Table 3.
Spectral fits with the optxagnf model to UV and X-ray data of XMMSL2 J1446+68.
Date | MBH | log L/Ledd(a) | rcor(b) | τ(c) | Lbol | χ2/d.o.f. |
---|---|---|---|---|---|---|
(M⊙) | (Rg) | ergs s−1 | ||||
2016-09-08 | 5 × 106 |
![]() |
46.3 ± 8.0 |
![]() |
1.0 × 1043 | 191/89 |
2017-08-14 | 5 × 106 |
![]() |
![]() |
![]() |
3.4 × 1042 | 8/15 |
2016-09-08 | 7 × 107 | −2.83 ± 0.02 |
![]() |
2.29 ± 0.04 | 1.3 × 1043 | 215/89 |
2017-08-14 | 7 × 107 |
![]() |
![]() |
![]() |
4.1 × 1042 | 10/15 |
Notes. Fit to the galaxy-subtracted UVM2 and UVW2 filter count rates and the X-ray spectrum from the XMM-Newton observation of 2016-09-08 and the Swift observation of 2017-08-14 with the optxagnf (Done et al. 2012) model. The hard power-law fraction is set to zero, the electron temperature (kTe) is fixed at 10 keV, the disc outer radius is fixed at 103Rg, and a Schwarzschild non-spinning black hole is assumed.
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