Metallocenes, including ferrocene, [(h 5 -C 5 H 5 ) 2 Fe], and its 18-electron analogues [(h 5 -E 5 ) 2 M] (E = P, N, As, Sb, and Bi; M = transition-metal atom), have found important applications in both fundamental research and materials science.[ (n = 4, 6). [9][10][11] In these sandwich-type structures, the transition-metal center, M, is coordinated between two aromatic h n -E n monocycles (n = 4-6), each of which has 6-p electrons. The p-d interactions between the delocalized p molecular orbitals (MOs) of the ligands and the partially occupied d orbitals of the transitionmetal center play a crucial role in stabilizing the systems. Designing new forms of metallocenes and their sandwich-type analogues requires the right match between the monocyclic ligands and transition-metal centers, both geometrically and electronically. Inspired by the proposed 6-p electron aromatic D 6h B 6 C 2À ion featuring a carbon atom in a planar hexacoordinate environment (denoted phC) at the center of a perfect B 6 hexagon, [12] we present herein an investigation by density functional theory (DFT) of a new class of sandwich-type complexes, D 6d [(h 6 -B 6 X) 2 M] (X = C, N; M = Mn, Fe, Co, Ni). These complexes are unique in that they contain two parallel h 6 -B 6 X hexagons centered with two nearly planar hexacoordinate carbon or nitrogen atoms (phN) located along the sixfold molecular axis. The results obtained in this work provide an important extension to the traditional concept of sandwich-type complexes by incorporating hexacoordinate carbon or nitrogen atoms in the systems and present a viable possibility to stabilize and characterize phC or phN atoms in future experiments. To the best of our knowledge, there have been no investigations reported to date on B 6 C 2À ligands in metallocene-like complexes.DFT structural optimizations at the B3LYP/6-311 + G-(3df) level [13][14][15] were performed on the sandwich complexes under investigation and imaginary frequencies and DFT wavefunction instabilities checked at the same theoretical level. Natural bond orbital (NBO) [16] analyses were implemented to gain insight into the bonding pattern of the complexes. Figure 1 and Figure 2 depict the optimized structures of Fe-containing complexes, and Figure 3 shows the MO pictures of the top 13 occupied energy levels of D 6d [(h 6 -B 6 C) 2 Fe] 2À (with one orbital shown for two degenerate MOs). These optimum structures are well-maintained when symmetry constraints are removed. Co-, Ni-, and Mncentered complexes have the same geometries and similar MOs but have different energy levels. Table 1 tabulates the calculated bond lengths, natural atomic charges, lowest vibrational frequencies (ñ min ), highest occupied molecular orbital (HOMO) energies, and total Wiberg bond indices (WBIs) [12,17] of the constituent atoms for the complexes under investigation. Detailed geometrical and electronic properties of 28 neutral and charged complex ions that contain B 6 X 2À