Danset Delphine, Alikhani Mohammad E, Manceron Laurent
LADIR/Laboratoire de Dynamique, Interactions et Réactivité/CNRS UMR 7075- Université Pierre et Marie Curie, case 49, 4 place Jussieu 75252 Paris, France.
J Phys Chem A. 2005 Jan 13;109(1):105-14. doi: 10.1021/jp0473265.
The nature of the reaction products between CoO(2) and molecular O(2), isolated in rare gas matrices, have been investigated using IR absorption spectroscopy. In this paper, we report on the vibrational spectrum of the CoO(4) molecule in its ground and first low-lying excited states. Isotopic substitutions using (16)O(2) and (18)O(2) precursors, as well as (16)O(2) + (18)O(2) and (16)O(2) +( 16)O(18)O + (18)O(2) mixtures in either excess argon or neon, enable demonstration of C(2)(v)() and C(s)() structures for the respective states. CoO(4) is formed following molecular diffusion by complexation of ground-state CoO(2) by an O(2) molecule. The molecule is first formed in the excited state and then spontaneously relaxes to the ground state after remaining in the dark. The kinetics of relaxation can be fitted to a first-order exponential decay with an excited-state lifetime estimated around 23 +/- 2 min in argon and 15 +/- 2 min in neon, indicative of a slow, spin-forbidden process. Population of the excited state is induced by photons around 4250 +/- 250 cm(-1). Experimental results are compared to density functional theory (DFT) calculations at the BPW91/6-311G(3df) level. Electronic and geometrical optimizations were carried out starting from the ground-state precursors (i.e., (3)Sigma(g)(-) for O(2) and (2)Sigma(g)(+) for CoO(2)). Calculations predict a (2)A(2) (C(2)(v)()) ground state and a (4)A' (C(s)()) first excited state 0.37 eV above, close to the 4250 +/- 250 cm(-1) experimental excitation energy. The transition pathway is found to involve two supplementary states with crossed potential energy surfaces (PESs): a (2)B(1) excited state, 0.48 eV above the ground state, reached first through an adiabatic transition with a photon around 4800 cm(-1), and a (4)B(1) transition state into which the system relaxes before finally attaining the (4)A' (C(s)()) excited state. Harmonic frequencies and absolute intensities are also calculated and compared with the experimental data, indicating however that the DFT underestimates the internuclear distances for both configurations. Force and interaction constants were obtained with a semiempirical harmonic force-field potential calculation. They were then used in an empirical rule of plot linking force constants and internuclear distances in order to obtain an estimate of the Co-O bond lengths for each state and are compared to the DFT predictions.
利用红外吸收光谱研究了在稀有气体基质中分离出的CoO₂与分子O₂之间反应产物的性质。在本文中,我们报道了CoO₄分子基态和首个低激发态的振动光谱。使用¹⁶O₂和¹⁸O₂前驱体进行同位素取代,以及在过量氩气或氖气中使用¹⁶O₂ + ¹⁸O₂和¹⁶O₂ + ¹⁶O¹⁸O + ¹⁸O₂混合物,能够证明相应状态下的C₂ᵥ和Cₛ结构。CoO₄是通过基态CoO₂与O₂分子络合进行分子扩散后形成的。该分子首先在激发态形成,然后在黑暗中停留后自发弛豫到基态。弛豫动力学可以拟合为一级指数衰减,氩气中激发态寿命估计约为23±2分钟,氖气中为15±2分钟,这表明这是一个缓慢的、自旋禁阻过程。激发态的布居是由4250±250 cm⁻¹附近的光子诱导的。将实验结果与BPW91/6 - 311G(3df)水平的密度泛函理论(DFT)计算进行了比较。从基态前驱体(即O₂的³Σg⁻和CoO₂的²Σg⁺)开始进行电子和几何结构优化。计算预测基态为²A₂(C₂ᵥ),首个激发态为⁴A′(Cₛ),比基态高0.37 eV,接近4250±250 cm⁻¹的实验激发能。发现跃迁路径涉及两个具有交叉势能面(PESs)的补充态:一个比基态高0.48 eV的²B₁激发态,首先通过与4800 cm⁻¹附近的光子进行绝热跃迁到达,以及一个⁴B₁过渡态,系统在最终达到⁴A′(Cₛ)激发态之前弛豫到该态。还计算了谐振频率和绝对强度并与实验数据进行比较,然而结果表明DFT低估了两种构型的核间距。通过半经验谐振力场势计算获得了力常数和相互作用常数。然后将它们用于将力常数与核间距联系起来的经验绘图规则,以估计每个状态下的Co - O键长,并与DFT预测结果进行比较。