- AGN feedback in action?

Similar documents
AGN winds and outflows

AGN feedback. Nadia Zakamska & Rachael Alexandroff Johns Hopkins University

UNRAVELLING THE COMPLEX STRUCTURE OF AGN-DRIVEN OUTFLOWS: II. PHOTOIONIZATION AND ENERGETICS

The Connection between Major Galaxy Mergers, Black Hole Growth and Galaxy Evolution from Multiwavelength Observations Ezequiel Treister

arxiv: v1 [astro-ph.ga] 24 Oct 2017

Connection between AGN and Star Formation activities, or not?

Co-evolution of galaxies and central black holes: Extended emission-line region around quasars

Black Holes and Active Galactic Nuclei

Active Galactic Nuclei

The parsec scale of. ac-ve galac-c nuclei. Mar Mezcua. International Max Planck Research School for Astronomy and Astrophysics

Circumnuclear Gaseous Kinematics and Excitation of Four Local Radio Galaxies

Thaisa Storchi Bergmann Instituto de Física, UFRGS, Porto Alegre, RS, Brazil

The Narrow-Line Region of Narrow-Line Seyfert 1 Galaxies

Evidence for AGN impact on star formation in (unresolved) galaxy populations

Introduction and Motivation

Luminous radio-loud AGN: triggering and (positive?) feedback

Measuring star formation in galaxies and its evolution. Andrew Hopkins Australian Astronomical Observatory

Revealing new optically-emitting extragalactic Supernova Remnants

Observational evidence for AGN feedback throughout the cosmic epochs. Roberto Maiolino

Nuclear Star Formation, The Torus, & Gas Inflow in Seyfert Galaxies

Gemini IFU Observations of Feedback from Radio-Quiet Quasars at z~0.5

Luminous Quasars and AGN Surveys with ELTs

Connection between phenomenon of active nucleus and disk dynamics in Sy galaxies

The Chandra Survey of Outflows in AGN with Resolved Spectroscopy (SOARS)

Star Formation Indicators

Multi-wavelength Surveys for AGN & AGN Variability. Vicki Sarajedini University of Florida

Active Galactic Nuclei - Zoology

Junfeng Wang, G. Fabbiano, G. Risaliti, M. Elvis, M. Karovska, A. Zezas (Harvard CfA/SAO), C. G. Mundell (Liverpool John Moores University, UK), G.

Multi-Phase Outflows in ULIRGs

Mpc scale effects on the inner pcs of galaxies

Revealing powerful outflows in z~1.5 obscured QSOs

AGN-driven turbulence revealed by extreme [CII]158µm line cooling in radio-galaxies

A TALE OF TWO MONSTERS: EMBEDDED AGN IN NGC6418 AND IRAS

Demographics of radio galaxies nearby and at z~0.55. Are radio galaxies signposts to black-hole mergers?

Jens Melinder. With financial support from CNES/CNRS convention #

The overall uncertainty of single-epoch virial black hole mass estimates and its implication to the M BH -σ relation

Spatially Resolved Kinematics of Binary Quasar Candidates

Methods of Measuring Black Hole Masses: Reverberation Mapping. Misty C. Bentz Georgia State University

Exploring the Origin of the BH Mass Scaling Relations

Physical properties of high-z star-forming galaxies with FMOS-COSMOS

3D Spectroscopy to Dissect Galaxies Down to Their Central Supermassive Black Holes. Kambiz Fathi. Stockholm University, Sweden

Quasars ASTR 2120 Sarazin. Quintuple Gravitational Lens Quasar

Neon Emission in HST Emission- Line Galaxies at z 2. Greg Zeimann

Active Galaxies & Emission Line Diagnostics

Determining Stellar Velocity Dispersion in Active Galaxies: Is the [OIII] Width a Valid Surrogate?

Stellar Populations: Resolved vs. unresolved

AGN feedback and the connection to triggering

Ionized gas kinematics in local active galaxies: a comprehensive view of inflows and outflows.

Introduction to AGN. General Characteristics History Components of AGN The AGN Zoo

A mid and far-ir view of the star formation activity in galaxy systems and their surroundings

Quasar Feedback in Galaxies

Observing the Formation of Dense Stellar Nuclei at Low and High Redshift (?) Roderik Overzier Max-Planck-Institute for Astrophysics

Multiwavelength signatures of AGN feedback in local AGN

Energy Sources of the Far IR Emission of M33

The Peculiar Case of Was 49b: An Over-Massive AGN in a Minor Merger?

Rest-frame Optical Spectra: A Window into Galaxy Formation at z~2

Orianne ROOS CEA-Saclay Collaborators : F. Bournaud, J. Gabor, S. Juneau

Astronomy c ESO 2016

Co-evolution of galaxies and black holes?

Paul Sell. University of Wisconsin-Madison Advisor: Christy Tremonti

The Evolution of BH Mass Scaling Relations

Optical polarization from AGN

Black Hole and Host Galaxy Mass Estimates

AGN Central Engines. Supermassive Black Holes (SMBHs) Masses and Accretion Rates SMBH Mass Determinations Accretion Disks

Thus Far. Intro / Some Definitions Hubble Classification Components of Galaxies. Specific Galaxy Types Star Formation Clusters of Galaxies

The Phenomenon of Active Galactic Nuclei: an Introduction

Radio AGN feedback on galaxy scales: What can Athena show us?

Coronal geometry at low mass- accretion rates from XMM and NuSTAR spectra. Felix Fürst Caltech for the NuSTAR AGN physics and binaries teams

X-raying galactic feedback in nearby disk galaxies. Q. Daniel Wang University of Massachusetts

Chien-Ting Chen! Dartmouth College

Measuring Black Hole Masses in Nearby Galaxies with Laser Guide Star Adaptive Optics

Compact Starbursts: Extreme Star Formation and Feedback at High Density Aleks Diamond-Stanic Grainger Fellow, University of Wisconsin

Fermi Bubbles: echoes of the last quasar outburst?

Roberto Soria (UCAS) Jets and outflows from super-eddington sources

Anatomy of an X-ray detected cluster at z = 2: low metallicities and enhanced specific star formation rates in star-forming galaxies.

Hunting for feeding and feedback signatures in a sample of hard X-ray selected NLS1

The Monster Roars: AGN Feedback & Co-Evolution with Galaxies

Astrophysical Quantities

Gas Masses and Gas Fractions: Applications of the Kennicutt- Schmidt Law at High Redshift

arxiv: v2 [astro-ph.ga] 27 May 2016

Probing the End of Dark Ages with High-redshift Quasars. Xiaohui Fan University of Arizona Dec 14, 2004

Clustering studies of ROSAT/SDSS AGN through cross-correlation functions with SDSS Galaxies

Studying Merger Driven BH Growth with Observations of Dual AGN

Observations of galaxy evolution. Pieter van Dokkum

HI clouds near the Galactic Center:

AGN Feedback at the Parsec Scale

Today. Practicalities

Halo Gas Velocities Using Multi-slit Spectroscopy

A zoo of transient sources. (c)2017 van Putten 1

Probing the Origin of Supermassive Black Hole Seeds with Nearby Dwarf Galaxies. Amy Reines Einstein Fellow NRAO Charlottesville

Radio emission from galaxies in the Bootes Voids

AST Cosmology and extragalactic astronomy. Lecture 20. Black Holes Part II

CALIFA galaxy dynamics across the Hubble sequence

Nuclear X-ray Emission and Mass Outflow From Broad Lined Radio Galaxies (Lorentz Center, Leiden 2009)

A Unified Model for AGN. Ryan Yamada Astro 671 March 27, 2006

Compact Obscured Nuclei in the ALMA era

A galaxy without its SMBH: implications for feedback

Krista Lynne Smith M. Koss R.M. Mushotzky

Spatially-Resolved Molecular Gas, Dust and Star Formation in Early-Types

Gas and stars in compact (young) radio sources

Transcription:

Gas outflows and star formation in type 2 AGNs - AGN feedback in action? Jong-Hak Woo (Seoul National Univ.) & Hyun-Jin Bae, Donghoon Son, Marios Karouzos Muse view of OIII outflows in NGC 7582 (Juneau+16 in prep.) OIII gas kinematics (Woo+16a)

Gas outflows AGN feedback? How common? Ionized gas outflows detected over galaxy scales (~1-10 kpc). (e.g., Nesvadha+07, Harrison+14, Karouzos+16a, Husemann+16). Suppress or trigger SF? AGN feedback mechanism? (e.g., Greene+12, Liu+13, Cresci+15, Vilar-Martin+16, Karouzos+16b).

Gas outflows AGN feedback? How common? Ionized gas outflows detected over galaxy scales (~1-10 kpc). (e.g., Nesvadha+07, Harrison+14, Karouzos+16a, Husemann+16). Suppress or trigger SF? AGN feedback mechanism? (e.g., Greene+12, Liu+13, Cresci+15, Vilar-Martin+16, Karouzos+16b). Important to investigate outflows in BH-galaxy evolution The M-sigma relation of active and inactive galaxies (e.g., Woo et al. 2015) σ * (km/s)

Gas outflows AGN feedback? How common? Ionized gas outflows detected over galaxy scales (~1-10 kpc). (e.g., Nesvadha+07, Harrison+14, Karouzos+16a, Husemann+16). Suppress or trigger SF? AGN feedback mechanism? (e.g., Greene+12, Liu+13, Cresci+15, Vilar-Martin+16, Karouzos+16b). Important to investigate outflows in BH-galaxy evolution Outflow demography based on a large sample is needed to understand outflows as a population (e.g., Boroson+05, Komossa 08, Zhang+11, Crenshaw+10, Wang+11, Mullaney+13).

Gas outflow studies at SNU 1. Outflow census: how strong, how common, relation to AGN energetics (Bae & Woo 14, Woo+16a) 2. Outflow model simulations: intrinsic properties of outflows - Talk by H.-J. Bae (Bae & Woo 16) 3. Connection to star formation: positive or negative feedback? (Woo+16b in prep.) 4. IFU follow-ups of AGNs with/without strong outflows (Karouzos+16a, Karouzos+16b, Bae+16b in prep.)

Statistical sample of AGNs and SF galaxies at z<0.3 We selected AGNs and SF galaxies with well-defined emission lines from SDSS (A/N>5). type N pure AGNs ~23,000 composite obj. ~16,000 SF galaxies ~69,000 For each AGN, we subtract stellar population model, and measure systemic velocity and stellar velocity dispersion (σ * ). Flux density 140 50 20 120 10 100 80 60 40 40 30 0 485048554860486548704875 00016 (z=25159142) 120 100 8 80 6 60 4 40 2 20 0 0 498049905000501050205030 628062906300631063206330 200 150 100 50 0 6540 6560 6580 6600 20 0 4000 5000 6000 7000 Rest-frame wavelength

[OIII] λ5007 traces ionized gas outflows. ~44% of AGNs have a broad wing in OIII, representing outflows. - Outflows are common. Hβ [OIII] We measure flux-weighted velocity (1 st moment), then calculate vel. shift (V OIII ) w.r.t systemic velocity. We measure vel. dispersion (σ OIII 2 nd moment), and compare with stellar VD. flux (10-16 erg/s/cm 2 /A ) H +[NII] [SII] wavelength (A )

OIII VD (σ OIII ) correlates with AGN luminosity. OIII kinematics are related to AGN energetics. For SF galaxies, no strong trend between L OIII and σ OIII Woo+16b (to be submitted)

σ OIII is larger than σ *, indicating non-virial motion. σ OIII correlates with stellar VD (σ * ), indicating galaxy gravitational potential plays a role (e.g., Nelson & Whittle 1995). σ OIII > σ *, indicating presence of non-gravitational kinematics (i.e., outflows). stellar VD log σ * (km/s) Woo+16a,b

Non-grav. component is comparable to grav. component For AGNs without OIII wing, gas and stellar kinematics are similar. For AGN with OIII wing, σ OIII is larger than σ * by a factor of 1.3-1.4, indicating σ non-gr ~ σ gr. single Gaussian [O III] double Gaussian [O III] < log (σ [O III] /σ * ) > 0.1 0.1 Seyfert only AGN AGN + composite 38 39 40 41 42 log L [O III] (erg s 1 ) σ OIII 2 = σ non-gr 2 + σ gr 2 = σ non-gr 2 + σ * 2 Woo+16a

Outflow fraction dramatically increases with AGN energetics Fraction of AGN with OIII wing dramatically increases with L and L/ L Edd, indicating that outflows are prevalent among high-l AGNs. Fraction of double Gaussian [O III] Seyfert only AGN AGN + composite Woo+16a 39 40 41 42 43 3 2 1 log L [O III] (erg s 1 ) log (L bol /L Edd )

Gas outflows are prevalent in AGNs. σ [O III] /σ * > detectable outflows Over all luminosity range, at least 50% of AGNs have outflows (i.e., σ OIII > σ * ). ~50% of high-l AGNs have extreme outflows (i.e., σ OIII > 1.4 σ * ). Fraction σ [O III] /σ * > 1.4 Seyfert only AGN AGN + composite extreme outflows The majority of high-l AGNs show strong outflow signature (see also Boroson+05, Crenshaw+10, Wang+11, Mullaney+13). 38 39 40 41 42 3 2 1 log L [O III] (erg s 1 ) log (L bol /L Edd ) Woo+16a

VVD (vel.-vel. dispersion) diagram reveals extreme gas kinematics VVD distribution is clearly different between AGNs and SF galaxies. σoiii (km/s) VOIII (km/s) Woo+16b in prep.

Luminosity dependence of VVD distribution VVD distribution expands with AGN luminosity. Outflow kinematics are connected to AGN radiation (AGN-driven). σoiii (km/s) VOIII (km/s) Woo+16b

Gas outflows do not depend on radio luminosity σ OIII increases with L radio, reflecting grav. potential. However, once normalized by σ *, there is no correlation. For most AGNs, ionized gas outflows are not directly related to radio activity. V OIII shows similar trend. Woo+16a V OIII (km/s) log σ OIII / σ * log σ OIII (km/s) log L 1.4GHz (erg/s) log (L 1.4GHz /L opt )

3-D outflow simulations (talk by H.-J. Bae) Bi-cone + dust disk (intrinsic velocity, opening angle, inclination of the cone, inclination of dust disk) Projected 2-D V OIII & σ OIII maps (calculated through each line of sight) Calculate flux-weighted V OIII & σ OIII Log flux velocity velocity dispersion Dust disk: -60 degree Bae & Woo 16 ApJ, in press

MC simulations of VVD diagram (talk by H.-J. Bae) Using random distribution of orientation angle of the bicone, dust plane, and intrinsic velocity, we simulated the VVD diagram. Dust extinction plays an important role. The intrinsic velocity ranges from ~200 to ~2,000 km/sec. Bae & Woo 16, ApJ, in press

AGN have lower SFR compared to SF galaxies (optical & X-ray) AGNs have lower SSFR than main sequence galaxies. AGNs feedback? Evolutionary sequence? stellar mass (M sun ) Shimizu+15 Ellison+16

SSFR correlates with outflow kinematics AGNs with outflow signatures have similar SSFR compared to SF galaxies. AGNs with no outflows have much lower SSFR. Woo+16b to be submitted

AGNs with no outflow have lower SSFR. log σ [O III] /σ * > 0.3 strong outflows All mass SF galaxies AGNs with strong outflows have similar SSFR compared to SF galaxies. No suppression, no enhancement. AGNs with no outflows show much lower SSFR. Woo+16b to be submitted Normalized number < log σ [O III] /σ * < 0.3 weak outflows log σ [O III] /σ * < no outflows -2.0-1.5 - -0.5 0.5 log SSFR (yr -1 )

All mass Low-Eddington AGNs have lower SSFR log L bol /L Edd > -2 high-edd. SF galaxies High-Eddington AGNs have similar SSFR compared to SF galaxies. Low-Eddington AGNs have much lower SSFR. Normalized number -3 < log L bol /L Edd < -2 Intermed. mid-ir selected AGNs = high low-edd. log L bol /L Edd < -3 Eddington AGNs Woo+16b to be submitted -2.0-1.5 - -0.5 0.5 log SSFR (yr -1 )

Delayed AGN feedback or gas depletion? high Eddington + strong outflow + MS SFR vs. low Eddington + no/weak outflow + low SFR All mass log σ [O III] /σ * > 0.3 All mass log L bol /L Edd > -2 Delayed AGN feedback? 1. Gas supply: AGN and SF coexist (Netzer 09) 2. Outflows impact on ISM after dynamical time scale (10 6-7 yrs) 3. Decrease SFR and AGN activity (low Eddington, no outflows) Normalized number < log σ [O III] /σ * < 0.3 log σ [O III] /σ * < Normalized number -3 < log L bol /L Edd < -2 log L bol /L Edd < -3 Transition due to gas depletion -2.0-1.5 - -0.5 0.5 log SSFR (yr -1 ) -2.0-1.5 - -0.5 0.5 log SSFR (yr -1 )

Gemini GMOS-IFU Follow up Hα OIII (Karouzos+16a;16b, submitted) OIII shows outflow kinematics while Hα shows rotation.

Gemini GMOS-IFU Follow up Hα OIII (Karouzos+16a;16b, submitted) SF ring is present at the edge of outflow region.

Summary Gas outflows are prevalent among local AGNs, based on 1) the presence of a broad wing component in OIII, and 2) based on the non-gravitational component (σ OIII > σ * ). In particular, the majority of high-l AGNs show strong outflows. OIII vel. & vel. disp. increase with AGN luminosity, suggesting that outflows are linked to AGN energetics. Ionized gas outflows are not related to radio activity. AGNs with strong outflows follow the SF main sequence while AGNs with no outflows have much lower SSFR, implying delayed AGN feedback.