Phase locked fourier transform linear ion trap mass spectrometry
A linear ion trap and mass analyzer technology, applied in the field of systems used in Fourier transform mass spectrometers, can solve problems such as low average signal intensity, loss of ion micro-motion information, etc.
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example 1
[0104] Sciex sells 4000 on the market mass spectrometer (similar to Figure 9The mass spectrometer shown) was modified according to the present teachings. A waveform generator (Keysight 33520B waveform generator) was used to generate a mass analysis quadrupole (e.g. Figure 9 The clock signal of the driving radio frequency of the quadrupole device Q3). The waveform generator triggers at the beginning of the sweep function and adjusts the number of cycles so that the signal ends at the falling / reset portion of the sweep, which lasts approximately the last 100 microseconds of the sweep function. The second channel and sync output of the waveform generator are also set to generate the signal and delay with respect to the trigger ground. Specifically, ion excitation and data acquisition were triggered approximately 10.25 ms after the waveform generator trigger. In this way, RF drive, excitation and detection are all phase locked at the beginning of the mass analysis section. ...
example 2
[0109] Figure 12 Transmission-mode FT-LIT transients of reserpine with (gray trace) and without (black trace) phase locking are shown, Figure 13 The corresponding mass spectra are depicted. The same mass spectrometer as used in the previous example was used, except for the reduced kinetic energy of the ions in the mass-analyzing quadrupole setup, resulting in higher-resolution micromotion information. Similar to the previous example, when the drive RF, excitation, and detection signals are phase locked, the signal amplitude increases because the timing associated with ion preferential ejection is substantially the same from one scan to the next.
[0110] This data demonstrates that ion micromotions are visible in the phase-locked transient and further demonstrates that the amplitude of the mass signal corresponding to the phase-locked transient is larger than that of the non-phase-locked transient The amplitude of the corresponding mass signal.
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