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

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

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carriers, because the NLSQ method requires a good seed phase <strong>in</strong> order<br />

to f<strong>in</strong>d a good local m<strong>in</strong>imum. By comb<strong>in</strong><strong>in</strong>g these methods <strong>and</strong> us<strong>in</strong>g<br />

the result <strong>of</strong> the best r<strong>and</strong>om phase approach as a seed phase for the<br />

NLSQ optimisation, the best results are found. The problem with a<br />

r<strong>and</strong>om phase approach is that for a large number <strong>of</strong> carriers, the number<br />

<strong>of</strong> phase-sets needed to achieve a good result becomes discourag<strong>in</strong>gly<br />

high [52].<br />

By us<strong>in</strong>g a genetic algorithm, a great improvement <strong>in</strong> f<strong>in</strong>d<strong>in</strong>g the<br />

worst case scenario <strong>in</strong> a short time has been achieved, especially for the<br />

non-equally spaced carrier case. This type <strong>of</strong> optimisation scheme has<br />

the advantage <strong>of</strong> be<strong>in</strong>g able to f<strong>in</strong>d not only a good local m<strong>in</strong>imum as<br />

<strong>in</strong> the NLSQ case, but the actual global m<strong>in</strong>imum can be found. The<br />

genetic algorithm was implemented by Merecki [40] <strong>and</strong> <strong>in</strong> addition to<br />

improv<strong>in</strong>g the optimisation part <strong>of</strong> the s<strong>of</strong>tware, he also implemented<br />

the threshold <strong>of</strong> the hybrid modes (see Fig. 2.16) as well as many other<br />

useful functions.<br />

The ma<strong>in</strong> problem with multipactor <strong>in</strong> microwave systems is the<br />

electric noise that is generated, which degrades the signal to noise ratio.<br />

Thus the worst case may not always be the maximum power with<strong>in</strong> the<br />

T20 period. Depend<strong>in</strong>g on the material properties some other case may<br />

produce a substantially larger amount <strong>of</strong> energetic electrons. Therefore,<br />

WCAT also <strong>in</strong>cludes the possibility <strong>of</strong> f<strong>in</strong>d<strong>in</strong>g the phase-set that will<br />

produce the largest amount <strong>of</strong> electrons.<br />

In addition to assess<strong>in</strong>g the risk for a vacuum discharge, it can also<br />

be <strong>of</strong> value to <strong>in</strong>vestigate if a multipactor free design may have a risk<br />

<strong>of</strong> corona breakdown if the component is not thoroughly vented when<br />

it is brought <strong>in</strong>to operation. In WCAT this is analysed us<strong>in</strong>g the mean<br />

carrier frequency <strong>and</strong> compar<strong>in</strong>g the corona threshold with the <strong>in</strong>-phase<br />

peak voltage. If the m<strong>in</strong>imum <strong>of</strong> the Paschen curve is greater than this<br />

voltage, then the corona marg<strong>in</strong> is displayed <strong>in</strong> the output w<strong>in</strong>dow <strong>of</strong><br />

WCAT. If the opposite is true, the pressure range with<strong>in</strong> which there is<br />

risk for corona discharge is presented (see Fig. 2.16).<br />

34

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