Table 4
Wolf–Rayet abundances model: tbabs× vphabs× ∑ vapec.
Name | NH (1022 cm−2) | kT (keV) | Norm | ![]() |
![]() |
![]() |
---|---|---|---|---|---|---|
WN abundances with He/H=100 solar | ||||||
A | (![]() |
0.11±0.01 | (![]() |
1.04(294.3/282) | (![]() |
(![]() |
![]() |
(![]() |
|||||
![]() |
(![]() |
|||||
B (a) | (![]() |
0.84±0.15 | (![]() |
1.13(164.38/145) | (![]() |
(![]() |
![]() |
(![]() |
|||||
U (b) | (![]() |
![]() |
(![]() |
1.13(110.71/98) | (![]() |
(![]() |
![]() |
(![]() |
|||||
L (c) | (![]() |
![]() |
(![]() |
0.89(58.86/66) | (![]() |
(![]() |
![]() |
(![]() |
|||||
O (d) | (![]() |
![]() |
(![]() |
1.1(22.05/20) | (![]() |
(![]() |
>9.9 | (![]() |
|||||
*W | (![]() |
![]() |
(![]() |
0.31(46.93/43) | (![]() |
(![]() |
![]() |
(![]() |
|||||
*J | (![]() |
![]() |
(![]() |
0.07(57.48/43) | (![]() |
(![]() |
![]() |
(![]() |
|||||
*R (e) | (![]() |
![]() |
(![]() |
0.61(33.01/36) | (![]() |
(![]() |
![]() |
(![]() |
|||||
*X | (![]() |
>3.38 | (![]() |
0.79(23.5/30) | (![]() |
(![]() |
*G (f) | 44 | ![]() |
(9.4±2.5)e−7 | 0.02(48.63/30) | (![]() |
(![]() |
*P | (![]() |
![]() |
(![]() |
0.16(22.8/17) | (![]() |
(![]() |
*I | (![]() |
![]() |
(![]() |
0.16(19.25/14) | (![]() |
(![]() |
![]() |
(![]() |
|||||
*Q | (![]() |
>3.1 | (![]() |
0.3(17.29/15) | (![]() |
(![]() |
*D | (![]() |
>1.0 | (![]() |
0.71(10.74/14) | (![]() |
(![]() |
*V | ![]() |
0.1 | (![]() |
0.58(10.39/12) | (![]() |
(![]() |
![]() |
(![]() |
|||||
*S | (![]() |
![]() |
(![]() |
0.83(1.47/4) | (![]() |
(![]() |
WC abundances with He/H=100 solar | ||||||
F (g) | (![]() |
![]() |
![]() |
1.03(49.66/48) | (![]() |
(![]() |
![]() |
(![]() |
|||||
![]() |
(![]() |
|||||
*N | (8.3±1.9)e−3 | ![]() |
![]() |
0.24(72.87/65) | (![]() |
(![]() |
![]() |
(![]() |
|||||
*E | (![]() |
![]() |
(![]() |
0.62(8.14/10) | (![]() |
(![]() |
*H | (![]() |
0.28 | (![]() |
0.08(12.88/7) | (![]() |
(![]() |
Notes. Same as in Table 3. Abundances of specific elements that were varied relative to that of helium (for reference, the generic values are reported in Sec. 3.5)(a) (b)S=96.1±31.0(c)S=85.09±38.0 (d)S=829, Ar=1000. (e)A Gaussian line was added in the model at 5.21 keV (see Notes in Table 3). (f) 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. (g)Si=2930, Ar=3100, Ca=8173, Fe=460.
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