THE GEOMETRICAL FACTOR OF INFINITELY LONG CYLINDRICAL ICR CELLS FOR COLLISION ENERGY-RESOLVED MASS-SPECTROMETRY - APPEARANCE ENERGIES OF EI(2)(-INDUCED DISSOCIATION OF EI(3)(+CENTER-DOT) AND [EI(2)CENTER-DOT-LIGAND](+) COMPLEXES() (E=P, AS, SB, AND BI) FROM COLLISION)
Hl. Sievers et al., THE GEOMETRICAL FACTOR OF INFINITELY LONG CYLINDRICAL ICR CELLS FOR COLLISION ENERGY-RESOLVED MASS-SPECTROMETRY - APPEARANCE ENERGIES OF EI(2)(-INDUCED DISSOCIATION OF EI(3)(+CENTER-DOT) AND [EI(2)CENTER-DOT-LIGAND](+) COMPLEXES() (E=P, AS, SB, AND BI) FROM COLLISION), International journal of mass spectrometry and ion processes, 158, 1996, pp. 233-247
Citations number
62
Categorie Soggetti
Spectroscopy,"Physics, Atomic, Molecular & Chemical
The geometrical factor beta of infinitely long cylindrical ICR cells i
s determined to employ collision energy-resolved mass spectrometry (CE
RMS) with a FT-ICR spectrometer. In case of four identical infinitely
long cylindrical electrodes beta equals 0.90. A cylindrical ICR cell e
mulating infinitely long electrodes is used to study the energy-depend
ent collision-induced dissociation (CID) of EI(3)(+) radical cations a
nd [EI(2) . ligand](+) complexes with E = P, As, Sb, and Bi and ligand
s benzene, propene and acetone. In the low collision energy regime the
EI(3)(+) precursor ions decompose by loss of I-. and the [EI(2) . lig
and](+) exclusively by breaking the EI(2)(+)-ligand bond and formation
of EI(2)(+). Appearance energies A(EI(2)(+)) of EI(2)(+) generated fr
om EI(3)(+) are A(PI2+) = 1.88 ev, A(AsI2+) = 1.15 eV, A(SbI2+) = 1.22
eV, and A(BiI2+ = 0.78 eV. Fission of the EI(2)-ligand bond requires
collision energies ranging from 1.88 eV in case of [PI2 . acetone](+)
down to 0.86 eV if [BiI2 . benzene](+) is studied. Appearance energy m
easurements of well characterized dissociations indicate an accuracy b
etter than +/- 0.20 eV.