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首页> 外文期刊>The journal of physical chemistry, A. Molecules, spectroscopy, kinetics, environment, & general theory >Structure and intermolecular vibrations of perylene· trans -1,2-dichloroethene, a weak charge-transfer complex
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Structure and intermolecular vibrations of perylene· trans -1,2-dichloroethene, a weak charge-transfer complex

机译:ylene-反式-1,2-二氯乙烯,一种弱电荷转移复合物的结构和分子间振动

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The vibronic spectra of strong charge-transfer complexes are often congested or diffuse and therefore difficult to analyze. We present the spectra of the π-stacked complex perylene trans-1,2-dichloroethene, which is in the limit of weak charge transfer, the electronic excitation remaining largely confined to the perylene moiety. The complex is formed in a supersonic jet, and its S_0 a?" S_1 spectra are investigated by two-color resonant two-photon ionization (2C-R2PI) and fluorescence spectroscopies. Under optimized conditions, vibrationally cold (T_(vib) ≈ 9 K) and well resolved spectra are obtained. These are dominated by vibrational progressions in the "hindered-rotation" Rc intermolecular vibration with very low frequencies of 11 (S_0) and 13 cm~(-1) (S_1). The intermolecular T_z stretch and the R_a and R_b bend vibrations are also observed. The normally symmetry-forbidden intramolecular 1a_u "twisting" vibration of perylene also appears, showing that the π- stacking interaction deforms the perylene moiety, lowering its local symmetry from D_(2h) to D_2. We calculate the structure and vibrations of this complex using six different density functional theory (DFT) methods (CAM-B3LYP, BH&HLYP, B97-D3, ωB97X-D, M06, and M06-2X) and compare the results to those calculated by correlated wave function methods (SCS-MP2 and SCS-CC2). The structures and vibrational frequencies predicted with the CAM-B3LYP and BH&HLYP methods disagree with the other calculations and with experiment. The other four DFT and the ab initio methods all predict a π-stacked "centered" structure with nearly coplanar perylene and dichloroethene moieties and intermolecular binding energies of D_e = -20.8 to -26.1 kJ/mol. The 000 band of the S_0 → S_1 transition is red-shifted by δν = -301 cm~(-1) relative to that of perylene, implying that the D_e increases by 3.6 kJ/mol or ~15% upon electronic excitation. The intermolecular vibrational frequencies are assigned to the calculated R_c, T_z, R_a, and Rb vibrations by comparing to the observed/calculated frequencies and S _0 a?" S_1 Franck-Condon factors. Of the three TD-DFT methods tested, the hybrid-meta-GGA functional M06-2X shows the best agreement with the experimental electronic transition energies, spectral shifts, and vibronic spectra, closely followed by the ωB97X-D functional, while the M06 functional gives inferior results.
机译:强电荷转移复合物的电子光谱通常是拥塞或分散的,因此难以分析。我们介绍了π-堆叠的复杂per反式1,2-二氯乙烯的光谱,这是在弱电荷转移的极限内,电子激发仍然主要局限于per部分。该复合物是在超音速喷射中形成的,其S_0 a?“ S_1光谱通过双色共振双光子电离(2C-R2PI)和荧光光谱研究。在优化条件下,振动冷(T_(vib)≈9 K)并获得了良好的分辨谱,这些谱以“受阻旋转” Rc分子间振动的振动级数占主导,其极低频率为11(S_0)和13 cm〜(-1)(S_1)。同时也观察到了ylene的正常对称的分子内1a_u“扭转”振动,也表明了π-堆积相互作用使the部分变形,将其局部对称性从D_(2h)降低到D_2。 。我们使用六种不同的密度泛函理论(DFT)方法(CAM-B3LYP,BH&HLYP,B97-D3,ωB97X-D,M06和M06-2X)计算该复合物的结构和振动,并将结果与​​通过相关波函数法S-MP2和SCS-CC2)。用CAM-B3LYP和BH&HLYP方法预测的结构和振动频率与其他计算和实验不一致。其他四种DFT和从头算方法都预测了一个π堆积的“中心”结构,该结构具有几乎共面的per和二氯乙烯部分,分子间结合能D_e = -20.8至-26.1 kJ / mol。 S_0→S_1跃迁的000带相对于band的红移δν= -301 cm〜(-1),这表明电子激发后D_e增大3.6 kJ / mol或〜15%。通过将观察到的/计算出的频率和S_0a?S_1 Franck-Condon因子进行比较,将分子间振动频率分配给计算出的R_c,T_z,R_a和Rb振动。在测试的三种TD-DFT方法中,混合动力meta-GGA功能M06-2X与实验的电子跃迁能,光谱位移和电子振动谱显示出最佳的一致性,紧随其后的是ωB97X-D功能,而M06功能的效果较差。

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