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Belonoshko, Anatoly B.

Publications and source records attributed to Belonoshko, Anatoly B..

Extreme Metastability of Diamond and its Transformation to the BC8 Post-Diamond Phase of Carbon

Diamond possesses exceptional physical properties due to its remarkably strong carbon–carbon bonding, leading to significant resilience to structural transformations at very high pressures and temperatures. Despite several experimental attempts, synthesis and recovery of the theoretically predicted post-diamond BC8 phase remains elusive. Through quantum-accurate multimillion atom molecular dynamics (MD) simulations, we have uncovered the extreme metastability of diamond at very high pressures, significantly exceeding its range of thermodynamic stability. We predict the post-diamond BC8 phase to be experimentally accessible only within a narrow high pressure–temperature region of the carbon phase diagram. The diamond to BC8 transformation proceeds through premelting followed by BC8 nucleation and growth in the metastable carbon liquid. Here we propose a double-shock compression pathway for BC8 synthesis, which is currently being explored in experiments at the National Ignition Facility.

70 PLASMA PHYSICS AND FUSION TECHNOLOGY↗

IC W13_fephases Highlight: Strong Size Dependence of Dynamic Instability Treatment in VASP Ab Initio Approach [Poster]

Phonon spectra at two different densities of bcc-Be at T slightly below the corresponding Tm. At P=0 the system is dynamically unstable at low T but stabilizes at T close to Tm=1560 K. However, unless the system size is 1458 atoms or higher (the number of valence electrons is ~ 3000 or more) dynamic instability is still present, in the form of an imaginary phonon branch at the Γ- point (Fig. 1). At P=300 GPa the system is dynamically stable for as low as 128 atoms (Fig. 2). This example demonstrates that at present it is unfeasible to treat bcc-Fe in the region of its dynamic instability (megabar pressure range) with the existing first-principles software (e.g., VASP) which only allows treating bcc-Fe with up to ~ 500 atoms (~7000 valence electrons).

36 MATERIALS SCIENCE↗

IC W13_fephases Highlight:Solid-Solid Phase Boundary in Fe

Temperature of the fcc-bcc (face-centered cubic – body-centered cubic) solid-solid phase transition in Fe calculated as Teq = Tinst ΔEfcc-bcc/ΔEbcc-m. (where m. stands for martensitic mixture that bcc-Fe converts into at Tinst) maps out a curve which is consistent with the line of the fast recrystallization threshold observed in the recent experiments on Fe at ESRF.

36 MATERIALS SCIENCE↗