Measuring the SPIN of Black Holes

Slides:



Advertisements
Similar presentations
Growth of massive black holes during radiatively inefficient accretion phases Xinwu Cao Shanghai Astronomical Observatory, CAS.
Advertisements

Strong gravity with Athena Jiří Svoboda Czech Academy of Sciences using simulations and figures done by the Athena Science working group “The Close Environments.
Neutron Stars and Black Holes Please press “1” to test your transmitter.
Copyright © 2010 Pearson Education, Inc. Chapter 13 Black Holes.
AGN in hierarchical galaxy formation models Nikos Fanidakis and C.M. Baugh, R.G. Bower, S. Cole, C. Done, C. S. Frenk Accretion and ejection in AGN, Como,
A reflection origin for the soft and hard X-ray excess of Ark 120 Ferrara, 2010 May in collaboration with: Andy Fabian, Rubens Reis, Dom Walton (Institute.
Soft X-ray line reflection in NLS1 galaxies Th. Boller, A. Müller, A. Ibarra MPE Garching Excellence Cluster Universe Munich XMM SOC, Villa Franca, Spain.
COSPAR Workshop, Udaipur 2003 Active Galactic Nuclei : I Keith Arnaud NASA Goddard University of Maryland.
X. Barcons, XEUS SAGXEUS: Physics of the hot evolving Universe XEUS: The Physics of the hot Evolving Universe Xavier Barcons.
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.
General Relativity Physics Honours 2006 A/Prof. Geraint F. Lewis Rm 557, A29 Lecture Notes 6.
Horizon and exotics. 2 Main reviews and articles gr-qc/ Black Holes in Astrophysics astro-ph/ No observational proof of the black-hole event-horizon.
Black Holes Old ideas for black holes Theory of black holes Real-life black holes Stellar mass Supermassive Speculative stuff (if time)
1 Astrophysical black holes Chris Reynolds Department of Astronomy.
Fe K  Line in AGN Shane Bussmann AGN Class 4/16/07.
Black Hole Physics with Constellation-X Chris Reynolds Department of Astronomy University of Maryland College Park.
Spectral Line Shapes from Black Hole Accretion Disks Tsing Wai Wong Advisors: Dr. Drew Milsom Dr. David Ballantyne (pictures from
Lecture 18 Black Holes (cont) ASTR 340 Fall 2006 Dennis Papadopoulos.
Christopher | Vlad | David | Nino SUPERMASSIVE BLACK HOLES.
Future prospects for probing strong gravity with X-ray spectroscopy Chris Reynolds Department of Astronomy University of Maryland, College Park & Joint.
Black holes: do they exist?
Ionized absorbers in Galactic Binaries Chris Done & Marek Gierlinski University of Durham.
Matteo Guainazzi (European Space Astronomy Centre) WHY CAN’T WE?
Quasars, black holes and galaxy evolution Clive Tadhunter University of Sheffield 3C273.
Measuring the black hole spin of GX 339-4: A systematic look at its very high and low/hard state. Rubens Reis Institute of Astronomy - Cambridge In collaboration.
Black Holes Escape velocity Event horizon Black hole parameters Falling into a black hole.
Radiatively Inefficient Accretion Flows Roman Shcherbakov, 28 November, 2007.
International Workshop on Astronomical X-Ray Optics Fingerprints of Superspinars in Astrophysical Phenomena Zdeněk Stuchlík and Jan Schee Institute of.
SUMMARY PROBING STRONG GRAVITY IN AGN Kirpal Nandra Imperial College London.
Thomas Boller One of the open questions which still requires further investigations is the detection of dramatic spectral drops above 7 keV in Narrow-Line.
Black Holes This one’s green. I like green.. What happens after a SN? Material remaining after a supernova is 3 times more massive than the sun or more.
Ramesh Narayan (McClintock, Shafee, Remillard, Davis, Li)
MEASURING SPIN PARAMETERS OF STELLAR-MASS BLACK HOLES Ramesh Narayan.
MEASUREMENT OF BRANY BLACK HOLE PARAMETERS IN THE FRAMEWORK OF THE ORBITAL RESONANCE MODEL OF QPOs MEASUREMENT OF BRANY BLACK HOLE PARAMETERS IN THE FRAMEWORK.
Death of Stars III Physics 113 Goderya Chapter(s): 14 Learning Outcomes:
AGN: Testing general relativity (Fe Kα line) and high resolution plasma diagnostics (Warm Absorber) Delphine Porquet MPE, Garching, Germany.
1 A. Streblyanska, G. Hasinger, A. Finoguenov, X. Barcons, S. Mateos, A. C. Fabian A relativistic Fe line in the mean X-ray spectra of type-1 and type-2.
On the spectra and variability of luminous inhomogeneous accretion flows Andrea Merloni Julien Malzac (CESR Toulouse) Andy Fabian (IoA Cambridge) Randy.
Light bending scenario for accreting black holes in X-ray polarimetry 王 炎 南京大学天文系 2011 年 4 月 11 日 arXiv: M. Dovciak, F. Muleri, R. W. Goosmann,
Spins of supermassive black holes in quasars and galaxies Jian-Min Wang ( 王建民 ) Institute of High Energy Physics Chinese Academy of Sciences, Beijing Dec.
The X-ray mirrors Giovanni Miniutti Institute of Astronomy, University of Cambridge SIMBOL-X May -Bologna.
Strong Gravity Effects: X-ray spectra, timing and polarimetry AC Fabian IoA Cambridge UK With help from Giovanni Miniutti, Josefin Larsson, Jamie Crummy,
Black Holes Accretion Disks X-Ray/Gamma-Ray Binaries.
Active Galactic Nuclei Chapter 25 Revised Active Galactic Nuclei Come in several varieties; Starburst Nuclei – Nearby normal galaxies with unusually.
Tiziana Di Salvo DSFA Università di Palermo In collaboration with: A. D'Aì, R. Iaria, N. R. Robba (Univ. Palermo), L. Burderi (Univ. Cagliari), G. Matt.
Broad-Band X-ray Variability of AGNs with Suzaku Y. Terashima Ehime Univ. and The Suzaku SWG team.
Black hole accretion history of active galactic nuclei 曹新伍 中国科学院上海天文台.
Black Holes Pierre Cieniewicz. What are they? A Black Hole (BH) is a place in space from which nothing can escape The reason for this is gravity Some.
Black Holes and the Evolution of Galaxies…. Summary Quasars and Evolution: the universe becomes interesting How we do it: things invisible to see. Demographics:
The central engine: relativistic effects Giovanni Miniutti AGN IX – Ferrara – May 2010.
The High Energy Emission of NGC 1365 and 1H Prague: 2010 DOM WALTON IoA, Cambridge In collaboration with Rubens Reis and Andy Fabian.
A deep view of the iron line and spectral variability in NGC 4051 James Reeves Collaborators:- Jane Turner, Lance Miller, Andrew Lobban, Valentina Braito,
The Cosmic Density and Distribution of Relativistic Iron Lines David R. Ballantyne Center for Relativistic Astrophysics, School of Physics, Georgia Tech.
Broad iron lines from accretion disks K. Iwasawa University of Cambridge.
STRONG RESONANT PHENOMENA IN BLACK HOLE SYSTEMS Institute of Physics, Faculty of Philosophy and Science, Silesian University in Opava, Bezručovo nám. 13,
IXO and strong gravity Measuring the black hole spin IXO and strong gravity Measuring the black hole spin GiorgioMatt Giorgio Matt (Dipartimento di Fisica.
Accretion #3 When is the thin disk model valid? Reynolds number, viscosity Time scales in disk BH spectra Using X-ray spectra to determine BH mass and.
Clocking Super-Massive Black Hole Spin with Accuracy Observations by Suzaku unambiguously confirm the extremely broad Fe K line in MCG– We accurately.
European X-ray CalorimeterUtrecht, October 2004 (Some) astrophysical drivers for a high-resolution imaging X-ray spectrometer Xavier Barcons Instituto.
연세대 특강 What is a Black Hole? Black-Hole Bomb(BHB) Mini Black Holes
18 October 2001Astronomy 102, Fall Today in Astronomy 102: “real” black holes, as formed in the collapse of massive, dead stars  Formation of a.
LINE SHIFT IN ACCRETION DISKS - THE CASE OF Fe Kα
Composite profile of the Fe Kα spectral line emitted from a binary system of supermassive black holes Predrag Jovanović1, Vesna Borka Jovanović2 and Duško.
The X-ray Universe Granada
Lecture 20 Accretion spectrum Gravitational redshift Iron Kα line
NuSTAR + XMM Observations of NGC 1365: A Constant Inner Disc
General Relativity in X-ray Astronomy Astrosat and Future Experiments
Supernova in images of Greg Thorne and Nick McCaw
An X-ray hysteresis cycle in ESO 511-G030
Black Holes Escape velocity Event horizon Black hole parameters
Presentation transcript:

Measuring the SPIN of Black Holes Andy Fabian Institute of Astronomy University of Cambridge

Astrophysical Black Holes have only MASS and SPIN (like elementary particles, except BH can have any mass )

BLACK HOLES Karl Schwarzschild Roy Kerr

MASS can be measured over wide range of radii but SPIN requires measuring properties at small radii What effects are characteristic of small radii around a Black Hole?

Strong Gravity Effects Gravitational redshift Gravitational light bending Dragging of inertial frames in Kerr metric (ISCO depends on BH spin)

GPS GR=45microsec/day (or ~10km/day)

GRAVITATIONAL LIGHT BENDING

Information from spectra and variability X-ray ‘reflection’ gives important clues in the spectrum Variability timescales and spectral changes show different spectral components

Reflection from photoionized matter (Ross & Fabian 93, 05) Also see Young+, Nayakshin+, Ballantyne+, Rozanska+, Dumont+

Fabian+89, Laor 90… Dovciak+04; Beckwith+Done05 Schwarzschild Kerr Fabian+89, Laor 90… Dovciak+04; Beckwith+Done05

MCG-6-30-15 Suzaku Red wing due to large gravitational redshift implying BH rapidly spinning Strength and behaviour of line implies GRAVITATIONAL LIGHT BENDING

Lockman Hole 800 ks XMM-Newton observation Hasinger

Lockman Hole 800 ks XMM-Newton observation Hasinger Streblyanskaya et al 2004

Radius of innermost stable circular orbit-ISCO Assumption: measurements of rISCO determine (or constrain) a

Probing Black Hole Spin

Light bending model in Kerr spacetime Miniutti et al 03; Miniutti & Fabian 04; earlier work by Martocchia, Matt+ see also Tsuebsuwong, Malzac+06

Armitage & Reynolds

SPIN also affects radiative efficiency of accretion, η

TNT Nuclear fusion Black Hole Accretion Max spin BH accretion

Accretion makes massive black holes Soltan 82 Mean redshift Radiative efficiency Light Mass density in BH η > 0.1 Observations Much of the radiation originates within 6Rg

Accretion makes massive black holes Soltan 82 Mean redshift Radiative efficiency Light Mass density in BH η > 0.1 Observations Most Massive BH are rapidly spinning