IODINE CHARGE-TRANSFER SALTS OF BENZENE-BRIDGED BIS(1,2,3,5-DISELENADIAZOLYL) DIRADICALS - ELECTROCRYSTALLIZATION AND SOLID-STATE CHARACTERIZATION OF 1,3-[(SE2N2C)C6H4(CN2SE2)][I] AND 1,4-[(SE2N2C)C6H4(CN2SE2)][I]

Citation
Cd. Bryan et al., IODINE CHARGE-TRANSFER SALTS OF BENZENE-BRIDGED BIS(1,2,3,5-DISELENADIAZOLYL) DIRADICALS - ELECTROCRYSTALLIZATION AND SOLID-STATE CHARACTERIZATION OF 1,3-[(SE2N2C)C6H4(CN2SE2)][I] AND 1,4-[(SE2N2C)C6H4(CN2SE2)][I], Chemistry of materials, 8(3), 1996, pp. 762-768
Citations number
24
Categorie Soggetti
Chemistry Physical","Material Science
Journal title
ISSN journal
08974756
Volume
8
Issue
3
Year of publication
1996
Pages
762 - 768
Database
ISI
SICI code
0897-4756(1996)8:3<762:ICSOBB>2.0.ZU;2-T
Abstract
Electroreduction of 1,3- and 1,4-benzene-bridged bis(diselenadiazolium ) salts [1,4-Se][SbF6](2) and [1,4-Se][SbF6](2) in acetonitrile, at a Pt wire and in the presence of iodine affords the 1:1 charge-transfer salts [1,4-Se][I] and [1,3-Se][I]. Crystals of [1,4-Se][I] belong to t he monoclinic space group C2/m, with FW = 598.9, a = 10.586(2), b = 16 .713(2), c = 3.5006(14) Angstrom, beta = 104.26(2)degrees, V = 600.2(3 ) Angstrom(3), Z = 2. Crystals of [1,3-Se][I] belong to the orthorhomb ic space group Ima2, with FW = 598.9, a = 28.489(7), b = 3.543(2), c = 12.283(2) Angstrom, V = 1239.8(8) Angstrom(3), Z = 4. In the presence of an excess of iodine, electrocrystallization of [1,4-Se](2+) afford s the mixed iodide/triiodide salt [1,4-Se][I][I-3], space group C2/c, FW = 979.59, a = 12.862(3), b = 15.063(2), c = 9.028(3) Angstrom, beta = 100.62(2)degrees, V = 1719.1(7) Angstrom(3), Z = 4. The structures of the two 1:1 compounds consist of perfectly superimposed stacks of m olecular units interspersed by columns of disordered iodines. Intersta ck contacts in both structures are limited, indicative of 1-dimensiona l electronic structures. Variable-temperature single-crystal conductiv ity measurements on [1,4-Se][I] reveal weakly metallic behavior at roo m temperature, with a phase transition to a semiconducting state occur ring at about 240 K. Magnetic susceptibility measurements on [1,4-Se][ I] are consistent with the conductivity data; the magnetic susceptibil ity of [1,3-Se][I] behaves similarly. The crystal structures and trans port properties are discussed in light of extended Huckel band structu re calculations.