2015
DOI: 10.1016/j.ijms.2015.06.011
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Using controlled ion extraction to combine a ring electrode trap with a reflectron time-of-flight mass spectrometer

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Cited by 13 publications
(14 citation statements)
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“…Selected fractions of reactive gas (that is, methane), in the buffer gas lead to reactions of the trapped clusters under multicollision conditions. After a specified storage time, a controlled ejection transports charged clusters and reaction products out of the RET into a home-built reflectron time-of-flight mass spectrometer that determines the mass-to-charge ratio ( m / z ) and abundance of all species. By systematic variation of the storage time, the progression of the reaction is recorded.…”
Section: Experimental and Theoretical Methodsmentioning
confidence: 99%
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“…Selected fractions of reactive gas (that is, methane), in the buffer gas lead to reactions of the trapped clusters under multicollision conditions. After a specified storage time, a controlled ejection transports charged clusters and reaction products out of the RET into a home-built reflectron time-of-flight mass spectrometer that determines the mass-to-charge ratio ( m / z ) and abundance of all species. By systematic variation of the storage time, the progression of the reaction is recorded.…”
Section: Experimental and Theoretical Methodsmentioning
confidence: 99%
“…The fitting parameters obtained from the simulation are rate coefficients of pseudo-first order ( k (1) ) for each reaction step and normalization to the methane particle density [CH 4 ] or the product of methane and helium particle density [He] results in bimolecular k (2) or termolecular rate coefficients k (3) , respectively (see eq ). Due to differential pumping of the RET from the axial openings and injection of the buffer gas via a channel into the center of the trap, there is an unknown pressure gradient throughout, and the locally measured pressure deviates from the mean value in the RET . To remedy this finding, which usually leads to a rather large uncertainty of the absolute value for the rate coefficients, the obtained rate coefficient for [TaCH 2 ] + formation is compared to a literature reference, and the corresponding ratio is used as a correction factor for all experimentally determined rate coefficients (see section S1 in the Supporting Information).…”
Section: Experimental and Theoretical Methodsmentioning
confidence: 99%
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“…Clusters with small rotational and vibrational temperatures (of 5–120 and 50–325 K, respectively) are typically generated in similar ablation sources. The cluster beam is guided by various ion optics into a quadrupole mass filter (model 5221, Extrel), which selects ions of a single mass, while the remainder is suppressed. Generally, a size-selected cluster beam generated by a single shot of the ablation laser is collected (within ∼5 ms) and stored for a specified reaction time in a homebuilt ring-electrode ion trap. , When the clusters initially enter the ion trap, their excess kinetic energy is quickly dispersed via collisions with the buffer gas (He 6.0, Westfalen) and solely ions with a sufficiently low energy are successfully stored. A constant stream of buffer gas facilitates a total pressure of 0.77 Pa inside the trap, which causes approximately 100 collisions of the clusters with the buffer gas per millisecond.…”
Section: Methodsmentioning
confidence: 99%
“…"Digital", i.e. rectangularly shaped, RF potentials have recently received much attention [33,34,35,36,37,38,39], as they provide stronger transverse confinement and facilitate adaptation across a broad frequency band [11].…”
Section: Introductionmentioning
confidence: 99%