DATA_SET_DESCRIPTION |
Data Set Overview
=================
This is a comprehensive tabulation of asteroid spin vector
determinations, compiled by Agnieszka Kryszczynska and based on
the earlier compilation by Per Magnusson. This is the Oct. 21,
2007 version of the compilation, containing 863 spin vector
determinations. Supplementary information on shape models and
albedo variegation is also included, but only when part of a spin
vector determination.
The following files are included in the data set:
data/spin.tab - A machine-readable ASCII version of the spin
vectors compilation
data/spinrefs.tab - A list of the references cited in spin.tab
data/spinnotes.tab - A list of the notes to the spin.tab table
documents/spin.pdf - An Adobe pdf version of the spin vectors
compilation, designed to be easily readable by eye. It contains
the same information as spin.tab
documents/spininfo.asc - An explanatory document about the spin
vectors compilation
For some asteroids a large number of independent solutions have
been published. This may be confusing for readers who are not
interested in the spin vector determination process as such. For
the benefit of readers who just want reliable results for their
own applications a 'synthesis' is included for each asteroid.
These synthesis results are estimated by Kryszczynska to have a
high reliability and an accuracy in the spin vector direction of
order 10 degrees or less. They were obtained by taking averages
of the most recent independent results, with weights based on the
method used and the amount and type of the input data. This
procedure is necessarily somewhat subjective, and can't replace a
careful evaluation of the original results.
The direction of the spin vectors (defined by the
'right-hand-rule') are given in degrees in the ecliptic system for
equinox B1950.0. The corresponding ecliptic coordinates for
equinox J2000.0 can be obtained by adding 0.7 degrees to all
tabulated longitudes, but this adjustment is far below the level
of accuracy for most spin vector determinations.
The table contains column space for four spin vector directions
per line. These reflect the symmetry properties of most spin
vector determinations. Methods based on aspect dependences (e.g.
amplitude and magnitude methods) tend to give two spin axis
solutions for main-belt asteroid with moderate orbital inclination
(due to the near symmetry of the observational geometries in the
ecliptic plane). Corresponding to each spin axis solution are two
opposite spin vector directions, which are given explicitly in the
table. Thus, whenever the method used does not contain
information on the sense of rotation, 'poles' are interpreted as
spin axis solutions and the implicit spin vector directions are
calculated. The result is generally four different solutions.
Generally the two prograde solutions are placed in the two left
columns and the two retrograde ones in the columns to the right.
If subsequent determinations agree reasonably then corresponding
solutions appear in the same column, making comparison easy. The
4-fold symmetry is not applicable to certain objects. The
distinction between the four groups may break down for objects in
high inclination orbits (e.g. 2 Pallas), for objects with spin
axes close to the ecliptic plane, and for objects whose
lightcurves are difficult to interpret (e.g. 532 Herculina). For
Earth-approaching objects it often reduces to a 2-fold clustering.
For a discussion and analysis of this data set see Kryszczynska et
al. 2007.
This compilation of asteroid spin vectors supersedes the earlier
compilations by Per Magnusson, upon which it has been based.
References
==========
Kryszcznska, A., A. La Spina, P. Paolicchi, A.W. Harris, S.
Breiter, and P. Pravec, New findings on asteroid spin-vector
distributions, Icarus 192, 223-237, 2007.
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CONFIDENCE_LEVEL_NOTE |
Confidence Level Overview
=========================
Sidereal Periods
==========
Only periods accurate enough to bridge inter-apparitional gaps and
produce absolute rotational phases for the whole data set are
included. Less accurate synodic period determinations exist for
many more objects. As evident from the table, the agreement
between sidereal period determinations tend to be either very good
or very bad. This is due to the non-uniform time-distribution of
the observations, which tend to give many well-defined local
chi-square minima.
Ellipsoidal Models
===========
Many pole determination methods are based on a tri-axial ellipsoid
model with semi-axes a>=b>=c rotating about the c-axis.
Corrections for non- geometric scattering and albedo variegation
have often not been made. A warning must therefore be made
against direct identification of the model axis-ratios with the
asteroid shape. Note that the table is not a comprehensive list
of asteroid shapes, but includes models obtained as by-products of
spin vector determinations only.
Albedo Variegation
============
Albedo models are also often by-products of spin-vector
determinations, and therefore noted in the table. However, the
table is not a complete collection of such models.
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