Model of the Corot satellite
|Organization||Centre National d'Etudes Spatiales
European Space Agency
|Launch date||2006-12-27 14:24:00 UTC|
|Launched from||Baikonur Cosmodrome
|Launch vehicle||Soyuz 2.1b/Fregat|
|Mission length||2.5 + 4 years
(6 years, 5 months, and 23 days elapsed)
|Type of orbit||Polar|
|Orbit height||827 km|
COROT (French: COnvection ROtation et Transits planétaires; English: COnvection ROtation and planetary Transits) is a space mission led by the French Space Agency (CNES) in conjunction with the European Space Agency (ESA) and other international partners. The mission's two objectives are to search for extrasolar planets with short orbital periods, particularly those of large terrestrial size, and to perform asteroseismology by measuring solar-like oscillations in stars.1 It was launched at 14:28:00 UTC on 27 December 2006, atop a Soyuz 2.1b carrier rocket,234 reporting first light on 18 January 2007.5 Subsequently, the probe started to collect science data on 2 February 2007.6 COROT is the first spacecraft dedicated to the detection of transiting extrasolar planets, opening the way for more advanced probes such as Kepler and possibly TESS and PLATO. It detected its first extrasolar planet, COROT-1b, in May 2007,7 just 3 months after the start of the observations. Mission flight operations were originally scheduled to end 2.5 years from launch8 but operations were extended to 2013.9 A new extension has been proposed to keep COROT in operation till 2015.10 On 2 November 2012, CoRoT suffered a computer failure that makes it impossible to retrieve any data from its telescope; efforts for recovery are currently under way.11As of January 2013, COROT's future is still uncertain.12
The COROT optical design minimizes stray light coming from the Earth and provides a field of view of 2.7° by 3.05°. The COROT optical path consists of a 27 cm (10.6 in) diameter off-axis afocal telescope housed in a two-stage opaque baffle specifically designed to block sunlight reflected by the Earth and a camera consisting of a dioptric objective and a focal box. Inside the focal box is an array of four CCD detectors protected against radiation by aluminum shielding 10mm thick. The asteroseismology CCDs are defocused by 760μm toward the dioptric objective to avoid saturation of the brightest stars. A prism in front of the planet detection CCDs gives a small spectrum designed to disperse more strongly in the blue wavelengths.13
The four CCD detectors are model 4280 CCDs provided by E2V Technologies. These CCDs are frame-transfer, thinned, back-illuminated designs in a 2048 pixel by 2048 pixel array. Each pixel is 13.5 × 13.5μm2 in size which corresponds to an angular pixel size of 2.32 arcsec. The CCDs are cooled to −40 °C (233.2 K; −40.0 °F). These detectors are arranged in a square pattern with two each dedicated to the planetary detection and asteroseismology. The data output stream from the CCDs are connected in two chains. Each chain has one planetary detection CCD and one asteroseismology CCD. The field of view for planetary detection is 3.5°.13
The satellite observes perpendicular to its orbital plane, meaning there will be no Earth occultations, allowing up to 150 days of continuous observation. These observation sessions, called "Long Runs", allow detection of smaller and long-period planets. During the remaining 30 days between the two main observation periods, COROT observes other patches of sky for a few weeks long "Short Runs", in order to analyze a larger number of stars for the asteroseismic program. After the loss of half the field of view due to failure of Data Processing Unit #1 in March 2009, the observation strategy changed to 3 months observing runs, in order to optimize the number of observed stars and detection efficiency.
In order to avoid the Sun entering in its field of view, during the northern summer COROT will observe in an area around Serpens Cauda, toward the galactic center, and during the winter it will observe in Monoceros, in the Galactic anticenter. Both these "eyes" of COROT have been studied in preliminary observations carried out between 1998 and 2005,14 allowing the creation of a database, called COROTSKY,15 with data about the stars located in these two patches of sky. This allows selecting the best fields for observation: the exoplanet research program requires a large number of dwarf stars to be monitored, and to avoid giant stars, for which planetary transits are too shallow to be detectable. The asteroseismic program requires stars brighter than magnitude 9, and to cover as many different types of stars as possible. In addition, in order to optimize the observations, the fields shouldn't be too sparse - fewer targets observed - or too crowded - too many stars overlapping. Several fields have been already observed:16
- IRa01, from 18 January 2007 to 3 April 2007 - 9879 stars observed;
- SRc01, from 3 April 2007 to 9 May 2007 - 6975 stars observed;
- LRc01, from 9 May 2007 to 15 October 2007 - 11408 stars observed;
- LRa01, from 15 October 2007 to 3 March 2008 - 11408 stars observed;
- SRa01, from 3 March 2008 to 31 March 2008 - 8150 stars observed;
- LRc02, from 31 March 2008 to 8 September 2008 - 11408 stars observed;
- SRc02, from 8 September 2008 to 6 October 2008 - 11408 stars observed;
- SRa02, from 6 October 2008 to 12 November 2008 - 10265 stars observed;
- LRa02, from 12 November 2008 to 30 March 2009 - 11408 stars observed;
- LRc03, from 30 March 2009 to 2 July 2009 - 5661 stars observed;
- LRc04, from 2 July 2009 to 30 September 2009 - 5716 stars observed;
- LRa03, from 30 September 2009 to 1 March 2010 - 5289 stars observed;
- SRa03, from 1 March 2010 to 2 April 2010;
- LRc05, from 2 April 2010 to 5 July 2010;
- LRc06, from 5 July 2010 to 27 September 2010;
- LRa04, from 27 September 2010 to 16 December 2010;
- LRa05, from 16 December 2010 to 5 April 2011;
- LRc07, from 5 April 2011 to 30 June 2011;
- SRc03, from 1 July 2011 to 5 July 2011 - a run made to reobserve the transit of COROT-9b;
- LRc08, from 6 July 2011 to 30 September 2011;
- SRa04, from 30 September 2011 to 28 November 2011;
- SRa05, from 29 November 2011 to 9 January 2012;
- LRa06, from 10 January 2012 to 29 March 2012 - a run dedicated to reobservation of COROT-7b;
- LRc09, from 10 April 2012, in progress.
The probe monitors the brightness of stars over time, searching for the slight dimming that happens in regular intervals when planets transit their primary sun. In every field, COROT records the brightness of thousands stars in the V-magnitude range from 11 to 16 for the extrasolar planet study. In fact, stellar targets brighter than 11 will saturate the exoplanets CCD detectors, yielding inaccurate data, whilst stars dimmer than 16 don't deliver enough photons to allow planetary detections. COROT will be sensitive enough to detect rocky planets with a radius two times larger than Earth, orbiting stars brighter than 14;17 it is also expected to discover new gas giants in the whole magnitude range.18
COROT will also undertake asteroseismology. It can detect luminosity variations associated with acoustic pulsations of stars. This phenomenon allows calculation of a star's precise mass, age and chemical composition and will aid in comparisons between the sun and other stars. For this program, in each field of view there will be one main target star for asteroseismology as well as up to nine other targets. The number of observed targets have dropped to half after the loss of Data Processing Unit #1.
The mission began on 27 December 2006 when a Russian Soyuz 2-1b rocket lifted the satellite into a circular polar orbit with an altitude of 827 km . The first scientific observation campaign started on 3 February 2007.19
Until March 2013, the mission's cost will amount to €170 million, of which 75% is paid by the French space agency CNES and 25% is contributed by Austria, Belgium, Germany, Spain, Brazil and the European Space Agency ESA.20
The primary contractor for the construction of the COROT vehicle was CNES,21 to which individual components were delivered for vehicle assembly. The COROT equipment bay, which houses the data acquisition and pre-processing electronics, was constructed by the LESIA Laboratory at the Paris Observatory and took 60 person-years to complete.21 The design and building of the instruments were done by the Laboratoire d'études spatiales et d'instrumentation en astrophysique (LESIA) de l'Observatoire de Paris, the Laboratoire d'Astrophysique de Marseille, the Institut d'Astrophysique Spatiale (IAS) from Orsay, the Centre spatial de Liège (CSL) in Belgium, the IWF in Austria, the DLR (Berlin) in Germany and the ESA Research and Science Support Department. The 30 cm afocal telescope Corotel has been realized by Alcatel Alenia Space in the Centre spatial de Cannes Mandelieu.
Before the beginning of the mission, the team stated with caution that COROT would only be able to detect planets few times larger than Earth or greater, and that it was not specifically designed to detect habitable planets. According to the press release announcing the first results, COROT's instruments are performing with higher precision than had been predicted, and may be able to find planets down to the size of Earth with short orbits around small stars.7 The transit method requires the detection of at least two transits, hence the planets detected will mostly have an orbital period under 75 day. Candidates that show only one transit have been found, but uncertainty remains about their exact orbital period.
COROT should be assumed to detect a small percentage of planets within the observed star fields, due to the low percentage of exoplanets that would transit from the angle of observation of our Solar System. The chances of seeing a planet transiting its host star is inversely proportional to the diameter of the planet's orbit, thus close in planets detections will outnumber outer planets ones. The transit method is also biased toward large planets, since their very depth transits are more easily detected than the shallows eclipses induced by terrestrial planets.
On March 8, 2009 the satellite suffered a loss of communication with Data Processing Unit #1, processing data from one of the two photo-detector chains on the spacecraft. Science operations resumed early April with Data Processing Unit #1 offline while Data Processing Unit #2 operating normally. The loss of photo-detector chain number 1 results in the loss of one CCD dedicated to asteroseismology and one CCD dedicated to planet detection. The field of view of the satellite is thus reduced by 50%, but without any degradation of the quality of the observations. The loss of channel 1 appears to be permanent.22
The rate of discoveries of transiting planets is dictated by the need of ground based follow-up observations, needed to verify the planetary nature of the transit candidates. Candidate detections have been obtained for about 2,3% of all COROT targets, but finding periodic transit events isn't enough to claim a planet discovery, since several configurations could mimic a transiting planet, such as stellar binaries, or an eclipsing fainter star very close to the target star, whose light, blended in the light curve, can reproduce transit-like events. A first screening is executed on the light curves, searching hints of secondary eclipses or a rather V-shaped transit, indicative of a stellar nature of the transits. For the brighter targets, the prism in front of the exoplanets CCDs provides photometry in 3 different colors, enabling to reject planet candidates that have different transit depths in the three channels, a behaviour typical of binary stars. These tests allow to discard 83% of the candidate detections,23 whilst the remaining 17% are screened with photometric and radial velocity follow-up from a network of telescopes around the world. Photometric observations, required to rule out a possible contamination by a diluted eclipsing binary in close vicinity of the target,24 is performed on several 1 m-class instruments, but also employs the 2 m Tautenburg telescope in Germany and the 3,6 m CFHT/Megacam in Hawaii. The radial velocity follow-up allows to discard binaries or even multiple star system and, given enough observations, provide the mass of the exoplanets found. Radial velocity follow-up is performed high-precision spectrographs, namely SOPHIE, HARPS and HIRES.25 Once the planetary nature of the candidate is established, high-resolution spectroscopy is performed on the host star, in order to accurately determine the stellar parameters, form which further derive the exoplanet characteristics. Such work is done with large aperture telescopes, as the UVES spectrograph or HIRES.
Interesting transiting planets could be further followed-up with the infrared Spitzer Space Telescope, to give an independent confirmation at a different wavelength and possibly detect reflected light from the planet or the atmospheric compositions. COROT-7b and COROT-9b have already been observed by Spitzer.
Papers presenting the results of follow-up operations of planetary candidates in the IRa01,26 LRc01,27 LRa01,28 SRc0129 fields have been published. Sometimes the faintness of the target star or its characteristics, such as a high rotational velocity or strong stellar activity, do not allow to determine unambiguously the nature or the mass of the planetary candidate.
Like a musical instrument a star vibrates according to pulsation modes similar to the variety of sounds emitted by the instrument. Listening to an air of guitar does not leave any doubt on the nature of the instrument and even, for a warned musician, on the cords' material and tension. Similarly stellar pulsation modes are characteristic of stellar global properties and of the internal physical conditions. Analyzing these modes is thus a way of probing stellar interiors to infer stellar chemical compositions, rotation profiles and internal physical properties such as temperatures and densities. Asteroseismology is the science which study the vibration modes of a star. Each of these modes can be mathematically represented by a spherical harmonic of degree l and azimuthal order m. Some examples are presented here below with a color code such that blue (red) indicates a contracting (expanding) material (Sébastien Salmon). The amplitudes have been widely exaggerated.
Applied to the Sun since a few decades now, this science is called helioseismology. The solar surface helium abundance was for the first time derived very accurately, which has definitely showed the importance of microscopic diffusion in the solar structure. Helioseismology analyses has also unveiled the solar internal rotational profile, the precise extent of the convective envelope and the location of the helium ionization zone. Despite enormous technical challenges, it was thus tempting to apply similar analyses to stars. From the ground this was only possible for stars close to the Sun such as α Centauri, Procyon, β Virginis... The goal is to detect extremely small light variations (down to 1 ppm) and to extract the frequencies responsible for these brightness fluctuations. This produces a frequency spectrum typical of the star under scrutiny. Oscillations periods vary from a few minutes to several hours depending of the type of stars and their evolution state. To reach such performances, long observing times devoid of day/night alternations are required. Space is thus the ideal asteroseismic laboratory. By revealing their microvariability, measuring their oscillations at the ppm level, COROT has provided a new vision at stars, never reached before by any ground-based observation.
At the beginning of the mission, two out of four CCDs were assigned to asteroseismic observations of bright stars (apparent magnitude 6 to 9) in the so-called sismo field while the other CCDs were reserved for exoplanet hunting in the so-called exo field. Albeit with a lower signal to noise ratio, interesting science on stars was obtained also on the exoplanets channel data, where the probe records several thousands of light curves from every observed field. Stellar activity, rotation periods, star spots evolution, star-planets interactions, multiple star systems are nice extras in addition to the main asteroseismic program. This exo field also turned out to be of incalculable richness in asteroseismic discoveries as well. During its six first years of mission, CoRoT has observed about 150 bright stars in the sismo field and more than 150 000 weak stars in the exo field. The figure locates most of them in the Hertzsprung–Russell diagram together with some others observed from the ground.
Discoveries were numerous.30 Let us cite the first detection of solar-like oscillations in stars other than the Sun,31 the first detection of non radial oscillations in red giant stars,32 the detection of solar-like oscillations in massive stars33 · ,34 the discovery of hundreds of frequencies in δ Scuti stars,35 the spectacular time evolution of the frequency spectrum of a Be (emission lines B) star during an outburst,36 the first detection of a deviation from a constant period spacing in gravity modes in an SPB (Slowly Pulsating B) star.37 Interpreting those results opened new horizons in our vision of stars and galaxies. In October 2009 the CoRoT mission was the subject of a special issue of the Astronomy and Astrophysics Journal, dedicated to the early results of the probe.38 Here are below some examples of CoRoT breakthrough contributions to stellar astrophysics:
Above the convective core where mixing of chemicals is instantaneous and efficient, some layers can be affected by partial or total mixing during the main sequence phase of evolution. The extent of this extra mixed zone as well as the mixing efficiency are however difficult to assess. This additional mixing has very important consequences since it involves longer time scales for nuclear burning phases and may in particular affect the value of the stellar mass at the transition between those stars which end up their life as white dwarfs and those which face a final supernova explosion. The impact on the chemical evolution of the Galaxy is obvious. Physical reasons for this extra-mixing are various, either a mixing induced by internal rotation or a mixing resulting from convective bubbles crossing the convective core boundary to enter the radiative zone where they finally loose their identity (overshooting), or even some other not well known processes.
- Solar-like stars: The solar-like star HD 49933 is illustrative of this extra-mixing problem.39 Its convective envelope is responsible for the presence of solar-like oscillations. Comparing the observed frequency spectrum with that obtained from theoretical models of 1.19 Mʘ computed with and without additional mixing clearly excludes a model without extra mixing.
- Sub-giant stars: Such an additional mixing also affects the structure of more evolved sub-giant stars since the mass extension of the helium core formed during core hydrogen burning is increased. The sub-giant star HD 49385 of 1.3 Mʘ was submitted to CoRoT scrutiny and although not fully conclusive, new constraints were brought to the modeling of such stars.
- SPB stars: More massive SPB (Slowly Pulsating B) stars show a frequency spectrum dominated by high order gravity modes excited by the κ mechanism at work in layers where ionizations of iron group elements produces an opacity peak. In such stars, the convective core is surrounded by a region of varying chemical composition, the so-called μ-gradient region, left by the progressive withdrawal of the convective core as hydrogen is transformed into helium. This region is rather thin and constitutes a sharp transition region, which bears a very subtle signature in the gravity modes frequency spectrum. Instead of a constant period spacing found in a homogeneous stellar model, periodic deviations from this constant value are expected in models affected by a sharp transition region. Moreover the period of the deviations is directly related to the precise location of the sharp transition.40 This phenomenon has been detected in two hybrid B stars (showing at the same time acoustic β Cephei and gravity SPB modes): (1) HD 5023037 where an extra-mixing with a somewhat smooth shape is clearly required in the modeling and (2) HD 43317.41
- Transition layers in stellar envelopes: Transition layers such as the helium ionization region or the lower boundary of the convective envelope in low mass and red giant stars also affect frequency spectra. In a structure devoid of such discontinuities, high order acoustic modes obey some regularities in their frequency distribution (large frequency separation, second difference...). Transition zones introduce periodic deviations with respect to these regularities and the periods of the deviations are directly related to the precise location of the transition zones. These deviations were predicted by theory and were first observed in the Sun.42 Thanks to CoRoT they were also detected in the solar-like star HD 4993343 and also in the red giant star HD 181907.44 In both cases the location of the helium ionization zone could be accurately derived.
- Amplitudes and line widths in solar-like oscillation spectra: One of the major successes of the CoRoT space mission has definitely been the detection of solar-like oscillations in stars slightly hotter than the Sun.45 As was previously done for the Sun, measurements of amplitudes and line widths in their frequency spectra resulted in new constraints in the modeling of stochastic excitations of acoustic modes by turbulent convection. The frequency spectrum of HD 4993346 was confronted to the stochastic excitation model developed by Samadi et al.47 · .48 Except at high frequencies, a good agreement can be reached by adopting a metallicity ten times smaller than the solar metallicity. With the solar value on the contrary, disagreements in amplitudes can reach a factor 2 at low frequencies.
- Granulation: The presence of granulation was detected in the frequency spectrum of HD 49933. Analyses have been done with 3D hydrodynamical model atmospheres computed at solar and ten times smaller than solar metallicities.49 Here again the model with the lowest metallicity shows up to be closer to the observations although significant disagreements still remain.
Following exhaustion of hydrogen in the core, the overall stellar structure drastically changes. Hydrogen burning now takes place in a narrow shell surrounding the newly processed helium core. While the helium core quickly contracts and heats up, the layers above the hydrogen-burning shell undergo important expansion and cooling. The star becomes a red giant whose radius and luminosity increase in time. These stars are now located on the so-called red giant branch of the Hertzsprung–Russell diagram; they are commonly named RGB stars. Once their central temperature reaches 100 106 K, helium starts burning in the core. For stellar masses smaller than about 2 Mʘ, this new combustion takes place in a highly degenerate matter and proceeds through a helium flash. The readjustment following the flash brings the red giant to the so-called red clump (RC) in the Hertzsprung-Russell diagram.
Whether RGB or RC, these stars all have an extended convective envelope favorable to the excitation of solar-like oscillations. A major success of CoRoT has been the discovery of radial and long-lived non radial oscillations in thousands of red giants in the exo field.32 For each of them, the frequency at maximum power νmax in the frequency spectrum as well as the large frequency separation between consecutive modes Δν could be measured50 · ,51 defining a sort of individual seismic passport.
- Red giant population in our Galaxy: Introducing these seismic signatures, together with an estimation of the effective temperature, in the scaling laws relating them to the global stellar properties,52 gravities (seismic gravities), masses and radii can be estimated and luminosities and distances immediately follow for those thousands of red giants. Histograms could then be drawn and a totally unexpected and spectacular result came out when comparing these CoRoT histograms with theoretical ones obtained from theoretical synthetic populations of red giants in our Galaxy. Such theoretical populations were computed from stellar evolution models, with adopting various hypotheses to describe the successive generations of stars along the time evolution of our Galaxy.53 Andrea Miglio and collaborators noticed that both types of histograms were spitting images of one another,54 as can be seen in the histograms picture. Moreover adding the knowledge of the distances of these thousands of stars to their galactic coordinates, a 3D map of our Galaxy was drawn. This is illustrated in the figure where different colors relate to different CoRoT runs and to Kepler observations (green points).
- Age-metallicity relation in our Galaxy: The age of a red giant is closely related to its former main sequence lifetime, which is in turn determined by its mass and metallicity. Knowing the mass of a red giant amounts to knowing its age. If the metallicity is known the uncertainty in age does not exceed 15%! Observational missions such as APOGEE (Apache Point Observatoty Galactic Evolution Environment) whose goal is to measure metallicities for 100 000 red giants in our Galaxy, HERMES (A High Efficiency and Resolution Multi-Element Spectrograph for the AAT) and GAIA (Global Astrometric Interferometer for Astrophysics) could of course widely benefit from these seismic gravities with the ultimate output of establishing the age-metallicity relation in our Galaxy. Asteroseismology has crossed the doorstep of the structure and chemical evolution of our Galaxy.55
- Seismic signatures and extension of mixed zones during central hydrogen and helium burning: Increasing even further the scrutiny in analyzing the CoRoT56 and Kepler57 frequency spectra of red giants brought new important discoveries. Small and subtle differences in seismic signatures allow us to distinguish RGB from RC stars notwithstanding their similar luminosities. This is now theoretically confirmed thanks to elaborate red giant modeling.58 The period spacings of gravity-dominated modes are expected to be especially meaningful. Their detection for a large number of red giants could give us clues to establishing the extent of the extra-mixed region above the convective core during core hydrogen burning, but also the extent of the extra-mixed region during core helium burning, both mixing processes being a priori totally unrelated.59
Massive variable main sequence stars have frequency spectra dominated by acoustic modes excited by the κ mechanism at work in layers where partial ionization of iron group elements produce a peak in opacity. In addition the most advanced of these stars present mixed modes i.e. modes with a g-character in deep layers and p-character in the envelope. Hydrogen burning takes place in a convective core surrounded by a region of varying chemical composition and an envelope mostly radiative except for tiny convective layers related to partial ionization of helium and/or iron group elements. As in lower mass stars the extent of the fully or partially mixed region located just above the convective core (extra-mixed zone) is one of the main uncertainties affecting theoretical modeling.
- β Cephei stars: Seismic analyses of β Cephei stars show that it is not obvious to derive a one-to-one extent of this extra-mixed zone.60 A rather large extent seems to be required to model θ Ophiuchi61 while a much smaller one is favored for HD 12992962 · ,63 for β Canis Majoris,64 for δ Ceti65 and for 12 Lacertae66 · .67 This extra-mixed zone could even be absent in the structure of V1449 Aquilae (HD 180642)68 and ν Eridani69 · .70 It would be extremely interesting to establish a relation between the extent of this zone and the rotation velocity and/or the magnetic field of the star. Seismic analysis of V2052 Ophiuchi71 shows that this star although rapidly rotating, which would favor extra-mixing, could be devoid of such a region. The magnetic field detected in this star could be the reason of this lack of extra-mixing.
- Be stars: Late Be type stars HD 181231 and HD 175869 are very rapid rotators, about 20 times more rapid than the Sun. Their seismic analysis seems to require a centrally mixed zone about 20% larger than what is expected from convection only.72 Another Be star, HD 49330, had a very exciting surprise in store. Observed by CoRoT during an outburst of matter towards its circumstellar disk, which is typical of such stars, its frequency spectrum suffered drastic changes. Firstly dominated by acoustic modes the spectrum showed the appearance of gravity modes with amplitudes strictly in line with the outburst.73 Such a link between the nature of the excited modes and a dynamical phenomenon is of course a gold mine in our quest for the internal structure of Be stars.
- O stars: A bunch of O stars have been observed by CoRoT. Among them HD 46150 and HD 46223 (members of the galactic cluster NGC 2264) and HD 46966 (member of the OB association Mon OB2) do not seem to pulsate, which is in agreement with stellar modeling of stars with similar global parameters.74 The frequency spectrum of the Plaskett's star HD 47129 on the contrary shows a peak with six harmonics in the frequency range expected from theoretical modeling.75
Another unexpected CoRoT discovery was the presence of solar-like oscillations in massive stars. The small convective shell related to the opacity peak resulting from the ionization of iron group elements at about 200 000 K (iron opacity peak) could indeed be responsible for the stochastic excitation of acoustic modes like those observed in our Sun.
- V1449 Aquilae (HD 180642): This CoRoT target is a β Cephei star whose frequency spectrum reveals high frequency and very small amplitude acoustic modes. A careful analysis has shown that they were solar-like oscillations excited by turbulent bubbles origination from this convective iron opacity peak zone or even from the convective core.33 This is indeed a major discovery since it was the first time that pulsations excited by the κ mechanism acting in the iron opacity peak zone were present side by side in the same star with pulsations stochastically excited by this very same zone. This is the reason why Kevin Belkacem, main discoverer of these solar-like oscillations in V1449 Aquilae, added a new baptismal certificate to this β Cephei star and named it Chimera. The figure illustrates the behavior of the frequency versus time for two modes in the frequency spectrum of Chimera, a solar-like mode (top) and a β Cephei mode (bottom). The stochastic nature of the solar-like mode reveals itself in the instability of its frequency as time goes on and in the spread in frequency on several μHz. The contrast with the stability in frequency and the narrow frequency range of the β Cephei mode is striking.
- HD 46149: Later on solar-like oscillations were even discovered in a more massive O star member of the binary system HD 46149.34 Constraints coming from the binary nature of the system coupled with seismic constraints led to the determination of the orbital parameters of the system as well as to the global properties of its members.
During a 23 day observing run in March 2008, CoRoT observed 636 members of the young open cluster NGC 2264. The so-called Christmas tree cluster, is located in the constellation Monoceros relatively close to us at a distance of about 1800 light years. Its age is estimated to be between 3 and 8 million years. At such a young age, the cluster is an ideal target to investigate many different scientific questions connected to the formation of stars and early stellar evolution. The CoRoT data of stars in NGC 2264 allow us to study the interaction of recently formed stars with their surrounding matter, the rotation and activity of cluster members as well as their distribution, the interiors of young stars by using asteroseismology, and planetary and stellar eclipses.
The stellar births and the stars’ childhoods remain mostly hidden from us in the optical light because the early stars are deeply embedded in the dense molecular cloud from which they are born. Observations in the infrared or X-ray enable us to look deeper into the cloud, and learn more about these earliest phases in stellar evolution. Therefore in December 2011 and January 2012, CoRoT was part of a large international observing campaign involving four space telescopes and several ground based observatories. All instruments observed about 4000 stars in the young cluster NGC 2264 simultaneously for about one month at different wavelengths. The Canadian space mission MOST targeted the brightest stars in the cluster in the optical light, while CoRoT observed the fainter members. MOST and CoRoT observed NGC 2264 continuously for 39 days.76 The NASA satellites Spitzer and Chandra measured at the same time the stars in the infrared (for 30 days) and the X-ray domains (for 300 kiloseconds). Ground-based observations were taken also at the same time, for example, with the ESO Very Large Telescope in Chile, the Canadian-French-Hawaiian Telescope in Hawaii, the McDonald Observatory in Texas, or the Calar Alto Observatory in Spain.
The CoRoT observations led to the discovery of about a dozen pulsating pre-main sequence (PMS) δ Scuti stars and the confirmation of the existence of γ Doradus pulsations in PMS stars.77 Also the presence of hybrid δ Scuti/γ Doradus pulsations was confirmed in members of NGC 2264. The CoRoT observations included also the well known pre-main sequence pulsators, V 588 Mon and V 589 Mon, which were the first discovered members of this group of stars. The precision attained in the CoRoT light curves also revealed the important role of granulation in pre-main sequence stars.78
The investigation of T Tauri stars and their interaction with their circumstellar matter using CoRoT data revealed the existence of a new class, the AA Tauri type objects.79 Previously to the CoRoT observations, T Tauri stars were known to either show sinusoidal light variations that are caused by spots on the stellar surface, or completely irregular variability that is caused by the gas and dust disks surrounding the young stars. AA Tauri type objects show periodically occurring minima that are different in depth and width, hence are semi-regular variables. With the CoRoT observations this class of objects could be established.80 Exciting insights into the earliest phases of stellar evolution also come from the comparison of the variability present in the optical light to that in the infrared and the X-ray regime.
A large number of binary systems with non-radially pulsating members were observed by CoRoT.81 Some of them, which were eclipsing binaries with members of γ Doradus type, were discovered during CoRoT runs.82 The eclipse phenomenon plays a keyhole since global parameters can immediately follow, bringing invaluable constraints, in addition to the seismic ones, to stellar modeling.
- AU Monocerotis: This semi-detached binary system contains a Be star interacting with its G star companion. Its observation by CoRoT provided an extremely high quality ligthcurve. Global parameters could then be improved and new ephemeris for the orbital motion as well as for another long term variation were derived. This long period variation seems to originate from a periodic light attenuation by circumstellar dust.83
- HD 174884: Tidally induced pulsations have been detected in the high eccentricity (e=0.29) and short period binary system HD 174884 consisting of two B stars.84 The upper panel of the figure shows the full light curve of the system. In the second panel tiny secondary eclipses are seen with a depth of about 1% of the depth of the primary eclipse. Actually the system is formed of stars of similar mass, size and temperature. Were the orbit circular, the eclipses would be similar in depth. However the orbit is highly eccentric and its orientation in space with respect to us is such that the secondary eclipse occurs when the stars are at a larger distance than at primary eclipse. The third panel of the figure shows the projection on the plane of the sky (i.e. the system as we see it) at different orbital phases.
- CoRoT 102918586: The relatively bright eclipsing system CoRoT 102918586 is a double-lined spectroscopic binary, observed by CoRoT, which revealed clear evidence of γ Doradus type pulsations. In addition to CoRoT photometry, a spectroscopic follow-up was performed which yielded the radial velocity curves, the component effective temperatures, the metallicity, and the line-of-sight projected rotational velocities. The eclipsing binary light curve analysis, combined with the spectroscopic results, provided system physical parameters with 1-2% accuracy while the comparison with evolutionary models led to constraints on the age of the system. After subtracting the best–fitting eclipsing binary model, the residuals were analyzed to determine the pulsation properties. The primary star pulsates with typical γ Dor frequencies and shows a period spacing consistent with high order g-modes of degree l=1.
- HR 6902: The binary system ζ Aurigae HR 6902 containing a red giant and a B star was observed by CoRoT during two runs, which allowed us to fully cover the primary as well as the secondary eclipses. This system is presently being analyzed with the ultimate goal of bringing new constraints on the internal structure of the red giant in particular.85
- A low mass binary: One of the binary system observed by CoRoT is of particular interest since the less massive component is a late M star of 0.23 M⊙ with an estimated effective temperature of about 3000 K.86 The primary component is a 1.5 M⊙ star MS star.
- A beaming effect in a binary: A binary system observed by CoRoT showed out of eclipses variations which were interpreted as a beaming effect (also called Doppler boosting). This effect results from the variation in brightness of source approaching or moving away from the observer, with an amplitude proportional to the radial velocity divided by the speed of light.87 The periodic variation in the velocity of an orbiting star will thus produce a periodic beaming variation in the light curve. Such an effect can confirm the binary nature of a system even without any detectable eclipses nor transits. One of the main advantages of the beaming effect is the possibility to determine the radial velocity directly from the light curve but very different luminosities of the binary components are required and a single radial velocity curve can only be obtained as in an SB1 binary system. The out of eclipse variations were modeled with the BEER (Beaming Ellipsoidal Reflection) algorithm.88
The COROT exoplanet science team has decided to publish confirmed and fully characterized planets only and not simple candidate lists. This strategy, different from the one pursued by the Kepler mission, where the candidates are regularly updated and made available to the public, is quite lengthy. On the other hand, the approach also increases the scientific return of the mission, as the set of published COROT discoveries constitute some of the best exoplanetary studies carried out so far.
COROT discovered its first two planets in 2007: the hot Jupiters COROT-1b and COROT-2b.790 Results on asteroseismology were published in the same year.91 By further analysis, COROT-1b became the first exoplanets to have its secondary eclipse detected in the optical,92 thanks to the high precision lightcurve delivered by COROT.
In May 2008, two new exoplanets of Jupiter size, COROT-4b and COROT-5b, as well as an unknown celestial object, COROT-3b, were announced by ESA. COROT-3b, for its mass, appears to be "something between a brown dwarf and a planet." According to the definition of planet proposed by the owners of the exoplanet.eu database93 three years later, COROT-3b, being less massive than 25 Jupiter masses, is classified as an exoplanet.
In February 2009, during the First Corot Symposium, the super-earth COROT-7b was announced, which at the time was the smallest exoplanet to have its diameter confirmed, at 1.58 Earth diameters. The discoveries of a second non transiting planet in the same system, COROT-7c, and of a new Hot Jupiter, COROT-6b, were also announced at the Symposium.
In March 2010 COROT-9b was announced. With 80% of Jupiter mass, and an orbit similar to the Mercury one, this is the first transiting temperate planet found known to be similar to those within our own Solar System.94 At the time of the discovery, it was the second longest period exoplanet found in transit, after HD80606 b.
In June 2010 the COROT team announced95 six new planets, COROT-8b, COROT-10b, COROT-11b, COROT-12b, COROT-13b, COROT-14b, and a brown dwarf, COROT-15b.96 All the planets announced are Jupiter sized, except COROT-8b, which appears to be somewhat between Saturn and Neptune.
In an August 2010 paper, COROT detected the ellipsoidal and the relativistic beaming effects in the COROT-3 lightcurve.97 The probe was also able to tentatively detect the reflected light at optical wavelengths of HD46375 b, a non transiting planet.98
In June 2011, during the Second Corot Symposium, the probe added ten new objects to the Exoplanet catalogue:99 COROT-16b, COROT-17b, COROT-18b, COROT-19b, COROT-20b, COROT-21b, COROT-22b, COROT-23b, COROT-24b, COROT-24c. The last two planets are of Neptune size, and orbit the same star, thus representing the first multiple transiting system detected by COROT. COROT-22b is also notable for its small size, having less than half the mass of Saturn.
As of November 2011, around 600 additional candidate exoplanets are being screened for confirmation.100
The following transiting planets have been announced by the mission.
Light green rows indicate that the planet orbits one of the stars in a binary star system.
|COROT-1||Monoceros||06h 48m 19s||−03° 06′ 08″||13.6||1560||G0V||b||1.03||1.49||1.5089557||0.0254||0||85.1||2007||101|
|COROT-2||Aquila||19h 27m 07s||+01° 23′ 02″||12.57||930||G7V||b||3.31||1.465||1.7429964||0.0281||0||87.84||2007||102|
|COROT-3||Aquila||19h 28m 13.265s||+00° 07′ 18.62″||13.3||2200||F3V||b||21.66||1.01||4.25680||0.057||0||85.9||2008||103|
|COROT-4||Monoceros||06h 48m 47s||−00° 40′ 22″||13.7||F0V||b||0.72||1.19||9.20205||0.090||0||90||2008||104|
|COROT-5||Monoceros||06h 45mm 07ss||+00° 48′ 55″||14||1304||F9V||b||0.459||1.28||4.0384||0.04947||0.09||85.83||2008||105|
|COROT-6||Ophiuchus||18h 44m 17.42s||+06° 39′ 47.95″||13.9||F5V||b||3.3||1.16||8.89||0.0855||< 0.1||89.07||2009||106|
|COROT-7||Monoceros||06h 43m 49.0s||−01° 03′ 46.0″||11.668||489||G9V||b||0.0151||0.150||0.853585||0.0172||0||80.1||2009||107|
|COROT-8||Aquila||19h 26m 21s||+01° 25′ 36″||14.8||1239||K1V||b||0.22||0.57||6.21229||0.063||0||88.4||2010||108|
|COROT-9||Serpens||18h 43m 09s||+06° 12′ 15″||13.7||1500||G3V||b||0.84||1.05||95.2738||0.407||0.11||>89.9||2010||109|
|COROT-10||Aquila||19h 24m 15s||+00 ° 44 ′ 46″||15.22||1125||K1V||b||2.75||0.97||13.2406||0.1055||0.53||88.55||2010||110|
|COROT-11||Serpens||18h 42m 45s||+05° 56′ 16″||12.94||1826||F6V||b||2.33||1.43||2.99433||0.0436||0||83.17||2010||111|
|COROT-12||Monoceros||06h 43m 04s||−01° 17′ 47″||15.52||3750||G2V||b||0.917||1.44||2.828042||0.04016||0.07||85.48||2010||112|
|COROT-13||Monoceros||06h 50m 53s||−05° 05′ 11″||15.04||4272||G0V||b||1.308||0.885||4.03519||0.051||0||88.02||2010||113|
|COROT-14||Monoceros||06h 53m 42s||−05° 32′ 10″||16.03||4370||F9V||b||7.58||1.09||1.51215||0.027||0||79.6||2010||114|
|COROT-16||Scutum||18h 34m 06s||−06° 00′ 09″||15.63||2740||G5V||b||0.535||1.17||5.3523||0.0618||0.33||85.01||2011||115|
|COROT-17||Scutum||18h 34m 47s||-06° 36′ 44 ″||15.46||3001||G2V||b||2.43||1.02||3.768125||0.0461||0||88.34||2011||116|
|COROT-18||Monoceros||06h 32m 41s||-00° 01′ 54″||14.99||2838||G9||b||3.47||1.31||1.9000693||0.0295||<0.08||86.5||2011||117|
|COROT-19||Monoceros||06h 28m 08s||-00° 01′ 01″||14.78||2510||F9V||b||1.11||1.45||3.89713||0.0518||0.047||87.61||2011||118|
|COROT-20||Monoceros||06h 30m 53s||+00° 13′ 37″||14.66||4012||G2V||b||4.24||0.84||9.24||0.0902||0.562||88.21||2011||119|
|COROT-22||Serpens||18h 42m 40s||+06° 13′ 08″||11.93||2052||G0IV||b||< 0.15||0.52||9.7566||0.094||< 0.6||89.4||2011|
|COROT-23||Serpens||18h 39m 08s||+04° 21′ 28″||15.63||1956||G0V||b||2.8||1.05||3.6314||0.0477||0.16||85.7||2011||121|
|COROT-24||Monoceros||06h 47m 41s||-03° 43′ 09″||4413||b||< 0.1||0.236||5.1134||2011|
|COROT-24||Monoceros||06h 47m 41s||-03° 43′ 09″||4413||c||0.173||0.38||11.749||2011|
The following table illustrates brown dwarf detected by COROT as well as non transiting planets detected in the follow-up program:
|COROT-7||Monoceros||06h 43m 49.0s||−01° 03′ 46.0″||11.668||489||G9V||c||planet||0.0264||-||3.69||0.046||0||-||2009||122|
|COROT-15||Monoceros||06h 28m 27.82s||+06° 11′ 10.47″||16||4140||F7V||b||brown dwarf||63.3||1.12||3.06||0.045||0||86.7||2010||123|
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- NASA Exoplanet Archive
- Kepler (spacecraft)
- Terrestrial Planet Finder
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- Space Interferometry Mission
- Darwin (spacecraft)
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