Endohedral complex of fullerene C60 with tetrahedrane, C4H4@C60
Introduction
Since lanthanum atom was firstly placed into the fullerene C60 cage [1], endohedral fullerenes, the spherical carbon molecules incorporating single atoms [2], [3], [4], [5] and noble gases [6], [7], [8] or small molecules and clusters [9], [10], [11] inside the framework have attracted great interest in their physical and/or chemical properties such as pseudoatom behavior, magnetism, nonlinear optical behaviors, and superconductivity. However, the production rate of the endohedral fullerenes is quite low compared with the ordinary fullerenes. The preparation of endohedral fullerenes has so far relied on hard to control physical processes, such as co-vaporization of carbon and metal atoms [2] or high-pressure/high-temperature treatment with noble gases [7], which yield only limited quantities (e.g., only a few milligrams) of a pure product after laborious isolation procedures. Due to the extreme difficulties in producing macroscopic quantities and isolating pure samples, theoretical studies are helpful tools in investigating and predicting the structural and electronic properties of endohedral fullerenes. For example, theoretical calculations on lanthanum metallofullerene La@C82 [12], [13] suggested that the La atom donated its three valence electrons to C82 to form an endohedral complex La3+C823−, which was confirmed by electron paramagnetic resonance (EPR) studies [14]. Gauge-independent atomic orbital (GIAO) and the nucleus-independent chemical shift (NICS) calculations for the encapsulated hydrogen in H2@C60 and its derivatives interpreted well the experimental data [11]. In N@C60, P@C60 and C@C60, the N, P and C atoms retain their atomic character when trapped in the cage [4], [15], [16], [17], while towards encaged small molecules, C60 acted as a polarizable sphere that stabilized the polar molecules and destabilized the nonpolar ones [18], [19].
Tetrahedrane C4H4 (THD) is a theoretically interesting molecule, and the problem of its synthesis was recognized more than half a century ago but only its derivatives had been obtained [20], [21]. As a result of the enormous angular strain [22], theoretical works predicted its stability in the absence of other reactants [23], while in the derivatives the lability of THD is circumvented by means of spatial shielding of the tetrahedrane framework by four bulky groups [21]. Since the fullerene cage may act as a partial Faraday cage that shields the atom on molecule trapped inside from the majority of the field applied [4], [24], it can be viewed as a nearly ideal “container” or “trap” for any highly reactive complex. Here we study the endohedral complexes of fullerenes C60 with THD. A question of major interest is whether the fullerene cage can stablize the trapped tetrahedrane. On the other hand, as tetrahedrane can isomerizes to cyclobutadiene [25], we also consider the inclusion of D2h cyclobutadiene in the fullerene cage. We hope that the present study will encourage further theoretical and experimental analysis of the system.
Section snippets
Computational details
Geometry optimizations were performed at the B3LYP/6–31G(d) hybrid HF/DFT level of theory. To ensure that true stationary points had been found, harmonic vibrational frequencies were also calculated by analytic evaluation of the second derivative of the energy with respect to nuclear displacement. The B3LYP functional was chosen because the inclusion of electron correlation was important for accurate geometry prediction. Our experiences of theoretical calculations on C60 related derivatives
Results and discussions
The B3LYP/6–31G(d) optimized geometries were shown in Fig. 1. Some geometry parameters were listed in Table 1. The bond lengths of C60 are 1.395 and 1.454 Å for the 6/6 and 6/5 bonds respectively. This calculation result agrees satisfactorily with the measured values [31] as well as the results of the previous highest level calculations, MP2 with triple ξ plus polarization basis set [32].
The optimized bond lengths and bond angles of tetrahedrane with Td symmetry are r1 = 1.073 Å, r2 = 1.480 Å, α1 =
Summary
We have studied the structural and electronic properties of C4H4@C60 via Hartree–Fock self-consistent field (SCF) and density functional B3LYP levels of theory with the STO-3G and 6–31G(d) basis sets. The Td C4H4 is seated in the center of the C60 cage and the highly symmetrical Ih of the cage is reduced to C3v for C4H4@C60. Both the fullerene cage and the encaged tetrahedrane experienced considerable structural changes. However, the encapsulated C4H4 only exists in a molecular form inside the
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