Reverse geometry: Difference between revisions
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{{ | {{Final | ||
|acronym= | |||
|def=[[Double-focusing mass spectrometer]] configuration in which the [[ion]] beam traverses the [[magnetic sector]] prior to the [[electric sector]]. | |||
|rel=[[forward geometry]] | |||
|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 ) | |||
}} | }} | ||
==Notes== | |||
The reverse geometry configuration is sometimes abbreviated "BE". | |||
[[Category:M/z Separation]] | [[Category:M/z Separation]] | ||
Latest revision as of 12:23, 8 January 2014
IUPAC RECOMMENDATIONS 2013 |
Reverse geometry |
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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".