利用DFT方法探究一类自组装[Pt2M4（C≡CH）8]（M=Cu，Ag）簇合物的电子结构和光谱性质

应用TD．DFT（time－dependent density functional theory）并PCMfpolarizable continuum model）模型研究了一类自组装的[Pt2M4（C＇≡CH）8]（M=Cu,Ag）簇合物的电子结构和光谱性质．应用DFT（density functional theory）方法优化了该簇合物的基态及激发态结构．综合计算结果,得到与试验结果相一致的结构与光谱特点．[Pt2Ag4（C≡CH）8]具有呈D4和D4h对称性的两个稳定的基态几何结构．Pt－M距离预示弱相互作用的存在．Cu—Cu距离大于俩个Cu原子的范德华半径和而Ag－Ag间距与俩个Ag原子的范德华半径和差别不大．激发过程使得Pt…M,Ag…Ag作用增强,虽然Cu…Cu距离也相应缩短,但是其仍大于范德华半径之和．[Pt2Cu4（C≡CH）8]、[Pt2Ag4（C≡CH）8]（A）和（B）的最低能吸收在450、365和375nm处,发射在611、431和435nm处．红外可见谱范围内,[Pt2M4（C≡CH）8]的吸收波带都有Cu或Ag成分的贡献,所以没有ILCT或MPtLCT跃迁特征出现（ILCT：intraligand charge transfer;MLCT：metal-to—ligand charge transfer）．由于最低能吸收和发射具有不同的跃迁特征,所以发射不是来自于最低能吸收．[Pt2Ag4（C≡CH）8]簇合物的MM相互作用在激发态增强,发射光谱具有显著的ILCT特点,这也是[Pt2Ag4（C≡CH）8]的发射波长相对于其对应的同配体前躯体[Pt（C≡CH）4]^2-有少许蓝移的原因．     

DFT evaluation of the electronic structures and spectroscopic properties of the self-assembled [Pt2M4(C ≡ CH)8] (M=Cu,Ag) clusters

Science China Chemistry - Electronic structures and spectroscopic properties of self-assembled [Pt2M4(C≡CH)8] (M=Cu, Ag) clusters have been studied by the TD-DFT (time-dependent density...     

DFT evaluation of the electronic structures and spectroscopic properties of the self-assembled [Pt2M4(C ≡ CH)8] (M=Cu, Ag) clusters

Electronic structures and spectroscopic properties of self-assembled [Pt₂M₄(C≡CH)₈] (M=Cu, Ag) clusters have been studied by the TD-DFT (time-dependent density functional theory) calculations with the polarizable continuum model (PCM). The ground- and excited-state structures were optimized by the DFT (density functional theory) methods. The calculated structures and spectroscopic properties are in agreement with the corresponding experimental results. The [Pt₂Ag₄(C≡CH)₈] clusters have two stable ground state geometries (D ₄ and D _4h symmetry). The calculated Pt-M distances suggest only very weak interactions. The Cu-Cu distances are larger than the van der Waals radii of two Cu atoms and the Ag-Ag distances are analogous with the sum of van der Waals radii of two Ag atoms. Upon excitation, the interaction of Pt⋯M, Ag⋯Ag is strengthened, while the Cu⋯Cu distances are shortened but they are still larger than the sum of van der Waals radii of two Cu atoms. The lowest-energy absorptions are at 450, 365 and 375 nm and the emissions are at 611, 431 and 435 nm for [Pt₂Cu₄(C≡CH)₈], [Pt₂Ag₄(C≡CH)₈] (A) and (B), respectively. The transitions are all perturbed by the Cu or Ag composition through the UV-Vis spectra region; therefore, there are not pure ILCT or M_PtLCT characteristics (ILCT: intraligand charge transfer; MLCT: metal-to-ligand charge transfer) in absorptions of heteropolynuclear [Pt₂M₄(C≡CH)₈] clusters. Since the emissions and the lowest-absorptions have different transition characteristics for each complex, the emissions should not come from the lowest-energy absorptions. Because the M⋯M interactions in the excited state of [Pt₂Ag₄(C≡CH)₈] are augmented, the emissions of [Pt₂Ag₄(C≡CH)₈] clusters bear prominent ILCT character, which is the reason why the emission wavelengths of [Pt₂Ag₄(C≡CH)₈] have a small hypsochromic shift relative to the emission wavelength of homoleptic [Pt(C≡CH)₄]²⁻ precursor.