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Table 6.

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

obsid d.o.f NHP NH Teff d ϵ σ EW fXa
(%) (1020 cm−2) (105 K) (pc) (eV) (eV) (eV)
pn
2012 1.19 184 4 3.0(4) 116(8) 6.622(23)
201 0.90 204 84 5.83(5) 130(5) 6.965(16)
301 1.07 195 25 2.9(3) 5.68(7) 116(6) 6.650(18)
401 0.97 195 62 2.2(3) 5.85(7) 6.912(21)
501 1.01 196 45 5.92(7) 137(7) 6.909(21)

MOSb
2012 1.05 181 30 2.2(5) 6.42(3)
201 1.11 199 14 1.81(4)
301 0.98 187 59 3.3(4) 5.70(7) 6.081(25)
401 1.08 185 23 1.9(5) 5.72(9) 6.682(29)
501 1.12 188 12 1.8(6) 7.02(3)

EPICc
2012 1.17 370 1.3 5.78(6) 124(5) 6.546(18)
201 1.02 408 36 5.81(4) 6.976(11)
301 1.03 387 31 3.03(23) 5.71(5) 129(6) 6.471(19)
401 1.03 385 34 2.03(28) 5.79(5) 129(5) 6.893(22)
501 1.10 389 8 2.18(28) 5.83(5) 6.974(16)

Multi-epoch fitsd
pn 1.04 994 17 2.45(14) 5.81(3) 87(4) 6.842(9)
MOS 1.13 1738 < 1 93(4) 7.016(13)
EPIC 1.15 1202 < 1 6.805(6)

Notes. Errors are 1σ confidence levels. The model fitted to the data in XSPEC is tbabs(nsa-gauss), assuming a magnetic field intensity of B = 1013 G and canonical neutron star mass and radius. The effective temperature is 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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