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

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Chapter 4<br />

<strong>Multipactor</strong> <strong>in</strong> irises<br />

A common microwave component is the waveguide iris, which is <strong>of</strong>ten<br />

used as a shunt susceptance for the purpose <strong>of</strong> match<strong>in</strong>g a load to the<br />

waveguide. There are many different types <strong>of</strong> irises, but a typical configuration<br />

consists <strong>of</strong> a step-like, short length, reduction <strong>of</strong> the waveguide<br />

height. Similar structures also appear <strong>in</strong> other configurations, e.g. as<br />

apertures <strong>in</strong> array antennas, as coupl<strong>in</strong>g slots <strong>in</strong> directional couplers,<br />

<strong>and</strong> as irises <strong>in</strong> waveguide filters. As the field strength <strong>in</strong> the iris can<br />

be very high <strong>and</strong> the gap height is small, there is a pronounced risk <strong>of</strong><br />

hav<strong>in</strong>g a multipactor discharge.<br />

So far <strong>in</strong> this thesis, all the models considered have been based on<br />

the plane-parallel model with a spatially uniform harmonic electric field.<br />

In general, most theoretical studies <strong>of</strong> the multipactor phenomenon have<br />

been limited to this or similar approximations. However, many RF devices<br />

<strong>in</strong>volve more complicated electric field structures where predictions<br />

based on the parallel-plate model are not applicable. This is true for<br />

e.g. the waveguide iris, where the electric field will be a comb<strong>in</strong>ation<br />

<strong>of</strong> several different electromagnetic modes, most <strong>of</strong> which typically are<br />

evanescent. However, due to the short length <strong>of</strong> the iris, these modes<br />

will be <strong>of</strong> importance. Nevertheless, <strong>in</strong> this analysis, which is described<br />

<strong>in</strong> more detail <strong>in</strong> paper D, it is only the importance <strong>of</strong> the r<strong>and</strong>om drift<br />

due to <strong>in</strong>itial velocity spread <strong>of</strong> the secondary electrons that has been<br />

considered. Thus, as far as the field is concerned, a spatially uniform<br />

harmonic field based on the parallel-plate model is used.<br />

Experiments [60, 61] as well as numerical studies [61, 62] <strong>of</strong> multipactor<br />

<strong>in</strong> an iris have shown that the discharge threshold <strong>in</strong>creases with<br />

decreas<strong>in</strong>g length <strong>of</strong> the iris. It has been suggested that the reason for<br />

59

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