ELECTRONIC-STRUCTURE, CONDUCTIVITY, AND SUPERCONDUCTIVITY OF ALKALI-METAL DOPED C-60
ELECTRONIC-STRUCTURE, CONDUCTIVITY, AND SUPERCONDUCTIVITY OF ALKALI-METAL DOPED C-60
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DOI:
10.1021/ar00015a005
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发表时间:
1992-03-01
影响因子:
18.3
通讯作者:
HADDON, RC
中科院分区:
文献类型:
--
作者:
HADDON, RC
This Accountsummarizes work carried out at AT&T Bell Laboratories on the fullerenes during the past few years. I begin with a discussion of the electronic structure of these molecules which was inferred from general theories soon after the fullerenes were identified by Kroto, Heath, O’Brien, Curl, andSmalley. 1 The high electron affinity2, 3 and the existence of radiating x-orbitals4 when combined with simple ideas for the design of molecular metals and superconductors led us to pursue conductivity and superconductivity in the alkali metal doped fullerenes immediatelyafter the synthesis of C60 and C70 by Kratschmer, Lamb, Fosti-ropoulos, and Huffman. 5 In the remainder of the Ac-count I discuss the progress in the preparation and characterization of conducting and superconducting solids and films based on these materials and the cur-rent state of understanding which has been attained in this field.The spheroidal geometry of the fullerenes is their most arresting feature, and it directly determines their singular electronic structure. As these molecules are solely composed of trivalent carbon atoms, the presence of a surface is implied, andgiven thefact that this valence state of carbon is best accommodated in sixmembered rings (6-MRs), there is a tendency toward benzenoid structures. If the fullerenes were composed solely of conjugated 6-MRs, such as occurs in benzene and graphite, they would be alternant hydrocarbons (AHs). 6 Among the more important properties this classification confers is symmetry between the occupied and unoccupied molecular orbitals, that is, the bonding and antibonding HMO energy levels are symmetrically disposed about the energy zero. 6 Thus it is to be ex-pected that benzenoid hydrocarbons and graphite will accept and donate electrons with equal ease. With appropriate adjustment of the reference potential, these compounds do exhibit mirror-image reduction and ox-idation potentials. 7 Furthermore, polyacetylene and graphite (the infinite one-and two-dimensional AHs), undergo both n-and p-type dopingin the solid state. 8 The homologation of benzene rings produces a sur-face, and ultimately graphite, but with the inevitable dangling bonds due to the unsatisfied carbon valencies at the periphery of the sheet. The genius in the pro-duction of the fullerenes was the creation of an environment in which the formation of other structural possibilities was competitive with the generation of a purely benzenoid fragment with dangling bonds. 1, 5 In order to remove the dangling bonds entirely, the edges of the surface must be eliminated, and this requires the