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The hypernetted chain equation has been solved numerically for the classical one-component plasma in a uniform background up to Γ=7000, where Γ=(Ze)2/kTa and a is the ion-sphere radius. Numerical results are presented. The distribution functions and thermodynamical quantities obtained are in good agreement with the Monte Carlo results in the fluid region. The average potential energy Ū/NkT is in error by less than 0.8% for 20≤Γ≤160 and approaches −0.8995Γ as Γ approaches infinity. The pressure and the free energy calculated do not show any evidence of a phase transition. However, the distribution function g(r) for Γ ≳ 1500 has an unusual behavior between 2.5r4.0, resembling somewhat that of a hcp crystal. If we assume the sum of the bridge diagram to be of the form B(r)=−λΓ/r where λ=0.6 erf (0.024Γ), the distribution function calculated agrees to within about ±0.02 with the Monte Carlo g(r) in the whole fluid region.
Kin-Chue Ng (Tue,) studied this question.