1 Introduction
The globular cluster Palomar 2 is a distant (30 kpc) stellar system in the direction
of the Galactic anticenter and close to the Galactic plane (
In the present paper we take advantage of an 11-year long time-series of CCD VI data, analyzed in the standard Differential Imaging Approach (DIA), to explore the light curves of nearly 500 stars in the field of view (FoV) of the cluster. We have found 21 new RR Lyrae stars (V1-V14 and SV1-SV7 in Table 1). In conjunction with the Gaia-DR3 variability index, we confirm the RRab nature of 6 more stars (G3, G11, G12, G13, G18 and G23), plus 1 RGB (G17), for a total of 28 variables in the field of view of our images. In what follows, we argue in favour of the membership of 18 of them and present their light curves and ephemerides. The mean distance and [Fe/H] of the cluster shall be calculated by the Fourier decomposition of RRab stars with the best quality light curves.
ID | Gaia variable | Type | P (d) | E |
V (mag) |
|
RA (J2000.0) | DEC (J2000.0) | PGaia (d) | Membership status | Gaia number |
---|---|---|---|---|---|---|---|---|---|---|---|
V1 | RRab | 0.542848 | 6312.3363 | 20.534 | 0.805 | 4:46:03.57 | +31:22:45.8 | M1 | 159504640014524672 | ||
V2 | G5 | RRab | 0.551396 | 5542.2114 | 21.342 | 1.056 | 4:46:04.60 | +31:23:41.5 | 0.5513624 | M1 | 159504747388302336 |
V3 | RRab | 0.554363 | 6948.4976 | 21.792 | 0.951 | 4:46:05.53 | +31:23:29.0 | M1 | 159504747388520064 | ||
V4 | G14 | RRab | 0.651889 | 5912.2228 | 21.413 | 0.814 | 4:46:05.61 | +31:23:43.2 | 0.6518656 | M1 | 159504747387726464 |
V5 | G4 | RRab | 0.511639 | 8896.2470 | 21.382 | 0.997 | 4:46:07.02 | +31:23:13.5 | 0.5067667 | M2 | 159504678667943552 |
V6 | G21 | RRab | 0.553259 | 9258.3356 | 21.461 | 1.168 | 4:46:07.82 | +31:23:07.7 | 0.5532034 | M2 | 159504678668831872 |
V7 | G16 | RRab | 0.655812 | 8407.3827 | 20.925 | 0.914 | 4:46:08.11 | +31:23:37.1 | - | M1 | 159504678667937024 |
V8 | G7 | RRc | 0.373408 | 5542.2114 | 20.757 | 0.548 | 4:46:08.06 | +31:22:21.7 | - | M1 | 159501689370744192 |
V9 | G6 | RRab | 0.629619 | 8896.1493 | 21.521 | 0.787 | 4:46:08.24 | +31:23:09.3 | 0.6129630 | M1 | 159504674373384320 |
V10 | G8 | RRab | 0.685890 | 5912.3072 | 20.700 | 0.512 | 4:46:09.11 | +31:22:38.0 | 0.6858277 | M1 | 159501723731340288 |
V11 | G19 | RRab | 0.575280 | 6222.3870 | 20.673 | 0.842 | 4:46:10.58 | +31:22:35.0 | 0.5752915 | M1 | 159501719435472896 |
V12 | G9 | RRab | 0.583630 | 6633.3246 | 20.894 | 0.603 | 4:46:12.82 | +31:22:26.3 | 0.5953860 | M1 | 159501650715992064 |
V13 | RRab | 0.546972 | 6948.4441 | 21.327 | 0.887 | 4:46:07.17 | +31:23:15.5 | M2 | 159504678668829184 | ||
V14 | G1 | RRab | 0.574697 | 6948.4591 | 21.842 | 1.610 | 4:46:07.21 | +31:22:47.2 | 0.5513435 | M2 | 159504678667961856 |
V15 | G12 | RRab | 0.508471 | 8781.4301 | 20.918 | 0.323 | 4:46:05.00 | +31:22:52.9 | - | M1 | 159504644308236672 |
V16 | G13 | RR? | 0.490213 | 5912.1144 | 19.179 | 0.330 | 4:46:04.64 | +31:22:42.0 | - | M1 | 159504644308250624 |
V17 | G17 | RGB | 19.0 | 0.9 | 4:46:02.96 | +31:23:09.2 | - | M1 | 159504708733123200 | ||
V18 | G11 | RR? | 0.510211 | 5912.1144 | 18.876 | 0.768 | 4:46:05.85 | +31:23:03.3 | - | M1 | 159504644308215808 |
SV1 | RRab | 0.588566 | 6634.1554 | 21.267 | 1.024 | 4:46:04.22 | +31:22:34.8 | UN | 159504644309111808 | ||
SV2 | RRab | 0.537325 | 8406.4629 | 21.876 | 1.299 | 4:46:06.39 | +31:23:54.0 | UN | 159504747388298112 | ||
SV3 | RRab | 0.661914 | 5868.4136 | 21.517 | 1.077 | 4:46:03.96 | +31:23:16.2 | FS | 159504713028573696 | ||
SV4 | RRab | 0.587210 | 8407.3175 | 21.585 | 1.363 | 4:46:06.56 | +31:23:27.2 | FS | 159504674373556992 | ||
SV5 | G15 | RRab | 0.490941 | 6221.4206 | 21.312 | 1.391 | 4:46:09.04 | +31:23:12.8 | 0.4909349 | FS | 159504678668828160 |
SV6 | G10 | RRab | 0.570669 | 6946.4683 | 20.840 | 0.960 | 4:46:12.31 | +31:22:45.3 | 0.5706582 | FS | 159501723731332480 |
SV7 | RRab | 0.551215 | 6634.1714 | 19.274 | 1.371 | 4:46:13.65 | +31:24:11.5 | FS | 159506190497880832 | ||
G3 | RRab | 0.531512 | 6633.3479 | 20.486 | 0.769 | 4:45:57.72 | +31:24:19.0 | 0.5242873 | FS | 159504987906469248 | |
G18 | RRab | 0.562320 | 6223.3662 | 20.700 | 0.576 | 4:46:09.50 | +31:23:01.9 | 0.5623196 | FS | 159501723732926208 | |
G23 | RRab | 0.595453 | 6633.3810 | 21.178 | 1.104 | 4:45:59.23 | +31:22:53.4 | 0.56065912 | FS | 159504609949939072 | |
G21 | 159501655012584064 | ||||||||||
G202 | 21.513 | 4:45:56.77 | +31:21:09.0 | 0.59148323 | FS | 159504128913233536 | |||||
G221 |
1Out of our FoV. 2Not measured by our photometry.
2 Observations and Data Reductions
The data were obtained between December 12, 2010 and February 12, 2021 with the 2.0-m telescope at the Indian Astronomical Observatory (IAO), Hanle, India. The detector used was a SITe ST-002 2Kx4K with a scale of 0.296 arcsec/pix, for a field of view of approximately 10.1×10.1 arcmin2. From October 14, 2018 and February 17, 2020 the detector used was a Thompson grade 0 E2V CCD44-82-0-E93 2Kx4K with a scale of 0.296 arcsec/pix, or a FoV of approximately 10.1×10.1 arcmin2. A total of 197 and 240 images were obtained in the V and I filters, respectively.
2.1 Difference Imaging Analysis
The image reductions were performed employing the software Difference Imaging Analysis (DIA) with its pipeline implementation DanDIA (Bramich 2008; Bramich 2013, Bramich 2015) to obtain high-precision photometry of all the point sources in the field of view (FoV) of our CCD. This allowed us to construct an instrumental light curve for each star. For a detailed explanation of the use of this technique, the reader is referred to the work by Bramich et al.(2011).
2.2 Transformation to the Standard System
Since two different detectors were used to achieve the observations as described in the previous section, we treated the transformation to the standard system as two independent instruments. Otherwise, the procedure was the standard one described in detail in previous publications, in summary; we used local standard stars taken from the catalog of Photometric Standard Fields (Stetson 2000) to set our photometry into the VI Johnson-Kron-Cousin standard photometric system (Landolt 1992).
The transformation equations carry a small but mildly significant colour term and
are of the form:
3 Star membership using Gaia-eDR3
We have made use of the latest data release Gaia-DR3 (Gaia Collaboration 2021) to perform a membership analysis of the stars in the field of Pal 2. To this end, we employed the method of Bustos Fierro Calder (2019), which is based on the Balanced Iterative Reducing and Clustering using Hierarchies (BIRCH) algorithm developed by Zhang et al. (1996). The method and our approach to it have been described in a recent paper by Deras et al.(2022). We recall here that our method is based on a clustering algorithm at a first stage and a detailed analysis of the residual overdensity at a second stage; member stars extracted in the first stage are labeled M1, and those extracted in the second stage are labeled M2. Stars without proper motions were retained, labeled as “unknown membership status” or UN.
The analysis was carried out for a 10 arcmin radius field centered in the cluster. We considered 1806 stars with measured proper motions, of which 407 were found to be likely members. Out of them, only 288 were in the FoV of our images, for which we could produce light curves.
From the distribution of the field stars in phase space we estimated the number expected to be located in the same region of the sky and the vector point diagram (VPD) of the extracted members; therefore, they could have been erroneously labelled as members. Within the M1 stars the resulting expected contamination is 36 (11%), and within the M2 stars it is 87 (7%); therefore, for a given extracted star its probability of being a cluster member is 89% if it is labelled M1, or 93% if it is labelled M2.
4 Differential Reddening and the CMD
Palomar 2 is a heavily reddened cluster subject to substantial differential
reddening, as it is evident in the crowded and deep HST color magnitude diagram
(CDM) shown by Sarajedini et~al.(2007). A
thorough treatment of the differential reddening in the cluster enabled Bonatto Chies-Santos(2020) to produce a
reddening map, which these authors have kindly made available to us. In Figure 2 the observed CMD and the dereddened
versions are shown. To deredden the CMD, the differential reddening map was added to
a foreground reddening of
5 The variable stars in Pal 2
No variable stars in Pal 2 have been reported thus far. The case of Pal 2 is a particularly challenging one since the cluster is not only distant, but it is also behind a heavy dust curtain; its horizontal branch (HB) is located below 21 mag. We have occasionally taken CCD VI images of Pal 2 since 2010 and until 2021 and we have attempted to take advantage of this image collection to search for variables in the FoV of the cluster. We were able to measure 400-500 point sources in the V and I images that span a range in magnitude and colour shown in the left panel of Figure 2. The HB being located at the bottom of the stellar distribution, we are in fact working at the very limit of our photometry in order to detect cluster member RR Lyrae.
To search for variability we proceeded as follows. By using the string-length method (Burke1970, Dworetsky1983), we phased each light curve in our data with a period varying between 0.2 d and 1.0 d, a range adequate for RR Lyrae stars, in steps of 10-6 d. For each phased light curve, the length of the line joining consecutive points, called the string-length and represented by the parameter S Q , was calculated. The best phasing occurs when S Q is minimum, and corresponds to the best period that our data can provide. A detailed visual inspection of the best phased light curve helped to confirm the variability of some stars. We noticed, however, that the seasonal scatter of the light curve could vary depending mainly on the prevailing seeing conditions and crowdedness of a particular star, a situation that worsens near the core of the cluster. Therefore, it may happen that in some seasons the light curve variation is dubious, but extremely clear in the runs of best quality, which turned out to be from the 2013 and 2018-2020 seasons.
With the above method we discovered 21 RR Lyrae variables, mostly of the RRab type.
Confronting with the membership analysis described in
In Table 1 we list the 32 variables in the field of Pal 2. The table is organized as follows. We have given the name with the prefix “V” only to those stars that seem likely cluster members (status M1 or M2), 18 in total, V1-V18. Arbitrarily, we identified the Gaia variables as G1-G22. This identification is listed in Column 2. In the bottom 14 rows of Table 1 we list the likely non-members (status FS). For non-member variables detected by us, we used the nomenclature with the prefix “SV”.
5.1 Variables in the CMD
In the right panel CMD of Figure 2, all variable stars have been marked with a red circle if they are cluster members or a black circle otherwise. As a reference we included two isochrones from the models of VandenBerg et al. (2014) for [Fe/H]= -1.6 and -2.0 and a theoretical horizontal branch built by Yepez et al. (2022). Isochrones and HB were placed at a distance of 26.1 kpc Bonatto Chies-Santos (2020). It is heartening to see nearly all the RR Lyrae stars fall in the whereabouts of the HB. In the following section we address some peculiar individual cases.
5.2 Individual Cases
V1. Its position on the CMD above the HB and in the mid-RGB is intriguing since the light curve and period suggest this star to be a member RRab star. An alternative possibility is that the star is a binary. Our data are not sufficient to explore this possibility.
V16, V17 and V18. Their position on the CMD near the tip of the RGB suggests these stars are red giant variables. However, our photometry was not extensive enough to confirm a long-term variability. Alternatively, we were able to identify short-therm variations in V16 and V18 (see Figure 3). The V17 light curve is, in fact, consistent with that of a long-term RGB.
SV1. It is a clear RRab star, falling much to the red of the HB. The star is not a cluster member.
SV7. We have detected clear RRab-like variations in our V data. However, no variation is seen in the I data. While variations might be spurious, we retain the star as a candidate variable to be confirmed.
SV4, SV5, SV6 and G23. These are the four non-member stars, hence identified by black circles or squares in the DCM. However, they lie very near the HB. Their non-membership status was assigned by the statistical approach to their proper motions, but they might be cluster members.
G3 and G20. G3 is a clear RRab star, not a cluster member. For G20 we got a very noisy light curve that makes its classification very difficult; however, the star is likely a non-member.
6 The Oosterhoff type of Pal 2
The average period of the member RRab star listed in Table 1 is 0.55 days which indicates that Pal 2 is of the Oo I type. We
can further confirm this from the distributions of the RRab stars in the
Amplitude-Period or Bailey diagram, shown in Figure
1. Given the dispersion of the light curves, the amplitude distribution
is also scattered. However, it is clear that the RRab stars follow the expected
sequence for unevolved stars typical of OoI clusters Cacciari et al.(2005), in both the V and
I bands. The upper sequence corresponds to evolved stars of the
Oo II clusters Kunder et al.(2013). Hence,
Pal 2 is an Oo I type cluster. We note that the stars V16 and V18, whose nature is
not clear due to their position in the RGB and short period (
7 Cluster distance and metallicity from member RR Lyrae stars
Although the scatter of all these faint cluster member stars may be large, we attempted an estimation of the mean distance and [Fe/H] via the Fourier light curve decomposition. This approach has been amply described in previous papers. Both the method details and the specific calibrations for M V and [Fe/H] for RRab stars can be found in a recent paper by Arellano Ferro (2022).
We selected the RRab members with the best quality light curves and restricted the
Fourier approach to this sample. These are the variables V2-V13 shown in Figure 3. The mean values for the distance
modulus
8 Summary
We have found and identified 32 variables in the field of the globular cluster Palomar 2. A membership analysis based on Gaia-DR3 proper motions and the positioning of the variables in the corresponding intrinsic CMD, demonstrates that at least 18 of these variables are cluster members. Most of the detected variables are of the RRab type but one RRc and at least one RGB were identified.
The mean cluster distance and metallicity, estimated from the Fourier light curve
decomposition of 11 cluster member RRab stars with the best quality available data,
lead to