“…The method used for the computation of pairwise electrostatic energies in the crystal may include either a multipole moment approximation (Buckingham, 1967(Buckingham, , 1978Buckingham et al, 1988;Stone, 1996) or a grid-based numerical integration (Gavezzotti, 2002b(Gavezzotti, , 2003(Gavezzotti, , 2005Ma & Politzer, 2004). In addition, very efficient computational methods, for example the Ewald-type summation (Cummins et al, 1976;de Leeuw et al, 1980;Heyes, 1981;Allen & Tildesley, 1987;Williams, 1989;Smith, 1998;Su & Coppens, 1995;Toukmaji & Board, 1996;Challacombe et al, 1997;Abramov et al, 2000;Nymand & Linse, 2000;Frenkel & Smit, 2002;Aguado & Madden, 2003;Sagui et al, 2004;Arnold & Holm, 2005;Stenhammar et al, 2011;Giese et al, 2015) and a clever workaround known as the Wolf formalism (Wolf et al, 1999;Zahn et al, 2002;Fennell & Gezelter, 2006;Lamichhane et al, 2014;Stenqvist et al, 2015), have been developed. Nevertheless, the major drawbacks of these methods are well known: the multipole approximation breaks down for overlapping charge distributions, while a numerical approach is rather computationally demanding and subject to grid limitations.…”