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Oscillations, Waves, and Interactions - GWDG

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Δf [µHz]<br />

100<br />

50<br />

0<br />

-50<br />

Large ring laser gyroscopes 299<br />

Kyrill@Wettzell<br />

-100<br />

15 16 17 18 19 20 21 22 23<br />

Time [days in 2007]<br />

Figure 20. Time series of G measurements taken over a week around the storm “Kyrill”<br />

in January 2007. When Earth tides <strong>and</strong> diurnal polar motion are removed from the data, a<br />

distinct transient feature remains in the dataset.<br />

period of 243 days. Both the main contributors to the daily polar motion signals <strong>and</strong><br />

the solid Earth tides show up clearly. They agree with the literature values to within<br />

the spectral resolution of the measurement of 50 nHz.<br />

Apart from these known <strong>and</strong> expected signals there are also non-periodic signatures<br />

in the time series of the ring laser, which cannot be unambiguously identified at this<br />

point in time. Figure 20 shows such an example. The displayed dataset was taken<br />

over 7 days around the storm “Kyrill”, which struck central Europe on the 18th of<br />

January, 2007. One can see the diurnal polar motion <strong>and</strong> solid Earth tides signal,<br />

which look very similar to Fig. 18. The second graph in the diagram shows the<br />

same dataset with these known components removed. A very distinct signal remains<br />

with a maximum on the day after the low pressure area had passed over Europe.<br />

Neither the signal itself nor the time delay has been understood so far. For a better<br />

illustration the actual time at which the storm passed over the gyroscope is also<br />

marked on this plot. Apart from crustal deformation <strong>and</strong> strain effects due to wind<br />

friction causing either tilt or some sort of local rotation also sensor internal artifacts<br />

may be responsible for such sensor responses <strong>and</strong> the investigation of these transient<br />

effects is still ongoing.<br />

7 Application in seismology<br />

With the availabilty of large ring lasers geophysical rotations became accessible at<br />

a global scale <strong>and</strong> at various timescales [23]. In particular rotation signals from<br />

teleseismic events became measurable for the first time [27, 29]. A specific project on<br />

rotational seismology, funded by the German Ministry of Education <strong>and</strong> Research<br />

(BMBF) within the geotechnology program, made the construction of a large ring<br />

laser for seismological studies possible. Results from this project eventually led to the

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