Charge-transfer complexes of metal dithiolenes XXVI Azobipyridinium dications and radical monocations as accepters

Citation
C. Handrosch et al., Charge-transfer complexes of metal dithiolenes XXVI Azobipyridinium dications and radical monocations as accepters, EUR J INORG, (8), 1999, pp. 1259-1269
Citations number
57
Categorie Soggetti
Inorganic & Nuclear Chemistry
Journal title
EUROPEAN JOURNAL OF INORGANIC CHEMISTRY
ISSN journal
14341948 → ACNP
Issue
8
Year of publication
1999
Pages
1259 - 1269
Database
ISI
SICI code
1434-1948(199908):8<1259:CCOMDX>2.0.ZU;2-Z
Abstract
Combination of the planar redox-active ions [ML2](2-) (L = mnt(2-) = maleon itrile-1,2- dithiolate; M = Ni (1), Pd (2), Pt (3); dmit(2-) = 2-thioxo-1,3 -dithiol-4,5-dithiolate: M = Ni (4), Pd (5) and trans-4,4'-azobis(1-methyl- pyridinium), (a(2+)) affords 1:1 ion pairs exhibiting partial and complete electron transfer as evidenced by UV-Vis and EPR spectra, Replacement of pl anar a(2+) by a non-planar dipyridinium ketone b(2+) leads to the complexes 1b and 4b, 1a, 2a, and 3a are predominantly composed of dications and dian ions while 4a, 5a, and 4b are rare examples of ion pairs consisting of two radical ions. Single crystal X-ray structural analyses was performed on 4a, a(PF6)(2) and a(MeSO4)(2) while the structure of 1a was resolved by powder X-ray diffractometry. The latter consists of mixed stacks of planar dianio ns and dications forming a slipped arrangement with the centers of the two ions displaced relative to each other by 250 pm. The short interplanar dist ances of 340 pm are in agreement with the presence of a weak charge-transfe r interaction as indicated by the corresponding absorption band at about 14 00 nm, A mean reorganization energy of 0.85 +/- 0.04 eV is calculated from the Hush equation for complexes 1a, 2a, and 3a. No ion pair charge-transfer band is observable for 4a, 5a, and 4b. Surprisingly, in the solid state st ructure of 4a the [Ni(dmit)2](-) monoanions do not form segregated columns as found in the many ion pairs with redox inert counterions, but prefer a m ixed stack arrangement as observed also for 1a. The specific electrical con ductivity of pressed powder pellets of complexes exhibiting a charge-transf er band is in the range of 2 x 10(-7) to 1 x 10(-5) Ohm(-1)cm(-1), increasi ng with increasing driving force of electron transfer in accordance with pr evious results. Different to that, the conductivity of the other complexes does not depend on driving force and is much higher (2 x 10(-4) to 4 x 10(- 4) Ohm(-1)cm(-1)).