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Updated: Oct 3, 2026
Magnetometric Characterization of Intermediates in the Solid-State Electrochemistry of Redox-Active Metal-Organic Frameworks
Published on: June 9, 2023
Electron Exchange and the Photophysics of Metal-Quinone Complexes. 1. Synthesis and Spectroscopy of Chromium-Quinone
Daniel E. Wheeler1, James K. McCusker
1Department of Chemistry, University of California at Berkeley, Berkeley, California 94720-1460.
Abstract:
The synthesis, structural and spectroscopic characterization of monosemiquinone and monocatechol complexes of chromium(III) are described. Compounds of the general form [Cr(N(4))Q](n+), where N(4) represents a tetradentate or bis-bidentate nitrogenous ligand or ligands and Q represents a reduced form of an orthoquinone, have been prepared by two different routes from Cr(III) and Cr(II) starting materials. The complex [Cr(tren)(3,6-DTBSQ)](PF(6))(2), where tren is tris(2-aminoethyl)amine and 3,6-DTBSQ is 3,6-di-tert-butylorthosemiquinone, crystallizes in the monoclinic space group P2(1)/c with a = 11.9560(2) Å, b = 17.0715(4) Å, c = 17.1805(4) Å, beta = 90.167(1) degrees, V = 3506.6(1) Å(3), Z = 4, with R = 0.056 and R(w) = 0.070. Alternating C-C bond distances within the quinoidal ligand confirm its semiquinone character. Variable temperature magnetic susceptibility data collected on solid samples of both [Cr(tren)(3,6-DTBSQ)](PF(6))(2) and [Cr(tren)(3,6-DTBCat)](PF(6)) in the range 5-350 K exhibit temperature-independent values of 2.85 +/- 0.1 &mgr;(B) and 3.85 +/- 0.1 &mgr;(B), respectively. These data are consistent with a simple Cr(III)-catechol formulation (S = (3)/(2)) in the case of [Cr(tren)(3,6-DTBCat)](PF(6)) and strong antiferromagnetic coupling (|J| > 350 cm(-)(1)) between the Cr(III) and the semiquinone radical in [Cr(tren)(3,6-DTBSQ)](PF(6))(2). The absorption spectrum of the semiquinone complex exhibits a number of sharp, relatively intense transitions in fluid solution. Group theoretical arguments coupled with a qualitative ligand-field analysis including the effects of Heisenberg spin exchange suggest that several of the observed transitions are a consequence of exchange interactions in both the ground- and excited-state manifolds of the compound. The effect of electron exchange on excited-state dynamics has also been probed through static emission as well as time-resolved emission and absorption spectroscopies. It is suggested that the introduction of exchange coupling and subsequent change in the molecule's electronic structure may contribute to an increase of nearly 4 orders of magnitude in the rate of radiative decay (k(r)), and a factor of ca. 10(7) in the rate of nonradiative decay (k(nr)).
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