instrument of the European X-Ray Free-Electron Laser facility and find that the texture-aware TDS model yields more accurate results than does the conventional powder model owed to Warren. Nevertheless, we further show: with sufficient angular detector coverage, the TDS signal is largely unchanged by sample orientation and in all cases strongly resembles the signal from a perfectly random powder; shot-to-shot fluctuations in the TDS signal resulting from grain-sampling statistics are at the percent level, in stark contrast to the fluctuations in the Bragg-peak intensities (which are over an order of magnitude greater); and TDS is largely unchanged even following texture evolution caused by compression-induced plastic deformation. We conclude that TDS is robust against texture variation, making it a flexible temperature diagnostic applicable just as well to off-the-shelf commercial foils as to ideal powders.
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