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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

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