Ion isolation apparatus used for ion trap mass spectrometer and isolation method
A technology for ion trap mass spectrometers and isolation devices, which is applied in the field of ion isolation devices for ion trap mass spectrometers, can solve the problems of band frequency component loss, affecting mass isolation performance, reducing device isolation resolution, etc., and achieves the goal of improving isolation resolution Effect
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Embodiment 1
[0074] The structure of a high-resolution ion isolation device is as follows image 3shown. The whole device contains three sets of transformer coils, wherein 303 is the primary coil of the first set of transformers, 304 is the secondary coil of the first set of transformers, and the input end of the secondary coil is connected to the original SWIFT signal (that is, the first signal occurs The signal output by the device), the output end is connected to the input end of the secondary coil of the second group of transformers, and 302 is a sine wave signal of a frequency value that needs to be coupled into the original SWIFT signal (that is, the signal output by the second signal generator) , 305 is a sine wave signal of another frequency value that needs to be coupled into the original SWIFT signal (that is, the signal output by the third signal generator), 306 is the primary coil of the second group of transformers, and 307 is the secondary of the second group of transformers ...
Embodiment 2
[0079] refer to Figure 4 Shown is the structure of another high-resolution ion isolation device. The difference between this device and Embodiment 1 is that the positions of the two signal generators are exchanged. Compared with Embodiment 1, the positions of SIN1 and SWIFT signals are exchanged. 403 is the primary coil of the first group of transformers, 404 is the secondary coil of the first group of transformers, the input end of the secondary coil is connected with a sine wave signal of a specific frequency value (ie the signal output by the first signal generator), The output end is connected to the input end of the secondary coil of the second group of signal generators, 402 is the original SWIFT signal that needs to be coupled in, and 401 is the signal output by the first signal generator (that is, a sine wave signal with a specific frequency value) , the subsequent connection methods are similar to those in Embodiment 1, and will not be repeated here. This device ca...
Embodiment 3
[0081] refer to Figure 5 Shown is the structure of another high-resolution ion isolation device. The difference between this device and Embodiment 1 is that two sets of transformers are added, and compared with Embodiment 1, it has a symmetrical structure. 509 is the primary coil of the newly added first group of transformers, both ends of the primary coil are grounded, 510 is the secondary coil of the newly added first group of transformers, the input end of the secondary coil is grounded, and 512 is the newly added second group of transformers The secondary coil, the input terminal of the secondary coil is connected to the output terminal of the secondary coil of the newly added first group of transformers, the output terminal of the secondary coil is connected to the secondary coil of the third transformer described in Embodiment 1 One input terminal (the input terminal described in Embodiment 1 is grounded), 511 is the primary coil of the newly added second group of trans...
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