Collision quadrupole: Difference between revisions
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|acronym= | |||
|def=[[Transmission quadrupole]] to which an oscillating radio frequency potential is applied so as to focus a beam of [[ion]]s through a [[collision gas]] or [[buffer gas]] with no ''[[m/z]]'' separation other than low ''m/z'' cut-off. | |||
:Note: Higher-order multipoles can also be used in this manner. | |||
|rel=[[RF-only quadrupole]] | |||
|ref=S. A. McLuckey, G. L. Glish, R. G. Cooks. Int. J. Mass Spectrom. Ion Phys. 39, 219 (1981). (http://dx.doi.org/10.1016/0020-7381(81)80034-4 ) | |||
R. A. Yost, C. G. Enke. J. Am. Chem. Soc. 100, 2274 (1978). (http://dx.doi.org/10.1021/ja00475a072 ) | |||
}} | }} | ||
[[Category:Reactions]] | [[Category:Reactions]][[Category:Fragmentation]] |
Latest revision as of 11:07, 8 August 2025
IUPAC RECOMMENDATIONS 2013 |
Collision quadrupole |
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Transmission quadrupole to which an oscillating radio frequency potential is applied so as to focus a beam of ions through a collision gas or buffer gas with no m/z separation other than low m/z cut-off.
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Related Term(s): RF-only quadrupole |
Reference(s):
S. A. McLuckey, G. L. Glish, R. G. Cooks. Int. J. Mass Spectrom. Ion Phys. 39, 219 (1981). (http://dx.doi.org/10.1016/0020-7381(81)80034-4 )
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From Definitions of Terms Relating to Mass Spectrometry (IUPAC Recommendations 2013); DOI: 10.1351/PAC-REC-06-04-06 © IUPAC 2013. |