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Vacuum Technology Know How - Triumf

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Formula 4-2<br />

Stability parameter a<br />

Formula 4-3<br />

Stability parameter q<br />

Ideal quadrupole fields require rods that have a hyperbolic profile. In actual practice, however,<br />

round rods are used, with the rod radius being equal to 1.144 times the field radius r . 0<br />

An electrical quadrupole field is formed between the rods. Ions of varying mass are shot<br />

axially into the rod system at approximately equal energy and move through the rod system<br />

at uniform velocity. The applied quadrupole field deflects the ions in the X and Y directions,<br />

causing them to describe helical trajectories through the mass filter. To solve the movement<br />

equations, the dimensionless variables<br />

and<br />

www.pfeiffer-vacuum.net<br />

Ions created through<br />

electron bombardment<br />

in the ion source<br />

Ion Optics<br />

Cathode<br />

Formation<br />

Area<br />

Ions separated by the m / e<br />

ratio in the rod system<br />

Figure 4.4: Operating principle of a quadrupole mass spectrometer<br />

a =<br />

q =<br />

8 . e . U<br />

m . 2 r . � 0<br />

2<br />

4 . e . V<br />

m . 2<br />

r0 . � 2<br />

are introduced to obtain Mathieu‘s differential equations. Their solutions yield the stable area<br />

with oscillation amplitudes of less than r beneath the triangle formed by the two solubility<br />

0<br />

curves in Figure 4.5. The values a = 0.23699 and q = 0.706 apply for the apex of the triangle.<br />

p p<br />

All solutions outside result in increasing oscillation amplitudes and thus in neutralization of<br />

the ions on the rods of the quadrupole filter.<br />

Dividing the two equations by one another yields:<br />

a U<br />

= 2 .<br />

q V<br />

This is the pitch of the so-called load line of the mass filter.<br />

Ions detected in the<br />

ion detector<br />

Page 89<br />

<strong>Vacuum</strong><br />

<strong>Technology</strong>

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