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LTQ Orbitrap XL Hardware Manual

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<strong>Orbitrap</strong> Analyzer<br />

Measuring Principle<br />

Curved Linear Trap<br />

Functional Description<br />

<strong>Orbitrap</strong> Analyzer<br />

This section describes the basic principle of the <strong>Orbitrap</strong> mass<br />

analyzer. The heart of the system is an axially-symmetrical mass analyzer.<br />

It consists of a spindle-shape central electrode surrounded by a pair of<br />

bell-shaped outer electrodes. See Figure 1-10. The <strong>Orbitrap</strong> employs<br />

electric fields to capture and confine ions.<br />

Figure 1-10. Schematic view of the <strong>Orbitrap</strong> cell and example of a stable<br />

ion trajectory<br />

In the mass analyzer shown in Figure 1-10, stable ion trajectories rotate<br />

around an axial central electrode with harmonic oscillations along it.<br />

The frequency ω of these harmonic oscillations along the z-axis depends<br />

only on the ion mass-to-charge ratio m/q and the instrumental<br />

constant k:<br />

Thermo Fisher Scientific <strong>LTQ</strong> <strong>Orbitrap</strong> <strong>XL</strong> <strong>Hardware</strong> <strong>Manual</strong> 1-13<br />

w<br />

=<br />

q<br />

m<br />

--- × k<br />

Two split halves of the outer electrode of the <strong>Orbitrap</strong> detect the image<br />

current produced by the oscillating ions. By Fast Fourier Transformation<br />

(FFT) of the image current, the instrument obtains the frequencies of<br />

these axial oscillations and therefore the mass-to-charge ratios of the<br />

ions.<br />

On their way from the linear trap to the <strong>Orbitrap</strong>, ions move through<br />

the gas-free RF octapole (Oct 1) into the gas-filled curved linear trap<br />

(C-Trap). See Figure 1-11 on page 1-14. Ions in the C-Trap are returned<br />

by the trap electrode. Upon their passage, the ions loose enough kinetic<br />

energy to prevent them from leaving the C-Trap through the Gate. The

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