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Asteroseismology of solar-type stars Revolutionizing the study of solar-type stars Hans Kjeldsen, Aarhus University
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Christensen-Dalsgaard et al. 1995 Asteroseismology: Solar-like stars 1.Measuring oscillation frequencies 2.Identify modes (p, g, mixed, l, n, m) 3.Compute model frequencies 4.Compare observed frequencies with the model CoRoT HD 49385 The Sun
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Observations: Challenges Accuracy of oscillation frequencies Mode identification, avoided crossings, (curvature in the Echelle diagram) Rotational splitting, mode lifetime, mode amplitudes, granulation
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Helioseismology asteroseismology
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UVES at the VLTUCLES at the AAT State-of-the-art Ground-based asteroseismology of solar-type stars HARPS at ESO 3.6m
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Ground-based In most cases: Low SNR Short obs. period
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(Fabien Carrier)
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High signal-to-noise observations of solar-like oscillations
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Mixed mode
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Martic et al. 2004: amp = 40 cm/s per mode = 6-7 ppm per mode
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Martic et al. 2004: amp = 40 cm/s per mode = 6-7 ppm per mode Brown et al.1991
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20 3 1 ??? 3 1 2 0
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Velocities of Cen A with UVES/VLT Precision: 50-70 cm/s. Cadence 26 seconds!
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UVES/VLT2 + UCLES/AAT 35 Butler, Bedding, Kjeldsen et al. 2003, 2004
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2 0 3 1
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Radial p-mode (radial orders)
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α Centauri system OPAL EOS, OPAL96 opacity, He, Z settling (Teixeira et al.)
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α Centauri A
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α Centauri B
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Models: Challenges Input physics Properties: rotation, mixing Surface frequency offset Avoided crossings – sensitivity to finer details in the models
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The Surface Offset O - C
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BiSON Model S
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The Surface Offset MODEL SGOLFradial order, n 1. Frequency (f)3038.953034.1517-25 (21) 2. Large separation 135.855 134.81017-25 (21) 3. f(n=17)2497.35 2496.0417 4. f(n=13)1957.46 1957.45 13 0.16 % 0.78 % 0.05 % 0.0005 %
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Observations: Challenges Accuracy of oscillation frequencies Mode identification, avoided crossings, (curvature in the Echelle diagram) Rotational splitting, mode lifetime, mode amplitudes, granulation
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How do we improve this?
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Higher frequency resolution
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How do we improve this? Higher frequency resolution Space missions
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How do we improve this? Higher frequency resolution Lower noise
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Granulation dominated Oscillations dominated
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How do we improve this? Higher frequency resolution Lower noise See the Poster on SONG!
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CoRoT (CNES) 2006 Seismology for a large number of stars
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CoRoT (CNES) 2006 HD 49385 HD 49933 HD 181420
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CoRoT (CNES) 2006 HD 49385 HD 49933 HD 181420
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Same problem as in Procyon…. l=0,2 and 1,3 ridges? The F-star problem
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HD 181420 Same problem as in Procyon and HD 49933 …. l=0,2 and 1,3 ridges?
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Simple asteroseismology…
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Asteroseismology as a tool Stellar properties based on the large separation 8-10% error in mass, 1% error for the large separation will give a 3% error for the stellar radius
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Asteroseismology as a tool Knowledge of the effective temperature (e.g. typical error of 2%) will then give the absolute luminosity (error 10%) This will improve the mass and radius estimate further
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NASA Kepler launched in March 2009
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HAT-P-7
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Days after launch Q0Q1
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Models: Challenges Input physics Properties: rotation, mixing Surface frequency offset Avoided crossings – sensitivity to finer details in the models
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Kepler Asteroseismic Activities Asteroseismology on exoplanet candidates Target selection for KASC Data distribution via KASOC Organizing data analysis Workshops; KASC III Publishing papers
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Based on the first half of the KASC Survey… hundreds of stars showing solar-like oscillations Chaplin et al… 2010
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The challenge… Accuracy of oscillation frequencies (Kepler will observe some stars for 3,5 years) Mode identification (“F-star problem”) Rotational splitting, mode lifetime, mode amplitudes, granulation, activity Input physics (EOS, opacities, convection, rotation, mixing) and the surface frequency offset Avoided crossings (sensitivity to finer details in the models) g-modes
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The challenge… CoRoT, Kepler, PLATO, SONG… will provide the data and challenge the theories of stellar evolution Improved stellar modelling will provide the deeper understanding Remember to enjoy those amazing data
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