Influence of 3d transition metals (Fe, Co) on the structural, electrical and magnetic properties of C60 nano-cage

被引:38
作者
Javan, M. Bezi [1 ]
Tajabor, N. [1 ]
Behdani, M. [1 ]
Rokn-Abadi, M. Rezaee [1 ]
机构
[1] Ferdowsi Univ Mashhad, Dept Phys, Mashhad, Iran
关键词
Transition metal; Endohedral fullerene; Exohedral fullerene; Heterofullerene; ELECTRONIC-PROPERTIES;
D O I
10.1016/j.physb.2010.09.035
中图分类号
O469 [凝聚态物理学];
学科分类号
070205 ;
摘要
Total energy calculations of C-60 nano-cage doped with transition metals (TM = Fe and Co atoms) endohedrally, exohedrally, and substitutionally were performed using the density functional theory with the generalized gradient approximation along five radial paths inside and outside of the fullerene. The full geometry optimization near the minimum of the binding energy curves shows that the most stable position of the Fe atom in the TM@C-60 system is below the carbon atom, while that of the Co atom is below the middle of the double bond between the carbon atoms. Also the most stable position of both TM atoms in TM: C-60 systems is above the double bond. Results reveal that for all examined structures, the Co atom has larger binding energy than that of Fe atom. It is also found that for all complexes additional peaks contributed by TM-3d, 4s and 4p states appear in the highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO) gap of the host cluster. The mid-gap states are mainly due to the hybridization between TM-3d, 4s and 4p orbitals and the cage pi orbitals. Because of the interaction between the TM atom and the fullerene cage, the charge depletion of TM-4s orbital to TM-3d and 4p orbitals occurs and the magnetic moment of the incorporated TM atom reduces in all cases. Furthermore, the Mulliken charge population analysis shows that overall charge transfer occurs from the TM atom to the cage. (C) 2010 Elsevier B.V. All rights reserved.
引用
收藏
页码:4937 / 4942
页数:6
相关论文
共 31 条
  • [1] DENSITY-FUNCTIONAL EXCHANGE-ENERGY APPROXIMATION WITH CORRECT ASYMPTOTIC-BEHAVIOR
    BECKE, AD
    [J]. PHYSICAL REVIEW A, 1988, 38 (06): : 3098 - 3100
  • [2] Experimental and computational studies of heterofullerenes
    Billas, IML
    Branz, W
    Malinowski, N
    Tast, F
    Heinebrodt, M
    Martin, TP
    Massobrio, C
    Boero, M
    Parrinello, M
    [J]. NANOSTRUCTURED MATERIALS, 1999, 12 (5-8): : 1071 - 1076
  • [3] Cage substitution in metal-fullerene clusters
    Branz, W
    Billas, IML
    Malinowski, N
    Tast, F
    Heinebrodt, M
    Martin, TP
    [J]. JOURNAL OF CHEMICAL PHYSICS, 1998, 109 (09) : 3425 - 3430
  • [4] THE GROUND AND EXCITED-STATES OF C60M AND C60M+ (M=O, F, K, CA, MN, CS, BA, LA, EU, U)
    CHANG, AHH
    ERMLER, WC
    PITZER, RM
    [J]. JOURNAL OF CHEMICAL PHYSICS, 1991, 94 (07) : 5004 - 5010
  • [5] DEAN JA, 1996, MATER SCI FORUM, V19, P217
  • [6] Ding CG, 1999, J CHEM PHYS, V111, P8481, DOI 10.1063/1.480188
  • [7] Fowler PW., 1995, An atlas of fullerenes
  • [8] Optical properties of endohedral Li@C60
    Gromov, A
    Krawez, N
    Lassesson, A
    Ostrovskii, DI
    Campbell, EEB
    [J]. CURRENT APPLIED PHYSICS, 2002, 2 (01) : 51 - 55
  • [9] SUPERCONDUCTIVITY AT 18-K IN POTASSIUM-DOPED C-60
    HEBARD, AF
    ROSSEINSKY, MJ
    HADDON, RC
    MURPHY, DW
    GLARUM, SH
    PALSTRA, TTM
    RAMIREZ, AP
    KORTAN, AR
    [J]. NATURE, 1991, 350 (6319) : 600 - 601
  • [10] BOND LENGTHS IN FREE MOLECULES OF BUCKMINSTERFULLERENE, C60, FROM GAS-PHASE ELECTRON-DIFFRACTION
    HEDBERG, K
    HEDBERG, L
    BETHUNE, DS
    BROWN, CA
    DORN, HC
    JOHNSON, RD
    DEVRIES, M
    [J]. SCIENCE, 1991, 254 (5030) : 410 - 412