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. 2016 Nov 2;7:13338. doi: 10.1038/ncomms13338

Table 1. Formal charge binding energies and metal charges.

Men+ BEPhCN qf BEDMMP qf BEDMMP–BEPhCN Disp. (Calc)* Disp. (Exp) Agreement
Al3+ −24.69 1.03 −19.82 1.74 4.87 No Yes No
Fe3+ −20.31 1.60 −19.63 1.51 0.68 No Yes No
La3+ −8.56 2.32 −10.15 2.35 −1.59 Yes Yes Yes
Cd2+ −6.49 1.22 −7.33 1.39 −0.84 Yes No No
Co2+ −6.88 0.87 −7.72 1.22 −0.84 Yes No No
Cu2+ −9.88 0.81 −8.52 1.31 1.36 No Yes No
Ni2+ −7.66 0.86 −8.26 1.23 −0.60 Yes No No
Zn2+ −6.81 1.34 −8.17 1.27 −1.36 Yes No No
Ag+ −2.21 0.73 −2.27 0.79 −0.06 No No bind No
Na+ −1.41 0.83 −1.71 0.89 −0.30 Yes No bind No

Binding energy [eV] and final metal charge (qf) for the minimum energy structures of Men+–PhCN and Men+–DMMP using the formal charge approach. Agreement regarding displacement events between theory and the original experiments was only seen in one of ten cases. After the follow-up experiments, agreement regarding displacement increased to three of ten cases (due to displacement of 5CB from Cd and Zn in the follow-up experiments).

*Computed displacement of PhCN by DMMP.

Experimental displacement of PhCN by DMMP, from previous studies11.

Agreement between computed and experimental displacement. ‘No bind' indicates no homeotropic anchoring of the liquid crystal to the metal cation. Displacement is assumed to occur when BEDMMP−BEPhCN<−0.20 eV.