Abstract Extensive efforts to develop the theory of Fourier Transform Mass Spectrometry (FTMS) have led to an understanding of the qualitative aspects of the technique and to quantitative predictions which have been experimentally verified. At the same time, a number of theoretical assertions have not yet been quantitatively tested. In particular, further quantitative comparisons between theoretical and experimental peak shapes, including determinations of height, width, area, and center position could prove useful to further development of the FTMS technique. All of these peak shape parameters are affected by the number of charged particles present in the analyser cell during FTMS analysis. Quantitative comparisons of experimental values of these parameters with the predictions of theory presumes accurate knowledge of the number of charged particles present in the analyser cell during the observation of ion cyclotron decay signals.
[1]
T. E. Sharp,et al.
Trapped-ion motion in ion cyclotron resonance spectroscopy
,
1972
.
[2]
R. L. Hunter,et al.
Theory for broadband detection of ion cyclotron resonance signals
,
1980
.
[3]
A. Marshall,et al.
Resolution‐enhanced Fourier transform ion cyclotron resonance spectroscopy
,
1975
.
[4]
R. T. McIver.
A Trapped Ion Analyzer Cell for Ion Cyclotron Resonance Spectroscopy
,
1970
.
[5]
M. B. Comisarow.
Signal modeling for ion cyclotron resonance
,
1978
.
[6]
Robert L. White,et al.
Exact mass measurement by Fourier transform mass spectrometry
,
1980
.