Linked scan at constant B(1-(E/E0))1/2/E: Difference between revisions

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{{Def|Linked Scan at Constant B[1-(E/E<sub>0</sub>)]<sup>1/2</sup>/E  
{{Def|Linked Scan at Constant B[1-(E/E<sub>0</sub>)]<sup>1/2</sup>/E  
|A linked scan at constant B[1-(E/E<sub>0</sub>)]<sup>1/2</sup>/E is performed on a [[sector instrument]] that incorporates at least one [[electric sector]] plus one [[magnetic sector]] placed in either order. The [[accelerating voltage]] is fixed while scanning the magnetic field, B, and electric field, E, simultaneously, so as to maintain the quantity B[1-(E/E<sub>0</sub>)]<sup>1/2</sup>/E at a constant value. This [[linked scan]] records a [[constant neutral mass loss (or gain) spectrum]] of dissociation or other reactions occurring in a [[field free region]] (FFR) preceding the two sectors. E<sub>0</sub> is the electric field required to transmit the singly charged analog of the desired neutral fragment. The term "B[1-(E/E<sub>0</sub>)]1/2/E linked scan" is not recommended.
|A [[linked scan]] at constant B[1-(E/E<sub>0</sub>)]<sup>1/2</sup>/E is performed on a [[sector instrument]] that incorporates at least one [[electric sector]] plus one [[magnetic sector]] placed in either order. The [[accelerating voltage]] is fixed while scanning the magnetic field, B, and electric field, E, simultaneously, so as to maintain the quantity B[1-(E/E<sub>0</sub>)]<sup>1/2</sup>/E at a constant value. This [[linked scan]] records a [[constant neutral mass loss (or gain) spectrum]] of dissociation or other reactions occurring in a [[field free region]] (FFR) preceding the two sectors. E<sub>0</sub> is the electric field required to transmit the singly charged analog of the desired neutral fragment. The term "B[1-(E/E<sub>0</sub>)]1/2/E linked scan" is not recommended.
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Revision as of 12:28, 14 December 2005