Transit Searches: Results I.Results from individual transit searche programs II. Interesting cases...
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Transcript of Transit Searches: Results I.Results from individual transit searche programs II. Interesting cases...
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Transit Searches: Results
I. Results from individual transit searche programs
II. Interesting cases
III. Spectroscopic Transits
IV. In-transit spectroscopy
V. Radiated light (secondary transits)
CoRoT results will be presented during the Space Missions lecture
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The first time I gave this lecture (2003) there was one transiting extrasolar planet
There are now 52 transiting extrasolar planets
First ones were detected by doing follow-up photometry of radial velocity planets. Now transit searches are discovering exoplanets
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Radial Velocity Curve for HD 209458
Period = 3.5 days
Msini = 0.63 MJup
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Charbonneau et al. (2000): The observations that started it all:
• Proof that RV variations are due to planet
• Mass = 0,63 MJupiter
• Radius = 1,35 RJupiter
• Density = 0,38 g cm–3
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Transit detection was made with the 10 cm STARE Telescope
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A light curve taken by amateur astronomers…
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..and by the Profis ( Hubble Space Telescope).
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Successful Transit Search Programs
• OGLE: Optical Gravitational Lens Experiment (http://www.astrouw.edu.pl/~ogle/)
• 1.3m telescope looking into the galactic bulge
• Mosaic of 8 CCDs: 35‘ x 35‘ field
• Typical magnitude: V = 15-19
• Designed for Gravitational Microlensing
• First planet discovered with the transit method
• 7 Transiting planets discovered so far
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The first planet found with the transit method
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Konacki et al.
Until this discovery radial velocity surveys only found planets with periods no shorter than 3 days. About ½ of the OGLE planets have periods less than 2 days.
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M = 1.03 MJup
R = 1.36 Rjup
Period = 3.7 days
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Successful Transit Search Programs
• WASP: Wide Angle Search For Planets (http://www.superwasp.org). Also known as SuperWASP
• Array of 8 Wide Field Cameras
• Field of View: 7.8o x 7.8o
• 13.7 arcseconds/pixel
• Typical magnitude: V = 9-13
• 15 transiting planets discovered so far
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CoordinatesRA 00:20:40.07 Dec +31:59:23.7
Constellation Pegasus
Apparent Visual Magnitude 11.79
Distance from Earth 1234 Light Years
WASP-1 Spectral Type F7V
WASP-1 Photospheric Temperature
6200 K
WASP-1b Radius 1.39 Jupiter Radii
WASP-1b Mass 0.85 Jupiter Masses
Orbital Distance 0.0378 AU
Orbital Period 2.52 Earth Days
Atmospheric Temperature 1800 K
Mid-point of Transit 2453151.4860 HJD
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Successful Transit Search Programs
• TrES: Trans-atlantic Exoplanet Survey (STARE is a member of the network http://www.hao.ucar.edu/public/research/stare/)
• Three 10cm telescopes located at Lowell Observtory, Mount Palomar and the Canary Islands
• 6.9 square degrees
• 4 Planets discovered
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Successful Transit Search Programs
• HATNet: Hungarian-made Automated Telescope (http://www.cfa.harvard.edu/~gbakos/HAT/
• Six 11cm telescopes located at two sites: Arizona and Hawaii
• 8 x 8 square degrees
• 8 Planets discovered
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Follow-up with larger telescope
HAT 1b
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Special Transits: GJ 436
Host Star:
Mass = 0.4 Mּס (M2.5 V)
Butler et al. 2004
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„Photometric transits of the planet across the star are ruled out for gas giant compositions and are also unlikely for solid compositions“
Special Transits: GJ 436
Butler et al. 2004
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The First Transiting Hot Neptune
Gillon et al. 2007
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Star
Stellar mass [ Mּס ] 0.44 ( ± 0.04)
Planet
Period [days] 2.64385 ± 0.00009
Eccentricity 0.16 ± 0.02
Orbital inclination 86.5 0.2
Planet mass [ ME ] 22.6 ± 1.9
Planet radius [ RE ] 3.95 +0.41-0.28
Special Transits: GJ 436
Mean density = 1.95 gm cm–3, in between Neptune (1.58) and Uranus (2.3)
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Mean density is first hints of the internal composition
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M = 3.11 MJup
Special Transits: HD 17156
Probability of a transit ~ 3%
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R = 0.96 RJup
Barbieri et al. 2007
Mean density = 4.88 gm/cm3
Mean M2 star ≈ 4.3 gm/cm3
Companion is probably more like a brown dwarf
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Rp = 0.7 RJup
Mp = 0.36 MJup
Sato et al. 2005
Special Transits: HD 149026
Mean density = 2.8 gm/cm3
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~70 Mearth core mass is difficult to form with gravitational instability
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HD 209458b and HAT-P-1b have anomalously large radii that still cannot be explained by planetary structure and evolution models
Mass Radius Relationship
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Mazeh et al. 2008 found a mass-period relationship for transiting planets. Suggest this is evidence of evaporation, only the most massive planets can survive
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Results from the Rossiter-McClaughlin Effect
The RM effect causes a distortion in the radial velocity curve during a transit whose strength depends on the radius of the planet and the rotation rate of the star
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So far all transiting planets for which an RM effect has been measured has shown prograde orbits
What about misalignment of the spin axis?
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HD 147506
Best candidate for misalignment is HD 147506 because of the high eccentricity
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Two possible explanations for the high eccentricities seen in exoplanet orbits:
• Scattering by multiple giant planets
• Kozai mechanism
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Planet-Planet Interactions
Initially you have two giant planets in circular orbits
These interact gravitationally. One is ejected and the remaining planet is in an eccentric orbit
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Recall that there are no massive planets in circular orbits
This mechanism has been invoked to explain the „massive eccentrics“
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Kozai Mechanism
Two stars are in long period orbits around each other.
A planet is in a shorter period orbit around one star.
If the orbit of the planet is inclined, the outer planet can „pump up“ the eccentricity of the planet. Planets can go from circular to eccentric orbits.
This was first investigated by Kozai who showed that satellites in orbit around the Earth can have their orbital eccentricity changed by the gravitational influence of the Moon
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Kozai Mechanism
The Kozai mechanism has been used to explain the high orbital eccentricity of 16 Cyg B, a planet in a binary system
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Winn et al. 2007: HD 147506b (alias HAT-P-2b)
If either mechanism is at work, then we should expect that planets in eccentric orbits not have the spin axis aligned with the stellar rotation. This can be checked with transiting planets in eccentric orbits
Spin axes are aligned within 14 degrees (error of measurement). No support for Kozai mechanism or scattering
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What about HD 17156?
Narita et al. (2007) reported a large (62 ± 25 degree) misalignment between planet orbit and star spin axes!
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Cochran et al. 2008: = 9.3 ± 9.3 degrees → No misalignment!
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In-transit Spectroscopy
• Take a spectrum of the star during the out-of-transit time
• Take a spectrum of the star during the transit
• Subtract the two and what remains is the spectrum of the planet atmosphere
In practice this is very difficult. One requires high signal-to-noise ratio data (≈ 1000) which means repeated measurements that have to be co-added.
Problem: In transit spectra can only be made during transits (infrequent) and only for about 3 hours!
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Fig. 1.— Flux of HD 209458 a (upper curve) and the transmitted flux through the planet’s transparent atmosphere (lower curve). Superimposed on the transmitted flux are the planetary absorption features, including the He i triplet line at 1083 nm. The other bound-bound lines are alkali metal lines (see Fig. 2 for details). The H2O and CH4 molecular absorption dominates in the infrared. The dotted line is a blackbody of 1350 K representative of the CEGP’s thermal emission, but the thermal emission can be larger than a blackbody blueward of 2000 nm.
From The Astrophysical Journal 537(2):916–921.© 2000 by The American Astronomical Society.For permission to reuse, contact [email protected].
In-transit Spectroscopy
Sasselov & Seager 2004
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Fig. 2.—Upper plot: The normalized in-transit minus out-of-transit spectra, i.e., percent occulted area of the star. In this model the cloud base is at bar. Rayleigh scattering is important in the UV. Lower plot: A model with cloud base at 0.2 bar. The stellar flux passes through higher pressures, densities, and temperatures of the planet atmosphere compared to the model in the upper plot. In addition, a larger transparent atmosphere makes the line depth larger. Observations will constrain the cloud depth. See text for discussion.
From The Astrophysical Journal 537(2):916–921.© 2000 by The American Astronomical Society.For permission to reuse, contact [email protected].
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Fig. 4.—Top: Unbinned time series nNa (Fig. 2, top panel). Bottom: These data binned in time (each point is the median value in each bin). There are 10 bins, with roughly equal numbers of observations per bin (42). The error bars indicate the estimated standard deviation of the median. The solid curve is a model for the difference of two transit curves (described in § 3), scaled to the observed offset in the mean during transit, ΔnNa = −2.32 × 10−4.
From The Astrophysical Journal 568(1):377–384.© 2002 by The American Astronomical Society.For permission to reuse, contact [email protected].
Charbonneau et al. 2001
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Redfield et al. 2007 Sodium
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Calcium
An element not expected to show excess absorption shows none
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Vidal-Majar et al. 2003
HD 209458 shows excess abroption in Hydrogen Lyman
Evidence for an evaporating atmosphere of Hydrogen?
Picture of the geocorona taken by the Apollo astronauts
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Fig. 3.— Comparison between Lyα line profiles in and out of transit period. The sky background spectral window is indicated by two dashed vertical lines. (a) The in-transit line profile (thin solid line) is accumulated for the time period starting 3900 s before TCT and ending 3900 s after it. To correct for the 8.9% obscuration derived in this study, the corresponding intensity is scaled by 1.098. ∼The resulting line profile (dotted curve) properly recovers the unperturbed line profile (histogram). (b) The first in-transit line profile, B1 (thin solid line), was accumulated over the time period starting 4000 s before the TCT and ending 600 s after it. The second in-transit line profile, B2 (dotted line), was accumulated over the time period starting 1800 s before TCT and ending 3900 s after it. ∼ ∼ ∼
From The Astrophysical Journal Letters 671(1):L61–L64.© 2007 by The American Astronomical Society.For permission to reuse, contact [email protected].
Ben-Jaffel 2007
Or not?
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Fig. 1.— Observed HD 209458 Lyα profiles as observed by VM03 before and during the planetary transit. The BJ07 reanalysis of nearly the same data set produced a similar Lyα line profile. The two vertical dashed lines define the limits and of the line core where H i planetary absorption takes place. In VM03 as well as in BJ07, the central part of the line (noted “Geo”) possibly perturbed by the Earth geocoronal emission is omitted from the analysis. The line wings are used by VM03 as a flux reference to correct for the stellar Lyα intrinsic variations.
From The Astrophysical Journal Letters 676(1):L57–L60.© 2008 by The American Astronomical Society.For permission to reuse, contact [email protected].
Vidal-Majar et al. 2008
Claim is that difference is due to different wavelength range used to calculate absorption depth
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Secondary Transits: The Planet Albedo
The planet reflects light, so one should see a modulation in the light curve, plus an eclipse of the planet
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Secondary Transits: The Planet Albedo
The planet reflects light, so one should see a modulation in the light curve, plus an eclipse of the planet
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Rowe et al. 2008
Albedo < 0.12
Jupiter: 0.5
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Fig. 7.— (a) Spherical albedo of a class III clear EGP. In addition to the isolated (thin curve) and modified (thick curve) T-P profile models, the dashed curve depicts what the albedo would look like in the absence of the alkali metals. (b) Spherical albedo of a class IV roaster. Theoretical albedo spectra of isolated (thin curve) and modified (thick curve) T-P profile class IV models are depicted.
Sudarsky et al. 2005.
900 < T < 1500 K
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Fig. 8.— Spherical albedo of a class V roaster. A silicate layer high in the atmosphere results in a much higher albedo than a class IV roaster. No ionization is assumed in this model.
From The Astrophysical Journal 538(2):885–903.© 2000 by The American Astronomical Society.For permission to reuse, contact [email protected].
T > 1500 K
Better upper limits will be found by CoRoT. Kepler may be able to detect the second transit.
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Secondary Transits with Kepler
For a short period giant in a 4 day orbit Kepler will observe more than 250 transits. It will be able to detect secondary transits (eclipses) for Albedos as low as 0.08
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Secondary Transits: Infrared Measurements with Spitzer
The „hot Jupiters“ have temperatures of ~ 1000 K. The radiated light can be much higher than the reflected light:
Reflected light = Lstar4d2 =
AR2
4d2
A = geometric albedo, R = planet radius, d = distance from star
For A = 0.1, d=0.05 AU, R = 1 RJup
Reflected light ≈ 10–5
AR2Lstar 1
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Secondary Transits: Infrared Measurements with Spitzer
In radiated light however, for a planet with Teff ≈ 1000 K:
Flux from planet = 2hc2/–5
ehc/kTp
–12Rp
2
Flux from star = 2hc2/–5
ehc/kT* –1
2R*2 Only looking at half
the star
Fp/F* = ehc/kT
* –1 Rp
2
ehc/kTp –1 R*
2
Fp/F* ≈ 0.0016
For a 1.5 RJup planet with Tp = 1000 K around a solar-type star (5800 K) at 8 m:
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Spitzer is a 0.85m telescope that can measure infrared radiation between 3 and 180 m
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HD 209458 secondary transit (eclipse) at 24 m
Teff = 1130 K
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Fig. 3.— Solid black line shows the Sudarsky et al. (2003) model hot Jupiter spectrum divided by the stellar model spectrum (see text for details). The open diamonds show the predicted flux ratios for this model integrated over the four IRAC bandpasses (which are shown in gray and renormalized for clarity). The observed eclipse depths at 4.5 and 8.0 μm are overplotted as black diamonds. No parameters have been adjusted to the model to improve the fit. The dotted line shows the best-fit blackbody spectrum (corresponding to a temperature of 1060 K), divided by the model stellar spectrum. Although the Sudarsky et al. (2003) model prediction is roughly consistent with the observations at 8.0 μm, the model overpredicts the planetary flux at 4.5 μm. The prediction of a relatively large flux ratio at 3.6 μm should be readily testable with additional IRAC observations.
From The Astrophysical Journal 626(1):523–529.© 2005 by The American Astronomical Society.For permission to reuse, contact [email protected].
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Spitzer Measurements of Radiated Light at 8 m of HD 189733
Knutson et al. 2007
Tmax = 1211 K
Tmin = 973 K
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Spitzer Measurements of Radiated Light at 8 m of HD 189733
Primary Secondary
Predicted time of secondary transit is off by 120 s → eccentricity?
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Brightest point is shifted by 16 degrees from the sub-stellar point
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GJ 836 Spitzer measurements
Radius = 4.33 ± 0.18 RE
Tp = 712 K
Eccentricity = 0.15
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Summary
1. 52 Transiting planets have been discovered so far. This is the Golden Era of transit detections
2. In 5 years more transiting planets than non-transiting planets will be known. My guess: 500
3. The measurement of the mean density is putting constraints on planet formation and structure theories
4. In-transit spectroscopy is yielding the first chemical composition of an extrasolar planet
5. Albedo measurements are placing contraints on atmospheric models
6. First indication of exoplanet „weather“
7. We are actually measuring the phyisical properties of the planets themselves: exoplanetary science
These are exciting times!