F.-J. Zickgraf 1 - J. Krautter 2 - S. Reffert 3 - J. M. Alcalá 4 - R. Mujica 5 - E. Covino4 - M. F. Sterzik 6
1 - Hamburger Sternwarte, Gojenbergsweg 112, 21029 Hamburg, Germany
2 - Landessternwarte Königstuhl, 69117 Heidelberg, Germany
3 - Sterrewacht Leiden, PO Box 9513, 2300 RA Leiden, The Netherlands
4 - Osservatorio Astronomico di Capodimonte, via Moiariello 16, 80131 Napoli,
Italy
5 - Instituto Nacional de Astrofisica, Optica y Electronica,
A. Postal 51 y 216 Z.P., 72000 Puebla, Mexico
6 - European Southern Observatory, Alonso de Cordova 3107, Santiago 19, Chile
Received 16 August 2004 / Accepted 3 December 2004
Abstract
We present results of an investigation of the X-ray properties, age distribution, and
kinematical characteristics of a high-galactic
latitude sample of late-type field stars selected from
the ROSAT All-Sky Survey (RASS). The sample comprises 254 RASS sources
with optical counterparts of spectral types F to M distributed over six study areas
located at
,
and
.
A detailed study was carried out for
the subsample of
200 G, K, and M stars. Lithium abundances
were determined for 179 G-M stars. Radial velocities were measured for
most of the 141 G and K type stars of the sample.
Combined with proper motions these data were used to study the age
distribution and the kinematical properties of the sample.
Based on the lithium abundances half of the G-K stars were
found to be younger than the Hyades (660 Myr). About 25% are
comparable in age to the Pleiades (100 Myr). A small
subsample of 10 stars is younger than the Pleiades.
They are therefore most likely pre-main sequence stars.
Kinematically the PMS and Pleiades-type stars appear to form a group
with space velocities close to the Castor moving group but
clearly distinct from the Local Association.
Key words: surveys - X-rays: stars - stars: late-type - stars: pre-main sequence - stars: kinematics - solar neighbourhood
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Figure 1: Location of the six study areas in galactic coordinates. The dots show the positions of the RASS X-ray sources with stellar counterparts in the respective area. The solid and dashed curves denote the position and width, respectively, of the Gould Belt according to Guillout et al. (1998). In addition positions of several associations are shown. |
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A first discussion of the properties of the late-type stellar component was given
by Zickgraf et al. (1998) (Paper VI). A subsample of stars in study area I
located some
south of the Taurus-Auriga star forming region (SFR) was found to contain a large fraction of very young, presumably pre-main
sequence stars. In order to investigate the age distribution of the complete
sample of coronal
X-ray emitters we obtained further low, medium and/or high resolution spectroscopic observations
for most G-M stars in our sample.
The goals were to carry out a lithium survey in order to identify lithium-rich high-galactic
latitude G-M type stars and to determine precise radial velocities.
In solar-like stars the lithium abundance can be used as an age estimator. Its knowledge
therefore allows to study the age distribution of the X-ray active stellar sample. Combining the
age information with proper motions and radial velocities would thus allow to investigate a possible
age dependence of the kinematical properties of the stellar RASS sample.
This paper is structured as follows. The sample is presented in Sect. 2. Observations and data reduction are described in Sect. 3. Observational results are presented in Sect. 4. Based on these results the sample properties are analysed and discussed in Sect. 5. Finally, conclusions are given in Sect. 6.
Table 1: Journal of observations.
For the spectroscopic follow-up investigation we selected the 200 X-ray sources from the catalogue with stellar counterparts of spectral types G to M. F stars were not included in the spectroscopic follow-up observations because for these stars the lithium abundance is not a good age estimator. In 19 cases two stars have been assigned as counterpart to the X-ray source in Paper III. Several of these secondary counterparts were also observed. As in Paper IV we will however only use the primary identifications for statistical purposes. The entire "coronal'' sample including the F type stars comprises 253 X-ray sources. The known RS CVn star HR 1099 (=V 711 Tau) which is X-ray source A031 in Paper III was excluded from the coronal sample discussed in the following. The sample finally selected for spectroscopic follow-up observations thus comprised 199 of the 200 X-ray sources with optical counterparts of spectral type G to M as listed in Paper III.
Infrared photometry in J, H, and K was taken from the Two Micron All Sky Survey
(2MASS) catalogue. From this data base infrared sources within 10
around the optical
position of the counterpart were extracted. A total of 267 2MASS sources was found of which 90% were located within 2
from the optical counterparts (including the 19 double
identifications, see above). We considered the 258 matches within 4
,
i.e. within
as reliable identifications. Matches between 4
and 10
were
individually checked and all found to be also correct. This means that for all but 5 RASS
sources (A035, A045, A065, D022, and D114) 2MASS measurements are available.
Table 2: Revised and original statistics of the distribution of spectral type among the RASS sources with stellar counterparts of spectral types F to M.
The spectra were reduced with the standard routines of the ESO-MIDAS software package. The low- and medium-resolution spectra and the high-resolution spectra observed with AURELIE were reduced with the Longslit package. For the FOCES and CASPEC data the routines of the Echelle package were applied.
Spectra could be secured for the counterpart of 172 out of 199 RASS sources with spectral types between G and M. High resolution observations were obtained for 118 of the 141 G and K stars of the selected sample (originally 143 G-K stars minus A031 and E020). Lithium equivalent widths and radial velocities for six of the stars not observed by us with high resolution were adopted from high-resolution spectroscopic studies by Wichmann et al. (2001) (5 stars: A154, B049, B194, C062, C197) and Neuhäuser et al. (1995) (1 star: A058). Ten G-K stars fainter than 12th magnitude were observed only with low resolution. Thus for 134 of the 141 G-K stars spectroscopic follow-up observations exist. For the remaining 7 stars no observations could be obtained. Further high resolution data were found for the secondary counterpart of A098 in Favata et al. (1997). With a few exceptions M stars were observed with low resolution only. Due to bad weather conditions during the OHP observing campaign the M stars in area V could not be observed. In total 38 M stars were observed with low resolution and 7 with high resolution. For 13 M stars no observations could be obtained.
In the following we give more technical details of the spectroscopic observations.
A few stars were observed in May 1998 with the focal reducer camera DFOSC attached to the
Danish 1.54 m telescope at ESO, La Silla. The spectra were obtained with grism No. 7
and a slit width of 1
.
The wavelength range covered by the spectra was 3840-6845 Å.
As detector the LORAL/LESSER CCD# C1W7 with a pixel size of 15
m was used.
The resulting spectral resolving power was 1300.
In October 1998 high-resolution spectra were obtained with the spectrograph AURELIE at the
1.52 m telescope of the OHP. A description of the spectrograph can be found in Gillet
et al. (1994). The spectra were observed with grating No. 2
with 1200 lines mm-1 giving a reciprocal linear dispersion of 8 Å mm-1.
The detector was a double-barrette Thomson TH7832 (2048 pixel with
13 m pixel size). The spectra cover the wavelength interval from
6540 Å to 6740 Å. The resolution of the spectra is 20 000. Wavelength
calibration was obtained with Neon and Argon lamps.
High-resolution spectra of 3 objects were obtained with the Cassegrain Echelle Spectrograph (CASPEC) at the ESO 3.6 m telescope on La Silla in February 1998. Wavelength calibration was obtained with a ThAr lamp. The CASPEC spectra cover the spectral range from 5350 to 7720 Å with a nominal resolving power of 22 000 (Sterzik et al. 1999).
During each high-resolution observing campaign radial and rotational velocity standard stars were observed in addition to the science targets.
During the observing runs a small set of spectroscopic standard stars, mainly of
luminosity class V, had been observed together with the science targets. The coverage of the spectral type -
luminosity class plane, however, was insufficient for a detailed two-dimensional classification. We
therefore extended the spectroscopic data base for the standard stars by making use of
the spectra available in the stellar
library of Prugniel & Soubiran
(2001) which is part of the HYPERCAT
data base.
We used the data set with a spectral resolution of 10 000. In
order to match this resolution our FOCES, AURELIE, and CASPEC spectra were smoothed
accordingly with an appropriate Gaussian filter. In this way the
signal-to-noise ratio improved while the necessary spectral resolution for the classification
was preserved. Spectral types and luminosity classes (LCs) of MK standard stars contained in
the stellar library were adopted from
Yamashita et al. (1976), Keenan & McNeil (1989),
Garcia (1989), Keenan & Barnbaum (1999), and
Gray et al. (2001). In a few cases we adopted the spectral classification
given in Prugniel & Soubiran (2001). The grid of spectroscopic
standard stars is listed in Table 3.
In a pilot study for the work presented here Ziegler (1993) studied the spectral
types of F, G and K-type stars from the RASS using spectra observed in the red spectral
region (
6200-6750 Å). He found various line ratios useful for
classification purposes. For the F- and G-type stars the
ratios Fe I
6394/Si II
6346, Fe II
6456/Ca I
6450 and
Fe II
6456/ Fe I
6394 were found
to be good indicators for the spectral type. In K stars the ratios TiO
6240 / V I
6296
and Fe I
6250/Ca I
6450 were useful classification criteria.
Table 3: Spectroscopic MK standard stars. The spectral types are listed in column "sp. type''. References for the spectral types are given in column "ref.'': 1 = Yamashita et al. (1976), 2 = Gray et al. (2001), 3 = Keenan & Barnbaum (1999), 4 = Garcia (1989), 5 = Keenan & McNeil (1989), 6 = Prugniel & Soubiran (2001).
We used these ratios for the refinement of the spectral types given in Paper III.
Figure 2 shows the histogram of the differences between the revised and
original spectral types. The narrow peak shows that with few
exceptions the overall agreement is good. We found a small mean difference
of -0.5 subclass between the high- and low-resolution spectral types with
a standard deviation of 2.2 subclasses. The original and the revised statistics of
spectral types are listed in Table 2. In nine cases the difference of the spectral
types was larger than 3 subclasses. The largest differences were found for B174 and E256
(-6 subclasses), B185 (7 subclasses), D018 (9 subclasses), and E022 and E067 (-9 subclasses).
The LFOSC spectrum of E256 was actually classified as K4,
but erroneously entered in Paper III as M0. For D018 which is a very bright star the original
LFOSC spectrum classified as G2V could suffer from saturation. In SIMBAD this star is listed
as K0III
(Schild 1973).
The classification based on the FOCES spectrum is K1III, which is in good agreement
with the literature. We adopt this spectral class in the following. For the remaining stars with large
deviations no LFOSC classification spectra were obtained. The spectral classes were adopted
from SIMBAD. In the following we use the improved FOCES classifications.
Following Gahm & Hultqvist (1972) and Ziegler (1993)
luminosity classes (LC) were obtained using the strength of the lines of
Ba II
5854 Å, 6497 Å, Sc II
6605 Å, and
La II
6390 Å. We added the Y II
6614 Å line which also shows a clear
luminosity dependence.
The ratio of Sc II
6605 Å and Y II
6614 Å is a good
luminosity indicator for spectral types earlier than about K5-7. For spectral types
later than K0 the
strength of La II was additionally useful to discriminate luminosity classes III and
higher from LC V and IV. For G stars LC III and higher could also be discriminated
from LC IV by the use of this line.
Comparing in this way the line strengths and ratios in the MK standards
with the sample stars LCs could be assigned to most stars. For a few stars the stellar
absorption lines were strongly broadened by rapid rotation (see below). In these cases it
was not possible to determine the luminosity class due to the
limited S/N of the spectra and to line blending. The limit was reached around
km s-1. For the rapid rotators we adopted LC V. As discussed in
Sect. 5.1.1 we used the luminosity classes to derive spectroscopic
parallaxes.
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Figure 2: Comparison of the spectral types derived from the classification spectra used in Paper III (Sp(old)) and from the new high resolution spectra (Sp(rev.)). The abscissa is the difference (in spectral classes) between the revised and the original spectral types. |
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The width of the cross-correlation function is a measure for the rotational
velocity .
We therefore calculated the cross-correlation function as
before but for rotational velocity standards.
Standard stars with low
and spectral type as
close as possible to that of the objects were used for the cross-correlation analysis
as well as to calibrate the FWHM vs.
relation. From the FWHM of the
cross-correlation function
was then determined following the method described
in Covino et al. (1997).
Observations of rotational standard stars yielded a detection limit of
of
about 5 km s-1. From the statistics of the differences between
measured rotational velocities of rotational standard stars and
from the
literature an uncertainty of
of 3 km s-1 could be estimated.
For rotational velocities above
40 km s-1 the shape of the peak of the
correlation function deviates increasingly from a Gaussian leading to larger
errors of 5-10 km s-1.
Figure 3 shows the histogram of the rotational velocities which
are listed in Table A.2.
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Figure 3: Distribution of rotational velocities of the G and K stars. |
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In the high-resolution spectra the equivalent widths were measured directly by integrating the
flux in the normalized spectra. The contribution of the neutral iron line
Fe I
Å was corrected according to the procedure described by Soderblom
et al. (1993b). For stars with rotational velocities
larger than
30 km s-1 the contribution of the Fe I lines near Li I
was
corrected in the following way.
From the stellar library of Prugniel & Soubiran a spectroscopic standard star
with a spectral type as close as possible to the target was selected. It was folded
with the appropriate rotational velocity to match the broadened lines of the target
spectrum. Then the EW of the Fe I absorption features was measured
in the same wavelength interval as used to determine the Li I EW in the
target spectrum. Finally the corrected lithium EW was obtained by subtracting
the contribution of the Fe I lines from the measured
lithium EW of the target spectrum.
Errors of the high-resolution EWs are typically 5-15 mÅ,
depending on the
signal-to-noise ratio and on the rotational velocity.
The EWs are listed in Table A.4.
In Fig. 4 the EWs obtained from the low- and
the high-resolution spectra are compared. In the low-resolution spectra the
EWs W(Li I ) are obviously slightly underestimated by about 40 mÅ. However,
the overall agreement is good
and the differences are only of the order the uncertainty of the low-resolution measurements.
This demonstrates that the fitting method applied to the low-resolution spectra works
remarkably well. In particular, W(Li I ) is not overestimated as it would be the case
if the EWs would be determined directly by flux integration without taking the contribution
of the Fe I lines into account.
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Figure 4: Comparison of the equivalent widths of Li I determined from the low- and the high-resolution spectra. The dashed line denotes a ratio of 1 of the two measurements. |
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In a few binaries lithium lines could be identified in one or both components. In order to
disentangle the lines of the individual components and to identify a possible Li I line
spectra from the Prugniel & Soubiran
sample with the appropriate spectral types were folded with the rotational profile for the
measured
and shifted with respect to the measured radial velocities. Then
the spectra were superimposed by using appropriate values for the relative flux contributions.
Finally the resulting artificial binary spectrum was compared with the observed spectrum.
Correction factors for the measured lithium equivalent widths were estimated from the artifical
spectrum. In most cases the spectra suggest a flux ratio of 1 to 2 for the individual
components at 6708 Å.
Exceptions are e.g. A001 and A071. In A001 the primary component is a fast rotator (
km s-1) whose broad lines dominate the spectrum.
Of the secondary component only the strongest lines of a mid to late type K star are detectable.
For this binary system we adopted a flux ratio of 5:1 for the continuum contributions of the primary and
secondary component at 6708 Å. In A071 both components are fast rotators with very broad lines.
In this case it was not possible to determine a lithium EW for each component.
The total EW was therefore assigned in equal shares to the individual components and
the lithium equivalent widths were corrected by assuming equal flux
contributions.
The triple system B160 is even more complicated. It consists of 3 early to mid G-type stars with
spectral types between
G2 and
G5.
Two of the three components exhibit a lithium absorption line.
It is clear that the equivalent widths of the binaries and the triple system are less reliable than those of the single stars due to the uncertainty of the continuum correction. In Table A.4 the lithium EW of the strongest component is given.
For 74 stars a spectroscopic parallax could be derived from the high-resolution spectra
by adopting the absolute V magnitudes, as appropriate for the spectroscopically
determined luminosity class, from Schmidt-Kaler (1982).
For the bulk of M stars we used infrared JHK measurements from the 2MASS catalogue
to derive a photometric distance. The two-colour diagram of J-H and H-K is displayed
in Fig. 5. It shows that the M stars
are distributed around the locus of main-sequence stars (solid line in
Fig. 5). For the further analysis distances of M stars
were therefore estimated by adopting MV for LC V from Schmidt-Kaler
(except for the 11 stars with trigonometric parallaxes).
This adds 43 more RASS sources with a distance estimate.
Thus total distances are available for 100 G-K and 54 M stars.
For the remaining
stars without a distance measurement we derived a lower limit for the
distance by assuming that they are main-sequence objects with LC V.
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Figure 5: Two-colour diagram for the infrared magnitudes from 2MASS. Circles denote M stars, crosses stars with spectral types F to K. The solid, dotted, and dashed lines denote the loci of main sequence stars, giants, and supergiants, respectively. |
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An estimate of the error of the spectroscopic and photometric distances,
,
may be obtained
from the following considerations. The error is due to the uncertainties of the absolute
visual magnitude, MV, and of V. For the latter we conservatively adopted the error of the
photographic GSC magnitudes
for all stars. The dominating source of
uncertainty is the error of MV. For G-K stars of LC V and IV and
correspondingly for LC III and II we used half of the
difference of MV of these luminosity classes as estimate for
.
This leads to an estimate for
of 30-50%. In the case of M stars the main
source of error of MV is due to the uncertainty of the spectral class. This also leads
in total to
% if an uncertainty of 1-2 spectral subclasses is
assumed. We finally adopted 50% as relative error for spectroscopic and
photometric distances.
For the derivation of the distances interstellar extinction was
not taken into account. Given the high galactic latitude of our sample it is
actually expected to be small. With the relation
given by Spitzer (1978) with the column
density of neutral hydrogen,
,
and colour excess E(B-V) upper limits of the
extinction can be estimated. We expect extinction
values,
,
of less than 0.2-0.3 in all study areas except area I. This region
could have a higher extinction of up to 0.6 magnitudes for the most distant stars.
For these estimates the
values given in Paper II were used.
For 20 stars in our sample both spectroscopic and Hipparcos parallaxes,
,
exist. They are compared in Fig. 6.
The agreement of the two distance measurements
for this subsample is good. The mean ratio of both parallaxes is
.
For the further analysis we adopted the spectroscopic parallaxes if no Hipparcos
parallax with
or other trigonometric
parallax was available. The adopted distances are listed in
Table A.2.
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Figure 6:
Comparison of the distances
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Figure 7 shows the number distribution of the distances for the 184 F-, G-, and M stars. Also shown is the distribution including the stars with minimum distances estimated by adopting LC V. The number distribution of the total sample has a maximum around 50 pc with a tail extending up to several 100 pc. Most stars are nearer than 200 pc, 33 stars have distances above 300 pc (including 16 stars with minimum distances), and in 4 cases (not shown in Fig. 7) we derived a distance above 1 kpc (including 3 stars with minimum distances). The identifications of the very distant RASS counterparts may be questionable.
For the stars with trigonometric parallaxes the absolute magnitude, MV, was calculated from the distance and visual magnitude given in Table A.2. A luminosity class was then assigned according to Schmidt-Kaler (1982). Likewise, bolometric corrections were taken from the same reference to determine the bolometric magnitudes for all stars with known distances.
As expected the majority of stars with a luminosity class determination, 90%,
have luminosity class V or IV. A small number of 17 stars was classified as giants
(LC III-IV, III, and II), 12 of these based on Hipparcos parallaxes.
In Fig. 8 the H-R diagram is shown for
all stars with a spectroscopic or trigonometric parallax.
M stars are shown only if a trigonometric parallax
was available.
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Figure 7: Histogram of the distance distribution. The solid lines represent the distribution of trigonometric, spectroscopic, and photometric parallaxes. The dashed lines include distance estimates derived from assuming absolute visual magnitude of main-sequence stars for the remaining stars without other distance estimate. |
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Figure 8: H-R-diagram for single stars with either a trigonometric parallax from Hipparcos or other sources (+ sign) or with a spectroscopic parallax (triangles). |
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Figure 9:
X-ray luminosity for single stars
vs. distance. + signs mark stars in study areas I, II, III, IV, and VI,
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Figure 10:
X-ray luminosity for single stars as a function of effective
temperature,
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Figure 11: X-ray luminosity for all single stars with trigonometric (+ sign), spectroscopic (triangles), or IR photometric parallaxes (circles) as a function of absolute visual magnitude, MV. The variability range of solar X-ray emission is marked by the vertical bar. |
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In Fig. 10
is plotted versus the effective temperature and Fig. 11
shows
as function of the absolute visual magnitude, MV. A weak trend
of
increasing with increasing
is visible.
The
-MV diagram shows a clear correlation with
decreasing for decreasing optical luminosity. This reflects the fact that
depends on the emitting surface.
The width of the
-MV distribution at a given MV tells
that the X-ray surface flux density of the stars in our sample spans a range of
a factor of
1000. Around MV = 5 the lower limit of the X-ray luminosities of
the sample stars is about a factor of 10 above the solar soft X-ray variability range
(
erg s-1, Schmitt 1997). The upper limit of
in our sample is about a factor of 10-30 higher than in the volume-limited
sample of Schmitt (1997).
The ratio of
and bolometric luminosity,
,
is plotted in Fig. 12 as function of
.
A clear correlation is visible with the
low luminosity stars with later spectral types having the highest ratio of
.
This is in agreement with the results of Fleming et al. (1995) who
studied the coronal X-ray activity of low-mass stars in a volume limited sample.
They found the highest ratios of
for dMe stars.
As discussed in Paper IV, most M stars in our sample
are actually dMe stars, that is of the 58 M stars listed originally in Paper III 53
exhibit H
emission lines. Note, however, that selection effects inherent
in our flux-limited sample may also play a role.
The X-ray surface flux density is displayed as a function of MV in Fig. 13 and
as a function of
in Fig. 14. Our sample contains
mainly stars with a high surface flux density which is on the average 1 to 2 orders of
magnitude above the solar flux level. This can be understood in view of the result
discussed below in Sect. 5.2.2 that our sample contains a large
fraction of young and hence very X-ray active stars.
Old solar-like stars are obviously not present in our sample. The maximum value
of the surface flux density of our sample stars is around
108 erg s-1 cm-2. This value is consistent with the result obtained by
Schmitt (1997) who found a maximum around
107-108 erg s-1 cm-2 in his volume-limited sample of solar-like stars.
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Figure 12:
Ratio of X-ray and bolometric luminosity for all single stars with
trigonometric (+ sign), spectroscopic (triangles), or IR photometric parallaxes
(circles) as a function of bolometric magnitude,
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Figure 13: X-ray surface flux density for all single stars with trigonometric (+ sign), spectroscopic (triangles), or IR photometric parallaxes (circles) as a function of absolute visual magnitude, MV. The vertical bar marks the typical flux level of solar coronal holes in the ROSAT-PSPC pass band. |
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Figure 14:
X-ray surface flux density for all single stars
as a function of effective temperature,
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Finally, in Fig. 15 the ratio
is displayed as
function of
projected rotational velocity,
.
No clear correlation can be seen, except that small ratios of
are only found
for small
,
whereas fast rotators exhibit high
ratios.
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Figure 15:
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The lithium equivalent widths were converted to abundances, N(Li),
by using the curves of
growth of Soderblom et al. (1993b) for stars with
K
and of Pavlenko & Magazzù (1996) and Pavlenko et al.
(1995) for cooler stars. As in Paper VI effective temperatures
were derived from the spectral types using the temperature calibrations of
de Jager & Nieuwenhuijzen (1987).
The uncertainty of
is typically 200 K. This leads to errors of the estimated Li
abundances of about 0.3 dex. Lithium abundances are shown in
Fig. 17 as function of effective temperature with
indicated by the symbol size.
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Figure 16:
Equivalent widths of Li I
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Figure 17:
Lithium abundances versus effective temperature for the complete sample.
Upper limits are plotted as
downward arrows. Circles denote high-resolution measurements with the symbol size
depending on ![]() ![]() ![]() |
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In Fig. 16 the upper and lower envelopes of the
(Li I ) distributions for stars in the Pleiades and the upper
envelope for the Hyades are shown. Likewise, Fig. 17
includes the upper envelopes of the lithium
abundances of stars in the Pleiades, the UMaG, and the Hyades, and in addition
the lower envelope for the Pleiades.
Using the lithium abundance data for the mentioned clusters and moving groups we
finally defined four age groups.
The age group "PMS'' consists of stars
above the Pleiades upper envelope and is thus younger than the
Pleiades, i.e. younger than 100 Myr. The group of stars between the upper and lower
Pleiades envelopes can be assumed to have an age similar to the Pleiades. In the
Pleiades the G and K stars are supposed to have reached the ZAMS. This group with
an age of 100 Myr is therefore designated "Pl_ZAMS''.
The age group "UMa'' comprises stars between the lower Pleiades and the upper
Hyades envelope. The age of the stars of this group is between
100 and
600 Myr, i.e. on the average
300 Myr, which is the age of the UMaG.
The age group "Hya+'' comprises G-K stars with either a lithium abundance below the
upper Hyades envelope or with an upper limit for the lithium abundance only.
The latter means that this group also contains stars for which the upper limit is
above the Hyades line. Evolved stars more luminous than LC IV are included in the age
group "Hya+'' if not stated otherwise in the following. It should be noted, however,
that due to the well-known scatter of the lithium abundances in clusters stars below the
upper envelope for the corresponding age group are not necessarily older than the
respective group. Therefore, the
"Hya+'' group might actually also contain some younger stars although it certainly is
dominated by truly old stars.
In M stars older than several 106 yr lithium has been destroyed already (e.g. D'Antona & Mazzitelli
1994). With the
exception of two stars we could not detect lithium in the M stars of our sample.
This means that the M stars are typically older than 10 Myr.
We thus only defined a group "M stars'' without assigning an
age. This group does not contain the two lithium rich M stars (see below).
We will return to the M stars in Sect. 5.3.1 where we use the kinematical properties to
estimate their age.
Figure 17 shows that a small but significant
group of 12 stars exists above the Pleiades upper limit. These objects appear
thus to be younger than 100 Myr and may be even younger than or comparable to the
age of IC 2602, i.e.
30 Myr.
Two of these stars, B002 and F0140, are however giants (LC III) and are therefore
not pre-main sequence (PMS) but evolved objects.
This leaves a group of 10 stars which appears to consist of PMS
objects, i.e. true members of the age group "PMS''.
Actually, 8 of these 10 stars are found in area I which is located south of the Tau-Aur SFR.
They represent the young stellar population in this region discussed in Paper VI.
The remaining two stars are located in area II.
The subsample of the lithium-rich stars including the giants is listed in Table 5.
Their high-resolution spectra are shown in Fig. 18 except for A058.
The spectrum of this star can be found in Neuhäuser et al. (1995).
For its low-resolution spectrum
see Paper VI. The spectrum of the M4 star B026 is displayed separately
in Fig. 19.
The rotational velocities of the Li-rich stars are high on the average. Only the
giants have
below 10 km s-1. Six of the ten PMS stars have
km s-1. Table 4 lists the median
for each age
group. It shows that
decreases on the average with increasing age.
Table 4:
Median
(in km s-1) for the different age groups. Giants
were not included in group Hya+.
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Figure 18:
Spectra of the lithium-rich sample listed in Table 5. The wavelengths of
Li I
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Figure 19:
Low-resolution spectrum of the M4 star B026. The dashed lines indicate
Li I
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Table 5:
Spectral types, lithium equivalent widths, EW(Li),
logarithmic abundances, (Li), and projected rotational velocities for
the subsample of stars with lithium abundance above the Pleiades upper envelope.
("PMS'' sample). Evolved
lithium-rich stars not belonging to the PMS sample are marked by the "
'' symbol.
Table 6:
Spectral types, lithium equivalent widths, EW(Li),
logarithmic abundances, (Li), and projected rotational velocities for
the subsample of stars with lithium abundance between the Pleiades lower and
upper envelope ("Pl_ZAMS'' sample). Lithium-rich evolved stars not belonging to the
Pl_ZAMS sample are marked by "
''.
The majority of stars has EWs and lithium abundances below the Pleiades
upper limits of EW and (Li), respectively. In the region between
the upper and lower envelope of the Pleiades 43 G-K stars are found.
This group is listed in Table 6. Three of these stars
are giants with LC IV-III, III, and II.
The 40 non-giants appear to constitute a population with an age similar to the
Pleiades, i.e.
100 Myr.
The region between the Hyades upper and the Pleiades lower envelope
contains 23 stars of which 4 are evolved objects.
The UMa age group with an age of
300 Myr thus consists of 19 stars.
Below the upper limit of the Hyades 57 non-giant stars are found and are
thus assigned an age of older than
600-700 Myr. Adding the 17 evolved
G-K stars which are certainly also older than
1 Gyr results in a total
of 74 stars for age group "Hya+''.
Thus lithium abundances and luminosity classification suggest that 47% of all G-K stars
in the sample have an age of less than about 600-700 Myr.
Restricting these statistical considerations to the later spectral types
increases the fraction of stars younger than the Hyades. Of the 114 G5-K9 stars 55,
i.e.
50%, have a lithium abundance higher than the
Hyades. With the above mentioned ambiguity of the age group definition
this means that at least half of the G5-K9 stars are
younger than the Hyades. Some statistics of the age distribution of our sample
stars for these age groups is summarized in Table 7.
As expected area IV located near the north galactic pole has
the lowest surface density of stars younger than the Hyades. In this area only 2 stars younger than 600-700 Myr are found in 72 deg2. This
corresponds to a surface density of
deg-2
at a RASS count-rate limit of 0.03 cts s-1.
In the other 5 areas (613.2 deg2) a total of 60 stars (including 5 stars in area V above 0.03 cts s-1) yields a surface density of
deg-2.
Counting stars of all age groups area IV has a surface density of
deg-2
compared to
deg-2in the other areas at the same count-rate limit.
A t-test shows that these differences are significant.
The very young stars of the PMS sample are apparently more abundant in area I
than in any other area: 80% of these stars are found in area I.
Adding up the numbers of stars younger than the Hyades in areas II, III, and VI
leads to an average surface density
deg-2.
This is less than half
of the value in area I which is
deg-2 .
Although indicative for a higher concentration of young stars in
area I the difference is not significant.
Table 7:
Statistics of the age distribution of the sample of G-K stars. "PMS'' denotes stars
younger than 100 Myr, "Pl_ZAMS'' stars as old as the Pleiades, "UMa'' stars
with an age of Myr, and "Hya+'' older than the Hyades. The latter age group also contains 17 evolved stars (LC IV-III, III, and II). The total number of G-K stars is 141.
Table 8: Statistics of the spatial distribution of the various age groups in the sample. For each age group the total number of stars and the number per square degree is given. The numbers are for a RASS count-rate limit of 0.03 cts s-1except for area V which has a count-rate limit of 0.01 cts s-1.
We compared the observed cumulative number distribution,
,
of our sample with model predictions by Guillout et al. (1996).
The median latitude for the combined areas I, II, III, V, and VI, which are distributed
between galactic latitudes of 20
and 50
,
is actually
,
thus matching this model
parameter well. The models of Guillout et al. (1996) give cumulative surface
densities,
,
as a function of ROSAT-PSPC count rate, S, for three age bins: age younger
then 150 Myr, age between 150 Myr and 1 Gyr, and older than 1 Gyr. We restricted
the comparison to the youngest model age bin and to the sum
of all model age bins because of the difficulty to separate observationally
stars with ages of several 100 Myr to
1 Gyr and older.
We further considered the combined sample of G and K stars. M stars were not included
because of the lack of an observational age determination for stars of this spectral type in
our sample.
The uncertainty of the ages derived observationally from lithium was taken into account by forming two
observational age samples matching as closely as possible the youngest age bin of
the models: a) a sample comprising the sum of G-K stars from the PMS and Pl_ZAMS age
group, and b) a sample containing in addition the corresponding UMa stars. The true
sample of stars younger than 150 Myr is expected to lie between these limits.
The result of the comparison of
is depicted in
Fig. 20 for three RASS X-ray count rates of 0.1, 0.3 and 0.01 cts s-1. The predicted numbers of G-K are in good agreement
with our sample in the 5 study areas located around
in galactic latitude. This holds for both the sum of all age groups and stars younger than
150 Myr obtained as described above and represented in the figure
by the filled symbols. Likewise, the predicted flattening of
at lower count rates is also found in our data for area V which has the lowest
count rate limit of 0.01 cts s-1.
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Figure 20:
Comparison of observed co-added number densities of G and K stars, ![]() ![]() |
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Figure 21:
Proper motions for the six study areas.
The different symbols denote the different age groups: filled circles = PMS, filled
triangles = Pl_ZAMS, open circles = UMa, open triangles = Hya+, ![]() |
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Altogether, we were able to assign proper motions to the counterparts of 129 RASS sources with spectral types G to M. In detail we found 55 of 56 G stars, 61 of 86 K stars and 13 of 56 M stars in the mentioned catalogs. In addition we also found 54 F stars. An equal number of proper motions comes from Tycho-2 and UCAC2, while only two proper motions each were taken from Hipparcos and TRC, and only one each from PPM and STARNET, while the ACT was not used in the end at all.
These proper motion data were supplemented for the optically faint stars (mainly of spectral type K and M) by data from other catalogs: 53 stars from USNO-B1.0 (Monet et al. 2003, 36 M stars, 16 K stars, and 1 G star), 1 M star from Carlsberg Meridian Catalogs (1999), and 1 M star from the NPM1 Catalog of the Lick Northern Proper Motion Program (Klemola et al. 1987). Note that the USNO-B1.0 proper motions are not absolute, but relative to the Yellow Sky Catalog YS4.0 in the sense that the mean motion of objects common to USNO-B1.0 and YS4.0 was set to zero in USNO-B1.0. According to Monet et al. (2003) the difference between these relative proper motions and the true absolute ones should, however, be small.
Thus in total proper motion data are available for all G stars, for 77 of 86 K stars, and for 51 of 56 M stars.
The proper motions are shown in Fig. 21 for the individual study areas. The diagram displays proper motions for six groups of stars, i.e. the "PMS'' "Pl_ZAMS'', "UMa'' and "Hya+'' age groups, evolved stars (giants) and the M stars without lithium detection.
Of particular interest are the proper motions of the stars of the youngest age groups in area I,
i.e. the "Pl_ZAMS'' and "PMS'' samples with ages of 100 Myr and less,
This study area is located near the Tau-Aur SFR and near the Gould Belt
(see Fig. 1) and has, probably due to its
location, the highest surface density of young stars.
Proper motions exist for all eight young stars of area I listed in Table 5.
They are plotted in the upper left panel of Fig. 21.
Four of the stars of age group PMS in area I were already identified as pre-main sequence objects
by Neuhäuser et al. (1995) (A058, A069, A090, and A104). They
assigned an age of 35 Myr to these stars.
Likewise, one star of the Pl_ZAMS sample, A120, was assigned an age of 100 Myr
by Neuhäuser et al. These stars were part of a sample investigated kinematically for
membership to the Taurus-Auriga SFR by Frink et al. (1997). They
studied stars in the central region of Tau-Aur and in a region south of Tau-Aur
which partially overlaps at the southern edge with our area I.
The sample studied by
these authors contains three further stars of our sample, A007, A107, and A122, for which
Neuhäuser et al. assigned an age
of older than 100 Myr. This is in agreement with our age estimate of older
than 660 Myr for A007 and A107, and of 300 Myr for A122.
In Table 9 the mean proper motions and their dispersions are
summarized for the PMS, Pl_ZAMS, UMa, and Hya+ age groups, and for M stars
without Li I detection.
Obviously, the 8 "PMS'' stars show a smaller spread in proper motions than the older stars.
They cluster around (
,
)
of (+16,
-8) mas yr-1 with a scatter of
15 mas yr-1 in each direction.
Frink (1999)
transformed the proper motions given by Frink et al. (1997) from the FK5 to the Hipparcos system and determined mean values of
(
+8.7,-11.2) mas yr-1 for the southern sample of Frink et al. (1997).
For the central region of Tau-Aur Frink (1999) derived mean proper motions
of (
+4.5,-19.7) mas yr-1. The comparison of our results with the findings of Frink
(1999) reveals an interesting trend in the mean proper motions
relative to the core region of Tau-Aur. The southern sample of Frink et al. moves away
from the centre of Tau-Aur with a mean proper motion of (+4.2, +8.5) mas yr-1. The
PMS stars in area I are located even more to the south of the centre and their relative
mean proper motion is actually even larger, (+12, +12) mas yr-1. Thus we find that
the stars in area I move in approximately the same direction as the southern stars of
Frink et al., but with an even higher proper motion.
Inspection of Fig. 2 in Frink et al. (1997) allows to estimate a dispersion of about 15 to 20 mas yr-1 for both subsamples which again is compatible with the 15 mas yr-1 derived for our PMS subsample. The Pl_ZAMS stars exhibit a dispersion of the proper motion which is larger by a factor of 2 to 3. On the other hand, the UMa sample though being older shows more coherent proper motions with a dispersion equal to the PMS stars. The old stars of the Hya+ group and the M stars exhibit the largest dispersions. Similar results are found for the other study areas.
Table 9: Mean proper motions and dispersions in area I for stars of age groups PMS, Pl_ZAMS, UMa, and M stars without lithium detection (in mas yr-1).
So far we have considered the proper motions which depend on the distance and contain a
contribution due to the solar motion. We therefore calculated
tangential velocity components, vl and vb, in galactic coordinates, l and b, by
using the distance estimates discussed above and the relations
km s-1
and
km s-1, with
and
being proper motions in galactic coordinates given
in arcsec yr-1 and the distance d in pc.
A table summarizing the resulting velocities
and their dispersions for the individual study areas can be found in the Appendix
(Table A.1).
The direction-dependent part of the tangential velocities due to the solar reflex motion
can finally be removed by transforming these velocities to the local standard
of rest (LSR). This is achieved by adding the corresponding solar velocity components.
We used the solar motion vector of Dehnen & Binney
(1998), (,
,
) = (+10.0, +5.25, +7.17) km s-1 (see
below for the definition of the space velocities) to determine the solar reflex motion:
In Table 10 mean proper motions in galactic coordinates with respect
to the LSR,
and
,
and
the corresponding tangential velocities,
and
are listed for the different age groups. As discussed before the
M stars
exhibit the largest dispersion of the proper motions. Taking the distance effect into account the
dispersions of the respective tangential velocities are reduced to values similar to those obtained
for the Pl_ZAMS and UMa age groups. This again leads to the conclusion that the M stars have
on the average an age of
100-600 Myr. The largest velocity dispersions are found
for the Hya+ age group.
Table 10: Mean proper motions (in mas s-1), and mean tangential velocities (in km s-1) in galactic coordinates, both with dispersions, reduced to the LSR. The values are listed for stars of the age groups PMS, Pl_ZAMS, UMa and Hya+ (split into dwarfs and giants), and M stars without lithium detection.
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Figure 22: Space velocities U, V, and W in the LSR frame. Stars of age groups "PMS'' and "Pl_ZAMS'' are plotted as filled circles. Open circles denote stars of the UMa and "Hya+'' age group. Giants are plotted as asterisks. |
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Figure 23: Upper panel: U-V velocity diagram for the youngest age groups "PMS'' (circles) and "Pl_ZAMS'' (triangles). The solid line encircles the region defined by Eggen (1984, 1989) to contain the young disk population. Also shown as large crossed circles are the U and V velocities of the Hyades supercluster, the Local Association (designated "local''), the Castor MG, and the UMa MG. Lower panel: W-V diagram for the same sample of stars. All velocities are in the LSR reference frame. |
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The space velocities components are plotted in Fig. 22. The plot contains stars of all age groups and also includes the evolved stars (giants). Figure 23 shows in an enlarged scale the V-U, and V-W diagrams for the two youngest stellar age groups only, i.e. PMS and Pl_ZAMS stars.
As can be seen in Fig. 22 the filled symbols representing the youngest age
groups, PMS and Pl_ZAMS, are more concentrated than the open symbols
and the asterisks denoting the older age groups and giants, respectively.
This can be tested by various statistical methods.
First, we combined on one hand
the PMS and Pl_ZAMS samples and on the other hand the older stars and giants
in order to create distributions of the space velocity
for the young and the old stars,
respectively.
A one-dimensional two-sample Kolmogorov-Smirnov (K-S) test on these
distributions yields a probability of <
that they are drawn from the same parent distribution.
Likewise, the K-S test on the PMS and the complementary non-PMS sample yields
a probability of only
for having the same distribution.
Therefore, PMS and non-PMS stars also have different space velocity distributions.
Contrary to this, with a probability of 0.31 PMS and Pl_ZAMS stars have
the same distribution.
An F-test on the individual velocity components U, V, and W of
the combined PMS-Pl_ZAMS and the
older age groups shows that with a very low probability P their
distributions are drawn from the same parent distribution, namely
PU = 0.006, PV= 0.02, and
.
In particular, the velocity
component perpendicular to the galactic plane, W, is significantly different
in the young and the old age groups (see below).
In the following we will discuss mean velocities and velocity dispersions of the
different age groups.
These were calculated
as maximum-likelihood (M-L)
estimate
which takes into account that the measurement errors are
different for each star.
Following Pryor & Meylan (1993) M-L estimates of the mean
velocity components
and dispersions
of U, V and W
were obtained together with errors by assuming that the velocities are drawn from
a normal distribution
In Table 11 the mean space velocities and velocity dispersions
of the different age groups
are summarized. Clearly the PMS sample has the smallest velocity dispersions.
For stars with weak or no lithium detection the dispersions are the largest. The
"Hya+'' subsample contains a significant fraction of older disk stars. This is
particularly evident for the velocity component perpendicular to the
galactic plane, W.
Its dispersion increases from 2 km s-1 for the PMS sample to
30 km s-1
for the old lithium weak sample. The increasing velocity dispersion with increasing
age reflects the effect of disk heating in the galaxy.
The PMS subsample in particular exhibits M-L mean space velocity components
km s-1 and
velocity dispersions of (
) km s-1. This suggests that the PMS stars are kinematically related and
may even form a kinematical group, but of course, the sample is small and the
indicated relation should be considered more as a working hypothesis to be tested with
extended samples.
At this point it should be noted that the
PMS star B206 in area II interestingly has space velocity components similar
to the stars in area I.
Unfortunately, no high resolution RV measurement is available for the second
PMS star in area II, the M4Ve dwarf B026. In order to obtain at least an estimate of its
space velocity components we measured the radial velocity using the low-resolution CAFOS
spectra and the emission lines of H
,
H
,
H
,
and Ca II K. This
yielded
km s-1 with an error of about 20 km s-1.
The resulting space velocity components are
km s-1,
km s-1, and
km s-1.
Within the errors the velocities of B026 are consistent with the
mean velocities of the PMS sample. But clearly, a more accurate RV measurement is needed
for B026 to confirm that both Li-rich stars in area II belong
to the same kinematical group as the corresponding stars in area I as indicated
by the presently available data.
Note also from Fig. A.1 that in areas I and II the numbers of Li-rich stars are higher
than in the other areas.
Enlarged sections of the U-V and W-V diagram are shown in Fig. 23 for the 35 stars of the two youngest age groups with measured space velocities. The U-V diagram in the upper panel includes the limits of the region occupied by the young disk stars as defined by Eggen (1984, 1989). Indeed, as expected for a young stellar sample many, albeit not all, stars have (U,V) velocities inside Eggen's box. Also indicated are the (U,V) velocities of several young stellar kinematical groups: the Hyades supercluster, the Ursa Major moving group (UMa MG), the Local Association (Pleiades MG), and the Castor moving group (Castor MG) (for references see e.g. Montes et al. 2001).
Table 11:
Mean (M-L) space velocity components,
,
and velocity dispersions,
,
,
,
of the different age groups in km s-1.
Figure 23 suggests the existence of a kinematical subgroup in the
combined PMS and Pl_ZAMS sample, which contains 35 stars with measured
U, V, and W velocities. The group is concentrated near
the velocity of the Castor MG at the upper V limit of Eggen's disk stars with 17 of the 35 stars found within a radius of 10 km s-1 around the velocity
of the Castor MG.
Six of these belong to the age group PMS and the rest to the Pl_ZAMS group.
The M-L mean velocities of the subgroup are
km s-1, and the velocity
dispersions are
km s-1.
In V the group of 17 stars is
somewhat off the Castor MG for which Palous & Piskunov (1985)
give (
km s-1.
Given the relatively small number of data points we may ask whether this
concentration is due to a chance coincidence in an actually random distribution.
We tested this possibility for the null
hypothesis that the true underlying distribution of
velocities in the U-V plane is random within a given circle around
the origin. In a Monte Carlo simulation we calculated a large number of random
velocity vectors in the U-V plane and counted the number of cases in which
we found 17 stars within
10 km s-1 around the Castor MG velocity. For a random velocity distribution within
a radius of 35 km s-1 containing 90% of the 35 stars, i.e. 31 stars,
these simulations showed that we can reject the null hypothesis on a
high significance level of >99.8%. The test radius of 35 km s-1 may be
too small because it excludes 10% of the stars. Increasing the radius
leads however to even higher significance levels. Decreasing the radius only leads to
significance levels of <99% if the random distribution is calculated
for radii smaller than
20 km s-1 which contains
65% of the
PMS-Pl_ZAMS stars. Therefore we are lead to the conclusion that with a
very high probability the concentration of velocities vectors in the U-V plane is
not a chance coincidence.
An interesting feature is the accumulation of the 6 "PMS'' stars around a mean velocity of
(
km s-1. This is not far
from the velocity of the Castor MG (see above),
but clearly distinct from the Local Association which has
(
U,V) = (-1.6, -15.8) km s-1 (Montes et al. 2001).
The velocity dispersions of this subgroup of PMS stars are
km s-1.
Two of the remaining PMS stars are found near
the velocity of the Local Association together with a loose accumulation
of some 5 or 6 further stars from the Pl_ZAMS age group. A relation of these stars
with the Local Association may exist,
but the errors and the scatter of the velocity vectors are quite large.
The W-V diagram displayed in the lower panel of Fig. 23 shows a similar trend in the distribution of the velocity vectors as in the U-V diagram, that is most PMS stars and many Pl_ZAMS stars are kinematically distinct from the Local Association.
Spectroscopic luminosity classification of the G-K stars based on the high resolution spectroscopy showed that 88% of the G-K stars are main-sequence stars or subgiants of luminosity classes V and IV, respectively. From IR photometric classification we concluded that all M stars are dwarf stars.
Significant lithium absorption lines were detected in a large fraction of
stars with equivalent widths and abundances, respectively, above the level of the
Hyades in about 50% of the stars.
For the age distribution of the high-galactic latitude coronal sample this means
that about half of the G-K stars are younger than the Hyades.
About 25% of the G-K stars have an age comparable to that of the Pleiades, i.e.
100 Myr. A small fraction of less than 10% of the G-K stars is younger
than the Pleiades. Most PMS stars, i.e. 8 out of 10, are located
in area I. Only two PMS stars are found in area II and none in the remaining
areas. This suggests a possible relation of the high-|b| PMS stars
to the Gould Belt indicated in Fig. 1. However, the subsample formed
by combining the stellar age groups PMS and Pl_ZAMS is
spatially distributed in all directions covered by our study areas. At the same time
half
of its members show similar kinematical parameters independent of
spatial location. This questions the relation to the Gould Belt. Rather, the space
velocities suggest that these stars are members of a loose moving group with a mean
velocity close to that of the Castor MG.
For the Castor MG an age of
Myr has been derived by
Barrado y Navascués (1998). This would still be consistent with the Pl_ZAMS
group. If some of the PMS stars are indeed kinematically related to the Castor MG
this would indicate a large age spread in this moving group as they appear
to be younger than 100 Myr, maybe even as young as
30 Myr.
Acknowledgements
We would like to thank the Deutsche Forschungsgemeinschaft for granting travel funds (Zi 420/3-1, 5-1, 6-1, 7-1). We further thank the staff at the German-Spanish Astronomical Centre, Calar Alto, in particular Santos Petraz, for carrying out part of the observing programme in service mode. This publication makes use of data products from the Two Micron All Sky Survey, which is a joint project of the University of Massachusetts and the Infrared Processing and Analysis Center/California Institute of Technology, funded by the National Aeronautics and Space Administration and the National Science Foundation. This research has made use of the SIMBAD and VIZIER databases, operated at CDS, Strasbourg, France.
Figure A.1 displays the measured lithium equivalent widths for each study area separately.
![]() |
Figure A.1:
Equivalent widths of Li I
![]() ![]() |
Table A.1:
Mean tangential velocities and dispersions (in km s-1) in galactic coordinates
for stars of age groups PMS, Pl_ZAMS, UMa, Hya+ (split into dwarfs and giants),
and M stars without lithium detection for the individual study areas.
The first two lines give the average solar velocity for each study area.
The mean distance
and its scatter
are given in pc. The number of stars used for the calculation of the mean values
are given in parentheses.
In Table A.2 the basic parameters of the stellar sample are listed.
The field and RASS names were taken from Paper III.
Coordinates RA (2000) and Dec. (2000) of the optical counterparts are in succession either from
Tycho-2, GSC-I, or GSC-II, whatever the source is for the V magnitude listed in column "V''.
In column "Sp.type'' the revised spectral types with luminosity
class are given for objects with new high resolution observations.
Otherwise, spectral types from Paper III are given.
Spectroscopic binaries are flagged by "SB2''. B160 is a triple system (SB3).
The flux ratio
is given
for the revised V magnitudes and the RASS fluxes from Paper III.
X-ray luminosities
were calculated
using the distances listed in column "dist''. The distances are flagged by "S'', "H'', "T''
or "I'', depending on whether they were derived from spectroscopy, Hipparcos,
trigonometric parallaxes, or from the infrared colours, respectively. Distance estimates
obtained by assuming luminosity class V are flagged by "M''. They should be considered
as lower limits only.
Table A.3 lists the kinematical parameters. Heliocentric radial velocities
and errors for single stars and for the primary component of spectroscopic binaries
are given in columns
and
,
respectively. For binaries columns
and
contain the heliocentric radial velocity and error
of the secondary component, respectively. Proper motions and associated errors are
listed in columns
and
for
right ascension, and
and
for declination,
respectively.
The source catalog of the proper motions is denoted by
respective flags: TY = Tycho-2, HI = Hipparcos, UC = UCAC2, US = USNO-B1.0, PP = PPM, ST =
STARNET, TR = TRC, NL = NLPM1, CA = Carlsberg Meridian Catalogs. Also given are the
galactic velocity components U, V, and W in the LSR frame
with errors
and
,
respectively.
If the errors were larger than 30 km s-1 the space velocity components were omitted.
Table A.4 lists lithium data and rotational velocities.
Equivalent widths of Li I
are listed in column W(Li I ).
Flags "h'', "l''or "m'' denote high-, low- or medium resolution measurements,
respectively. Lithium abundances derived from W(Li I ) for the effective temperatures given in
column
are listed in column
(Li).
The last two columns list the rotational velocities,
for single stars or primary
components of binaries, and in the latter case
for the secondary component.
Table A.2: Basic optical and X-ray parameters of the sample of G-, K-, and M-type stars.
Table A.3: Kinematical parameters.
Table A.4: Lithium abundances and rotational velocities.