1997
DOI: 10.1016/s0168-1176(97)00087-6
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Efficient cationization by Cs+ adduct ion formation in a supersonic beam

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Cited by 3 publications
(4 citation statements)
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“…The protonated species is relatively more difficult to dissociate due to the need to break covalent bonds in the molecule (∼50−100 kcal/mol for a covalent bond) as opposed to losing the adduct for the M + Cs + ion complexes (∼12 kcal/ mol). 52 Overall, similar modes are observed between the two calculated spectra for [M + Cs + ] and [M + H + ], with some shifts in the position and intensity, possibly due to the lack of the delocalized charge in the neutral and the presence of the Cs + ion altering the dipole moment and its vibration-induced oscillations. The lowest-energy structure is the tautomer with N2 carrying the proton and both the carbonyl and the lone pair on N5 solvating the Cs + ion (Figure 2b, right).…”
Section: Resultsmentioning
confidence: 99%
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“…The protonated species is relatively more difficult to dissociate due to the need to break covalent bonds in the molecule (∼50−100 kcal/mol for a covalent bond) as opposed to losing the adduct for the M + Cs + ion complexes (∼12 kcal/ mol). 52 Overall, similar modes are observed between the two calculated spectra for [M + Cs + ] and [M + H + ], with some shifts in the position and intensity, possibly due to the lack of the delocalized charge in the neutral and the presence of the Cs + ion altering the dipole moment and its vibration-induced oscillations. The lowest-energy structure is the tautomer with N2 carrying the proton and both the carbonyl and the lone pair on N5 solvating the Cs + ion (Figure 2b, right).…”
Section: Resultsmentioning
confidence: 99%
“…The major difference between the two spectra is the absolute intensity of the spectral bands (even more striking if one takes into account that the M + Cs + spectrum has been measured with one pulse and the protonated is with two pulses). The protonated species is relatively more difficult to dissociate due to the need to break covalent bonds in the molecule (∼50–100 kcal/mol for a covalent bond) as opposed to losing the adduct for the M + Cs + ion complexes (∼12 kcal/mol) . Overall, similar modes are observed between the two calculated spectra for [M + Cs + ] and [M + H + ], with some shifts in the position and intensity, possibly due to the lack of the delocalized charge in the neutral and the presence of the Cs + ion altering the dipole moment and its vibration-induced oscillations.…”
Section: Resultsmentioning
confidence: 99%
“…The relative abundance of clusters is influenced by various parameters during their formation: the energy and focal width of the desorption laser, its peak intensity, the nozzle temperature, the time delay between desorption and cooling gas injection, the refreshing rate for the exposed molecular surface and more [29]. Also the detection parameters influence the observed cluster distribution: the ionization laser energy determines the probability for the absorption of a second photon by the already ionized complex.…”
Section: Resultsmentioning
confidence: 99%
“…charge control of biomolecules in the gas phase is relevant for molecular trapping, 7 , 8 optical 9 and photo-electron spectroscopy, 10 , 11 as well as for electron or femto-second X-ray diffraction. 12 , 13 Several methods for charge manipulation have been studied in the past, such as atomic collisions, 14 chemical reactions, 15 and low-energy electron attachment. 16 …”
Section: Introductionmentioning
confidence: 99%