Stellar obliquities in exoplanetary systems

Slides:



Advertisements
Similar presentations
Tidal Constraints on Planetary Habitability
Advertisements

Spin-Orbit Misalignment in Planetary Systems and Magnetic Star -- Disk Interaction IAU Astrophysics of Planetary Systems, Torino, Italy, Oct.14, 2010 Dong.
Sang Gak Lee, Masateru Ishiguro, YunA Yang, Won Suk Kang, Keun Hong Park (Seoul National University) Sung Ho Lee, Hyun Il Sung, Dong Whan Cho (KASI) 6/21/2010.
Kozai Migration Yanqin Wu Mike Ramsahai. The distribution of orbital periods P(T) increases from 120 to 2000 days Incomplete for longer periods Clear.
1 X 2  : NO C 2  : z z  = 3/2  = 1/2 Spin-orbit interaction Orbit-rot. interaction z  = 3/2  = 1/2 Spin-orbit interaction Orbit-rot. interaction.
Tidal Dynamics of Transiting Exoplanets Dan Fabrycky UC Santa Cruz 13 Oct 2010 Photo: Stefen Seip, apod/ap At: The Astrophysics of Planetary Systems:
Asteroid Resonances [1]
Norio Narita National Astronomical Observatory of Japan
Planet Characterization by Transit Observations Norio Narita National Astronomical Observatory of Japan.
1. Global Properties 2. The Rossiter-McClaughlin Effect II. Results from Transiting Planets.
Mapping the Realm of Hot Jupiters Bun’ei Sato, Shigeru Ida ( Titech ), Eri Toyota ( Kobe Univ. ), Masashi Omiya ( Tokai Univ. ), Debra Fischer ( SFSU ),
Status of RV Sub-Catelogy Norio Narita (NAOJ) Yasuhiro H. Takahashi (Univ. of Tokyo) Bun’ei Sato (Titech) Ryuji Suzuki (NAOJ) and SEEDS/HiCIAO/AO188 teams.
1 Determining the internal structure of extrasolar planets, and the phenomenon of retrograde planetary orbits Rosemary Mardling School of Mathematical.
Tidal Influence on Orbital Dynamics Dan Fabrycky 4 Feb, 2010 Collaborators: Scott Tremaine Eric Johnson Jeremy Goodman Josh.
A unified normal modes approach to dynamic tides and its application to rotating stars with realistic structure P. B. Ivanov and S. V. Chernov, PN Lebedev.
Transits and Starspots Jeremy Tregloan-Reed Ph.D. Research Student Supervisor: John Southworth.
Exoplanet- Asteroseismology Synergies Bill Chaplin, School of Physics & Astronomy University of Birmingham, UK EAHS2012, Oxford, 2012 March 15.
1 Why exoplanets have so high eccentricities - By Line Drube - November 2004.
Nonlinear Tides in Exoplanet Host Stars (Extreme Solar Systems II) Phil ArrasUniversity of Virginia Josh BurkartU. C. Berkeley Eliot QuataertU. C. Berkeley.
Effects of Kozai Migration on Formation of Close-in Planets Soko Matsumura (University of Maryland) Douglas P. Hamilton (University of Maryland)
Ge/Ay133 What have radial velocity surveys told us about (exo)-planetary science?
Ge/Ay133 What have radial velocity surveys told us about (exo)-planetary science?
Characterizing Extrasolar Planets from their Transit Lightcurves Jason W. Barnes Assistant Professor Department of Physics University of Idaho ECE Seminar.
New Results from Kepler: Systems of Multiple Transiting Planets w/ Correlated TTVs Eric B. Ford Extreme Solar Systems II September 12, 2011 Based on a.
Ge/Ay133 What have radial velocity surveys told us about (exo)-planetary science?
Eccentric Extrasolar Planets: The Jumping Jupiter Model HD217107b as imagined by Lynette Cook Stacy Teng TERPS Conference Dec. 9, 2004.
Extrasolar Planets Z:\exo\presentations\EGS2001_exo.ppt, :54AM, 1 Tidal interactions of close-in extrasolar planets with their host stars.
Norio Narita (NAOJ Fellow) Special Thanks to IRD Transit Team Members
Nadiia Kostogryz & Svetlana Berdyugina
Adriana V. R. Silva CRAAM/Mackenzie COROT /11/2005.
EXONEST The Exoplanetary Explorer Kevin H. Knuth and Ben Placek Department of Physics University at Albany (SUNY) Albany NY.
MARTIN STILL – IAU XXVIII General Assembly – SpS #13: High-Precision Tests of Stellar Physics from High-Precision Photometry – Aug 27, a NEW STELLAR.
1 29 August 2012IAU SS13, Beijing Stellar Physics Revealed by Planetary Transits Willie Torres Harvard-Smithsonian Center for Astrophysics IAU General.
Further Science of IRD: Synergy with Transiting Planets
Discriminating Migration Mechanisms of Tilted or Eccentric Planetary Systems Norio Narita (NAOJ/University of Hawaii)
Observational Studies for Understanding Planetary Migration Norio Narita National Astronomical Observatory of Japan.
Jean-Pierre needs to be brought up to date on what’s really going on in astronomy these days!
Simultaneous Subaru/MAGNUM Observations of Extrasolar Planetary Transits Norio Narita (U. Tokyo, JSPS Fellow, Japan) Collaborators Y. Ohta, A. Taruya,
Search for Transiting Planets around Nearby M Dwarfs Norio Narita (NAOJ)
Aligned, Tilted, Retrograde Exoplanets and their Migration Mechanisms Norio Narita (JSPS Fellow) National Astronomical Observatory of Japan.
Toward Detections and Characterization of Habitable Transiting Exoplanets Norio Narita (NAOJ)
Testing Planet Migration Theories by Observations of Transiting Exoplanetary Systems 1/39 University of Tokyo Norio Narita.
Discriminating Planetary Migration Mechanisms by Direct Imaging Norio Narita National Astronomical Observatory of Japan on behalf of SEEDS/HiCIAO/AO188.
Atmospheric circulation of hot Jupiters on highly eccentric orbits Tiffany Kataria 1, Adam Showman 1, Nikole Lewis 1, Jonathan Fortney 2, Mark Marley 3,
Extra-Solar Planet Populations Stephen Eikenberry 4 November 2010 AST
1 Neptune Mass Exoplanets Jeff Valenti M Jupiter / 19 = M Neptune = 17 M Earth Geoff Marcy (Berkeley)Debra Fischer (Yale) Andrew Howard (Berkeley)John.
Spectroscopic Transits
Spin-Orbit Alignment Angles and Planetary Migration of Jovian Exoplanets Norio Narita National Astronomical Observatory of Japan.
Detection of Extrasolar Giant Planets Hwihyun Kim 03/30/06.
Transiting Extrasolar Planets Recent Progress, XO Survey, and the Future Christopher J. Burke.
© 2012 Boise State University1 The SuPerPiG Search for Short-Period Planets Using the K2 Dataset Brian Jackson 1
Gijs Mulders, Ilaria Pascucci, Daniel Apai University of Arizona An Increase in Planet Formation Efficiency around Low-Mass Stars.
Transiting Exoplanet Search and Characterization with Subaru's New Infrared Doppler Instrument (IRD) Norio Narita (NAOJ) On behalf of IRD Transit Group.
Chaotic Dynamics of Stellar Spin in Binaries and the Production of Misaligned Hot Jupiters Natalia Storch, Kassandra Anderson & Dong Lai Cornell University.
Extra-Solar Planet Populations George Lebo 10 April 2012 AST
Sarah, Ellie, Adan and Sruthy. The Transit Method.
Kepler + Keck: Planet Masses and Densities Kepler + Keck: Planet Masses and Densities Geoff Marcy UC Berkeley + Preliminary Results.
Subaru Measurements of the Rossiter-McLaughlin Effect and Direct Imaging Observations for Transiting Planetary Systems Norio Narita (NAOJ) and SEEDS/HiCIAO/AO188.
Companion Candidates around Transiting Planetary Systems: SEEDS First/Second Year Results Norio Narita (NAOJ) Yasuhiro H. Takahashi (Univ. of Tokyo) and.
Recent Results from the Kepler Mission Ron Gilliland - STScI - 9 June 2010.
Results of HARPS-N observations of the transiting system Qatar-1 in GAPS E. Covino M. Esposito, M. Barbieri, S. Desidera, L. Mancini, V. Nascimbeni, J.
Characterizing Planets from their Transit Lightcurves Jason W. Barnes NASA Postdoctoral Program Fellow NASA Ames Research Center Advisor: William J. Borucki.
Measuring the Spin-Orbit Alignments of Transiting Exoplanetary Systems: The Case for TrES-1 Norio Narita, Keigo Enya, Bun'ei Sato, Yasuhiro Ohta, Joshua.
IAU253 Transiting Planets: May
1 / 12 Simultaneous Spectroscopic & Photometric Observations of a Transit of TrES-1b Norio Narita (UT, JSPS Fellow) Collaborators K. Enya (JAXA), B. Sato.
Past and Future Studies of Transiting Extrasolar Planets
Ge/Ay133 What have radial velocity surveys told
Subaru Measurements of the Rossiter-McLaughlin Effect
News from the McDonald Observatory Planet Search
Norio Narita National Astronomical Observatory of Japan
Presentation transcript:

Stellar obliquities in exoplanetary systems Josh Winn Massachusetts Institute of Technology Simon Albrecht, Roberto Sanchis-Ojeda, Teruyuki Hirano Andrew Howard, John Johnson, Geoff Marcy Bill Cochran, Dan Fabrycky, the Kepler team

obliquity (n.) 1 : deviation from parallelism 2 : a deviation from moral rectitude or sound thinking

Eccentricity Semimajor axis [AU] Jupiter

Disk-planet interactions Eccentricity Low obliquity Disk-planet interactions Semimajor axis [AU]

Disk-planet interactions Few-body dynamics High obliquity Eccentricity Tidal dissipation Low obliquity Disk-planet interactions Semimajor axis [AU]

The Sanchis–Nutzman effect

l = 0°

l = 0°

l = 0°

l = 0°

l = 0°

l = 0°

l = 0° l = 100°

l = 0° l = 100°

l = 0° l = 100°

l = 0° l = 100°

l = 0° l = 100° …

l = 0° l = 100° …

l = 0° l = 100° …

… The starspot-anomaly pattern reveals the stellar obliquity Sanchis-Ojeda et al. (2011 a,b) Nutzman, Fabrycky, & Fortney (2011) …

Corot-2 Nutzman, Fabrycky, & Fortney (2011)

Corot-2 l = 5 ± 12° Observed Calculated (l = 0°) Nutzman, Fabrycky, & Fortney (2011) — see also Désert et al. (2011)

HAT-P-11 Sanchis-Ojeda & Winn (2011)

Time from midtransit [days] Sanchis-Ojeda & Winn (2011)

Sanchis-Ojeda & Winn (2011)

Sanchis-Ojeda & Winn (2011)

Christoph Scheiner (1573-1650)

The Rossiter-McLaughlin effect Flux Time The Rossiter-McLaughlin effect

The Rossiter-McLaughlin effect Doppler shift Time The Rossiter-McLaughlin effect

The Rossiter-McLaughlin effect Doppler shift Time The Rossiter-McLaughlin effect

The Rossiter-McLaughlin effect Doppler shift Time The Rossiter-McLaughlin effect

The Rossiter-McLaughlin effect Doppler shift Time The Rossiter-McLaughlin effect

The Rossiter-McLaughlin effect Doppler shift Time The Rossiter-McLaughlin effect

Measuring the projected obliquity Queloz et al. (2000); Ohta, Taruya, & Suto (2005); Gaudi & Winn (2007)

Low obliquity HD 189733 l = –1.4° ± 1.1° Winn et al. (2006); see also Triaud et al. (2009)

Moderate obliquity XO-3 l = 37.3° ± 3.0° Hirano et al. (2011); see also Hébrard et al. (2008), Winn et al. (2009)

High obliquity (retrograde) Winn et al. (2009) Narita et al. (2009) Triaud et al. (2010)

Valenti & Fischer (2005) Pinsonneault et al. (2001)

(Zahn 1977)

Problem: Orbit decays on same timescale as realignment

Solution: Realign only the convective zone?

Reality

Constant-Q model

Different Q’s for realignment and orbital decay (D. Lai, in preparation)

KOI-63 1.0 M , 1.0 R P = 9.4 days Rp = 6.5 R

Prot = 5.4 days ≈ (4/7) Porb

KOI-63

Current obliquity measurements

Current obliquity measurements Kepler candidates

Current obliquity measurements Kepler candidates Kepler multi-planet candidates

Rossiter-McLaughlin effect Starspot anomalies Rossiter-McLaughlin effect Rotation-rate statistics (Schlaufman 2010) Gravity darkening (Barnes 2010, Szabo et al. 2011) Rotational Doppler boosting (van Kerkwijk et al. 2010) Spin precession TDVs (Damiani & Lanza 2011) Current obliquity measurements Kepler candidates Kepler multi-planet candidates