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Does anyone do mass spectrometry with a magnetic sector to separate ions by mass and an array of detectors in a line to measure the ions? If not, why don't they?

Something like this this setup for measuring the spectrum of light?

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  • $\begingroup$ Yes, this is done in Medium Energy Ion Scattering, for example. $\endgroup$
    – Jon Custer
    Commented Apr 4, 2018 at 15:01
  • $\begingroup$ Probably not any more for mass spectrometry. Time of flight (TOF) methods are far better (both in mass resolution and signal to noise) as it is very easy to measure nanosecond time intervals. Also, only a single detector is needed and no expensive magnet. $\endgroup$
    – porphyrin
    Commented Apr 5, 2018 at 14:01
  • $\begingroup$ Triple quadrupole mass spectrometers sort of work this way when they are in "MRM" mode. But they only detect a single fragment ion from a single parent ion; they don't really monitor multiple ions with several detectors separated in space. (They can switch very rapidly from looking at one parent/fragment pair to looking at another one, though.) $\endgroup$
    – Curt F.
    Commented Apr 16, 2021 at 17:37
  • $\begingroup$ It's also worth noting Ron Heeren's work on imaging mass spectrometry. He has developed instrumentation with spatially resolved detectors for e.g. qTOFs. Those instruments have the feature of spatially separated (pixelated) detectors for ions, but rather than use that spatial separation to assess m/z, he and his group use the spatial separation to measure the spatial location of the origin of the ion, i.e. to do MS imaging. en.wikipedia.org/wiki/Ron_Heeren $\endgroup$
    – Curt F.
    Commented Apr 16, 2021 at 17:40

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Yes, this is called distance-of-flight mass spectrometry. It offers some advantages for large (e.g. biological) molecules and because of its high speed for identifying multiple targets, in chemical and biological warfare.

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Indeed mass spectrometers that disperse the ions in space according to there m/z do exist. The main question is how the detection is done: the detector needs to have a rather large surface compared to the detector in a standard mass spectrometer. In the early times of mass spectrometry, these were called "mass spectrographs", using a photographic plate as the detector. Standard detectors (multi-channel plates, conversion dynodes, electron multipliers) either are not well adapted to a large surface collection or are expensive to produce with large surfaces. Thus currently, only some specific instruments such as isotope ration mass spectrometers still rely on using several collectors and a magnetic sector, placed at an adequate position to measure simultaneously the various isotopes of a given element. This brings much better accuracies on the abundances.

Dispersion is space is not the only way to achieve simultaneous detection of several m/z values (thus achieving a non scanning mass spectrometer): dispersion in time or in frequency can also be a method to measure simultaneously the m/z of ions without scanning the m/z range. Time of flight mass spectrometers disperse the ions in time (the smallest m/z arriving before larger ones) and FT-MS instruments (Orbitrap or FT-ICR, when using, respectively, an electrostatic field or a magnetic field) use the dispersion in frequencies to separate ions and measure simultaneously the frequencies of the ions present through their image current. The limitation of these mass analysers is that although they do not technically scan the entire mass range (all m/z that are present are detected), they do work in a sequential manner: ions are only admitted in the dispersion region at precise times. If an ion storage region is added ahead of the mass analyser, even with a continuous ion source it is possible to store the ions until the next analysis event and lose very little ions.

Thus as other methods do exist which paralellize ion detection over the full m/z range, the mass spectrographs have mostly gone out of the market.

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