Workers: Dan Chen, Misato Onishi
We performed monthly Pcal-Y calibration on 2026/01/20.
After the calibration, we updated EPICS parameters related to the Pcal-Y system. No issues were found.
| EPICS Key | Before | After | Δ (After − Before) |
|---|---|---|---|
| K1:CAL-PCAL_EY_1_OE_R_SET | 0.99001 | 0.98973 | -0.00028 |
| K1:CAL-PCAL_EY_1_OE_T_SET | 0.99001 | 0.98973 | -0.00028 |
| K1:CAL-PCAL_EY_1_PD_BG_RX_V_SET | -0.00483 | -0.00484 | -0.00001 |
| K1:CAL-PCAL_EY_1_PD_BG_TX_V_SET | 0.02263 | 0.02704 | 0.00441 |
| K1:CAL-PCAL_EY_1_RX_V_R_SET | 0.50319 | 0.50319 | 0.00001 |
| K1:CAL-PCAL_EY_2_INJ_V_GAIN | 0.51359 | 0.51512 | 0.00153 |
| K1:CAL-PCAL_EY_2_OE_R_SET | 0.98589 | 0.98618 | 0.00029 |
| K1:CAL-PCAL_EY_2_OE_T_SET | 0.98589 | 0.98618 | 0.00029 |
| K1:CAL-PCAL_EY_2_PD_BG_TX_V_SET | 0.02549 | 0.02955 | 0.00406 |
| K1:CAL-PCAL_EY_2_RX_V_R_SET | 0.49681 | 0.49681 | -0.00001 |
| K1:CAL-PCAL_EY_WSK_PER_RX_SET | 1.84186 | 1.84214 | 0.00028 |
| K1:CAL-PCAL_EY_WSK_PER_TX1_SET | 0.33344 | 0.33376 | 0.00032 |
| K1:CAL-PCAL_EY_WSK_PER_TX2_SET | 0.90362 | 0.90500 | 0.00138 |
[Ushiba, Washimi]
We tuned the Y4 filter more (decrease gain, bandwidth 10%->30%)
With Yokozawa-san
We performed initial alignment.
With Yokozawa-san
We offloaded ITMY MN because the MN coiloutf signals were saturating.
We used the moving mass for P and BF SET filters Y for Y
A CAL Tcam session was performed to obtain beam position information necessary for Pcal. The parameters have already been updated, and SDF at safe state has been accepted.
Operator: Dan Chen
Update Time: 2026/01/20 06:10:12
| EPICS Key | Before [mm] | After [mm] | Δ (After - Before) [mm] |
|---|---|---|---|
| K1:CAL-PCAL_EX_TCAM_PATH1_X | 0.45668 mm | 0.07325 mm | -0.38343 mm |
| K1:CAL-PCAL_EX_TCAM_PATH1_Y | 67.54717 mm | 66.15693 mm | -1.39024 mm |
| K1:CAL-PCAL_EX_TCAM_PATH2_X | 0.21250 mm | 0.56752 mm | +0.35502 mm |
| K1:CAL-PCAL_EX_TCAM_PATH2_Y | -63.32961 mm | -68.50339 mm | -5.17378 mm |
Update Time: 2026/01/20 06:12:05
| EPICS Key | Before [mm] | After [mm] | Δ (After - Before) [mm] |
|---|---|---|---|
| K1:CAL-PCAL_EY_TCAM_PATH1_X | 0.66534 mm | 1.33223 mm | +0.66689 mm |
| K1:CAL-PCAL_EY_TCAM_PATH1_Y | 65.06913 mm | 65.85923 mm | +0.79010 mm |
| K1:CAL-PCAL_EY_TCAM_PATH2_X | -1.14349 mm | -0.29757 mm | +0.84592 mm |
| K1:CAL-PCAL_EY_TCAM_PATH2_Y | -69.90162 mm | -69.75503 mm | +0.14659 mm |
For some filters, the coefficients were not loaded. So I measured the OLG again (and also tuned again):
L3, L5, T2, T3, V1, Y2, Y3, Y4
Now the coefficient differences are not remain.
After the modification, I found that ETMX cannot be damped well for a long time when the suspension was kicked due to the lockloss (fig1).
Figure 2 shows the enlarged view of oscillation, which is at 1.67 Hz.
Since 1.67 Hz is close to 2nd mode of yaw and NBDAMP_L5 frequency, I checked both of them.
First, I checked MN_MNOLDAMP_Y loop to confirm the yaw loop is fine.
Figure 3 shows the OLTF of MN_MNOLDAMP_Y loop with Y1 and Y2 NBDAMP, which seems fine.
Note that MNOLDAMP_Y is designed to damp only 1st (0.3Hz) and 2nd (1.7Hz) resonances, so NBDAMP for 3rd (3.1Hz) and MNR(4.1Hz) should be turned on during the measurement to avoid kicking the resonance at high frequency.
Then, I measured OLTF of NBDAMP_L5 (fig4), which damps 1.67Hz longitudinal mode of Type-A tower.
During the measurement, I turned on MN_MNOLDAMP_Y and NBDAMP_{Y1,Y2} to avoid kicking the yaw resonances.
Since the resonant frequency of 2nd mode of yaw and tower longitudinal mode are very close, the yaw resonance is growing up during the measurement if there is no yaw damping.
This might be the reason of large peaking reported in klog36109.
Anyway, the OLTF of NBDAMP_L5 also seems fine, so I modified the ETMX guardian so that NBDAMP_L5 is engaged at LOCK_ACQUISITION state and disengaged at CARM_DOWN state (fig5 and fig6).
We performed the initial alignment for the Xarm, Yarm, OMC, and PRMI.
Xarm, Yarm, and OMC were done by the Guardian automatically, but for the PRMI, a manual tuning of the PRM pitch by Ushiba-san was necessary.
RECODE_GOOD_VALUES has been done.
We are checking why the ETMX suspsneion went to TRIPPED stat.
We found that the MN COILOUTF outputs gave high signal just before the state change.
(There was not earthquack observed.)
I found this L5 filter which is not used in the main pass was set to be ON in ENGAGE_RAPIDDAMP state.
So I comment-outed this line in the guardian.
Then, the ETMX suspension could reach the LOCK_AQUISITION state.
The error was at the CLOSE_MASTERSWITCH state.
While investigating the system in the situation, I found the NBDAMP L5 was ON.
After manually turing it OFF, the suspension was able to reach the SAFE state.
We need to check why the L5 was turned ON (while the state transition?).
After that, the suspension can not reach SAFE state as the guardian gives errors saying BF_COILOUTFs have outputs. (fig1)
It seems they have provided the very hight values from around 1/17 20:20. (They are still high values now.)
The TM oplev values are still oscilating.(fig2)
The ETMX have tripped around 3:50 on Jan 18.
It seemed MN H3 triged the tripped.
As the value was much lower than the trigged point, I reseted the WD.
There was not any earthquakes on the time?
After that, the suspension can not reach SAFE state as the guardian gives errors saying BF_COILOUTFs have outputs. (fig1)
It seems they have provided the very hight values from around 1/17 20:20. (They are still high values now.)
The TM oplev values are still oscilating.(fig2)
The error was at the CLOSE_MASTERSWITCH state.
While investigating the system in the situation, I found the NBDAMP L5 was ON.
After manually turing it OFF, the suspension was able to reach the SAFE state.
We need to check why the L5 was turned ON (while the state transition?).
I found this L5 filter which is not used in the main pass was set to be ON in ENGAGE_RAPIDDAMP state.
So I comment-outed this line in the guardian.
Then, the ETMX suspension could reach the LOCK_AQUISITION state.
We are checking why the ETMX suspsneion went to TRIPPED stat.
We found that the MN COILOUTF outputs gave high signal just before the state change.
(There was not earthquack observed.)
After the modification, I found that ETMX cannot be damped well for a long time when the suspension was kicked due to the lockloss (fig1).
Figure 2 shows the enlarged view of oscillation, which is at 1.67 Hz.
Since 1.67 Hz is close to 2nd mode of yaw and NBDAMP_L5 frequency, I checked both of them.
First, I checked MN_MNOLDAMP_Y loop to confirm the yaw loop is fine.
Figure 3 shows the OLTF of MN_MNOLDAMP_Y loop with Y1 and Y2 NBDAMP, which seems fine.
Note that MNOLDAMP_Y is designed to damp only 1st (0.3Hz) and 2nd (1.7Hz) resonances, so NBDAMP for 3rd (3.1Hz) and MNR(4.1Hz) should be turned on during the measurement to avoid kicking the resonance at high frequency.
Then, I measured OLTF of NBDAMP_L5 (fig4), which damps 1.67Hz longitudinal mode of Type-A tower.
During the measurement, I turned on MN_MNOLDAMP_Y and NBDAMP_{Y1,Y2} to avoid kicking the yaw resonances.
Since the resonant frequency of 2nd mode of yaw and tower longitudinal mode are very close, the yaw resonance is growing up during the measurement if there is no yaw damping.
This might be the reason of large peaking reported in klog36109.
Anyway, the OLTF of NBDAMP_L5 also seems fine, so I modified the ETMX guardian so that NBDAMP_L5 is engaged at LOCK_ACQUISITION state and disengaged at CARM_DOWN state (fig5 and fig6).
The SR3 have tripped around 3:50 on Jan 18.
An eathquake was observed around that time.
I reset it as the values monitored by the WD looks nomal now.
(same as SRM: klog36161)
The SRM have tripped around 3:50 on Jan 18.
An eathquake was observed around that time.
I reset it as the values monitored by the WD looks nomal now.
About the ~3 Hz oscillation of the yaw during the pitch OLG measurement, Ushiba-san suggested me to apply the NBDAMP Y1 filter (3.13Hz).
I followed his suggestion and confirmed the oscillation was not occurred in the yaw.
I measured the OLG of the ITMX MNOLDAMP Filter of roll. It's coherence and phase were looked OK, but the gain was smaller than the reference, about -60dB. [Fig. 1]
At that time, the ROL oplev light was almost only in thee SEG4.
Yokozawa-san went into the mine to perform the centering, and I measured the OLG. Then the result was similer to the reference. [Fig. 2]
We changed FM5 to FM1 in the T1 loop filter. As a result, the saturation disappeared.
The values of COILOUTF are now slightly larger than they were in O4c. So we decided to keep this situation.
The TF of this T1 loop when using FM1 is the attached figure.