Abstract
For the purpose of obtaining the semiempirical formulas for the pair correlation energy of various types of atoms and ions having the electron configurations 1s22sm2pn(m=0, 1, 2; n=0, 1, ..., 6), semiempirical values of the correlation energies of such atoms are analyzed. It is pointed out that the correlation energy in the average of a configuration is more convenient than the correlation energy in each of the stationary states belonging to the configuration, for the purpose of this analysis. The correlation energy in the average of the configuration is shown to be equal to EAvcorr, the average of the correlation energy in various states belonging to the configuration. The EAvcorr values are obtained for a wide variety of the 1s22sm2pn atoms and regularities are found among these EAvcorr values. From the analysis of these regularities, it is found that the EAvcorr values of the 1s22sm2pn atoms can be reproduced very well with an equation EAvcorr = C1 + C2m + C3n + C4m2 + C5mn + C6n2 + C7m2n + C8mn2 + C9m2n2 + C10 m (m − 1)Z + C11m(m − 1) nZ + C12m (m − 1)Z2 , where Z is the atomic number, along with the numerical values of the coefficients Ci's (i=1, 2,..., 12) determined from a least‐squares fitting of this equation to various empirical EAvcorr values. The concept of the average pair correlation energy of the configuration εkl is also proposed. Expressions for ε kl's are given in terms of the pair correlation energies of various type in each of the states belonging to the configuration. It is shown that EAvcorr can be expressed in a simple form in terms of εkl's. From this expression and the semiempirical expression of EAvcorr mentioned above, a semiempirical formula for the average pair correlation energy is obtained for each type of electron pairs. It is found that these semiempirical formulas are in accord with the results of the Sinanoğlu theory for the ground and the excited states and of nonempirical calculations of pair correlation energies, rather than with those of a previous purely empirical analysis of the correlation energies by Allen, Clementi, and Gladney.