2008A&A...477..213C


Query : 2008A&A...477..213C

2008A&A...477..213C - Astronomy and Astrophysics, volume 477213-221 (2008/1-1)

The initial-final mass relationship from white dwarfs in common proper motion pairs.

CATALAN S., ISERN J., GARCIA-BERRO E., RIBAS I., ALLENDE PRIETO C. and BONANOS A.Z.

Abstract (from CDS):

The initial-final mass relationship of white dwarfs, which is poorly constrained, is of paramount importance for different aspects of modern astrophysics. From an observational perspective, most of the studies up to now have been done using white dwarfs in open clusters. In order to improve the initial-final mass relationship, we explore the possibility of deriving a semi-empirical relation studying white dwarfs in common proper motion pairs. If these systems are comprised of a white dwarf and a FGK star, the total age and the metallicity of the progenitor of the white dwarf can be inferred from the detailed analysis of the companion. We have performed an exhaustive search for common proper motion pairs containing a DA white dwarf and a FGK star using the available literature and crossing the SIMBAD database with the Villanova White Dwarf Catalog. We have acquired long-slit spectra of the white dwarf members of the selected common proper motion pairs, as well as high resolution spectra of their companions. From these observations, a full analysis of the two members of each common proper motion pair leads to the initial and final masses of the white dwarfs. These observations have allowed us to provide updated information for the white dwarfs, since some of them were misclassified. In the case of the DA white dwarfs, their atmospheric parameters, masses, and cooling times have been derived using appropriate white dwarf models and cooling sequences. From a detailed analysis of the FGK star spectra we have inferred the metallicity. Then, using either isochrones or X-ray luminosities we have obtained the main-sequence lifetime of the progenitors, and subsequently their initial masses. This work is the first one using common proper motion pairs to improve the initial-final mass relationship, and has also allowed us to cover the poorly explored low-mass domain. As in the case of studies based on white dwarfs in open clusters, the distribution of the semi-empirical data presents a large scatter, which is higher than the expected uncertainties in the derived values. This suggests that the initial-final mass relationship may not be a single-valued function.

Abstract Copyright: ∼

Journal keyword(s): stars: evolution - stars: white dwarfs - open clusters and associations: individual : common proper motion pairs - binaries: visual

CDS comments: WD 0023+109 is a probable misprint for WD 0023-109 (§3.2, table 4), WD 0413-017 is a probable misprint for WD 0413-077 (table 12)

Simbad objects: 31

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Number of rows : 31
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 LP 705-30 PM* 00 26 00.2960313336 -10 37 00.186103632   14.6 12.90     K6 18 0
2 EGGR 166 WD* 00 26 02.2880266968 -10 37 51.863301444   16.483 16.156 16.156   DA4.8 50 0
3 * 95 Cet ** 03 18 22.4263835016 -00 55 49.034196624           G9IV 121 0
4 * 95 Cet C WD* 03 18 24.8111421456 -00 55 16.085104320           DA 23 0
5 Cl Melotte 22 OpC 03 46 38.0 +24 10 41           ~ 3679 0
6 * omi02 Eri PM* 04 15 16.3196189945 -07 39 10.330779018 5.69 5.25 4.43 3.74 3.29 K0V 879 0
7 * omi02 Eri B WD* 04 15 21.7957181469 -07 39 29.203986789 9.147 9.83 9.53     DA2.9 357 0
8 Cl Melotte 25 OpC 04 30 27.4 +16 46 43           ~ 3309 0
9 * alf CMa SB* 06 45 08.91728 -16 42 58.0171 -1.51 -1.46 -1.46 -1.46 -1.43 A0mA1Va 1610 0
10 NGC 2632 OpC 08 39 58.4 +19 36 33           ~ 1733 0
11 HD 79371 PM* 09 15 08.1044327352 +44 02 59.693720784   9.68   8.6   G5V 40 0
12 EGGR 64 WD* 09 16 40.7559432984 +43 59 41.590579092   15.56   15.3   DA5.8 73 0
13 BD-02 3214 Em* 10 46 12.0732326832 -03 39 52.904972052   11.96 11.46 11.15 10.57 G1 13 0
14 G 163-B9B HS* 10 46 16.1907534984 -03 40 33.408622092     14.14 15.85 14.72 sdB 9 0
15 BD+23 2539 PM* 13 07 14.1480913344 +22 27 25.018704540   10.49 9.75     G8V 19 0
16 BD+34 2473 PM* 13 57 05.5018639032 +33 48 25.187290272   9.63   8.7   F8 28 0
17 BD+34 2473B WD* 13 57 09.6172493496 +33 48 02.455483104   16.46   16.15   DA3.5 50 0
18 HD 131250 PM* 14 52 30.5771561136 +00 06 37.546819632   9.35   8.2   G3V 40 0
19 Wolf 555 PM* 14 52 32.1590472673 +00 10 08.142839171   13.8   12.214   M2.5V 38 0
20 EGGR 113 HS* 15 46 42.8507660088 +00 45 28.391352948   15.25 14.97 15.54 15.54 sdO 32 0
21 HD 141025 * 15 46 43.9213206360 +00 45 25.664221548   10.25 9.82     G0V 18 0
22 HD 140901 PM* 15 47 29.1010163043 -37 54 58.722921986   6.73 6.01     G7IV 223 0
23 HD 140901B WD* 15 47 30.0209908033 -37 55 08.460010675   13.10 12.80 13.53 12.34 DA4.8 108 0
24 CD-38 10980 WD* 16 23 33.8380498896 -39 13 46.161043572 9.916 10.885 11.029 10.936 10.841 DA2 526 0
25 HD 147513 PM* 16 24 01.2911377368 -39 11 34.729913940 6.17 6.02 5.376     G5V 389 1
26 WG 32 WD* 17 02 56.3376554088 -53 14 36.566115900   13.57 13.48 13.73 13.60 DA3.2 50 0
27 * eps02 Ara ** 17 03 08.7535948608 -53 14 12.969631572   5.750 5.278     F5VFe+0.5 97 0
28 HD 162867B WD* 17 52 55.7628039984 +09 47 52.033904952   15.82   15.97   DC5 40 0
29 HD 162867 PM* 17 52 56.5709264496 +09 48 13.656618180       9.25   K2V 20 0
30 HD 216777B WD* 22 55 49.4725742919 -07 50 02.387855249   16.92 16.50     DA7.4 82 0
31 HD 216777 PM* 22 55 49.9773604202 -07 49 21.386964536 8.73 8.65 8.01 7.47 7.10 G6V 168 0

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