2010
DOI: 10.1021/jp911209w
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Structure and Stability of M6N8 Clusters (M = Si, Ge, Sn, Ti)

Abstract: The structures and stabilities of the M(6)N(8) clusters (M = Si, Ge, Sn, Ti) have been theoretically studied at DFT and ab initio levels of theory. Two new isomers have been considered: cage-like molecules and propeller-like molecules. It is shown that only for M = Si are both isomers true minima on the potential energy surface. The thermodynamics of the dissociation process (1/6)M(6)N(8) --> (1/3)M(3)N(4) is discussed. For each M(3)N(4) molecule, four structures with different multiplicity are considered. The… Show more

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Cited by 9 publications
(2 citation statements)
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“…To investigate the relative stability of B-coronene with different spin states, the single-point energies of them have been plotted in Figure 6, while the relative energies are presented in Table S2. As the spin-projected MP2 (PMP2) [40] is known to provide energy results less influenced by spin contamination 41 than the UMP2 method for open shell systems, the single-point energies are calculated at the PMP2/6-31 + G(d, p) to minimize the errors caused by the spin contamination. 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 From Table S2 and Figure 6, it is noted that the singlet structure is the lowest-energy one among these structures with different spin states for both the pristine and boron-substituted coronene, and the total energies are gradually increased as the spin multiplicity increases.…”
Section: Spin States Of B-coronenementioning
confidence: 99%
“…To investigate the relative stability of B-coronene with different spin states, the single-point energies of them have been plotted in Figure 6, while the relative energies are presented in Table S2. As the spin-projected MP2 (PMP2) [40] is known to provide energy results less influenced by spin contamination 41 than the UMP2 method for open shell systems, the single-point energies are calculated at the PMP2/6-31 + G(d, p) to minimize the errors caused by the spin contamination. 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 From Table S2 and Figure 6, it is noted that the singlet structure is the lowest-energy one among these structures with different spin states for both the pristine and boron-substituted coronene, and the total energies are gradually increased as the spin multiplicity increases.…”
Section: Spin States Of B-coronenementioning
confidence: 99%
“…This may be because the nitrogen atom has three 2p-electrons, which easily form three σ bonds with other neighbour atoms, while the silicon atom has two 3s-and two 3p-electrons, which prefer forming covalent bonds with other atoms by sp 3 hybridization. In this case, the N atom forms threefold coordinated to neighbour Si atoms, which is similar to the atomic configuration character of silicon nitride clusters (such as Si 6 N 8 [43,44] and Si n−1 N [45] clusters). Furthermore, these results show that doping with the N atom leads to significant structural distortion compared with their corresponding pure Si n C n clusters.…”
Section: Methodsmentioning
confidence: 74%