کد مقاله | کد نشریه | سال انتشار | مقاله انگلیسی | نسخه تمام متن |
---|---|---|---|---|
1192996 | 1492271 | 2013 | 11 صفحه PDF | دانلود رایگان |
![عکس صفحه اول مقاله: Variable field ion traps Variable field ion traps](/preview/png/1192996.png)
• We modify a cylindrical ion trap splitting each electrode into several parts.
• The split electrodes are excited by different multiples of a single RF voltage.
• Linear or desired nonlinear field can be obtained by proper choice of amplitudes.
• Increase in field linearity is obtained keeping the simplicity of the CIT.
• Capacitor terminations can generate all required voltages from a single source.
This paper presents a technique to vary the electric field within a cylindrical ion trap (CIT) mass spectrometer while it is in operation. In this technique, the electrodes of the CIT are split into number of mini-electrodes and different voltages are applied to these split-electrodes to achieve the desired field.In our study we have investigated two geometries of the split-electrode CIT. In the first, we retain the flat endcap electrodes of the CIT but split the ring electrode into five mini-rings. In the second configuration, we split the ring electrode of the CIT into three mini-rings and also divide the endcaps into two mini-discs. By applying different potentials to the mini-rings and mini-discs of these geometries we have shown that the field within the trap can be optimized to desired values. In our study, two different types of fields were targeted. In the first, potentials were adjusted to obtain a linear electric field and, in the second, a controlled higher order even multipole field was obtained by adjusting the potential.We have shown that the different potentials required can be derived from a single RF generator by connecting appropriate capacitor terminations to split electrodes. The field within the trap can be modified by changing the values of the external capacitors.
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Journal: International Journal of Mass Spectrometry - Volume 356, 15 December 2013, Pages 60–70