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

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

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