1997A&A...319..928S


Query : 1997A&A...319..928S

1997A&A...319..928S - Astronomy and Astrophysics, volume 319928-947 (1997/3-3)

Elemental abundances in normal late-B and HgMn stars from co-added IUE spectra V. Mercury.

SMITH K.C.

Abstract (from CDS):

Atmospheric mercury abundances are derived for a sample of 40 main-sequence, late-B stars, of which 14 are classified normal, and 26 are known chemically peculiar stars of HgMn or related He-weak types. The observational material for this study comprises co-added, short-wavelength IUE spectra encompassing the HgII λ1942 resonance line, coupled with a selection of new and published measurements (equivalent widths and centroid wavelengths) of the optical HgII λ3984 and HgI λ4358 lines. The analysis includes an explicit treatment of the isotopic and hyperfine structure of these lines, and allows for star-to-star variations in the isotopic composition of mercury within the framework of an assumed, mass-dependent fractionation model. The relative isotopic abundances of mercury (as defined by a dimensionless mix parameter, q) are determined using the graphical method pioneered by White et al. In agreement with previous studies, q is found to be strongly anti-correlated with effective temperature, in the sense that the coolest stars are dominated by the heaviest isotopes (e.g., 202Hg and 204Hg). New isotopic-mix parameters for three programme stars - 87 Psc (q=0.3), 28 Her (q=2.8), and HR 7775 (q=1.5) - reinforce that anti-correlation. Synthetic reconstruction of the λ3984 line in those programme stars for which high-resolution spectra are available tends to confirm the isotopic mixtures derived using the graphical method, and lends validity to the mass-dependent fractionation model in general. However, the λ3984 feature observed in the cool HgMn star HR 7775 can only be satisfactorily reproduced by using a tailored isotopic mixture, which departs significantly from that predicted by the q-formalism. The λ1942 resonance line is detected in 10 normal B stars, for which the mean isotope-summed mercury abundance of 1.96±0.34dex (on the scale where logN(H)=12) exceeds the meteoritic value by nearly 3σ. The mercury abundances derived for the HgMn stars vary between ∼5 and 7dex, except for two objects (53 Tau and HR 2676) in which the abundances are consistent with those observed in the normal stars. The He-weak stars in the programme (33 Gem, HR 6000, 36 Lyn, and 46 Aql) appear to be mildly enriched in mercury, but to an extent rendered uncertain by unknown isotopic-mix parameters. The abundances obtained from the optical and ultraviolet lines agree to within their estimated errors, which lends weight to the view that the metastable lower level of λ3984 (5d96s22D5/2) is not overpopulated with respect to its LTE value. The isotope-summed mercury abundances are not correlated with the effective temperatures, surface gravities, or degree of isotopic fractionation of the programme stars; nor is there evidence for systematic changes in the surface mercury abundances of HgMn stars along evolutionary tracks in the H-R diagram.

Abstract Copyright: ∼

Journal keyword(s): stars: abundances - stars: chemically peculiar - stars: early-type - ultraviolet: stars

Simbad objects: 40

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Number of rows : 40
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 * 87 Psc SB* 01 14 07.6281618312 +16 08 00.514454568   5.873 5.962     B8III 148 0
2 * phi Phe SB* 01 54 22.0319152104 -42 29 48.942141036   5.055 5.109     A3V 120 0
3 * pi. Cet SB* 02 44 07.3477594066 -13 51 31.279407049 3.66 4.112 4.236     B8IV 349 0
4 * 53 Tau a2* 04 19 26.0975894496 +21 08 32.298968148   5.413 5.482     B9Vsp 283 0
5 * mu. Lep a2* 05 12 55.9029641016 -16 12 19.668599100 2.78 3.18 3.29 3.30 3.42 B9IV:HgMn 294 1
6 HD 35548 ** 05 25 31.0794483731 -00 32 38.128886484 6.34 6.52 6.56     B9III 159 0
7 * 134 Tau * 05 49 32.9303335271 +12 39 04.760685507 4.68 4.811 4.875     B9V 208 0
8 * 33 Gem Pe* 06 49 49.8362378064 +16 12 10.382708016 5.24 5.72 5.87     B9III 158 0
9 HD 53929 * 07 07 06.4712319600 +04 54 38.091397320 5.52 5.961 6.088     B9III 105 0
10 HD 58661 SB* 07 28 51.4870582200 +48 11 02.180139576   5.61 5.71     B9IIIpSr 112 0
11 * nu. Cnc SB* 09 02 44.2677118128 +24 27 10.392222600   5.404 5.447     A0III 205 0
12 * kap Cnc a2* 09 07 44.8095541176 +10 40 05.519586828 4.70 5.13 5.24     B8IIImnp 376 0
13 * 36 Lyn Ro* 09 13 48.2131781112 +43 13 04.193952924 4.72 5.148 5.282     B9IVpHgMn 223 0
14 V* ET UMa a2* 10 24 07.8468791760 +65 33 59.121373140   4.889 4.930     A1:VpSiSrHg 284 0
15 * tet Leo PM* 11 14 14.4056705348 +15 25 46.455911128 3.40 3.33 3.35 3.32 3.34 A2IV 353 0
16 * chi Lup SB* 15 50 57.5453432166 -33 37 37.728345509 3.77 3.909 3.946     B9III 318 0
17 * iot CrB SB* 16 01 26.5649192496 +29 51 03.819408336   4.921 4.971     A0IIIspHgMnEu 275 0
18 * ups Her PM* 16 02 47.8978183032 +46 02 12.133917132 4.33 4.616 4.709     B9.5III 248 0
19 V* V1027 Sco a2* 16 08 34.5616203192 -39 05 34.278268848   6.552 6.629 6.66   A0/3III 204 0
20 * phi Her a2* 16 08 46.1762180496 +44 56 05.661355344 3.92 4.20 4.27 4.27 4.36 B9VspHgMn 304 1
21 * tau Her Pu* 16 19 44.4367980146 +46 18 48.102135319 3.190 3.73 3.87 4.00 4.16 B5V 417 0
22 * n Her * 16 32 35.6854246680 +05 31 16.391769564 5.39 5.57 5.63     B9.5III 126 0
23 * zet Dra ** 17 08 47.1877295740 +65 42 52.723177105 2.63 3.06 3.17 3.23 3.35 B8III 248 0
24 HD 172044 SB* 18 36 37.3442332272 +33 28 08.537976300 4.8 5.301 5.410     B8IIpHgMn 156 0
25 * alf Lyr dS* 18 36 56.33635 +38 47 01.2802 0.03 0.03 0.03 0.07 0.10 A0V 2787 1
26 HD 174567 * 18 49 44.0870486208 +31 37 46.054879392   6.615 6.632     A0Vs 66 0
27 * 112 Her SB* 18 52 16.4279808528 +21 25 30.512193132 4.83 5.304 5.393     B9pHg 207 0
28 HD 175640 * 18 56 22.6598858520 -01 47 59.503936200 5.86 6.149 6.196     B9IIIpHgMnEu 160 0
29 * 21 Aql a2* 19 13 42.7011956712 +02 17 37.310297604 4.67 5.08 5.15     B8III 243 0
30 HD 181470 SB* 19 19 01.1490176496 +37 26 43.241751420 6.190 6.260 6.260     A0III 88 0
31 HD 182308 Pe* 19 19 46.1395312128 +64 23 26.907669564   6.413 6.504     B9pHgMn 106 0
32 * 46 Aql * 19 42 12.8123363760 +12 11 35.740659732   6.234 6.321     B9III 120 0
33 * 14 Sge SB* 20 03 30.0147595968 +16 01 52.508306604 5.39 5.550 5.658     B9pHgMn 141 0
34 * kap Cep * 20 08 53.3487448872 +77 42 41.115549672   4.35 4.40     B9III 145 0
35 * nu. Cap * 20 20 39.8157949497 -12 45 32.690284207 4.61 4.72 4.76 4.75 4.81 B9IV 279 0
36 * bet02 Cap SB* 20 20 46.5478935096 -14 47 05.603724348   6.08 6.10     B9/A0III/IV 143 0
37 HD 196426 * 20 37 18.3814212168 +00 05 49.053778404 5.73 6.112 6.211     B8IIIpec 94 0
38 * 21 Peg * 22 03 19.0326115488 +11 23 11.574375540   5.762 5.822     B9.5V 160 0
39 * ksi Oct Pu* 22 50 22.8139009656 -80 07 25.841844408 4.7 5.180 5.311     B6V 100 0
40 * bet Scl PM* 23 32 58.2607029954 -37 49 05.825575113 3.92 4.28 4.37 4.37 4.44 B9.5IIIpHgMnSi 194 0

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