DOE OSTI · 2997953
Quantum Ornstein-Zernike theory for two-temperature two-component plasmas
Abstract
Laboratory plasma production almost always preferentially heats either the ions or electrons, leading to a two-temperature state. In this state, density functional theory molecular dynamic simulation is the state of the art for modeling bulk material properties. We construct a statistical mechanics model for the two temperature limit that is theoretically consistent with the molecular dynamics method. We proceed to derive the electron-ion multi-temperature quantum Ornstein-Zernike equations for the first time. This allows the construction of a two-temperature two-component plasma model using the average atom from which we can compute bulk material properties at a fraction of the computation time of the two-temperature density functional theory simulation. The accuracy of the model is benchmarked against ion pair correlation and self-diffusion results from ab initio simulation. Here, we proceed to compute the viscosity and ion thermal conductivity as a function of both ion and electron temperature.
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Johnson, Zachary A. [Michigan State University, East Lansing, MI (United States)] (ORCID:0000000244552021), Shaffer, Nathaniel R. [University of Rochester, NY (United States)] (ORCID:0000000207100026), Murillo, Michael S. [Michigan State University, East Lansing, MI (United States)]. 2025-08-18. Quantum Ornstein-Zernike theory for two-temperature two-component plasmas. https://doi.org/10.1103/5c29-kdx1
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