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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allows for another design marg<strong>in</strong>, which is set with respect to the so<br />
called P20 power level. The P20 level corresponds to the “peak power <strong>of</strong><br />
the multicarrier waveform whose width at the s<strong>in</strong>gle carrier multipaction<br />
threshold is equal to the time taken for the electrons to cross the multipact<strong>in</strong>g<br />
region 20 times” [50]. This level is illustrated <strong>in</strong> Fig. 2.15.<br />
Figure 2.15: An example where the <strong>in</strong>-phase peak power is above the s<strong>in</strong>gle<br />
carrier threshold, while the P20 level is more than 4 dB below the<br />
same threshold. The peak voltage is 128.4 V, the s<strong>in</strong>gle carrier<br />
threshold is 91 V, <strong>and</strong> the P20 voltage is 57 V. Signal data: 12<br />
carriers, equally spaced, fm<strong>in</strong> = 1.545 GHz, ∆f = 24 MHz <strong>and</strong><br />
each carrier amplitude is 10.7 V. Material properties: W1 =<br />
23 eV <strong>and</strong> σse,max = 3.<br />
In the case when a design is made with respect to the P20 level, the<br />
design marg<strong>in</strong>s range from 4-6 dB depend<strong>in</strong>g on the type <strong>of</strong> test<strong>in</strong>g. A<br />
problem with the P20 level is that it is not a trivial problem to f<strong>in</strong>d the<br />
peak power level for 20 electron gap cross<strong>in</strong>gs. This power level is usually<br />
referred to as the worst case scenario, even though it may not always be<br />
the worst case from a multipactor po<strong>in</strong>t <strong>of</strong> view. A number <strong>of</strong> different<br />
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