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. 2017 Sep 7;7:10855. doi: 10.1038/s41598-017-11360-4

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.