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Table D.1.

Summary of the XMM-Newton and Chandra pointed observations of GSN 069.

ObsID Date (start) Exposure Lbol,  quiesc QPEs
XMM1 0657820101 2010-12-02 13 ∼5.2 ×
XMM2 0740960101 2014-12-05 92 ∼3.8 ×
XMM3 0823680101 2018-12-24 50 ∼2.5
XMM4 0831790701 2019-01-16 134 ∼2.4
Chandra 22096 2019-02-14 73 ∼0.09 − 1.1
XMM5 0851180401 2019-05-31 132 ∼2.0
XMM6 0864330101 2020-01-10 131 ∼2.9
XMM7 0864330201 2020-05-28 125 ∼4.0 ×
XMM8 0864330301 2020-06-03 126 ∼3.7 ×
XMM9 0864330401 2020-06-13 118 ∼4.0 ×
XMM10 0884970101 2021-06-30 48 ∼4.0 ×
XMM11 0884970201 2021-12-03 45 ∼3.7 ×
XMM12 0913990201 2022-07-07 56 ∼2.4

Notes. The (usable) exposure for all XMM-Newton observations (in ks) refers to the EPIC-pn camera. We also report the quiescent bolometric luminosity (in units of 1043 erg s−1) for all observations. For the XMM1 to XMM11 observations, Lbol,  quiesc was taken from Miniutti et al. (2023), and we used exactly the same procedure and spectral model to estimate it during the XMM12 observation. As for the Chandra observation, we report Lbol,  quiesc as estimated by Miniutti et al. (2019), but we point out that Lbol,  disc in the Chandra observation is highly uncertain due to the degradation of the Chandra ACIS detector that forced them to ignore data below 0.4 keV, as well as to the possible appearance of a soft X-ray excess component not easily disentangled from the disc emission above 0.4 keV. Lbol,  disc may be underestimated by up to a factor of ∼2.5 even in XMM-Newton observations due to systematic uncertainties on the intrinsic optical and UV disc emission (as discussed by Miniutti et al. 2023). The last column indicates whether (unambiguous) QPEs were detected during the exposure.

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