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Oscillations, Waves, and Interactions - GWDG

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302 Schreiber<br />

PSD [*10 16 (rad/s) 2 /Hz]<br />

36<br />

27<br />

18<br />

9<br />

0<br />

0<br />

8<br />

0.05 0.1 0.15 0.2<br />

6<br />

4<br />

2<br />

M = 8.3<br />

D ≈ 8850 km<br />

M = 5.4<br />

D ≈ 400 km<br />

0<br />

0 1 2 3 4 5<br />

Frequency [Hz]<br />

Figure 22. Comparison of recorded rotation spectra from an teleseismic event (Hokkaido:<br />

Sept. 9, 2003) <strong>and</strong> a regional earthquake (France: Feb. 22, 2003). The much higher<br />

b<strong>and</strong>width of the rotational wave spectra requires alternative data acquisition techniques<br />

such as the demodulator.<br />

of 0.1 Hz, one can still see some signal signature up to about 4 Hz for the regional<br />

event. Frequencies with a rate of change above 2 Hz, however, are already outside the<br />

regime of reliable representation in phase <strong>and</strong> amplitude by conventional frequency<br />

counting <strong>and</strong> second-order autoregression frequency analysis [28].<br />

Figure 23 illustrates some basic characteristics for the detection of rotations from<br />

seismic signals. The diagram shows most of the measurement range of interest for<br />

seismic studies. The relevant frequency window is plotted horizontally, while the<br />

Rotation Rate [rad/s]<br />

10 -5<br />

10 -6<br />

10 -7<br />

10 -8<br />

10 -9<br />

10 -10<br />

10 -11<br />

10 -12<br />

10 -13<br />

Fiber Optic Gyro<br />

Sumatra (9.3)<br />

Algeria (6.8)<br />

France (5.4)<br />

Ring Laser<br />

0.001 0.01 0.1<br />

Frequency [Hz]<br />

1 10<br />

Figure 23. Sensor resolution of<br />

different rotation sensor concepts<br />

in relation to the observed signal<br />

strength of some earthquakes at<br />

different epicentral distances.

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