
78 Perturbation Theories for Fluids and Solids
where c
HS
(r) is the HS DCF, for which one can choose a Yukawa form, as in the
GMSA equation (4.17), or an expression known in advance by any other means.
SCOZA can be extended to soft-core potentials by exploiting the fact that many
simple continuous potentials can be approximated by linear combinations of Yukawa
tails (Kahl et al. 2002, Schöll-Paschinger and Kahl 2003), by introducing an effective
hard-core diameter (Høye and Reiner 2006), by removing the condition r > σ in
Equation 4.25 (Raineri et al. 2004, Mladek et al. 2006), or by replacing c
HS
(r) in
Equation 4.26 with a suitable DCF for the soft ...