posted on 2020-11-19, 05:43authored byZarina
M. Efimenko, Anastasiya A. Eliseeva, Daniil M. Ivanov, Bartomeu Galmés, Antonio Frontera, Nadezhda A. Bokach, Vadim Yu. Kukushkin
Cocrystallization of the nitrosoguanidinate
complexes [Ni{NHC(NR2)NN(O)}2] (R2 = Me2 (1), Me/Ph (2),
C5H10 (3)) with 1,2-diiodotetrafluorobenzene
(1,2-FIB), 1,4-diiodotetrafluorobenzene
(1,4-FIB), 1,3,5-triiodotrifluorobenzene (1,3,5-FIB), and tetraiodoethylene
(C2I4) gave new cocrystals (1–3)·2(1,2-FIB), 2·(1,4-FIB), 3·2(1,3,5-FIB), 1·C2I4, and 2·2C2I4; all of these
solids were studied by single-crystal X-ray diffraction. Each structure
exhibits the asymmetric bifurcated halogen bond μ2-I···(N,O) as a characteristic feature and a structure-directing
contact. DFT calculations were used to evaluate the energetic features
of the bifurcated halogen bonds that range from −6.7 to −8.3
kcal/mol; in general, the I···O contact is stronger
that the I···N contact. Molecular electrostatic potential
(MEP) surfaces along with the quantum theory of “atoms in molecules”
(QTAIM) and the noncovalent interaction plot index (NCIPlot) computational
tools were used to characterize the bifurcated halogen bonds in the
cocrystals of 1–3. Various types
of bifurcated halogen bonds involving nonmetal atoms as halogen-bond-accepting
centers were systematized and categorized.