Lattice structure of the fullerene ferromagnet TDAE–C60
Lattice structure of the fullerene ferromagnet TDAE–C60
复制标题
DOI:
10.1038/355331a0
复制
发表时间:
1992
期刊:
影响因子:
64.8
通讯作者:
P. Stephens;D. Cox;J. Lauher;L. Mihály;J. Wiley;P. Allemand;A. Hirsch;K. Holczer;Q. Li;J. Thompson;F. Wudl
中科院分区:
文献类型:
--
作者:
P. Stephens;D. Cox;J. Lauher;L. Mihály;J. Wiley;P. Allemand;A. Hirsch;K. Holczer;Q. Li;J. Thompson;F. Wudl
IN the brief time since the development of techniques for the purification of condensed phases of C60(refs 1, 2), compounds of C60have been synthesized that exhibit the important solid-state properties of superconductivity3,4and ferromagnetism5. The fact that the C60molecule participates in these two disparate effects is in itself striking; furthermore, the C60-based material has the highestTcof any molecular organic ferromagnet6. An understanding of the physical origin of this ferromagnetism is sure to require a knowledge of the crystal structure. Here we report on an X-ray diffraction study of the ferromagnet TDAE–C60, where TDAE is tetrakis(dimethylamino)ethylene, C2N4(CH3)8. We find that the composition is stoichiometric with 1:1 ratio of TDAE to C60. The structure has ac-centred monoclinic unit cell suggestive of an anisotropic, low-dimensional band structure. Any theory for the ferromagnetic behaviour will have to take this anisotropy into account.