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Gas Sampling Glow Discharge: A Versatle Ionization Source for Gas Chromatography Time-of-Flight Mass Spectrometry

机译:气体采样辉光放电:气相色谱飞行时间质谱的通用电离源

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A gas chromatograph has been coupled to a direct-current gas sampling glow discharge (GSGD) ionization source for the mass spectrometric analysis of halogenated hydro-carbons. The continuous discharge is contained within the first vacuum stage of the differentially pumped specirom-eter interface. The discharge can be operated statically or rapidly switched between atomic and molecular ionization modes; both atomic and molecular spectra could be generated in the helium-supported plasma. In the switched configuration, the duty cycle is 50% for each mode. The ionization mode is selected by application of either a positive (molecular) or negative (atomic) potential to the sample introduction electrode, and the two kinds of spectra can be sequentially collected by changing the voltage and current between two preset values. Similar ion-optical voltage settings could be employed for both modes of operation, with the exception of the steering-plate potential, which had to be modulated between two different values (at the plasma switching frequency) to obtain the greatest atomic and molecular signal levels. The source is capable of generating mass spectra resembling those from an electron-impact source while operated in the molecular ionization mode (both static and dynamic). The best atomic detection limits (1—25 fg of analyte! second) were obtained when the plasma was operated in the static mode with single-channel gated ion counting. Atomic detection limits obtained with boxcar averager data collection were comparable for static and switched opera-tion of the source (1—30 pg/s). Ukewise, the molecular detection limits were similar for the static and switched modes and span the range of 7—140 pg/s (boxcar aver-agers). Precision was better than 7% RSI) under all conditions. The atomic and molecular chrornatographic peak heights were nearly unchanged over a range of modulation rates from 5 to 100 Hz. The elemental ratio (35Cl~/12&) for chloroform was also measured over a range of plasma modulation rates (5—90 Hz) and found to be randomly distributed about the sample mean. Several chlorinated hydrocarbons were introduced into the discharge and could be successfully differentiated (or speciated) on the basis of their aSCI±/12C± ratios.
机译:气相色谱仪已与直流气体采样辉光放电(GSGD)电离源耦合,用于卤代烃的质谱分析。连续放电包含在差动泵式电子计量器接口的第一真空级内。放电可以静态操作,也可以在原子和分子电离模式之间快速切换。氦支撑等离子体中可同时产生原子光谱和分子光谱。在开关配置中,每种模式的占空比为50%。通过将正(分子)或负(原子)电势施加到样品引入电极来选择电离模式,并且可以通过在两个预设值之间改变电压和电流来依次收集两种光谱。两种操作模式均可采用类似的离子光学电压设置,但方向盘电势除外,该方向盘电势必须在两个不同的值之间(在等离子体切换频率下)进行调制,以获得最大的原子和分子信号电平。在分子电离模式下(静态和动态)运行时,该离子源能够产生类似于电子撞击源的质谱。当等离子体以单通道门控离子计数在静态模式下运行时,可获得最佳原子检测限(1-25%fg分析物!秒)。通过Boxcar平均器数据收集获得的原子检测限对于源的静态和切换操作(1-30 pg / s)是可比的。顺便说一句,静态和切换模式的分子检测限相似,范围为7至140 pg / s(棚车平均)。在所有条件下,精度均优于7%RSI)。原子和分子色谱峰高在5至100 Hz的调制率范围内几乎没有变化。在一定范围的血浆调制速率(5-90 Hz)上也测量了氯仿的元素比(35Cl〜/ 12&),发现它在样品平均值周围随机分布。几种氯化碳氢化合物被引入到排放物中,并可以根据它们的aSCI±/ 12C±比率成功地区分(或指定)。

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