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

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

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

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can be said that there are three ma<strong>in</strong> effects that affect the low pressure<br />

multipactor threshold. The friction force tends to <strong>in</strong>crease the threshold<br />

as a higher electric field is needed to reach the necessary impact velocity.<br />

The thermalisation, on the other h<strong>and</strong>, <strong>in</strong>creases the total impact energy<br />

<strong>and</strong> thus a lower electric field is needed to achieve the required impact<br />

velocity. For materials with a low first cross-over po<strong>in</strong>t, the first effect<br />

dom<strong>in</strong>ates for the first order <strong>of</strong> resonance, while for higher order modes,<br />

the latter plays the ma<strong>in</strong> role. In addition to these two effects, the model<br />

also <strong>in</strong>cludes contribution from impact ionisation to the total number<br />

<strong>of</strong> electrons. This addition also tend to lower the multipactor threshold<br />

<strong>and</strong> the effect becomes very prom<strong>in</strong>ent for materials with a high first<br />

cross-over energy as a consequence <strong>of</strong> the concomitant high ionisation<br />

cross-section.<br />

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