Transiting Exoplanets: Characterisation in the Presence of Stellar Activity

Total Page:16

File Type:pdf, Size:1020Kb

Transiting Exoplanets: Characterisation in the Presence of Stellar Activity —————————————————— Transiting exoplanets: characterisation in the presence of stellar activity Aude Ekundayo Pauline ALAPINI ODUNLADE —————————————————— Submitted by Mrs Aude Ekundayo Pauline Alapini Odunlade, to the University of Exeter as a thesis for the degree of Doctor of Philosophy in Physics, March 2010. This thesis is available for Library use on the understanding that it is copyright material and that no quo- tation from the thesis may be published without proper acknowledgement. I certify that all material in this thesis which is not my own work has been identified and that no material has previously been submitted and approved for the award of a degree by this or any other University. Mrs Aude E. P. Alapini Odunlade March 2010 This thesis was supervised by Dr. Suzanne Aigrain – University of Exeter, University of Oxford Abstract The combined observations of a planet’s transits and the radial velocity variations of its host star allow the determination of the planet’s orbital parameters, and most inter- estingly of its radius and mass, and hence its mean density. Observed densities provide important constraints to planet structure and evolution models. The uncertainties on the parameters of large exoplanets mainly arise from those on stellar masses and radii. For small exoplanets, the treatment of stellar variability limits the accuracy on the de- rived parameters. The goal of this PhD thesis was to reduce these sources of uncertainty by developing new techniques for stellar variability filtering and for the determination of stellar temperatures, and by robustly fitting the transits taking into account external constraints on the planet’s host star. To this end, I developed the Iterative Reconstruction Filter (IRF), a new post-detection stellar variability filter. By exploiting the prior knowledge of the planet’s orbital period, it simultaneously estimates the transit signal and the stellar variability signal, using a com- bination of moving average and median filters. The IRF was tested on simulated CoRoT light curves, where it significantly improved the estimate of the transit signal, particu- lary in the case of light curves with strong stellar variability. It was then applied to the light curves of the first seven planets discovered by CoRoT, a space mission designed to search for planetary transits, to obtain refined estimates of their parameters. As the IRF preserves all signal at the planet’s orbital period, t can also be used to search for secondary eclipses and orbital phase variations for the most promising cases. This en- abled the detection of the secondary eclipses of CoRoT-1b and CoRoT-2b in the white (300–1000 nm) CoRoT bandpass, as well as a marginal detection of CoRoT-1b’s orbital phase variations. The wide optical bandpass of CoRoT limits the distinction between thermal emission and reflected light contributions to the secondary eclipse. I developed a method to derive precise stellar relative temperatures using equiv- alent width ratios and applied it to the host stars of the first eight CoRoT planets. For stars with temperature within the calibrated range, the derived temperatures are con- sistent with the literature, but have smaller formal uncertainties. I then used a Markov Chain Monte Carlo technique to explore the correlations between planet parameters derived from transits, and the impact of external constraints (e.g. the spectroscopically derived stellar temperature, which is linked to the stellar density). Globally, this PhD thesis highlights, and in part addresses, the complexity of perform- ing detailed characterisation of transit light curves. Many low amplitude effects must be taken into account: residual stellar activity and systematics, stellar limb darkening, and the interplay of all available constraints on transit fitting. Several promising areas for further improvements and applications were identified. Current and future high precision photometry missions will discover increasing numbers of small planets around relatively active stars, and the IRF is expected to be useful in characterising them. Contents 1 Introduction 13 1.1 A brief history on the search for exoplanets . 13 1.2 The detection of exoplanets . 15 1.2.1 The methods . 15 1.2.2 Properties of the exoplanets discovered to date . 17 1.3 Characterising exoplanets . 20 1.3.1 Analytic equations to derive the planet parameters from the transit light curve . 20 1.3.2 Analytic equations for the radial velocity variations of a star due to an orbiting planet . 28 1.3.3 Planetary atmospheres . 30 1.4 Challenges for the detection and characterisation of exoplanets . 32 1.4.1 Stellar systems mimicking planetary transits . 32 1.4.2 Systematics . 33 1.4.3 Stellar activity . 33 1.4.4 Uncertainties on the planet parameters . 35 1.5 Instruments for the detection and characterisation of transiting exoplanets 37 1.5.1 Current . 37 1.5.2 Future of the transiting exoplanet search and characterisation . 39 1.6 This thesis . 40 1.6.1 Motivations . 40 1.6.2 Structure . 40 2 Transit signal reconstruction 42 2.1 Motivation . 42 2.2 Data set . 43 2.2.1 BT2 light curves . 43 2.2.2 Reference light curve sample . 44 2.3 Quantifying transit deformation with the Non-linear Iterative Filter . 45 2.3.1 Definition of the NIF . 46 2.3.2 NIF quantitative impact on transit parameters . 47 3 CONTENTS 4 2.4 A new stellar variability filter: the Iterative Reconstruction Filter . 49 2.4.1 Definition of the IRF . 49 2.4.2 Comparison with the Trend Filtering Algorithm (TFA) . 52 2.4.3 Performance of the IRF on the BT2 transits . 52 2.5 Discussion on the IRF performance . 54 2.5.1 Star-planet parameters . 54 2.5.2 Application to orbital signal reconstruction . 57 2.5.3 Potential application to transit detection . 57 2.6 Conclusion . 58 2.7 Appendix . 60 2.7.1 Best-fit parameters to BT2 transits . 60 2.7.2 Full BT2 light curve sample . 60 3 IRF applied to the transit of CoRoT planets 67 3.1 Description of the CoRoT data . 67 3.1.1 Instrument . 67 3.1.2 Light curve generation . 68 3.1.3 Additional light curve pre-processing . 70 3.1.4 Planetary transit detection and confirmation . 71 3.2 Primary transit parameters with the IRF-filtering . 71 3.2.1 Method . 71 3.2.2 CoRoT-1b . 75 3.2.3 CoRoT-2b . 77 3.2.4 CoRoT-3b . 79 3.2.5 CoRoT-4b . 81 3.2.6 CoRoT-5b . 83 3.2.7 CoRoT-6b . 85 3.2.8 CoRoT-7b . 87 3.2.9 Discussion . 89 3.3 IRF performance on CoRoT space data . 90 3.3.1 Limitations . 90 3.3.2 Future work . 90 4 Detecting photons from the CoRoT planets 92 4.1 Theory of the secondary eclipse and orbital phase variations . 93 4.1.1 Planet’s emission . 93 4.1.2 Secondary eclipse . 94 4.1.3 Planet’s equilibrium temperature . 94 4.1.4 Variations of secondary eclipse’s depth with Rp=R?, a=R?, AB and f 96 4.1.5 Expected depth and phase for the secondary eclipse of CoRoT planets . 100 CONTENTS 5 4.2 Method . 102 4.2.1 The IRF as a reconstruction tool . 102 4.2.2 Light curve processing . 103 4.2.3 Search for secondary eclipses and orbital phase variations . 104 4.2.4 Optimising the parameters of the IRF . 109 4.3 Application to CoRoT planets . 113 4.3.1 CoRoT-1b . 113 4.3.2 CoRoT-2b . 119 4.4 Discussion . 123 4.4.1 Comparison with the literature . 123 4.4.2 Performance of the IRF . 124 4.4.3 Limitations . 125 4.4.4 Future work . 126 4.5 Conclusions . 127 5 Stellar temperatures using equivalent width line-ratios 128 5.1 Teff calibration of equivalent width line-ratios . 129 5.1.1 Choosing the line ratios . 130 5.1.2 Calibrating the line ratios with temperature . 131 5.1.3 Using the calibration to derive stellar temperatures . 134 5.1.4 Testing the calibration . 136 5.1.5 Discussion . 139 5.2 Comparison to the calibration of Sousa et al. (2009) . 141 5.3 Applying the calibration to the host stars of CoRoT planets . 143 5.3.1 Spectra and equivalent width measurements . 143 5.3.2 Deriving the effective temperatures . 144 5.3.3 Discussion . 146 5.4 Conclusion . 147 5.5 Appendix . 148 5.5.1 Line list . 148 5.5.2 List of the calibration stars . 149 5.5.3 Plot of the line ratio and their calibration . 150 5.5.4 List of the line ratios and their calibration coefficients . 157 6 Joint modelling of transit and stellar temperature using an MCMC approach 161 6.1 Markov Chain Monte Carlo . 162 6.1.1 MCMC implementation . ..
Recommended publications
  • And Space-Based Photometry
    Mon. Not. R. Astron. Soc. 000, 1–17 (2002) Printed 5 December 2018 (MN LATEX style file v2.2) Transit analysis of the CoRoT-5, CoRoT-8, CoRoT-12, CoRoT-18, CoRoT-20, and CoRoT-27 systems with combined ground- and space-based photometry St. Raetz1,2,3⋆, A. M. Heras3, M. Fern´andez4, V. Casanova4, C. Marka5 1Institute for Astronomy and Astrophysics T¨ubingen (IAAT), University of T¨ubingen, Sand 1, D-72076 T¨ubingen, Germany 2Freiburg Institute of Advanced Studies (FRIAS), University of Freiburg, Albertstraße 19, D-79104 Freiburg, Germany 3Science Support Office, Directorate of Science, European Space Research and Technology Centre (ESA/ESTEC), Keplerlaan 1, 2201 AZ Noordwijk, The Netherlands 4Instituto de Astrof´ısica de Andaluc´ıa, CSIC, Apdo. 3004, 18080 Granada, Spain 5Instituto Radioastronom´ıa Milim´etrica (IRAM), Avenida Divina Pastora 7, E-18012 Granada, Spain Accepted 2018 November 8. Received: 2018 November 7; in original from 2018 April 6 ABSTRACT We have initiated a dedicated project to follow-up with ground-based photometry the transiting planets discovered by CoRoT in order to refine the orbital elements, constrain their physical parameters and search for additional bodies in the system. From 2012 September to 2016 December we carried out 16 transit observations of six CoRoT planets (CoRoT-5b, CoRoT-8b, CoRoT-12b, CoRoT-18b, CoRoT-20 b, and CoRoT-27b) at three observatories located in Germany and Spain. These observations took place between 5 and 9 yr after the planet’s discovery, which has allowed us to place stringent constraints on the planetary ephemeris. In five cases we obtained light curves with a deviation of the mid-transit time of up to ∼115 min from the predictions.
    [Show full text]
  • Naming the Extrasolar Planets
    Naming the extrasolar planets W. Lyra Max Planck Institute for Astronomy, K¨onigstuhl 17, 69177, Heidelberg, Germany [email protected] Abstract and OGLE-TR-182 b, which does not help educators convey the message that these planets are quite similar to Jupiter. Extrasolar planets are not named and are referred to only In stark contrast, the sentence“planet Apollo is a gas giant by their assigned scientific designation. The reason given like Jupiter” is heavily - yet invisibly - coated with Coper- by the IAU to not name the planets is that it is consid- nicanism. ered impractical as planets are expected to be common. I One reason given by the IAU for not considering naming advance some reasons as to why this logic is flawed, and sug- the extrasolar planets is that it is a task deemed impractical. gest names for the 403 extrasolar planet candidates known One source is quoted as having said “if planets are found to as of Oct 2009. The names follow a scheme of association occur very frequently in the Universe, a system of individual with the constellation that the host star pertains to, and names for planets might well rapidly be found equally im- therefore are mostly drawn from Roman-Greek mythology. practicable as it is for stars, as planet discoveries progress.” Other mythologies may also be used given that a suitable 1. This leads to a second argument. It is indeed impractical association is established. to name all stars. But some stars are named nonetheless. In fact, all other classes of astronomical bodies are named.
    [Show full text]
  • The Midnight Sky: Familiar Notes on the Stars and Planets, Edward Durkin, July 15, 1869 a Good Way to Start – Find North
    The expression "dog days" refers to the period from July 3 through Aug. 11 when our brightest night star, SIRIUS (aka the dog star), rises in conjunction* with the sun. Conjunction, in astronomy, is defined as the apparent meeting or passing of two celestial bodies. TAAS Fabulous Fifty A program for those new to astronomy Friday Evening, July 20, 2018, 8:00 pm All TAAS and other new and not so new astronomers are welcome. What is the TAAS Fabulous 50 Program? It is a set of 4 meetings spread across a calendar year in which a beginner to astronomy learns to locate 50 of the most prominent night sky objects visible to the naked eye. These include stars, constellations, asterisms, and Messier objects. Methodology 1. Meeting dates for each season in year 2018 Winter Jan 19 Spring Apr 20 Summer Jul 20 Fall Oct 19 2. Locate the brightest and easiest to observe stars and associated constellations 3. Add new prominent constellations for each season Tonight’s Schedule 8:00 pm – We meet inside for a slide presentation overview of the Summer sky. 8:40 pm – View night sky outside The Midnight Sky: Familiar Notes on the Stars and Planets, Edward Durkin, July 15, 1869 A Good Way to Start – Find North Polaris North Star Polaris is about the 50th brightest star. It appears isolated making it easy to identify. Circumpolar Stars Polaris Horizon Line Albuquerque -- 35° N Circumpolar Stars Capella the Goat Star AS THE WORLD TURNS The Circle of Perpetual Apparition for Albuquerque Deneb 1 URSA MINOR 2 3 2 URSA MAJOR & Vega BIG DIPPER 1 3 Draco 4 Camelopardalis 6 4 Deneb 5 CASSIOPEIA 5 6 Cepheus Capella the Goat Star 2 3 1 Draco Ursa Minor Ursa Major 6 Camelopardalis 4 Cassiopeia 5 Cepheus Clock and Calendar A single map of the stars can show the places of the stars at different hours and months of the year in consequence of the earth’s two primary movements: Daily Clock The rotation of the earth on it's own axis amounts to 360 degrees in 24 hours, or 15 degrees per hour (360/24).
    [Show full text]
  • Arxiv:0809.1275V2
    How eccentric orbital solutions can hide planetary systems in 2:1 resonant orbits Guillem Anglada-Escud´e1, Mercedes L´opez-Morales1,2, John E. Chambers1 [email protected], [email protected], [email protected] ABSTRACT The Doppler technique measures the reflex radial motion of a star induced by the presence of companions and is the most successful method to detect ex- oplanets. If several planets are present, their signals will appear combined in the radial motion of the star, leading to potential misinterpretations of the data. Specifically, two planets in 2:1 resonant orbits can mimic the signal of a sin- gle planet in an eccentric orbit. We quantify the implications of this statistical degeneracy for a representative sample of the reported single exoplanets with available datasets, finding that 1) around 35% percent of the published eccentric one-planet solutions are statistically indistinguishible from planetary systems in 2:1 orbital resonance, 2) another 40% cannot be statistically distinguished from a circular orbital solution and 3) planets with masses comparable to Earth could be hidden in known orbital solutions of eccentric super-Earths and Neptune mass planets. Subject headings: Exoplanets – Orbital dynamics – Planet detection – Doppler method arXiv:0809.1275v2 [astro-ph] 25 Nov 2009 Introduction Most of the +300 exoplanets found to date have been discovered using the Doppler tech- nique, which measures the reflex motion of the host star induced by the planets (Mayor & Queloz 1995; Marcy & Butler 1996). The diverse characteristics of these exoplanets are somewhat surprising. Many of them are similar in mass to Jupiter, but orbit much closer to their 1Carnegie Institution of Washington, Department of Terrestrial Magnetism, 5241 Broad Branch Rd.
    [Show full text]
  • The Kinematics of Arp 295 in H-Alpha Emission: an Interacting Galaxy
    Revista Mexicana de Astronom´ıa y Astrof´ısica, 00, ??–?? () THE KINEMATICS OF ARP 295 IN Hα EMISSION: AN INTERACTING GALAXY WITH HIGHLY ASYMMETRIC ROTATION Nathan Roche,1 Received November 4, 2018; accepted November 4, 2018 RESUMEN El resumen ser´atraducido al espa˜nol por los editores. We investigate Arp 295, a pair of interacting spirals at z = 0.023, using optical spectroscopy, Hα imaging, and Hα velocity mapping with the Manchester Echelle Spectrograph. Scalelengths are rexp =5.24 for Arp 295a and 2.52 kpc for 295b. A much smaller Im galaxy, Arp 295c, is associated with the larger spiral. Arp 295b is asymmetric with the disk more extended eastwards but with the brightest star-formation regions on its western side. The spectrum of Arp 295b shows strong emission lines with [OII]3727 equivalent width 36A.˚ The total Hα luminosities of Arp 295b and Arp 295c are 4.69 × 1041 and 6.76 × 1040 ergs s−1, corresponding to star-formation −1 rates 3.7 and 0.53 M⊙yr . For Arp 295b, we measure the maximum disk rotation velocity as 252.6 ± 9.9 km s−1 and find the rotation curve is very asymmetric. The east (approaching) side has a higher radial velocity than the west with the maximum difference (at r = 5 arcsec) 88 km s−1 or a factor 1.675. ABSTRACT We investigate Arp 295, a pair of interacting spirals at z =0.023, using optical spectroscopy, Hα imaging, and Hα velocity mapping with the Manchester Echelle Spectrograph. Scalelengths are rexp = 5.24 for Arp 295a and 2.52 kpc for 295b.
    [Show full text]
  • A Basic Requirement for Studying the Heavens Is Determining Where In
    Abasic requirement for studying the heavens is determining where in the sky things are. To specify sky positions, astronomers have developed several coordinate systems. Each uses a coordinate grid projected on to the celestial sphere, in analogy to the geographic coordinate system used on the surface of the Earth. The coordinate systems differ only in their choice of the fundamental plane, which divides the sky into two equal hemispheres along a great circle (the fundamental plane of the geographic system is the Earth's equator) . Each coordinate system is named for its choice of fundamental plane. The equatorial coordinate system is probably the most widely used celestial coordinate system. It is also the one most closely related to the geographic coordinate system, because they use the same fun­ damental plane and the same poles. The projection of the Earth's equator onto the celestial sphere is called the celestial equator. Similarly, projecting the geographic poles on to the celest ial sphere defines the north and south celestial poles. However, there is an important difference between the equatorial and geographic coordinate systems: the geographic system is fixed to the Earth; it rotates as the Earth does . The equatorial system is fixed to the stars, so it appears to rotate across the sky with the stars, but of course it's really the Earth rotating under the fixed sky. The latitudinal (latitude-like) angle of the equatorial system is called declination (Dec for short) . It measures the angle of an object above or below the celestial equator. The longitud inal angle is called the right ascension (RA for short).
    [Show full text]
  • September 2020 BRAS Newsletter
    A Neowise Comet 2020, photo by Ralf Rohner of Skypointer Photography Monthly Meeting September 14th at 7:00 PM, via Jitsi (Monthly meetings are on 2nd Mondays at Highland Road Park Observatory, temporarily during quarantine at meet.jit.si/BRASMeets). GUEST SPEAKER: NASA Michoud Assembly Facility Director, Robert Champion What's In This Issue? President’s Message Secretary's Summary Business Meeting Minutes Outreach Report Asteroid and Comet News Light Pollution Committee Report Globe at Night Member’s Corner –My Quest For A Dark Place, by Chris Carlton Astro-Photos by BRAS Members Messages from the HRPO REMOTE DISCUSSION Solar Viewing Plus Night Mercurian Elongation Spooky Sensation Great Martian Opposition Observing Notes: Aquila – The Eagle Like this newsletter? See PAST ISSUES online back to 2009 Visit us on Facebook – Baton Rouge Astronomical Society Baton Rouge Astronomical Society Newsletter, Night Visions Page 2 of 27 September 2020 President’s Message Welcome to September. You may have noticed that this newsletter is showing up a little bit later than usual, and it’s for good reason: release of the newsletter will now happen after the monthly business meeting so that we can have a chance to keep everybody up to date on the latest information. Sometimes, this will mean the newsletter shows up a couple of days late. But, the upshot is that you’ll now be able to see what we discussed at the recent business meeting and have time to digest it before our general meeting in case you want to give some feedback. Now that we’re on the new format, business meetings (and the oft neglected Light Pollution Committee Meeting), are going to start being open to all members of the club again by simply joining up in the respective chat rooms the Wednesday before the first Monday of the month—which I encourage people to do, especially if you have some ideas you want to see the club put into action.
    [Show full text]
  • IAU Division C Working Group on Star Names 2019 Annual Report
    IAU Division C Working Group on Star Names 2019 Annual Report Eric Mamajek (chair, USA) WG Members: Juan Antonio Belmote Avilés (Spain), Sze-leung Cheung (Thailand), Beatriz García (Argentina), Steven Gullberg (USA), Duane Hamacher (Australia), Susanne M. Hoffmann (Germany), Alejandro López (Argentina), Javier Mejuto (Honduras), Thierry Montmerle (France), Jay Pasachoff (USA), Ian Ridpath (UK), Clive Ruggles (UK), B.S. Shylaja (India), Robert van Gent (Netherlands), Hitoshi Yamaoka (Japan) WG Associates: Danielle Adams (USA), Yunli Shi (China), Doris Vickers (Austria) WGSN Website: https://www.iau.org/science/scientific_bodies/working_groups/280/ ​ WGSN Email: [email protected] ​ The Working Group on Star Names (WGSN) consists of an international group of astronomers with expertise in stellar astronomy, astronomical history, and cultural astronomy who research and catalog proper names for stars for use by the international astronomical community, and also to aid the recognition and preservation of intangible astronomical heritage. The Terms of Reference and membership for WG Star Names (WGSN) are provided at the IAU website: https://www.iau.org/science/scientific_bodies/working_groups/280/. ​ ​ ​ WGSN was re-proposed to Division C and was approved in April 2019 as a functional WG whose scope extends beyond the normal 3-year cycle of IAU working groups. The WGSN was specifically called out on p. 22 of IAU Strategic Plan 2020-2030: “The IAU serves as the ​ internationally recognised authority for assigning designations to celestial bodies and their surface features. To do so, the IAU has a number of Working Groups on various topics, most notably on the nomenclature of small bodies in the Solar System and planetary systems under Division F and on Star Names under Division C.” WGSN continues its long term activity of researching cultural astronomy literature for star names, and researching etymologies with the goal of adding this information to the WGSN’s online materials.
    [Show full text]
  • Transiting Exoplanets from the Corot Space Mission. XI. Corot-8B: a Hot
    Astronomy & Astrophysics manuscript no. corot-8b c ESO 2018 October 23, 2018 Transiting exoplanets from the CoRoT space mission XI. CoRoT-8b: a hot and dense sub-Saturn around a K1 dwarf? P. Borde´1, F. Bouchy2;3, M. Deleuil4, J. Cabrera5;6, L. Jorda4, C. Lovis7, S. Csizmadia5, S. Aigrain8, J. M. Almenara9;10, R. Alonso7, M. Auvergne11, A. Baglin11, P. Barge4, W. Benz12, A. S. Bonomo4, H. Bruntt11, L. Carone13, S. Carpano14, H. Deeg9;10, R. Dvorak15, A. Erikson5, S. Ferraz-Mello16, M. Fridlund14, D. Gandolfi14;17, J.-C. Gazzano4, M. Gillon18, E. Guenther17, T. Guillot19, P. Guterman4, A. Hatzes17, M. Havel19, G. Hebrard´ 2, H. Lammer20, A. Leger´ 1, M. Mayor7, T. Mazeh21, C. Moutou4, M. Patzold¨ 13, F. Pepe7, M. Ollivier1, D. Queloz7, H. Rauer5;22, D. Rouan11, B. Samuel1, A. Santerne4, J. Schneider6, B. Tingley9;10, S. Udry7, J. Weingrill20, and G. Wuchterl17 (Affiliations can be found after the references) Received ?; accepted ? ABSTRACT Aims. We report the discovery of CoRoT-8b, a dense small Saturn-class exoplanet that orbits a K1 dwarf in 6.2 days, and we derive its orbital parameters, mass, and radius. Methods. We analyzed two complementary data sets: the photometric transit curve of CoRoT-8b as measured by CoRoT and the radial velocity curve of CoRoT-8 as measured by the HARPS spectrometer??. Results. We find that CoRoT-8b is on a circular orbit with a semi-major axis of 0:063 ± 0:001 AU. It has a radius of 0:57 ± 0:02 RJ, a mass of −3 0:22 ± 0:03 MJ, and therefore a mean density of 1:6 ± 0:1 g cm .
    [Show full text]
  • Comprehensive Time Series Analysis of the Transiting Extrasolar Planet WASP-33B,
    A&A 553, A44 (2013) Astronomy DOI: 10.1051/0004-6361/201219642 & c ESO 2013 Astrophysics Comprehensive time series analysis of the transiting extrasolar planet WASP-33b, G. Kovács1,2,T.Kovács1,J.D.Hartman3,G.Á.Bakos3,, A. Bieryla4,D.Latham4,R.W.Noyes4, Zs. Regály1, and G. A. Esquerdo4 1 Konkoly Observatory, 1121 Budapest, Hungary e-mail: [email protected] 2 Department of Physics and Astrophysics, University of North Dakota, 58202-7129 Grand Forks, ND, USA 3 Department of Astrophysical Sciences, Princeton University, 08544 Princeton, NJ, USA 4 Harvard–Smithsonian Center for Astrophysics, 02138 Cambridge, MA, USA Received 22 May 2012 / Accepted 5 March 2013 ABSTRACT Context. HD 15082 (WASP-33) is the hottest and fastest rotating star known to harbor a transiting extrasolar planet (WASP-33b). The lack of high precision radial velocity (RV) data stresses the need for precise light curve analysis and gathering further RV data. Aims. By using available photometric and RV data, we perform a blend analysis, compute more accurate system parameters, confine the planetary mass, and, attempt to cast light on the observed transit anomalies. Methods. We combined the original HATNet observations and various followup data to jointly analyze the signal content and extract the transit component and used our RV data to aid the global parameter determination. Results. The blend analysis of the combination of multicolor light curves yields the first independent confirmation of the planetary nature of WASP-33b. We clearly identify three frequency components in the 15–21 d−1 regime with amplitudes 7–5 mmag. These frequencies correspond to the δ Scuti-type pulsation of the host star.
    [Show full text]
  • Hawaii Telescope by Dennis Crabtree (NRC-HIA) and Liz Bryson (CFHT) ● QSO Imaging with the CFHT by John Hutchings, HIA ● « the Seeing at the CFHT Is Very Good
    Winter Solstice 2004 NO. 123 Solstice d'hiver 2004 Winter Solstice ISSN 0715-474 A publication of CASCA Une publication de la Casca Special Issue Celebrating 25 years of Science at CFHT Potential Astronomical Sites in the Canadian Arctic Events at NRC's HIA (2004 Sept.- Dec.) / Du neuf à l'IHA du CNRC (sept.-déc. 2004) Legacy Survey Plans for the JCMT Towards a National Science Data Archive Gemini News An ALMA Update Reports file:///C|/kings/public_html/astro/ecass/issues/2004-ws/index2.htm (1 of 2) [12/21/2004 9:59:25 PM] TOC A montage of stunning CFHT On the images. For more images visit Cover the CFHT web site at this link. (return to front cover) CASCA ● From the Editor ● From the President Soap Box Features ● The Scientific Impact of the Canada-France-Hawaii Telescope by Dennis Crabtree (NRC-HIA) and Liz Bryson (CFHT) ● QSO imaging with the CFHT by John Hutchings, HIA ● « The seeing at the CFHT is very good. » by René Racine ● 25 years of spectacular discoveries with the CFHT coudé spectrographs - it was all in the detail by Gordon A.H. Walker ● Towards a National Science Data Archive by Elizabeth Griffin and David Schade Reports ● CTAC report for Gemini & CFHT for semester 2005a / Rapport du CATC de Gémini & TCFH pour le semestre 2005a ● JCMT CTAG Semester Report 2005a / Rapport Semestriel du GATC du TJCM 2005a ● Coalition for Canadian Astronomy - Report on Recent Activities by Gretchen Harris file:///C|/kings/public_html/astro/ecass/issues/2004-ws/toc.html (1 of 2) [12/21/2004 5:53:34 PM] TOC News ● An Alma Update by Chris Wilson ● Events at NRC's HIA (2004 Sept.-Dec.) / Du neuf à l'IHA du CNRC (sept.-déc.
    [Show full text]
  • Astronomical Coordinate Systems
    Appendix 1 Astronomical Coordinate Systems A basic requirement for studying the heavens is being able to determine where in the sky things are located. To specify sky positions, astronomers have developed several coordinate systems. Each sys- tem uses a coordinate grid projected on the celestial sphere, which is similar to the geographic coor- dinate system used on the surface of the Earth. The coordinate systems differ only in their choice of the fundamental plane, which divides the sky into two equal hemispheres along a great circle (the fundamental plane of the geographic system is the Earth’s equator). Each coordinate system is named for its choice of fundamental plane. The Equatorial Coordinate System The equatorial coordinate system is probably the most widely used celestial coordinate system. It is also the most closely related to the geographic coordinate system because they use the same funda- mental plane and poles. The projection of the Earth’s equator onto the celestial sphere is called the celestial equator. Similarly, projecting the geographic poles onto the celestial sphere defines the north and south celestial poles. However, there is an important difference between the equatorial and geographic coordinate sys- tems: the geographic system is fixed to the Earth and rotates as the Earth does. The Equatorial system is fixed to the stars, so it appears to rotate across the sky with the stars, but it’s really the Earth rotating under the fixed sky. The latitudinal (latitude-like) angle of the equatorial system is called declination (Dec. for short). It measures the angle of an object above or below the celestial equator.
    [Show full text]