2002A&A...385..111D


Query : 2002A&A...385..111D

2002A&A...385..111D - Astronomy and Astrophysics, volume 385111-130 (2002/4-1)

The presence of Nd and Pr in HgMn stars.

DOLK L., WAHLGREN G.M., LUNDBERG H., LI Z.S., LITZEN U., IVARSSON S., ILYIN I. and HUBRIG S.

Abstract (from CDS):

Optical region spectra for a number of upper main sequence chemically peculiar (CP) stars have been observed to study singly and doubly ionized praseodymium and neodymium lines. In order to improve existing atomic data of these elements, laboratory measurements have been carried out with the Lund VUV Fourier Transform Spectrometer (FTS). From these measurements wavelengths and hyperfine structure (hfs) have been studied for selected PrII, PrIII and NdIII lines of astrophysical interest. Radiative lifetimes for some excited states of PrII have been determined with the aid of laser spectroscopy at the Lund Laser Center (LLC) and have been combined with branching fractions measured in the laboratory to calculate gf values for some of the stronger optical lines of PrII. With the aid of the derived gf values and laboratory measurements of the hfs, a praseodymium abundance was derived from selected PrII lines in the spectrum of the Am star 32 Aqr. This abundance was used to derive astrophysical gf values for selected PrIII lines in 32 Aqr, and these gf values were used to get a praseodymium abundance for the HgMn star HR 7775. The praseodymium abundance in HR 7775 was then utilized to derive astrophysical gf values for all observable PrIII lines in this star. The neodymium abundance, derived from unblended lines of NdII in HR 7775, has been utilized to establish astrophysical gf values for observed NdIII lines in the optical region of this star. Selected PrIII and NdIII lines have been identified and studied in a number of HgMn stars and three hot Am stars. The praseodymium and neodymium abundance change rapidly from an approximate 1-1.2dex enhancement for the hot Am stars to 1.5-3dex enhancement for the cool HgMn stars, indicating a well-defined boundary between the hot Am and HgMn stars in the vicinity of 10500K. The enhancement of praseodymium and neodymium in Am and HgMn stars may be explained by diffusive processes active in the stellar atmosphere, while the observed discontinuity might be explained by a thin hydrogen convection zone thought to be present for the Am stars, but absent in the HgMn stars. The absence of a convection zone would cause the diffused elements to gather higher in the atmosphere of HgMn stars compared to Am stars, and explain the observed increase in abundance.

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Journal keyword(s): atomic data - stars: abundances - stars: chemically peculiar

Simbad objects: 25

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Number of rows : 25
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 HD 35548 ** 05 25 31.0794483731 -00 32 38.128886484 6.34 6.52 6.56     B9III 159 0
2 * alf CMa SB* 06 45 08.91728 -16 42 58.0171 -1.51 -1.46 -1.46 -1.46 -1.43 A0mA1Va 1610 0
3 HD 72660 * 08 34 01.6141823952 -02 09 05.600032848   5.797 5.792     A0V 146 0
4 * nu. Cnc SB* 09 02 44.2677118128 +24 27 10.392222600   5.404 5.447     A0III 205 0
5 * kap Cnc a2* 09 07 44.8095541176 +10 40 05.519586828 4.70 5.13 5.24     B8IIImnp 376 0
6 V* ET UMa a2* 10 24 07.8468791760 +65 33 59.121373140   4.889 4.930     A1:VpSiSrHg 284 0
7 * gam Crv PM* 12 15 48.37081 -17 32 30.9496 2.12 2.47 2.58 2.62 2.71 B8III 249 1
8 * pi.01 Boo * 14 40 43.5589117488 +16 25 05.975961096 4.18 4.792 4.893 4.47 4.49 B9IIIpHgMnSi 212 0
9 * chi Lup SB* 15 50 57.5453432166 -33 37 37.728345509 3.77 3.909 3.946     B9III 318 0
10 * iot CrB SB* 16 01 26.5649192496 +29 51 03.819408336   4.921 4.971     A0IIIspHgMnEu 275 0
11 * ups Her PM* 16 02 47.8978183032 +46 02 12.133917132 4.33 4.616 4.709     B9.5III 248 0
12 * phi Her a2* 16 08 46.1762180496 +44 56 05.661355344 3.92 4.20 4.27 4.27 4.36 B9VspHgMn 304 1
13 * n Her * 16 32 35.6854246680 +05 31 16.391769564 5.39 5.57 5.63     B9.5III 126 0
14 HD 158704 SB* 17 31 44.3739544896 -26 16 10.957302300   5.983 6.052     B9pHgMn 79 0
15 HD 165493 * 18 08 30.1115839488 -45 46 01.234303212   6.061 6.163     B7/8II 41 0
16 * 112 Her SB* 18 52 16.4279808528 +21 25 30.512193132 4.83 5.304 5.393     B9pHg 207 0
17 HD 175640 * 18 56 22.6598858520 -01 47 59.503936200 5.86 6.149 6.196     B9IIIpHgMnEu 160 0
18 HD 178065 SB* 19 07 09.0293341368 +00 38 27.491355672 6.31 6.584 6.538     B9III 103 0
19 * 46 Aql * 19 42 12.8123363760 +12 11 35.740659732   6.234 6.321     B9III 120 0
20 * 15 Vul a2* 20 01 06.0485823565 +27 45 12.862874097   4.829 4.651     A4III 245 0
21 * 14 Sge SB* 20 03 30.0147595968 +16 01 52.508306604 5.39 5.550 5.658     B9pHgMn 141 0
22 * bet02 Cap SB* 20 20 46.5478935096 -14 47 05.603724348   6.08 6.10     B9/A0III/IV 143 0
23 * bet01 Cap SB* 20 21 00.6665981712 -14 46 53.067367488 4.14 3.87 3.08 2.53 2.03 G9II:+B8p:Si: 192 0
24 * 32 Aqr SB* 22 04 47.4224193480 -00 54 22.839762708   5.519 5.271     A5IV 185 0
25 * omi Peg * 22 41 45.4041684504 +29 18 27.631023336 4.77 4.78 4.79 4.75 4.77 A1IV 296 0

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