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

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Chapter 5<br />

<strong>Multipactor</strong> <strong>in</strong> coaxial l<strong>in</strong>es<br />

The coaxial l<strong>in</strong>e is a very common <strong>and</strong> important component <strong>in</strong> microwave<br />

systems. It is a transmission l<strong>in</strong>e that consists <strong>of</strong> an <strong>in</strong>ner<br />

cyl<strong>in</strong>drical conductor <strong>and</strong> a coaxial outer conductor. A constant crosssection<br />

is ma<strong>in</strong>ta<strong>in</strong>ed by means <strong>of</strong> a dielectric medium, which is conta<strong>in</strong>ed<br />

between the conductors. In some space applications, as well as <strong>in</strong><br />

other systems, the dielectric medium has been partly omitted <strong>in</strong> order to<br />

save weight or to reduce the dielectric losses. In a vacuum environment,<br />

the l<strong>in</strong>e may become evacuated, which makes it exposed to the risk <strong>of</strong> a<br />

multipactor discharge.<br />

The electric field <strong>in</strong> a coaxial l<strong>in</strong>e is nonuniform, which makes analytical<br />

analysis difficult, s<strong>in</strong>ce the the equation <strong>of</strong> motion for an electron becomes<br />

a non-l<strong>in</strong>ear differential equation. However, multipactor <strong>in</strong> a coaxial<br />

l<strong>in</strong>e has been studied experimentally [63] <strong>and</strong> numerically [64–67]. In<br />

these studies it was found that two different types <strong>of</strong> resonant multipactor<br />

can occur, namely a two-sided discharge between the outer <strong>and</strong><br />

the <strong>in</strong>ner conductors <strong>and</strong> the one-sided analogue on the outer conductor.<br />

In an attempt to underst<strong>and</strong> the effect <strong>of</strong> vary<strong>in</strong>g the relative <strong>in</strong>ner<br />

radius, i.e. vary<strong>in</strong>g the characteristic impedance <strong>of</strong> the coaxial l<strong>in</strong>e,<br />

different scal<strong>in</strong>g laws were suggested <strong>in</strong> these studies. Another study focused<br />

on the current due to the multipact<strong>in</strong>g electrons <strong>and</strong> treated this<br />

as a radially oriented Hertzian dipole <strong>in</strong> order to determ<strong>in</strong>e the electric<br />

field generated by the multipactor discharge [68].<br />

In paper E resonant multipactor <strong>in</strong> a coaxial l<strong>in</strong>e is analysed by<br />

means <strong>of</strong> an approximate analytical solution <strong>of</strong> the non-l<strong>in</strong>ear differential<br />

equation <strong>of</strong> motion, which <strong>in</strong> a large range <strong>of</strong> microwave frequencies<br />

<strong>and</strong> amplitudes agrees very well with the numerical solution. As<br />

69

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