“…Typically, simple two-body potentials with Coulomb and Lennard-Jones terms served as energy functions; such simple potentials were sufficient because the combination of experimental input and theoretical energy function delivered a high synergy by eliminating many unrealistic local minima on the energy landscape. One up-todate implementation, the program ENDEAVOUR (Putz, 2000), has already been very successful in 'real life' applications, generating convincing structure candidates for such different systems as K 2 CN 2 (Becker & Jansen, 2000), sulfur (Crichton et al, 2001), Na 3 PSO 3 (Pompetzki & Jansen, 2002), Ag 2 NiO 2 (Schreyer & Jansen, 2002), Ag 2 PdO 2 (Schreyer & Jansen, 2001), GaAsO 4 (Santamaría-Pé rez et al, 2006, ammonium metatungstate (Christian & Whittingham, 2008), the zeolite-like structure Na 1Àx Ge 3þz (Beekman et al, 2007), Tl 2 CS 3 (Beck & Benz, 2009) and BiB 3 O 6 (Dinnebier et al, 2009).…”