Linear
Coordination Fullerene C<sub>60</sub> Polymer
[{Ni(Me<sub>3</sub>P)<sub>2</sub>}(μ‑η<sup>2</sup>,η<sup>2</sup>‑C<sub>60</sub>)]<sub>∞</sub> Bridged
by Zerovalent Nickel Atoms
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Abstract
Coordination nickel-bridged fullerene
polymer [{Ni(Me<sub>3</sub>P)<sub>2</sub>}(μ-η<sup>2</sup>,η<sup>2</sup>-C<sub>60</sub>)]<sub>∞</sub> (<b>1</b>) has been obtained via reduction of a Ni<sup>II</sup>(Me<sub>3</sub>P)<sub>2</sub>Cl<sub>2</sub> and C<sub>60</sub> mixture. Each nickel
atom is linked in the polymer with two fullerene units by η<sup>2</sup>-type Ni–C(C<sub>60</sub>) bonds of 2.087(8)–2.149(8)
Å length. Nickel atoms are coordinated to the 6–6 bonds
of C<sub>60</sub> as well as two trimethylphosphine ligands to form
a four-coordinated environment around the metal centers. Fullerene
cages approach very close to each other in the polymer with a 9.693(3)
Å interfullerene center-to-center distance, and two short interfullerene
C–C contacts of 2.923(7) Å length are formed. Polymer
chains are densely packed in a crystal with interfullerene center-to-center
distances between fullerenes from neighboring polymer chains of 9.933(3)
Å and multiple interfullerene C···C contacts.
As a result, three-dimensional dense fullerene packing is formed in <b>1</b>. According to optical and electron paramagnetic resonance
spectra, fullerenes are neutral in <b>1</b> and nickel atoms
have a zerovalent state with a diamagnetic d<sup>10</sup> electron
configuration. The density functional theory calculations prove the
diamagnetic state of the polymer with a singlet–triplet gap
wider than 1.37 eV