4.6 Article

First-principles equation-of-state table of deuterium for inertial confinement fusion applications

期刊

PHYSICAL REVIEW B
卷 84, 期 22, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevB.84.224109

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资金

  1. US Department of Energy Office of Inertial Confinement Fusion [DE-FC52-08NA28302]
  2. University of Rochester
  3. New York State Energy Research and Development Authority
  4. National Science Foundation (NSF) [PHY110009]
  5. NASA
  6. Division Of Astronomical Sciences
  7. Direct For Mathematical & Physical Scien [1008045] Funding Source: National Science Foundation

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Understanding and designing inertial confinement fusion (ICF) implosions through radiation-hydrodynamics simulations relies on the accurate knowledge of the equation of state (EOS) of the deuterium and tritium fuels. To minimize the drive energy for ignition, the imploding shell of DT fuel must be kept as cold as possible. Such low-adiabat ICF implosions can access to coupled and degenerate plasma conditions, in which the analytical EOS models become inaccurate due to many-body effects. Using the path-integral Monte Carlo (PIMC) simulations we have derived a first-principles EOS (FPEOS) table of deuterium that covers typical ICF fuel conditions at densities ranging from 0.002 to 1596 g/cm(3) and temperatures of 1.35 eV to 5.5 keV. We report the internal energy and the pressure and discuss the structure of the plasma in terms of pair-correlation functions. When compared with the widely used SESAME table and the revised Kerley03 table, discrepancies in the internal energy and in the pressure are identified for moderately coupled and degenerate plasma conditions. In contrast to the SESAME table, the revised Kerley03 table is in better agreement with our FPEOS results over a wide range of densities and temperatures. Although subtle differences still exist for lower temperatures (T < 10 eV) and moderate densities (1 to 10 g/cm(3)), hydrodynamics simulations of cryogenic ICF implosions using the FPEOS table and the Kerley03 table have resulted in similar results for the peak density, areal density (rho R), and neutron yield, which differ significantly from the SESAME simulations.

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