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Oscillations, Waves, and Interactions - GWDG

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Variation in Area [*1e6]<br />

3.0<br />

2.0<br />

1.0<br />

0.0<br />

-1.0<br />

-2.0<br />

-3.0<br />

Large ring laser gyroscopes 293<br />

970<br />

0 4 8 12 16<br />

Time [days in 2006]<br />

Figure 12. Time series of the variations in effective ring laser area superimposed with the<br />

atmospheric pressure at that time.<br />

series of the atmospheric pressure as measured inside the cavern shows significant<br />

correlation with these changes in area. From that one may conclude that pressure<br />

induced deformations of the cave are causing small tilts at the mirror mounts, which<br />

in turn cause beamwalk on the next mirror. A similar result is obtained for the<br />

instantaneous orientation of the UG2 ring laser as shown in Fig. 13. The contributions<br />

from ring laser reorientation are smaller by a factor of about two compared to the<br />

variations in area. Nevertheless the corrections to the orientation vector are also in<br />

the parts per million regime <strong>and</strong> can not be neglected. Again there is some correlation<br />

with the atmospheric pressure evident as well as a linear overall trend. As opposed to<br />

orientation <strong>and</strong> area, the computed perimeter changes are approximately six orders<br />

of magnitude smaller as shown in Fig. 14. This is compatible with the general<br />

observation that longitudinal mode index changes are infrequent.<br />

Variation in Orientation [ * 1e6]<br />

1.0<br />

0.0<br />

-1.0<br />

-2.0<br />

-3.0<br />

-4.0<br />

1030<br />

1020<br />

1010<br />

1000<br />

990<br />

980<br />

970<br />

0 4 8 12 16<br />

Time [days in 2006]<br />

Figure 13. Time series of the variations in effective ring laser orientation superimposed<br />

with the atmospheric pressure.<br />

1030<br />

1020<br />

1010<br />

1000<br />

990<br />

980<br />

Atmospheric Pressure [hPa]<br />

Atmospheric Pressure [hPa]

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