4 research outputs found

    Sc<sub>2</sub>O@<i>C</i><sub>2<i>v</i></sub>(5)‑C<sub>80</sub>: Dimetallic Oxide Cluster Inside a C<sub>80</sub> Fullerene Cage

    No full text
    A new oxide cluster fullerene, Sc<sub>2</sub>O@<i>C</i><sub>2<i>v</i></sub>(5)-C<sub>80</sub>, has been isolated and characterized by mass spectrometry, UV–vis–NIR absorption spectroscopy, cyclic voltammetry, <sup>45</sup>Sc NMR, DFT calculations, and single crystal X-ray diffraction. The crystallographic analysis unambiguously elucidated that the cage symmetry was assigned to <i>C</i><sub>2<i>v</i></sub>(5)-C<sub>80</sub> and suggests that the Sc<sub>2</sub>O cluster is ordered inside the cage. The crystallographic data further reveals that the Sc1–O–Sc2 angle is much larger than that found in Sc<sub>2</sub>O@<i>T<sub>d</sub></i>(19151)-C<sub>76</sub> but almost comparable to that in Sc<sub>2</sub>O@<i>C</i><sub><i>s</i></sub>(6)-C<sub>82</sub>, suggesting that the endohedral Sc<sub>2</sub>O unit is flexible and can display large variation in the Sc–O–Sc angle, which depends on the size and shape of the cage. Computational studies show that there is a formal transfer of four electrons from the Sc<sub>2</sub>O unit to the C<sub>80</sub> cage, i.e., (Sc<sub>2</sub>O)<sup>4+</sup>@(C<sub>80</sub>)<sup>4–</sup>, and the HOMO and LUMO are mainly localized on the C<sub>80</sub> framework. Moreover, thermal and entropic effects are seen to be relevant in the isomer selection. Comparative studies between the recently reported Sc<sub>2</sub>C<sub>2</sub>@C<sub>2<i>v</i></sub>(5)-C<sub>80</sub> and Sc<sub>2</sub>O@<i>C</i><sub>2<i>v</i></sub>(5)-C<sub>80</sub> reveal that, despite their close structural resemblance, subtle differences exist on the crystal structures, and the clusters exert notable impact on their spectroscopic properties as well as interactions between the clusters and corresponding cages

    Sc<sub>2</sub>O@<i>C</i><sub>3<i>v</i></sub>(8)‑C<sub>82</sub>: A Missing Isomer of Sc<sub>2</sub>O@C<sub>82</sub>

    No full text
    By introducing CO<sub>2</sub> as the oxygen source during the arcing process, a new isomer of Sc<sub>2</sub>O@C<sub>82</sub>, Sc<sub>2</sub>O@<i>C</i><sub>3<i>v</i></sub>(8)-C<sub>82</sub>, previously investigated only by computational studies, was discovered and characterized by mass spectrometry, UV–vis–NIR absorption spectroscopy, cyclic voltammetry, <sup>45</sup>Sc NMR, density functional theory (DFT) calculations, and single-crystal X-ray diffraction. The crystallographic analysis unambiguously elucidated that the cage symmetry was assigned to <i>C</i><sub>3<i>v</i></sub>(8) and suggests that Sc<sub>2</sub>O cluster is disordered inside the cage. The comparative studies of crystallographic data further reveal that the Sc1–O–Sc2 angle is in the range of 131.0–148.9°, much larger than that of the Sc<sub>2</sub>S@<i>C</i><sub>3<i>v</i></sub>(8)-C<sub>82</sub>, demonstrating a significant flexibility of dimetallic clusters inside the cages. The electrochemical studies show that the electrochemical gap of Sc<sub>2</sub>O@<i>C</i><sub>3<i>v</i></sub>(8)-C<sub>82</sub> is 1.71 eV, the largest among those of the oxide cluster fullerenes (OCFs) reported so far, well correlated with its rich abundance in the reaction mixture of OCF synthesis. Moreover, the comparative electrochemical studies suggest that both the dimetallic clusters and the cage structures have major influences on the electronic structures of the cluster fullerenes. Computational studies show that the cluster can rotate and change the Sc–O–Sc angle easily at rather low temperature

    Isomeric Sc<sub>2</sub>O@C<sub>78</sub> Related by a Single-Step Stone–Wales Transformation: Key Links in an Unprecedented Fullerene Formation Pathway

    No full text
    It has been proposed that the fullerene formation mechanism involves either a top-down or bottom-up pathway. Despite different starting points, both mechanisms approve that particular fullerenes or metallofullerenes are formed through a consecutive stepwise process involving Stone–Wales transformations (SWTs) and C<sub>2</sub> losses or additions. However, the formation pathway has seldomly been defined at the atomic level due to the missing-link fullerenes. Herein, we present the isolation and crystallographic characterization of two isomeric clusterfullerenes Sc<sub>2</sub>O@<i>C</i><sub>2<i>v</i></sub><i>(3)</i>-C<sub>78</sub> and Sc<sub>2</sub>O@<i>D</i><sub>3<i>h</i></sub><i>(5)</i>-C<sub>78</sub>, which are closely related via a single-step Stone–Wales (SW) transformation. More importantly, these novel Sc<sub>2</sub>O@C<sub>78</sub> isomers represent the key links in a well-defined formation pathway for the majority of solvent-extractable clusterfullerenes Sc<sub>2</sub>O@C<sub>2<i>n</i></sub> (<i>n</i> = 38–41), providing molecular structural evidence for the less confirmed fullerene formation mechanism. Furthermore, DFT calculations reveal a SWT with a notably low activation barrier for these Sc<sub>2</sub>O@C<sub>78</sub> isomers, which may rationalize the established fullerene formation pathway. Additional characterizations demonstrate that these Sc<sub>2</sub>O@C<sub>78</sub> isomers feature different energy bandgaps and electrochemical behaviors, indicating the impact of SW defects on the energetic and electrochemical characteristics of metallofullerenes

    Facile Synthesis of an Extensive Family of Sc<sub>2</sub>O@C<sub>2<i>n</i></sub> (<i>n</i> = 35–47) and Chemical Insight into the Smallest Member of Sc<sub>2</sub>O@<i>C</i><sub>2</sub>(7892)–C<sub>70</sub>

    No full text
    An extensive family of oxide cluster fullerenes (OCFs) Sc<sub>2</sub>O@C<sub>2<i>n</i></sub> (<i>n</i> = 35–47) has been facilely produced for the first time by introducing CO<sub>2</sub> as the oxygen source. Among this family, Sc<sub>2</sub>O@C<sub>70</sub> was identified as the smallest OCF and therefore isolated and characterized by mass spectrometry, <sup>45</sup>Sc nuclear magnetic resonance, UV–vis–near-infrared absorption spectroscopy, cyclic voltammetry, and density functional theory calculations. The combined experimental and computational studies reveal a non-isolated pentagon rule isomer Sc<sub>2</sub>O@C<sub>2</sub>(7892)–C<sub>70</sub> with reversible oxidative behavior and lower bandgap relative to that of Sc<sub>2</sub>S@<i>C</i><sub>2</sub>(7892)–C<sub>70</sub>, demonstrating a typical example of unexplored OCF and underlining its cluster-dependent electronic properties
    corecore