COMPARISON OF SOLITON GEOMETRY AND CHARGE-DENSITY-WAVE STRUCTURE, ANDBAND-GAPS, BETWEEN ODD POLYENE AND SYMMETRICAL POLYMETHINE CYANINE (BROOKER) IONS AND T-POLYACETYLENE-SCF AND MODEL HAMILTONIAN APPROACHES WITH IMPLICATIONS FOR MOLECULAR WIRES AND SWITCHES
Jr. Reimers et al., COMPARISON OF SOLITON GEOMETRY AND CHARGE-DENSITY-WAVE STRUCTURE, ANDBAND-GAPS, BETWEEN ODD POLYENE AND SYMMETRICAL POLYMETHINE CYANINE (BROOKER) IONS AND T-POLYACETYLENE-SCF AND MODEL HAMILTONIAN APPROACHES WITH IMPLICATIONS FOR MOLECULAR WIRES AND SWITCHES, Molecular crystals and liquid crystals science and technology. Section A, Molecular crystals and liquid crystals, 234, 1993, pp. 51-57
The geometric and electronic structures of odd polyene anions and the
isoelectronic Brooker ions are examined by SCF quantum chemical method
s in both the small and large (infinite chain) limit. For both types o
f ion, a geometric and charge density wave soliton is established, wit
h half widths 6.9-7.2 and 9.4 CH units respectively. The odd polyene a
nions retain C2v symmetry, but the Brooker ions are predicted to break
symmetry for chain lengths larger than about 15 CH units. Where the f
inite-length ions are used as bridges (molecular wires) linking donor
and acceptor groups, rates of charge transfer will be considerably enh
anced over those of even-membered polyenes in symmetrical structures;
where symmetry is broken, the ion may function as a charged soliton mo
lecular switch. Relations between properties of finite-length ions and
those of t-polyacetylene are discussed.