Since most of the Cepheids are believed to be in their second crossing of the
instability strip, their period of pulsation is directly related to the stellar
mass, and hence, to the main sequence life time of the star. Hence a rough
estimate of the age of the star can be obtained from the observed pulsation
period of the Cepheids. We have used the following relation given by Magnier
et al. (1997b) to estimate the age of Cepheids:
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(3) |
In Table 4, we present characteristics of these 26 Cepheid variables detected
in our study. The identification number of the star, celestial coordinate for
J2000, phase weighted mean magnitude in both R and I filters, amplitude of
variability in R filter, period, age of the Cepheid (estimated using Eq. (3))
and total number of points in R filter used for the light curve study are
given. The Cepheids are sorted in the increasing order of their periods. The
reference to variability reported in the literature and corresponding period,
if known, are listed in the last two columns. Out of the catalogued 26 Cepheids,
the variability is reported for the first time for stars V22 and V24;
moreover 13 of the variables are identified as Cepheids for the first time.
The remaining 13 Cepheids have been known from earlier studies. The present
data confirms their variability and our periods are generally in good
agreement with the reported value.
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Figure 4: Phase-magnitude diagram is plotted for 26 Cepheids detected in the present study. Filled and open circles represents R and Imagnitudes respectively. |
Star | ![]() |
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Period | Age | N | Other | Period |
ID | (deg) | (deg) | (mag) | (mag) | (mag) | (days) | (Myrs) | Identification | (days) | |
V1 | 10.9321 | 41.1970 | 20.48 | 19.98 | 0.27 | 7.459![]() |
75 | 123 | K V883 | 7.459 |
V2* | 10.8469 | 41.1737 | 20.17 | 19.69 | 0.15 | 8.566![]() |
69 | 124 | TC 170 | - |
V3* | 10.8669 | 41.2320 | 20.61 | 20.28 | 0.22 | 8.836![]() |
68 | 120 | TC 18 | - |
V4 | 10.9366 | 41.2503 | 20.28 | 19.54 | 0.11 | 9.160![]() |
67 | 86 | K V1219 | 9.173 |
V5 | 10.9721 | 41.2128 | 20.56 | 20.04 | 0.19 | 9.790![]() |
64 | 92 | K V2879 | 9.790 |
V6* | 10.8770 | 41.0601 | 20.43 | 19.76 | 0.15 | 10.383![]() |
62 | 93 | TC 76 | - |
V7* | 10.8736 | 41.2367 | 20.42 | 20.27 | 0.28 | 10.500![]() |
61 | 123 | TC 16 | - |
V8 | 10.7500 | 41.1426 | 19.89 | 19.55 | 0.17 | 11.17![]() |
59 | 95 | M 65 | 25.0![]() |
V9* | 10.8594 | 41.2004 | 20.21 | 19.60 | 0.26 | 13.773![]() |
52 | 126 | TC 20 | - |
V10* | 10.9290 | 41.1715 | 20.77 | 19.84 | 0.48 | 14.420![]() |
51 | 116 | TC 85 | - |
V11 | 10.9255 | 41.2489 | 19.57 | 18.87 | 0.16 | 15.26![]() |
49 | 96 | K V635 | 15.255 |
V12 | 10.9576 | 41.2227 | 20.84 | 20.08 | 0.32 | 15.46![]() |
49 | 89 | K V2286 | 15.464 |
V13 | 10.8259 | 41.1386 | 19.82 | 19.46 | 0.40 | 15.76![]() |
48 | 94 | M 68 | 14.0![]() |
V14* | 10.9049 | 41.2419 | 19.93 | 19.58 | 0.22 | 15.90![]() |
48 | 121 | TC 194 | - |
V15* | 10.9115 | 41.2396 | 20.79 | 19.91 | 0.30 | 15.95![]() |
48 | 126 | TC 196 | - |
V16 | 10.9775 | 41.2348 | 20.28 | 19.74 | 0.40 | 16.38![]() |
47 | 47 | K V3198 | 16.345 |
V17* | 10.9069 | 41.1868 | 20.12 | 19.60 | 0.39 | 16.60![]() |
47 | 124 | B 4614 | - |
V18 | 10.9853 | 41.2176 | 19.47 | 19.09 | 0.21 | 17.73![]() |
45 | 91 | K V3583 | 17.703 |
V19 | 10.9839 | 41.2374 | 19.83 | 19.60 | 0.32 | 17.83![]() |
45 | 18 | K V3551 | 16.699 |
V20* | 10.9526 | 41.1540 | 19.20 | 18.99 | 0.35 | 20.09![]() |
42 | 96 | TC 207 | - |
V21 | 10.8379 | 41.1514 | 19.74 | 19.31 | 0.39 | 21.44![]() |
40 | 96 | M 69 | 13.0![]() |
V22![]() |
10.8272 | 41.1071 | 20.01 | 19.19 | 0.29 | 26.99![]() |
35 | 92 | - | - |
V23* | 10.9059 | 41.2379 | 19.78 | 18.92 | 0.34 | 28.78![]() |
33 | 127 | TC 30 | - |
V24![]() |
10.9002 | 41.1823 | 20.55 | 19.57 | 0.23 | 35.1![]() |
30 | 121 | - | - |
V25 | 10.9293 | 41.2475 | 18.89 | 18.35 | 0.31 | 43.53![]() |
26 | 97 | K V836 | 43.371 |
V26 | 10.9183 | 41.1856 | 19.36 | 18.82 | 0.22 | 56.02![]() |
22 | 124 | K V164 | 56.116 |
In Fig. 4, we show the phase-magnitude diagram for all the 26 Cepheids in
both R and I filters. The I-band light curves show more scattering
particularly for short period and low amplitude Cepheids. This could arise
due to the following reason: the amplitude of Cepheids decreases with increasing
wavelength (e.g. Freedman et al. 1985) and Freedman (1988) found a
ratio of 1.00:0.67:0.44:0.34 in amplitudes of B:V:R:I filters. As
most of these Cepheids have a pulsation of 0.1-0.2 mag in Rfilter, the amplitude of pulsation in the I filter is even less and becomes
comparable to the photometric errors.
BVI photometry has been carried out by Kaluzny et al. (1999, hereafter referred to as KAL99) under the DIRECT project. Out of 35 Cepheids detected in DIRECT project in the field M 31D, 11 are located in our field of observations. We have identified 10 of them and notice that except in the case of V19, the periods determined in the two surveys are in excellent agreement. The discrepancy in the period of V19 appears to be due to inadequate data in the present study (see Table 4). One of the Cepheid (K V952) reported in KAL99 could not be detected in our data due to blending effect as this star is highly blended by a neighbouring bright red star.
For Cepheids V7, V9, V14, V15, V17, V23 and V26, the parameters given in Table 4 supersedes our earlier results given in Paper I, as these are derived using data with much longer temporal coverage.
Using a set of 32 LMC Cepheid variables, Madore & Freedman (1991) have
obtained an equation of the ridge line in P-L diagram for Cousin Rfilter as:
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(4) |
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(5) |
The apparent mean magnitudes of 26 Cepheids are plotted as a function of in Fig. 5. The slope of the straight line is fixed as -2.94 and -2.96 for
R and I filters respectively. The Cepheids V24 and V26 are located by
about 1.0-1.5 mag below the ridge line in the P-L diagram which makes them
a possible Population II Cepheid variables. Therefore, we did not consider
these two Cepheids for the zero points evaluation. Using remaining 24 Cepheids,
we found a zero points of
and
mag in R and I
filters respectively. The dashed envelope lines are drawn 0.5 mag from
the fitted line, representing the expected intrinsic scatter of P-L relation
due to the finite width of the instability strip in the H-R diagram (Sandage
1958; Sandage & Tammann 1968), blending of Cepheids as well as the range of
interstellar extinction.
The above zero points give us a mean apparent distance modulus of
and
mag in R and I filters respectively. This
yields a mean colour excess of
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(6) |
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Figure 6:
The colour-magnitude diagram for the Cepheids under discussion.
Symbols are the same as in Fig. 7. The solar metallicity isochrones by Bertelli
et al. (1994) for
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V19 -- KAL99 obtained a period of 16.999 days for this Cepheid while we
obtained a period of 17.830.03 days using 18 data points. The light curve
for this Cepheid is extremely under-sampled and poorly distributed in phase in
our data which could be the reason for discrepancy between two periods.
V22 -- It is discovered in the present study with a period of 26.960.04
days. A small bump in the falling branch can be seen in both filters.
V24 -- This is another Cepheid discovered by us. It has a period of
35.120.05 days and an exceptionally large value of (R-I) colour of 0.98
mag. In the P-L diagram, this Cepheid deviates maximum towards the fainter
side in both filters and could be a possible Population II Cepheid.
V26 -- This is the longest period Cepheid in our sample. We obtained its
period as 56.020.08 days in agreement with a period of 56.116 days
derived by KAL99. In the P-L diagram, this Cepheid is also located downwards
in both filters and it could also be a Population II type Cepheid.
Copyright ESO 2003