Dependence of Field Switched Ordered Arrays of Dinuclear
Mixed-Valence Complexes on the Distance between the
Redox Centers and the Size of the Counterions
posted on 2005-11-02, 00:00authored byHua Qi, Anuradha Gupta, Bruce C. Noll, Gregory L. Snider, Yuhui Lu, Craig Lent, Thomas P. Fehlner
<i>trans</i>-[(H<sub>2</sub>NCH<sub>2</sub>CH<sub>2</sub>C⋮N)(dppe)<sub>2</sub>Ru(C⋮C)<sub>6</sub>Ru(dppe)<sub>2</sub>(N⋮CCH<sub>2</sub>CH<sub>2</sub>NH<sub>2</sub>)][PF<sub>6</sub>]<sub>2</sub>, <b>2</b>[PF<sub>6</sub>]<sub>2</sub>, a derivative of <i>trans</i>-[Cl(dppe)<sub>2</sub>Ru(C⋮C)<sub>6</sub>Ru(dppe)<sub>2</sub>Cl] functionalized for binding to a silicon substrate, has been
prepared and characterized spectroscopically, electrochemically, and with a solid state, single-crystal
structure determination. Covalent binding via reaction of one amine group to a boron-doped, smooth Si−Cl substrate is verified by XPS measurements and surface electrochemistry. Vertical orientation is
demonstrated by film thickness measurements. Synthesis of the <b>2</b>[PF<sub>6</sub>]<sub>3</sub> mixed-valence complex on the
surface is established by electrochemical techniques. Measurement of the ac capacitance of the film at 1
MHz as a function of voltage across the film with a pulse−counter pulse technique demonstrates controlled
electric field generation of the two stable mixed-valence forms differing in the spatial location of one electron,
that is, switching. As compared to [<i>trans</i>-Ru(dppm)<sub>2</sub>(C⋮CFc)(NCCH<sub>2</sub>CH<sub>2</sub>NH<sub>2</sub>)][PF<sub>6</sub>][Cl], <b>1</b>[PF<sub>6</sub>][Cl], the
magnitude of the capacitance signal per complex observed on switching is shown to increase with increasing
distance between the metal centers. Additional experiments on <b>1</b>[X][Cl] show that the potential for switching
<b>1</b>[X][Cl] increases in the order [X]<sup>-</sup> = [SO<sub>3</sub>CF<sub>3</sub>]<sup>-</sup> < [PF<sub>6</sub>]<sup>-</sup> < [Cl]<sup>-</sup>. A simple electrostatic model suggests
that the smaller is the counterion, the greater is the perturbation of the metal sites and the larger is the
barrier for switching.