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One can satisfy g (0) = (1/2) [1-1.372 rs +O (rs2)] by imposing E=A+1.372 in Eq. 9; however, we found the corresponding fits to be poor because it is inappropriate to use the high-density expansion to determine the exponent which controls how rapidly g (0) falls off at low density.
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One can satisfy g (0) = (1/2) [1-1.372 rs +O (rs2)] by imposing E=A+1.372 in Eq. 9; however, we found the corresponding fits to be poor because it is inappropriate to use the high-density expansion to determine the exponent which controls how rapidly g (0) falls off at low density.
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