Mass-analyzed ion kinetic energy spectrometry: Difference between revisions
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{{DefName|In a [[reverse geometry]] [[sector mass spectrometer]], the measurement of the kinetic energies of the fragment ions formed in the region between the magnteic and electric sectors. A beam of [[precursor ion]s is isolated with a constant B value in the [[magnetic sector]] and the field E in the electric is scanned to determine the fragment ion masses. The width of the resulting peaks gives the kinetic energy released during fragmentation}} | {{DefName|In a [[reverse geometry]] [[sector mass spectrometer]], the measurement of the kinetic energies of the fragment ions formed in the region between the magnteic and electric sectors. A beam of [[precursor ion]s is isolated with a constant B value in the [[magnetic sector]] and the field E in the electric is scanned to determine the fragment ion masses. The width of the resulting peaks gives the kinetic energy released during fragmentation}} | ||
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Revision as of 00:27, 4 March 2005
{{DefName|In a reverse geometry sector mass spectrometer, the measurement of the kinetic energies of the fragment ions formed in the region between the magnteic and electric sectors. A beam of [[precursor ion]s is isolated with a constant B value in the magnetic sector and the field E in the electric is scanned to determine the fragment ion masses. The width of the resulting peaks gives the kinetic energy released during fragmentation}}
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See additional comments on the Mass-analyzed ion kinetic energy spectrometry discussion page (archive of discussion between 2004 and 2006) |
