CR Workshop – Leiden (H), 14 – 18 / 03 / 2011

Slides:



Advertisements
Similar presentations
High Energy Astrophysics
Advertisements

X-ray Astronomy with High Spectral Resolution: Astro-E2 / ISAS Y. Tanaka.
Optical Astronomy Imaging Chain: Telescopes & CCDs.
Basic Principles of X-ray Source Detection Or Who Stole All Our Photons?.....
S.Mereghetti - Simbol-X: The hard X-ray Universe in focus - Bologna -15/5/20071 Studying the Galactic Ridge Emission with SIMBOL-X Sandro Mereghetti IASF.
The HEROES Balloon- borne Hard X-ray Telescope Colleen A. Wilson-Hodge, J. Gaskin, S. Christe, A. Shih, K. Kilaru, D.A. Swartz, A. F. Tennant, B. Ramsey.
X-ray transients with Astrosat
Chapter 6 Optics and Telescopes
Gamma-Ray Astronomy Call no Assoc. Prof. Markus Böttcher Clippinger # 339 Phone:
DEPARTMENT OF PHYSICS AND ASTRONOMY ©M.A.Barstow – 2009 Telescopes for High Energy Astrophysics.
X-ray Astronomy Lee Yacobi Selected Topics in Astrophysics July 9.
Astro-E2 and Japanese future space programs for high energy astrophysics Astro-E2 NeXT XEUS Small satellite programs Tadayasu Dotani (ISAS)
Telescopes and Spacecraft Astronomy 311 Professor Lee Carkner Lecture 7.
Chapter 3: Telescopes. Goals Describe basic types of optical telescopes Explain why bigger is better for telescopes Describe how the Earth’s atmosphere.
Some Chandra Basics. Chandra X-Ray Observatory.
Probing the X-ray Universe: Analysis of faint sources with XMM-Newton G. Hasinger, X. Barcons, J. Bergeron, H. Brunner, A. C. Fabian, A. Finoguenov, H.
High energy perspectives (and conclusions) Philippe Ferrando APC Laboratory (UMR 7164) - Service d’Astrophysique CEA/Saclay APC Conference High Energy.
Telescopes (Chapter 6). Based on Chapter 6 This material will be useful for understanding Chapters 7 and 10 on “Our planetary system” and “Jovian planet.
Potential Positron Sources around Galactic Center Department of Physics National Tsing Hua University G.T. Chen 2007/11/29.
The all-sky distribution of 511 keV electron-positron annihilation emission Kn ö dlseder, J., Jean, P., Lonjou, V., et al. 2005, A&A, 441, 513.
Main detector types Multi Pixel Photon Counter (MPPC) and Charge Coupled Devices (CCDs) How does it work? 1. Photon hits a pixel producing electron hole.
This Set of Slides This set of slides deals with telescopes. Units covered: 26, 27, 28, 29, and 30.
The 511 keV Annihilation Emission From The Galactic Center Department of Physics National Tsing Hua University G.T. Chen 2007/1/2.
COSPAR Workshop, Udaipur 2003 An Introduction to X-ray Astronomy Keith Arnaud NASA Goddard University of Maryland.
Astronomical Spectroscopy
Science Specification of SOLAR-C payload SOLAR-C Working Group 2012 July 23.
Chapter 6 Optics and Telescopes.
ISNS Phenomena of Nature The Eye The eye consists of pupil that allows light into the eye - it controls the amount of light allowed in through the.
Chapter 6: The Tools of the Astronomer. Telescopes come in two general types Refractors use lenses to bend the light to a focus Reflectors use mirrors.
How do Astronomers know what they know? Almost everything we know about Astronomy was learned by gathering and studying light from distant sources Properties.
July 2004, Erice1 The performance of MAGIC Telescope for observation of Gamma Ray Bursts Satoko Mizobuchi for MAGIC collaboration Max-Planck-Institute.
New Improved Eyes Telescopes and “Invisible” Astronomy.
High-Energy Astrophysics
NASSP Masters 5003F - Computational Astronomy Lecture 19 EPIC background Event lists and selection The RGA Calibration quantities Exposure calculations.
Problems associated with Earth based observation Optical band = stars and planets and nebulae. Infrared band = low energy heat sources. Radio band = dust.
Optics and Telescopes. Optics and Telescopes: Guiding Questions 1.How do reflecting and refracting telescopes work? 2.Why is it important that professional.
Laue lenses for hard X-rays (> 60 keV) F. Frontera and A. Pisa on behalf of a Large Collaboration Rome, 18 March 2005.
Studying for the Exam Relevant chapters: E, 1, 2 & 3 To prepare for the exam it is helpful to … –review readings –review lecture notes online (esp. concept.
© 2004 Pearson Education Inc., publishing as Addison-Wesley Telescopes.
Gamma-Ray Bursts observed with INTEGRAL and XMM- Newton Sinead McGlynn School of Physics University College Dublin.
Jacques Paul Soft Gamma-Ray Astronomy 23 January 2001 Rencontres de Moriond Les Arcs Expected Impact on VHE Phenomena Panorama in the Coming Years INTEGRAL.
Gamma-Ray Telescopes. Brief History of Gamma Ray Astronomy 1961 EXPLORER-II: First detection of high-energy  -rays from space 1967 VELA satelllites:
Telescopes.
Hard X and Gamma-ray Polarization: the ultimate dimension (ESA Cosmic Vision ) or the Compton Scattering polarimetery challenges Ezio Caroli,
Instrumental Development in Japan for Future Missions 1.Si strip detectors(GLAST) 2.Supermirror technology 3.New hard-X/  detectors 4.TES calorimeters.
The mission Simbol-X : the hard X-ray universe in focusMay 14, 2007 Simbol-X the hard X–ray Universe in focus 0.5 – 80 keV formation flight Philippe Ferrando.
What does mean neighbours ? At the same epoch –simultaneous (transient phenomenae) –before (can affect the SIMBOL-X observing plan) –after (can complement.
Silicon Optics for Wide Field X-ray Imaging Dick Willingale et al. – SPIE August 2013 Silicon Optics for Wide Field X-ray Imaging Dick Willingale University.
X-ray Astronomy School 2005 An Introduction to X-ray Astronomy Keith Arnaud NASA Goddard University of Maryland.
Observational techniques meeting #15
14 Sep 2000ASTR103, GMU, Dr. Correll1 ASTR 103--Week 3.
“The SIMBOL-X optics”, Bologna, 14 May 2007 SIMBOL-X SIMBOL-X OPTICS SIMBOL-X OPTICS Giovanni Pareschi INAF - Osservatorio Astronomico di Brera Lower Spider.
MeV Gamma Ray Nuclear Astrophysics Yesterday: Science and Observations
X-ray Astronomy School 2002 The Future of X-ray Astronomy Keith Arnaud NASA/GSFC and UMCP.
Chapter 24 Sec. 1 Light Sec. 2: Tools of Astronomy
Hard X-ray Telescope for the FFAST project 1. The FFAST project Hironori Matsumoto (Nagoya University) Miyata, Y., Furuzawa, A., Kunieda, H. (Nagoya Univ.),
NuSTAR, ITS BACKGROUND AND CLUSTERS OF GALAXIES FABIO GASTALDELLO INAF, IASF-Milano And The Galaxy Clusters NuSTAR Team.
Exploring an evidence of supermassive black hole binaries in AGN with MAXI Naoki Isobe (RIKEN, ) and the MAXI
High Energy Astrophysics in the Next Decade International Workshop on NeXT and Future Missions Tokyo Metropolitan University June 21-23, 2006.
MPI Semiconductor Laboratory, The XEUS Instrument Working Group, PNSensor The X-ray Evolving-Universe Spectroscopy (XEUS) mission is under study by the.
Astronomical Observations TypeAtmosphere  Radio WavesNo effect  MicrowavesMostly blocked  InfraredBlocked  Visible LightSlight blurring  UltravioletBlocked.
MAXI - Monitor of All-sky X-ray Image Performance of the engineering model of the MAXI/SSC Katayama H. a, Tomida H. a, Matsuoka M. a, Tsunemi H. a,b, Miyata.
Lecture 3 X-ray and gamma-ray satellites Absorption in X-rays:
Chapter 6 Telescopes: Portals of Discovery
Homework #4 What is the maximum resolution of your eyes (assume the wavelength range that your eyes are sensitive to is 300 – 700 nm and that your iris.
HARD X-RAY/SOFT g-RAY OBSERVATIONS OF THE GALACTIC DIFFUSE EMISSION WITH INTEGRAL/SPI SPI SPECTROMETER (20 keV – 8 MeV, foV 30°) ONBOARD INTEGRAL OBSERVATORY.
Periodicity Search in X-ray data of RX J
WPOL Wide field camera with POLarimetry
Monitor of All sky X-ray Image (MAXI)
Astronomical Observations What Wavelengths To Use?
Presentation transcript:

CR Workshop – Leiden (H), 14 – 18 / 03 / 2011 Instrumentation for X-Ray Astronomy A. Goldwurm AstroParticule et Cosmologie Service d’Astrophysique / CEA – Saclay France A. Goldwurm 1 CR Workshop – Leiden (H), 14 – 18 / 03 / 2011

Specific Issues of X-ray Astronomy Earth atmosphere is opaque to X-rays => balloons, rockets or satellites needed Optics: difficult or even impossible to focalize X-rays Detectors of Photoelectric and Compton interactions Sources have intrinsically weak photon fluxes (non-thermal spectra or HE tail of thermal very hot medium) Detectors sensitive to particles and particle-generated X-rays => high level of background => Low S/N ratios

The early days of X-ray Astronomy X-ray astronomy starts after the WW II 1962 discovery of the 1st extra-solar X-ray source with Sounding Rocket det 1970 First X-ray satellite Uhuru Instruments based on Proportional Counters + collimators End of ’70s : focusing telescopes

Focalisation of Soft X-rays X and gamma - rays radio, IR, visible, UV waves Soft X - rays Jacques Paul Planche 4 L’observatoire spatial INTEGRAL – Lycée Arago – Perpignan

X-ray Grazing incidence reflection Since EX > Eebind then refraction index for X-rays nX < 1 => it exists an incident angle of total external reflection (grazing angle) given by cos θr = nX For nX = (1-δ), θr = (2δ)½ with δ = N0Zreρλ2/A 2π (e.g. Giacconi+ 69) For Heavy Elements Z/A ~ 0.5 and therefore θr  ρ1/2/ EX Good reflectors are Au, Ni, Ir, Pt and critical angle are in the range 10’ - 2° for X-rays of 0.1 to 10 keV

WOLTER Type I X-ray Mirror System 1 Paraboloid + 1 Hyperboloid polished and coated mirrors Emax = k f/D keV for D=1 m diameter & f=10 m focal length => Emax~ 10 keV

Nesting W-I Mirrors in a telescope

A Focusing X-ray Telescope Several nested W-I mirrors and coated in Ni, Au or Ir focalize grazing incident X-rays Into a focal plane position sensitive detector, e.g. a CCD for X-rays Images are formed with effective area given by nested mirrors and a low background that depends on the detector volume.

Major Mirror X-ray Telescopes (untill 2000) 1999

XMM - Newton

XMM Optical System and the Reflection Grating Spectrometer 70 cm 58 mirror shells 0.5 – 1 mm thick

Images from XMM Newton EPIC Observations: stabilized pointing of target sources for typical exposures of 5 - 200 ks Data are in form of event lists (x, y, t, E) Analysis: correct, filter, bin and combine event lists into images, spectra, light curves, and then derive source parameters.

Imaging performances of XMM 110” Images of a point source by the 3 EPIC cameras (MOS1 MOS2 and PN) PSF as function of distance from source: 6" (FWHP), 15" (HEW)

XMM Performances Effective area of XMM mirrors plus focal plane instruments Typical spectra otained with XMM EPIC Calibration +background spectrum with XMM EPIC PN

The Chandra Observatory

The concept of a Pinhole camera And … for E > 10-15 keV ? The concept of a Pinhole camera

The concept of Coded Mask Imaging source à l’infini masque codé détecteur sensible à la position

source 1 masque codé détecteur sensible à la position

source 2 masque codé détecteur sensible à la position

The ESA INTEGRAL Mission A Gamma Ray Observatory 2 main -ray Telescopes Energy: 15 keV – 8 MeV High angular res.: ~ 12’ (IBIS) High spectral Res: DE/E ~=500 (SPI) + 2 Monitors (opt, X) Launched with a Proton on 17/10/2002 The First Gamma-Ray OBSERVATORY for the Astronomical Community

SPI γ-ray spectrometer IBIS / ISGRI Performances Energy Band 20 keV-1 MeV Angular Resolution 12’ FOV at 100% s. 9° x 9° at 0 sensitivity 29° x 29° Point Source Location Err. 30” (S/N~30) Temporal resolution 60 s 100 keV Sensitivity (ph cm-2 s-1 keV-1) 4 10-7 (for 106 s, 3, E=E) 1 mCrab Narrow line sens. (cm-2 s-1) 10-5 Spectral resolution 8 keV OMC (visible band) IBIS γ-ray imager JEM-X (X-ray monitor) ISGRI camera SPI γ-ray spectrometer

IBIS: Imager onBoard Integral Satellite

IBIS Data Analysis Reconstructed Sky Mask Pattern Detector Image Sum of Sky Images

Active X-Ray Missions MISSSION LAUNCH ENERGY OPTICS DETECTORS FOV Ang Res Area cm2 En.Res (eV) RXTE 1995 2-60 keV Collimator PropCount 1° 5000 1125 (6 keV) Chandra 1999 0.1 – 10 keV Mirrors CCD 17’ 0.5" 230 170 Newton 30’ 6" 850 130 INTEGRAL 2002 20 keV - 10 MeV Cod Mask CdTe Det Ge Det 30° 12’ 2000 (1MeV) SWIFT 2004 1 – 150 keV Mirror Suzaku 2005 0.1 – 700 keV Si Det 20’ 4.5° 1.5’ 1000 6 keV 120 MAXI (on ISS) 2008 2 - 30 keV Collimator (ASM) Gas PC Solid St. C 16 0° x 1.5° 1.5°

Same examples of Images obtained with X-ray Focussing Telescopes and Coded Mask hard X-ray / soft gamma-ray Telescopes

Chandra & XMM Surveys of the GC Commenting the talk

6.4 keV Neutral Iron K line

XMM-Newton GC Survey 0.3-9 keV INTEGRAL GC Survey Sgr A 20-40 keV 0.0° XMM-Newton GC Survey 0.3-9 keV 0.0° (Belanger et al. 2006) (Decourchelle et al. 2003) INTEGRAL GC Survey Sgr A 20-40 keV Sgr B2 0.0° 1.0° 359.0°

INTEGRAL / SPI 511 keV Line Spherical shape (Bulge) 2D Gaussian profile with FWHM ~ 8º Positronium fraction: 0.91 - 0.97 Annihilation in warm ionized medium Origin of positrons unknown Originated at the GC ? (Knodelseder et al. 2004, Churazov etal 04, Jean etal 2005, ..) Centroid: 511.06+0.17/-0.10 keV Line width: 2.95+0.45/-0.51 keV (FWHM) Flux: (1.05±0.06)×10-3 ph cm-2 s-1

Perspectives and Future Missions Focalization at E > 10 keV, using multilayer coating + long focal L (> 10 m) with extendable mats or formation flying: Nu-Star (US, 2013) Astro-H (JAXA, +, 2014): Emax ~ 80 keV but Ang.Res > 40’ Several non-selected EU projects: Simbol-X (F-I), COSPIX (M3), NHXM (M3) Focal-Plane Micro-calorimeters for high spectral res.: Astro-H (and IXO) Light mirrors (glass layers, silicon pore layers) to obtain large effective areas and sensitivities (IXO) Small / medium missions: X-ray polarimeters (GEM US 2014) or Large sensitive areas for timing / spectral studies (LOFT) Coded masks for HE monitoring of transients and GRBs (SVOM Ch – F 2014) Compton telescopes and Bragg diffusion lenses (M3) for the 1 MeV range.

X-Ray Astronomy Programmatics Chandra, XMM-Newton, INTEGRAL missions extended to 2014 Nu-Star, Astro H, SRG, GEM in development phase IXO delayed by US Decadal to after 2025 In competition for ESA Cosmic Vision Large class Mission (decision 2011) No HE mission in the ESA Medium class Missions M1/M2 Missions (Launch 2018) 1 HE mission selected for the ESA M3 call (L 2020): LOFT