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用于气体离子源的热离子电子束电流和加速电压控制器

Thermionic Electron Beam Current and Accelerating Voltage Controller for Gas Ion Sources.

作者信息

Sikora Jarosław, Kania Bartosz, Mroczka Janusz

机构信息

Department of Automatics and Metrology, Lublin University of Technology, 20-618 Lublin, Poland.

Department of Electronic and Photonic Metrology, Wroclaw University of Science and Technology, 50-370 Wroclaw, Poland.

出版信息

Sensors (Basel). 2021 Apr 20;21(8):2878. doi: 10.3390/s21082878.

DOI:10.3390/s21082878
PMID:33923949
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8073282/
Abstract

Thermionic emission sources are key components of electron impact gas ion sources used in measuring instruments, such as mass spectrometers, ionization gauges, and apparatus for ionization cross-section measurements. The repeatability of the measurements taken with such instruments depends on the stability of the ion current, which is a function, among other things, of the electron beam current and electron accelerating voltage. In this paper, a laboratory thermionic electron beam current and accelerating voltage controller is presented, based on digital algorithm implementation. The average value of the percentage standard deviation of the emission current is 0.021%, and the maximum electron accelerating voltage change versus the emission current is smaller than 0.011% in the full operating range of the emission current. Its application as a trap current or emission current-regulated ion source power supply could be useful in many measuring instruments, such as in microelectromechanical system (MEMS) mass spectrometers as universal gas sensors, where a stable emission current and electron energy are needed.

摘要

热电子发射源是用于测量仪器(如质谱仪、电离规和电离截面测量装置)的电子碰撞气体离子源的关键部件。使用此类仪器进行测量的重复性取决于离子电流的稳定性,而离子电流稳定性除其他因素外,还与电子束电流和电子加速电压有关。本文基于数字算法实现,介绍了一种实验室热电子束电流和加速电压控制器。发射电流百分比标准偏差的平均值为0.021%,在发射电流的整个工作范围内,电子加速电压相对于发射电流的最大变化小于0.011%。它作为陷阱电流或发射电流调节的离子源电源,可应用于许多测量仪器,如作为通用气体传感器的微机电系统(MEMS)质谱仪,这类仪器需要稳定的发射电流和电子能量。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ccd5/8073282/945ac35cd20b/sensors-21-02878-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ccd5/8073282/46857cb4af59/sensors-21-02878-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ccd5/8073282/3e19cefcc9c1/sensors-21-02878-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ccd5/8073282/258a09ed29ce/sensors-21-02878-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ccd5/8073282/1e4a6dece022/sensors-21-02878-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ccd5/8073282/09565597e528/sensors-21-02878-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ccd5/8073282/24f8e492690a/sensors-21-02878-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ccd5/8073282/945ac35cd20b/sensors-21-02878-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ccd5/8073282/46857cb4af59/sensors-21-02878-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ccd5/8073282/3e19cefcc9c1/sensors-21-02878-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ccd5/8073282/258a09ed29ce/sensors-21-02878-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ccd5/8073282/1e4a6dece022/sensors-21-02878-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ccd5/8073282/09565597e528/sensors-21-02878-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ccd5/8073282/24f8e492690a/sensors-21-02878-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ccd5/8073282/945ac35cd20b/sensors-21-02878-g007.jpg

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本文引用的文献

1
Absolute electron total ionization cross-sections: molecular analogues of DNA and RNA nucleobase and sugar constituents.绝对电子总电离截面:DNA和RNA核碱基及糖成分的分子类似物。
Phys Chem Chem Phys. 2014 Jun 14;16(22):10743-52. doi: 10.1039/c4cp00490f.
2
Programmable smart electron emission controller for hot filament.用于热灯丝的可编程智能电子发射控制器。
Rev Sci Instrum. 2011 Feb;82(2):025111. doi: 10.1063/1.3555340.
3
A novel circuit for independent control of electron energy and emission current of a hot cathode electron source.
一种用于独立控制热阴极电子源电子能量和发射电流的新型电路。
Rapid Commun Mass Spectrom. 2011 Mar 30;25(6):689-92. doi: 10.1002/rcm.4915.
4
The Brookhaven National Laboratory electron beam ion source for RHIC.用于相对论重离子对撞机(RHIC)的布鲁克海文国家实验室电子束离子源。
Rev Sci Instrum. 2010 Feb;81(2):02A509. doi: 10.1063/1.3292937.