Bulletin of the American Physical Society
65th Annual Meeting of the APS Division of Plasma Physics
Monday–Friday, October 30–November 3 2023; Denver, Colorado
Session BO03: HED Warm Dense Matter; EOS - Theory
9:30 AM–11:54 AM,
Monday, October 30, 2023
Room: Governor's Square 10
Chair: Georges Jaar, University of Nevada, Reno
Abstract: BO03.00009 : Study of the H2/H-He mixtures at extreme conditions: demixing, insulator-metal transition and miscibility boundaries*
11:06 AM–11:18 AM
Presenter:
Valentin V Karasiev
(Laboratory for Laser Energetics, University of Rochester)
Authors:
Valentin V Karasiev
(Laboratory for Laser Energetics, University of Rochester)
Joshua Hinz
(Laboratory for Laser Energetics, University of Rochester)
Rati M Goshadze
(Laboratory for Laser Energetics, University of Rochester)
Suxing Hu
(Laboratory for Laser Energetics, University of Rochester)
Armin Bergermann
(University of Rostock)
Ronald A Redmer
(University of Rostock)
Accurate knowledge of the H-He demixing conditions and location of the insulator-metal-transition (IMT) boundary at Mbar pressures is important for planetary models. The most successful approach, to date, is the evaluation of the Gibbs free-energy of mixing based on the non-ideal entropy of mixing. Here, we explore a different approach. Using an NPT ensemble, large-scale ab-initio molecular dynamics (AIMD) simulations are performed along a set of selected isobars. At low-T the system spontaneously separates resulting in two regions, one that is He-rich and one that is molecular hydrogen-rich. Calculations of the conductivity indicate this demixed system is an insulator. Admixture with a small fraction of He makes the H2 bonds stronger leading to a H2 dissociation and related IMT that occurs at temperatures significantly higher as compared to pure H2. With further increase of temperature the H-He mixing will occur. Analysis of the first peak of the H-He radial distribution function provides a sharp signature of the transition from the demixed to the perfectly mixed phase. The use of a thermal exchange-correlation (XC) functional in our AIMD simulations shifts the miscibility boundary by about 10% up in temperature as compared to the standard ground-state XC functional.
*This material is based upon work supported by the Department of Energy National Nuclear Security Administration under Award Number DE-NA0003856 and US National Science Foundation PHY Grant No. 2205521.
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