Active intermediate-mass black holes (MBH<106 Msun)

Slides:



Advertisements
Similar presentations
X-RAY NATURE of the LINER nuclear sources Isabel Márquez (IAA, Spain) 1. Introduction 2. The sample and the data 3. Reduction and analysis X-ray data:
Advertisements

AY202a Galaxies & Dynamics Lecture 14: Galaxy Centers & Active Galactic Nuclei.
The ubiquitous UV murmurs of sleeping supermassive BHs Dani Maoz With: Neil Nagar, Heino Falcke, Andrew Wilson.
Infrared Space Astrometry mission for the Galactic Bulge
Supermassive Black Holes in Radio-loud AGNs
The Phenomenon of Active Galactic Nuclei: an Introduction.
ACTIVE GALAXIES and GALAXY EVOLUTION
What can we learn on the BLR from the smallest AGN? Or, how do the BLR properties change with luminosity, and what is it telling us? Specifically The BLR.
Sean Farrell XMM-Newton Survey Science Centre University of Leicester, UK In collaboration with… N. Webb, D. Barret, O. Godet & B. Plazolles – CESR, France.
Active Galactic Nuclei Very small angular size: point like High luminosity: compared to host galaxies Broad-band continuum emission: radio to TeV Strong.
An XMM-Newton view of Q : an AGN without Broad Line Region? Mario Gliozzi (GMU) L. Foschini (IASF Bo) R. Sambruna (GSFC) L. Kedziora-Chudczer (Sidney)
COSPAR Workshop, Udaipur 2003 Active Galactic Nuclei : I Keith Arnaud NASA Goddard University of Maryland.
Disk Winds and Dusty Tori: Theory & Observations Moshe Elitzur University of Kentucky.
X-ray Bright, Optically Normal Galaxies - XBONGS Forman, Anderson, Hickox, Jones, Murray, Vikhlinin, Kenter and the Bootes Team Bootes Survey 9.3 sq. degrees.
How Do Supermassive Black Holes Get Starved? Q. D. Wang, Z. Y. Li, S.-K. Tang University of Massachusetts B. Wakker University of Wisconsin.
The Ultra-luminous X-Ray Sources Near the Center of M82 NTHU 10/18/2007 Yi-Jung Yang.
Active Galactic Nuclei Thomas Schlenker University of Washington Department of Physics PHYS 496 -What is an AGN? -What kinds of AGN’s are out there? -Unified.
Active Galactic Nuclei Ay 16, April 8, AGN DEFINITION PROPERTIES GRAVITATIONAL LENSES BLACK HOLES MODELS.
The Phenomenon of Active Galactic Nuclei: an Introduction.
Obscured AGN and XRB models Andrea Comastri (INAF-OABologna-Italy) Roberto Gilli (INAF-OABologna-Italy) F. Fiore (INAF-OARoma-Italy) G. Hasinger (MPE-Garching-
THE HST VIEW OF LINERS AND OTHER LOCAL AGN MARCO CHIABERGE CNR - Istituto di Radioastronomia - Bologna Alessandro Capetti (INAF-OATo) Duccio Macchetto.
The Evolution of AGN Obscuration
The Evolution of AGN Obscuration
Disk-outflow Connection and the Molecular Dusty Torus Moshe Elitzur University of Kentucky.
University of Leicester, UK X-ray and Observational Astronomy (XROA) Group Estelle Pons - The X-ray Universe June 2014.
Black Hole - Bulge Relation of High Redshift Quasars Xue-Bing Wu (Dept. of Astronomy, Peking University)
The Fundamental Plane of Quasars Timothy Scott Hamilton NASA/GSFC, National Research Council …Putting the “fun” back in “Fundamental Plane”!
NGC 3147: a 'true' type 2 Seyfert galaxy without the broad-line region THE X-RAY UNIVERSE Granada, May 28 th 2008 Stefano Bianchi A. Corral 1, F.
Growing black holes: from the first seeds to AGN Mar Mezcua Harvard-Smithsonian Center for Astrophysics T. Miyaji, F. Civano, G. Fabbiano, M. Karouzos,
The Differences in the SEDs of Type 1 and Type 2 AGNs: Contributions from starbursts Xue-Bing Wu Collaborator: Ran Wang (Astronomy Department, Peking University)
Galaxies with Active Nuclei Chapter 14:. Active Galaxies Galaxies with extremely violent energy release in their nuclei (pl. of nucleus).  “active galactic.
An alternative track of Black hole – galaxy co-evolution An alternative track of Black hole – galaxy co-evolution Smita Mathur The Ohio State University.
Black hole accretion history of active galactic nuclei 曹新伍 中国科学院上海天文台.
AGN Demographics Christine Black 3/1/12
Stellar Populations in the Central 10 pc of low-luminosity AGNs and Seyfert 2 Marc Sarzi (University of Hertfordshire, UK) In Collaboration with H.-W.
Active Galaxies Galaxies with extremely violent energy release in their nuclei (pl. of nucleus). → “Active Galactic Nuclei” (= AGN) Up to many thousand.
Nature of Broad Line Region in AGNs Xinwen Shu Department of Astronomy University of Science and Technology of China Collaborators: Junxian Wang (USTC)
J. Miguel Mas Hesse Elena Jiménez Bailón María de Santos Luis Colina Rosa González-Delgado When UV meets IR. Moriond 2005.
HMXB, ULX and star formation
A RULER FOR AGN in X-rays
Quasars: old black holes with young stars (?)
Yuichi Terashima (Ehime U.)
Virgo cluster survey with MXT
MODELS OF EMISSION LINE PROFILES AND SPECTRAL ENERGY DISTRIBUTIONS
AY202a Galaxies & Dynamics Lecture 14: AGN: The Unified Model
ASTR 1040 – November 30 Planetarium, December 5
The INTEGRAL NLSy1 FRANCESCA PANESSA The X-ray Universe 2011
XMM-NEWTON reveals a dipping black-hole X-ray binary in NGC 55
Why are Massive Black Holes Small in Disk Galaxies ?
GALAXIES!.
Paola Rodriguez Hidalgo High Energy Astrophysics
Active galaxies / Active galactic nuclei (AGN)
Chapter 21 Galaxy Evolution and Black Holes
The origin nuclear X-ray emission in the nuclei of radio galaxy-FR Is
Shuang-Nan Zhang, Yuan Liu, Jin Zhang Institute of High Energy Physics
Risolvere il Background X al suo picco
Black Hole Growth in the Local Universe
ACTIVE GALAXIES and GALAXY EVOLUTION
Note that the following lectures include animations and PowerPoint effects such as fly ins and transitions that require you to be in PowerPoint's Slide.
Active Galaxies General Description
QSO2 and their host galaxies
Black Holes in the Deepest Extragalactic X-ray Surveys
Suzaku discovery of a transient ultra-luminous X-ray source,
Galaxies With Active Nuclei
Group Nov. 01, USTC 4/18/2019 Group Nov. 01, USTC AGN-dominated SFG-dominated.
NOTES: Active Galactic Nuclei (AGN)
Galaxies With Active Nuclei
Radio-loud quasars in SDSS DR3
Suzaku Observation of Two Ultraluminous X-Ray Sources in NGC1313
Borislav Nedelchev et al. 2019
Presentation transcript:

Active intermediate-mass black holes (MBH<106 Msun) Population census, a case study & how to find more Mónica Valencia-S. I. Physikalisches Institut. Universität zu Köln In collaboration with: A. Eckart, J. Zuther, C. Iserlohe, M. Garcia-Marin, A. Zensus, S. Smajic, M. Vitale, G. Busch, S. Fisher, L. Moser, M. Bremer, C. Straubmeier

Over-classification vs. Unification SDSS J092600+442736 z=0.187. (c) SDSS Cen A .(c) NASA, CXC, CfA, R.Kraft+, MPIfR, ESO, WFI, APEX, A.Weis+ NGC 6240. (c) NASA, CXC, MIT, STSc I, C. Canizares, and M. Nowak Galactic Center. (c) NASA,CXC,MIT, F.Baganoff+ HE0450-2958 HE1239-2426 (c) NASA,ESA, F. Courbin, and P. Magain

Geometrical Unification of Active Galactic Nuclei (AGN) Low obscuration Broad Lines (10 000 km/s) + Narrow Lines (100 km/s) Type 1 BH Accretion Disk BLR Torus NLR Type 2 Obscuration (NH >1022 cm-2) Narrow Lines (100 km/s) Composed illustration. Originals (c) NASA/CXC/M.Weiss, K..Meisenheimer

Unification parameter 2? UV signature of SS disk “Big Blue Bump” Lbol/LEdd ~0.1 (BL AGN) High Accretion rate Thin disk BBB Broad lines Radio quietness QSOs Seyferts NLSy1s Advection Dominated / Radiatively Inefficient Accretion Flow Lbol/LEdd ~10-2.5 (no BLR) Low Accretion rate Thick disk (ADAF/RIAF) No BBB No Broad lines Radio loudness FR I sources LINERs LLAGNs Trump + 2011. see also Nicastro 200, Elitzur &Ho 2009

IRAS 01072+4954 in brief IRAS 01072+4954 Low-luminosity AGN (LLAGN) Starburst galaxy: ~5 Msun/yr Pseudo-bulge <--Secular evolution Unobscured Sy2: LX(2-10keV)= 1041.5 erg/s NH < 4.0 x 1020 cm-2 Low-mass black hole: MBH ~ 105Msun High accretion rate: Lbol~1042.5 erg/s, m~0.2 FWHMbroad lines~500 km/s LBT/LUCI. Infrared: K-band. Courtesy: J. Zuther No Broad lines in optical, no FeII GEMINI/NIFS 3’’x3’’ Field-Of-View

Unification parameter 2? Lbol/LEdd ~0.1 (BL AGN) High Accretion rate Thin disk BBB Broad lines Radio quietness QSOs Seyferts NLSy1s Lbol/LEdd ~10-2.5 (no BLR) Low Accretion rate Thick disk (ADAF/RIAF) No BBB No Broad lines Radio loudness FR I sources LINERs LLAGNs Trump + 2011. see also Nicastro 200, Elitzur &Ho 2009

Brγ λ 2.164 μm F(Brγ) = 1.0 x 10-16 erg s-1 cm-2 FWHM(Brγ) = 420 km/s S/N~2.8 IRAS 01072+4954 BH Accretion: Lbol/LEdd~0.2 M ~ 4.4 x 10-4 Msun/yr Broad Line Region: rBLR ~ 1 light-day ≈ 105 RS F(Hα) = (1.7 - 4.8) x 10-14 erg s-1 cm-2 FWHM(Hα) = 430 – 600 km/s F(Brγ) ≈ F(Hα) / 100

Unification parameter 2? Lbol/LEdd ~0.1 (BL AGN) BL AGN Stern & Laor 2012 Lbol/LEdd ~10-2.5 (no BLR) LINER 1s Trump + 2011. see also Nicastro 200, Elitzur &Ho 2009 Younes+ 2012

Unification parameter 3? Sy1 Sy2 Singh+,2011 TrueSy2 candidates Laor,2003 IMBH & NLSy1 Dewegan+,2008 Low Mass Sy2 Carol+,2009 LEdd

Unification parameter 3? Sy1 Sy2 Singh+,2011 TrueSy2 candidates Laor,2003 IMBH & NLSy1 Dewegan+,2008 Low Mass Sy2 Carol+,2009 IRAS01072

Unification parameter 3? Radio Loud NLSy1 Foschini (2013)

Unification parameter 3? Radio Loud NLSy1 Foschini (2013) Jet (radio) vs. disk luminosity in BHs Foschini (2012) IRAS01072

Why are IMBHs important?

Why to study IMBHs? IMBHs are the connection between SMBHs and stellar BHs

Why to study IMBHs? IMBHs are the connection between SMBHs and stellar BHs IMBHs are fundamental to probe models of SMBH seeds Greene 2012

Why to study IMBHs? IMBHs are the connection between SMBHs and stellar BHs IMBHs are fundamental to probe models of SMBH seeds IMBHs are the most active population of BHs in the local universe (dowinsizing) IMBHs seem to be in an early stage of evolution, therefore they can help on understanding how BHs grow

Why to study IMBHs? IMBHs are the connection between SMBHs and stellar BHs IMBHs are fundamental to probe models of SMBH seeds IMBHs are the most active population of BHs in the local universe (dowinsizing) IMBHs seem to be in an early stage of evolution, therefore they can help on understanding how BHs grow IMBHs seem to reside in young galaxies (starbursts), therefore they are important to recognize the nature of the star formation – AGN relation IMBHs seem to prefer spiral galaxies with bars or pseudobulges, therefore they might probe a different type of BH fueling IMBHs show signatures that might allow to probe the metal enrichment of the BLR in AGNs

How many IMBHs have been detected? Extracted from: Hubble Ultra Deep Field. (c) NASA/ESA/S. Beckwith(STScI) and The HUDF Team.

From optical observations Population census From optical observations SDSS DR7 Stern & Laor 2011: 106<MBH<109.5 10-3<Lbol/LEdd<1 SDSS DR4 Dong+2012: 8x104<MBH<2x106  3% are LINER 1 3% host an AGN 3% host an AGN

From optical observations Population census From optical observations SDSS DR7 Stern & Laor 2011: 106<MBH<109.5 10-3<Lbol/LEdd<1 SDSS DR4 Dong+2012: 8x104<MBH<2x106  3% are LINER 1 3% host an AGN 3% host an AGN From X-rays: Desroches & Ho 2009, Ghosh+ 2008 M*,gal<1010Msun 20% - 25 % Lx >2.3x1038 erg/s

From optical observations From multiwavelength campaigns Population census From optical observations From multiwavelength campaigns SDSS DR7 Stern & Laor 2011: 106<MBH<109.5 10-3<Lbol/LEdd<1 SDSS DR4 Dong+2012: 8x104<MBH<2x106  3% are LINER 1 Foschini 2011: From 76 NLSy1  46 radio loud  30 radio quiet From 49 RLNLSy1  12 γ-emitters 3% host an AGN 3% host an AGN From X-rays: ~ 310 low-mass BH (z<0.35) Desroches & Ho 2009, Ghosh+ 2008 M*,gal<1010Msun 20% - 25 % Lx >2.3x1038 erg/s

How to find more IMBHs?

From optical observations How to find more? From optical observations Problems: - Obscuration - Dilution of the AGN by the stellar continuum LAGN,B Lbol/LEdd (M*,gal / Lgal,B) B Lhost,B 0.1 (Msun/Lsun) T B/T : ratio stellar mass of the bulge to total stellar mass = NGC 4395. (c) Cord Scholz For maximal accreting BHs: LAGN/Lhost (Sa) ~ 45 LAGN/Lhost (Sc) ~ 7

From optical observations How to find more? From optical observations Problems: - Obscuration - Dilution of the AGN by the stellar continuum LAGN,B Lbol/LEdd (M*,gal / Lgal,B) B Lhost,B 0.1 (Msun/Lsun) T B/T : ratio stellar mass of the bulge to total stellar mass = LAGN Lhost α MBH MBH M*,bulge ~ 0.001

How to find more? MBH – M*,bulge relation log (MBH) = -1.0 (MK + 22.5) + 7.55 Valencia-S+ 2012 IRAS 01072 Graham+2012 IRAS 01072

How to find more? MBH – LK,bulge relation log (MBH) = -1.0 (MK + 22.5) + 7.55 Valencia-S+ (Jun.) 2012 IRAS 01072 log (MBH) = -1.09 (MK + 22.5) + 7.39 Graham & Scott (Dec.) 2012

From optical observations How to find more? From optical observations Problems: - Obscuration - Dilution of the AGN by the stellar continuum LAGN,B Lbol/LEdd (M*,gal / Lgal,B) B Lhost,B 0.1 (Msun/Lsun) T = For MBH > 7x107 Msun: For IMBHs with 105 Msun < MBH < 106 Msun: MBH M*,bulge ~ 0.001 MBH M*,bulge ~ 10-5 – 10-4

From X-ray observations How to find more? From X-ray observations A max. accreting BH with MBH=105 Msun: LEdd = 1043 erg/s  LX(2-10kev) ~ 1042 erg/s

From X-ray observations How to find more? From X-ray observations A max. accreting BH with MBH=105 Msun: Like IRAS 01072 (z=0.0236): MBH~105 Msun Lbol/LEdd ~ 0.2 FX(2-10keV)=3.1 x 10-13 erg s-1 cm-2 Chandra (~ 25 ks) LEdd = 1043 erg/s  LX(2-10kev) ~ 1042 erg/s Sensitivity limit Chandra (2-10keV): FX~ 10-15 erg s-1 cm-2 (~ 20ks)  not detectable z > 0.2

From X-ray observations How to find more? From X-ray observations A max. accreting BH with MBH=105 Msun: Like IRAS 01072 (z=0.0236): MBH~105 Msun Lbol/LEdd ~ 0.2 FX(2-10keV)=3.1 x 10-13 erg s-1 cm-2 Chandra (~ 25 ks) LEdd = 1043 erg/s  LX(2-10kev) ~ 1042 erg/s Sensitivity limit Chandra (2-10keV): FX~ 10-15 erg s-1 cm-2 (~ 20ks)  not detectable z > 0.2 IMBHs: 105 Msun < MBH < 106 Msun Dong+2013 42/49 detections (S/N>3) z < 0.08 (D < 350 Mpc) FX(2-10keV) > 10-14 erg s-1 cm-2

From X-ray observations How to find more? From X-ray observations Stellar BH with MBH~ 10 Msun: LEdd = 1039 erg/s  LX(2-10kev) ~ 1038 erg/s Threshold on the Eddington ratio of IMBHs: Artist impression. (c)ESO/ L.Casada LX(AGN)min ~ 1040 erg/s For MBH = 105 Msun  Lbol/LEdd ~ 0.001

There is still some hope From Infrared observations Volume-weighted space density of active SMBH in the local Universe Goulding+ 2010

Thanks!