Mattauch-Herzog geometry: Difference between revisions
From Mass Spec Terms
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{{DefName|An arrangement for a double-focusing mass spectrometer in which a deflection of ????????????????/(4 ???????????????????(2)) radians in a radial electrostatic field is followed by a magnetic deflection of ????????????????/2 radians.}} | {{DefName|An arrangement for a [[double-focusing mass spectrometer]] in which a deflection of ????????????????/(4 ???????????????????(2)) radians in a radial [[electrostatic field]] is followed by a [[magnetic deflection]] of ????????????????/2 radians.}} | ||
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== Related Terms == | == Related Terms == | ||
[[Double-focusing Mass Spectrometer]] | *[[Double-focusing Mass Spectrometer]] | ||
[[Forward Geometry]] | *[[Forward Geometry]] | ||
[[Reverse Geometry]] | *[[Reverse Geometry]] | ||
[[Electric Sector]] | *[[Electric Sector]] | ||
[[Magnetic Sector]] | *[[Magnetic Sector]] | ||
[[Category:M/z Separation]] | [[Category:M/z Separation]] | ||
Revision as of 17:28, 30 November 2005
| DRAFT DEFINITION |
| Mattauch-Herzog geometry |
|---|
| An arrangement for a double-focusing mass spectrometer in which a deflection of ????????????????/(4 ???????????????????(2)) radians in a radial electrostatic field is followed by a magnetic deflection of ????????????????/2 radians. |
| Considered between 2004 and 2006 but not included in the 2006 PAC submission |
| This is an unofficial draft definition presented for information and comment. |
Orange Book Entry
An arrangement for a double-focusing mass spectrograph in which a deflection of π/(4 √(2)) radians in a radial electrostatic field is followed by a magnetic deflection of π/2 radians.
