Refractive index of standard oils as a function of wavelength and temperature

The refractive indices (n) of eight standard oils from Physikalisch Technische Bundesanstalt, Germany were determined with an accuracy of ±1×10⁻⁴ by using Abbe Refractometer. The measurements were performed at temperature 20°C in the spectral range 0.4–0.7 μm. The experimental data were fitted to the simple Cauchy dispersion formula and the results were found to be consistent within the limits of experimental error. In all cases, the refractive index decreased monotonically with increasing wavelength. The refractive indices (n) of these oils have been measured as a function of the temperature t (20°C up to 50°C) at λ=0.589 μm and were found to have linear temperature dependencies. The refractive indices of the studied oils and the uncertainty in their values are calculated at λ=0.589. The Lorentz–Lorenz (L–L) formula has been tested and it was found to be valid with a maximum deviation of 0.4% and was used to calculate the molecular polarizability θ.     

丙烯腈-尿素包合物的形成过程及特征

利用差示扫描量热法(DSC)和X射线衍射(XRD)研究了在不同丙烯腈/尿素投料比情况下的丙烯腈-尿素包合物的形成过程和组成. 实验结果表明DSC是一种研究包合物的客主比及分解热的有效方法. 测定了丙烯腈-尿素包合物的客主比和分解热分别为1.17和5361.53 J/mol. 同时发现丙烯腈-尿素包合物的形成依赖于冷冻时间,在足够长的冷冻时间之后丙烯腈-尿素包合物的组成达到稳定状态. 实验结果表明,丙烯腈分子可能是采用堆叠的方式排布在尿素晶道结构中. XRD结果表明只要丙烯腈分子进入尿素晶格中,丙烯腈-尿素包合物的结构便形成了,并且这种结构与形成过程终了时的结构是一致的. 只要丙烯腈是足量的,包合物中的丙烯腈分子排列会随冷冻时间的延长而增长,直到尿素的晶道结构被丙烯腈分子填满.     

高Q值超薄完美吸波体设计方法研究

为了增强完美吸波体的吸波性能,提出了一种高Q值超薄完美吸波体的设计方法. 该方法将基片集成波导技术与一般完美吸波体设计方法有机结合,通过合理添加金属过孔实现了高Q值的完美吸波体设计. 利用该方法设计出了厚度0.0065λ、半波功率带宽5.8%的完美吸波体,其吸波率Q值为33.9,比普通完美吸波体吸波率Q值提升了20%以上;其1.5和3 dBsm的雷达散射截面缩减Q值分别提高了54%和67%以上;同时该方法消除了传统设计中的频率偏移问题. 实测与仿真结果表明所设计的吸波体具有高Q值特征,也具有良好的雷达散射截面缩减效果,散射截面缩减最高达14 dBsm. 仿真和实测验证了设计方法的可靠性. 关键词： 基片集成波导技术 频率偏移 吸波率 雷达散射截面     

Molar extinction coefficients of some carbohydrates in aqueous solutions

Molar extinction coefficients of some carbohydrates viz. l-arabinose (C₅H₁₀O₅), d-glucose (C₆H₁₂O₆), d-mannose (C₆H₁₂O₆), d-galactose (C₆H₁₂O₆), d(-) fructose (C₆H₁₂O₆) and maltose (C₁₂H₂₄O₁₂) in aqueous solutions have been determined at 81, 356, 511, 662, 1173 and 1332 keV by gamma ray transmission method in a narrow beam good geometry set-up. These coefficients have been found to depend upon the photon energy following a 4-parameter polynomial. These extinction coefficients for different sugars having the same molecular formula have same values varying within experimental uncertainty. Within concentration ranges studied, Beer-Lambert law is obeyed very well.     

卟啉钯敏化剂构效性质与三线态-三线态湮灭上转换性能研究

上转换发光是一种将长波长的激发光转化为短波长发射的反斯托克斯发光现象,三线态-三线态湮灭上转换（TTA-UC）能够在较低密度能量下被激发,且上转换量子产率高,因此获得研究者们广泛关注。关于敏化剂分子结构与上转换发光性能相关性的研究一直是TTA-UC研究领域的重要热点,选择两种代表性的卟啉钯光敏剂[PdOEP-八乙基卟啉钯(Ⅱ)和PdBrTPP-四溴苯基卟啉钯(Ⅱ)]与蒽衍生物9,10-(4-羟甲基)苯基蒽p-DHMPA发光剂组合上转换体系作为研究模型,通过一系列合成工作获得材料分子后,进一步比较两种敏化剂的光谱性质与体系最终上转换性能之间关系。通过细致研究敏化剂和发光剂的荧光发射和寿命等光谱性质对敏化剂系间窜越,三线态-三线态能量转移及三线态-三线态湮灭等能量传递过程的影响后,发现在532 nm处的摩尔吸光系数PdBrTPP (10.8 cm-1·mmol-1)大于PdOEP (3.0 cm-1·mmol-1);三线态寿命PdBrTPP (173.13 μs)大于PdOEP (109.21 μs)。但与p-DHMPA配对时光敏剂与发光剂的三线态能级差ΔE_TT,PdOEP (0.140 eV)却高于PdBrTPP (0.062 eV),通过Stern-Volmer方程得到Stern-Volmer猝灭常数K_SV和双分子猝灭常数k_q值也是PdOEP略高,最终表现出上转换阈值PdOEP/p-DHMPA (22.40 mW·cm-2)小于PdBrTPP/p-DHMPA (29.78 mW·cm-2),上转换发光效率Φ_UC,PdOEP/p-DHMPA (28.3％)大于PdBrTPP/p-DHMPA (26.8％)。因此,卟啉钯敏化剂的构效对三重态湮灭上转换发光效率影响最为重要的决定因素是敏化剂三线态高低。对于不同的敏化剂,在分子主体结构、摩尔吸光系数与三线态寿命等光谱参数差别不大的情况下,敏化剂的三线态能级越高,就将会具有更大的上转换发光效率。然而如果以总上转换能力指标来评价,PdBrTPP的共轭结构能够提升其在激发波长处吸收更多光子的能力,具有比PdOEP更高的摩尔吸光系数,造成其总上转换能力η比PdOEP高3.4倍。因此从上转换总效能指标来评价,通过敏化剂分子设计调控其在激发光波长处的摩尔吸光系数也不失为一种简单易行的方法。     

光辐射吸收材料表面形貌与吸收率关系研究

光辐射吸收材料不同的表面形貌对入射光具有不同的多重反射吸收效果,对光辐射的吸收有较大的影响,合适的表面形貌可以提高光辐射有效吸收率.本文通过光线追迹的方法对V形表面、正弦表面、具有正态倾角(平均倾角)分布的表面以及具有正态高度分布的表面进行模拟, 分析了这四种表面对光辐射吸收率的提升效果及其入射角特性.通过倾角分布分析,得出不同表面形貌提升吸收率共同的必要条件,即倾角中心分布至少大于30°,并指出V形表面在正入射时对吸收率提升的优越性. 关键词： 光吸收材料 表面形貌 吸收率 表面倾角分布     

Effects of pressure and temperature on the solubility of monosodium L-glutamate monohydrate in water

Abstract

The solubility of monosodium L-glutamate monohydrate (MSG.H₂O) in water was measured at pressures in the range of 0.10-300MPa and 298.15K. The density of MSG solution at high concentrations and heat of solution at saturated concentration were also measured at atmospheric pressure. The solubility, m_s, increased with increasing pressure and the pressure coefficient, Θ_p, [?(? In m_s,? p)_T] at 0.10 MPa was (2.0 ± 0.1) × 10-¹⁰Pa-1. It agrees well with (2.1 ±0.2)× 10-¹⁰ Pa-¹ thermodynamically estimated using the partial molar volume, the activity coefficient of the solute in solution, and the molar volume of the crystal. The excellent agreement at 0.10MPa gives us confidence in the solubility data at higher pressures. The heat of solution data and other pertinent values were used to calculate the temperature coefficient of solubility, Θ_T [? (? In m_s/?(1/T))_p], by a thermodynamic equality. The resulting Θ_T compares well with the data directly measured by Ogawa.     

基于波长调制-直接吸收光谱方法的CO分子1567 nm处谱线参数高精度标定

直接吸收光谱(DAS)可直接测量分子吸收率函数,并通过拟合吸收率函数确定待测气体参数.波长调制-直接吸收光谱(WM-DAS)在DAS基础上,结合了波长调制光谱(WMS)中谐波分析思想,利用傅里叶变换复现吸收率函数,可有效提高吸收率函数的测量精度.本文利用WM-DAS方法结合长光程气体吸收池,在室温低压条件下,对CO分子1567 nm处R5-R11近红外弱吸收谱线吸收率函数进行了精确复现,其拟合残差标准差低至3×10^-5,随后根据测得的吸收率函数对谱线的碰撞展宽、Dicke收敛以及速度依赖的碰撞展宽系数等光谱参数进行了高精度标定,并将其与高灵敏度的连续波腔衰荡光谱(CW-CRDS)测量结果进行了比较,实验结果表明该方法与CW-CRDS测量结果具有高度一致性,更具有系统简单、测量速度快、对环境要求低等优点.     

Refractive Indices, Densities and Excess Molar Volumes of Monoalcohols + Water

The refractive index, n _D , and density, ρ, of binary mixtures of monoalcohols + water, have been measured at a temperature of 298.15,K and atmospheric pressure. The variation of the refractive indices of these solutions has also been determined with temperature in the range T = (278.15 to 338.15) K and atmospheric pressure. A comparative study has been made of the refractive indices obtained experimentally and those calculated by means of the Lorentz-Lorenz [Theory of Electrons, Dover Phoenix (1952)] and Gladstone-Dale relations [Trans. R. Soc. London 148:887–902 (1858)]; in all cases, the Gladstone–Dale equation was seen to afford values similar to those obtained experimentally. Calculations have been made of the excess molar volumes, V ^E, and the molar refraction deviations, ΔR, of these mixtures and the differences between the experimental values for refractive index and those obtained by means of the Gladstone–Dale equation. Values of V ^E were compared with others in the literature. In all cases the V ^E values were negative, and in all cases, except in the methanol + water, ΔR showed a maximum for x = 0.8.     

Advanced analytical methods for the structure elucidation of polystyrene-b-poly(n-butyl acrylate) block copolymers prepared by reverse iodine transfer polymerisation

Reverse iodine transfer polymerisation (RITP) is a living radical polymerisation technique that has shown to be feasible in synthesising segmented styrene-acrylate copolymers. Polymers synthesised via RITP are typically only described regarding their bulk properties using nuclear magnetic resonance spectroscopy and size exclusion chromatography. To fully understand the complex composition of the polymerisation products and the RITP reaction mechanism, however, it is necessary to use a combination of advanced analytical methods. In the present RITP procedure, polystyrene was synthesised first and then used as a macroinitiator to synthesise polystyrene-block-poly(n-butyl acrylate) (PS-b-PBA) block copolymers. For the first time, these PS-b-PBA block copolymers were analysed by a combination of SEC, in situ¹H NMR and HPLC. ¹H NMR was used to determine the copolymer composition and the end group functionality of the samples, while SEC and HPLC were used to confirm the formation of block copolymers. Detailed information on the living character of the RITP process was obtained.