Table 2.
Best-fit parameters of XMM-Newton EPIC-pn 1.0–10 keV spectra of SAX J1808 during the high- and low-flux intervals.
| High-flux values | Low-flux values | |
|---|---|---|
| TBABS | ||
| NH [1022 cm−2] | 0.21(a) | 0.21(a) |
| BBODYRAD | ||
| kTBB [keV] | ![]() |
![]() |
| RBB (d3.5 km) | ![]() |
2.86 ± 0.14 |
| F0.5 − 10b | ![]() |
![]() |
| GAUSSIAN LINES | ||
| Si K-edge Eline [keV] | 1.91 ± 0.02 | – |
| σ [keV] | 0(a) | – |
| Norm [10−5] | ![]() |
– |
| Au M-edge Eline [keV] | ![]() |
– |
| σ [keV] | 0(a) | – |
| Norm [10−5] | 6.5 ± 0.7 | – |
| Ar XVIII Eline [keV] | 3.49 ± 0.05 | – |
| σ [keV] | 0.37 ± 0.07 | – |
| Norm [10−5] | 9 ± 2 | – |
| NTHCOMP | ||
| Γ | ![]() |
![]() |
| kTe [keV] | 30(a) | 30(a) |
| kTseed [keV] | < 0.11 | < 0.15 |
| Redshift | 0(a) | 0(a) |
| Norm | 0.0300 ± 0.001 | ![]() |
![]() |
![]() |
0.23 ± 0.04 |
| REFLECTION | ||
| β | ![]() |
![]() |
| Rin [Rg]c | < 6.7 | < 14.7 |
| Rout [Rg]c | 1000(a) | 1000(a) |
| Incl. [deg] | ![]() |
![]() |
| Refl. frac. | −0.62(a) | −0.62(a) |
| Fe abund. [solar] | 1(a) | 1(a) |
| log ξ | 2.32 ± 0.01 | 2.7 ± 0.2 |
![]() |
![]() |
![]() |
| TOTAL | ||
| F0.5 − 10b | ![]() |
![]() |
| χ2/d.o.f. | 179.3/142 | 159.4/134 |
Notes. The fit models are TBabs*(bbodyrad + gaussian + gaussian + gaussian + nthComp + rdblur*rfxconv*nthComp) for the high-flux state and TBabs*(bbodyrad + nthComp + rdblur*rfxconv*nthComp) for the low-flux state. Uncertainties are given at a 1σ confidence level. aParameter kept frozen during the fit.
bUnabsorbed flux in the 0.5–10 keV band and reported in units of 10−10 erg cm−2 s−1.
cRg = GM/c2 is the gravitational radius.
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