Table 1.

X-ray observation log, and 0.3–10 keV fluxes.

TelescopeObservationObservationExposure|$F_{\mathrm{0.3-10}}$|Joint
 dateIDtime (s)(10|$^{-12}$| erg cm|$^{-2}$| s|$^{-1}$|⁠)data set
(1)(2)(3)(4)(5)(6)
XMM–Newton2002-01-010109130301113498.6 
 2004-07-04020102020111267411.3 
 2020-07-0408654702012700010.8 
 2021-01-0308654703012700012.6J21
 2021-08-110870840101, 08708404011799818.8HF
 2022-01-240870840201258003.8LF
 2022-07-280912400101270009.3 
 2023-02-060870840301380006.8LF; F23
 2024-01-2509124002012700021.5HF
NuSTAR2016-02-0560160095002212054.9LF
 2016-12-0290201043002510015.0LF
 2018-10-27804026100022106914.8 
 2019-08-31805026300026812321.8HF
 2020-01-21805026300045016820.9HF
 2021-01-10805026300064151710.9J21
 2021-08-18607610120021864922.1HF
 2021-12-2280602604002533118.4 
 2023-02-0680602604004409778.0F23
 2023-09-2980802652002208255.5LF
 2024-01-25808026520046204624.7HF
NICER2022-07-16566701040117439.6 
 2022-07-265667010501337110.4 
 2022-08-155667010702205214.7 
 2022-08-24566701080110158.0 
 2022-08-25566701080220437.7 
 2022-09-14566701100126369.9 
 2022-09-25566701110125228.7 
 2022-10-045667011201178617.6 
 2022-10-24566701140119176.1 
 2022-11-12566701160118156.2 
 2022-12-03566701180115055.2 
 2023-01-08566701210134985.0 
TelescopeObservationObservationExposure|$F_{\mathrm{0.3-10}}$|Joint
 dateIDtime (s)(10|$^{-12}$| erg cm|$^{-2}$| s|$^{-1}$|⁠)data set
(1)(2)(3)(4)(5)(6)
XMM–Newton2002-01-010109130301113498.6 
 2004-07-04020102020111267411.3 
 2020-07-0408654702012700010.8 
 2021-01-0308654703012700012.6J21
 2021-08-110870840101, 08708404011799818.8HF
 2022-01-240870840201258003.8LF
 2022-07-280912400101270009.3 
 2023-02-060870840301380006.8LF; F23
 2024-01-2509124002012700021.5HF
NuSTAR2016-02-0560160095002212054.9LF
 2016-12-0290201043002510015.0LF
 2018-10-27804026100022106914.8 
 2019-08-31805026300026812321.8HF
 2020-01-21805026300045016820.9HF
 2021-01-10805026300064151710.9J21
 2021-08-18607610120021864922.1HF
 2021-12-2280602604002533118.4 
 2023-02-0680602604004409778.0F23
 2023-09-2980802652002208255.5LF
 2024-01-25808026520046204624.7HF
NICER2022-07-16566701040117439.6 
 2022-07-265667010501337110.4 
 2022-08-155667010702205214.7 
 2022-08-24566701080110158.0 
 2022-08-25566701080220437.7 
 2022-09-14566701100126369.9 
 2022-09-25566701110125228.7 
 2022-10-045667011201178617.6 
 2022-10-24566701140119176.1 
 2022-11-12566701160118156.2 
 2022-12-03566701180115055.2 
 2023-01-08566701210134985.0 

Note. All parameter uncertainties are quoted at the 90th percentile confidence interval. (1) Telescope name. (2) Date of observation start, YYYY-MM-DD. (3) Observation identifier in the HEASarc archive. (4) On-source integration time. This is measured before event screening. (5) Integrated 0.3–10 keV model flux, determined using the phenomenological model (Section 3.2). As NuSTAR is not sensitive below 3 keV, the best-fitting model is extrapolated, to facilitate comparison with the other telescopes. (6) Data set(s) that this observation is included in for the joint analysis described in Section 3.3.

Table 1.

X-ray observation log, and 0.3–10 keV fluxes.

TelescopeObservationObservationExposure|$F_{\mathrm{0.3-10}}$|Joint
 dateIDtime (s)(10|$^{-12}$| erg cm|$^{-2}$| s|$^{-1}$|⁠)data set
(1)(2)(3)(4)(5)(6)
XMM–Newton2002-01-010109130301113498.6 
 2004-07-04020102020111267411.3 
 2020-07-0408654702012700010.8 
 2021-01-0308654703012700012.6J21
 2021-08-110870840101, 08708404011799818.8HF
 2022-01-240870840201258003.8LF
 2022-07-280912400101270009.3 
 2023-02-060870840301380006.8LF; F23
 2024-01-2509124002012700021.5HF
NuSTAR2016-02-0560160095002212054.9LF
 2016-12-0290201043002510015.0LF
 2018-10-27804026100022106914.8 
 2019-08-31805026300026812321.8HF
 2020-01-21805026300045016820.9HF
 2021-01-10805026300064151710.9J21
 2021-08-18607610120021864922.1HF
 2021-12-2280602604002533118.4 
 2023-02-0680602604004409778.0F23
 2023-09-2980802652002208255.5LF
 2024-01-25808026520046204624.7HF
NICER2022-07-16566701040117439.6 
 2022-07-265667010501337110.4 
 2022-08-155667010702205214.7 
 2022-08-24566701080110158.0 
 2022-08-25566701080220437.7 
 2022-09-14566701100126369.9 
 2022-09-25566701110125228.7 
 2022-10-045667011201178617.6 
 2022-10-24566701140119176.1 
 2022-11-12566701160118156.2 
 2022-12-03566701180115055.2 
 2023-01-08566701210134985.0 
TelescopeObservationObservationExposure|$F_{\mathrm{0.3-10}}$|Joint
 dateIDtime (s)(10|$^{-12}$| erg cm|$^{-2}$| s|$^{-1}$|⁠)data set
(1)(2)(3)(4)(5)(6)
XMM–Newton2002-01-010109130301113498.6 
 2004-07-04020102020111267411.3 
 2020-07-0408654702012700010.8 
 2021-01-0308654703012700012.6J21
 2021-08-110870840101, 08708404011799818.8HF
 2022-01-240870840201258003.8LF
 2022-07-280912400101270009.3 
 2023-02-060870840301380006.8LF; F23
 2024-01-2509124002012700021.5HF
NuSTAR2016-02-0560160095002212054.9LF
 2016-12-0290201043002510015.0LF
 2018-10-27804026100022106914.8 
 2019-08-31805026300026812321.8HF
 2020-01-21805026300045016820.9HF
 2021-01-10805026300064151710.9J21
 2021-08-18607610120021864922.1HF
 2021-12-2280602604002533118.4 
 2023-02-0680602604004409778.0F23
 2023-09-2980802652002208255.5LF
 2024-01-25808026520046204624.7HF
NICER2022-07-16566701040117439.6 
 2022-07-265667010501337110.4 
 2022-08-155667010702205214.7 
 2022-08-24566701080110158.0 
 2022-08-25566701080220437.7 
 2022-09-14566701100126369.9 
 2022-09-25566701110125228.7 
 2022-10-045667011201178617.6 
 2022-10-24566701140119176.1 
 2022-11-12566701160118156.2 
 2022-12-03566701180115055.2 
 2023-01-08566701210134985.0 

Note. All parameter uncertainties are quoted at the 90th percentile confidence interval. (1) Telescope name. (2) Date of observation start, YYYY-MM-DD. (3) Observation identifier in the HEASarc archive. (4) On-source integration time. This is measured before event screening. (5) Integrated 0.3–10 keV model flux, determined using the phenomenological model (Section 3.2). As NuSTAR is not sensitive below 3 keV, the best-fitting model is extrapolated, to facilitate comparison with the other telescopes. (6) Data set(s) that this observation is included in for the joint analysis described in Section 3.3.

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