Imaging Analysis Aneta Siemiginowska Chandra X-ray Center Harvard-Smithsonian Center for Astrophysics.

Slides:



Advertisements
Similar presentations
X-ray Astronomy with High Spectral Resolution: Astro-E2 / ISAS Y. Tanaka.
Advertisements

X-ray Imaging Spectrometers (XIS) of Astro-E2 Hironori Matsumoto (Kyoto University) and the XIS team 1. Overview Astro-E2 is the fifth Japanese X-ray Astronomy.
X-Ray Measurements of the Mass of M87 D. Fabricant, M. Lecar, and P. Gorenstein Astrophysical Journal, 241: , 15 October 1980 Image:
Optical Astronomy Imaging Chain: Telescopes & CCDs.
Basic Principles of X-ray Source Detection Or Who Stole All Our Photons?.....
Status report on Light Simulator Claudia Cecchi Francesca Marcucci Monica Pepe Software meeting Udine January
Chandra Calibration Status ACIS 1.Gain corrections for epochs 28 and 29 (Nov – April 2007) were released in CALDB 3.4 on May 16, Gain corrections.
Chandra Calibration Status  Gain correction files for epochs 35 (Aug. – Oct. 2008) and 36 (Nov Jan.2009) were released in CALDB versions
RHESSI/GOES Observations of the Non-flaring Sun from 2002 to J. McTiernan SSL/UCB.
Chandra Calibration Status  Recent releases  Current Calibration projects  Cross-Calibration between Chandra and other X-ray telescopes  Revisions.
Growth of Structure Measurement from a Large Cluster Survey using Chandra and XMM-Newton John R. Peterson (Purdue), J. Garrett Jernigan (SSL, Berkeley),
I. Balestra, P.T., S. Ettori, P. Rosati, S. Borgani, V. Mainieri, M. Viola, C. Norman Galaxies and Structures through Cosmic Times - Venice, March 2006.
Deriving and fitting LogN-LogS distributions Andreas Zezas Harvard-Smithsonian Center for Astrophysics.
China’s Future Missions in Space High Energy Astrophysics Shuang Nan Zhang 张双南 Tsinghua University and Institute of High Energy Physics, Chinese Academy.
3C 186 A Luminous Quasar in the Center of a Strong Cooling Core Cluster at z>1 Aneta Siemiginowska CfA Tom Aldcroft (CfA) Steve Allen (Stanford) Jill Bechtold.
1 XMM-Newton Extended Source Analysis Software Steve Snowden & Kip Kuntz  Publicly Released 5 April 2006  XMM-Newton Extended Source Analysis Software.
Chandra X-Ray Observatory CXC Paul Plucinsky EPIC Cal Nov ACIS Calibration: Planned Updates & Future Issues 2.ACIS Operations: Controlling the.
An XMM-ESAS Update Steve Snowden NASA/Goddard Space Flight Center EPIC Operations and Calibration Meeting - BGWG Palermo - 11 March 2007.
Deterministic Modeling of the MOS Background Steve Snowden NASA/Goddard Space Flight Center EPIC Operations and Calibration Meeting Mallorca 1-3 February.
Source detection at Saclay Look for a fast method to find sources over the whole sky Provide list of positions, allowing to run maximum likelihood locally.
Chandra X-ray Center Martin Elvis Smithsonian Astrophysical Observatory Welcome to the 4 th Chandra – CIAO Workshop 20 – 22 May 2002.
Chandra X-Ray Observatory CXC Paul Plucinsky February A Comparison of Spectral Fit Results of E0102 from the Chandra and XMM CCDs Paul Plucinsky.
C&A 10April06 1 Point Source Detection and Localization Using the UW HealPixel database Toby Burnett University of Washington.
CXC CUC September SDS Page 1 CUC Sep 2007 Science Data Systems – Jonathan McDowell.
An X-ray Study of the Bright Supernova Remnant G with XMM-Newton SNRs and PWNe in the Chandra Era Boston, MA – July 8 th, 2009 Daniel Castro,
1 TEV PA Meeting July 2009 Preliminary Fermi-LAT Limits on High Energy Gamma Lines from WIMP Annihilation Yvonne Edmonds representing the Fermi-LAT Collaboration.
Can people meet from 2:40 to 3:30 on Tuesday, September 5?
1 XMM-Newton Extended Source Analysis Software Steve Snowden & Kip Kuntz  Publicly Released 5 April 2006  XMM-Newton Extended Source Analysis Software.
1 Arecibo Synergy with GLAST (and other gamma-ray telescopes) Frontiers of Astronomy with the World’s Largest Radio Telescope 12 September 2007 Dave Thompson.
The Hot Plasma in the Galactic Center with Suzaku Masayoshi Nobukawa, Yoshiaki Hyodo, Katsuji Koyama, Takeshi Tsuru, Hironori Matsumoto (Kyoto Univ.)
NASSP Masters 5003F - Computational Astronomy Lecture 19 EPIC background Event lists and selection The RGA Calibration quantities Exposure calculations.
10/20/2005 GLAST Lunch Seminar Deconvolution of ASCA Images1 Deconvolution of ASCA Images of Galaxy Clusters and SNRs Mutsumi Sugizaki, Tune Kamae SLAC.
14 October Observational Astronomy SPECTROSCOPY and spectrometers Kitchin, pp
SYSTEMATICS ON CHANDRA X-RAY MASS ESTIMATES Elena Rasia Dipartimento di Astronomia, Padova,Italy Lauro Moscardini Giuseppe Tormen Stefano.
The Environments of Galaxies: from Kiloparsecs to Megaparsecs August 2004 Cool Cores in Galaxy Groups Ewan O’Sullivan Harvard-Smithsonian Center for Astrophysics.
Gamma-Ray Bursts observed with INTEGRAL and XMM- Newton Sinead McGlynn School of Physics University College Dublin.
X-ray astronomy 7-11 September 2009, Bologna, Italy XMM-Newton slew survey hard band sources XMM-Newton slew survey hard band sources R.D. Saxton a, A.M.
X-rays from Mars K. Dennerl, C. Lisse, A. Bhardwaj, V. Burwitz, J. Englhauser, H. Gunell, M. Holstrom, F. Jansen, V. Kharchenko, and P. Rodriguez-Pascual.
Initial Results from the Chandra Shallow X-ray Survey in the NDWFS in Boötes S. Murray, C. Jones, W. Forman, A. Kenter, A. Vikhlinin, P. Green, D. Fabricant,
GLAST LAT Project Catalogs and Diffuse Emissions Working Groups G. Tosti et al.SLAC, May Gino Tosti, Claudia Cecchi INFN Perugia based on Francesca.
The IceCube Neutrino Observatory is a cubic kilometer detector at the geographic South Pole. We give an overview of searches for time-variable neutrino.
Main-Cluster XIS0XIS1XIS3 Weighted mean Chandra Figure 2 : XIS spectra of the main-cluster XIS keV Main-Cluster Sub-Cluster Search for Bulk Motion.
X-ray sky survey of bright, serendipitous sources with 2XMMi at the AIP Speaker: Alexander Kolodzig Origin: Humboldt-Uni Berlin, Germany Institute:AIP.
PSF in-flight calibration - PN IFC/CNRRingberg, April 2-4, 2002 PSF in-flight calibration for PN camera Simona Ghizzardi Silvano Molendi.
X-ray Astronomy School 2002 Clusters of Galaxies (and some Cosmology) Scientific and Data Analysis Issues Keith Arnaud NASA/GSFC and UMCP.
XMM slew survey Richard Saxton 1, Andy Read 2, Pili Esquej 3, Michael Freyberg 3, Bruno Altieri 1 1. ESAC 2. University of Leicester 3. MPE XMM slew survey.
C. Y. Hui & W. Becker X-Ray Studies of the Central Compact Objects in Puppis-A & RX J Max Planck Institute for Extraterrestrial Physics, Giessenbachstrasse.
MASS PROFILES OF X-RAY BRIGHT RELAXED GROUPS: METHODS AND SYSTEMATICS FABIO GASTALDELLO IASF-INAF MILANO & UC IRVINE D. BUOTE UCI P. HUMPHREY UCI L. ZAPPACOSTA.
Outline Cosmic Rays and Super-Nova Remnants
Takayasu Anada ( anada at astro.isas.jaxa.jp), Ken Ebisawa, Tadayasu Dotani, Aya Bamba (ISAS/JAXA)anada at astro.isas.jaxa.jp Gerd Puhlhofer, Stefan.
1 John Nousek & David Burrows (Penn State University) Alberto Moretti (Osservatorio Astronomico di Brera) X-Ray Telescope (XRT): Performance after Five.
RGS observations of cool gas in cluster cores Jeremy Sanders Institute of Astronomy University of Cambridge A.C. Fabian, J. Peterson, S.W. Allen, R.G.
Finding Black Hole Systems in Nearby Galaxies With Simbol-X Paul Gorenstein Harvard-Smithsonian Center for Astrophysics.
Lecture 13 Light: the Cosmic Messenger Telescopes and Observational Astronomy.
Rapture of the Deep Sky Mel Ulmer Dept of Physics & Astronomy Northwestern University This talk posted on
Observations Tanaka, Nandra, Fabian. Nature, 1995, 375, 659. Galaxy MCG , ASCA satellite, SIS detectors Sy 1 type The line profile of iron K.
Exploring an evidence of supermassive black hole binaries in AGN with MAXI Naoki Isobe (RIKEN, ) and the MAXI
Digital Aperture Photometry ASTR 3010 Lecture 10 Textbook 9.5.
In conclusion the intensity level of the CCD is linear up to the saturation limit, but there is a spilling of charges well before the saturation if.
Chandra Science Highlight
The X-ray Universe 2008 Granada, 29 May 2008
Wavelet Analysis for Sources Detection
High Energy emission from the Galactic Center
Basics of Photometry.
Wavelet method for source detection in GLAST photon-counting images
XMM-Newton Observation of the composite SNR G0. 9+0
The spectral properties of Galactic X-ray sources at faint fluxes
TRAINEE PRESENTATION The North and South Ecliptic Pole fields population Project supervisors: R. Saxton N. Loiseau Trainee student: Jaime Abella Payá.
Black Holes in the Deepest Extragalactic X-ray Surveys
Chandra Science Highlight
Presentation transcript:

Imaging Analysis Aneta Siemiginowska Chandra X-ray Center Harvard-Smithsonian Center for Astrophysics

What are the goals of Image Analysis in Astronomy? ● Create a nice picture. ● Understand the nature of the source: ● Understand the shape and size of the emitting regions ● Understand temperature distribution, velocity density distribution, composition and metallicity etc. ● Differentiate between emission processes. ● Understand energy and power involved in the observed emission ● Evolution of the source and how it relates to other sources.

First X-ray Imaging Telescope The Einstein Observatory (HEAO-2) Tycho Supernova Remnant (1572) Energy: keV Angular resolution ~6 arcsec! High Resolution Imager Effective Area FOV ~25 arcmin 5-20 cm2 Nov April 1981 Credit: HEASARC

XMM Newton Tycho Supernova Remnant Aschenbach et al (2000) Launched in Dec.1999 Energy Range: keV Effective Area: 1500 cm2 at 1 keV FOV ~27-33arcmin Angular resolution ~6 arcsec Energy resolution: E/DE ~ 20-50

CHANDRA X-ray Observatory ● Launched in July 1999 ● Energy Range: keV ● Effective Area: ● ACIS-I ~ 500 cm2 ● HRC-I ~ 225 cm2 ● FOV: ACIS-I 16'x16' HRC-I: 30'x30' ● Energy Resolution: E/DE ~ at 1keV ● Angular Resolution < 1 arcsec Color-coded image Credit: CXC Tycho Supernova

Angular Resolution Chandra Einstein XMM FWHM ~ 6 arcsec FWHM ~ 0.5 arcsec

Galactic Center GRANAT/SIGMA in high energy X-rays and gamma-rays 14x14 deg field Credit: SIGMA team keV Angular resolution: 10 arcmin keV

Summary I will use CIAO software in image analysis. (but see IRAF, FTOOLS, XIMAGE, XSPEC) * Difference between Image and the Event file? Binning options * Display data in different coordinates, detector vs. sky * Understanding the instrument. * Instrument characteristics * Detecting sources building the source list for further spectral analysis excluding the sources for the extended source analysis * PSF effects * Radial Profile * 2D fitting in Sherpa * Smoothing the image * Image Reconstruction and Deconvolution

Event list and Binning PRISM view of the Event file.

X-ray Images ● Intensity Maps ● color represents variations in the intensity ● Raw vs. Smoothed images ● true counts per pixel ● average counts/pixel ● True/False color images ● color represents energy ● Temperature maps ● Color represents temperature ● Images from different bands: X- rays/radio/optical

Raw Color coded Smoothed Fabian et al (2000) Perseus A CHANDRA ACIS-S

Perseus A X-ray/Radio Optical Fabian et al (2000)

Coordinates and WCS SKY DET

Detector Coordinates: dmcopy "evt.fits[bin det=16]" det_by_16.img ds9 det_by_16.img

Instrumental Features ● Understanding the instrument: ● CCD is different than microchannel plate ● Bad pixels or columns: ● Hot pixels, node boundaries ● Trail images

Chandra ACIS McDowell 2001

Instrument Characteristics ● Exposure Maps ● Background: instrumental and cosmic ● Point Spread Function (PSF)

Exposure Maps CHANDRA ACIS Filtered Includes: detector quantum efficiency (QE), non-uniformity across the detector (QUE), mirrors vignietting, bad pixels and columns, chip gaps etc. Units [cm 2 cts /photon]

Exposure Maps McDowell 2001

CHANDRA Image of Tycho Supernova S = Data / (ExpMap*ExpTime) Credit: CXC

Point Spread Function ● Describes the shape of the image produced by a point source (delta function) on the detector: “blurring” ● Depends on photon energy and the location on the sky in respect to the optical axis of the telescope. ● Usually consists of the core and wings => dynamic range

CHANDRA PSF 5 arcmin off-axis

CHANDRA PSF off- axis 10 arcmin

0.277 keV 9.7 keV Chandra/HRMA on axis PSF Encircled Energy: Radius (arcsec) ● Fraction of Counts enclosed within the area of a given radius. ● Energy keV 95% in 9.7 keV 75% in 1''

ACIS-S data Simulated PSF Fruscione et al 2002

Analysis Challenges ● PSF needs to be included in the X-ray analysis. ● PSF variations across the detector have to be taken into account in any multi-scale analysis. ● PSF affects determination of a shape of the source. ● Separation of overlapping sources: ● Size and boundaries of each source ● Luminosity of each source ● Pile-up modification of the PSF

Background ● Background radiation is common to X-ray detectors: ● Background due to diffuse X-ray background emission => contribution from unresolved sources ● Charged particle background => non-X-ray background ● Unrecognizable source contribution (trail images)

Chandra ACIS

Analysis Challenges ● Non-uniformity of the background radiation. ● Time-Variability in background intensity. ● Spurious events not recognized as background and interpreted as source.

CHANDRA ACIS BACKGROUND Effect of a Charged Particle Event FI CCD BI CCD

Energy Dependence of Non-X-ray Background Chandra ACIS-S

Variability and Background Flares Chandra ACIS-S TIME CXC/CAL

Radial Profile Simulated PSF Data Fruscione et al 2002

Excluded SE -Region NW-Region Profile file in FITS format: Fruscione et al 2002

Fitting Radial Profile in Sherpa Fruscione et al 2002

Image Fitting in Sherpa * Read data: binned image * Read error image or use Sherpa statistics * Display image “image data” * Filter the image using ds9 or supply 2D filter * Define 2D models * Use PSF as a model or convolution kernel * Use Exposure Maps

Image Data PSF Model Residuals

Create a Nice Picture! => Smoothed Images Convolution of an Image with a kernel function usually: Gaussian, Box or Top Hat (wavelet) => aconvolve in CIAO CSMOOTH – adaptive smoothing with circular Gaussian or TopHat kernel functions. NGC 4038/39 Credit: CXC

Galactic Center X-ray Image of the CHANDRA ACIS 2-8 keV Red: keV Green: keV Blue: keV 8.4x8.4 arcmin Baganoff etal (2003) Exposure time 164 hrs => Smoothed Image

Multiscale Statistical Methods ● Multi-resolution methods => disentangle structures on different resolution scales in the observed image ● Includes wavelet transforms, adaptive smoothing, slicing of the image. ● Applications in Astronomy: filtering, image restoration, enhancements, image characterization. => Mirroring human visual and mental processes, in observing and interpreting phenomena simultaneously on multiple scales

Goals of Image Analysis ● What are the shape, size and boundaries of my source? ● “What degree of credibility is attached to the wispy arm structure we see emanating from the ring of supernova 1987a?” ( Murtagh 1992) ● How real is the X-ray jet seen in the Galactic Center?

Galactic Center Chandra/ACIS (2-8) KeV 1.23x1.23 arcmin Baganoff et al (2003) 1. Where is the supermassive black hole in Galactic Center? 2. Is the X-ray jet real? Questions:

Summary

Some typical Questions ● What is the flux of my source? ● What is the detection limit in my image? ● Modeling the surface brightness. ● Obtaining a source centroid. ● Is my source a point source? Is there an extended structure associated with this source? What is the statistical significance of this extended emission? ● What is the source shape?