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Oscillations, Waves, and Interactions - GWDG

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4<br />

1<br />

5<br />

4<br />

3<br />

1<br />

1<br />

2<br />

cam 1<br />

Large ring laser gyroscopes 291<br />

d 1 = 39.703 m<br />

d 2 = 21.015 m<br />

cam 3 3<br />

Figure 9. Basic layout of the UG2 ring laser. The laser beams are steered around the<br />

cavity by mirrors with precise mounting on the corner monuments.<br />

UG2 has a rectangular layout spanning an area of 39.703 m by 21.015 m. The<br />

basic design is shown in Fig. 9. Because of the long beam trajectories of 39.703 m <strong>and</strong><br />

21.015 m of the laser, small mirror tilts in the range of a few seconds of arc are causing<br />

already a noticable beam displacement on the next mirror. Since this corresponds<br />

to a change in the geometric scale factor, the beamwalk was monitored <strong>and</strong> the<br />

instantaneous area <strong>and</strong> ring laser orientation (relative to the ring laser hardware<br />

structure) was computed. By placing a CCD camera behind the mirrors at the<br />

locations 1–3 indicated in Fig. 9 <strong>and</strong> recording the light leakage of the laser beam<br />

through the mirrors, beamwalks on the order of a micrometer in displacement could<br />

be monitored. Measurements were conducted by averaging over 4000 individual<br />

images taken one after the other, with the maximum supported exposure time of the<br />

cameras of 8 ms. Figure 10 shows a sample measurement sequence of the movement<br />

of the beam spot center postion with time. In this particular dataset the excursion of<br />

the horizontal position of the laser beam is two times larger compared to the vertical<br />

movement. On other occasions both movements were of the same proportion.<br />

Since the determination of scale factor variations are required with a relative precision<br />

of 10 −9 one can expect a substantial improvement from the geometrical scale<br />

factor correction. After the alignment of the UG2 ring laser to optimize it for minimum<br />

losses, <strong>and</strong> after the laser was refilled with a clean supply of Helium <strong>and</strong> Neon,<br />

a measurement sequence of approximately two weeks was started on Dec. 30, 2005<br />

<strong>and</strong> lasted until Jan. 15, 2006. The Sagnac frequency was recorded with an integration<br />

time of 30 minutes. Figure 11 shows the measurement sequence of raw data<br />

as recorded on the logging system. From the experimental setup, one would expect<br />

1<br />

1<br />

cam 2<br />

2

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