Extrasolar Planets & The Power of the Dark Side David Charbonneau California Institute of Technology www.astro.caltech.edu/~dc Fermilab – 24 April 2002.

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Presentation transcript:

Extrasolar Planets & The Power of the Dark Side David Charbonneau California Institute of Technology Fermilab – 24 April 2002

Gravitational Wobble

First Planet Detected 51 Pegasi – November 1995

First Planet System Detected Upsilon Andromedae – April 1999 Used with permission of the artist.

The Radial Velocity Surveys

Masses of Extrasolar Planets

Close-In Extrasolar Giant Planets and Planetary Migration

Protoplanetary Disks Around Young Stars D. Padgett (IPAC/Caltech), M. McCaughrean (A I Potsdam), C. Burrows (STScI), K. Stapelfeldt (JPL/Caltech)

Transits: A Little Closer To Home… Where will you be June 8, 2004?

Transit Characteristics Probability Probability p t = R star / a = 0.1 = 0.1 Depth Depth  I / I = (R pl / R star ) 2 = 0.01 = 0.01 Period Period P = 3 – 7 days Duration Duration t = 3 hours

The Observational Challenge The fraction of stars with transits is: f = f s f MS f CEGP p t f s = fraction of stars that are single = 0.5 f MS = fraction of those on the main sequence = 0.5 f CEGP = fraction of those that have a close-in planet = 0.01 p t = fraction of those with an inclination to transit = 0.1 Need to look at 4000 stars to find 1 that transits. Need to look at 4000 stars to find 1 that transits. Need to sample often compared to transit duration. Need to sample often compared to transit duration. Need 1% accuracy for a 3  detection of a 2 hour transit. Need 1% accuracy for a 3  detection of a 2 hour transit. Need to look on sky for at least 1 orbital period. Need to look on sky for at least 1 orbital period. Require 1,000, minute samples with 1% accuracy to detect one transit.

The STARE Project Delivers high-cadence time series photometry on roughly 30,000 stars (9 < V < 13) in a typical field centered on the galactic plane. We obtain sufficient precision on 5,000 stars to detect a close-in Jupiter-sized companion.

The Search Is On!

The Benefits of a Network

HD b The First Transiting Planet

The Effects of Stellar Insolation Burrows et al. (2000)

The Effects of a Planetary Core and Tidal Dissipation Bodenheimer et al. (2001)

Radial Velocity with Orbit Removed G. Marcy et al. (2000)

STARE Photometry of HD

HST STIS Photometry of HD

Unphased HST STIS Photometry of HD

Planetary Satellites from Photometric Residuals

Planetary Satellites from Transit Timing

Transmission Spectroscopy Brown (2001)

A Prediction of Sodium Absorption Hubbard et al. (2001)

Detection of an Extrasolar Planet Atmosphere

STIS Transmission Spectrum BANDPASSES

STIS Transmission Spectrum DATA

STIS Transmission Spectrum THEORY

STIS Transmission Spectrum NEAR FUTURE

Reflected Light Combination of: Transiting planet with a well- determined value for the radius Transiting planet with a well- determined value for the radius Excellent photometric precision with STIS Excellent photometric precision with STIS Desire to measure the planetary albedo, p Desire to measure the planetary albedo, p We have 20 orbits of STIS data (290 – 1030 nm) spanning 4 times of secondary eclipse. The photon noise limit of these data would permit a detection threshold of p = 0.1, averaged over the entire bandpass. These data will allow us to quantify the net energy deposition into the planet.

The Kepler Project

The Kepler Project Parameter Space

The Kepler Project Technology Demonstration

The Kepler Project