The fluctuations of the sensitivity are dominated by the power fluctuations of B1p, which are due to the fact that the ITF alignment is not yet controlled by the quadrants (fig 1).
When the noise is high a lot of structures grow, which resamble to mechanical resonances (fig 2).
A good candidate to be the source of that noise is the angular control of SDB1. Fig 3 is the transfer function between SDB1_LC_TX_corr and DARM, when the noise is maximally coupled.