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Revista mexicana de astronomía y astrofísica

versión impresa ISSN 0185-1101

Rev. mex. astron. astrofis vol.59 no.1 Ciudad de México abr. 2023  Epub 21-Oct-2024

https://doi.org/10.22201/ia.01851101p.2023.59.01.03 

Articles

Physical Properties and Membership Determination of the Open Clusters IC 4665, NGC 6871 and Dzim 5 Through uvby−β Photoelectric Photometry1

J. H. Peña2  3  4 

A. Rentería2  3 

J. D. Paredes2  5 

D. S. Piña2  4 

2 Instituto de Astronomía, Universidad Nacional Autónoma de México, México.

3 Observatorio Astrónomico Nacional de Tonantzintla, Universidad Nacional Autónoma de México, México.

4 Facultad de Ciencias, Universidad Nacional Autónoma de México, México.

5 Facultad de Ciencias, Universidad Central de Venezuela, Venezuela


ABSTRACT

uvby−β photoelectric photometry of stars in the direction of the open clusters IC 4665, NGC 6871 and Dzim 5 is presented. From this uvby−β photometry we classified the spectral types which allowed us to determine the reddening and, hence, the distance. Membership of the stars to the cluster was determined. Our results are compared with those obtained by GAIA DR2.

Key Words: galaxies; photometry - open clusters and associations; general - parallaxes

RESUMEN

Se presenta fotometría uvby−β de estrellas en la dirección de los cúmulos abiertos IC 4665, NGC 6871 y Dzim 5. A partir de la fotometría fotoel´ectrica uvby−β de las estrellas en la dirección de estos cúmulos clasificamos los tipos espectrales de cada estrella lo que nos permitió la determinación de su enrojecimientoy de sus distancias y, por ende, la pertenencia de las estrellas al cúmulo. Nuestros resultados se comparan con GAIA DR2.

1 Motivation

Open clusters are a gold mine for the development of many astrophysical topics. They offer a unique opportunity, for example, to compare theoretical studies with observations; they provide opportunities to develop models of chemical enrichment with respect to the center of the galaxy, and serious studies on stability can be tested only through an analysis of open clusters. However, despite the importance of these topics, research in these fields begins with the determination of the cluster member stars.

Membership determination in open clusters is done, canonically, with proper motion studies; but in practice, main-sequence fitting is used since it is easier, although less accurate and cannot be used on a star-by-star basis. However, for distant or faint clusters membership determination is not an easy task. uvby-β   photometry of open clusters provides an accurate method for determining distances to each star and, through the global behavior, throws light on the distance to the cluster and, hence, the membership of each star to the cluster.

In this paper we present our results on three clusters: two, IC 4665 and NGC 6871, are relatively well-studied and the other, Dzim 5, has very little published information.

The open cluster IC 4665 has been a subject of many studies. The membership in the cluster has been determined in many different ways. The classical proper motions studies were done by Vasilevskis (1955) and the spectral classification of its members was done through classical spectroscopy.

With respect to the photometric studies, there are some classical works like that of Johnson (1954). With intermediate photometric bands there is the work of Crawford & Barnes (1972) who, with uvby-β   photometry, found an average cluster reddening E(b - y) of 0.14, and a cluster distance modulus of 7.5, corresponding to a distance of 316 pc. They obtained the same values from an analysis of the B-type stars and the A- and F- type stars.

Finding variables in the cluster has been a subject of some research. Barannikov (1994) confirmed that the star HD 161573 in the IC 4665 cluster has periodic (P = 19 d) variability.

With respect to NGC 6871 much research has been carried out. A good summary of its characteristics can be found in Southworth et al. (2004). They stated that the open cluster NGC 6871 was a concentration of bright OB stars which form the nucleus of the Cyg OB3 association. For this reason it is an important object in the study of the evolution of high-mass stars. The cluster itself has been studied photometrically several times, but the scarce data on its nature mean that determination of its physical parameters is difficult. They further note that: “UBV photometry of the 30 brightest stars was published by Hoag et al. (1961). Crawford, Barnes & Warren (1974) observed 11 stars in the Strömgren uvby system and 24 stars in the Crawford β system, finding significantly variable reddening and a distance modulus of 11.5 mag. This uvby-β   photometry was extended to 40 stars by Reimann (1989), who found reddening E(b - y) with a mean value of 0.348 mag and an intercluster variation of about 0.1 mag. His derived distance modulus of 11.94 ± 0.08 and age of 12 Myr are both greater than previous literature values”.

Southworth et al. (2004) carried out a study of the eclipsing binary V453 Cyg (W31) which, they claimed, is a member of NGC 6871. As we will see later, this is not the case.

The other cluster, Dzim 5 was reported by Dolidze & Jimsheleishvili (1966) but after this, there is only one reference to one of its members. WEBDA does not list distance, reddening age, metallicity or any other quantity except its coordinates. They refer only to the study of Kazlauskas et al., (2013) related to a new spectroscopic binary with which they establish that Dol-Dzim 5 is not a real open cluster.

Table 1 presents a summary of the most relevant findings of several papers for these clusters.

Table 1 Compilation of the determined data of the clusters  

Author E(B - V) E(b - y) DM Dst
pc
[Fe/H] Age
log (age)
Technique
members/total
IC 4665
Vasilevskies (1955) proper motion
Alcaino (1965) 0.152 UBV
Becker & Fenkart (1971) 0.17 8.11 330 UBV
Crawford & Barnes (1972) 0.14 7.5 316 uvby-β
Sanders & Van Altena (1972) 8.556 proper motion
Patenaude (1978) 7.6 theory and UBV
Nicolete (1981) 7.8 ± 0.022 379 ± 46 Geneva photometric boxes
Morrel & Abt (1991) 0.04 spectroscopy
Stetson (1991) 0.112 335 0.04 8.703 compiled
Cargile & James (2010) 357 ± 12 7.623
PP 01.43 ± 0.046 7.5 ± 0.3 323 ± 49 -0.20 ± 0.09 8.160 uvby-β
NGC 6871
Cohen (1969) 0.38 11.4 β
Crawford et al. (1974) 11.5 uvby-β
Schild & Ramashin (1976) 11.1 Be
Babu (1983) 1600 Spectroscopy
Nicolet (1981) 11.19 ± 0.52 1730 ± 450 Geneva
PP 0.307 ± 0.044 10.9 ± 0.04 7.088 uvby-β
DZIM 5
Kazlauskas et al. (2013) 0.02 400 -0.09 ± 0.17 Strömvil phot and rv
PP 0.1 ± 0.1 6.62 ± 0.46 215 ± 45 -0.4 ± 0.30 uvby-β

2 Observations

This article is a sequel to a paper on NGC 6633 that has already been published (Peña et al., 2017, Paper I). The observations were carried out over a long season by two different observers, one from June 22th to 30th and the other from July 1st to 8th, 2016 (ARL and CVR, respectively) with different objects in each one although some were taken continuously (NGC 6633, Peña et al., 2017, and V 2455 Cyg, Peña et al., 2019). The open cluster IC 4665 was observed for four nights from June 22nd to June 25th. NGC 6871 was observed for two nights, July 2nd and 3rd and Dzim 5 from July 5th to the 8th. The observing and reduction procedures were described in detail in Paper I. The reduction was done considering both seasons together as one long season to increase the accuracy of the standard stars.

The observations were all taken at the Observatorio Astronómico Nacional de San Pedro Mártir, México. The 0.84 m telescope, to which a spectrophotometer was attached, was utilized at all times. The stars to be observed were selected randomly by drawing concentric circles on the ID charts provided by WEBDA and observing all the bright stars in each circle.

The limit was the faintness of the stars, since to reach the desired accuracy faint stars would require an exceedingly long time of observation. Hence, no astrophysical considerations, nor previous knowledge of the selected stars, was considered. For IC 4665 we measured thirty stars, sixteen for NGC 6871 and fourteen for Dzim 5. Although some of the stars had already been observed, a comparison between the sets gave us confidence in the data as shown from the standard deviations of the values for the same star from several studies, in some cases from three or four different measurements. In the case of Dzim 5 averaging the large discrepancy in the color indexes m 1 and c 1 could have led to possible misinterpretations of the physical characteristics of the stars and, hence, of the cluster.

2.1 Data Acquisition and Reduction

During all the observed nights the following procedure was utilized: at least five ten-second integrations of each star and one ten-second integration of the sky for the uvby filters and the narrow and wide filters that define Hβ were done for each measurement. The reduction procedure was done with the numerical package NABAPHOT (Arellano-Ferro & Parrao, 1988). A series of standard stars was also observed on each night to transform the data into the standard system. The chosen standard system was that defined by the standard values of Olsen (1983), although some of the standard bright stars were also taken from the Astronomical Almanac (1996). The transformation equations are those defined by Crawford & Barnes (1970) and by Crawford & Mander (1966). See Paper I for details.

In these transformation equations the coefficients D, F, H, and L are the slope coefficients for (b - y), m 1 , c 1 ,and β, respectively. The coefficients B, J and I are the color terms of V, m 1 , and c 1. The averaged transformation coefficients of each night were listed in Table 2 of Paper I along with their standard deviations. Season errors, Table 2, were evaluated by means of the nineteen standard stars observed for a total of 133 observed points. These uncertainties were calculated through the differences in magnitude and colors for all nights, for (V, b - y, m 1 , c 1 and β) as (0.024, 0.010, 0.011, 0.015, 0.015), respectively, which provide a numerical evaluation of our uncertainties of the season. Emphasis is made on the large range of the standard stars in the magnitude and the color indexes: V:(5.2, 8.8); (b - y):(0.00, 0.80); m 1 :(0.09, 0.68); c 1:(0.08, 1.05) and β:(2.50, 2.90).

Table 2: Seasonal standard deviations of the standard stars  

ID σV σ(b-y) σm1 σc1 σβ
Mean 0.029 0.013 0.008 0.020 0.017
Stand. Dev. 0.012 0.011 0.007 0.018 0.004

The numerical results obtained are presented in Table 3 of Paper I. In Column 1 we present the ID; in Columns two to six, the mean photometric values V, (b - y), m 1 , c 1 and β for each star. The corresponding unreddened indexes are presented in the subsequent columns. The mean values of the individual standard deviations are presented at the bottom of the last two rows of Table 2 of Paper I, as well as the standard deviation of the individual standard deviations. These values are a few hundredths or thousandths of magnitude for each color index and provide the accuracy of our photometry.

Table 3: Observed uvby-β   photoelectric photometry of the open cluster IC 4665  

ID V (b - y) m1 c1 σV σ(b-y) σm1 σc1 σHβ N
01 6.857 0.079 0.030 0.321 2.702 0.057 0.015 0.006 0.017 0.012 3
02 7.353 0.078 0.032 0.455 2.715 0.060 0.010 0.002 0.009 0.011 3
03 7.603 0.063 0.039 0.413 2.721 0.050 0.012 0.006 0.010 0.015 3
04 7.705 0.071 0.048 0.459 2.744 0.087 0.010 0.003 0.008 0.006 2
05 9.090 0.140 0.103 0.920 2.883 0.042 0.010 0.003 0.015 0.009 3
06 10.092 0.097 0.130 0.946 2.895 0.039 0.018 0.009 0.008 0.033 3
07 9.364 0.205 0.155 0.914 2.888 0.035 0.011 0.003 0.013 0.006 3
08 10.673 0.376 0.101 0.473 2.691 0.029 0.010 0.016 0.010 0.037 3
09 10.896 0.739 0.423 0.113 2.588 0.038 0.040 0.126 0.001 0.007 3
10 9.080 0.197 0.109 0.916 2.895 0.037 0.014 0.004 0.008 0.012 3
11 7.928 0.314 0.131 0.460 2.694 0.037 0.015 0.004 0.012 0.011 3
12 10.262 0.812 0.378 0.203 2.582 0.012 0.011 0.042 0.041 0.037 3
13 8.870 0.137 0.029 0.627 2.709 0.046 0.021 0.001 0.003 0.004 2
14 8.375 0.780 0.385 0.301 2.581 0.031 0.015 0.016 0.014 0.007 3
15 9.792 0.473 0.136 0.467 2.655 0.033 0.015 0.002 0.008 0.014 3
16 10.549 0.806 0.502 0.160 2.581 0.049 0.015 0.009 0.045 0.017 3
17 8.217 0.128 0.054 0.541 2.750 0.042 0.014 0.002 0.006 0.005 3
18 10.869 0.278 0.142 0.695 2.751 0.040 0.011 0.017 0.028 0.03 3
19 8.300 1.095 0.804 0.012 2.595 0.045 0.016 0.011 0.046 0.025 3
20 9.852 0.169 0.129 0.983 2.872 0.036 0.016 0.011 0.036 0.018 3
21 10.880 0.976 0.676 -0.049 2.602 0.023 0.008 0.015 0.089 0.002 2
22 7.771 0.063 0.038 0.345 2.703 0.027 0.019 0.009 0.017 0.015 3
23 7.995 0.102 0.034 0.442 2.725 0.026 0.020 0.010 0.013 0.010 3
24 7.123 0.084 0.026 0.431 2.687 0.038 0.013 0.003 0.009 0.009 3
25 8.807 0.164 0.131 0.995 2.904 0.037 0.011 0.003 0.008 0.025 3
26 10.395 0.210 0.159 0.864 2.843 0.025 0.018 0.008 0.019 0.026 3
27 10.942 0.433 0.070 0.409 2.609 0.030 0.020 0.012 0.039 0.033 3
28 7.480 0.077 0.159 0.979 2.899 0.029 0.009 0.003 0.001 0.003 2
29 9.745 0.373 0.123 0.277 2.597 0.033 0.007 0.004 0.011 0.008 2
30 10.188 0.800 0.550 0.254 2.595 0.032 0.016 0.042 0.094 0.021 3

Tables 3, 4 and 5 report the observed uvby-β   photoelectric photometry for IC 4665, NGC 6871 and Dzim 5, respectively. In Tables 3 and 4 we list the following: in Column 1 the ID in WEBDA, subsequent columns report the magnitude V and the color indexes (b - y), m 1 , c 1, and β. Since each star was observed over several nights, mean values and their standard deviations were calculated. They are also presented in the tables, as well as the number of entries in the mean. This is number N presented in the last column of each table. For the open cluster Dzim 5 we present our uvby-β   photoelectric photometry with the ID numbers shown as in Kalauskas et al. (2013).

Table 4: Observed uvby-β   photoelectric photometry of the open cluster NGC 6871 

ID V (b - y) m1 c1 σV σ(b-y) σm1 σc1 σHβ N
01 6.782 0.088 0.167 -0.240 2.473 0.017 0.010 0.000 0.015 0.001 2
03 7.339 0.252 -0.053 -0.055 2.541 0.016 0.003 0.008 0.016 0.006 2
05 7.889 0.262 -0.047 -0.076 2.553 0.035 0.003 0.001 0.007 0.005 2
08 8.700 0.225 -0.050 0.049 2.611 0.076 0.008 0.003 0.040 0.005 2
25 11.662 0.276 -0.039 0.275 2.718 0.029 0.010 0.013 0.020 0.018 2
24 11.721 0.233 0.026 0.279 2.699 0.029 0.011 0.007 0.039 0.018 2
153 8.474 0.884 0.532 0.332 2.558 0.006 0.004 0.020 0.006 0.006 2
07 8.779 0.225 -0.056 0.006 2.596 0.025 0.016 0.021 0.016 0.006 2
04 7.746 0.200 -0.022 -0.148 2.564 0.006 0.000 0.001 0.004 2
09 9.473 0.384 0.175 0.275 2.575 0.003 0.001 0.009 0.008 0.012 2
02 7.270 0.252 -0.055 -0.038 2.547 0.003 0.001 0.001 0.005 0.008 2
13 10.368 0.217 -0.024 0.126 2.690 0.021 0.000 0.013 0.011 0.011 2
31 8.423 0.222 -0.037 -0.021 2.575 0.234 0.001 0.004 0.008 0.008 2
12 10.347 0.343 0.157 0.321 2.628 0.007 0.008 0.012 0.012 0.018 2
15 10.791 0.246 -0.006 0.075 2.639 0.006 0.009 0.006 0.002 0.066 2
10 10.404 0.259 0.145 0.797 2.727 0.408 0.011 0.012 0.017 0.003 2

Table 5: Observed uvby-β   photoelectric photometry of the open cluster Dzim 5  

ID V (b - y) m1 c1 σV σ (b - y) σm1 σc1 σ Hβ N
K07 9.254 0.815 0.780 0.194 2.570 0.003 0.000 0.008 0.021 0.013 3
K06 10.179 0.393 0.247 0.292 2.619 0.009 0.008 0.016 0.011 0.037 3
K10 11.444 0.331 0.130 0.324 2.605 0.014 0.010 0.014 0.014 0.031 3
K11 11.920 0.385 0.181 0.327 2.598 0.009 0.020 0.031 0.009 0.037 3
K12 10.357 0.538 0.375 0.323 2.560 0.006 0.001 0.009 0.012 0.007 3
K13 11.293 0.405 0.228 0.285 2.597 0.082 0.016 0.024 0.021 0.017 3
K14 10.001 0.315 0.145 0.397 2.655 0.043 0.003 0.008 0.010 0.028 3
K09 10.556 0.316 0.154 0.385 2.658 0.052 0.017 0.017 0.008 0.016 3
K08 10.608 0.646 0.523 0.323 2.562 0.012 0.008 0.011 0.011 0.029 3
K05 10.752 0.486 0.192 0.382 2.632 0.078 0.012 0.006 0.013 0.014 2
K15 11.828 0.406 0.237 0.382 2.674 0.104 0.030 0.040 0.045 0.044 3
K01 10.378 0.305 0.169 0.424 2.668 0.009 0.006 0.014 0.013 0.003 3
K02 11.178 0.820 0.726 0.245 2.571 0.017 0.020 0.048 0.059 0.036 3
K04 11.943 0.298 0.167 0.305 2.653 0.027 0.027 0.038 0.029 0.048 3

3 Comparison with other photometries

A comparison with previous uvby-β   photoelectric photometry had to be done in order to test the goodness of our results and to enhance the sample by considering the previously measured stars in the direction of each cluster. A search, mostly from WEBDA, was done for references on uvby-β   photometry. These are presented in Table 6, in which the references and the number of the reported stars are listed. However, in our comparison, we only take into account those studies with a significant number of observed stars devoted to each cluster. Those stars with few points taken randomly in studies not devoted to the cluster were not included in the mean. Later, as we will see, a compilation of the stars in the direction of each cluster was done increasing the number of stars in the direction of the cluster, with the proven quality of their values.

Table 6: References with uvby-β   photometry for the three clusters 

Source Number of reported stars
IC 4665
Crawford & Barnes (1972) 47
Perry & Johnston (1982) 2
Schmidt (1982) 1
Olsen (1983) 2
Schuster & Nissen (1988) 2
Sinachopoulos (1990) 2
Stetson (1991) 6
Olsen (1993) 1
Present Paper (2022) 29
Total Number 57
NGC 6871
Cohen (1969) 8
Crawford et al. (1974) 8
Crawford (1975) 1
Reimann (1989) 18
Present Paper (2022) 16
Total Number 23
DZIM 5
Kazlauskas, (2013) 14
Present Paper (2022) 14
Total Number 15

Fig. 1: ID chart of the observed stars in the direction of Dzim 5. The ID number follows that of Kalauskas et al. (2013) 

Instead of considering the averaged values reported by WEBDA, we opted to include the original sources, because the mean value combined with our photometry would be biased; this saved us from cases like those presented for the open cluster IC 4665. The star W108, which we did not observe, but appears in the compilation of WEBDA, had two radically different values in magnitude reported: 7.508 and 9.820. Equally discrepant are the color indexes. To check which magnitude value was correct, we compared both with those reported in UBV in WEBDA which lists 7.460 and 7.490 mag inV. These systematic differences suggest a variable star. Nevertheless, the value corresponding to 9.820 was not further considered in our analysis.

All the analysis of the data of the three clusters is calculated in a linear fit in which the oldest source data are considered on the X axis and the newest, on the Y axis. A linear relation was calculated in a formula Ynew=A+BXold. The goodness of the fit is demonstrated by both the correlation coefficient R and the standard deviation of the points. For a good fit, A should be small and A close to 1. The correlation coefficient, R, has to be near unity and the standard deviation, small. All the values obtained for each cluster are presented in Table 7. The final column in the table presents N, the number of entries. Figures 2, 3 and 4 present the comparisons among the principal data sets for IC 4665 (Crawford and Barnes (1972) vs present paper; for NGC 6871 Crawford et al. (1974) vs. Reimann (1989) and Kazlauskas (2013) vs. present paper, respectively.

Table 7: Linear regression of the uvby-β   color indexes: present paper’s data Vs. the literature  

IC 4665
Index A B R Std Dev N
Crawford & Barnes (1972) vs. Stetson (1991)
V -0.1437 1.0020 0.9999 0.0411 6
(b - y) -0.0011 0.9647 0.9995 0.0029 6
m1 -0.0076 1.0369 0.9974 0.0036 6
c1 -0.0170 1.0396 0.9996 0.0088 6
β -0.4740 1.1725 0.9999 0.0011 6
Crawford & Barnes (1972) vs. Present Paper
V 0.0460 0.9950 0.9990 0.0454 18
(b - y) 0.0308 0.9075 0.9903 0.0131 18
m1 -0.0322 1.1326 0.9863 0.0090 18
c1 -0.0230 0.9812 0.9959 0.0234 18
β -0.0217 1.0089 0.9812 0.0179 17
NGC 6871
Crawford et al. (1974) vs. Reimann (1989)
(b - y) 0.0087 0.9554 0.9908 0.0102 8
m1 -0.0219 0.6423 0.9784 0.0128 8
c1 0.0101 0.9139 0.9796 0.0209 8
β 0.0087 0.9966 0.9996 0.0030 15
Reimann (1989) vs. Present Paper
V -0.0305 1.0017 0.9979 0.1143 14
(b - y) 0.0131 0.9664 0.9797 0.0141 14
m1 -0.0086 1.3661 0.9578 0.0279 14
c1 -0.0247 1.3017 0.9872 0.0433 14
β -1.0105 1.3866 0.9797 0.0143 10
Cohen (1969) vs. Present Paper
β -1.2661 1.4849 0.9746 0.0071 6
DZIM 5
Kazkalauskas et al (2013) vs. Present Paper
V -0.0921 1.0068 0.9998 0.0181 12
(b - y) 0.0078 0.9695 0.9987 0.0103 12
m1 0.0959 0.5963 0.1167 0.2419 12
c1 0.3938 -0.2354 -0.7397 0.0451 12

Figure 2: Comparison of Crawford and Barnes (1972) vs. present paper’s photometry for IC 4665. 

Figure 3: Comparison of Crawford et al. (1974) vs. Reimann’s photometry for NGC 6871. 

Figure 4: Comparison of Kazlauskas (2013) vs. present paper photometry for Dzim 5. 

For the cluster IC 4665 we considered the original sources of Crawford & Barnes (1972) with forty-five entries; of Stetson (1991) with only six measured stars; and our photometry (58 stars), to calculate the mean values of the stars. Of all the sets only star W32 showed anomalies. Its reported V magnitude in Crawford & Barnes (1972) is 10.188, whereas the V magnitude in Stetson (1991), is 8.330. The large difference could be due to either intrinsic variability or eclipses. We ended up with a sample of fifty-six stars of which ten are presented for the first time, four measured in the three sets and thirteen in the intersection of Crawford & Barnes (1972) and the present paper’s photometry. Only two were measured in both data sets of the literature, Crawford & Barnes (1972) and Stetson (1991). The mean value for each star is presented in Table 8 along with the standard deviation of each color index.

Table 8: Compiled uvby-β   photoelectric photometry of IC 4665 

ID V (b - y) m1 c1 σV σ (b - y) σm1 σc1 σ Hβ Photom. Source SpTyp
7 9.310 0.315 0.163 0.744 2.774 1 A9Vp
22 8.780 0.089 0.077 0.798 2.771 A0V1
23 8.060 0.070 0.093 0.825 2.826 1 A0V
27 10.320 0.172 0.160 0.978 2.899 1 A4V
28 7.432 0.240 0.105 0.978 2.775 0.003 0.005 0.000 0.008 0.004 1,2 A2V
32 8.330 0.067 0.066 0.964 2.733 1 A8I
34 11.000 0.457 0.091 0.474 2.712 1 F2V
37 11.360 0.384 0.114 0.574 2.698 1 F0V
38 10.702 0.382 0.100 0.512 2.690 0.040 0.009 0.001 0.054 0.002 1,3 F0V
39 9.377 0.199 0.159 0.943 2.887 0.026 0.006 0.004 0.030 0.011 1,2,3 A3V
42 10.896 0.739 0.423 0.056 2.588 3 LATE
43 9.090 0.125 0.120 0.931 2.871 0.000 0.022 0.024 0.015 0.017 1 A2V
44 10.092 0.097 0.130 0.946 2.895 3 A2V
47 9.764 0.380 0.118 0.287 2.623 3 F7V
48 11.580 0.392 0.088 0.510 2.669 1 F0V
49 7.691 0.057 0.072 0.471 2.735 0.006 0.001 0.007 0.001 0.002 1,3 A V
50 9.085 0.190 0.118 0.927 2.885 0.007 0.011 0.013 0.015 0.015 1,3 A2V
51 9.850 0.270 0.100 0.962 2.889 1 A2V
53 11.410 0.366 0.113 0.527 2.702 1 F0V
56 7.504 0.079 0.162 0.999 2.904 0.008 0.005 0.004 0.030 0.001 1,3 A2V
57 11.130 0.327 0.137 0.602 2.698 1
58 7.599 0.049 0.058 0.424 2.714 0.008 0.012 0.016 0.010 0.007 1,2,3 B V
59 11.030 0.907 0.466 0.485 2.582 1 LATE
62 6.857 0.065 0.043 0.337 2.692 0.003 0.012 0.011 0.014 0.010 1,2,3 B V
63 10.560 0.222 0.167 0.837 2.834 1 A4V
64 7.357 0.067 0.048 0.462 2.709 0.005 0.016 0.022 0.011 0.009 1,3 B V
65 10.600 0.278 0.165 0.716 2.760 1 A8Vp
66 10.403 0.203 0.165 0.884 2.877 0.011 0.010 0.009 0.029 0.004 1,3 A5V
67 8.803 0.155 0.139 1.010 2.897 0.005 0.013 0.011 0.021 0.011 1,3 A3V
68 7.936 0.309 0.139 0.471 2.685 0.010 0.008 0.011 0.015 0.013 1,3 F0V
70 10.262 0.812 0.378 0.203 2.582 3 LATE
71 10.942 0.433 0.070 0.409 2.656 3
72 7.765 0.048 0.053 0.360 2.704 0.008 0.009 0.013 0.021 0.001 1,3 B V
73 7.126 0.070 0.040 0.442 2.688 0.005 0.020 0.020 0.015 0.001 1,3 B V
74 10.549 0.806 0.502 0.160 2.581 3 LATE
76 8.213 0.115 0.066 0.554 2.747 0.005 0.017 0.017 0.019 0.003 1,3 B V
81 8.924 0.136 0.036 0.644 2.705 0.092 0.035 0.014 0.033 0.004 1,2,3 A0V
82 7.993 0.091 0.046 0.455 2.732 0.004 0.015 0.016 0.018 0.009 1,3 B V
83 10.210 0.191 0.137 0.996 2.888 1 A3V
84 9.792 0.473 0.136 0.467 2.655 3 G0V
86 10.390 0.412 0.102 0.574 2.663 1 F0V
88 10.858 0.281 0.141 0.747 2.778 0.017 0.004 0.000 0.074 0.038 1,3 A6V
89 9.846 0.156 0.136 1.006 2.877 0.009 0.018 0.010 0.032 0.007 1,3 A0V
90 8.300 1.095 0.804 0.012 2.595 3 LATE
92 10.845 0.974 0.676 0.281 2.562 3 LATE
95 9.880 1.256 0.470 0.591 0.000 1 LATE
96 8.907 0.490 0.335 0.284 2.555 1 LATE
98 8.375 0.780 0.385 0.301 2.581 3 LATE
99 7.530 1.259 0.232 0.904 0.000 1 LATE
102 9.290 0.111 0.136 1.092 2.908 1 A2V
105 7.490 0.040 0.084 0.535 2.732 1 B V
111 10.000 0.282 0.168 0.727 2.765 1 A9Vp
115 9.150 0.275 0.182 0.705 2.788 1 A8Vp
118 10.320 0.235 0.120 0.986 2.910 1 A3V
121 8.610 0.245 0.166 1.056 2.838 1 A4V
125 9.700 0.142 0.130 1.156 2.882 1 F2Ib
178 7.705 0.071 0.048 0.459 2.744 3 B V

Note: 1 Crawford, 1971; 2 Stetson, 1991; 3 PP.

The column of photometric sources lists the authors whose values we consider in the mean; these are listed at the bottom of the table. The last column presents the spectral type determined from the uvby-β   photoelectric photometry in a procedure described below.

These coefficients are adequate despite the fact that the span of the color index limits is rather low, particularly in (b - y) from 0 to 0.4; m 1 from 0 to 0.2. On the other hand, the magnitude V limits go from 7 to 11 mag. The linear fit in β was done without W88 which showed a relatively large difference (0.064).

The final list of compiled uvby-β   photoelectric photometry of IC 4665 is presented in Table 8. Column 1 lists the ID of WEBDA, subsequent columns present the mean magnitudes V and color indexes (b - y), m 1 , c 1, and β. The standard deviations are also presented, as well as the references utilized in the mean. The references are presented at the bottom of the table.

For NGC 6871 Crawford et al. (1974) observed 8 stars in the complete uvby-β   system and 12 only in β; Reimann (1989) presented the majority of the observed stars, a sample of 18 stars in the uvby-β   system and 22 stars in uvby only. His star 101 is considered to be W31. One more source, Cohen (1969) observed eight stars of the cluster but only in β. The same procedure as in IC 4665 was done, and the coefficients of the cross fits are presented in Table 7. The mean values of the three sources are listed in Table 9, along with the standard deviation and the number of sources involved in the mean. The whole sample is constituted of 23 stars.

Table 9: Compiled uvby-β   photoelectric photometry of NGC 6871  

ID V (b - y) m1 c1 σV σ (b - y) σm1 σc1 σ Hβ Photom. Source SpTyp
1 6.788 0.087 0.162 -0.220 2.473 0.008 0.006 0.050 0.026 1,2,3,4
2 7.288 0.251 -0.035 -0.016 2.558 0.025 0.001 0.018 0.019 0.010 1,2,3,4 B V
3 7.353 0.248 -0.037 -0.027 2.556 0.021 0.007 0.023 0.029 0.011 1,2,3,4 B V
4 7.767 0.202 -0.011 -0.124 2.571 0.029 0.007 0.011 0.020 0.006 1,2,3,4 B V
5 7.902 0.260 -0.037 -0.039 2.570 0.018 0.002 0.014 0.037 0.013 1,2,4 B V
6 8.187 0.339 -0.088 -0.188 2.276 0.002 0.003 0.018 0.175 1,2,4 B V
7 8.792 0.217 -0.025 0.005 2.600 0.019 0.010 0.027 0.005 0.162 1,2,3,4 B V
8 8.790 0.220 -0.029 0.062 2.608 0.127 0.004 0.020 0.014 0.003 1,2,3,4 B V
9 9.452 0.383 0.159 0.256 2.575 0.030 0.001 0.022 0.028 2,3 F9V
10 10.263 0.262 0.122 0.822 2.727 0.199 0.005 0.032 0.035 2,3 A2V
11 10.332 0.205 -0.005 0.075 2.636 2 B V
12 10.335 0.345 0.133 0.314 2.628 0.017 0.003 0.034 0.009 1,2 F9V
13 10.372 0.210 -0.002 0.116 2.660 0.006 0.011 0.031 0.014 0.026 1,2 B V
14 10.796 0.210 -0.004 0.244 2.637 0.006 1,2 B V
15 10.776 0.254 -0.020 0.118 2.639 0.021 0.012 0.020 0.061 0.000 1,2,3 B V
16 10.980 0.203 0.009 0.255 2.550 0.141 1,2 B V
17 11.251 0.320 -0.019 0.238 2 B V
18 11.319 0.171 0.094 1.225 2 F2Ib
19 11.542 0.194 0.024 0.298 2 B V
20 11.558 0.256 0.015 0.612 2.571 2 B V
21 11.661 0.244 -0.040 0.380 2.666 0.000 1,2 B V
22 11.646 0.214 0.110 0.896 2 A2V
23 11.638 0.172 0.084 0.177 2
24 11.732 0.229 0.032 0.253 2.690 0.017 0.005 0.008 0.036 0.008 1,2,3 B V
25 11.761 0.256 -0.017 0.293 2.699 0.140 0.029 0.031 0.025 0.016 1,2,3 B V
26 11.830 0.230 0.102 0.832 2 A2V
27 11.874 0.286 -0.016 0.335 2.732 0.000 1,2 B V
28 2.77 1
29 2.782 1
30 2.788 1
31=R101 8.402 0.218 -0.025 -0.010 2.583 0.029 0.006 0.018 0.014 0.011 2,3 B V
R102 9.780 1.094 0.431 0.274 2 LATE
R103 12.117 0.220 0.024 0.481 2 B V
R104 11.259 0.260 0.012 0.479 2 B V
R105 11.756 0.388 0.056 0.431 2 A0V
R106 11.718 0.261 -0.002 0.227 2
R107 10.775 0.239 0.077 0.857 2 B V

Note: 1 Crawford, 1974; 2 Reimann, 1989; 3 PP, 4 Cohen.

In this table all but three stars have standard deviations on the order of hundredths of magnitude. These three stars are W08, W10 and W25. W08 and W25 which were observed by us and are listed in the table, presented dispersions on the order of hundredths of magnitude, so the high dispersion found in Table 9 is due to either the photometry among the different sources Crawford et al. (1974), Reimann (1989) and Cohen (1969) and ours for star W08 or Crawford et al. (1974), Reimann (1989) and ours for star W25. For W10 we found a dispersion of 0.408, the highest of all the sample. This value was compared with that of Reimann (1989). There is always the possibility that this might show a variable nature of the star.

For the open cluster Dzim 5 there are only two sources with Strömgren photometry, that of Kazlauskas et al., (2013) with only 13 measured stars and ours, with 14 stars. In both sets, basically the same stars were measured. Only two, one in each set, were observed separately. Star 5 was identified but no uvby-β   measurements are presented. The whole sample therefore contains fifteen stars. Studying the results of the coefficients derived from the linear regression of the uvby-β   color indexes (newest data vs. older data in the literature) for the three clusters, we observe that R, the correlation coefficient, is always larger than 0.9, and that the standard deviation is less than few hundredths of magnitude implying that all data sets are consistent, except for those in DZIM 5. In DZIM 5 the correlation coefficient R gave anomalous values in m 1 and c 1 implying, of course, no correlation between both sets. In view of this, we averaged only V and (b - y) in the sets of Dzim 5 between Kazlauskas et al. (2013) vs. present paper. Their photometry did not include H β. The averaged values are presented in Table 10, following Kazlauskas et al., (2013) ID numbers: In Figure 1, star 15 was added because it was not observed by Kazlauskas et al., (2013). Because of the poor linear regression in m 1 and c 1 the average was done only for V and (b - y). Table 10 presents the mean of the uvby-β   photometry and the standard deviation of the sources.

Table 10: Compiled uvby-β   photoelectric photometry of DZIM 5  

ID V (b - y) m1 c1 Hβ σV σ(b - y) Photom. Source
1 10.390 0.308 0.169 0.424 2.668 0.018 0.004 1,2 F9V
2 11.198 0.828 0.726 0.245 2.571 0.027 0.012 1,2 LATE
3 08.763 1.115 0.719 0.528 1
4 11.944 0.309 0.167 0.305 2.653 0.000 0.016 1,2 G0
5 10.752 0.486 0.192 0.382 2.632 2 LATE
6 10.188 0.397 0.247 0.292 2.619 0.013 0.005 1,2 LATE
7 09.275 0.823 0.780 0.194 2.570 0.031 0.011 1,2 LATE
8 10.622 0.654 0.523 0.323 2.562 0.021 0.012 1,2 LATE
9 10.557 0.313 0.154 0.385 2.658 0.001 0.003 1,2 F9V
10 11.456 0.326 0.130 0.324 2.605 0.016 0.008 1,2 F8
11 11.932 0.378 0.181 0.327 2.598 0.018 0.010 1,2 G1V
12 10.374 0.542 0.375 0.323 2.560 0.024 0.006 1,2 LATE
13 11.284 0.410 0.228 0.285 2.597 0.012 0.007 1,2 LATE
14 10.002 0.317 0.145 0.397 2.655 0.001 0.003 1,2 F8V
15 11.828 0.406 0.237 0.382 2.674 2 LATE

Note: 1 Kazlauskas (2013, V and (b - y) only; 2 PP.

4 Determination of cluster parameters

In order to determine the physical characteristics of the stars in the three clusters, IC 4665, NGC 6871 and Dzim 5, the same procedure as in Paper I for NGC 6633 was carried out. This procedure briefly, consists of the following steps:

To evaluate the reddening we first established to which spectral class the stars belong: early (B and early A) or late (late A and F stars) types; the later class stars (G or later) were not considered in the analysis since there is no reddening calibration for MS stars.

To determine the spectral type of each star we utilized the compiled uvby-β   photoelectric photometry of each open cluster calculating the unreddened indexes [m1], [c1] and compared their position with the stars of the open cluster Alpha Per (Peña & Sareyan, 2006) for which the stars have well-defined spectral class. The results are presented schematically in Figures 5, 6 and 7 for IC 4665, NGC 6871 and Dzim 5, respectively. The last column of each compiled uvby-β   photoelectric photometry presents the assigned spectral type.

Figure 5: Position of the stars of IC 4665 in the [m1] - [c1] (filled squares) diagram of α Per (Peña & Sareyan, 2006), dots. The color figure can be viewed online. 

Figure 6: Position of the stars of NGC 6871 in the [m1] - [c1] (filled squares) diagram of α Per (Peña & Sareyan, 2006), dots. The color figure can be viewed online. 

Figure 7: Position of the stars of Dzim 5 in the [m1] - [c1] (filled squares) diagram of Alpha Per (Peña & Sareyan, 2006). 

The photoelectrically classified spectral types of the stars are in very good agreement with those obtained by spectroscopy and reported by WEBDA. It can be seen that the observed stars, which are the brightest in the field, are of all spectral types in the case of NGC 6871 but all late type stars for Dzim 5.

The reddening was determined through Strömgren photometry once the spectral types were classified. The application of the calibrations for each spectral type, of Balona & Shobbrook (1984) and Shobbrook (1984) for O and early A type and of Nissen (1988) for late A and F stars, respectively, allowed us to determine their reddening and hence, their unreddened color indexes. As has been said, no determination of reddening was calculated for G or later spectral types. The procedure has been extensively described in Peña & Martínez (2014). Once the reddening is calculated, the distances can be determined for each star.

The output for the three clusters is presented in Tables 11, 12, and 13 for IC 4665, NGC 6871 and Dzim 5, respectively. In each table Column 1 lists the ID of the star, Column 2 the reddening E(b - y); Columns 3 to 5 the unreddened indexes (b - y), m1, c1; Column six lists Hβ, the remaining columns list the V0 and the absolute magnitude MV. The next two columns present the distance modulus, in magnitudes, and the distance in parsecs. In the case of F type stars we present [Fe/H]. The last column provides the assigned membership, either M for the member stars or N for the non-members. Member stars within one sigma from the mean are considered members, the others, non-members. Figures 8, 10 and 11 present the histograms of the distance modulus for the stars.

Figure 8: Histogram of the distance modulus (X axis) of the stars in the direction of IC 4665. 

As can be seen in Figure 8, in the case of IC 4665, the Gaussian peak is at 7.5 ± 0.6. Those stars within these limits are considered to be member stars and are denoted by M in Table 11. Those outside these limits are considered to be non-members and are denoted by NM in the same table. The last column of Table 11 lists the membership probabilities reported by WEBDA. For IC 4665 out of forty-four compiled stars within the spectral class limits, twenty five can be considered members of the cluster. Of these, eleven stars have high membership probability reported by WEBDA, larger than 0.7 and only four have very low membership probability. Of the nineteen stars that we considered out of the cluster limits, only three have been assigned a high membership probability in the literature. So, overall, the agreement is not bad and, hence, the membership that we assigned for those eight stars that did not have previously assigned probability is a new and important result. Among the F type stars that are within the distance limits there are five stars with determined [Fe/H]. The mean value gives -0.221±0.230 if the large value of -0.597 of W71 is considered; without this value the mean value of [Fe/H] is -0.127±0.107. At any rate, for our analysis we considered a solar value. WEBDA does not assign a metallicity value for IC 4665. Figure 9 presents the distance modulus histograms for each spectral type. In Figure 9 it can be seen the peaks for each spectral group, F, A, B and combined; they are all centered at the same distance modulus.

Table 11: Reddening and unrreddened parameters of IC 4665 

ID E(b - y) (b - y)0 m0 c0 V0 MV DM Distance [Fe/H] Membership Probab
PP Webda
49 0.000 0.228 0.072 0.471 2.735 7.69 4.54 3.15 43 NM 0.85
68 0.052 0.257 0.155 0.461 2.685 7.71 3.53 4.19 69 -0.09 NM
47 0.053 0.327 0.134 0.276 2.623 9.53 4.99 4.54 81 -0.50 NM
115 0.112 0.163 0.216 0.683 2.788 8.67 3.26 5.41 121 NM
65 0.096 -0.017 0.191 0.981 2.904 7.09 1.31 5.78 143 NM
34 0.227 0.230 0.159 0.429 2.712 10.02 4.06 5.97 156 -0.11 M
07 0.145 0.170 0.206 0.715 2.774 8.69 2.69 5.99 158 M
84 0.171 0.302 0.187 0.433 2.655 9.06 3.02 6.04 161 0.26 M 0
28 0.266 -0.026 0.185 0.927 2.775 6.29 -0.19 6.48 197 M
71 0.153 0.280 0.116 0.378 2.656 10.28 3.75 6.54 203 -0.60 M
67 0.173 -0.018 0.191 0.977 2.897 8.06 1.25 6.81 231 M 0.74
111 0.103 0.179 0.199 0.706 2.765 9.56 2.71 6.85 234 M
38 0.135 0.247 0.141 0.485 2.690 10.12 3.20 6.92 242 -0.30 M 0.04
50 0.221 -0.031 0.184 0.885 2.885 8.13 1.17 6.96 247 M 0.84
23 0.107 -0.037 0.125 0.805 2.826 7.60 0.61 6.99 250 M
66 0.130 0.073 0.204 0.858 2.877 9.84 2.69 7.15 270 M 0.86
121 0.158 0.087 0.213 1.024 2.838 7.93 0.77 7.17 271 M
38 0.229 -0.03 0.228 0.900 2.887 8.39 1.18 7.21 277 M 0.86
51 0.299 -0.029 0.190 0.905 2.889 8.56 1.20 7.36 297 M
62 0.147 -0.082 0.087 0.309 2.692 6.23 -1.15 7.38 299 M 0.02
43 0.154 -0.029 0.166 0.902 2.871 8.43 1.03 7.39 301 M 0.83
63 0.110 0.112 0.200 0.815 2.834 10.09 2.69 7.39 301 M
178 0.137 -0.066 0.089 0.433 2.744 7.11 -0.34 7.45 309 M 0
65 0.094 0.184 0.193 0.697 2.760 10.20 2.74 7.46 311 M 0.87
53 0.130 0.236 0.152 0.501 2.702 10.85 3.36 7.49 314 -0.17 M 0.23
102 0.101 0.010 0.166 1.073 2.908 8.86 1.30 7.56 325 M 0
65 0.097 -0.057 0.113 0.516 2.732 7.07 -0.49 7.56 325 M 0
53 0.133 -0.066 0.088 0.437 2.709 6.79 -0.84 7.62 335 M 0.83
102 0.114 0.167 0.175 0.724 2.778 10.37 2.73 7.64 337 M 0.84
105 0.138 -0.068 0.082 0.416 2.688 6.53 -1.20 7.73 352 M 0.47
64 0.172 -0.057 0.118 0.521 2.747 7.47 -0.28 7.75 355 M 0.78
88 0.158 -0.067 0.093 0.425 2.732 7.31 -0.50 7.81 365 M 0.8
73 0.260 -0.025 0.198 0.937 2.910 9.20 1.38 7.83 368 M
76 0.119 -0.070 0.094 0.401 2.714 7.09 -0.76 7.85 372 M 0.88
86 0.139 0.273 0.144 0.546 2.663 9.79 1.90 7.89 379 -0.25 M
37 0.145 0.239 0.158 0.545 2.698 10.73 2.79 7.94 388 -0.08 M 0.1
89 0.175 -0.019 0.188 0.973 2.877 9.09 1.06 8.04 405 M 0.22
83 0.213 -0.022 0.201 0.956 2.888 9.29 1.17 8.12 421 M 0.8
72 0.126 -0.078 0.091 0.336 2.704 7.22 -0.95 8.17 430 M 0.46
27 0.196 -0.024 0.219 0.941 2.899 9.48 1.28 8.20 436 M
57 0.089 0.238 0.164 0.584 2.698 10.75 2.51 8.24 444 0.00 M 0.67
48 0.127 0.265 0.126 0.485 2.669 11.03 2.78 8.26 448 -0.45 M
32 0.000 0.18 0.066 0.964 2.733 8.33 0.06 8.27 451 M 0.58
22 0.128 -0.039 0.115 0.774 2.771 8.23 -0.07 8.30 457 M
44 0.124 -0.027 0.167 0.922 2.895 9.56 1.25 8.31 459 NM
81 0.185 -0.049 0.092 0.609 2.705 8.13 -1.03 9.15 677 NM 0.86
Mean 0.152 7.43 319 -0.19
Std dev 0.056 0.64 85 0.25

Figure 9 Histogram of the distance modulus (X axis) of the stars in the direction of IC 4665 for each spectral type. 

For NGC 6871 most of the observed stars could not be analyzed with the prescriptions to determine the reddening because many of them did not have Hβ measurements. With the compiled sample of Table 9, represented schematically in Figure 3, we realized that most of the stars lie in the early type stars branch. The applicable prescription for early type stars gives the results presented in Table 12. In this table we have separated the stars in three categories depending on their distance; the first group labelled as non-members, and for the second and third group, those below and above distance modulus of 11.5, were labelled as “close” and “far”, respectively. Mean values and standard deviation were calculated for the second and third groups. As can be seen, no overlap is possible, even considering the limits of the standard deviation, assuring us of a separate existence. The histogram of the distance is presented in Figure 10 in which the two groups are clearly discernible.

Table 12: REDDENING AND UNREDDENED PARAMETERS OF NGC 6871 

ID E(b - y) (b - y)0 m0 c0 V0 Mv DM Distance (pc) Membership (pp)
12 0.012 0.328 0.134 0.308 2.620 10.3 4.6 5.6 134 NM
25 0.022 0.228 -0.003 0.286 2.690 11.7 5.5 6.1 168 NM
37 0.484 -0.034 0.135 0.848 2.950 10.4 1.7 8.7 541 NM
10 0.057 0.203 0.137 0.809 2.720 10.0 1.1 9.0 621 NM
8 0.335 -0.115 0.080 -0.004 2.600 7.4 -3.6 11.0 1574 close
27 0.368 -0.088 0.100 0.260 2.730 10.3 -0.7 11.0 1581 close
13 0.320 -0.110 0.096 0.049 2.660 9.0 -2.2 11.2 1734 close
7 0.329 -0.119 0.079 -0.063 2.600 7.4 -3.9 11.3 1806 close
5 0.383 -0.123 0.085 -0.103 2.570 6.3 -5.1 11.4 1886 close
31 0.338 -0.120 0.076 -0.074 2.583 6.95 -4.47 11.42 1924 close
24 0.316 -0.096 0.125 0.190 2.690 10.4 -1.4 11.7 2208 far
11 0.314 -0.114 0.094 0.010 2.630 9.0 -2.9 11.9 2354 far
14 0.307 -0.097 0.092 0.182 2.630 9.5 -2.5 12.0 2459 far
15 0.361 -0.111 0.088 0.041 2.630 9.2 -2.8 12.0 2483 far
21 0.320 -0.080 0.056 0.319 2.660 10.3 -1.8 12.0 2549 far
4 0.330 -0.130 0.089 -0.183 2.570 6.3 -5.8 12.2 2711 far
Mean (close) 11.2 1751 close
Std dev 0.2 149
Mean (far) 12.0 2461 far
Std dev 0.2 171

Figure 10: Histogram of the distance (pc) (X axis) of the stars in the direction of NGC 6871. 

In this figure the stars are grouped in two peaks. A Gaussian fit determined one at a distance of 1750 ± 80 pc and the other at 2430 ± 194 pc. Given the uncertainties one cannot group all the stars in just one cluster because the spread would be too large. We encountered this situation before when we studied the cluster of NGC 6882/5 (Peña et al., 2008) where we found two clusters at distances of 289 ± 92 pc and 1019 ± 134 pc. At the bottom of each group in Table 12 we present the mean values and the standard deviation of reddening E(b - y), distance modulus and distance for the stars that we consider to be members of each cluster. Unfortunately, the membership probability reported in the literature is for only five stars, none of which was measured in this paper.

In the case of the open cluster Dzim 5 it has been suggested in the literature that there is no clear evidence of the existence of the cluster. We have measured, as did Kazlauskas (2013), the fourteen brightest stars in the field. Given the limitation imposed by the telescope-spectrophotometer system, no fainter stars could be observed. In the [m1] - [c1] diagram we can see that all the stars are of spectral types F and later, and there is no evidence of earlier stars. Hence, the analysis with the prescription of Nissen (1988) has to be considered and yields the results presented in Table 13 for the five F type stars shown schematically in Figure 11. They are all located at nearly the same distance, 215 ± 45 pc, and have a [Fe/H] value of -0.14 ± 0.30. This value is close to that determined from the values reported in Column nine of Table 2 of Kazlauskas (2013). The mean values and the standard deviation of reddening E(b - y), distance modulus, and distance for the stars that we consider to be members are presented at the bottom of Table 13. However, the question of the real existence of a cluster constituted by only four or five late type stars still remains.

Table 13: Reddening and unreddened parameters of Dzim 5 

ID E(b - y) (b - y)0 m0 c0 V0 MV DM Distance [Fe/H]
12 0.020 0.285 0.175 0.420 2.668 10.29 3.76 6.53 203 0.164
8 0.022 0.294 0.161 0.381 2.658 10.46 4.07 6.39 190 -0.051
7 0.021 0.294 0.151 0.393 2.655 9.91 3.88 6.03 161 -0.174
14 0.000 0.306 0.167 0.305 2.653 11.94 4.98 6.96 247 0.004
3 0.000 0.340 0.130 0.324 2.605 11.44 4.26 7.19 274 -0.627
Mean 0.01 6.62 215 -0.14
Std dev 0.01 0.46 45 0.30

Figure 11: Histogram of the distance modulus (X axis) of the stars in the direction of Dzim 5. 

Figure 12: Histogram of the distances (pc) to the cluster IC 4665 determined through the GAIA Data Release 2 (GAIA DR2). 

Figure 13: Histogram of the distances (pc) to the cluster NGC 6871 determined through the GAIA Data Release 2 (GAIA DR2). 

Figure 14: Histogram of the distances (pc) to the cluster Dzim 5 determined through the GAIA Data Release 2 (GAIA DR2). 

To determine age one must first determine the temperature of the hottest main sequence stars. The effective temperature of these hottest stars was calculated by plotting the location of all stars on the theoretical grids of Lester, Gray and Kurucz (1986, hereinafter LGK86), after we calculated the unreddened colors (Figures 15, 16 and 17) for the correct chemical composition of the considered model.

Figure 15: Location of the unreddened points of IC 4665 (filled squares) in the LGK86 grids. The values of the effective temperature, indicated in thousands Kelvins as a vertical dashed line and surface gravity, indicated as a horizontal straight line, can be measured. 

Figure 16: As in Figure 15 but for NGC 6871. Location of the unreddened points of the open cluster NGC 6871 (filled squares) in the LGK86 grids. As in Figure 15 the values of effective temperature indicated in thousands Kelvins as a vertical dashed line and surface gravity, indicated as a horizontal straight line, can be measured. 

Figure 17: Location of the unreddened points of Dzim 5 (filled squares) in the LGK86 grids. Values of effective temperature, in Kelvins, and surface gravity are indicated. 

For IC 4665 we have utilized the c 0 vs. Hβ diagram of LGK86 which allows the determination of the temperatures of the hottest star with an accuracy of a few hundreds of degrees (Figure 15). This star is W62 at 16900 K.

For NGC 6871 we had to consider the existence of the two overlapped clusters. For the closest, the two hottest stars over the MS are stars W11 and W15 of 25000K and 23000K, whereas for the other cluster, the hottest star on the MS is star W13 at 35000K (Figure 16). For Dzim 5, Figure 17 represents the unreddened points in the (b - y) vs. c 0 diagram. The hottest star, W15 has a temperature of 6,200 K.

Once the membership and effective temperature have been established, age is determined through the calibrations of Meynet, Mermilliod & Maeder (1993) as a function of the temperature:

• if the logTe is in the range [4.25, 4.56],

log10age=-.3499×logTe+22.476, (1)

• if the logTe is in the range [3.98, 4.25],

log10age=-3.611×logTe+22.956, (2)

• if the logTe is in the range [3.79, 3.98],

log10age=15.142log10Te2 -122.810log10Te+257.518 (3)

The location of the member stars in the isochrones provided by WEBDA has also been done. Since this figure is presented in the customary HR diagram (B - V) vs. V those stars that were determined to be members have been identified in the data set of Hogg & Kron (1955). The chemical composition that best fits the data is 0.019. This model correctly describes the evolutive path. The other important parameters from the isochrone plot of Webda (Geneva) are a distance modulus of 7.73, E(B - V) of 0.174, Av of 0.158 and a log age of 7.65.

In the case of NGC 6871, WEBDA does not report metallicity values and all the stars measured turned out to be early type stars. There was one star of spectral type A which does not belong to the cluster and two more of spectral type G or later for which there is no calibration. In view of this we considered a solar composition. The location of the stars in the LGK86 grids for this cluster is presented in Figure 16. The value of log age is presented in Table 14.

Table 14: Distance and Age determination for each cluster 

Cluster Distance Star Te logTe log age
pc K
IC 4665 343 ± 71 62 16000 4.204 7.775
NGC 6781-I 1713 ± 123 5,7 25000 4.398 7.088
NGC 6781-II 2464 ± 156 4 35000 4.544 6.576
Dzim 5 152 ± 32 15 6200 3.792 9.550

5 Distances to the clusters determined through the GAIA data release 2 (GAIA DR2)

The above mentioned membership determined through the distance distribution on a histogram has been tested on the open cluster Alpha Per (Peña & Sareyan, 2006). However, this determination can be verified using more modern and advanced techniques such as GAIA Data Release 2 for 2018, providing astrometric data from more than a billion sources. The distances cannot be determined merely by inverting the parallax since going from parallax to distance is not trivial. The way to obtain the pure geometric distance is by considering a Bayesian statistical analysis (Luri et al. 2018). Once the parallax has been obtained, the parallax data can be used to infer geocentric distance taking this correction to account for the non-linearity of the transformations and the asymmetry of the resulting probability distribution as mentioned by Bailer-Jones (2018). In their paper they present a set of data of 1.3 billion stars with corrected pure geometric distances from the GAIA DR2 sources.

The data of the 1.3 billion sources are now accessible in the GAIA archive (http://gea.esac.esa.int/archive/) and were used in the present paper to look for the existence of the studied clusters, IC 4665, NGC 6871 and Dzim 5. To do so, we performed a cone search centered on the coordinates (RA/Dec) of the cluster with a radius greater than that assumed by Webda for the cluster, using the whole sample and taking 20 as a magnitude limit.

In the case of NGC 6871 the radius was chosen through visual inspection. In Table 15, Column 1 lists the ID, Column 2, the coordinates from Webda, Column 3, the assumed cluster diameter in arcmin, Column 4, the considered radius which contains the whole cluster, Column 5 the number of stars contained in the cone and Column 6 the distance in parsecs in the histograms (Figures 12, 13 and 14). The uncertainties are the RMS error of the fit. These results are also presented in Table 15 for IC 4665, NGC 6871 and Dzim 5, respectively.

Table 15 Distances to the clusters determined through GAIA data release 2 

ID RA/Dec Assumed cluster diameter Used radius No. Stars in Cone GAIA distance
hh:mim:sec deg:min:sec arcmin arcmin pc
IC 4665 17:46:18 +05:43:00 45 30 33101 342 ± 32
NGC 6871 20:05:59 +35:46:36 18 11 19032 1477 ± 26
DZIM 5 16:27:24 +38:04:00 27 15 1113 238 ± 13

The comparison of our determined distance measures with those in the Gaia catalog DR2 were also done on a star-by-star basis. These are presented in Tables 16, 17 and 18 for IC 4665, NGC 6871 and Dzim 5, respectively; Column 1 lists the ID of Webda, Column 2, the ID of GAIA DR2 ordered by the distance obtained in the present paper (Column 3). Column 4 presents GAIA’s distance and the final column lists the assumed membership in the present paper.

Table 16: IC 4665, star by star distance comparison between GAIA and the present paper 

ID WBDA ID GAIA Dst PP (pc) Dst GAIA (pc) Membership PP
68 4473856639546336640 69 119 N
47 4474127634803192448 81 110 N
56 4474079015773324928 143 155 N
67 4474058984045718400 231 313 N
50 4473670783424690816 247 326 M
66 4474073518215093632 270 340 M
62 4474048263807307776 289 272 M
43 4474064447244215168 301 357 M
65 4474102036798006912 311 343 M
49 4474066504530306688 333 339 M
64 4474059087124940672 335 352 M
76 4474053727005666816 339 307 M
73 4474061835904011776 352 362 M
65 4474071147393145344 364 347 M
82 4474057437857436032 373 322 M
89 4474081588455448320 398 336 M
72 4474106297406021632 430 336 M
44 4474062523098811904 459 616 N
81 4473855501377642368 619 455 N
Mean 334 334
Std dev 51 24

Table 17: NGC 6871, star by star distance comparison between GAIA and the present paper 

ID Webda ID GAIA (DR2) Dst PP (pc) Dst GAIA (pc) Membership (GAIA)
12 2059099444490880000 134 167 NM
25 2059076041181621888 168 1819 close
37 2059070681062443904 541 409 NM
10 2059101604826977152 621 557 NM
8 2059075839349023104 1574 1754 close
27 2059112913509204352 1581 1626 close
13 2059071887978880512 1734 1870 close
7 2059073159271061632 1806 2439 far
5 2059075873709364864 1886 1754 close
31 2059095424401407232 1924 1459 close
24 2059076041181622144 2208 1570 close
11 2059075255233453824 2354 1777 close
14 2059076389104969856 2459 2158 far
15 2059099856807768960 2483 1748 close
21 2059075804989882496 2549 1711 close
4 2059070135632404992 2711 1936 far
Mean (close) 1709 close
Std dev 123
Mean (far) 2178 far
Std dev 252

Table 18: Dzim 5, star by star distance comparison between GAIA and the present paper 

ID Webda ID GAIA Dst PP (pc) Dst GAIA (pc) Membership PP
7 1331325688646042624 161 247 N
8 1331330292850992256 190 246 N
12 1331988758581273600 203 316 M
14 1332086683834797312 247 360 M
3 1332082427523975168 274 790 M
Mean 241 489
Std dev 36 262

6 Discussion and conclusions

Our study of the three clusters through uvby-β   photoelectric photometry has been done and led us to derive interesting results. The first cluster, IC 4665, is a well-known cluster which has served as a prototype for classical works. This allowed us to do two things with our photometry. First, to corroborate the goodness of our photometric values; and second, with an extended basis, to corroborate the previous findings.

Although the observational data of NGC 6871 are scarce, with the GAIA DR2 results we were able to confirm the existence of two accumulations of stars, which, as in the case of NGC 6882/5 (Peña et al. 2008), show up as two distinct clusters in the line of sight. However, there are some differences in interpretation between the GAIA DR2 results and those we obtained through Strömgren photometry: W11, W15, W21, W24, and W31 are placed in the nearest cluster, while we put them in the farthest one; W7 appears in the farthest cluster with the GAIA DR2 results, but in the nearest with ours. There is also the case of W25. We discarded it as a member of either cluster, but GAIA places it in the nearest cluster. As was mentioned in § 3, in our analysis this star presents a high dispersion, as can be seen in Table 9, and this dispersion could have caused the differences in interpretation. There is one star, W101, which we did not observe. We listed it in Table 9 but different sources assigned very discordant values to its magnitude. In view of these discrepancies we did not consider it in the analysis. At any rate, there are two clusters in the same direction regardless of the distance determination technique.

The final cluster, Dzim 5, as here stated and according to previous works, might not be a cluster despite the claim of its existence by Dolidze & Jimsheleishvili (1966). Our findings are puzzling. We found that there is a small group of five or six stars, basically at the same distance, and all are of late spectral type. There is no indication of early type stars, present or past. The comparison with GAIA DR2 confirms the validity of our results since of the five distances determined, four are of the same order of magnitude.

We have compared our findings with those of GAIA DR2. For IC 4665 the results are amazingly coincident, corroborating the goodness of the uvby-β   photometric calibration. For NGC 6871 we found two clusters in the same direction, such as for NGC 6882/5 (Peña at al. 2008). Our comparison with GAIA DR2 is in accordance with the existence of two clusters. Star W25 gives very different results: we determined a distance of 168 pc whereas GAIA fixed its distance at 1682 pc. Stars W4, W5, W7 and W101 do not have distances reported by GAIA. Finally, for Dzim 5 there is an accumulation of a few stars at the same distance determined by GAIA DR2, within the uncertainties. These results, particularly IC 4665, prove, as we did for the open cluster Alpha Per, that the results inferred from uvby-β   photoelectric photometry are trustworthy.

Unveiling the truth of open clusters is not a simple task. The nitty gritty obviously rests on determining the membership of the stars to the cluster. uvby-β   photoelectric photometry is a well-known canonical method. Results like those of the open cluster Alpha Per (Peña & Sareyan, 2006) ensure the credibility of the results. One of these open clusters presented here, IC 4665, which has been well studied, corroborates the goodness of our results since it gives the same results as those previously determined through different methods. There are other clusters which apparently are well-observed, like NGC 6871 but that, when carefully analyzed, reveal that there are few observations (only twenty-three stars with full uvby-β   photoelectric photometry). What was unexpected was the presence of not one, but of another cluster in the same line of sight; the clusters are at distance modulus of 11.2 ± 0.1 and 12.0 ± 0.1. The histogram of the distances to the cluster determined through the GAIA Data Release 2 (GAIA DR2) suggests the presence of another peak. Finally, with respect to Dzim 5 we only add little to the puzzle beyond the categorical statement of its existence by Dolidze & Jimsheleishvili (1966) to the denial of its existence by Kazlauskas et al., (2013), we could not add much. The results of this study showed that the m 1 and c 1 indexes of provided by Kazlauskas et al. had serious errors that could have led the authors to erroneous conclusions. Our findings suggest the presence of a small group of only late type stars at the same distance, a cluster by definition, but we could not find any vestiges of early type stars either in the present or in the past. The GAIA DR2 results also show an accumulation of stars at 238 ± 13 pc, close to the value determined in the present work (152 ± 32 pc).

Acknowledgements

We would like to thank the staff of the OAN for their assistance in securing the observations. This work was partially supported by Papiit IN104917, IG10062 and PAPIME 113016. ARL & CVR thank the IA-UNAM for the opportunity to carry out the observations. Proofreading was done by J. Miller. C. Guzmán, F. Salas, B. Juarez, C. Villarreal, J. Calderón, J. Guillen and J. Díaz assisted us at different stages. Comments and suggestions of an anonymous referee improved the paper. This research has made use of the Simbad databases operated at CDS, Strasbourg, France and the NASA ADS Astronomy Query Form.

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1Based on observations collected at the San Pedro Mártir Observatory, México.

Received: December 04, 2017; Accepted: September 13, 2022

J. D. Paredes: Facultad de Ciencias, Universidad Central de Venezuela, Venezuela.

J. D. Paredes, J. H. Peña, D. S. Piña, and A. Rentería: Instituto de Astronomia, UNAM, Apdo. Postal 70-264, Ciudad de México, México (jhpena@astroscu.unam.mx).

J. H. Peña and A. Rentería: Observatorio Astronómico Nacional de Tonantzintla, Universidad Nacional Autónoma de México, México.

J. H. Peña and D. S. Piña: Facultad de Ciencias, Universidad Nacional Autónoma de México, México.

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