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Benzoquinone-Bridged Heterocyclic Zwitterions as Building Blocks for Molecular Semiconductors and Metals.
Lekin, Kristina; Leitch, Alicea A; Assoud, Abdeljalil; Yong, Wenjun; Desmarais, Jacques; Tse, John S; Desgreniers, Serge; Secco, Richard A; Oakley, Richard T.
Afiliação
  • Lekin K; Department of Chemistry , University of Waterloo , Waterloo , Ontario N2L 3G1 , Canada.
  • Leitch AA; Department of Chemistry , University of Waterloo , Waterloo , Ontario N2L 3G1 , Canada.
  • Assoud A; Department of Chemistry , University of Waterloo , Waterloo , Ontario N2L 3G1 , Canada.
  • Yong W; Department of Earth Sciences , University of Western Ontario , London , Ontario N6A 5B7 , Canada.
  • Desmarais J; Department of Physics , University of Saskatchewan , Saskatoon , Saskatchewan S7N 5E2 , Canada.
  • Tse JS; Department of Physics , University of Saskatchewan , Saskatoon , Saskatchewan S7N 5E2 , Canada.
  • Desgreniers S; Department of Physics , University of Ottawa , Ottawa , Ontario K1N 6N5 , Canada.
  • Secco RA; Department of Earth Sciences , University of Western Ontario , London , Ontario N6A 5B7 , Canada.
  • Oakley RT; Department of Chemistry , University of Waterloo , Waterloo , Ontario N2L 3G1 , Canada.
Inorg Chem ; 57(8): 4757-4770, 2018 Apr 16.
Article em En | MEDLINE | ID: mdl-29620356
ABSTRACT
In pursuit of closed-shell building blocks for single-component organic semiconductors and metals, we have prepared benzoquino-bis-1,2,3-thiaselenazole QS, a heterocyclic selenium-based zwitterion with a small gap (λmax = 729 nm) between its highest occupied and lowest unoccupied molecular orbitals. In the solid state, QS exists in two crystalline phases and one nanocrystalline phase. The structures of the crystalline phases (space groups R3 c and P21/ c) have been determined by high-resolution powder X-ray diffraction methods at ambient and elevated pressures (0-15 GPa), and their crystal packing patterns have been compared with that of the related all-sulfur zwitterion benzoquino-bis-1,2,3-dithiazole QT (space group Cmc21). Structural differences between the S- and Se-based materials are interpreted in terms of local intermolecular S/Se···N'/O' secondary bonding interactions, the strength of which varies with the nature of the chalcogen (S vs Se). While the perfectly two-dimensional "brick-wall" packing pattern associated with the Cmc21 phase of QT is not found for QS, all three phases of QS are nonetheless small band gap semiconductors, with σRT ranging from 10-5 S cm-1 for the P21/ c phase to 10-3 S cm-1 for the R3 c phase. The bandwidths of the valence and conduction bands increase with applied pressure, leading to an increase in conductivity and a decrease in thermal activation energy Eact. For the R3 c phase, band gap closure to yield an organic molecular metal with a σRT of ∼102 S cm-1 occurs at 6 GPa. Band gaps estimated from density functional theory band structure calculations on the ambient- and high-pressure crystal structures of QT and QS correlate well with those obtained experimentally.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Revista: Inorg Chem Ano de publicação: 2018 Tipo de documento: Article País de afiliação: Canadá

Texto completo: 1 Base de dados: MEDLINE Idioma: En Revista: Inorg Chem Ano de publicação: 2018 Tipo de documento: Article País de afiliação: Canadá