[Fujimoto, Yokozawa, Saito]
A mirror was installed inside the OMMT chamber so that the light reflected from OMMT2 would reach the optical table on the X+ side. The reflected light was then directed into the RFPD. However, the DC output was approximately 1.3 V, with fluctuations in the signal also observed. Since the DC output was several volts when the RFPD was placed at OMC REFL, the position of the RFPD will be fine-tuned next time to maximize the DC output, and the condition of the RFPD will also be investigated.
- First, a mirror was installed inside the OMMT chamber so that the light reflected from OMMT2 would reach the optical table on the X+ side (Photo 1). The beam was then lowered using a periscope, and the optical power was measured to be approximately 12 mW. An ND filter with OD = 1.0, a mirror, a lens with a focal length of 50 mm, and the RFPD were then installed. The optical power measured just before the RFPD was approximately 1.5 mW. Next, a rotatable polarizer was placed in front of the lens (Photo 2), and the polarizer angle was adjusted to maximize the optical power. The measured power was approximately 1.0 mW. The BNC cable that had been used for the OMC REFL PD was then connected to the DC output of the RFPD so that the signal could be monitored through CDS. The mirror alignment was adjusted to maximize the DC count, resulting in approximately 2200 counts, corresponding to approximately 1.3 V. When the RFPD was placed at OMC REFL and approximately 1 mW of light was injected, the DC output reached several volts after optimizing the mirror alignment. Therefore, it is likely that not all of the incident light is being coupled into the RFPD. Fluctuations in the signal were also observed. Next time, the position of the RFPD will be fine-tuned to maximize the DC output, and the condition of the RFPD will be investigated.