毛细管流动池在光声检测中的应用

设计了适于激光诱导光声流动检测的毛细管流动池,讨论了池的特点及其在分析化学中的应用,用该池检测Co~(2+),检测限相当于2×10~(-6)cm~(-1)光吸收。     

色谱中的光声光谱检测

光声光谱是本世纪七十年代初期重新兴起的高灵敏度光谱分析新技术。它适用于透明、不透明,甚至强散射样品在紫外,可见,红外光区的光热性质研究,已在物理、化学、工程材料、生物、医学等领域得到广泛的应用。 光声光谱(简称PAS)是一种光热吸收光谱,当用一束调制后的(或脉冲的)单色光照射样品时,样品吸收以后,以无辐射弛豫方式将吸收的光能部分或全部地转换成热,样品受热体积膨胀,产生以光源为中心向外扩展的压力波,用置于其中的声传感器便可接收到光声信号。用波长扫描方法得到样品的光声图谱可做定性分析。根据光声信号大小与物质吸光度成正比的关系进行定量分     

光声位相理论及其在化学中的应用研究进展

光声位相作为光声光谱重要的一部分, 包含着很多有价值的信息, 对它的研究可以获得其它光谱甚至光声振幅谱都不能得到的信息。光声位相在测定样品的光学和热学性质、样品无辐射弛豫过程的研究以及深度剖面分析等方面显示了特有的能力。本文结合本实验室近几年的工作, 在光声光谱理论的基础上,对光声位相理论及其在化学中的应用作一综述。     

用温度敏感高分子为载体的激光光声免疫分析及其应用

将单克隆抗乙肝表面抗原体抗与温度敏感高分子聚Ｎ－异丙基丙烯酰胺连接，中液相中与抗原、酶标抗体反应，通过热沉淀实现与游离酶标体抗体的异相分离。高分子载休的引入能减少非特异性吸附，罗大相载体聚乙烯酶标板更有利于激光光声技术高灵敏度优势的。同时，采用０．５％的十二烷基硫酸钠水溶液作显色终止剂，易与Ｈｅ－Ｎｅ激光波长匹配，实现了对低值乙肝表面抗原阳性血清的检测。     

膜上痕量亚甲蓝样品的间接光声检测

介绍了一种新的膜上痕量样品分析方法与实验装置。利用间接光声效应对光吸收物质进行检测，全文对方法原理、实验装置以及影响因素进行了详尽讨论。膜上亚甲蓝定量线性范围１×１０＾－６￣１×１０＾－４ｍｏｌ／Ｌ，检出限为４６ｐｇ。     

透明质酸纳米材料在荧光/光声成像和光疗中的应用

荧光/光声成像和光疗技术的生物医学应用引起了人们越来越多的关注, 然而很多荧光/光声造影剂存在生物相容性较差, 缺乏肿瘤靶向性, 信噪比较低, 功能单一等共性问题, 严重限制其诊疗应用. 透明质酸具有优异的生物相容性和主动肿瘤靶向性, 可被透明质酸酶降解, 并且易于化学修饰和实现多种超分子弱相互作用力协同工作. 因此, 人们将透明质酸与荧光/光声造影剂结合制备纳米材料, 使其在细胞乃至活体的标记性能和治疗效果获得了很大的改善. 本文综述了将两类物质结合制备纳米材料的方法, 着重阐述了纳米材料的结构与性能关系, 为其未来设计和开发提供了指导, 最后对存在的主要问题以及未来的重要研究方向进行了分析和展望.     

溶液中三价稀土Ho3+、Nd3+的脉冲激光光声光谱研究及其测定

采用自制的液体光声传感器,研究了在620～665nm波长范围不同溶剂中稀土Ho³⁺的光谱精细结构;探讨了入射激光脉冲能量、测试温度以及各种与水混溶的有机溶剂对光声信号强度的影响。在乙腈水溶液中测定稀土Ho³⁺、Nd³⁺检测限分别为5×10^-8mol/L和1.0×10^-7mol/L,相应的吸光度为1.5×10^-7和6.3×10^-7。     

激光反射光声测定及其应用

详细研究了激光反射光声法的测定原理、实验装置及影响参数。利用反射光声效应进行膜上痕量样品检测，对精氨酸定量线性范围达２个数量级（５×１０－２～５×１０－４ｍｏｌ／Ｌ）。检出限为１５２ｐｍｏｌ。方法用于药物中精氨酸的测定，结果满意。     

Time-Resolved Photoacoustic Calorimetry: From Carbenes to Proteins

Why have molecules only been seen but not heard? For over a century chemists have probed reactions with various spectroscopic methods to learn about structures, dynamics, and reactivities of their molecules. What they have not done is to listen to their molecules react. Although the photoacoustic phenomenon has been known since 1880, it is only in the last twenty years that technology has developed to the point where sound waves produced by reacting molecules can be time resolved and the information contained within the waves deciphered. The information content within the photoacoustic wave is indeed rich, for one can learn about the dynamics and the magnitude of enthalpy changes associated with the reaction as well as the changes in molecular volume. This review article chronicles the development of time-resolved photoacoustic calorimetry and its application to a variety of reactions encountered in organic and organometallic chemistry and biochemistry.     

A Biocompatible Probe for the Detection of Neutrophil Elastase Free from the Interference of Structural Changes and Its Application to Ratiometric Photoacoustic Imaging In Vivo

Neutrophil elastase (NE) plays a key role in chronic inflammation and acute responses to infection and injury. Effective disease interventions thus call for precise identification of NE to aid the clinical treatment of such diseases. However, the detection process suffers from the interference of structural changes of NE. Herein, we introduce a molecular probe with high biocompatibility to overcome the interference, which was achieved by combining theoretical calculations and experimental studies, that permits highly specific and sensitive detection of NE in cells and in vivo. The upregulated NE accumulation was specifically measured in inflammation by ratiometric photoacoustic and near-infrared fluorescence imaging, providing a new method for developing more specific fluorogenic probes for other enzymes.     

Photoacoustic spectroscopy of solids and surfaces

After briefly reviewing the theory and instrumentation, results from a variety of experiments carried out by the authors on the photoacoustic spectroscopy of solids and surfaces by employing an indigenous spectrometer are discussed in the light of the recent literature. Some of the important findings discussed are, phase angle spectroscopy, anomalous behaviour of monolayers, unusual frequency dependence in small cell volumes, spectra of a variety of solids including amorphous arsenic chalcogenides, photoacoustic detection of phase transitions and determination of surface areas and surface acidities of oxides. Recent developments such as piezoelectric photoacoustic spectroscopy, depth profiling and subsurface imaging are also presented. Contribution No. 124 from the Solid State and Structural Chemistry Unit.     

Photoacoustic spectroscopy of condensed matter.

Photoacoustic spectroscopy is a new analytical tool that provides a simple nondestructive technique for obtaining information about the electronic absorption sprctrum of samples such as powders, semisolids, gels, and liquids. It can also be applied to samples which cannot be examined by conventional optical methods. Numerous applications of this technique in the field of inorganic and organic semiconductors, biology, and catalysis have been described. Among the advantages of photoacoustic spectroscopy, the signal is almost insensitive to light scattering by the sample and information can be obtained about nonradiative deactivation processes. Signal saturation, which can modify the intensity of individual absorption bands in special cases, is a drawback of the method.     

Photoacoustic infrared spectroscopy of polymer beads

Photoacoustic (PA) spectra of four types of polymer resin beads, ranging in size from 35 to 150 μm, were acquired using a Fourier transform infrared spectrometer capable of both rapid- and step-scan mirror movement. Thermal diffusion lengths were on the order of the particle sizes of the beads. The PA magnitude spectra were similar to absorption spectra; both positive- and negative-going features occurred in the phase spectra. The frequency dependences of the total PA intensities of the polymer resins and carbon black differed by a factor of about f^−0.30. The intensities of the weak bands in the ratioed spectra (resin beads/carbon black) displayed a similar dependence. Partial saturation caused a more gradual variation for the stronger bands, where the intensity is proportional to f^−0.1–f^−0.2.