Penning ion trap: Difference between revisions
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|acronym= | |||
|def=[[Ion]] trapping device using a static magnetic field and a static electric potential well. The magnetic field confines the ion motion to circular orbits around the magnetic force line direction, which aligns with the direction of the trap axis, whereas the electric potential well confines the ion motion axially. | |||
:Note: This device is used for the mass analyzer of [[Fourier transform-ion cyclotron resonance-mass spectrometers]]. | |||
|rel= | |||
|ref=K. P. Wanczek. Int. J. Mass Spectrom. Ion Processes 95, 1 (1989). (http://dx.doi.org/10.1016/0168-1176(89)83044-7 ) | |||
}} | |||
[[Category:Mass spectrometer type]] | |||
Latest revision as of 16:13, 6 August 2025
| IUPAC RECOMMENDATIONS 2013 |
| Penning ion trap |
|---|
Ion trapping device using a static magnetic field and a static electric potential well. The magnetic field confines the ion motion to circular orbits around the magnetic force line direction, which aligns with the direction of the trap axis, whereas the electric potential well confines the ion motion axially.
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| Related Term(s): |
| Reference(s):
K. P. Wanczek. Int. J. Mass Spectrom. Ion Processes 95, 1 (1989). (http://dx.doi.org/10.1016/0168-1176(89)83044-7 ) |
| From Definitions of Terms Relating to Mass Spectrometry (IUPAC Recommendations 2013); DOI: 10.1351/PAC-REC-06-04-06 © IUPAC 2013. |
