Sh. Guan et Ag. Marshall, STORED WAVE-FORM INVERSE FOURIER-TRANSFORM (SWIFT) ION EXCITATION IN TRAPPED-ION MASS SPECTOMETRY - THEORY AND APPLICATIONS, International journal of mass spectrometry and ion processes, 158, 1996, pp. 5-37
Citations number
78
Categorie Soggetti
Spectroscopy,"Physics, Atomic, Molecular & Chemical
Stored waveform excitation produced by inverse Fourier transformation
of a specified magnitude/phase excitation spectrum offers the most gen
eral and versatile means for broadband mass-selective excitation and e
jection in Penning (FT-ICR) and Paul (quadrupole) ion trap mass spectr
ometry. Since the last comprehensive review of SWIFT excitation in 198
7, the technique has been adopted, modified, and extended widely in bo
th the ICR and quadrupole ion trap communities. Here, we review the pr
inciples, variations, algorithms, hardware implementation, and some ap
plications of SWIFT for both ICR and quadrupole ion trap mass spectrom
etry. We show that the most desirable SWIFT waveform is that optimized
to reduce both the time-domain SWIFT maximum amplitude and the amplit
ude near the start and end of the SWIFT waveform. We examine the ''tru
e'' magnitude excitation spectrum, obtained by zero-filling and forwar
d Fourier transforming the SWIFT time-domain waveform, in order to eva
luate the trade-off between spectral magnitude uniformity and frequenc
y (mass) selectivity. Apodization of the SWIFT waveform is optimally c
onducted by smoothing the excitation magnitude spectrum prior to gener
ation of the SWIFT waveform by inverse FT. When (as for broadband ejec
tion in a quadrupole ion trap) it is important that ions be excited ne
ar-simultaneously over a wide mass range, the phase spectrum (before i
nverse FT to generate the SWIFT waveform) may be overmodulated or rand
omly modulated (''filtered noise field''), with the recognition that v
ery substantial non-uniformity in the ''true'' excitation magnitude sp
ectrum will result.