Venus Transit of 2012 Observed by the Helioseismic and Magnetic Imager (HMI) on board the Solar Dynamics Observatory (SDO)

Similar documents
Side Note on HMI Distortion

arxiv: v1 [astro-ph.sr] 8 Jun 2016

Observables Processing for the Helioseismic and Magnetic Imager Instrument on the Solar Dynamics Observatory

Observables Processing for the Helioseismic and Magnetic Imager Instrument Onboard the Solar Dynamics Observatory

Observables Processing for the Helioseismic and Magnetic Imager Instrument on the Solar Dynamics Observatory

Alain Hauchecorne, Mustapha Meftah, Abdanour Irbah, Sebastien Couvidat, Rock Bush, Jean-François Hochedez. To cite this version:

Line-of-sight observables algorithms for HMI tested with Interferometric BI-dimensional Spectrometer (IBIS) spectro-polarimetric observations

Calculation of Observables from HMI Data (REVISED ON JULY 15, 2011)

4+ YEARS OF SCIENTIFIC RESULTS WITH SDO/HMI

Received: 21 September 2011 / Accepted: 19 March 2012 / Published online: 6 April 2012 Springer Science+Business Media B.V. 2012

arxiv: v2 [astro-ph.sr] 22 Sep 2014

HMI multi height Dopplergram study

Acoustic Power Absorption in Sunspots and Quiet-Sun from Hankel-Fourier Transform on HMI and AIA Data. Sébastien Couvidat, 04/13/2012

Helioseismic and Magnetic Imager Calibration Status

Interpreting HMI multi-height velocity measurements Kaori Nagashima

Application of Precision Deformable Mirrors to Space Astronomy

Extraction of Point Source Spectra from STIS Long Slit Data

Observation of Chromospheric Sunspot at. Millimeter Range with the Nobeyama 45 m. Telescope

On solar radius measurements during the rising phase of solar cycle 24

Wavelength Dependence of the Helioseismic and Magnetic Imager (HMI) Instrument onboard the Solar Dynamics Observatory (SDO)

Helioseismology. Jesper Schou Max Planck Institute for Solar System Research

Instrument Calibration Plan December 13, HMI Instrument Calibration Plan

HMI Filter Calibration

Absolute calibration in solar scattering polarization measurements with ZIMPOL

arxiv: v1 [astro-ph.sr] 17 Sep 2014

SODISM-2 A ground based multi-wavelength full disk solar imager

The Solar System LEARNING TARGETS. Scientific Language. Name Test Date Hour

Venus 2012 transit: spectroscopy and high resolution observations proposals

Center-to-limb Variation of Quiet Sun Intensity Contrasts. Alex Feller

The Michelson Doppler Imager on. The Michelson Doppler Imager èhereafter referred to as MDIè is an instrument designed

The Solar System. Name Test Date Hour

The Sun as an exoplanet-host star: testbed for radial-velocity variations. Raphaëlle D. Haywood Sagan Fellow, Harvard College Observatory

Solar Observation Class Project

Sun Size. Our Galaxy. Sun Location. The Solar System The hottest chapter yet. 7 th Grade Solar System

BigBOSS Data Reduction Software

Lecture 19: The Moon & Mercury. The Moon & Mercury. The Moon & Mercury

THE TOTAL IRRADIANCE MONITOR (TIM): SCIENCE RESULTS

Astronomy. Astrophysics. Ground-based measurements of the solar diameter during the rising phase of solar cycle 24

Temperature Reconstruction from SDO:AIA Filter Images

Inner Planets (Part II)

Characterization of High-Degree Modes using MDI, HMI and GONG data

Lab 4: Differential Photometry of an Extrasolar Planetary Transit

Ground-based measurements of the solar diameter during the rising phase of solar cycle 24

Derivation of the Solar Plage Index using the Flare Monitoring Telescope at the Hida Observatory

9/13/18. ASTR 1040: Stars & Galaxies. Topics for Today and Tues. Nonvisible Light X-ray, UV, IR, Radio. SPITZER Infrared Telescope

Impressions: First Light Images from UVIT in Orbit

September 14, Monday 4. Tools for Solar Observations-II

Data Processing in DES

Transiting Hot Jupiters near the Galactic Center

Tools of Astronomy Tools of Astronomy

Designing a Space Telescope to Image Earth-like Planets

Why Go To Space? Leon Golub, SAO BACC, 27 March 2006

Keywords: Sun: radio magnetic fields Sun: chromosphere Sun: corona Sun: active regions

Space weather. Introduction to lectures by Dr John S. Reid. Image courtesy:

arxiv: v1 [astro-ph.sr] 6 Aug 2009

A Parameterization of the Chandra Point Spread Function

Photospheric and chromospheric polarimetry of solar flares

Physical Properties of Wave Motion in Inclined Magnetic Fields Within Sunspot Penumbrae

Design and Correction of optical Systems

Exam# 1 Review Gator 1 Keep the first page of the exam. Scores will be published using the exam number Chapter 0 Charting the Heavens

Physical Properties of Wave Motion in Inclined Magnetic Fields within Sunspot Penumbrae

METIS- ESA Solar Orbiter Mission: internal straylight analysis

The Law of Ellipses (Kepler s First Law): all planets orbit the sun in a

Fundamentals of Exoplanet Observing

Fundamentals of Exoplanet Observing

THE PICARD mission. Gérard Thuillier 1, Steven Dewitte 2, Werner Schmutz 3, and the PICARD team 4

a. 0.5 AU b. 5 AU c. 50 AU d.* AU e AU

Reduction procedure of long-slit optical spectra. Astrophysical observatory of Asiago

Accurate Determination of the Solar Photospheric Radius

ANALYSIS OF LIMB BRIGHTENING ON THE QUIET SUN AT 21 CM USING A THREE-ELEMENT INTERFEROMETER

Solar Orbiter. T.Appourchaux, L.Gizon and the SO / PHI team derived from M.Velli's and P.Kletzkine's presentations

Astronomy 111 Review Problems Solutions

TECH NOTE. New Mean Sea Surface for the CryoSat-2 L2 SAR Chain. Andy Ridout, CPOM, University College London

Credit: NASA/Kepler Mission/Dana Berry. Exoplanets

AIA DATA ANALYSIS OVERVIEW OF THE AIA INSTRUMENT

SCIAMACHY Level 1b-2 Data Processing Status & Changes

Recent Solar Spectral Irradiance Observations

Amateur Astronomer Participation in the TESS Exoplanet Mission

Calculating the Occurrence Rate of Earth-Like Planets from the NASA Kepler Mission

Development of a 3D-Imaging Calorimeter in LaBr 3 for Gamma-Ray Space Astronomy

Simulations for H.E.S.S.

IHEP-BINP CEPC accelerator collaboration workshop Beam energy calibration without polarization

September 9, Wednesday 3. Tools for Solar Observations-I

Using This Flip Chart

Human Understanding of both Earth and Space has Changed Over Time. Unit E: Topic One

Toward Interplanetary Space Weather: Strategies for Manned Missions to Mars

Explain how Earth's movement and the moon's orbit cause the phases of the moon. Explain the difference between a solar eclipse and a lunar eclipse.

TEKS Cluster: Space. identify and compare the physical characteristics of the Sun, Earth, and Moon

Opaque Atmosphere. Astronomy 210. Question. Why would it be useful to place telescopes in. Section 1 MWF Astronomy Building. space?

A NEW GENERATION OF GAMMA-RAY TELESCOPE

The Helioseismic and Magnetic Imager

Astronomy 114. Lecture 26: Telescopes. Martin D. Weinberg. UMass/Astronomy Department

Kanzelhöhe Observatory Flare observations and real-time detections Astrid Veronig & Werner Pötzi

What is an eclipse? Lunar Eclipses. By NASA, adapted by Newsela staff on Word Count 866 Level 940L

Science Space Lessons 1-5 Notes

The art of Stokes inversions. Luis R. Bellot Rubio Instituto de Astrofísica de Andalucía (CSIC), Spain National Astronomical Observatory, Japan

Polarization Calibration of the Helioseismic and Magnetic Imager (HMI) onboard the Solar Dynamics Observatory (SDO)

Educational Objectives Determine which variable affects the frequency of a simple pendulum.

MERIS US Workshop. Instrument Characterization Overview. Steven Delwart

NICMOS Status and Plans

Transcription:

Venus Transit of 2012 Observed by the Helioseismic and Magnetic Imager (HMI) on board the Solar Dynamics Observatory (SDO) Sébastien Couvidat and the HMI team PICARD Workshop, September 25-26, 2013

What we learned from the Venus transit of June 5-6, 2012 Rock Bush will present the HMI instrument in details tomorrow HMI images the Sun onto 4096x4096 CCDs, in Fe I line at 6173 A Cadence of 45 s on front camera: 6 wavelengths, 2 polarizations Cadence of 135 s on side camera: 6 wavelengths, 6 polarizations Previous Venus transit was in June 2004, next one is in December 2117 The transit of June 2012 proved very useful to HMI team To improve the calibration of HMI: - roll angle (satellite + instrument) -> keyword CROTA2 - plate scale -> keyword CDELT1 - Point Spread Function (PSF) To test the quality of HMI s ground calibration - instrument distortion To access science data: - measurement of the solar radius (work in collaboration with Picard team members at LATMOS: Hauchecorne, A., Irbah, A., and Meftah, M.) - measurement of linear polarization in Venus atmosphere will briefly present some of these results, starting by the measurement of the solar radius

Venus transit of June 5-6, 2012: an overview Venus radius = 57.8 pixels During transit side camera of HMI took true continuum at 4 polarizations (I+U,I-U,I+Q, and I-Q)

Credit: Data courtesy of NASA/SDO, HMI, and AIA science teams.

Solar Radius Measurement Image Processing (I) - based on Emilio, Kuhn, Bush, and Scholl (2012) - using hmi.lev1 data from side camera only: 25 min for ingress and egress - gap filling of hmi.lev1 (to correct bad pixels) - un-distortion - removing PSF (using Richardson-Lucy algorithm). PSF from A.A. Norton, T.L. Duvall, and J. Schou Front camera distortion From Wachter et al., 2012

Side note on HMI distortion - obtained from ground data (random-dot target + moving alignment legs, Wachter et al. 2012) - distortion as a function of field position is expanded into Zernike polynomials up to 23rd order - when we correct images for distortion to obtain HMI observables, we use polynomials of order 6 separately for x and y. Distortion is mostly pincushion type in upper half, and barrel type in lower half (aka mustache distortion) - elliptical distortion could be further corrected using roll data from space Front camera at best focus: Max distortion: 2 pixels Front side cameras: From Wachter et al. (2012) Max difference: 0.28 pixels

Solar radius determination: Image Processing (II) Raw image / background NB: image upside-down Undistorted + PSF removed / background - dividing each image by background images (average from 80 images prior to, and after the, transit, i.e. 5 min) - finding the limb on each image (limb finder results corrected by undistortion), and masking - thresholding and pixel counting (pixels below threshold assumed to be part of Venus) - determining times at which center of Venus crosses solar radius (NB: contact between center and radius happens when 49.6% of surface area is inside solar disk) Interpolation on fine time grid - comparing total transit time with ephemeris provided by GSFC: we determine solar radius which, based on ephemeris, returns closest transit time to observed one

Example of processed images that have been thresholded and masked

Measuring the surface area of part of Venus inside the solar disk egression ingression RESULTS: - total transit time from HMI data: 6h 8m 9s - compared to ephemeris, corresponds to average radius at 1 AU: 959.7 ± 0.2 (i.e. 145 km at least) Close to 959.86 from Meftah et al. (2013) Close to the 959.9 measured by Alain Hauchecorne (for HMI) But: result is sensitive to PSF used and removal details, to threshold used, to limb position...

HMI residual distortion along the path of Venus Comparison of Venus center locations with ephemeris locations - images are un-distorted - PSF is removed - images are divided by background image - Venus center defined as center of gravity of all pixels below given threshold Assuming the platescale is correct

Residual distortion in the x and y directions (adapted from J. Schou) To determine accurate residuals in x and y, it is necessary to also fit for plate-scale (CDELT1) and roll angle (CROTA2). Non-linear LSQ fit using Levenberg-Marquardt algorithm Residual distortion 0.1 pixel

Roll Angle of HMI Venus transit data are used to determine error on the CROTA2 keyword (satellite roll angle + instrument roll angle) Analysis from J. Schou and R. Shine based on un-distorted level 1 images Average angle error: 0.0834 Figure provided by J. Schou CROTA2 corrected in all hmi.lev1 records after 2012.08.29

Point Spread Function Several PSFs have been obtained: From Venus data - K.L. Yeo et al. -> 5 Gaussians whose amplitudes have a sinelike azimuthal dependence - A. Norton, T. L. Duvall, and J. Schou -> Airy function + Lorentzian + minor azimuthal dependence From ground data - R. Wachter et al. -> 1 Gaussian + tail described as a power drop-off From Yeo et al., submitted FWHM=0.96 or 1.9 pixels

Measurement of Linear Polarization in Venus Atmosphere (work in progress) - scattering of sunlight by Venus mesosphere expected to produce some amount of linear polarization - difficult to observe due to phase angle close to 180 + instrument defects & limb polarization - during Venus transit side camera took I+/-U and I+/-Q in continuum, at cadence of 3.75 s (horizontal linear polarization seen from the instrument is I + Q, while I + U is polarization at 45 counterclockwise from horizontal (Schou et al., 2012)) Venus observed during ingression outside solar disk. Average aureole intensity measured. Raw level 1 images Background removed, cosmic ray hit removed

Result of average linear polarization measurement 2 U/I and Q/I 2 Degree of linear polarization (U +Q )/I Average = 2.11% (background: average = 0.34% and σ=0.22%) μ=1.06% 3σ=0.75% μ=0.92% 3σ=0.72%

Conclusion - Venus transit provided HMI team unique opportunity to better know and improve calibration of instrument (roll angle, plate scale, distortion) - to measure the solar radius (collaborative work with Picard group) - to determine PSF (work in progress, papers by A.A. Norton, T.L. Duvall, J. Schou, et al. and by K.L. Yeo, A. Feller, S.K. Solanki, et al.) - to measure linear polarization in Venus atmosphere (work in progress) Hopefully we will observe the May 2016 transit of Mercury! Many thanks to Alain Hauchecorne, Abdenour Irbah, and Mustapha Meftah for the invitation to the workshop!