ROSAT Roentgen Satellite. Chandra X-ray Observatory

Similar documents
Introduction to SDSS -instruments, survey strategy, etc

Chandra was launched aboard Space Shuttle Columbia on July 23, 1999!!!

Analysis of Off-Nuclear X-Ray Sources in Galaxy NGC Sarah M. Harrison

Problem Solving. radians. 180 radians Stars & Elementary Astrophysics: Introduction Press F1 for Help 41. f s. picture. equation.

Data Release 5. Sky coverage of imaging data in the DR5

SDSS-IV and eboss Science. Hyunmi Song (KIAS)

Introduction to the Sloan Survey

Dark Energy. Cluster counts, weak lensing & Supernovae Ia all in one survey. Survey (DES)

JINA Observations, Now and in the Near Future

Galaxy formation and evolution. Astro 850

X- & γ-ray Instrumentation

Cosmic Distance Determinations

The Large Area Telescope on-board of the Fermi Gamma-Ray Space Telescope Mission

The effect of large scale environment on galaxy properties

Astronomical imagers. ASTR320 Monday February 18, 2019

From quasars to dark energy Adventures with the clustering of luminous red galaxies

A NEW GENERATION OF GAMMA-RAY TELESCOPE

The quest for Type 2 quasars: What are the X-ray observations of optically selected QSOs2 telling us?

Clusters and Groups of Galaxies

Chapter 0 Introduction X-RAY BINARIES

Lecture 11: SDSS Sources at Other Wavelengths: From X rays to radio. Astr 598: Astronomy with SDSS

9. Evolution with redshift - z > 1.5. Selection in the rest-frame UV

BAO and Lyman-α with BOSS

What to measure? X-ray emission carries various information quantify:

Large-Scale Structure

Active Galactic Nuclei OIII

Black Holes and Active Galactic Nuclei

arxiv:astro-ph/ v1 10 Nov 1999

The Cosmological Redshift. Cepheid Variables. Hubble s Diagram

Astr 323: Extragalactic Astronomy and Cosmology. Spring Quarter 2014, University of Washington, Željko Ivezić. Lecture 1:

Cosmology on the Beach: Experiment to Cosmology

Results from the Chandra Deep Field North

AS 101: Day Lab #2 Summer Spectroscopy

(Present and) Future Surveys for Metal-Poor Stars

Excerpts from previous presentations. Lauren Nicholson CWRU Departments of Astronomy and Physics

QSO ABSORPTION LINE STUDIES with the HUBBLE SPACE TELESCOPE

Doing astronomy with SDSS from your armchair

Chandra: Revolution through Resolution. Martin Elvis, Chandra X-ray Center

Chapter 5: Telescopes

Publ. Astron. Obs. Belgrade No. 86 (2009), TURKISH NATIONAL OBSERVATORY (TUG) VIEW OF CLUSTERS OF GALAXIES

Objectives. HR Diagram

Test #2 results. Grades posted in UNM Learn. Along with current grade in the class

arxiv:astro-ph/ v1 6 Dec 1999

The Sloan Digital Sky Survey

1. Give short answers to the following questions. a. What limits the size of a corrected field of view in AO?

The J-PAS Survey. Silvia Bonoli

Background Picture: Millennium Simulation (MPA); Spectrum-Roentgen-Gamma satellite (P. Predehl 2011)

SDSS-IV MaStar: a Large, Comprehensive, and High Quality Empirical Stellar Library

Detectors for 20 kev 10 MeV

Multi-wavelength Astronomy

Astronomy 330 Lecture Dec 2010

Lecture 12: Distances to stars. Astronomy 111

Lab 1: Introduction to the sky and making telescopic observations with the CCD camera. AST 152M Lab Instructor: Greg Doppmann Due: Feb 11, 2000

Comets observed with XMM-Newton

Hubble s Law. Tully-Fisher relation. The redshift. λ λ0. Are there other ways to estimate distances? Yes.

Astronomical Techniques

Astronomical image reduction using the Tractor

Introduction to SDSS-IV and DESI

Cherenkov Telescope Array Status Report. Salvatore Mangano (CIEMAT) On behalf of the CTA consortium

Clusters, lensing and CFHT reprocessing

Overview: Astronomical Spectroscopy

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

High Energy and Time Resolution Astronomy and Astrophysics: 1. X-ray Astronomy. 1. X-ray Astronomy. PhD Course, University of Padua Page 1

Project: Hubble Diagrams

Hubble s Law and the Cosmic Distance Scale

Galaxy classification

Astrophysical techniques. Lecture 3: X-ray astronomy

Chandra Observation of Point Sources in the X-Ray Elliptical Galaxy NGC 1407

New physics is learnt from extreme or fundamental things

Scintillation Detector

The J-PAS survey: pushing the limits of spectro-photometry

Searching for Needles in the Sloan Digital Haystack

TMT and Space-Based Survey Missions

Clusters of galaxies

Astr Resources

Galaxy Clusters. Giants of the Universe. Maciej Soltynski. ASSA Symposium Virgo cluster around M86

SDSS Data Management and Photometric Quality Assessment

Surveys at z 1. Petchara Pattarakijwanich 20 February 2013

A very bright (i = 16.44) quasar in the redshift desert discovered by the Guoshoujing Telescope (LAMOST)

The Hamburg/RASS Catalogue of Optical Identifications of ROSAT-BSC X-ray Sources

Constraining Dark Energy with BOSS. Nicolas Busca - APC Rencontres de Moriond 19/10/2010

Quasar identification with narrow-band cosmological surveys

arxiv:astro-ph/ v1 6 May 2004

Quasars in the SDSS. Rich Kron NGC June 2006 START CI-Team: Variable Quasars Research Workshop Yerkes Observatory

Foundations of Astronomy 13e Seeds. Chapter 6. Light and Telescopes

arxiv:astro-ph/ v1 30 Aug 2001

Clusters of Galaxies " High Energy Objects - most of the baryons are in a hot (kt~ k) gas." The x-ray luminosity is ergs/sec"

Detecting high energy photons. Interactions of photons with matter Properties of detectors (with examples)

Luke Leisman Calvin College. Photo Credit: SLOAN Digital Sky Survey. Great Lakes Cosmology Workshop June 15, 2010

Rajib Ganguly (University of Michigan-Flint)

The Large Synoptic Survey Telescope

Astronomical "color"

A SPEctra Clustering Tool for the exploration of large spectroscopic surveys. Philipp Schalldach (HU Berlin & TLS Tautenburg, Germany)

CONTENTS AIM OF THE PROJECT. INTRODUCTION: AGNs, XMM-Newton, ROSAT. TECHNIQUES: IDL, SQL, Catalogues RESULTS SUMMARY DESIRED OUTPUTS QUESTIONS

MASSIVE BLACK HOLES AMY REINES IN NEARBY DWARF GALAXIES HUBBLE FELLOW NATIONAL OPTICAL ASTRONOMY OBSERVATROY

Radioactivity. Lecture 6 Detectors and Instrumentation

Physics 24: The Big Bang, Week 3: Hubble s Law David Schlegel, LBNL

Active Galaxies & Quasars

EUCLID Spectroscopy. Andrea Cimatti. & the EUCLID-NIS Team. University of Bologna Department of Astronomy

Hughes et al., 1998 ApJ, 505, 732 : ASCA. Westerlund, 1990 A&ARv, 2, 29 : Distance to LMC 1 ) ) (ergs s F X L X. 2 s 1. ) (ergs cm

Transcription:

ROSAT Roentgen Satellite Joint facility: US, Germany, UK Operated 1990 1999 All-sky survey + pointed observations Chandra X-ray Observatory US Mission Operating 1999 present Pointed observations

How do you focus X-rays? Wolter X-ray telescope What is the collecting area (the size) of the telescope? How can we improve the collecting area?

ROSAT Instrumentation Position Sensitive Proportional Counter (PSPC) 20 resolution, 2 degree FOV Energy range 0.1 2.5 kev Effective area ~ 240 cm 2 at 1 kev Conducted all-sky survey Also did pointed observations High Resolution Imager (HRI) 5 resolution, 38 FOV Effective area ~ 80 cm 2 at 1 kev Pointed observations

Chandra Instrumentation Advanced CCD Imaging Spectrometer (ACIS) Imaging: 2 spatial resolution, ten 8 x8 CCDs Moderate resolution spectroscopy Energy range 0.4 10 kev Effective area ~ 600 cm 2 at 1 kev High Resolution Camera (HRC) 0.4 resolution, 30 FOV Effective area ~ 200 cm 2 at 1 kev High Energy Transmission Grating (HETG) E/ΔE = 1000 0.4 10 kev Low Energy Transmission Grating (LETG) Optimized for low energy (0.08-0.2 kev) spectroscopy

Chandra vs ROSAT: The Crab Nebula Optical image

Chandra vs ROSAT: The Crab Nebula

But how do you detect X-rays? Proportional Counters (ROSAT PSPC) Pass X-rays into a gas-filled chamber X-ray enters chamber, ionizes an atom (primary electron) Primary electrons can have enough energy to ionize other atoms (secondary electrons) Electrons accelerate towards anode wire, ionizing more atoms ( gas gain ~ 2-3 orders of magnitude) Multiple anode wires give positional sensitivity Energy information comes from signal strength Limited by gas supply Scintillation Detectors For X-ray energies > 50 kev, the gas density needed to stop an X-ray becomes prohibitive Scintillation detectors use solid crystal (NaI or CsI for example) which emits light upon absorption of a photon Detect photons using a photomultiplier tube

Microchannel plates (Chandra HRC) Material with many pores/channels, with a voltage applied. X-ray hits side of channel, kicks out electron Electron accelerates, kicks out more electrons Signal measured for each channel Long life-time (no gas supply issues) Good spatial resolution, poor energy resolution X-ray CCDs (Chandra ACIS) Conceptually like optical CCDs Optical photon produces 1 electron, X-ray photon produces many Optical CCDs integrate to build up charge X-ray CCDs can be read out fast, so charge tells you energy of X-ray

The Sloan Digital Sky Survey Dedicated 2.5m telescope at Apache Point, NM Main Survey ( Legacy ) operated 2000 2008, through Data Release 7 (DR7) Additional projects since then: SEGUE, BOSS, APOGEE, MARVELS (DR12) Imaging: Multiband ugriz, median seeing ~ 1.3 54s exposure time by scanning gives g lim = 22.2 ~ 1% photometric uncertainty 14,500 square degrees 208M galaxies, 260M stars Fiber spectroscopy: R ~ 2000 spectra from 3800 9200 Å Redshift accuracy ~ 30 km/s Galaxies (r<17.77) and Quasars (i<19.1 or 20.2) ~ 2.4M galaxy spectra, 0.5M quasar spectra, 0.85M stellar spectra

SDSS Data Products Calibrated Images and Spectra: Quick look format Reduced fits files Data Products (Imaging): Magnitudes, colors For galaxies: size, structural information, photo-z Data Products (Spectra): Redshift/velocity Line indices Spectral classification Catalogs, for example: Luminous Red Galaxies Quasar catalog White dwarf catalog Moving objects

The ROSAT Brightest Cluster Sample (Ebeling et al 1998) Flux limited catalog of bright X-ray clusters (N=206)

Picking Clusters 1: Sky position: must be on SDSS footprint. (N ~ 159)

Picking Clusters 2: Cluster properties: we want massive clusters. (N = 111) Vikhlinin et al (2006) M 500 M 2500 M N = mass contained within a radius with an density of N times the average density of the universe. kt > 4 kev

Picking Clusters 3. Distance: We want them to fit on ACIS field of view (array of 8 x8 CCDs). z>0.035 We want to understand their optical morphology and nuclear spectra. (SDSS imaging resolution ~ 1 and fiber diameter ~ 3 ) z D A (Mpc) 1 Mpc (arcmin) 1 arcsec (kpc) 0.025 102 34 0.5 0.035 142 24 0.7 0.05 199 17 1.0 0.075 290 12 1.4 0.1 376 8 1.8 z<0.075 N = 14

Picking Clusters so far. SDSS footprint kt > 4 kev 0.035 < z < 0.075 What s the next criterion? Chandra ACIS pointings!

Final Cluster Targets Cluster RA (deg) Dec (deg) Redshift Abell 2065 230.6215 +27.7076 0.07 Abell 2063 230.7712 +8.6086 0.035 Abell 1795 207.2189 +26.5916 0.06 Notes: Cluster redshifts are approximate; you should refine these estimates using the SDSS data. When calculating intrinsic properties (physical sizes, luminosities, etc) remember that at these distances you must use the cosmologically correct luminosity distance (D L ) and angular size distance (D A ) to do the calculations.