10,10’-二甲基-3,3’-二磺酸基-9,9’-双吖啶的电致化学发光行为

研究了新试剂10,10'-二甲基-3,3'-二磺酸基-9,9'-双吖啶(简称DMDSBA)的电致化学发光(ECL)行为. 考察了电化学参数、反应介质以及pH等条件对DMDSBA电致化学发光信号的影响. 结果表明, 在玻碳电极上施加适当电压时, DMDSBA在KNO₃溶液介质中产生很强的电化学发光信号, 于优化的实验条件下, 发光强度的自然对数与DMDSBA浓度的自然对数在1.0×10^-5-1.0×10^-8 mol·L^-1范围内呈良好的线性关系,检出限可达2.3×10^-9 mol·L^-1. 并用循环伏安法、电致化学发光光谱以及荧光光谱, 研究了DMDSBA的电致化学发光机理.     

中心对称双酞菁铥LB膜二次谐波产生特性

利用二次谐波产生(SHG)方法研究了中心对称分子稀土夹心双酞菁铥(TmPc₂) Langmuir-Blodgett (LB)膜二阶非线性光学特性, 测量了二次谐波强度随入射基频光入射角的关系, 并对其二阶非线性产生机制进行了讨论. 实验结果表明, TmPc₂分子LB膜具有较好的二次谐波信号, 二次谐波信号强度的最大值在基频光入射角为45°的地方, 其二阶非线性极化率χ⁽²⁾和分子超极化率β分别为1.152×10^-8和1.905×10^-30 esu. 通过测量样品二次谐波信号的偏振特性, 并与理论分析相比较, 得出其二阶非线性起源于电四极子作用机制.     

C2(X1Σg+)自由基与不饱和碳氢化合物反应的温度效应

运用脉冲激光光解-激光诱导荧光(PLP-LIF)的方法在293-573 K的温度范围内测量了C₂(X¹Σ_g⁺)自由基与不饱和碳氢化合物(C₂H₄和C₂H₂)气相反应的双分子反应速率常数. 获得的速率常数可以用Arrhenius 公式表达如下(单位: cm³·molecule^-1·s^-1): k(C₂H₄)=(1.16±0.10)×10^-10exp[(290.68±9.72)/T], k(C₂H₂)=(1.36±0.02)×10^-10exp[(263.85±7.60)/T], 误差为2σ. 由获得的双分子反应速率常数及其所呈现的负温度效应, 我们认为在293-573 K温度范围内C₂(X¹Σ_g⁺)自由基和不饱和碳氢化合物的反应遵循加成机理.     

二氧化硅栅绝缘层的制备与表面修饰

研究了有机薄膜晶体管的二氧化硅栅绝缘层的性质。二氧化硅绝缘层的制备采用热生长法，氧化气氛是O₂(g)+H₂O(g)，工艺为干氧-湿氧-干氧的氧化过程。制得的绝缘层漏电流在10^-9 A左右。以该二氧化硅作为有机薄膜晶体管的栅绝缘层，并五苯作为有源层制作了有机薄膜晶体管器件。实验表明采用十八烷基三氯硅烷(OTS)进行表面修饰的器件具有OTS/SiO₂双绝缘层结构，可以有效地降低SiO₂栅绝缘层的表面能并改善表面的平整度。修饰后器件的场效应迁移率提高了1.5倍、漏电流从10^-9 A降到10^-10 A、阈值电压降低了5 V、开关电流比从10⁴增加到10⁵。结果显示具有OTS/SiO₂双绝缘层的器件结构能有效改进有机薄膜晶体管的性能。     

等离激元增强上转换发光及其分子检测应用

针对荧光分子检测普遍灵敏度低和检测范围窄的问题,制备了具有等离子激元共振特性的重掺杂半导体纳米结构Cu_2-xS和典型的稀土掺杂上转换发光纳米颗粒NaYF₄∶Yb,Er,通过三相界面自组装方法获得了Cu_2-xS/NaYF₄∶Yb,Er薄膜基底。结合有限元模拟,计算了不同摆放情况下Cu_2-xS周围的局域电场分布,研究了在实际薄膜中Cu_2-xS纳米盘之间产生的等离激元耦合对上转换发光性能以及对拉曼信号增强的影响。结果表明,Cu_2-xS等离激元层与NaYF₄∶Yb,Er发光层的耦合,不仅得到了上转换 3个数量级的提高,还实现了分子检测 10^-7 mol·L^-1的检测极限,并且获得了 10^-3~10^-7 mol·L^-1的宽线性响应,从而达到高灵敏度的定性和定量双功能的精确检测。     

等离激元增强上转换发光及其分子检测应用

针对荧光分子检测普遍灵敏度低和检测范围窄的问题,制备了具有等离子激元共振特性的重掺杂半导体纳米结构Cu_2-xS和典型的稀土掺杂上转换发光纳米颗粒NaYF₄：Yb,Er,通过三相界面自组装方法获得了Cu_2-xS/NaYF₄：Yb,Er薄膜基底。结合有限元模拟,计算了不同摆放情况下Cu_2-xS周围的局域电场分布,研究了在实际薄膜中Cu_2-xS纳米盘之间产生的等离激元耦合对上转换发光性能以及对拉曼信号增强的影响。结果表明,Cu_2-xS等离激元层与NaYF₄：Yb,Er发光层的耦合,不仅得到了上转换3个数量级的提高,还实现了分子检测10^-7 mol·L^-1的检测极限,并且获得了10^-3~10^-7 mol·L^-1的宽线性响应,从而达到高灵敏度的定性和定量双功能的精确检测。     

黄曲霉素B2分子吸附在银团簇的表面增强拉曼散射机理

采用密度泛函理论（DFT）B3LYP方法,6-311G（d,p）（C,H,O）/LANL2DZ（Ag）基组,计算了黄曲霉素B₂（AFB₂）分子吸附在Ag₂团簇的表面增强拉曼散射（SERS）光谱和预共振拉曼光谱,并与实验结果比较. 结果显示：AFB₂分子在基态Ag₂团簇表面吸附时,增强因子最大达到10²,对应吡喃（pyrane）环C=O伸缩振动,主要是由AFB₂分子周围化学环境改变而引起的基态静极化率改变导致的化学增强. 不同激发波长下的AFB₂分子预共振拉曼光谱的增强强度不同：电荷转移态激发波长为1144 和544 nm时拉曼信号增强了10²倍,而选择电荷转移预共振波长432和410 nm作为入射光时,其拉曼信号增强了10⁴倍,增强机理为银团簇和黄曲霉素分子之间的电荷转移共振增强. 因此通过改变入射光波长,选择电荷转移共振激发波长,更有利于强致癌物AFB₂分子的痕量检测.     

锌族和钛族卤化物振动光谱的理论计算

采用ab initio RHF,MP2和B3LYP方法以及LanL2DZ和SDD基组计算了四面体锌族卤素阴离子化合物(MX₄^2-,M=Zn(Ⅱ),Cd(Ⅱ),Hg(Ⅱ);X=F^-,Cl^-,Br^-,I^-)和钛族卤化物(MX₄,M=Ti(Ⅳ),Zr(Ⅳ),Hf(Ⅳ);X=F^-,Cl^-,Br^-,I^-)的几何构型和振动频率。计算结果表明,LanL2DZ基组是合适的基组,能得到合理的电荷分布,几何参数以及振动频率。在锌族卤化物的计算中发现,角弯曲振动频率与实测值相当一致,键伸缩振动频率略为偏低,这主要是由于计算的键长略为偏长所致。MP2方法计算的振动频率更接近于实测值。在钛族卤化物的计算中,三种计算方法都相当地再现了实测值,而以B3LYP方法更为满意。     

一种基于壳聚糖固定葡萄糖氧化酶的葡萄糖生物传感器的研究

本文选用生物相容性好的壳聚糖作为基体材料，使其与戊二醛交联成网状结构包埋葡萄糖氧化酶制成电化学传感器。这种壳聚糖膜不仅可以减小葡萄糖氧化酶的流失，而且能为酶提供了适宜的微环境。用红外光谱、紫外光谱及透射电镜对膜的形态和性质进行了表征。实验结果表明该传感器具有很快的响应速度，很好的稳定性和重现性，能选择性地催化葡萄糖并测定其浓度。该传感器的制备方法简单，成本低，于冰箱中放置两周信号保持在90％以上，对葡萄糖测量的线性范围为1×10^-5 - 3.4×10^-3mol•L^-1，当信噪比为3:1时检测限为5×10^-6mol•L^-1。     

含双-NH结合位点的新型阴离子识别受体的合成及结合能力研究

合成了基于含有双功能-NH结合位点的选择识别阴离子的新型有色识别受体。与其它卤素阴离子相比，其在二甲基亚砜中的紫外可见光谱显示了F^-存在时具有高选择性，当存在四丁基氟化胺（5X10^-5mol.dm^-3）时颜色明显的由无色变到黄色. 当受体与四丁基醋酸胺、四丁基磷酸二氢胺、四丁基氢氧化胺作用时紫外可见光谱也出现了类似的变化。受体与四丁基氯化胺、四丁基溴化胺、四丁基碘化胺几乎没有作用。该受体与球形卤素阴离子的结合能力取决于卤素离子的直径和形成氢键能力大小，而其与三角型（AcO^-）、四面体型（H₂PO₄^-）、直线型（OH^-）结合能力的差异是由几何构形所决定的。     

Estimation of the optimal sampling frequency for process analyzers

The sampling theorem states that the sampling frequency should be twice the highest frequency of the studied signal. This sets limits to the lowest allowable sampling frequency of a process analyzer. Economic criteria together with the instrument analysis time define the highest sampling frequency. The stability of the control loop requires that the roots of the characteristic equation of the control loop in the z plane should lie inside the unit circle. An example is discussed. In order to minimize the error in the estimation of parameters of a system using an impulse excitation signal, the sampling time should be equal to the dominant time constant of the system.     

Thin-layer chromatography/electrospray ionization triple-quadrupole linear ion trap mass spectrometry system: analysis of rhodamine dyes separated on reversed-phase C8 plates

The direct analysis of separated rhodamine dyes on reversed-phase C(8) thin-layer chromatography plates using a surface sampling/electrospray emitter probe coupled with a triple-quadrupole linear ion trap mass spectrometer is presented. This report represents continuing work to advance the performance metrics and utility of this basic surface sampling electrospray mass spectrometry system for the analysis of thin-layer chromatography plates. Experimental results examining the role of sampling probe spray end configuration on liquid aspiration rate and gas-phase ion signal generated are discussed. The detection figures-of-merit afforded by full-scan, automated product ion and selected reaction monitoring modes of operation were examined. The effect of different eluting solvents on mass spectrum signal levels with the reversed-phase C(8) plate was investigated. The combined effect of eluting solvent flow-rate and development lane surface scan rate on preservation of chromatographic resolution was also studied. Analysis of chromatographically separated red pen ink extracts from eight different pens using selected reaction monitoring demonstrated the potential of this surface sampling electrospray mass spectrometry system for targeted compound analysis with real samples.     

Multi-ion quantitative mass spectrometry by orthogonal projection method with periodic signal of electrostatic ion beam trap

In this article, orthogonal projection method (OPM) is introduced which could perform multi-ion quantitative MS with signal of electrostatic ion beam trap (EIBT), and its application has been demonstrated by numerical modeling. To acquire periodic current signal, a model of EIBT with cylindrical-detector is set up to simulate ions' oscillatory motion. Whereafter, OPM is introduced and applied for quantitative MS with sampling time being as short as 200 μs. Comparing with fast Fourier transform (FFT), the MS acquired by OPM is characterized by a more readable spectrum, a much shortened sampling time and the ability to do quantitative analysis. Within the optimum sampling time range, quantitative MS could be performed with accuracy of over 90%. It is found that the lower limit and the upper limit of the optimum sampling time range are all proportional to M(3/2)/δM and its relation is specified by linear regression. Aided by the results of FFT, OPM is applied to a compound tested signal induced by three kinds of ions. It shows that OPM could be performed respectively to each kind of ions without interference from other component of the signal. The resolving power acquired by OPM is about 75 000 with sampling time as short as 10 ms, and the quantitative result that acquired is quite accurate.     

用于痕量分析的高精度色谱数据采集卡

设计了一由双电压频率转换器（ＶＦＣ）构成高精度色谱数据采集方法，具有原理简单、精度高、噪声小、价格低等特点，可广泛应用于色谱分析中分析信号的采集．     

Improved desorption electrospray ionization mass spectrometry performance using edge sampling and a rotational sample stage

The position of the surface to be analyzed relative to the sampling orifice or capillary into the mass spectrometer has been known to dramatically affect the observed signal levels in desorption electrospray ionization mass spectrometry (DESI‐MS). In analyses of sample spots on planar surfaces, DESI‐MS signal intensities as much as five times greater were routinely observed when the bottom of the sampling capillary was appropriately positioned beneath the surface plane (‘edge sampling’) compared with when the capillary just touched the surface. To take advantage of the optimum ‘edge sampling’ geometry and to maximize the number of samples that could be analyzed in this configuration, a rotational sample stage was integrated into a typical DESI‐MS setup. The rapid quantitative determination of caffeine in two diet sport drinks spiked with an isotopically labeled internal standard demonstrated the utility of this approach. Published in 2008 by John Wiley & Sons, Ltd.     

Consideration of some sampling problems in the on-line analysis of batch processes by low-field NMR spectrometry

A low-field medium-resolution NMR spectrometer, with an operating frequency of 29 MHz for 1H, has been assessed for on-line process analysis. A flow cell that incorporates a pre-magnetisation region has been developed to minimise the decrease in the signal owing to incomplete polarisation effects. The homogeneous esterification reaction of crotonic acid and 2-butanol was monitored using a simple sampling loop; it was possible to monitor the progression of the reaction through changes in CH signal areas of butanol and butyl crotonate. On-line analysis of heterogeneous water-toluene mixtures proved more challenging and a fast sampling loop system was devised for use with a 5 L reactor. The fast sampling loop operated at a flow rate of 8 L min(-1) and a secondary sampling loop was used to pass a sub-sample through the NMR analyser at a slower (mL min(-1)) rate. It was shown that even with super-isokinetic sampling conditions, unrepresentative sampling could occur owing to inadequate mixing in the reactor. However, it was still possible to relate the 1H NMR signal obtained at a flow rate of 60 mL min(-1) to the composition of the reactor contents.     

微流动注射进样-加热雾室-等离子体质谱测定血清中的铂

开发了一种基于雾化室加热的微流动注射进样系统,并用于血清中Pt的测定。该进样系统由微量毛细管雾化器、加热微型雾化室、八通道十六孔多功能旋转阀、蠕动泵和注射泵组成。研究了雾化室尺寸、加热温度和采样环体积对信号强度的影响。当雾化室内径为9 mm、加热段长度为6 cm,雾化室温度90 ℃,采样环体积为5 μL时,195Pt的信号强度提高了2.31倍,同时信号精密度从5.1%降至2.2%,并得到峰形良好的信号峰。该进样系统的试样消耗小、灵敏度和检出限均优于常规进样系统。10次测定10 μg/L的Pt标准溶液和血清样品溶液,峰高的RSD分别为2.9%和3.3%。该进样系统测得10个血清中的Pt含量与常规进样系统的测试结果无显著差异,在样品量稀少的情况下具有良好的应用价值。     

流动注射在线离子交换预富集-氢化物发生原子荧光光谱法测定痕量碲的研究

研究了流动注射在线离子交换预富集及在线氢化物发生法与原子荧光光谱法的联用技术。设计了双柱交替正向富集和反向洗脱的在线离子交换流路系统。在采样频率为３０次／ｈ下，灵敏度较常规流动注射氢化物发生原子荧光光谱法提高１１倍。应用于环境水样中痕量碲的分析，获得了满意的结果。     

Accelerating Diffusion‐Ordered NMR Spectroscopy by Joint Sparse Sampling of Diffusion and Time Dimensions

Diffusion‐ordered multidimensional NMR spectroscopy is a valuable technique for the analysis of complex chemical mixtures. However, this method is very time‐consuming because of the costly sampling of a multidimensional signal. Various sparse sampling techniques have been proposed to accelerate such measurements, but they have always been limited to frequency dimensions of NMR spectra. It is now revealed how sparse sampling can be extended to diffusion dimensions.     

Sampling frequency,response times and embedded signal filtration in fast,high efficiency liquid chromatography: A tutorial

With increasingly efficient columns, eluite peaks are increasingly narrower. To take full advantage of this, choice of the detector response time and the data acquisition rate a.k.a. detector sampling frequency, have become increasingly important. In this work, we revisit the concept of data sampling from the theorem variously attributed to Whittaker, Nyquist, Kotelnikov, and Shannon. Focusing on time scales relevant to the current practice of high performance liquid chromatography (HPLC) and optical absorbance detection (the most commonly used method), even for very narrow simulated peaks Fourier transformation shows that theoretical minimum sampling frequency is still relatively low (<10 Hz). However, this consideration alone may not be adequate for real chromatograms when an appreciable amount of noise is present. Further, depending on the instrument, the manufacturer's choice of a particular data bunching/integration/response time condition may be integrally coupled to the sampling frequency. In any case, the exact nature of signal filtration often occurs in a manner neither transparent to nor controllable by the user. Using fast chromatography on a state-of-the-art column (38,000 plates), we evaluate the responses produced by different present generation instruments, each with their unique black box digital filters. We show that the common wisdom of sampling 20 points per peak can be inadequate for high efficiency columns and that the sampling frequency and response choices do affect the peak shape. If the sampling frequency is too low or response time is too large, the observed peak shapes will not remain as narrow as they really are – this is especially true for high efficiency and high speed separations. It is shown that both sampling frequency and digital filtering affect the retention time, noise amplitude, peak shape and width in a complex fashion. We show how a square-wave driven light emitting diode source can reveal the nature of the embedded filter. We discuss time uncertainties related to the choice of sampling frequency. Finally, we suggest steps to obtain optimum results from a given system.