WFIRST & Euclid Jason Rhodes NASA Jet Propulsion Laboratory California Institute of Technology Copyright 2011 California Institute of Technology. Government.

Slides:



Advertisements
Similar presentations
EUCLID : From Dark Energy to Earth mass planets and beyond Jean-Philippe Beaulieu Institut dAstrophysique de Paris Dave Bennett University of Notre Dame.
Advertisements

JDEM Update 1 Richard Griffiths (NASA HQ) JDEM Program Scientist Neil Gehrels (NASA GSFC) JDEM Project Scientist February 3, 2010.
General Astrophysics with TPF-C David Spergel Princeton.
Slide 1 11 Oct 2008 Dark Energy - Leopoldina Munich Euclid A Space Mission to Map the Dark Universe R. Laureijs (ESA), A. Refregier (CEA), A. Cimatti (Univ.
TIGER The TIGER Instrument Overview Phil Hinz - PI July 13, 2010.
R. Pain9/18/2008 LSST-SNAP complementarity Reynald Pain IN2P3/LPNHE Paris, France Page 1.
July 7, 2008SLAC Annual Program ReviewPage 1 Future Dark Energy Surveys R. Wechsler Assistant Professor KIPAC.
The Gravitational Microlensing Planet Search Technique from Space David Bennett & Sun Hong Rhie (University of Notre Dame) Gravitational Lensing Time Series.
KDUST Supernova Cosmology
Ge/Ay133 What (exo)-planetary science can be done with microlensing?
The SNAP Project at SLAC Phil Marshall SLAC/KIPAC Slide 1.
The Galactic Exoplanet Survey Telescope (GEST) D. Bennett (Notre Dame), J. Bally (Colorado), I. Bond (Auckland), E. Cheng (GSFC), K. Cook (LLNL), D. Deming,
PLAnetary Transits and Oscillations of stars Thierry Appourchaux for the PLATO Consortium
Detection of Terrestrial Extra-Solar Planets via Gravitational Microlensing David Bennett University of Notre Dame.
Synergies with multi-wavelength surveys Matt Jarvis University of Hertfordshire.
X-ray Optical microwave Cosmology at KIPAC. The Survey 5000 square degrees (overlap with SPT and VISTA) Five-band (grizY) + VISTA (JHK) photometry to.
Progress on Cosmology Sarah Bridle University College London.
Review for Exam 3.
Black holes: do they exist?
DRM1 & Exoplanet Microlensing David Bennett University of Notre Dame.
P olarized R adiation I maging and S pectroscopy M ission Probing cosmic structures and radiation with the ultimate polarimetric spectro-imaging of the.
NAOKI YASUDA, MAMORU DOI (UTOKYO), AND TOMOKI MOROKUMA (NAOJ) SN Survey with HSC.
Eric V. Linder (arXiv: v1). Contents I. Introduction II. Measuring time delay distances III. Optimizing Spectroscopic followup IV. Influence.
Quotes from NWNH 2/3/ Two complementary approaches to understanding dark energy have been considered by this survey: one on the ground and the.
Searches for exoplanets
1 The Precision Radial Velocity Spectrometer Science Case.
PHYSPAG JANUARY 2015 DARK ENERGY UPDATE RACHEL BEAN (CORNELL UNIVERSITY) Image Credit: NASA/GSFC Image Credit: ESA 1.
20 Nov Jean-Paul KNEIB - prospective spatial PNG 1 A wide field imager for dark energy … and more ! SNAP-L Jean-Paul KNEIB LAM, Marseille, France.
The Wide Field Infrared Survey Telescope (WFIRST) James Green and Paul Schechter Co-Chairs of the Science Definition Team Neil Gehrels: Project study scientist.
A Short Talk on… Gravitational Lensing Presented by: Anthony L, James J, and Vince V.
Lecture Outlines Astronomy Today 8th Edition Chaisson/McMillan © 2014 Pearson Education, Inc. Chapter 25.
A Search for Earth-size Planets Borucki – Page 1 Roger Hunter (Ames Research Center) & Kepler Team March 26, 2010.
Observational test of modified gravity models with future imaging surveys Kazuhiro Yamamoto (Hiroshima U.) Edinburgh Oct K.Y. , Bassett, Nichol,
JDEM-Omega Overview Neil Gehrels, WFIRST Project Scientist February 3, /3/
Jenam 2010 Exoplanet Targets for Upcoming Cosmic Visions Space Missions James Frith September 8 th 2010 University of Hertfordshire.
Dark Energy Probes with DES (focus on cosmology) Seokcheon Lee (KIAS) Feb Section : Survey Science III.
1 System wide optimization for dark energy science: DESC-LSST collaborations Tony Tyson LSST Dark Energy Science Collaboration meeting June 12-13, 2012.
WFIRST-AFTA Mission Science Alan Dressler, AAS Seattle, January 7, /30/2014WFIRST-AFTA SDT Report 1.
DARK ENERGY IN SPACE: WFIRST AND EUCLID RACHEL BEAN (CORNELL UNIVERSITY) ON BEHALF OF THE PHYSPAG DARK ENERGY COMMUNITY Image Credit: NASA/GSFC Image Credit:
Weak Lensing from Space with SNAP Alexandre Refregier (IoA) Richard Ellis (Caltech) David Bacon (IoA) Richard Massey (IoA) Gary Bernstein (Michigan) Tim.
Surveying the Universe with SNAP Tim McKay University of Michigan Department of Physics Seattle AAS Meeting: 1/03 For the SNAP collaboration.
The WFIRST Microlensing Exoplanet Survey: Figure of Merit David Bennett University of Notre Dame WFIRST.
Michael Levi (Lawrence Berkeley National Laboratory), M. Lampton (UCBerkeley Space Sciences Lab), and M. Sholl (UCBerkeley Space Sciences Lab) WFIRST:
A. Ealet, S. Escoffier, D. Fouchez, F. Henry-Couannier, S. Kermiche, C. Tao, A. Tilquin September 2012.
G. Miknaitis SC2006, Tampa, FL Observational Cosmology at Fermilab: Sloan Digital Sky Survey Dark Energy Survey SNAP Gajus Miknaitis EAG, Fermilab.
The Future of the Hubble Space Telescope Steven Beckwith April 25, 2005 Space Telescope Science Institute.
SNAP Calibration Program Steps to Spectrophotometric Calibration The SNAP (Supernova / Acceleration Probe) mission’s primary science.
1. Exoplanet detection (500+) 2 Gravitational attraction between a stellar mass (sun) and planets (bigger the better, why?) makes sun’s position wobble.
NRO Telescopes David Spergel. History meter telescopes meter mirror “Residual space hardware” from Future Imagery Architecture, failed program.
Astrophysics Missions in ESA’s Cosmic Vision Program
The Instrument The focal plane is like an HEP detector, larger than any present astronomical camera, but smaller than a vertex detector. ½ Billion pixels.
Future observational prospects for dark energy Roberto Trotta Oxford Astrophysics & Royal Astronomical Society.
ISWG - December 7, Destiny, The Dark Energy Space Telescope.
FIRST LIGHT A selection of future facilities relevant to the formation and evolution of galaxies Wavelength Sensitivity Spatial resolution.
Brenna Flaugher for the DES Collaboration; DPF Meeting August 27, 2004 Riverside,CA Fermilab, U Illinois, U Chicago, LBNL, CTIO/NOAO 1 Dark Energy and.
The Search for Another Earth Exoplanets and the Kepler Spacecraft.
Probing Dark Energy with Cosmological Observations Fan, Zuhui ( 范祖辉 ) Dept. of Astronomy Peking University.
Astronomy 3040 Astrobiology Spring_2016 Day-7. Homework -1 Due Monday, Feb. 8 Chapter 2: 1, 3, 16 23, 24, 26 29, 30, , 54, 56 The appendices will.
Chapter 25 Galaxies and Dark Matter. 25.1Dark Matter in the Universe 25.2Galaxy Collisions 25.3Galaxy Formation and Evolution 25.4Black Holes in Galaxies.
NIRSS: the Near-Infrared Sky Surveyor WFIRST Meeting 2011 February 3 Daniel Stern (JPL/Caltech)
The Euclid Mission Jason Rhodes (Caltech/JPL) March 7, 2013 © 2013, government sponsorship acknowledged.
NIR, MIR, & FIR.  Near-infrared observations have been made from ground based observatories since the 1960's  Mid and far-infrared observations can.
Jochen Weller Decrypting the Universe Edinburgh, October, 2007 未来 の 暗 黒 エネルギー 実 験 の 相補性.
Next Generation Data Sets: An Overview of CMB-S4 and WFIRST David Spergel Princeton University Center for Computational Astrophysics, Flatiron Institute.
Euclid Big Data Opportunities Tom Kitching (UCL MSSL) – Euclid Science Lead.
PLANCK TEAM of the DISCOVERY Center. The most mysterious problems.
NEW Telescope Meeting , Princeton
What (exo)-planetary science can be done with microlensing?
Observational Prospect of NIREBL
CHEOPS - CHaracterizing ExOPlanet Satellite
Presentation transcript:

WFIRST & Euclid Jason Rhodes NASA Jet Propulsion Laboratory California Institute of Technology Copyright 2011 California Institute of Technology. Government sponsorship acknowledged.

Overview Fundamental Scientific Questions Dark Matter and Energy The abundance of Earth-like planets The Evolution of Galaxies & Near Infrared Survey Science The Missions: Euclid- ESA Cosmic Visions Wide Field Infrared Survey Telescope - NASA

Dark Energy 73% 23% Dark Matter H, He Gas 4% Stars 0.4% Neutrinos 0.3% The Components of the Universe All of chemistry, biology, physics…

The Next Piece of the Pie What is that stuff???? One of the most compelling and important questions in science!

Are We Alone? The search for planets is fundamental to the search for alien life Multiple techniques exist for finding planets Gravitational microlensing allows a statistical census for planets near the “interesting” region: We want to find Earth- like planets in the habitable zone µl

Microlensing of Stars When the path of a foreground star crosses near a background star, its gravity bends and focuses the light from the background star. The background star is the ‘source’, and the foreground star is the ‘lens’. The result is a time- dependent magnification of the light we receive from the ‘source’ star.

Stellar and exoplanetary microlensing Typical time scale for a stellar event is 1 to 2 months. If the ’lens’ star has a planet, its gravity may also contribute to lensing the light from the ’source’. This produces a secondary peak in the light curve. Typical exoplanetary deviation lasts only hours to days.

Exoplanet microlensing

Exoplanet surveys Exoplanetary microlensing is a low probability phenomenon. In order to monitor many potential events, we need —A Wide-field survey —Pointed at a region that is dense in stars, e.g. the galactic bulge High-cadence continuous sampling IR telescope, because —Can see farther through dust, and —Most stars are M stars, which strongly radiate in the IR Typical ‘Source’ star is a giant or dwarf in the bulge. Typical ‘Lens’ star is a red main- sequence star in the foreground disk or bulge

The Missions

Euclid Mapping the geometry of the Dark Universe 2004: Dark Universe Mission proposed as a Theme to ESA’s Cosmic Vision programme Oct 2007: DUNE and SPACE jointly selected for an ESA Assessment Phase April 2010: Formation of single Euclid Consortium : Definition phase July 2011: Final Euclid Proposal- Red Book Oct : Cosmic Vision Selection of Euclid : Implementation phase 2019: launch

Euclid goals Understand the nature of Dark Energy and Dark Matter by: Measuring the DE equation of state parameters w 0 and w a to a precision of 2% and 10%, respectively, using both expansion history and structure growth. Measuring the growth factor exponent γ with a precision of 2%, enabling to distinguish General Relativity from the modified-gravity theories Testing the Cold Dark Matter paradigm for structure formation, and measure the sum of the neutrino masses to a precision better than 0.04eV when combined with Planck. Improving by a factor of 20 the determination of the initial condition parameters compared to Planck alone.

Euclid concept Optimized for two complementary cosmological probes: —Weak Gravitational Lensing —Baryonic Acoustic Oscillations Additional probes: clusters, redshift space distortions, ISW 15,000 square degree survey —Imaging (WL): High precision imaging at visible wavelengths Photometry/Imaging in the near-infrared —Near Infrared Spectroscopy (BAO) No SN, exoplanet microlensing for now

Euclid Mission Baseline Mission elements: L2 Orbit 5-6 year mission Telescope: three mirror astigmat (TMA) with 1.2 m primary Instruments: –VIS: Visible imaging channel: 0.5 deg 2, 0.10’’ pixels, 0.16’’ PSF FWHM, broad band R+I+Z ( mu), 36 CCD detectors, galaxy shapes –NISP: NIR channel: 0.5 deg 2, 16 HgCdTe detectors, 1-2mu: Photometry: 0.3’’ pixels, 3 bands Y,J,H, photo-z’s Spectroscopy: slitless, R=500, redshifts

Impact on Cosmology f = dln  m /dlna   m  w(a)=w p +w a (a p -a) Primary: Five year survey with weak lensing and galaxy clustering from 15,000 deg 2 of optical/NIR imaging and slitless spectroscopy (RIZ > 24.5, YJH > 24) and DES/PS2 ground-based data All: Including RSD, ISW and clusters from same survey data FoM=1/(dw p dw a )

WFIRST Wide Field Infrared Survey Telescope Dark energy and modified gravity Microlensing searches for exoplanets Near infrared survey for galaxy formation and evolution

WFIRST = JDEM-Ω MPFNIRSS ++

WFIRST History and Philosophy Decadal Survey Astro2010 top large space recommendation: do WFIRST to accomplish as many of the JDEM, NIRSS, and MPF goals as possible Several high-priority science areas required similar hardware Near infrared (500nm -2+ micron) detectors w ~100Mpix meter mirror Stable platform in space Current design has imaging and spectroscopy up to 2 microns on a 1.3m telescope

WFIRST – Science Objectives 1) Complete the statistical census of planetary systems in the Galaxy, from habitable Earth-mass planets to free floating planets, including analogs to all of the planets in our Solar System except Mercury. 2) Determine the expansion history of the Universe and its growth of structure in order to test explanations of its apparent accelerating expansion including Dark Energy and possible modifications to Einstein's gravity. 3) Produce a deep map of the sky at NIR wavelengths, enabling new and fundamental discoveries ranging from mapping the Galactic plane to probing the reionization epoch by finding bright quasars at z>10.

WFIRST Status Science Definition Team has delivered interim report and associated design reference mission Must be sold to OMB (Congress) and the OSTP (President) Negotiations with ESA will likely take place after Euclid downselect Could start an 84 month development and implementation cycle as soon as 2013 (funding permitting) Earth-Sun L2 orbit, 5 year lifetime, 10 year goal 1.3 m unobstructed telescope NIR instrument with ~36 HgCdTe detectors

WFIRST – A Survey Telescope Approximate HST/JWST field of view. These telescopes cannot do WFIRST wide surveys. imaging spectroscopy Off-axis design gives high throughput and excellent point spread function WFIRST Focal plane design

Planet detection to 0.1 Earth mass (M Earth ) Detects  30 free floating planets of 1 M Earth in a 500 day survey* Detects  125 planets of M Earth (in 2 year orbits) in a 500 day survey* Detects  25 habitable zone† planets (0.5 to 10 M Earth ) in a 500 day survey * * Assuming one such planet per star; “500 day surveys” are concurrent † AU, scaling with the square root of host star luminosity Exoplanet Microlensing Survey Capability 22 Data Set Rqts include: Observe  2 square degrees in the Galactic Bulge at ≤ 15 minute sampling cadence; Minimum continuous monitoring time span: ~60 days; Separation of ≥4 years between first and last observing seasons.

BAO/RSD:... “WIDE” survey mode - 11,000 deg 2 /dedicated year - Redshift errors σ z ≤ 0.001(1+z), over redshift range 0.7 ≤ z ≤ 2 Weak Lensing:... “DEEP” survey mode deg 2 /dedicated year - Effective galaxy density  30/amin 2, shapes resolved plus photo-zs SNe-Ia Survey: - >100 SN per  z= 0.1 bin for most bins 0.4 < z < 1.2, per dedicated 6 months - Redshift error σ z ≤ per supernova Dark Energy Survey Capabilities

Comparison WFIRST IDRMEuclid Aperture1.3m unobstructed (equivalent to 1.5m obstructed) 1.2 m obstructed Wavelength range760nm-2μm500nm-2μm Pixel size018’’ NIR imaging 0.45’’ NIR spectro 0.1” optical imaging 0.3” NIR imaging and spectro Science goalsDE and modified gravity, exoplanet microlensing, IR surveys DE and modified gravity, dark matter Lifetime5 years primary, 10 years goal5.5-6 years primary Instruments 1.NIR imaging instrument with filter wheel (0.29 deg 2 ) and prism 2.2 NIR spectrographs (0.26 deg 2 ) 1.Optical imager (VIS) with fixed filter(s) (0.5 deg 2 ) 2.NIR instrument (NISP) with filter wheel and grism (0.5 deg 2 ) More info?