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For the FPCM calculations with MP2 method, the MP2 perturbation procedure was performed for electron correlation correction after the converged HF wave function of solute in reaction field is obtained
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(d) For the FPCM calculations with MP2 method, the MP2 perturbation procedure was performed for electron correlation correction after the converged HF wave function of solute in reaction field is obtained.
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(e) Regarding the detail of the FPCM computation on a given solute under a given quantum mechanical approximation level, once the solute cavity is defined and the dielectric constant is known, the accuracy of the FPCM numerical computation depends only on the number of surface nodes (N) representing the cavity surface and number of layers (M) describing the volume polarization charge distribution within a certain, sufficiently large three-dimensional space outside the solute cavity. If one could use an infinite number of nodes and an infinite number of layers, then the numerical results obtained from the FPCM computation would be exactly the same as those determined by the exact solution of the Poisson's equation for describing the solvent polarization potential. We have shown that the accuracy of the FPCM numerical computations employed in this study with N = 590 and M = 40 (for a step of 0.3 Å) are higher than what required for listing Tables 1 and 2 in this paper. The dielectric constant of water used for the FPCM calculations is 78.5.
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