Fig 1 shows the optimized geometries of the molecules. All these molecules are closed shell singlet in their global minima with C3v symmetry. The relative energies of different possible isomers are listed in Table S1, supporting information. Among the studied systems, the frontier molecular orbitals of the Be3-Fe and Be3-Zn has been shown (Fig 2). The Be-Be distance in metal free cyclic Be3 molecule is 2.210 Å which significantly shortens in the half sandwich complexes (Fig 1). The Wiberg bond indices for the TM-Be bonds, a measure of bond strength, are close to 0.9 for Fe, Ru and Os complexes while they are lower (~0.2) for the Zn, Cd and Hg complexes.
To investigate the mode of binding of Be3 fragment with the transition metals, we calculated the energy changes while displacing the transition metal atom from the centre to a distance r as shown in Scheme 2. Results based on single point calculations at PBE1PBE level of theory (Fig 3) reveals that all these complexes have the lowest energy at r = 0, i.e., Be3 fragment in these complexes feature η3 coordination mode.
Further to investigate the nature of bonding, we have performed charge decomposition analysis (CDA) Fe and Zn complexes respectively as representative case. Fig 4 shows the interaction diagram. The LUMO (lowest unoccupied molecular orbital) and LUMO+1 of Be3 fragment interact with the metal dz2 and s orbital. It is to be noted that the LUMO of Be3 fragment is a delocalized unoccupied π symmetric oribital while the LUMO+1 is the σ orbital. Occupation of these orbitals in the sandwich complex is expected to enhance aromaticity in the cyclic Be3 fragment.
We then turned to the aromaticity of the proposed molecules by performing nucleus independent chemical shift (NICS) calculations at the centre of the Be3 fragment in the complexes which is known as NICS(0) and 1 Å above the plane which we designated as NICS(1) [49] (Scheme 3, Table 1). It is worth mentioning that Be3 ring is anti-aromatic which is backed by positive NICS(0) value of 20 ppm. Upon complexation with the considered transition metals, significant aromaticity is induced in the Be3-TM complexes. In all the complexes, aromaticity is dominated by NICS(0), a measure of σ aromaticity. However, NICS(1) values, a measure of π aromaticity, are also significant. Thus, the calculated values of NICS suggest that the proposed sandwich complexes have dual σ and π aromaticity [51]. The presence of dual aromaticity is expected to increase the stability of the complexes. We therefore, calculated the bond dissociation energies (BDE, Table 2) and change in Gibbs free energies (∆G298) of their formation according to the following equation
Table 1: PBE1PBE calculated NICS values (ppm) of the proposed half-sandwich complexes.
Complexes
|
NICS (0) (ppm)
|
NICS (1) (ppm)
|
Be3-Fe
|
-31.57
|
-4.33
|
Be3-Ru
|
-25.45
|
-7.71
|
Be3-Os
|
-34.53
|
-11.4
|
Be3-Zn
|
-38.38
|
-15.72
|
Be3-Cd
|
-35.48
|
-14.15
|
Be3-Hg
|
-32.45
|
-12.81
|
Table 2: Bond dissociation energies (BDE, kcal/mol), ∆G298 (kcal/mol) of formation of proposed sandwich complexes and force constant, k (mDyne/Å).
Complex
|
BDE
|
∆G298
|
k
|
Be3-Fe
|
96.17
|
-88.14
|
1.278
|
Be3-Ru
|
154.86
|
-146.71
|
1.546
|
Be3-Os
|
187.83
|
-179.65
|
1.323
|
Be3-Zn
|
37.33
|
-29.67
|
0.62
|
Be3-Cd
|
32.56
|
-25.05
|
0.43
|
Be3-Hg
|
24.70
|
-17.25
|
0.32
|
The BDE values were calculated by considering the neutral Be3 and transition metal fragment. It is evident from Table 2 that all these complexes have high bond strength. The calculated BDE values are higher for Fe, Ru and Os while they are lower for Zn, Cd and Hg. The calculated values of the force constant (k, Table 2) are also higher for Fe, Ru and Os. Moreover, the change in Gibbs free energies (∆G298) for their formation is more negative for Fe, Ru and Os. However, ∆G298 values are negative in all cases suggesting their favorable thermodynamics of formation.
We then further analyzed the topological feature of electron density within the realm of quantum theory of atoms in molecules (QTAIM) [46] and electron localization function (ELF) [47-48]. QTAIM is based on topological properties of electron density and its derivatives. It describes the concept of bonding with the help of bond paths and critical points. The electron density (q) exhibits a maximum, a minimum, or a saddle point in space. These points are referred to as Critical Points (CPs). At this point, the first derivatives of q(rc) vanishes. The Laplacian (∇2ρ) plays a very vital role in the characterization of chemical bonding. Generally, for covalent interactions (also referred to as ‘‘open-shell” or ‘‘sharing” interactions), the electron density at the bond critical point (BCP), ρb, is large (>0.2 a.u) while its laplacian, ∇2ρ is large and negative. On the other hand, for closed-shell interactions (e.g., ionic, van der Waals, or hydrogen bonds), ρb is small (<0.10 au) and ∇2ρ is positive. However, a clear distinction between the closed-shell and covalent type of interaction is impossible without determination of the local electronic energy density, H(r). The local electronic energy density, H(r), given by H(r) = G(r) + V(r), where G(r) and V(r) are the local kinetic and potential energy densities, is negative for an interaction with significant covalent character and accounts for the lowering of potential energy of electrons at BCPs. The magnitude of H(r) reflects the ‘‘degree of covalency” present in a given interaction. Thus, some covalent (some polar bonds, donor–acceptor bonds, etc.) bonds are associated with positive values of r2 q and negative values of H(r) [52]. Table 3 contains the numerical data at different bond critical points. The Be-TM bonds are characterized by positive values of laplacian, ∇2ρ and negative values of local electronic energy density, H(r) suggesting polar covalent character of these bonds [52]. The presence of significant amount of electron density at the Be-Be-Be ring critical points is an indication of aromaticity [46].
Table 3. Electron density, ρ, at the bond critical point (bcp) and ring critical points (rcp), laplacian of electron density, ∇2ρ, local electronic energy density, H(r) and electron localization function, ELF values. All values are in a. u.
Molecule
|
bcp/rcp
|
ρ
|
∇2ρ
|
H(r)
|
ELF
|
Be3-Fe
|
Be-Fe bcp
Be-Be-Be rcp
|
0.058
0.043
|
0.077
0.044
|
-0.028
-0.006
|
0.22
0.43
|
Be3-Ru
|
Be-Ru bcp
Be-Be-Be rcp
|
0.073
0.041
|
0.068
0.041
|
-0.035
-0.005
|
0.18
0.45
|
Be3-Os
|
Be-Os bcp
Be-Be-Be rcp
|
0.076
0.038
|
0.070
0.036
|
-0.035
-0.007
|
0.16
0.48
|
Be3-Zn
|
Be-Zn bcp
Be-Be-Be rcp
|
0.067
0.041
|
0.068
0.042
|
-0.032
-0.008
|
0.18
0.34
|
Be3-Cd
|
Be-Cd bcp
Be-Be-Be rcp
|
0.071
0.032
|
0.062
0.040
|
-0.033
-0.005
|
0.16
0.28
|
Be3-Hg
|
Be-Hg bcp
Be-Be-Be rcp
|
0.061
0.034
|
0.057
0.044
|
-0.031
-0.005
|
0.14
0.28
|