Structure of [60]fullerene with a mobile lithium cation inside

Author:

Aoyagi Shinobu1ORCID,Miwa Kazuhira1,Ueno Hiroshi2,Okada Hiroshi3ORCID,Matsuo Yutaka234ORCID,Kokubo Ken5ORCID

Affiliation:

1. Department of Information and Basic Science, Nagoya City University, Nagoya 467-8501, Japan

2. School of Chemistry, Northeast Normal University, 5268 Renmin Street, Changchun, Jilin 130024, People's Republic of China

3. Department of Mechanical Engineering, School of Engineering, The University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-8656, Japan

4. Hefei National Laboratory for Physical Sciences at the Microscale, University of Science and Technology of China, 96 Jinzhai Road, Hefei, Anhui 230026, People's Republic of China

5. Division of Applied Chemistry, Graduate School of Engineering, Osaka University, Suita, Osaka 565-0871, Japan

Abstract

The structure of crystalline [60]fullerene with a lithium cation inside (Li + @C 60 ) was determined by synchrotron radiation X-ray diffraction measurements to understand the electrostatic and thermal properties of the encapsulated Li + cation. Although the C 60 cages show severe orientation disorder in [Li + @C 60 ](TFPB )·C 4 H 10 O and [Li + @C 60 ](TFSI )·CH 2 Cl 2 , the Li + cations are rather ordered at specific positions by electrostatic interactions with coordinated anions outside the C 60 cage. The Li + @C 60 molecules in [Li + @C 60 ](ClO 4 ) with a rock-salt-type cubic structure are fully disordered with almost uniform spherical shell charge densities even at 100 K by octahedral coordination of ClO 4 tetrahedra and show no orientation ordering, unlike [Li + @C 60 ](PF 6 ) and pristine C 60 . Single-bonded (Li + @C 60 ) 2 dimers in [Li + @C 60 ](NiOEP)⋅CH 2 Cl 2 are thermally stable even at 400 K and form Li + –C bonds which are shorter than Li + –C bonds in [Li + @C 60 ](PF 6 ) and suppress the rotational motion of the Li + cations.

Funder

The Mitsubishi Foundation

The Murata Science Foundation

Publisher

The Royal Society

Subject

Multidisciplinary

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