Asteroseismology with the Kepler Mission Travis Metcalfe NCAR
- Slides: 14
Asteroseismology with the Kepler Mission Travis Metcalfe (NCAR) We are the stars which sing, We sing with our light; We are the birds of fire, We fly over the sky. SONG OF THE STARS Algonquin Mythology
• Why is asteroseismology important to the primary science goal of Kepler? • Transit only gives radius of planet relative to the unknown stellar radius • Asteroseismology will measure the stellar radius with a precision of 2 -3%
• Why is asteroseismology important to the primary science goal of Kepler? • Transit only gives radius of planet relative to the unknown stellar radius • Asteroseismology will measure the stellar radius with a precision of 2 -3%
Kepler mission overview • NASA mission currently scheduled for launch in mid-February 2009 • 105 square degrees just above galactic plane in the constellation Cygnus • Single field for 4 -6 years, 100, 000 stars 30 minute sampling, 512 at 1 minute
Surface differential rotation • Three seasons of precise MOST photometry for the solar-type star k 1 Ceti • Latitudinal differential rotation pattern has same functional form as Sun Ca HK period Walker et al. (2007) • Kepler will obtain similar rotation measurements for 105 solar-type stars
Stellar density and age Elsworth & Thompson (2004) • Large frequency spacing <Dn> scales with average density of the star • Small frequency spacing <dn> sensitive to interior gradients, proxy for age • Probe evolution of activity and rotation as a function of stellar mass and radius Christensen-Dalsgaard (2004)
Radial differential rotation Fletcher et al. (2006) • WIRE 50 -day time series of a Cen A has resolved the rotational splitting • Splitting as a function of radial order can indirectly probe differential rotation Gough & Kosovichev (1993) • Even low-degree modes allow rough inversions of the inner 30% of radius
Convection zone depth • Expected seismic signal from a Co. Ro. T 5 -month observation of HD 49933 • Second differences (d 2 n) measure deviations from even frequency spacing • Base of the convection zone and He ionization create oscillatory signals Baglin et al. (2006)
Oscillations and magnetic cycles Salabert et al. (2004) • Solar p-mode shifts first detected in 1990, depend on frequency and degree • Even the lowest degree solar p-modes are shifted by the magnetic cycle • Unique constraints on the mechanism could come from asteroseismology Libbrecht & Woodard (1990)
Cycle-induced frequency shifts • Solar p-mode shifts show spread with degree and frequency dependence • Normalizing shifts by our parametrization removes most of the dependencies • Kepler will document similar shifts in hundreds of solar-type stars Metcalfe et al. (2007)
Stellar modeling pipeline • Genetic algorithm probes a broad range of possible model parameters • 0. 75 0. 002 0. 22 1. 0 < < Mstar Zinit Yinit amlt < < 1. 75 0. 05 0. 32 3. 0 • Finds optimal balance between asteroseismic and other constraints
Application to Bi. SON data • Fit to 36 frequencies with l = 0 -2 and constraints on temperature, luminosity • Matches frequencies with scaled surface correction better than 0. 6 m. Hz r. m. s. • Temperature and age within +0. 1%, luminosity and radius within +0. 4%
Tera. Grid portal • Web interface to specify observations with errors, or upload as a text file • Specify parameter values to run one instance of the model, results archived • Source code available for those with access to large cluster or supercomputer
Summary • Kepler needs asteroseismology to determine the absolute sizes of any potentially habitable Earthlike planets that may be discovered. • The mission will yield a variety of data to calibrate dynamo models, sampling many different sets of physical conditions and evolutionary phases. • A uniform analysis of the asteroseismic data will help minimize the systematic errors, facilitated by a Tera. Grid-based community modeling tool.