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Time-of-flight (TOF) mass spectrometer without pulses of any kind, with continuous ion introduction

机译:飞行时间(TOF)质谱仪,不带任何类型的脉冲,可连续引入离子

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摘要

A new concept for time-of flight (TOF) mass spectrometry is presented. Currently, TOF instruments use pulsed ion introduction with a 10 ns or so pulsed width, followed by a waiting period roughly 100 μs. Accordingly, the sample is sunder excitation in 10~(-1) part of the total measuring time, which limits the sensitivity of the method. Secondly, the ion bunch generated is strongly confined, which gives rise to space charge problems deteriorating the signal intensity and the mass resolution. The concept presented here uses a continuously operating ion source and a special dual modulation technique [Patent pending]. The expected advantages are higher sensitivity and minor space charge limitations. The space charge limitations are obviously easier if the charges are distributed uniformly in an ion beam rather than being confined in a bunch. Moreover, the necessary detection bandwidth is as low as some hundred Hz, which enables to operate the electrometer electronics with amplification as high as 10~(10) V/A. Because of the high signal level, it was possible to omit any electrostatic mirror configuration for bunching the ions. Rather a cylindrical energy filter was installed to remove the ions with undesired energies. The drift tube is roughly 2 m long. The measurement is controlled by a PC via a home made board. The data are collected and the fast Fourier transformation is performed by the software. The objective of the experimental setup is to demonstrate the operation of this novel measuring principle. The analytical capabilities in present stage are admittedly poor, however its potential improvement is far less limited by physics than in the case of the pulsed TOF techniques.
机译:提出了飞行时间(TOF)质谱的新概念。当前,TOF仪器使用脉冲宽度为10 ns左右的脉冲离子引入,然后等待大约100μs。因此,样品在总测量时间的10〜(-1)部分被激发激发,这限制了该方法的灵敏度。其次,所产生的离子束受到严格限制,从而引起空间电荷问题,从而使信号强度和质量分辨率恶化。此处介绍的概念使用连续运行的离子源和特殊的双调制技术[正在申请专利]。预期的优势是更高的灵敏度和较小的空间电荷限制。如果电荷均匀地分布在离子束中,而不是束缚在束中,则空间电荷限制显然会更容易。而且,必要的检测带宽低至几百Hz,这使得静电计电子设备的放大倍数高达10〜(10)V / A。由于信号电平高,因此可以省略任何静电镜配置来束聚离子。而是安装了圆柱形能量过滤器以除去具有不希望有的能量的离子。漂移管大约2 m长。测量是由PC通过自制板控制的。收集数据并通过软件执行快速傅里叶变换。实验装置的目的是演示这种新颖的测量原理的操作。公认的是,现阶段的分析能力较差,但是与脉冲TOF技术相比,其潜在的改进受到物理学的限制要小得多。

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