Twelve pentagons in six pyracylene units designed C60 fullerene cage with icosahedral (Ih) symmetry which led to a single type of carbon atom and two types of C-C bonds including the [6, 6] and [5, 6] ring fusion sites. The length of the bond at [6, 6] and [5, 6] ring fusions in the optimized structure of C60 were estimated about 1.392 and 1.455 Å respectively, at the M06-2X/6-311 + G(d, p) level. They are in a perfect agreement with the previously reported values (1.401 and 1.458 Å correspondingly) [48, 49, 50, 51]. Each amination reaction added the elements NRR and H across a [6, 6] π-bond on [60] fullerene. A number of regiochemistry are possible but experimental evidence recommends that aminations prefer either a 1,2- or a 1,4-addition. The addition reaction of C60 with amines is a widely studied topic [21–23]. Moreover, 1,2-addition of amine to the [6, 6]-bond of fullerene C60 led to formation of two newly C-N bonds with 1.469 Å at the M06-2X/6-311 + G(d, p) level of theory. The [6, 6] C-C bond lengths of 1,2-diamino fullerene were equal to 1.628 Å, which are lengthier than normal C-C bond lengths in fullerene (1.401 Å) [30, 31]. To design of nine pincer fullerene ligands in this study, 1,2-diamino fullerene were utilized as precursors. The geometries of these pincer fullerene ligands together and the significant geometrical parameters are illustrated in Fig. 3. Table S1 (supplementary material) shows the geometrical coordination of the considered structures, calculated at the M06-2X/6-311G+(d, p) level of theory. The geometrical characteristics of the optimized structures of the pincer fullerene ligands are discussed shortly to have better pictures of these derivatives. There is a change from 108° in the pristine C60 fullerene and 95.5° in the diamino fullerene to ~ 99.1–99.3° in the pincer fullerenes in the obtained calculated bond angle between each of the attached sites and the two first neighboring atoms of the pentagon changes. In addition, the hexagon-hexagon bond is pulled outward from the fullerene surface with the bond length decreasing from 1.628 Å (in the C60(NH2)2) to 1.603–1.609 Å in pincer fullerenes. The selected bond distances (Å) i.e. Ccage-N 1.465–1.469, N − Si 1.760–1.767, Si − H 1.494–1.499, C − N 1.451–1.456, C − P 1.920–1.930 Å are consistent with the reported values for N-Heterocyclic σ-siliyl pincer ligands [20]. As mentioned above, the IR vibrational frequencies were computed for the systems at the same level of theory. In addition, the actual frequencies showed that they were structures with minimized energy. The distinctive IR spectroscopic fingerprints yielded valuable insight into the future experimental detections. However, it is notable that at the beginning, theoretical frequencies are overestimated universally in comparison with the results even in the case of more accurate methods. Therefore, the preset study is not an attempt to predict the exact frequencies. This study is aimed at finding patterns in the data than can help us determining different forms of pincer fullerenes. Figure 4 shows the simulated IR vibrational spectra of the SiH2-(NCH2PH2)2C60, and the prominent peaks are quite clear. Thus, it is better to discuss the spectra region by region. In the different vibrational frequencies theoretically found for SiH2(NCH2PH2)2C60, two lowest-energy modes of 505.6 and 612.0 cm− 1 correspond to out-of-plane bending of C-C bonds and breathing mode of fullerene cage. On the other hand, the following vibrations frequencies at 830.8 and 1011.6 cm− 1 are due to the out of plane wagging and in-plane scissoring of HSiH angles, respectively. The vibrational frequency at 2285 cm− 1 with highest intensity is assigned to the symmetric stretching of the SiH bonds coupled with the symmetric stretching of the PiH bonds. The SiH2(NCH2PH2)2C60 exhibits symmetric and asymmetric stretching of CH bonds at 3034 and 3113 cm− 1 respectively. Similar data were obtained for the pincer fullerene ligands, which are in agreement with those values obtained for N-Heterocyclic σ-siliyl pincer ligands.
In order to investigate the formation of the pincer fullerene ligands SiHR(NCH2PL2)2C60, R and L = H, CH3 and phenyl, the reactions of C60(NHCH2PPh2)2 with chlorosilanes SiHRCl2 (R = H, CH3 and phenyl) were taken into account (Fig. 2), and the reaction energies, Er were obtained in the standard way as follows:
Er = ESiHR(NCH2PL2)2C60 + E[Cl2] - E[C60(NHCH2PPh2)2] - E[SiHRCl2] (1)
where ESiHR(NCH2PL2)2C60 and E[C60(NHCH2PPh2)2] are total energies of the pincer fullerenes and C60(NHCH2PPh2)2 and E[Cl2] and E[SiHRCl2] refer to energies of Cl2 and chlorosilanes, respectively. As listed in Table 1, the calculated Er values of the formation of the considered pincer fullerenes is in 46.8–61.6 kcal/mol range, which are lower than the Er values obtained for the SiHR(NCH2PPh2)2C6H4 at the same theory level. In comparison between the calculated reaction energies of pincer fullerenes, some important results were found. As noted, to analyze the influence of the nature of the flanking arms and central silicon atom on fullerene pincer ligands, the substitution of flanking arms and central silicon atom with CH3 and phenyl groups was changed. Clearly, substituting flanking arms with CH3 and phenyl groups increased the reaction energies of the pincer fullerene ligands formation. While substituting of hydrogen of SiH2 with methyl led to a slight increase of the reaction energies, replacing of hydrogen with phenyl groups decreased the reaction energies of the considered pincer fullerenes.
Table 1
The total energies (Et in hartree), reacton energies (Er in kcal/mol), electrophilicities (ω in eV) and natural charge Q/e (e = 1.6 × 10− 19 C), for for the N‑Heterocyclic Silyl Pincer Fullerenes RSiH-(NCH2PL2)2C60 at the M06-2X/6-311 + G(d, p) level of theory.
|
|
Et
|
Er
|
ω
|
Q/e(Si)
|
Q/e(P)
|
1
|
SiH2(NCH2PH2)2C60
|
-3430.441947
|
49.8
|
4.12
|
1.367
|
0.234
|
2
|
SiH2(NCH2P(CH3)2)2C60
|
-3586.817778
|
60.8
|
4.17
|
1.373
|
0.77
|
3
|
SiH2(NCH2(PpH)2)2C60
|
-4349.193209
|
59.9
|
4.11
|
1.375
|
0.806
|
4
|
SiHCH3(NCH2PH2)2C60
|
-3469.548665
|
50.6
|
4.14
|
1.65
|
0.229
|
5
|
SiHCH3(NCH2P(CH3)2)2C60
|
-3625.924495
|
61.6
|
4.16
|
1.661
|
0.766
|
6
|
SiHCH3(NCH2(PpH)2)2C60
|
-4388.2994
|
61.0
|
4.12
|
1.659
|
0.797
|
7
|
SiHPh(NCH2PH2)2C60
|
-3660.144867
|
46.8
|
4.13
|
1.654
|
0.236
|
8
|
SiHPh(NCH2P(CH3)2)2C60
|
-3816.519828
|
58.4
|
4.22
|
1.653
|
0.779
|
9
|
SiHPh(NCH2(PpH)2)2C60
|
-4578.897951
|
55.8
|
4.23
|
1.664
|
0.815
|
To examine the electronic properties of the considered pincer ligands, electrophilicity was calculated, which can be used as a base to examine the electrophilic competency of the system under consideration through using the electronic chemical potential (µ) to measure tendency of the system to obtain an extra electron from next electron-rich species. At the same time, it uses hardness (η) to describe the system resistance to electron exchange with the environment. Parr et al. defined a general index for the electrophilicity strength [32]. The definition is based on the quantitative chemical concepts in DFT such as the electronic chemical potential (µ) and hardness (η) [33, 34]. Employing a quadratic and finite difference approximation, Parr et al. [32] interpreted that µ and η may be equal to µ= -(IP + EA)/2 and η = IP - EA [73]. The values of IP = E(M+) – E(M) and the EA = E(M) – E(M− ) were obtained based on vertical ionization potentials and electron affinities. Finally, the electrophilicity index was defined as ω = µ2/2η [33]. Therefore, electrophilicity ω values were obtained for the pincer ligands based the mentioned formula and listed in Table 1. As listed Table 1, the obtained electrophilicity values of the pincer fullerenes are in 4.11–4.23 eV range, which are larger than the electrophilicity values obtained for the fullerene derivatives with heterocyclic ring systems. It is notable that the substitution of hydrogen atoms of central SiH2 and PH2 do not have noticeable impact on the electrophilicity values of the pincer fullerenes, except for SiHPh(NCH2PH2)2C60 in which substituting flanking arms with CH3 and phenyl increases the electrophilicity of the considered pincer fullerenes.
The pincer-ligated metal complexes were prepared by adding a transition metal (Fe, Co, Ni and Cu) to the pincer bites. Through this, their formation based on structure, electronic properties, stability was predicted. Two five-member metallocyclic rings were formed by the complexation of a metal to three adjacent coplanar sites of pincer fullerene ligands. Figure 5 illustrates the geometries and the important geometrical parameters of these complexes. The criteria of stability of different pincer-ligated metal complexes namely the difference between the total energy of pincer-ligated metal complexes, the constituent, and individual transition metals, and pincer fullerene ligands were used to calculate binding energies (Eb). Using the counterpoise (CP) method [25], the binding energies were corrected for basis set superposition error (BSSE). Clearly, binding energies range from − 84.24 to -88.59 eV. It is notable that the metal-silicon bonds are shorter than expected for single covalent bonds. For example, Co-Si and Co-P bond lengths in Co-SiHPh(NCH2PH2)2C60 (2.271 and 2.201 Å) is smaller than the corresponding single Co-Si and Co-P bond lengths (2.43 and 2.19 Å). When the hybrid orbitals of the ligands and the hybrid orbitals of the metal atoms in the metal complexes are overlapped, delocalization of electrons happens. Therefore, we perform NBO analysis to have a deeper insight into the nature of electronic conjugation among the bonds in the pincer-ligated metal complexes. The NBO analysis is a useful tool to determine these delocalizations of the electrons. The NBOs have close relationship with the picture of localized bonds and lone pairs as basic units of molecular structure. It is possible therefore, to interpret ab initio wave-functions based on the classical Lewis structure concepts through transforming these functions to NBO form [28]. The present study is mostly about the results of second-order perturbation theory analysis of Fock matrix in NBO of the complexes. With regard to each donor NBO(i) and acceptor NBO(j), the stabilization energy E(2) pertinent to delocalization is obtained as follows [28, 29].
where qi represents the donor orbital occupancy, ϵi and ϵj represent the orbital energies, and
stands for the off-diagonal NBO Fock matrix element. With higher values of the E(2), the interaction between the donors and acceptors is intensified [10]. The strongest interactions of n* orbitals of transition metal atoms with lone pairs of phosphorous atoms and the Si-H σ* orbitals of central silicon atoms are listed Table 2. As seen, the strongest interaction of all happens because of the delocalization of electrons from lone pairs of phosphorous atoms (donor) in the flanking arms to the LP* of transition metals (acceptor) followed by the Si-H σ* orbitals of central silicon atoms (donor) to the LP* of transition metals (acceptor). For example the delocalization of electrons from the lone pairs of flanking arms phosphorous atoms to the n* orbitals of Fe atom resulted in the interaction of LP P with LP* Fe stabilizing the complex by about 48.41 kcal/mol. On the other hand, the delocalization of electrons from the Si-H σ* orbitals of central silicon atoms to the LP* orbitals of Fe atom stabilizes the complex by only 13.37 kcal/mol. Therefore, it seems that the delocalization of electrons from the lone pairs of flanking arms phosphorous atoms to the n* orbitals of Fe atoms is a more important factor for stabilizing the complexes in comparison to the orbitals of central silicon atoms.
Table 2
Binding energies (Eb in kcal/mol), M-Si and M-P bond lengths in A together with the second-order perturbation theory analysis of Fock matrix within NBO of the pincer-ligated metal complexes.
|
Eb
|
M-Si
|
M-P
|
E(2)*
|
E(2)**
|
Fe-SiHPh(NCH2PH2)2C60
|
-85.47
|
2.267
|
2.184
|
12.99
|
48.41
|
Co-SiHPh(NCH2PH2)2C60
|
-88.59
|
2.271
|
2.201
|
13.37
|
50.65
|
Ni-SiHPh(NCH2PH2)2C60
|
-87.31
|
2.259
|
2.211
|
13.28
|
50.05
|
Cu-SiHPh(NCH2PH2)2C60
|
-84.24
|
2.244
|
2.209
|
13.1
|
48.25
|
* BD SiH (donor)→ LP* Fe (acceptor) in kcal/mol |
** LP P (donor)→ LP* Fe (acceptor) in kcal /mol |