4.7 Article

First-principles equation-of-state table of silicon and its effects on high-energy-density plasma simulations

期刊

PHYSICAL REVIEW E
卷 95, 期 4, 页码 -

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AMER PHYSICAL SOC
DOI: 10.1103/PhysRevE.95.043210

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资金

  1. Department of Energy National Nuclear Security Administration [DE-NA0001944]
  2. University of Rochester
  3. New York State Energy Research and Development Authority
  4. Scientific Campaign 10 at the Los Alamos National Laboratory
  5. U.S. Department of Energy [DE-AC5206NA25396]

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Using density-functional theory-based molecular-dynamics simulations, we have investigated the equation of state for silicon in a wide range of plasma density and temperature conditions of rho = 0.001-500 g/cm(3) and T = 2000-10(8) K. With these calculations, we have established a first-principles equation-of-state (FPEOS) table of silicon for high-energy-density (HED) plasma simulations. When compared with the widely used SESAME-EOS model (Table 3810), we find that the FPEOS-predicted Hugoniot is similar to 20% softer; for off-Hugoniot plasma conditions, the pressure and internal energy in FPEOS are lower than those of SESAME EOS for temperatures above T approximate to 1-10 eV (depending on density), while the former becomes higher in the low-T regime. The pressure difference between FPEOS and SESAME 3810 can reach to similar to 50%, especially in the warm-dense-matter regime. Implementing the FPEOS table of silicon into our hydrocodes, we have studied its effects on Si-target implosions. When compared with the one-dimensional radiation-hydrodynamics simulation using the SESAME 3810 EOS model, the FPEOS simulation showed that (1) the shock speed in silicon is similar to 10% slower; (2) the peak density of an in-flight Si shell during implosion is similar to 20% higher than the SESAME 3810 simulation; (3) the maximum density reached in the FPEOS simulation is similar to 40% higher at the peak compression; and (4) the final areal density and neutron yield are, respectively, similar to 30% and similar to 70% higher predicted by FPEOS versus the traditional simulation using SESAME 3810. All of these features can be attributed to the larger compressibility of silicon predicted by FPEOS. These results indicate that an accurate EOS table, like the FPEOS presented here, could be essential for the precise design of targets for HED experiments.

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