Characterizing ultra-cool dwarfs on the search for exoplanets
the SPECULOOS project & the Trappist-1 system
F F = ✓ Rp R⇤ ◆2
c.fernandes@ulg.ac.be | speculoos@astro.ulg.ac.be & trappist@astro.ulg.ac.be
Catarina S. Fernandes with the SPECULOOS and the TRAPPIST teams
• 3 planets in the Habitable Zone
• Assuming Earth-like atmospheres these could
harbour liquid water oceans on their surface
• Ultra-cool dwarf stars (UCDs) (M6-M9) are the smallest,
dimmest, coolest and most abundant stars in our galaxy
M*=0.07 — 0.10 M , R*=0.09 — 0.15 R
Teff=2,000 — 2,600 K, logg = 5.0 — 5.5
• High probability of detecting small planets
• Studying the host star sets the physical constraints for
exoplanets and for the potential to sparkle life
Trappist-1 system
Ultra-cool dwarfs & transiting exoplanets
Seven earth-sized planets orbiting a M8 dwarf at 12 pc
2MASS J23062928 − 0502285
Trappist-1e transit. Combined light-curve observed with “Europa” and “Io” telescopes
Stellar evolution code developed at the University of Liege
Planets
Host star
7-planet resonant chain
• Trappist-1 h period confirmed: 18.77 days
• No additional planets detected • 3-body orbital-resonance
3
© 2017 Macmillan Publishers Limited, part of Springer Nature. All rights reserved. © 2017 Macmillan Publishers Limited, part of Springer Nature. All rights reserved.
NATURE ASTRONOMY 1, 0129 (2017) | DOI: 10.1038/s41550-017-0129 | www.nature.com/nastronomy
LETTERS
NATURE ASTRONOMY
less frequent than active M6–M9 dwarfs29) are consistent with a
low-activity M8 star, also arguing in favour of a relatively old system. An energetic flare erupted near the end of the K2 Campaign and was observed by Kepler. Full modelling of flares will be presented in a forthcoming p.
m
aper.
The K2 observations of the TRAPPIST-1 star have enabled the detection of the orbital period of TRAPPIST-1 h, continuing the pattern of Laplace resonance among adjacent triplets of planets. We search for, but do not detect, additional planets in the system. Compared with previous ground-based and Spitzer observations, the continuous coverage, high precision and shorter wavelength of the K2 observations enable a robust estimate of the rotational period and flare activity of the star, motivating further study of the atmospheres and dynamical evolution of the planetary system.
Q6
Although the long spin-down times of ultra-cool dwarfs pre-vent the derivation of a robust gyrochronology relation25, the
rota-tional period of TRAPPIST-1 can be used to derive a provisional age estimate for the system. Fourier analysis of the detrended K2 data (Fig. 2), which is visibly modulated by star spots, leads to the determination of a rotational period of ~3.3 days for the host star (see Methods). This rotation corresponds to an angular momentum of ~1% of that of the Sun. It is roughly in the middle of the period distribution of nearby late M dwarfs26, suggesting an age in the range
3–8 Gyr based on a star formation history that decreases slightly over time27. Such an age is consistent with the star’s solar
metallic-ity1 and borderline thin disk–thick disk kinematics28. The amplitude
of the modulation due to star spots and infrequent weak optical flares (0.26 day−1 for peak fluxes > 1% of the continuum, 40 times
70 60 50 40 0.985 0.990 0.995 1.000 1.005 a b c d 101 100 90 80 0.985 0.990 0.995 1.000 1.005 –0.05 0.00 0.05 0.90 0.92 0.94 0.96 0.98 1.00 –0.06 –0.04 –0.02 0.00 0.02 0.04 0.06 –0.06 –0.04 –0.02 0.00 0.02 0.04 0.06
K2 long cadence data
Barycentric julian date 2,457,700 (day)
Relative brightness
Relative brightness
K2 in safe mode
1b 1c 1d 1e 1f 1g 1h
1b 1c 1d 1e 1f 1g 1h
Time from mid–transit (day)
Relative brightness Transit 1 Transit 2 Transit 3 Transit 4 Folded lightcurve
Orbital separation (au)
Figure 1 | Long cadence K2 light curve of TRAPPIST-1 detrended with EVEREST. a, b, Full detrended K2 light curve with stellar variability removed. m
via LOESS regression (order = 1; width = 0.15 day). Data points are in black and our highest likelihood transit model for all seven planets is plotted in thin grey. Coloured diamonds indicate which transit belongs to which planet. Four transits of TRAPPIST-1 h are observed (light blue diamonds). c, Top four curves
show the detrended and whitened short cadence in light blue, with a transit model based on the Spitzer parameters in dark blue. Binned data is over-plotted in white for clarity. The folded light curve is displayed at the bottom. d, View from above (observer to the right) of the TRAPPIST-1 system at the
date when the first transit was obtained for this system. The grey region is the surface liquid water habitable zone.
Q22
Gillon et al. 2016 Nature 533, 221
Illustration: NASA
K2 data. Long cadence (texp = 30 min) one in 78 days (K2 data length)Super flare
Low-activity, middle-aged, late M-dwarf
• Flare rate above 1% of the continuum: 0.26 events/day • Stellar rotational period: 3.3 days
• Stellar age: 3 — 8 Gyr
Luger et al. 2017 Nat. Astron, 1, 0129
• The SPECULOOS project will search for transiting
exoplanets
• This is a survey targeting the nearest UCDs with
four 1-m robotic telescopes at Paranal, Chile
• This concept has been tested with the
Trappist-South and North telescopes
Stellar models for UCDs and the Trappist-1 star
Conclusion and what is next
Gillon et al. 2017 Nature 542, 456
CLES
Scuflaire et al. 2008 Astrophys. Space. Sci.316, 83Code Liégeois d’Évolution Stellaire Van Grootel et al.
in prep.
• UCDs are excellent targets for searching transiting earth-sized planets • Trappist-1 system was discovered while surveying UCDs
• CLES stellar evolution code is ready to carry-on studies with UCDs
• To account for an age > 7Gyr for Trappist-1, the stellar models suggest a
revision of the stellar mass which has an affect on planetary-star relations
• New discoveries made with the SPECULOOS project are potential targets for
the Extremely Large Telescopes and the JWST/NASA with further studies on atmospheric characterisation and searching biosignatures
• Continuing working on improving stellar evolution models for low-mass stars
Fernandes et al. in prep.
Recently adapted to account for low-mass stars
• Include meaningful equation of state [1], [2]
• Adapt public atmosphere model grid: BT-Settl [3]
• Able to choose different metallicities, other than solar
• Compared with low-mass stellar evolution code (BHAC15) [4]
with the same input physics (differences less than 1%)
• Testing with M7 binary [5]: M (dynamical [5]) = 0.088 ± 0.001 M
Updated CLES
• Stellar parameters from observations and from combining
observations and stellar models
L*=(0.000524 ± 0.000034)L , ρ*= ρ
[Fe/H]= 0.04 ± 0.08, Age > 500 Myr
M*=(0.082 ± 0.011)M , R*=(0.116 ± 0.006)R , Teff= 2,555 ± 85 K
data-analysis from the K2 campaign 12
Testing new age
Stellar luminosity and density for CLES and BHAC15 evolution models for 0.08 M⊙ and 0.09 M⊙ with various metallicities, compared to luminosity and density measured for Trappist-1. If Trappist-1 star was ‘young’: M* = 0.08 M would agree with observations
Trappist-1 is not a young-star
• Indications of a middle-aged star has recently been constrained in [7] to 7.6 ± 2.2 Gyr
References
• [1] Saumon, D., Chabrier, G., & van Horn, H. M. 1995, ApJS, 99, 713• [2] Fontaine, G., Graboske, Jr., H. C., & van Horn, H. M. 1977, ApJS, 35, 293
• [3] Allard, F., Homeier, D., & Freytag, B. 2012a, Philosophical Transactions of the Royal
Society of London Series A, 370, 2765
Kepler-2 mission
View from above at the date when the first transit was obtained. The grey region is the surface liquid water HZ
New-mass from stellar models
•
M
*=0.09 M , with CLES and also confirmed by BHAC15 for measured luminosity
•Need to increase the metallicity to further account for the stellar density derived
from transits
• [4] Baraffe, I., Homeier, D., Allard, F., & Chabrier, G. 2015, A&A, 577, A42 • [5] Dupuy, T. J., Forbrich, J., Rizzuto, A., et al. 2016, ApJ, 827, 23
• [6] Press, W. H., Teukolsky, S. A., Vetterling, W. T., & Flannery, B. P. 1992, Numerical recipes in FORTRAN • [7] Burgasser & Mamajek 2017, arxiv: 1706.02018
Sponsors
“Europa” and “Io” telescopes at SPECULOOS Southern Observatory at ESO Paranal Observatory, Chile. Credit: P. Annual
{
Search for Planets EClipsing ULtra-cOOl Stars
PI: Michaël Gillon, Uni. Liège, michael.gillon@ulg.ac.be
{
The SPECULOOS project is an international collaboration
project
Time
• M (CLES & [6]) = 0.078 ± 0.03 M (with [Fe/H] (1σ) = 0.12) • M (BHAC15) = M