Measuring methods for ion cyclotron resonance mass spectrometers
View Patent ↗The invention relates to measuring methods and corresponding measuring cells for ion cyclotron resonance mass spectrometers (FTMS). The invention provides measuring methods with measuring cells, the ends of which each incorporate a large number of trapping electrodes, DC voltages of opposite polarities being applied across adjacent electrodes. For orbiting ions this builds up a repelling pseudopotential, which holds the ions in the measuring cell by reflection. This facilitates measurement of the image currents without the disturbing influence of RF voltages.
1. Method of operating an ion cyclotron resonance mass spectrometer with a measuring cell having two ends with trapping plates at both ends, wherein each trapping plate carries a plurality of trapping electrodes across which there are DC potentials of alternating polarity during a measurement of image currents.
2. Method of operating an ion cyclotron resonance mass spectrometer comprising the following steps:
(a) providing a measuring cell in the magnetic field of the mass spectrometer which measuring cell has two ends and incorporates both longitudinal excitation and detection electrodes as well as trapping plates at both ends, wherein each trapping plate carries a plurality of trapping electrodes,
(b) supplying the trapping electrodes of the trapping plates with potentials which repel ions and thus keep them in the measuring cell,
(c) filling the measuring cell with ions,
(d) exciting the ions to cyclotron motions by excitation pulses applied to the excitation electrodes,
(e) applying two DC potentials with opposite polarity to the trapping electrodes of the trapping plates, whereby DC potentials of different polarity are connected in turn to adjacent trapping electrodes,
(f) measuring the image currents generated by the orbiting ions in the detection electrodes and converting the measuring values in the usual way into specific masses.
3. Method according to claim 2 , wherein the trapping electrodes are lengthy and predominantly arranged in radial direction.
4. Method according to claim 2 , wherein the potentials applied in Step (b), which repel the ions, are DC potentials which are applied uniformly across all the trapping electrodes.
5. Method according to claim 2 , wherein the potentials applied in Step (b), which repel the ions, are pseudopotentials which are formed by an RF voltage the phases of which are connected in turn to adjacent trapping electrodes.
6. Method according to claim 2 , wherein a pure cyclotron motion without magnetron motion is produced by quadrupolar irradiation of a two-phase frequency mixture before the alternating DC potential in Step (e) is applied.
7. Measuring cell for an ion cyclotron resonance mass spectrometer the cell being located in a magnetic field, having two ends and comprising longitudinal excitation electrodes for exciting ions to a cyclotron motion in the magnetic field; detection electrodes, and trapping plates at both ends, wherein the trapping plates each carry a plurality of lengthy trapping electrodes which are predominantly arranged radially.
8. Measuring cell according to claim 7 , wherein it contains more than two longitudinal detection electrodes to measure the image currents.
9. Measuring cell according to claim 8 , wherein it has at least eight longitudinal electrodes, of which at least four are used for detection and at least two longitudinal electrodes positioned opposite each other to excite the ions to cyclotron motions.
10. Measuring cell according to claim 7 , wherein the trapping plates each have a central aperture through which the measuring cell is filled with ions.
11. Measuring cell according to claim 10 , wherein the central aperture is bridged with a grid.
12. Measuring cell according to claim 7 , wherein the trapping electrodes of the trapping plates are mounted on ceramic plates, on glass or on plastic boards.
13. Measuring cell according to claim 7 , wherein the trapping electrodes of the trapping plates are divided into fields which approximately represent the potential distribution as it is generated by the excitation electrodes in a central cross-section of the measuring cell, and these fields are fed with mixtures of DC voltages and stepwise attenuated excitation pulses in such a way that the electric excitation potential distributions in the measuring cell are as similar as possible in each cross-section through the measuring cell.
14. An ion cyclotron resonance mass spectrometer, incorporating a measuring cell according to claim 7 .
15. Ion cyclotron resonance mass spectrometer according to claim 14 , additionally incorporating an electron source for the generation of low-energy electrons.
16. Ion cyclotron resonance mass spectrometer according to claim 14 , additionally incorporating an infrared laser for a multiphoton dissociation.
17. Method for confining ions in a measuring cell of an ion cyclotron resonance mass spectrometer in an axial direction, the measuring cell being located in a magnetic field, having two ends and electrodes for exciting ions to cyclotron motion in the magnetic field and the method comprising:
generating spatially alternating DC potentials at both ends of the measuring cell in order to form reflecting pseudopotentials for ions excited to cyclotron motion.
18. Measuring cell for an ion cyclotron resonance mass spectrometer, the cell being located in a magnetic field and having two ends, longitudinal excitation electrodes for exciting ions to cyclotron motion in the magnetic field and detection electrodes, wherein a plurality of lengthy trapping electrodes are radially arranged at both ends of the measuring cell and wherein two DC voltages of opposite polarities are applied to adjacent trapping electrodes.