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平面和鞍状铜(III)中-三芳基卟吩的电子吸收、共振拉曼光谱及电化学研究。高取代基敏感性的Soret带作为高价过渡金属卟吩的一个显著特征。

Electronic absorption, resonance Raman, and electrochemical studies of planar and saddled copper(III) meso-triarylcorroles. Highly substituent-sensitive Soret bands as a distinctive feature of high-valent transition metal corroles.

作者信息

Wasbotten Ingar H, Wondimagegn Tebikie, Ghosh Abhik

机构信息

Department of Chemistry, Universty of Tromsø, N-9037 Tromsø, Norway.

出版信息

J Am Chem Soc. 2002 Jul 10;124(27):8104-16. doi: 10.1021/ja0113697.

Abstract

We present here a first systematic study of substituent effects in metallocorroles, based on electronic absorption, resonance Raman (RR), and infrared (IR) spectroscopic studies and electrochemical measurements on 10 copper(III) meso-triarylcorroles, Cu(III)[beta-Y(8)TArC], where the beta-substituent Y = H or Br and the meso-aryl group Ar = C(6)F(5) or p-X-C(6)H(4) and X = CF(3), H, CH(3), and OCH(3). The results afford a number of significant inisights. (1) The RR (and IR) results show that at least two and possibly more high-frequency bands in the 1400-1550 cm(-1) region exhibit significant frequency downshifts on beta-octabromination and, thus, qualify as structure-sensitive marker bands. DFT geometry optimizations indicate that the saddled conformation should be clearly preferred for the beta-octabromo-meso-triarylcorrole derivatives studied and that beta-octabromination results in expansion of a number of skeletal bond distances of the corrole macrocycle, consistent with observed frequency downshifts. (2) Electrochemical measurements on planar Cu(III)[TArC] derivatives have shown that the para substituents on the meso-aryl groups exert a strong influence on the half-wave potentials for oxidation (rho(ox) = DeltaE(1/2ox)/Delta(3sigma) = 95 mV), suggesting that oxidation involves removal of an electron from the corrole "b(1)" HOMO, which has significant amplitudes at the meso postions and crudely resembles a porphyrin a(2u) HOMO in shape. In contrast, the Hammett rho(ox) is much lower for the nonplanar Cu(III)[Br(8)TArC] derivatives and we suggest that this ultimately results from a b(1)-to-a(2) HOMO reversal which in turn stems from a metal (d(x2-y2)-corrole ("b(1)") orbital interaction that becomes symmetry-allowed under a saddle distortion of the corrole macrocycle. In contrast to what has been observed for metallotetraphenylporphyrins, beta-octabromination dramatically raises the half-wave potential for one-electron oxidation of the triarylcorrole derivatives studied. This appears to be due to the fact that both the "a(2)" and "b(1)" HOMOs of a corrole (in C(2v) notation) have significantly higher amplitudes at the beta positions, compared to a porphyrin a(2u) HOMO. Thus, although many metallocorroles are significantly more easily oxidizable than analogous metalloporphyrins, certain beta-octahalogeno-meso-triarylcorrole derivatives can indeed be extremely electron deficient and oxidation resistant and may, therefore, find use as rugged catalysts or reagents under highly oxidizing conditions. (3) Finally, the Soret absorption maxima of high-valent metallotriarylcorroles exhibit a uniquely sensitive dependence on the substituents on the meso-aryl groups. Thus, on going from Cu(III)[T(p-CF(3)-P)C] (T(p-CF(3)-P)C = meso-tris((p-trifluoromethyl)phenyl)corrolato) to Cu(III)[T(p-OM-P)C] (T(p-OM-P)C = meso-tris(p-methoxyphenyl)corrolato), the Soret maximum red shifts by 26 nm, from 407 to 433 nm. Similarly, on going from Cu(III)[Br(8)T(p-CF(3)-P)C] (Br(8)T(p-CF(3)-P)C = beta-octabromo-meso-tris((p-trifluoromethyl)phenyl)corrolato) to Cu(III)[Br(8)T(p-OM-P)C] (Br(8)T(p-CF(3)-P)C = beta-octabromo-meso-tris(p-methoxyphenyl)corrolato), the Soret maximum red shifts by 34 nm, from 434 to 468 nm. Time-dependent DFT calculations suggest that this substituent dependence reflects significant ligand-to-metal charge-transfer character of certain transitions in the Soret region. The optical spectra of free-base and non-high-valent transition metal tetrapyrroles, in general, do not exhibit a similar substituent dependence.

摘要

我们在此展示了对金属卟吩中取代基效应的首次系统研究,该研究基于对10种三芳基卟吩铜(III)配合物Cu(III)[β - Y(8)TArC]的电子吸收光谱、共振拉曼(RR)光谱、红外(IR)光谱研究以及电化学测量,其中β - 取代基Y = H或Br,中位芳基Ar = C(6)F(5)或对 - X - C(6)H(4)且X = CF(3)、H、CH(3)和OCH(3)。研究结果提供了许多重要的见解。(1) RR(和IR)结果表明,在1400 - 1550 cm(-1)区域中至少有两个甚至可能更多的高频带在β - 八溴化后出现显著的频率下移,因此可作为结构敏感标记带。密度泛函理论(DFT)几何优化表明,对于所研究的β - 八溴 - 中位 - 三芳基卟吩衍生物,鞍形构象应明显更受青睐,并且β - 八溴化导致卟吩大环的一些骨架键长增加,这与观察到的频率下移一致。(2) 对平面Cu(III)[TArC]衍生物的电化学测量表明,中位芳基上的对位取代基对氧化半波电位有强烈影响(ρ(ox) = ΔE(1/2ox)/Δ(3σ) = 95 mV),这表明氧化过程涉及从卟吩“b(1)”最高占据分子轨道(HOMO)移除一个电子,该轨道在中位位置具有显著振幅,并且形状粗略类似于卟啉a(2u) HOMO。相比之下,对于非平面的Cu(III)[Br(8)TArC]衍生物,哈米特ρ(ox)要低得多,我们认为这最终是由于b(1)到a(2) HOMO的反转,这又源于金属(d(x2 - y2)-卟吩(“b(1)”)轨道相互作用,在卟吩大环的鞍形畸变下该相互作用变为对称允许。与金属四苯基卟啉的情况相反,β - 八溴化显著提高了所研究的三芳基卟吩衍生物单电子氧化的半波电位。这似乎是由于卟吩(以C(2v)表示法)的“a(2)”和“b(1)”HOMO在β位置的振幅都比卟啉a(2u) HOMO显著更高。因此,尽管许多金属卟吩比类似的金属卟啉更容易被氧化,但某些β - 八卤代 - 中位 - 三芳基卟吩衍生物确实可能具有极高的缺电子性和抗氧化性,因此可能在高氧化条件下用作坚固的催化剂或试剂。(3) 最后,高价金属三芳基卟吩的Soret吸收最大值对中位芳基上的取代基表现出独特的敏感依赖性。因此,从Cu(III)[T(p - CF(3)-P)C](T(p - CF(3)-P)C = 中位 - 三((对 - 三氟甲基)phenyl)卟吩铜(III))到Cu(III)[T(p - OM - P)C](T(p - OM - P)C = 中位 - 三(p - 甲氧基苯基)卟吩铜(III)),Soret最大值红移26 nm,从407 nm到433 nm。类似地,从Cu(III)[Br(8)T(p - CF(3)-P)C](Br(8)T(p - CF(3)-P)C = β - 八溴 - 中位 - 三((对 - 三氟甲基)phenyl)卟吩铜(III))到Cu(III)[Br(8)T(p - OM - P)C](Br(8)T(p - CF(3)-P)C = β - 八溴 - 中位 - 三(p - 甲氧基苯基)卟吩铜(III)),Soret最大值红移34 nm,从434 nm到468 nm。含时DFT计算表明,这种取代基依赖性反映了Soret区域某些跃迁中显著的配体到金属的电荷转移特性。一般来说,游离碱和非高价过渡金属四吡咯的光谱不表现出类似的取代基依赖性。

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