z-logo
Premium
Instrument‐independent database for collisionally activated dissociation in RF‐only quadrupoles. The case of C 2 H 3 O + and C 3 H   7 +
Author(s) -
Martinez Richard I.,
Ganguli B.
Publication year - 1989
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.1290031102
Subject(s) - chemistry , analytical chemistry (journal) , dissociation (chemistry) , mass spectrometry , ion , collision induced dissociation , tandem mass spectrometry , tandem , quadrupole , branching (polymer chemistry) , ethylene , atomic physics , physics , materials science , organic chemistry , chromatography , composite material , catalysis , biochemistry
Dynamically correct (i.e., instrument‐independent) branching ratios can be measured under single‐collision conditions in tandem mass spectrometers incorporating RF‐only quadrupole collision cells. The absolute branching ratios were measured as a function of the center‐of‐mass interaction energy E CM for the collisionally activated dissociation (CAD) of CH 3 CO + (m/z43) from several source compounds (ethanol, oxirane), and CH 3 CO‐X (where X = H, CH 3 , CH 3 CH 2 , CH 3 CO, CH 3 COCH 2 , and C 6 H 5 )). The energy dependences of the branching ratios for C 2 H 3 O + from CH 3 CO‐X source compounds are quite distinct from those observed for C 2 H 3 O + from ethanol or ethylene oxide, or for the C 3 H + 7 ions (also m / z 43) from n ‐pentane. Hence, one can use the CAD of m / z 43 to distinguish CH 3 CO‐X compounds from other source compounds, including sources of C 3 H 7 + ions. Therefore, the characteristic branching ratios of ionic substructures may provide for tandem mass spectrometry a „fingerprinting” capability analogous to the use of group frequencies in infrared spectroscopy.

This content is not available in your region!

Continue researching here.

Having issues? You can contact us here
Accelerating Research

Address

John Eccles House
Robert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom