Abstract
The ground-state energy of solid hydrogen and deuterium is calculated by means of a modified variational lowest order constrained-variation (LOCV) method. Both fcc and hcp H2 and D2 are considered, and the calculations are done for five different two-body potentials. For solid H2 we obtain theoretical results for the ground-state binding energy per particle from −74.9 K at an equilibrium particle density of 0.700 σ−3 or a molar volume of 22.3 cm3/mole to −91.3 K at a particle density of 0.725 σ−3 or a molar volume of 21.5 cm3/mole, where σ=2.958 A. The corresponding experimental result is −92.3 K at a particle density of 0.688 σ−3 or a molar volume of 22.7 cm3/mole. For solid D2 we obtain theoretical results for the ground-state binding energy per particle from −125.7 K at an equilibrium particle density of 0.830 σ−3 or a molar volume of 18.8 cm3/mole to −140.1 K at a particle density of 0.843 σ−3 or a molar volume of 18.5 cm3/mole. The corresponding experimental result is −137.9 K at a particle density of 0.797 σ−3 or a molar volume of 19.6 cm3/mole.
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