TY - JOUR
T1 - Granulation in Red Giants: Observations by The Kepler Mission and Three-Dimensional Convection Simulations
AU - Mathur, S
AU - Hekker, S
AU - Trampedach, R
AU - Ballot, J
AU - Kallinger, T
AU - Buzasi, D
AU - García, RA
AU - Huber, D
AU - Jiménez, A
AU - Mosser, B
AU - Bedding, TR
AU - Elsworth, Yvonne
AU - Régulo, C
AU - Stello, D
AU - Chaplin, William
AU - De Ridder, J
AU - Hale, Steven
AU - Kinemuchi, K
AU - Kjeldsen, H
AU - Mullally, F
AU - Thompson, SE
PY - 2011/11/10
Y1 - 2011/11/10
N2 - The granulation pattern that we observe on the surface of the Sun is due
to hot plasma rising to the photosphere where it cools down and descends
back into the interior at the edges of granules. This is the visible
manifestation of convection taking place in the outer part of the solar
convection zone. Because red giants have deeper convection zones than
the Sun, we cannot a priori assume that their granulation is a scaled
version of solar granulation. Until now, neither observations nor
one-dimensional analytical convection models could put constraints on
granulation in red giants. With asteroseismology, this study can now be
performed. We analyze ~1000 red giants that have been observed by Kepler
during 13 months. We fit the power spectra with Harvey-like profiles to
retrieve the characteristics of the granulation (timescale
τgran and power P gran). We search for a
correlation between these parameters and the global acoustic-mode
parameter (the position of maximum power, νmax) as well as
with stellar parameters (mass, radius, surface gravity (log g), and
effective temperature (T eff)). We show that
τeffvpropν-0.89 max and P
granvpropν-1.90 max, which is
consistent with the theoretical predictions. We find that the
granulation timescales of stars that belong to the red clump have
similar values while the timescales of stars in the red giant branch are
spread in a wider range. Finally, we show that realistic
three-dimensional simulations of the surface convection in stars,
spanning the (T eff, log g) range of our sample of red
giants, match the Kepler observations well in terms of trends.
AB - The granulation pattern that we observe on the surface of the Sun is due
to hot plasma rising to the photosphere where it cools down and descends
back into the interior at the edges of granules. This is the visible
manifestation of convection taking place in the outer part of the solar
convection zone. Because red giants have deeper convection zones than
the Sun, we cannot a priori assume that their granulation is a scaled
version of solar granulation. Until now, neither observations nor
one-dimensional analytical convection models could put constraints on
granulation in red giants. With asteroseismology, this study can now be
performed. We analyze ~1000 red giants that have been observed by Kepler
during 13 months. We fit the power spectra with Harvey-like profiles to
retrieve the characteristics of the granulation (timescale
τgran and power P gran). We search for a
correlation between these parameters and the global acoustic-mode
parameter (the position of maximum power, νmax) as well as
with stellar parameters (mass, radius, surface gravity (log g), and
effective temperature (T eff)). We show that
τeffvpropν-0.89 max and P
granvpropν-1.90 max, which is
consistent with the theoretical predictions. We find that the
granulation timescales of stars that belong to the red clump have
similar values while the timescales of stars in the red giant branch are
spread in a wider range. Finally, we show that realistic
three-dimensional simulations of the surface convection in stars,
spanning the (T eff, log g) range of our sample of red
giants, match the Kepler observations well in terms of trends.
KW - stars: late-type
KW - methods: data analysis
U2 - 10.1088/0004-637X/741/2/119
DO - 10.1088/0004-637X/741/2/119
M3 - Article
SN - 1538-4357
VL - 741
SP - 119-
JO - The Astrophysical Journal
JF - The Astrophysical Journal
IS - 2
ER -