载气流速对高场不对称波形离子迁移谱的影响

载气流速是影响高场不对称波形离子迁移谱(FAIMS)的重要参数.以自制的高场不对称波形离子迁移谱仪为实验平台,在射频电场幅值3 kV/cm,频率500 kHz,占空比0.36的条件下,研究了载气流速对苯离子迁移谱谱峰强度和半峰宽的影响.实验结果表明: 载气流速为3.7 L/min时,苯样品的谱峰强度最大,仪器的灵敏度最高.随着载气流速的增加,谱峰半峰宽变宽,仪器的分辨率下降.载气流速为3 .0～3.7 L/min时仪器综合性能最佳.此结果对于控制迁移谱仪载气流速有重要的参考意义.     

激光剥蚀-电感耦合等离子体质谱分析中激光剥蚀池载气对信号响应影响的研究

该文以玻璃标准参考物质NIST SRM 612为样本,选择轻、中、重质量元素Li(7)、Cu(63)、Y(89)、Cs(140)、Ru(175)、Th(232)、U(238)为研究对象,探讨了氩气和氦气分别作为激光剥蚀-电感耦合等离子体质谱(LA-ICP-MS)中剥蚀池载气时对质谱分析信号的影响。结果显示:当激光剥蚀池载气为氩气时,载气流量为0.80 L/min,补偿气流量为0.70 L/min或者补偿气流量为0.85 L/min,载气流量为0.70L/min时获得最佳分析信号,信号值稳定(RSD为4%),氧化物离子干扰值小(UO/U为0.27%)。当激光剥蚀池载气为氦气时,补偿气氩气流量为0.95 L/min,载气氦气流量为0.95 L/min时获得最佳的信号强度值,且信号值稳定(RSD为4%,UO/U为0.32%)。对比发现,氦气作为激光剥蚀池载气时质谱分析信号强度明显高于氩气作为载气时的最佳分析信号强度值,各元素的信号强度值平均增强3倍,且背景值低。因此采用氦气作为激光剥蚀池载气,可显著提高分析灵敏度。     

团簇尺寸对奇数和偶数磷团簇离子信号强度差异的影响

磷原子形成的奇数和偶数团簇离子的信号存在明显的强度差异. 当团簇离子尺寸n>25时, 奇数团簇离子的信号强度一般会远远超过其邻近的偶数团簇离子. 为更好地理解团簇尺寸对这一现象的影响, 本文通过真空中激光溅射红磷的方法, 利用质谱对磷团簇离子进行了研究和分析. 结果表明这种方法可以产生较大尺寸(n~500)的磷团簇离子. 进一步对团簇离子的强度分布进行分析表明: 随着正负离子团簇尺寸的增加, 奇/偶数离子强度差异都会逐渐减小. 根据它们的变化趋势, 可以预测: 当n>1000时, 奇/偶数离子强度交替的现象可能会消失. 这一结果正反映出团簇在从原子演变到凝聚态物质过程中的桥梁作用.     

[BxAl13-x]-(x=0～13)二元团簇的密度泛函理论研究

采用遗传算法（Genetic algorithm,GA）对B-Al二元团簇[B_xAl_13-x]^-（x=0～13）进行了全局结构搜索,并在密度泛函理论（Density Functional Theory,DFT）下对其进行了优化计算. 结果表明在二元团簇中,随着硼原子的数量逐渐增加,团簇的结构由二十面体（3D）逐渐转化为准平面（2D）且团簇结构由B与Al原子的比例所决定的. 当x=0～7时,Al原子占多数,团簇保持3D结构;反之团簇呈现2D构型;在x=7～8时,团簇的结构发生由3D向2D的转变. 能量决定着团簇的稳定性（例如相对能量）. 能量越小,其结构越稳定. 在计算相对能量E_rel,当x=1时,其相对能量最低,团簇结构最稳定. 为了进一步了解团簇的稳定性,计算了[B_xAl_13-x]^- 团簇的HOMO-LUMO能级差（E_H-L）和垂直电离能（Vertical Detachment Energies,VDE）,并且发现它们的值在整体上是随着B原子数量的增加而减小,表明其团簇的稳定性逐渐减弱. 在所有的团簇中,BAl₁₂^-的能级差最大,结构最稳定. 因此文章中对其进行了分子轨道分析,发现当一个B原子替代了Al₁₃^-团簇中的中心Al原子时,所得到的BAl₁₂^-的电子壳层结构的1s²和1p⁶几乎和Al₁₃^-团簇保持一致. 此外,对于x=13时的准平面全硼团簇B₁₃^-,文章中用适应性自然密度划分（Adaptive Natural Density Partitioning,AdNDP）对其化学成键进行了分析,结果显示B₁₃^-有8个π电子,具有π反芳香性.     

气相色谱法测定室内空气中苯系物含量的研究

优化了固体吸附/热解吸-气相色谱法测定室内空气中苯、甲苯、乙苯、对二甲苯、间二甲苯、异丙苯、邻二甲苯和苯乙烯等8种苯系物的方法。结果表明,目标物色谱峰分离度均大于1.5;在10～500 ng范围内,8种苯系物质量与色谱峰面积呈良好的线性,相关系数r为0.999 7～0.999 9;该方法的检出限为0.50～3.48ng,当采气量为2L时,最低检出浓度为0.25×10~(-3)～1.74×10~(-3)mg/m~3,相对标准偏差为1.2%～9.1%(n=6),回收率在94.0%～99.5%之间。该方法分离效果好,灵敏度高,精密度好,结果准确,可用于室内空气中苯系物含量的检测。     

整体柱电渗泵的流量控制研究

通过制备丙烯酸酯类整体柱电渗泵,在nL/s～μL/s级流量范围内,考察了操作电压、有机调节剂浓度、盐浓度、pH值等对流量的影响.实验结果表明,在3～17 kV范围内,操作电压与流量呈线性关系,线性相关系数达到0.9991;当选择乙腈(0.55～0.8 mmol/L浓度范围)与MES缓冲溶液混合作为输运溶液时,电渗泵流量随有机调节剂浓度增加而呈减小趋势,且当盐浓度在0.5～2.0 mmol/L范围内逐渐增加时,电渗泵流量逐渐减小;pH值在3～9时,电渗泵流量基本不变.结果表明, 丙烯酸酯类整体柱电渗泵较ODS柱电渗泵具有一定优势.     

团簇离子枪对CH3NH3PbI3钙钛矿薄膜的影响研究

以氩离子团簇为溅射源,对采用一步旋涂法制备的CH₃NH₃PbI₃钙钛矿薄膜进行溅射实验,通过XPS分析检测样品表面Pb元素的价态变化。结果表明,新制备的钙钛矿薄膜材料表面没有检测出Pb⁰,而经过团簇离子枪溅射的样品中部分Pb²⁺还原成Pb⁰,证明了氩离子团簇刻蚀对钙钛矿材料具有破坏作用。一方面,溅射时间的增加以及团簇离子枪能量的增大均会加大钙钛矿材料的损伤程度;另一方面,离子枪团簇规模大小与溅射损伤程度呈近抛物线关系。因此,在进行此类样品表面清洁时,应尽量减小离子枪能量和溅射时间,选择较小或较大的团簇规模以减少对样品的损伤。该研究对于钙钛矿样品在进行XPS检测和数据分析时具有参考价值。     

胶束电动毛细管色谱法测定海洋沉积物中的苯、甲苯和二甲苯

 建立了用胶束电动毛细管色谱法（MECC）对海洋沉积物中的苯、甲苯和二甲苯进行 分析测定的方法 。用45 cm（到检测窗口40 cm）×75　μm i.d.毛细管柱,以75　mmol/L SDS-2　mmol/L 四硼酸钠溶液（外加体积分数为20%的甲醇）为缓冲液（pH 9.16）。当电压为25 kV、检测 波长为200 nm时,苯、甲苯和二甲苯在20 min内得到了良好的分离。用峰面积定量,线性范 围为4～50 mg/L,相对标准偏差在6.2%以内。测得海洋沉积物中的这些苯系物的质量比范围 为3.79～17.36 μg/g。     

利用紫外光离子源高场不对称波形离子迁移谱快速、现场检测水中氨的含量

氨是水体主要的污染物之一,其含量是水质评估的重要参数。本研究采用真空紫外光离子源-高场不对称波形离子迁移谱(Ultraviolet photoionization high field asymmetric waveform ion mobility spectrometry, UVFAIMS)技术,发展一种的水中氨含量的现场快速检测方法。通过对比标准氨样品和水中微量氨UV-FAIMS 谱图峰的特征补偿电压(Compensation voltage, CV)值,确定了水中HN+4的特征离子峰位置;研究了不同分离电压(Dispersion voltages, DV)下HN+4谱图峰位置的关系,获得了HN+4的特征识别系数α2和α4分别为2.21×10-5 Td-2和-1.45323×10-9 Td-4;通过不同浓度样品的信号响应,研究了UV-FAIMS 对水中氨的检出限,在信噪比为3的情况下达到了9.2 μg/ L。本研究为水中氨现场检测提供了一种快速、无需前处理的技术手段。     

纳秒强激光场中苯电离产生高价离子的研究

用25 ns脉冲Nd-YAG 532 nm的激光，在1010～1011 W•cm－2的光场强度下，利用飞行时间质谱对He、 N2、Ar载气条件下苯的激光电离过程进行了研究.发现当利用氩作为载气时，除观察到C2＋、C2H2+、C3H3+、C6H6+离子外，还观察到很强的Cq＋(q=1～3)高价离子.这些离子都有很高的平动能， C2＋的最可几平动能为12.9 eV， C3＋为37.5 eV.通过改变载气种类和压力及在不同光场强度条件下的实验，可以认为这些高价离子来源于含苯团簇的库仑爆炸过程.     

紫外离子迁移谱在线监测芳香族化合物

利用自制紫外离子迁移谱仪,在迁移电场为311V/cm、离子门开门时间0.2ms和室温的条件下,测定了空气中的苯、甲苯、二甲苯以及萘、芴、蒽、1,2,3-三氯苯、5-氯苯酚等芳香族化合物,得到苯的校正迁移率为1.86cm2V-1s-1,且校正迁移率随着分子量的增大而减小。仪器对苯的检出限达到1mg/m3;线性范围达到4个数量级;响应时间小于10s。研究发现,电场强度增大有利于提高仪器的灵敏度,测定时载气流速100mL/min,迁移气流速300mL/min时,效果最佳。     

Behaviour of tetraalkylammonium ions in high‐field asymmetric waveform ion mobility spectrometry

High‐field asymmetric waveform ion mobility spectrometry (FAIMS) is an ion‐filtering technique recently adapted for use with liquid chromatography/mass spectrometry (LC/MS) to remove interferences during analysis of complex matrices. This is the first systematic study of a series of singly charged tetraalkylammonium ions by FAIMS‐MS. The compensation voltage (CV) is the DC offset of the waveform which permits the ion to emerge from FAIMS and it was determined for each member of the series under various conditions. The electrospray ionization conditions explored included spray voltage, vaporizer temperature, and sheath and auxiliary gas pressure. The FAIMS conditions explored included carrier gas flow rate, electrode temperature and composition of the carrier gas. Optimum desolvation was achieved using sufficient carrier gas (flow rate ≥2 L/min) to ensure stable response. Low‐mass ions (m/z 100–200) are more susceptible to changes in electrode temperature and gas composition than high mass ions (m/z 200–700). As a result of this study, ions are reliably analyzed using standard FAIMS conditions (dispersion voltage ?5000 V, carrier gas flow rate 3 L/min, 50% helium/50%nitrogen, inner electrode temperature 70°C and outer electrode temperature 90°C). Variation of FAIMS conditions may be of great use for the separation of very low mass tetraalkylammonium (TAA) ions from other TAA ions. The FAIMS conditions do not appear to have a major effect on higher mass ions. Copyright © 2010 John Wiley & Sons, Ltd.     

一种微型FAIMS传感器芯片的研制

基于微机电系统(MEMS)技术,研制了一种微型高场非对称波形离子迁移谱(FAIMS)传感器芯片.芯片尺寸为18.8mm×12.4mm×1.2mm,由离子化区、迁移区、离子检测区组成.采用真空紫外灯离子源在大气压环境下对样品进行离子化,经过离子化区中聚焦电极的电场作用,实现离子在进入迁移区之前的聚焦,提高离子信号的强度.通过在上下玻璃上溅射Au/Cr(300nm/30nm)金属,并与厚度为200μm、采用感应耦合等离子体(ICP)工艺刻蚀的硅片键合,形成迁移区的矩形通道,尺寸为10mm×5mm×0.2mm.离子检测区为三排直径200μm、间距100μm交错排列的圆柱阵列式微法拉第筒,能同时检测正负离子.采用频率为2MHz,最大电压为364V,占空比为30%的高场非对称方波电压进行FAIMS芯片实验.以丙酮和甲苯为实验样品,载气流速80L·h-1,补偿电压从-10V到3V以0.1V的步长进行扫描,得到了丙酮和甲苯的FAIMS谱图,验证了FAIMS芯片的性能.丙酮和甲苯的FAIMS-MS实验进一步表明FAIMS系统实现了离子分离和过滤功能.     

热解析-高场非对称波形离子迁移谱(FAIMS)技术快速检测合成色素

采用热解析-高场非对称波形离子迁移谱(FAIMS)技术快速检测柯衣定、 孔雀石绿、 罗丹明B和甲基红4种合成色素. 通过对热解析温度和载气流量进行优化, 确定了不同色素的离子特征信号. 在最佳分析条件下, 热解析温度为160 ℃, 载气流量为1.6 L/min, 采用不同模式下补偿电压(CV)值定性, 以FAIMS在正模式下检测柯衣定(CV=0.41 V)和罗丹明B(CV=-0.89 V), 在负模式下检测甲基红(CV=-0.67 V)和孔雀石绿(CV=0.02 V); 用外标法定量检测了样品中的4种合成色素, 线性关系R²≥0.9967, 检出限为2.5~10 μg/L, 定量限为5~20 μg/L, 加标回收率≥78.2%, 相对标准偏差RSD≤8%. 本文为FAIMS技术快速检测合成色素提供了一定的技术基础.     

Peak Profile Analysis in High Field Asymmetric Wave Ion Mobility Spectrometry

High field asymmetric wave ion mobility spectrometry (FAIMS) is a powerful tool to detect and characterize gas-phase ions, while the unsolvable partial differential equation of ions moving in ion drift tube poses a big challenge to FAIMS spectral peak analysis. In this work, a universal and effective model of FAIMS spectral peak profile has been proposed by introducing ion trajectory and loss height. With this model, the influence of the structure of ion drift tube, dispersion voltages, compensation voltages, and carrier gas flow rate on the FAIMS spectral peak characteristics like peak shape, full width at half maximum and peak height is analyzed and discussed. The results show that the influence of different factors on the FAIMS spectral peak profile can be qualitatively described by the model which agrees with the experimental data.     

电动流动分析的色谱分离研究

建立了一种基于增压电渗泵驱动、整体柱分离和紫外检测相结合的电动流动分析系统。研究了载流溶液中甲醇的体积分数对电渗泵空载流量、输出压强、移动相流量和分离度的影响。在4950V的外加电压下,以含0.5mmol/L六亚甲基四胺的45%甲醇溶液为泵载流,电渗泵的流量和输出压强分别为0.58mL/min和0.79MPa,以泵载流为流动相,该系统对苯和萘进行了反相色谱分离。电动流动分析系统设备简单、操作方便、功能多样。对苯和萘的分离结果表明,电动流动分析系统可用于样品的色谱分离。     

Development of an on-line low gas pressure cell for laser ablation-ICP-mass spectrometry.

An on-line low gas pressure cell device has been developed for elemental analysis using laser ablation-ICP-mass spectrometry (LA-ICPMS). Ambient gas in the sample cell was evacuated by a constant-flow diaphragm pump, and the pressure of the sample cell was controlled by changing the flow rate of He-inlet gas. The degree of sample re-deposition around the ablation pit could be reduced when the pressure of the ambient gas was lower than 50 kPa. Produced sample aerosol was drawn and taken from the outlet of the diaphragm pump, and directly introduced into the ICP ion source. The flow rate of He gas controls not only the gas pressure in the sample cell, but also the transport efficiency of the sample particles from the cell to the ICP, and the gas flow rate must be optimized to maximize the signal intensity of the analytes. The flow rates of the He carrier and Ar makeup gas were tuned to maximize the signal intensity of the analytes, and in the case of (238)U from the NIST SRM610 glass material, the signal intensity could be maximized with gas flow rates of 0.4 L/min for He and 1.2 L/min for Ar. The resulting gas pressure in the cell was 30 - 35 kPa. Using the low gas pressure cell device, the stability in the signal intensities and the resulting precision in isotopic ratio measurements were evaluated. The signal intensity profile of (63)Cu obtained by laser ablation from a metallic sample (NIST SRM976) demonstrated that typical spikes in the transient signal, which can become a large source of analytical error, were no longer found. The resulting precision in the (65)Cu/(63)Cu ratio measurements was 2 - 3% (n = 10, 2SD), which was half of the level obtained by laser ablation under atmospheric pressure (6 - 10%). The newly developed low-pressure cell device provides easier optimization of the operational conditions, together with smaller degrees of sample re-deposition and better stability in the signal intensity, even from a metallic sample.     

Enhanced mass resolution tandem mass spectrometry method for 2,3,7,8-tetrachlorodibenzo-p-dioxin detection with ion trap mass spectrometry using high damping gas pressure

Damping gas flow was optimized for 2,3,7,8-tetrachlorodibenzo-p-dioxin (TCDD) determination using ion trap mass spectrometer. A tandem mass spectrometry (MS-MS) method with better than unit-mass resolution (mass width, 0.3 u) was developed at a damping gas flow of 1.5 ml/min and a collision-induced dissociation (CID) voltage of 3.30 V. The relative standard deviation (R.S.D.) at the enhanced resolution was 2.9% in 24 h of consecutive injections. The detection limit was significantly improved because the efficiency of both precursor ion trapping and fragmentation increased with the damping gas flow. Product ion yield was 4.5 times higher and limit of detection was 3.2 times lower than at the default flow (0.3 ml/min and 1.65 V).