Like the Sun and its
sunspots,
cool stars or chemically peculiar stars are know to exhibit abundance,
brightness and/or magnetic surface inhomogeneities. If we cannot yet resolve these stars
with direct stellar surface imaging techniques (i.e. interferometry) yet,
indirect methods have been developed to help us examine the detailed distribution
of such surface inhomogeneities, as we do for instance on our Sun, and get some information
of the underlying physical processes, namely the dynamo and
microscopic diffusion phenomena.
For rapidly rotating objects, spectroscopic observations recorded with both high spectral
and temporal resolution can be converted into spatially
resolved maps of stellar surfaces. We first use the fact that stellar rotation (through
the
Doppler effect) associates different radial velocities to different regions of the visible
stellar hemisphere, for instance negative and positive radial velocities for the approaching
and receding limbs respectively. Therefore, as the star rotates and surface inhomogeneities
get carried accross the visible hemisphere, the associated spectral line profile distortions
will successively appear at different radial velocities. Following such spot-induced profile
distortions in either unpolarised or polarised light in dynamic spectra can tell us (with the
help of tomographic techniques) where the parent spots are located at the surface of the star,
what is the brightness, abundance or magnetic field strength inside the spots, but also
how field lines are oriented within these spots. These techniques are known as
Doppler imaging (DI) when the aim is to image brightness/abundance
inhomogeneities imaging of stellar surfaces, and Zeeman-Doppler imaging
(ZDI) in the case of magnetic field imaging. With ZDI, we obtained the
first magnetic image (i.e. with no a priori constraint on
the large-scale field topology) of a star other than the Sun.
Below is an example of unpolarised (Stokes I, left panel) and
circularly polarised (Stokes V, right panel) dynamic spectra
one can obtain, in the particular case of AB Dor, a very young star that arrived very recently
on the main sequence. One can distinctly see on these graphs line profile distoritions
moving from the left side of the line profile (depicted with
a vertical line at velocity -60 km/s) to the right side of the
line profile (depicted with a vertical line at velocity 120 km/s). In such a graph,
spots at different latitudes cross the line profile at different rates: a spot near the
equator crosses the whole line profile from the blue wing (at
-60 km/s) to the red wing (at 120 km/s), while a spot near the
rotation pole only affects the central part of the line profile (around a radial
velocity of 30 km/s). Similarly, the way the amplitude
of the Stokes V signatures are modulated throughout their transit across the spectral line
tells us (to a certain extent) how the magnetic field is oriented
within the corresponding magnetic region.
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The brightness (upper panel) and magnetic
(lower panels) maps reconstructed from the above data set are presented below.
One can see that fairly detailed maps of the stellar surface (typical longitude resolution
of about 3 degrees close to the equator in this particular example) can be obtained with
such a technique.
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Monitoring the long-term evolution of such magnetic topologies can tell us which type of dynamo process is operating in these objects, and gives us a unique opportunity of studying magnetic activity cycles in stars other than the Sun. In the particular maps shown above, up to ten different brightness features and twelve magnetic regions of opposite polarities can be identified. Note in particular that the azimuthal component of the vector field is significant, and is probably generated by a non-solar type dynamo, distributed throughout the whole convective zone.
Comparing different brightness/magnetic maps obtained several rotation cycles apart also enables us to measure the amount of surface differential rotation on a star. In the particular case of AB Dor, we proved that the differential rotation of this object is very similar to that of the Sun both in sense (with a pole rotating slower than the equator) and magnitude (about 120 d are required for the equator to lap the pole by one complete rotational cycle) even though this star rotates more than 50 times faster than the Sun.
Yet another potential application is to extrapolate the reconstructed photospheric field up to the corona (see above in the particular case of one of our AB Dor images). In a second step, we compare the resulting 3D magnetic structure (and its temporal evolution) with successive maps of the magnetically confined prominences (the stellar analogue of solar prominences, see below) that orbit the star (detected through the signatures they imprint in strong spectral lines such as Halpha for instance). It gives us the opportunity of studying the dynamics of stellar coronae in a very broad context by extending the solar studies to rapid rotators where the centrifugal force plays a major role. This work is done in collaboration with M. Jardine and, A. Collier Cameron, from the School of Physics and Astronomy at the University of St. Andrews in Scotland: many other similar images and movies can be found on their own web sites.
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