For any star, its component of radial motion may become visible as a secular
change in its parallax and proper motion. Although the theoretical
possibility of thus deducing radial velocities was realized long ago, only
Hipparcos space astrometry reached an accuracy level permitting a meaningful
search for differences to spectroscopic velocities. There exist different
ways to astrometrically determine stellar radial motion:
(A) Changing trigonometric parallax: This very direct method requires extremely accurate measurements, e.g., even for Barnard's star the expected parallax rate is only 34 microarcsec/yr.
(B) Proper motion varies as the angle to the space-velocity vector changes. Combining Hipparcos data with old stellar positions reaches accuracies around 10 km/s.
(C) Observations of the changing angular separation of stars sharing the same space velocity (e.g., in a moving cluster), yields high accuracies (0.4 km/s) already with Hipparcos data.
D.Dravins, L.Lindegren & S.Madsen: Astrometric Radial Velocities. I. Non-Spectroscopic Methods for Measuring Stellar Radial Velocity; A&A 348, 1040, 1999 .
Moving clusters, whose stars are grouped around the same average velocity
vector, offer a special possibility to determine astrometric radial velocities.
As the cluster moves in the radial direction, it appears to contract or
expand at a rate equal to the relative rate of change in distance.
This can be converted to a linear velocity (in km/s) if the stellar distances
are known, e.g., from trigonometric parallaxes.
Figure: The moving-cluster method for determining astrometric radial velocities. Stars in open moving clusters share the same velocity vector. Parallaxes give the distance, while proper-motion vectors show the fractional change with time of the cluster's angular size. The latter equals the time derivative of distance, yielding the radial velocity.
D.Dravins, L.Lindegren, S.Madsen & J.Holmberg, Astrometric Radial Velocities from Hipparcos, in Proc. ‘Hipparcos - Venice ’97’, ESA SP402, pp.733738, 1997
In essence, this inverts the classical problem of determining the cluster
distance from proper motions and radial velocities, which (due to geometric
projection effects) change across the angle subtended by the cluster.
With the distance accurately known, one solves the problem for the radial
velocity instead. A stringent application of the method, however,
demands a careful consideration of the stellar dynamics in the cluster,
possible cluster expansion, and other effects. (L.Lindegren,
S.Madsen & D.Dravins: Astrometric Radial Velocities. II. Maximum-Likelihood
Estimation of Radial Velocities in Moving Clusters, A&A
356, 1119, 2000).
The application of Hipparcos data to the Ursa Major, Hyades, Coma
Berenices, Pleiades, and Praesepe clusters, and for the
Scorpius-Centaurus, Alpha Persei, and 'HIP 98321' associations has
given astrometric radial velocities for more than 1,000 stars. The
radial motion of the Hyades cluster is determined to within 0.4 km s-1
(standard error), and that of its individual stars to within 0.6 km s-1.
For other clusters, typical accuracies are a few km s-1.
A comparison of these astrometric values with spectroscopic values shows
a good general agreement and, in the case of the best-determined Hyades
cluster, also permits searches for subtle astrophysical differences,
such as evidence for enhanced convective blueshifts of F-dwarf spectra,
and decreased gravitational redshifts in giants.
Figure: Map of the full sky, showing those stars in clusters and associations, whose radial velocities were astrometrically determined from Hipparcos data. Symbol shape identifies different clusters; symbol size denotes apparent magnitude Hp , while symbol shading denotes B-V (note how some clusters are dominated by very blue stars). The Aitoff projection in equatorial coordinates is used.
A full-resolution PostScript image is available (690 kb).
Figure: Proper motions of the program stars over 200,000 years. Best radial-velocity accuracy is obtained in rich nearby clusters with large angular extent, and large proper motions. However, the accuracy in the largest associations (Ursa Major, Scorpius-Centaurus) is limited by the partly unknown expansion of these systems. Stellar paths in the Ursa Major group (green) cover large areas of the sky. The thickness of the proper-motion vectors is inversely proportional to stellar distance: the closest star is Sirius and the two next ones are faint red dwarfs. Proper motions vary greatly among different clusters.
A full-resolution PostScript image is available (650 kb).
S.Madsen, D.Dravins & L.Lindegren: Astrometric Radial Velocities. III. Hipparcos Measurements of Nearby Star Clusters and Associations, A&A 381, 446, 2002.
Differences between astrometric and spectroscopic velocities permit to
better understand physical processes on stellar surfaces (convective lineshifts);
stellar interior structure (gravitational redshifts); and to understand
which spectral features are the best sensors for the true stellar center-of-mass
motion and/or its variations, e.g. for studying small internal motions
in star clusters, or detecting the slight variations induced by exoplanets.

Figure: Systematic differences between spectroscopic radial velocities, and true stellar motions. The plot shows the differences between spectroscopic velocities in the Hyades (mainly from Gunn et al., AJ 96, 198, 1988), and astrometric determinations. An increased blueshift of spectral lines in stars somewhat hotter than the Sun (B-V approx. 0.3-0.5) is theoretically predicted from hydrodynamic models (Dravins & Nordlund, A&A 228, 203, 1990) due to their more vigorous surface convection, causing greater convective blueshifts. Gravitational redshifts of white-dwarf spectra place them far off main-sequence stars. Work is in progress to analyze spectroscopic data for several of these stars.
A full-resolution PostScript image is available (100 kb).
S.Madsen, D.Dravins & L.Lindegren: Astrometric Radial Velocities. III. Hipparcos Measurements of Nearby Star Clusters and Associations, A&A 381, 446, 2002.
Future space astrometry
The accuracies in absolute radial velocities will be improved by future
space astrometry missions such as DIVA
, FAME and GAIA
(Global Astrometric Interferometer for Astrophysics - ESA).
Astrometric radial velocities will be determined not only for stars in
clusters, but also for individual ones, e.g. by measuring their secular
change in proper motion. The astrometry
group at Lund Observatory is actively involved in the planning
of such future projects.
A stringent
definition of "astrometric radial velocity"
The radial velocity determined through purely geometric methods does, in
principle, depend on the coordinate frames and timescales chosen, why there
is a need for a stringent definition for the fundamental concept of "astrometric
radial velocity". A resolution for its stringent definition was
adopted at the IAU XXIV:th General Assembly, Manchester (August 2000).
Publications
Updated JD 2,452,300