Continuous dynode particle multiplier: Difference between revisions

Latest revision as of 11:50, 25 October 2013

Continuous dynode particle multiplier
IUPAC RECOMMENDATIONS 2013
continuous dynode particle multiplier channel electron multiplier Ion-to-electron detector in which the ion strikes the inner surface of a continuous tube device and induces the production of secondary electrons that, in turn, impinge on the inner surfaces of the device to produce more secondary electrons. This avalanche effect produces an increase in the final measured current pulse.
Related Term(s): discrete dynode particle multiplier
Reference(s): S. S. Brenner, J. T. McKinney. Rev. Sci. Instrum. 43, 1264 (1972). (http://dx.doi.org/10.1063/1.1685899 )
From Definitions of Terms Relating to Mass Spectrometry (IUPAC Recommendations 2013); DOI: 10.1351/PAC-REC-06-04-06 © IUPAC 2013.
Index of Recommended Terms

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-{{def2|
+{{Final
-An ion-to-electron detector in which the ion strikes the inner surface of the device and induces the production of secondary electrons that in turn impinge on the inner surfaces to produce more secondary electrons.  This avalanche effect produces an increase in signal in the final measured current pulse.
+|acronym=
+|def='''continuous dynode particle multiplier'''
+'''[[channel electron multiplier]]'''
+Ion-to-electron detector in which the [[ion]] strikes the inner surface of a continuous tube device and induces the production of secondary electrons that, in turn, impinge on the inner surfaces of the device to produce more secondary electrons. This avalanche effect produces an increase in the final measured current pulse.
+|rel=[[discrete dynode particle multiplier]]
+|ref=S. S. Brenner, J. T. McKinney. Rev. Sci. Instrum. 43, 1264 (1972). (http://dx.doi.org/10.1063/1.1685899 )
 }}