The previously described calibration curve was applied to
50 CP2 stars from the catalog of stellar spectrophotometry
(Adelman et al. 1989) and to 18 CP2 stars from the Pulkovo
spectrophotometric catalog of bright stars (Alekseeva et al.
1996). For these stars
the HD number, name, peculiarity according to General Catalogue of
Ap and Am stars by Renson et al. (1991), number of the visual
scans, temperature and error obtained from the relationships (1) and (2),
respectively are given in Table 1.
An asterisk following (
) means that this
datum was computed from energy distribution of the PSC.
To test the validity of the proposed method of determination of
for CP2 stars, the temperatures derived from
were compared with those derived by the infrared
flux method, by the Stepien & Dominiczak (1989) method
and with temperatures derived from (B2-G) color index of Geneva photometry.
In the literature there are five papers concerning the CP2 stars
where the effective temperatures are derived by the infrared flux method.
These papers are those by Shallis & Blackwell (1979),
Shallis et al. (1985), Lanz (1985),
Glushneva (1987), Megessier (1988). The star HD 35497
( Tau) is mentioned in the paper by Underhill et al.
(1979), where the effective temperatures are derived by the
same way. The effective temperature for this star derived by Underhill
et al. was taken into consideration as well.
If there are several determinations of
by IRFM
for individual star then the latest determination is considered.
For example, all the CP2 stars investigated by Lanz are mentioned in
Mégessier's paper.
For the common stars with those of Table 1, their
values and the references are given in Cols. 7 and 8, respectively.
The values of
derived from
are compared with those obtained by IRFM for 13 common stars
(see Fig. 2, where the straight line denotes the relation
(IRFM) =
(
)).
One can see, that the agreement appears to be very good.
It is confirmed by the following results:
= 41
127 K, r = 0.972,
= 0.904.
Only for two cool stars: HD 176232 (10 Aql) and
HD 201601 (
Equ) the temperatures derived by Shallis et al.
(1985) and by Shallis & Blackwell (1979),
respectively, are relatively low. Glushneva (1987) has
noted the same disagreement with Shallis &
Blackwell (1979) determinations. So she has redetermined the
effective temperature of the star HD 112185 (
UMa), obtaining
a value of 9470 K, which is higher than that of 8920 K by Shallis &
Blackwell. For this star the effective temperature derived from
is equal 9340 K, this value is in agreement with
the temperature obtained by Glushneva.
Hauck & North (1993) also noted that the temperature derived
by Shallis & Blackwell (1979) for the star HD 358
(
And) is relatively low.
Finally, the effective temperatures derived from
(with the exception of two cool stars) are in the excellent agreement
with
obtained by IRFM.
Stepien & Dominiczak (1989) proposed the new method to
determine the effective temperatures of CP2 stars.
From a fit of the observed visual energy distribution
of CP stars with a solar-composition model, they derived the
flux deficit relative to the model, and then a temperature
correction to the model temperature.
Practically, the method includes two steps: first, the model
temperature is found from the detailed
fit of the Kurucz's model to the observed visual energy
distribution and second, the obtained
should be
transformed to
by using the relation,
defined by Stepien & Dominiczak as:
![]() |
(3) |
Based on this temperature comparison as well as on the conclusions
given by Mégessier (1988) and by Stepien & Dominiczak
(1989) on importance of the Balmer jump in the determination of
the temperature, the values of as mean from the T (PC)
and the T (BJ) were calculated for all stars of Table 2 from
paper of Adelman (1985).
After that, this mean value of
was corrected for
the blanketing effect by using Eq. (3). The resulting temperatures
(
(S&D)) are reported in Col. 9 of Table 1.
Figure 3 gives a plot of
derived from
versus
(S&D) for 47 common stars.
The straight line corresponds to the relation
(
)=
(S&D).
As one can see from Fig. 3, for most of the stars the agreement
between
(
) and
(S&D)
appears to be very good, but for some stars the difference between two
determinations is more than one sigma error. This discrepancy can be the
result of the errors in the computation of the mean value of
from the T (PC) and the T (BJ) or the value of
in our method for individual stars.
The effect of variability of these CP2 stars should be excluded,
because for both methods the same observed energy distribution was
used.
Basically, there are no systematical differences between two sets
of the data that is confirmed by the following results:
= 38
69 K, r = 0.952,
= 0.965.
![]() |
Figure 3:
Comparison of ![]() ![]() |
The photometric methods to determine of CP stars
were proposed in many photometric systems. As a rule, these methods
are based on colors in the visible region of spectrum, thus it is
necessary to correct the color temperature for blanketing effect
to obtain an effective one. Comparisons of
derived by IRFM or by the method of Stepien & Dominiczak
with
(
) and
given
by Hauck & North (1993) show that (
)
color index is a very good estimator of
for CP2 stars.
Moreover the color index (
)can be used without a correction for the blanketing effect,
because this effect is included in the temperature calibration, while
the reddening - free parameters X and Y should be corrected for that.
It should be noted, that the (
) color index
is to be corrected for the interstellar reddening, but the
parameters X and Y are reddening-free.
In order to estimate photometrically the effective temperatures
of CP2 stars the (
) color index was used.
The values of
(
) were taken
from Table 1 of Hauck & North paper for the sample of 21 common stars.
In addition, the values of
(
)for the 38 stars are computed according to the procedure
described by Hauck & North (1993)
and by using the photometric data from the paper by Hauck &
North (1982). The values of
(
) for
the 59 common stars are presented in Col. 10 of Table 1.
Figure 4 gives a plot of the
derived from
versus
(
).
One can see, there are no systematic differences between two
sets of the data, though the scattering of the points in Fig. 4
is high enough (up to 1000 K), especially for the stars with
K.
So, the comparison of
derived from
with
(
) shows that
for 28 stars with
K the agreement
between two sets of data is very good.
The mean difference between
(
)and
(
) is 42
80 K.
For all the stars in our sample the mean effective temperature
difference is
=
(
(
)
= 102
76 K, with a linear correlation coefficient r = 0.938,
and
= 0.975 for the slope of the regression line of
(
) versus
(
).
The comparison of the stars with
K shows
that
(
) are slightly less than
(
).
For these stars the mean difference
is equal
154
124 K.
Probably this difference can be explained by the correction of
(
) color index for interstellar reddening
because it is very hard to separate the effects due to interstellar
reddening from those due to the non-normal energy distribution
of CP2 stars.
It is also confirmed by the conclusion of Hauck &
North (1993) that for CP2 stars with
K the
values of
(
) are less reliable.
For these stars they propose to use the reddening-free parameters
X and Y.
The X and Y parameters of Geneva photometry are primarily related
to and
respectively, but they can be
affected by the stars's peculiarity, especially for CP2 stars
cooler than 11000 K (North & Cramer 1984).
However, for CP2 stars Hauck & North (1993) propose to use
the X and Y parameters and transform
to
through relation between
and
obtained by these authors.
On the other hand, according to results presented by Lanz et al.
(1993) the significant scattering (up to 2000 K) can be observed
for some values of X and the uncertainties in temperatures are rather
large (about 1000 K). In other words, the X parameter may give the same
scattering of points when comparing
(
) with
.
Generally, there are no significant systematical differences between
the temperatures derived from and those
derived from fluxes by other methods. The temperature calibration
derived for B, A and F main sequence stars is applicable to CP2 stars
as well. The temperature derived from
for CP2 stars may be identified with their effective one,
because the influence of the stars's peculiarity on
the Balmer continuum slope near the Balmer jump is negligible.
Taking into account the observational uncertainties of the slope,
the calibration errors, as well as the errors for the mean
interstellar extinction law and for the value E(B-V) for
the reddened stars the error of are calculated
for each star of our sample. The statistical errors of the
temperature determination vary from star to star with their values
ranging from 5% to 10%.
As a rule, the large errors in the temperature determination
related to the stars with large photometric variations.
In our study only Si, Cr and SiCrEu types of CP stars were used,
but this method can be extended to other types of CP stars when
a blanketing effect is less and the temperature derived
from should be close to the effective one.
For example, Hauck & North (1993) have shown that the colour
temperature of CP1 (Am) and of CP4 (He-wk) stars may be
identified with their effective temperature. In the case of
CP3 (MgMn) stars it is less clear, because for these stars
there are a few of direct
determinations.
The fact that their UV flux is normal (Jamar et al. 1978)
suggests that the colour temperature of CP3 stars may be also identified
with their effective one.
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