Table 3
Solar abundances model: tbabs× phabs× ∑ vapec.
Name | ![]() |
kT (keV) | Norm | ![]() |
![]() |
![]() |
---|---|---|---|---|---|---|
A | ![]() |
![]() |
(![]() |
1.05(296.39/283) | (![]() |
(![]() |
![]() |
(![]() |
|||||
![]() |
(![]() |
|||||
B | ![]() |
![]() |
(![]() |
1.11(162.61/146) | (![]() |
(![]() |
![]() |
(![]() |
|||||
U (a) | ![]() |
![]() |
(![]() |
1.05(102.76/98) | (![]() |
(![]() |
![]() |
(![]() |
|||||
L | ![]() |
![]() |
(![]() |
0.90(59.99/67) | (![]() |
(![]() |
![]() |
(![]() |
|||||
F(b) | ![]() |
![]() |
(![]() |
1.19(54.73/46) | (![]() |
(![]() |
![]() |
(![]() |
|||||
![]() |
(![]() |
|||||
O(c) | ![]() |
![]() |
(![]() |
0.94(18.78/20) | (![]() |
(![]() |
>9.2 | (![]() |
|||||
*N | ![]() |
![]() |
(![]() |
0.1(79.85/65) | (![]() |
(![]() |
![]() |
(![]() |
|||||
*W | ![]() |
0.25±0.1 | (![]() |
0.25(48.78/43) | (![]() |
(![]() |
![]() |
(![]() |
|||||
*J | ![]() |
![]() |
(![]() |
0.06(58.54/43) | (![]() |
(![]() |
![]() |
(![]() |
|||||
*R(d) | ![]() |
![]() |
(![]() |
0.8(27.89/35) | (![]() |
(![]() |
![]() |
(![]() |
|||||
*X | ![]() |
>3.4 | (![]() |
0.77(23.96/30) | (![]() |
(![]() |
*G(e) | 44 | ![]() |
(3.6±1.0)e−5 | 0.02(47.71/30) | (![]() |
(![]() |
*P | ![]() |
![]() |
(![]() |
0.12(23.8/17) | (![]() |
(![]() |
*I | ![]() |
![]() |
(![]() |
0.15(19.45/14) | (![]() |
(![]() |
![]() |
(![]() |
|||||
*Q | ![]() |
>2.7 | (![]() |
0.28(17.69/15) | (![]() |
(![]() |
*D | ![]() |
>1.0 | (![]() |
0.73(10.47/14) | (![]() |
(![]() |
*V | ![]() |
0.1 | (![]() |
0.54(10.82/12) | (![]() |
(![]() |
![]() |
(![]() |
|||||
*E | ![]() |
![]() |
(![]() |
0.66(7.67/10) | (![]() |
(![]() |
*H | ![]() |
![]() |
(![]() |
0.01(19.47/7) | (![]() |
(![]() |
*S | ![]() |
![]() |
(![]() |
0.61(2.72/4) | (![]() |
(![]() |
Notes. Sources that are fitted with the wstat statistic are marked with an asterisk; the null hypothesis probability is reported instead of the . 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)
,
(c)S:9.77 Ar:28.08. (d)A Gaussian line was added in the model
(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.
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