Rosokha Sergiy V, Neretin Ivan S, Sun Duoli, Kochi Jay K
Department of Chemistry, University of Houston, Houston, Texas 77204-5003, USA.
J Am Chem Soc. 2006 Jul 26;128(29):9394-407. doi: 10.1021/ja060393n.
The charge-resonance phenomenon originally identified by Badger and Brocklehurst lies at the core of the basic understanding of electron movement and delocalization that is possible within p-doped aromatic (face-to-face) arrays. To this end, we now utilize a series of different aryl-donor groups (Ar) around a central platform to precisely evaluate the intramolecular electron movement among these tethered redox centers. As such, the unique charge-resonance (intervalence) absorption bands observed upon the one-electron oxidation or p-doping of various hexaarylbenzenoid arrays (Ar6C6) provide quantitative measures of the reorganization energy (lambda) and the electronic coupling element (H(ab)) that are required for the evaluation of the activation barrier (deltaG(ET)) for electron-transfer self-exchange according to Marcus-Hush theory. The extensive search for viable redox centers is considerably aided by the application of a voltammetric criterion that has led in this study to Ar = N,N-dialkyl-p-anilinyl, in which exceptionally low barriers are shown to lie in the range deltaG(ET) = 0.3-0.7 kcal mol(-1) for very fast electron hopping or peregrination around the hexagonal circuit among six equivalent Ar sites. Therefore, at transition temperatures T(t) > 0.5/R or roughly -20 degrees C, the electron-transfer dynamics become essentially barrierless since the whizzing occurs beyond the continuum of states and effectively achieves complete pi-delocalization.
巴杰尔和布罗克赫斯特最初发现的电荷共振现象,是理解p型掺杂芳香族(面对面)阵列中电子移动和离域的基础核心。为此,我们现在在一个中心平台周围使用一系列不同的芳基供体基团(Ar),以精确评估这些相连的氧化还原中心之间的分子内电子移动。因此,在各种六芳基苯类阵列(Ar6C6)发生单电子氧化或p型掺杂时观察到的独特电荷共振(价间)吸收带,提供了重组能(λ)和电子耦合元件(H(ab))的定量测量值,根据马库斯-胡什理论,这些值是评估电子转移自交换活化能垒(ΔG(ET))所必需的。通过应用一种伏安法标准,大大有助于广泛寻找可行的氧化还原中心,在本研究中该标准得出Ar = N,N-二烷基对苯胺基,其中在六个等效Ar位点之间的六边形回路中,显示出极低的能垒处于ΔG(ET) = 0.3 - 0.7 kcal mol⁻¹范围内,实现非常快速的电子跳跃或迁移。因此,在转变温度T(t) > 0.5/R或大约 -20℃时,电子转移动力学基本上变得无势垒,因为快速旋转发生在态的连续区之外,并有效地实现了完全的π离域。