Atmospheric Remote- Sensing Infrared Exoplanet Large-Survey)
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The Planck Satellite and the Cosmic Microwave Background
The Cosmic Microwave Background, Dark Matter and Dark Energy Anthony Lasenby, Astrophysics Group, Cavendish Laboratory and Kavli Institute for Cosmology, Cambridge Overview The Cosmic Microwave Background — exciting new results from the Planck Satellite Context of the CMB =) addressing key questions about the Big Bang and the Universe, including Dark Matter and Dark Energy Planck Satellite and planning for its observations have been a long time in preparation — first meetings in 1993! UK has been intimately involved Two instruments — the LFI (Low — e.g. Cambridge is the Frequency Instrument) and the HFI scientific data processing (High Frequency Instrument) centre for the HFI — RAL provided the 4K Cooler The Cosmic Microwave Background (CMB) So what is the CMB? Anywhere in empty space at the moment there is radiation present corresponding to what a blackbody would emit at a temperature of ∼ 2:74 K (‘Blackbody’ being a perfect emitter/absorber — furnace with a small opening is a good example - needs perfect thermodynamic equilibrium) CMB spectrum is incredibly accurately black body — best known in nature! COBE result on this showed CMB better than its own reference b.b. within about 9 minutes of data! Universe History Radiation was emitted in the early universe (hot, dense conditions) Hot means matter was ionised Therefore photons scattered frequently off the free electrons As universe expands it cools — eventually not enough energy to keep the protons and electrons apart — they History of the Universe: superluminal inflation, particle plasma, -
Coryn Bailer-Jones Max Planck Institute for Astronomy, Heidelberg
What will Gaia do for the disk? Coryn Bailer-Jones Max Planck Institute for Astronomy, Heidelberg IAU Symposium 254, Copenhagen June 2008 Acknowledgements: DPAC, ESA, Astrium 1 Gaia in a nutshell • high accuracy astrometry (parallaxes, proper motions) • radial velocities, optical spectrophotometry • 5D (some 6D) phase space survey • all sky survey to G=20 (1 billion objects) • formation, structure and evolution of the Galaxy • ESA mission for launch in late 2011 2 Gaia capabilities Hipparcos Gaia Magnitude limit 12.4 G = 20.0 No. sources 120 000 1 000 000 000 quasars 0 1 million galaxies 0 10 million Astrometric accuracy ~ 1000 μas 12-25 μas at G=15 100-300 μas at G=20 Photometry 2 bands spectra 330-1000 nm Radial velocities none 1-10 km/s to G=17 Target selection input catalogue real-time onboard selection 3 How the accuracy varies • astrometric errors dominated by photon statistics • parallax error: σ(ϖ) ~ 1/√flux ~ distance, d for fixed MV • fractional parallax error: σ(ϖ)/ϖ ~ d2 • fractional distance error: fde ~ d2 • transverse velocity accuracy: σ(v) ~ d2 • Example accuracy • K giant at 6 kpc (G=15): fde = 2%, σ(v) = 1 km/s • G dwarf at 2 kpc (G=16.5): fde = 8%, σ(v) = 0.4 km/s 4 Distance statistics 8kpc At larger distances may use spectroscopic parallaxes 100 000 stars with fde <0.1% 11 million stars with fde <1% panther-observatory.com NGC4565 from Image: 150 million stars with fde <10% 5 Payload overview 6 Instruments 7 Radial velocity spectrograph • R=11 500 • CaII triplet (848-874 nm) • more detailed APE for V < 14 (still millions of stars) 8 Spectrophotometry Figure: Anthony Brown Anthony Figure: Dispersion: 7-15 nm/pixel (red), 4-32 nm/pixel (blue) 9 Stellar parameters • Infer via pattern recognition (e.g. -
Interferometric Orbits of New Hipparcos Binaries
Interferometric orbits of new Hipparcos binaries I.I. Balega1, Y.Y. Balega2, K.-H. Hofmann3, E.V. Malogolovets4, D. Schertl5, Z.U. Shkhagosheva6 and G. Weigelt7 1 Special Astrophysical Observatory, Russian Academy of Sciences [email protected] 2 Special Astrophysical Observatory, Russian Academy of Sciences [email protected] 3 Max-Planck-Institut fur¨ Radioastronomie [email protected] 4 Special Astrophysical Observatory, Russian Academy of Sciences [email protected] 5 Max-Planck-Institut fur¨ Radioastronomie [email protected] 6 Special Astrophysical Observatory, Russian Academy of Sciences [email protected] 7 Max-Planck-Institut fur¨ Radioastronomie [email protected] Summary. First orbits are derived for 12 new Hipparcos binary systems based on the precise speckle interferometric measurements of the relative positions of the components. The orbital periods of the pairs are between 5.9 and 29.0 yrs. Magnitude differences obtained from differential speckle photometry allow us to estimate the absolute magnitudes and spectral types of individual stars and to compare their position on the mass-magnitude diagram with the theoretical curves. The spectral types of the new orbiting pairs range from late F to early M. Their mass-sums are determined with a relative accuracy of 10-30%. The mass errors are completely defined by the errors of Hipparcos parallaxes. 1 Introduction Stellar masses can be derived only from the detailed studies of the orbital motion in binary systems. To test the models of stellar structure and evolution, stellar masses must be determined with ≈ 2% accuracy. Until very recently, accurate masses were available only for double-lined, detached eclipsing binaries [1]. -
Herschel, Planck to Look Deep Into Cosmos
Jet APRIL Propulsion 2009 Laboratory VOLUME 39 NUMBER 4 Herschel, Planck to look In a cleanroom at Centre Spatial Guy- deep into anais, Kourou, French Guyana, the Herschel spacecraft is raised cosmos from its transport con- tainer to begin launch Thanks in large part to the preparations. contributions of instruments By Mark Whalen and technologies developed by JPL, long-range views of the universe are about to become much clearer. European European Space Agency When the European Space Agency’s Herschel and wavelengths, continuing to move further into the far like the Hubble Space Telescope and ground-based Planck missions take to the sky together, onboard will infrared. There’s overlap with Spitzer, but Herschel telescopes to view galaxies in the billions, and millions be JPL’s legacy in cosmology studies. extends the range: Spitzer’s wavelength range is 3.5 to more with spectroscopy. In comparison, in the far infra- The pair are scheduled for launch together aboard an 160 microns; Herschel will go from 65 to 672 microns. red we have maybe a few hundred pictures of galaxies Ariane 5 rocket from Kourou, French Guyana on April Herschel’s mirror is much bigger than Spitzer’s and its that emit primarily in the far-infrared, but we know they 29. Once in orbit, Herschel and Planck will be sent angular resolution at the same wavelength will be sub- are important in a cosmological sense, and just the tip on separate trajectories to the second Lagrange point stantially better. of the iceberg. With Herschel, we will see hundreds of (L2), outside the orbit of the moon, to maintain an ap- “Herschel is really critical for studying important pro- thousands of galaxies, detected right at the peak of the proximately constant distance of 1.5 million kilometers cesses like how stars are formed,” said Paul Goldsmith, wavelengths they emit.” (900,000 miles) from Earth, in the opposite direction NASA Herschel project scientist and chief technologist A large fraction of the time with Herschel will be than the sun from Earth. -
Epo in a Multinational Context
→EPO IN A MULTINATIONAL CONTEXT Heidelberg, June 2013 ESA FACTS AND FIGURES • Over 40 years of experience • 20 Member States • Six establishments in Europe, about 2200 staff • 4 billion Euro budget (2013) • Over 70 satellites designed, tested and operated in flight • 17 scientific satellites in operation • Six types of launcher developed • Celebrated the 200th launch of Ariane in February 2011 2 ACTIVITIES ESA is one of the few space agencies in the world to combine responsibility in nearly all areas of space activity. • Space science • Navigation • Human spaceflight • Telecommunications • Exploration • Technology • Earth observation • Operations • Launchers 3 →SCIENCE & ROBOTIC EXPLORATION TODAY’S SCIENCE MISSIONS (1) • XMM-Newton (1999– ) X-ray telescope • Cluster (2000– ) four spacecraft studying the solar wind • Integral (2002– ) observing objects in gamma and X-rays • Hubble (1990– ) orbiting observatory for ultraviolet, visible and infrared astronomy (with NASA) • SOHO (1995– ) studying our Sun and its environment (with NASA) 5 TODAY’S SCIENCE MISSIONS (2) • Mars Express (2003– ) studying Mars, its moons and atmosphere from orbit • Rosetta (2004– ) the first long-term mission to study and land on a comet • Venus Express (2005– ) studying Venus and its atmosphere from orbit • Herschel (2009– ) far-infrared and submillimetre wavelength observatory • Planck (2009– ) studying relic radiation from the Big Bang 6 UPCOMING MISSIONS (1) • Gaia (2013) mapping a thousand million stars in our galaxy • LISA Pathfinder (2015) testing technologies -
Michael Perryman
Michael Perryman Cavendish Laboratory, Cambridge (1977−79) European Space Agency, NL (1980−2009) (Hipparcos 1981−1997; Gaia 1995−2009) [Leiden University, NL,1993−2009] Max-Planck Institute for Astronomy & Heidelberg University (2010) Visiting Professor: University of Bristol (2011−12) University College Dublin (2012−13) Lecture program 1. Space Astrometry 1/3: History, rationale, and Hipparcos 2. Space Astrometry 2/3: Hipparcos science results (Tue 5 Nov) 3. Space Astrometry 3/3: Gaia (Thu 7 Nov) 4. Exoplanets: prospects for Gaia (Thu 14 Nov) 5. Some aspects of optical photon detection (Tue 19 Nov) M83 (David Malin) Hipparcos Text Our Sun Gaia Parallax measurement principle… Problematic from Earth: Sun (1) obtaining absolute parallaxes from relative measurements Earth (2) complicated by atmosphere [+ thermal/gravitational flexure] (3) no all-sky visibility Some history: the first 2000 years • 200 BC (ancient Greeks): • size and distance of Sun and Moon; motion of the planets • 900–1200: developing Islamic culture • 1500–1700: resurgence of scientific enquiry: • Earth moves around the Sun (Copernicus), better observations (Tycho) • motion of the planets (Kepler); laws of gravity and motion (Newton) • navigation at sea; understanding the Earth’s motion through space • 1718: Edmond Halley • first to measure the movement of the stars through space • 1725: James Bradley measured stellar aberration • Earth’s motion; finite speed of light; immensity of stellar distances • 1783: Herschel inferred Sun’s motion through space • 1838–39: Bessell/Henderson/Struve -
Arxiv:2008.02789V1 [Astro-Ph.EP] 6 Aug 2020 Common Planet Size; and Compact Multiple Planet Sys- Tems
Draft version August 7, 2020 Typeset using LATEX twocolumn style in AASTeX63 LOW ALBEDO SURFACES OF LAVA WORLDS Zahra Essack ,1, 2 Sara Seager ,1, 3, 4 and Mihkel Pajusalu 1, 5 1Department of Earth, Atmospheric and Planetary Sciences, Massachusetts Institute of Technology, Cambridge, MA 02139, USA 2Kavli Institute for Astrophysics and Space Research, Massachusetts Institute of Technology, Cambridge, MA 02139, USA 3Department of Physics, and Kavli Institute for Astrophysics and Space Research, Massachusetts Institute of Technology, Cambridge, MA 02139, USA 4Department of Aeronautics and Astronautics, MIT, 77 Massachusetts Avenue, Cambridge, MA 02139, USA 5Tartu Observatory, University of Tartu, Observatooriumi 1, 61602 Toravere, Estonia (Accepted June 12, 2020) Submitted to ApJ ABSTRACT Hot super Earths are exoplanets with short orbital periods (< 10 days), heated by their host stars to temperatures high enough for their rocky surfaces to become molten. A few hot super Earths exhibit high geometric albedos (> 0.4) in the Kepler band (420-900 nm). We are motivated to determine whether reflection from molten lava and quenched glasses (a product of rapidly cooled lava) on the surfaces of hot super Earths contributes to the observationally inferred high geometric albedos. We experimentally measure reflection from rough and smooth textured quenched glasses of both basalt and feldspar melts. For lava reflectance values, we use specular reflectance values of molten silicates from non-crystalline solids literature. Integrating the empirical glass reflectance function and non-crystalline solids reflectance values over the dayside surface of the exoplanet at secondary eclipse yields an upper limit for the albedo of a lava-quenched glass planet surface of ∼0.1. -
ARIEL Payload Design Description
Doc Ref: ARIEL-RAL-PL-DD-001 ARIEL Payload ARIEL Payload Design Issue: 2.0 Consortium Description Date: 15 February 2017 ARIEL Consortium Phase A Payload Study ARIEL Payload Design Description ARIEL-RAL-PL-DD-001 Issue 2.0 Prepared by: Date: Paul Eccleston (RAL Space) Consortium Project Manager Reviewed by: Date: Kevin Middleton (RAL Space) Payload Systems Engineer Approved & Date: Released by: Giovanna Tinetti (UCL) Consortium PI Page i Doc Ref: ARIEL-RAL-PL-DD-001 ARIEL Payload ARIEL Payload Design Issue: 2.0 Consortium Description Date: 15 February 2017 DOCUMENT CHANGE DETAILS Issue Date Page Description Of Change Comment 0.1 09/05/16 All New document draft created. Document structure and headings defined to request input from consortium. 0.2 24/05/16 All Added input information from consortium as received. 0.3 27/05/16 All Added further input received up to this date from consortium, addition of general architecture and background section in part 4. 0.4 30/05/16 All Further iteration of inputs from consortium and addition of section 3 on science case and driving requirements. 0.5 31/05/16 All Completed all additional sections except 1 (Exec Summary) and 8 (Active Cooler), further updates and iterations from consortium including updated science section. Added new mass budget and data rate tables. 0.6 01/06/16 All Updates from consortium review of final document and addition of section 8 on active cooler (except input on turbo-brayton alternative). Updated mass and power budget table entries for cooler based on latest modelling. 0.7 02/06/16 All Updated figure and table numbering following check. -
The Atmospheric Remote-Sensing Infrared Exoplanet Large-Survey
ariel The Atmospheric Remote-Sensing Infrared Exoplanet Large-survey Towards an H-R Diagram for Planets A Candidate for the ESA M4 Mission TABLE OF CONTENTS 1 Executive Summary ....................................................................................................... 1 2 Science Case ................................................................................................................ 3 2.1 The ARIEL Mission as Part of Cosmic Vision .................................................................... 3 2.1.1 Background: highlights & limits of current knowledge of planets ....................................... 3 2.1.2 The way forward: the chemical composition of a large sample of planets .............................. 4 2.1.3 Current observations of exo-atmospheres: strengths & pitfalls .......................................... 4 2.1.4 The way forward: ARIEL ....................................................................................... 5 2.2 Key Science Questions Addressed by Ariel ....................................................................... 6 2.3 Key Q&A about Ariel ................................................................................................. 6 2.4 Assumptions Needed to Achieve the Science Objectives ..................................................... 10 2.4.1 How do we observe exo-atmospheres? ..................................................................... 10 2.4.2 Targets available for ARIEL .................................................................................. -
Herschel Space Observatory-An ESA Facility for Far-Infrared And
Astronomy & Astrophysics manuscript no. 14759glp c ESO 2018 October 22, 2018 Letter to the Editor Herschel Space Observatory? An ESA facility for far-infrared and submillimetre astronomy G.L. Pilbratt1;??, J.R. Riedinger2;???, T. Passvogel3, G. Crone3, D. Doyle3, U. Gageur3, A.M. Heras1, C. Jewell3, L. Metcalfe4, S. Ott2, and M. Schmidt5 1 ESA Research and Scientific Support Department, ESTEC/SRE-SA, Keplerlaan 1, NL-2201 AZ Noordwijk, The Netherlands e-mail: [email protected] 2 ESA Science Operations Department, ESTEC/SRE-OA, Keplerlaan 1, NL-2201 AZ Noordwijk, The Netherlands 3 ESA Scientific Projects Department, ESTEC/SRE-P, Keplerlaan 1, NL-2201 AZ Noordwijk, The Netherlands 4 ESA Science Operations Department, ESAC/SRE-OA, P.O. Box 78, E-28691 Villanueva de la Canada,˜ Madrid, Spain 5 ESA Mission Operations Department, ESOC/OPS-OAH, Robert-Bosch-Strasse 5, D-64293 Darmstadt, Germany Received 9 April 2010; accepted 10 May 2010 ABSTRACT Herschel was launched on 14 May 2009, and is now an operational ESA space observatory offering unprecedented observational capabilities in the far-infrared and submillimetre spectral range 55−671 µm. Herschel carries a 3.5 metre diameter passively cooled Cassegrain telescope, which is the largest of its kind and utilises a novel silicon carbide technology. The science payload comprises three instruments: two direct detection cameras/medium resolution spectrometers, PACS and SPIRE, and a very high-resolution heterodyne spectrometer, HIFI, whose focal plane units are housed inside a superfluid helium cryostat. Herschel is an observatory facility operated in partnership among ESA, the instrument consortia, and NASA. The mission lifetime is determined by the cryostat hold time. -
Part 1: the 1.7 and 3.9 Earth Radii Rule
Hi this is Steve Nerlich from Cheap Astronomy www.cheapastro.com and this is What are exoplanets made of? Part 1: The 1.7 and 3.9 earth Radii rule. As of August 2016, the current count of confirmed exoplanets is up around 3,400 in 2,617 systems – with 590 of those systems confirmed to be multiplanet systems. And the latest thinking is that if you want to understand what exoplanets are made of you need to appreciate the physical limits of planet-hood, which are defined by the boundaries of 1.7 and 3.9 Earth radii . Consider that the make-up of an exoplanet is largely determined by the elemental make up of its protoplanetary disk. While most material in the Universe is hydrogen and helium – these are both tenuous gases. In order to generate enough gravity to hang on to them, you need a lot of mass to start with. So, if you’re Earth, or anything up to 1.7 times the radius of Earth – you’ve got no hope of hanging onto more than a few traces of elemental hydrogen and helium. Indeed, any exoplanet that’s less than 1.7 Earth radii has to be primarily composed of non-volatiles – that is, things that don’t evaporate or blow away easily – to have any chance of gravitationally holding together. A non-volatile exoplanet might be made of rock – which for our Solar System is a primarily silicon/oxygen based mineral matrix, but as we’ll hear, small sub-1.7 Earth radii exoplanets could be made of a whole range of other non-volatile materials. -
ARIEL Payload Design Overview
ARIEL Open Science Conference ARIEL Payload DesiGn Overview Paul Eccleston ARIEL Mission Consortium ManaGer Chief EnGineer – RAL Space – UKRI STFC 14th January 2020 ARIEL Science, Mission & Community 2020 Conference, ESA - ESTEC 1 Introduction • Overview of current baseline desiGn of payload: – System architecture – Telescope system – ARIEL InfraRed Spectrometer (AIRS) – FGS / NIRSpec – Thermal, Mechanical & Electronics overall concepts and performance – Ground Support equipment and calibration planninG • ManaGement and ProGrammatic Considerations 14th January 2020 ARIEL Science, Mission & Community 2020 Conference, ESA - ESTEC 2 Key PayloaD Performance Requirements • > 0.6m2 collecting area telescope, high throughput • Diffraction limiteD performance beyonD 3 microns; minimal FoV required • Observing efficiency of > 85% • Brightest Target: Kmag = 3.25 (HD219134) • Faintest target: Kmag = 8.8 (GJ1214) • Photon noise dominated including jitter • Temporal resolution of 90 seconDs (goal 1s for phot. channels) • Average observation time = 7.7 hours, separateD by 70° on sky from next target • Continuous spectral coverage between bands 14th January 2020 ARIEL Science, Mission & Community 2020 Conference, ESA - ESTEC 3 Evolution of PayloaD Design Phase A / B1 Design Work 14th January 2020 ARIEL Science, Mission & Community 2020 Conference, ESA - ESTEC 4 Overview of Payload Module - Front Common Optical Bench Telescope Assembly Telescope Assembly M1 Baffle Tube Metering Structure Cooler Pipework Telescope Assembly interface M2 Baffle Plate Spacecraft