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通过射频电场匀场消除傅里叶变换离子回旋共振质谱中的z喷射。

Elimination of z-ejection in Fourier transform ion cyclotron resonance mass spectrometry by radio frequency electric field shimming.

作者信息

Wang M D, Marshall A G

机构信息

Department of Chemistry, Ohio State University, Columbus 43210.

出版信息

Anal Chem. 1990 Mar 1;62(5):515-20. doi: 10.1021/ac00204a017.

Abstract

In Fourier transform ion cyclotron resonance (FT/ICR) mass spectrometry, coherent ion cyclotron orbital motion is produced by resonant radio frequency (rf) electric field excitation. However, because the excitation electrodes are of finite dimensions, the desired transverse (to the applied magnetic field) rf electric field is accompanied by an rf electric field component along the z- (magnetic field) direction, resulting in mass-dependent z-ejection and mass-dependent FT/ICR mass spectral peak relative magnitudes. Addition of several "guard wires" of voltage-divided rf amplitude allows the rf electric field to be "shimmed" to near-perfect uniformity. In this paper (see also the accompanying paper by Russell et al.), we introduce two types of rf-shimmed ion traps. In the first type, guard wires are placed only in front of the trapping electrodes. In the second type, guard wire rings are placed inside the detector and trapping electrodes. For either arrangement, simion simulations were used to adjust the rf voltages applied (by use of voltage dividers) to the guard wires or rings so as to produce an optimally uniform rf field within the trap. The virtual elimination of z-excitation is confirmed by plots of magnitude-mode relative peak height vs ICR orbital radius. Because the guard wires (or rings) tend to shield the ions from the trapping electrode potential, the shift in ICR frequency with trapping voltage is also reduced, but not as well as by a screened trap.(ABSTRACT TRUNCATED AT 250 WORDS)

摘要

在傅里叶变换离子回旋共振(FT/ICR)质谱中,相干离子回旋轨道运动是由共振射频(rf)电场激发产生的。然而,由于激发电极尺寸有限,所需的横向(相对于外加磁场)射频电场伴随着沿z轴(磁场)方向的射频电场分量,导致质量依赖的z轴喷射和质量依赖的FT/ICR质谱峰相对大小。添加几根分压射频幅度的“保护线”可使射频电场“匀场”至接近完美的均匀性。在本文中(另见Russell等人的附文),我们介绍了两种类型的射频匀场离子阱。在第一种类型中,保护线仅放置在捕获电极前方。在第二种类型中,保护线环放置在检测器和捕获电极内部。对于这两种布置,使用Simion模拟来调整通过分压器施加到保护线或环上的射频电压,以便在阱内产生最佳均匀的射频场。通过幅度模式相对峰高与ICR轨道半径的关系图证实了z轴激发的虚拟消除。由于保护线(或环)倾向于使离子免受捕获电极电位的影响,ICR频率随捕获电压的偏移也会减小,但不如屏蔽阱减小得那么好。(摘要截短于250字)

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