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Table 7.

Results of the best-fit partially ionized neutron star atmosphere model with a Gaussian absorption line (per observation and camera).

obsid d.o.f. NHP NH Teff d Rem ϵ σ EW fXa
(%) (1020 cm−2) (105 K) (3σ, pc) (km) (eV) (eV) (eV)
pn
2012 1.18 185 5 4.07(17) < 107 89(5) 6.581(23)
201 0.88 205 89 < 120
301 1.07 196 25 < 105 390(6) 84(4) 6.589(18)
401 0.96 196 65 < 110 50(5)
501 1.00 197 50 113(6)

MOSb
2012 1.06 182 29 3.4(4) < 117 87(8)
201 1.10 200 16 3.12(29) < 110 104(6)
301 0.98 188 54 < 105 396(7) 82(4) 6.072(25)
401 1.07 186 25 < 110
501 1.12 189 12 < 110 6.602(27)

EPICc
2012 1.16 371 1.8 < 110 6.419(18)
201 1.01 409 44 3.50(16) < 110 6.391(10)
301 1.03 388 31 4.11(10) 6.18(7) < 105 392(4) 83.2(2.5)
401 1.02 386 39 < 110 8.7(6) 91(6) 58(4) 6.769(16)
501 1.10 390 10 < 110 62(3)

Multi-epoch fitsd
pn 1.03 995 26 4.85(14)
MOS 1.13 1739 < 1 < 105
EPIC 1.14 1203 < 1 3.82(10) < 105

Notes. Errors are 1σ confidence levels. The model fitted to the data in XSPEC is tbabs(nsmaxg-gauss), assuming a magnetic field intensity of B = 1013 G and a 1.4 M neutron star. The effective temperature and radius are given at the source’s rest frame (unredshifted).

(a)

The observed model flux is in units of 10−12 erg s−1 cm−2 in energy band 0.2–12 keV.

(b)

Simple fit of combined MOS1 and MOS2 spectra (per observation).

(c)

Simultaneous fit of pn and combined MOS spectra (per observation).

(d)

Simultaneous fit per instrument (5 pn, 10 MOS1/2, and 6 pn and stacked MOS spectra).

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