Upload
hedley-boone
View
40
Download
3
Embed Size (px)
DESCRIPTION
Precise Characterisation of Exoplanet-host Stars Parameters in connexion with the Formation and Evolution of Planetary Systems. Sylvie Vauclair Laboratoire d’Astrophysique de Toulouse-Tarbes, CNRS, Université de Toulouse, Institut universitaire de France. - PowerPoint PPT Presentation
Citation preview
Sylvie VauclairLaboratoire d’Astrophysique de Toulouse-Tarbes, CNRS,Université de Toulouse, Institut universitaire de France
Precise Characterisation of Exoplanet-host Stars Parametersin connexion with the Formation and Evolution of Planetary Systems
IAU symposium 276, The Astrophysics of Planetary Systems, Torini October 11 to 15, 2010
Collaborations: Maria Eliana Escobar, Sylvie Théado, Noël Dolez, Gérard Vauclair and Corot team
• Asteroseismology of exoplanet-host stars: - determination of masses, radii, ages, luminosities, temperatures,evolutionary stages of the central stars- Rotation period and inclination of rotation axis
• Importance of chemical composition: metallicity and helium content,links with the theories for planets formation and migration, andaccretion on the central star (lithium tests)
SOPHIE OHP, T193August 2007
Asteroseismology :ground based and space
observations
Same instruments as for the detection of exoplanets
Ground: radial velocity methodsHARPS (La Silla), SOPHIE (OHP), AAT, VLT, Keck, etc…future: SONG
Space: photometric methodsMOST, COROT, KEPLER…
Four exoplanets-host stars observed on large periods (8 or 9 consecutive nights)
from the ground (solar-type stars all oscillate) :
mu Arae, HARPS 2004 iota Hor, HARPS 2006
51 Peg, SOPHIE 2007 and 201094 Cet, HARPS 2007
Stochastic excitation of pressure waves.
Spherical harmonics:
is a Legendre polynomial
is a normalisation factor, so that the integral of
on the sphere is 1.
Basics of asterosismology(for slowly rotating stars) -1
Basics of asterosismology(for slowly rotating stars) -2
« asymptotic theory » (Tassoul 1980) :
Large separations : (n,l) = (n+1, l) – (n,l)
Small separations :
o
échelle diagram
Y = 0.282
Evolutionary trackscomputed with the same metallicitybut different initial helium
(from Soriano and Vauclair, with TGEC)
The Y problem
1.14Msun
1.24Msun
1.20Msun1.28Msun
M/Mo = 1.25 +/- 0.01log g = 4.40 +/- 0.01Y = 0.255 +/- 0.015[Fe/H] = 0.16 +/- 0.03Age = 625 +/- 5 MyrR/Ro = 1.36+/- 0.01
M/Mo = 1.10+/- 0.01log g = 4.215+/- 0.01Y = 0.30+/- 0.01[Fe/H] = 0.30 +/- 0.03Age = 6.34+/- 0.4 GyrR/Ro = 1.84 +/- 0.01
Note: does not include uncertainties on physics: opacities, EOS, nuclear reactions rates, etc.
Arae Hor
Radial velocity curve during 9 nights and best planet-orbital fitting for 51 Peg (august 2010)
51 Peg1.06 Msun1.15 Rsun1.30 Lsun5665K8 Gyr
1 planetP=4.2j0.052 ua0.5 MJ
Observational échelle diagram for 51 Peg. Comparison models: 1.1 M with [Fe/H]=0.20 and Y=0.3
Preliminary !
Coralie : ESO/FEROS:Teff = 6076 +/- 57 Teff = 6131 +/- 47log g = 4.20 +/- 0.17 log g = 4.35 +/- 0.13 [Fe/H] = 0.20 +/- 0.07 [Fe/H] = 0.25 +/- 0.06
Mpsini = 1.09 MjPeriod : 119 dayse= 0.32; a = 0.5 AU
V = 6.2 , 35.6 mas Distance: 28 pcL/Lo = 1.94 +/- 0.16
HD52265 : COROT main target
LRA2, 117 days
HD52265 : COROT main target
LRA2, 117 days
42 modes p detected (l=0, 1, 2)Large separation 98.4 µHz ; small separation ~8.3 µHzrotation period: 11 daysinclination: 12°<i<37°1.8Mj<Mp<5.4Mj
log g = 4.285 +/- 0.01Teff = 6026L/Lo = 2.19age = 2.7 Gyrmass = 1.24
initial diffusion-induced profile (just
before accretion)accretion-induced profile (just after the accretion event)-profile at 4 Myr-profile at 9 Myr-profile at 12 Myr
convective zone
radiative interior
Consequences ofaccretion-induced mixing:
See Poster
Sylvie Théado and Sylvie Vauclair
The stellar lithium as a tracer for intense planetesimal bombardment