Learning heat transport kernels using a nonlocal heat transport theory-informed neural network

Physical Review Research American Physical Society (APS) 7:4 (2025) L042017

Authors:

Mufei Luo, Charles Heaton, Yizhen Wang, Daniel Plummer, Mila Fitzgerald, Francesco Miniati, Sam M Vinko, Gianluca Gregori

Abstract:

<jats:p>We present a data-driven framework for the modeling of nonlocal heat transport in plasmas using a nonlocal theory-informed neural network trained on kinetic particle-in-cell simulations that span both local and nonlocal regimes. The model learns spatio-temporal heat flux kernels directly from simulation data, capturing dynamic transport behaviors beyond the reach of classical formulations. Unlike time-independent kernel models such as Luciani-Mora-Virmont and Schurtz-Nicolaï-Busquet models, our approach yields physically grounded, time-evolving kernels that adapt to varying plasma conditions. The resulting predictions show strong agreement with kinetic benchmarks across regimes. This offers a promising direction for data-driven modeling of nonlocal heat transport and contributes to a deeper understanding of plasma dynamics.</jats:p>

High-quality ultra-fast total scattering and pair distribution function data using an X-ray free electron laser

IUCrJ International Union of Crystallography 12:5 (2025) 12

Authors:

Adam F Sapnik, Philip A Chater, Dean S Keeble, Elodie Harbourne, Andrew Goodwin, Celine Crepisson, Justin Wark

Abstract:

High-quality total scattering data, a key tool for understanding atomic-scale structure in disordered materials, require stable instrumentation and access to high momentum transfers. This is now routine at dedicated synchrotron instrumentation using high-energy X-ray beams, but it is very challenging to measure a total scattering dataset in less than a few microseconds. This limits their effectiveness for capturing structural changes that occur at the much faster timescales of atomic motion. Current X-ray free-electron lasers (XFELs) provide femtosecond-pulsed X-ray beams with maximum energies of ~24 keV, giving the potential to measure total scattering and the attendant pair distribution functions (PDFs) on femtosecond timescales. Here, we show that this potential has been realised using the HED scientific instrument at the European XFEL and present normalised total scattering data for 0.35Å−1 < Q < 16.6Å−1 and their PDFs from a broad spectrum of materials, including crystalline, nanocrystalline and amorphous solids, liquids, and clusters in solution. We analyse the data using a variety of methods, including Rietveld refinement, small-box PDF refinement, joint reciprocal–real space refinement, cluster refinement, and Debye scattering analysis. The resolution function of the setup is also characterised. We conclusively show that high-quality data can be obtained from a single ~30 fs XFEL pulse for multiple different sample types. Our efforts not only significantly increase the existing maximum reported Q-range for an S(Q) measured at an XFEL but also mean that XFELs are now a viable X-ray source for the broad community of people using reciprocal space total scattering and PDF methods in their research.

Isostructural phase transition of Fe2O3 under laser shock compression

Physical Review Letters American Physical Society 134:17 (2025) 176102

Authors:

Alexis Amouretti, Celine Crepisson, Sam Azadi, Francois Brisset, Delphine Cabaret, Thomas Campbell, David Chin, Gilbert Rip Collins, Linda Hansen, Guillaume Fiquet, Alessandro Forte, Thomas Gawne, Francois Guyot, Patrick Heighway, Eva Heripre, Eric Cunningham, Hae Ja Lee, David McGonegle, Bob Nagler, Juan Pintor, Danae Polsin, Gaelle Rousse, Yuanfeng Shi, Ethan Smith, Justin Wark, Sam Vinko, Marion Harmand

Abstract:

We present in situ x-ray diffraction and velocity measurements of Fe2⁢O3 under laser shock compression at pressures between 38–122 GPa. None of the high-pressure phases reported by static compression studies were observed. Instead, we observed an isostructural phase transition from 𝛼−Fe2⁢O3 to a new 𝛼′−Fe2⁢O3 phase at a pressure of 50–62 GPa. The 𝛼′−Fe2⁢O3 phase differs from 𝛼−Fe2⁢O3 by an 11% volume drop and a different unit cell compressibility. We further observed a two-wave structure in the velocity profile, which can be related to an intermediate regime where both 𝛼 and 𝛼′ phases coexist. Density functional theory calculations with a Hubbard parameter indicate that the observed unit cell volume drop can be associated with a spin transition following a magnetic collapse.

Evolution of autoresonant plasma wave excitation in two-dimensional particle-in-cell simulations

Journal of Plasma Physics Cambridge University Press (CUP) 91:1 (2025) e31

Authors:

M Luo, C Riconda, A Grassi, N Wang, JS Wurtele, T Fülöp, I Pusztai

Shock-driven amorphization and melting in Fe2⁢O3

Physical Review B American Physical Society 111:2 (2025) 024209

Authors:

Celine Crépisson, Alexis Amouretti, Marion Harmand, Chrystele Sanloup, Patrick Heighway, Sam Azadi, David McGonegle, Thomas Campbell, Juan Pintor, David A Chin, Ethan Smith, Linda Hansen, Alessandro Forte, Thomas Gawne, Hae Ja Lee, Bob Nagler, Yuanfeng Shi, Guillaume Fiquet, Francois Guyot, Makita Mikako, Alessandra Bennuzi-Mounaix, Tommaso Vinci, Kohei Miyanishi, Norimasa Ozaki, Tatiana Pikuz, Hirotaka Nakamura, Keiichi Sueda, Toshinori Yabuushi, Makina Yabashi, Justin S Wark, Danae N Polsin, Sam M Vinko

Abstract:

We present measurements on Fe2O3 amorphization and melt under laser-driven shock compression up to 209(10) GPa via time-resolved in situ x-ray diffraction. At 122(3) GPa, a diffuse signal is observed indicating the presence of a noncrystalline phase. Structure factors have been extracted up to 182(6) GPa showing the presence of two well-defined peaks. A rapid change in the intensity ratio of the two peaks is identified between 145(12) and 151(12) GPa, indicative of a phase change. The noncrystalline diffuse scattering is consistent with shock amorphization of Fe2O3 between 122(3) and 145(12) GPa, followed by an amorphous-to-liquid transition above 151(12) GPa. Upon release, a noncrystalline phase is observed alongside crystalline α-Fe2O3. The extracted structure factor and pair distribution function of this release phase resemble those reported for Fe2O3 melt at ambient pressure.