A. I. Ivanov, A. A. Sysoev, A. N. Konenkov, N. V. Konenkov
{"title":"Modeling of a linear ion trap with driving rectangular waveforms","authors":"A. I. Ivanov, A. A. Sysoev, A. N. Konenkov, N. V. Konenkov","doi":"10.1002/jms.5030","DOIUrl":null,"url":null,"abstract":"<p>We consider the operation of a digital linear ion trap with resonant radial ejection. A sequence of rectangular voltage pulses with a dipole resonance signal is applied to the trap electrodes. The periodic waveform is piecewise constant, has zero mean, and is determined by an asymmetry parameter <span></span><math>\n <semantics>\n <mrow>\n <mi>d</mi>\n </mrow>\n <annotation>$$ d $$</annotation>\n </semantics></math>: one value is taken on interval <span></span><math>\n <semantics>\n <mrow>\n <mfenced>\n <mn>0</mn>\n <mi>dT</mi>\n </mfenced>\n </mrow>\n <annotation>$$ \\left(0, dT\\right) $$</annotation>\n </semantics></math> and another on <span></span><math>\n <semantics>\n <mrow>\n <mfenced>\n <mi>dT</mi>\n <mi>T</mi>\n </mfenced>\n </mrow>\n <annotation>$$ \\left( dT,T\\right) $$</annotation>\n </semantics></math>, where <span></span><math>\n <semantics>\n <mrow>\n <mi>T</mi>\n </mrow>\n <annotation>$$ T $$</annotation>\n </semantics></math> is the RF period. Ion mass scanning is performed by varying the asymmetry parameter <span></span><math>\n <semantics>\n <mrow>\n <mi>d</mi>\n </mrow>\n <annotation>$$ d $$</annotation>\n </semantics></math> and amplitude of the negative pulse part with time. The ion oscillation frequencies and acceptance of the linear trap are calculated. The dependence of the ion mass to charge ratio <span></span><math>\n <semantics>\n <mrow>\n <mi>m</mi>\n <mo>/</mo>\n <mi>z</mi>\n </mrow>\n <annotation>$$ m/z $$</annotation>\n </semantics></math> on the parameter <span></span><math>\n <semantics>\n <mrow>\n <mi>d</mi>\n </mrow>\n <annotation>$$ d $$</annotation>\n </semantics></math> is <span></span><math>\n <semantics>\n <mrow>\n <mi>m</mi>\n <mo>/</mo>\n <mi>z</mi>\n <mo>~</mo>\n <msup>\n <mi>d</mi>\n <mn>2</mn>\n </msup>\n </mrow>\n <annotation>$$ m/z\\sim {d}^2 $$</annotation>\n </semantics></math>. The maximum value is about <span></span><math>\n <semantics>\n <mrow>\n <mi>m</mi>\n <mo>/</mo>\n <mi>z</mi>\n <mo>=</mo>\n <mn>30</mn>\n </mrow>\n <annotation>$$ m/z=30 $$</annotation>\n </semantics></math> kDa for typical parameters of the linear trap: frequency 0.5 MHz, rod radius 4 mm, and negative pulse amplitude 1 kV. The dipolar excitation frequency is 0.125 MHz at which the LIT acceptance is maximal.</p>","PeriodicalId":16178,"journal":{"name":"Journal of Mass Spectrometry","volume":null,"pages":null},"PeriodicalIF":1.9000,"publicationDate":"2024-05-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Mass Spectrometry","FirstCategoryId":"92","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1002/jms.5030","RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"BIOCHEMICAL RESEARCH METHODS","Score":null,"Total":0}
引用次数: 0
Abstract
We consider the operation of a digital linear ion trap with resonant radial ejection. A sequence of rectangular voltage pulses with a dipole resonance signal is applied to the trap electrodes. The periodic waveform is piecewise constant, has zero mean, and is determined by an asymmetry parameter : one value is taken on interval and another on , where is the RF period. Ion mass scanning is performed by varying the asymmetry parameter and amplitude of the negative pulse part with time. The ion oscillation frequencies and acceptance of the linear trap are calculated. The dependence of the ion mass to charge ratio on the parameter is . The maximum value is about kDa for typical parameters of the linear trap: frequency 0.5 MHz, rod radius 4 mm, and negative pulse amplitude 1 kV. The dipolar excitation frequency is 0.125 MHz at which the LIT acceptance is maximal.
我们考虑了带有共振径向喷射的数字线性离子阱的运行。在阱电极上施加一串带有偶极共振信号的矩形电压脉冲。周期波形是片断常数,均值为零,由不对称参数 d $$ d $$ 决定:一个值取于间隔 0 dT $$ \left(0, dT\right) $$,另一个取于 dT T $$ \left( dT,T\right) $$,其中 T $$ T $$ 是射频周期。离子质量扫描是通过随时间改变不对称参数 d$ d$ 和负脉冲部分的振幅来实现的。计算了离子振荡频率和线性阱的接受度。离子质量与电荷比 m / z $ m/z $ 与参数 d $ d $ 的关系为 m / z ~ d 2 $ $ m/z\sim {d}^2 $ $。线性阱的典型参数为:频率 0.5 MHz,杆半径 4 mm,负脉冲振幅 1 kV,最大值约为 m / z = 30 $$ m/z=30 $$ kDa。双极激励频率为 0.125 MHz,在此频率下,LIT 的接受度达到最大。
期刊介绍:
The Journal of Mass Spectrometry publishes papers on a broad range of topics of interest to scientists working in both fundamental and applied areas involving the study of gaseous ions.
The aim of JMS is to serve the scientific community with information provided and arranged to help senior investigators to better stay abreast of new discoveries and studies in their own field, to make them aware of events and developments in associated fields, and to provide students and newcomers the basic tools with which to learn fundamental and applied aspects of mass spectrometry.