Open Access

Table 3

Solar abundances model: tbabs× phabs× ∑ vapec.

Name NHlocal $\[\mathrm{N}_{\mathrm{H}}^{\text {local }}\]$ (1022 cm−2) kT (keV) Norm χν2$\[\chi_\nu^2\]$ or Prob (χ2/dof) FX[ FXISMcor]$\[\mathrm{F}_X\left[\mathrm{~F}_{\mathrm{X}}^{\mathrm{ISMcor}}\right]\]$ (erg cm−2 s−1) LX[ LXISMcor ]$\[\mathrm{L}_X\left[\mathrm{~L}_{\mathrm{X}}^{\text {ISMcor }}\right]\]$ (erg s−1)
A 4.180.49+0.51$\[4.18_{-0.49}^{+0.51}\]$ 0.110.01+0.02$\[0.11_{-0.01}^{+0.02}\]$ (0.080.07+0.25$\[0.08_{-0.07}^{+0.25}\]$)e2 1.05(296.39/283) (1.680.1+0.01$\[1.68_{-0.1}^{+0.01}\]$[2.51])e−13 (3.590.22+0.02$\[3.59_{-0.22}^{+0.02}\]$[5.37])e32
0.760.09+0.06$\[0.76_{-0.09}^{+0.06}\]$ (1.940.42+0.69$\[1.94_{-0.42}^{+0.69}\]$)e−3
3.81.0+1.1$\[3.8_{-1.0}^{+1.1}\]$ (1.570.36+0.84$\[1.57_{-0.36}^{+0.84}\]$)e−4
B 3.140.38+0.49$\[3.14_{-0.38}^{+0.49}\]$ 0.770.12+0.11$\[0.77_{-0.12}^{+0.11}\]$ (3.40.92+1.89$\[3.4_{-0.92}^{+1.89}\]$)e−4 1.11(162.61/146) (5.810.44+0.03$\[5.81_{-0.44}^{+0.03}\]$[7.92])e−14 (1.240.09+0.01$\[1.24_{-0.09}^{+0.01}\]$[1.7])e32
5.31.2+1.7$\[5.3_{-1.2}^{+1.7}\]$ (5.71.0+1.5$\[5.7_{-1.0}^{+1.5}\]$)e−5
U (a) 1.880.36+0.51$\[1.88_{-0.36}^{+0.51}\]$ 0.660.16+0.3$\[0.66_{-0.16}^{+0.3}\]$ (2.330.82+2.32$\[2.33_{-0.82}^{+2.32}\]$)e−4 1.05(102.76/98) (3.070.42+0.01$\[3.07_{-0.42}^{+0.01}\]$[5.65])e−14 (6.580.9+0.02$\[6.58_{-0.9}^{+0.02}\]$[12.09])e31
2.530.53+2.53$\[2.53_{-0.53}^{+2.53}\]$ (0.40.24+0.21$\[0.4_{-0.24}^{+0.21}\]$)e−4
L 2.960.95+1.62$\[2.96_{-0.95}^{+1.62}\]$ 0.530.25+0.47$\[0.53_{-0.25}^{+0.47}\]$ (1813+235$\[18_{-13}^{+235}\]$)e−5 0.90(59.99/67) (2.180.56+0.01$\[2.18_{-0.56}^{+0.01}\]$[3.1])e−14 (4.661.2+0.02$\[4.66_{-1.2}^{+0.02}\]$[6.63])e31
2.490.54+1.61$\[2.49_{-0.54}^{+1.61}\]$ (0.470.24+0.16$\[0.47_{-0.24}^{+0.16}\]$)e−4
F(b) 6.72.3+3.7$\[6.7_{-2.3}^{+3.7}\]$ 0.080.03+0.07$\[0.08_{-0.03}^{+0.07}\]$ (0.920.92+592.67$\[0.92_{-0.92}^{+592.67}\]$)e2 1.19(54.73/46) (3.230.75+0.01$\[3.23_{-0.75}^{+0.01}\]$[3.77])e−14 (6.911.6+0.02$\[6.91_{-1.6}^{+0.02}\]$[8.08])e31
0.620.4+0.82$\[0.62_{-0.4}^{+0.82}\]$ (1513+376$\[15_{-13}^{+376}\]$)e−5
5.72.2+3.2$\[5.7_{-2.2}^{+3.2}\]$ (4.260.99+2.48$\[4.26_{-0.99}^{+2.48}\]$)e−5
O(c) 1.580.98+1.37$\[1.58_{-0.98}^{+1.37}\]$ 0.530.15+0.2$\[0.53_{-0.15}^{+0.2}\]$ (4.53.3+16.7$\[4.5_{-3.3}^{+16.7}\]$)e−5 0.94(18.78/20) (1.030.89+0.25$\[1.03_{-0.89}^{+0.25}\]$[1.6])e−14 (2.211.9+0.53$\[2.21_{-1.9}^{+0.53}\]$[3.43])e31
>9.2 (8.02.1+1.5$\[8.0_{-2.1}^{+1.5}\]$)e−6
*N 20.35.6+4.7$\[20.3_{-5.6}^{+4.7}\]$ 0.10.03+0.04$\[0.1_{-0.03}^{+0.04}\]$ (2727+1040$\[27_{-27}^{+1040}\]$)e2 0.1(79.85/65) (1.40.71+0.01$\[1.4_{-0.71}^{+0.01}\]$[1.53])e−14 (2.991.52+0.02$\[2.99_{-1.52}^{+0.02}\]$[3.29])e31
2.170.58+1.08$\[2.17_{-0.58}^{+1.08}\]$ (1.060.56+0.86$\[1.06_{-0.56}^{+0.86}\]$)e−4
*W 21.57.8+17.9$\[21.5_{-7.8}^{+17.9}\]$ 0.25±0.1 (8.78.5+219.4$\[8.7_{-8.5}^{+219.4}\]$)e−2 0.25(48.78/43) (0.970.58+0.01$\[0.97_{-0.58}^{+0.01}\]$[1.06])e−14 (2.081.24+0.02$\[2.08_{-1.24}^{+0.02}\]$[2.28])e31
4.62.6+3.2$\[4.6_{-2.6}^{+3.2}\]$ (0.270.1+0.65$\[0.27_{-0.1}^{+0.65}\]$)e−4
*J 6.83.9+10.7$\[6.8_{-3.9}^{+10.7}\]$ 0.180.16+0.31$\[0.18_{-0.16}^{+0.31}\]$ (7.57.5+396.9$\[7.5_{-7.5}^{+396.9}\]$)e−3 0.06(58.54/43) (6.683.54+0.10$\[6.68_{-3.54}^{+0.10}\]$[7.67])e−15 (1.430.76+0.02$\[1.43_{-0.76}^{+0.02}\]$[1.64])e31
5.43.4+6.2$\[5.4_{-3.4}^{+6.2}\]$ (1.10.35+3.69$\[1.1_{-0.35}^{+3.69}\]$)e−5
*R(d) 15.77.5+10.3$\[15.7_{-7.5}^{+10.3}\]$ 0.280.13+0.23$\[0.28_{-0.13}^{+0.23}\]$ (1.21.2+21.8$\[1.2_{-1.2}^{+21.8}\]$)e−2 0.8(27.89/35) (6.145.31+0.10$\[6.14_{-5.31}^{+0.10}\]$[6.9])e−15 (1.311.14+0.02$\[1.31_{-1.14}^{+0.02}\]$[1.48])e31
3.31.5+3.9$\[3.3_{-1.5}^{+3.9}\]$ (1.220.70+2.43$\[1.22_{-0.70}^{+2.43}\]$)e−5
*X 6.02.3+3.2$\[6.0_{-2.3}^{+3.2}\]$ >3.4 (8.12.1+6.0$\[8.1_{-2.1}^{+6.0}\]$)e−6 0.77(23.96/30) (5.522.22+0.16$\[5.52_{-2.22}^{+0.16}\]$[6.11])e−15 (11.824.75+0.34$\[11.82_{-4.75}^{+0.34}\]$[13.09])e30
*G(e) 44 3.960.93+1.92$\[3.96_{-0.93}^{+1.92}\]$ (3.6±1.0)e−5 0.02(47.71/30) (6.311.19+0.28$\[6.31_{-1.19}^{+0.28}\]$[8.0])e−15 (1.350.26+0.06$\[1.35_{-0.26}^{+0.06}\]$[1.71])e31
*P 3211+24$\[32_{-11}^{+24}\]$ 4.12.5+5.0$\[4.1_{-2.5}^{+5.0}\]$ (2.01.0+9.4$\[2.0_{-1.0}^{+9.4}\]$)e−5 0.12(23.8/17) (4.664.66+0.01$\[4.66_{-4.66}^{+0.01}\]$[4.88])e−15 (9.989.98+0.02$\[9.98_{-9.98}^{+0.02}\]$[10.44])e30
*I 3511+12$\[35_{-11}^{+12}\]$ 0.10.04+0.03$\[0.1_{-0.04}^{+0.03}\]$ (3.43.4+117.6$\[3.4_{-3.4}^{+117.6}\]$)e4 0.15(19.45/14) (3.533.39+0.01$\[3.53_{-3.39}^{+0.01}\]$[3.78])e−15 (7.567.26+0.02$\[7.56_{-7.26}^{+0.02}\]$[8.09])e30
5.12.7+6.4$\[5.1_{-2.7}^{+6.4}\]$ (0.130.05+0.22$\[0.13_{-0.05}^{+0.22}\]$)e−4
*Q 8.43.6+5.3$\[8.4_{-3.6}^{+5.3}\]$ >2.7 (6.92.7+8.0$\[6.9_{-2.7}^{+8.0}\]$)e−6 0.28(17.69/15) (3.83.25+0.02$\[3.8_{-3.25}^{+0.02}\]$[4.16])e−15 (8.146.97+0.04$\[8.14_{-6.97}^{+0.04}\]$[8.9])e30
*D 6241+29$\[62_{-41}^{+29}\]$ >1.0 (2.22.2+10$\[2.2_{-2.2}^{+10}\]$)e−4 0.73(10.47/14) (2.752.75+0.01$\[2.75_{-2.75}^{+0.01}\]$[2.88])e−15 (5.895.89+0.02$\[5.89_{-5.89}^{+0.02}\]$[6.16])e30
*V 9927+43$\[99_{-27}^{+43}\]$ 0.1 (1616+718$\[16_{-16}^{+718}\]$)e8 0.54(10.82/12) (5.014.95+0.01$\[5.01_{-4.95}^{+0.01}\]$[5.23])e−15 (10.7310.59+0.02$\[10.73_{-10.59}^{+0.02}\]$[11.2])e30
1.660.54+4.78$\[1.66_{-0.54}^{+4.78}\]$ (0.350.32+2.45$\[0.35_{-0.32}^{+2.45}\]$)e−3
*E 0.060.06+1.84$\[0.06_{-0.06}^{+1.84}\]$ 3.01.4+2.4$\[3.0_{-1.4}^{+2.4}\]$ (2.430.76+2.76$\[2.43_{-0.76}^{+2.76}\]$)e−6 0.66(7.67/10) (1.530.8+0.05$\[1.53_{-0.8}^{+0.05}\]$[2.99])e−15 (3.281.71+0.12$\[3.28_{-1.71}^{+0.12}\]$[6.4])e30
*H 4.53.6+9.7$\[4.5_{-3.6}^{+9.7}\]$ 0.280.17+0.48$\[0.28_{-0.17}^{+0.48}\]$ (2.82.8+81.1$\[2.8_{-2.8}^{+81.1}\]$)e−4 0.01(19.47/7) (2.972.97+0.01$\[2.97_{-2.97}^{+0.01}\]$[7.21])e−16 (6.356.35+0.02$\[6.35_{-6.35}^{+0.02}\]$[15.44])e29
*S 2.42.4+6.4$\[2.4_{-2.4}^{+6.4}\]$ 1.71.1+13$\[1.7_{-1.1}^{+13}\]$ (2.02.0+3.2$\[2.0_{-2.0}^{+3.2}\]$)e-6 0.61(2.72/4) (5.15.1+0.08$\[5.1_{-5.1}^{+0.08}\]$[7.1])e-16 (1.11.1+0.02$\[1.1_{-1.1}^{+0.02}\]$[1.5])e30

Notes. Sources that are fitted with the wstat statistic are marked with an asterisk; the null hypothesis probability is reported instead of the χν2$\[\chi_\nu^2\]$. We show the absorbed 0.5–8.0 keV flux, the corresponding luminosity, and in brackets the ISM-corrected values (not corrected for local absorption). Errors are not reported for parameters that were kept frozen (Sect. 3.5.1). Abundances of specific elements that were varied: (a)S=1.39±0.50 (b)Ar=8.77.7+11.3$\[\mathrm{Ar}{=}8.7_{-7.7}^{+11.3}, \mathrm{Ca}{=}21_{-14}^{+26}\]$, Ca=2114+26$\[\mathrm{Ar}{=}8.7_{-7.7}^{+11.3}, \mathrm{Ca}{=}21_{-14}^{+26}\]$ (c)S:9.77 Ar:28.08. (d)A Gaussian line was added in the model ( lineE =5.210.11+0.15 keV, norm =(6.74.4+5.6)×108)$\[\left(\text { lineE }{=}5.21_{-0.11}^{+0.15} ~\mathrm{keV} \text {, norm }{=}\left(6.7_{-4.4}^{+5.6}\right) \times 10^{-8}\right)\]$ (e)A model of the form tbabs× pcfabs× ∑vapec was used in this particular case with the parameter for the covering fraction frozen at 0.95.

Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.

Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.

Initial download of the metrics may take a while.