Continuous dynode particle multiplier: Difference between revisions
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{{ | {{Final | ||
|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 ) | |||
}} | }} | ||
Latest revision as of 11:50, 25 October 2013
| IUPAC RECOMMENDATIONS 2013 |
| Continuous dynode particle multiplier |
|---|
| continuous dynode particle 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. |
