Matches in SemOpenAlex for { <https://semopenalex.org/work/W2024998519> ?p ?o ?g. }
- W2024998519 endingPage "259" @default.
- W2024998519 startingPage "243" @default.
- W2024998519 abstract "Abstract The Fourier transform operating mode applied to a quadrupole ion trap results in an axial secular frequency spectrum of the simultaneously confined ions. During confinement, the ion trajectory must be as pure as possible, giving only one frequency peak for an ion population with the same mass-to-charge ratio. The simulation work presented here examines the harmful influences of the spatial defects (here, mainly electrode truncation) of the ion trap leading to a non-linear confinement field. The observed harmful influences on the ion’s axial trajectory and its corresponding frequency spectrum is studied based on a case of a single confined ion. Secular frequency of the motion is calculated as a function of the maximum amplitude of the axial and radial trajectories. In the operating mode used in this work, amplitude and frequency of the confinement potential remain constant. As a result, mass analysis is impaired on mass range sustaining the influence of a resonance line. Secular frequency peak amplitude is modified, coupling peaks gain amplitude and ions could be lost. Defective mass ranges have been estimated for a trap truncated at 2 r 0 and 3 r 0 and different maximum amplitudes of the ion motion. The Fourier transform operating mode requires an external ion source and a large amplitude of the ion motion during confinement. Consequently, even far from a resonance line, ions experience non-linearity effects during confinement due to the maximum amplitude dispersion of the ion cloud during confinement connected to that at the beginning of the confinement. For a same mass-to-charge ratio ion cloud, spectrum is constituted by the superimposition of close-frequency peaks. As a result, mass resolution is limited by peak splitting. In addition to the case of a single confined ion, the operating mode is simulated based on an ion cloud’s with initial positions and velocities drawn from Gaussian laws. The mass resolution limit is reported as a function of the initial-condition broadening of the ion cloud. For example, simulation results give a mass resolution of 3250 at the mass 130 u for an operating point β z = 0.74 and with an ion cloud having, at the beginning of the confinement for the axial direction, 4 mm for the mean position and 2 mm for the standard deviation." @default.
- W2024998519 created "2016-06-24" @default.
- W2024998519 creator A5011417544 @default.
- W2024998519 creator A5028601819 @default.
- W2024998519 creator A5039128980 @default.
- W2024998519 date "2007-06-01" @default.
- W2024998519 modified "2023-10-18" @default.
- W2024998519 title "Harmful influences of confinement field non-linearities in mass identifying for a Fourier transform quadrupole ion trap mass spectrometer" @default.
- W2024998519 cites W1601316042 @default.
- W2024998519 cites W1966583794 @default.
- W2024998519 cites W1969539814 @default.
- W2024998519 cites W1981777685 @default.
- W2024998519 cites W1994993664 @default.
- W2024998519 cites W2010561289 @default.
- W2024998519 cites W2016766664 @default.
- W2024998519 cites W2026718477 @default.
- W2024998519 cites W2027725229 @default.
- W2024998519 cites W2036994328 @default.
- W2024998519 cites W2044354316 @default.
- W2024998519 cites W2047745555 @default.
- W2024998519 cites W2051759258 @default.
- W2024998519 cites W2059567693 @default.
- W2024998519 cites W2061520355 @default.
- W2024998519 cites W2063721312 @default.
- W2024998519 cites W2073369167 @default.
- W2024998519 cites W2073781313 @default.
- W2024998519 cites W2077437671 @default.
- W2024998519 cites W2084428717 @default.
- W2024998519 cites W2085505728 @default.
- W2024998519 cites W2087238751 @default.
- W2024998519 cites W2091748656 @default.
- W2024998519 cites W2093528733 @default.
- W2024998519 cites W2095152786 @default.
- W2024998519 cites W2130314097 @default.
- W2024998519 cites W2137050079 @default.
- W2024998519 cites W2144198290 @default.
- W2024998519 cites W2534285183 @default.
- W2024998519 cites W319980450 @default.
- W2024998519 cites W3829115 @default.
- W2024998519 doi "https://doi.org/10.1016/j.ijms.2007.02.048" @default.
- W2024998519 hasPublicationYear "2007" @default.
- W2024998519 type Work @default.
- W2024998519 sameAs 2024998519 @default.
- W2024998519 citedByCount "5" @default.
- W2024998519 countsByYear W20249985192016 @default.
- W2024998519 crossrefType "journal-article" @default.
- W2024998519 hasAuthorship W2024998519A5011417544 @default.
- W2024998519 hasAuthorship W2024998519A5028601819 @default.
- W2024998519 hasAuthorship W2024998519A5039128980 @default.
- W2024998519 hasConcept C102519508 @default.
- W2024998519 hasConcept C103232671 @default.
- W2024998519 hasConcept C106289968 @default.
- W2024998519 hasConcept C113196181 @default.
- W2024998519 hasConcept C121099081 @default.
- W2024998519 hasConcept C121332964 @default.
- W2024998519 hasConcept C145148216 @default.
- W2024998519 hasConcept C153294291 @default.
- W2024998519 hasConcept C162356407 @default.
- W2024998519 hasConcept C170552419 @default.
- W2024998519 hasConcept C172493649 @default.
- W2024998519 hasConcept C178790620 @default.
- W2024998519 hasConcept C184779094 @default.
- W2024998519 hasConcept C185592680 @default.
- W2024998519 hasConcept C202444582 @default.
- W2024998519 hasConcept C27826464 @default.
- W2024998519 hasConcept C31827203 @default.
- W2024998519 hasConcept C33923547 @default.
- W2024998519 hasConcept C39984356 @default.
- W2024998519 hasConcept C43617362 @default.
- W2024998519 hasConcept C62520636 @default.
- W2024998519 hasConcept C71043704 @default.
- W2024998519 hasConcept C710854 @default.
- W2024998519 hasConcept C9652623 @default.
- W2024998519 hasConceptScore W2024998519C102519508 @default.
- W2024998519 hasConceptScore W2024998519C103232671 @default.
- W2024998519 hasConceptScore W2024998519C106289968 @default.
- W2024998519 hasConceptScore W2024998519C113196181 @default.
- W2024998519 hasConceptScore W2024998519C121099081 @default.
- W2024998519 hasConceptScore W2024998519C121332964 @default.
- W2024998519 hasConceptScore W2024998519C145148216 @default.
- W2024998519 hasConceptScore W2024998519C153294291 @default.
- W2024998519 hasConceptScore W2024998519C162356407 @default.
- W2024998519 hasConceptScore W2024998519C170552419 @default.
- W2024998519 hasConceptScore W2024998519C172493649 @default.
- W2024998519 hasConceptScore W2024998519C178790620 @default.
- W2024998519 hasConceptScore W2024998519C184779094 @default.
- W2024998519 hasConceptScore W2024998519C185592680 @default.
- W2024998519 hasConceptScore W2024998519C202444582 @default.
- W2024998519 hasConceptScore W2024998519C27826464 @default.
- W2024998519 hasConceptScore W2024998519C31827203 @default.
- W2024998519 hasConceptScore W2024998519C33923547 @default.
- W2024998519 hasConceptScore W2024998519C39984356 @default.
- W2024998519 hasConceptScore W2024998519C43617362 @default.
- W2024998519 hasConceptScore W2024998519C62520636 @default.
- W2024998519 hasConceptScore W2024998519C71043704 @default.
- W2024998519 hasConceptScore W2024998519C710854 @default.
- W2024998519 hasConceptScore W2024998519C9652623 @default.
- W2024998519 hasIssue "2-3" @default.