Contents

A&A 477, 917-929 (2008)
DOI: 10.1051/0004-6361:20078581

$\beta $ Cephei stars in the ASAS-3 data

II. 103 new $\beta $ Cephei stars and a discussion of low-frequency modes[*],[*]

A. Pigulski1 - G. Pojmanski2


1 - Instytut Astronomiczny Uniwersytetu Wroc\lawskiego, Kopernika 11, 51-622 Wroc\law, Poland
2 - Obserwatorium Astronomiczne Uniwersytetu Warszawskiego, Al. Ujazdowskie 4, 00-478 Warszawa

Received 30 August 2007 / Accepted 7 November 2007

Abstract
Context. The $\beta $ 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 $\beta $ 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 $\beta $ 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 $\beta $ Cephei stars. We were particularly interested in $\beta $ 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 $\beta $ 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 $\beta $ 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 $\beta $ Cephei stars that show low-frequency periodic variations, very likely due to pulsations. We therefore regard them as candidate hybrid $\beta $ Cephei/SPB pulsators. All these stars are potentially very useful for seismic modeling. Moreover, we found $\beta $ 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

1 Introduction

This is the second paper in the series presenting results of a search for $\beta $ Cephei-type pulsating variables in the V-filter photometry in the third phase of the All Sky Automated Survey, ASAS-3 (Pojmanski 2000,1997; Pojmanski et al. 2005). In the first paper of the series (Pigulski & Pojmanski 2008, hereafter Paper I), we published the results of an analysis of the ASAS-3 photometry for 41 of about 112 presently known $\beta $ Cephei-type stars, that is, all that had sufficiently good photometry in the ASAS-3 database. The analysis allowed us to detect amplitude changes in three $\beta $ Cephei stars, BW Cru, V836 Cen and V348 Nor, and period changes in KK Vel and V836 Cen. In addition, new modes were found or ambiguities in the frequencies of previously detected modes were removed for some stars.


  \begin{figure}
\par\includegraphics[width=14cm,clip]{8581f01.eps}\end{figure} Figure 1: Location in equatorial coordinates of all stars with V > 7 mag, $\delta < +5^\circ $ and of spectral type B5 or earlier, selected from Michigan Catalogues as candidates for $\beta $ Cephei stars.

The published ASAS catalogues, containing photometry of variable star candidates, have already been used to discover $\beta $ 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 $\beta $ 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 $\beta $ 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 $\beta $ 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.

2 Selection of early-type stars

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$^{\circ}$. The stars are the same as those in The Henry Draper Catalogue (Cannon & Pickering 1918-1924), i.e., are brighter than $\sim$10 mag in V. This means that all stars fainter than $\sim$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 $\beta $ 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).
        V B-V U-B    
HD CPD/BD ASAS name N [mag] [mag] [mag] MK sp. type Notes
46994 -25$^{\circ}$1525 063513-2550.4 1 7.86 -0.17 - B2/3 V (4) in CMa OB2
48553 +02$^{\circ}$1369 064410+0223.5 1 9.03 - - B2 III (5) in the CoRoT field
67600 -20$^{\circ}$3392 080754-2109.0 1 9.18 - - B3/5 V (4)  
68962 -35$^{\circ}$2054 081323-3618.7 1 7.34 +0.15 -0.65 B2/3 V (3) in BH 23
69016 -27$^{\circ}$2973 081401-2743.1 1 10.22 - - B3 IV (3)  
69824 -48$^{\circ}$1585 081638-4826.2 1 9.10 - - B4/6 V (2)  
73568 -44$^{\circ}$2824 083719-4512.5 2 8.35 +0.30 -0.57 B2/3 IV (2) in Vela OB1
74339 -47$^{\circ}$2545 084133-4801.5 6 9.30 +0.14 -0.67 B2/3 II/III (2) in IC 2395
77769 -46$^{\circ}$3350 090248-4657.9 1 9.38 - - B3 IV (2) in Platais 9
86085 -38$^{\circ}$3738 095519-3845.8 1 8.94 -0.09 -0.85 B1 Vn (6) halo star


86214

-59$^{\circ}$1528 095458-5949.8 6 9.21 -0.02 -0.79 B2 Ib (1)  
86248 -30$^{\circ}$3001 095633-3126.5 1 9.63 -0.19 -0.89 B2 III (3) high-velocity star, very distant
87592 -58$^{\circ}$1860 100409-5922.9 5 8.96 - - B1 IV (1)  
88844 -60$^{\circ}$1765 101302-6110.7 2 8.53 -0.16 -0.93 B0.5 III (1) ALS 1453
90075 -59$^{\circ}$2079 102206-6011.2 1 8.88 +0.07 -0.76 B1 II (1) ALS 1517
90987 -57$^{\circ}$3308 102849-5746.0 4 9.64 +0.13 -0.70 B1/2 III/IVp (1) ALS 1601, in IC 2581 ?
91651 -59$^{\circ}$2214 103330-6007.7 2 8.85 -0.01 -0.89 O8/9 V (1) ALS 1647, in Car OB1
92291 -60$^{\circ}$2077 103756-6116.5 5 9.07 -0.07 -0.86 B2 Ib/II (1) ALS 1702
93113 -57$^{\circ}$3449 104400-5741.1 1 8.71 +0.03 -0.76 B1/2 II/III (1) ALS 1818
93341 -56$^{\circ}$3759 104524-5659.4 1 9.64 +0.02 -0.74 B1/2 II/III (1) ALS 1876


94065

-61$^{\circ}$1905 105007-6148.3 5 8.95 -0.05 -0.83 B0/1 III-IV (1)  
94345 -59$^{\circ}$2802 105210-5957.3 3 9.00 +0.06 -0.77 B0/1 IV (1)  
94900 -59$^{\circ}$2859 105611-5955.8 1 9.25 +0.17 -0.66 B1/2 III (1) ALS 2034
95568 -61$^{\circ}$2021 110040-6236.9 2 9.56 +0.12 - O9/B0 V (1) ALS 2084
96882 -60$^{\circ}$2553 110824-6117.1 1 9.03 -0.03 -0.86 B1 II/III (1)  
96901 -63$^{\circ}$1845 110820-6436.1 2 8.87 +0.20 -0.62 B1 III/IV (1)  
97629 -60$^{\circ}$2677 111308-6106.8 1 9.53 +0.11 -0.65 B3/5 Ib/II (1) ALS 2250
98260 -60$^{\circ}$2783 111719-6130.7 3 9.70 +0.26 -0.63 B1/2 Ib/II (1) ALS 2292
99024 -59$^{\circ}$3411 112303-6031.2 1 9.66 +0.03 -0.77 B2 Ib/II (1) ALS 2327
99205 -69$^{\circ}$1537 112356-7008.0 2 9.59 +0.01 -0.73 B1 III (1) ALS 2336


100355

-61$^{\circ}$2391 113216-6232.8 3 9.23 0.00 -0.67 B2/3 III (1)  
101794 -61$^{\circ}$2541 114225-6228.6 2 8.68 +0.06 -0.74 B0/1 n (1) ALS 2460, eclipsing, Be star,
                in Stock 14
101838 -61$^{\circ}$2550 114249-6233.9 1 8.42 +0.02 -0.81 B0.5/1 III (1) ALS 2463, eclipsing, in Stock 14
102505 -69$^{\circ}$1588 114720-7025.0 2 9.02 +0.08 - B1 IV (1) ALS 2495
103007 -61$^{\circ}$2696 115118-6159.8 3 9.29 -0.01 -0.82 B2/3 (III) (1) ALS 2519
103320 -59$^{\circ}$3910 115341-6016.0 1 8.82 -0.03 - B2 III (1)  
103764 -61$^{\circ}$2814 115652-6236.6 1 9.48 -0.06 -0.80 B2 II/III (1)  
104257 -65$^{\circ}$1757 120012-6604.7 1 8.85 +0.05 -0.73 B1/2 II/III (1) ALS 2562
104465 -62$^{\circ}$2526 120137-6333.8 2 9.07 -0.05 -0.81 B2 II/III (1)  
104795 -58$^{\circ}$4048 120400-5843.4 1 9.09 +0.11 - B2 III (1)  


106345

-67$^{\circ}$1921 121416-6744.4 1 9.08 - - B2 III (1)  
108628 -61$^{\circ}$3220 122906-6228.0 2 9.16 - - B2 II (1)  
108769 -33$^{\circ}$3261 123003-3429.9 1 9.03 - - B2 III (3)  
110498 -60$^{\circ}$4253 124316-6138.9 1 9.67 +0.49 -0.49 B0.5 III (1) ALS 2737, in Cen OB1
111377 -60$^{\circ}$4309 124938-6057.9 1 9.52 +0.13 -0.68 B2/5 II-III (1) ALS 2775
111578 -59$^{\circ}$4488 125057-6026.8 1 9.13 +0.16 -0.57 B2/3 II (1) ALS 2785
113013 -59$^{\circ}$4653 130141-6026.4 2 9.40 +0.12 - B2 III (1) ALS 2871
114444 -74$^{\circ}$1029 131304-7518.9 2 10.32 -0.02 -0.80 B1 II/III (1) ALS 2963
114733 -57$^{\circ}$5952 131330-5821.7 1 9.52 +0.27 -0.55 B2/3 III (1) ALS 2980
115533 -61$^{\circ}$3586 131901-6153.7 1 10.04 +0.08 -0.76 B2/5 (Ib/II) (1) ALS 3026, Vis. double, Sep. 6 $^{\prime\prime}$


116538

-51$^{\circ}$6048 132512-5150.5 1 7.90 -0.06 -0.89 B2 Ib/II (2)  
116827 -61$^{\circ}$3706 132735-6207.1 2 9.51 +0.11 -0.57 B2/5 (Vn) (1) Be star
117357 -61$^{\circ}$3760 133116-6144.0 2 9.02 +0.23 -0.72 O9.5/B0 V (1) ALS 3103, Be star
117687 -60$^{\circ}$4759 133330-6126.8 1 9.33 +0.12 -0.71 B2 Ib/II (1) ALS 3115
117704 -61$^{\circ}$3793 133337-6219.1 1 8.89 +0.20 -0.59 B1/2 III (1) ALS 3116, close to WR 55
119252 -47$^{\circ}$6162 134309-4748.3 1 10.34 - - B3 III (2)  
119910 -60$^{\circ}$4978 134754-6053.0 2 8.31 -0.07 - B2 III/IV (1)  
122831 -67$^{\circ}$2491 140701-6834.1 2 9.60 +0.05 - B1 III (1) ALS 3196
123077 -42$^{\circ}$6537 140637-4327.8 4 10.30 -0.23 - B2/3 II (2)  
126357 -59$^{\circ}$5569 142709-5944.2 3 9.07 +0.22 -0.64 B1 III (1) ALS 3238, in NGC 5606
131805 -73$^{\circ}$1416 150055-7347.7 1 8.47 - - B5 V (1) long-term variability superimposed
132320 -59$^{\circ}$5775 150106-5953.7 1 9.40 +0.31 -0.53 B1 III (1)  
137405 -60$^{\circ}$5814 152854-6048.1 1 9.36 +0.13 -0.64 B0.5/1 Iab (1) ALS 3356
142754 -40$^{\circ}$7155 155749-4059.8 1 8.60 +0.17 -0.60 B2 III (2)  
145537 -34$^{\circ}$6468 161255-3439.3 2 10.41 +0.10 -0.78 B2 Ib/II (3)  
146442 -45$^{\circ}$7845 161823-4550.4 3 9.04 +0.30 -0.51 B2 III (2)  
147421 -53$^{\circ}$7928 162445-5327.8 1 9.02 +0.09 -0.81 B0 II (1) ALS 3596
149100 -53$^{\circ}$8064 163521-5338.9 1 7.19 -0.06 -0.76 B2 III (1)  
150927 -37$^{\circ}$6738 164544-3810.1 2 9.44 +0.32 -0.52 B2/3 Ib (3)  
151158 -42$^{\circ}$7512 164734-4252.7 1 8.20 +0.22 -0.49 B2 Ib/II (2) ALS 3754


152060

-41$^{\circ}$7683 165300-4124.5 2 9.58 +0.06 -0.73 B1 III (2)  
152162 -45$^{\circ}$8186 165354-4600.9 2 8.59 +0.18 - B2 III (2)  
152372 -48$^{\circ}$8913 165517-4848.3 3 8.85 +0.20 -0.60 B2 III/IV (2)  
153772 -50$^{\circ}$9813 170400-5105.0 1 8.32 +0.06 -0.61 B2 V (2) in R assoc. vdBH81a
154500 -34$^{\circ}$6724 170721-3428.7 2 9.94 +0.22 -0.56 B2 Iab/b (3)  
155407 -45$^{\circ}$8378 171332-4527.2 1 9.52 - - B2 II (2)  
156172 -41$^{\circ}$7933 171800-4203.6 1 8.18 +0.40 -0.58 O9.5/B0.5 Ia/Iab (2) ALS 4037
156321 -32$^{\circ}$4462 171820-3219.6 1 8.15 +0.01 -0.77 B2 V (3)  
159792 -46$^{\circ}$8786 173850-4618.9 3 9.43 +0.15 -0.63 B2 II (2)  
161633 -46$^{\circ}$8909 174900-4656.4 4 9.94 +0.12 -0.95 B1 Iab/b (2)  


164188

-15$^{\circ}$4767 180039-1548.1 1 8.67 +0.19 -0.71 B1 Ib/II (4) ALS 4546
164741 -25$^{\circ}$6269 180344-2518.7 5 9.03 +0.31 -0.55 B2 Ib/II (4) ALS 4590
165955 -34$^{\circ}$7625 180958-3452.1 2 9.20 -0.05 -0.82 B2 II/III (3) ALS 4702, high-velocity star
166304 -16$^{\circ}$4739 181043-1642.8 3 9.33 +0.19 -0.63 B2 II (4)  
167003 -33$^{\circ}$4963 181442-3308.5 4 8.45 -0.13 -0.94 B1 Ib/II (3) ALS 4801, V4386 Sgr, eclipsing
167451 -13$^{\circ}$4897 181555-1334.5 1 8.24 +0.78 -0.29 B1 Ib (4) ALS 4844, in Ser OB1
168015 -13$^{\circ}$4919 181822-1323.2 2 9.11 +0.36 - B3/5 II (4) ALS 9488
168050 -19$^{\circ}$6762 181839-1906.2 2 9.81 - - B3/5 Ib (4) eclipsing
168675 -17$^{\circ}$5154 182143-1753.8 2 8.94 +0.28 - B2 Ib/II (4) ALS 4964
168750 -26$^{\circ}$6414 182221-2625.0 3 8.27 +0.08 -0.74 B1 Ib (3) ALS 4969


169173

-17$^{\circ}$5179 182408-1751.8 1 9.93 - - B3 Ib (4)  
169601 -17$^{\circ}$5192 182607-1747.3 3 9.88 - - B0/1 Iab/b (4)  
171141 -46$^{\circ}$9389 183516-4556.4 1 8.37 -0.22 -0.97 B2 II/III (2) halo star
171305 -04$^{\circ}$4497 183416-0448.8 1 8.70 +0.45 - B2 II (5) ALS 9749, in the CoRoT field
171344 -13$^{\circ}$5039 183457-1352.2 1 9.52 +0.29 - B2 Ia (4) ALS 9758
172140 -29$^{\circ}$5634 183948-2920.4 5 9.95 -0.05 -0.89 B1 II (3)  
172427 -10$^{\circ}$4749 184032-1043.1 1 9.46 +0.48 -0.44 B0.5/1 Ib (5) ALS 9832, in Sct OB2
173006 -05$^{\circ}$4737 184326-0546.8 1 10.03 +0.27 -0.55 B0.5 IV (5) ALS 9902, in the CoRoT field
173502 -30$^{\circ}$5678 184656-2957.6 4 9.73 -0.10 -0.91 B1/2 Ib (3) halo star
178987 -47$^{\circ}$9208 191259-4709.7 1 9.83 - - B2 II (2)  


180032

-14$^{\circ}$5352 191531-1355.1 2 9.49 -0.07 - B2 III/IV (4) ALS 10219
186610 -03$^{\circ}$4698 194527-0309.1 4 9.67 -0.01 -0.77 B2 Ib/II (5) ALS 10480, in the CoRoT field
187536 -28$^{\circ}$7032 195125-2813.5 1 9.46 -0.08 -0.86 B3 II (3)  


3 The results

In total, 103 $\beta $ 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).

3.1 Detected modes

With a detection threshold typical for one-site ground-based data, up to several modes were detected in a single $\beta $ Cephei star. Currently, the largest number of independent modes, fourteen, was observed in $\nu$ Eridani as a result of a large photometric campaign (Jerzykiewicz et al. 2005). Another $\beta $ Cephei star with large number of detected modes, namely eleven, is 12 (DD) Lacertae (Handler et al. 2006). A histogram showing the number of detected modes in our sample of the 103 new $\beta $ Cephei stars is shown in Fig. 15. In total, 198 independent modes were detected. Up to six modes were found in a single star; there are two such objects, HD 74339 and HD 86214. Some stars with the largest number of detected modes will be discussed in Sect. 3.3. The detection threshold, DT, defined as four times the average amplitude in the Fourier periodogram of the residuals in the range 0-40 d-1, is shown with open circles in Fig. 16 and listed in Table 2. Typically, it amounts to 3-5 mmag. On the other hand, the standard deviation of the residuals, RSD, which can be regarded as the mean accuracy of a single measurement, equals to 10-15 mmag, depending on the magnitude (Fig. 16, see also Table 2). In addition, it can be seen from Fig. 16 that all but several stars have V magnitudes in the range between 8 and 10, i.e., are quite bright. The brightest $\beta $ Cephei-type star we found, at magnitude V = 7.19, is HD 149100.

3.2 Amplitudes and periods


  \begin{figure}
\par\includegraphics[width=6.7cm,clip]{8581f15.eps}\end{figure} Figure 15: The histogram of the number of detected modes for the 103 new $\beta $ Cephei-type stars.


  \begin{figure}
\par\includegraphics[width=6.7cm,clip]{8581f16.eps}\end{figure} 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 $\beta $ Cephei stars, plotted against their V magnitude. Detection theshold was defined as corresponding to ${\it S/N} = 4$.

Among stars listed in the review paper of Stankov & Handler (2005), the well-known $\beta $ 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$^{\circ}$2707, a harmonic of the main mode, an indication of non-sinusoidal light curve, was detected. In our list of newly discovered $\beta $ Cephei stars there is another star with an exceptionally large amplitude, HD 173006.

  \begin{figure}
\par\includegraphics[width=8.3cm,clip]{8581f17.eps}\end{figure} Figure 17: V-filter semi-amplitude of the main mode, $A_{\rm V, main}$, plotted as a function of the period of this mode, $P_{\rm main}$. Black dots denote $\beta $ Cephei stars listed by Stankov & Handler (2005); $\alpha $ Vir and $\omega ^1$ Sco are not plotted. Stars discovered by Handler (2005) and Pigulski (2005) are shown with asterisks, and those listed in Table 1, as open squares. The four stars discussed in the text are labelled.

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 $\beta $ 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 $\beta $ Cephei stars.

There were ten known $\beta $ 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 $\hbox{$^\prime$ }$ 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 $\chi$ 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 $\beta $ 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.

3.3 Multiplicity and splittings

As mentioned in Sect. 3.1 (see also Fig. 15), about half of the new $\beta $ Cephei stars are multiperiodic. In order to show how the modes are spread over the frequencies, in Fig. 19 we plot the differences, $\Delta f$, between frequency of a given mode, $f_{\rm i}$, 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 $\Delta f$ is usually small in comparison with f1 and the value of $\vert\Delta f\vert/f_1$ 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 $f_{\rm i} = 2f_1$ line in Fig. 19. Next, we have five stars with modes that are placed below $f_{\rm i} = f_1$/2 line (asterisks in Fig. 19). We will discuss these stars in Sect. 3.4.

  \begin{figure}
\par\includegraphics[width=12cm,clip]{8581f18.eps}\end{figure} Figure 18: Light curves of three large-amplitude $\beta $ Cephei stars discovered in the ASAS-3 data and BW Vulpeculae. Continuous lines are fits including the main frequency and five lowest harmonics. For the ASAS-3 stars, the ordinate is the V magnitude, for BW Vul, differential Strömgren b magnitude. Observations of BW Vul were taken from the 1982 campaign data (Sterken et al. 1986).

Rotational splittings are observed in some $\beta $ Cephei stars. Good examples are $\nu$ Eri (Jerzykiewicz et al. 2005), V836 Cen (Aerts et al. 2004), and $\theta$ 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 $\ell$ 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 $\beta $ 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 $\ell = 1$ or 2 modes. This, however, needs to be verified by mode identification, as was done for 12 Lac.

  \begin{figure}
\par\includegraphics[width=8cm,clip]{8581f19.eps}\end{figure} Figure 19: The difference, $\Delta f$ = $f_{\rm i} - f_1$, where $f_{\rm i}$ is the frequency of a given mode and f1, the frequency of the main mode, for 49 multiperiodic $\beta $ Cephei stars discovered in this paper. Low-frequency modes (see Sect. 3.4) are shown as asterisks. In addition, long-period modes for HD 133823 (Paper I) are shown with open circles.


 

 
Table 3: Possible rotational splittings for seven stars from our sample. Designation of frequencies is the same as in Table 2.

Star
$\Delta f$ Splitting [d-1] Note
HD 74339 f3-f5 0.01690(4) quadruplet
  f4-f3 0.01673(4)  
  f6-f4 0.01669(4)  
HD 86214 f2-f5 0.00468(5) quadruplet
  f3-f2 0.00505(4)  
  f4-f3 0.00495(4)  
HD 94065 f5-f3 0.00155(4) triplet
  f2-f5 0.00139(4)  
HD 98260 f3-f2 0.03716(4) triplet
  f1-f3 0.03386(4)  
HD 168750 f3-f2 0.01833(2) triplet
  f1-f3 0.01838(4)  
HD 173502 f3-f4 0.17543(9) triplet
  f1-f3 0.16308(3)  
HD 186610 f1-f3 0.03871(4) triplet
  f4-f1 0.03863(5)  


3.4 Stars with long periods

The longest periods observed in Galactic $\beta $ 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 $\beta $ 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 $\beta $ Cephei stars, $\nu$ 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 $\beta $ 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 $\beta $ index (Johansson 1981; Klare & Neckel 1977; Kaltcheva 2003; Moffat & Vogt 1975) and H$\alpha $ photometry (McSwain & Gies 2005).


  \begin{figure}
\par\includegraphics[width=17cm,clip]{8581f20.eps}\end{figure} Figure 20: Schematic frequency spectra in the vicinity of the possible rotationally split modes of seven new $\beta $ Cephei stars. For all stars but HD 173502 the frequency range shown is equal to 0.1 d-1. Modes which are not components of the suggested multiplets are plotted with dashed lines. See also Table 3.


 

 
Table 4: Stars with periods longer than 0.4 d.
  Short Long  
Star period [d] period [d] Note
HD 99205 0.26161 0.80203  
HD 101794 0.22447 0.54362 V916 Cen, Be
HD 116827 0.22429 0.45217 Be
HD 117357 0.15291 0.48052 Be
HD 122831 0.19968 0.54730  


HD 101794 was discovered as variable by Hipparcos and was subsequently named V916 Cen. The star was assigned the variability type of $\gamma$ 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 $\beta $ Cephei domain ( P = 0.22447 d) and this is the reason for including the star in the list of $\beta $ Cephei stars. Another periodicity, with a period of about 0.54362 d, can be attributed to a $\lambda$ 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$\beta $ line may be partially filled in, a clear indication of a weak emission.

The third new $\beta $ 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$\beta $ is confirmed by two measurements of the $\beta $ 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 $\beta $ 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.

3.5 Period and amplitude changes

Period and amplitude changes are observed in some $\beta $ 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 $\beta $ 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 ${\rm d}P_2/{\rm d}t = 104 \pm 8$ s century-1. This is the fastest change of period ever detected in a $\beta $ Cephei-type star. Times of maximum light for both modes of HD 168050 are given in Table 5.


  \begin{figure}
\par\includegraphics[width=8cm,clip]{8581f21.eps}\end{figure} 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.


 

 
Table 5: Time of maximum light for both modes detected in HD 168050.
$T_{\rm max,1}$ $T_{\rm max,2}$
[HJD 2450000.0+]
2047.1099(20) 2047.0437(33)
2142.0830(33) 2142.0758(40)
2434.5649(21) 2434.5908(33)
2819.8627(12) 2819.8428(18)
2874.6522(18) 2874.5004(32)
3135.9806(26) 3135.9672(59)
3190.9553(18) 3191.0019(19)
3520.4374(29) 3520.4664(39)
3613.9949(28) 3613.9773(51)


As far as the long-term amplitude changes are concerned, we found no clear evidence for them among the newly discovered $\beta $ Cephei stars.

3.6 O-type stars

Although B0 is the earliest spectral type of known $\beta $ Cephei stars, from the theoretical point of view the instability strip of $\beta $ Cephei stars extends to O-type stars (see, e.g., Pamyatnykh 1999). The searches for $\beta $ 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 $\zeta$ Oph (Vogt & Penrod 1983; Kambe et al. 1990). They were usually attributed to pulsations in modes with relatively high $\ell$, undetectable in photometry. A recent MOST satellite photometry of $\zeta$ Oph (Walker et al. 2005a) clearly revealed $\beta $ Cephei-type pulsations. It is therefore reasonable to regard $\zeta$ Oph and several other late O-type stars showing non-radial pulsations in line profiles (Balona & Dziembowski 1999; Fullerton et al. 1996) as $\beta $ Cephei stars.

Among the new $\beta $ 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.

3.7 Components of detached eclipsing binaries

If a $\beta $ 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 $\beta $ 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), $\eta$ Ori (Kuntz & Stebbins 1916; Waelkens & Lampens 1988; De Mey et al. 1996), and $\lambda$ 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.

3.7.1 HD 101794 = ALS 2460 = HIP 57106 = V916 Cen = Stock 14-13

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 $\beta $ Cephei stars in eclipsing systems.
HD $P_{\rm orb}$ [d] HJD of $T_{\rm min,0}$ Remarks
101794   1.4632361(21) 2450561.9213(15) V916 Cen, Be star, member of Stock 14
101838   5.41166(7) 2452014.633(13) member of Stock 14
167003 10.79824(11) 2452692.824(11) V4386 Sgr
168050   5.02335(6) 2452096.224(10)  



  \begin{figure}
\par\includegraphics[width=7.7cm,clip]{8581f22.eps} \end{figure} 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 $H_{\rm p}$ data (crosses). The long-term changes and the contribution from pulsation were removed.

3.7.2 HD 101838 = ALS 2463 = Stock 14-14
HD 101838 is also a member of the same cluster, Stock 14. Like in V916 Cen, presumably the primary component is a $\beta $ Cephei-type star. The pulsation period revealed from the ASAS-3 photometry is quite long, amounting to 0.31973 d. The star is classified as B1 III (Walker 1963; Feast et al. 1961), B0.5/1 III (Houk & Cowley 1975), B1 II-III (Garrison et al. 1977), or B0 III (FitzGerald & Miller 1983).

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.


  \begin{figure}
\par\includegraphics[width=7.7cm,clip]{8581f23.eps} \end{figure} 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.


  \begin{figure}
\par\includegraphics[width=7.8cm,clip]{8581f24.eps} \end{figure} 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.

3.7.3 HD 167003 = ALS 4801 = HIP 89404 = V4386 Sgr

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 $\beta $ 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).

3.7.4 HD 168050
The fourth $\beta $ Cephei star we discovered in an eclipsing system is HD 168050. From the analysis of the ASAS-3 data we found two periodic terms with frequencies 5.549 and 5.251 d-1, certainly coming from pulsations. It is interesting to note that the first mode shows large period increase (see Sect. 3.5), a phenomenon which is rather rare among $\beta $ Cephei stars. The eclipsing light-curve of this star is shown in Fig. 25. The orbital period is equal to 5.02335 d and the eclipses are rather shallow. The depth of the secondary minimum is about 1/3 of that of the primary one which indicates that the secondary component is relatively massive. This also means that the contribution of the secondary to the spectrum of the system is significant and may explain why the spectral type given by Houk & Smith-Moore (1988), B3/5 Ib, is slightly too late for a $\beta $ Cephei-type star.


  \begin{figure}
\par\includegraphics[width=7.8cm,clip]{8581f25.eps} \end{figure} 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.

3.8 Distribution in Galactic coordinates

Since $\beta $ Cephei stars are very young, we expect to find them rather close to the Galactic plane. As discussed by Pigulski (2005), the known stars of this type are indeed located at low Galactic latitudes, except for a few nearby stars and an interesting high-latitude star, HN Aqr (Lynn et al. 2002; Waelkens & Rufener 1988). A strip of stars belonging to the Gould Belt could be also identified. However, the observed distribution was biased due to observational selection effects. The homogeinity of the ASAS-3 data and the Michigan catalogues allows studying this distribution quantitatively. As can be seen in Fig. 26, the new members of the $\beta $ Cephei family are distributed very unevenly in Galactic coordinates: they tend to form at least three large groups. The largest group, with a center approximately at (l, $b) = (300^\circ$, 0$^{\circ}$) agrees with the direction in which we look along the Sagittarius-Carina spiral arm. We postpone a detailed discussion of this distribution until a future paper, in which the data for the remaining $\beta $ Cephei stars will be given. We just indicate here that there are several stars with quite large Galactic latitudes which, taking into account their absolute magnitudes and low reddenings, are situated at large distances both from the Sun and from the Galactic plane. Their distances might be comparable to the distance of the Galactic center, while the distance from the Galactic plane might be as large as 1 kpc or even larger.
  \begin{figure}
\includegraphics[width=12cm,clip]{8581f26.eps}\end{figure} Figure 26: Distribution of $\beta $ Cephei stars in Galactic coordinates. Only stars with V magnitudes between 7 and 11 mag are shown. Open circles denote stars from Stankov & Handler (2005), filled circles, stars found in the ASAS-3 data. "NP'' and "SP'' indicate the northern and southern celestial pole, respectively. Dashed line is the celestial equator.

3.9 Stars in open clusters and associations

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 $\beta $ 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 $\beta $ 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 $\beta $ Cephei stars in clusters and their distribution in the Galaxy will be discussed in the next paper of the series.

3.10 Hipparcos stars

The original work on Hipparcos data resulted in the discovery of six $\beta $ 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 $\beta $ 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$^{\circ}$, 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.
    ASAS V $f_{\rm Hipp}$ $A_{\rm Hipp}$ $f_{\rm ASAS}$ $A_{\rm ASAS}$ S/N DT  
HIP HD(E) name [mag] [d-1] [mmag] [d-1] [mmag]   [mmag] Remarks

29429
42597 061159+0723.5 7.04 10.67562 6.7 - - - 8.0  
30393 44597 062329+2023.5 9.04 3.25095 9.9 - - - 7.3  
35355 56847 071810-1537.7 8.92 10.68006 26.4 - - - 10.3 MU CMa
36727 60308 073313-1527.2 8.20 11.20005 16.9 - - - 9.1  
38896 65658 075738-4635.6 7.23 11.76946 7.2 - - - 4.3  
40268 68962 081323-3618.7 7.34 4.83740 7.6 4.76251 7.4 6.9 4.3 new $\beta $ Cephei star
46876 82830 093309-4645.9 9.23 7.35793 16.9 - - - 9.2  
48652 86085 095519-3845.8 8.93 7.85499 11.6 7.87529 9.2 9.4 3.9 new $\beta $ Cephei star
50598 89767 102012-5236.1 7.21 11.08927 12.6 - - - 8.4 V342 Vel
55499 306387 112159-6101.8 9.58 4.80836 31.6 4.80836 34.5 26.5 5.2 new $\beta $ Cephei star,
            4.99402 14.6 11.2   V906 Cen
62115 311884 124351-6305.2 10.82 11.41452 40.3 0.16028 52.9 19.8 10.7 CD Cru (E), W-R star
63489 112842 130031-6022.5 7.07 11.26044 8.4 - - - 7.1  
67060 119608 134431-1756.2 7.50 10.55676 13.8 - - - 7.9  
69847 124788 141742-6047.3 8.98 0.45821 52.8 0.22917 70.5 97.8 5.6 V999 Cen (E or Ell)
        9.13446 21.0 - - -    
70228 125545 142204-5817.4 7.42 11.50208 14.9 - - - 7.7  
76642 137179 153903-8314.0 8.75 10.08788 13.0 - - - 4.0  
80408 147421 162445-5327.8 9.02 5.35481 25.1 5.35473 27.1 19.0 2.8 new $\beta $ Cephei star
81216 149100 163521-5338.9 7.20 5.16114 6.0 5.16118 8.1 7.7 3.8 new $\beta $ Cephei star
83603 154043 170519-4704.1 7.08 11.17594 15.8 - - - 9.7 V863 Ara
91822 173003 184318-0138.7 7.68 7.98590 9.1 - - - 3.2  
98807 339483 200401+2616.3 8.94 3.72410 23.4 3.72413 22.5 14.0 6.4 new $\beta $ Cephei star
99327 191531 200940+2104.7 8.35 6.08588 26.5 6.08589 26.0 12.2 8.6 $\beta $ Cephei (Handler 2005)


Of these 22 stars, only seven can be classified as $\beta $ Cephei stars. One, HD 191531, was already discovered by Handler (2005), see also Paper I. The remaining six are new $\beta $ 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 $\beta $ 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 $\Delta f = f_{\rm ASAS} - f_{\rm Hipp} =
-$0.0749 and +0.0203 d-1, respectively. This can be explained in terms of aliasing in the periodograms of Hipparcos data.

4 Discussion and conclusions

According to theory (see, e.g., Pamyatnykh 1999), for the zero-age main-sequence models of massive stars, acoustic (p) and gravity (g) modes separate very well in frequency. This separation is not so good for evolved stars because in the course of the main-sequence evolution frequencies of g modes increase and eventually replace those of p modes through avoided crossing (Dziembowski & Pamyatnykh 1993). Such modes have a "mixed'' character: of a p mode in the envelope and of a g mode in the stellar interior. When only unstable modes are considered, however, the separation in frequency of p and g modes is, for a given model, preserved. Pulsations in p modes and mixed modes are attributed to $\beta $ Cephei-type variability, whereas those in g modes, to the SPB type. As $\beta $ Cephei stars populate mainly the later stages of main-sequence evolution, mixed modes are expected to be excited in these stars.

Theoretical calculations show also (Pamyatnykh 1999) that $\beta $ 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 $M_\odot$. 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 $\beta $ Cephei stars are known to rotate fast. The region of $\beta $ 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 $\lambda$ 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 $\beta $ 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 $\beta $ Cephei stars, $\nu$ Eri (Jerzykiewicz et al. 2005) and 12 Lac (Handler et al. 2006). In the ASAS-3 data (Sect. 3.4), we found five $\beta $ Cephei stars in which low-frequency modes were detected. In addition, another $\beta $ 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 $\beta $ Cephei and SPB star. Mode identification becomes a neccessity if we want to classify stars pulsating in p modes as $\beta $ Cephei stars, while those pulsating in g modes, as SPB stars.

The other important results that come from the discovery of 103 $\beta $ Cephei stars can be summarized as follows:

1.
The number of known $\beta $ Cephei stars has grown to over 200 and thus some statistical studies become possible. The sample of new stars is particularly well suited for this purpose because the stars were selected and observed in a homogeneous way.
2.
From the new sample, a selection of excellent targets for asteroseismology can be done. These would include stars with large amplitudes (Sect. 3.2), large number of modes, equidistant multiplets (Sect. 3.3) and components of eclipsing binaries (Sect. 3.7).
3.
We have found three O-type $\beta $ Cephei stars (Sect. 3.6); this type of pulsation was also found in $\zeta$ Oph from the MOST data (Walker et al. 2005a). Thus, we may conclude that $\beta $ Cephei-type instability extends towards O-type stars, but seems to be confined to very late subtypes (O8-09). This still does not agree well with the theory because calculations do not predict an upper luminosity limit for p-mode instability (Pamyatnykh 1999). However, these calculations have not included the effect of stellar wind which may stabilize pulsations for hotter O-type stars.
4.
The very recent stability calculations using new opacities (Miglio et al. 2007) indicate a much wider region in the H-R diagram where hybrid, $\beta $ Cephei/SPB-type behaviour, should be observed. The inclusion of fast rotation seems to have a similar effect (Townsend 2005). Observationally, this fact is confirmed by the growing number of detections of hybrid stars, including five $\beta $ Cephei stars with long periods we found (Sect. 3.4) as candidates. In order to verify their hybridity, mode identification is needed. A detailed study of these stars may allow testing the physics used in calculations of the evolutionary models of massive stars but also in the theoretical predictions of their pulsational stability.
Finally, it is interesting to note that four stars from our sample, HD 48553, 171305, 173006, and 186610 are located within the "CoRoT eyes'' (Baglin et al. 2002) and, if selected for observations by this satellite, could be studied in unprecedented detail.

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.

References

 

  
5 Online Material


 

 
Table 2: Parameters of the sine-curve fits to the V magnitudes of new $\beta $ Cephei-type stars listed in Table 1. $N_{\rm obs}$ is the number of observations, the initial epoch T0 is equal to 2 450 000.0. The other parameters are the following: $T_{\rm max}^i$, time of maximum light for the ith mode, $\sigma _{\rm res}$, standard deviation of the residuals, DT, detection threshold.
      $f_{\rm i}$ Ai $T_{\rm max}^i - T_0$ $\sigma _{\rm res}$ DT
Star name Freq. $N_{\rm obs}$ [d-1] [mmag] [d] [mmag] [mmag]
HD 46994 f1 322 3.90041(4) 7.8(10) 2942.1701(54) 12.8 5.1
HD 48553 f1 215 5.59806(4) 9.1(10) 3143.6502(31) 10.2 4.9
HD 67600 f1 375 3.78661(2) 8.8(08) 2901.9390(35) 10.2 3.8
HD 68962 f1 191 4.76251(6) 7.4(09) 3069.0758(38) 8.4 4.3
HD 69016 f1 616 5.01186(4) 6.4(09) 2816.8526(46) 15.3 4.4
HD 69824 f1 351 6.06354(4) 5.2(07) 2826.1460(37) 9.5 3.6
HD 73568 f1 576 4.54531(3) 4.8(06) 2865.8111(42) 9.7 2.9
  f2   6.58022(5) 3.4(06) 2865.6858(41)    
HD 74339 f1 432 5.220103(10) 27.7(09) 2900.6750(10) 13.1 4.5
  f2   5.195216(13) 20.7(09) 2900.7085(14)    
  f3   5.22221(2) 13.7(09) 2900.6380(21)    
  f4   5.23894(3) 11.5(09) 2900.6309(25)    
  f5   5.20531(3) 10.6(09) 2900.6775(26)    
  f6   5.25563(3) 10.3(09) 2900.6234(27)    
HD 77769 f1 373 5.46831(4) 5.5(08) 2849.0965(46) 11.5 4.2
HD 86085 f1 379 7.87529(2) 9.2(08) 2840.1421(17) 10.5 3.9
HD 86214 f1 512 4.442908(13) 14.3(08) 2958.9401(20) 11.5 3.6
  f2   4.40462(2) 10.9(07) 2959.0537(24)    
  f3   4.40967(3) 8.3(07) 2958.9773(32)    
  f4   4.41462(3) 9.0(07) 2958.9914(29)    
  f5   4.39994(4) 6.3(08) 2958.8671(42)    
  f6   4.44618(4) 5.7(08) 2959.0029(48)    
HD 86248 f1 395 8.25590(5) 5.5(08) 2835.6249(29) 11.4 4.2
HD 87592 f1 790 5.15127(2) 6.9(06) 2828.1611(26) 11.3 2.8
  f2   5.09753(3) 6.8(06) 2828.1263(26)    
  f3   5.43571(3) 6.3(06) 2828.1232(27)    
  f4   5.30697(4) 4.1(06) 2828.1605(43)    
  f5   5.33044(6) 2.9(06) 2828.1757(60)    
HD 88844 f1 373 5.37589(3) 7.5(07) 2881.4701(27) 9.6 3.5
  f2   6.03797(3) 5.9(07) 2881.4999(31)    
HD 90075 f1 371 4.09526(3) 10.3(09) 2902.7893(34) 12.2 4.5
HD 90987 f1 368 4.702781(07) 39.6(10) 2873.8688(08) 13.2 4.9
  f2   4.56652(2) 16.1(10) 2874.0208(21)    
  f3   4.59644(3) 8.7(10) 2873.8866(39)    
  f4   4.36623(4) 6.7(10) 2873.9638(54)    
HD 91651 f1 525 7.38876(3) 5.6(06) 2876.1314(23) 9.7 3.0
  f2   7.10851(5) 3.5(06) 2876.1737(38)    
HD 92291 f1 385 5.528817(10) 23.3(09) 2884.2608(11) 11.8 4.2
  f2   5.454284(13) 17.5(09) 2884.2939(15)    
  f3   5.90508(3) 8.9(09) 2884.3169(26)    
  f4   5.46980(3) 7.4(09) 2884.2436(34)    
  f5   5.72446(4) 6.2(08) 2884.2426(40)    
HD 93113 f1 690 5.57541(5) 3.7(06) 2856.9991(46) 11.2 3.1
HD 93341 f1 691 5.08749(3) 8.2(07) 2881.2753(24) 12.1 3.3
HD 94065 f1 364 4.810101(10) 20.3(08) 2861.4725(13) 10.3 3.8
  f2   5.02213(3) 11.1(08) 2861.4386(24)    
  f3   5.01919(2) 13.5(08) 2861.5756(19)    
  f4   5.48660(3) 9.3(08) 2861.4498(24)    
  f5   5.02074(3) 8.5(08) 2861.4767(30)    
HD 94345 f1 487 5.16834(2) 9.4(07) 2994.2366(23) 10.6 3.4
  f2   5.17063(4) 5.4(07) 2994.3449(39)    
  f3   5.57486(5) 3.8(07) 2994.2818(53)    
HD 94900 f1 468 4.842766(11) 16.8(08) 2930.6143(14) 11.2 3.7
HD 95568 f1 365 6.152355(15) 16.9(10) 2857.4896(15) 12.7 4.7
  f2   6.13549(3) 10.4(10) 2857.4369(24)    
HD 96882 f1 355 6.22739(4) 6.6(09) 2909.9008(33) 11.3 4.3
HD 96901 f1 340 4.163209(11) 19.2(08) 2900.2036(16) 10.1 3.9
  f2   4.128028(17) 11.4(08) 2900.2624(27)    
HD 97629 f1 366 5.178579(17) 13.3(08) 2920.9323(19) 11.0 4.1
HD 98260 f1 350 4.514510(19) 14.2(09) 2896.2087(23) 12.0 4.6
  f2   4.44349(3) 9.8(09) 2896.1907(34)    
  f3   4.48065(3) 10.3(09) 2896.0648(31)    
HD 99024 f1 406 7.03125(4) 7.0(08) 2992.2193(28) 12.0 4.2
HD 99205 f1 645 3.822544(10) 18.1(07) 2882.5932(16) 12.3 3.5
  f2   1.24684(4) 5.7(07) 2882.334(16)    
HD 100355 f1 670 7.507394(15) 10.3(06) 2865.7310(13) 10.9 3.0
  f2   7.112278(16) 10.2(06) 2865.7452(13)    
  f3   6.93375(4) 4.2(06) 2865.6535(32)    
HD 101794 f1 311 4.45140(3) 14.6(13) 2737.1557(31) 15.4 6.2
  f2   1.83951(4) 11.2(13) 2736.998(10)    
HD 101838 f1 352 3.12760(3) 10.3(09) 2865.5247(45) 11.8 4.9
HD 102505 f1 332 4.750770(15) 13.7(08) 2865.3997(19) 9.9 3.9
  f2   4.52947(4) 5.8(08) 2865.4186(47)    
HD 103007 f1 346 5.707239(18) 12.2(09) 2849.9655(20) 11.2 4.2
  f2   5.75454(3) 10.5(09) 2849.9456(23)    
  f3   5.67467(3) 9.9(09) 2849.9219(25)    
HD 103320 f1 351 4.71222(2) 8.0(08) 2894.0787(32) 9.8 3.7
HD 103764 f1 330 5.582626(18) 12.2(09) 2859.0861(20) 10.9 4.3
HD 104257 f1 321 6.868277(11) 20.6(09) 2852.5829(10) 11.0 4.4
HD 104465 f1 330 5.518702(17) 14.8(10) 2862.6886(19) 12.2 4.8
  f2   5.395199(19) 14.2(10) 2862.7541(20)    
HD 104795 f1 330 6.23215(4) 5.3(07) 2883.9586(31) 8.4 3.3
HD 106345 f1 440 6.612477(12) 15.0(07) 2843.0066(11) 10.2 3.4
HD 108628 f1 637 6.74262(4) 4.9(06) 2867.9268(30) 10.9 3.1
HD 108769 f1 317 7.54085(4) 5.4(08) 2816.7267(32) 10.1 4.0
HD 110498 f1 325 4.15383(2) 10.3(09) 2875.1748(30) 10.5 4.1
HD 111377 f1 342 8.83122(4) 6.4(09) 2933.8111(25) 11.4 4.4
HD 111578 f1 344 4.71676(3) 8.8(09) 2914.2855(34) 11.7 4.5
HD 113013 f1 393 6.47119(3) 9.5(08) 2986.8716(22) 11.7 4.2
  f2   6.26890(4) 6.4(08) 2986.8920(34)    
HD 114444 f1 508 4.81618(4) 8.0(10) 2709.0849(43) 16.3 5.1
  f2   5.11817(5) 6.6(10) 2709.1424(49)    
HD 114733 f1 620 7.24916(3) 8.3(07) 2854.8118(19) 12.4 3.5
HD 115533 f1 330 14.57715(3) 11.8(11) 2869.9716(10) 14.0 5.5
HD 116538 f1 365 4.52246(3) 10.6(11) 2859.5868(36) 14.4 5.4
HD 116827 f1 555 2.21158(3) 12.5(09) 2968.2039(52) 15.0 4.5
  f2   4.45852(3) 10.4(09) 2967.9669(31)    
HD 117357 f1 561 2.08106(3) 8.8(07) 2967.5187(57) 11.0 3.3
  f2   6.53990(4) 6.2(07) 2967.7211(26)    
HD 117687 f1 515 6.17482(3) 6.8(07) 2944.0268(25) 10.6 3.3
HD 117704 f1 559 4.65537(3) 8.4(08) 2971.8997(34) 13.8 4.2
HD 119252 f1 326 8.78623(3) 13.3(11) 2863.9353(14) 13.5 5.3
HD 119910 f1 314 7.03488(5) 6.9(07) 3161.7560(24) 9.2 3.7
  f2   5.95546(6) 4.6(07) 3161.7249(43)    
HD 122831 f1 462 5.008025(17) 14.9(09) 3023.4327(19) 12.7 4.1
  f2   1.82715(5) 4.9(08) 3023.337(15)    
HD 123077 f1 444 7.043592(14) 23.6(11) 2811.6284(10) 15.7 5.3
  f2   6.95371(3) 10.2(10) 2811.6703(25)    
  f3   6.62910(4) 9.8(11) 2811.5793(27)    
  f4   7.70277(6) 6.4(11) 2811.5844(35)    
HD 126357 f1 516 4.06927(3) 8.4(09) 2754.2463(38) 13.1 4.1
  f2   8.54271(4) 8.1(08) 2754.1686(19)    
  f3   8.07010(4) 7.8(08) 2754.0913(21)    
HD 131805 f1 546 7.38299(4) 5.9(08) 2808.2366(28) 12.8 3.9
HD 132320 f1 377 8.44635(3) 7.6(09) 2808.8232(22) 12.1 4.4
HD 137405 f1 677 4.334276(15) 11.3(06) 2924.5163(19) 10.9 2.9
HD 142754 f1 289 8.51115(5) 6.8(10) 2880.1249(28) 11.9 5.0
HD 145537 f1 284 5.481110(17) 22.9(13) 2849.0793(17) 15.3 6.5
  f2   5.18768(3) 16.4(13) 2849.0567(24)    
HD 146442 f1 328 6.57248(3) 9.1(09) 2899.1253(22) 10.7 4.3
  f2   6.76650(4) 6.0(09) 2899.0557(33)    
  f3   5.50073(5) 5.4(08) 2899.0582(46)    
HD 147421 f1 642 5.354726(06) 27.1(06) 2899.7481(06) 9.9 2.8
HD 149100 f1 284 5.16118(4) 8.1(08) 3128.9118(30) 9.2 3.8
HD 150927 f1 328 4.834676(15) 24.7(11) 2916.1050(16) 14.5 5.7
  f2   4.854070(16) 22.4(12) 2916.1120(17)    

HD 151158

f1 307 5.501130(17) 17.5(10) 2892.7554(17) 12.4 5.3
HD 152060 f1 303 9.57323(3) 8.5(08) 2884.4547(17) 10.3 4.2
  f2   12.19261(3) 8.8(08) 2884.4692(12)    
HD 152162 f1 490 6.031971(06) 33.1(06) 2867.8221(05) 9.7 3.3
  f2   6.02169(2) 8.6(06) 2867.7874(19)    
HD 152372 f1 479 8.64280(3) 8.6(07) 2840.2601(15) 10.6 3.5
  f2   8.33283(4) 5.7(07) 2840.2841(23)    
  f3   8.68004(5) 4.4(07) 2840.3162(28)    
HD 153772 f1 351 3.275788(10) 23.9(08) 2874.3683(16) 10.8 4.1
HD 154500 f1 911 6.98730(3) 8.6(06) 2991.7359(17) 13.1 3.6
  f2   7.05945(3) 7.9(06) 2991.8199(18)    
HD 155407 f1 319 5.552652(09) 28.9(09) 2865.0140(09) 11.2 4.4
HD 156172 f1 294 6.97258(3) 10.8(10) 2909.6293(21) 12.4 5.1
HD 156321 f1 631 8.72485(5) 4.0(05) 3098.6986(22) 8.3 2.5
HD 159792 f1 536 7.000049(10) 25.7(09) 2801.4000(08) 14.7 4.5
  f2   7.24311(3) 8.4(09) 2801.3910(24)    
  f3   6.91847(5) 5.6(09) 2801.3297(37)    
HD 161633 f1 332 6.10395(2) 12.8(10) 2828.7628(21) 12.9 5.0
  f2   6.26392(3) 11.4(10) 2828.6801(23)    
  f3   5.90006(3) 10.6(10) 2828.6718(26)    
  f4   5.60499(5) 5.9(10) 2828.7392(49)    
HD 164188 f1 413 5.71220(4) 5.8(07) 2903.4761(30) 9.3 3.3
HD 164741 f1 474 5.119632(19) 13.9(08) 2846.7981(19) 12.0 3.9
  f2   5.16521(2) 12.0(08) 2846.8063(20)    
  f3   5.56809(3) 8.6(08) 2846.8316(27)    
  f4   5.12946(4) 6.6(08) 2846.6758(38)    
  f5   4.96110(5) 5.1(08) 2846.7909(51)    
HD 165955 f1 762 11.906129(19) 11.0(06) 3383.4615(07) 10.9 3.2
  f2   10.16581(4) 7.4(06) 3383.4489(12)    
HD 166304 f1 633 7.03862(3) 5.9(06) 2888.9596(20) 9.3 2.7
  f2   6.33937(6) 3.3(06) 2888.9669(39)    
  f3   7.55353(6) 3.3(06) 2888.8784(33)    
HD 167003 f1 758 6.77267(3) 10.5(06) 3395.4748(13) 10.8 3.2
  f2   7.54580(4) 6.8(06) 3395.5124(18)    
  f3   7.01603(4) 6.2(06) 3395.4349(21)    
  f4   5.37835(4) 5.7(06) 3395.5481(29)    
HD 167451 f1 330 4.37474(3) 11.5(09) 2849.3065(29) 11.2 4.4
HD 168015 f1 349 6.324050(17) 12.4(07) 2830.9715(14) 9.0 3.4
  f2   5.07961(2) 10.1(07) 2831.0446(21)    
HD 168050 f1 698 5.5486... [var] 27.7(10) see Table 5 12.2 3.7
  f2   5.251039(15) 20.7(10) 2921.1561(15)    
HD 168675 f1 596 6.35906(2) 8.7(06) 2867.6437(17) 9.7 2.8
  f2   4.18134(4) 5.1(06) 2867.6660(42)    
HD 168750 f1 547 4.061855(12) 15.5(06) 2849.0681(16) 10.2 3.1
  f2   4.025154(19) 9.5(06) 2849.1496(26)    
  f3   4.04348(4) 5.1(06) 2849.2132(49)    
HD 169173 f1 798 5.31303(3) 6.7(07) 2883.5407(29) 13.0 3.6
HD 169601 f1 612 5.173682(11) 23.0(08) 2844.3032(10) 12.3 3.9
  f2   5.231036(18) 14.2(07) 2844.3146(16)    
  f3   5.08657(3) 8.2(07) 2844.2888(28)    
HD 171141 f1 349 11.19358(4) 7.1(07) 2845.9130(14) 9.0 3.5
HD 171305 f1 288 5.15860(2) 10.0(08) 2937.3750(24) 9.3 3.9
HD 171344 f1 316 5.41534(5) 7.5(10) 2828.6084(37) 11.8 4.7
HD 172140 f1 1346 6.61531(3) 8.8(04) 2867.4248(11) 9.5 2.1
  f2   6.29880(3) 7.8(04) 2867.3434(14)    
  f3   7.17605(4) 6.2(04) 2867.4152(14)    
  f4   6.25128(6) 4.2(04) 2867.4350(25)    
  f5   7.56117(9) 2.6(04) 2867.4188(30)    
HD 172427 f1 283 4.01969(3) 10.6(09) 2840.9159(32) 9.9 4.2
HD 173006 f1 269 5.878262(06) 87.8(18) 2892.8486(05) 20.7 9.0
  2f1   11.756524 22.9(18) 2892.7824(11)    
HD 173502 f1 1342 5.496527(07) 37.3(04) 2865.1104(04) 9.5 2.2
  f2   5.540236(15) 16.4(04) 2865.0533(07)    
  f3   5.33345(3) 8.1(04) 2865.0716(15)    
  f4   5.15802(8) 3.2(04) 2865.0158(37)    
HD 178987 f1 339 7.14660(3) 10.5(11) 2854.0577(23) 14.4 5.7
HD 180032 f1 287 6.86806(3) 8.6(08) 2820.2828(21) 9.3 3.9
  f2   7.18637(4) 5.9(08) 2820.4152(29)    
HD 186610 f1 726 5.499983(17) 15.6(06) 3023.3878(11) 10.8 2.9
  f2   5.76342(3) 13.0(06) 3023.3979(12)    
  f3   5.46127(3) 11.4(06) 3023.4022(15)    
  f4   5.53861(5) 5.3(06) 3023.5457(31)    
HD 187536 f1 285 4.58572(4) 6.7(09) 2796.7750(46) 10.7 4.5



  \begin{figure}\par\includegraphics[width=17cm]{8581f02.eps}\end{figure} Figure 2: Fourier periodograms of the ASAS-3 data of ten $\beta $ Cephei-type stars discussed in the paper: HD 46994, 48553, 67600, 68962, 69016, 69824, 73568, 74339, 77769, and 86085. Lower panels show consecutive steps of prewhitening. Frequencies of the detected modes are indicated by inverted triangles. Ordinate is the amplitude expressed in mmag.


  \begin{figure}\par\includegraphics[width=17cm]{8581f03.eps}\end{figure} Figure 3: The same as in Fig. 2, but for HD 86214, 86248, 87592, 88844, 90075, 90987, and 91651.


  \begin{figure}\par\includegraphics[width=17cm]{8581f04.eps}\end{figure} Figure 4: The same as in Fig. 2, but for HD 92291, 93113, 93341, 94065, 94345, 94900, and 95568.


  \begin{figure}\par\includegraphics[width=17cm]{8581f05.eps}\end{figure} Figure 5: The same as in Fig. 2, but for HD 96882, 96901, 97629, 98260, 99024, 99205, 100355, and 101794.


  \begin{figure}\par\includegraphics[width=17cm]{8581f06.eps}\end{figure} Figure 6: The same as in Fig. 2, but for HD 101838, 102505, 103007, 103320, 103764, 104257, 104465, 104795, and 106345.


  \begin{figure}\par\includegraphics[width=17cm]{8581f07.eps}\end{figure} Figure 7: The same as in Fig. 2, but for HD 108628, 108769, 110498, 111377, 111578, 113013, 114444, 114733, 115533, 116538, and 116827.


  \begin{figure}\par\includegraphics[width=17cm]{8581f08.eps}\end{figure} Figure 8: The same as in Fig. 2, but for HD 117357, 117687, 117704, 119252, 119910, 122831, 123077, and 126357.


  \begin{figure}\par\includegraphics[width=17cm]{8581f09.eps}\end{figure} Figure 9: The same as in Fig. 2, but for HD 131805, 132320, 137405, 142754, 145537, 146442, 147421, 149100, and 150927.


  \begin{figure}\par\includegraphics[width=17cm]{8581f10.eps}\end{figure} Figure 10: The same as in Fig. 2, but for HD 151158, 152060, 152162, 152372, 153772, 154500, 155407, 156172, and 156321.


  \begin{figure}\par\includegraphics[width=17cm]{8581f11.eps}\end{figure} Figure 11: The same as in Fig. 2, but for HD 159792, 161633, 164188, 164741, 165955, and 166304.


  \begin{figure}\par\includegraphics[width=17cm]{8581f12.eps}\end{figure} Figure 12: The same as in Fig. 2, but for HD 167003, 167451, 168015, 168050, 168675, 168750, and 169173.


  \begin{figure}\par\includegraphics[width=17cm]{8581f13.eps}\end{figure} Figure 13: The same as in Fig. 2, but for HD 169601, 171141, 171305, 171344, 172140, 172427, 173006, and 178987.


  \begin{figure}\par\includegraphics[width=17cm]{8581f14.eps}\end{figure} Figure 14: The same as in Fig. 2, but for HD 173502, 180032, 186610, and 187536.



Copyright ESO 2008