A&A 477, 917-929 (2008)
DOI: 10.1051/0004-6361:20078581
A. Pigulski1 - G. Pojmanski2
1 - Instytut Astronomiczny Uniwersytetu Wrocawskiego,
Kopernika 11, 51-622 Wroc
aw, Poland
2 -
Obserwatorium Astronomiczne Uniwersytetu Warszawskiego,
Al. Ujazdowskie 4, 00-478 Warszawa
Received 30 August 2007 / Accepted 7 November 2007
Abstract
Context. The Cephei stars have been studied for over a hundred years. Despite this, many interesting problems related to this class of variable stars remain unsolved. Fortunately, these stars seem to be well-suited to asteroseismology. Hence, the results of seismic analysis of
Cephei stars should help us to better understand pulsations and the main sequence evolution of massive stars, particularly the effect of rotation on mode excitation and internal structure. It is therefore extremely important to increase the sample of known
Cephei stars and select targets that are useful for asteroseismology.
Aims. We analysed ASAS-3 photometry of bright early-type stars with the goal of finding new Cephei stars. We were particularly interested in
Cephei stars that would be good for seismic analysis, i.e., stars that (i) have a large number of excited modes; (ii) show rotationally split modes; (iii) are components of eclipsing binary systems; (iv) have low-frequency modes, that is, are hybrid
Cephei/SPB stars.
Methods. Our study was made with a homogeneous sample of over 4100 stars having MK spectral type B5 or earlier. For these stars, the ASAS-3 photometry was analysed by means of a Fourier periodogram.
Results. We have discovered 103 Cephei stars, nearly doubling the number of previously known stars of this type. Among these stars, four are components of eclipsing binaries, seven have modes equidistant or nearly equidistant in frequency. In addition, we found five
Cephei stars that show low-frequency periodic variations, very likely due to pulsations. We therefore regard them as candidate hybrid
Cephei/SPB pulsators. All these stars are potentially very useful for seismic modeling. Moreover, we found
Cephei-type pulsations in three late O-type stars and fast period changes in one, HD 168050.
Key words: stars: early-type - stars: oscillations - stars: binaries: eclipsing - stars: variables: general - surveys
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Figure 1:
Location in equatorial coordinates of all stars with V > 7 mag,
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The published ASAS catalogues, containing photometry of variable star candidates, have already been used to discover Cephei stars.
In total, 19 new members of this group have been found in the ASAS data (Handler 2005; Pigulski 2005). However, owing to the fact that the method
of selection of variable stars was biased towards large-amplitude variables, all these 19 stars had relatively large amplitudes.
Therefore, it was obvious that once a detailed analysis of the whole ASAS-3 database has been done, many new stars
of this type, with smaller amplitudes, will be found. Such an analysis will be carried out in the future, but because the whole ASAS database contains millions
of stars and the period(s) alone are not sufficient to classify a given star as a
Cephei variable, we decided to proceed in a different way.
Using the information in the existing stellar catalogues, we selected stars that are known to be either O-type or early B-type stars and
analysed ASAS-3 photometry for these stars only. The selection criteria are explained in Sect. 2. As a result, nearly 300
Cephei stars were discovered of which the first part is discussed in this paper. This will allow us to define the properties of the whole class much better and,
in view of the increasing interest in the study of these stars by means of asteroseismology, to select appropriate targets for subsequent work.
In the present paper we describe the results of the search for
Cephei-type stars among objects selected
from the five volumes of the Michigan Catalogue for HD stars. The ASAS-3 photometry for stars selected using other catalogues
will be discussed in the next paper.
The existing catalogues contain many different types of data that allow selecting early-type stars. The early B and O-type stars can
be best selected using either the information on spectral types or the UBV photometry. For this reason, the obvious choice
of the source of the information on spectral types was the Michigan Catalogue of Two-Dimensional Spectral Types for the HD stars
(Houk 1982; Houk & Cowley 1975; Houk & Smith-Moore 1988; Houk 1978; Houk & Swift 1999).
The five volumes of this catalogue contain MK spectral types for 161 472 stars south of declination +5.
The stars are the same as those
in The Henry Draper Catalogue (Cannon & Pickering 1918-1924), i.e., are brighter than
10 mag in V.
This means that all stars fainter than
7 mag with HD numbers will have good ASAS-3 photometry because the ASAS survey covers
the range of V magnitudes between 7 and 14 mag.
While selecting stars from the Michigan Catalogue, we used only two conditions: (i) V > 7 mag (brighter stars are overexposed in the ASAS V-filter frames); (ii) MK spectral type B5 or earlier. In this way, about 4100 stars were selected. Their equatorial coordinates are plotted in Fig. 1. As expected, the stars concentrate along the Galactic plane. For all these stars, the ASAS-3 photometry was extracted, and subsequently analysed by means of Fourier periodograms in the frequency range from 0 to 40 d-1.
A star was regarded as variable if the signal-to-noise (S/N) of the highest peak in the periodogram exceeded 5.
Table 1:
New Cephei stars. N is the number of independent modes found in the ASAS-3 photometry,
the remaining columns are self-explanatory. References to the MK spectral types in the eighth column are the following:
(1) Houk & Cowley (1975); (2) Houk (1978); (3) Houk (1982); (4) Houk & Smith-Moore (1988); (5) Houk & Swift (1999); (6) Hill (1970).
In total, 103 Cephei stars were
found in the sample of about 4100 stars selected using Michigan Catalogue. These stars are listed in Table 1;
the frequencies, amplitudes and times of maximum light for the detected modes are presented in Table 2, available online. In addition,
periodograms showing the consecutive steps of prewhitening are shown in Figs. 2-14, also available at CDS.
The ASAS-3 photometry we analysed was carried out with a Johnson V filter. The data cover the time interval between the beginning of the project in 2000 and the end of February, 2006. As already shown in Paper I, the ASAS-3 data suffer from daily aliases. Consequently, the frequencies of some modes we provide in Table 2, especially of those with the smallest amplitudes, might be in error by 1 or even 2 cycles per sidereal day. On the other hand, the yearly aliases are relatively low in the ASAS-3 data (see Paper I).
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Figure 15:
The histogram of the number of detected modes for the 103 new ![]() |
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Figure 16:
Detection threshold, DT (open circles), and standard deviation of the residuals, SDR (filled circles), for the ASAS-3 photometry of the 103 new ![]() ![]() |
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Among stars listed in the review
paper of Stankov & Handler (2005), the well-known Cephei-type BW Vul is exceptional because of its high amplitude.
As we can see from Fig. 17,
the stars discovered in the ASAS data by Handler (2005) and Pigulski (2005) fill the gap in amplitudes between BW Vul and the other stars.
One star from that sample, HDE 328862, has the amplitude similar to that of BW Vul. For another one, CPD -62
2707,
a harmonic of the main mode, an indication of non-sinusoidal light curve, was detected.
In our list of newly discovered
Cephei stars there is another star with an exceptionally large amplitude, HD 173006.
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Figure 17:
V-filter semi-amplitude of the main mode,
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BW Vulpeculae is known for its unusual non-sinusoidal light curve, with a standstill on the raising branch (Fig. 18). It is interesting to note that a standstill was also found in the low-amplitude mode of 15 (EY) CMa (Shobbrook et al. 2006). In Fig. 18, we plot phase diagrams for the main modes of BW Vul and the three large-amplitude stars mentioned above. It can be seen that HD 173006 and HDE 328862 also exhibit a standstill although it is not so clearly visible as for BW Vul due to the larger scatter of datapoints. The light curve for BW Vul shown in Fig. 18 was obtained in Strömgren b filter, but it is very similar in shape to that in V (see, e.g., Sterken et al. 1993).
As can be seen in Fig. 17, the periods of modes detected in the new Cephei stars match very well the range covered by
already known stars. It seems that the largest amplitudes occur in stars with intermediate periods; for
the shortest and the longest periods amplitudes are rather small. This result qualitatively agrees with the recent non-linear calculations of Smolec & Moskalik (2007)
for radial modes in
Cephei stars.
There were ten known Cephei stars having modes with periods shorter than 0.1 d, of which six are members of the open cluster
NGC 6231 (see, e.g., Balona & Laney 1995). We detect four next ones, HD 115313, 152060, 165955, and 171141. The shortest
period, 0.0686 d, was found in HD 115313. It is interesting to note that
HD 152060 = Braes 122 = NGC 6231-308 is located 28
off the centre of NGC 6231. It is thus possible that this star is a member of the
cluster or of the Sco OB1 association surrounding NGC 6231.
On the other side of the period range we knew two stars with periods slightly longer than 0.3 days, V986 Oph with period equal to 0.303 d (Cuypers et al. 1989)
and Oo 2299 in the open cluster
Persei with period of 0.31788 d (Krzesinski & Pigulski 1997).
We found two stars with periods longer than 0.3 d (see, however, Sect. 3.4): HD 101838 (
P = 0.31973 d, a member
of the open cluster Stock 14 and a component of an eclipsing binary, see Sect. 3.7) and HD 153772 = vdBH 81a (
P = 0.30527 d), in the core of
the R association vdBH 81 (Herbst 1975; van den Bergh & Herbst 1975).
As we already explained in the Introduction, we expected to detect Cephei stars with smaller amplitudes than those
found earlier in the ASAS data by Handler (2005) and Pigulski (2005). Figure 17 shows that this is indeed the case.
As mentioned in Sect. 3.1 (see also Fig. 15), about half of the new Cephei stars are multiperiodic. In order to show how the
modes are spread over the frequencies, in Fig. 19 we plot the differences,
,
between frequency of a given mode,
,
and the
frequency of the main mode, f1, as a function of f1. By the main mode we mean the mode with the largest amplitude and period shorter than
0.32 d. We see from Fig. 19 that
is usually small in comparison with f1 and the value of
rarely exceeds 0.2; in most cases it is much smaller. There are, however, a few exceptions. First, for HD 126357, the frequencies of two modes,
f2 = 8.54271 d-1and
f3 = 8.07010 d-1, are about twice the frequency of the main mode (
f1 = 4.06927 d-1). This situates these two modes close to
the
line in Fig. 19. Next, we have five stars with modes that
are placed below
/2 line (asterisks in Fig. 19). We will discuss these stars in Sect. 3.4.
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Figure 18:
Light curves of three large-amplitude ![]() |
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Rotational splittings are observed in some Cephei stars. Good examples are
Eri (Jerzykiewicz et al. 2005),
V836 Cen (Aerts et al. 2004), and
Oph (Handler et al. 2005).
The presence of two modes closely spaced in frequency does not prove that we deal with rotational splitting although
this possibility
has to be considered in such a case. When three or more equally (or almost equally) spaced modes are observed,
the rotational splitting is an obvious conclusion. However, it can happen accidentally that three modes of different
form an equidistant triplet, as found for 12 (DD) Lac (Handler et al. 2006).
The rotationally split modes are potentially very useful for mode identification and asteroseismology.
We therefore checked the frequencies of the detected modes in the new Cephei stars
for possible rotational splittings. The results are summarized in Table 3 and shown in Fig. 20.
We list only stars in which inequality of separations is smaller than 20%. The most interesting are the first
two stars in Table 20, HD 74339 and HD 86214, those that in our sample have the largest number of detected modes. In both
stars equidistant quadruplets are observed. It is quite likely that modes listed in Table 3 are parts
of a rotationally split
or 2 modes. This, however, needs to be verified by mode identification, as
was done for 12 Lac.
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Figure 19:
The difference, ![]() ![]() ![]() ![]() |
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Table 3: Possible rotational splittings for seven stars from our sample. Designation of frequencies is the same as in Table 2.
The longest periods observed in Galactic Cephei stars rarely exceed 0.3 d (see Fig. 17) and until recent years there was no clear evidence for
the presence of low-frequency g modes in these stars. From the theoretical point of view, however, some overlap of the instability strips
of
Cephei and slowly pulsating B (SPB) stars (e.g., Pamyatnykh 1999) indicated that some hybrid objects might be found.
The recent campaigns on two well-known
Cephei stars,
Eri (Jerzykiewicz et al. 2005) and 12 (DD) Lac (Handler et al. 2006),
led to the discovery of low-frequency mode(s) in these stars.
On the other hand, Koaczkowski et al. (2006,2004) announced the discovery of a large number of short-period variable stars
in the Magellanic Clouds showing long-period mode(s) (periods in the range of 0.4-1 d) in addition to mode(s) typical for Cephei stars.
The origin of these long-period modes still needs to be explained. We will come back to the discussion of this problem in Sect. 4.
In the ASAS-3 data we have found five stars having periods considerably longer than 0.3 d (Fig. 19), namely, in the range between 0.45 and 0.80 d.
These stars are listed in Table 4. The most interesting of the five stars listed in Table 4 is HD 101794 = V916 Cen = Stock14-13. The star is
a member of the loose open cluster Stock 14 = Lodén 462/465 (Lodén 1973), although Humphreys (1978) and Kaltcheva et al. (1994) include it to the association Cru OB1.
The star was classified as B1 IVne by Garrison et al. (1977). Its Be status was confirmed by measurements of the
index (Johansson 1981; Klare & Neckel 1977; Kaltcheva 2003; Moffat & Vogt 1975)
and H
photometry (McSwain & Gies 2005).
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Figure 20:
Schematic frequency spectra in the vicinity of the possible rotationally split modes of seven new ![]() |
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Table 4: Stars with periods longer than 0.4 d.
HD 101794 was discovered as variable by Hipparcos and was subsequently named V916 Cen. The star was assigned the variability type of Cas,
which labels B-type stars showing erratic long-term changes with a range up to 0.5 mag. Suprisingly, HD 101794 is also an eclipsing star (see Sect. 3.7).
There are at least two other periodic terms superimposed
on the variability due to eclipses (Table 4). One of them has a period in the
Cephei domain (
P = 0.22447 d) and this is the reason for
including the star in the list of
Cephei stars. Another periodicity, with a period
of about 0.54362 d, can be attributed to a
Eridani-type variability.
Another star from Table 4, HD 116827, is also known to be a Be star (MacConnell 1981).
Houk & Cowley (1975) classify the star as B2/5 (Vn) and
note that the H
line may be partially filled in, a clear indication of a weak emission.
The third new Cephei star with both short and long-period variability, is HD 117357. It shows even stronger emission
than HD 101794 in hydrogen Balmer lines (Yudin 2001; Schmidt-Kaler 1964; Garrison et al. 1977; Wiegert & Garrison 1998).
The emission in H
is confirmed by two measurements of the
index: 2.522 (Deutschmann et al. 1976)
and 2.502 (Klare & Neckel 1977).
There is no recorded evidence for emission in hydrogen lines for the two remaining stars
in Table 4, HD 99205 and HD 122831.
Since three of five stars in Table 4 show Balmer-line emission and only two of the remaining 98 Cephei stars are known as
Be stars, it is hard to believe that the occurence of long periods and Balmer-line emission remains unrelated.
We will come back to the discussion of the origin of long periods in these stars in Sect. 4.
Period and amplitude changes are observed in some Cephei stars (Jerzykiewicz & Pigulski 1998, Paper I);
they usually take place on a time scale of years or decades. Because ASAS-3 data cover five years, we
may expect detecting period changes only if they are very fast. Indeed, only one star, HD 168050, shows
pronounced period changes. The photometry of HD 168050 reveals not only two modes attributable to the
Cephei-type variability (Table 2), but also eclipses (see Sect. 3.7), indicating that
the pulsating star is a component of an eclipsing binary. For one of the detected pulsation modes, the period is stable,
while for the other the period increases rapidly.
We show the O-C diagram for both modes in Fig. 21. Assuming constant rate of period change for P2, we get
s century-1. This is the fastest change of period ever detected in a
Cephei-type star.
Times of maximum light for both modes of HD 168050 are given in Table 5.
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Figure 21: The O-C diagram for both modes detected in HD 168050. The dashed line represents constant rate of period change equal to 104 s century-1. |
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Table 5: Time of maximum light for both modes detected in HD 168050.
As far as the long-term amplitude changes are concerned, we found no clear evidence for them among the newly discovered Cephei stars.
Although B0 is the earliest spectral type of known Cephei stars, from the theoretical point of view the instability strip
of
Cephei stars extends to O-type stars (see, e.g., Pamyatnykh 1999). The searches for
Cephei-type
pulsations in O-type stars, both in the Galactic field (Balona 1992) and Cygnus OB2 association (Pigulski & Koaczkowski 1998),
were not conclusive, however. On the other hand, line-profile variations were observed in some fast-rotating late O-type stars
such as
Oph (Vogt & Penrod 1983; Kambe et al. 1990). They were usually attributed to pulsations in modes with relatively high
,
undetectable
in photometry. A recent MOST satellite photometry of
Oph (Walker et al. 2005a) clearly revealed
Cephei-type pulsations.
It is therefore reasonable to regard
Oph and several other late O-type stars showing non-radial pulsations
in line profiles (Balona & Dziembowski 1999; Fullerton et al. 1996) as
Cephei stars.
Among the new Cephei stars, there are at least two O-type stars. The first one is HD 91651 = HIP 51681, a member
of Car OB1 association. Its published MK spectral types are the following:
O9 Vp? (Morgan et al. 1955), O9 Vn: (Feast et al. 1957), O9 V:n (Walborn 1973), O8/9 V (Houk & Cowley 1975),
O9 Vnp (Garrison et al. 1977), and O9.5 III (Mathys 1988). The star is fast-rotating, the projected radial velocity amounting
280-300 km s-1 (Penny 1996; Penny et al. 2004; Howarth et al. 1997). The star is known to have strong nitrogen
lines for its spectral type (Howarth & Prinja 1989; Garrison et al. 1977; Schild 1985). The variability of radial velocity of HD 91651
was indicated by Levato et al. (1988) and Lehner et al. (2003). Levato et al. (1988) suspected even that the star is a double-lined
spectroscopic binary with an orbital period of 9.275 d. It is interesting to note that from the study of line profiles in this star, Penny (1996)
already suggested the possibility of non-radial pulsations.
The other O-type star is HD 156172 with two published spectral types: O9.5/B0.5 Ia/Iab (Houk 1978) and O9 Vnne (Garrison et al. 1977). The star is located in the region of the HI bubble surrounding O5 Vn((f)) star HD 155913, and could belong to an unknown association (Cappa & Benaglia 1998).
Two other stars are classified as O9/B0 V and O9.5/B0 V by Houk & Cowley (1975), namely, HD 95568 and HD 117357. For HD 95568 this is the only MK spectral type available, for HD 117357 there are several other classifications indicating that it is rather a fast-rotating B0 star.
Although we cannot exclude that variability we detected in O-type stars is due to the pulsations of their, presently unknown, early B-type companions, this seems to be rather unlikely.
If a Cephei star is a component of an eclipsing system, one has an opportunity of deriving its accurate mass and radius.
Of the 112 previously known
Cephei stars, there were four components of eclipsing systems (see Pigulski 2006):
16 (EN) Lac (Pigulski & Jerzykiewicz 1988; Jerzykiewicz et al. 1978), V381 Car in NGC 3293 (Freyhammer et al. 2005; Jerzykiewicz & Sterken 1992; Engelbrecht & Balona 1986),
Ori (Kuntz & Stebbins 1916; Waelkens & Lampens 1988; De Mey et al. 1996),
and
Sco (Shobbrook & Lomb 1972; Uytterhoeven et al. 2004; Bruntt & Buzasi 2006).
We add four stars to this list. Surprisingly, two are members of a loose open cluster Stock 14 (Peterson & FitzGerald 1988; Moffat & Vogt 1975; FitzGerald & Miller 1983): HD 101794 and HD 101838. The other two are HD 167003 and HD 168050. It is interesting to note that at least in two stars, HD 101794 and HD 168050 the secondary eclipses are deep enough to expect that spectroscopically they will be double-lined systems. If this were the case, the follow-up studies should allow deriving the masses and radii of the components.
As mentioned in Sect. 3.4, photometric variability of HD 101794, a Be star and a member of Stock 14, was discovered by the Hipparcos satellite. Its eclipsing nature was revealed by Pojmanski (2000) with the I-filter ASAS-2 data. The orbital period amounted to 1.4632 d. As already explained in Sect. 3.4, the star shows also low-amplitude periodic variations. The eclipsing light curve of HD 101794 is shown in Fig. 22. We see that after removing the contribution from the long-term and sinusoidal variations, the eclipses are clearly seen both in the 1997-1999 ASAS-2 data and the ASAS-3 data. Although barely, they can be even seen in the Hipparcos data. The ephemerides for eclipses of V916 Cen and the other three stars are given in Table 6.
Table 6:
Data for the four new Cephei stars in eclipsing systems.
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Figure 22:
The eclipsing light curve of V916 Cen folded with the orbital period of 1.4632361 d for ASAS-2 I-filter data (dots), ASAS-3
V-filter data (open circles) and Hipparcos ![]() |
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The eclipsing light-curve of HD 101838 is shown in Fig. 23. When folded with the period of 5.41166 d, it shows no sign of a secondary minimum. However, we cannot exclude the possibility that the true orbital period is twice as long, i.e., it is equal to about 10.82 d. If this were the case, the system would consist of two similar components.
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Figure 23: The ASAS-3 V-filter light-curve of HD 101838, freed from the contribution of pulsation and folded with the orbital period of 5.41166 d. |
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Figure 24: The ASAS-3 V-filter light curve of HD 167003 (V4386 Sgr) freed from the contribution of pulsations and folded with the orbital period of 10.79824 d. The upper figure shows the whole light curve, the lower, only phases close to the primary minimum. In addition, Hipparcos data (not corrected for the contribution from pulsations) are plotted in the lower figure as open circles. |
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The variability of HD 167003 was detected by the Hipparcos satellite. Since five observational points obtained within half a day
deviated by about 0.2 mag from the remaining observations, it was concluded that the star is possibly an eclipsing binary. The star was
classified as an unsolved variable and named V4386 Sgr. There were about a dozen or so deviating points in the ASAS-3 data,
clearly indicating the presence of a narrow eclipse. Fortunately, the ASAS-3 data are better distributed in time than those from Hipparcos,
allowing to unambiguously derive the orbital period. The period is equal to 10.79824 d. The light curve (Fig. 24) shows also a small
reflection effect. The analysis of the out-of-eclipse data reavealed the presence of at least four pulsational components with frequencies
between 5.38 and 7.55 d-1 (Table 2), indicating clearly that the primary component is a Cephei-type pulsator.
This is in agreement with
the published MK spectral types of this star: B0.5 III (Hill et al. 1974), B1 II (Garrison et al. 1977), and B1 Ib/II (Houk 1978).
As can be seen in Fig. 24, the eclipse covers only about 0.04 in phase, corresponding to about 10 hours, and is probably total. In the lower panel of Fig. 24, Hipparcos data obtained close to the primary minimum are also plotted. The five deviating points mentioned earlier fit the eclipse quite well. However, due to the small number of data points, the contribution from pulsations could not be removed from the Hipparcos data. This may account for the deviations with respect to the ASAS-3 light curve (dots).
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Figure 25: The ASAS-3 V-filter light curve of HD 168050 freed from the contribution of two pulsating modes and folded with the orbital period of 5.02343 d. |
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Figure 26:
Distribution of ![]() |
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We have already indicated in Paper I that owing to the poor spatial resolution, the ASAS-3 data are not well suited for the detection
of Cephei stars in open clusters. However, if a cluster is sparse or the variable is far from the central area of the cluster,
the ASAS-3 photometry can allow detection. In the sample of the 103 new
Cephei stars we can indicate six stars which are
members or likely members of young open clusters, and other six which are members of OB associations. This is indicated in the last
column of Table 1. The membership of new
Cephei stars in clusters and their distribution in the Galaxy will be discussed in the next
paper of the series.
The original work on Hipparcos data resulted in the discovery of six Cephei stars (Waelkens et al. 1998; Aerts 2000). Later on,
some follow-up work was done (Koen 2001; Koen & Eyer 2002) yielding about 60 candidates for short-period variables among O and early
B-type stars of which at least some are expected to be
Cephei stars. Due to the unfavourable distribution of the Hipparcos
data in time, this discovery needs, however, to be confirmed by independent observations. With the ASAS-3 data,
we could verify the variability of 22 of these candidates; they are listed
in Table 7. The remaining stars are either saturated in the ASAS-3 data or are located north of declination +28
,
i.e., outside the area in the sky
covered by the ASAS-3 observations.
Table 7: The results of the verification of variability of 22 O and early B-type candidate short-period variables observed by Hipparcos and found by Koen (2001) and Koen & Eyer (2002). DT is the detection threshold in the ASAS-3 photometry.
Of these 22 stars, only seven can be classified as
Cephei stars. One, HD 191531, was already discovered by Handler (2005), see also Paper I.
The remaining six are new
Cephei stars, but only four are listed in Table 1, while two,
HDE 306387 = V909 Cen and HDE 339483, are not included because they do not appear in the Michigan catalogues.
These two stars will be discussed in the next paper of the series.
For the remaining 15 stars from Table 7, the short-period variability was not confirmed by the ASAS-3 data, although for all but HD 42597 the detection threshold was smaller than the amplitude reported from the analysis of the Hipparcos data. It can be seen from Table 7 that frequencies for most of them range between 10 and 12 d-1. As already explained by Jerzykiewicz & Pamyatnykh (2000) and Koen & Eyer (2002), these spurious frequencies are due to aliasing originating from the convolution of the low-frequency changes and the spectral window dominated by the rotation frequency of the satellite (11.25 d-1).
For five of the seven Cephei stars in Table 7, the agreement between frequencies derived from the Hipparcos and ASAS-3 data
is very good. Only for HD 68962 and 86065 the differences are significant, amounting to about
0.0749 and +0.0203 d-1, respectively. This can be explained in terms of aliasing in the periodograms of Hipparcos data.
Theoretical calculations show also (Pamyatnykh 1999) that Cephei and SPB instability strips partially overlap, which means that hybrid stars,
showing pulsations of both types, might exist. This possibility was already indicated by Dziembowski et al. (1993) for a region around spectral type B2-B3 and masses
equal to 7-8
.
Newer calculations (Pamyatnykh 1999) confirmed this and showed in addition that g-mode instability extends towards higher masses.
The latter instability is confined, however, to the very late main-sequence stages.
This picture of p and g mode instability domains was calculated neglecting the effects of rotation on pulsations. The theory that includes fast rotation is still not fully satisfactory, but it is already clear that rotation changes stability of modes. A good example of the theoretical calculations that include the effect of rotation on the stability of g modes was published by Townsend (2005), who showed that for fast-rotating stars the SPB instability strip widens towards higher masses. The region of possible hybrid behaviour becomes therefore much larger. In addition, the frequencies of modes, especially of non-axisymmetric modes, change considerably. In particular, frequencies of retrograde sectoral mixed modes are shifted to much lower frequencies than they would have in non-rotating stars, i.e., will occur in the range where normally the g modes are observed. On the other hand, frequencies of prograde sectoral g modes shift to the region occupied normally by p modes. It must be also remembered that in the presence of fast rotation modes can no longer be classified in a simple scheme described by three quantum numbers because the geometry of such modes differs from spherical harmonics.
The effects related to fast rotation are impontant not only because some Cephei stars are known to
rotate fast. The region of
Cephei and SPB stars in the H-R diagram is populated by Be stars which,
by definition, rotate very fast. These stars were known to
show both short-period variability and line-profile variations. The short-period photometric variability called, after the prototype, the
Eri-type (Balona 1990) was
usually attributed to rotationally-induced effects because no clear evidence for multiperiodicity was found (see, e.g., Balona & James 2002). On the other hand, there
were many convincing examples of line-profile variations in Be stars that were interpreted in terms of non-radial pulsations
(Floquet et al. 2000; Yang et al. 1990; Stefl et al. 1995; Baade 1984), including
multiperiodic behaviour (Rivinius et al. 1998). Despite this, it was not widely accepted that non-radial pulsations are present in Be stars mainly because
there was no clear relation between periods seen in photometry and spectroscopy. An excellent review of variabilities observed in Be stars
was recently given by Porter & Rivinius (2003).
A strong argument in favour of non-radial pulsations in Be stars, as seen in photometry, came from the observations carried out by the MOST satellite, in particular, those of an early Be star, HD 163868, in which Walker et al. (2005b) found over 60 periodicities in three distinct groups. A theoretical interpretation of this variability (Walker et al. 2005b; Savonije 2007; Dziembowski et al. 2007) includes pulsations in g modes. It is therefore reasonable to use the term "SPBe stars'' for Be stars with detected g-mode pulsations, as proposed by Walker et al. (2005b), although it has to be remembered that many previous investigators already indicated a common cause of periodic variability in SPB and Be stars.
The two grouping of modes seen in HD 163868 around 1.7 and 3.4 d-1 might be a clue to understanding a grouping of modes
in Cephei and SPB candidates in the LMC and SMC, found by Koaczkowski et al. (2006,2004). In many of these stars, the frequencies of
modes grouped around two values whose ratio was close to 2.
Whether fast rotation is responsible for this could be verified by future spectroscopic observations.
For the SMC we know that many of these stars are fast-rotating because they show emission in Balmer lines.
Since inclusion of fast rotation enhances the possibility of getting unstable low-frequency modes among early and mid-B stars, we should see them observationally.
It seems that we get more and more examples that confirm these predictions. First, low-frequency modes were detected in two classical Cephei stars,
Eri (Jerzykiewicz et al. 2005) and 12 Lac (Handler et al. 2006). In the ASAS-3 data (Sect. 3.4), we found five
Cephei stars in which low-frequency
modes were detected. In addition, another
Cephei star with low-frequency modes, HD 133823, was found in Paper I
(see also Fig. 19). On the other hand, periodic variations with very short periods were found in some mid and late B-type stars like
V2104 Cyg (Uytterhoeven et al. 2007) and stars in NGC 3293 (Handler et al. 2007). A preliminary analysis of the data obtained for the other young open cluster,
h Persei (NGC 869) also reveals the presence of mid-B stars, of which some are known as Be stars, showing relatively short periods, even below 0.3 d
(Majewska-Swierzbinowicz et al., in preparation).
The complexity of mode behaviour in the presence of fast rotation may
pose a problem as far as the classification of hot pulsators is concerned. This is because period(s) alone may not be sufficient to
recognize Cephei and SPB star. Mode identification becomes a neccessity if we want to classify stars pulsating in p modes as
Cephei stars, while those pulsating in g modes, as SPB stars.
The other important results that come from the discovery of 103 Cephei stars can be summarized as follows:
Acknowledgements
The work was supported by the MNiI/MNiSzW grants No. 1 P03D 016 27 and N203 007 31/1328. We greatly acknowledge comments made by Prof. M. Jerzykiewicz and Dr. Gerald Handler, the referee. This research has made use of the SIMBAD database, operated at CDS, Strasbourg, France.
Table 2:
Parameters of the sine-curve fits to the V magnitudes of new Cephei-type stars listed in Table 1.
is the number of observations, the initial epoch T0 is equal to 2 450 000.0. The other parameters are the following:
,
time of maximum light for the ith mode,
,
standard deviation of the residuals, DT, detection threshold.
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Figure 2:
Fourier periodograms of the ASAS-3 data of ten ![]() |
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Figure 3: The same as in Fig. 2, but for HD 86214, 86248, 87592, 88844, 90075, 90987, and 91651. |
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Figure 4: The same as in Fig. 2, but for HD 92291, 93113, 93341, 94065, 94345, 94900, and 95568. |
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Figure 5: The same as in Fig. 2, but for HD 96882, 96901, 97629, 98260, 99024, 99205, 100355, and 101794. |
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Figure 6: The same as in Fig. 2, but for HD 101838, 102505, 103007, 103320, 103764, 104257, 104465, 104795, and 106345. |
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Figure 7: The same as in Fig. 2, but for HD 108628, 108769, 110498, 111377, 111578, 113013, 114444, 114733, 115533, 116538, and 116827. |
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Figure 8: The same as in Fig. 2, but for HD 117357, 117687, 117704, 119252, 119910, 122831, 123077, and 126357. |
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Figure 9: The same as in Fig. 2, but for HD 131805, 132320, 137405, 142754, 145537, 146442, 147421, 149100, and 150927. |
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Figure 10: The same as in Fig. 2, but for HD 151158, 152060, 152162, 152372, 153772, 154500, 155407, 156172, and 156321. |
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Figure 11: The same as in Fig. 2, but for HD 159792, 161633, 164188, 164741, 165955, and 166304. |
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Figure 12: The same as in Fig. 2, but for HD 167003, 167451, 168015, 168050, 168675, 168750, and 169173. |
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Figure 13: The same as in Fig. 2, but for HD 169601, 171141, 171305, 171344, 172140, 172427, 173006, and 178987. |
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Figure 14: The same as in Fig. 2, but for HD 173502, 180032, 186610, and 187536. |
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