Contents

A&A 454, 917-931 (2006)
DOI: 10.1051/0004-6361:20064968

Analysis of 26 barium stars[*],[*],[*]

II. Contributions of s-, r-, and p-processes in the production of heavy elements

D. M. Allen[*] - B. Barbuy

Instituto de Astronomia, Geofísica e Ciências Atmosféricas, Universidade de São Paulo, Rua do Matão 1226, 05508-900 São Paulo, Brazil

Received 4 February 2006 / Accepted 16 March 2006

Abstract
Context. Barium stars show enhanced abundances for the slow neutron capture (s-process) heavy elements, so they are suitable objects for studying s-process elements.
Aims. The aim of this work is to quantify the contributions of the s-, r-, and p-processes for the total abundance of heavy elements from abundances derived for a sample of 26 barium stars. The abundance ratios between these processes and neutron exposures were studied.
Methods. The abundances of the sample stars were compared to those of normal stars, thus identifying the fraction relative to the main component of the s-process.
Results. The fittings of the $\sigma N$ curves (neutron-capture cross-section times abundance, plotted against atomic mass number) for the sample stars suggest that the material from the companion asymptotic giant branch star had approximately the solar isotopic composition as concerns fractions of abundances relative to the s-process main component. The abundance ratios of heavy elements, hs, ls, and s and the computed neutron exposure are similar to those of post-AGB stars. For some sample stars, an exponential neutron exposure fits the observed data well, whereas a single neutron exposure provides a better fit for others.
Conclusions. The comparison of barium and AGB stars supports the hypothesis of binarity for the barium star formation. Abundances of r-elements that are part of the s-process path in barium stars are usually higher than those in normal stars, so barium stars also seemed to be enriched in r-elements, although to a lower degree than s-elements. No dependence on luminosity classes was found in the abundance-ratio behaviour among the dwarfs and giants of the sample of barium stars.

Key words: nuclear reactions, nucleosynthesis, abundances - stars: abundances

1 Introduction

Nucleosynthesis of elements has benefitted from the dispute between George Gamow and Fred Hoyle in explaining how the known chemical elements were formed (Hoyle 1946; Alpher et al. 1948). Since then, our knowledge of primordial and stellar nucleosynthesis has greatly improved. Burbidge et al. (1957, B2FH) based their work on solar abundances and defined eight nucleosynthetic processes in stars that would be responsible for the formation of the chemical elements. Wallerstein et al. (1997) present a review of B2FH, including recent and accurate experimental results and observations, where they show that some processes defined by B2FH have been confirmed, others redefined, and new processes not known by B2FH have been included in the list.

Three of the eight processes defined by B2FH are the focus of the present work: the s-, r-, and p-processes. We present the abundance ratios between these processes and abundance distribution for a number of heavy elements in a sample of barium stars. The abundance determination for the sample stars was described in Allen & Barbuy (2006, Paper I hereafter).

The abundance ratios for the best representatives of s- and r-processes provide clues to the formation and evolution of the Galaxy, since each of them is related to a different formation site, including stars of different characteristics and evolutionary stages. As an example, Mashonkina et al. (2003) estimate the timescale for the thick disk and halo formation based on the abundance ratios of [Eu/Ba], [Mg/Fe], and [Eu/Fe] and on the calculations of chemical evolution by Travaglio et al. (1999). Burris et al. (2000) conclude from abundances of metal-poor giant stars that the contributions of s-processes can be seen at metallicities as low as [Fe/H] = -2.75, and they are present in stars of [Fe/H] > -2.3, indicating that the s-process acts at lower metallicities than predicted by previous works.

Considering the scenario of barium star formation through enriched material transfer from a companion AGB star, it is worth comparing abundances of AGBs and barium stars. Such study can provide clues to the enrichment of barium stars in heavy elements, given that they should conserve the surface characteristics of AGB stars.

This work intends to address the following questions:

1. What are the s-element abundances of normal stars?

2. Considering the hypothesis of the transfer of material enriched in carbon and s-elements from a more evolved companion for barium star formation, is it possible to estimate from observed abundances which proportions these elements are received?

3. What is the isotopic composition of the material received? Is it possible to consider the solar system mix?

4. How is the $\sigma N$ curve behaviour for barium stars?

5. What kind of neutron exposures were involved in the nucleosynthesis of the transferred material?

This paper is organised as follows. Section 2 is a brief description of atmospheric parameters and of the abundance determination carried out in Paper I; Sect. 3 briefly explains the s-, r-, and p-processes; Sect. 4 shows the contributions of s-, r-, and p-processes in normal stars compared to barium stars; Sect. 5 evaluates two kinds of neutron exposures and shows ratios involving s, hs, and ls. In Sect. 6 conclusions are drawn.

2 Atmospheric parameters and abundance calculations

The observations, atmospheric parameters, and abundance calculations have already been described in detail in Paper I. Here, we outline only the more important steps.

Photometric data were taken in several runs at the ZEISS 60 cm telescope at the LNA (Laboratório Nacional de Astrofísica) and from the literature. Optical spectra were obtained at the 1.52 m telescope at ESO, La Silla, using the Fiber Fed Extended Range Optical Spectrograph (FEROS) (Kaufer et al. 2000). A set of atmospheric parameters (temperature, surface gravity, metallicities, and microturbulent velocity) was obtained in an iterative way.

Photospheric 1D models were extracted from the NMARCS grid (Plez et al. 1992) for gravities $\log~ g < 3.3$, and from Edvardsson et al. (1993) for less evolved stars, with $\log ~g \geq 3.3$. The LTE abundance analysis and the spectrum synthesis calculations were performed using the codes by Spite (1967, and subsequent improvements in the past thirty years), described in Cayrel et al. (1991) and Barbuy et al. (2003). Line lists and respective parameters are given in Paper I.

  \begin{figure}
\par\includegraphics[width=14cm,clip]{4968fig1}
\end{figure} Figure 1: $\log\epsilon$(X) vs. atmospheric parameters ([Fe/H], $T_{\rm eff}$, $\log~ g$) for normal stars. Symbols indicate different references: open squares: Gratton & Sneden (1994); open circles: Burris et al. (2000); open triangles: Tomkin & Lambert (1999); filled triangles: Jehin et al. (1999); crosses: Edvardsson et al. (1993) and Woolf et al. (1995); filled squares: Smith et al. (2000); open pentagon Mashonkina & Gehren (2001). Uncertainties were taken from the respective references; otherwise, the values of $\pm $0.1 for [Fe/H] and $\pm $0.05 for $\log\epsilon$(X) were used. These values were also attributed to Jehin et al. (1999), given that their uncertainties seem underestimated.


  \begin{figure}
\par\includegraphics[width=13.5cm,clip]{4968fig2}
\end{figure} Figure 2: Same as Fig. 1 for other elements.

3 s-, r-, and p-processes

Several important references describe the s-, r-, and p-processes in detail: B$\sp 2$FH, Meyer (1994), and Wallerstein et al. (1997) for a more general description; Käppeler et al. (1989), Busso et al. (1999), Lugaro et al. (2003), Lamb et al. (1977), and Raiteri et al. (1993) for the s-process; Woosley & Hoffman (1992), Wanajo et al. (2003), and Argast et al. (2004) for the r-process; Rayet et al. (1995) and Goriely et al. (2005) for the p-process, among others.

Typical s-elements are mainly produced by the s-process, but a smaller fraction of their abundance is due to the r-process. Analogously, the major production of r-elements is due to the r-process with a smaller contribution from s-process. Beyond these main processes, the p-process contributes with a small fraction of heavy elements production, as shown in Fig. 1 of Meyer (1994).

In the s-process, neutrons are captured by seed nuclei, which are the iron-peak elements, on a long timescale relative to $\beta$ decay, denominated "s'' (slow) by B$\sp 2$FH. This process has been subdivided into three components according to the site and the nucleosynthetic products: main, weak, and strong.

The s-process main component is responsible for many nuclides in the range of atomic mass $63 \leq A \leq 209$. Abundance peaks can be observed near A = 90, 138, and 208. In the classical analysis (Käppeler et al. 1989) the element formation through the s-process occurs in a chain, starting with the seed nucleus $\sp {56}$Fe. Following this analysis, it is possible to obtain an expression for the $\sigma N$, where $\sigma $ is the neutron capture cross-section and N the abundances due to the s-process only for each nuclide. This expression involves the mean distribution of neutron exposure $\tau _{\rm o}$, the abundance fraction of $\sp {56}$Fe required as seed to s-process G, and the solar abundance of $\sp {56}$Fe N $_{56}^\odot$,

 \begin{displaymath}
\sigma_kN_k = {G {\rm N}_{56}^\odot\over{\tau_{\rm o}}}\prod_{i=56}^{k}
\left(1+{1\over {\tau_{\rm o}\sigma_i}}\right)^{-1}
\end{displaymath} (1)

where k is the atomic mass number.

For the solar system, the corresponding curve from classical analysis represents the abundances of s-process nuclei for A > 90 very well. For lighter nuclides, this line appears below the empirical data, suggesting another form of synthesis of s-process nuclides in stars, with the first one called the main component and the second, the weak component. The good agreement between the classical model and the observed data of this curve for the solar system represents an interesting characteristic of the s-process, taking the large number of nuclides between Fe and Bi into account.

The s-process main component is believed to occur during the thermal pulses - asymptotic giant branch (TP-AGB) phase of intermediate or low mass stars. In this phase, the star consists of an inert CO core and the He and H burning shells. The region between the two shells is the so-called He intershell, where neutrons released by the 13C ($\alpha$, n)16O reaction during the interpulse period and by the 22Ne ($\alpha$, n)25Mg reaction during the convective thermal pulse are captured by iron-peak nuclei.

The s-process weak component is responsible for part of the abundance of nuclides with atomic mass in the range $23 \leq A \leq 90$ (Raiteri et al. 1993; Lamb et al. 1977). The nucleosynthetic site is probably the core helium burning of stars with masses $\geq$10  $M\sb \odot$, where temperature is high enough for the main neutron source to be the 22Ne ($\alpha$, n)25Mg reaction. Neutron density is low compared to the main component.

The s-process strong component was postulated in order to provide part of the Pb abundance (see Käppeler et al. 1989). However, according to Busso et al. (1999), it is possible to explain the 208Pb galactic abundance without it.

The r-process occurs in an environment that is rich in neutrons, where several of them are captured by nuclides on a short timescale compared to $\beta$ decay, and for this reason, this process was denominated as "r'' (rapid) by B$\sp 2$FH. In this case, the neutron density is higher than for the s-process. Sites that favour such high neutron density are the final stages of massive stars such as core collapse supernovae (SN II, Ib, Ic) (Qian 2000; Wasserburg & Qian 2000; Qian 2001) or those involving neutron stars (Freiburghaus et al. 1999; Woosley & Hoffman 1992; Meyer 1994; Rosswog et al. 2000,1999).

The fact that r-elements are observed in very metal-poor stars suggests that these elements were produced in supernovae events resulting from the evolution of the first massive stars in the Galaxy (Cowan et al. 2002; Sneden et al. 2003; Hill et al. 2002; Sneden et al. 1996; Ishimaru et al. 2004; Honda et al. 2004). Despite the promise of these scenarios, some difficulties have been found; for instance, Wanajo et al. (2001) show that to reproduce a solar abundance of r-elements, proto neutron stars must have 2 $M_{\odot}$ and 10 km of radius, characteristics not observed so far.

The p-process forms nuclei rich in protons. Some s- or r-nuclei, where s- and r-processes were blocked, capture protons with $\gamma$ emission (p, $\gamma$). The p-nuclei may also be synthesised by photodesintegration ($\gamma$, n) of a pre-existing nucleus rich in neutrons (especially s-nuclei), followed by possible cascades of ($\gamma$, p) and/or ($\gamma$, $\alpha$) reactions.

The p-process site should be rich in hydrogen, with proton density $\geq$10$\sp 2$ g/cm$\sp 3$, at temperatures of $T = 2{-}3 \times 10^9$ K. This process site is most likely related to SN II, according to Arnould (1976), Woosley & Howard (1978, and references therein), Arnould et al. (1992), and Rayet et al. (1993) or the explosion of a moderately massive white dwarf due to the accretion of He-rich matter (Goriely et al. 2005, and references therein). A quantitative study of the p-process is presented in Rayet et al. (1995).

4 Abundance distribution for s-, r-, and p-processes

4.1 s-, r-, and p-processes in normal stars

One way to quantify the enrichment of s-elements in barium stars is to compare their abundances with normal stars. For the s-, r-, and p-elements, the total abundance for the element can be described by the sum of the abundances corresponding to the three nucleosynthetic processes, taking into account all contributing isotopes "i'':

\begin{displaymath}\epsilon(X) = \sum_i{\epsilon_{\rm s}^i} + \sum_i{\epsilon_{\rm r}^i} + \sum_i{\epsilon_{\rm p}^i}.\end{displaymath}

In order to quantify the contribution of each process to the total abundance of several heavy elements in normal stars, an extensive set of stars from the literature was used. Peculiar stars were withdrawn from these samples in order to obtain more reliable results. Figures 1 and 2 show the behaviour of the abundances ( $\log\epsilon(X)$) of several heavy elements as a function of atmospheric parameters ( $T_{\rm eff}$, $\log~ g$, [Fe/H]). It is clear from these figures that $\log\epsilon(X)$ vs. [Fe/H] is a linear correlation ( $\log\epsilon_{\rm nor}(X) = A{\rm [Fe/H]} + B$), while $\log\epsilon(X)$ vs. $T_{\rm eff}$ and $\log~ g$ are not. Results of least-square fittings for $\log\epsilon(X)$ vs. [Fe/H] are shown in Table 1.
 

 
Table 1: Results obtained from least-square fitting of $\log\epsilon_{\rm nor}(X)$vs. [Fe/H] of normal stars: $\log\epsilon_{\rm nor}(X)$ = A[Fe/H] + B; "cov'' is the covariance between A and B; "d.o.f.'' is the number of degrees of freedom.

X
A B $\chi^2_{\rm red}$ cov (10-4) d.o.f.

Sr
1.013 $\pm $ 0.024 2.908 $\pm $ 0.021 1.197 4.18 82
Y 1.112 $\pm $ 0.016 2.239 $\pm $ 0.013 1.002 1.58 160
Zr 0.939 $\pm $ 0.019 2.625 $\pm $ 0.015 1.385 2.06 66
Mo 0.970 $\pm $ 0.212 1.895 $\pm $ 0.342 1.472 715.2 7
Ba 0.992 $\pm $ 0.014 2.095 $\pm $ 0.011 1.978 1.07 214
La 1.190 $\pm $ 0.031 1.377 $\pm $ 0.039 4.891 10.91 47
Ce 1.009 $\pm $ 0.047 1.500 $\pm $ 0.047 0.923 20.20 34
Pr 0.867 $\pm $ 0.048 0.748 $\pm $ 0.050 1.180 19.99 13
Nd 0.950 $\pm $ 0.019 1.460 $\pm $ 0.017 1.635 2.46 99
Sm 0.811 $\pm $ 0.045 0.951 $\pm $ 0.045 1.407 18.76 34
Eu 0.783 $\pm $ 0.019 0.581 $\pm $ 0.015 1.263 2.20 165
Dy 0.840 $\pm $ 0.031 1.080 $\pm $ 0.044 4.312 11.70 22


From $\log\epsilon(X)$ vs. [Fe/H] fittings, it is possible to determine the total abundance of a certain element in a normal star of a given metallicity. The first line of Table 2 shows $\log\epsilon_{\rm nor}(X)$obtained directly from fittings for normal stars with metallicities corresponding to the barium star, indicated in the header. Data for molibdenium are rarely available in the literature in the same metallicity range as the present sample, and for this reason the least-square fitting was done using data derived for the globular cluster $\omega$ Centauri by Smith et al. (2000), with results shown in Col. 2 of Table 3. In order to verify the reliability of these results, Mo abundances were calculated through $\log\epsilon_{\rm nor}$(Mo) =  $\log\epsilon_\odot$(Mo) + [Fe/H] + [Mo/Fe], considering [Mo/Fe] = 0, and results are shown in Col. 3 of Table 3. The agreement between results from these two columns means that, according to the fitting, [Mo/Fe] $\approx$ 0 at metallicities near solar. Data for Gd and Pb are also rare in the literature for normal stars in the range of metallicities of the present sample. For this reason, $\log\epsilon_{\rm nor}$(Gd) and $\log\epsilon_{\rm nor}$(Pb) were determined by considering [Gd/Fe] = [Pb/Fe] =  $0 \pm 0.05$, near the solar metallicity. Gadolinium is expected to behave like dysprosium given that both are produced mainly through the r-process in almost the same proportions (Arlandini et al. 1999). Columns 4 and 5 of Table 3 show $\log\epsilon_{\rm nor}$(Dy) values determined by least-square fitting and by summing the star metallicity to the solar value, and Cols. 6 and 7 show $\log\epsilon_{\rm nor}$(Gd) and $\log\epsilon_{\rm nor}$(Pb).


 

 
Table 2: Abundances obtained from least-square fittings for normal stars with metallicities corresponding to our sample of barium stars. Each set of five lines corresponds to the normal star with the same metallicity as the barium star indicated in parenthesis. $\log\epsilon(X)$ corresponds to $\log\epsilon_{\rm nor}(X)$ and $\epsilon \sb {\rm s,r,p}(X)$ corresponds to $\epsilon _{\rm s,r,p} (X)_{\rm nor}$ from Eq. (2). $\epsilon _{\rm o}(X)$ is from Eq. (6). The full table is only available in electronic form at the CDS.
  Sr Y Zr Mo Ba La Ce ...
    [Fe/H] = -0.06 (HD 749)    
$\log\epsilon(X)$ $2.85\pm0.18$ $2.17\pm0.20$ $2.57\pm0.17$ $1.84\pm0.37$ $2.04\pm0.18$ $1.31\pm0.22$ $1.44\pm0.19$ ...
$\epsilon\sb {\rm s}(X)$ $594.4\pm51.0$ $136.8\pm63.2$ $307.4\pm20.1$ $34.1\pm29.2$ $87.7\pm36.1$ $12.5\pm6.3$ $20.9\pm9.0$ ...
$\epsilon\sb {\rm r}(X)$ $0.00\pm0.00$ $11.9\pm5.5$ $58.9\pm23.0$ $17.9\pm15.4$ $20.6\pm8.5$ $7.7\pm3.8$ $6.5\pm2.8$ ...
$\epsilon\sb {\rm p}(X)$ $109.0\pm46.0$ $0.0\pm0.0$ $4.1\pm1.6$ $16.7\pm14.3$ $0.2\pm0.1$ $0.0\pm0.0$ $0.1\pm0.0$ ...
$\epsilon\sb {\rm o}(X)$ $109.0\pm46.0$ $11.9\pm5.5$ $63.0\pm24.6$ $34.6\pm29.7$ $20.8\pm8.6$ $7.7\pm3.8$ $6.6\pm2.8$ ...
. . . . . . . . ...
. . . . . . . . ...



 

 
Table 3: Abundances [ $\log\epsilon_{\rm nor}$(X)] of Mo, Dy, Gd, and Pb for normal stars. Symbol "*'' indicates that the column was obtained from a least-square fitting.

star
Mo* Mo Dy* Dy Gd Pb

HD 749
1.84 1.86 1.03 1.14 $1.06\pm0.19$ $1.89\pm0.20$
HR 107 1.55 1.56 0.78 0.84 $0.76\pm0.07$ $1.59\pm0.10$
HD 5424 1.36 1.37 0.62 0.65 $0.57\pm0.19$ $1.40\pm0.20$
HD 8270 1.49 1.50 0.73 0.78 $0.70\pm0.07$ $1.53\pm0.10$
HD 12392 1.78 1.80 0.98 1.08 $1.00\pm0.19$ $1.83\pm0.20$
HD 13551 1.47 1.48 0.71 0.76 $0.68\pm0.07$ $1.51\pm0.10$
HD 22589 1.63 1.65 0.85 0.93 $0.85\pm0.07$ $1.68\pm0.10$
HD 27271 1.81 1.83 1.00 1.11 $1.03\pm0.19$ $1.86\pm0.20$
HD 48565 1.29 1.30 0.56 0.58 $0.50\pm0.07$ $1.33\pm0.10$
HD 76225 1.59 1.61 0.82 0.89 $0.81\pm0.07$ $1.64\pm0.10$
HD 87080 1.47 1.48 0.71 0.76 $0.68\pm0.07$ $1.51\pm0.10$
HD 89948 1.60 1.62 0.83 0.90 $0.82\pm0.07$ $1.65\pm0.10$
HD 92545 1.78 1.80 0.98 1.08 $1.00\pm0.07$ $1.83\pm0.10$
HD 106191 1.61 1.63 0.84 0.91 $0.83\pm0.07$ $1.66\pm0.10$
HD 107574 1.36 1.37 0.62 0.65 $0.57\pm0.07$ $1.40\pm0.10$
HD 116869 1.58 1.60 0.81 0.88 $0.80\pm0.19$ $1.63\pm0.20$
HD 123396 0.74 0.73 0.08 0.01 - $0.07\pm0.19$ $0.76\pm0.20$
HD 123585 1.43 1.44 0.68 0.72 $0.64\pm0.07$ $1.47\pm0.10$
HD 147609 1.46 1.47 0.70 0.75 $0.67\pm0.07$ $1.50\pm0.10$
HD 150862 1.80 1.82 1.00 1.10 $1.02\pm0.07$ $1.85\pm0.10$
HD 188985 1.60 1.62 0.83 0.90 $0.82\pm0.07$ $1.65\pm0.10$
HD 210709 1.86 1.88 1.05 1.16 $1.08\pm0.19$ $1.91\pm0.20$
HD 210910 1.54 1.55 0.77 0.83 $0.75\pm0.19$ $1.58\pm0.20$
HD 222349 1.28 1.29 0.55 0.57 $0.49\pm0.07$ $1.32\pm0.10$
BD+18 5215 1.38 1.39 0.63 0.67 $0.59\pm0.07$ $1.42\pm0.10$
HD 223938 1.56 1.57 0.79 0.85 $0.77\pm0.19$ $1.60\pm0.20$


Considering that the total abundance of an element is the sum of the contributions of s-, r-, and p-processes, one can write:

 
$\displaystyle \epsilon_{\rm nor}(X) = \epsilon_{\rm s}(X)_{\rm nor} + \epsilon_...
...t}(X)_{\rm nor} + \epsilon_{\rm r}(X)_{\rm nor}
+ \epsilon_{\rm p}(X)_{\rm nor}$     (2)

where $\epsilon _{\rm s} (X)_{\rm nor}$, $\epsilon_{\rm sw}(X)_{\rm nor}$, and $\epsilon_{\rm st}(X)_{\rm nor}$ are, respectively, the contributions of main, weak, and strong components of s-process and $\epsilon_{\rm r} (X)_{\rm nor}$ and $\epsilon_{\rm p} (X)_{\rm nor}$ the r- and p-processes. Arlandini et al. (1999) provide detailed information about the s-process main component and r-process. According to Lugaro et al. (2003), around 50% of $\sp {86}$Sr and $\sp {87}$Sr in the solar system results from the s-process weak component; hence, the missing abundance that completes the total abundance in Arlandini et al. (1999) for these Sr isotopes was attributed to the weak component. Around 45% of $\sp {96}$Zr abundance missing in Arlandini et al. was also attributed to the s-process weak component. A few nuclides are formed mainly through the p-process, and they are not in Arlandini et al. (1999), such as $\sp {138}$La, $\sp {136,138}$Ce, $\sp {144}$Sm, $\sp {156,158}$Dy (Rayet et al. 1995). The total solar abundances adopted by Arlandini et al. (1999) were those from Anders & Grevesse (1989), and it is possible to deduce the abundance of each p-only nuclide. For nuclides that are partially p, the difference between the total abundance and the sum of s- and r-fractions from Arlandini et al. (1999) was computed, such as for $\sp {94}$Mo, $\sp {142}$Nd, $\sp {152,154}$Gd, and $\sp {160}$Dy. The isotopes $\sp {142,150}$Nd are missing in Rayet et al. (1995), however they were considered p-partial or p-only according to the missing of part or all in Arlandini et al. Once all abundance percentages were identified, it was possible to derive the abundance fractions of each process relative to the total abundance of an element, shown in Cols. 3-7 of Table 4. The total abundance of each element, taking into account its n isotopes for normal stars, can be written as

 \begin{displaymath}
\epsilon_{\rm nor}(X)= \bigg(\sum_{i}^n g_{\rm s}^i+\sum_{i}...
...\rm r}^i+
\sum_{i}^n g_{\rm p}^i \bigg)\epsilon_{\rm nor}(X)
\end{displaymath} (3)

where $g_{\rm s}^i$, $g_{\rm sw}^i$, $g_{\rm st}^i$, $g_{\rm r}^i$, and $g_{\rm p}^i$ are fractions of total abundance relative to the three s-process components, r- and p-processes, respectively, for each isotope "i''.


 

 
Table 6: Results relative to the s-, r-, and p-processes for barium stars. $\epsilon _{\rm s}(X)$, $\epsilon _{\rm sw}(X)$, and $\epsilon _{\rm st}(X)$: abundance fractions of s-process main, weak, and strong components; $\epsilon _{\rm r}(X)$ and $\epsilon _{\rm p}(X)$: abundance fractions of r- and p-processes; $\sigma N$ and $\sigma N$ (Si): cross-section times abundance fraction corresponding to the s-process main component taking the overabundance of barium stars into account on the usual scale and Si scale; $\epsilon _{\rm s} (X)_{\rm nor}$: abundance fractions of the s-process main component for normal stars; diff: $\epsilon _{\rm s}(X)- \epsilon _{\rm s}(X)_{\rm nor}$; $\sigma N$$_{\rm gs}$: cross-section times abundance fraction corresponding to the s-process main component without the overabundance of barium stars. The full table is only available in electronic form at the CDS.
A el $\epsilon _{\rm s}(X)$ $\sigma_{\epsilon_{\rm s}(X)}$ $\epsilon _{\rm sw}(X)$ $\epsilon _{\rm st}(X)$ $\epsilon _{\rm r}(X)$ $\sigma_{\epsilon_{\rm r}(X)}$ $\epsilon _{\rm p}(X)$ $\sigma_{\epsilon_{\rm p}(X)}$ $\sigma N$ $\sigma_{\sigma N}$ $\epsilon _{\rm s}(X)$ $_{\rm nor}$ $\sigma_{\epsilon \rm s(X){\rm nor}}$ diff $\sigma N$ (Si) $\sigma_{\sigma\rm N(Si)}$ $\sigma N$$_{\rm gs}$

                  HD 749              
84 Sr ... ... ... ... ... ... 4.2 1.8 ... ... ... ... ... ... ... ...
86 Sr 208.7 118.7 $37\pm16$ ... ... ... ... ... 13357 7621 32.80 13.85 175.89 0.373E+03 0.213E+03 0.324E+03
87 Sr 145.5 82.7 $23\pm9$ ... ... ... ... ... 13387 7635 22.87 9.66 122.64 0.374E+03 0.213E+03 0.325E+03
88 Sr 3427.1 1948.9 $45\pm19$ ... ... ... ... ... 21248 12127 538.70 227.51 2888.40 0.593E+03 0.339E+03 0.516E+03
89 Y 2260.2 994.0 ... ... 11.9 5.5 ... ... 42944 18935 136.79 63.17 2123.40 0.120E+04 0.529E+03 0.111E+04
90 Zr 4297.9 1992.2 ... ... 53.0 20.7 ... ... 90255 42711 137.63 53.75 4160.22 0.252E+04 0.119E+04 0.211E+04
91 Zr 1247.0 578.0 ... ... 1.8 0.7 ... ... 74821 36089 39.93 15.60 1207.09 0.209E+04 0.101E+04 0.175E+04
92 Zr 1854.7 859.7 ... ... 4.2 1.6 ... ... 61205 29325 59.39 23.20 1795.30 0.171E+04 0.820E+03 0.143E+04
94 Zr 2021.7 937.2 ... ... ... ... ... ... 52565 24450 64.74 25.29 1956.98 0.147E+04 0.683E+03 0.123E+04
96 Zr 178.5 82.7 $4.1\pm1.6$ ... ... ... ... ... 1910 890 5.72 2.23 172.75 0.533E+02 0.249E+02 0.445E+02


The uncertainty on $\log\epsilon_{\rm nor}(X)$ is calculated with

$\displaystyle \sigma_{\log\epsilon_{\rm nor}(X)}= \bigg([{\rm Fe/H}]^2\sigma_A^2+A^2\sigma^2_{[{\rm Fe/H}]}+\sigma_B^2
+ 2{\rm [Fe/H]cov}(A,B) \bigg)^{0.5}$     (4)

where ${\rm cov}(A,B)$ is the covariance between A and B. The uncertainties on abundances relative to s-, r-, and p-processes are given by


\begin{displaymath}\sigma_{\epsilon j}=\epsilon_j\sigma_{\log\epsilon_{\rm nor}(X)}\ln{10}
\end{displaymath} (5)

where "j'' corresponds to the process involved (s: main, sw: weak, st: strong, components of s-process, r: r-process, or p: p-process).

Finally, the sum of abundances from other processes except the s-process main component was computed, i.e., the sum of fractions sw, st, r, and p, indicated by subscript "o'' and its uncertainty are

 \begin{displaymath}
\epsilon_{\rm o}(X)= \bigg(\sum_{i}^n g_{\rm sw}^i+\sum_{i}^...
...g_{\rm r}^i+\sum_{i}^n g_{\rm p}^i \bigg)\epsilon_{\rm nor}(X)
\end{displaymath} (6)

and

\begin{displaymath}\sigma_{\epsilon \rm o}(X)=\epsilon_{\rm o}(X)\sigma_{\log\epsilon_{\rm nor}(X)}\ln{10}. \nonumber \\
\end{displaymath}  

Lines 2, 3, and 4 of Table 2 show abundances due to the s-process main component, r- and p-process, respectively, and line 5 shows  $\epsilon _{\rm o}(X)$.

4.2 The s-, r-, and p-processes in barium stars

Barium stars are enriched in neutron capture elements, and the excess of heavy elements can be deduced from a comparison with normal stars of similar metallicities. If the excess is due to the s-process main component, one can consider that abundances due to other processes (r, p, and other s-process components) are similar to those of normal stars with the same metallicity, i.e., $\epsilon_{\rm r} (X) = \epsilon_{\rm r}(X)_{\rm nor}$, $\epsilon_{\rm p}(X) = \epsilon_{\rm p}(X)_{\rm nor}$, $\epsilon_{\rm sw}(X) = \epsilon_{\rm sw}(X)_{\rm nor}$, and $\epsilon_{\rm st} (X) = \epsilon_{\rm st}(X)_{\rm nor}$. In this way, $\epsilon _{\rm o}(X)$ (line 5 of Table 2) was attributed to each barium star as the fraction corresponding to processes other than the s-process main component. The logarithmic mean abundances ( $\log\epsilon(X)$) shown in Tables 16 and 17 of Paper I were used to compute the fractions corresponding to each process.

The abundance fraction corresponding to the s-process main component of an element is

 \begin{displaymath}
\epsilon_{\rm s}(X)=\epsilon(X)-\epsilon_{\rm o}(X).
\end{displaymath} (7)

Table 5 shows abundances relative to the s-process main component calculated with Eq. (8). In order to characterise the overabundance of neutron capture elements in barium stars, $\epsilon _{\rm s}(X)$ values were compared to $\epsilon _{\rm s} (X)_{\rm nor}$ from Table 2, which is the fraction relative to the s-process main component in a normal star of same metallicity. Table 5 also shows the percentages $\epsilon _{\rm s}(X)/\epsilon _{\rm s}(X)_{\rm nor} \times 100$. The r-elements, Sm, Eu, Gd, and Dy, also show large overabundances, similar to those of s-elements in some cases.

Normal stars are expected to have lower abundances of heavy elements than barium stars ( $\epsilon_{\rm nor} (X) < \epsilon(X)$); however, for some elements in some stars, abundances in barium stars obtained for the present sample were much lower than those of normal stars. This is the case of Mo (HD 27271, HD 116869, HD 123396, HD 210709, HD 210910, HD 223938), Eu (HR 107), Gd (HD 210709), Dy (HD 89948), and Pb (HD 22589, HD 210910). It is not clear why these barium stars show such low abundances for these elements. For these cases, the Eq. (8) does not apply, and there is no $\epsilon _{\rm s}(X)$ for them (Table 5).

After computing the abundance relative to the s-process main component for an element in barium stars using Eq. (8), the abundance of each isotope and for each process can be determined with

 \begin{displaymath}
\epsilon_{\rm s}^i(X)=f_{\rm s}^i\epsilon_{\rm s}(X); \hskip...
...igma_{\epsilon^i_{\rm s}(X)}=f_{\rm s}^i\sigma_{\epsilon_s(X)}
\end{displaymath} (8)


\begin{displaymath}\epsilon_{\rm sw}^i(X)=f_{\rm sw}^i\epsilon_{\rm sw}(X); \hsk...
...silon^i_{\rm sw}(X)}=f_{\rm sw}^i\sigma_{\epsilon_{\rm sw}(X)}
\end{displaymath} (9)


\begin{displaymath}\epsilon_{\rm st}^i(X)=f_{\rm st}^i\epsilon_{\rm st}(X); \hsk...
...silon^i_{\rm st}(X)}=f_{\rm st}^i\sigma_{\epsilon_{\rm st}(X)}
\end{displaymath} (10)


\begin{displaymath}\epsilon_{\rm r}^i(X)=f_{\rm r}^i\epsilon_{\rm r}(X); \hskip ...
...\epsilon^i_{\rm r}(X)}=f_{\rm r}^i\sigma_{\epsilon_{\rm r}(X)}
\end{displaymath} (11)


\begin{displaymath}\epsilon_{\rm p}^i(X)=f_{\rm p}^i\epsilon_{\rm p}(X); \hskip ...
...\epsilon^i_{\rm p}(X)}=f_{\rm p}^i\sigma_{\epsilon_{\rm p}(X)}
\end{displaymath} (12)

where $f_{\rm s}^i$, $f_{\rm sw}^i$, $f_{\rm st}^i$, $f_{\rm r}^i$, and $f_{\rm p}^i$ are the abundance fractions of the corresponding isotope "i'', respectively, of the three s-process components, the r- and p-processes relative to total abundance of the involved process, shown in Cols. 8 to 12 of Table 4. The total abundance can be described by the equation
$\displaystyle \epsilon(X)= \sum_{i}^nf_{\rm s}^i\epsilon_{\rm s}(X)+\sum_{i}^nf...
...m_{i}^nf_{\rm r}^i\epsilon_{\rm r}(X)+\sum_{i}^nf_{\rm p}^i\epsilon_{\rm p}(X).$     (13)

Abundances relative to the s-process main component for each nuclide of the sample barium stars are shown in Col. 3 of Table 6, and for normal stars in Col. 13. The difference between these two columns is shown in Col. 15.
  \begin{figure}
\par\includegraphics[width=8.2cm,clip]{4968fig3}
\end{figure} Figure 3: Total abundances of heavy elements for the barium ( $\log\epsilon(X)$) and normal ( $\log\epsilon_{\rm nor}(X)$) stars with the same metallicities. Solid lines indicate $\log\epsilon_{\rm nor}(X) = \log\epsilon(X)$.


  \begin{figure}
\par\includegraphics[width=8cm,clip]{4968fig4}
\end{figure} Figure 4: Abundance fraction of heavy elements due to all processes except the s-process main component ( $\log\epsilon_{\rm o}(X)$) vs. total abundance of barium stars ( $\log\epsilon(X)$). Solid lines indicate $\log\epsilon_{\rm o}(X) = \log\epsilon(X)$.

Some elements of Table 2 are formed in larger amounts through the r-process. They are Eu (94.2%), Gd (84.54%), Dy (84.8%), and Sm (67.4%), according to Arlandini et al. (1999). For these elements, barium stars are expected to have abundance values closer to normal stars than for s-elements. It can be verified that this supposition is valid for Eu by comparing data from Tables 16 and 17 of Paper I to those from Table 2. Figure 3 shows the behaviour of $\log\epsilon_{\rm nor}(X)$ of normal stars calculated by least-square fitting with $\log\epsilon(X)$ of barium stars, and Fig. 4 shows the behaviour of $\log\epsilon(X)$ for barium stars with $\log\epsilon_{\rm o}(X)$. It is important to point out that Figs. 3 to 10, the elements were arranged in increasing order of the contribution by the s-process main component, following Arlandini et al. (1999), Eu, Gd, Dy, Sm, Pb, Pr, Mo, Nd, La, Ce, Ba, Zr, Sr, and Y. Behaviours tend to be approximately constant; however, Eu data are very close to a straight line with tangent = 1, differently from the other elements. The larger the distance of the data from tangent = 1, the larger the abundance of barium stars compared to normal stars. If the fraction corresponding to the s-process main component is withdrawn as in Fig. 4, the behaviours of Eu, Gd, and Dy are almost unaltered relative to Fig. 3; however, the change in ordinates due to the missing abundance is remarkable for the other elements.

  \begin{figure}
\par\includegraphics[width=8cm,clip]{4968fig5}
\end{figure} Figure 5: Abundances corresponding to the s-process main component for heavy elements of barium stars ( $\log\epsilon_{\rm s} (X)$) vs. normal stars ( $\log\epsilon_{\rm s}(X)_{\rm nor}$) with the same metallicities. Solid lines indicate $\log\epsilon_{\rm s} (X)_{\rm nor} = \log\epsilon_{\rm s}(X)$.


  \begin{figure}
\par\includegraphics[width=8cm,clip]{4968fig6}
\end{figure} Figure 6: $\log\epsilon_{\rm s} (X)$ vs. [Fe/H], where $\log\epsilon_{\rm s} (X)$are the abundances corresponding to the s-process main component of heavy elements in barium stars.

Figure 5 shows the behaviour of $\log\epsilon_{\rm s} (X)$ with $\log\epsilon_{\rm s}(X)_{\rm nor}$, which are the abundance fractions of the s-process main component of barium stars (Eq. (8)) and normal stars of the same metallicity, respectively. Unlike in Fig. 4, the changes in ordinates due to the missing fraction r in Eu, Gd, and Dy abundances in Fig. 5 are remarkable in comparison with Fig. 3. Figure 5 shows similar differences from tangent = 1 as in Figs. 3 and 4, making it clear that the fraction s of the abundance of barium stars leads their behaviour. The difference between the maximum and minimum values of the abundance fraction corresponding to the s-process main component of normal stars is $\Delta\log\epsilon_{\rm s}(X)_{\rm nor} \approx 1$ in the range of metallicities of the sample stars. For barium stars this difference is larger, $\Delta\log\epsilon_{\rm s}(X) \approx 2$.

According to Fig. 6, the abundance relative to the s-process main component of heavy elements is essentially independent of [Fe/H] for the present sample of barium stars.


  \begin{figure}
\par\includegraphics[width=8.4cm,clip]{4968fig7}
\end{figure} Figure 7: $\log\epsilon$(X) vs. [Fe/H] for present sample of barium stars and post-AGBs from Reyniers et al. (2004) and van Winckel & Reyniers (2000). Filled symbols indicate barium stars; squares: $\log g \ge 3.7$; triangles: $2.4 < \log g < 3.7$; circles: $\log g \le 2.4$. Open circles are post-AGBs.

4.3 Abundance ratios involving s- and r-processes

The r-process is related to the final stages of evolution of massive stars ( $M > 8 ~M \sb \odot$), whereas the s-process main component occurs in AGB stars of low (1-3  $M\sb \odot$) or intermediate (4-8  $M\sb \odot$) masses. The timescale for stars to reach the SN II ( $t < 10\sp 8$ yr) stage is less than that for stars to reach the AGB phase ($t>10\sp 8$ yr); therefore, the first heavy elements ejected in the interstellar medium of the Galaxy, which is observed in very metal-poor stars, are expected to be mainly due to the r-process (Truran et al. 2002). The products of nucleosynthesis of AGB stars to the interstellar medium, particularly the s-process main component appeared later.

It is usual to investigate the starting point of the s-process contribution by analyzing the [Eu/Ba] abundance ratio, since they are, respectively, the best representatives of the r- and s-processes. Figure 6 from Burris et al. (2000) shows the behaviour of Ba relative to Eu for normal stars of metallicities $-3 <\rm [Fe/H] <+0.5$. From the moment that the s-process starts to produce Ba, an increase in its abundance relative to Eu can be seen, since the s-process is responsible for $\sim$81% of its production, according to Arlandini et al. (1999).

Figure 7 shows $\log\epsilon$(X) vs. [Fe/H] for barium stars from the present sample and post-AGB stars from Reyniers et al. (2004) and van Winckel & Reyniers (2000). Abundances of post-AGBs are larger or similar to those of barium stars, except for Sm in one star. This is expected considering that barium stars were enriched by an AGB companion.

Figure 8 shows $\log\epsilon$(Eu) vs. $\log\epsilon(X)$, where X are heavy elements other than Eu for the present sample of barium stars and stars from the literature. From Nd to Y, for which the s-process contribution is larger, barium stars and post-AGBs are clearly overabundant, located on the high abundance end.

In the Ba panel of Fig. 8, the lowest values of $\log\epsilon$(Eu) corresponding to normal stars are close to the upper line where [Ba/Eu] = -0.70, representing Ba production only by r-process (Mashonkina et al. 2003). As $\log\epsilon$(Eu) increases, data become closer to the lower line, where data are compatible with [Ba/Eu] values for the solar ratio. Both barium and post-AGB stars values are very different from the solar ratio line.

In Fig. 9, the r-process fraction of Eu abundance [ $\log (0.942\epsilon$(Eu))] correlates with the s-process main component abundance fraction of other elements in barium stars. In Fig. 10, the r-process fraction of Eu is plotted against fractions of r-process of other elements, for the data given in Table 2. In the second, the correlation is linear with no dispersion, indicating that the s-process main component contribution causes a scatter in earlier figures. This linear correlation in Fig. 10 is expected, given that only the r part of the abundances for all involved elements were used. Strontium was not included in this figure because it does not have an r-process contribution (see Table 4).


  \begin{figure}
\par\includegraphics[width=17cm,clip]{4968fig8}
\end{figure} Figure 8: $\log\epsilon$(Eu) vs. $\log\epsilon(X)$ for normal, post-AGB, and barium stars. Normal stars from the literature are represented by symbols as in Fig. 1. Starred squares are the present sample of barium stars. Starred triangles are post-AGB from Reyniers et al. (2004) and van Winckel & Reyniers (2000). Solid lines in the Ba panel represent r-only production of Ba (upper line) and solar [Ba/Eu] (lower line).

Table 7 and Fig. 11 show [X/Eu] vs. [Fe/H] for barium and post-AGB stars. The star HD 210910 shows lower values of [X/Eu] for Y, Zr, Ba, La, Ce, Nd, Pr, and Pb, reaching negative values for [Zr/Eu] = -0.18. The value of [Sr/Eu] is low for the star HD 123396, [Sr/Eu] = -0.1. This result is expected from Fig. 13 of Paper I, which shows that the stars HD 123396 and HD 210910 present the lowest values of [SrII/Fe] and [ZrII/Fe], respectively, and their [Eu/Fe] = 0.50 and 0.54, thus very close. For other stars, [X/Eu] is in the range of $0 \leq {\rm [\textit{X}/Eu]} \leq 1.3$. The post-AGBs are also mainly in this range, the lowest value being [Zr/Eu] = -0.01. For all elements, [X/Eu] vs. [Fe/H] is approximately constant in the range of metallicities of the sample stars.

For Mo, which has a contribution of 49.76% of the s-process main component, 26.18% of the r-process and 24.06% of the p-process, [Mo/Eu] are mainly in the range $-0.4 < {\rm [Mo/Eu]} < 0.6$. Relative to Ba, the values are lower, in the range $-1.5 \leq {\rm [Mo/Ba]} \leq -0.35$. Regarding the ratios involving Pr, that has 49% of the contribution from the s-process main component and 51% from the r-process, data are mainly in the ranges $-1.01 \leq {\rm [Pr/Ba]} \leq -0.04$ and $0.12 \leq {\rm [Pr/Eu]} \leq 0.92$. There is no r-process contribution in the Pb abundance, according to Arlandini et al. (1999), while 46% of the contribution comes from s-process main component and 54% has been attributed in previous work to the s-process strong component. Data are in the ranges $-1.03 \leq \rm [Pb/Ba] \leq 0.07$and $-0.58 \leq \rm [Pb/Eu] \leq 0.86$. Abundances of Pb obtained for barium stars are usually higher than those of Mo, which are higher than those of Pr, and the same is true for solar abundances. Only for 5 stars the Mo abundance is higher than those of Pb and for one star Pr abundance is higher than that of Mo. However, the [X/Fe] values are such that the values of [Mo/Ba, Eu] are usually lower than [Pr, Pb/Ba, Eu]. As a consequence, the range for Mo involves lower values in Fig. 11.

Elements formed mainly by the s-process main component can be divided into two groups: light s-elements around the magic neutron number 50 and heavy s-elements around the magic neutron number 82. In this work, Sr, Y, Zr were included in light s-elements and Ba, La, Ce, Nd in the heavy s-elements groups. For these elements, the s-process main component contribution is larger than 50% according to Arlandini et al. (1999). It is worth emphasising that Sm is rather an r-element because its s-process contribution is less than 30%, while the r-process contributes with 67.4% of its production. The presence of light s-elements in very metal-poor stars cannot be explained entirely by an r-process contribution. For instance, there is no production of Sr by the r-process, as shown in Table 4, and it is observed in the most metal-poor stars. Another nucleosynthetic process related to massive stars is needed in order to explain such observed abundances. Figure 9, from Burris et al. (2000), shows an increasing trend of [Sr/Ba] toward lower metallicities $\rm [Fe/H] < -1$. It has been suggested that beyond the observational uncertainties, another nucleosynthesis source would explain the increasing [Sr/Ba] at lower metallicities, and this source could be the s-process weak component. According to Table 4, 14.9% of the solar abundance of Sr comes from the s-process weak component and 0.56% from the p-process. At metallicities as low as $\rm [Fe/H] < -3$, the Sr production is expected to be low, given that the s-process weak component is secondary and that in such environment there is a lack of pre-existing seed nuclei.

Abundance ratios of light s-elements relative to Ba are shown in Table 7 and Fig. 11. In the range of metallicities studied, the ratios are approximately constant in the ranges $-1 \leq \rm [Sr/Ba] \leq 0.1$, $-0.75 \leq \rm [Y/Ba] \leq 0.05$, and $-0.80 \leq \rm [Zr/Ba] \leq 0.30$. The AGB stars are included in the same range for [Zr/Ba], while for [Y/Ba] two of them show higher values, 0.25 and 0.66. Figure 9, from Burris et al. (2000), shows a dispersion around $\rm [Fe/H] \approx -1$with $ -0.55 \leq\rm [Sr/Ba] \leq 0.1$, similar to the present sample of barium stars.


  \begin{figure}
\par\includegraphics[width=8cm,clip]{4968fig9}
\end{figure} Figure 9: $\log\epsilon_{\rm r}$(Eu) vs. $\log\epsilon_{\rm s} (X)$, where $\log\epsilon_{\rm r}$(Eu) is the abundance fraction due to r-process for Eu and $\log\epsilon_{\rm s} (X)$ is that due to s-process main component for other heavy elements in barium stars.


  \begin{figure}
\par\includegraphics[width=8cm,clip]{4968fi10}
\end{figure} Figure 10: $\log\epsilon_{\rm r}$(Eu) vs. $\log\epsilon_{\rm r}(X)$, where $\log\epsilon_{\rm r}$(Eu) and $\log\epsilon_{\rm r}(X)$ are the abundance fractions due to r-process for Eu and other heavy elements in barium stars, respectively.


  \begin{figure}
\par\includegraphics[width=8cm,clip]{4968fi11}
\end{figure} Figure 11: Abundance ratios involving s- and r-processes, light and heavy s-elements. Uncertainties indicated are the highest values of Table 7 for each panel. Symbols are the same as in Fig. 7.

5 Neutron exposures

5.1 Theoretical predictions of Malaney (1987)

The s-element nucleosynthesis depends on the neutron exposure to which the seed nuclei were submitted inside the AGB star. Considering the scenario of material transfer for the barium star formation, it is reasonable to expect that the abundance patterns of barium stars show signatures of the neutron exposure during the occurrence of the s-process in the AGB companion.

Models trying to reproduce the resulting abundances of the s-process were presented by Cowley & Downs (1980), who calculated theoretical abundances by using exact solutions from Clayton & Ward (1974) for models of exponential distribution and the approximate solution from Clayton et al. (1961) for a model of single exposure.

Malaney (1987a) presented theoretical predictions of abundances from the s-process starting on iron seeds, considering single neutron exposure for several values of $\tau _{\rm o}$ and neutron density $n\sb {\rm n}$ = 10$\sp 8$ cm$\sp {-3}$. Malaney (1987b) also provides theoretical predictions, but considering an exponential neutron distribution for several values of $\tau _{\rm o}$ and two different values of neutron density, 108 cm$\sp {-3}$ and 1012 cm$\sp {-3}$.

Abundances resulting from theoretical predictions are usually normalised for $\log\epsilon_{\rm c}$(Sr) = 20. Tomkin & Lambert (1983) provide an expression to transform observational data to this scale

 \begin{displaymath}
\epsilon_{\rm c}(X)=C(y-1)\epsilon_\odot(X)
\end{displaymath} (14)

where y is the relative abundance between barium and normal stars of same metallicity

\begin{displaymath}\log y = \log\epsilon(X) - \log\epsilon_{\rm nor}(X)\end{displaymath}

where $\log\epsilon(X)$ of barium stars are those from Tables 16 and 17 of Paper I and $\log\epsilon_{\rm nor}(X)$ are those from Table 2. The value of C for each star is known by setting $\log\epsilon_{\rm c}$(Sr) = 20.

In order to check the fit, Cowley & Downs (1980) used an expression largely used in the literature (e.g. Pereira & Junqueira 2003; van Winckel & Reyniers 2000). There

 \begin{displaymath}
S^2={1\over N}\sum_{i=1}^N{(O_i-P_i)^2\over \sigma_i^2}
\end{displaymath} (15)

where O$\sb i$ are abundances $\log\epsilon_{\rm c}(X)$ for each element "i'', $P\sb i$ are theoretical predictions, N is the number of elements, and $\sigma $ is the uncertainty on $\log\epsilon_{\rm c}(X)$ calculated by

 \begin{displaymath}
\sigma_{\log\epsilon_{ \rm c}}=\sqrt{\sigma_{\log C}^2+{\sig...
...y}\over (1-10^{-\log y})^2} + \sigma^2_{\log\epsilon\odot(X)}}
\end{displaymath} (16)

with

\begin{displaymath}\sigma_{\log y}=\sqrt{\sigma^2_{\log\epsilon(X)}+\sigma^2_{\log\epsilon {\rm nor}(X)}}
\end{displaymath} (17)

and the uncertainty on C

\begin{displaymath}\sigma_{\log C}=\sqrt{{\sigma^2_{\log y}\over (1-10^{-\log y})^2} + \sigma^2_{\log\epsilon\odot(Sr)}}
\end{displaymath} (18)

where y represents Sr, considering $\sigma_{\log\epsilon _{\rm c}(Sr)} = 0$.

The best fit between theoretical predictions and observational data corresponds to the lowest value of $S\sp 2$, where $S\sp 2$ was calculated for all P values from Malaney (1987a) and Malaney (1987b) tables. Table 8 shows the best fittings of $S\sp 2$ and $\tau _{\rm o}$ for each table in Malaney. Figures 12 to 15 show the best fittings obtained for each present sample of barium star, showing the values of $\tau _{\rm o}$ and neutron density $n_{\rm n}$, in Cols. 8 and 9 of Table 8.

  \begin{figure}
\par\includegraphics[width=8.6cm,clip]{4968fi12}
\end{figure} Figure 12: Fittings of observed data to theoretical predictions by Malaney (1987b,a).


  \begin{figure}
\par\includegraphics[width=8.5cm,clip]{4968fi13}
\end{figure} Figure 13: Same as Fig. 12 for 6 other sample stars.


  \begin{figure}
\par\includegraphics[width=8.5cm,clip]{4968fi14}
\end{figure} Figure 14: Same as Fig. 12 for 6 other sample stars.


  \begin{figure}
\par\includegraphics[width=8.5cm,clip]{4968fi15}
\end{figure} Figure 15: Same as Fig. 12 for 8 other sample stars.

For some elements of some barium stars, the differences between abundances of barium and normal stars were too small, although $\epsilon_{\rm nor} (X) < \epsilon(X)$. This is the case for Mo (HD 749), Eu (HD 89948, HD 116869, HD 210709), and Gd (HD 22589). In these cases, the uncertainty on $\log\epsilon_{\rm c}(X)$ is too large, decreasing the quality of the fit. They were withdrawn before using Eq. (16), and are easily seen in Figs. 12 to 15 due their discrepant values with respect to theoretical predictions, and there are no error bars for them. Except for such cases, there is good agreement between observed and theoretical data shown in Figs. 12 to 15. For most stars, the best fit was that for which theoretical predictions consider an exponential neutron exposure distribution, with neutron density 10$\sp {12}$ cm$\sp {-3}$ for 5 stars and 10$\sp 8$ cm$\sp {-3}$ for 14 stars. For 7 stars, the best fit was found for a single neutron exposure and neutron density 10$\sp 8$ cm$\sp {-3}$. This result is curious since the exponential neutron exposure distribution is better accepted in the literature. However, Busso et al. (1999) suggest that s-process is a result of a number of single exposures instead of an exponential distribution. Pereira & Junqueira (2003) also obtained a single exposure and neutron density 10$\sp 8$ cm$\sp {-3}$ as the best fit for 2 barium stars. One of them, HD 87080 for which they found $\tau = 1.0$, is in common with the present sample, for which we found a best fit with an exponential distribution of $\tau = 0.6$ and neutron density 10$\sp 8$ cm$\sp {-3}$. The reason for this difference is unclear. The metallicities adopted were very close (see Tables 9 and 11 from Paper I); however, values of $\log\epsilon(X)$ in this work are usually higher than those from Pereira & Junqueira (2003). Least-square fittings were used here to compute abundances of normal stars (Eq. (15)), while Pereira & Junqueira (2003) use the sum of solar abundance with star metallicity as a reference.


  \begin{figure}
\par\includegraphics[width=14cm,clip]{4968fi16}
\end{figure} Figure 16: Example of the fit of parameters G and $\tau _{\rm o}$ for the barium star HD 123585. Open symbols correspond to the use of ${\partial \chi \over \partial G}=0$ and filled symbols, ${\partial \chi \over \partial \tau _{\rm o}}=0$. From left to right the plot is zoomed in order to visualise the crossing of the two functions better.

5.2 The $\sigma $N curve

Another way to evaluate the neutron exposure nature is through $\sigma N$ curves. For such, the cross-section values ( $\sigma_{\rm c}$ (30 keV), Col. 13 of Table 4) and abundances related to the s-process main component of each nuclide (from Eq. (9)) are needed. Results of the $\sigma N$ curve for each barium star are shown in Col. 11 of Table 6.

The uncertainty on $\sigma N$ is given by the expression

\begin{displaymath}\sigma_{\sigma N}=\sigma_{\rm c}\epsilon_{\rm s}(X)\sqrt{\big...
...iggl({\sigma_{\sigma\rm c}\over \sigma_{\rm c}}\biggr)^2}\cdot
\end{displaymath} (19)

In the literature, $\sigma N$ is found in Si scale, where $\epsilon$(Si) = 10$\sp 6$. Anders & Grevesse (1989) provide the following relation between the Si scale and the scale where $\log\epsilon (X)=\log(n_x/n_{\rm H}) + 12$:

\begin{displaymath}\epsilon(X)_{\rm Si} = 10^{\log\epsilon(X) - x}
\end{displaymath} (20)

where $x = 1.554 \pm 0.020$, and the uncertainty is

\begin{displaymath}\sigma_{\epsilon \rm Si}=\epsilon(X)_{\rm Si}\sqrt{(\ln{10}\sigma_{\log\epsilon \rm Si})^2+\sigma_x^2}.
\end{displaymath} (21)

To compute abundances relative to the s-process main component in the Si scale, it is necessary to transform abundances of normal stars to this scale. Then the distribution relative to each process on the Si scale is done in the same way as for the usual scales. Column 16 of Table 6 shows the results of $\sigma N = \sigma_{\rm c}\epsilon_{\rm s}(X)_{\rm Si}$ for the nuclides of barium stars.

For comparison purposes, the distribution of abundance in several nucleosynthetic processes were also done. The total abundance of the element of a barium star was distributed in solar proportions, with fractions corresponding to s-, r-, and p-processes, shown in Cols. 3 to 7 in Table 4. Results for this $\sigma N$ curve are shown in Col. 18 of Table 6, and they are represented by open symbols in Figs. 18 to 21. These results are lower than others because the overabundance derived from the s-process is neglected.

A theoretical $\sigma N$ curve is calculated with Eq. (1), where two parameters ( $\tau _{\rm o}$ and G) must be determined by fitting observed data. A robust statistics was used, which, in this work, consists in finding values of G and  $\tau _{\rm o}$ that simultaneously minimise the sum of absolute deviations represented by

\begin{displaymath}\chi = \sum\mid{f(x_k)-y_k}\mid,\end{displaymath}

where f(xk) is the theoretical value calculated with Eq. (1) and yk is the value calculated directly for $\sigma N$ by using observed data. Data very far from the curve were neglected. Figure 16 shows the functions that minimise $\chi$ relative to each parameter. The crossing point of these functions provides the values of G and $\tau _{\rm o}$ that minimise both functions simultaneously. More details on this procedure are found in Allen & Horvath (2000). Table 8 shows results of the fittings and their $\chi_{\rm red}=\chi/(n-2)$, where n is the number of data, representing the goodness of fits.


  \begin{figure}
\par\includegraphics[width=13.7cm,clip]{4968fi17}
\end{figure} Figure 17: Solar $\sigma N$ curve. Abundances related to s-process main component were taken from Arlandini et al. (1999).

The method was tested for the Sun by using data from Arlandini et al. (1999). The resulting line from the fitting is shown in Fig. 17, in which $\tau_{\rm o} = 0.345 \pm 0.005$ mb$\sp {-1}$ and G =  $0.043 \pm 0.002$%. Figure 19b from Käppeler et al. (1989) shows their solar $\sigma N$ curve, resulting in $\tau_{\rm o} = 0.30 \pm 0.01$ mb$\sp {-1}$ and $G = 0.043 \pm 0.002$%. Figures 18 to 21 show that the uncertainties, represented by error bars, are very large for barium stars, so they were neglected in computing the quality of the fit. Branching and the too discrepant data were also neglected.

For the present sample, theoretical $\sigma N$ curves fit the observed data very well, as shown in Figs. 18 to 21. This confirms that the solar isotopic composition is adequate for barium stars and that the transfer of enriched material keeps approximately the solar proportions of each nuclide. In order to build the theoretical curve, one considers that abundances of all elements heavier than iron are null at the beginning of the neutron capture chain. This supposition becomes less reasonable as the metallicity increases. Furthermore, the fit creates more than one difficulty: a) there is a lack of elements along the curve due to the difficulty in finding lines in the spectrum, thereby preventing a higher quality of the fit between theoretical and observed curves; b) barium star data show a large dispersion; c) branching values were not considered; d) the numerical solution of Eq. (1) is difficult, given that two parameters to be fitted appear in non linear form in the equation. The good agreement between theoretical and observed curves is interesting, taking all assumptions and difficulties found in their building into account.

5.3 The s-process indices

One way to relate light and heavy s-elements is through hs and ls indices, defined as the mean of the abundances of light and heavy elements, respectively. According to Sect. 4.3, Sr, Y, and Zr were included in ls, and Ba, La, Ce, and Nd were included in hs. For the s index, all these heavy and light s-elements were considered. In the case of missing abundances, such an element was excluded from the index. Figure 22 and Table 9 show [hs/ls], [ls/Fe], [hs/Fe], and [s/Fe] vs. [Fe/H], with [hs/ls] = [hs/Fe] - [ls/Fe]. Uncertainties on [s/Fe], [ls/Fe], and [hs/Fe] have to take into account the contribution of the uncertainties on abundances of each element included in the index.

A behaviour of [hs/ls] as a function of $\tau _{\rm o}$ can be inferred from the slope of the $\sigma N$ curve. The larger $\tau _{\rm o}$, the smaller the slope, and, at the same time, a smaller slope means larger abundance of heavy s-elements located at the right end of the curve. The conclusion is that the larger $\tau _{\rm o}$, the larger [hs/ls], as shown in Fig. 17 of Wallerstein et al. (1997). This is reasonable considering that the chain of formation of s-elements cannot go far if the neutron flux is low.

  \begin{figure}
\par\includegraphics[width=8.2cm,clip]{4968fi22}
\end{figure} Figure 22: [hs/ls], [ls/Fe], [hs/Fe], and [s/Fe] vs. [Fe/H]. Filled symbols indicate barium stars, as in Fig. 7; open circles are post-AGBs; crosses are data from Junqueira & Pereira (2001); open squares are data from Luck & Bond (1991); open triangles are data from North et al. (1994). The uncertainties indicated are the higher values shown in Table 9.

During the third dredge-up, a given amount of protons is introduced into the intershell, a region composed of helium located between helium and hydrogen burning shells. These protons are captured by 12C and form 13C through the reaction 12C(p, $\gamma$)13N( $\beta^+\nu$)13C or 14N through 13C(p, $\gamma$)14N, creating the 13C pocket. If the thermal pulse is independent of metallicity, protons are introduced into the intershell in the same amounts for higher or lower metallicities. It means that the neutron source $\sp {13}$C($\alpha$n)$\sp {16}$O, probably the main neutron source in AGB stars, is independent of metallicity. However, the neutron number by seed iron nucleus will be larger at low metallicities (Clayton 1988). If $\tau _{\rm o}$ is proportional to [hs/ls] and inversely proportional to [Fe/H], [hs/ls] will also be inversely proportional to [Fe/H], so it is expected that the lower the metallicity, the higher the ratio [hs/ls]. Figure 24 confirms a correlation between $\tau _{\rm o}$ and [hs/ls] for barium and post-AGB stars. However, the anticorrelation between [hs/ls] and [Fe/H] is weak for barium and post AGBs stars, as shown in Fig. 22. In the same way, the anticorrelation between $\tau _{\rm o}$ and [Fe/H] is not confirmed in Fig. 24. The yield of all s-elements to decrease with decreasing metallicities is compatible with the secondary characteristic of the s-process, which requires pre-existing seed nuclei. At intermediate metallicities ($\approx$-0.8), the Ba peak is dominant among s-process products in AGB models (Busso et al. 1999). For higher metallicities the Zr peak dominates. If giant, as well as dwarf, barium stars have the same physical origin for the accretion of enriched material from a more evolved companion, it is reasonable to expect that if the neutron exposure is higher for dwarf and more metal-deficient stars, the same occurs for giants.

In Fig. 24, $\tau _{\rm o}$ derived from the $\sigma N$ curve are mainly within 1.8 <  $\tau _{\rm o}$ < 0.6, with less spread as compared to those derived from theoretical predictions by Malaney (1987b,a), although both show the same trend. For giant stars, $\tau_{\rm o} \approx 1$ was found from theoretical predictions, but not from the $\sigma N$ curves.

Solid and dashed lines in Fig. 24 are least-square fittings, with parameters:

 \begin{displaymath}[{\rm hs/ls}]= (0.423 \pm 0.095)\tau_{\rm o} + (0.011 \pm 0.043)
\end{displaymath} (22)


 \begin{displaymath}[{\rm hs/ls}]= (0.899 \pm 0.173)\tau_{\rm o} + (-0.160 \pm 0.068)
\end{displaymath} (23)

where Eq. (23) uses $\tau _{\rm o}$ values from theoretical predictions by Malaney (1987b,a), with $\chi^2_{\rm red} = 1.710$ and Eq. (24) uses $\tau _{\rm o}$ values derived from $\sigma N$ curves, with $\chi^2_{\rm red}= 1.464$. Regarding $\chi^2_{\rm red}$, in both cases the linear and increasing correlation toward higher values of $\tau _{\rm o}$ have good quality.


  
Table 9: s-process indices: s, ls, and hs for the present sample of barium stars.
\begin{displaymath}\begin{tabular}{lrrrr}
\hline\hline
\noalign{\smallskip }
sta...
...& $0.38\pm0.32$ \\
\hline
\noalign{\smallskip }
\end{tabular} \end{displaymath}



  
Table 10: s-process indices s, ls, and hs for barium stars collected in the literature. References: N94 - North et al. (1994); LB91 - Luck & Bond (1991).
\begin{displaymath}\begin{tabular}{lrrrrr}
\hline\hline
\noalign{\smallskip }
st...
... 0.08 & N94 \\
\hline
\noalign{\smallskip }
\end{tabular}
\end{displaymath}


Figure 10 from van Winckel & Reyniers (2000) shows [hs/ls] vs. [Fe/H], including data from several previous work. Despite the dispersion, [hs/ls] increases toward higher [Fe/H]. The dependence of neutron exposure on [Fe/H] could indicate that other important parameters affect dredge-up events and nucleosynthetic processes along the red giant branch evolution.


  \begin{figure}
\par\includegraphics[width=8.6cm,clip]{4968fi23}
\end{figure} Figure 23: [hs/ls] vs. [s/Fe]. Symbols are the same as in Fig. 7. Error bars in the bottom right corner show the largest uncertainties.


  \begin{figure}
\par\includegraphics[width=8cm,clip]{4968fi24}
\end{figure} Figure 24: [hs/ls] vs. $\tau _{\rm o}$ ( upper panel), and $\tau _{\rm o}$ vs. [Fe/H] ( lower panel). Crosses are post-AGBs from Reyniers et al. (2004) and van Winckel & Reyniers (2000). Circles, triangles, and squares represent the sample of barium stars according to log g, as in Fig. 7. Open symbols correspond to $\tau _{\rm o}$ values derived from theoretical predictions by Malaney (1987b,a) and filled symbols are those from $\sigma N$ curves. The solid line is the least-square fitting with $\tau _{\rm o}$ from $\sigma N$ curves and dotted, with $\tau _{\rm o}$ from theoretical predictions.

For the present sample of barium stars, [s, ls, hs/Fe] and [hs/ls] decrease slightly toward higher metallicities in the range 0.45 $\leq$ [s/Fe] $\leq$ 1.6, 0.4 $\leq$ [ls/Fe] $\leq$ 1.6, 0.7 $\leq$ [hs/Fe] $\leq$ 1.75, and -0.2 $\leq$ [hs/ls] $\leq$ 0.7. According to Wheeler et al. (1989), [s/Fe] = 0 for less evolved stars in this same range of metallicities; therefore, the results found for the present sample show the overabundance of s-elements in barium stars.

One has to be careful in comparing the indices of the present work to those of post-AGBs in Figs. 1122, and 23, given that Reyniers et al. (2004) and van Winckel & Reyniers (2000) included Sm and not Ce in s and hs, and only Y and Zr in ls. Figure 23 shows that [hs/ls] vs. [s/Fe] has a large dispersion for barium stars, whereas there is a linear correlation for post-AGBs. Figure 8 from Reyniers et al. shows the same correlation but using different combinations of the elements included in the indices. One of them uses Ce, but the linear correlation is still present comparing with using Ba, La, Nd, and Sm in hs. Other configurations show larger dispersion, hence the presence of Ce in hs and s is not the origin of the dispersion for barium stars.

According to Table 7 and Fig. 11, there is no difference as a function of log g, confirming that the overabundances characteristic of a barium star do not depend on luminosity classes.

6 Conclusions

In this work, s-, r-, and p-processes in barium stars were studied relative to normal stars.

Abundances of elements with a lower contribution from the s-process main component are closer to the normal stars, whereas elements with a higher s-contribution are more overabundant. However, r-elements such as Sm, Eu, Gd, and Dy are also enriched in barium stars, sometimes at similar magnitudes to s-elements, and this occurs because the s-process main component chain includes the r-elements with A < 209.

The ratios involving light s-elements (Sr, Y, and Zr) and Ba, a heavy s-element, are approximately constant in the range of metallicities of the present sample, with a dispersion similar to normal stars and post-AGBs.

Considering that the abundance fraction due to all processes, except the s-process main component, was present in the proto-barium star, it was possible to isolate the fraction corresponding to the s-process main component for barium stars. The solar isotopic distribution of this abundance fraction was used to build the observed $\sigma N$ curves. Their fittings to theoretical curves indicate that it is possible to use a solar isotopic mix to estimate the contribution of the s-process main component for each isotope of an element.

The derivation of $\tau _{\rm o}$ was obtained by fitting observed data to theoretical predictions and $\sigma N$ curves. Theoretical predictions for abundances starting with Sr fit the observed data very well for the present sample, thereby providing an estimation for neutron exposure that occurred in AGB supplying the s-process. The [hs/ls] vs. $\tau _{\rm o}$ considering these theoretical predictions increases linearly, whereas no conclusion was reached for $\tau _{\rm o}$ vs. [Fe/H]. The $\tau _{\rm o}$ values from $\sigma N$ fittings also provide linear and increasing $\tau _{\rm o}$ vs. [hs/ls], but data in this case are in the range 0.2 $\leq$  $\tau _{\rm o}$ $\leq$ 0.8, showing lower dispersion than those for theoretical predictions.

Abundances obtained for barium stars are close to those for AGBs stars, but they are usually lower. This is reasonable considering that only part of the surface material of AGBs is transferred to the companion, which becomes a barium star.

Acknowledgements
We acknowledge partial financial support from the Brazilian Agencies CNPq and FAPESP. DMA acknowledges a FAPESP PhD fellowship No. 00/10405-8 and a FAPERJ post-doctoral fellowship No. 152.680/2004. We are grateful to Marcelo Porto Allen for making his robust statistics code available, and to the referee, Nils Ryde, for useful comments.

References

 

  
7 Online Material


  \begin{figure}
\par\includegraphics[width=17.4cm,clip]{4968fi18}
\end{figure} Figure 18: The $\sigma N$ curves for the sample of barium stars. Open squares represent the solar distribution of abundances (Col. 18 of Table 6) and filled squares represent the distribution taking the overabundance of barium stars into account (Col. 16 of Table 6). Error bars in the HD 749 panel at A=190 and A=195 indicate the typical errors in each region of the logarithmic scale.


  \begin{figure}
\par\includegraphics[width=17.4cm,clip]{4968fi19}
\end{figure} Figure 19: Same as Fig. 18 for 6 other sample stars.


  \begin{figure}
\par\includegraphics[width=17.4cm,clip]{4968fi20}
\end{figure} Figure 20: Same as Fig. 18 for 6 other sample stars.


  \begin{figure}
\par\includegraphics[width=17.3cm,clip]{4968fi21}
\end{figure} Figure 21: Same as Fig. 18 for 8 other sample stars.


 

 
Table 4: Cross-sections in mb$\sp {-1}$ for 30, 23, and 8 keV and abundance fractions for s-, r-, and p-processes relative to total abundance and to total abundance of each process.
A el $g_{\rm s}$ $g_{\rm sw}$ $g_{\rm st}$ $g_{\rm r}$ $g_{\rm p}$ $f_{\rm s}$ $f_{\rm sw}$ $f_{\rm st}$ $f_{\rm r}$ $f_{\rm p}$ $\sigma_{\rm c}$(30 keV) $\sigma_{\rm c}$(23 keV) $\sigma_{\rm c}$(8keV) Ref.
84 Sr ... ... ... ... 5.650e-03 ... ... ... ... 1.000e00 $368\pm126$ ... ... 1
86 Sr 4.666e-02 5.265e-02 ... ... ... 5.519e-02 3.534e-01 ... ... ... $64\pm3$ 66.80 80.10 1
87 Sr 3.253e-02 3.210e-02 ... ... ... 3.848e-02 2.155e-01 ... ... ... $92\pm4$ 101.60 126.00 1
88 Sr 7.662e-01 6.421e-02 ... ... ... 9.063e-01 4.310e-01 ... ... ... $6.2\pm0.3$ 6.60 6.00 1
    84.54% 14.90%     0.56%                  
89 Y 9.203e-01 ... ... 8.000e-02 ... 1.000e00 ... ... 1.000e00 ... $19.0\pm0.6$ 19.60 24.50 1
    92.03%     8.00%                    
90 Zr 3.716e-01 ... ... 1.429e-01 ... 4.477e-01 ... ... 8.993e-01 ... $21\pm2$ 20.80 18.90 1
91 Zr 1.078e-01 ... ... 4.785e-03 ... 1.299e-01 ... ... 3.012e-02 ... $60\pm8$ 64.70 90.50 1
92 Zr 1.604e-01 ... ... 1.122e-02 ... 1.932e-01 ... ... 7.062e-02 ... $33\pm4$ 34.60 47.20 1
94 Zr 1.748e-01 ... ... ... ... 2.106e-01 ... ... ... ... $26\pm1$ 26.60 30.10 1
96 Zr 1.542e-02 1.100e-02 ... ... ... 1.859e-02 1.000e00 ... ... ... $10.7\pm0.5$ 11.10 18.10 1
    83.00% 1.10%   15.89%                    
92 Mo ... ... ... ... 1.509e-01 ... ... ... ... 6.156e-01 $70\pm10$ ... ... 1
94 Mo 5.995e-04 ... ... ... 9.165e-02 1.205e-03 ... ... ... 3.844e-01 $102\pm20$ 103.70 120.30 1
95 Mo 8.816e-02 ... ... 7.093e-02 ... 1.772e-01 ... ... 2.710e-01 ... $292\pm12$ 301.40 322.00 1
96 Mo 1.665e-01 ... ... ... ... 3.347e-01 ... ... ... ... $112\pm8$ 118.00 150.40 1
97 Mo 5.604e-02 ... ... 3.958e-02 ... 1.126e-01 ... ... 1.512e-01 ... $339\pm14$ 352.90 387.80 1
98 Mo 1.826e-01 ... ... 5.839e-02 ... 3.669e-01 ... ... 2.231e-01 ... $99\pm7$ 100.10 111.80 1
100 Mo 3.691e-03 ... ... 9.237e-02 ... 7.418e-03 ... ... 3.548e-01 ... $108\pm14$ 106.90 110.90 1
    49.76%     26.18% 24.06%                  
130 Ba ... ... ... ... 1.060e-03 ... ... ... ... 5.124e-01 $760\pm110$ ... ... 1
132 Ba ... ... ... ... 1.009e-03 ... ... ... ... 4.876e-01 $379\pm137$ ... ... 1
134 Ba 2.427e-02 ... ... ... ... 3.003e-02 ... ... ... ... $176.0\pm5.6$ 172.10 157.90 1
135 Ba 1.726e-02 ... ... 4.877e-02 ... 2.135e-02 ... ... 2.570e-01 ... $455\pm15$ 463.50 498.40 1
136 Ba 7.860e-02 ... ... ... ... 9.726e-02 ... ... ... ... $61.2\pm2.0$ 62.20 68.60 1
137 Ba 7.348e-02 ... ... 3.875e-02 ... 9.092e-02 ... ... 2.042e-01 ... $76.3\pm2.4$ 77.40 81.90 1
138 Ba 6.146e-01 ... ... 1.022e-01 ... 7.604e-01 ... ... 5.387e-01 ... $4.0\pm0.2$ 4.00 4.80 1
    80.82%     18.97% 0.21%                  
138 La ... ... ... ... 8.893e-04 ... ... ... ... 1.000e00 ... ... ... 1
139 La 6.205e-01 ... ... 3.786e-01 ... 1.000e00 ... ... 1.000e00 ... $31.6\pm0.8$ 37.50 70.10 2
    62.05%     37.86% 0.09%                  
136 Ce ... ... ... ... 1.901e-03 ... ... ... ... 4.320e-01 $328\pm21$ ... ... 1
138 Ce ... ... ... ... 2.500e-03 ... ... ... ... 5.680e-01 $179\pm5$ ... ... 1
140 Ce 7.359e-01 ... ... 1.488e-01 ... 9.677e-01 ... ... 6.327e-01 ... $10.6\pm0.5$ ... ... 3
142 Ce 2.456e-02 ... ... 8.636e-02 ... 3.230e-02 ... ... 3.673e-01 ... $28.3\pm1.0$ ... ... 3
    76.05%     23.52%   0.44%                
141 Pr 4.868e-01 ... ... 5.132e-01 ... 1.000e00 ... ... 1.000e00 ... $111.4\pm1.4$ ... ... 3
    48.68%     51.32%                    
142 Nd 2.515e-01 ... ... ... 2.056e-02 4.535e-01 ... ... ... 2.669e-01 $35.0\pm0.7$ ... ... 1
143 Nd 3.821e-02 ... ... 8.271e-02 ... 6.890e-02 ... ... 2.246e-01 ... $245\pm3$ ... ... 1
144 Nd 1.209e-01 ... ... 1.171e-01 ... 2.180e-01 ... ... 3.178e-01 ... $81.3\pm1.5$ ... ... 1
145 Nd 2.285e-02 ... ... 6.022e-02 ... 4.121e-02 ... ... 1.635e-01 ... $425\pm5$ ... ... 1
146 Nd 1.102e-01 ... ... 6.155e-02 ... 1.986e-01 ... ... 1.671e-01 ... $91.2\pm1.0$ ... ... 1
148 Nd 1.094e-02 ... ... 4.680e-02 ... 1.973e-02 ... ... 1.270e-01 ... $147\pm2$ ... ... 1
150 Nd ... ... ... ... 5.647e-02 ... ... ... ... 7.331e-01 $159\pm10$ ... ... 1
    55.46%     36.84% 7.70%                  
144 Sm ... ... ... ... 3.096e-02 ... ... ... ... 1.000e00 $92\pm6$ ... ... 1
147 Sm 3.193e-02 ... ... 1.227e-01 ... 1.082e-01 ... ... 1.821e-01 ... $973\pm1$ ... ... 1
148 Sm 1.091e-01 ... ... ... ... 3.697e-01 ... ... ... ... $241\pm2$ ... ... 1
149 Sm 1.722e-02 ... ... 1.208e-01 ... 5.835e-02 ... ... 1.792e-01 ... $1820\pm17$ ... ... 1
150 Sm 7.392e-02 ... ... ... ... 2.504e-01 ... ... ... ... $422\pm4$ ... ... 1
152 Sm 6.115e-02 ... ... 2.055e-01 ... 2.072e-01 ... ... 3.050e-01 ... $473\pm4$ ... ... 1
154 Sm 1.815e-03 ... ... 2.249e-01 ... 6.149e-03 ... ... 3.337e-01 ... $206\pm12$ ... ... 1
    29.51%     67.39% 3.1%                  
151 Eu 3.124e-02 ... ... 4.471e-01 ... 5.409e-01 ... ... 4.744e-01 ... $3775\pm150$ ... ... 1
153 Eu 2.652e-02 ... ... 4.954e-01 ... 4.591e-01 ... ... 5.256e-01 ... $2780\pm100$ ... ... 1
    5.78%     94.25%                    
152 Gd 1.767e-03 ... ... ... 2.334e-04 1.151e-02 ... ... ... 1.846e-01 $1049\pm17$ ... ... 1
154 Gd 2.076e-02 ... ... ... 1.031e-03 1.352e-01 ... ... ... 8.153e-01 $1028\pm12$ ... ... 1
155 Gd 8.730e-03 ... ... 1.391e-01 ... 5.684e-02 ... ... 1.646e-01 ... $2648\pm30$ ... ... 1
156 Gd 3.486e-02 ... ... 1.700e-01 ... 2.270e-01 ... ... 2.011e-01 ... $615\pm5$ ... ... 1
157 Gd 1.676e-02 ... ... 1.397e-01 ... 1.091e-01 ... ... 1.653e-01 ... $1369\pm15$ ... ... 1
158 Gd 6.820e-02 ... ... 1.804e-01 ... 4.440e-01 ... ... 2.133e-01 ... $324\pm3$ ... ... 1
160 Gd 2.507e-03 ... ... 2.161e-01 ... 1.632e-02 ... ... 2.556e-01 ... $154\pm28$ ... ... 1
    15.36%     84.53% 0.13%                  
156 Dy ... ... ... ... 5.601e-04 ... ... ... ... 1.256e-01 $1567\pm145$ ... ... 1
158 Dy ... ... ... ... 9.580e-04 ... ... ... ... 2.149e-01 $1060\pm400$ ... ... 1
160 Dy 2.043e-02 ... ... ... 2.940e-03 1.385e-01 ... ... ... 6.595e-01 $890\pm12$ ... ... 1
161 Dy 1.044e-02 ... ... 1.784e-01 ... 7.079e-02 ... ... 2.104e-01 ... $1964\pm19$ ... ... 1
162 Dy 4.156e-02 ... ... 2.144e-01 ... 2.818e-01 ... ... 2.528e-01 ... $446\pm4$ ... ... 1
163 Dy 8.921e-03 ... ... 2.400e-01 ... 6.048e-02 ... ... 2.830e-01 ... $1112\pm11$ ... ... 1
164 Dy 6.615e-02 ... ... 2.152e-01 ... 4.485e-01 ... ... 2.537e-01 ... $212.0\pm3.0$ ... ... 1
    14.75%     84.80% 0.45%                  
204 Pb 1.841e-02 ... 1.119e-03 ... ... 3.997e-02 ... 2.074e-03 ... ... $89.0\pm5.5$ ... ... 1
206 Pb 1.096e-01 ... 7.992e-02 ... ... 2.380e-01 ... 1.481e-01 ... ... $15.8\pm0.8$ ... ... 1
207 Pb 1.311e-01 ... 7.481e-02 ... ... 2.845e-01 ... 1.387e-01 ... ... $9.7\pm1.3$ ... ... 1
208 Pb 2.014e-01 ... 3.836e-01 ... ... 4.372e-01 ... 7.111e-01 ... ... $0.36\pm0.03$ ... ... 1
    46.05%   53.94%                      

Cross-section references: 1 - Bao et al. (2000), 2 - O'Brien et al. (2003), 3 - Arlandini et al. (1999).


 

 
Table 5: Abundance fractions corresponding to the s-process main component for barium stars calculated with Eq. (8) (upper table) and percentage of abundance (lower table) relative to the s-process main component of a barium star compared to normal stars of a same metallicity ( $\epsilon _{\rm s}(X)/\epsilon _{\rm s}(X)_{\rm nor} \times 100$).

Star
$\epsilon_{\rm s}$(Sr) $\epsilon_{\rm s}$(Y) $\epsilon_{\rm s}$(Zr) $\epsilon_{\rm s}$(Mo) $\epsilon_{\rm s}$(Ba) $\epsilon_{\rm s}$(La) $\epsilon_{\rm s}$(Ce) $\epsilon_{\rm s}$(Pr) $\epsilon_{\rm s}$(Nd) $\epsilon_{\rm s}$(Sm) $\epsilon_{\rm s}$(Eu) $\epsilon_{\rm s}$(Gd) $\epsilon_{\rm s}$(Dy) $\epsilon_{\rm s}$(Pb)

HD 749
$3781\pm2150$ $2260\pm994$ $9600\pm4450$ $63\pm64$ $1771\pm784$ $207\pm94$ $1364\pm600$ $28\pm18$ $512\pm241$ $70\pm35$ $3\pm3$ $14\pm21$ $106\pm74$ $144\pm126$
HR 107 $2237\pm791$ $294\pm28$ $614\pm74$ $127\pm45$ $512\pm60$ $24\pm4$ $53\pm7$ $5\pm1$ $20\pm4$ $6\pm2$ ... $16\pm5$ ... $288\pm135$
HD 5424 $1012\pm579$ $522\pm230$ $2517\pm1169$ $26\pm23$ $1132\pm498$ $131\pm58$ $1027\pm450$ $30\pm18$ $410\pm190$ $52\pm25$ $1.4\pm1.4$ $7\pm9$ $197\pm129$ $303\pm211$
HD 8270 $2790\pm980$ $580\pm54$ $1475\pm173$ $110\pm39$ $652\pm76$ $48\pm7$ $127\pm15$ $4\pm1$ $52\pm8$ $6\pm2$ $0.92\pm0.61$ $5\pm2$ $2\pm1$ $89\pm47$
HD 12392 $4179\pm2362$ $2147\pm944$ $6854\pm3182$ $169\pm118$ $3331\pm1465$ $406\pm181$ $1792\pm786$ $83\pm49$ $647\pm302$ $226\pm106$ $5\pm4$ $28\pm32$ $60\pm44$ $918\pm638$
HD 13551 $3366\pm1178$ $758\pm70$ $1481\pm174$ $176\pm58$ $704\pm82$ $45\pm7$ $144\pm17$ $5\pm1$ $50\pm8$ $8\pm2$ $0.33\pm0.47$ $13\pm4$ $3\pm1$ $85\pm45$
HD 22589 $3748\pm1318$ $619\pm58$ $2463\pm288$ $49\pm26$ $543\pm64$ $32\pm5$ $71\pm9$ $3\pm1$ $24\pm4$ $3\pm1$ $0.70\pm0.69$ $2\pm2$ $3\pm1$ ...
HD 27271 $3177\pm1812$ $1075\pm475$ $3459\pm1620$ ... $816\pm365$ $51\pm26$ $182\pm82$ $9\pm7$ $67\pm36$ $16\pm10$ $2.4\pm2.8$ $10\pm17$ $12\pm14$ $109\pm100$
HD 48565 $2451\pm857$ $421\pm39$ $1462\pm170$ $53\pm20$ $620\pm72$ $77\pm11$ $474\pm55$ $13\pm2$ $136\pm19$ $20\pm4$ $0.59\pm0.42$ $13\pm4$ $16\pm3$ $467\pm209$
HD 76225 $8244\pm2868$ $1259\pm117$ $3524\pm410$ $142\pm50$ $1457\pm169$ $105\pm15$ $281\pm33$ $11\pm2$ $74\pm11$ $13\pm3$ $0.85\pm0.69$ $12\pm4$ $10\pm2$ $285\pm135$
HD 87080 $3366\pm1178$ $812\pm75$ $3196\pm371$ $61\pm24$ $1476\pm171$ $265\pm37$ $977\pm113$ $27\pm4$ $365\pm51$ $46\pm9$ $3.8\pm1.3$ $34\pm9$ $75\pm11$ $346\pm159$
HD 89948 $5506\pm1923$ $915\pm85$ $2078\pm244$ $112\pm42$ $651\pm76$ $54\pm8$ $125\pm15$ $7\pm1$ $56\pm9$ $10\pm3$ $0.33\pm0.58$ $6\pm3$ ... $76\pm44$
HD 92545 $3670\pm1300$ $563\pm53$ $1624\pm193$ $128\pm52$ $1113\pm130$ $47\pm7$ $147\pm18$ $7\pm1$ $46\pm8$ $8\pm3$ $2.4\pm1.2$ $5\pm3$ $7\pm2$ $302\pm148$
HD 106191 $2088\pm743$ $723\pm67$ $2352\pm275$ $114\pm43$ $515\pm61$ $28\pm4$ $102\pm12$ $14\pm2$ $36\pm6$ $11\pm3$ $0.55\pm0.64$ $11\pm4$ $10\pm2$ $179\pm90$
HD 107574 $3277\pm1144$ $442\pm41$ $978\pm115$ $175\pm56$ $1923\pm222$ $53\pm8$ $145\pm17$ $5\pm1$ $54\pm8$ $10\pm2$ $1.45\pm0.65$ $5\pm2$ $6\pm1$ $268\pm123$
HD 116869 $735\pm440$ $314\pm140$ $869\pm417$ ... $660\pm294$ $55\pm26$ $187\pm84$ $8\pm6$ $92\pm45$ $14\pm8$ $0.3\pm1.3$ $5\pm10$ $21\pm18$ $279\pm202$
HD 123396 $144\pm84$ $56\pm25$ $394\pm184$ ... $170\pm75$ $16\pm7$ $134\pm59$ $4\pm3$ $64\pm30$ $9\pm5$ $0.26\pm0.36$ $5\pm5$ $15\pm10$ $88\pm61$
HD 123585 $4987\pm1737$ $1248\pm115$ $2980\pm346$ $262\pm83$ $2716\pm314$ $199\pm28$ $804\pm93$ $30\pm4$ $236\pm33$ $51\pm10$ $5.9\pm1.7$ $12\pm4$ $19\pm3$ $1031\pm458$
HD 147609 $112924\pm4479$ $2291\pm211$ $5047\pm584$ $144\pm48$ $1755\pm203$ $203\pm28$ $768\pm89$ $25\pm4$ $204\pm29$ $42\pm8$ $4.8\pm1.5$ $25\pm7$ $24\pm4$ $173\pm83$
HD 150862 $3616\pm1283$ $1647\pm153$ $4128\pm482$ $177\pm67$ $1116\pm131$ $60\pm9$ $134\pm16$ $8\pm1$ $38\pm7$ $8\pm3$ $1.15\pm0.98$ $9\pm4$ $9\pm3$ $317\pm155$
HD 188985 $4358\pm1527$ $900\pm83$ $2957\pm345$ $112\pm42$ $1070\pm125$ $95\pm14$ $425\pm49$ $14\pm2$ $149\pm21$ $23\pm5$ $1.14\pm0.76$ $17\pm5$ $7\pm2$ $374\pm174$
HD 210709 $944\pm587$ $526\pm235$ $2158\pm1024$ ... $639\pm289$ $50\pm26$ $242\pm109$ $8\pm6$ $97\pm50$ $13\pm9$ $0.3\pm2.1$ ... $11\pm14$ $185\pm154$
HD 210910 $2807\pm1580$ $254\pm114$ 357 $\pm180$ ... $547\pm244$ $29\pm14$ $93\pm42$ $13\pm8$ $37\pm20$ $8\pm5$ $3.1\pm2.4$ $16\pm18$ $8\pm9$ ...
HD 222349 $2442\pm945$ $439\pm185$ $1536\pm948$ $52\pm22$ $758\pm434$ $69\pm29$ $297\pm108$ $7\pm4$ $118\pm70$ $16\pm12$ $0.20\pm0.32$ $9\pm12$ $12\pm15$ $578\pm248$
BD+18 5215 $3880\pm1353$ $515\pm48$ $2072\pm241$ $111\pm37$ $1151\pm133$ $59\pm8$ $189\pm22$ $9\pm1$ $52\pm8$ $13\pm3$ $0.3\pm0.4$ $52\pm13$ $13\pm2$ $60\pm33$
HD 223938 $1654\pm853$ $418\pm41$ $2024\pm179$ ... $982\pm88$ $63\pm10$ $242\pm34$ $6\pm1$ $145\pm17$ $22\pm3$ $1.5\pm1.8$ $9\pm3$ $18\pm2$ $350\pm258$

Star
Sr(%) Y(%) Zr(%) Mo(%) Ba(%) La(%) Ce(%) Pr(%) Nd(%) Sm(%) Eu(%) Gd(%) Dy(%) Pb(%)

HD 749
636 1652 3123 185 2020 1654 6526 1166 3650 2987 1508 795 6715 404
HR 107 758 464 382 728 1159 440 514 392 274 421 ... 1755 ... 1609
HD 5424 534 1337 2362 224 3955 4015 15334 3274 8525 5487 1657 1293 32236 2619
HD 8270 1087 1066 1045 724 1691 1029 1398 341 813 514 888 609 268 570
HD 12392 809 1830 2539 568 4357 3820 9851 3890 5253 10711 2604 1844 4262 2953
HD 13551 1374 1466 1096 1206 1912 1019 1664 439 821 671 334 1755 358 570
HD 22589 1029 775 1261 231 1000 452 553 183 276 176 513 142 317 ...
HD 27271 573 849 1201 ... 996 439 934 396 506 732 1280 595 804 326
HD 48565 1522 1290 1596 545 2542 2862 8336 1591 3306 2377 824 2621 2914 4749
HD 76225 2485 1746 1968 731 2942 1666 2404 756 915 910 673 1251 981 1422
HD 87080 1374 1570 2365 419 4011 5984 11296 2417 5971 3973 3848 4627 9942 2322
HD 89948 1621 1236 1136 560 1285 828 1042 497 671 676 259 606 ... 369
HD 92545 710 480 601 430 1456 444 810 343 374 402 1336 342 483 972
HD 106191 601 953 1258 560 993 418 831 946 429 746 417 1093 1002 854
HD 107574 1729 1134 918 1532 6716 1604 2164 605 1118 1083 1773 943 1023 2322
HD 116869 227 447 496 ... 1364 896 1641 559 1156 977 241 539 2257 1422
HD 123396 337 737 1474 ... 2565 2817 8848 1743 5382 3318 1004 2514 8375 3328
HD 123585 2235 2673 2404 1964 8085 5023 10199 2859 4219 4747 6372 1755 2702 495
HD 147609 5400 4546 3815 1010 4879 4725 9087 2297 3414 3666 4903 3533 3192 1193
HD 150862 668 1334 1464 569 1395 534 702 356 298 388 623 542 613 972
HD 188985 1283 1216 1616 560 2112 1461 3552 903 1791 1547 881 1691 672 1820
HD 210709 152 365 672 ... 696 381 1106 299 660 517 137 ... 673 81
HD 210910 973 411 227 ... 1267 533 914 986 512 606 2718 1808 982 ...
HD 222349 1553 1380 1714 545 3176 2643 5333 958 2931 2008 282 1869 2203 6009
BD+18 5215 1954 1255 1862 930 3840 1717 2692 980 1041 1307 353 8625 1978 7596
HD 223938 547 642 1233 ... 2173 1107 2274 454 1950 1629 1288 979 1988 495



 

 
Table 7: [X/Eu] ( upper table) and [X/Ba] ( lower table) for the barium stars.

Star
[Sr/Eu] [Y/Eu] [Zr/Eu] [Mo/Eu] [Ba/Eu] [La/Eu] [Ce/Eu] [Nd/Eu] [Pr/Eu] [Pb/Eu]

HD 749
$0.35\pm0.21$ $0.85\pm0.12$ $1.12\pm0.14$ $-0.20\pm0.21$ $0.85\pm0.13$ $0.93\pm0.12$ $1.17\pm0.13$ $1.00\pm0.13$ $0.56\pm0.25$ $0.05\pm0.27$
HR 107 $0.71\pm0.18$ $0.56\pm0.10$ $0.53\pm0.10$ $0.56\pm0.16$ $0.91\pm0.11$ $0.63\pm0.10$ $0.37\pm0.10$ $0.28\pm0.10$ $0.48\pm0.18$ $0.86\pm0.22$
HD 5424 $0.14\pm0.21$ $0.57\pm0.12$ $0.89\pm0.14$ $-0.26\pm0.21$ $1.02\pm0.13$ $1.09\pm0.12$ $1.40\pm0.13$ $1.26\pm0.13$ $0.92\pm0.25$ $0.64\pm0.27$
HD 8270 $0.58\pm0.18$ $0.63\pm0.10$ $0.68\pm0.10$ $0.28\pm0.16$ $0.79\pm0.11$ $0.68\pm0.10$ $0.51\pm0.10$ $0.41\pm0.10$ $0.16\pm0.18$ $0.18\pm0.22$
HD 12392 $0.30\pm0.21$ $0.73\pm0.12$ $0.88\pm0.14$ $0.02\pm0.21$ $1.03\pm0.13$ $1.13\pm0.12$ $1.19\pm0.13$ $1.01\pm0.13$ $0.91\pm0.25$ $0.67\pm0.27$
HD 13551 $0.79\pm0.18$ $0.87\pm0.10$ $0.81\pm0.10$ $0.59\pm0.16$ $0.95\pm0.11$ $0.78\pm0.10$ $0.70\pm0.10$ $0.52\pm0.10$ $0.36\pm0.18$ $0.29\pm0.22$
HD 22589 $0.67\pm0.18$ $0.62\pm0.10$ $0.86\pm0.10$ $-0.01\pm0.16$ $0.67\pm0.11$ $0.49\pm0.10$ $0.24\pm0.10$ $0.11\pm0.10$ $0.06\pm0.18$ $-0.36\pm0.22$
HD 27271 $0.33\pm0.21$ $0.58\pm0.12$ $0.73\pm0.14$ $-0.35\pm0.21$ $0.57\pm0.13$ $0.41\pm0.12$ $0.35\pm0.13$ $0.22\pm0.13$ $0.18\pm0.25$ $0.00\pm0.27$
HD 48565 $0.69\pm0.18$ $0.66\pm0.10$ $0.84\pm0.10$ $0.15\pm0.16$ $0.94\pm0.11$ $1.04\pm0.10$ $1.25\pm0.10$ $0.96\pm0.10$ $0.74\pm0.18$ $1.00\pm0.22$
HD 76225 $1.01\pm0.18$ $0.92\pm0.10$ $1.01\pm0.10$ $0.35\pm0.16$ $1.10\pm0.11$ $0.97\pm0.10$ $0.81\pm0.10$ $0.52\pm0.10$ $0.50\pm0.18$ $0.60\pm0.22$
HD 87080 $0.34\pm0.18$ $0.45\pm0.10$ $0.69\pm0.10$ $-0.26\pm0.16$ $0.82\pm0.11$ $1.08\pm0.10$ $1.07\pm0.10$ $0.90\pm0.10$ $0.58\pm0.18$ $0.39\pm0.22$
HD 89948 $0.92\pm0.18$ $0.86\pm0.10$ $0.87\pm0.10$ $0.34\pm0.16$ $0.83\pm0.11$ $0.77\pm0.10$ $0.55\pm0.10$ $0.49\pm0.10$ $0.44\pm0.18$ $0.19\pm0.22$
HD 92545 $0.41\pm0.18$ $0.32\pm0.10$ $0.43\pm0.10$ $0.08\pm0.16$ $0.72\pm0.11$ $0.40\pm0.10$ $0.28\pm0.10$ $0.10\pm0.10$ $0.12\pm0.18$ $0.38\pm0.22$
HD 106191 $0.45\pm0.18$ $0.71\pm0.10$ $0.87\pm0.10$ $0.30\pm0.16$ $0.68\pm0.11$ $0.46\pm0.10$ $0.41\pm0.10$ $0.28\pm0.10$ $0.64\pm0.18$ $0.45\pm0.22$
HD 107574 $0.63\pm0.18$ $0.49\pm0.10$ $0.48\pm0.10$ $0.43\pm0.16$ $1.24\pm0.11$ $0.69\pm0.10$ $0.55\pm0.10$ $0.39\pm0.10$ $0.23\pm0.18$ $0.58\pm0.22$
HD 116869 $0.09\pm0.21$ $0.43\pm0.12$ $0.52\pm0.14$ $-0.36\pm0.21$ $0.86\pm0.13$ $0.80\pm0.12$ $0.74\pm0.13$ $0.70\pm0.13$ $0.48\pm0.25$ $0.69\pm0.27$
HD 123396 $-0.10\pm0.21$ $0.20\pm0.12$ $0.69\pm0.14$ $-0.70\pm0.21$ $0.80\pm0.13$ $0.77\pm0.12$ $1.12\pm0.13$ $1.05\pm0.13$ $0.70\pm0.25$ $0.70\pm0.27$
HD 123585 $0.38\pm0.18$ $0.51\pm0.10$ $0.53\pm0.10$ $0.17\pm0.16$ $0.96\pm0.11$ $0.82\pm0.10$ $0.86\pm0.10$ $0.58\pm0.10$ $0.48\pm0.18$ $0.72\pm0.22$
HD 147609 $0.85\pm0.18$ $0.83\pm0.10$ $0.82\pm0.10$ $-0.01\pm0.16$ $0.83\pm0.11$ $0.89\pm0.10$ $0.90\pm0.10$ $0.58\pm0.10$ $0.48\pm0.18$ $0.04\pm0.22$
HD 150862 $0.50\pm0.18$ $0.88\pm0.10$ $0.92\pm0.10$ $0.30\pm0.16$ $0.83\pm0.11$ $0.60\pm0.10$ $0.35\pm0.10$ $0.14\pm0.10$ $0.25\pm0.18$ $0.50\pm0.22$
HD 188985 $0.69\pm0.18$ $0.73\pm0.10$ $0.89\pm0.10$ $0.21\pm0.16$ $0.91\pm0.11$ $0.87\pm0.10$ $0.94\pm0.10$ $0.75\pm0.10$ $0.53\pm0.18$ $0.66\pm0.22$
HD 210709 $0.01\pm0.21$ $0.45\pm0.12$ $0.71\pm0.14$ $-0.38\pm0.21$ $0.65\pm0.13$ $0.60\pm0.12$ $0.66\pm0.13$ $0.55\pm0.13$ $0.31\pm0.25$ $0.37\pm0.27$
HD 210910 $0.32\pm0.21$ $0.00\pm0.12$ $-0.18\pm0.14$ $-0.73\pm0.21$ $0.45\pm0.13$ $0.20\pm0.12$ $0.11\pm0.13$ $0.01\pm0.13$ $0.32\pm0.25$ $-0.58\pm0.27$
HD 222349 $0.81\pm0.18$ $0.79\pm0.10$ $0.98\pm0.10$ $0.26\pm0.16$ $1.14\pm0.11$ $1.11\pm0.10$ $1.16\pm0.10$ $1.02\pm0.10$ $0.65\pm0.18$ $1.21\pm0.22$
BD+18 5215 $0.91\pm0.18$ $0.77\pm0.10$ $1.01\pm0.10$ $0.46\pm0.16$ $1.22\pm0.11$ $0.95\pm0.10$ $0.87\pm0.10$ $0.59\pm0.10$ $0.64\pm0.18$ $0.21\pm0.22$
HD 223938 $0.24\pm0.21$ $0.37\pm0.12$ $0.69\pm0.14$ $-0.45\pm0.21$ $0.85\pm0.13$ $0.67\pm0.12$ $0.67\pm0.13$ $0.71\pm0.13$ $0.20\pm0.25$ $0.60\pm0.27$

Star
[Sr/Ba] [Y/Ba] [Zr/Ba] [Mo/Ba] [Pb/Ba] [Pr/Ba] [Sm/Ba] [Gd/Ba] [Dy/Ba]  

HD 749
$-0.50\pm0.20$ $0.00\pm0.10$ $0.27\pm0.13$ $-1.05\pm0.20$ $-0.80\pm0.26$ $-0.29\pm0.24$ $-0.25\pm0.13$ $-0.86\pm0.35$ $-0.26\pm0.23$  
HR 107 $-0.20\pm0.17$ $-0.35\pm0.07$ $-0.38\pm0.07$ $-0.35\pm0.14$ $-0.05\pm0.21$ $-0.43\pm0.17$ $-0.65\pm0.11$ $-0.40\pm0.12$ ...  
HD 5424 $-0.88\pm0.20$ $-0.45\pm0.10$ $-0.13\pm0.13$ $-1.28\pm0.20$ $-0.38\pm0.26$ $-0.10\pm0.24$ $-0.21\pm0.13$ $-1.03\pm0.35$ $0.17\pm0.23$  
HD 8270 $-0.21\pm0.17$ $-0.16\pm0.07$ $-0.11\pm0.07$ $-0.51\pm0.14$ $-0.61\pm0.21$ $-0.63\pm0.17$ $-0.74\pm0.11$ $-0.86\pm0.12$ $-1.07\pm0.09$  
HD 12392 $-0.73\pm0.20$ $-0.30\pm0.10$ $-0.15\pm0.13$ $-1.01\pm0.20$ $-0.36\pm0.26$ $-0.12\pm0.24$ $-0.04\pm0.13$ $-0.94\pm0.35$ $-0.76\pm0.23$  
HD 13551 $-0.16\pm0.17$ $-0.08\pm0.07$ $-0.14\pm0.07$ $-0.36\pm0.14$ $-0.66\pm0.21$ $-0.59\pm0.17$ $-0.71\pm0.11$ $-0.61\pm0.12$ $-1.07\pm0.09$  
HD 22589 $0.00\pm0.17$ $-0.05\pm0.07$ $0.19\pm0.07$ $-0.68\pm0.14$ $-1.03\pm0.21$ $-0.61\pm0.17$ $-0.80\pm0.11$ $-0.85\pm0.12$ $-0.84\pm0.09$  
HD 27271 $-0.24\pm0.20$ $0.01\pm0.10$ $0.16\pm0.13$ $-0.92\pm0.20$ $-0.57\pm0.26$ $-0.39\pm0.24$ $-0.47\pm0.13$ $-0.63\pm0.35$ $-0.68\pm0.23$  
HD 48565 $-0.25\pm0.17$ $-0.28\pm0.07$ $-0.10\pm0.07$ $-0.79\pm0.14$ $0.06\pm0.21$ $-0.20\pm0.17$ $-0.34\pm0.11$ $-0.60\pm0.12$ $-0.60\pm0.09$  
HD 76225 $-0.09\pm0.17$ $-0.18\pm0.07$ $-0.09\pm0.07$ $-0.75\pm0.14$ $-0.50\pm0.21$ $-0.60\pm0.17$ $-0.82\pm0.11$ $-0.91\pm0.12$ $-1.06\pm0.09$  
HD 87080 $-0.48\pm0.17$ $-0.37\pm0.07$ $-0.13\pm0.07$ $-1.08\pm0.14$ $-0.43\pm0.21$ $-0.24\pm0.17$ $-0.36\pm0.11$ $-0.58\pm0.12$ $-0.34\pm0.09$  
HD 89948 $0.09\pm0.17$ $0.03\pm0.07$ $0.04\pm0.07$ $-0.49\pm0.14$ $-0.64\pm0.21$ $-0.39\pm0.17$ $-0.56\pm0.11$ $-0.74\pm0.12$ $-1.30\pm0.09$  
HD 92545 $-0.31\pm0.17$ $-0.40\pm0.07$ $-0.29\pm0.07$ $-0.64\pm0.14$ $-0.34\pm0.21$ $-0.60\pm0.17$ $-0.80\pm0.11$ $-0.90\pm0.12$ $-0.95\pm0.09$  
HD 106191 $-0.23\pm0.17$ $0.03\pm0.07$ $0.19\pm0.07$ $-0.38\pm0.14$ $-0.23\pm0.21$ $-0.04\pm0.17$ $-0.42\pm0.11$ $-0.48\pm0.12$ $-0.59\pm0.09$  
HD 107574 $-0.61\pm0.17$ $-0.75\pm0.07$ $-0.76\pm0.07$ $-0.81\pm0.14$ $-0.66\pm0.21$ $-1.01\pm0.17$ $-1.07\pm0.11$ $-1.35\pm0.12$ $-1.37\pm0.09$  
HD 116869 $-0.77\pm0.20$ $-0.43\pm0.10$ $-0.34\pm0.13$ $-1.22\pm0.20$ $-0.17\pm0.26$ $-0.38\pm0.24$ $-0.46\pm0.13$ $-0.80\pm0.35$ $-0.47\pm0.23$  
HD 123396 $-0.90\pm0.20$ $-0.60\pm0.10$ $-0.11\pm0.13$ $-1.50\pm0.20$ $-0.10\pm0.26$ $-0.10\pm0.24$ $-0.11\pm0.13$ $-0.49\pm0.35$ $-0.11\pm0.23$  
HD 123585 $-0.58\pm0.17$ $-0.45\pm0.07$ $-0.43\pm0.07$ $-0.79\pm0.14$ $-0.24\pm0.21$ $-0.48\pm0.17$ $-0.59\pm0.11$ $-1.24\pm0.12$ $-1.15\pm0.09$  
HD 147609 $0.02\pm0.17$ $0.00\pm0.07$ $-0.01\pm0.07$ $-0.84\pm0.14$ $-0.79\pm0.21$ $-0.35\pm0.17$ $-0.48\pm0.11$ $-0.77\pm0.12$ $-0.87\pm0.09$  
HD 150862 $-0.33\pm0.17$ $0.05\pm0.07$ $0.09\pm0.07$ $-0.53\pm0.14$ $-0.33\pm0.21$ $-0.58\pm0.17$ $-0.80\pm0.11$ $-0.80\pm0.12$ $-0.89\pm0.09$  
HD 188985 $-0.22\pm0.17$ $-0.18\pm0.07$ $-0.02\pm0.07$ $-0.70\pm0.14$ $-0.25\pm0.21$ $-0.38\pm0.17$ $-0.48\pm0.11$ $-0.66\pm0.12$ $-1.01\pm0.09$  
HD 210709 $-0.64\pm0.20$ $-0.20\pm0.10$ $0.06\pm0.13$ $-1.03\pm0.20$ $-0.28\pm0.26$ $-0.34\pm0.24$ $-0.43\pm0.13$ $-0.78\pm0.35$ $-0.58\pm0.23$  
HD 210910 $-0.13\pm0.20$ $-0.45\pm0.10$ $-0.63\pm0.13$ $-1.18\pm0.20$ $-1.03\pm0.26$ $-0.13\pm0.24$ $-0.58\pm0.13$ $-0.43\pm0.35$ $-0.69\pm0.23$  
HD 222349 $-0.33\pm0.17$ $-0.35\pm0.07$ $-0.16\pm0.07$ $-0.88\pm0.14$ $0.07\pm0.21$ $-0.49\pm0.17$ $-0.50\pm0.11$ $-0.81\pm0.12$ $-0.79\pm0.09$  
BD+18 5215 $-0.31\pm0.17$ $-0.45\pm0.07$ $-0.21\pm0.07$ $-0.76\pm0.14$ $-1.01\pm0.21$ $-0.58\pm0.17$ $-0.76\pm0.11$ $-0.31\pm0.12$ $-0.92\pm0.09$  
HD 223938 $-0.61\pm0.20$ $-0.48\pm0.10$ $-0.16\pm0.13$ $-1.30\pm0.20$ $-0.25\pm0.26$ $-0.65\pm0.24$ $-0.47\pm0.13$ $-0.85\pm0.35$ $-0.71\pm0.23$  



 

 
Table 8: Results of neutron exposures. Columns 2 and 3 correspond to results of the fittings to the theoretical predictions of Malaney (1987a) and Cols. 4 to 7 to those of Malaney (1987b). $S\sp 2$(u), $S\sp 2$(e8), $S\sp 2$(e12) are the fit quality, respectively, for single exposure, exponential exposure under neutron density 10$\sp 8$ cm$\sp {-3}$, and exponential exposure under neutron density 10$\sp {12}$ cm$\sp {-3}$. $\tau _{\rm o}^{\rm a}$, $\tau _{\rm o}^{\rm b}$, and $\tau _{\rm o}^{\rm c}$ are the mean distributions of neutron exposure corresponding to $S\sp 2$(u), $S\sp 2$(e8), and $S\sp 2$(e12), respectively. $\tau _{\rm o}$(f) and $n\sb {\rm n}$ are results corresponding to smaller $S\sp 2$. Column 10 shows if the best fit corresponds to exponential (exp) or single (sing) exposure. Columns 11 to 13 correspond to the results of the fit of $\sigma N$ curves, with $\chi _{\rm red}$ as the quality of the fit. Numbers in parenthesis are errors in last decimals and were estimated directly from the fittings. The uncertainties on $\tau _{\rm o}^{\rm a}$, $\tau _{\rm o}^{\rm b}$, and  $\tau _{\rm o}^{\rm c}$ were estimated in 0.1 mb$\sp {-1}$. For all cases, $\tau _{\rm o}$ is given in mb$\sp {-1}$.

Star
S2(u) $\tau _{\rm o}^{\rm a}$ S2(e8) $\tau _{\rm o}^{\rm b}$ S2(e12) $\tau_{\rm o}^c$ $\tau _{\rm o}$(f) $n_{\rm n}$ exp $\tau _{\rm o}$($\sigma N$) G(%) $\chi _{\rm red}$

HD 749
0.69 1.00 0.52 0.80 0.77 0.80 0.8 108 exp 0.406(5) 0.568(19) 0.73
HR 107 0.98 0.10 1.47 0.20 1.30 0.30 0.1 108 sing 0.43(6) 0.083(20) 0.56
HD 5424 0.85 1.10 1.15 0.80 1.71 0.80 1.1 108 sing 1.05(1) 0.086(1) 0.94
HD 8270 1.33 0.90 1.21 0.20 1.46 0.30 0.2 108 exp 0.27(1) 0.35(3) 0.41
HD 12392 0.46 1.10 0.38 0.80 0.79 0.80 0.8 108 exp 0.40(2) 0.73(3) 0.59
HD 13551 1.57 0.90 1.25 0.20 1.44 0.30 0.2 108 exp 0.22(1) 1.06(56) 0.50
HD 22589 1.10 0.80 0.89 0.20 1.27 0.20 0.2 108 exp 0.187(23) 1.25(54) 0.52
HD 27271 0.26 0.90 0.24 0.40 0.16 0.05 0.05 1012 exp 0.272(14) 0.568(19) 0.35
HD 48565 3.14 1.00 1.34 0.40 2.66 0.05 0.4 108 exp 0.659(10) 0.0631(23) 0.32
HD 76225 0.80 0.10 0.71 0.20 1.83 0.30 0.2 108 exp 0.25(1) 0.83(12) 0.38
HD 87080 2.22 1.00 1.17 0.60 2.49 0.80 0.6 108 exp 0.71(1) 0.145(5) 0.48
HD 89948 0.67 0.10 0.45 0.20 1.65 0.30 0.2 108 exp 0.24(2) 0.77(36) 0.30
HD 92545 1.42 0.90 1.22 0.20 0.85 0.30 0.3 1012 exp 0.291(3) 0.261(14) 0.40
HD 106191 1.36 0.90 1.16 0.40 0.72 0.05 0.05 1012 exp 0.383(1) 0.130(1) 0.38
HD 107574 1.91 0.90 2.28 0.20 2.05 0.30 0.9 108 sing 0.298(2) 0.245(5) 0.42
HD 116869 0.14 1.10 0.18 0.80 0.33 0.80 1.1 108 sing 0.55(2) 0.0646(22) 0.55
HD 123396 0.46 1.10 0.84 0.80 1.24 0.80 1.1 108 sing 0.54(2) 0.0315(22) 0.54
HD 123585 2.17 1.00 0.98 0.40 2.14 0.50 0.4 108 exp 0.46(1) 0.275(15) 0.46
HD 147609 2.33 0.10 1.90 0.20 2.42 0.30 0.2 108 exp 0.288(7) 1.07(11) 0.41
HD 150862 0.66 0.90 1.57 0.20 1.11 0.30 0.9 108 sing 0.271(3) 0.489(26) 0.47
HD 188985 1.83 0.90 1.77 0.40 1.94 0.40 0.4 108 exp 0.401(4) 0.225(5) 0.39
HD 210709 0.11 1.10 0.19 0.80 0.26 0.80 1.1 108 sing 0.314(3) 0.303(9) 0.38
HD 210910 0.55 0.10 0.63 0.20 0.38 0.30 0.3 1012 exp 0.44(4) 0.075(13) 0.52
HD 222349 3.02 0.90 1.28 0.40 2.00 0.05 0.4 108 exp 0.379(8) 0.170(12) 0.46
BD+18 5215 2.41 0.90 2.74 0.40 1.50 0.05 0.05 1012 exp 0.274(1) 0.503(2) 0.63
HD 223938 0.26 1.00 0.20 0.50 0.29 0.70 0.5 108 exp 0.384(5) 0.229(9) 0.34




Copyright ESO 2006