Table name: PPM Records: 326518 Spectral Band: OPT Kind of Object: Star Mode: Proper Motion,Astrometry PreView: Coordinates: J2000
Name Type Meaning
ppm i PPM star number
sao i SAO star number
hd i HD star number
agk3 c AGK3 star number
name c Durchmusterung star number
sp c Spectral type
mag i Visual magnitude (99.9 if unknown)
r_a i Right ascension for epoch + equinox J2000, FK5
dec i Declination for epoch + equinox J2000, FK5
e_pos f Standard position error, in arcsec
pma f Annual proper motion (mu)_(alp) (arcsec/yr)
pmd f Annual proper motion (mu)_(del) (arcsec/yr)
e_pma f Mean error on (mu)_(alp) (arcsec)
e_pmd f Mean error on (mu)_(del) (arcsec)
ep_ra i Weighted mean epoch for RA in years since 1900
ep_dec i Weighted mean epoch for Dec in years since 1900
notes c Notes with the following meaning:
P problem case, preferably not to be used as
astrometric reference star.
C a critical remark on this object is given in the
List of Critical Remarks, it should not be used
as astrometric refe- rence star.
D double star, preferably not to be used as
astrometric reference star.
H member of the High-Precision Subset (HPS) of PPM.
F member of FK5, high precision stars, mostly very
bright stars.
R a remark on this star is given in the List of
Remarks on Individual Stars.
Computed Fields
_ra I Right ascension for epoch + equinox B1950, FK4
_de I Declination for epoch + equinox B1950, FK4
_lii I Galactic Longitude
_bii I Galactic Latitude
The stars in each of the source catalogues were identified with the objects of the star list. This was done in a fully automatic process. Problem cases recognized in this process were investigated manually to detect typing errors in the source catalogues, to correctly identify double star components, to avoid the effect of grossly incorrect positions in the star list etc.
Prior to the identification of Astrographic Catalogue data (given as x,y plate coordinates originally) a rough plate reduction was performed, using published approximate plate constants.
Another group of stars was subject to manual checks: Those AGK3 stars not found in any source catalogue except AGK2 and AGK3 (about 60 cases). We checked these for coarse errors of AGK3 by locating the stars on Palomar Sky Survey prints - with a precision of a few arcsec. In most cases they were found at the predicted positions. Nine cases were indeed caused by errors in both AGK2 and AGK3. We kept the data for these nine objects, but marked them as severe problem cases (see flag 'C' in column 19.1 of the printed catalogue).
The first part became necessary because of the discovery of two sorts of systematic deviations between the preliminary system and the FK4 system:
More details on the construction and properties of the system of PPM will be given by Roeser (1989).
Much manual labour went into the provision of cross-references. They were determined by different methods, ranging from direct cross-identification (based on positions only) to simply copying historic work done by others (in the cases of catalogues having low positional accuracy such as DM and HD). Cross-references are given explicitly for four catalogues: Bonner Durchmusterung (abbreviated DM), SAO Catalogue, Henry Draper Catalogue (HD) and AGK3. Three more cross-references are given implicitly by flags (see columns 19 of the printed catalogue): Flag 'F' in column 19.4 denotes the stars contained in FK5 (Parts I and II). Flag 'H' in column 19.3 indicates stars that are contained in AGK3R and/or one of the CMC catalogues. The double star flag 'D' (column 19.2) was created by cross-referencing PPM with the Catalogue of Components of Double and Multiple Stars (Dommanget, 1988).
The magnitudes and spectral types were copied either from AGK3 or from FK5, see Chapter 8 for details.
Various sorts of auxiliary information are given in the List of Critical Comments and in the List of Remarks (Chapters 5 and 6),
Error budget of PPM
set of stars No. No. mean epochs mean err. mean err.
stars obs. prop. mot. pos. 1990
PPM, all stars 181731 6.2 1931.5 1930.7 0.43 0.42 0.27 0.27
PPM, HPS stars 31841 7.8 1950.3 1948.0 0.24 0.25 0.12 0.12
PPM, FK5 stars 1365 --- 1954.2 1945.2 0.08 0.10 0.04 0.05
AGK3 181581 2.0 1945 1945 0.95 0.95 0.45 0.45
SAOC, north 133000 2.0 1930 1930 1.5 1.5 0.9 0.9
Three subsets of PPM are shown in the table: The first line refers to the
entire catalogue, the last line to the 1365 FK5 stars and the second line to
the High-Precision Subset (HPS) of PPM. This subset will be briefly
discussed now.PPM essentially was constructed by combining AGK3 with early-epoch catalogues. So the mean epochs of PPM are quite early and the present-day accuracy is dominated by the accuracy of the proper motions. Therefore it would be highly desirable to have a repetition of AGK3 at present epoch. This not being available, we decided to introduce the Carlsberg Meridian Circle (CMC) catalogues, nos. 1 to 4. (CMC 1985 -1988). In addition we introduced AGK3R because of its higher accuracy compared to AGK3. The High-Precision Subset of PPM is defined as the set of PPM stars for which either CMC or AGK3R observations are available. Its superior precision in present-day positions is mainly due to the fine work done at the Carlsberg Meridian Circle.
Note that (on average) more than 6 measured positions are available per star. This redundancy allowed us to discover (and avoid) a large number of coarse errors in the source catalogues. It ensures that PPM contains very few coarse errors. For 1064 PPM stars the redundancy was not sufficient to resolve discrepancies between the source positions. They carry the 'P' flag mentioned above.
Source Catalogues Astrographic Catalogue zones 466 278 AGK3 181 581 AGK2 181 581 AGK1 141 146 Yale zone catalogues 80 574 Gyllenberg, 1926 11 498 Prager, 1923 8 602 CMC 1, 2, 3, 4 25 656 AGK3R 20 581 Total 1 117 497
These numbers do not hold, however, for a few special groups of objects: The very blue stars (spectral types B2 and earlier), the very faint stars (fainter than about 12 in photographic magnitude) and the very bright stars (brighter than about 7, but not in HPS or FK5). Because these groups are very small by number it was neither possible to check our preliminary system to the desired accuracy, nor could we correct the individual source catalogues to this system with the desired accuracy. So we just do not know anything about possible systematic errors for these small groups.
Another possible systematic error stands out clearly from our data, but still cannot be removed. It is a magnitude equation in right ascension, affecting stars fainter than about 10.5 mag (photographic). It shows up as a systematic difference between PPM and the CMC catalogues (remember that, by definition, the magnitude dependence of the proper motion system of PPM is that of AGK3. The CMC catalogues were transformed to that system before inclusion into PPM). It has a mean value of about 0.08 arcsec for stars between 10.6 and 11.0 mag, and 0.15 arcsec for stars fainter than 11.0 mag. The cause of this systematic difference cannot be identified with existing astrometric data. Therefore it cannot be removed in a reasonable way. More details will be given by Roeser (1989).
We gratefully acknowledge the help of Hamburger Sternwarte (C. de Vegt and H. M. Steinbach) and of Observatoire de Strasbourg (D. Egret and A. Fresneau) in providing the raw Astrographic Catalogue on punched cards. Several tons of cards were moved with the help of many hands in Strasbourg. Also we thank T. Corbin of US Naval Observatory for providing a magnetic tape containing part of the Strasbourg punched data already.
Heidelberger Druckmaschinen AG is gratefully acknowledged for technical help in the reading of the punched cards.
We thank the CMC group at La Palma for giving the CMC 4 catalogue to us prior to publication.
Last but not least we have to thank many people at our institute, especially E. Roehl and E. Mueller for careful checks and completion of the Astrographic Catalogue data, M. Erbach, M. Fleischer and T. Lederle for much valuable information on source catalogues, H. Schwan for many fruitful discussions and for his data on systematic differences between several catalogues, R. Bien for the determination of weights for the CMC catalogues and H. Bernstein for advice on mathematical statistics. Finally we want to thank R. Wielen, director of ARI, for giving us the opportunity to do this work.
To apply PPM as astrometric reference at a different observational epoch, but still in the J2000 coordinate system, proper motions must be taken into account. For most purposes a simple linear formula (position difference equals epoch difference times proper motion) is sufficient. But note that this procedure will give inaccurate results close to the pole. Better formulae are given e.g. by Murray (1983) and in the introduction to FK5.
To apply PPM as astrometric reference for a different equator and equinox, but still in the IAU (1976) system of astronomical constants, precession has to be taken into account. The relevant formulae and numerical values are given e.g. by Lieske (1979) and in the introduction to FK5.
Note that simply precessing from J2000 to B1950 will still not give results in the old (FK4) astronomical coordinate system. This differs from the new IAU (1976) system by a correction to the precessional constant, a correction to the position of the vernal equinox, by the treatment of elliptical aberration and by complicated zonal corrections. All this adds up to several tenths of an arcsec in position and a few tenths of an arcsec per century in proper motion.
Application of proper motion and precession still gives mean positions. In order to derive apparent positions for PPM objects one has to apply nutation, aberration, stellar parallax, and relativistic light-bending, in addition (see e.g. Murray, 1983). For most practical uses of PPM these effects can be ignored. But PPM contains a small number of stars with fairly large paral- laxes. They are not indicated in the catalogue.
For each star PPM gives mean errors for right ascension and declination at their respective mean epochs T. Standard error propagation calculus can be used to calculate the mean error of a PPM position for an epoch t different from the mean epoch: Denoting the mean error of one coordinate at mean epoch by E(T), the mean error of proper motion by E(PM), the mean error of position at epoch t is given by
E(t)^2 = E(T)^2 + E(PM)^2 * (T-t)^2
Using more PPM stars in an application will usually give better results because of the partial cancellation of the purely accidental errors of the PPM data. However, this improvement will never get beyond the systematic errors of PPM, as discussed in the previous chapter.
Applications demanding utmost accuracy rather than high star density should use HPS stars only.