Endohedral complex of fullerene C60 with tetrahedrane, C4H4@C60

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Abstract

B3LYP/6–31G(d) hybrid HF/DFT calculations were carried out to determine the structural and electronic properties of the endohedral complex of C60 with tetrahedrane C4H4. It was demonstrated that C4H4 was seated in the center of the C60 cage and existed in a molecular form inside the fullerene. The formation of this complex was endothermic with inclusion energy of 141.05 kcal/mol. C4H4 endohedral doping slightly perturbed the molecular orbitals of C60. The calculated HOMO–LUMO gaps, the electron affinity (EA) and the ionizational potential (IP) indicated that C4H4@C60 seemed to be more kinetically reactive than C60. The IR active modes and harmonic vibrational frequencies of C4H4@C60 were also discussed.

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

References (44)

  • D.E. Manolopoulos et al.

    Theoretical studies of the fullerenes: C34 to C70

    Chem. Phys. Lett.

    (1991)
  • X. Liu et al.

    Favorable structures for higher fullerenes

    Chem. Phys. Lett.

    (1992)
  • R.C. Haddon et al.

    Unified theory of the thermodynamic and kinetic criteria of aromatic character in the [4n + 2] annulenes

    Tetrahedron Lett.

    (1980)
  • J.R. Heath et al.

    Lanthanum complexes of spheroidal carbon shells

    J. Am. Chem. Soc.

    (1985)
  • H. Shinohara

    Endohedral metallofullerenes

    Rep. Prog. Phys.

    (2000)
  • H. Shiotani et al.

    Quantum chemical study on the configurations of encapsulated metal ions and the molecular vibration modes in endohedral dimetallofullerene La2@C80

    J. Am. Chem. Soc.

    (2004)
  • E. Shabtai et al.

    3He NMR of He@C606− and He@C706−. New records for the most shielded and the most deshielded 3He inside a fullerene

    J. Am. Chem. Soc.

    (1998)
  • M. Saunders et al.

    Noble gas atoms inside fullerenes

    Science

    (1996)
  • M. Saunders et al.

    Stable compounds of helium and neon: He@C60 and Ne@C60

    Science

    (1993)
  • Y. Murata et al.

    100% encapsulation of a hydrogen molecule into an open-cage fullerene derivative and gas-phase generation of H2@C60

    J. Am. Chem. Soc.

    (2003)
  • M. Murata et al.

    Synthesis and properties of endohedral C60 encapsulating molecular hydrogen

    J. Am. Chem. Soc.

    (2006)
  • K. Laasonen et al.

    Structural and electronic properties of La@C82

    Science

    (1992)
  • Cited by (0)

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