A&A 368, 250-266 (2001)
DOI: 10.1051/0004-6361:20000572
A. Arellano Ferro1 - Sunetra Giridhar2 - P. Mathias3
1 - Instituto de Astronomía, Universidad Nacional Autónoma de México,
Apdo. Postal 70-264, México D.F.,
CP 04510, México
2 -
Indian Institute of Astrophysics, Bangalore 560034, India
3 -
Observatoire de la Côte d'Azur, Département Fresnel, UMR 6528, BP
4229, 06304 Nice Cedex 04, France
Received 23 August 2000 / Accepted 19 December 2000
Abstract
Detailed atmospheric abundances have been calculated for a
sample of A-G supergiant stars with IR fluxes and/or
high galactic latitudes. HD 172481 and HD 158616 show clear indications
of being post-AGB stars that have experienced third dredge-up.
HD 158616 is carbon-rich while the abundance pattern of
HD 172481 and its large Li enhancement gives support to the hot
bottom burning scenario that
explains paucity of carbon-rich stars among AGB stars.
HD 172324 is very likely a hot post-AGB star that shows a strong
carbon deficiency.
HD 725, HD 218753 and HD 331319 also appear
to be evolved objects between the red giant and the AGB.
HD 9167, HD 173638 with a few
exceptions, reflect solar abundances and no signs of post red giant evolution.
They are most likely young massive disk supergiants. Further analysis of proto-Planetary Nebula HDE 341617
reveals that He lines show signs of velocity stratification.
The emission lines have weakened
considerably since 1993.
The envelope expands at 19 km s-1 relative to the star. Atmospheric abundances,
evolutionary tracks and isochrones are used to estimate masses and
ages of all stars in the sample.
Key words: stars: post-AGB - stars: chemically peculiar - stars: evolution
Post-AGB stars, as they evolve across the H-R diagram towards the white dwarf stage, form families of rather exotic objects like the R CrB stars, other subgroups of H-deficient and He-rich stars, planetary nebulae etc. In the H-R diagram, they populate the region generally occupied by massive young supergiants evolving redwards from the main sequence, and having similar temperatures and luminosities. To differentiate the massive and young stars from the highly evolved low-mass post-AGB stars, detailed atmospheric abundance analysis is crucial. Chemical analysis of high galactic latitude A-F supergiants have led to the discovery of many interesting post-AGB stars such as HR 7671 (Luck et al. 1990), HR 4912 (Lambert et al. 1983), HR 4114 (Giridhar et al. 1997) or of selected IRAS sources such as IRAS 22223+4327 and IRAS 04296+3429 (Decin et al. 1998). However, most of these high galactic latitude stars are field stars of unknown distances. It is therefore likely that a significant fraction of them could possibly turn out to be disk objects of nearly solar compositions. A search of post-AGB stars among high galactic latitude stars could be more rewarding if we put the additional constraint of IR detection. The wavelength dependence of IR fluxes and also the detection of submillimeter fluxes could give valuable information on the circumstellar matter surrounding the evolved star. The IRAS two colour diagrams such as those published by Olnon et al. (1984), van der Veen & Habing (1988) etc., are extremely useful in separating stars with different kinds of envelopes.
In this study, we have undertaken the abundance analysis of a
selected sample of stars likely to be
post-AGB stars. From the published lists of high galactic latitude
stars (
)
(e.g. Bidelman 1990 and others)
we chose the ones with known infrared fluxes. Among them, the ones
falling into the regions VIa and VIb of Fig. 5b of
van der Veen & Habing (1988) were preferred as they were more likely
to be post-AGB stars. We have also included a few objects belonging
to the regions IIIa and IIIb that are likely to be
evolved stars with oxygen-rich envelopes.
The hot star HD 172324 was also included in spite of not being an IRAS source since it has high radial velocity (-110 km s-1) and very complex structures in hydrogen line profiles. It appeared to be a possible hot post-AGB star similar to those investigated by Conlon et al. (1993a,b).
A search for post-AGB stars among supergiant-like stars of high galactic latitude is expected to be more efficient since the possibility of forming stars at truly large distances from the galactic plane is low.
This program is also aimed at providing calibrators for photometric empirical calibrations of atmospheric abundances (Arellano Ferro & Mantegazza 1996), temperatures, and gravities in particular, since gravities are better determined from the ionization equilibrium.
This paper is organized in the following way: Sect. 2 describes the observations and data reduction; Sect. 3 discusses the methodology of abundance calculation; Sect. 4 gives an account of the sources of uncertainty in the derived abundances; in Sect. 5 the results are given and discussed for each star; in Sect. 6 these results are discussed in terms of the evolutionary status of each star while in Sect. 7 we summarize our results.
The observational material for this work was obtained during July 6 - July 12, 1999 with the 1.93 m telescope of the Haute-Provence Observatory (OHP), which is equipped with the high resolution (42000) echelle spectrograph ELODIE. Details about the performance and characteristics of the instrument have been thoroughly described by Baranne et al. (1996). We have used one spectrum of HD 172324 taken on June 1995 with the Sandiford echelle spectrograph at 2.1 m telescope of McDonald Observatory. This instrument giving a resolution of 50000 has been described in McCarthy et al. (1993). One spectrum of HD 172481 was obtained with the 2.7 m 2d coudé echelle spectrograph described in Tull et al. (1995). These spectra were reduced using spectroscopic data reduction tasks available in the IRAF package.
Table 1 contains the list of stars studied in this work, their spectral types, magnitudes, galactic positions and, when available, the IRAS infrared fluxes.
Star | Sp.T. | V | l | b | IRAS | 12![]() |
25![]() |
60![]() |
100![]() |
(mag) |
![]() |
![]() |
(Jy) | (Jy) | (Jy) | (Jy) | |||
HD 725 |
F5Ib-II | 7.08 | 117.56 | -5.19 | 00091+5659 | .36 | .25 | .40 | 14.43 |
HD 9167 | F1II | 8.19 | 127.73 | -0.97 | 01285+6115 | .47 | .25 | .40 | 8.14 |
HD 158616 | F8 | 9.69 | 13.23 | +12.17 | 17279-1119 | 3.52 | 2.90 | 1.60 | 1.98 |
HD 172324 | B9Ib | 8.16 | 66.18 | +18.58 | |||||
HD 172481 | F2Ia0 | 9.09 | 6.72 | -10.37 | 18384-2800 | 5.41 | 5.22 | .59 | 1.85 |
HD 173638 | F2Ib-II | 5.73 | 23.38 | -3.56 | 18439-1010 | 1.41 | .39 | .67 | 55.03 |
HD 218753 | A5III | 5.69 | 110.28 | -1.02 | |||||
HD 331319 | F3Ib | 9.50 | 67.16 | +2.73 | 19475+3119 | .54 | 37.99 | 55.83 | 14.76 |
HDE 341617 | A5 | 9.40 | 50.67 | +19.79 | 18062+2410 | 3.98 | 19.62 | 2.90 | 1.00 |
All spectra were bias-subtracted and flat-field corrected using standard OHP procedures described by Baranne et al. (1996). The spectra were wavelength calibrated with Th-Ar hollow cathode lamp spectra taken after each stellar exposure. More than one exposure was taken and spectra were combined to attain S/N of at least 50. The ELODIE spectrograph gives a resolution of 42000 and the wavelength coverage goes from 3906 to 6811 Å in 67 echelle orders with some overlaps in adjacent orders.
The equivalent widths were measured using the splot task of the IRAF package and their accuracy is generally better than 10% for spectra with S/N ratio larger than 50. We generally restricted ourselves to unblended weak features and avoided using lines stronger than 200 mÅ.
We have used ATLAS9 (Kurucz 1993) model atmospheres as an input to the 1997 version of LTE line synthesis program MOOG first described in Sneden (1973). The procedure assumes plane-parallel atmospheres, hydrostatic equilibrium and LTE. The oscillator strength or gf value is an important atomic datum that affects the abundance calculations. For elements C, N and O we used gf values from Wiese et al. (1996). For Fe I, the values were taken in order of preference from; Table A1 of Lambert et al. (1996), Luck's compilation (1996, private communication), and Giridhar & Arellano Ferro (1989). For Fe II lines we used the Table A2 of Lambert et al. (1996), Giridhar & Arellano Ferro (1995) and Luck's compilation (1996, private communication).
For elements other than Fe, the large compilation by Luck (1996, private communication) was preferentially used and for some heavy s-process elements gf values were taken from the work of Thévenin (1989, 1990).
In addition to abundances, the line strengths are strongly affected by
atmospheric parameters like the effective temperature (
), gravity (log g)
and turbulent velocity (
).
It is therefore necessary to determine these parameters before
using line strengths for abundance determinations.
Temperature calibrations exist that are valid for specific spectral type ranges. These methods are not only useful but also complement the spectroscopic efforts by providing initial values for the atmospheric parameters for calculating the atmospheric abundances. Here we briefly describe some of those calibrations that have been used for the stars of our sample. Later in Sect. 5, comparison with the finally adopted spectroscopic results is made in the discussion of each individual star.
Firstly, a rough estimate of
can be made from
the given spectral type and the calibration of Schmidt-Kaler (1982).
However, more accurate values can be obtained from precise
photometric colours. For our sample, we have used
photometric data and our
own unpublished calibrations for F-G stars (HD 725, HD 9167, HD 172481).
In addition, the calibration of
Napiwotzki et al. (1993) for hotter stars like HD 172324,
the 13-colour photometric system and the calibration of
Bravo Alfaro et al. (1997), and the
Geneva colour indices and the calibration of Cramer & Maeder (1979)
were used as appropriate. These empirical calibrations provide
with accuracies of
K or better and serve as excellent starting
values that are further refined by
spectroscopic approaches. Any drastic difference
between the two approaches deserves attention.
Yet another independent approach to estimate
is from the
Balmer lines profiles fitting (e.g. Arellano Ferro 1985; Venn 1995a). Theoretical Balmer profiles for grids of model atmospheres
have been calculated by Kurucz (1993). For stars of
intermediate temperature, this method does not
lead to unique
,
but rather it defines loci of possible temperatures and gravities.
On the other hand, similar loci can be found
from species where two states of ionization are well represented.
Again, the solution is not unique but rather a locus on the
-
plane is defined for each element.
This approach will be illustrated in Fig. 3 for H
,
H
,
Mg and
Si for the star HD 218753. The above solution is of special
importance for hot stars where no Fe I lines are present.
For hotter stars, lines of Fe I are not only very weak but are also
influenced by non-LTE effects. For A-F supergiants non-LTE effects could cause errors in the range of 0.2 to 0.3 dex in the iron abundance
derived using Fe I lines (Boyarchuck et al. 1985). For example, in
the well-known star Vega (A0V), the neglect of departure
from LTE for Fe I lines leads to the underestimation of Fe abundance by 0.3 dex (Gigas 1986).
For stars cooler than 7500 K the lines of Fe I and Fe II with wide range in line strengths and lower excitation potential are adequate for estimating the effective temperature, microturbulence and gravity for any given star.
The finally adopted
for our stars is that for which abundance
consistency is obtained from neutral and ionized lines of well represented species such as Fe, Ti and Cr.
Star |
![]() |
![]() |
![]() |
![]() |
V(LSR) |
![]() |
log
![]() |
(K) | (km s-1) | (km s-1) | (km s-1) | (km s-1) | |||
HD 725 |
7000 | 1.0 | 4.65 | -56.9 | -48.8 | 0.8 | 4.2 |
HD 9167 | 7250 | 0.5 | 4.20 | -45.7 | -40.2 | 1.1 | 4.2 |
HD 158616 | 7300 | 1.5 | 4.6 | +68.8 | +78.6 | 2.1 | 4.5 |
+63.7 | +78.5 | 1.5 | |||||
HD 172324 | 11000 | 2.5 | 5.0 | -126.1 | -106.4 | 1.1 | 2.7 |
11500 | 2.5 | 7.5 | -117.3 | -97.5 | 2.5 | ||
HD 172481 | 7250 | 1.5 | 4.60 | -73.1 | -76.9 | 1.8 | 4.1, 4.5 |
7250 | 1.5 | 5.10 | -84.4 | -74.0 | 2.1 | ||
HD 173638 | 7500 | 1.5 | 4.30 | +11.6 | +26.9 | 1.2 | 4.5 |
HD 218753 | 8000 | 2.0 | 3.35 | +3.2 | +13.9 | 1.0 | 1.6 |
HD 331319 | 7750 | 1.0 | 5.35 | -2.5 | +15.8 | 1.5 | 4.5 |
HDE 341617 | 23000 | 3.0 | 15.00 | +67.9 | +87.8 | 2.9 | 4.6 |
A good discussion of atmospheric parameters determination for A type
stars can be found in Venn (1995a), who points out
that H
and
H
,
being very sensitive to temperature and gravity
in A type stars, provide a locus of possible temperature-gravity pairs,
and that ionisation equilibrium of Mg I and
Mg II gives another useful locus of temperature-gravity pair as
the non-LTE effects are expected to be very small in magnesium lines.
Since ionisation equilibrium of Si I and Si II give a temperature-gravity
pair very similar to that given by Mg I and Mg II, the latter
can also serve as yet another indicator of these parameters.
Intersection of the above mentioned loci could lead to reliable
temperature and gravity for each star, as demonstrated in Fig. 3.
The hydrogen lines were distorted in many of the program stars
due to underlying emission,
and therefore could not be used to derive temperature-gravity loci.
We used excitation equilibrium of Fe I lines to get a preliminary estimate of
.
It was followed by ionisation equilibrium
of Mg I/Mg II, Si I/Si II and Cr I/Cr II
to arrive at a satisfactory estimate of
and
.
For HD 725,
HD 9167, HD 158616, HD 172481 and HD 173638 the excitation equilibrium of
Fe I lines (requiring derived abundances to be independent
of the lower excitation energy of the lines) gave very good estimates
of the temperature which were further verified using lines
of other species, as mentioned above. Similarly, for gravities,
the values giving a good consistency for neutral and ionised Mg,
Ti, Cr and Fe were adopted.
The star HD 172324 required an altogether different approach as described in Sect. 5.4.
All our program stars turned out to be hotter than 7000 K (see Table 2). For hotter stars, Fe I lines were difficult to measure. The Fe II lines on the other hand, had good range in equivalent widths. We therefore relied upon Fe II lines to derive microturbulence. The microturbulence was derived by requiring that weak, medium and strong lines give a consistent value of abundance.
The final atmospheric parameters derived for the program stars are
given in Table 2,
along with their radial velocities relative to the
Sun and to the Local Standard of Rest (LSR).
The log
values in Table 2 were estimated from the
effective temperatures determined spectroscopically,
and the calibration of
Schmidt-Kaler (1982). For HD 172481 a red spectrum obtained at
McDonald Observatory in May, 2000,
allowed us to measure the three components of the OI feature near 7774 Å.
The combined equivalent width
W(7774) = 1.3 Å and the
calibration of Arellano Ferro et al.
(1991) lead to
= -5.6 or log
= 4.1,
which is in good agreement with the value 4.5
obtained from Schmidt-Kaler's calibration. For homogeneity we have adopted
the latter value for our discussion about the evolutionary status
of this object in Sect. 6.
The uncertainties in the derived abundances are caused by errors in the determination
of the atmospheric parameters, in the equivalent width measurements, and
also in the quality of oscillator strengths.
For spectra with S/N ratios larger than 50
the errors in the equivalent widths are between 5 and 8%.
The errors in gf values vary from element to element. For Fe I lines,
experimental values of good accuracies (better than 10%) do exist,
for other Fe-peak
elements the range in errors could be within 10 to 25%. For heavier elements,
particularly for s-process elements, the errors could be larger than 25%.
For the stars HD 725, HD 158616, HD 172481, HD 173638, HD 218753
and HD 331319 we could measure a very large number of unblended lines, and the estimated errors in
,
and
are
K,
and
km s-1, respectively.
The sensitivity of the
derived abundances to changes in the model atmospheric parameters
are described in Table 4 of Gonzalez et al. (1997) for two RV Tau stars.
We have used the same grid of atmospheric models and the same database
for line oscillator strengths, hence the procedure will not be repeated here.
For the Fe-peak elements we could measure a sufficiently large number
of lines and the gf values used being of good quality, we expect these
abundances to
be accurate within 0.2 to 0.25 dex. For heavier elements, particularly
the s-process elements,
the uncertainty could be above 0.3 dex. Similarly for light elements like
oxygen where few lines are available the uncertainty could be above 0.3 dex.
For HD 172324 and HDE 341617, we will discuss the uncertainties
in their respective sections.
This star is an IRAS source (00091+5659).
It was classified as F5Ib-II
by Griffin & Redman (1960) suggesting a
temperature of 6900 K if we follow the calibration of
Schmidt-Kaler (1982).
Using the uvby photometry of Perry (1969),
Olsen (1983), Hauck & Mermilliod
(1998), reddening free colours and our own
unpublished calibrations for F-G supergiant stars, we estimated
K. Balmer line fitting was not performed because the profiles
display complex structure and
underlying emission is suspected.
Species |
![]() |
[X/H] | s.d. | N | [X/Fe] |
C I | 8.55 | -0.38 | ![]() |
3 | -0.08 |
Na I | 6.32 | +0.21 | ![]() |
3 | +0.51 |
Mg I | 7.58 | -0.18 | ![]() |
4 | +0.12 |
Si I | 7.55 | +0.05 | ![]() |
2 | +0.35 |
Si II | 7.55 | +0.12 | 1 | +0.42 | |
S I | 7.21 | -0.10 | ![]() |
3 | +0.20 |
Ca I | 6.35 | -0.16 | ![]() |
12 | +0.14 |
Sc II | 3.13 | -0.03 | ![]() |
7 | +0.27 |
Ti II | 4.98 | -0.31 | ![]() |
6 | -0.02 |
Cr I | 5.67 | -0.16 | ![]() |
7 | +0.14 |
Cr II | 5.67 | -0.19 | ![]() |
11 | +0.11 |
Mn I | 5.39 | -0.27 | ![]() |
6 | +0.03 |
Fe I | 7.51 | -0.26 | ![]() |
51 | |
Fe II | 7.51 | -0.33 | ![]() |
11 | |
Ni I | 6.25 | +0.04 | ![]() |
3 | +0.33 |
Y II | 2.23 | +0.12 | ![]() |
3 | +0.42 |
Zr II | 2.60 | -0.07 | ![]() |
2 | +0.22 |
Ba II | 2.13 | +0.15 | 1 | +0.45 | |
Ce II | 1.58 | -0.17 | ![]() |
2 | +0.13 |
Notes - The solar abundances are taken from Grevesse et al. (1996).
- N is the number of lines included in the calculation.
The finally adopted parameters are
K,
and
km s-1. We relied upon Fe II lines for calculating
microturbulence velocity. A large number of Fe I lines were measured
and used in estimating
.
Also
neutral and ionized lines
of Ti and Cr were employed to derive a satisfactory pair of
and
values.
A competing solution could have been
K,
but the adopted parameters gave
marginally better consistency in the abundances of neutral and ionized lines.
HD 725 appears to be very marginally metal-poor (Table 3) and
it has a moderately high radial velocity of -57 km s-1.
The elemental abundances relative to Fe, i.e. [X/Fe] = [X/H]-[Fe/H]
,
given in the last column of
Table 3 and subsequent tables, were calculated adopting the average value
of [Fe/H] from Fe I and Fe II lines.
For HD 725 the [X/Fe] values are similar
to those in normal unevolved stars for many elements. [Na/Fe] = +0.5 dex
indicates relative enrichment of Na which is a well-known feature of
A-F supergiants (Takeda & Takada-Hidai 1994; Venn 1995a,b).
But Na I abundances are likely to be affected by non-LTE effect.
Non-LTE analysis of Na I lines has been done by Gigas (1986),
Takeda & Takada-Hidai (1994) and others. The errors introduced
by the neglect of non-LTE becomes more severe for higher temperatures.
According to Takeda & Takada-Hidai (1994), the
log
in Na I lines at 5682, 5688, 6154 and 6160 Å is -0.09, -0.10,
-0.07 and -0.07 dex respectively at temperature 7500 K. At temperature
7000 K the correction is 0.01 dex smaller for all lines than the
values mentioned above. According to Gigas (1986) the non-LTE
correction could be +0.1 to +0.2 dex. The use of [Na/Ca]
instead of [Na/Fe] is recommended by Lambert (1992) for LTE
calculations. The [Na/Ca] of +0.4 dex found from our analysis shows
that Na enrichment appears to be real. The Na might have been synthesized
in the H-burning region where the NeNa cycle might operate together
with the CNO cycle. The suggestion that the proton capture on 22Ne
could lead to enhancement of 23Na is followed up by
Langer et al. (1993). These authors used a nuclear reaction network
to examine the changes in abundances caused by proton capture at
T9 =0.040. Mixing of this region just below the oxygen shell
over a timescale of 30000 yr would cause enhancement of
14N, 23Na and 27Al
at the expense of 16O, 22Ne, 25Mg and
26Mg. These authors also suggested that the abundant 20Ne could
also be transformed into 23Na on longer timescales, and
pointed out that the depletion of 25Mg and 26Mg would not modify
the Mg abundance.
Globular cluster giants are known to display Na-O anticorrelation
as reported by Sneden et al. (1991) and Kraft et al. (1992).
Since our spectrum
does not go to wavelengths longer than 6800 Å,
we could not measure N I abundance nor could we measure the O abundance.
In metal-poor stars, relative enrichment of
elements is
to be expected but the effect becomes evident for [Fe/H] < -0.5 dex.
At [Fe/H] -0.2 to -0.3 dex the spread in observed abundances is
large and a large number of stars have [
.
For HD 725, the
element Si shows small enhancement
but the number of lines used are woefully small to make a
definite claim.
Among Fe-peak elements, Ni, represented by 3 Ni I lines,
appears to be enriched, with [Ni/Fe]
of +0.3 dex. HD 218753 and HD 173638 of our sample show a
positive [Ni/Fe] but the value is not above abundance
errors.
As such, for HR 725 the value is slightly above twice the
standard error, nevertheless
a more extensive analysis based on a larger number of lines is
required to see if the enrichment is real.
Luck & Bond (1983, 1985) have reported [Ni/Fe]
for
metal-poor star. Wheeler et al. (1989)
on the other hand report very large scatter in [Fe/H] vs. [Ni/Fe]
relation. These authors suggest that non-zero [Ni/Fe] can be
observed at all metallicities.
Another interesting finding is [Y/Fe] of +0.4 dex.
The three Y II lines used are quite well separated and have good
estimates of oscillator strengths,
but out of the three lines, one is a little
strong. The same is true for the Ba II line used.
Mild enrichment of s-process elements in the moderately metal-poor
star HD 70379 has already been reported (Reddy 1996). Hence, our average
[s/Fe] ratio +0.3 does not come as a surprise. In addition,
its radial velocity
of -57 km s-1 lends support to our view that it is a
low-mass evolved object.
These results are highly suggestive though not conclusive indicators of
evolution beyond the red giant branch.
However, making use of its proper motions and
parallax from the Hipparcos catalogue we have calculated
the galactocentric velocities
km s-1,
km s-1 and
Z = +5.4 km s-1 that indicate a space velocity of
193.2 km s-1with a small pitch angle of 9.7
relative to the
circular orbit and on the
galactic plane. This indicates that the star is at a lower galactic
latitude than the Sun and placed in
a mildly eccentric orbit.
This star has infrared flux and is an IRAS source (01285+6115).
It appears to be another moderately metal-poor star (Table 4).
We did not find any remarkable abundance peculiarity for this object.
With radial velocity of -45 km s-1 and [Fe/H] of -0.3 dex,
one could be optimistic of seeing positive [/Fe].
Unfortunately, we could not measure good Si I and Si II lines and Mg, Ca and Ti
do not show any enrichment. But on the other hand, for stars with
[Fe/H] in the
range of 0.0 to -0.5 dex, the observed abundance ratios of
-process
elements have very
large scatter, hence finding evolutionary changes is
almost as probable as not finding them. Likewise HD 725, rather large
radial velocity implies a space velocity of 208.2 km s-1with a small pitch angle of 5.7
relative to the circular orbit and on the
galactic plane. The orbit is even less eccentric than that of HD 725 and it is
at a lower galactic latitude than the Sun.
Species |
![]() |
[X/H] | s.d. | N | [X/Fe] |
Mg I | 7.58 | -0.37 | ![]() |
2 | -0.04 |
Ca I | 6.35 | -0.22 | ![]() |
6 | +0.12 |
Sc II | 3.13 | -0.28 | ![]() |
3 | +0.05 |
Ti II | 4.98 | -0.48 | ![]() |
10 | -0.15 |
Cr I | 5.67 | -0.19 | 1 | +0.15 | |
Cr II | 5.67 | -0.27 | ![]() |
9 | +0.07 |
Mn I | 5.39 | -0.35 | 1 | -0.02 | |
Fe I | 7.51 | -0.32 | ![]() |
29 | |
Fe II | 7.51 | -0.35 | ![]() |
10 | |
Y II | 2.23 | -0.23 | ![]() |
3 | +0.11 |
Ba II | 2.13 | -0.22 | ![]() |
2 | +0.12 |
Notes - same as Table 3.
This star is an IRAS source (17279-1119) with significant infrared fluxes at shorter wavelengths.
The spectral type as listed in the SAO catalogue is F8, which suggests a
temperature between 6100-6200 K (Schmidt-Kaler 1982),
depending upon the luminosity class. No photometric data
are available and hence no other temperature estimate was made.
Two spectra were obtained for this star at the OHP. The S/N for these two
spectra are 34 and 53. Since the spectrum from July 7 is better,
it was decided to use it to determine
,
and
,
complete the abundance analysis and
then simply use the same parameters on the lower S/N spectrum
from July 6 to verify the abundance pattern. The results are given in Table 5. The
second entries for each species are for the lower S/N spectrum. One can see
that the results from both spectra are in a good agreement.
Species |
![]() |
[X/H] | s.d. | N | [X/Fe] |
C I | 8.55 | -0.25 | ![]() |
4 | +0.33 |
-0.23 | ![]() |
4 | +0.35 | ||
O I | 8.87 | -0.54 | ![]() |
2 | +0.04 |
-0.55 | 1 | +0.03 | |||
Na I | 6.32 | +0.05 | ![]() |
3 | +0.63 |
-0.05 | 1 | +0.49 | |||
Mg I | 7.58 | -0.40 | ![]() |
3 | +0.18 |
-0.56 | 1 | -0.02 | |||
Si I | 7.55 | +0.03 | ![]() |
3 | +0.61 |
Si II | 7.55 | -0.06 | ![]() |
2 | +0.52 |
+0.04 | ![]() |
2 | +0.58 | ||
S I | 7.21 | +0.08 | ![]() |
6 | +0.66 |
+0.10 | ![]() |
2 | +0.64 | ||
Ca I | 6.35 | -0.36 | ![]() |
12 | +0.22 |
-0.34 | ![]() |
9 | +0.20 | ||
Sc II | 3.13 | +0.00 | ![]() |
8 | +0.58 |
-0.09 | ![]() |
4 | +0.45 | ||
Ti I | 4.98 | +0.08 | ![]() |
2 | +0.66 |
+0.18 | 1 | +0.72 | |||
Ti II | 4.98 | -0.01 | ![]() |
13 | +0.57 |
-0.13 | ![]() |
8 | +0.41 | ||
Cr I | 5.67 | -0.55 | 1 | +0.03 | |
Cr II | 5.67 | -0.39 | ![]() |
14 | +0.19 |
-0.47 | ![]() |
7 | +0.07 | ||
Mn I | 5.39 | -0.17 | 1 | +0.41 | |
Fe I | 7.51 | -0.58 | ![]() |
39 | |
-0.61 | ![]() |
20 | |||
Fe II | 7.51 | -0.57 | ![]() |
19 | |
-0.51 | ![]() |
7 | |||
Ni I | 6.25 | -0.41 | ![]() |
4 | +0.17 |
-0.39 | 1 | +0.19 | |||
Zn I | 4.60 | -0.48 | ![]() |
2 | +0.10 |
-0.40 | 1 | +0.18 | |||
Y II | 2.23 | +0.37 | ![]() |
4 | +0.95 |
+0.48 | ![]() |
2 | +1.02 | ||
Ba II | 2.13 | +0.04 | ![]() |
3 | +0.62 |
+0.10 | ![]() |
2 | +0.64 | ||
La II | 1.21 | -0.11 | 1 | +0.47 | |
Ce II | 1.58 | +0.13 | ![]() |
5 | +0.71 |
+0.21 | 1 | +0.75 |
Notes - same as Table 3.
- Second entries are results from a lower S/N spectrum.
HD 158616 was also studied by Van Winckel (1995, 1997). While he
had better data for C, N, O due to extended coverage in the long wavelength
region,
for other elements, our spectra contained more lines per element,
and more elements are included.
This star is Fe-poor by a factor of 4 or so and
shows very clear indications of CNO processing and
enrichment of s-process elements.
We get
whereas Van Winckel (1995) got this
ratio significantly larger than one (see Table 14).
His carbon abundance is based on more lines in the 7100 Å
region. His choice of
is also hotter than our adopted value
that can also account for the higher carbon abundance derived. Van
Winckel (1995) found [N/Fe] of +0.2 dex. This clearly shows that the star has
gone through CNO cycle and its products have been brought to the surface.
The carbon enrichment could be caused by the helium-shell burning
when oxygen is also manufactured.
The enhancement of Si and S could be
present in ISM from which the star is formed.
With the [Fe/H] of -0.6 dex, the star is moderately metal-poor
and therefore it is possible that the parent
ISM might have received ejecta from type II SNe.
Although the effect of departure from LTE has been discussed for
the light elements C, N, O and also for Mg by different investigators, we
did not come across similar discussion on Si and S. Hence, at this stage,
we chose not to offer any detailed explanation.
The most interesting feature of the derived abundances is definitely the
enrichment of s-process elements Y, Ba, La and Ce.
This star is undoubtedly a post-AGB star that has brought the products
of helium burning as well as elements formed by s-processing to the surface.
Our analysis covers the light s-process element Y (one of the
three elements referred as ls) and the
heavy s-process elements Ba, La and Ce, representing
heavy (hs) s-process elements. We have made an estimate of
[hs/ls]. We have not corrected the ls-index for the lack of
light elements Sr and Zr since for light elements the odd-even effect is not
strong as pointed out by Van Winckel & Reyniers 2000).
We estimated [hs/ls] = -0.3 and [ls/Fe] of +1.0.
When plotted on the [hs/ls] vs. [ls/Fe] plot of Busso et al. (1999),
(their Fig. 7 giving theoretical predictions),
we found
mbarn-1.
Incidentally, the data point falls near the thick line
which for solar metallicity would indicate C/O = 1 but for [Fe/H]
of -0.6, it indicates a C/O
3, whereas we get C/O
1.
This reduction of carbon abundance, while hs and ls indices point
to larger C/O added to small but significant enhancement of nitrogen, as
reported by Van Winckel (1995),
strongly favour the hot bottom burning scenario described and discussed
in Sect. 5.5.
More extensive coverage of s-process elements
will enable a meaningful comparison with third dredge-up models
developed by Straniero et al. (1995) and Busso et al. (1995).
Another star of similar temperature and showing a similar trend in abundances is HR 6144 (Luck et al. 1990), however, in this star, the s-process enhancement is not so significant and C/O is less than 1.
![]() |
Figure 1:
H![]() ![]() |
Open with DEXTER |
This star has been classified as B9Ib by Morgan & Roman (1950) which suggests a temperature of 10280 K (Schmidt-Kaler 1982). The Strömgren colours (Hauck & Mermilliod 1998) however point towards higher temperature: 13100 K using the calibration of Napiwotzki et al. (1993). An independent temperature calibration of the Geneva photometric system (Cramer & Maeder 1979) gives a temperature of 13215 K.
The He I lines have been used to estimate
and luminosity class
of the star.
Didelon (1982) gives very useful plots of the dependence of
many He I, Si II, Mg II, C II, O II and N II line strengths on the
spectral type and luminosity class.
The equivalent widths in our spectrum for the He I lines at 4120, 4143, 4387
and 4471 Å very clearly suggest a
spectral type of B9. A luminosity class Ib was suggested by the strengths
of Si II line at 4128 Å, Mg II line at 4481 Å and C II
feature at 4267 Å, this
is in good agreement with the spectral type above.
An estimate of
has been made by requiring the He I
lines to give solar
abundance.
The best estimate is 11500 K. Given the class Ib,
must not be very different from 2.0. In any case, at the high
temperature end the Kurucz (1993) models do not reach very low gravities.
Fortunately, Mg I and Mg II lines are present in the OHP
spectrum and Si II and Si III lines can be measured on the McDonald spectrum.
Our derived
and
appear to be good estimates for
the epoch of OHP spectrum. However there is indication that at the epoch at which
the McDonald spectrum was taken, the gravity was somewhat lower.
Species |
![]() |
[X/H] | s.d. | N | [X/Fe] |
He I | 10.99 | -0.08 | ![]() |
4 | +0.54 |
He I* | 10.99 | -0.19 | ![]() |
12 | +0.44 |
C II* | 8.55 | -1.30 | syn | -0.68 | |
O I | 8.87 | +0.41 | ![]() |
2 | +1.03 |
O I* | 8.87 | +0.26 | ![]() |
4 | +0.89 |
Ne I* | 8.09 | +0.05 | 1 | +0.68 | |
Mg I* | 7.58 | -0.63 | 1 | 0.00 | |
Mg II | 7.58 | -0.66 | ![]() |
2 | -0.04 |
Mg II* | 7.58 | -0.65 | ![]() |
3 | -0.02 |
Al II | 6.47 | -0.59 | 1 | +0.03 | |
Al II* | 6.47 | -0.65 | 1 | -0.02 | |
Si II | 7.55 | -0.16 | ![]() |
2 | +0.47 |
Si II* | 7.55 | -0.29 | ![]() |
6 | +0.39 |
Si III | 7.55 | +0.25 | 1 | +0.88 | |
S II | 7.21 | -0.19 | 1 | +0.43 | |
S II* | 7.21 | -0.47 | 1 | +0.16 | |
Ti II | 4.98 | -0.03 | ![]() |
8 | +0.59 |
Ti II* | 4.98 | -0.28 | ![]() |
3 | +0.35 |
Cr II | 5.67 | -0.43 | ![]() |
11 | +0.19 |
Cr II* | 5.67 | -0.48 | ![]() |
3 | +0.15 |
Fe II | 7.51 | -0.62 | ![]() |
17 | |
Fe II* | 7.51 | -0.63 | ![]() |
11 |
-
= 11000 K,
= 2.5 and
= 7.00 km s-1 for McD spectrum.
-
= 11500 K,
= 2.5 and
= 5.40 km s-1 for OHP spectrum.
* Result from OHP spectrum.
This star appears to be deficient in Fe by a factor of 3-4 and
has a large radial velocity of -110 km s-1 making it a likely
halo or old disk object.
Carbon abundance is very important in ascertaining the evolutionary
status. We could observe only the blend at 4267 Å while supposedly
strong lines at 6578 and 6582 Å were too weak to be measured.
By computing the blend of two C II lines at 4267 Å we find
[C/H] of -1.3 dex, for which Takeda et al.
(1996) found zero non-LTE correction. In the neighbourhood of
10000 K the non-LTE abundance correction for carbon
using C I lines is
-0.4 dex (Venn 1995b). Our iron abundance is based
on Fe II lines that are not strongly affected by non-LTE effects.
For O I line at 6156-6158 Å the non-LTE correction is
-0.3 dex (Takeda & Takada-Hidai 1998).
For A-type supergiants of solar metallicity, Venn (1995a) found
a mean enrichment of 0.6 dex for Na and
0.3 dex for
S. Venn (1995b) reported CNO abundances for the same sample after
applying non-LTE corrections to the derived abundances.
The mean values found were: [C/H] = -0.4 dex, [N/H] = +0.08 dex and [O/H] = -0.2 dex.
Nevertheless, the hottest star of Venn's sample, HD 161695, is about
1500 K cooler than HD 172324.
McErlean et al. (1999) have plotted LTE and non-LTE line profiles for a range of temperatures 10000 K to 35000 K. At 11000 K the non-LTE correction for C II lines at 4267 Å is very small, in agreement with the prediction of Takeda et al. (1996). Hence our values [C/H] = -1.3 dex and [C/Fe] = -0.68 dex are realistic estimates.
For an A-type star of solar metallicity, a mean value [C/H] = -0.4 was reported by Venn (1995b), whereas for B supergiants McErlean et al. (1999) report mean values of [C/H] = -0.35 dex and [O/H] = -0.32 dex. After applying non-LTE correction for oxygen we get [O/H] of +0.1 dex and [O/Fe] of +0.7 dex. Our derived carbon and oxygen abundances in Table 6 are much different from what is expected for a young B9 supergiant. It has been suggested by Boothroyd & Sackmann (1999) that the carbon deficiency can also be caused by deep circulating mixing below the base of the convective envelope followed by cool bottom processing (CBP) of the CNO isotopes. They also showed that the CBP became more extensive at reduced metallicities or at low masses. The high radial velocity for HD 172324 (more than 100 kms-1) and significantly low [Fe/H] makes it very likely that it has experienced CBP.
The only trace of an odd Z element we could observe was
a single line of Al I, providing [Al/Fe]
0. One does
not see [Al/Fe]
+0.30 dex reported by Edvardsson et al. (1993),
but with single line being used in our study not much significance
could be attached to our estimated [Al/Fe].
Hot stars at high galactic latitude were studied by Conlon et al. (1993a) who found very large Fe and C deficiencies in them. But the stars studied by these authors are much hotter than HD 172324. Neverthless, the abundance pattern of HD 172324 is similar to those studied by Conlon et al. (1993a,b) and McCausland et al. (1992). This star being most likely an oxygen-rich post-AGB star deserves an extended analysis covering CNO and as significant spectral variations can be seen in four years (see Fig. 1), a monitoring of hydrogen line profiles over long time scales will be of interest.
This star shows light variations of very small amplitude, 0.15 mag
(Van Winckel 1995).
The spectral energy distribution of this star
has an unusual multi-peaked shape (Bogart 1994).
It was included in the study of Van Winckel (1995)
who, by fitting the observed flux distribution to that of Kurucz
(1993) model atmosphere, derived
= 7000 K. Van Winckel also found
that the strength of emission components in hydrogen lines varied strongly.
From the study of radial velocity variation spread
over a decade, he reported that
there is not enough evidence for the binarity of the
star. However, his spectra show considerable line splitting attributed
to the passage of a shock.
Fortunately, we obtained the spectrum of HD 172481
when the atmosphere of the star was stable and therefore
no line splitting was observed, as can be seen in the Fig. 2.
Species |
![]() |
[X/H] | s.d. | N | [X/Fe] |
Li I | 1.16 | +2.54: | 1 | +3.16: | |
C I | 8.55 | -0.62 | ![]() |
12 | -0.01 |
N I | 7.97 | -0.63 | ![]() |
3 | -0.02 |
O I | 8.87 | -0.58 | ![]() |
2 | +0.04 |
Mg I | 7.58 | -0.13 | ![]() |
2 | +0.48 |
Mg II | 7.58 | -0.06 | ![]() |
3 | +0.55 |
Si I | 7.55 | -0.05 | ![]() |
6 | +0.57 |
Si II | 7.55 | -0.10 | ![]() |
3 | +0.52 |
S I | 7.21 | -0.04 | ![]() |
7 | +0.58 |
K I | 5.12 | -0.28 | 1 | +0.34 | |
Ca I | 6.35 | -0.28 | ![]() |
12 | +0.34 |
Sc II | 3.13 | -0.20 | ![]() |
6 | +0.41 |
Ti I | 4.98 | -0.31 | 1 | +0.31 | |
Ti II | 4.98 | -0.28 | ![]() |
6 | +0.34 |
V II | 4.00 | -0.00 | ![]() |
2 | +0.62 |
Cr I | 5.67 | -0.34 | ![]() |
3 | +0.28 |
Cr II | 5.67 | -0.41 | ![]() |
10 | +0.21 |
Mn I | 5.39 | -0.51 | ![]() |
3 | +0.11 |
Fe I | 7.51 | -0.62 | ![]() |
43 | |
Fe II | 7.51 | -0.61 | ![]() |
13 | |
Ni I | 6.25 | -0.31 | ![]() |
6 | +0.30 |
Zn I | 4.60 | -0.23 | ![]() |
2 | +0.39 |
Y II | 2.23 | +0.08 | ![]() |
4 | +0.69 |
Zr II | 2.60 | -0.14 | 1 | +0.46 | |
Ba II | 2.13 | +0.03 | ![]() |
2 | +0.65 |
La II | 1.21 | -0.55 | ![]() |
2 | +0.07 |
Ce II | 1.55 | -0.24 | ![]() |
7 | +0.38 |
Nd II | 1.50 | +0.03 | ![]() |
3 | +0.64 |
Eu II | 0.51 | +0.24 | 1 | +0.86 |
Note - same as Table 3.
Sadly, the S/N ratio of our spectrum is not very high. We could
measure very few lines of important elements like C and O,
hence we were not satisfied with the limited
data to carry out abundance analysis.
But it was known beyond doubt that the star is highly evolved since we could
identify lines of C I and also saw Li I line at 6708 Å. However,
the Li I feature was falling at the end of our CCD frame
and was showing distinct doubling. One component coming nearest to Li I
wavelength gave log (Li) of 1.8.
But S/N being very poor at the end of the CCD frame, we decided
to follow this object with more spectra.
At our request, David Yong of McDonald Observatory got a spectrum
using the 2d coudé echelle spectrograph at the 2.7 m telescope of McDonald
Observatory on May 13, 2000. The spectrum has resolution
of 30000 and wide spectral coverage from 3900 Å to 10200 Å.
In this spectrum, we found Li I feature to be single with some asymmetry
in the blue wing but much deeper than in July 1999.
In all HD 172481 spectra, the H
has a broad absorption,
a narrow absorption and a possible red shifted emission component.
The H
also has a broad absorption and a narrow
absorption at the centre of broad absorption. There is no
indication of emission component.
The H
has a complex profile with one shallow absorption,
one deep absorption that has emission components in both the wings.
The blue emission component is stronger than the red one.
The extensive spectral coverage of McDonald spectrum enabled us to measure a
large number of unblended lines for several light and heavy elements.
As one can see from the Table 7, we could carry out a very comprehensive
analysis of this object.
![]() |
Figure 2: Three spectral regions in the spectrum of HD 172481 clearly showing no line splitting. Hence we believe the star was in a stable phase |
Open with DEXTER |
From Fe I and Fe II lines we derived
= 7250 K and
= 1.5
and was supported by Si I, Si II, Mg I and Mg II lines.
We derived the Li abundance by spectrum synthesis. All the four
components of Li I feature at the 6708 Å region were included.
We find log
(Li) of +3.7, which is surprisingly high.
We were puzzled by the change in appearance of Li I feature at 6707,
so on August 11 one more spectrum was obtained with the same set-up
and by the same observer.
The spectrum again showed a suggestion of doubling at the line core
though the components were not well separated. It is not clear if the
line is splitting periodically or the emission at the core is causing
it to appear double. The overall strength of Li I feature in the
August spectrum has reduced. For May 2000 spectrum,
our estimated Li abundance (derived by synthesis) is
shown in Table 7 with a colon. In the light of the large variation exhibited
by Li I feature in strength as well as in profile shape, this value
should be regarded with caution. However, the presence of Li I feature
in the spectrum cannot be refuted. Another Li I feature at 6103 Å
fell in between the echelle orders and therefore could not be used.
We could measure a large number of C I lines to estimate the carbon abundance.
The three N I lines in the near infrared also enabled us to derive the
nitrogen abundance. We get [N/Fe]
for HD 172481 whereas for
HD 158616 [N/Fe]= +0.3 is reported by Van Winckel (1995).
The estimated C/O is +0.43.
The element Li is considered a fragile element that gets destroyed
in the course of evolution. The primordial abundance of Li (based
on population II objects) is considered near log
(Li) = 2.2. The excess abundance
must therefore be caused by AGB evolution of HD 172481 or might
owe its origin to binarity.
Our analysis covers light s-process elements (ls) Y and Zr and heavy s-process elements (hs) Ba, La, Ce and Nd. We derive a mean [ls/Fe] of 0.6 and mean [hs/Fe] of 0.4. That leads to [hs/ls] of -0.2. With this value of [hs/ls] and [Fe/H] of -0.6 this star is remarkably similar to IRAS 04296+3429 and IRAS 19500-1709 studied by Van Winckel & Reyniers (2000), although [ls/Fe] and [hs/Fe] are much larger for these two stars.
The stars mentioned above and HD 158616 are very interesting post-AGB
objects as they are, most likely, evolved from intermediate-mass stars (IMS).
According to Travaglio et al. (1999), stars in the
mass range 4-8 ,
activate 22Ne(
,
n)25Mg reaction during their TP-AGB
phase more effectively than the low-mass stars due to the high
temperatures reached at the bottom of the convective pulse
(
3.5 108 K).
IMS contribute more to the first s-peak represented
by the elements Sr, Y and Zr. Actually, the number of known
post-AGB IMS is very small.
For IMS, the formation of a 13C
pocket is less certain because of the reduced mass of the
H-He intershell
by about one order of magnitude. It is shown by Straniero et al.
(1997) and Gallino et al. (1998) that the 13C neutron source
active
during the interpulse phase of low-mass TP-AGB accounts for most
of the
production of the second s-peak elements Ba, La, Ce, Sm
and Eu.
It is obvious from the relative enhancement of Y and Sr presented
in Tables 5 and 7 that HD 158616 and HD 172481 belong
to the relatively rare post-AGB IMS.
We would therefore try to understand the observed abundances of
HD 172481 in the framework of AGB models developed by Lattanzio and
others for IMS.
Lattanzio (1997) in his AGB calculation has predicted
that for stars more massive than 4
the bottom of the
convective envelope penetrates into the hotter regions of the
envelope where proton captures already modified the original CNO composition.
This is called "hot bottom burning'' (HBB) and results in
many important changes in chemical composition of the envelope.
Lattanzio (1997) predicted the production of Li by the
Cameron-Fowler mechanism operating at bottom of the envelope.
Sackmann & Boothroyd (1992) showed that log
(Li)
4.5 could be produced in stars with bolometric
magnitude between -6 and -7 when the temperature at the base of the
convective envelope exceeds
50 106 K.
From the study of AGB stars in SMC and LMC, Smith et al.
(1995) found them to have bolometric
magnitudes in the range -6 to -7.2 and to
show lithium values of log
(Li)
1.0 - 4.0.
However, these are cool luminous S stars.
Lattanzio (1997) also predicted the destruction of carbon via CN cycle
that could prevent C/O ratio from exceeding one.
Theoretical models for AGB stars of mass 4, 5 and 6
computed by Boothroyd et al. (1993)
encountered HBB with a temperature at the base of the convective
envelope reaching 80 106 K. These models predict C/O of 0.4 to
0.5 for
103 yr on the AGB.
Species |
![]() |
[X/H] | s.d. | N | [X/Fe] |
C I | 8.55 | -0.16 | ![]() |
5 | -0.09 |
Mg I | 7.58 | -0.05 | ![]() |
5 | +0.03 |
Si I | 7.55 | +0.36 | ![]() |
2 | +0.44 |
Si II | 7.55 | +0.41 | 1 | +0.49 | |
Ca I | 6.35 | +0.04 | ![]() |
12 | +0.12 |
Ca II | 6.35 | -0.03 | 1 | +0.05 | |
Sc II | 3.13 | +0.16 | ![]() |
6 | +0.24 |
Ti I | 4.98 | +0.01 | 1 | +0.09 | |
Ti II | 4.98 | -0.1 | ![]() |
17 | -0.04 |
Cr I | 5.67 | +0.08 | ![]() |
3 | +0.16 |
Cr II | 5.67 | -0.02 | ![]() |
15 | +0.06 |
Mn I | 5.39 | +0.00 | 1 | -0.08 | |
Fe I | 7.51 | -0.07 | ![]() |
62 | |
Fe II | 7.51 | -0.08 | ![]() |
19 | |
Ni I | 6.25 | +0.06 | ![]() |
7 | +0.14 |
Zn I | 4.60 | -0.06 | ![]() |
2 | +0.02 |
Y II | 2.23 | +0.02 | ![]() |
5 | +0.10 |
Zr II | 2.60 | -0.02 | 1 | +0.06 | |
Ba II | 2.13 | +0.15 | ![]() |
2 | +0.23 |
Ce II | 1.58 | +0.02 | 1 | +0.10 | |
Nd II | 1.48 | +0.11 | 1 | +0.19 |
Note - same as Table 3.
The abundance pattern of HD 172481 bears some resemblance to those
found for HR 7671 though the latter is more metal-poor.
Interestingly, HR 7671 also shows the Li I feature though Li
is not as overabundant as in HD 172481.
The estimated C/O for HR 7671 is 0.4. The mean [/Fe] is
lesser than what we find for HD 172481 but [s/Fe] is comparable.
The existence of objects like HD 172481 and HR 7671 lend further support to the HBB scenario, put forward to explain the paucity of carbon-rich stars among AGB stars. The observed variation of Li I feature in HD 172481 makes it a very promising candidate for binarity search.
While the present paper was under the refereeing process, the referee
called our attention to the
then unpublished work on HD 172481 by Reyniers & Van Winckel
(2001). Thus a comparison with their results is most appropriate.
These authors have derived atmospheric parameters (
K and
= 1.5) that are in excellent agreement with those derived by us.
A small difference in
of 0.6 km s-1 is seen. These authors
also find a large lithium abundance similar to our finding. The [Fe/H]
and other Fe-peak elements have very good agreement. The s-process
elements La, Nd and Eu however, show some disagreement.
We have measured 3 lines
of Nd II so we are surprised by the lower limits placed by these authors.
For Eu, we measured a fairly clean line at 6645 Å whereas Reyniers
& Van Winckel used spectrum synthesis. It should be noted that the
oscillator strengths used by these authors are quite different from
those employed by us, that can possibly explain the abundance differences
for the s-process elements. The gf values for the lines of these
elements are known to
have larger uncertainties compared to those of the Fe-peak elements.
Another important finding by Reyniers & Van Winckel is the detection
of a red luminuous companion, found from the presence of TiO bands in the
red and also from the observed spectral energy distribution.
As mentioned above,
the presence of the companion might explain the Li I feature variations
observed by us.
This star (HR 7055) was observed in the 13-Colour photometric system and its
temperature was calculated by various approaches by Bravo Alfaro et al. (1997).
The photometric temperature estimates range between 7486 K and 8100 K.
The spectrum being of S/N = 95, we could measure a large
number of lines covering many important
elements like C, -process elements and Fe-peak elements.
From the ionisation equilibrium of Fe I/Fe II, Cr I/Cr II,
Ti I/Ti II, Si I/Si II and even Ca I/Ca II the
atmospheric parameters are well-determined and listed in Table 2.
The star appears to have near-solar abundances for most elements except Si which is overabundant by a factor of 3 (Table 8). With its small radial velocity (+11 km s-1), it is most likely a young star belonging to the disk population. But it can serve as excellent calibrator of photometric indices in the 7500 K temperature range.
This star was classified as A5III by Cowley et al. (1969). These and
the Sp.T. - Colour -
calibration of Schmidt-Kaler (1982) give a temperature of 8091 K.
![]() |
Figure 3:
H![]() ![]() |
Open with DEXTER |
Species |
![]() |
[X/H] | s.d. | N | [X/Fe] |
C I | 8.55 | -0.49 | ![]() |
5 | -0.30 |
O I | 8.87 | -0.14 | 1 | +0.05 | |
Na I | 6.32 | +0.32 | ![]() |
2 | +0.51 |
Mg I | 7.58 | -0.27 | ![]() |
5 | -0.08 |
Mg II | 7.58 | -0.29 | ![]() |
4 | -0.10 |
Si I | 7.55 | +0.11 | ![]() |
3 | +0.20 |
Si II | 7.55 | +0.00 | ![]() |
4 | +0.26 |
S I | 7.21 | +0.17 | ![]() |
2 | +0.36 |
Ca I | 6.35 | -0.08 | ![]() |
15 | +0.11 |
Ca II | 6.35 | -0.09 | 1 | +0.10 | |
Sc II | 3.13 | +0.00 | ![]() |
8 | -0.19 |
Ti I | 4.98 | -0.27 | 1 | -0.08 | |
Ti II | 4.98 | -0.25 | ![]() |
19 | -0.06 |
Cr I | 5.67 | -0.01 | ![]() |
3 | +0.18 |
Cr II | 5.67 | -0.16 | ![]() |
14 | +0.03 |
Mn I | 5.39 | -0.23 | ![]() |
3 | -0.04 |
Fe I | 7.51 | -0.20 | ![]() |
82 | |
Fe II | 7.51 | -0.18 | ![]() |
30 | |
Ni I | 6.25 | -0.06 | ![]() |
9 | +0.13 |
Zn I | 4.60 | +0.18 | 1 | +0.37 | |
Y II | 2.23 | -0.24 | ![]() |
7 | -0.05 |
Zr II | 2.60 | +0.18 | 1 | +0.37 | |
Ba II | 2.13 | -0.08 | ![]() |
2 | +0.11 |
Notes - same as Table 3.
Photometric data in the Strömgren's system can also be used to estimate
,
through the
relation
of Crawford (1979) (his Table 1) and adopting
(b-y) = 0.236 and
(Hauck & Mermilliod 1998).
This leads to
(b-y)0 = 0.176 and
E(b-y) = 0.054. While (b-y)0 leads
to
(B-V)0 = 0.20-0.25 (Crawford 1970), this implies
K.
Also, if the above colour excess and photometry are used in combination of
Napiwotzki et al. (1993) calibration we
find
K.
However, it must be emphasized that
the calibration has been computed using only stars of luminosity classes
V and IV, while HD 218753 could be of luminosity class III or II.
Balmer line fitting can also be used to estimate
.
Theoretical profiles have been extracted
from Kurucz's (1993) models for H
,
H
,
H
and H
.
The observed
profiles were fitted with theoretical profiles of given
and
.
The solution is not unique but in fact the best fits define a locus on the
-
plane for each Balmer line. As underlying core emission may be
present in some stars, we chose to fit the wings H
and H
.
Following the above fitting process we found the loci for H
and H
profiles
shown in Fig. 3.
In hot stars, magnesium and silicon lines can be used as
indicators (since
Fe I lines are strongly affected by non-LTE effects).
Given a pair (
,
)
one searches for abundance
consistency between
neutral and ionized lines of Mg and Si.
Again, the solution is not unique
but rather a locus on the
-
plane is defined for each element, as illustrated in
Fig. 3. The intersections of the Mg and Si loci with the H
and H
loci
point to the proper temperature and gravity. In this fashion
we estimated
between
7600 and 7900 K and
between 1.75 and 2.0.
The turbulent velocity,
,
was estimated from Fe II lines by requiring abundance to be independent of line strength. We found
km s-1.
Species |
![]() |
[X/H] | s.d. | N | [X/Fe] |
C I | 8.55 | -0.33 | ![]() |
5 | -0.09 |
O I | 8.87 | +0.06 | ![]() |
2 | +0.30 |
Na I | 6.32 | -0.03 | 1 | +0.21 | |
Mg I | 7.58 | -0.32 | ![]() |
3 | -0.08 |
Mg II | 7.58 | -0.18 | ![]() |
3 | +0.06 |
Al I | 6.47 | +0.07 | 1 | +0.31 | |
Si II | 7.55 | -0.18 | ![]() |
2 | +0.06 |
S I | 7.21 | +0.29 | ![]() |
5 | +0.53 |
Ca I | 6.35 | -0.29 | ![]() |
10 | -0.05 |
Sc II | 3.13 | -0.19 | ![]() |
5 | +0.05 |
Ti II | 4.98 | -0.33 | ![]() |
22 | -0.09 |
V II | 4.01 | +0.19 | ![]() |
3 | +0.43 |
Cr I | 5.67 | -0.01 | ![]() |
3 | +0.23 |
Cr II | 5.67 | +0.02 | ![]() |
18 | +0.22 |
Mn I | 5.39 | -0.17 | 1 | +0.07 | |
Fe I | 7.51 | -0.27 | ![]() |
48 | |
Fe II | 7.51 | -0.20 | ![]() |
21 | |
Ni I | 6.25 | +0.00 | ![]() |
4 | -0.24 |
Ni II | 6.25 | -0.13 | 1 | +0.11 | |
Sr II | 2.90 | +0.01 | 1 | +0.25 | |
Y II | 2.23 | -0.58 | ![]() |
3 | -0.34 |
Ba II | 2.13 | -0.51 | ![]() |
3 | -0.27 |
Notes - same as Table 3.
For HD 218753 we finally adopted
= 8000 K,
= 2.0 dex and
= 3.3 km s-1. With these
parameters the abundances for the rest of the detected species were
calculated and the results are given in Table 9.
For this star our spectrum has S/N = 67 and we could
measure a large number of clean weak lines for most important elements.
HD 218753 shows a significant carbon deficiency most likely caused by
CNO processing. There is also a significant enrichment of sodium
that has been found in many A-F supergiants as discussed before for HD 725
(Takeda & Takada-Hidai 1994).
Among
-capture elements, only S shows enrichment above
detection limit. These are indications of the star having
experienced the first dredge-up (e.g. [C/Fe] = -0.3 dex).
However its position in the H-R diagram of Fig. 5 is consistent with
a
and an age of about
7.9 108 yr.
This star is an IRAS source (19475+3119). The IR fluxes are quite large (Table 1), the heliocentric radial velocity is very small (-2.5 km s-1). With a spectrum of S/N = 98 we could measure a large number of lines and hence derive the atmospheric parameters as well as abundances with good accuracy (Table 10). The star is Fe-poor by about 1.8 times, but shows significant enrichment of sulphur. The derived abundances are based on 5 good lines hence the derived sulphur abundance cannot be ascribed to measurement errors. Similarly, vanadium also shows some enrichment. Sulphur enrichment appears to be a common feature of our sample stars. The derived abundance of carbon for HD 331319 clearly indicates the effect of CN processing. The star is most likely a young massive disk supergiant or bright giant ascending the red giant branch. The IR fluxes are probably caused by material ejected at this evolutionary stage.
It is an interesting object that has been showing relatively
fast changes in temperature and brightness. It has faded from
reported in BD catalogue to
estimated by Stephenson (1986). Extensive photometry was taken up
by Arkhipova et al. (1999), who found rapid light variations with an
amplitude of up to 0.3 mag during 1996-1997. These authors also obtained
a spectrum and describe the absorption and emission lines present.
The light variations of HDE 341617 and spectral appearance
confirmed the suggestion of Volk & Kwok (1989), based on IRAS
color indices, that it is a candidate post-AGB star.
From spectral type A5 given in HDE, it had changed to class Be (1986)
as reported by Downes & Keyes (1988).
A very extensive spectral investigation by Parthasarathy et al. (2000)
has shown the star to have
= 22000 K with large deficiency
of carbon. These authors derived
of 10000 K and
of 2.5 104 cm-3 for the nebula from the study of emission lines.
The spectra used by Parthasarathy et al. were taken
in 1993. As this object presents rapid variations, we felt we could
examine the spectrum at our epoch (1999) and study the changes.
A comparison of the emission features common to
Parthasarathy et al.
(2000) 1993 spectrum and ours from 1999 is presented in Fig. 4. Figure 4a
shows that in 1999 the emission lines were weaker while Fig. 4b shows
that the differences in equivalent widths are not a function of wavelength.
Unfortunately, we did not observe any flux standard and so were unable to
measure the fluxes
in the emission lines. The shape of the pseudo continuum used for each
echelle order may also be affected by instrumental sensitivity
function. The large scatter is due to this fact.
Weakening of lines (if it is not caused by resolution difference)
might indicate further increase in temperature of the central star.
Systematic monitoring of this fast evolving object could be very rewarding.
![]() |
Figure 4: A comparison of equivalent widths of the emission spectrum of HDE 341617 as observed in 1993 and in 1999. a) The weakening of the emission spectrum is evident despite the fact that the 1999 spectra have not been flux calibrated. b) The equivalent widths are not a function of wavelength. However, the large scatter is probably due to the lack of calibration. See text for discussion |
Open with DEXTER |
According to Arkhipova et al. (1999) HDE 341617
has a mass of 0.7
with
an envelope of
10-3
undergoing rapid evolution towards
the PN phase which, according to the
predictions from Blöcker's (1995) models, should be
reached within 100 years. This and the rapid photometric variations reported
by Arkhipova et al. (1999), most likely caused
by variations in the stellar wind,
make the star a very interesting target for continuous monitoring.
We have two relatively low S/N spectra that were used for identification and measurement of absortion and emission lines. We present in Tables 11 and 12 the line strengths and velocities for absorption and emission lines for this object.
Several absortion lines of He I, O II, Si III and Fe II are
detected. The radial velocity, for each individual line
unambiguously identified is given in Table 11. For He I two groups of
lines are identified at average velocities of
km s-1(4 lines) and
km s-1 (4 lines). This suggests
some stratification in the atmosphere. The rest of the species however average
km s-1 (15 lines). The low dispersion in the radial
velocity suggests that all these lines are formed in the same region of the stellar atmosphere and no stratification is evident.
The emission spectrum, formed in the outer envelope and/or in the nebulosity,
consists of lines of Fe II, [Fe II],
Fe III, [S II], O I, [N II] and Si II.
The radial velocities of emission lines are all very
consistent and average
km s-1.
The difference of radial velocities between the
absorption and emission lines indicates that the
nebulosity expands at about 19 km s-1.
The Balmer lines show emission on top of the stellar absorption.
The emission is shifted relative to the absorption and
is consistent with the radial velocities of other emission features,
showing that it is also produced in the same region.
Though the number of absorption lines were relatively small, we have
done an abundance analysis for a few elements.
The O II lines were used for fixing the microturbulence velocity.
Since the line data was not adequate to do a detailed excitation
equilibrium, we chose to use the temperature and gravity estimated
by Parthasarathy et al. (2000) as starting value and tried models both
hotter and cooler than their estimate. We got more consistent
values for
K,
dex and
km s-1 and hence these
parameters were adopted although available lines were not particularly sensitive
to the temperature. Temperature errors of
500 K or more
are possible.
With these parameters the atmospheric chemical abundances
for the central star
are those reported in Table 13.
Species |
![]() |
[X/H] | s.d. | N |
C II | 8.55 | -1.43 | 1 | |
N II | 7.97 | -0.50 | ![]() |
3 |
O II | 8.87 | -0.51 | ![]() |
14 |
Mg II | 7.58 | -1.13 | 1 | |
Si III | 7.55 | -0.63 | ![]() |
2 |
Notes - same as Table 3.
![]() |
Figure 5:
H-R diagram showing the positions of sample stars
along evolutionary tracks (continuous lines) and isochrones (dashed lines).
![]() ![]() ![]() ![]() ![]() ![]() ![]() ![]() ![]() ![]() ![]() ![]() ![]() ![]() ![]() ![]() |
Open with DEXTER |
In order to estimate the mass and the age of each of the program stars
we have plotted them on the H-R diagram as can be seen in Fig. 5.
The effective temperatures are those derived from the chemical analysis,
and the luminosities were obtained from the above
temperatures and the calibration of Schmidt-Kaler (1982); these quantities
are listed in Table 2. Despite
parallaxes do exist in the Hipparcos catalogue for some of the stars in
our sample, we have
preferred the above approach for the luminosity calculation
for the following reasons. While a very respected version of the
Period-Luminosity relation
for cepheids has been calculated using Hipparcos parallaxes
(Feast & Catchpole 1997) using the most well-known 26 cepheids
as calibrators,
individual parallaxes seem to be of little use. We have taken 21 cepheids
such that the distances could be estimated without requiring the use
of parallaxes. A straight comparison of
distance moduli obtained from the Hipparcos parallaxes and from the
P-L relation shows, in many cases,
large differences. We have also noticed that Hipparcos parallaxes place some stars
at unacceptable positions on the H-R diagram given the derived atmospheric
parameters and elemental
abundances.
For example, for stars
HD 172324 and HD 172481 the parallax
data suggest values of log
.
The situation is further
complicated by unknown circumstellar reddening, which could be
substantial for some of the stars, given their high infrared fluxes.
Therefore we decided not to use individual parallaxes in the present context.
All pre-AGB evolutionary model tracks plotted in Fig. 5 are those of Schaller et al. (1992), while the post-AGB models are from Blöcker (1995). All isochrones are from the work of Bertelli et al. (1994).
Star | [Fe/H] | [C/Fe] | [O/Fe] | [Mg/Fe] | [Si/Fe] | [S/Fe] | [Ca/Fe] | [s/Fe] | C/O | reference |
HD 725 |
-0.29 | -0.08 | +0.12 | +0.40 | +0.20 | +0.14 | +0.27 | 1 | ||
HD 9167 | -0.34 | -0.04 | +0.12 | +0.12 | 1 | |||||
HD 172324 | -0.63 | -0.68 | +0.96 | -0.02 | +0.43 | +0.42 | +0.01 | 1 | ||
HD 173638 | -0.08 | -0.09 | +0.03 | +0.46 | +0.09 | +0.14 | 1 | |||
HD 218753 | -0.19 | -0.30 | +0.05 | -0.09 | +0.23 | +0.36 | +0.11 | +0.14 | +0.21 | 1 |
HD 331319 | -0.24 | -0.09 | +0.30 | -0.01 | +0.06 | +0.53 | -0.05 | -0.30 | +0.19 | 1 |
HD 158616 | -0.57 | +0.34 | +0.04 | +0.08 | +0.56 | +0.62 | +0.21 | +0.66 | +0.95 | 1 |
HD 158616 | -0.70 | +0.64 | -0.04 | +0.68 | +0.70 | +0.71 | +1.30 | +1.90 | 2 | |
HD 172481 | -0.61 | -0.01 | +0.04 | +0.51 | +0.54 | +0.58 | +0.34 | +0.52 | +0.43 | 1 |
HR 7671 | -1.10 | -0.40 | -0.30 | +0.25 | +0.40 | +0.15 | +0.32 | +0.60 | +0.38 | 6 |
HD 187785 | -0.40 | +1.00 | +0.60 | +0.67 | +0.82 | +0.57 | +0.49 | +1.30 | +1.20 | 4 |
HD 187785 | -0.60 | +1.00 | +0.70 | +0.38 | +0.26 | +0.49 | +1.10 | 11 | ||
HD 56126 | -1.00 | +1.08 | +0.63 | +0.97 | +0.95 | +0.63 | +0.46 | +1.78 | +1.35 | 3 |
HD 56126 | -1.00 | +1.10 | +0.80 | +0.06 | +0.40 | -0.11 | +1.50 | 11 | ||
IRAS 04296+3429 | -0.60 | +0.80 | +0.79 | +0.43 | +0.18 | +1.50 | 11 | |||
IRAS 05341+0852 | -0.80 | +1.00 | +0.60 | +0.59 | +0.28 | +0.08 | +2.20 | 11 | ||
IRAS 22223+4237 | -0.30 | +0.30 | -0.10 | +0.29 | +0.04 | -0.17 | +0.90 | 11 | ||
IRAS 23304+6147 | -0.80 | +0.90 | +0.20 | +0.79 | +0.56 | +0.29 | +1.60 | 11 | ||
HR 4049 | <-3.2 | >+3.0 | >+2.7 | >+1.7 | >+0.40 | >+3.0 | <-2.1 | +0.95 | 5 | |
HD 44179 | -3.30 | +3.30 | +2.90 | +1.2 | +1.50 | +3.00 | +0.20 | +1.20 | 2 | |
HD 46703 | -1.57 | +0.98 | +1.10 | +0.09 | -0.38 | +1.20 | +0.02 | -0.49 | +0.74 | 7, 8 |
HD 52961 | -4.80 | +4.40 | +4.20 | +3.80 | +0.60 | +0.76 | 2 | |||
HD 70379 | -0.31 | +0.42 | +0.38 | +0.01 | +0.47 | +0.34 | -0.17 | +0.20 | +0.47 | 9 |
BD+39 4926 | -2.85 | +2.45 | +2.75 | +1.35 | +1.15 | +2.95 | -0.75 | +1.60 | +0.25 | 10 |
References: 1 - This work, 2 - Van Winckel (1995) , 3 -Klochkova (1995), 4 - Van Winckel et al. (1996), 5 - Lambert et al. (1988), 6 - Luck et al. (1990), 7 - Luck & Bond (1984), 8 - Bond & Luck (1987), 9 - Reddy (1996), 10 - Kodaira (1973), 11 - Van Winckel & Reyniers (2000).
In terms of evolution, we could distinguish three groups among our sample
stars. First, HD 158616, HD 172324, HD 172481, and HDE 341617
show clear indications of being post-AGB stars, these are shown in panel c
of Fig. 5. The post-AGB model sequences of Blöcker (1995) suggest that all
four stars had initial ZAMS masses larger than 7
and remnant or core
mass of
.
HD 158616 and HD 172481
might be starting their trajectory towards the
white dwarfs region, i.e. they are near the zero age of central star evolution
(Blöcker 1995), while HD 172324 is a bit more evolved. Since the evolution
in this region of the H-R diagram is very fast, they are all expected to
become planetary nebulae within a few hundreds of years. HDE 341617
has been found to be in the early stages of PN (Arkhipova et al. 1999;
Parthasarathy et al. 2000). Our remnant mass estimate of
is substantially larger than 0.7
estimated by Arkhipova et al. (1999)
from the rate of temperature evolutionary change and a comparison with the theoretical rates from Blöcker's (1995) models.
Our value is a consequence of the spectroscopic determination of
K
and hence log
(Schmidt-Kaler 1982) as well as a comparison with the
luminosities of Blöcker's (1995) models. While the
Arkhipova et al. (1999) estimation is quite convincing the luminosity of the
adopted model
seems too low as it would imply
18000 K for bright giant star of luminosity class II. Such low
a temperature is not supported by the detailed spectroscopic analyses. Thus
an independent estimate of the luminosity seems necessary to settle the core
mass of this star.
In the second evolutionary group we include the stars HD 725, HD 218753 and HD 331319. These are all moderately iron-deficient but otherwise show nearly solar abundances. The heliocentric radial velocities for HD 218753 and HD 331319 are small. They are most likely young massive disk supergiants or bright giants that have gone through some nuclear processing. This is suggested by the C depletion and Na enhancement, indicating the effect of CN processing and post first dredge-up stage. HD 725 is an interesting star since three Y II and one Ba II lines indicate mild enhancement of s-process elements. Since we count on very scarce number of lines of s-process elements, we can only say that the star shows signs of evolution beyond RGB.
The tracks and isochrones in Figs. 5a and 5b suggest
and age of
7.9 108 yr for HD 218753 and
and age of
2.2 107 yr for HD 331319.
From tracks in Fig. 5b we estimate a mass of
and age of
2.5 107 yr. Its rather
large heliocentric radial velocity of -57 km s-1 calls
for attention, however, a calculation of the
galactocentric motion indicates that the star moves on the galactic plane and
has a mildly
eccentrical galactic orbit.
Its radial velocity could owe its origin to
pulsations and/or orbital motions, although variability has not been reported.
The last two stars in our sample, HD 9167 and HD 173638,
display, with few exceptions, solar abundances and no signs of
nuclear processing. They are probably evolving very near the giant branch.
The estimated masses and ages from Fig. 5b are respectively
and 2.6 107 yr and
and
1.7 107 yr. The
only peculiarity of HD 9167 is its high
radial velocity of -45.7 km s-1 however, like HD 725,
its galactocentric orbit seems to be on the galactic plane and mildly
eccentric. Also the possibility, that their observed radial
velocities are attained from pulsation and/or
orbital motion cannot be discarded.
It should be noted that although HD 172481 and HD 158616 are post-AGB
stars, they do not show the effect of selective removal
of condensable elements such as Fe and Sc, observed in some well-known post-AGB stars like
HR 4049, and HD 52961 and RV Tau stars of subclass B (Giridhar et al. 2000 and references therein).
While studying a sample of RV Tau stars, these authors had
noticed a strong dependence on temperature for the selective removal
of refractory elements to occur. The effect is very prominent at temperature range 5500 to
6000 K
and declines for lower temperatures. For stars cooler than 5000 K
the effect was barely
perceptible. At temperatures higher than 7000 K, we expect the effect to be larger. It is indeed true for HR 4049 (Lambert et al. 1988) which has
= 7500 K, i.e. similar to HD 158616 and HD 172481.
However, for these
two stars we did not see any indication of dust condensation and subsequent
removal of grain-forming elements.
HD 158616 is a carbon-rich post-AGB star similar to HD 56126
(Klochkova 1995) and
HD 187785 (Van Winckel et al. 1996) also showing significant
enhancement of s-process elements.
Stars like HR 4049, HD 52961 and RV Tau stars of subclass B show C/O
1 and mild s-process enhancement.
As a matter of fact,
most stars showing abundance peculiarities caused by dust condensation
have C/O
1.
Stars HR 4049, HD 44179, HD 46703, HD 52961 and BD +39
4926 possibly
belong to this subgroup. For these objects, since Fe gets locked in grains,
[S/H] is considered
a better indicator of metallicity. For these stars [S/H]
ranges between +0.1 to -1.0 dex with a mean around -0.4 dex. In other words,
they are mildly metal-deficient. Carbon-rich post-AGB stars with enhanced s-process elements, like HD 158616, HD 56126 and HD 187785 have [Fe/H] (which
would be a true reflection of their metallicity since these stars are not affected by dust condensation) in the range -0.4 to -1.0 dex. These values
are not radically different from those found for the subgroup having
dust-grain condensation and
C/O
1. We, therefore, do not visualize large differences in
their ages though the O-rich phase in the AGB is expected to precede
the C-rich phase.
The abundances of hot post-AGB stars studied by Conlon et al. (1993a) and McCausland et al. (1992) bear close resemblance to HD 172324. The hot post-AGB stars show strong deficiency of carbon and significant oxygen enrichment. These stars probably belong to a subgroup of post-AGB star that have evolved without experiencing third dredge-up. This carbon deficiency is also found in the proto-Planetary Nebula HDE 341617 (see Table 13). Caution is however needed with C II spectra since they are known to show large non-LTE effects (Eber & Butler 1988; Takeda & Takada-Hidai 1994). McCausland et al. (1992) have discussed at length two scenarios to explain the carbon deficiency. HBB occuring during interpulse phase could cause the production of 14N at the expense of 12C. However, overabundance of He like the one found in the SMC planetary nebula SMP 28 is not evident for HD 172324 and HD 341617 to make HBB the sole mechanism responsible for carbon deficiency. Another possibility suggested by McCausland et al. (1992) that the carbon deficiency might be inherent to the precursor itself is quite attractive. To substantiate their argument they pointed out the carbon-poor stars HR 4912 and HR 7671 as possible precursors to more evolved carbon-poor hot post-AGB stars. HR 4912 was included in our recent work and we found [C/H] = -1.27 (Giridhar et al. 1997) in good agreement with [C/H] of -1.15 found by Lambert et al. (1983). HR 7671 has [C/H] of -1.53 (Luck et al. 1990). It seems therefore that HD 172324 and HDE 341617 might form a special carbon-poor post-AGB stars evolutionary sequence. Search for carbon-poor objects in all temperature ranges may help in finding the precursors or successors of these objects.
We have found a new post-AGB star HD 172481 for which abundance
analysis had not been carried out before, however the referee pointed out
in a rather late stage of revision,
the then unpublished work by Reyniers & Van Winckel (2001)
where an independent
abundance analysis has been carried out. We have highlighted a comparison
of results in Sect. 5.5 and found both analyses to be in fairly good agreement.
We have done a more
complete analysis of HD 158616. This star can be now considered a
post-AGB star beyond any doubt. Among the post-AGB stars, the number of
stars showing C/O 1 or greater and also enhancement of s-process
elements are very few. There are clear indications of stars having
experienced the third dredge-up. The stars HD 158616 and HD 172481
belong to this important class.
C/O of HD 172481 might have been prevented from exceeding one
by HBB. The same may be responsible for large Li
abundance but other possibilities like binarity cannot be ruled out.
A long-term light and radial velocity monitoring of this object
is planned for the future.
We found a very likely hot post-AGB candidate
in HD 172324 but will feel more confident of its status after
important elements like N are included and a more comprehensive study is made.
Continuous monitoring of its spectrum in the H
region is required
to detect activity possibly related to stellar pulsations.
HD 218753 and HD 331319 have passed the giant branch and are in the He-core and H-shell burning stages. HD 9167 and HD 173638 essentially show solar abundance. HD 725 and HD 9167 show large radial velocities, however their galactocentric orbits are on the galactic plane and mildly eccentric, thus they are most likely massive and young disk stars. However, their large radial velocity could also be due to pulsations and/or orbital motions.
In the proto-Planetary Nebula HDE 341627 the He lines show two velocity components possibly indicating velocity stratification. The emission lines appear to have weakened since 1993.
Acknowledgements
AAF acknowledges Commission 38 of the IAU for a travel grant and the Indian Institute of Astrophysics for hospitality and financial support. We thank David Yong for getting us two spectra of HD 172481. We are also indebted to Ms. T. Sivarani for her help in identifying the lines for HDE 341617. We are grateful to the referee, Dr. R. Gallino, for helpful discussions and suggestions. This project has been supported at different stages by grants from DGAPA-UNAM (IN113599) and CONACyT (Mexico) (E130.2060) and CNRS (France).
Species |
![]() |
![]() |
EW | ![]() |
Species |
![]() |
![]() |
EW | ![]() |
(Å) | (Å) | (m Å) | (km s-1) | (Å) | (Å) | (m Å) | (km s-1) | ||
He I |
4010.217 | 4009.270 | 223.2 | 70.9 | O II | 4642.973 | 4641.811 | 233.6 | 75.1 |
He I |
4027.047 | 4026.362 | 337.0 | 48.6 | O II | 4643.039 | 4641.82 | 302.9 | 78.8 |
He I |
4144.569 | 4143.759 | 391.9 | 51.0 | O II | 4650.29 | 4649.139 | 309.0 | 74.3 |
O II: | 4350.53 | 4349.426 | 267.7 | 76.1 | O II | 4662.795 | 4661.635 | 150.4 | 74.7 |
O II |
4367.922 | 4366.896 | 208.3 | 70.5 | O II+C III | 4674.776 | 4673.91/73.75 | 58.6 | |
He I |
4389.027 | 4387.929 | 325.8 | 75.1 | O II | 4677.389 | 4676.234 | 84.8 | 74.1 |
O II |
4415.984 | 4414.909 | 141.5 | 73.0 | O II | 4706.507 | 4705.355 | 70.2 | 73.4 |
O II |
4418.081 | 4416.975 | 104.7 | 75.1 | He I | 4714.39 | 4713.143 | 160.8 | 79.4 |
He I |
4472.59 | 4471.477 | 446.8 | 74.7 | He I | 4922.992 | 4921.929 | 516.4 | 64.8 |
Si III |
4553.727 | 4552.654 | 322.4 | 70.7 | He I: | 5015.647 | 5015.675 | 217.2 | |
Si III | 4568.918 | 4567.872 | 280.0 | 68.7 | Fe II | 5796.901 | 5795.870 | 152.8 | 53.4 |
Si III | 4575.818 | 4574.777 | 229.7 | 68.3 | He Ibld | 5875.849 | 5875.618+75.650 | 542.5 | |
O II | 4592.136 | 4590.971 | 209.9 | 76.1 | He I | 6679.176 | 6678.149 | 841.9 | 46.1 |
O II |
4639.951 | 4638.854 | 136.3 | 70.9 |
Species |
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EW | ![]() |
Species |
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EW | ![]() |
(Å) | (Å) | (m Å) | (km s-1) | (Å) | (Å) | (m Å) | (km s-1) | ||
[S II] |
4069.357 | 4068.600 | 545.7 | 55.8 | [Cr I: ] | 5147.604 | 5146.550 | 86.5 | 61.4 |
[Fe II] |
4244.732 | 4243.980 | 266.3 | 53.1 | [Fe II] | 5158.931 | 5158.000 | 155.2 | 54.1 |
[Fe II] |
4245.566 | 4244.810 | 50.0 | 53.4 | [Fe II] | 5159.702 | 5158.810 | 367.9 | 51.8 |
[Fe II] |
4277.632 | 4276.83 | 237.5 | 56.2 | [Fe II] | 5164.910 | 5163.940 | 108.9 | 56.4 |
[Fe II] |
4306.718 | 4305.900 | 60.2 | 57.0 | Fe II | 5169.933 | 5169.030 | 164.1 | 52.4 |
H |
4341.315 | 4340.475 | 1030.0 | [Fe II] | 5182.956 | 5181.970 | 89.0 | 57.1 | |
[Fe II] |
4353.553 | 4352.78 | 100.5 | 58.8 | [Fe II] | 5200.056 | 5199.180 | 43.0 | 50.5 |
[Fe II] |
4359.146 | 4358.370 | 117.9 | 53.4 | [Fe II] | 5221.008 | 5220.060 | 74.3 | 54.5 |
[Fe II] |
4360.112 | 4359.190 | 496.6 | 53.1 | [Fe II] | 5262.580 | 5261.610 | 463.8 | 55.3 |
O I |
4369.018 | 4368.30 | 100.9 | 49.3 | [Fe II] | 5269.799 | 5268.880 | 58.5 | 52.3 |
Fe II |
4373.130 | 4372.220 | 37.1 | 62.4 | [Fe II] | 4288.157 | 4287.40 | 625.2 | 53.0 |
[Fe II] |
4383.621 | 4382.750 | 81.0 | 59.6 | [Fe II] | 5274.345 | 5273.380 | 383.7 | 54.9 |
Fe II | 4385.381 | 4384.330 | 24.7 | 71.9 | O I | 5276.020 | 5275.080 | 29.2 | 53.5 |
[Fe II] |
4414.564 | 4413.780 | 398.2 | 53.3 | Fe II | 5279.221 | 5278.265 | 21.1 | 54.3 |
[Fe II] |
4417.075 | 4416.270 | 356.9 | 54.7 | Fe III | 5292.588 | 5291.780 | 46.7 | 45.0 |
[FeII] |
4458.737 | 4457.95 | 221 | 52.9 | [Fe II] | 5297.799 | 5296.840 | 78.1 | 54.3 |
[Fe II] |
5413.604 | 5412.640 | 50.3 | 53.4 | O I | 5299.961 | 5299.000 | 117.2 | 54.4 |
[FeII] |
4475.767 | 4474.91 | 85 | 53.0 | Fe II | 5317.554 | 5316.609 | 23.9 | 53.3 |
[FeII] |
4489.560 | 4488.75 | 85 | 51.0 | [Fe II] | 5334.587 | 5333.650 | 295.0 | 52.7 |
[FeII] |
4493.412 | 4492.64 | 38 | 53.4 | [Fe II] | 5348.652 | 5347.690 | 30.0 | 54.0 |
[FeII] |
4529.249 | 4528.39 | 18 | 56.4 | [Fe II] | 5377.438 | 5376.470 | 234.3 | 54.0 |
[FeII] |
4728.955 | 4728.07 | 170 | 56.4 | [Fe II] | 5434.124 | 5433.150 | 86.1 | 53.8 |
Fe III |
4734.765 | 4733.900 | 14.9 | 54.8 | [Fe II] | 5478.195 | 5477.250 | 43.9 | 51.8 |
[FeII] |
4775.615 | 4774.74 | 110 | 54.4 | O I | 5513.699 | 5512.710 | 30.0 | 53.8 |
[Fe II] |
4799.149 | 4798.29 | 25.9 | 53.7 | O I | 5555.937 | 5554.940 | 60.0 | 53.8 |
[Fe II] |
4815.394 | 4814.5 | 325.9 | 52.8 | [Fe II] | 5747.997 | 5746.960 | 130.2 | 54.1 |
H |
4862.284 | 4861.332 | 2921.0 | 58.7 | [N II] | 5755.637 | 5754.800 | 157.5 | 43.6 |
[Fe II] |
4875.354 | 4874.490 | 116.5 | 53.2 | Si II | 5958.641 | 5957.612 | 149.5 | 51.8 |
[Fe II] |
4890.511 | 4889.630 | 288.0 | 54.1 | O I | 5959.607 | 5958.46+58.630 | ||
[Fe II] |
4906.204 | 4905.350 | 256.0 | 52.2 | Si II o FeIII | 5979.989 | 5978.970 | 425.3 | 51.1 |
Fe II | 4924.813 | 4923.921 | 86.3 | 54.3 | O I bld | 6047.481 | 6046.26+6046.46 | 427.2 | 60.6 |
[Fe II] |
4951.656 | 4950.740 | 46.0 | 55.5 | Si II(2)+[NII] | 6348.259 | 6347.090 | 517.8 | 55.3 |
[Fe II] |
4974.283 | 4973.390 | 101.5 | 53.9 | [O I] | 6364.896 | 6363.88 | 277.7 | 47.9 |
uf1 | 4981.034 | 113.5 | uf1 | 6366.259 | 126.3 | ||||
[Fe II] |
5006.441 | 5005.520 | 69.1 | 43.2 | Si II(2) | 6372.505 | 6371.359 | 242.9 | 54.0 |
Fe II | 5019.322 | 5018.434 | 97.5 | 53.17 | [N II](1) | 6549.274 | 6548.100 | 666.1 | 53.8 |
[Fe II] |
5021.110 | 5020.240 | 107.4 | 52.0 | H![]() |
6564.138 | 6562.817 | 43.97 | 60.3 |
Si II | 5041.962 | 5041.063 | 61.9 | 53.5 | [N II](1) | 6584.646 | 6583.6 | 2105.0 | 47.7 |
[Fe II] |
5044.422 | 5043.530 | 58.1 | 53.1 | [O II] | 6668.000 | 6666.940 | 160.2 | 47. |
Si II | 5056.882 | 5056.020 | 178.0 | 51.1 | [S II] | 6717.786 | 6716.470 | 81.1 | 58.8 |
[Fe II] |
5108.814 | 5107.950 | 57.1 | 50.7 | [S II] | 6731.874 | 6730.850 | 93.3 | 45.6 |
[Fe II] |
5112.558 | 5111.630 | 88.8 | 54.5 | [S II] | 6732.169 | 6731.300 | 114.5 | 38.72 |
1 - uf = unidentified feature.