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Multipactor in Low Pressure Gas and in ... - of Richard Udiljak

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s<strong>of</strong>tware <strong>and</strong> the time evolution <strong>of</strong> the electron density can be studied.<br />

The probe does not have to be located <strong>in</strong>side or close to the area where<br />

the discharge will take place. Even though it is advantageous for higher<br />

sensitivity to have the probe po<strong>in</strong>t<strong>in</strong>g at the critical gap it is also reliable<br />

when located outside the device under test <strong>and</strong> thus it can be used<br />

for waveguides <strong>and</strong> coaxial transmission l<strong>in</strong>es. It is not completely clear<br />

from the paper, however, how the electrons escape from a completely<br />

conf<strong>in</strong>ed device like a typical waveguide or coaxial cable <strong>and</strong> one will<br />

have to assume that there must be some small open<strong>in</strong>g somewhere <strong>in</strong><br />

the system, where electrons can leak out.<br />

Furthermore, the method can be used to quantitatively measure the<br />

amount <strong>of</strong> generated electrons. however, this requires some k<strong>in</strong>d <strong>of</strong> calibration<br />

<strong>of</strong> each test setup <strong>and</strong> that may prove to be problematic. When<br />

used <strong>in</strong> this way, the method can no longer be viewed as a global method,<br />

which can detect a multipactor event anywhere <strong>in</strong> the system, <strong>in</strong>stead it<br />

has become a local method. Among the ma<strong>in</strong> advantages <strong>of</strong> the method<br />

is the low cost <strong>in</strong>volved, s<strong>in</strong>ce no expensive microwave <strong>in</strong>struments are<br />

needed.<br />

Residual mass<br />

A very slow global method <strong>of</strong> detection is to detect the gas molecules,<br />

which are outgassed from the device walls due to the electron bombardment<br />

dur<strong>in</strong>g a multipactor event. The gas molecules consist <strong>of</strong> residuals<br />

<strong>of</strong> water, air <strong>and</strong> contam<strong>in</strong>ants, <strong>and</strong> us<strong>in</strong>g a mass spectrometer,<br />

the different molecules can be identified. It has been noted [31] that a<br />

detectable <strong>in</strong>crease <strong>in</strong> the water spectrum can be seen dur<strong>in</strong>g a multipactor<br />

discharge. The major drawback <strong>of</strong> this method <strong>of</strong> detection is<br />

its <strong>in</strong>ability to detect fast multipactor transients (not enough molecules<br />

are released from the walls) <strong>and</strong> thus it is not a suitable method for<br />

multicarrier multipactor studies. Another disadvantage is that there is<br />

a certa<strong>in</strong> delay between onset <strong>of</strong> the discharge <strong>and</strong> <strong>in</strong>dication <strong>in</strong> the <strong>in</strong>strumentation.<br />

However, it can be useful as a diagnostic tool together<br />

with one or two <strong>of</strong> the other described methods.<br />

6.1.2 Local methods<br />

In cases where it is not sufficient to only confirm the existence <strong>of</strong> a<br />

discharge <strong>in</strong> the system, but also to determ<strong>in</strong>e the exact position, local<br />

methods <strong>of</strong> detection will have to be used. The two most common local<br />

99

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