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* Summary of current measurements * X-arm round-trip loss from reflectivity is 86(3) ppm https://klog.icrr.u-tokyo.ac.jp/osl/?r=7307 * Y-arm round-trip loss: NOT MEASURED YET |
* Summary of measurements so far * X-arm round-trip loss from reflectivity is 86(3) ppm (if we assume no birefringence) https://klog.icrr.u-tokyo.ac.jp/osl/?r=7307 |
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* Power recycling gain for the sidebands are * DRMI on 1f is fine. Lasts 30 min or so |
* Power recycling gain for the sidebands are 2 or so (very rough estimate). * DRMI on 1f is fine. Lasts 30 min or so. |
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* CMRR for intensity noise. https://klog.icrr.u-tokyo.ac.jp/osl/?r=13028 * Summary of calculations * Effect of ITM asymmtery to sensitivity: https://gwdoc.icrr.u-tokyo.ac.jp/cgi-bin/private/DocDB/ShowDocument?docid=10352 * Effect of ITM asymmetry to ASC: https://gwdoc.icrr.u-tokyo.ac.jp/cgi-bin/private/DocDB/ShowDocument?docid=10359 * Effect of inhomogeneity (without birefringence): https://journals.aps.org/prd/abstract/10.1103/PhysRevD.100.082005 |
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* Try DRFPMI locking for one more week. * X-arm and Y-arm reflectivity/loss measurements with polarization considered * Re-measurement of CMRR for frequency noise https://klog.icrr.u-tokyo.ac.jp/osl/?r=13069 * Measure power recycling gain for sidebands (POP 2f with FPMI locked and PRFPMI locked) * Measure MICH contrast defect with MICH locked and FPMI locked * OMC cavity scan to scan mode content of AS beam * Scattered light measurement in PRC by sweeping PRM and PR2/3 deferentially. |
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* DRFPMI LSC and ASC sensing matrix with birefringence and ITM transmission asymmetry * Frequency noise and intensity noise coupling with birefringence and ITM transmission asymmetry * MICH/PRCL/SRCL to DARM coupling with birefringence and ITM transmission asymmetry * O4 Schedule https://gwdoc.icrr.u-tokyo.ac.jp/cgi-bin/private/DocDB/ShowDocument?docid=9209 |
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* | * We are not sure yet whether birefringence is limiting our sensitivity and stability. DRFPMI locking probably possible with current interferometer. * Putting polarizers inside PRC and SRC might improve the sensitivity and stability, but it might introduce some extra issue (thermal lens, extra loss, scattered light etc). * May be better to focus on characterization of the interferometer and the preparation of better ITMs rather than the preparation of polarizers. * It is always good to prepare for the unexpected if we have manpower and money. Preparing polarizers now might save our lives in the future. * Measurement listed above must be performed before the vent for O4 to characterize the current situation and to make a plan for O4. |
ISC Meeting on 2020/03/09 14:00 - 15:00
Participants:
Zoom meeting: https://zoom.us/j/6676627462
Next meeting
TBD
Minutes
Agenda
- We want to know what to do for O4 with birefringence and ITM transmission asymmetry
- Summary of measurements so far
X-arm round-trip loss from reflectivity is 86(3) ppm (if we assume no birefringence) https://klog.icrr.u-tokyo.ac.jp/osl/?r=7307
ITMX and ITMY single bounce has 12% and 15% loss, respectively, including ITM transmission and losses to p-pol. Losses to p-pol measured at POP was 9.4% for ITMX and 4.6% for ITMY. Considering BS reflectivity is different for s-pol and p-pol., this corresponds to 6.1% for ITMX single bounce and 11% for ITMY single bounce. https://klog.icrr.u-tokyo.ac.jp/osl/?r=9314 https://gwdoc.icrr.u-tokyo.ac.jp/cgi-bin/private/DocDB/ShowDocument?docid=10369
Carrier power recycling gain for PRMI was about 3, which corresponds to PRC intra-cavity loss of 25% or so. Considering ITMX and ITMY single bounce losses, this means that Michelson contrast defect is 10% or so. http://klog.icrr.u-tokyo.ac.jp/osl/?r=9300
The mount of p-pol from ITMX is smaller by a factor of 3 with X-arm locked (mode healing effect). http://klog.icrr.u-tokyo.ac.jp/osl/?r=9393
Carrier power recycling gain when PRFPMI is locked is 12 for X-arm and 10 for Y-arm. http://klog.icrr.u-tokyo.ac.jp/osl/?r=12639
X-arm round-trip loss, finesse, and mode healing effect altogether gives X-arm loss on reflection give 86 ppm * ~1000 + 6.1 % / 3 = 11 % loss. So may be PRG of 10-12 for the carrier is reasonable. This is also consistent with X-arm reflectivity measurement done before we are aware of birefringence issue. https://klog.icrr.u-tokyo.ac.jp/osl/?r=7307
- Power recycling gain for the sidebands are 2 or so (very rough estimate).
- DRMI on 1f is fine. Lasts 30 min or so.
DRMI on 3f lasts 5 min or so. https://klog.icrr.u-tokyo.ac.jp/osl/?r=12535
CMRR for intensity noise. https://klog.icrr.u-tokyo.ac.jp/osl/?r=13028
- Summary of calculations
Effect of ITM asymmtery to sensitivity: https://gwdoc.icrr.u-tokyo.ac.jp/cgi-bin/private/DocDB/ShowDocument?docid=10352
Effect of ITM asymmetry to ASC: https://gwdoc.icrr.u-tokyo.ac.jp/cgi-bin/private/DocDB/ShowDocument?docid=10359
Effect of inhomogeneity (without birefringence): https://journals.aps.org/prd/abstract/10.1103/PhysRevD.100.082005
- List of measurements to be done before the vent for O4
- Try DRFPMI locking for one more week.
- X-arm and Y-arm reflectivity/loss measurements with polarization considered
Re-measurement of CMRR for frequency noise https://klog.icrr.u-tokyo.ac.jp/osl/?r=13069
- Measure power recycling gain for sidebands (POP 2f with FPMI locked and PRFPMI locked)
- Measure MICH contrast defect with MICH locked and FPMI locked
- OMC cavity scan to scan mode content of AS beam
- Scattered light measurement in PRC by sweeping PRM and PR2/3 deferentially.
- List of calculations to be done
- DRFPMI LSC and ASC sensing matrix with birefringence and ITM transmission asymmetry
- Frequency noise and intensity noise coupling with birefringence and ITM transmission asymmetry
- MICH/PRCL/SRCL to DARM coupling with birefringence and ITM transmission asymmetry
O4 Schedule https://gwdoc.icrr.u-tokyo.ac.jp/cgi-bin/private/DocDB/ShowDocument?docid=9209
- Executive summary (tentative)
- We are not sure yet whether birefringence is limiting our sensitivity and stability. DRFPMI locking probably possible with current interferometer.
- Putting polarizers inside PRC and SRC might improve the sensitivity and stability, but it might introduce some extra issue (thermal lens, extra loss, scattered light etc).
- May be better to focus on characterization of the interferometer and the preparation of better ITMs rather than the preparation of polarizers.
- It is always good to prepare for the unexpected if we have manpower and money. Preparing polarizers now might save our lives in the future.
- Measurement listed above must be performed before the vent for O4 to characterize the current situation and to make a plan for O4.