DIAR黄成色剂的合成

DIAR黄成色剂的合成;DIAR成色剂;异丙氨基苯硫酚;固体光气     

CuI/BtH催化苯硫酚与对甲氧基溴苯C–S偶联合成(4-甲氧基)(苯基)硫醚反应机理理论研究

采用密度泛函理论(DFT)中的B3LYP方法对CuI/BtH催化苯硫酚与对甲氧基溴苯C–S偶联合成(4-甲氧基)(苯基)硫醚反应机理进行了理论研究.在6-31+G(d)基组水平上,全参数优化了气相条件和N,N-二甲基甲酰胺(DMF)溶剂化条件下反应机理中所有反应物、过渡态、中间体和产物构型,对优化后各化合物的构型在B3LYP/6-311++G(d,p)基组下进行了单点能计算和零点能矫正,通过能量和振动频率分析以及内禀反应坐标(IRC)计算证实了中间体和过渡态的合理性.并且在优化计算相同基组水平上,应用自然键轨道(NBO)理论和分子中的原子(AIM)理论分析了复合物的成键特征和轨道间相互作用.在CuI单独催化此反应的机理中,计算得到一条反应路径,控制步骤所需活化能是180.49 kJ/mol(sol).而当CuI/BtH共同催化反应时,计算得到两条反应通道IA和IB,其中IA为最优反应通道,控制步骤所需活化能为101.77kJ/mol(sol);IB反应通道控制步骤活化能为143.78 kJ/mol(sol).配体苯并三唑(BtH)加入反应有效地降低了反应控制步骤所需活化能,同时有利于产物和催化剂的分离,这与实验所得结论一致.     

Reactions of thiols and organic disulfides with iron and its oxides

The influence of O₂ and H₂O on the formation of iron dithiolates (IDTs) by the reactions of thiols and organic disulfides with the iron powder was studied under the static (without mechanical activation of the reaction) and dynamic (with mechanical activation of the reaction) conditions. Under the static conditions in the absence of O₂ or H₂O, only BnSH and PhSH give IDTs, whereas DdSH (Dd is dodecyl) produces IDTs in the presence of O₂ or H₂O. For the mechanical activation of the reactions of organic disulfides with the iron powder, the formation of IDTs is possible if the reaction mixture contains H₂O. On the interaction with iron oxides excess thiols are oxidized to organic disulfides and also afford IDTs. Published in Russian in Izvestiya Akademii Nauk. Seriya Khimicheskaya, No. 8, pp. 1383–1386, August, 2006.     

Measurement of the absolute Raman scattering cross section of the 1584‐cm−1 band of benzenethiol and the surface‐enhanced Raman scattering cross section enhancement factor for femtosecond laser‐nanostructured substrates

The absolute Raman scattering cross section (σ_RS) for the 1584‐cm⁻¹ band of benzenethiol at 897 nm (1.383 eV) has been measured to be 8.9 ± 1.8 × 10⁻³⁰ cm² using a 785‐nm pump laser. A temperature‐controlled, small‐cavity blackbody source was used to calibrate the signal output of the Raman spectrometer. We also measured the absolute surface‐enhanced Raman scattering cross section (σ_SERS) of benzenethiol adsorbed onto a silver‐coated, femtosecond laser‐nanostructured substrate. Using the measured values of 8.9 ± 1.8 × 10⁻³⁰ and 6.6 ± 1.3 × 10⁻²⁴ cm² for σ_RS and σ_SERS respectively, we calculate an average cross‐section enhancement factor (EF) of 0.8 ± 0.3 × 10⁶. Copyright © 2009 John Wiley & Sons, Ltd.     

Oxone‐Mediated Oxidative 3‐Arylthio Substitution of Indoles

Oxone‐mediated oxidative 3‐arylthio substitution of indoles with benzenethiols in methanol has been succeeded, giving 3‐arylthioindoles. Indoles bearing a 2‐methyl group particularly exhibited higher activities toward 3‐arylthio substitutions. 3‐(2′‐Pyridylthio)indoles used as selective COX‐2 inhibitors were prepared in good to excellent yields.     

Measurement of the third‐order nonlinear optical susceptibility χ(3) for the 1002‐cm–1 mode of benzenethiol using coherent anti‐Stokes Raman scattering with continuous‐wave diode lasers

The components of the third‐order nonlinear optical susceptibility χ⁽³⁾ for the 1002‐cm^–1 mode of neat benzenethiol have been measured using coherent anti‐Stokes Raman scattering with continuous‐wave diode pump and Stokes lasers at 785.0 and 852.0 nm, respectively. Values of 2.8 ± 0.3 × 10^–12, 2.0 ± 0.2 × 10^–12, and 0.8 ± 0.1 × 10^–12 cm·g^–1·s² were measured for the xxxx, xxyy, and xyyx components of |3χ⁽³⁾|, respectively. We have calculated these quantities using a microscopic model, reproducing the same qualitative trend. The Raman cross‐section σ_RS for the 1002‐cm^–1 mode of neat benzenethiol has been determined to be 3.1 ± 0.6 × 10^–29 cm² per molecule. The polarization of the anti‐Stokes Raman scattering was found to be parallel to that of the pump laser, which implies negligible depolarization. The Raman linewidth (full‐width at half‐maximum) Γ was determined to be 2.4 ± 0.3 cm^–1 using normal Stokes Raman scattering. The measured values of σ_RS and Γ yield a value of 2.1 ± 0.4 × 10^–12 cm·g^–1·s² for the resonant component of 3χ⁽³⁾. A value of 1.9 ± 0.9 × 10^–12 cm·g^–1·s² has been deduced for the nonresonant component of 3χ⁽³⁾. Copyright © 2011 John Wiley & Sons, Ltd.