School of Chemistry, Cardiff University, Main Building, Park Place, Cardiff CF10 3AT, UK.
Phys Chem Chem Phys. 2013 Sep 28;15(36):15214-22. doi: 10.1039/c3cp52464g.
ENDOR spectroscopy and DFT calculations have been used to thoroughly investigate the ligand hyperfine couplings for the bis(acetylacetonato)-copper(ii) complex [Cu(acac)2] in frozen solution. Solutions of [Cu(acac)2] were prepared under anhydrous conditions, and EPR revealed that the g and (Cu)A values were affected by traces of water present in the solvent. The ligand (H)Ai hyperfine couplings were subsequently investigated by CW and pulsed ENDOR spectroscopy. Anisotropic hyperfine couplings to the methine protons ((H)Ai = 1.35, -1.62, -2.12 MHz; a(iso) = -0.80 MHz) and smaller couplings to the fully averaged methyl group protons ((H)Ai = -0.65, 1.658, -0.9 MHz; a(iso) = 0.036 MHz) were identified by simulation of the angular selective ENDOR spectra and confirmed by DFT. Since the barrier to methyl group rotation was estimated to be ca. 5 kJ mol(-1) by DFT, rapid rotation of these -CH3 groups, even at 10 K, leads to an averaged value of (H)Ai. However, variable temperature X-band Mims ENDOR revealed an additional set of hyperfine couplings which showed a pronounced temperature dependency. Using CW Q-band ENDOR, these additional couplings were characterised by the hyperfine parameters (H)Ai = 3.45, 2.9, 2.62 MHz, a(iso) = 2.99 MHz and assigned to a hindered methyl group rotation. This hindered rotation of a sub-set of methyl groups occurs in 120° jumps, such that a large A(dip) and a(iso) component is always observed. Whilst the majority of the methyl groups undergo free rotation, a sub-set of methyl groups experience hindered rotation in frozen solution, through proton tunnelling. This hindered rotation appears to be caused by weak outer-sphere solvent interactions with the complex.
已使用 ENDOR 光谱和 DFT 计算彻底研究了固态中二(乙酰丙酮基)合铜(II)配合物[Cu(acac)2]的配体超精细耦合。在无水条件下制备[Cu(acac)2]溶液,EPR 表明 g 和(Cu)A 值受溶剂中痕量水的影响。随后通过 CW 和脉冲 ENDOR 光谱研究了配体(H)Ai 超精细耦合。通过对各向异性 ENDOR 光谱的模拟,确定了亚甲基质子((H)Ai = 1.35、-1.62、-2.12 MHz;a(iso) = -0.80 MHz)和较小的甲基质子((H)Ai = -0.65、1.658、-0.9 MHz;a(iso) = 0.036 MHz)的各向异性超精细耦合,并通过 DFT 得到了证实。由于通过 DFT 估计甲基旋转的势垒约为 ca. 5 kJ mol(-1),因此即使在 10 K 下,这些-CH3 基团也会快速旋转,导致(H)Ai 的平均值。然而,变温 X 波段 Mims ENDOR 揭示了一组额外的超精细耦合,这些耦合表现出明显的温度依赖性。使用 CW Q 波段 ENDOR,通过超精细参数(H)Ai = 3.45、2.9、2.62 MHz,a(iso) = 2.99 MHz 对这些额外的耦合进行了特征描述,并将其分配给受阻的甲基旋转。在 120°跳跃中,会发生一小部分甲基的受阻旋转,从而总是观察到较大的 A(dip)和 a(iso)分量。虽然大多数甲基经历自由旋转,但在冷冻溶液中,一小部分甲基通过质子隧道经历受阻旋转。这种受阻旋转似乎是由配合物与弱的外球溶剂相互作用引起的。