Sz. Csizmadia
German Aerospace Center
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by Sz. Csizmadia.
Astronomy and Astrophysics | 2013
J. M. Almenara; F. Bouchy; P. Gaulme; M. Deleuil; M. Havel; D. Gandolfi; Hans J. Deeg; G. Wuchterl; T. Guillot; B. Gardes; T. Pasternacki; S. Aigrain; Roi Alonso; M. Auvergne; A. Baglin; A. S. Bonomo; P. Bordé; J. Cabrera; S. Carpano; William D. Cochran; Sz. Csizmadia; C. Damiani; R. F. Díaz; R. Dvorak; Michael Endl; A. Erikson; S. Ferraz-Mello; M. Fridlund; G. Hébrard; Michaël Gillon
We report the discovery of two transiting exoplanets, CoRoT-25b and CoRoT-26b, both of low density, one of which is in the Saturn mass-regime. For each star, ground-based complementary observations through optical photometry and radial velocity measurements secured the planetary nature of the transiting body and allowed us to fully characterize them. For CoRoT-25b we found a planetary mass of 0.27 similar to 0.04 M-Jup, a radius of 1.08(-0.10)(+0.3) R-Jup and hence a mean density of 0.15(-0.06)(+ 0.15) g cm(-3). The planet orbits an F9 mainsequence star in a 4.86-day period, that has a V magnitude of 15.0, solar metallicity, and an age of 4.5(-2.0) (+1.8)-Gyr. CoRoT-26b orbits a slightly evolved G5 star of 9.06 +/- 1.5-Gyr age in a 4.20-day period that has solar metallicity and a V magnitude of 15.8. With a mass of 0.52 +/- 0.05 MJup, a radius of 1.26(-0.07)(+0.13) R-Jup, and a mean density of 0.28(-0.07)(+0.09) g cm(-3), it belongs to the low-mass hot-Jupiter population. Planetary evolution models allowed us to estimate a core mass of a few tens of Earth mass for the two planets with heavy-element mass fractions of 0.52(-0.15)(+0.08) and 0.26(-0.08)(+0.05), respectively, assuming that a small fraction of the incoming flux is dissipated at the center of the planet. In addition, these models indicate that CoRoT-26b is anomalously large compared with what standard models could account for, indicating that dissipation from stellar heating could cause this size.
Nature | 2010
Hans J. Deeg; Claire Moutou; A. Erikson; Sz. Csizmadia; B. Tingley; P. Barge; H. Bruntt; M. Havel; S. Aigrain; J. M. Almenara; R. Alonso; M. Auvergne; A. Baglin; M. Barbieri; Willy Benz; A. S. Bonomo; P. Bordé; F. Bouchy; J. Cabrera; L. Carone; S. Carpano; David R. Ciardi; M. Deleuil; R. Dvorak; S. Ferraz-Mello; M. Fridlund; D. Gandolfi; J.C. Gazzano; Michaël Gillon; P. Gondoin
Of the over 400 known exoplanets, there are about 70 planets that transit their central star, a situation that permits the derivation of their basic parameters and facilitates investigations of their atmospheres. Some short-period planets, including the first terrestrial exoplanet (CoRoT-7b), have been discovered using a space mission designed to find smaller and more distant planets than can be seen from the ground. Here we report transit observations of CoRoT-9b, which orbits with a period of 95.274 days on a low eccentricity of 0.11 ± 0.04 around a solar-like star. Its periastron distance of 0.36 astronomical units is by far the largest of all transiting planets, yielding a ‘temperate’ photospheric temperature estimated to be between 250 and 430 K. Unlike previously known transiting planets, the present size of CoRoT-9b should not have been affected by tidal heat dissipation processes. Indeed, the planet is found to be well described by standard evolution models with an inferred interior composition consistent with that of Jupiter and Saturn.
Astronomy and Astrophysics | 2013
Sz. Csizmadia; T. Pasternacki; C. Dreyer; J. Cabrera; A. Erikson; H. Rauer
Context. The radius of an exoplanet is one of its most important parameters. Studies of planetary interiors and their evolution require 1% precision in the radius determination. Transiting exoplanets offer a unique oppurtunity to measure the radius of exoplanets in stellar units. These radius measurements and their precision are strongly affected by our knowledge of limb darkening. Aims. We study how the precision of the exoplanet radius determination is affected by our present knowledge of limb darkening in two cases: when we fix the limb darkening coefficients and when we adjust them. We also investigate the effects of spots in one-colour photometry. Methods. We study the effect of limb darkening on the planetary radius determination both via analytical expressions and by numerical experiments. We also compare some of the existing limb darkening tables. When stellar spots affect the fit, we replace the limb darkening coefficients, calculated for the unspotted cases, with effective limb darkening coefficients to describe the effect of the spots. Results. There are two important cases. (1) When one fixes the limb darkening values according to some theoretical predictions, the inconsistencies of the tables do not allow us to reach accuracy in the planetary radius of better than 1−10% (depending on the impact parameter) if the host star’s surface effective temperature is higher than 5000 K. Below 5000 K the radius ratio determination may contain even 20% error. (2) When one allows adjustment of the limb darkening coefficients, the a/Rs ratio, the planet-to-stellar radius ratio, and the impact parameter can be determined with sufficient accuracy (<1%), if the signal-to-noise ratio is high enough. However, the presence of stellar spots and faculae can destroy the agreement between the limb darkening tables and the fitted limb darkening coefficients, but this does not affect the precision of the planet radius determination. We also find that it is necessary to fit the contamination factor, too. Conclusions. We conclude that the present inconsistencies of theoretical stellar limb darkening tables suggests one should not fix the limb darkening coefficients. When one allows them to be adjusted, then the planet radius, impact parameter, and the a/Rs can be obtained with the required precision.
Astronomy and Astrophysics | 2009
H. Rauer; D. Queloz; Sz. Csizmadia; M. Deleuil; R. Alonso; S. Aigrain; J. M. Almenara; M. Auvergne; A. Baglin; P. Barge; P. Bordé; F. Bouchy; H. Bruntt; J. Cabrera; L. Carone; S. Carpano; R. de la Reza; Hans J. Deeg; R. Dvorak; A. Erikson; M. Fridlund; D. Gandolfi; M. Gillon; Tristan Guillot; E. W. Guenther; A. Hatzes; G. Hébrard; P. Kabath; L. Jorda; H. Lammer
Aims. The CoRoT space mission continues to photometrically monitor about 12 000 stars in its field-of-view for a series of target fields to search for transiting extrasolar planets ever since 2007. Deep transit signals can be detected quickly in the “alarm-mode” in parallel to the ongoing target field monitoring. CoRoT’s first planets have been detected in this mode. Methods. The CoRoT raw lightcurves are filtered for orbital residuals, outliers, and low-frequency stellar signals. The phase folded lightcurve is used to fit the transit signal and derive the main planetary parameters. Radial velocity follow-up observations were initiated to secure the detection and to derive the planet mass. Results. We report the detection of CoRoT-5b, detected during observations of the LRa01 field, the first long-duration field in the galactic anticenter direction. CoRoT-5b is a “hot Jupiter-type” planet with a radius of 1.388+0.046 −0.047 RJup, a mass of 0.467 +0.047 −0.024 MJup, and therefore, a mean density of 0.217+0.031 −0.025 g cm −3. The planet orbits an F9V star of 14.0 mag in 4.0378962 ± 0.0000019 days at an orbital distance of 0.04947+0.00026 −0.00029 AU.Aims. The CoRoT space mission continues to photometrically monitor about 12 000 stars in its field-of-view for a series of target fields to search for transiting extrasolar planets ever since 2007. Deep transit signals can be detected quickly in the “alarm-mode” in parallel to the ongoing target field monitoring. CoRoT’s first planets have been detected in this mode. Methods. The CoRoT raw lightcurves are filtered for orbital residuals, outliers, and low-frequency stellar signals. The phase folded lightcurve is used to fit the transit signal and derive the main planetary parameters. Radial velocity follow-up observations were initiated to secure the detection and to derive the planet mass. Results. We report the detection of CoRoT-5b, detected during observations of the LRa01 field, the first long-duration field in the galactic anticenter direction. CoRoT-5b is a “hot Jupiter-type” planet with a radius of 1.388 +0.046 −0.047 RJup ,am ass of 0.467
Astronomy and Astrophysics | 2004
Sz. Csizmadia; P. Klagyivik
We have compiled a catalogue of light curve solutions of contact binary stars. It contains the results of 159 light curve solutions. The properties of contact binary stars were studied using the catalogue data. As is well known since Lucys ([CITE],b) and Mochnackis ([CITE]) studies, primary components transfer their own energy to the secondary star via the common envelope around the two stars. This transfer was parameterized by a transfer parameter (ratio of the observed and intrinsic luminosities of the primary star). We prove that this transfer parameter is a simple function of the mass and luminosity ratios. We introduced a new type of contact binary stars: H subtype systems which have a large mass ratio (
Astronomy and Astrophysics | 2014
S. C. C. Barros; J. M. Almenara; M. Deleuil; R. F. Díaz; Sz. Csizmadia; J. Cabrera; S. Chaintreuil; A. Collier Cameron; A. Hatzes; R. D. Haywood; A. Lanza; S. Aigrain; R. Alonso; P. Bordé; F. Bouchy; H. J. Deeg; A. Erikson; Malcolm Fridlund; S. Grziwa; D. Gandolfi; T. Guillot; E. W. Guenther; A. Léger; Claire Moutou; M. Ollivier; T. Pasternacki; M. Pätzold; H. Rauer; D. Rouan; A. Santerne
q>0.72
Astronomy and Astrophysics | 2004
P. Ábrahám; Á. Kóspál; Sz. Csizmadia; A. Moór; M. Kun; Guy S. Stringfellow
). These systems show behaviour in the luminosity ratio- transfer parameter diagram that is very different from that of other systems and according to our results the energy transfer rate is less efficient in them than in other types of contact binary stars. We also show that different types of contact binaries have well defined locations on the mass ratio – luminosity ratio diagram. Several contact binary systems do not follow Lucys relation (
Astronomy and Astrophysics | 2009
J. M. Almenara; Hans J. Deeg; S. Aigrain; R. Alonso; M. Auvergne; A. Baglin; M. Barbieri; P. Barge; P. Bordé; F. Bouchy; H. Bruntt; J. Cabrera; L. Carone; S. Carpano; Claude Catala; Sz. Csizmadia; R. De La Reza; M. Deleuil; R. Dvorak; A. Erikson; M. Fridlund; D. Gandolfi; M. Gillon; P. Gondoin; E. W. Guenther; Tristan Guillot; A. Hatzes; G. Hébrard; L. Jorda; H. Lammer
L_2/L_1 = (M_2/M_1)^{0.92}
Astronomy and Astrophysics | 2004
P. Ábrahám; Á. Kóspál; Sz. Csizmadia; Mária Kun; Attila Moor; Timo Prusti
). No strict mass ratio – luminosity ratio relation of contact binary stars exists.
Astronomy and Astrophysics | 2005
T. Borkovits; M. M. Elkhateeb; Sz. Csizmadia; J. Nuspl; Imre Barna Biro; T. Hegedus; R. Csorvási
The first super-Earth with measured radius discovered was CoRoT-7b and it has opened the new field of rocky exoplanet characterisation. To better understand this interesting system, new observations were taken with the CoRoT satellite. During this run 90 new transits were obtained in the imagette mode. These were analysed together with the previous 151 transits obtained in the discovery run and HARPS radial velocity observations to derive accurate system parameters. A difference is found in the posterior probability distribution of the transit parameters between the previous CoRoT run (LRa01) and the new run (LRa06). We propose that this is due to an extra noise component in the previous CoRoT run suspected of being transit spot occultation events. These lead to the mean transit shape becoming V-shaped. We show that the extra noise component is dominant at low stellar flux levels and reject these transits in the final analysis. We obtained a planetary radius, Rp = 1.585 ± 0.064 R⊕, in agreement with previous estimates. Combining the planetary radius with the new mass estimates results in a planetary density of 1.19 ± 0.27 ρ⊕ which is consistent with a rocky composition. The CoRoT-7 system remains an excellent test bed for the effects of activity in the derivation of planetary parameters in the shallow transit regime.