Summary:
- We had a powerful flash with the OMC locked in CARM null and the fast shutter closed only after the flash finished
- That flash could have damaged the OMC (based on the O3 experience)
- The good news is that the OMC seems to unlock by itself due to thermal absorption in the fused silica
- We shouldn't open the OMC shutter in CARM null until a solution is found
While investigating past unlock flashes to find what a safe threshold for the dark fringe power could be for the OMC I have found that the worst case scenario has already happened on Aug 30.
Figure 1 is a zoom on the unlock flash, the OMC was then on resonance, locked using B1 PD3. This was a failed attempt to hand off DARM to DC read-out
On B1p PD2 one can see the power quickly increasing in 2ms, the 15mW peak corresponds to 150W on SDB1. This triggers the closure of the shutter of the PD itself at 35.5ms and the switch off its voltage bias. So the top of the peak is not visible on B1p PD2. The fast shutter is triggers at 31ms, but it takes 9ms to close, so it cuts the beam at 40ms, which is beyond the edge of this figure.
On B1 PD3 one can see the OMC power transmission, it is a 0.1% pick-off from the transmission, so the 1.7mW peak, corresponds to 1.7W in transmission of the cavity and 566W resonating inside the cavity. For comparison, a flash of 500W peak power on an unlocked OMC has burned a hole in the coating of an OMC in 2018. That was well below the damage threshold of the coating, and the theory is that some dust on the coating had burned the hole back in 2018.
Figure 2 is a zoom that higliths that the power evolution in transmission of the OMC does not match the impinging beam.
B1 PD3 has a maximum at 32.5ms, while B1p PD2 is increasing continously to 34.5ms. The ratio of the two power (zz_mwas_ch) has a maximum earlier on at 31.5ms, at the same time the OMC error signal starts decreasing, has a large deviation at 31.7ms. Note that the OMC error signal is low passed at 200Hz, so these evolutions are actually much faster than the bandwidth of the error signal. I expect that what is happening is that the absorption in the OMC unlocks the cavity. The power ratio shows us that at 31.5ms the OMC transmission efficiency start falling off as the OMC is driven off resonce by the temperature dependence of the optical index, and we partially see it with some delay on the error signal. The thermal diffusion time scale for a size comparable to the beam waist is 1s, so any thermal deposition that happens faster than that stays were it is. I.e. the heat / temperature increase is not removed from the beam path by thermal conductance.
Also one can see that the B1p PD2 is increasing by a factor 10 in 2ms, this correspond to an e-folding time of 0.9ms, much shorter than the 2.8ms cavity storage time. This is somewhat unexpected, but it does make sense. SR is lowering the finesse of arm cavities towards the anti-symmetric port, if the double pole cavity is at 450Hz, in principle the storage time could be as short as 0.35ms.
Figure 3 The OMC control itself turnes off the PZT only at 38ms, and the control loop bandwidth is ~3Hz, so the PZT is not doing anything during this transient.
Figure 4 Looking at the trend data we can look on B1pP (the P-polarized PD), it is not saved in the raw, only in the raw full that last 7 days. But the maximum in the trend will give us a good idea of the peak. It is at 0.75mW, and the ratio of power between B1pP and B1p PD2 is a factor 0.023 when looking at other less bright flashes a few minutes later. So the peak power was ~320W on the SDB1 bench.
Figure 5 Looking on a log scale at B1 PD3, the loss of control start to be visible earlier on, with B1 PD3 going above 1e-2mW at 24ms. So if that was the trigger the fast shutter would have closed at 33ms, when there was 30W on the bench.
Figure 6 Looking at the trends data, B1pP is available only in terms of counts. This 320W flash corresponds to 1500 ADC counts, and the brightes flashes over a month of data seem to be 2500 counts, so 530W.