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Mass-Analyzing Linear Quadrupole Ion Trap with Axial Ejection

2 Mass-Analyzing Linear Quadrupole Ion Trap with Axial Ejection [Pg.158]

As with the linear quadrupole before, the potential (x,y.z,t) in the two-dimensional quadrupole field of the LIT is expressed by a DC voltage U and an RF drive voltage V with the frequency Q. ([108,118] and Chap. 5 in [ 119]) [Pg.159]

In practice, there is no DC conponent, and thus, only the Mathieu parameter q is required, which is obtained by solving the above equations [Pg.159]

The voltage V is the zero-to-peak anplitude of the RF drive voltage. For an ion inside the quadrupole field the fundamental resonant frequency con is obtained as [Pg.159]

Note The QqLIT setup combines into one single instrument different kinds of mass analyzers, a scanning linear quadrupole, and a scanning linear quadrupole ion trap all connected via an RF-only ion guide. Instmments combining different types of mass analyzers are termed hybrid instruments. Most modem mass spectrometers are assembled from different elements to achieve optimum capabilities in the sense of creating instmments uniting the best of two worlds [114]. An overview of hybrids is presented at the end of the analyzer section. [Pg.160]




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Analyzer quadrupole

Axial ejection

Ejection

Ion trap

Ion trap mass analyzer

Ion trapping

Ion-quadrupole

Linear analyzers

Linear ion traps

Linear quadrupole analyzer

Linear quadrupole ion trap

Linear trap quadrupole mass

Linear-trap quadrupole

Mass analyzer

Mass analyzer quadrupole

Mass analyzers ion-trapping

Mass analyzers quadrupole ion trap

Mass quadrupole

Mass trapping

Quadrupole ion trap

Quadrupole ion trap analyzer

Quadrupole linear

Quadrupole mass analyze

Quadrupole trap

Trapped ions

Trapping analyzers

Trapping quadrupole

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