1996A&A...311L..17H


Query : 1996A&A...311L..17H

1996A&A...311L..17H - Astronomy and Astrophysics, volume 311L17-20 (1996/7-3)

On the hot ends of the white dwarf spectral sequences: Hot white dwarfs containing helium from the Hamburg-Schmidt survey.

HEBER U., DREIZLER S. and HAGEN H.-J.

Abstract (from CDS):

We report on the discovery of twelve very hot white dwarf stars containing helium by follow-up spectroscopy of candidates selected by the Hamburg-Schmidt survey. These stars belong to the sparsely populated spectral subclasses DAO, DO and PG1159 tracing the hottest ends of the white dwarf spectral sequences. Eight stars show helium dominated spectra (four DOs, two PG1159 stars and two very hot DO/sdO transition objects). Four stars have hydrogen dominated spectra (DAO), out of which one is a spectroscopic binary. Metal absorption lines are detected in one DO and one DAO star. The latter is unique and has to be classified as the first known DAOZ star. Spectral comparison indicates that all stars lie beyond the DB gap with Teff exceeding 45000K. Evidence is given for Teff as high as 100000K or more in some stars. With these new discoveries the Hamburg-Schmidt survey has increased the number of known DO and DAO white dwarfs and PG1159 stars by 55%, 30% and 40%, respectively, an important step towards deriving statistically meaningful samples of the hottest white dwarfs.

Abstract Copyright: ∼

Journal keyword(s): Stars: abundances - binaries: spectroscopic - Stars: AGB and post-AGB, white dwarfs

Errata: erratum vol. 319, p. 363

Simbad objects: 27

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Number of rows : 27
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 HS 0103+2947 WD* 01 06 12.8074869648 +30 03 28.249863588   17.6   17.6   DO 10 0
2 PB 6330 WD* 01 13 46.7761796520 +00 28 28.644373920   15.040 15.239 15.635   DO 39 0
3 PG 0231+051 WD* 02 33 41.3574299856 +05 18 43.649856216 14.562 15.776 16.096 16.267 16.639 DAO.6 149 0
4 SH 2-216 PN 04 43 21.2638228056 +46 42 05.835192876   12.50 12.87 13.04   DAO.6 175 2
5 HS 0444+0453 WD* 04 47 04.5045887496 +04 58 41.340500616   15.9   16.1   DQZO.5 31 0
6 HS 0505+0112 WD* 05 08 30.8836691232 +01 16 39.612553356   14.9       DAOZ.8 15 0
7 PN K 1-27 PN 05 57 02.1748457640 -75 40 22.478040120     16.04 16.27 16.41 sdOHe 91 0
8 V* IN CMa CV* 07 20 47.9109655416 -31 47 02.732961552           DAO+dM 93 0
9 HS 0742+6520 WD* 07 47 25.1559163368 +65 13 01.158279528   17.0       DO 20 0
10 HE 1013-0505 WD* 10 16 28.6043334312 -05 20 35.222859276     14.1     DAO.9 108 0
11 PG 1034+001 HS* 10 37 03.8002625256 -00 08 19.118365188 11.589 12.863 13.228 13.383 13.587 sdB/sdO 131 0
12 HS 1136+6646 WD* 11 39 05.7718884456 +66 30 17.776235160           DAO.6 42 0
13 V* BE UMa CV* 11 57 44.8279856952 +48 56 18.313757772   15.437 15.373 14.867   DO+M1/5e 140 0
14 Feige 55 WD* 12 04 38.5359546168 +60 32 08.086967232 11.974 13.224 13.568 13.717 13.896 DAO.9 84 0
15 HZ 21 WD* 12 13 56.2641545952 +32 56 31.358609412 13.125 14.361 14.688 14.837 15.038 DO1 143 0
16 V* GK Vir ** 14 15 36.4128319176 +01 17 18.226779000   17.0       DAe+M 109 0
17 PG 1424+535 WD* 14 25 55.4615842224 +53 15 25.138507140   15.412 15.963     PG1159 79 0
18 HS 1517+7403 WD* 15 16 46.4260387056 +73 52 06.953282400   16.4   16.9   DO 43 0
19 HS 1522+6615 WD* 15 22 56.6956117920 +66 04 42.031760016   16.4       DO 25 0
20 PN A66 39 PN 16 27 33.7199223168 +27 54 33.471380376   15.27 15.60     DAO.70 132 0
21 HS 1830+7209 WD* 18 30 04.7117378448 +72 11 35.945177640   16.1   17.1   DO 12 0
22 RX J2013.1+4002 ** 20 13 09.3685663800 +40 02 24.241439184     14.6     DAO+M2/3e 94 1
23 HS 2033+0327 HS? 20 35 44.6712151656 +03 37 43.435826508   16.12 16.29 16.53   ~ 6 1
24 HS 2033+0507 HS* 20 36 28.8633940776 +05 17 45.982233384   17.3   17.1   sdB 14 1
25 HS 2209+8229 WD? 22 08 25.8763154304 +82 44 51.409027968   16.0       DO/sdO 14 0
26 PG 2303+013 HS* 23 06 38.1663340920 +01 35 09.182309496   15.74 15.74 16.36   sdO(He) 10 0
27 GD 561 WD* 23 45 02.2994571480 +80 56 59.720782524   14.32 14.59 14.87   DAO.7 50 0

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