A Simulations

Coronal abundances of X-ray bright pre-main sequence stars in the Taurus Molecular Cloud

Key Words.:
X-rays: stars – Galaxy: Open Clusters and Associations: Individual: Name: Taurus Molecular Cloud – stars: abundances – stars: coronae – stars: pre-main-sequence
1

Abstract

Context:

Aims:We studied the thermal properties and chemical composition of the X-ray emitting plasma of a sample of bright members of the Taurus Molecular Cloud to investigate possible differences among classical and weak-lined T Tauri stars and possible dependences of the abundances on the stellar activity level and/or on the presence of accretion/circumstellar material.

Methods:We used medium-resolution X-ray spectra obtained with the sensitive EPIC/PN camera in order to analyse the possible sample. The PN spectra of 20 bright ( erg s) Taurus members, with at least counts, were fitted using thermal models of optically thin plasma with two components and variable abundances of O, Ne, Mg, Si, S, Ar, Ca, and Fe. Extensive preliminary investigations were employed to study the performances of the PN detectors regarding abundance determinations, and finally to check the results of the fittings.

Results:We found that the observed X-ray emission of the studied stars can be attributed to coronal plasma having similar thermal properties and chemical composition both in the classical and in the weak-lined T Tauri stars. The results of the fittings did not show evidence for correlations of the abundance patterns with activity or accretion/disk presence. The iron abundance of these active stars is significantly lower than ( of) the solar photospheric value. An indication of slightly different coronal properties in stars with different spectral type is found from this study. G-type and early K-type stars have, on average, slightly higher Fe abundances (Fe solar) with respect to stars with later spectral type (Fe solar), confirming previous findings from high-resolution X-ray spectroscopy; stars of the former group are also found to have, on average, hotter coronae.

Conclusions:

1 Introduction

Studies on the chemical composition of stellar atmospheres are important to address several issues in astrophysics, such as the evolution of stellar galactic populations, the enrichment of the interstellar medium, the influence of elemental abundances on star formation processes and on the structure of stellar interiors through opacity effects. In the framework of coronal physics, solar and stellar observations in the UV and X-ray bands during the last two decades have suggested abundance anomalies that, if understood, could provide powerful new diagnostics for the physics of stellar outer atmospheres. In particular, previous observations of the Sun (Meyer, 1985; Feldman, 1992), showed different chemical abundances in corona with respect to the photosphere, with a pattern depending on the First Ionization Potential (FIP) of the various elements. The present view is that elements with FIP  eV (low-FIP elements Mg, Si, Ca, Ni, Fe) are overabundant in the solar corona with respect to the photosphere by a factor ; elements with FIP  eV (high-FIP elements C, S, O, Ne, Ar, with C and S lying close to the boundary of this definition) have coronal abundances similar to the corresponding photospheric values. This solar-type FIP effect is most clearly present in long-lived active regions, while it is much less marked (or even absent) in coronal holes (Widing & Feldman, 1992; Sheeley, 1996). In order to compare solar and spatially-integrated stellar observations, Laming et al. (1994) investigated full-disk solar EUV spectra, and detected the FIP effect also in this case.

Analyses of EUV line emission spectra from the coronae of low- and intermediate-activity stars ( Centauri, Bootis, Eridani, observed with the EUVE satellite) revealed solar-like abundance anomalies, suggesting that the FIP effect is not an isolated solar phenomenon (Laming et al., 1996; Drake et al., 1997; Laming & Drake, 1999). New studies, based on XMM-Newton and high-resolution X-ray spectra, have led to claims of different FIP-dependent abundance patterns in the coronae of other stars: in particular, observations of very active stars, both single stars and active binary systems, suggested a dependence of coronal abundances on FIP which is reversed with respect to the Sun and the other low-activity stars mentioned above, i.e. a depletion of low-FIP elements with respect to high-FIP elements (inverse FIP effect; (Brinkman et al., 2001; Audard et al., 2003; Robrade & Schmitt, 2005)). Telleschi et al. (2005) derived coronal abundances for 6 solar analogs (i.e. G-type main sequence stars) with different ages and rotation periods, and hence activity levels: this work suggested a change from an inverse FIP effect to a solar-type FIP effect with increasing age, and hence with decreasing activity.

On the contrary, other authors found evidence for neither a FIP nor an inverse FIP effect in the coronae of active late-type stars (Sanz-Forcada et al., 2003; Argiroffi et al., 2004; Scelsi et al., 2005), but instead a minimum in the abundance pattern occurring at FIP  eV, with increasing abundances at both lower and higher FIP values. In any case, a systematic result emerging from stellar abundance studies is that the coronae of high-activity stars appear significantly metal-poor relative to the solar photosphere, with typical iron abundances times the Anders & Grevesse (1989) solar photospheric value.

A major problem encountered in coronal abundance studies is related to data analysis issues. The requirements for an accurate analysis are good quality X-ray spectra (i.e. high ratios), a careful selection of emission lines (not affected by blends and independent from the plasma density), accurate line emissivity functions describing the physics of atomic transitions, and a precise knowledge of the instrumental response. All these difficulties introduce errors that are often not accounted for in the reported (just statistical) measurement uncertainties, which therefore are likely underestimated in many studies.

While the coronal metal deficiency of active stars seems to be a rather solid result, the question whether coronal abundances are different from the photospheric values, with a pattern possibly dependent on the FIP, is still debated and deserves further investigation, especially because photospheric abundances of active, rapid rotators are mostly unavailable. Better observational evidence is definitely required to test theoretical models proposed to explain the physical mechanism(s) responsible for such differences (e.g. Schwadron et al., 1999; Laming, 2004).

In classical T Tauri stars (CTTSs) material from the circumstellar disk accretes onto the stellar surface and shock waves at the base of the accretion funnel are expected to heat the gas to X-ray emitting temperatures of a few million degrees. From recent analyses of XMM-Newton and spectra of pre-main sequence stars, interesting peculiarities in the abundances of some CTTSs were also noted: TW Hydrae, TWA 5, and BP Tauri show anomalous Ne/Fe abundance ratios ( solar, Stelzer & Schmitt, 2004; Argiroffi et al., 2005; Robrade & Schmitt, 2006), significantly higher than those typically found for other stars (). Such peculiarities could be inherited from the original cloud where these stars formed, but they might also be due to some process of chemical segregation during the evolution of circumstellar disks. In fact, most of the soft X-ray emission of TW Hydrae and part of the emission of BP Tauri have been attributed to accretion shocks (while the situation for TWA 5 is more uncertain). Iron and other metals in the disk could condense in grains, as predicted by some models of cloud chemistry (Savage & Sembach, 1996; Charnley, 1997). If we suppose that the gas and dust phases in the circumstellar disk are separated for some reason, with the metals remaining at larger distance from the star, while neon and other noble elements in the gas phase accrete more efficiently onto the stellar surface, then the gas heated by the shock at X-ray emitting temperatures is expected to be metal-deficient and enriched in neon. The high Ne/O ratio of TW Hydrae may be another sign of such a segregation process occurred in the circumstellar disk of this star, as argued by Drake et al. (2005). Should this scenario be proven correct for the CTTSs and the gas-dust separation mechanism understood, the chemical composition of the hot plasma could provide new insight into the study of circumstellar disks. The relevance for our understanding of planetary formation could also be significant.

Most recently, Maggio et al. (2007) studied a sample of 146 X-ray bright sources associated with members of the young Orion Nebula Cluster (ONC), and found that their emission originates from a plasma with temperatures and elemental abundances very similar to those of active coronae in older stars. Moreover, the abundance distributions are compatible with a single pattern vs. FIP for all stars for all elements with the only possible exception of the Calcium abundance. Comparison with abundances in stellar photospheres and in the gaseous component of the nebula indicate a significant underabundance at coronal level only for iron (by a factor 1.5–3), while there is agreement (and hence no evidence of a FIP-related effect) for all the other elements with available measurements.

In another recent study based on nine high-resolution RGS spectra from the XEST survey, Telleschi et al. (2007) found similar abundances in accreting and non-accreting stars and indication of higher Fe abundances in the G-type stars of their sample compared to stars with later spectral type. They also found that CTTSs display a soft excess when compared to WTTSs or zero-age main-sequence stars, and that high electron densities and Ne/Fe abundance ratios are not characteristic of all accreting PMS stars.

In this paper we analyze X-ray spectra taken with XMM-Newton to derive the thermal properties and chemical composition of the X-ray emitting plasma of a sample of 20 young stellar objects (7 CTTSs and 13 WTTSs) belonging to the Taurus-Auriga star forming region and spanning an age range of  Myr. This region has been recently the subject of the XMM-Newton Extended Survey of Taurus (XEST, Güdel et al., 2007), which allowed us to study the X-ray emission from more than 150 classical and weak-lined T Tauri stars in the Taurus Molecular Cloud (TMC). The present work focuses on some of the most active members of the TMC, with the aim to understand whether accreting and non-accreting pre-main sequence stars show any systematic difference in the abundance pattern, and to investigate possible dependences of the coronal abundances on the activity level.

The paper is organized as follows. Section 2 summarizes relevant information about the TMC and the XEST observations. In Sect. 3 we describe the strategy employed to select the sample and we report the spectral fitting results, whose discussion is presented in Sect. 4. Finally, we draw our conclusions in Sect. 5. Appendix A details the simulations performed for this work.

2 The TMC and the XEST observations

The TMC is a cloud complex at 140 pc from the Sun, which contains about 400 known low-mass members; they are spread over a relatively large portion of the sky ( square degrees) and their ages cover a range between and years, with most stars being typically 1–10 million years old. The XEST survey consists of 19 recent observations (fields XEST-02 to XEST-20), obtained in two separate periods (August-September 2004 and February-March 2005) and with exposures ranging from 27 to 35 ks, to which 8 more previous fields2 from the XMM-Newton archive were added, having longer exposure times in the range 43–131 ks. In total, the surveyed area covers only square degrees of the Taurus Molecular Cloud; however, since the observed fields were chosen so as to include the densest regions of the TMC with the largest concentrations of stars, the total number of detections associated to Taurus members in the EPIC images is 159. Including non-resolved companions that might be contributing to the X-ray emission, the XEST survey likely detected around 210 members, that is about a half of the entire known stellar population in Taurus. This sample contains mainly classical and weak-lined T Tauri stars, but also protostars, brown dwarfs and a few Herbig Ae/Be stars and other members with uncertain classification.

The present study is based on X-ray spectra taken with the most sensitive instrument onboard XMM-Newton, the EPIC PN camera (Strüder et al., 2001). This non-dispersive CCD detector has an effective area of  cm at 1.5 keV and provides moderate spectral resolution in the range  keV. Bright sources in the field XEST-26 (around SU Aur), which lacks PN data, were excluded from the analysis to ensure homogeneity of the results. For the XEST observations, the PN was operated in full window mode and the medium filter was applied in all observations, with the exception of the field XEST-27 (around Per) where the thick filter was used.

We refer to the paper by Güdel et al. (2007) for more details about all the observations of the XEST project, which were processed using SAS v6.1, and the data reduction steps.

3 Data analysis

3.1 Preliminary simulations and choice of the sample

A study of the chemical composition and of possible effects due to activity or accretion processes requires a large sample of stars and accurate and precise abundance measurements. Accurate estimates of abundances can be derived with the analysis of high-resolution spectra, where individual emission lines of several chemical elements are well resolved. The XEST survey has provided useful RGS spectra for nine TMC members, which have been analysed by Telleschi et al. (2007).

In order to consider a larger sample of T Tauri stars, we based our study on the medium resolution spectra taken with the PN camera, which is times more sensitive than the RGS spectrometers and, unlike the latter, can also provide data for sources located off-axis in the field-of-view. The use of PN data required a preliminary feasibility study to understand the reliability of the results obtained from their analysis. In fact, the blending of the lines of many elements (neon, iron, nickel, oxygen) and the method used to analyze these spectra (i.e. global fitting with a plasma emission model with few isothermal components) might lead to systematic uncertainties in the abundances derived for some of the elements. In particular, we addressed two issues: (i) Is the global fitting of PN spectra able to recover the true values of elemental abundances, considering sources in a variety of physical conditions? (ii) What minimum number of detected source counts are required to obtain measurements with relatively low abundance uncertainties, say within a factor of 2?

These two issues are clearly not unrelated, since the ability of deriving an accurate and precise abundance value for a given element depends on a) whether the lines of that element have a good signal, and hence on the element abundance, on the thermal structure of the plasma and also on the amount of interstellar absorption, b) the statistics of the entire spectrum, which must allow a good determination of the source thermal properties. We also point out that facing these issues requires the most accurate knowledge of the instrumental response function allowed by the instrument calibration.

To answer the above questions, we performed a large number of simulations exploring a variety of source conditions. At the same time, this procedure allowed us to put a rough threshold on the total number of source counts, below which the fitting parameters begin to be poorly constrained, and hence to define the sample of stars to be studied. The approach is analogous to that employed by Maggio et al. (2007) for their abundance study on a sample of stars in Orion, observed with /ACIS.

In brief, our simulations, whose details are reported in Appendix A, showed that the abundances of most elements can be rather accurately derived from fitting of PN spectra and set an indicative threshold of total counts in order to have useful PN data for abundance studies. Uncertainties at 90% level are usually better than a factor 2.5 for spectra with counts, and better than a factor 2 for spectra with counts. The iron abundance is the best constrained in most simulations, although some caveats must be noted in a few cases (see Appendix A). Instead, the abundances of Ar and Ca are generally very poorly constrained, as well as the O abundance in case of high absorption ( cm).

Therefore, we selected all the TMC members with more than counts in the PN spectra ( keV), integrated over time intervals not affected by high background levels. We also added to the sample the two stars Anon 1 and L1551-51 with counts. The sample defined in this way is listed in Table 1 and consists of 20 TMC members, 13 of which are weak-lined T Tauri stars, and the remaining 7 are accreting PMS stars (1 Herbig Be star and 6 CTTSs). Note that the Herbig Be star in this sample, V892 Tauri, has a close companion ( separation) with an estimated mass of  M (Smith et al., 2005), which therefore is likely to be the main source of X-ray emission, rather than the Herbig Be star itself. It is also likely that such a companion is an accreting star, based on previous studies (Duchêne et al., 1999; König et al., 2001; Hartigan & Kenyon, 2003) showing that mixed binary systems, i.e. systems that include both accreting and non-accreting stellar components, are very uncommon. Using the evolutionary models by Siess et al. (2000) and age equal to that of the primary star ( Myr), the spectral type of this companion is K3 for  M, K2 for  M and K1 for  M. In the following we will assume a spectral type of K2.

Name XEST id Total GTI PN TTS Spec
Exp. cts type type
(ks) (ks)
Anon 1 20-005 26.8 26.8 4520 W M0
CoKu Tau 3 12-059 26.4 25.7 10454 W M1
DN Tau 12-040 26.4 25.7 5169 C M0
IT Tau 18-030 26.8 23.8 8605 C K2
L1551-51 22-089 48.9 45.4 4506 W K7
V773 Tau 20-042 26.8 26.8 29971 W K2
V826 Tau 22-100 48.9 45.4 16950 W K7
V830 Tau 04-016 27.6 26.1 8765 W K7
DH Tau 15-040 27.4 23.3 14780 C M1
HD 283572 21-039 41.1 33.9 79424 W G5
HP Tau/G2 08-051 33.7 31.2 15033 W G0
Hubble 4 23-056 62.6 51.9 16394 W K7
KPNO-Tau 15 08-043 33.7 31.2 6017 W M2.75
RY Tau 21-038 41.1 33.9 5685 C K1
V410 Tau 24-028 36.9 27.4 26740 W K4
V819 Tau 23-074 62.6 51.9 5524 W K7
V892 Tau 23-047 62.6 51.9 10886 C K2 ?
BP Tau 28-100 116.4 88.0 17770 C K7
T Tau 01-045 67.2 37.5 29960 C K0
RXJ0422.1+1934 01-054 67.2 37.5 11296 W -
The light curve suggests that the emission is affected by the
   final stage of a flare decay.
A flare occurred during the observation is excluded from the
   GTIs.
Secondary of the binary system.
Table 1: Sample of TMC members selected for the abundance study. “XEST id” is the identification label in the XEST catalog, the first two digits referring to the XEST field. For each source, both the total exposure time of the relevant observation and the screened time (GTI) selected for this study are reported; “PN cts” are the source counts during the GTIs. “W” and “C” stand for WTTS and CTTS, respectively. TTS types and spectral types are taken from Güdel et al. (2007) and references therein, except where noted.

3.2 Spectral fittings of TMC members

The PN counts of the selected TMC members were extracted from circular regions around the sources, having typical radii of . For each source, the background events were extracted from an annulus around the source; contamination from close X-ray sources within the annulus was also avoided (see Güdel et al. 2007 for more details about the calculation of the source and background extraction regions). The standard tasks of SAS were used to build the instrumental responses for all sources. In Table 1 we report both the total exposure times of the fields where the selected targets lie and the Good Time Intervals obtained by excluding from the present analysis those time intervals affected by high background emission (due to solar events), in order to increase the ratios of the studied spectra at high energies; in the case of BP Tau, a  ks interval when the source exhibited a strong flare was also excluded, so as to avoid possible effects of time variation of the abundances, as suggested by a number of previous studies (Tsuboi et al., 1998; Güdel et al., 1999; Favata & Schmitt, 1999).

All PN spectra were fitted with the software XSPEC, limiting the fitting of each source to those energy bins where the background spectrum does not affect significantly the source emission (usually  keV, in very few cases we excluded the energy bins at  keV). We used a two-component thermal, optically thin plasma based on the APEC emissivity code, plus interstellar absorption, which is the same model employed for the simulations. The model has 13 free parameters: the hydrogen column density , the temperatures and and the emission measures and of the two components, and the abundances of O, Ne, Fe, Mg, Si, S, Ca and Ar. For each source, the value, the two temperatures and the ratio of the emission measures of the best-fitting model are reported in Table 2, together with the unabsorbed X-ray luminosity derived from the model, the average temperature and the surface X-ray flux derived from and the stellar radius (the latter is taken from the Tables in Güdel et al. 2007). Average temperatures are weighted by the emission measure and are useful to compare the global thermal properties of the emitting plasma in different stars; they are indicative values and are reported without errors in the table. The surface fluxes are also reported without errors, owing to uncertainties in the adopted stellar radii. In Fig. 1 we plot the observed spectra with their relevant model spectra, for some example cases.

Name (d.o.f.)
( cm) (MK) (MK) ( erg s) (MK) ( erg s cm)
Anon 1 0.96 (141) 7.4 10.0
CoKu Tau 3 0.88 (284) 12.2 20.6
DN Tau 1.18 (142) 18.4 3.4
IT Tau 0.92 (256) 30.7 22.8
L1551-51 1.04 (128) 12.3 14.0
V773 Tau 1.07 (434) 17.9 40.2
V826 Tau 1.16 (304) 11.0 21.6
V830 Tau 1.17 (237) 14.5 28.7
DH Tau 1.04 (319) 17.3 37.7
HD 283572 1.02 (599) 19.1 30.7
HP Tau/G2 0.94 (329) 18.0 24.1
Hubble 4 1.14 (341) 12.0 9.1
KPNO-Tau 15 0.95 (200) 27.0 36.7
RY Tau 0.79 (203) 19.8 10.7
V410 Tau 1.04 (364) 14.4 14.9
V819 Tau 0.95 (175) 12.6 10.0
V892 Tau 0.94 (325) 20.8 20.7
BP Tau 0.99 (338) 14.1 6.0
T Tau 1.22 (513) 22.2 9.4
RXJ0422.1+1934 0.93 (302) 13.6 -
Table 2: Parameters of the best-fit models for the 20 TMC members, with errors. The unabsorbed X-ray luminosity and the surface flux are calculated in the  keV band. is defined as .
Figure 1: Examples of PN spectra (points with error bars) and best-fit model spectra (histogram) of selected TMC members in the present study. The bottom of each plot shows the residuals in units of .

Figure 2 shows the properties of the X-ray emitting plasma of the studied sample. The distributions of temperatures and EM ratios are very similar in the subsamples of WTTSs and CTTSs; the latter seems to have, on the whole, average temperatures slightly greater with respect to the WTTS (the medians of the distributions of are 13.5 MK and 19.5 MK, respectively), although a Kolmogorov-Smirnov test gives 7% probability that the distributions for WTTSs and CTTSs are not distinguishable.

Figure 2: Temperature, emission measure and X-ray luminosity values for the WTTSs and the CTTSs of the studied sample. The values on the axis have different units, for each quantity, as reported in the -axis labels.
Figure 3: Abundances of the 20 TMC members for each element, ordered for increasing FIP. The size of the circles gives a rough indication of the accuracy of the measurements: large circles for abundances derived from spectra with less than 10 000 counts, medium circles for counts , and small circles for counts . At the bottom of the plot, close to the label of each element, the number of stars with abundances lying outside the plot (i.e. lower than 0.01 solar) are indicated. The short thick segments mark the medians of the abundance distributions, while the long thin segments mark the values assumed by Güdel et al. (2007) to fit EPIC spectra of Taurus members (see Sect. 4.1).

In Fig. 3 we plot the derived abundances (in solar units of Anders & Grevesse 1989) of the TMC members, where the elements are ordered by increasing FIP. The 20 values of abundances are rather widely distributed. The medians of their distributions show a pattern with a minimum around Fe and Si, a trend already obtained from the analysis of high-resolution spectra for several main sequence, pre-main sequence and giant stars with high X-ray luminosity (Sanz-Forcada et al., 2003; Argiroffi et al., 2004; Scelsi et al., 2004; Argiroffi et al., 2005; Scelsi et al., 2005; Telleschi et al., 2005). However, as mentioned above, the Ca abundance was generally ill-constrained in the simulations, which showed that nearly solar values can be frequently obtained even when the input Ca abundance is significantly subsolar; hence, if we do not consider calcium, the pattern of the medians resembles an inverse FIP effect.

It is important to note, however, that the medians of the abundance distributions express average properties of the studied sample, while the abundances of individual stars might be correlated with other stellar parameters. Yet, comparison of Fig. 3 with the results of the simulations shows that the spread of the derived abundances for a given element is roughly of the same magnitude as the one found from the simulations (in comparing Fig.3 and Fig. 11 consider that half of our sample stars have less than counts). This implies that with the available data we can hardly distinguish between the abundances of any given element in different stars of the present sample, and hence it is not meaningful to search for possible correlations with other parameters. This result also suggests that the derived sets of abundances of these TMC members could be drawn from a single set of abundances, i.e. the spread of the values for any given element is not due to differences among the sources, but rather to statistical fluctuations. To check this idea, we proceeded as follows: we simulated 10 000 PN spectra starting from a two-temperature model which reflects the average observed properties of the studied sample, that is , , , and elemental abundances equal to the medians of the relevant observed distributions (Table 3). The total number of counts in the 10 000 simulated spectra reflects the distribution of counts observed in the real spectra of the 20 TMC members. Afterwards, we fitted these spectra with a 2-T model with the same (13) free parameters as before.

Ca Mg Fe Si S O Ar Ne
2 7 23 1.2 0.67 0.23 0.195 0.20 0.29 0.45 0.37 0.86
Table 3: Medians of the distributions of absorption, temperatures, emission measures and abundances derived from the PN spectra of the studied sample. Abundances are in solar units, in  cm, and in MK.

The result of this test is reported in Fig. 4, which shows the distributions of the abundances (in the upper panel) and the abundances normalized to iron (in the lower panel) obtained from the real data, compared with the central 90% ranges of values obtained from the simulations, for each element. In both panels, the spread of the values derived from real data is comparable to that indicated by the simulations, for all elements. Exception is the Ne/Fe abundance ratio, whose distribution is significantly larger in the case of the real data. This is better quantified by a K-S test which shows that for the case of the Ne/Fe ratio the two distributions are different with a significance of more than . The range of O/Fe ratios also appears to exceed the 90% bounds of the range of the simulations, but the difference between the two distributions is not statistically significant (K-S probability of undistinguishable distributions equal to 7%). The result about the Ne/Fe ratio is intriguing and deserves to be further investigated, because neon and iron are chemical elements having different properties related to their tendency of forming dust grains, with the volatile noble gas neon remaining in the gaseous phase while iron more easily condensing in grains. Moreover, Ne is a high-FIP element, while Fe is a low-FIP element. In the next Sect. 4.2 we discuss the Ne/Fe ratio for the stars of the present sample together with some possibilities that could explain the above result.

Figure 4: Distributions of abundances (upper panel) and abundances relative to iron (lower panel) found for the 20 TMC members, compared with the results of simulations (see text). The boxes contain the central 90% of the abundance values obtained from the simulations, the median being indicated by the thick black segment within each box. The thin, longer segments mark the medians of the abundance distributions derived from real data; they are practically coincident with the median values of the simulations. Numbers at the bottom of the plot are as in Fig. 3.

In Fig. 5 we separate the abundance distributions of the classical and the weak-lined T Tauri stars: the plot shows that there is no significant difference between the distributions for the two classes of sources, indicating that both the thermal properties (Fig. 2) and chemical composition of the X-ray-emitting plasma are similar.

Figure 5: Scatter plot of abundances obtained for the classical (open circles) and weak-lined (filled circles) T Tauri stars in the studied sample. Numbers at the bottom of the plot are as in Fig. 3.

4 Discussion

4.1 Medians of the abundance distributions

A robust result of this analysis is the low iron abundances of the X-ray bright Taurus members with respect to the solar photospheric value (Fe solar), since the abundance of this element is generally well-determined and with relatively small uncertainties (as indicated by the simulations). This analysis thus confirms the results of other previous studies on high-luminosity stars (pre-main sequence stars and RS CVn binary systems) which indicate a low coronal metallicity, with respect to the solar case, in such active stars (e.g. Maggio et al., 2007; Drake et al., 2001; Huenemoerder et al., 2001; Audard et al., 2003).

In Fig. 3 we also report the fixed values of abundances used by Güdel et al. (2007) for fitting the EPIC spectra of more than a hundred Taurus members, with the aim of deriving absorption column densities, characteristic plasma temperatures and X-ray luminosities. The values adopted by these authors (see also Appendix A) were chosen as representative of the coronal abundances in active stars. Our detailed analysis confirms the validity of this assumption, because the medians of the abundance distributions for all elements are very similar to the previously adopted values, with the possible exception of calcium.

In Sect. 3.2 we showed that the medians of the abundance distributions follow a pattern vs. FIP similar to that derived from the analysis of high-resolution X-ray spectra for a number of active stars (Sanz-Forcada et al., 2003; Argiroffi et al., 2004; Scelsi et al., 2004; Argiroffi et al., 2005; Scelsi et al., 2005; Telleschi et al., 2005); given the large uncertainties of the Ca abundances, our analysis might also suggest a systematic pattern of increasing abundances for increasing FIP. However, such a pattern is obtained by adopting solar photospheric abundances as reference, while any FIP-related effect should be studied by comparison with the stellar photospheric abundances; unfortunately, they are not available for any of the stars in our sample. Measuring abundances in stellar photospheres is a difficult task, due to the limited quality of stellar optical spectra, to uncertainties in stellar parameters (gravity, effective temperature, macro-turbulence) and atmospheric models (LTE approximations), to line blending (especially for cool M-type stars) and rotational broadening effects which is typically the case of active young stars; furthermore, the effects of possible stellar spots and of the chromospheric activity on abundance determinations are not well understood, and binarity requires the non-trivial procedure of untangling composite spectra. An assumption usually adopted is that stars in the solar neighbourhood have photospheric abundances similar to the solar ones, because they belong to the same galactic population; moreover, we expect that stars younger than the Sun have on average higher metallicities because they have formed from material enriched in high-Z elements by the remnants of an older stellar population. However, extensive surveys show that there is a large scatter in metallicity among stars of similar age (Nordström et al., 2004). Sanz-Forcada et al. (2004) studied the coronal abundances of four stars with accurately known photospheric abundances and showed indeed that the pattern of coronal-to-photospheric abundance ratios vs. FIP can be different if stellar or solar photospheric abundances are used. The recent study by Maggio et al. (2007) on the X-ray brightest stars in Orion also indicates that a clear trend vs. FIP is no longer observed when the photospheric abundances of the Orion stars or the composition of the gaseous phase in the nebula are considered instead of the solar ones. On the other hand, Sanz-Forcada et al. (2003) derived coronal abundances that are not photospheric for AB Dor, which has well measured photospheric abundances, and Telleschi et al. (2005) found the FIP and inverse FIP patterns in six solar analogs for which several photospheric abundances are rather clearly known. It is important to dedicate more observing time to collecting optical spectra in order to measure stellar photosperic abundances and hence to address in a proper manner the issue of any FIP-related difference between the photospheric and coronal composition.

4.2 Ne/Fe abundance ratio

We now return to the spread of abundances found for the sample stars, for each element. The only quantity showing a spread of the values larger than expected from the simulations is the Ne/Fe ratio (Fig. 4), which varies between and , with a median around Ne/Fe. The ratio between the abundance of a given element and that of iron is generally better constrained than absolute abundance values, because systematic errors in the elemental and iron abundances, due e.g. to a wrong estimate of the continum emission, usually go in the same direction and can compensate when calculating their ratio. The result we obtained deserves to be investigated for several reasons.

A plausible assumption is that the photospheric abundances of iron and neon are about the same in all the stars studied here, because they belong to the same region and hence they were born from the same cloud material; then, the Ne/Fe ratio in their coronal plasma could vary depending on the stellar activity level if FIP-related effects are really present in stellar coronae, as suggested by previous studies (Brinkman et al., 2001; Audard et al., 2003). The X-ray luminosities of the sample stars are in the range  erg s, therefore the study is biased towards active TMC members. However, Audard et al. (2003) found that a transition from an inverse FIP effect to a flat pattern with decreasing coronal activity is visible in a sample of RS CVn binary systems spanning about the same X-ray luminosity range as that of the present study. In particular, they report an anticorrelation between Fe/O vs. the average coronal temperature of five active RS CVn-like systems as well as a constant value of the Ne/O ratio, which translates into a correlation between Ne/Fe and . When adding a sample of solar analogs studied by Güdel et al. (2002), reaching lower activity levels, such a correlation becomes much more evident and a trend from inverse to normal FIP effect is seen.

We plot in Fig. 6 the Ne/Fe ratio for our sample of TMC stars as a function of various activity indicators (X-ray luminosity, , average temperature, , and surface X-ray flux, ), in order to search for possible transitions from a FIP effect to an inverse FIP effect with increasing activity. However, no significant correlation of Ne/Fe with any of the considered parameters is found from the available data, which therefore do not support the existence of different FIP-related effects in the coronae of the studied stars.

However, we also note an apparent drop of the Ne/Fe ratios for stars with average temperature  MK. Based on the analysis of RGS spectra of a few stars in the XEST project, Telleschi et al. (2007) also found a bimodality in the Fe abundance and Ne/Fe ratio for their sample stars, although this behaviour was observed to be linked to the spectral type. In particular, the above authors found larger Fe abundances and lower Ne/Fe ratios in three G-type stars with respect to six K- and M-type stars. To check their result, we divided our sample into two groups, i.e. stars with spectral type earlier and later than K2 (7 sources belong to the first group, while 12 stars have spectral type later than K2, the spectral type of the star RXJ 0422.1+1934 being not available), and we observe in Fig. 6 that most of the stars cooler than 15 MK have indeed spectral type later than K2. The K-S test gives 0.15% probability that the distributions of for the two groups are drawn from the same parent distribution. We noted that this difference derives from earlier-type stars having typically higher and values.

Figure 6: Ne/Fe ratios of all sample stars plotted as a function of three activity indicators: X-ray luminosity (upper panel), average temperature (middle panel) and surface X-ray flux (lower panel). In the plot of Ne/Fe vs. , different spectral types are shown (see text): stars with spectral type later than K2 are plotted as filled circles, while open circles refer to spectral type earlier than K2 (an open square superimposed to the circle marks the Herbig Be star V892 Tau); the cross represents the WTTS RXJ0422.1+1934, whose spectral type is not available.

Figure 7 shows the cumulative distributions of the iron and neon abundances and of the Ne/Fe ratio for the stars of the two groups: there is a systematic difference in the neon abundance against the spectral type, and an even more clear evidence for lower Fe abundances in K- and M-type stars which implies larger Ne/Fe ratios than in earlier-type stars. The probability that the Fe distributions for the two groups are not distinguishable is 0.6%; for the cases of the Ne/Fe and Ne distributions, the probabilities are 8% and 17%, respectively. Franciosini et al. (2006) studied the G-type Taurus member SU Aur ( MK) and found Fe times the solar value and Ne abundance about equal to the solar one, with independent analyses of MOS and RGS data. If we consider also the abundances obtained for SU Aurigae in this picture, the result for Fe and for Ne/Fe is statistically more significant; the three K-S test probabilities mentioned above are 0.4% (Fe), 4.5% (Ne/Fe) and 29% (Ne). In this calculation we have assumed that the spectral type of the companion of V928 Tau (the probable source of X-rays) is K2; we have verified that the above conclusions do not change assuming for this star a spectral type later than K2.

Figure 7: Ne and Fe abundance distributions and Ne/Fe ratios for stars with spectral type earlier and later than K2 (three upper panels); the circle size decreases with increasing number of total counts in the PN spectrum. In the three lower panels the relevant cumulative distributions are shown.

A possible dependence of Fe and Ne/Fe on the spectral type has not been claimed in the past, before the report by Telleschi et al. (2007), and high-quality spectra of a larger sample of stars are needed to confirm it. Since the stars in our sample with spectral type later than K2 have, on average, cooler coronae, this result may also reflect a dependence on (although this is not evident in the Telleschi et al. sample). However, for stars with the highest (in the range  MK), such a dependence would be in the opposite direction with respect to that found by Audard et al. (2003), who report increasing Ne/Fe with increasing in the range  MK.

In the light of the above result, we run simulations analogous to those described in Sect. 3.2, but taking into account a possible bimodality of the iron abundance with the spectral type, i.e. we assumed Fe and Fe for stars with spectral type earlier and later than K2, respectively. Figure 8, analogous to the lower panel of Fig. 4, shows that the spread of Ne/Fe in real data can be explained in this way (K-S test probability %).

Figure 8: Distributions of abundances relative to iron for the 20 TMC members compared with the results of simulations taking into account a possible bimodality of the iron abundance (see text). Symbols and lines are as in Fig. 4.

Another issue of potential importance is that Fe forms grains much more readily than Ne: as explained in Sect. 1, if iron settles in dust grains in the disk of CTTSs and the dust and gas components are separated for some reason, X-ray emission from accreting stars may reveal a metal-depleted plasma. We note that such a result may be expected if accretion-driven emission dominates over a coronal component, since in this case the abundances we are measuring are essentially those of the accreted plasma.

The X-ray emitting plasmas of the stars in our sample have rather high average temperature ( MK), and similar properties in both the CTTSs and the WTTSs, indicating that we are probably seeing a dominant contribution from a coronal emission. Figure 9 shows the Ne/Fe ratio of our sample stars as a function of two stellar parameters linked to the presence of circumstellar material, i.e. and the accretion rate. For comparison, we report also the ratios for the two classical T Tauri stars TW Hydrae (Robrade & Schmitt, 2006) and MP Muscae (Argiroffi et al., 2007); for the CTTS BP Tauri, previously studied by other authors, we note that our Ne/Fe ratio is in very good agreement with that found by Robrade & Schmitt (2006). As expected, we do not find evidence of any relation between Ne/Fe and these two parameters; moreover, as shown in Fig. 9, high Ne/Fe ratios may be present both in CTTSs and in WTTSs and are therefore not a peculiar characteristic of accreting stars. This is consistent with the findings of Telleschi et al. (2007) that high Ne/Fe ratios are not present in all accreting stars.

Figure 9: Ne/Fe ratios as a function of the photoelectric absorption (upper panel) and accretion rate (lower panel). Errors are . Filled and open circles mark WTTSs and CTTSs respectively. In both plots, the positions of the two CTTS TW Hydrae and MP Muscae are shown as open circles without error bars. In the lower panel, only stars with measured accretion rates are shown; all WTTSs have upper limits indicated by left arrows. Accretion rates for the TMC members, for TW Hydrae and for MP Muscae are taken from the tables in Güdel et al. (2007), from Alencar & Batalha (2002) and from Sacco G. G. (private comunication), respectively.

4.3 Ne/O ratio

The Ne/O ratio shares some similarities with the Ne/Fe one, in that oxygen can easily combine with dust grains; Drake & Testa (2005) analyzed high-resolution spectra of a variety of stars (dwarfs, giants, multiple systems, subgiants) and found that the Ne/O ratio is remarkably constant in stellar coronae (Ne/O , the solar value by Anders & Grevesse 1989 being ). This is true also for the classical T Tauri stars BP Tauri and TWA 5, but not for the CTTS TW Hydrae, whose higher Ne/O value () was interpreted by Drake et al. (2005) in terms of depletion of grain-forming elements in the X-ray emitting gas which is accreting onto the star: such a depletion is supposed to be more pronounced in the case of the more evolved and older circumstellar disk of TW Hydrae, where coagulation of grains into larger bodies orbiting the star could have happened; in the younger CTTS BP Tauri, where part of the emission is accretion-driven, the dust particles could be still small and can release, after heating, the elements locked into the grains. However, very recently Argiroffi et al. (2007) obtained Ne/O for the CTTS MP Muscae, which is even older than TW Hydrae, but still shows evidence for a substantial contribution to the X-ray emission from accretion shocks in the high plasma density derived from the analysis of the O vii triplet; the average plasma temperature of this star is relatively high and hence the derived abundances are likely affected by the coronal emission. What is also emerging from these abundance studies is the need for a criterion to understand which abundances (coronal or accretion-related) we are measuring in these stars, perhaps also with the help of modeling. For the stars we studied here, the Ne/O ratio is affected by large uncertainties in those sources with high absorption, because of the difficulty of constraining the O abundance in this case. If we consider the 12 stars with  cm, we find that the Ne/O ratio is in the range , with the values equally spread around (Fig. 10). In particular, this is true also for the classical T Tauri stars DN Tauri, DH Tauri, T Tauri and BP Tauri3, among the 12 we are considering. They are rather young, with ages in the range  Myr, and their high average plasma temperatures imply a large coronal contribution, as already discussed. Therefore, our result does not go against the scenario mentioned above.

Figure 10: Ne/O ratios as a function of the photoelectric absorption, for stars with  cm. Errors are . Filled and open circles mark WTTSs and CTTSs, respectively. For comparison, the positions of the two CTTSs TW Hydrae and MP Muscae are also shown (open circles without error bars). The dotted line marks the average value of 0.41 found by Drake & Testa (2005) for stars of various activity levels.

5 Summary and conclusions

The thermal properties and chemical composition of the X-ray emitting plasma in a sample of bright Taurus members have been studied in this work with the aim of investigating possible systematic differences between classical and weak-lined T Tauri stars, and of understanding whether the pattern of abundances in such stars is related to some stellar or environmental characteristics. We used data from the XEST survey; since there are very few useful RGS spectra of Taurus members, we used the PN data in order to enlarge as much as possible the sample to be analyzed. Preliminary extensive simulations showed that PN spectra with counts or more in the  keV band can provide reliable estimates of elemental abundances and 68% statistical errors usually within a factor for most of the elements; exceptions may be O, Ca and Ar in some cases, depending on the statistics and source absorption. The sample of stars considered for this work therefore consists of 20 TMC members: 13 weak-lined T Tauri stars and 7 accreting stars, having at least 4500 total counts in the spectrum. Their medium-resolution spectra were globally fitted with an absorbed two-temperature thermal model with variable abundances of O, Ne, Mg, Si, S, Ar, Ca and Fe.

The temperatures of the two components were found in the ranges  MK and  MK, and the hot-to-cool emission measure ratios range between and 4. Average temperatures are in the range  MK, with the classical T Tauri stars being slightly hotter than the WTTSs.

The spread of the 20 abundance values for each element (Fig. 3) is more or less compatible with the errors obtained from the simulations; a posteriori tests, also based on simulations, have shown that our results are consistent with these TMC stars sharing a unique set of abundances, with the possible exception of iron.

The main conclusions from the present work are summarized as follows.

Hot coronal plasma is responsible for most of the X-ray emission from both CTTSs and WTTSs studied here. The coronal plasma has similar properties in the two classes of T Tauri stars, in particular similar characteristic temperatures and chemical composition. Late-type stars therefore develop hot coronae early in their life (within  Myr), whose properties change little during the following pre-main sequence evolution, at least up to an age of  Myr. The reason why the coronal emission appears suppressed in some CTTSs, such as TW Hydrae, and not in most of the others is to be clarified with future work.

The available data do not allow us to evaluate quantitatively the presence, in the CTTSs considered here, of a cool X-ray emission excess that might be present due to shock-heating.

The iron abundance is significantly subsolar ( times the solar photospheric value) in all the sample stars. Since the abundance of this element is the best-constrained one, this result is rather robust and confirms previous finding for PMS and active stars.

We found indication of coronae in G-type and early K-type stars hotter than in stars with later spectral type. We also find strong support for a bi-modality of the Fe abundance (and the Ne/Fe ratio), depending on the spectral type (or perhaps on the average temperature), with higher Fe values and lower Ne/Fe ratios for G-type and early K-type stars compared to stars of later spectral type. The latter result supports the findings from high-resolution spectroscopy by Telleschi et al. (2007). A larger sample is needed, however, to find out if this trend is merely the result of the limited statistics presently available.

The analysis of the abundance distributions of this sample of bright TMC members did not reveal any significant difference in the abundances related to the presence of accretion/circumstellar material. Ne/Fe abundance ratios between 2 and 9 times the solar value are found both for the classical and the weak-lined T Tauri stars, confirming the findings by Telleschi et al. (2007) based on a smaller sample of high-resolution X-ray spectra of T Tauri stars. Regarding the Ne/O ratio, we do not observe in the classical T Tauri stars a behaviour analogous to that of TW Hydrae, all values being below .

Acknowledgements.
We acknowledge financial support by the International Space Science Institute (ISSI) in Bern to the XMM-Newton XEST team. The Palermo group acknowledges financial contribution from contract ASI-INAF I/023/05/0. X-ray astronomy research at PSI has been supported by the Swiss National Science Foundation (grants 20-66875.01 and 20-109255/1). This research is based on observations obtained with XMM-Newton, an ESA science mission with instruments and contributions directly funded by ESA member states and the USA (NASA).

Appendix A Simulations

In this section we describe the simulations we run before fitting the real data in order to assess the performances of the PN regarding abundance determinations. This part of the investigation can be summarized as follows:

  1. Fourteen input coronal models were chosen, each consisting of an EM distribution and a set of elemental abundances, plus interstellar absorption.

  2. Three different numbers of source counts were considered:  5 000, 10 000 and 20 000 counts in the  keV band of the PN spectrum. This choice is motivated by the fact that most of the brightest TMC members have total PN counts within the above range; moreover, previous fittings of Taurus members with less than 5000 counts in the PN, using 2-T models with a fixed set of abundances (Güdel et al. 2007) already provided good descriptions of the PN spectra, a result which implies no need to treat the abundances as free parameters.

  3. For each simulated observation, i.e. for each coronal model at each number of total counts, 1000 PN spectra were simulated (using the standard PN response function and assuming no background contamination) which have a Poissonian distribution of the total number of counts.

  4. For each simulated observation, the 1000 PN spectra were fitted with an automatic routine, using a 2-T coronal model with the following starting values for the fitting parameters: abundances and equal to the values of the input coronal model, and given by the results of interactive fittings of a few simulated spectra for each of the fourteen input models.

Moreover, for the input models 1 and 2 (see Table 4 below) the fitting of simulated spectra was repeated for each of the three values of the total counts, starting from different initial values of and temperatures, and initial abundances equal to the solar values: for each of these 6 simulations, 300 spectra were automatically fitted by performing an extensive exploration of the , and space so as to simulate the approach to real data. The results obtained in this way are practically undistinguishable from those derived with the procedure described in item #4 above. For the input models 9 and 10, non-solar abundances as starting values for the fitting of simulated spectra were also used. Again, the results in these cases are very similar to those obtained with the procedure in item #4.

Note that using the same instrumental response both to simulate and to fit the spectra implies that this investigation leads to estimate the errors in the determination of the plasma parameters due to the photon counting statistics and to the instrument spectral resolution. The method cannot provide estimates of possible systematic errors due to uncertainties in the instrumental calibration and in the atomic parameters used to calculate theoretical plasma emissivities.

The input coronal models were chosen so as to explore characteristic absorption values and physical conditions of the coronal plasma (in terms of EMD and abundances), among those commonly found in the literature for active T Tauri stars. For the abundances, some extreme cases were also explored (see below). The emission measure distributions we have considered for these simulations are defined in the temperature range as:

(1)

Based on EMD reconstructions with high-resolution spectra of intermediate- and high-activity stars by Laming & Drake (1999); Argiroffi et al. (2004); Scelsi et al. (2005); Argiroffi et al. (2005); Telleschi et al. (2005); Güdel et al. (2007), we chose the values of and in the range and , respectively, while two values of were explored ( K and  K). Four sets of abundances were adopted: (i) the abundance set used by Güdel et al. (2007) to fit the spectra of known TMC members (hereafter “TMC set”): with respect to the solar photospheric values by Anders & Grevesse (1989), the abundances of this set are: C=0.45, N=0.788, O=0.426, Ne=0.832, Mg=0.263, Al=0.5, Si=0.309, S=0.417, Ar=0.55, Ca=0.195, Fe=0.195, Ni=0.195; (ii) all abundances equal to 0.2 times the solar photospheric values of Anders & Grevesse (1989); (iii) solar photospheric values for all abundances, except for iron ( solar); (iv) the “TMC set”, except for iron ( solar). We finally considered two absorption levels: “low” absorption with  cm, and “high” absorption with  cm. The fourteen input models are listed in Table 4.

Model Abundances Absorption
1 7 3 2 TMC low
2 7 3 2 TMC high
3 7 5 2 TMC low
4 7 5 2 TMC high
5 7 2 1 TMC low
6 7 2 1 TMC high
7 7 3 2 0.2 solar low
8 7 3 2 0.2 solar high
9 7 3 2 solar (Fe=0.2 solar) low
10 7 3 2 solar (Fe=0.2 solar) high
11 7 3 2 TMC (Fe=0.5 solar) low
12 7 3 2 TMC (Fe=0.5 solar) high
13 6.7 2 1 TMC low
14 6.7 2 1 TMC high
Table 4: Input models for simulations. “TMC” is the abundance set used by Güdel et al. (2007) (see text). “Low” and “high” absorption mean  cm and  cm, respectively.

The two-temperature thermal models used to fit the simulated spectra are based on the APEC emissivity code and have the following 13 free parameters: the interstellar hydrogen column density (), the temperature and emission measure of each plasma component, and the abundances of O, Ne, Fe, Mg, Si, S, Ar, Ca. We fixed the abundances of C, N and Ni to the respective values in the TMC set, because they are generally not well-constrained from PN fitting; in fact, the C and N lines fall at low energies where the PN resolution is quite poor (and moreover the PN calibration is probably uncertain), while the Ni lines are blended with the (usually) stronger iron and neon lines.

As representative examples of the results of all simulations, we report in Fig. 11 those obtained for the abundances in terms of medians of the distributions of the 1000 best-fit values, and error bars corresponding to the central 90% of the distributions, for ten different cases illustrating the effects of different input models, statistics, absorptions and choice of starting abundance values for the fittings.

Figure 11: Medians (diamonds) and central 90% of the distributions of the abundances found from eight sample simulations, for different models and/or statistics. The input values of abundances are shown as squares. The input EMDs are equal in models 1, 2, 7 and 9, with . The EMD of model 3 is steeper, while the EMD of model 5 is flatter. The EMD of model 13 peaks at . The input models have low absorption, with the exception of model 2. The two bottom panels show the results obtained when the starting abundances for the fitting are different from the “input value” of the relevant model.

The results indicated that, for all the cases analyzed here, the derived abundances are generally in good agreement with the values of the input models. The medians of the abundance distributions obtained from fitting simulated spectra are, for all elements, compatible with the input value within 90% statistical errors, and within the 68% errors in the great majority of the cases. Some systematic effects must be noted in a few cases: Ne results overestimated by a factor in models 7 and 11, while Fe and O are underestimated by about the same factor in model 13.

As to the magnitude of the statistical uncertainties, errors at 90% confidence level within a factor 2.5 are obtained for most of the elements using PN spectra with 5000 counts, and within a factor 2 with 10 000 counts. Exceptions are oxygen, argon and calcium in some cases (see below). Iron is the best-determined element, constrained within a factor 1.6 when absorption is relatively low, already with spectra containing 5000 counts. For the other elements, 90% errors on the medians can be a factor 1.4 up to 3 (spectra with 10 000 counts), depending on the model.

The abundance of oxygen is very poorly constrained (even for the highest statistics) when the is of the order of  cm, as one could expect because of the strong attenuation of the spectrum at low energies ( keV; recall that the strongest lines of the He–like and H–like ions of oxygen lie at  keV). Regarding argon, its abundance can be better constrained in the case of high absorption; this can be easily understood by noting that, for fixed number of total counts, a larger fraction of all the spectral counts goes in the Ar lines ( keV) when the low-energy region of the spectrum is strongly suppressed by the interstellar absorption. Instead, although the strongest Ca lines fall at  keV, i.e. close to the Ar lines in the high-energy tail of the spectrum, the abundance of this element is generally ill-constrained, unless the abundance is of the order of the solar value, or higher, and the statistics are high. Since the PN effective area is about the same at  keV and  keV, the difference with the case of Ar is likely due to the lower emissivity of the calcium lines, compared to those of the Ar lines.

It is important to note also that the results of the simulations are practically the same, in terms both of magnitude of the errors and agreement between medians of the abundance distributions and input values, regardless of the starting abundance values used to fit the spectra.

Finally, note that the simulations described in this section assumed no background contamination, which may not be negligible at the highest energies. For the bright stars discussed in this paper, we verified that only in a couple of cases the background spectrum dominates over the source spectrum in the energy range  keV, which was therefore excluded from the fitting. To investigate the effect of the exclusion of the Fe xxv 6.7 keV complex on the ability to constrain the iron abundance and the other parameters of the model, we repeated the simulations for the models 1 and 2 by fitting the simulated spectra in the energy range  keV. The results obtained in these cases are very similar to those obtained employing a larger spectral range.

Footnotes

  1. offprints: L. Scelsi,
  2. The field L1495 around V410 Tau was observed twice; the two observations are labelled XEST-23 and XEST-24.
  3. The value Ne/O found in this study for BP Tauri is in good agreement with that obtained by Robrade & Schmitt (2006).

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