Next-Generation Radial Velocity Surveys Center for Exoplanets and Habitable Worlds Benjamin Nelson (Data Science Scholar) Collaborators Kat Deck (Caltech), Debra Fischer (Yale), Eric Ford (PSU), Andrew Howard (Hawaii), Howard Isaacson (Berkeley), Matt Payne (CfA), Seth Pritchard (UT San Antonio), Paul Robertson (PSU), Kaspar von Braun (Lowell), Jason Wright (PSU) MSU Astro Seminar 10/28/15
H E F I G <1995: sparse observations 1995: 51 Peg b (Mayor & Queloz) 1998: 55 Cnc b (Butler+) 2002: 55 Cnc c and d (Marcy+) 2002-2004: Keck, HJST, HET start searches 2004: 55 Cnc e (McArthur+) MSU Astro Seminar 10/28/15
H E F I G <1995: sparse observations 1995: 51 Peg b (Mayor & Queloz) 1998: 55 Cnc b (Butler+) 2002: 55 Cnc c and d (Marcy+) 2002-2004: Keck, HJST, HET start searches 2004: 55 Cnc e (McArthur+) 2008: 55 Cnc f (Fischer+) MSU Astro Seminar 10/28/15
H E F I G <1995: sparse observations 1995: 51 Peg b (Mayor & Queloz) 1998: 55 Cnc b (Butler+) 2002: 55 Cnc c and d (Marcy+) 2002-2004: Keck, HJST, HET start searches 2004: 55 Cnc e (McArthur+) 2008: 55 Cnc f (Fischer+) 2010: New period for 55 Cnc e (Dawson & Fabrycky) MSU Astro Seminar 10/28/15
chi-square minimum with LM BOOTTRAN (Wang+ 2012): Bootstrap to get uncertain\es in model parameters Disadvantages: - long orbital periods - poor phase coverage Time Velocity MSU Astro Seminar 10/28/15
model parameter distribu\ons with mul\ple modes or highly covariant structure. Performance most sensi\ve to number of Markov chains. Best choice: number of Markov chains ≈ 3 × number of dimensions Sidenote: emcee3 will have differen\al evolu\on! (Foreman-Mackey et al. 2013) Nelson+ 2014a Take-away points for DEMCMC MSU Astro Seminar 10/28/15
Oscillations < 15 min a few m/s Granulation 15 min - 2 days a few m/s Active Regions 10-50 days 40-140 cm/s Magnetic Cycles ~10 years 1-20 m/s Dumusque+ 2011 MSU Astro Seminar 10/28/15
Likelihood The probability of a radial velocity dataset {d} being generated from some model M parameterized by {θ} is given by… To choose between two competing models M1 and M2 , take the ratio of their FMLs… Bayes Factor = p(d|M2) p(d|M1) Bayesian Model Comparison MSU Astro Seminar 10/28/15
Likelihood The probability of a radial velocity dataset {d} being generated from some model M parameterized by {θ} is given by… There are efficient ways to do this! Nested Sampling (Feroz+ 2008) Transdimensional MCMC (Brewer & Donovan 2015) Geometric Path Monte Carlo (Hou+ 2015) Importance Sampling (Nelson+ 2015) Bayesian Model Comparison MSU Astro Seminar 10/28/15
planets vs. outer 3 planets ~1031 Round 2: inner 3 planets vs. inner 3 planets + ~120 day sinusoid ~109 Round 3: all 4 planets vs. inner 3 planets + ~120 day sinusoid ~30 Round 4: all 4 planets vs. all 4 + putative 5th planet ~103 Nelson+ 2015 And the best Gliese 876 model is… MSU Astro Seminar 10/28/15
planets vs. outer 3 planets ~1031 Round 2: inner 3 planets vs. inner 3 planets + ~120 day sinusoid ~109 Round 3: all 4 planets vs. inner 3 planets + ~120 day sinusoid ~30 Round 4: all 4 planets vs. additional 5th planet ~103 Nelson+ 2015 And the best Gliese 876 model is… MSU Astro Seminar 10/28/15
and RV precision is getting below 1 m/s. • Some multi-planet systems require high-dimensional (30-40) models and n- body integrations. But we have efficient code to deal with their data! • We can infer very detailed dynamical properties of exoplanet systems (e.g. mutual inclination, resonant/secular interactions, chaotic motion). • Stellar activity is becoming a problem in the 1 m/s regime but there seem to be some promising tractable methods (e.g. Gaussian processes to model activity, Bayes factors for model comparison) • Keplerian Fitting Challenge: https://rv-challenge.wikispaces.com/ Summary MSU Astro Seminar 10/28/15
X ✓i ⇠g(✓) p(✓i)p(d|✓i) g(✓i) FML = Z p(✓)p(d|✓)d✓ = Z p(✓)p(d|✓) g(✓) g(✓)d✓ [ FML ⇡ k N X ✓i ⇠g⌧ (✓) p(✓i)p(d|✓i) g⌧ (✓i) MSU Astro Seminar 10/28/15 Importance Sampling with MCMC Samples