Table 2.
Optimized hexagonsX 6R6 with D 6h symmetry.
| X | R | Stationary pointa | Imaginary Mode of 1st TS | Structureb |
|---|---|---|---|---|
| Si | Na | 3rd TS | B | |
| Si | K | 1st TS | Our-of-plane motion of K | B |
| Si | Mg | 2nd TS | B | |
| Si | Ca | 6th TS | B | |
| Si | Cu | 1st TS | Out-of-plane ring deformation | A |
| Si | Zn | 1st TS | Our-of-plane motion of Zn | B |
| Si | C≡N | 1st TS | Out-of-plane ring deformation | A |
| Si | MgH | MIN | A | |
| Si | CaH | 6th TS | A | |
| Ge | BeH | MIN | A | |
| Ge | MgH | 1st TS | Our-of-plane motion of MgH | A |
| Ge | CaH | 17th TS | A | |
| Si | H | 1st TS | Out-of-plane ring deformation | A |
| Si | Li | 6th TS | A |
Full geometry optimizations were performed at the B3LYP/6-311++ G(3df,3pd) level for K, Ca, Cu, Zn and CaH substitution, and at the B3LYP/cc-pVTZ level for H, Li, Na, Mg, C≡N, BeH and MgH substitution. aMIN: minimum, TS: transition state. bTwo D 6h structures A and B are shown in Fig. 6. More stable structure between the two D 6h structures is listed for the terminal substituent of metals (R = Na, K, Mg, Ca, Cu, Zn). For comparison, the results of Si6H6 and Si6Li6 of structure A are listed.