By Michelle V. Buchanan
content material: ideas and contours of Fourier rework mass spectrometry / Michelle V. Buchanan and Melvin B. Comisarow --
New excitation and detection ideas in Fourier rework ion cyclotron resonance mass spectrometry / Alan G. Marshall, Tao-Chin Lin Wang, Ling Chen, and Tom L. Ricca --
difficulties of Fourier rework mass spectrometry : a path to tool advancements / Richard P. Grese, Don L. Rempel, and Michael L. Gross --
software of the dual-cell Fourier rework mass spectrometer / Robert B. Cody, Jr. and James A. Kinsinger --
Instrumentation and alertness examples in analytical Fourier rework mass spectrometry / Frank H. Laukien, M. Allemann, P. Bischofberger, P. Grossmann, Hp. Kellerhals, and P. Kofel --
Fourier rework mass spectrometry of huge (m/z>5,000) biomolecules / Curtiss D. Hanson, Mauro E. Castro, David H. Russell, Donald F. Hunt, and Jeffrey Shabanowitz --
Tandem Fourier remodel mass spectrometry of enormous molecules / Fred W. McLafferty, I. Jonathan Amster, Jorge J.P. Furlong, Joseph A. bathroom toilet, Bing H. Wang, and Evan R. Williams --
Analytical purposes of laser desorption-Fourier rework mass spectrometry for nonvolatile molecules / R.S. Brown and C.L. Wilkins --
Infrared multiphoton dissociation of laser-desorbed ions / Clifford H. Watson, Gökhan Baykut, and John R. Eyler --
Gas-phase photodissociation of transition steel ion complexes and clusters / Robert L. Hettich and Ben S. Freiser --
Fourier rework mass spectrometry stories of unfavorable ion methods / Michelle V. Buchanan and Marcus B. Wise.
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Extra info for Fourier Transform Mass Spectrometry. Evolution, Innovation, and Applications
Decreases i r a d i a l d i f f u s i o n w i l l occur; but the ion abundance increases shown i n Figure 5 are more unexpected. 2. Model: Ion losses from an FTMS c e l l can occur by mechanisms other than chemical reaction and r a d i a l d i f f u s i o n . Ions that have acquired s u f f i c i e n t k i n e t i c energy from fragmentation processes can overcome the potential b a r r i e r of the trapping f i e l d especially when low trapping voltages are used. Ion loss owing to fragmentation was demonstrated by Riggin, et a l .
2. M A R S H A L L E T A L . New Excitation and Detection Techniques 25 varies inversely with the duration of the rf pulse. 1MS), and thus an impractically high magnitude (>10,000 V/cm) would be needed (11). Therefore, the second (15) and virtually a l l subsequent FT/ICR experiments have been performed via frequency-sweep excitation, in which the time-domain rf waveform is swept linearly across the frequency bandwidth corresponding the the m/z-range of interest. Although successful in exciting ICR signals over a wide mass range at relatively low excitation magnitude (ca.
J . Chem. Phys. 1980, 73, 1581-1590. Marshall, A. -C. ; Ricca, T. L. Chem. Phys. Lett. 1984, 105, 233-236. Marshall, A. -C. ; Ricca, T. L. J . Amer. Chem. Soc. 1985, 107, 7893-7897. Comisarow, M. ; Marshall, A. G. Chem. Phys. Lett. 1974, 26, 489-490. ; ACS Symposium Series; American Chemical Society: Washington, DC, 1987. 2. M A R S H A L L E T A L . New Excitation and Detection Techniques 16. ZZ Ijames, C. ; Wilkins, C. L. Chem. Phys. Lett. 1984, 108, 58-62. 17. Marshall, A. -C. ; Ricca, T. L.
Fourier Transform Mass Spectrometry. Evolution, Innovation, and Applications by Michelle V. Buchanan