|
A Japanese/US collaboration led by a researcher from the University of Tokyo
observed the transiting extrasolar planetary system TrES-1 and measured the
angle between the stellar spin axis and the planetary orbital axis using
the Subaru Telescope High Dispersion Spectrograph (HDS). By measuring the
degree of alignment in transiting systems, one can constraint planetary
formation models proposed to explain the diverse properties of extrasolar
planets. It was the third case and the faintest target so far for which
the spin-orbit alignment has been measured.
There are over 200 extrasolar planets that have been discovered so far.
The discovery and characterization of extrasolar planets have revealed a
diversity of planetary systems, and variety of theoretical models have
been proposed to explain the complex process of planet formation.
The alignment of the stellar spin axis and the planetary orbital axis
(Figure 1) is known to be a promising diagnostic for discriminating planet
formation mechanisms by observations. For example, models considering
giant planet scattering naturally predict tilts from the original orbital
axis and thereby such planets would usually have significant misalignments.
However planets which form and migrate inward within proto-planetary disks
would generally have negligible misalignments.
In transiting extrasolar planetary system (Note 1), one can measure the
spin-orbit alignments by exploiting the Rossiter-McLaughlin effect (Figure 2).
Such measurements have been conducted for two bright transiting systems with
the Keck Telescope by an international research team led by Prof. Joshua Winn,
one of the co-investigators of the Subaru team, at MIT. On the other hand,
a Japanese/US collaboration led by a graduate student Norio Narita at
the University of Tokyo (Japan Society for Promotion of Science Fellow, DC2)
observed a faint transiting system TrES-1 (Note 2) with the Subaru Telescope
High Dispersion Spectrograph (HDS) at Mauna Kea and the MAGNUM 2 m Telescope
at Haleakala, both in Hawaii (Figure 3). The team succeeded in detecting the
Rossiter-McLaughlin effect (Figure 4) for the first time for this target and
constrained the alignment angle as 30 degrees with an error of plus or minus
21 degrees, clearly indicating the prograde orbital motion of TrES-1b.
It was the third case for which the spin-orbit alignment has been measured,
and importantly it is the faintest target (with a visual magnitude of about
12, which is only about 2 % as bright as the previous targets) so far.
The team has demonstrated for the first time that such measurements
are possible for such a faint target. This is important because most of the
newly discovered transiting planets from ongoing transit surveys have
relatively faint host stars. Norio Narita says, "by combining future
observations of the Rossiter-McLaughlin effect in other transiting systems,
we will be able to determine the distribution of the spin-orbit alignment
angles for exoplanetary systems. Moreover, further observations would have
the potential to discover large spin-orbit misalignments, if any, which
would inspire numerous theoretical investigations."
This result will be published in the August 25, 2007 issue of
Publications of Astronomical Society of Japan.
Measurement of the Rossiter--McLaughlin Effect
in the Transiting Exoplanetary System TrES-1
Narita, N., Enya, K., Sato, B., Ohta, Y., Winn, J. N., Suto, Y., Taruya, A.,
Turner, E. L., Aoki, W., Tamura, M., Yamada, T., Yoshii, Y. 2007,
Publ. Astron. Soc. Japan, vol 59, No. 4, 763-770
Note 1: Extrasolar planetary systems in which a planet's orbit passes in front of
its host star (namely, causing eclipse) are called transiting extrasolar
planetary systems.
Note 2: TrES-1 is a main sequence K0 star and its planet TrES-1b was discovered by
a transit survey in 2004. TrES-1b is a gaseous giant orbiting the host star
with a period of about 3 days (one of the so called "hot Jupiter" class of
extrasolar planets).
|
Figure1: An illustration of the concept of the spin-orbit alignment (described by
lambda) in an exoplanetary system.
|
|
Figure 2: The Rossiter-McLaughlin effect is defined as the radial velocity anomaly
during a transit from the known Keplerian orbit caused by the partial
occultation of the rotating stellar disk. For example, if a planet occults
part of the blue-shifted (approaching) half of the stellar disk, then the
radial velocity of the star will appear to be slightly red-shifted, and vice-versa. The radial velocity anomaly depends on the trajectory of the
planet across the disk of the host star, and in particular on the spin-orbit
alignment of the system. Thus by monitoring the Rossiter-McLaughlin effect
one can measure the spin-orbit alignment.
|
|
Figure 3: A photometric light curve of TrES-1 from the MAGNUM observation (top),
and radial velocities obtained with the Subaru/HDS (bottom). The light curve
shows that the observations were conducted around a transit of TrES-1b. |
|
Figure 4: Orbital plots of TrES-1 radial velocities and the best-fitting models
including the Kepler motion and the Rossiter-McLaughlin effect.
Left panel: A radial velocity plot for the whole orbital phase.
Right panel: A close-up of the radial velocity plot around the transit phase.
The waveform around the central transit time (phase = 0) is caused by the
Rossiter-McLaughlin effect.
Bottom panels: Residuals from the best-fit curve. |
August 23 , 2007 |