The distance moduli of calibrators come from two independent calibrations of Cepheid Period-luminosity relations (Paturel et al. 2002a,b) based on the sample by Gieren et al. (1998) and on the HIPPARCOS Cepheid sample (Lanoix et al. 1999). The apparent magnitudes come from the LEDA database (http://www-obs.univ-lyon1.fr). They are corrected for galactic extinction and inclination effects following the precepts of Schlegel et al. (1998) and Bottinelli et al. (1995), respectively.
The Malmquist bias introduces a major difficulty in estimating
distances of astronomical objects.
It is caused to the fact that faint galaxies are missing in the sample
because of the limiting apparent magnitude (see the review paper by
Teerikorpi 1997).
To reach large distances with limited bias, we have to consider only
intrinsically bright galaxies.
Then, because the method of sosie galaxies selects galaxies having almost the same absolute
magnitude as calibrators, we have to consider the brightest calibrators.
On the other hand, we need a large sample and should not reject too many
calibrators.
The best compromise was judged from histograms of B- and I-absolute magnitudes.
We kept only calibrators satisfying either MB < -19 or MI < -21.
One calibrator (NGC 4603) was rejected because of the large uncertainty
on its distance modulus (0.86 mag).
The 21 remaining calibrators are presented in Table 1
as follows:
Column 1: PGC number from LEDA.
Column 2: NGC number.
Column 3: Distance modulus and its mean error (Paturel et al. 2002a,b).
Column 4: Morphological type from LEDA.
Column 5: Adopted inclination from LEDA following Fouqué et al. (1990).
Column 6: Internal extinction in B following Bottinelli et al. (1995).
Column 7: Galactic Extinction from Schlegel et al. (1998).
Column 8: ,
corrected B-magnitude from LEDA with its actual
uncertainty (Paturel et al. 1997).
Column 9: Same as Col. 8 for I-band magnitudes. The corrections are 0.44 times
the B-band ones (Cols. 6 and 7). This 0.44 factor should be slightly
larger for the internal extinction (Han 1992) but for the method of sosie this correction vanishes
because the inclination is the same for the calibrator and its sosies.
Column 10: log of maximum rotation velocity and its actual uncertainty taken from LEDA.
It is calculated as a weighted mean of
from both the 21-cm line width and
rotation curve.
PGC | NGC | ![]() |
Type | i | Ai | Ag | ![]() |
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0002557 | NGC 224 |
![]() |
Sb | 78.0 | 0.67 | 0.46 |
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0005818 | NGC 598 |
![]() |
Sc | 55.0 | 0.38 | 0.18 |
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|
0013179 | NGC 1365 |
![]() |
SBb | 57.7 | 0.32 | 0.09 |
![]() |
![]() |
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0013602 | NGC 1425 |
![]() |
Sb | 69.5 | 0.54 | 0.06 |
![]() |
![]() |
![]() |
0017819 | NGC 2090 |
![]() |
Sc | 68.3 | 0.54 | 0.17 |
![]() |
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![]() |
0028630 | NGC 3031 |
![]() |
Sab | 59.0 | 0.38 | 0.35 |
![]() |
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![]() |
0030197 | NGC 3198 |
![]() |
SBc | 70.0 | 0.80 | 0.05 |
![]() |
![]() |
![]() |
0031671 | NGC 3319 |
![]() |
SBc | 59.1 | 0.48 | 0.06 |
![]() |
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0032007 | NGC 3351 |
![]() |
SBb | 41.5 | 0.33 | 0.12 |
![]() |
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![]() |
0032192 | NGC 3368 |
![]() |
SBab | 54.7 | 0.21 | 0.11 |
![]() |
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![]() |
0034554 | NGC 3621 |
![]() |
SBcd | 65.6 | 0.64 | 0.35 |
![]() |
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![]() |
0034695 | NGC 3627 |
![]() |
SBb | 57.3 | 0.48 | 0.14 |
![]() |
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0039600 | NGC 4258 |
![]() |
SBbc | 72.0 | 0.65 | 0.07 |
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![]() |
0040692 | NGC 4414 |
![]() |
Sc | 54.0 | 0.41 | 0.08 |
![]() |
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![]() |
0041471 | NGC 4496A |
![]() |
SBd | 48.1 | 0.23 | 0.11 |
![]() |
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|
0041812 | NGC 4535 |
![]() |
SBc | 44.0 | 0.20 | 0.08 |
![]() |
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0041823 | NGC 4536 |
![]() |
SBbc | 58.9 | 0.62 | 0.08 |
![]() |
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0041934 | NGC 4548 |
![]() |
SBb | 37.0 | 0.12 | 0.16 |
![]() |
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0042741 | NGC 4639 |
![]() |
SBbc | 52.0 | 0.30 | 0.11 |
![]() |
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![]() |
0043451 | NGC 4725 |
![]() |
SBab | 54.4 | 0.23 | 0.05 |
![]() |
![]() |
![]() |
0069327 | NGC 7331 |
![]() |
Sbc | 75.0 | 0.62 | 0.39 |
![]() |
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The use of some calibrators (e.g., NGC 598 and NGC 4496A) is debatable because they are faint with poor photometry. This point is discussed in Sect. 5.
Copyright ESO 2002