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Systematic Studies of Early Actinide Complexes: Thorium(Ⅳ) Fluoroketimides

机译:早期Act系元素配合物的系统研究:ium(Ⅳ)氟化亚胺

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Reaction of (C_5Me_5)_2Th(CH_3)_2 with 2 equiv of N ≡ C-Ar_F gives the corresponding fluorinated thorium(Ⅳ) bis(ketimide) complexes (C_5Me_5)_2Th[-N=C(CH_3)(Ar_F)]_2 (where Ar_F = 3-F-C_6H_4 (4), 4-F-C_6H_4 (5), 2-F-C_6H_4 (6), 3,5-F_2-C_6H_3 (7), 3,4,5-F_3-C_6H_2 (8), 2,6-F_2-C_6H_3 (9), 2,4,6-F_3-C_6H_2 (10), and C_6F_5 (11)). The complexes have been characterized by a combination of single-crystal X-ray diffraction, cyclic voltammetry and NMR, and UV-visible absorption and low-temperature luminescence spectroscopies. Density functional theory (DFT) and time-dependent DFT (TD-DFT) results are reported for complexes 5, 11, and (C_5Me_5)_2Th[-N=C(Ph)_2]_2 (1) for comparison with experimental data and to guide in the interpretation of the spectroscopic results. The most significant structural perturbation imparted by the fluorine substitution in these complexes is a rotation of the fluorophenyl group (Ar_F) out of the plane defined by the N=C(C_(Me))-(C_(ipso)) fragment in complexes 9-11 when the Ar_F group possesses two ortho fluorine atoms. Excellent agreement is obtained between the optimized ground state DFT calculated structures and crystal structures for 11, which displays the distortion, as well as 5, which does not. In complexes 9-11, the out-of-plane rotation results in large interplanar angles (φ) between the planes formed by ketimide atoms N=C(C_(Me))-(C_(ipso)) and the ketimide aryl groups in the range φ = 49.1-88.8°, while in complexes 5, 7, and 8, φ = 5.7-34.9°. The large distortions in 9-11 are a consequence of an unfavorable steric interaction between one of the two ortho fluorine atoms and the methyl group [-N=C(CH_3)] on the ketimide ligand. Excellent agreement is also observed between the experimental electronic spectroscopic data and the TD-DFT predictions that the two lowest lying singlet states are principally of nonbonding nitrogen p orbital to antibonding C=N π~* orbital (p_N→π~*_(C=N) or nπ~*) character, giving rise to moderately intense transitions in the mid-visible spectral region that are separated in energy by less than 0.1 eV. Low-temperature (77 K) luminescence from both singlet and triplet excited states are also observed for these complexes. Emission lifetime data at 77 K for the triplet states are in the range 50-400 μs. These emission spectral data also exhibit vibronic structure indicative of a small Franck-Condon distortion in the ketimide M-N=C(R_1)(R_2) linkage. Consistent with this vibronic structure, resonance enhanced Raman vibrational scattering is also observed for (C_5Me_5)_2Th[-N=C(Ph)(CH_2Ph)]_2 (2) when exciting into the visible excited states. These systems represent rare examples of Th(Ⅳ) complexes that engender luminescence and resonance Raman spectral signatures.
机译:(C_5Me_5)_2Th(CH_3)_2与2当量N≡C-Ar_F的反应得到相应的氟化th(Ⅳ)双(酮亚胺)配合物(C_5Me_5)_2Th [-N = C(CH_3)(Ar_F)] _ 2(其中Ar_F = 3-F-C_6H_4(4),4-F-C_6H_4(5),2-F-C_6H_4(6),3,5-F_2-C_6H_3(7),3,4,5-F_3-C_6H_2 (8),2,6-F_2-C_6H_3(9),2,4,6-F_3-C_6H_2(10)和C_6F_5(11))。配合物的特征是结合了单晶X射线衍射,循环伏安法和NMR,以及紫外可见吸收和低温发光光谱学。报告了配合物5、11和(C_5Me_5)_2Th [-N = C(Ph)_2] _2(1)的密度泛函理论(DFT)和随时间变化的DFT(TD-DFT)结果,以便与实验数据进行比较,并指导对光谱结果的解释。在这些配合物中,氟取代所引起的最显着的结构扰动是配合物中的氟苯基(Ar_F)旋转出配合物9中N = C(C_(Me))-(C_(ipso))片段所定义的平面当Ar_F基团具有两个邻氟原子时为-11。在优化的基态DFT计算的结构和11的晶体结构之间显示出极好的一致性,而5的晶体结构没有畸变。在配合物9-11中,平面外旋转会导致由ketimide原子N = C(C_(Me))-(C_(ipso))与ketimide中的ketimide芳基形成的平面之间存在较大的平面角范围φ= 49.1-88.8°,而在复合物5、7和8中,φ= 5.7-34.9°。 9-11中的大变形是两个邻氟原子之一与酮亚胺配体上的甲基[-N = C(CH_3)]之间不利的空间相互作用的结果。在实验电子光谱数据和TD-DFT预测之间还观察到极好的一致性,即两个最低的单重态主要是非键合氮p轨道与反键合C = Nπ〜*轨道(p_N→π〜* _(C = N)或nπ〜*)特性,在中可见光谱区域产生中等强度的跃迁,其能量间隔小于0.1 eV。对于这些配合物,还观察到了来自单重态和三重态激发态的低温(77 K)发光。三重态的77 K发射寿命数据在50-400μs范围内。这些发射光谱数据还表现出表明在酮亚胺M-N = C(R_1)(R_2)键中出现小的Franck-Condon变形的振动电子结构。与此振动结构一致,当激发到可见激发态时,对于(C_5Me_5)_2Th [-N = C(Ph)(CH_2Ph)] _ 2(2)也观察到共振增强的拉曼振动散射。这些系统代表了引起发光和共振拉曼光谱特征的Th(Ⅳ)配合物的稀有例子。

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