# Abundance analysis of 5 early-type stars in the young open cluster IC 2391

Ch. Stütz, S. Bagnulo, E. Jehin, C. Ledoux, Rémi Cabanac, C. Melo, J.

Smoker

► To cite this version:

Ch. Stütz, S. Bagnulo, E. Jehin, C. Ledoux, Rémi Cabanac, et al. Abundance analysis of 5 early-type stars in the young open cluster IC 2391. Astronomy & Astrophysics - A&A, 2006, 451 (1), pp.285-291. 10.1051/0004-6361:20053905 . hal-04863424

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# Abundance analysis of 5 early-type stars in the young open cluster IC 2391★★

Ch. Stütz<sup>1,2</sup>, S. Bagnulo<sup>2</sup>, E. Jehin<sup>2</sup>, C. Ledoux<sup>2</sup>, R. Cabanac<sup>3</sup>, C. Melo<sup>2</sup>, and J. V. Smoker<sup>2,4</sup>

Received 25 July 2005 / Accepted 23 January 2006

## ABSTRACT

**Aims.** It is unclear whether chemically peculiar stars of the upper main sequence represent a class completely distinct from normal A-type stars, or whether there exists a continuous transition from the normal to the most peculiar late F- to early B-type stars. A systematic abundance analysis of open cluster early-type stars would help to relate the observed differences of the chemical abundances of the photospheres to other stellar characteristics, without being concerned by possible different original chemical composition. Furthermore, if a continuous transition region from the very peculiar to the so called normal A–F stars exists, it should be possible to detect objects with mild peculiarities.

**Methods.** As a first step of a larger project, an abundance analysis of 5 F–A type stars in the young cluster IC 2391 was performed using high resolution spectra obtained with the UVES instrument of the ESO VLT.

**Results.** Our targets seem to follow a general abundance pattern: close to solar abundance of the light elements and iron peak elements, heavy elements are slightly overabundant with respect to the sun, similar to what was found in previous studies of normal field A-type stars of the galactic plane. We detected a weakly chemically peculiar star, HD 74044. Its element pattern contains characteristics of CP1 as well as CP2 stars, enhanced abundances of iron peak elements and also higher abundances of Sc, Y, Ba and Ce. We did not detect a magnetic field in this star (detection limit was 2 kG). We also studied the star SHJM 2, proposed as a pre-main sequence object in previous works. Using spectroscopy we found a high surface gravity, which suggests that the star is very close to the ZAMS.

**Key words.** Galaxy: open clusters and associations: individual: IC 2391 – stars: abundances – stars: evolution – stars: chemically peculiar – stars: pre-main sequence

## 1. Introduction

The atmospheres of main sequence A-type stars should be relatively simple to understand and to model. Convection is apparently absent, stellar winds are very weak, and little or no photospheric microturbulence is generally present. Yet, in this group of stars, a large variety of peculiarities are observed. Among A- and B-type stars, about 10% are chemically peculiar, i.e., the analysis of their spectra reveal overabundances (e.g., of iron-peak and/or rare-earths elements) and/or underabundances (e.g., of He, Ca, and Sc), compared to the composition of the solar photosphere. Many of these chemically peculiar (CP) stars exhibit large scale magnetic fields with a typical strength of a few hundreds up to a few tens of

thousands of Gauss. Furthermore, many of the CP stars reveal very inhomogeneous atmospheric distributions of numerous elements. Another characteristic of CP stars is that, compared to the normal A and B-type stars, most have long rotation periods – typically several days, but up to a few decades for some magnetic CP stars. For a more detailed introduction to the variety of phenomena observed in A and B-type stars see, e.g., Preston (1974), Wolff (1983).

An important question to address is whether the CP stars represent a group that is well separated from “normal” A and B-type stars, or whether CP stars are the extreme cases of a group of stars spanning all grades of peculiarity. If a continuous transition from the very peculiar to the so called normal A–F stars exists, it should be possible to detect objects with mild peculiarities.

There are several reasons why these stars are so difficult to identify. Rotation velocities of normal A-type stars are in most cases too high (⟨v sin i⟩ ~ 150 km s⁻<fnref n="1" />) to allow precise

<footnote n="1">¹ Institute of Astronomy (IfA), University of Vienna, Türkenschanzstrasse 17, 1180 Vienna, Austria</footnote>

<footnote n="2">² European Southern Observatory, Casilla 19001, Santiago 19, Chile</footnote>

<footnote n="3">³ Canada-France-Hawaii Telescope Corporation, 65-1238 Mamalahoa Hwy. Kamuela, Hawaii 96743, USA</footnote>

<footnote n="4">⁴ Astrophysics & Planetary Science Research Division, Department of Physics and Astronomy, The Queen's University of Belfast, University Road, Belfast, BT7 1NN, UK</footnote>

<footnote>* Based on observations made with ESO Telescopes at the Paranal Observatory under programme ID 266.D-5655.</footnote>

<footnote>** Tables 4 and 5 are only available in electronic form at http://www.edpsciences.org</footnote>
abundance determination. Pronounced chemical peculiarity is mostly found in slow rotators (⟨v sin i⟩ ~ 40 km s⁻¹), whereas studying a transition from CP to normal stars also implies analysing objects with higher projected rotation velocities. Thus it is not clear whether this anticorrelation of v sin i and peculiarity is a physical one, or if it is due to a selection effect. In other words, is rotation preventing chemical peculiarity or is it hiding chemical peculiarity? Hill & Landstreet (1993) explicitly showed for narrow lined A stars (v sin i ≤ 25 km s⁻¹) of the galactic plane that the variations in the individual elemental abundances can be quite large (±0.4 dex). The same is reflected in the work of Adelman and collaborators (e.g. Kocer et al. 2003; Pintado & Adelman 2003).

The proper way to address the questions above is to perform a detailed abundance analysis of early-type stars of different ages and rotational velocities. Members of open clusters are of special interest because one can safely assume that members of the same cluster are more or less of the same age and chemical composition. They should differ from each other only by their initial mass. Furthermore, the cluster age can be determined with much more accuracy than the age of individual stars in the field. We thus carried out a detailed study of 5 main sequence stars of spectral type B–F belonging to the young open cluster IC 2391. For our investigations we used spectra obtained with UVES, the high resolution spectrograph of the ESO VLT. As the stars of IC 2391 we analysed are roughly the same age and were formed from similar initial chemical composition, we expect that if significant deviations from the abundance pattern typical for IC 2391 are found, they will be nearly independent of these two stellar properties. Thus the probability that weak chemical peculiarity dates back to the birth of the star is higher than for stars located in the galactic field. Since the cluster is very young (~36 Mys, Lyngå 1987), main sequence (MS) evolutionary effects are small. One star of our sample, SHMJ 2, may have not reached the MS yet.

## 2. Observations and data reduction

### 2.1. Observations

IC 2391 was observed from 7 to 12 February 2001 with the UVES instrument of the ESO VLT Unit 2 Kueyen within the framework of the UVES Paranal Observatory Project (Bagnulo et al. 2003). Target selection was performed mainly with the WEBDA open cluster database (http://www.univie.ac.at/webda/) developed by J.-C. Mermilliod at the Institute for Astronomy of the University of Lausanne and maintained by E. Paunzen at the University of Vienna. Some additional pre-main sequence stars were selected using the work by Stauffer et al. (1989). Spectra for about 50 candidate cluster members were obtained using the settings DIC1 (346+580) and DIC2 (437+860) (see UVES user manual VLT-MAN-ESO-13200-1825) with a 0.5" slit width. The resulting spectra cover almost the entire spectral range from 305 nm to 1040 nm with a spectral resolution of about 80 000. The raw data are available at the ESO archive under programme ID 266.D-5655.

<table><caption>**Table 1.** Candidate target stars for abundance analysis. Rotation velocities from Noterdaeme et al. (in preparation). M? denotes questionable membership, v sin i in km s⁻¹. The Δa index that is sensitive to CP2 type peculiarity is taken from Maitzen & Catalano (1986). A * indicates stars that were selected for the abundance analysis.</caption><thead><tr><th>Star</th><th>sp. type</th><th>m<sub>v</sub></th><th>v sin i</th><th>Notes</th></tr></thead><tbody><tr><td>HD 73722</td><td>F5 V</td><td>8.92</td><td>6.8</td><td>*</td></tr><tr><td>HD 73778</td><td>F0 V</td><td>8.76</td><td>40</td><td>M?</td></tr><tr><td>HD 74044</td><td>A3</td><td>8.48</td><td>32</td><td>Δa = 1, Am? *</td></tr><tr><td>HD 74275</td><td>A0 V</td><td>7.27</td><td>62</td><td>*</td></tr><tr><td>HD 74535</td><td>B8</td><td>5.55</td><td>37</td><td>Δa = 26, Si</td></tr><tr><td>HD 75029</td><td>A2/3</td><td>9.45</td><td>24</td><td>Δa = -7, M? *</td></tr><tr><td>CPD-52 1568</td><td>F5 V</td><td>9.62</td><td>19</td><td></td></tr><tr><td>SHJM 2</td><td>F9</td><td>10.3</td><td>10</td><td>PMS? *</td></tr></tbody></table>

### 2.2. Target selection

In total, 50 stars of IC 2391 were observed. For 8 early-type stars among them, the rotational velocity is low enough and the quality of the spectral data sufficient for our purposes of detailed abundance analysis. These stars are listed in Table 1.

Information about membership was extracted from Robichon et al. (1999), Levato et al. (1988), Perry & Hill (1969), and Stauffer et al. (1989). Membership was cross-checked using Hipparcos parallaxes, the most recent E(b - y) data found in the SIMBAD database and new radial velocity measurements of UVES POP stars by Noterdaeme et al. (in preparation). For two objects of Table 1, membership remains questionable. HD 75029 is not stated as a member in Perry & Hill (1969), however, its astrometric parameters agree well with the cluster mean. On the other hand HD 73778, according to Levato et al. (1988), very likely is not a member of IC 2391. The Si star HD 74535 was investigated by Lüftinger et al. (in prep.) parallel to our study. We analysed HD 73722, HD 74044, HD 74275, HD 75029 and SHJM 2. This target selection is the result of a compromise between keeping the spread of spectral types large and the projected rotation velocities low.

### 2.3. Data reduction

Data have been reduced by the UVES POP team using an automatic procedure based on the MIDAS UVES pipeline (Ballester et al. 2000). Science frames were bias-subtracted and divided by the extracted flat-field, except for the 860 setting, where the 2D (pixel-to-pixel) flat-fielding was used in order to better correct for fringing. Because of the high flux of the spectra the *average extraction* method was used instead of the *optimal extraction* method that is recommended for spectra characterised by a signal to noise ratio (SNR) ≤ 100. Further details about the reduction procedure can be found in Bagnulo et al. (2003). All reduced spectra can be obtained with the UVES POP web interface at http://www.eso.org/uvespop/

Taking advantage of the quality control parameters produced by the UVES pipeline, we performed a check of the instrument stability and actual performance. The accuracy of the wavelength calibration was found to be of the order of
300 m s⁻¹ only because the Th-Ar reference frames were taken the following morning and not before and after each observation (the temperature difference between science exposures and calibrations was typically 1 K). For this work we used the following wavelength intervals: 3730–4990 Å (characterised by a mean resolution 〈R〉 = 76 000 and a SNR of 100–150); 4760–5770 Å (〈R〉 = 82 000 and SNR = 210–150); 5840–6840 Å (〈R〉 = 73 000 and SNR = 170–130). We found a maximum variation of 3.7% for these mean resolutions.

## 2.4. Continuum normalisation

The targets selected for the abundance analysis include objects with rotation velocities up to ≈60 km s⁻¹. For such fast rotating stars, the determination of the elemental abundances depends critically on the accuracy of the continuum normalisation. To be sure to perform accurate continuum fitting, we performed some tests using the spectra of HD 74169, a slow rotating cluster member Ap star that will be analysed in detail in a forthcoming paper by Lüftinger et al. We normalised the star’s high SNR (≈300) spectra in two independent ways: using the merged output of the UVES pipeline, and using the intermediate “2D unmerged” spectra, i.e., the spectra corresponding to the individual echelle orders (also available through the UVES POP web interface). The fully merged spectra are affected by some artefacts mainly due to an imperfect merging of the echelle orders (for details see Bagnulo et al. 2003, and references therein), hence better results are expected to be obtained by normalisation of the unmerged spectra. However, an optimum normalisation could be obtained by dividing the merged spectra into sub-spectra of a maximum length of 100 Å, and by treating these individually. This way we obtained an agreement to better than 1% over the whole spectral range for the two different techniques. The maximum size of the differences in the normalised spectra obtained with the two methods does not generally occur at the wavelengths of the the extremes of the echelle orders. This suggests that the order merging performed by the UVES pipeline is sufficiently accurate and does not lead to major artefacts in the abundance analysis.

Our comparison showed that we could not clearly define the continuum for the hydrogen lines (which are in general broader than 100 Å) and thus we did not use them to determine fundamental atmospheric parameters.

To identify telluric lines we used the star HD 74196 as reference. The spectrum of this cluster member does not contain many lines (spectral type B7V) which are heavily broadened due to the high rotational velocity of $v \sin i = 300$ km s⁻¹.

## 3. Abundance analysis

The starting values for the fundamental parameters of the atmosphere of the selected stars were estimated via Strömgren photometry (Johnson *UBV* photometry in the case of SHJM 2) and evolutionary tracks for the cluster interpolated from Schaller et al. (2004). The uncertainties of these estimates are quite large (typically 200 K in $T_{eff}$ and 0.25 in log g), thus we tried to improve the fundamental parameters by spectroscopic means. $T_{eff}$ estimates were improved via elimination of an

abundance-$\chi_{excit}$ correlation (see Fig. 1). log g estimates were improved by making sure that there is no systematic difference in abundances between different ionisation stages of chemical elements (called in the following “ionisation equation condition”). The presence of a magnetic field was checked looking at the correlation of abundances with Landéfactors, and by searching for magnetically split lines. Together with the mean metallicity of the cluster ([Fe/H] = -0.03, Randich et al. 2001), these parameters defined the first atmosphere calculated with LLmodels (Shulyak et al. 2004) in ODF mode (ODF: estimating line absorption via a pre calculated opacity distribution function). Using this model we calculated the emerging flux at the center of lines extracted from the VALD database (Piskunov et al. 1995; Kupka et al. 1999; Ryabchikova et al. 1999) and preselected only those that make an important contribution to the opacity ($\kappa_{vL}/\kappa_{vC} \ge 1\%$, $\kappa_{vL}$ and $\kappa_{vC}$ are the line and continuum absorption coefficient).

We determined the initial microturbulence and element abundance pattern from equivalent widths of unblended lines using the *widthV* software written by Tsymbal. Assuming that for our set of spectral lines non-LTE and stratification effects are negligible, there should be no correlation between abundances determined from the equivalent widths and the widths themselves or the excitation energy, and the ionisation equation condition should be fulfilled. Eliminating the above correlations for the elements where we found the most unblended or marginally blended lines in the spectra (typically Fe, Cr, Ti, Ni, Ca) resulted not only in a fairly good determination of microturbulence and first abundances, but also in an improvement of effective temperature and surface gravity. For HD 74275 we had to perform this step via synthetic line fitting, since this star rotates with $v \sin i = 60.5$ km s⁻¹ and shows only a few unblended lines. For synthetic line fitting all our models were calculated with LLmodels in the line-by-line modus (Shulyak et al. 2004). This means that the individual abundance pattern is included in our atmospheric models as well. The hydrogen lines were treated using VCS theory (Vidal et al. 1973). Convection was modelled according to the formalism of Canuto & Mazzitelli (1991). For atmospheric modelling as well as for the line synthesis with Synth3 (Piskunov 1992; Valenti et al. 1998) we extracted the atomic lines from the

<figure><img src="image_2.png" /><figcaption>**Fig. 1.** Excitation potential vs. abundance for the final values of $T_{eff}$ and log g of HD 74044. Open circles – FeI, filled circles – FeII. A least squares linear regression yields: $abn = -0.0002\chi_{excit}^2 - 4.18$.</figcaption></figure>
<table><caption>**Table 2.** Starting and final set of atmospheric parameters. UP – UVES POP number.</caption><thead><tr><th rowspan="2">star</th><th rowspan="2">UP</th><th colspan="4">initial set</th><th colspan="4">final set</th></tr><tr><th><i>T</i><sub>eff</sub><sup>a</sup></th><th>log <i>g</i><sup>a</sup></th><th>log <i>g</i><sup>b</sup></th><th><i>v</i> sin <i>i</i><sup>c</sup></th><th><i>T</i><sub>eff</sub> [K]</th><th>log <i>g</i> [cgs]</th><th><i>v</i><sub>mic</sub> [km s<sup>-1</sup>]</th><th><i>v</i> sin <i>i</i></th></tr></thead><tbody><tr><td>HD 73722</td><td>04</td><td>6550</td><td>4.25</td><td>4.35</td><td>6.8</td><td>6480</td><td>4.30</td><td>1.30</td><td>6.7</td></tr><tr><td>HD 74044</td><td>11</td><td>8000</td><td>4.20</td><td>4.30</td><td>32</td><td>8130</td><td>4.45</td><td>2.65</td><td>33.7</td></tr><tr><td>HD 74275</td><td>23</td><td>10500</td><td>4.42</td><td>4.29</td><td>62</td><td>10200</td><td>4.40</td><td>1.30</td><td>60.5</td></tr><tr><td>HD 75029</td><td>43</td><td>7770</td><td>4.20</td><td>4.30</td><td>24</td><td>7800</td><td>4.30</td><td>2.00</td><td>22.0</td></tr><tr><td>SHJM 2<sup>d</sup></td><td>73</td><td>5950<sup>e</sup></td><td></td><td>4.40</td><td>10.3</td><td>6100</td><td>4.40</td><td>1.15</td><td>10.6</td></tr></tbody></table>

<sup>a</sup> Obtained from Strömgren photometry.

<sup>b</sup> Obtained using tracks from Schaller (2004).

<sup>c</sup> Taken from Noterdaeme et al. (in prep.).

<sup>d</sup> Taken from Stauffer et al. (1989).

<sup>e</sup> Obtained from Johnson *UBV* photometry.

VALD line database. To analyse the spectra, in the sense of deriving noise, deviations between observed and synthesized spectra, measuring equivalent widths, etc., we developed the “Little Spectrum Analyser” (Lispan). The graphical interface for the codes which also controls the automatic line core fitting is called ATC. The set of atmospheric modelling and analysis software used for this investigation can be reviewed on the web at http://ams.astro.univie.ac.at/computer/ChrSoft/chrsoft.html Once we had fixed $v \sin i$ and $v_{mic}$ (see Table 2) by synthetic line fitting of the unblended lines, we determined the elemental abundances in an iterative process:

* Automatic line core fitting with ATC, Synth3 and Lispan. This is faster than fitting the whole line, but one has to be sure of $v \sin i$, $v_{mic}$ and if present, the magnetic field. The only free parameters here are the abundances.

* Check for peculiarities and magnetic fields.

* Fine tuning of fundamental parameters ($T_{eff}$, log g, $v_{mic}$, $v \sin i$). Check the conditions mentioned above and whether they hold when peculiarities have been found.

* Edit line selection if blends have been overlooked, certain lines show non-LTE effects, the quality of line parameters are uncertain, etc.

This procedure resulted in fundamental atmospheric parameters with internal errors lower than 150 K in $T_{eff}$, 0.20 dex in log g, 0.20 km s⁻¹ in $v_{mic}$, 0.3 km s⁻¹ in $v \sin i$ and accurate element abundances (0.1–0.3 dex in general) for all the program stars except HD 75029 which very likely is a spectroscopic binary. For more detailed discussions on internal and absolute errors in modern abundance analyses see Andrievsky et al. (2002) or Hill & Landstreet (1993).

## 4. Results

The atmospheric parameters of our stars were checked by fits of the H lines. Atomic lines blended by the wings of H Balmer lines were not used for abundance analysis because we could not precisely determine the continuum. In some cases the number of lines suitable for deriving abundances of a certain element was very small. For four stars these lines are listed in Table 5. For the star HD 74044 the complete list of lines used for the abundance analysis is presented in Table 4. We found no

indications for mean magnetic surface fields larger than 1 kG in HD 73722, HD 75029 and SHJM 2, or larger than 2 kG in HD 74044 and HD 74275. We did not find any published high quality abundance analyses of stars of IC 2391 for a comparison with our work. In the following we will present the results for the 5 stars we have analysed.

**HD 74044:** For HD 74044 we determined a projected rotation velocity of 33.7 km s⁻¹. Fundamental atmospheric parameters were derived from Fe, Ca, Cr, Mg, Ni and Ti. We could determine relatively precise abundances for 10 elements and abundance estimates for C, Ce, Cu, Mn, O, Y and Zn (see Table 3). Comparing the abundance pattern of HD 74044 to the other stars we see indications for a mild chemical peculiarity, which is supported by the higher abundances of Sc, Y, Ba and Ce (Fig. 2). The element pattern of HD 74044 contains characteristics of CP1 stars (enhanced iron peak elements) as well as CP2 stars (enhanced Sc, and heavy elements). A similar pattern but much more pronounced can be seen in the cluster star HD 74169 known to be of type CP2 (Lüftinger et al., in prep.). Due to the rotation velocity of 33.7 km s⁻¹ our detection limit for a mean surface magnetic field is about 2 kG. Polarimetric observations will be necessary to check for the presence of a magnetic field.

**HD 73722:** This slowly rotating star ($v \sin i$ = 6.7 km s⁻¹) is listed in the catalogue of eclipsing and spectroscopic binary stars by Popova & Kraicheva (1984). But after carefully scanning our spectra we found no hints of line patterns that could originate from a stellar companion or a close background star. Temperature, surface gravity and microturbulence (Table 2) were confirmed with lines from Fe, Cr, Ti, Ni, Ca, Si and Mn. TiI and TiII deviated noticeably from the ionisation equilibrium condition. Their abundances are –7.08 and –7.16 respectively. Typical for this analysis was $|[N_{El}/N_{tot}]_I - [N_{El}/N_{tot}]_II| < 0.05$ for different ionisation stages of the same element. The abundance of Sr is uncertain because both lines we analysed (SrI 4161.792 Å and SrI 4607.327 Å) are blended. The result for oxygen should be considered as an upper limit.
<table><caption>**Table 3.** Abundances [$N_{El}/N_{tot}$] of members of IC 2391. Solar values according to Grevesse & Sauval (1998).</caption><thead><tr><th rowspan="2">El</th><th colspan="3">HD 73722</th><th colspan="3">HD 74044</th><th colspan="3">HD 74275</th><th colspan="3">HD 75029</th><th colspan="3">SHJM 2</th><th rowspan="2">sun<br>abn</th></tr><tr><th>abn<sup>a</sup></th><th>(err)<sup>b</sup></th><th>[n]<sup>c</sup></th><th>abn</th><th>(err)</th><th>[n]</th><th>abn</th><th>(err)</th><th>[n]</th><th>abn</th><th>(err)</th><th>[n]</th><th>abn</th><th>(err)</th><th>[n]</th></tr></thead><tbody><tr><td>He</td><td></td><td></td><td></td><td></td><td></td><td></td><td>-1.08</td><td>(-)</td><td>[1]</td><td></td><td></td><td></td><td>-3.32</td><td>(22)</td><td>[2]</td><td>-1.11</td></tr><tr><td>C</td><td>-3.43</td><td>(6)</td><td>[4]</td><td>-3.47</td><td>(-)</td><td>[2]</td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td>-3.52</td></tr><tr><td>O</td><td>-3.10</td><td>(-)</td><td>[1]</td><td>-3.41</td><td>(-)</td><td>[2]</td><td>-3.24</td><td>(-)</td><td>[2]</td><td></td><td></td><td></td><td></td><td></td><td></td><td>-3.21</td></tr><tr><td>Na</td><td>-5.82</td><td>(4)</td><td>[4]</td><td></td><td></td><td></td><td>-5.03</td><td>(24)</td><td>[2]</td><td></td><td></td><td></td><td>-5.80</td><td>(8)</td><td>[4]</td><td>-5.71</td></tr><tr><td>Mg</td><td>-4.53</td><td>(7)</td><td>[5]</td><td>-4.45</td><td>(5)</td><td>[6]</td><td>-4.19</td><td>(6)</td><td>[7]</td><td>-4.44</td><td>(38)</td><td>[5]</td><td>-4.41</td><td>(9)</td><td>[3]</td><td>-4.46</td></tr><tr><td>Al</td><td></td><td></td><td></td><td></td><td></td><td></td><td>-5.21</td><td>(-)</td><td>[1]</td><td></td><td></td><td></td><td>-5.82</td><td>(1)</td><td>[2]</td><td>-5.57</td></tr><tr><td>Si</td><td>-4.96</td><td>(26)</td><td>[20]</td><td>-4.83</td><td>(17)</td><td>[6]</td><td>-4.52</td><td>(24)</td><td>[3]</td><td>-4.48</td><td>(25)</td><td>[10]</td><td>-4.74</td><td>(30)</td><td>[19]</td><td>-4.49</td></tr><tr><td>S</td><td>-4.90</td><td>(2)</td><td>[4]</td><td>-4.81</td><td>(3)</td><td>[3]</td><td></td><td></td><td></td><td>-4.92</td><td>(5)</td><td>[6]</td><td>-4.74</td><td>(-)</td><td>[1]</td><td>-4.71</td></tr><tr><td>Ca</td><td>-5.71</td><td>(26)</td><td>[29]</td><td>-5.64</td><td>(9)</td><td>[10]</td><td>-5.64</td><td>(5)</td><td>[2]</td><td>-6.02</td><td>(37)</td><td>[10]</td><td>-5.46</td><td>(7)</td><td>[13]</td><td>-5.68</td></tr><tr><td>Sc</td><td>-8.92</td><td>(10)</td><td>[9]</td><td>-8.61</td><td>(13)</td><td>[3]</td><td>-9.18</td><td>(-)</td><td>[1]</td><td>-9.36</td><td>(27)</td><td>[3]</td><td>-8.89</td><td>(13)</td><td>[6]</td><td>-8.87</td></tr><tr><td>Ti</td><td>-7.14</td><td>(7)</td><td>[51]</td><td>-6.27</td><td>(25)</td><td>[15]</td><td>-6.98</td><td>(7)</td><td>[6]</td><td>-7.17</td><td>(21)</td><td>[18]</td><td>-6.97</td><td>(13)</td><td>[29]</td><td>-7.02</td></tr><tr><td>V</td><td>-8.24</td><td>(10)</td><td>[5]</td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td>-8.02</td><td>(6)</td><td>[9]</td><td>-8.04</td></tr><tr><td>Cr</td><td>-6.39</td><td>(7)</td><td>[37]</td><td>-5.75</td><td>(11)</td><td>[21]</td><td>-6.27</td><td>(7)</td><td>[8]</td><td>-6.20</td><td>(21)</td><td>[24]</td><td>-6.23</td><td>(10)</td><td>[20]</td><td>-6.37</td></tr><tr><td>Mn</td><td>-6.80</td><td>(9)</td><td>[18]</td><td>-6.33</td><td>(-)</td><td>[1]</td><td></td><td></td><td></td><td>-6.44</td><td>(12)</td><td>[2]</td><td>-6.56</td><td>(6)</td><td>[9]</td><td>-6.65</td></tr><tr><td>Fe</td><td>-4.59</td><td>(10)</td><td>[298]</td><td>-4.19</td><td>(12)</td><td>[147]</td><td>-4.45</td><td>(12)</td><td>[29]</td><td>-4.41</td><td>(17)</td><td>[96]</td><td>-4.46</td><td>(9)</td><td>[169]</td><td>-4.54</td></tr><tr><td>Co</td><td>-7.31</td><td>(3)</td><td>[4]</td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td>-7.17</td><td>(7)</td><td>[6]</td><td>-7.12</td></tr><tr><td>Ni</td><td>-5.91</td><td>(7)</td><td>[50]</td><td>-5.34</td><td>(6)</td><td>[11]</td><td></td><td></td><td></td><td>-5.75</td><td>(29)</td><td>[17]</td><td>-5.82</td><td>(7)</td><td>[32]</td><td>-5.79</td></tr><tr><td>Cu</td><td>-8.20</td><td>(13)</td><td>[2]</td><td>-7.17</td><td>(-)</td><td>[1]</td><td></td><td></td><td></td><td>-7.85</td><td>(-)</td><td>[1]</td><td>-7.76</td><td>(-)</td><td>[1]</td><td>-7.83</td></tr><tr><td>Zn</td><td>-7.74</td><td>(-)</td><td>[1]</td><td>-7.13</td><td>(-)</td><td>[1]</td><td></td><td></td><td></td><td></td><td></td><td></td><td>-7.55</td><td>(-)</td><td>[1]</td><td>-7.44</td></tr><tr><td>Sr</td><td>-8.76</td><td>(37)</td><td>[2]</td><td></td><td></td><td></td><td>-9.32</td><td>(-)</td><td>[1]</td><td></td><td></td><td></td><td>-8.77</td><td>(36)</td><td>[3]</td><td>-9.07</td></tr><tr><td>Y</td><td>-9.82</td><td>(3)</td><td>[6]</td><td>-9.49</td><td>(-)</td><td>[1]</td><td></td><td></td><td></td><td>-9.96</td><td>(7)</td><td>[2]</td><td>-9.74</td><td>(9)</td><td>[4]</td><td>-9.80</td></tr><tr><td>Zr</td><td>-9.44</td><td>(-)</td><td>[1]</td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td>-9.48</td><td>(11)</td><td>[2]</td><td>-9.44</td></tr><tr><td>Ba</td><td>-9.53</td><td>(19)</td><td>[3]</td><td>-8.46</td><td>(16)</td><td>[3]</td><td></td><td></td><td></td><td></td><td></td><td></td><td>-9.30</td><td>(2)</td><td>[2]</td><td>-9.91</td></tr><tr><td>Ce</td><td>-10.48</td><td>(-)</td><td>[2]</td><td>-9.70</td><td>(-)</td><td>[1]</td><td></td><td></td><td></td><td></td><td></td><td></td><td>-10.40</td><td>(-)</td><td>[2]</td><td>-10.46</td></tr><tr><td>Nd</td><td>-10.40</td><td>(9)</td><td>[5]</td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td>-10.25</td><td>(8)</td><td>[2]</td><td>-10.54</td></tr><tr><td>Eu</td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td>-11.27</td><td>(-)</td><td>[1]</td><td>-11.53</td></tr></tbody></table>

<sup>a</sup> abn element abundance: [$N_{El}/N_{tot}$] = $10^6 \log (N_{Element}/N_{Total})$.

<sup>b</sup> (err) internal errors in units of the last digit.

<sup>c</sup> [n] number of lines used for the final iteration step.

<figure><img src="image_3.png" /><figcaption>**Fig. 2.** Comparison of the abundances in HD 74044 (open circles) with those of the CP star HD 74169 (open triangles, Lüftinger, in prep.) and to the mean of the other members of IC 2391 (filled circles). Abundances are in units of [$N_{El}/N_{tot}$] - [$N_{El}/N_{tot}]_{\odot}$ (solar abundances according to Grevesse and Sauval 1998). Error bars indicate maximum deviations from the mean.</figcaption></figure>

**HD 74275:** With $v \sin i = 60.5$ km s$^{-1}$, this is the fastest rotating star we have analysed. It is also the hottest one. Thus

only few lines could be used and the quality of our Ca, O, Si and Na abundances is not as good as our internal error estimates may suggest. The atmospheric parameters were refined from Fe, Cr, Ti and Mg. In 5 lines (NaI 5889.951, NaI 5895.924, SiII 6347.109, SiII 6371.371 and HeI 5875.615) we corrected for atmospheric features (see Sect. 2.4). The remarkable overabundance of Na (≈0.7 dex) is probably a non-LTE effect we could not account for. Takeda (2003) and Asplund (2005) both suggest non-LTE abundance corrections of up to -0.5 dex for these two lines. The abundance of helium, determined from 1 line (HeI 5875.615 Å), is more or less solar.

**HD 75029:** although the membership of this star may be questionable, we included it in our analysis, since it was the only slowly rotating star ($v \sin i = 22$ km s$^{-1}$) with spectral type between A0 and F5 and no known peculiarities. A posteriori we found that its abundances fit quite well in the overall pattern we see for IC 2391. The star very likely has a faint fast rotating spectroscopic companion, also noticed by Popova & Kraicheva (1984). We could not directly separate the spectrum of the companion, but we found our continuum to be systematically too low for regions around deeper lines. Strong contamination due to twilight can be ruled out as the cause because we do not
<figure><img src="image_4.png" /><figcaption>**Fig. 3.** Elemental abundances relative to the sun. Solar values according to Grevesse & Sauval (1998). Data points of elements with consecutive atomic numbers are connected with lines. Errors as in Table 3.</figcaption></figure>

see this behaviour in the spectra of HD 74275 which has been observed at a time even closer to dawn. Unfortunately no details about the possible companion are known so far, hence our results for HD 75029 are not as accurate as they should be.

SHJM2: Using the UVES observations we could analyse in detail the spectrum of a very slowly rotating ($v \sin i = 10.6$ km s⁻¹) possible PMS star. Stauffer et al. (1989, 1997) suggested that SHJM2 has not yet reached the ZAMS. The surface gravity we determined by spectroscopic means ($\log g = 4.40$) is surprisingly high if we consider the star to be a PMS object. Evolutionary tracks for cluster stars give the same value for cluster members with this effective temperature situated on the ZAMS. Therefore SHJM2 is probably at the very end of its pre main sequence phase or has already reached the ZAMS. Since SHJM2 is already in the final stage of its PMS phase and very close to the main sequence, we applied the techniques developed for main sequence stars for an abundance analysis. Examining the iron lines FeII 6149.258 and FeI 6336.8243 we could detect no magnetic field. The star

<figure><img src="image_5.png" /><figcaption>**Fig. 4.** Mean abundance pattern of IC 2391 (HD 74044 excluded) derived in this work compared to the abundance pattern found for field stars by Hill & Landstreet (1993) and Hill (1995). Elemental abundances are relative to the sun with solar values according to Grevesse and Sauval (1998). Data points of elements with consecutive atomic numbers are connected with lines. Error bars are variances of the mean abundances.</figcaption></figure>

generally reflects the pattern of the other cluster members (except HD 74044 of course).

## 5. Discussion and conclusions

We have carried out a detailed analysis of the atmospheres of 5 A–F stars in the cluster IC 2391 and have obtained reasonably accurate fundamental parameters and element abundances accurate within 0.1–0.3 dex. Specific element patterns were included in our atmospheric models and the presence of magnetic fields and the possibility of stratification were checked too (when $v \sin i \le 25$ km s⁻¹).

Understanding HD 74044 contributes to our knowledge of the A star phenomenon. This star shows a mild peculiarity of the type CP1 and CP2: Sc, Ti, Cr, Mn, Fe, Ni, Cu, Zn, Y and Ce are enhanced by 0.3–0.8 dex relative to the mean of the other cluster members, and even more so Ba. Nevertheless we neither can confidently assign HD 74044 to the group of CP2 nor CP1 stars. We situate this object in the continuous transition region from the very peculiar to the normal A–F stars. We did not detect a magnetic surface field, but our detection limit is rather high (2 kG). Therefore follow-up polarimetric observations are necessary to clarify its status.

The abundance star to star scatter of the other cluster stars is, as expected, small (0.1–0.3 dex) compared to what was found for stars in the galactic plane (0.3–0.5 dex) by Hill & Landstreet (1993) and Hill (1995) for 6 and 9 objects
respectively. A comparison of a cluster abundance pattern derived in this work for 26 elements to the abundances of early A stars in the galactic plane is shown in Fig. 4. Note that not only the star to star variations of element abundances are larger in the galactic plane, but they also seem to increase for faster rotating stars. The latter may not be an intrinsic effect of rotation, but due to the fact that detailed abundance studies become rather difficult for faster rotating stars. For the needed accuracy our technique is limited to a $v \sin i \le 60.5$ km s$^{-1}$, measured for HD 74275.

Our sample includes the star SHJM 2, probably a PMS star already close to the ZAMS considering the findings of Stauffer et al. (1989) and the star's high surface gravity. Assuming that its atmosphere can be modelled applying the same physics and approximations as for MS A–F stars, we performed a detailed abundance analysis in the optical range for this star. Its abundances reflect the general abundance pattern of IC 2391.

*Acknowledgements.* We like to thank Theresa Lüftinger for insight in her analysis of HD 74169 and Pasquier Noterdaeme for his most recent $v \sin i$ data for this cluster. We also thank Martin Stift for his helpful suggestions on presentation of the results. Ch. Stütz acknowledges ESO DGDF for a three month studentship at ESO Santiago/Vitacura and the FWF (project P17890).

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**Online Material**
<table><caption>**Table 4.** Lines used for abundance determination of HD 74044.</caption><thead><tr><th>Identity</th><th>λ[Å]</th><th>log gf</th><th>Identity</th><th>λ[Å]</th><th>log gf</th><th>Identity</th><th>λ[Å]</th><th>log gf</th><th>Identity</th><th>λ[Å]</th><th>log gf</th></tr></thead><tbody><tr><td>C1</td><td>4932.049</td><td>-1.884</td><td>Cr2</td><td>5308.408</td><td>-1.846</td><td>Fe1</td><td>5107.447</td><td>-3.087</td><td>Fe1</td><td>5572.842</td><td>-0.275</td></tr><tr><td>C1</td><td>6014.834</td><td>-1.585</td><td>Cr2</td><td>5310.687</td><td>-2.280</td><td>Fe1</td><td>5107.641</td><td>-2.418</td><td>Fe1</td><td>5576.089</td><td>-1.000</td></tr><tr><td>O1</td><td>6158.176</td><td>-0.996</td><td>Cr2</td><td>5313.563</td><td>-1.650</td><td>Fe1</td><td>5121.639</td><td>-0.810</td><td>Fe1</td><td>5586.756</td><td>-0.120</td></tr><tr><td>O1</td><td>6158.186</td><td>-0.409</td><td>Cr2</td><td>5334.869</td><td>-1.562</td><td>Fe1</td><td>5125.117</td><td>-0.140</td><td>Fe1</td><td>5615.644</td><td>0.050</td></tr><tr><td>Mg2</td><td>4481.126</td><td>0.740</td><td>Cr2</td><td>5407.604</td><td>-2.151</td><td>Fe1</td><td>5133.689</td><td>0.140</td><td>Fe1</td><td>5624.542</td><td>-0.755</td></tr><tr><td>Mg2</td><td>4481.150</td><td>-0.560</td><td>Cr2</td><td>5478.365</td><td>-1.908</td><td>Fe1</td><td>5139.252</td><td>-0.741</td><td>Fe1</td><td>5633.947</td><td>-0.270</td></tr><tr><td>Mg1</td><td>4702.991</td><td>-0.666</td><td>Cr2</td><td>5508.606</td><td>-2.110</td><td>Fe1</td><td>5139.463</td><td>-0.509</td><td>Fe1</td><td>5686.530</td><td>-0.446</td></tr><tr><td>Mg1</td><td>5172.684</td><td>-0.402</td><td>Cr2</td><td>5510.702</td><td>-2.452</td><td>Fe1</td><td>5148.036</td><td>-0.629</td><td>Fe1</td><td>5709.378</td><td>-1.028</td></tr><tr><td>Mg1</td><td>5183.604</td><td>-0.180</td><td>Cr2</td><td>6089.632</td><td>-1.265</td><td>Fe1</td><td>5148.225</td><td>-0.274</td><td>Fe1</td><td>5731.762</td><td>-1.300</td></tr><tr><td>Mg1</td><td>5528.405</td><td>-0.620</td><td>Mn1</td><td>6021.819</td><td>0.034</td><td>Fe1</td><td>5159.058</td><td>-0.820</td><td>Fe1</td><td>5775.081</td><td>-1.298</td></tr><tr><td>Si1</td><td>5675.417</td><td>-1.030</td><td>Fe1</td><td>4438.343</td><td>-1.630</td><td>Fe1</td><td>5162.273</td><td>0.020</td><td>Fe1</td><td>5862.353</td><td>-0.058</td></tr><tr><td>Si1</td><td>5747.667</td><td>-0.780</td><td>Fe1</td><td>4447.717</td><td>-1.342</td><td>Fe2</td><td>5197.577</td><td>-2.100</td><td>Fe1</td><td>5930.180</td><td>-0.230</td></tr><tr><td>Si1</td><td>6145.016</td><td>-0.820</td><td>Fe1</td><td>4466.552</td><td>-0.600</td><td>Fe1</td><td>5202.336</td><td>-1.838</td><td>Fe1</td><td>6020.169</td><td>-0.270</td></tr><tr><td>Si1</td><td>6243.815</td><td>-0.770</td><td>Fe2</td><td>4472.929</td><td>-3.430</td><td>Fe1</td><td>5229.845</td><td>-1.127</td><td>Fe1</td><td>6024.058</td><td>-0.120</td></tr><tr><td>Si1</td><td>6244.466</td><td>-0.690</td><td>Fe1</td><td>4476.019</td><td>-0.819</td><td>Fe1</td><td>5229.880</td><td>-0.236</td><td>Fe1</td><td>6027.051</td><td>-1.089</td></tr><tr><td>Si1</td><td>6254.188</td><td>-0.600</td><td>Fe1</td><td>4476.077</td><td>-0.370</td><td>Fe2</td><td>5234.625</td><td>-2.230</td><td>Fe1</td><td>6056.005</td><td>-0.460</td></tr><tr><td>S1</td><td>6743.531</td><td>-0.920</td><td>Fe1</td><td>4484.220</td><td>-0.864</td><td>Fe1</td><td>5250.646</td><td>-2.181</td><td>Fe1</td><td>6065.482</td><td>-1.530</td></tr><tr><td>S1</td><td>6748.837</td><td>-0.600</td><td>Fe1</td><td>4485.676</td><td>-1.020</td><td>Fe1</td><td>5253.462</td><td>-1.573</td><td>Fe2</td><td>6084.111</td><td>-3.780</td></tr><tr><td>S1</td><td>6757.171</td><td>-0.310</td><td>Fe2</td><td>4491.405</td><td>-2.700</td><td>Fe2</td><td>5254.929</td><td>-3.227</td><td>Fe2</td><td>6113.322</td><td>-4.110</td></tr><tr><td>Ca1</td><td>4425.437</td><td>-0.286</td><td>Fe1</td><td>4494.563</td><td>-1.136</td><td>Fe1</td><td>5273.164</td><td>-0.993</td><td>Fe1</td><td>6127.907</td><td>-1.399</td></tr><tr><td>Ca2</td><td>5019.971</td><td>-0.501</td><td>Fe2</td><td>4508.288</td><td>-2.250</td><td>Fe1</td><td>5273.374</td><td>-2.158</td><td>Fe2</td><td>6147.741</td><td>-2.721</td></tr><tr><td>Ca1</td><td>5581.965</td><td>-0.569</td><td>Fe2</td><td>4515.339</td><td>-2.450</td><td>Fe1</td><td>5281.790</td><td>-0.834</td><td>Fe2</td><td>6149.258</td><td>-2.720</td></tr><tr><td>Ca1</td><td>5588.749</td><td>0.313</td><td>Fe2</td><td>4520.224</td><td>-2.600</td><td>Fe1</td><td>5288.525</td><td>-1.508</td><td>Fe1</td><td>6191.558</td><td>-1.417</td></tr><tr><td>Ca1</td><td>5590.114</td><td>-0.596</td><td>Fe2</td><td>4522.634</td><td>-2.030</td><td>Fe1</td><td>5302.302</td><td>-0.720</td><td>Fe1</td><td>6230.723</td><td>-1.281</td></tr><tr><td>Ca1</td><td>5857.451</td><td>0.257</td><td>Fe1</td><td>4528.614</td><td>-0.822</td><td>Fe2</td><td>5316.615</td><td>-1.850</td><td>Fe1</td><td>6232.641</td><td>-1.223</td></tr><tr><td>Ca1</td><td>6122.217</td><td>-0.386</td><td>Fe2</td><td>4541.524</td><td>-2.790</td><td>Fe2</td><td>5316.784</td><td>-2.760</td><td>Fe2</td><td>6238.392</td><td>-2.630</td></tr><tr><td>Ca1</td><td>6162.173</td><td>-0.167</td><td>Fe2</td><td>4555.893</td><td>-2.160</td><td>Fe1</td><td>5324.179</td><td>-0.103</td><td>Fe1</td><td>6252.555</td><td>-1.687</td></tr><tr><td>Ca1</td><td>6439.075</td><td>0.394</td><td>Fe2</td><td>4576.340</td><td>-2.920</td><td>Fe2</td><td>5325.553</td><td>-3.120</td><td>Fe1</td><td>6265.134</td><td>-2.550</td></tr><tr><td>Ca1</td><td>6717.681</td><td>-0.596</td><td>Fe2</td><td>4583.837</td><td>-1.860</td><td>Fe1</td><td>5341.024</td><td>-1.953</td><td>Fe1</td><td>6336.824</td><td>-0.856</td></tr><tr><td>Sc2</td><td>5031.021</td><td>-0.400</td><td>Fe1</td><td>4602.941</td><td>-2.209</td><td>Fe1</td><td>5353.374</td><td>-0.840</td><td>Fe2</td><td>6369.462</td><td>-4.160</td></tr><tr><td>Sc2</td><td>5239.813</td><td>-0.765</td><td>Fe1</td><td>4607.647</td><td>-1.545</td><td>Fe2</td><td>5362.869</td><td>-2.739</td><td>Fe2</td><td>6383.722</td><td>-2.070</td></tr><tr><td>S-c2</td><td>5526.790</td><td>0.024</td><td>Fe1</td><td>4611.284</td><td>-1.017</td><td>Fe1</td><td>5367.467</td><td>0.443</td><td>Fe1</td><td>6393.601</td><td>-1.432</td></tr><tr><td>Ti2</td><td>4450.482</td><td>-1.510</td><td>Fe2</td><td>4620.521</td><td>-3.240</td><td>Fe1</td><td>5373.709</td><td>-0.860</td><td>Fe1</td><td>6411.649</td><td>-0.595</td></tr><tr><td>Ti2</td><td>4468.507</td><td>-0.600</td><td>Fe1</td><td>4625.045</td><td>-1.340</td><td>Fe1</td><td>5383.369</td><td>0.645</td><td>Fe2</td><td>6416.919</td><td>-2.650</td></tr><tr><td>Ti2</td><td>4518.327</td><td>-2.640</td><td>Fe1</td><td>4632.912</td><td>-2.913</td><td>Fe1</td><td>5389.479</td><td>-0.410</td><td>Fe1</td><td>6419.950</td><td>-0.240</td></tr><tr><td>Ti2</td><td>4529.474</td><td>-1.650</td><td>Fe2</td><td>4635.316</td><td>-1.650</td><td>Fe1</td><td>5391.461</td><td>-0.825</td><td>Fe1</td><td>6421.351</td><td>-2.027</td></tr><tr><td>Ti2</td><td>4552.294</td><td>-2.890</td><td>Fe1</td><td>4643.463</td><td>-1.147</td><td>Fe1</td><td>5393.168</td><td>-0.715</td><td>Fe1</td><td>6430.846</td><td>-2.006</td></tr><tr><td>Ti1</td><td>4552.453</td><td>-0.340</td><td>Fe1</td><td>4654.605</td><td>-1.077</td><td>Fe1</td><td>5400.502</td><td>-0.160</td><td>Fe2</td><td>6446.410</td><td>-1.960</td></tr><tr><td>Ti2</td><td>4563.761</td><td>-0.790</td><td>Fe1</td><td>4678.846</td><td>-0.833</td><td>Fe1</td><td>5405.775</td><td>-1.844</td><td>Fe1</td><td>6677.987</td><td>-1.418</td></tr><tr><td>Ti2</td><td>4571.968</td><td>-0.230</td><td>Fe1</td><td>4707.275</td><td>-1.080</td><td>Fe1</td><td>5410.910</td><td>0.398</td><td>Nil</td><td>4604.982</td><td>-0.250</td></tr><tr><td>Ti2</td><td>4589.958</td><td>-1.620</td><td>Fe1</td><td>4903.310</td><td>-0.926</td><td>Fe1</td><td>5415.199</td><td>0.642</td><td>Nil</td><td>4714.408</td><td>0.260</td></tr><tr><td>Ti2</td><td>5010.212</td><td>-1.300</td><td>Fe1</td><td>4920.503</td><td>0.068</td><td>Fe1</td><td>5424.068</td><td>0.520</td><td>Nil</td><td>4715.757</td><td>-0.320</td></tr><tr><td>Ti2</td><td>5185.913</td><td>-1.370</td><td>Fe2</td><td>4923.927</td><td>-1.320</td><td>Fe2</td><td>5427.826</td><td>-1.664</td><td>Nil</td><td>4904.407</td><td>-0.170</td></tr><tr><td>Ti2</td><td>5188.680</td><td>-1.050</td><td>Fe1</td><td>4930.315</td><td>-1.201</td><td>Fe1</td><td>5429.505</td><td>-1.016</td><td>Nil</td><td>5115.389</td><td>-0.110</td></tr><tr><td>Ti2</td><td>5211.536</td><td>-1.356</td><td>Fe1</td><td>4946.388</td><td>-1.170</td><td>Fe1</td><td>5429.697</td><td>-1.879</td><td>Nil</td><td>5176.559</td><td>-0.440</td></tr><tr><td>Ti2</td><td>5418.751</td><td>-2.110</td><td>Fe1</td><td>4962.572</td><td>-1.182</td><td>Fe1</td><td>5429.827</td><td>-0.527</td><td>Nil</td><td>5663.975</td><td>-0.430</td></tr><tr><td>Ti2</td><td>5490.690</td><td>-2.650</td><td>Fe1</td><td>4966.089</td><td>-0.871</td><td>Fe2</td><td>5432.967</td><td>-3.629</td><td>Nil</td><td>5694.977</td><td>-0.610</td></tr><tr><td>Cr2</td><td>4539.595</td><td>-2.290</td><td>Fe1</td><td>4973.102</td><td>-0.950</td><td>Fe1</td><td>5434.524</td><td>-2.122</td><td>Nil</td><td>5715.066</td><td>-0.352</td></tr><tr><td>Cr2</td><td>4558.650</td><td>-0.449</td><td>Fe1</td><td>4962.572</td><td>-1.182</td><td>Fe1</td><td>5445.042</td><td>-0.020</td><td>Nil</td><td>6086.276</td><td>-0.530</td></tr><tr><td>Cr2</td><td>4565.740</td><td>-1.820</td><td>Fe1</td><td>4966.089</td><td>-0.871</td><td>Fe1</td><td>5446.917</td><td>-1.914</td><td>Nil</td><td>6176.807</td><td>-0.260</td></tr><tr><td>Cr2</td><td>4588.199</td><td>-0.627</td><td>Fe1</td><td>4973.102</td><td>-0.950</td><td>Fe1</td><td>5455.441</td><td>0.291</td><td>Cu1</td><td>5105.537</td><td>-1.516</td></tr><tr><td>Cr2</td><td>4634.070</td><td>-0.990</td><td>Fe1</td><td>4988.950</td><td>-0.890</td><td>Fe1</td><td>5455.610</td><td>-2.091</td><td>Zn1</td><td>4722.153</td><td>-0.338</td></tr><tr><td>Cr1</td><td>4646.148</td><td>-0.700</td><td>Fe2</td><td>5004.195</td><td>0.497</td><td>Fe1</td><td>5473.901</td><td>-0.760</td><td>Y2</td><td>5200.406</td><td>-0.570</td></tr><tr><td>Cr1</td><td>4652.152</td><td>-1.030</td><td>Fe2</td><td>5018.440</td><td>-1.220</td><td>Fe1</td><td>5497.516</td><td>-2.849</td><td>Ba2</td><td>4554.029</td><td>0.170</td></tr><tr><td>Cr1</td><td>5204.506</td><td>-0.208</td><td>Fe1</td><td>5044.211</td><td>-2.038</td><td>Fe2</td><td>5529.932</td><td>-1.875</td><td>Ba2</td><td>5853.668</td><td>-1.000</td></tr><tr><td>Cr2</td><td>5237.329</td><td>-1.160</td><td>Fe1</td><td>5049.820</td><td>-1.355</td><td>Fe1</td><td>5554.895</td><td>-0.440</td><td>Ba2</td><td>6141.713</td><td>-0.076</td></tr><tr><td>Cr2</td><td>5249.437</td><td>-2.489</td><td>Fe2</td><td>5061.718</td><td>0.217</td><td>Fe1</td><td>5560.212</td><td>-1.190</td><td>Ce2</td><td>4562.359</td><td>0.310</td></tr><tr><td>Cr2</td><td>5279.876</td><td>-2.100</td><td>Fe1</td><td>5065.014</td><td>-0.134</td><td>Fe1</td><td>5565.704</td><td>-0.285</td><td></td><td></td><td></td></tr><tr><td>Cr2</td><td>5280.054</td><td>-2.011</td><td>Fe1</td><td>5074.748</td><td>-0.200</td><td>Fe1</td><td>5569.618</td><td>-0.486</td><td></td><td></td><td></td></tr></tbody></table>
<table><caption>**Table 5.** Selected lines ([n] < 5) used for abundance determination of HD 73722, HD 74275, HD 75029 and SHJM 2.</caption><thead><tr><th colspan="3">HD 73722</th><th colspan="3">HD 74275</th><th colspan="3">HD 75029</th><th colspan="3">SHJM 2</th></tr><tr><th>Identity</th><th>λ[Å]</th><th>log gf</th><th>Identity</th><th>λ[Å]</th><th>log gf</th><th>Identity</th><th>λ[Å]</th><th>log gf</th><th>Identity</th><th>λ[Å]</th><th>log gf</th></tr></thead><tbody><tr><td>C1</td><td>4770.026</td><td>-2.439</td><td>He1</td><td>5875.615</td><td>0.409</td><td>Sc2</td><td>5031.021</td><td>-0.400</td><td>C1</td><td>4932.049</td><td>-1.884</td></tr><tr><td>C1</td><td>4932.049</td><td>-1.884</td><td>O1</td><td>6156.756</td><td>-0.899</td><td>Sc2</td><td>5239.813</td><td>-0.765</td><td>C1</td><td>5380.337</td><td>-1.842</td></tr><tr><td>C1</td><td>5052.167</td><td>-1.648</td><td>O1</td><td>6158.186</td><td>-0.409</td><td>Sc2</td><td>5526.790</td><td>0.024</td><td>Na1</td><td>4497.657</td><td>-1.560</td></tr><tr><td>C1</td><td>5380.337</td><td>-1.842</td><td>Na1</td><td>5889.951</td><td>0.117</td><td>Mn1</td><td>5377.637</td><td>-0.109</td><td>Na1</td><td>5688.205</td><td>-0.450</td></tr><tr><td>O1</td><td>6156.776</td><td>-0.694</td><td>Na1</td><td>5895.924</td><td>-0.184</td><td>Mn1</td><td>6021.819</td><td>0.034</td><td>Na1</td><td>6154.226</td><td>-1.560</td></tr><tr><td>Na1</td><td>5682.633</td><td>-0.700</td><td>A12</td><td>4663.046</td><td>-0.284</td><td>Cu1</td><td>5105.537</td><td>-1.516</td><td>Na1</td><td>6160.747</td><td>-1.260</td></tr><tr><td>Na1</td><td>5688.205</td><td>-0.450</td><td>Si2</td><td>5978.930</td><td>0.004</td><td>Y2</td><td>5087.416</td><td>-0.170</td><td>Mg1</td><td>4167.271</td><td>-1.004</td></tr><tr><td>Na1</td><td>6154.226</td><td>-1.560</td><td>Si2</td><td>6347.109</td><td>0.297</td><td>Y2</td><td>5200.406</td><td>-0.570</td><td>Mg1</td><td>4571.096</td><td>-5.691</td></tr><tr><td>Na1</td><td>6160.747</td><td>-1.260</td><td>Si2</td><td>6371.371</td><td>-0.003</td><td></td><td></td><td></td><td>Mg1</td><td>5711.088</td><td>-1.833</td></tr><tr><td>S1</td><td>4695.443</td><td>-1.920</td><td>Ca1</td><td>4226.728</td><td>0.265</td><td></td><td></td><td></td><td>All</td><td>6696.023</td><td>-1.347</td></tr><tr><td>S1</td><td>4696.252</td><td>-2.140</td><td>Ca1</td><td>4454.779</td><td>0.335</td><td></td><td></td><td></td><td>All</td><td>6698.673</td><td>-1.647</td></tr><tr><td>S1</td><td>6052.583</td><td>-1.330</td><td>Sc2</td><td>4246.822</td><td>0.242</td><td></td><td></td><td></td><td>S1</td><td>6052.674</td><td>-0.740</td></tr><tr><td>S1</td><td>6757.171</td><td>-0.310</td><td>Sr2</td><td>4215.519</td><td>-0.145</td><td></td><td></td><td></td><td>Cu1</td><td>5105.537</td><td>-1.516</td></tr><tr><td>Co1</td><td>4792.846</td><td>-0.067</td><td></td><td></td><td></td><td></td><td></td><td></td><td>Zn1</td><td>4722.153</td><td>-0.338</td></tr><tr><td>Co1</td><td>5212.691</td><td>-0.110</td><td></td><td></td><td></td><td></td><td></td><td></td><td>Sr2</td><td>4161.792</td><td>-0.502</td></tr><tr><td>Co1</td><td>5342.695</td><td>0.690</td><td></td><td></td><td></td><td></td><td></td><td></td><td>Sr2</td><td>4215.519</td><td>-0.145</td></tr><tr><td>Co1</td><td>5352.045</td><td>0.060</td><td></td><td></td><td></td><td></td><td></td><td></td><td>Sr1</td><td>4607.327</td><td>-0.570</td></tr><tr><td>Cu1</td><td>5105.537</td><td>-1.516</td><td></td><td></td><td></td><td></td><td></td><td></td><td>Y2</td><td>5087.416</td><td>-0.170</td></tr><tr><td>Cu1</td><td>5218.197</td><td>0.476</td><td></td><td></td><td></td><td></td><td></td><td></td><td>Y2</td><td>5119.112</td><td>-1.360</td></tr><tr><td>Zn1</td><td>4722.153</td><td>-0.338</td><td></td><td></td><td></td><td></td><td></td><td></td><td>Y2</td><td>5402.774</td><td>-0.510</td></tr><tr><td>Sr2</td><td>4161.792</td><td>-0.502</td><td></td><td></td><td></td><td></td><td></td><td></td><td>Y2</td><td>5544.611</td><td>-1.090</td></tr><tr><td>Sr1</td><td>4607.327</td><td>-0.570</td><td></td><td></td><td></td><td></td><td></td><td></td><td>Zr2</td><td>4208.977</td><td>-0.460</td></tr><tr><td>Zr2</td><td>4208.977</td><td>-0.460</td><td></td><td></td><td></td><td></td><td></td><td></td><td>Zr2</td><td>5112.297</td><td>-0.590</td></tr><tr><td>Ba2</td><td>4166.000</td><td>-0.420</td><td></td><td></td><td></td><td></td><td></td><td></td><td>Ba2</td><td>4554.029</td><td>0.170</td></tr><tr><td>Ba2</td><td>5853.668</td><td>-1.000</td><td></td><td></td><td></td><td></td><td></td><td></td><td>Ba2</td><td>5853.668</td><td>-1.000</td></tr><tr><td>Ba2</td><td>6496.897</td><td>-0.377</td><td></td><td></td><td></td><td></td><td></td><td></td><td>Ce2</td><td>4562.359</td><td>0.310</td></tr><tr><td>Ce2</td><td>4562.359</td><td>0.310</td><td></td><td></td><td></td><td></td><td></td><td></td><td>Ce2</td><td>4628.161</td><td>0.220</td></tr><tr><td>Ce2</td><td>4628.161</td><td>0.220</td><td></td><td></td><td></td><td></td><td></td><td></td><td>Nd2</td><td>4706.543</td><td>-0.775</td></tr><tr><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td>Nd2</td><td>5311.453</td><td>-0.437</td></tr><tr><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td></td><td>Eu2</td><td>4205.042</td><td>0.120</td></tr></tbody></table>