2010
DOI: 10.1016/j.ijms.2010.05.001
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An optimised compact electron impact ion storage source for a time-of-flight mass spectrometer

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Cited by 22 publications
(7 citation statements)
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“…The repetition frequency of the pulser can be adjusted (≤10 kHz; rise time, approximately 4.6 ns) for optimal measurement conditions. Note that the lower the pulse frequency, the more ions can be stored in the ion source . However, a longer storage time of the ions in the source region can also result in unwanted nonlinear effects, ie, detector saturation, sensitivities, or fractionation factors that depend on the gas amounts.…”
Section: Methodsmentioning
confidence: 99%
“…The repetition frequency of the pulser can be adjusted (≤10 kHz; rise time, approximately 4.6 ns) for optimal measurement conditions. Note that the lower the pulse frequency, the more ions can be stored in the ion source . However, a longer storage time of the ions in the source region can also result in unwanted nonlinear effects, ie, detector saturation, sensitivities, or fractionation factors that depend on the gas amounts.…”
Section: Methodsmentioning
confidence: 99%
“…In this work, the mesh has a pitch of 0.2 mm and the mesh wires have a circular cross-section, with a diameter of 0.0127 mm. While it has been known for some time that meshes can give rise to fringe effects and local field distortions [18][19][20][21][22][23][24], it is still rare to see the mesh region of an experimental set-up explicitly described in simulations. While the optical transmission of a mesh is often considered, it is otherwise usually treated as a featureless plane or ideal grid in simulations carried out using software packages such as SIMION.…”
Section: Simulationsmentioning
confidence: 99%
“…The helical electron path increases the neutral−electron interaction time to improve ionization efficiency and generates a weak space-charge potential well that stores ions (storage ion source), improving source sensitivity. 50 To extract the ions into the TOF analyzer, we apply two independent, fast, push/pull pulses (∼5 ns rise-time for 3 μs) to energize the pusher grid with a more positive voltage relative to the extractor grid and provide constant energy per charge acceleration. The ion packet is accelerated out of the ion source and a series of beam defining optics guides the ions into the mass analyzer.…”
Section: ■ Experimental Sectionmentioning
confidence: 99%