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Single-Ion Reorganization Free Energy of Aqueous Ru(bpy)_3~(2+/3+) and Ru(H_2O)_6~(2+/3+) from Photoemission Spectroscopy and Density Functional Molecular Dynamics Simulation

机译:Ru(bpy)_3〜(2 + / 3 +)和Ru(H_2O)_6〜(2 + / 3 +)水溶液的单离子重组自由能的光发射光谱和密度泛函分子动力学模拟

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Photoelectron spectroscopy and density functional molecular dynamics simulations are combined to quantify and characterize the redox properties of Ru(bpy)_3~(2+/3+) and Ru(H_2O)_6~(2+/3+) in aqueous solution. We report the energy-resolved photoelectron spectrum of aqueous Ru(bpy)_3~(2+/3+) at 200 eV photon energy. From the peak position of the highest molecular orbital at 6.81 eV, an experimental value for the single-ion reorganization free energy of Ru(bpy)_3~(3+) is determined to be 1.21 ± 0.04 eV. Density functional molecular dynamics calculations give a value of 0.84-1.20 eV for Ru(bpy)_3~(3+) and 1.92-2.42 eV for Ru(H_2O)_6~(3+) depending on the method used to extrapolate the results to the infinite dilution limit. Since linear response is an excellent approximation for these systems, we report the same reorganization free energies for the divalent ions. The relatively small reorganization free energy of Ru(bpy)_3~(3+) is a consequence of the small changes in the Ru-N bond lengths upon reduction (0.04 eV inner sphere contribution) and of the large hydrophobic cavity formed by the bulky bipyridine ligands, which effectively reduces the dipolar response of the solvent in qualitative agreement with continuum theory. The large difference in redox potential between Ru(bpy)_3~(2+/3+) and Ru(H_2O)_6~(2+/3+) (1 eV) is mainly associated with the difference in reorganization free energy rather than vertical ionization energy. Finally, the measured photoelectron spectrum of Ru(bpy)_3~(2+) is compared with the Kohn-Sham density of states for interpretation of occupied as well as computed virtual energy levels. This computational approach, in conjunction with first-ever photoelectron spectroscopy measurements of an aqueous transition metal ion, provides a quantitative benchmark for understanding the effect of water on metal redox potential and lays the groundwork for future studies of redox properties.
机译:结合光电子能谱和密度泛函分子动力学模拟,定量分析了Ru(bpy)_3〜(2 + / 3 +)和Ru(H_2O)_6〜(2 + / 3 +)的氧化还原性质。我们报告了在200 eV光子能量下,Ru(bpy)_3〜(2 + / 3 +)水溶液的能量分辨光电子谱。从最高分子轨道的峰位置在6.81 eV处,Ru(bpy)_3〜(3+)的单离子重组自由能的实验值确定为1.21±0.04 eV。根据用于将结果外推到的方法,密度泛函分子动力学计算得出Ru(bpy)_3〜(3+)的值为0.84-1.20 eV,Ru(H_2O)_6〜(3+)的值为1.92-2.42 eV。无限稀释极限。由于线性响应是这些系统的极佳近似值,因此我们报告了二价离子具有相同的重组自由能。 Ru(bpy)_3〜(3+)的重组自由能较小,这是由于还原时Ru-N键长度的小变化(0.04 eV内球贡献)和大体积形成的大疏水腔的结果联吡啶配体,可有效降低溶剂的偶极响应,与连续性理论定性一致。 Ru(bpy)_3〜(2 + / 3 +)和Ru(H_2O)_6〜(2 + / 3 +)(1 eV)之间的氧化还原电势的较大差异主要与重组自由能的差异有关,而不是与垂直电离能。最后,将测得的Ru(bpy)_3〜(2+)的光电子能谱与Kohn-Sham状态密度进行比较,以解释所占据的和计算的虚拟能级。这种计算方法与水性过渡金属离子的首次光电子能谱测量相结合,为了解水对金属氧化还原电势的影响提供了定量基准,并为进一步研究氧化还原性能奠定了基础。

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  • 来源
    《Journal of the American Chemical Society》 |2009年第44期|16127-16137|共11页
  • 作者单位

    Helmholtz-Zentrum Berlin fuer Materialien und Energie, and BESSY, Albert-Einstein-Strasse 15,D-12489 Berlin, Germany;

    Max-Planck-Institut fuer Dynamik and Selbstorganisation,Bunsenstrasse 10, D-37073 Goettingen, Germany;

    Helmholtz-Zentrum Berlin fuer Materialien und Energie, and BESSY, Albert-Einstein-Strasse 15,D-12489 Berlin, Germany;

    Department of Chemistry, University of Cambridge, Lensfield Road, Cambridge CB2 1EW, U.K.;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);美国《化学文摘》(CA);
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  • 正文语种 eng
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  • 入库时间 2022-08-18 03:17:26

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