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The Various Packing Structures of Tb@C(82) (I, II) Isomers in Their Cocrystals with Ni(OEP)

Soot-containing terbium (Tb)-embedded fullerenes were prepared by evaporation of Tb(4)O(7)-doped graphite rods in an electric arc discharge chamber. After 1,2,4-trichlorobenzene extraction of the soot and rotary evaporation of the extract, a solid product was obtained and then dissolved into toluene...

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Detalles Bibliográficos
Autores principales: Dong, Wei, Zhou, Qin, Shen, Wangqiang, Yang, Le, Jin, Peng, Lu, Xing, Lian, Yongfu
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10054076/
https://www.ncbi.nlm.nih.gov/pubmed/36985888
http://dx.doi.org/10.3390/nano13060994
Descripción
Sumario:Soot-containing terbium (Tb)-embedded fullerenes were prepared by evaporation of Tb(4)O(7)-doped graphite rods in an electric arc discharge chamber. After 1,2,4-trichlorobenzene extraction of the soot and rotary evaporation of the extract, a solid product was obtained and then dissolved into toluene by ultrasonication. Through a three-stage high-pressure liquid chromatographic (HPLC) process, Tb@C(82) (I, II) isomers were isolated from the toluene solution of fullerenes and metallofullerenes. With the success of the growth of cocrystals of Tb@C(82) (I, II) with Ni(OEP), the molecular structures of Tb@C(82) (I) and Tb@C(82) (II) were confirmed to be Tb@C(2v)(9)-C(82) and Tb@Cs(6)-C(82), respectively, based on crystallographic data from X-ray single-crystal diffraction. Moreover, it was found that Tb@C(82) (I, II) isomers demonstrated different packing behaviors in their cocrystals with Ni(OEP). Tb@C(2v)(9)-C(82) forms a 1:1 cocrystal with Ni(OEP), in which Tb@C(2v)(9)-C(82) is aligned diagonally between the Ni(OEP) bilayers to form zigzag chains. In sharp contrast, Tb@Cs(6)-C(82) forms a 2:2 cocrystal with Ni(OEP), in which Tb@Cs(6)-C(82) forms a centrosymmetric dimer that is aligned linearly with Ni(OEP) pairs to form one-dimensional structures in the a–c lattice plane. In addition, the distance of a Ni atom in Ni(OEP) to the Cs(6)-C(82) cage is much shorter than that to the C(2v)(9)-C(82) one, indicative of a stronger π-π interaction between Ni(OEP) and the C(82) carbon cage in the cocrystal of Tb@C(S)(6)-C(82) and Ni(OEP). Density functional theory calculations reveal that the regionally selective dimerization of Tb@C(S)(6)-C(82) is the result of a dominant unpaired spin existing on a particular C atom of the C(S)(6)-C(82) cage.