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[vsnet-obs 4896] Bright BVRI standard stars
- Date: Mon, 20 Jan 1997 01:33:06 -0700
- To: aavso-ccd@physics.mcmaster.ca, vsnet-obs@kusastro.kyoto-u.ac.jp
- From: bas@lowell.Lowell.Edu (Brian Skiff)
- Subject: [vsnet-obs 4896] Bright BVRI standard stars
- Sender: owner-vsnet-obs@kusastro.kyoto-u.ac.jp
20 January 1997
Northern-hemisphere CCD photometrists:
In March 1995 I sent out to 'vsnet' a long note containing a list of 42
BVRI standard stars of intermediate brightness (ranging from about mag. 5 down
to mag. 8). This was by way of encouraging common use of standard photometric
filter passbands among the amateur observers, and to provide a reliable list of
standards for northern hemisphere observers with small telescopes. As most
of you probably know, the AAVSO and other variable-star organizations do not
accept CCD photometry done without filters. Unfiltered photometry simply
cannot be merged with other data to get meaningful astrophysical results.
Since several prominent 'vsnet' contributors report unfiltered photometry, I
should note that such data is fine in the case of dwarf novae, at least in the
case where you want to find out simply if the star is in outburst or not.
The well-known equatorial standard stars observed by Landolt are fine for
many purposes. But because they appear quite low in the sky for many amateur
observers, particularly Europeans, it is not possible to use them to determine
good instrumental color transformations or for extinction. And even those of
us at lower latitudes would like to have some stars more nearly overhead to
determine atmospheric extinction. It turns out there is very little photometry
really good of moderately bright northern stars on the well-established Cousins
VRI system, and clearly a program to establish some new northern standards is
needed to fill this gap.
In the last few weeks I have been prompted to re-examine the situation.
After immersing myself fairly thoroughly in the Cousins VRI literature, I have
compiled a somewhat more complete list of brighter stars for which published
BVRI photometry could be fairly said to be good enough for use as "standards"
(as compared with sequences around variable stars, say, which are not really
standards). There are still far more equatorial stars than I would like, but
any new set will have to be referenced to these higher-weight bona fide
standards. The list of authors involved is quite short, the data coming mainly
from Cousins himself, Landolt, Taylor's work on adjusting various sources to
the Cousins system, and Taylor & Joner's own photometry, plus a few extraneous
sources (such as myself) for some values. The Cousins and Landolt stars can
be regarded as "primary" standards, and the remainder as "secondary" standards.
I'll outline the details of the star and data selection and so on later,
but first I'd like to explain why such a list is even necessary. It will be
convenient to discuss various topics in a question-and-answer form.
1) "What is the difference between the Johnson and Cousins R and I
passbands?"
The effective wavelengths are different, with the Cousins filters
centered at shorter (bluer) wavelengths than Johnson's. Cousins R peaks near
6200A, but has a long redward tail, extending beyond 8000A; the Johnson R
filter is nearly symmetrical and centered at about 6900A. Cousins I covers
the range from about 7200A - 8500A, centered at about 7900A, whereas Johnson I
has a broad passband from about 7500A out past 1 micron, centered near 8800A.
See Figure 1 in Bessell (1983) for a graphic comparison. For what it's worth,
the Cousins and Johnson V systems of magnitudes are (by design) identical
within very small errors---no need to worry about V.
2) "I've been using the bright UBVRI standards out of the annual
'Astronomical Almanac'; what's wrong with these stars?"
Plenty! Too much, in fact. The first problem is that VRI colors are on
the original Johnson system, which has now fallen into disuse because of the
better-defined and fainter Landolt standards. (The rise in detector
sensitivity and increase in telescope apertures among professionals especially
has meant that very few people could even observe the very bright Johnson
standards without completely saturating or risking harm to their instruments.)
This means if you measure V-R and/or R-I colors on the Johnson system, you will
not be able to compare them with practically anyone else's numbers.
The Johnson "Almanac" stars have other problems as well. The Almanac
data derive from a major publication by Johnson et al. (1966) containing an
all-sky survey of bright stars. Although based on measurements using (among
others) the original UBV filters and 1P21 photomultiplier---and hence in effect
defining the system, the data there are noisy by contemporary standards, with
rms scatter in the +/-0.03 range (Landolt's data have an internal precision of
+/-0.005 mag.). In addition, compared to the Cousins system, the VRI colors
show zero-point variations as a function of star color, with reddening (for hot
stars), and even with Right Ascension. The latter effect appears in both V-R
and R-I. It means that observations made at one season will be systematically
bluer or redder from observations taken at another time. For instance, you
observe a program star when it first comes up at dawn, and calibrate against
standards somewhat higher in the sky to the west. Then at the end of the
observing season for that star, you do some more observing, but calibrate now
with stars east of the variable. With the Almanac standards, even if your data
is perfect, your results would differ simply because the colors of the
calibration stars were systematically different between the two sets of data.
Not good!
Why hasn't anybody mentioned these problems before? The news is 10 to 20
years old: the large accidental errors were found by Barry et al. in 1977 and
by Kunkel & Rydgren in 1979; the shifts as a function of RA were first found by
Cousins in 1981; a more thorough analysis of all these problems can be found in
Taylor (1986).
Obviously, the Almanac data should be avoided; the list is also in serious
need of revision/replacement. It is possible to transform data between the
Johnson and Cousins VRI systems, at least for stars of ordinary color. Again,
see Taylor (1986) for the excruciating details.
As an additional aside, much of the data in the 1966 Johnson et al. paper
was summarized in a famous article in the July 1965 issue of "Sky & Telescope"
(Iriarte et al. 1965). These data were also once frequently cited by
professional astronomers (who should have known better!) as having been used
as standards---even though the article states explicitly that they are not, to
wit: "It should be remembered that the new Catalina-Tonantzintla observations
do not define the UBV system." Again, avoid this list as well.
3) "To get some fainter Johnson VRI standards, I've been using stars from
Moffett & Barnes (see, for instance, Moffett & Barnes 1979). Are these OK?"
The internal precision is lots better in these data than for the older
Johnson et al. series. But again, they are on the Johnson system, reduced
against the Johnson et al. 1996 paper. They thus also inherit the zero-point
drift with Right Ascension. You needn't worry about the details in this case,
however, because all the useful data from these papers and several others has
been transformed to Cousins VRI in Taylor's 1986 paper (see his Tables 6, 7,
and 8). Use Taylor's numbers instead of the originals.
4) "Neckel & Chini (1980) published a list of faint UBVRI standards that
cover a wide range of colors and include some stars fairly far north. This
list still gets widely used, too. How about those guys?"
For their VRI data, Neckel & Chini (NC) used a Cousins-like tube/filters
combination to obtain Johnson-system data, using the Iriarte et al. "Sky &
Telescope" article for their standards, which we just trashed. There were
bound to be problems. Taylor et al. (1989) obtained good quality Cousins VRI
data for 54 of the 60 NC stars. They found the V magnitudes to have a strong
systematic error as a function of V-R color; the full amplitude of the
relationship is about 0.04 mag. between the bluest and reddest stars, although
it is not so bad for stars of intermediate color. Again, probably because
they used the Johnson data as calibration, the NC VRI colors also exhibit an
RA drift, amounting to 0.06 mag. at maximum in R-I. Yow! Since Taylor et al.
have obtained much better Cousins data for nearly all the NC stars, you can
continue using these as standards, but with the values presented by Taylor et
al. (see their Table II). I have included a few of these stars in the list
below. That the NC stars had problems was not news even when Taylor et al.
did their work: they were first pointed out by Bessell (1983).
5) "I was able to get a copy of Tarmo Oja's recent paper (Oja 1996),
which contains Johnson-Cousins UBVRI observations of northern stars he reckons
to be used as standards. Are you gonna trash these, too?"
This paper summarizes a set of primary standards and other much-observed
stars he's measured in the course of an extensive program lasting more than a
decade. Since much of the work was done from Scandinavia, some quite far-north
stars are included. Because a large number of observations is involved (some
of the stars measured more than 100 times), these averaged results might be
okay. Alas, the observations and reductions are only very sketchily described,
and there is no statistical analysis in search of problems such as I've
mentioned above, nor comparison with other work---stuff you want to see for
results claiming to define standards. I have been able to compare his V data
for a number of the fainter stars with reliable independent sources, and this
suggests the V magnitudes are good, at least for stars of intermediate color
(I was not able to test very blue or red stars). This is a good sign, but
pending further tests, I don't yet have a "warm, fuzzy feeling" about Oja's
numbers. Even so, I have added four of his stars to the table below.
6) "You've mentioned this RA zero-point drift problem several times. How
do we know the same thing doesn't appear in the Landolt and Cousins data?"
This has indeed been a concern. For many of the Landolt equatorial
standards, "alternative" data is published by Menzies et al. (1991), based on
observations from the South Africa Astronomical Observatory. These results
were carefully tied to the Cousins E-region standards and have small internal
errors. There are clear systematic differences between Landolt and the SAAO
group arising from instrumental effects, but for the purposes of most amateur
observing (i.e. from relatively poor photometric sites), the differences are
"down in the noise". In making reductions with equatorial standards, choose
one set of data or the other, don't average them.
When they compared their data to Landolt's, Menzies et al. found a
disturbing trend as a function of RA in the V magnitudes (see Figure 3 in
Menzies et al. 1991). Later comparison against a third homogeneous dataset
showed that the problem appears to lie in the SAAO data, not in Landolt's (see
the mea culpa in Cousins & Menzies 1993). This three-way intercomparison,
by the way, also showed that the original Cousins E-region standards at -45 Dec
do not have any detectable RA-drift problems. If you're a southern-hemisphere
observer and managed to read this far, you should be using nothing else than
these stars as standards (most recently defined by Menzies et al. 1989).
7) "Okay, you've convinced me I need to use high-quality standard stars
and adopt the Cousins system for V-R and R-I (or V-I). What do I do about
filters?"
This whole business is very nicely covered in Mike Bessell's article in
"CCD Astronomy" magazine, Fall 1995 issue, page 20. This describes the
filter passbands, gives filter recipes for each, and lists (USA) suppliers of
the filters.
The main concern here is to avoid interference filters whose bandpasses
have steep sides, which lead to problems when transforming your data to the
standard system. The litany of problems resulting from CCD data taken with
such rectangular passbands is outlined in a series of publications by Bessell;
particularly see Bessell (1990) for a list of earlier papers, and which also
includes an earlier take on UBVRI filter prescriptions for CCDs. The colored-
glass filters Bessell recommends greatly reduce such problems, and are much
less expensive than interference filters.
This is probably as good a place as any to mention that if you want to
determine even differential magnitudes in one filter, you need to observe in
at least two. The reason is that no matter what you do vis-a-vis CCD chip,
filters, or reductions, your instrumental color system will never match the
original standard system perfectly. You will always need to make at least a
small adjustment to your data to place them on the standard system. This is
necessary even in differential photometry because of the differing colors of
the comparison stars and the variable. This is usually done by finding the
correction as a function of star color. The process is too involved to explain
here in detail, but is well-covered in guides to doing photometry.
Well, which two should you choose? A natural choice for most CCD
observing will be V and R: these provide a tie to familiar V magnitudes, and
the R filter will take advantage of the peak wavelength sensitivity of the CCD
chip, allowing you to go as faint as possible. You might also consider using
V and I instead. The I passband is more useful on Miras and other red stars,
and the added color baseline gives you a better handle on temperature changes
in all variable stars. An I filter also is outside the range of the worst of
light-pollution, so your observations will not be limited so much by city
lights, but instead by the natural skyglow.
+++++++++++++++
Star Selection for Primary and Secondary Standards
Since most observers are using small telescopes, and evidently have been
using some quite bright stars to calibrate their data, the list includes only
stars brighter than about V ~10, and most are brighter than V = 8. (The
brightest has V = 5.2.) This makes them easy to find, and in general each star
is much the brightest one in the field, so that identification is unambiguous.
The CCD exposure nomograms by Zissell (1996) for a typical CCD system on a
60cm (24-inch) telescope show that a 10-second exposure achieves a signal-to-
noise ratio greater than 100 for stars brighter than about mag. 11 in V, R, and
I. A smaller 25cm (10-inch) telescope more commonly used by amateurs will
get the same results for stars about 1.5 magnitude brighter. Thus choosing
standard stars between about mag. 6 and 10 seems a reasonable choice. This
allows exposures short enough so as not to consume much time on standards, but
not so short as to risk shutter-timing errors nor to add scatter to the data
due to atmospheric scintillation.
I first selected stars brighter than V = 7.5 from the main 1983 Landolt
paper (Landolt 1983a), avoiding wide double stars (difficult to do aperture
photometry on) and those having large uncertainty values, indicative of
variability. A few stars were drawn from the unjustly neglected "instrument
stability" paper by Landolt (1983b). These were supplemented by brighter stars
from Taylor's (1986) summary of VRI colors for equatorial standards. As
mentioned above, in this paper VRI photometry from many sources (e.g. Moffett
& Barnes 1979; Crawford, Golson, & Landolt 1971) was transformed to the Cousins
system. Because bright stars are relatively scarce in these lists, this
initial set had several gaps in RA coverage. I thus added selected stars from
Landolt (1983a) and Taylor between V = 7.5 and 8.0 to fill in both in RA and
in color. Some good red-blue pairs are included as "extinction" stars (e.g.
HD 30544 and 30545) as well as for determining rough color transformations.
More exact color transformations should be done with stars throughout the color
range.
To get additional stars farther north, I have scanned papers by Cousins
and by Taylor & Joner. I chose Cousins stars north of +5 Dec, and several
stars in the Hyades and Coma star clusters observed by Taylor & Joner. The
particular stars selected in the two clusters are all mid-F type stars which
served as comparisons for a decade-long study of variability among somewhat
cooler solar-type stars in which I participated (see Radick et al. 1995 and
Radick et al. 1990). These stars are constant at the 0.001 mag. level on the
timescale of a decade. In another open cluster, M67, I have included two
well-observed stars in the "dipper" asterism in the south side of the cluster.
Unlike the fainter "dipper" stars, these two are isolated enough for use with
telescopes of short focal length. Four northern Oja secondary standards are
included as mentioned earlier. In several cases where the published V
magnitudes from UBV photometry are not of high weight, I have opted to use V
magnitudes determined by Erik Olsen from Stromgren photometry. These are tied
directly to the Johnson et al. 1966 data, which closely define the system and
are free of color and seasonal RA-drift effects.
The working list below contains stars from most parts of the HR diagram,
including reddened hot stars, cool dwarfs, a few supergiants, and even a few
extreme O subdwarfs used as spectrophotometric flux standards. All the cooler
dwarfs selected have low chromospheric activity, so shouldn't be spotted
variables (although my 12 years of photometry on HD 10476 shows that it is
variable at the 0.01 mag. level over decadal timescales). Some known variables
of very small amplitude are nevertheless retained; likewise some slightly
variable M giants, kept in order to extend the color range.
The table is largely self-explanatory. I have used HD numbers in
preference to all other designations. The star-name list is repeated at the
bottom with notes added, including Selected Area and HR numbers, etc. The
J2000 positions are from the PPM catalogue, and are given to 1s/0'.1
precision, sufficient to center a star in the typical CCD frame. Next come
the V magnitudes and BVRI colors. The VRI colors are on the Cousins system.
Some of the data are given to just two decimal places when the third decimal
is either not available or I felt the precision was not justified. The
spectral types were drawn from wide variety of sources, sought using the SIMBAD
database. The final column shows the source of the numbers; the codes are
explained at the bottom of the table.
Some other comments:
For many observers the most practical approach to using this list is to
have previously determined color coefficients for your system using a large
number of stars observed over several clear nights. Then assuming these values
as constants, two or three stars can be used on any given night to set
zero-points for a new "unknown" field. This avoids having to establish
instrumental coefficients each night, which requires two or three dozen stars,
and simply can't be done regularly from most sites.
Even if you use no filter, you should try to determine the color term
of your system by using the red and blue stars in the list. Probably the best
method would be to adjust your "wide-open" CCD magnitudes to the R scale as a
function of V-R or R-I. Adjusting to V as a function of V-R or V-I might work
as well for some CCDs. Of course, R = V - (V-R), and V-I = (V-R) + (R-I).
Meanwhile, work on getting some filters for your system!
Finally, it should be noted once again that in principle there is no
way to transform data for emission-line objects like novae and supernovae to
any standard photometric scale based on ordinary stars. The spectra are
simply too dissimilar to avoid systematic errors between different
filter/detector combinations. The problem is most acute toward the blue, but
workable with broadband filters in the red---as long as each system is well
calibrated. This does not mean such data are not useful, but the results will
be on a purely instrumental system that will differ for each observer.
\Brian Skiff (bas@lowell.edu)
++++++++++++++++++++++++++++++
Bright northern BVRI standards
version: 5 January 1997
Name RA (2000) Dec V B-V V-R R-I MK source
HD 315 0 07 44 -2 32.9 6.440 -0.145 -0.037 -0.064 B8IIISi L83a
HD 5612 0 57 54 +13 41.8 6.32 0.90 0.462 0.421 G8III J66/T86
HD 7615 1 16 28 +23 35.4 6.693 0.047 0.06 -0.01 A0 L83b
HD 8949 1 28 23 +7 57.7 6.205 1.12 0.559 0.490 K1III C80/J66
HD 10476 1 42 30 +20 16.1 5.240 0.84 0.461 0.406 K1V Olsen/T86
HD 11257 1 50 52 +11 02.6 5.927 0.30 0.199 0.193 F2Vwl J66/T86
HD 14827 2 25 13 +55 15.3 7.633 0.045 0.028 0.066 A0II Oja96
HD 16160 2 36 05 +6 53.2 5.801 0.987 0.578 0.485 K3-V C80/C84
HD 18145 2 54 47 -0 02.9 6.528 1.048 0.529 0.497 G8II T86
HD 18175 2 55 14 +0 26.2 7.033 1.129 0.572 0.526 K0II T86
HD 18369 2 57 10 +0 26.9 6.628 0.327 0.193 0.191 F0IV T86
HD 19525 3 08 39 +8 28.3 6.286 1.051 0.536 0.481 G9III C80/C84
HD 22211 3 34 49 +6 25.1 6.487 0.634 0.357 0.339 G0 C80/C84
HD 23432 3 45 54 +24 33.3 5.780 -0.04 0.006 -0.027 B8V K91/T86
HD 23441 3 46 03 +24 31.7 6.446 -0.02 0.007 -0.027 A0Vn K91/T86
HD 23841 3 48 31 +9 38.8 6.689 1.233 0.663 0.612 K1III C80/C84
HD 25102 3 59 40 +10 19.8 6.356 0.42 0.252 0.228 F5V J66/T86
HD 27848 4 24 22 +17 04.7 6.962 0.443 0.267 0.250 F6V Olsen/T89
HD 28406 4 29 30 +17 51.8 6.902 0.453 0.276 0.259 F6V Olsen/T89
HD 29225 4 36 41 +15 52.2 6.636 0.433 0.263 0.249 F5V Olsen/T89
HD 30197 4 46 17 +18 44.1 6.01 1.21 0.620 0.533 K4III J66/T86
HD 30544 4 48 39 +3 39.0 7.316 -0.062 -0.016 -0.016 B9 T86
HD 30545 4 48 45 +3 35.3 6.031 1.207 0.598 0.565 K1III T86
HD 31331 4 54 51 +0 28.0 5.992 -0.128 -0.046 -0.055 B5V T86
HD 33647 5 11 41 +0 30.9 6.67 -0.07 -0.020 -0.046 B9Vn J66/T86
HD 34317 5 16 41 +1 56.8 6.422 -0.02 0.015 0.009 A0V J66/T86
HD 35215 5 24 28 +30 11.5 9.411 0.08 0.088 0.070 B1V T89
HD 35407 5 24 36 +2 21.2 6.320 -0.15 -0.055 -0.092 B4IVn J66/T86
HD 37334 5 37 37 -4 56.0 7.150 -0.160 -0.07 -0.09 B1.5V L83b
HD 37352 5 39 15 +30 09.0 7.71 0.12 0.12 0.09 A0 L83b
HD 37557 5 40 36 +28 58.6 7.03 1.15 0.61 0.53 K0 L83b
HD 37981 5 42 58 +14 10.7 6.731 1.096 0.58 0.51 K1IV L83b
HD 39632 5 54 13 +10 35.2 6.111 1.461 0.759 0.686 G9II C80/C84
HD 40210 5 57 25 +0 01.6 6.905 -0.005 0.012 0.014 A0V T86
HD 47240 6 37 53 +4 57.4 6.152 0.152 0.108 0.126 B1Ib C80/C84
HD 48099 6 41 59 +6 20.7 6.349 -0.037 0.018 0.001 O6.5Ve C80/C84
HD 50167 6 52 04 +1 15.1 7.861 1.535 0.826 0.757 K5 L83a
HD 268518 7 04 05 +20 35.8 7.579 0.614 0.352 0.353 G0 Oja96
HD 65079 7 57 04 +2 57.0 7.832 -0.182 -0.055 -0.075 B2Vne L83a
HD 75012 8 47 35 +0 04.7 7.815 0.088 0.047 0.059 B9 T86
M67 F81 8 51 12 +11 45.4 10.027 -0.086 -0.032 -0.036 B8V see note
M67 F170 8 51 30 +11 47.3 9.645 1.357 0.702 0.625 K3III see note
HD 75700 8 51 49 +11 53.7 7.85 1.12 0.567 0.519 K0 TJ85
BD-00 2084 8 53 14 -0 43.5 9.150 1.276 0.649 0.553 K2 L92
HD 79097 9 11 51 -6 58.8 7.601 1.628 0.990 1.100 M0 L83a
HD 82106 9 29 55 +5 39.3 7.201 1.022 0.582 0.493 K3V C80/C84
HD 84542 9 46 10 +6 42.5 5.807 1.636 0.921 0.991 M1.5III C80/C84
HD 85990 9 55 35 -1 07.6 7.997 1.108 0.575 0.515 K0III L83a
HD 86135 9 56 39 -0 27.7 7.835 1.485 0.795 0.728 K5 L83a
HD 94864 10 57 08 -0 18.7 6.877 0.421 0.250 0.243 F5 T86
HD 97991 11 16 12 -3 28.3 7.391 -0.227 -0.102 -0.140 B1V T86
HD100600 11 34 43 +16 47.8 5.948 -0.158 -0.056 -0.100 B4V+B6 Jz66/T86
HD101906 11 43 47 +24 00.6 7.41 0.86 0.48 0.44 G2IV L83b
HD102056 11 44 44 +28 40.2 7.02 -0.00 -0.00 -0.00 Am L83b
HD103095 11 52 59 +37 43.1 6.427 0.753 0.460 0.437 G9Vwl Olsen/T86
HD106542 12 15 14 +16 54.4 6.819 1.184 0.59 0.53 K2 L83b
HD106691 12 16 08 +25 45.6 8.083 0.407 0.238 0.244 F2V Olsen/JT
HD107146 12 19 06 +16 32.9 7.028 0.602 0.33 0.31 G2V L83b
HD107877 12 23 41 +26 58.8 8.364 0.443 0.264 0.257 F5V Olsen/JT
HD108154 12 25 22 +23 13.7 8.569 0.453 0.270 0.269 F8V Olsen/JT
HD108976 12 31 03 +27 43.8 8.554 0.475 0.275 0.271 F7V Olsen/JT
BD+35 2349 12 32 45 +34 35.0 9.53 1.32 0.698 0.613 K2III Oja96
BD+35 2352 12 34 24 +34 19.9 10.19 0.99 0.533 0.475 K0III Oja96
BD+25 2534 12 37 23 +25 04.0 10.510 -0.29 -0.145 -0.17 sdO T89
HD111165 12 47 15 +7 00.5 8.461 1.169 0.568 0.506 K0 T86
HD111397 12 48 54 +14 07.4 5.70 0.02 0.007 0.018 A1V J66/T86
HD118330 13 36 15 -0 55.9 7.062 0.528 0.313 0.311 F8 L83a
BD+30 2431 13 38 25 +29 22.0 10.055 -0.14 -0.065 -0.074 sdB T89
HD122563 14 02 32 +9 41.2 6.196 0.912 0.550 0.545 G8:II: C80/C84
HD126271 14 24 18 +8 05.1 6.189 1.203 0.630 0.555 K4III C80/C84
HD129956 14 45 30 +0 43.0 5.685 -0.022 -0.010 -0.003 B9.5V T86
HD134047 15 07 40 +5 29.9 6.166 0.947 0.487 0.451 G7IIIa C80/C84
HD139195 15 36 30 +10 00.6 5.265 0.945 0.480 0.440 K0IIICN C80
HD139137 15 36 34 -0 33.7 6.509 0.725 0.431 0.412 G8III+A5 T86
HD139308 15 37 29 -0 53.1 7.779 1.275 0.663 0.585 K0III L83a
HD139590 15 39 01 -0 18.7 7.500 0.543 0.312 0.297 G0V L83a
HD140775 15 45 23 +5 26.8 5.578 0.04 0.019 0.014 A0V J66/T86
HD140873 15 46 06 -1 48.3 5.393 -0.032 0.000 -0.009 B8III T86
HD149845 16 37 21 -0 24.8 7.964 1.303 0.682 0.589 K2 L83a
HD157881 17 25 45 +2 06.7 7.540 1.356 0.854 0.768 K7V L83a
HD160233 17 38 41 +4 20.2 9.095 -0.054 -0.003 -0.023 B1V L83a
HD161198 17 43 16 +21 36.5 7.521 0.745 0.45 0.42 G8V L83b
HD161223 17 44 04 +6 03.7 7.435 0.326 0.22 0.24 A2 L83b
HD161242 17 44 13 +5 15.0 7.806 1.284 0.661 0.637 K2 T86
HD161817 17 46 41 +25 45.0 6.982 0.147 0.12 0.14 A7wl L83b
BD+04 3508 17 47 33 +4 50.4 9.326 1.753 0.974 0.900 K5 L83b
HD163153 17 54 58 -7 44.0 6.926 0.759 0.41 0.35 G8IV L83b
HD172365 18 39 37 +5 15.9 6.375 0.79 0.435 0.416 F8Ib-II C80
HD172651 18 41 27 +0 33.9 7.474 1.449 0.767 0.681 K2 L83a
HD172829 18 42 18 +0 09.3 8.447 2.002 1.186 1.120 K5III L83a
HD175544 18 55 47 +0 15.9 7.395 0.107 0.074 0.077 B2V L83a
HD180028 19 14 45 +6 02.9 6.934 0.837 0.475 0.465 F6Ib C80/C84
HD181122 19 18 53 +9 37.1 6.311 1.067 0.537 0.505 G9III C80/C84
HD185025 19 37 16 +0 11.0 8.963 0.206 0.119 0.144 A0 L92
HD185297 19 38 22 +0 20.7 7.216 0.278 0.154 0.166 A7IV L83a
HD186408 19 41 49 +50 31.5 5.980 0.648 0.357 0.341 G1.5V Olsen/T86
HD186427 19 41 52 +50 31.1 6.235 0.660 0.363 0.343 G2.5V Olsen/T86
HD186293 19 43 05 +9 29.4 7.833 1.160 0.575 0.525 K0Ib C80/C84
HD186312 19 43 16 +9 29.8 7.856 1.458 0.765 0.695 K3II C80/C84
HD186535 19 44 41 +8 43.6 6.419 0.952 0.482 0.450 G8III C80/C84
HD195919 20 33 18 +27 27.4 8.981 0.05 0.031 0.038 A2 T89
HD196426 20 37 18 +0 05.8 6.206 -0.087 -0.039 -0.044 B8IIIp T86
HD196573 20 38 16 +1 01.0 7.885 1.641 0.931 0.955 K5 L83a
HD199280 20 56 18 -3 33.7 6.566 -0.076 -0.034 -0.043 B8Vn L83a
HD200340 21 03 00 -0 55.5 6.498 -0.099 -0.037 -0.045 B6V L83a
HD200644 21 04 35 +5 30.2 5.593 1.651 0.860 0.785 K5III C80/C84
HD205556 21 35 56 +5 28.6 8.301 -0.054 -0.021 -0.032 B9 L83a
HD205584 21 36 14 +6 08.2 7.711 1.264 0.617 0.579 K2 T86
BD+28 4211 21 51 11 +28 51.9 10.53 -0.34 -0.147 -0.17 sdO J53/T89
HD209905 22 06 39 +2 26.4 6.496 -0.068 -0.011 -0.036 B9 T86
HD215077 22 42 43 +0 04.3 7.177 0.367 0.224 0.230 F0 T86
HD215093 22 42 49 +0 13.9 6.969 0.311 0.187 0.189 F0 L83a
HD217014 22 57 28 +20 46.1 5.455 0.67 0.373 0.326 G2.5IV Olsen/T86
HD218155 23 05 33 +14 57.6 6.783 0.004 -0.01 -0.01 A0V L83b
HD218537 23 07 48 +63 38.0 6.25 -0.01 0.025 -0.030 B3V J66/T86
HD219134 23 13 17 +57 10.1 5.57 1.010 0.584 0.478 K3V J66/T86
HD223963 23 54 03 -9 17.4 7.200 1.581 0.91 0.95 M0III L83b
HD224155 23 55 38 +8 13.4 6.818 -0.003 -0.015 -0.010 A0V C80/C84
sources: C80 = Cousins 1980, C84 = Cousins 1984,
L83a = Landolt 1983a, L83b = Landolt 1983b, L92 = Landolt 1992;
T86 = Taylor 1986, T89 = Taylor et al. 1989 ;
Jz66 = Jerzykiewicz 1966, J66 = Johnson et al. 1966;
K91 = Kornilov et al 1991; TJ85 = Taylor & Joner 1985;
GO76 = Gronbech & Olsen 1976, Olsen = various pubs by Olsen;
Oja96 = Oja 1996.
Notes:
HD 315 HR 11.
HD 5612 HR 276.
HD 7615
HD 8949 HR 426 = NSV 519. the brighter of a wide pair: BD+07 214 at 1'.1,
V=8.0, G0.
HD 10476 HR 493 = 107 Psc. large proper motion.
HD 11257 HR 534. V from K91+AT95.
HD 14827
HD 16160 HR 753. large proper motion.
HD 18145 SA 94-32.
HD 18175 SA 94-293.
HD 18369 SA 94-319.
HD 19525 HR 942.
HD 22211 HR 1089.
HD 23432 HR 1151 = 21 Tau = Asterope in Pleiades.
HD 23441 HR 1152 = 22 Tau in Pleiades.
HD 23841
HD 25102 HR 1233. V from K91.
HD 27848 vB 51 in Hyades.
HD 28406 vB 78 in Hyades.
HD 29225 vB 101 in Hyades.
HD 30197 HR 1517, near open cluster NGC 1647.
HD 30544
HD 30545 HR 1534.
HD 31331 HR 1574 = SA 96-837.
HD 33647 HR 1690 = V1085 Ori (very small amplitude). V from K91+GO76.
HD 34317 HR 1724. V from GO76.
HD 35215 B-V from Hiltner (1956).
HD 35407 HR 1786. V from GO76.
HD 37334 NSV 2471, probably slightly variable in V, but colors stable.
HD 37352
HD 37557
HD 37981
HD 39632 HR 2048.
HD 40210 SA 97-257.
HD 47240 HR 2432.
HD 48099 HR 2467.
HD 50167 ADS 5533: sep. ~2" with large delta-mag.
HD 268518
HD 65079
HD 75012 northern star of a wide pair.
M67 F81 blue straggler in M67. VRI from Joner & Taylor 1990
(PASP 102, 1004), B-V from Montgomery et al. 1993 (AJ 106, 181).
M67 F170 BD+12 1926 (sic, this BD name applies to the entire cluster).
V from BSkiff, BVRI colors as for M67 F81.
HD 75700 bright field star on northeast side of M67. BV data from Eggen
(1964 ApJ 140,130).
BD-00 2084 SA 100-162.
HD 79097 possibly slightly variable in V, but colors stable.
HD 82106 bright, large proper motion star not in PPM.
HD 84542 HR 3876; slightly variable in V, but colors stable.
HD 85990 SA 101-24.
HD 86135 SA 101-333.
HD 94864 SA 102-1085.
HD 97991 also V = 7.394, B-V = -0.224 (C84).
HD100600 HR 4456.
HD101906
HD102056
HD103095 HR 4550. V from Olsen, B-V from Jz66. very high proper motion.
HD106542
HD106691 in Coma star cluster.
HD107146
HD107877 in Coma star cluster.
HD108154 in Coma star cluster.
HD108976 in Coma star cluster.
BD+25 2534 Feige 66; B-V adopted from Colina & Bohlin 1994 (AJ 108, 1931).
BD+30 2431 Feige 86; B-V is mean of several published values.
HD111133 HR 4854. also V = 6.327, B-V = -0.051 (C84).
HD111165 also V = 8.465, B-V = 1.167 (C84).
HD111397 HR 4865 = 29 Com.
HD118330 SA 105-214.
HD122563 HR 5270. extreme metal-weak giant.
HD126271 HR 5394 = NSV 6655.
HD129956 108 Vir = HR 5501.
HD134047 HR 5631.
HD139137 14 Ser = HR 5799 = SA 107-298. composite spectrum.
HD139195 HR 5802 = 16 Ser.
HD139308 SA 107-35.
HD139590 SA 107-595.
HD140775 HR 5859. V from GO76.
HD140873 25 Ser = HR 5863.
HD149845 SA 108-827.
HD157881 large proper motion.
HD160233
HD161198
HD161223 in region of open cluster IC 4665.
HD161242 in region of open cluster IC 4665.
HD161817
BD+04 3508
HD163153
HD172365 HR 7008 in open cluster IC 4756. B-V from Cousins 1965
(MNSSA 24, 120).
HD172651 SA 110-471.
HD172829 HK Aquilae (constant) = SA 110-353. the reddest Landolt standard
brighter than V mag. 10.
HD175544
HD180028
HD181122 HR 7325.
HD185025 SA 111-773.
HD185297 SA 111-1496 = ADS 12708: sep. ~1".
HD186408 HR 7503 = 16 Cyg A. B-V from USNO.
HD186427 HR 7504 = 16 Cyg B. B-V from USNO.
HD186293 preceding of two stars.
HD186312 following of two stars.
HD186535
HD195919 B-V uncertain.
HD196426 HR 7878.
HD196573
HD199280 HR 8014.
HD200340 HR 8054.
HD200644 HR 8066 = 3 Equ.
HD205556
HD205584
BD+28 4211
HD209905
HD215077 SA 114-69.
HD215093 SA 114-172.
HD217014 HR 8729 = 51 Peg. B-V from J66.
HD218155
HD218537 HR 8808.
HD219134 HR 8832.
HD223963
HD224155 B-V uncertain.
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