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Pfeiffer <strong>Vacuum</strong><br />
Page 76<br />
<strong>Vacuum</strong> <strong>Technology</strong><br />
Cold cathode ionization vacuum gauges<br />
Cold cathode ionization vacuum gauges essentially consist of only two electrodes, a cathode<br />
and an anode, between which a high voltage is applied via a series resistor. Negatively charged<br />
electrons leave the cathode because of the high voltage, moving at high velocity from the<br />
cathode toward the anode. As they travel this path, they ionize neutral gas molecules, which<br />
ignites a gas discharge. The measured gas discharge current (Figure 3.5) is a parameter for<br />
pressure. <strong>How</strong>ever only few molecules are ionized with straight electron trajectories, which<br />
results in lower sensitivity and interruption of the gas discharge at approximately 1 mbar.<br />
A design that avoids this disadvantage is the inverted magnetron after Hobsen and Redhead.<br />
A metal pin (anode) is surrounded by a rotationally symmetrical measurement chamber<br />
(cathode) (Figure 3.5). An axially magnetized, cylindrical, permanent-magnet ring is placed on<br />
the exterior of the measurement chamber to generate a magnetic field within the chamber.<br />
3 kV<br />
mbar<br />
Figure 3.5: Design of an inverted magnetron<br />
The electrons travel through the magnetic field on spiral trajectories (Figure 3.6). The electron<br />
paths extended in this manner increase the probability of collisions with the gas molecules<br />
and ensure that sufficient ions are generated to maintain the gas discharge, even at pressures<br />
of less than 1 mbar. The pressure reading will depend upon the type of gas in question<br />
due to the different ionization probabilities of the various gases. For example, a lower<br />
pressure will be indicated for helium than for air.<br />
Cold cathode vacuum gauges can be easily contaminated under the following conditions:<br />
If the device is activated at pressures p of more than 10 - 1 mbar<br />
Argon is often used for applications in sputtering systems. This results in sputtering of<br />
the cathode, as well, which can cause short circuits and thus failures of the gauges<br />
Gases are also gettered on the surfaces of the cathode. This produces a pumping effect<br />
that will falsify the measurement signal.<br />
N<br />
S<br />
R<br />
Cathode Anode<br />
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