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 Technique
Technique| Peremennye Zvezdy (Variable Stars) 33, No. 8, 2013 Received 21 November; accepted 10 December. 
 N.L. Kroussanova, A.V. Mironov, A.I. Zakharov 
Sternberg Astronomical Institute, Lomonosov Moscow
 State University, 13, University Ave., Moscow 119991, Russia 
 
 
 | Article in PDF | 
 Magnitudes of Bright Northern Stars". The catalog was based on
observations in the
Magnitudes of Bright Northern Stars". The catalog was based on
observations in the  photometric system acquired in the
high-altitude observatory of the Sternberg Astronomical Institute
(SAI) of the Lomonosov Moscow State University (MSU). This
observatory was located in Trans-Ili Alatau mountains (near the
city of Alma-Ata) at an altitude of about 3000 meters above the
sea level. The catalog is often called the Tien Shan Sternberg
catalog. It was demonstrated in several subsequent papers
(Zakharov et al. 2000; Krutyakov et al. 2000; Mironov and Zakharov
2002; Zakharov et al. 2004), from comparison to Hipparcos Hp
magnitudes (ESA, 1997), that the rms error of magnitudes in the
Tien Shan Sternberg catalog was about
 photometric system acquired in the
high-altitude observatory of the Sternberg Astronomical Institute
(SAI) of the Lomonosov Moscow State University (MSU). This
observatory was located in Trans-Ili Alatau mountains (near the
city of Alma-Ata) at an altitude of about 3000 meters above the
sea level. The catalog is often called the Tien Shan Sternberg
catalog. It was demonstrated in several subsequent papers
(Zakharov et al. 2000; Krutyakov et al. 2000; Mironov and Zakharov
2002; Zakharov et al. 2004), from comparison to Hipparcos Hp
magnitudes (ESA, 1997), that the rms error of magnitudes in the
Tien Shan Sternberg catalog was about 
 .
.
This comparison was performed using a special algorithm, so that
coefficients of the non-linear polynomial relating the  difference to
difference to  ,
,  , and
, and  color indices were
calculated. The comparison proved that the difference of the
observed
 color indices were
calculated. The comparison proved that the difference of the
observed  and that calculated using the polynomial,
 and that calculated using the polynomial,
 , namely
, namely 
 did not exceed
 did not exceed 
 for 8766 stars. The
frequency distribution of the differences is shown in Fig. 1. The
rms deviation is
 for 8766 stars. The
frequency distribution of the differences is shown in Fig. 1. The
rms deviation is 
 .
.
Obviously, the spectral energy distributions of these stars give a
possibility to calculate magnitudes in one catalog (Hipparcos)
from magnitudes in the other catalog  rather accurately.
This property allows us to consider the stars of this sample as
candidate photometric standards in the northern sky. Since common
stars in the two catalogs were observed at different times, using
completely different methods, and from different positions (in
space and on the Earth), the close agreement between calculated
and observed values indicates that these stars are not variable
or, at least, have low variability amplitudes. However, to be
valuable standards, the stars should be carefully examined for
variability.
 rather accurately.
This property allows us to consider the stars of this sample as
candidate photometric standards in the northern sky. Since common
stars in the two catalogs were observed at different times, using
completely different methods, and from different positions (in
space and on the Earth), the close agreement between calculated
and observed values indicates that these stars are not variable
or, at least, have low variability amplitudes. However, to be
valuable standards, the stars should be carefully examined for
variability.
Observations obtained during the Hipparcos mission and contained
in the "Hipparcos Epoch Photometry Annex" and "Tycho Epoch
Photometry Annex" lists provide such an opportunity. A technique
was developed in the SAI (Mironov et al. 2003) permitting to
discover brightness variations of stars on the basis of
simultaneous multichannel observations. According to this
technique, an  parameter is calculated; this parameter
evaluates the degree of correlation of individual magnitude
measurements in several channels.
 parameter is calculated; this parameter
evaluates the degree of correlation of individual magnitude
measurements in several channels.
Suppose that, for a star with the number  in the pair of
channels with numbers
 in the pair of
channels with numbers  and
 and  , we have
, we have  simultaneous
observations. Then we can calculate the linear correlation
coefficient, assuming a normal distribution of the variables
 simultaneous
observations. Then we can calculate the linear correlation
coefficient, assuming a normal distribution of the variables  and
and  , according to the formula:
, according to the formula:
 , we have
suggested that the statistics
, we have
suggested that the statistics 
 :
:
Since there exist  channels, one can construct a vector
 channels, one can construct a vector
 with
 with 
 components being generally correlated. From components of the
vector, one can calculate an integrated statistics
components being generally correlated. From components of the
vector, one can calculate an integrated statistics  for
every star:
 for
every star:
 is a projection of the
 is a projection of the
 -dimensional vector
-dimensional vector 
 onto the
 onto the
 -dimensional cube diagonal passing through the point of
origin. We will call this diagonal the main diagonal. For the
three channels,
-dimensional cube diagonal passing through the point of
origin. We will call this diagonal the main diagonal. For the
three channels,  ,
,  and
 and  :
:
 , the star is variable with the probability
0.997. If
, the star is variable with the probability
0.997. If 
 , the probability of the star being
variable is 0.976.
, the probability of the star being
variable is 0.976.
Note that 
 does not mean that the
star cannot be considered variable. It only means that the
Hipparcos material is not good enough to discover its variability.
This is primarily due to the fact that the standard error of
measurements in the
 does not mean that the
star cannot be considered variable. It only means that the
Hipparcos material is not good enough to discover its variability.
This is primarily due to the fact that the standard error of
measurements in the  and
 and  channels is large (about
 channels is large (about
 ).
).
 .
For 130 of them, either the "Tycho Epoch Photometry Annex" does
not provide information about individual measurements in the
.
For 130 of them, either the "Tycho Epoch Photometry Annex" does
not provide information about individual measurements in the  and
and  channels or the table of individual measurements
contains very few reliable data points. For the remaining 8636
stars, the
 channels or the table of individual measurements
contains very few reliable data points. For the remaining 8636
stars, the  statistics was calculated from the formula
(6). These stars will be called "stars of our
sample". The distributions of the
 statistics was calculated from the formula
(6). These stars will be called "stars of our
sample". The distributions of the  parameters for all
stars of our sample and for all three pairs of channels:
 parameters for all
stars of our sample and for all three pairs of channels:  and
 and
 ,
,  and
 and  ,
,  and
 and  are shown in Fig. 2.
 are shown in Fig. 2.
|  | 
| Fig. 2.
Histograms of the three  | 
Most stars of our sample are not variables; nevertheless, their
distribution modes are not zero, as it should be for independent
random variables. For the pair of  and
 and  , the mode was
found to be 0.11865; for the pair of
, the mode was
found to be 0.11865; for the pair of  and
 and  , 0.1672; and
for the pair of
, 0.1672; and
for the pair of  and
 and  , 0.8047. Thus, all the channels
are correlated. The same conclusion was earlier made from other
considerations (Zakharov et al. 2000; Krutyakov et al. 2000). The
correlation for the channel pairs
, 0.8047. Thus, all the channels
are correlated. The same conclusion was earlier made from other
considerations (Zakharov et al. 2000; Krutyakov et al. 2000). The
correlation for the channel pairs  and
 and  ,
,  and
 and  is poor, but for the pair of
is poor, but for the pair of  and
 and  it is strong enough.
The presence of a correlation shifts the
 it is strong enough.
The presence of a correlation shifts the  parameter from
zero, even when there is no true variability. Before calculating
the generalized statistics
 parameter from
zero, even when there is no true variability. Before calculating
the generalized statistics  according to formula
(6), it is necessary to take into account the
influence of the cross-correlation and to subtract corresponding
values of the distribution modes, found for non-variable stars,
from the obtained
 according to formula
(6), it is necessary to take into account the
influence of the cross-correlation and to subtract corresponding
values of the distribution modes, found for non-variable stars,
from the obtained 
 , getting
, getting
 and
 and 
 . The corrected
data points are denoted
. The corrected
data points are denoted 
 ,
,  ,
,
 , and generalized as
, and generalized as  .
.
An analysis of the  statistics for the stars identified
as variables allows us to estimate the effectiveness of the
 statistics for the stars identified
as variables allows us to estimate the effectiveness of the
 technique for discovering low-amplitude stars on the
base of Hipparcos and Tycho data.
 technique for discovering low-amplitude stars on the
base of Hipparcos and Tycho data.
First, consider the stars with GCVS names. There are 181 of them in our sample of 8636 stars.
The fields H49-50 in the Hipparcos catalog contain respectively
the 5th and 95th percentiles of the epoch photometry, i.e.
 (0.05) and
(0.05) and  (0.95). Thus, they provide an estimate of the
magnitudes at maximum and minimum brightness detected during the
time of observations.
(0.95). Thus, they provide an estimate of the
magnitudes at maximum and minimum brightness detected during the
time of observations.
We compared the 
 differences to
the
 differences to
the  parameter. The results for the 181 GCVS stars
are shown in Figs. 3, 5, and 7.
 parameter. The results for the 181 GCVS stars
are shown in Figs. 3, 5, and 7.
|  | 
| Fig. 3.
The relation between  | 
|  | 
| Fig. 4.
The light curves of the variable V2093 Cyg in the  | 
Figure 3 shows that most points are grouped in an area where
 does not exceed 10 and the
 does not exceed 10 and the 
 difference is not larger than
difference is not larger than 
 . The highest values of
. The highest values of
 were found for the stars TX UMa, V505 Per, and
V2093 Cyg. TX UMa is an eclipsing system of the EA/SD type. It has
an amplitude of
 were found for the stars TX UMa, V505 Per, and
V2093 Cyg. TX UMa is an eclipsing system of the EA/SD type. It has
an amplitude of 
 in
 in  band and the period
 band and the period 
 .
It is clear that the star was observed by Hipparcos in different
phases and is easily detected by the
.
It is clear that the star was observed by Hipparcos in different
phases and is easily detected by the  technique. The
eclipsing variable V505 Per belongs to the EA/DM type, its
amplitude being
 technique. The
eclipsing variable V505 Per belongs to the EA/DM type, its
amplitude being 
 . Hipparcos observed four eclipses,
permitting the
. Hipparcos observed four eclipses,
permitting the  technique to detect the variability
reliably. V2093 Cyg has the type LB and an amplitude of
 technique to detect the variability
reliably. V2093 Cyg has the type LB and an amplitude of 
 .
As an example, the light curve of V2093 Cyg is shown in Fig. 4.
Synchronous brightness changes in the three channels are clearly
seen.
.
As an example, the light curve of V2093 Cyg is shown in Fig. 4.
Synchronous brightness changes in the three channels are clearly
seen.  is about 50; this value is very reliable and
indicates that the star is variable.
 is about 50; this value is very reliable and
indicates that the star is variable.
The area of 
 is shown in more detail in Fig. 5.
 is shown in more detail in Fig. 5.
The variables in the 
 range are marked in
the figure. The figure convinces us that the
 range are marked in
the figure. The figure convinces us that the  -technique
makes it possible  to discover such variables as OW Hya, AF Ari,
IO UMa, and MP Del without difficulties. These stars are eclipsing
variables with amplitudes not exceeding
-technique
makes it possible  to discover such variables as OW Hya, AF Ari,
IO UMa, and MP Del without difficulties. These stars are eclipsing
variables with amplitudes not exceeding 
 . More
interesting are the discoveries of EN UMa (DSCTC, amplitude
. More
interesting are the discoveries of EN UMa (DSCTC, amplitude
 ) and V1133 Tau (LPB, amplitude
) and V1133 Tau (LPB, amplitude 
 ). They confirm
that the method is able to detect variability with amplitudes
below the standard error in most channels. The light curve of
EN UMa is shown in Fig. 6.
). They confirm
that the method is able to detect variability with amplitudes
below the standard error in most channels. The light curve of
EN UMa is shown in Fig. 6.
|  | 
| Fig. 6.
Brightness of EN UMa in the  | 
Figure 7 shows, in most detail, the area of the smallest
 values.
 values.
It follows from Fig. 7  that if 
 , then, according
to the theory, we should expect the star to be variable. 54 stars
are situated in the
, then, according
to the theory, we should expect the star to be variable. 54 stars
are situated in the 
 range. The area of
 range. The area of
 mainly contains variables with amplitudes of
 mainly contains variables with amplitudes of
 . They are not detected, primarily
because of large errors in the
. They are not detected, primarily
because of large errors in the  and
 and  channels.
 channels.
Figure 8 shows the light curve of  Eri. The star's
variability type is BY. Despite the small number of observations
(only 9 reliable simultaneous measurements in
 Eri. The star's
variability type is BY. Despite the small number of observations
(only 9 reliable simultaneous measurements in  ,
,  , and
, and
 ), there is a strong correlation.
), there is a strong correlation.
Thus, on the base of simultaneous measurements in individual  ,
,
 , and
, and  bands of the Hipparcos experiment, from 174 GCVS
stars having
 bands of the Hipparcos experiment, from 174 GCVS
stars having 
 below
 below 
 , the
, the  technique found 43 variables (25%) at
technique found 43 variables (25%) at 
 and 59
variables (34%) at
 and 59
variables (34%) at 
 .
.
Consider now the stars of our sample contained in the NSV list.
There are 504 such stars. They all lie in the 
 range. Their positions in the
 range. Their positions in the 
 diagram are shown in Fig. 9. The following
distribution of
 diagram are shown in Fig. 9. The following
distribution of  was found for these 504 stars:
 was found for these 504 stars:
|  | Number of stars | 
|  | 164 | 
|  | 112 | 
|  | 106 | 
|  | 62 | 
|  | 28 | 
|  | 20 | 
|  | 13 | 
| Total | 504 | 
Among the stars under consideration, 
 for 123
objects (24.4%);
 for 123
objects (24.4%); 
 for 61 stars (12%);
 for 61 stars (12%);
 for 33 stars; and
 for 33 stars; and 
 for 13 stars.
Many of these stars should actually be variable. For example, the
relation  of
 for 13 stars.
Many of these stars should actually be variable. For example, the
relation  of  ,
,  ,
,  on the serial number of
observation for NSV 24420 = HIP 89981 is shown in Fig. 10, and a
similar relation for NSV 24923 = HIP 97757, in Fig. 11.
 on the serial number of
observation for NSV 24420 = HIP 89981 is shown in Fig. 10, and a
similar relation for NSV 24923 = HIP 97757, in Fig. 11.
|  | 
| Fig. 10.
Simultaneously measured  | 
|  | 
| Fig. 11.
Simultaneously measured  | 
Both diagrams show repeated simultaneous deviations of brightness from the mean values.
Among the 504 NSV stars, 467 are listed in the AAVSO VSX database; 47 NSV stars do not enter the AAVSO list. The latter stars have the following NSV numbers:
| 02990, | 05426, | 09915, | 13336, | 15165, | 15478, | 15594, | 15755, | 15816, | 16228, | 
| 16351, | 16353, | 16390, | 16738, | 16744, | 17418, | 17882, | 18090, | 19580, | 19751, | 
| 19940, | 20099, | 20109, | 20215, | 20429, | 20619, | 20902, | 20927, | 23672, | 23850, | 
| 24040, | 24405, | 24406, | 24626, | 24669, | 24848, | 24872, | 24881, | 24891, | 24943, | 
| 25003, | 25772, | 25781, | 25891, | 25922, | 25999, | 26115. | 
The numbers in boldface are stars with 
 .
.
Let us now consider briefly the stars from the AAVSO list. Among the 8636 stars in our sample, 792 stars enter the AAVSO Variable Star Index (VSX). 632 of them have GCVS names or NSV numbers (173 and 459 stars, respectively). 160 AAVSO stars are present neither in the GCVS nor in the NSV catalog, while 140 of them, according to the AAVSO data, are periodic variables with known periods.
Of the 181 stars listed in the GCVS, 8 stars are not contained in the VSX. We present these stars, with their MZ0 values, in Table 1.
| star | MV Dra | V0668 Lyr | V0831 Her | EZ UMa | 
|  | -0.695 | -0.512 | 0.894 | 1.304 | 
|  |  |  |  |  | 
| star | FX UMa | V0917 Ori | V0449 Aur | DP Cet | 
|  | 4.704 | 0.244 | 5.673 | 10.596 | 
|  |  |  |  |  | 
The table shows that the  -technique confirms the
variability only for FX UMa, V0449 Aur, and DP Cet, but it should
be remembered that using Hipparcos data for stars with amplitudes
that low permits to detect only about 20% of all variables by
means of the
-technique confirms the
variability only for FX UMa, V0449 Aur, and DP Cet, but it should
be remembered that using Hipparcos data for stars with amplitudes
that low permits to detect only about 20% of all variables by
means of the  technique.
 technique.
First, we quote the description of the variability characteristics (flags in the field H52), as it is given in the documentation of the Hipparcos catalog.
"C" : "constant" stars or, more strictly, stars not detected as variable. These include stars used as photometric standards. The category also included cases noted as variable in the Hipparcos Input Catalogue. Caution must be exercised in assuming that entries flagged "C" are non-variable: they may be variable at levels below the Hipparcos detectability threshold, or they may have shown variability in the past (e.g. Be stars, or long-period eclipsing binaries);
"D": a "duplicity-induced variability" flag was assigned
according to the difference between the "dc" and "ac"
magnitudes and according to the angular separation and magnitude
difference of a double or multiple system. If "D" is set the
entry is not necessary a physical variable, and not necessary seen
as variable in  ("dc scale");
 ("dc scale");
"M": "possibly micro-variable", with amplitude below 0.03 mag (stars classified with high confidence as micro-variable are flagged "U");
"P": "periodic variable". This flag may supersede entries for which flag "D" is also appropriate;
"R": "revised colour index". When the flag "R" is set the  index was corrected during the variability analysis, The
effect of an erroneous
 index was corrected during the variability analysis, The
effect of an erroneous  index is a spurious linear trend in
the
 index is a spurious linear trend in
the  magnitude of the epoch photometry, with no physical
origin. When identified during the data analysis, this could be
taken into account in classifying the type of variability, i.e.
whether spurious or not;
 magnitude of the epoch photometry, with no physical
origin. When identified during the data analysis, this could be
taken into account in classifying the type of variability, i.e.
whether spurious or not;
"U": "unsolved variable". Entries are classified as "unsolved" if they do not fall into the other variability categories - this class also includes irregular or semi-irregular variables, and possible variables with amplitudes more than 0.03 mag;
" ": a "blank" indicates that the entry could not be
classified as variable or constant with any degree of certainty
(e.g. due to presence of one of more outliers in the epoch
photometry).
": a "blank" indicates that the entry could not be
classified as variable or constant with any degree of certainty
(e.g. due to presence of one of more outliers in the epoch
photometry).
181 GCVS stars of our sample have the following types of variability by Hipparcos:
| "  " (blank) | 39 | 
| "M" (possibly micro-variable) | 13 | 
| "P" (periodic variable) | 49 | 
| "U" (unsolved variable) | 58 | 
| "C" (constant) | 22 | 
22 stars are of type "C". They are V1728 Aql, AY Ari, KZ Cam,
AV Cap, HT Cet, EP Cnc, KX Cnc, KU Com, LW Com, LS Com, LU Del,
V0377 Gem, V0831 Her, V0401 Hya, HR Lib, V2711 Oph, V1260 Ori,
V0400 Peg, BU Psc, PV UMa, FI UMa and EV Vir. All these stars have
 , therefore, the
, therefore, the  technique, strictly
speaking, does not permit to establish variability of these stars
based on the results of Hipparcos and Tycho photometry.
 technique, strictly
speaking, does not permit to establish variability of these stars
based on the results of Hipparcos and Tycho photometry.
Among the 49 stars of "P" type, 33 stars have 
 ,
and 29 of them have
,
and 29 of them have 
 . Thus, the
. Thus, the  technique confirms variability for most "P"-type stars.
technique confirms variability for most "P"-type stars.
Among the 58 stars of "U" type, 34 stars have 
 ,
and their variability is not in doubt. V2093 Cyg has the largest
parameter,
,
and their variability is not in doubt. V2093 Cyg has the largest
parameter, 
 .
.
Among the 13 stars of "M" type, three stars have large
probabilities to be variable. These are  Eri (see
Fig 8),
 Eri (see
Fig 8),  Vir,
 Vir,  Aqr. For these stars,
 Aqr. For these stars, 
 . All the others have
. All the others have 
 .
.
39 stars of  the "blank" type have  values ranging
from
 values ranging
from  to
 to  . Only two stars have
. Only two stars have 
 ,
and 3 stars have
,
and 3 stars have 
 . It appears that most stars of
the "blank" type are not variable.
. It appears that most stars of
the "blank" type are not variable.
We have decided that, in spite of the particular
 -parameter, all stars contained in the GCVS, NSV
catalog, in the AAVSO VSX database, or having the  "U", "P",
"D", and "M" Hipparcos variability types, as well as stars for
which we are not able to calculate the
-parameter, all stars contained in the GCVS, NSV
catalog, in the AAVSO VSX database, or having the  "U", "P",
"D", and "M" Hipparcos variability types, as well as stars for
which we are not able to calculate the  parameter,
should be excluded from the candidate standard stars. A total of
7249 stars was left at this stage.
 parameter,
should be excluded from the candidate standard stars. A total of
7249 stars was left at this stage.
Our further examination showed that there were numerous cases of
stars with only one value: 
 , or
, or
 , or
, or 
 , considerably in
excess of 3, while the other parameters were within 2, or maybe
even negative. Most often, we encounter
, considerably in
excess of 3, while the other parameters were within 2, or maybe
even negative. Most often, we encounter 
 , while
, while 
 and
 and 
 do
not suggest simultaneous brightness variations. An example of
deviations that are not due to the star's variability but to other
causes is shown in Fig. 12. Such cases require additional future
analysis.
 do
not suggest simultaneous brightness variations. An example of
deviations that are not due to the star's variability but to other
causes is shown in Fig. 12. Such cases require additional future
analysis.
|  | 
| Fig. 12.
An example of the relation of 
 | 
As a result, we have decided to exclude all stars that have
 as well as those for which at least one of the
parameters,
 as well as those for which at least one of the
parameters, 
 ,
, 
 , or
, or
 exceeds 3, from the list of the
7249 candidate standards.  Thus, the list of candidates was
reduced to 6484 stars. This list is given in Table 2. The columns of
the Table contain HIP numbers; HD numbers; RA(J2000), DE(J2000);
spectral types from the Hipparcos catalog;
 exceeds 3, from the list of the
7249 candidate standards.  Thus, the list of candidates was
reduced to 6484 stars. This list is given in Table 2. The columns of
the Table contain HIP numbers; HD numbers; RA(J2000), DE(J2000);
spectral types from the Hipparcos catalog;  magnitudes,
 magnitudes,  ,
,
 , and
, and  color indices from the Tien Shan catalog; and the
 color indices from the Tien Shan catalog; and the
 parameters.
 parameters.
We recommend to use these stars as standards in various astrophotomeric measurements.
 and
 and  channels and by
the presence of strong correlations between the channels. The
results of individual observations obtained in the process of
preparation of catalogs like 2MASS and SDSS are not available. In
addition, the results of ground-based observations are always
distorted by the presence of correlation between the channels due
to temporal variations of atmospheric extinction. It is hoped that
the data to be obtained during the execution of the planned space
experiments Gaia (Perryman et al. 2005) and Lyra (Zakharov et al.
2013a,b,c), will provide an opportunity to discover and
investigate a large number of new variable stars and to get
representative samples of different types of variables in
different regions of the Galaxy. This will give a chance to obtain
new data on the structure and development of the Milky Way.
 channels and by
the presence of strong correlations between the channels. The
results of individual observations obtained in the process of
preparation of catalogs like 2MASS and SDSS are not available. In
addition, the results of ground-based observations are always
distorted by the presence of correlation between the channels due
to temporal variations of atmospheric extinction. It is hoped that
the data to be obtained during the execution of the planned space
experiments Gaia (Perryman et al. 2005) and Lyra (Zakharov et al.
2013a,b,c), will provide an opportunity to discover and
investigate a large number of new variable stars and to get
representative samples of different types of variables in
different regions of the Galaxy. This will give a chance to obtain
new data on the structure and development of the Milky Way.
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