39 research outputs found
Sesame-Style Decomposition of KS-DFT Molecular Dynamics for Direct Interrogation of Nuclear Models
A common paradigm used in the construction of equations of state is to
decompose the thermodynamics into a superposition of three terms: a
static-lattice cold curve, a contribution from the thermal motion of the
nuclei, and a contribution from the thermal excitation of the electrons. While
statistical mechanical models for crystals provide tractable framework for the
nuclear contribution in the solid phase, much less is understood about the
nuclear contribution above the melt temperature () and how it should transition to the high-temperature limit
(). In this work, we describe an
algorithm for extracting both the thermal nuclear and thermal electronic
contributions from quantum molecular dynamics (QMD). We then use the VASP QMD
package to probe thermal nuclear behavior of liquid aluminum at normal density
to compare the results to semi-empirical models -- the Johnson generic model,
the Chisolm high-temperature liquid model, and the CRIS model.Comment: 6 pages, 4 figures, APS Shock Compression of Condensed Matter
Conference Proceedings 201
{\em Ab initio} Quantum Monte Carlo simulation of the warm dense electron gas in the thermodynamic limit
We perform \emph{ab initio} quantum Monte Carlo (QMC) simulations of the warm
dense uniform electron gas in the thermodynamic limit. By combining QMC data
with linear response theory we are able to remove finite-size errors from the
potential energy over the entire warm dense regime, overcoming the deficiencies
of the existing finite-size corrections by Brown \emph{et al.}~[PRL
\textbf{110}, 146405 (2013)]. Extensive new QMC results for up to
electrons enable us to compute the potential energy and the
exchange-correlation free energy of the macroscopic electron gas with
an unprecedented accuracy of . A comparison of our new data to the recent parametrization of
by Karasiev {\em et al.} [PRL {\bf 112}, 076403 (2014)] reveals
significant deviations to the latter