T. Jayasekharan (1912891)T. K. Ghanty (2297782)
The structure, stability, energy partition analysis, and charge redistribution of endohedral complexes formed between Au<sub>32</sub> cluster with alkali metal cations, such as Li<sup>+</sup>, Na<sup>+</sup>, K<sup>+</sup>, Rb<sup>+</sup>, and Cs<sup>+</sup>, have been investigated using the density functional theory method. All alkali metal cations can be stably encapsulated in both the <i>I</i><sub><i>h</i></sub> and the <i>C<sub>s</sub></i> symmetry structural forms [<i>I</i><sub><i>h</i></sub>-(X@Au<sub>32</sub>)<sup>+</sup> and <i>C</i><sub><i>s</i></sub>-(X@Au<sub>32</sub>)<sup>+</sup>]. Smaller cations are found to be more stable in the <i>C<sub>s</sub></i> symmetry structure. A higher charge-transfer characteristic is noted when the Au<sub>32</sub> cage is encapsulated with smaller-sized alkali ions than larger-sized ions in both the structures. Vibrational frequency calculation data show imaginary frequency values for Li<sup>+</sup> and Na<sup>+</sup> ions in the <i>I</i><sub><i>h</i></sub>-(X@Au<sub>32</sub>) system, which indicates the free movements of these ions in the cage, whereas all dopant ions show positive IR frequency values for <i>C</i><sub><i>s</i></sub>-(X@Au<sub>32</sub>), suggesting the existence of weak bonding between dopants and the cage. The analysis of structural, energetic, and charge-transfer data indicates that the K<sup>+</sup>, Rb<sup>+</sup>, and Cs<sup>+</sup> dopant ions occupy the central position of the Au<sub>32</sub> cage and retain the <i>I</i><sub><i>h</i></sub> symmetric structure of the Au<sub>32</sub> cluster, whereas the smaller-sized Li<sup>+</sup> and Na<sup>+</sup> occupy the off-center site and are more stable in <i>C</i><sub><i>s</i></sub>-(X@Au<sub>32</sub>). Morokuma-type energy decomposition analysis data indicate a significantly higher Pauli repulsion energy with Li<sup>+</sup> and Na<sup>+</sup> dopants in the <i>C</i><sub><i>s</i></sub>-(X@Au<sub>32</sub>) structure than in the <i>I</i><sub><i>h</i></sub>-(X@Au<sub>32</sub>) structure; however, for other dopant ions, this interaction is almost the same for both <i>I</i><sub><i>h</i></sub> and <i>C</i><sub><i>s</i></sub> structures. A similar trend is reflected in the variation in the orbital interaction energy term, which is considerably higher for Li<sup>+</sup> and Na<sup>+</sup> ions in the <i>C</i><sub><i>s</i></sub> structure and is almost the same for other ions in the <i>C</i><sub><i>s</i></sub> and <i>I</i><sub><i>h</i></sub> structures. From the charge-transfer data, a halogen-like behavior of Au<sub>32</sub> is noted when the cluster is doped with the Cs<sup>+</sup> ion, which is rather unusual. Thus, encapsulation of larger cations, such as K<sup>+</sup>, Rb<sup>+</sup>, and Cs<sup>+</sup>, into the Au<sub>32</sub> fullerene may be one of the possible ways of detecting the elusive <i>I</i><sub><i>h</i></sub> structure of Au<sub>32</sub> by mass spectrometry.
Kohei Sambe (8654118)Norihisa Hoshino (1358646)Takashi Takeda (339511)Takayoshi Nakamura (1410913)Tomoyuki Akutagawa (1358634)
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