Reverse geometry: Difference between revisions
From Mass Spec Terms
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|ref=M. J. Farncombe, R. S. Mason, K. R. Jennings, J. Scrivens. Int J. Mass Spectrom. Ion Phys. 44, 91 (1982). (http://dx.doi.org/10.1016/0020-7381(82)80041-7 ) | |ref=M. J. Farncombe, R. S. Mason, K. R. Jennings, J. Scrivens. Int J. Mass Spectrom. Ion Phys. 44, 91 (1982). (http://dx.doi.org/10.1016/0020-7381(82)80041-7 ) | ||
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==Notes== | |||
The reverse geometry configuration is sometimes abbreviated "BE". | |||
[[Category:M/z Separation]] | [[Category:M/z Separation]] | ||
Revision as of 12:23, 8 January 2014
| IUPAC RECOMMENDATIONS 2013 |
| Reverse geometry |
|---|
| Double-focusing mass spectrometer configuration in which the ion beam traverses the magnetic sector prior to the electric sector. |
| Related Term(s): forward geometry |
| Reference(s):
M. J. Farncombe, R. S. Mason, K. R. Jennings, J. Scrivens. Int J. Mass Spectrom. Ion Phys. 44, 91 (1982). (http://dx.doi.org/10.1016/0020-7381(82)80041-7 ) |
| From Definitions of Terms Relating to Mass Spectrometry (IUPAC Recommendations 2013); DOI: 10.1351/PAC-REC-06-04-06 © IUPAC 2013. |
Notes
The reverse geometry configuration is sometimes abbreviated "BE".
