Bibcode
Rodler, F.; Del Burgo, C.; Witte, S.; Helling, Ch.; Hauschildt, P. H.; Martín, E. L.; Alvarez-Iglesias, C. A.; Deshpande, R.
Referencia bibliográfica
Astronomy and Astrophysics, Volume 532, id.A31
Fecha de publicación:
8
2011
Revista
Número de citas
19
Número de citas referidas
13
Descripción
Context. Radial velocity monitoring of very cool dwarfs such as late M-
and hot L-dwarfs has become a promising tool in the search for rocky
planets as well as follow-up planetary candidates around dwarfs detected
by transit surveys. These stars are faint at optical wavelengths, as
their spectral flux distribution peaks at near-infrared (NIR)
wavelengths. For this reason, it is desirable to measure the radial
velocities in this wavelength regime. However, in the NIR very few
medium- and high-resolution spectrographs are available at large
telescopes. In the near future, high-resolution spectrographs for the
NIR will be built, which will allow us to search for rocky planets
around cool M-dwarfs and L-dwarfs from radial velocities monitoring. Aims: We investigate the precision that can be attained in radial
velocity measurements of very cool dwarfs in the NIR. The goal is to
determine in which atmospheric window of the Earth's atmosphere the
highest radial velocity precision can be achieved to help in designing
the next generation of NIR high-resolution spectrographs.
Methods: We use stellar atmosphere synthetic models for an M- and an
L-dwarf with temperatures of 2200 K and 1800 K, respectively, and a
theoretical spectrum of the Earth's transmission in the spectral range
from 0.9 to 2.5 μm. We simulate a series of Doppler-shifted spectra
observed with different resolving powers and signal-to-noise ratios, and
for different rotational broadenings of the dwarf. For different
combinations of the input parameters, we recover the radial velocity by
means of cross-correlation with a high signal-to-noise ratio template
and determine the associate uncertainties. Results: The highest
precision in radial velocity measurements for the cool M-dwarf is found
in the Y band around 1.0 μm, while for the L-dwarf it is determined
in the J band around 1.25 μm. We note that synthetic models may lack
some faint absorption features or underestimate their abundances. In
addition, some instrumental/calibration aspects that are not taken into
account in our estimations would increase the uncertainties.