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ELECTRONIC PROPERTIES OF HEAVILY DOPED TRANS

Stafstrom, S., "Electronic Properties of Heavily Doped Trans-Polyacetylene", p.ll3 in Br6das, J.L. Silbey, R. (Eds.), Conjugated Polymers The Novel Science and technology of Highly Conducting and Nonlinear Optically Active Materials, Kluwer Academic Publishers, Norwell, MA, USA (1991). [Pg.658]

ELECTRONIC PROPERTIES OF HEAVILY DOPED TRANS-POLYACETYLENE... [Pg.115]

Within the continuum model of Takayama, Lin-Liu, and Maki (the TLM model) [27], Dinter [28] has shown that a new type of superlattice exists for tranS (CH). This new type of lattice, which contains considerable dimerization, has a lower total energy than that of the soliton lattice for doping levels above 8%. The electronic band structure corresponding to this lattice configuration contains a partially filled band, i.e., a gapless metallic state exists for this type of lattice. A crossover from the soliton lattice to this new superlattice could therefore explain the onset of metallic properties in heavily doped trans-(CH)y, However, as pointed out by Dinter, calculations using the more realistic discrete SSH model have to be performed in order to check whether or not the new lattice is a mere artifact of the TLM model. [Pg.117]

The metallic properties of the heavily-doped polymers provided the initial focus of interest in the electronic properties, but the theoretical framework for the modelling of the electronic excitations due to Rice [5] and Su et al [6], which for the case of trans-polyacetylene take the form of solitary-wave excitations of the chain, has broadened the area of interest to cover, in particular, the optical and non-linear optical properties of this class of polymos. [Pg.556]


See other pages where ELECTRONIC PROPERTIES OF HEAVILY DOPED TRANS is mentioned: [Pg.116]    [Pg.65]   


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