Electronic Effects of Ligand Substitution on Spin Crossover in a Series of Diiminoquinonoid-Bridged Fe super(II) sub(2) Complexes

A series of four isostructural Fe super(II) sub(2) complexes, [(TPyA) sub(2)Fe sub(2)( super(X)L)] super(2+) (TPyA = tris(2-pyridylmethyl)amine; super(X)L super(2-) = doubly deprotonated form of 3,6-disubstituted-2,5-dianilino-1,4-benzoquinone; X = H, Br, CI, and F), were synthesized to enable a sys...

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Published inInorganic chemistry Vol. 54; no. 1; pp. 359 - 369
Main Authors Park, Jesse G, Jeon, Ie-Rang, Harris, T David
Format Journal Article
LanguageEnglish
Published 05.01.2015
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Summary:A series of four isostructural Fe super(II) sub(2) complexes, [(TPyA) sub(2)Fe sub(2)( super(X)L)] super(2+) (TPyA = tris(2-pyridylmethyl)amine; super(X)L super(2-) = doubly deprotonated form of 3,6-disubstituted-2,5-dianilino-1,4-benzoquinone; X = H, Br, CI, and F), were synthesized to enable a systematic study of electronic effects on spin crossover behavior. Comparison of X-ray diffraction data for these complexes reveals the sole presence of high-spin Fe super(II) at 225 K and mixtures of high-spin and low-spin Fe super(II) at 100 K, which is indicative of incomplete spin crossover. In addition, crystal packing diagrams show that these complexes are well-isolated from one another in the solid state, owing primarily to the presence of bulky tetra(aryl)borate counteranions, such that spin crossover is likely not significantly affected by intermolecular interactions. Variable-temperature dc magnetic susceptibility data confirm the structural observations and reveal that 54(1), 56(1), 62(1), and 84(1)% of Fe super(II) centers remain high-spin even below 65 K. Moreover, fits to magnetic data provide crossover temperatures of T sub(1/2) = 160(1), 124(1), 121(1), and 110(1) K for X = H, Br, CI, and F, respectively, along with enthalpies of Delta H = 11.4(3), 8.5(3), 8.3(3), and 7.5(2) kJ/mol, respectively. These parameters decrease with increasing electronegativity of X and thus increasing electron-withdrawing character of super(X)L super(2-), suggesting that the observed trends originate primarily from inductive effects of X. Moreover, when plotted as a function of the Pauling electronegativity of X, both T sub(1/2) and Delta H undergo a linear decrease. Further analyses of the low-temperature magnetic data and variable-temperature Mossbauer spectroscopy suggest that the incomplete spin crossover behavior in [(TPyA) sub(2)Fe sub(2)( super(X)L)] super(2+) is best described as a transition from purely [Fe sub(HS)-Fe sub(HS)] (HS = high-spin) complexes at high temperature to a mixture of [Fe sub(HS)-Fe sub(HS)] and [Fe sub(HS)-Fe sub(LS)] (LS = low-spin) complexes at low temperature, with the number of [Fe sub(HS)-Fe sub(HS)] species increasing with decreasing electron-withdrawing character of super(X)L super(2-).
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ISSN:0020-1669
DOI:10.1021/ic5025586