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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(dBm)<br />
(dBm)<br />
−55<br />
−60<br />
−65<br />
−70<br />
−75<br />
−80<br />
−85<br />
−90<br />
−80<br />
−100<br />
−120<br />
−140<br />
Noise Power (32 − 52 s)<br />
34 36 38 40 42<br />
Time (s)<br />
44 46 48 50 52<br />
Fourier transform (32 − 52 s)<br />
−160<br />
0 50 100 150 200 250<br />
frequency (Hz)<br />
300 350 400 450 500<br />
Figure 6.5: The beg<strong>in</strong>n<strong>in</strong>g <strong>of</strong> a multipactor test sequence show<strong>in</strong>g the time<br />
before onset <strong>of</strong> the discharge. The FFT (fast Fourier transform)<br />
gives no <strong>in</strong>dication <strong>of</strong> dom<strong>in</strong>ant frequency components.<br />
(dBm)<br />
(dBm)<br />
−55<br />
−60<br />
−65<br />
−70<br />
−75<br />
−80<br />
−85<br />
−90<br />
−80<br />
−100<br />
−120<br />
−140<br />
Noise Power (52 − 72 s)<br />
54 56 58 60 62<br />
Time (s)<br />
64 66 68 70 72<br />
Fourier transform (52 − 72 s)<br />
−160<br />
0 50 100 150 200 250<br />
frequency (Hz)<br />
300 350 400 450 500<br />
Figure 6.6: The end <strong>of</strong> the same test sequence as <strong>in</strong> Fig. 6.5. The sudden <strong>in</strong>crease<br />
<strong>in</strong> the noise floor <strong>in</strong>dicates onset <strong>of</strong> multipactor. The FFT<br />
shows dom<strong>in</strong>ant frequency components at 100 Hz <strong>and</strong> multiples<br />
there<strong>of</strong>.<br />
102