4 research outputs found
Sc<sub>2</sub>O@<i>C</i><sub>2<i>v</i></sub>(5)âC<sub>80</sub>: Dimetallic Oxide Cluster Inside a C<sub>80</sub> Fullerene Cage
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,
UVâvisâNIR 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 Sc1âOâSc2 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 ScâOâSc 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>4â</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)âC<sub>82</sub>: A Missing Isomer of Sc<sub>2</sub>O@C<sub>82</sub>
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, UVâvisâNIR 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 Sc1âOâSc2
angle is in the range of 131.0â148.9°, 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 ScâOâSc angle easily at rather low temperature
Isomeric Sc<sub>2</sub>O@C<sub>78</sub> Related by a Single-Step StoneâWales Transformation: Key Links in an Unprecedented Fullerene Formation Pathway
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 StoneâWales
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 StoneâWales
(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> = 38â41), 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> = 35â47) and Chemical Insight into the Smallest Member of Sc<sub>2</sub>O@<i>C</i><sub>2</sub>(7892)âC<sub>70</sub>
An extensive family of oxide cluster
fullerenes (OCFs) Sc<sub>2</sub>O@C<sub>2<i>n</i></sub> (<i>n</i> = 35â47) 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, UVâvisânear-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)âC<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)âC<sub>70</sub>, demonstrating a typical
example of unexplored OCF and underlining its cluster-dependent electronic
properties