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Artifacts in four‐sector tandem mass spectrometry
Author(s) -
Falick A. M.,
Medzihradszky Katalin F.,
Walls F. C.
Publication year - 1990
Publication title -
rapid communications in mass spectrometry
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.528
H-Index - 136
eISSN - 1097-0231
pISSN - 0951-4198
DOI - 10.1002/rcm.1290040905
Subject(s) - chemistry , tandem mass spectrometry , tandem , mass spectrometry , chromatography , aerospace engineering , engineering
Abstract Several types of artifacts were shown to be present in 4‐sector tandem collision‐induced dissociation (CID) mass spectra. In CID spectra of protonated peptides produced by liquid secondary‐ion mass spectrometry (LSIMS), peaks corresponding to successive losses of matrix molecules from the precursor ion were observed. In addition, peaks corresponding to MH + ions of smaller peptides that were also present in the sample/matrix mixture in greater abundance than the selected precursor ion were observed. Both of these types of artifact peaks were shown to originate from the ‘peak‐at‐every‐mass’ chemical noise at the same nominal mass as that selected by the first 2 sectors (MS1). These noise ions are transmitted through to the collision cell and produce fragments that are analysed and detected in the next 2 sectors (MS2). A second, unrelated, kind of artifact was found to be due to decompositions in the second field‐free region of MS2 in an EBEB geometry machine. These artifacts, which are detectable over only a very limited mass range when using a conventional single‐point detector, can be present over a much greater mass range when an array detector is used and when the collision cell is floated above ground potential. A clear understanding of the origins of all peaks in a CID spectrum is important in order to have a firm foundation for interpretation, manual or computer‐aided, of the spectra of unknown compounds.