Shiotani Masaru, Lund Anders, Lunell Sten, Williams Ffrancon
Department of Applied Chemistry, Graduate School of Engineering, Hiroshima University, Higashi-Hiroshima 739-8527, Japan.
J Phys Chem A. 2007 Jan 18;111(2):321-38. doi: 10.1021/jp064891u.
Anisotropic electron spin resonance (ESR) spectra are reported for the radical anions of hexafluorocyclopropane (c-C(3)F(6)(-)), octafluorocyclobutane (c-C(4)F(8)(-)), and decafluorocyclopentane (c-C(5)F(10)(-)) generated via gamma-irradiation in plastically crystalline tetramethylsilane (TMS) and rigid 2-methyltetrahydrofuran (MTHF) matrices. By combining the analysis of these experimental ESR spectra involving anisotropic hyperfine (hf) couplings with a series of quantum chemical computations, the geometrical and electronic structure of these unusual perfluorocycloalkane radical anions have been characterized more fully than in previous studies that considered only the isotropic couplings. Unrestricted Hartree-Fock (UHF) computations with the 6-311+G(d,p) basis set predict planar ring structures for all three radical anions, the ground electronic states being (2)A(2)(") for c-C(3)F(6)(-) (D(3h) symmetry), (2)A(2u) for c-C(4)F(8)(-) (D(4h)), and (2)A(2)(") for c-C(5)F(10)(-) (D(5h)), in which the respective six, eight, and ten 19F-atoms are equivalent by symmetry. A successful test of the theoretical computation is indicated by the fact that the isotropic 19F hf couplings computed by the B3LYP method with the 6-311+G(2df,p) basis set for the optimized geometries are in almost perfect agreement with the experimental values: viz., 19.8 mT (exp) vs 19.78 mT (calc) for c-C(3)F(6)(-); 14.85 mT (exp) vs 14.84 mT (calc) for c-C(4)F(8)(-); 11.6 mT (exp) vs 11.65 mT (calc) for c-C(5)F(10)(-). Consequently, the same computation method has been applied to calculate the almost axially symmetric anisotropic 19F hf couplings for the magnetically equivalent 19F atoms: (-4.90 mT, -4.84 mT, 9.75 mT) for c-C(3)F(6), (-3.54 mT, -3.48 mT, 7.02 mT) for c-C(4)F(8)(-), and (-2.62 mT, -2.56 mT, 5.18 mT) for c-C(5)F(10)(-). ESR spectral simulations performed using the computed principal values of the hf couplings and the spatial orientations of the 19F nuclei as input parameters reveal an excellent fit to the experimental anisotropic ESR spectra of c-C(3)F(6)(-), c-C(4)F(8)(-), and c-C(5)F(10)(-), thereby providing a convincing proof of the highly symmetric D(nh) structures that are predicted for these negative ions. Furthermore, using the computed 19F principal values and their orientations, the effective 19F anisotropic hf couplings along the molecular symmetry axes were evaluated for c-C(3)F(6)(-) and c-C(4)F(8)(-) and successfully correlated with the positions of the characteristic outermost features in both the experimental and calculated anisotropic spectra. In addition, the electronic excitation energies and oscillator strengths for the c-C(3)F(6)(-) , c-C(4)F(8)(-), and c-C(5)F(10)(-) radical anions were computed for the first time using time-dependent density functional theory (TD-DFT) methods.
报道了通过在塑性晶体四甲基硅烷(TMS)和刚性2-甲基四氢呋喃(MTHF)基质中进行γ辐照产生的六氟环丙烷(c-C₃F₆⁻)、八氟环丁烷(c-C₄F₈⁻)和十氟环戊烷(c-C₅F₁₀⁻)自由基阴离子的各向异性电子自旋共振(ESR)光谱。通过将这些涉及各向异性超精细(hf)耦合的实验ESR光谱分析与一系列量子化学计算相结合,这些不寻常的全氟环烷自由基阴离子的几何和电子结构比以往仅考虑各向同性耦合的研究得到了更充分的表征。使用6-311 + G(d,p)基组的无限制Hartree-Fock(UHF)计算预测所有三种自由基阴离子的平面环结构,基态电子态对于c-C₃F₆⁻(D₃h对称性)为(²)A₂″,对于c-C₄F₈⁻(D₄h)为(²)A₂u,对于c-C₅F₁₀⁻(D₅h)为(²)A₂″,其中各自的六个、八个和十个¹⁹F原子通过对称性是等效的。通过B3LYP方法使用6-311 + G(2df,p)基组对优化几何结构计算的各向同性¹⁹F hf耦合与实验值几乎完美吻合,这一事实表明理论计算的成功测试:即,对于c-C₃F₆⁻,19.8 mT(实验值)对19.78 mT(计算值);对于c-C₄F₈⁻,14.85 mT(实验值)对14.84 mT(计算值);对于c-C₅F₁₀⁻,11.6 mT(实验值)对11.65 mT(计算值)。因此,相同的计算方法已被应用于计算磁等效¹⁹F原子的几乎轴向对称的各向异性¹⁹F hf耦合:对于c-C₃F₆为(-4.90 mT,-4.84 mT,9.75 mT),对于c-C₄F₈⁻为(-3.54 mT,-3.48 mT,7.02 mT),对于c-C₅F₁₀⁻为(-2.62 mT,-2.56 mT,5.18 mT)。使用计算的hf耦合主值和¹⁹F核的空间取向作为输入参数进行的ESR光谱模拟显示与c-C₃F₆⁻、c-C₄F₈⁻和c-C₅F₁₀⁻的实验各向异性ESR光谱非常吻合,从而为预测这些负离子的高度对称D(nh)结构提供了令人信服的证据。此外,使用计算的¹⁹F主值及其取向,评估了c-C₃F₆⁻和c-C₄F₈⁻沿分子对称轴的有效¹⁹F各向异性hf耦合,并成功地与实验和计算的各向异性光谱中特征最外层特征的位置相关联。此外,首次使用含时密度泛函理论(TD-DFT)方法计算了c-C₃F₆⁻、c-C₄F₈⁻和c-C₅F₁₀⁻自由基阴离子的电子激发能和振子强度。