Evolution of the Highest Redshift Quasars

Size: px
Start display at page:

Download "Evolution of the Highest Redshift Quasars"

Transcription

1 Evolution of the Highest Redshift Quasars Xiaohui Fan University of Arizona Collaborators: Becker, Bertoldi, Carilli, Cox, Diamond-Stanic, Hennawi, Ivezic, Jiang, Kelly, Richards, Schneider, Strauss, Vestergaard, Walter, Wang, White, SDSS collaboration

2 What have changed in quasar properties since z~6? Luminous, normal looking quasars existed at z>6, half Gyr after the first star-formation Timescale for formation of the first billion-m sun BH? Timescale for the establishment of AGN structure: do quasar spectra at z~6 really look the same as at z~0? Timescale for the establishment of M-sigma relation? Study of quasar evolution needs: Large survey to increase sample size Deep survey to break redshift/luminosity degeneracy Multiwavelength study to probe different scales of AGN structure

3 Outline Update on high-redshift quasar searches Quasar luminosity function and BH mass function Evolution in accretion properties? Quasar SEDs at high-redshift First signs of cosmic evolution? Star-formation and dust in quasar host galaxies Evolution of M-sigma relation? Summary

4 The Highest Redshift Quasars Today z>4: >1000 known z>5: >60 z>6: 13 (12 SDSS discoveries) SDSS i-dropout Survey: Current Status: >7000 deg 2 23 luminous quasars at 5.7<z<6.4 By this June: Completion of a colorselected flux-limited sample of luminous high-z quasars in the entire SDSS highlatitude area (~8000 deg 2 )

5 The Highest Redshift Quasars Today Other on-going z~6 quasar surveys: AGES (Cool et al.): Spitzer selected, one quasar at z=5.8 FIRST-Bootes (Becker et al.): radio selected, one quasar at z=6.1 QUEST, CFHT: i-dropout surveys similar to SDSS Future IR-based survey: UKIDSS, VISTA, allows detection up to z~8-9. SDSS 2 : faint quasars in the deep SDSS stripe (Jiang, XF et al.), ~10-30 additional z~6 quasars in next three years (three z~6 quasar in pilot obs)

6

7 redshift Lyα forest 46,420 Quasars from the SDSS Data Release Three Lyα CIV CIII MgII 1 FeII FeII 0 OIII 4000 A wavelength 9000 A Hα

8 Quasar Density at z~6 From SDSS i-dropout survey Density declines by a factor of ~40 from between z~2.5 and z~6 Cosmological implication M BH ~ M sun M halo ~ M sun rare, 5-6 sigma peaks at z~6 (density of 1 per Gpc 3) Assembly of massive dark matter halo environment? Assembly of supermassive BHs? Fan et al. 2004

9 Simulating z~6 Quasars z=6.2 z=0 Dark matter galaxy Springel et al The largest halo in Millennium simulation (500 Mpc cube) at z=6.2 Virial mass 5x10 12 M_sun Stellar mass 5x10 10 M_sun Resembles properties of SDSS quasars Such massive halos existed at z~6, but.. How to assemble such mass BHs and their host galaxies in less than 1Gyr?? The universe was ~20 t edd old Initial assembly from seed BH at z>>10 Low radiative efficiency or massive seed BH Little or no feedback to stop BH/galaxy growth

10 Evolution of Quasar LF Shape Richards, et al.; Fan et al High-z quasar LF different from low-z Bright-end slope of QLF is a strong function of redshift Transition at z~2.5 (where quasar density peaks in the universe) Different formation mechanism at low and high-z? Faint quasar surveys needed!

11 Probing the Evolution of Faint Quasar SDSS Southern Deep Spectroscopic Survey 270 deg along Fall Equator in the Southern Galactic Cap Down to ~25 mag in SDSS bands with repeated imaging Spectroscopic follow-up using 300-fiber Hectospec spectrograph on 6.5-meter MMT Reaches AGN luminosity at z~2.5 Few hundred faint quasars at z> at z~6 Status after Year One: Large number of z>3 quasar to probe LF evolution Three z~6 quasar to demonstrate target selection

12 BH mass determination at high-z CIV Upper Limit? Fan et al. >1000 quasars at z>3 McLure et al. SDSS DR 1 Virial BH mass estimate using optical spectra: Emission line width to approximate gravitational velocity Bolometric luminosity vs. BLR size scaling relation Accurate to a factor of 3-5 locally Applying virial method to high-z (Vestergaard et al.) Lack of spectral evolution in highredshift quasars quasar BH estimate valid at high-z Using Hβ MgII and CIV for different redshift ranges BH mass at high-z: M sun existed at z~6 Upper envelop of BH mass at several M sun? Negative feedback?

13 BH mass distribution Mass L BOL L BOL /L Edd SDSS: DR3 Vestergaard, XF et al. in prep.

14 Evolution of Eddington Ratio Luminous quasars at all redshifts have L bol /L edd ~ Luminosity dependence (expected) L bol /L edd ~ 1 at several L * Redshift dependence: At constant luminosity: L bol /L edd increase by ~3 from z=1 to z=5 At z>4, all quasars basically shining at Eddington Next step: Full MF Extend to low-l To what extent is quasar evolution driven by accretion rate changes? Vestergaard, XF et al. in prep.

15 The Lack of Evolution in Quasar Emission Line Properties Ly a Ly a forest NV OI SiIV Fan et al.2004 Rapid chemical enrichment in quasar vicinity Quasar env has supersolar metallicity : no metallicity evolution Does this lack of evolution in rest-frame UV also apply to other wavelength?

16 High Metallicity at high-z Strong metal emission consistent with supersolar metallicity NV emission multiple generation of star formation from enriched pops Fe II emission type II SNe some could be Pop III? Does this lack of evolution in rest-frame UV also apply to other wavelength? Barth et al Nagao et al. 2006

17 Quasar spectral energy distribution BLR hot dust Dust torus disk Spitzer Cool Dust in host galaxy

18 Evolution of Quasar SEDs: X-ray to radio To the first order, average SEDs of z~6 quasar consistent with low-z template However, detailed analysis might be indicating first signs of SED evolution: Dust properties (Spitzer and extinction) Fraction of radio-loud quasars X-ray - optical flux ratio? A population of lineless highz quasars? Jiang, XF et al. 2006a

19 Hot dust in z~6 Quasars Lack of evolution in UV, emission line and X-ray disk and emission line regions form in very short time scale But how about dust? Timescale problem: running out of time for AGB dust Spitzer observations of z~6 quasars: probing hot dust in dust torus (T~1000K) Two unusual SEDs among 13 objects observed. dust No hot dust?? Jiang, XF et al. 2006a

20 Where did the hot dust go? typical J μm 4.8μm 5.6μm J0005 (z=5.85): SED consistent with disk continuum only No similar objects known at low-z formation of the first dust? Larger sample 8.0μm Host dust contribution 24μm luminosity Jiang, XF 2006a

21 Supernova Dust in z~6 quasar? (Maiolino et al. 2004) SDSS J1048 (z=6.2) Highest-z Low-BAL Typical SED at near UV moderate dust But blue in far-uv SED suggesting unusual dust extinction Age of the universe < 1Gr No time for dust from evolved low intermediate mass stars Dust extinction produced by SN dust fits the data

22 Evolution of Radio-loudness Match all SDSS quasars to FIRST and NVSS catalog: For the whole fluxlimited sample, radioloud fraction doesn t strongly depend on luminosity or redshift However, this seems to be an artifact of marginal distribution Jiang, XF et al. 2006b

23 Radio-loud fraction is a strong function of luminosity and redshift Luminosity dependence: RLF ~ L 0.5 At z~1: RLF changes from 17% (M=-27) to 2% (M=-22) Redshift dependence: RLF ~ (1+z) -1.7 For M=-27: RLF changes from 17% (z=1) to 2% (z=5) log(radio-loud fraction) Log(1+z) Jiang, XF et al. 2006b Mi

24 X-ray properties: evolution? Studies of α ox as function of luminosity and redshift: Luministy dependence Strong degeneracy of L and z mild evolution at high-z? High-z quasars are X-ray bright? (Kelly et al.) No strong evolution? (Steffen et al.) Faint high-z quasars! Redshift dependence

25 Lineless quasars: radio quiet BL Lac or quasars with no BLR? No emission line, radio-quiet quasars at z>4 ~1% of high-z quasars No obvious low-z counterparts No BL Lac signature A separate population of quasars? Ly α distribution Lineless Quasars: EW(Lyα)<10 Log EW (Ly α) Diamond-Stanic et al Fan et al. 2006

26 Probing the Host Galaxy Assembly Dust torus Spitzer ALMA Cool Dust in host galaxy

27 Sub-mm and Radio Observation of High-z Quasars Probing dust and star formation in the most massive high-z systems Advantage: No AGN contamination Negative K-correction for both continuum and line luminosity at high-z Give measurements to Star formation rate Gas morphology Gas kinematics

28 Sub-mm Observations of High-z Quasars Using IRAM and SCUBA: ~30% of radio-quiet quasars at z>4 detected at 1mm (observed frame) at 1mJy level submm radiation in radio-quiet quasars come from thermal dust with mass ~ 10 8 M sun Among z~6 quasars: 5(+2)/19 detected in submm If dust heating came from starburst star formation rate of Arp M sun /year Support for star formation origin of FIR luminosity: z~6 quasars follow starburst galaxy FIR/radio relation No correlation between FIR and UV Heating source still open question Bertoldi et al.

29 Submm and CO observation of z=6.42 quasar: probing the earliest ISM Strong submm source: Dust T: 50K Dust mass: 7x10 8 M sun Strong CO source (multiple transitions) T kin ~ 100K Gas mass: 2x10 10 M sun n H2 ~ 10 5 Gas/dust, Temp, density typical of local SB Bertoldi et al.

30 [CII] detection of z=6.42 quasar [CII] 158μm line: Brightest ISM line Direct probe of SF region J1148 (z=6.42) Both [CII] and L FIR consistent with the brightest local ULIRGs SFR~ 10 3 M sum Mailino et al. 2005

31 High-resolution CO Observation of z=6.42 Quasar Spatial Distribution Radius ~ 2 kpc Two peaks separated by 1.7 kpc CO brightness similar to typical ULIRG SF core. Velocity Distribution CO line width of 280 km/s Dynamical mass within central 2 kpc: ~ M_sun Total bulge mass ~ M_sun < M-sigma prediction VLA CO 3 2 map 1 kpc BH formed before complete galaxy assembly? Channel Maps Walter et al km/s

32 M-σ relation at high-z Host mass from CO 15 CO detections at z>2 Line width all ~ km/s Taking at face value: Strong evolution of M-σ BH forms early Similar results from HST studies of lensed quasar host (Peng et al.) Caveats: Are luminous quasars biased? Are CO observations biased? Need detailed simulations of dust and gas properties of high-z quasar host galaxies Shields et al. 2006

33 Summary: High-z vs. Low-z Quasars LF and BH mass evolution: Flattening of luminosity/mass functions Billion solar mass BH existed at z~6 Average Eddington ratio might be increasing at high-z Are high-z and low-z quasars accreting differently? Spectral evolution: Little or no evolution in continuum/emission line properties Strong evolution in radio, Dust and X-ray properties might be evolving as well. Approaching the epoch of AGN structure formation? BH/galaxy co-evolution ISM of high-z quasar hosts similar to that of local ULIRGs narrow CO line width Large BH in small hosts at high-z? Wish list: 1. Larger sample and fainter quasars to break degeneracy 2. Better models/observations in dust/gas

34 z=6.42: Dust and Gas detection L_FIR = 1.2e13 L_sun, M_dust =7e8M_sun S_250 = 5.0 +/- 0.6 mjy M(H_2) = 2e10 M_sun GHz CO 3-2 Off channels Rms=60uJy Dust formation: 1.4e9yr (AGB winds) > t_univ (8.7e8yr) => dust formed in high mass stars? => silicate grains? C, O production (3e7 M_sun): few e8 yr => Star formation started early (z = 10)?

35 : Masses M(dust) = 7e8 M_sun M(H_2) = 2e10 M_sun M_dyn (r=2.5kpc) = 5e10 M_sun M_BH = 3e9 M_sun => M_bulge = 1.5e12 M_sun Gas/dust = 30, typical of starburst Dynamical vs. gas mass => baryon dominated? Dynamical vs. bulge mass => M σ breaks-down at high z? [SMBH forms first?]

36 : radio-fir SED Beelen et al. S_1.4= 55 +/- 12 ujy T_D = 50 K Star forming galaxy characteristics: radio-fir SED, Gas/Dust, CO excitation and T_B => Coeval starburst/agn? SFR = 1e3 M_sun/yr Stellar spheroid formation in few e7 yrs = e-folding time for SMBH => Coeval formation of galaxy/smbh at z = 6.4?

37 VLA imaging of CO3-2 at 0.4 and 0.15 resolution rms=50ujy at 47GHz CO extended to NW by 1 (=5.5 kpc) tidal(?) feature Separation = 0.3 = 1.7 kpc T_B = 20K Typical of starburst nuclei Merging galaxies?

38 IRAM Plateau de Bure ν 2 (6-5) (3-2) (7-6) FWHM = 305 km/s z = / T kin =100K, n H2 =10 5 cm -3 Typical of starburst nuclei (eg. NGC253, Arp220)

39 PSS J (z=4.12) CO Einstein ring Modeled by starforming disk with 2kpc radius CO line-width 280km/s BH Mass ~10^9 solar Star formation rate 900 solar mass/year 15 detections of CO at z>2 (5/6 known CO sources at z>4 are quasars) Carilli et al. 2003

40 PSS J (z=4.12) CO Einstein ring Modeled by starforming disk with 2kpc radius CO line-width 280km/s BH Mass ~10^9 solar Star formation rate 900 solar mass/year 15 detections of CO at z>2 (5/6 known CO sources at z>4 are quasars Carilli et al. 2003

41

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

Probing the End of Dark Ages with High-redshift Quasars. Xiaohui Fan University of Arizona Dec 14, 2004 Probing the End of Dark Ages with High-redshift Quasars Xiaohui Fan University of Arizona Dec 14, 2004 High-redshift Quasars and the End of Cosmic Dark Ages Existence of SBHs at the end of Dark Ages BH

More information

Evolution of high-redshift quasars

Evolution of high-redshift quasars New Astronomy Reviews 50 (2006) 665 671 www.elsevier.com/locate/newastrev Evolution of high-redshift quasars Xiaohui Fan Steward Observatory, The University of Arizona, Tucson, AZ 85721, USA Available

More information

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

Demographics of radio galaxies nearby and at z~0.55. Are radio galaxies signposts to black-hole mergers? Elaine M. Sadler Black holes in massive galaxies Demographics of radio galaxies nearby and at z~0.55 Are radio galaxies signposts to black-hole mergers? Work done with Russell Cannon, Scott Croom, Helen

More information

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

Probing the Origin of Supermassive Black Hole Seeds with Nearby Dwarf Galaxies. Amy Reines Einstein Fellow NRAO Charlottesville Probing the Origin of Supermassive Black Hole Seeds with Nearby Dwarf Galaxies Amy Reines Einstein Fellow NRAO Charlottesville Motivation: The origin of supermassive BH seeds Motivation: The origin of

More information

Black Holes and Active Galactic Nuclei

Black Holes and Active Galactic Nuclei Black Holes and Active Galactic Nuclei A black hole is a region of spacetime from which gravity prevents anything, including light, from escaping. The theory of general relativity predicts that a sufficiently

More information

Wagg ea. [CII] in ALMA SV 20min, 16 ants. 334GHz. SMA 20hrs

Wagg ea. [CII] in ALMA SV 20min, 16 ants. 334GHz. SMA 20hrs BRI1202-0725 z=4.7 HyLIRG (10 13 L o ) pair SFR ~ few 10 3 M o yr -1 4 + SMG + Salome ea. CO 5-4 + M H2 ~ 10 11 M o QSO + HST 814 Hu ea 96 SMA [CII] 158um 334GHz, 20hrs Iono ea 2007 [CII] in 1202-0725

More information

Empirical Evidence for AGN Feedback

Empirical Evidence for AGN Feedback Empirical Evidence for AGN Feedback Christy Tremonti MPIA (Heidelberg) / U. Wisconsin-Madison Aleks Diamond-Stanic (U. Arizona), John Moustakas (NYU) Much observational and theoretical evidence supports

More information

High Redshift Universe

High Redshift Universe High Redshift Universe Finding high z galaxies Lyman break galaxies (LBGs) Photometric redshifts Deep fields Starburst galaxies Extremely red objects (EROs) Sub-mm galaxies Lyman α systems Finding high

More information

IRS Spectroscopy of z~2 Galaxies

IRS Spectroscopy of z~2 Galaxies IRS Spectroscopy of z~2 Galaxies Houck et al., ApJ, 2005 Weedman et al., ApJ, 2005 Lutz et al., ApJ, 2005 Astronomy 671 Jason Marshall Opening the IR Wavelength Regime for Discovery One of the primary

More information

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

Observing the Formation of Dense Stellar Nuclei at Low and High Redshift (?) Roderik Overzier Max-Planck-Institute for Astrophysics Observing the Formation of Dense Stellar Nuclei at Low and High Redshift (?) Roderik Overzier Max-Planck-Institute for Astrophysics with: Tim Heckman (JHU) GALEX Science Team (PI: Chris Martin), Lee Armus,

More information

Formation of z~6 Quasars from Hierarchical Galaxy Mergers

Formation of z~6 Quasars from Hierarchical Galaxy Mergers Formation of z~6 Quasars from Hierarchical Galaxy Mergers Yuexing Li et al Presentation by: William Gray Definitions and Jargon QUASAR stands for QUASI-stellAR radio source Extremely bright and active

More information

Feeding the Beast. Chris Impey (University of Arizona)

Feeding the Beast. Chris Impey (University of Arizona) Feeding the Beast Chris Impey (University of Arizona) Note: the box is growing due to cosmic expansion but this is factored out. Heirarchical Structure Active Galactic Nuclei (AGN) Nuclear activity in

More information

A Monster at any other Epoch:

A Monster at any other Epoch: A Monster at any other Epoch: Are Intermediate Redshift ULIRGs the Progenitors of QSO Host Galaxies? Barry Rothberg Large Binocular Telescope Observatory/George Mason University Co-Is: J. Fischer (NRL),

More information

arxiv:astro-ph/ v1 23 Jul 2003

arxiv:astro-ph/ v1 23 Jul 2003 Astronomy & Astrophysics manuscript no. bertoldi j1148 July 23, 2003 (DOI: will be inserted by hand later) High-excitation CO in a quasar host galaxy at z = 6.42 F. Bertoldi 1, P. Cox 2, R. Neri 3, C.L.

More information

EVLA + ALMA represent > 10x improvement in observational capabilities from 1GHz to 1 THz

EVLA + ALMA represent > 10x improvement in observational capabilities from 1GHz to 1 THz What is EVLA? Build on existing infrastructure, replace all electronics (correlator, Rx, IF, M/C) => multiply ten-fold the VLA s observational capabilities 80x Bandwidth (8 GHz, full stokes), with 4000

More information

Active Galactic Nuclei - Zoology

Active Galactic Nuclei - Zoology Active Galactic Nuclei - Zoology Normal galaxy Radio galaxy Seyfert galaxy Quasar Blazar Example Milky Way M87, Cygnus A NGC 4151 3C273 BL Lac, 3C279 Galaxy Type spiral elliptical, lenticular spiral irregular

More information

Lecture 9. Quasars, Active Galaxies and AGN

Lecture 9. Quasars, Active Galaxies and AGN Lecture 9 Quasars, Active Galaxies and AGN Quasars look like stars but have huge redshifts. object with a spectrum much like a dim star highly red-shifted enormous recessional velocity huge distance (Hubble

More information

Galaxy Formation: The Radio Decade (Dense Gas History of the Universe) Chris Carilli (NRAO) Santa Fe, March 2011

Galaxy Formation: The Radio Decade (Dense Gas History of the Universe) Chris Carilli (NRAO) Santa Fe, March 2011 Galaxy Formation: The Radio Decade (Dense Gas History of the Universe) Chris Carilli (NRAO) Santa Fe, March 2011 Recombination (t univ ~ 0.4Myr) Power of radio astronomy: dust, cool gas, and star formation

More information

Galaxies with Active Nuclei. Active Galactic Nuclei Seyfert Galaxies Radio Galaxies Quasars Supermassive Black Holes

Galaxies with Active Nuclei. Active Galactic Nuclei Seyfert Galaxies Radio Galaxies Quasars Supermassive Black Holes Galaxies with Active Nuclei Active Galactic Nuclei Seyfert Galaxies Radio Galaxies Quasars Supermassive Black Holes Active Galactic Nuclei About 20 25% of galaxies do not fit well into Hubble categories

More information

Introduction and Motivation

Introduction and Motivation 1 Introduction and Motivation This last two days at this conference, we ve focused on two large questions regarding the role that AGNs play in galaxy evolution: My research focuses on exploring these questions

More information

Active Galactic Alexander David M Nuclei

Active Galactic Alexander David M Nuclei d.m.alexander@durham.ac.uk Durham University David M Alexander Active Galactic Nuclei The Power Source QuickTime and a YUV420 codec decompressor are needed to see this picture. Black hole is one billionth

More information

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

Luminous radio-loud AGN: triggering and (positive?) feedback Luminous radio-loud AGN: triggering and (positive?) feedback Clive Tadhunter University of Sheffield ASA, ESA, NRAO Collaborators: C. Ramos Almeida, D. Dicken," R. Morganti,T. Oosterloo, " R. Oonk, M.

More information

Dusty star-forming galaxies at high redshift (part 5)

Dusty star-forming galaxies at high redshift (part 5) Dusty star-forming galaxies at high redshift (part 5) Flow of story 4.1.1 4.1.2 4.1.3 Millimetric Spectroscopic Redshifts Millimetric Photometric Redshifts Redshift Distributions of 24 μm selected DSFG

More information

Galaxies 626. Lecture 10 The history of star formation from far infrared and radio observations

Galaxies 626. Lecture 10 The history of star formation from far infrared and radio observations Galaxies 626 Lecture 10 The history of star formation from far infrared and radio observations Cosmic Star Formation History Various probes of the global SF rate: ρ* (z) M yr 1 comoving Mpc 3 UV continuum

More information

High-z QSO (HSC #123)

High-z QSO (HSC #123) Jan. 6 th, 2016 HSC/AGN meeting Next DL = 21 April High-z QSO follow-up @mm/submm (HSC #123) - especially z > 6 objects - Takuma Izumi@IoA/UTokyo takumaizumi@ioa.s.u-tokyo.ac.jp This is a submm follow-up

More information

Quasars ASTR 2120 Sarazin. Quintuple Gravitational Lens Quasar

Quasars ASTR 2120 Sarazin. Quintuple Gravitational Lens Quasar Quasars ASTR 2120 Sarazin Quintuple Gravitational Lens Quasar Quasars Quasar = Quasi-stellar (radio) source Optical: faint, blue, star-like objects Radio: point radio sources, faint blue star-like optical

More information

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

Introduction to AGN. General Characteristics History Components of AGN The AGN Zoo Introduction to AGN General Characteristics History Components of AGN The AGN Zoo 1 AGN What are they? Active galactic nucleus compact object in the gravitational center of a galaxy that shows evidence

More information

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

Clustering studies of ROSAT/SDSS AGN through cross-correlation functions with SDSS Galaxies Clustering studies of ROSAT/SDSS AGN through cross-correlation functions with SDSS Galaxies Mirko Krumpe (ESO, UCSD) mkrumpe@eso.org Collaborators: Takamitsu Miyaji (UNAM-E, UCSD), Alison L. Coil (UCSD),

More information

Multiwavelength Study of Distant Galaxies. Toru Yamada (Subaru Telescope, NAOJ)

Multiwavelength Study of Distant Galaxies. Toru Yamada (Subaru Telescope, NAOJ) Multiwavelength Study of Distant Galaxies Toru Yamada (Subaru Telescope, NAOJ) Studying Galaxy Formation with ALMA 1. Studying Galaxy Forming Region with ALMA 2. Multi-wavelength Study of Galaxy Formation/Evolution

More information

ACTIVE GALACTIC NUCLEI: optical spectroscopy. From AGN classification to Black Hole mass estimation

ACTIVE GALACTIC NUCLEI: optical spectroscopy. From AGN classification to Black Hole mass estimation ACTIVE GALACTIC NUCLEI: optical spectroscopy From AGN classification to Black Hole mass estimation Second Lecture Reverberation Mapping experiments & virial BH masses estimations Estimating AGN black hole

More information

Caitlin Casey, Jacqueline Hodge, Mark Lacy

Caitlin Casey, Jacqueline Hodge, Mark Lacy Next Generation VLA: Galaxy Assembly through Cosmic Time High-z working group: Caitlin Casey, Jacqueline Hodge, Mark Lacy Katherine Alatalo, Amy Barger, Sanjay Bhatnagar, Chris Carilli, Christopher Hales,

More information

Galaxies 626. Lecture 9 Metals (2) and the history of star formation from optical/uv observations

Galaxies 626. Lecture 9 Metals (2) and the history of star formation from optical/uv observations Galaxies 626 Lecture 9 Metals (2) and the history of star formation from optical/uv observations Measuring metals at high redshift Metals at 6 How can we measure the ultra high z star formation? One robust

More information

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

Paul Sell. University of Wisconsin-Madison Advisor: Christy Tremonti A SAMPLE OF EXTREME MERGER-DRIVEN STARBURST GALAXIES AS VIEWED BY THE CHANDRA AND HUBBLE SPACE TELESCOPES Paul Sell University of Wisconsin-Madison Advisor: Christy Tremonti Collaboration: Aleks Diamond-Stanic,

More information

Astr 2320 Thurs. April 27, 2017 Today s Topics. Chapter 21: Active Galaxies and Quasars

Astr 2320 Thurs. April 27, 2017 Today s Topics. Chapter 21: Active Galaxies and Quasars Astr 2320 Thurs. April 27, 2017 Today s Topics Chapter 21: Active Galaxies and Quasars Emission Mechanisms Synchrotron Radiation Starburst Galaxies Active Galactic Nuclei Seyfert Galaxies BL Lac Galaxies

More information

Luminous Quasars and AGN Surveys with ELTs

Luminous Quasars and AGN Surveys with ELTs Luminous Quasars and AGN Surveys with ELTs Roberto J. Assef Núcleo de Astronomía Universidad Diego Portales This Talk Will focus on two topics: 1. The most luminous (obscured) quasars 2. AGN surveys Big

More information

Active Galactic Nuclei: Making the Most of the Great Observatories

Active Galactic Nuclei: Making the Most of the Great Observatories Active Galactic Nuclei: Making the Most of the Great Observatories Niel Brandt (Penn State) AGN Spectral Energy Distribution 3.6-160 µm 1150-25000 A 0.3-8 kev Host galaxy Richards et al. (2006) Active

More information

Active Galaxies & Emission Line Diagnostics

Active Galaxies & Emission Line Diagnostics Active Galaxies & Emission Line Diagnostics Review of Properties Discussed: 1) Powered by accretion unto a supermassive nuclear black hole 2) They are the possible precursors to luminous massive galaxies

More information

Two Main Techniques. I: Star-forming Galaxies

Two Main Techniques. I: Star-forming Galaxies p.1/24 The high redshift universe has been opened up to direct observation in the last few years, but most emphasis has been placed on finding the progenitors of today s massive ellipticals. p.2/24 Two

More information

Gas Accretion & Outflows from Redshift z~1 Galaxies

Gas Accretion & Outflows from Redshift z~1 Galaxies Gas Accretion & Outflows from Redshift z~1 Galaxies David C. Koo Kate Rubin, Ben Weiner, Drew Phillips, Jason Prochaska, DEEP2, TKRS, & AEGIS Teams UCO/Lick Observatory, University of California, Santa

More information

The Phenomenon of Active Galactic Nuclei: an Introduction

The Phenomenon of Active Galactic Nuclei: an Introduction The Phenomenon of Active Galactic Nuclei: an Introduction Outline Active Galactic Nuclei (AGN): > Why are they special? > The power source > Sources of Continuum Emission > Emission & absorption lines

More information

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

AST Cosmology and extragalactic astronomy. Lecture 20. Black Holes Part II AST4320 - Cosmology and extragalactic astronomy Lecture 20 Black Holes Part II 1 AST4320 - Cosmology and extragalactic astronomy Outline: Black Holes Part II Gas accretion disks around black holes, and

More information

The first black holes

The first black holes The first black holes Marta Volonteri Institut d Astrophysique de Paris M. Habouzit, Y. Dubois, M. Latif (IAP) A. Reines (NOAO) M. Tremmel (University of Washington) F. Pacucci (SNS) High-redshift quasars

More information

Feedback and Galaxy Formation

Feedback and Galaxy Formation Heating and Cooling in Galaxies and Clusters Garching August 2006 Feedback and Galaxy Formation Simon White Max Planck Institute for Astrophysics Cluster assembly in ΛCDM Gao et al 2004 'Concordance'

More information

BUILDING GALAXIES. Question 1: When and where did the stars form?

BUILDING GALAXIES. Question 1: When and where did the stars form? BUILDING GALAXIES The unprecedented accuracy of recent observations of the power spectrum of the cosmic microwave background leaves little doubt that the universe formed in a hot big bang, later cooling

More information

Multi-wavelength ISM diagnostics in high redshift galaxies

Multi-wavelength ISM diagnostics in high redshift galaxies Multi-wavelength ISM diagnostics in high redshift galaxies Alexandra Pope (UMass Amherst) Transformational Science in the ALMA Era: Multi-Wavelength Studies of Galaxy Evolution Conference Charlottesville,

More information

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

Multi-wavelength Surveys for AGN & AGN Variability. Vicki Sarajedini University of Florida Multi-wavelength Surveys for AGN & AGN Variability Vicki Sarajedini University of Florida What are Active Galactic Nuclei (AGN)? Galaxies with a source of non-stellar emission arising in the nucleus (excessive

More information

Active Galactic Nuclei

Active Galactic Nuclei Active Galactic Nuclei Optical spectra, distance, line width Varieties of AGN and unified scheme Variability and lifetime Black hole mass and growth Geometry: disk, BLR, NLR Reverberation mapping Jets

More information

The Evolution of BH Mass Scaling Relations

The Evolution of BH Mass Scaling Relations The Evolution of BH Mass Scaling Relations Nicola Bennert UCSB in collaboration with Tommaso Treu (UCSB), Jong-Hak Woo (UCLA), Alexandre Le Bris (UCSB), Matthew A. Malkan (UCLA), Matthew W. Auger (UCSB),

More information

UV/optical spectroscopy of Submilliimeter Galaxies

UV/optical spectroscopy of Submilliimeter Galaxies UV/optical spectroscopy of Submilliimeter Galaxies Scott C. Chapman (Caltech), A. Blain (Caltech), I. Smail (Durham), M. Swinbank (Durham) R. Ivison (Edinburgh) SFR_Hα = SFR_FIR SFR_Hα = 1/10 SFR_FIR Outline:

More information

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

Orianne ROOS CEA-Saclay Collaborators : F. Bournaud, J. Gabor, S. Juneau Orianne ROOS CEA-Saclay Collaborators : F. Bournaud, J. Gabor, S. Juneau Bachelor of Physics, Master of Astrophysics Université de Strasbourg PhD, Université Paris-Diderot Observatoire de Strasbourg Les

More information

Active Galaxies & Quasars

Active Galaxies & Quasars Active Galaxies & Quasars Normal Galaxy Active Galaxy Galactic Nuclei Bright Active Galaxy NGC 5548 Galaxy Nucleus: Exact center of a galaxy and its immediate surroundings. If a spiral galaxy, it is the

More information

2. Active Galaxies. 2.1 Taxonomy 2.2 The mass of the central engine 2.3 Models of AGNs 2.4 Quasars as cosmological probes.

2. Active Galaxies. 2.1 Taxonomy 2.2 The mass of the central engine 2.3 Models of AGNs 2.4 Quasars as cosmological probes. 2. Active Galaxies 2.1 Taxonomy 2.2 The mass of the central engine 2.3 Models of AGNs 2.4 Quasars as cosmological probes Read JL chapter 3 Active galaxies: interface with JL All of JL chapter 3 is examinable,

More information

ALMA Synergy with ATHENA

ALMA Synergy with ATHENA ALMA Synergy with ATHENA Françoise Combes Observatoire de Paris 9 September 2015 ALMA & Athena: common issues Galaxy formation and evolution, clustering Surveys of galaxies at high and intermediate redshifts

More information

Dominik A. Riechers Cornell University

Dominik A. Riechers Cornell University JVLA ALMA CCAT First year of full science Finishing construction The next big thing The Interstellar Medium in High Redshift Galaxies Dominik A. Riechers Cornell University Phases of the ISM MPIA Summer

More information

Far-infrared Herschel SPIRE spectroscopy reveals physical conditions of ionised gas in high-redshift lensed starbursts

Far-infrared Herschel SPIRE spectroscopy reveals physical conditions of ionised gas in high-redshift lensed starbursts Far-infrared Herschel SPIRE spectroscopy reveals physical conditions of ionised gas in high-redshift lensed starbursts Zhi-Yu (Z-Y) Zhang 张智昱 U. Edinburgh/ESO Outline Background Sample description Herschel

More information

THE CONNECTION BETWEEN STAR FORMATION AND DARK MATTER HALOS AS SEEN IN THE INFRARED

THE CONNECTION BETWEEN STAR FORMATION AND DARK MATTER HALOS AS SEEN IN THE INFRARED ESLAB 2013 04/04/2013 Noordwijk THE CONNECTION BETWEEN STAR FORMATION AND DARK MATTER HALOS AS SEEN IN THE INFRARED Material at http://irfu.cea.fr/sap/phocea/page/index.php?id=537 Matthieu Béthermin In

More information

MOS: A critical tool for current & future radio surveys Daniel J.B. Smith, University of Hertfordshire, UK.

MOS: A critical tool for current & future radio surveys Daniel J.B. Smith, University of Hertfordshire, UK. MOS: A critical tool for current & future radio surveys Daniel J.B. Smith, University of Hertfordshire, UK www.herts.ac.uk/~dsmith/ MOS: A critical tool for current & future radio surveys Outline Why study

More information

Black Holes in the Early Universe Accretion and Feedback

Black Holes in the Early Universe Accretion and Feedback 1 1 Black Holes in the Early Universe Accretion and Feedback 1 1 Black Holes in the Early Universe Accretion and Feedback Geoff Bicknell & Alex Wagner Australian National University 1 1 High redshift radio

More information

Massive molecular outflows from ULIRGs - Dynamics and Energetics - E. Sturm for the SHINING and QUEST Team

Massive molecular outflows from ULIRGs - Dynamics and Energetics - E. Sturm for the SHINING and QUEST Team Massive molecular outflows from ULIRGs - Dynamics and Energetics - E. Sturm for the SHINING and QUEST Team NGC253 AGN- ULIRGs SB- ULIRGs Sturm+ 2011 Massive molecular outflows detected in ULIRGs v (OH)

More information

Radio Afterglows. What Good are They? Dale A. Frail. National Radio Astronomy Observatory. Gamma Ray Bursts: The Brightest Explosions in the Universe

Radio Afterglows. What Good are They? Dale A. Frail. National Radio Astronomy Observatory. Gamma Ray Bursts: The Brightest Explosions in the Universe Radio Afterglows What Good are They? Dale A. Frail National Radio Astronomy Observatory Gamma Ray Bursts: The Brightest Explosions in the Universe The 2 nd Harvard-Smithsonian Conference on Theoretical

More information

Outline: Part II. The end of the dark ages. Structure formation. Merging cold dark matter halos. First stars z t Univ Myr.

Outline: Part II. The end of the dark ages. Structure formation. Merging cold dark matter halos. First stars z t Univ Myr. Outline: Part I Outline: Part II The end of the dark ages Dark ages First stars z 20 30 t Univ 100 200 Myr First galaxies z 10 15 t Univ 300 500 Myr Current observational limit: HST and 8 10 m telescopes

More information

Chapter 17. Active Galaxies and Supermassive Black Holes

Chapter 17. Active Galaxies and Supermassive Black Holes Chapter 17 Active Galaxies and Supermassive Black Holes Guidepost In the last few chapters, you have explored our own and other galaxies, and you are ready to stretch your scientific imagination and study

More information

ASTRON 449: Stellar (Galactic) Dynamics. Fall 2014

ASTRON 449: Stellar (Galactic) Dynamics. Fall 2014 ASTRON 449: Stellar (Galactic) Dynamics Fall 2014 In this course, we will cover the basic phenomenology of galaxies (including dark matter halos, stars clusters, nuclear black holes) theoretical tools

More information

The Herschel Multi-tiered Extragalactic Survey (HerMES) The Evolution of the FIR/SMM Luminosity Function and of the Cosmic SFRD

The Herschel Multi-tiered Extragalactic Survey (HerMES) The Evolution of the FIR/SMM Luminosity Function and of the Cosmic SFRD The Herschel Multi-tiered Extragalactic Survey (HerMES) The Evolution of the FIR/SMM Luminosity Function and of the Cosmic SFRD Lucia Marchetti University of Padova - Open University Mattia Vaccari - University

More information

Coevolution (Or Not) of Supermassive Black Holes and Galaxies

Coevolution (Or Not) of Supermassive Black Holes and Galaxies Coevolution (Or Not) of Supermassive Black Holes and Galaxies Luis C. Ho ( 何子山 ) The Observatories of the Carnegie Institution for Science Ho 2008, ARA&A Nuclear Activity in Nearby Galaxies Kormendy &

More information

ISM and Galaxy Evolution the ELT View Alvio Renzini, INAF Padova

ISM and Galaxy Evolution the ELT View Alvio Renzini, INAF Padova ISM and Galaxy Evolution the ELT View Alvio Renzini, INAF Padova Starlight, HII & AGN Dust & Molecules Where we stand and looking in perspective The current generation of ground & space telescopes are

More information

Multiwavelength signatures of AGN feedback in local AGN

Multiwavelength signatures of AGN feedback in local AGN Multiwavelength signatures of AGN feedback in local AGN Chiara Feruglio Institut de RadioAstronomie Millimétrique, Grenoble Thanks to: G. FABBIANO (CfA), F. FIORE (INAF) INAF - Bologne, 6 Mai 2013 1 Galaxy

More information

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

Gas Masses and Gas Fractions: Applications of the Kennicutt- Schmidt Law at High Redshift Gas Masses and Gas Fractions: Applications of the Kennicutt- Schmidt Law at High Redshift Dawn Erb (CfA) Kennicutt-Schmidt Workshop, UCSD December 19, 2006 Overview Properties of star-forming galaxies

More information

Astronomy 730. Evolution

Astronomy 730. Evolution Astronomy 730 Evolution Outline } Evolution } Formation of structure } Processes on the galaxy scale } Gravitational collapse, merging, and infall } SF, feedback and chemical enrichment } Environment }

More information

Quick report of the project 123 (submm follow-up)

Quick report of the project 123 (submm follow-up) HSC-AGN f2f meeting Aug. 26, 2016 @IPMU/Tokyo Quick report of the project 123 (submm follow-up) Takuma Izumi IoA/UTokyo 1 #123 Investigation of rest-frame far-ir to submm properties of z = 6-7 QSO-host

More information

Dusty star-forming galaxies at high redshift (part 5)

Dusty star-forming galaxies at high redshift (part 5) Dusty star-forming galaxies at high redshift (part 5) Flow of story 4.1 4.2 4.3 Acquiring Spectroscopic or Photometric Redshifts Infrared SED Fitting for DSFGs Estimating L IR, T dust and M dust from an

More information

Quasars in the epoch of reioniza1on

Quasars in the epoch of reioniza1on Big Bang Dark Ages Quasars in the epoch of reioniza1on Carnegie-Princeton Fellow Illumina9ng the Dark Ages June 27, Heidelberg, Germany Universe Today Quasars and galaxies in the reioniza1on epoch Quasars

More information

Clustering of Star-forming Galaxies and connections with AGN activity

Clustering of Star-forming Galaxies and connections with AGN activity Clustering of Star-forming Galaxies and connections with AGN activity MANUELA MAGLIOCCHETTI IAPS-INAF Collaborators: Herschel PEP team (D.Lutz, P.Popesso, D.Rosario et al.) & A.Lapi, M.Negrello, G.De Zotti.,

More information

Part 2. Hot gas halos and SMBHs in optically faint ellipticals. Part 3. After Chandra?

Part 2. Hot gas halos and SMBHs in optically faint ellipticals. Part 3. After Chandra? Hot gas and AGN Feedback in Nearby Groups and Galaxies Part 1. Cool cores and outbursts from supermassive black holes in clusters, groups and normal galaxies Part 2. Hot gas halos and SMBHs in optically

More information

Vivienne Wild. Timing the starburst AGN connection

Vivienne Wild. Timing the starburst AGN connection Vivienne Wild Timing the starburst AGN connection There are many theories successful in explaining the observed correlations between black holes and their host galaxies. In turn, these theories play a

More information

- AGN feedback in action?

- AGN feedback in action? 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

More information

The Cosmic History of Star Formation. James Dunlop Institute for Astronomy, University of Edinburgh

The Cosmic History of Star Formation. James Dunlop Institute for Astronomy, University of Edinburgh The Cosmic History of Star Formation James Dunlop Institute for Astronomy, University of Edinburgh PLAN 1. Background 2. Star-formation rate (SFR) indicators 3. The last ~11 billion years: 0 < z < 3 4.

More information

HIGH REDSHIFT OBJECTS. Alain Omont (IAP)

HIGH REDSHIFT OBJECTS. Alain Omont (IAP) Post-Herschel FIR (20-500µm) science objectives HIGH REDSHIFT OBJECTS. Alain Omont (IAP) A deep spectral window into the young Universe complementary to JWST and ALMA Thanks to: F. Bertoldi, P. Cox, C.

More information

High-redshift galaxies

High-redshift galaxies High-redshift galaxies Houjun Mo May 4, 2004 Galaxies can now be observed to z 6 Normal galaxies with 0.2 < z < 1 The Lyman-break population at z 3 The sub-mm sources at z 3 Between 1 2, spectroscopy desert,

More information

High-Redshift Galaxies: A brief summary

High-Redshift Galaxies: A brief summary High-Redshift Galaxies: A brief summary Brant Robertson (Caltech) on behalf of David Law (UCLA), Bahram Mobasher (UCR), and Brian Siana (Caltech/Incoming CGE) Observable Cosmological History t~3.7x10 5

More information

Massively Star-Forming Dusty Galaxies. Len Cowie JCMT Users Meeting

Massively Star-Forming Dusty Galaxies. Len Cowie JCMT Users Meeting Massively Star-Forming Dusty Galaxies Len Cowie JCMT Users Meeting The luminous dusty star-formation history: We are using SCUBA-2 to address three questions What fraction of the SF is in luminous dusty

More information

Active Galactic Nuclei OIII

Active Galactic Nuclei OIII Active Galactic Nuclei In 1908, Edward Fath (1880-1959) observed NGC 1068 with his spectroscope, which displayed odd (and very strong) emission lines. In 1926 Hubble recorded emission lines of this and

More information

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

The Monster Roars: AGN Feedback & Co-Evolution with Galaxies The Monster Roars: AGN Feedback & Co-Evolution with Galaxies Philip Hopkins Ø (Nearly?) Every massive galaxy hosts a supermassive black hole Ø Mass accreted in ~couple bright quasar phase(s) (Soltan, Salucci+,

More information

ALMA and the high redshift Universe. Simon Lilly ETH Zürich

ALMA and the high redshift Universe. Simon Lilly ETH Zürich Simon Lilly ETH Zürich 2012 will be an exciting year 2012 a great year ? Cool material is central to this process Galaxy formation at high z (Hauser and Dwek ARAA 2001) Extragalactic background light:

More information

Astro2010 Science White Paper: Tracing the Mass Buildup of Supermassive Black Holes and their Host Galaxies

Astro2010 Science White Paper: Tracing the Mass Buildup of Supermassive Black Holes and their Host Galaxies Astro2010 Science White Paper: Tracing the Mass Buildup of Supermassive Black Holes and their Host Galaxies Anton M. Koekemoer (STScI) Dan Batcheldor (RIT) Marc Postman (STScI) Rachel Somerville (STScI)

More information

AGN in hierarchical galaxy formation models

AGN in hierarchical galaxy formation models AGN in hierarchical galaxy formation models Nikos Fanidakis and C.M. Baugh, R.G. Bower, S. Cole, C. Done, C. S. Frenk Physics of Galactic Nuclei, Ringberg Castle, June 18, 2009 Outline Brief introduction

More information

Warm Molecular Hydrogen at high redshift with JWST

Warm Molecular Hydrogen at high redshift with JWST Warm Molecular Hydrogen at high redshift with JWST Pierre Guillard Institut d Astrophysique de Paris Université Pierre et Marie Curie he Warm H 2 with JWST Outline and take-home messages 1. Observations

More information

ngvla: Galaxy Assembly through Cosmic Time

ngvla: Galaxy Assembly through Cosmic Time ngvla: Galaxy Assembly through Cosmic Time Dominik A. Riechers (Cornell) On behalf of the ngvla high-z working group: Caitlin Casey, Jacqueline Hodge, Mark Lacy, Katherine Alatalo, Amy Barger, Sanjay Bhatnagar,

More information

Quasars and AGN. What are quasars and how do they differ from galaxies? What powers AGN s. Jets and outflows from QSOs and AGNs

Quasars and AGN. What are quasars and how do they differ from galaxies? What powers AGN s. Jets and outflows from QSOs and AGNs Goals: Quasars and AGN What are quasars and how do they differ from galaxies? What powers AGN s. Jets and outflows from QSOs and AGNs Discovery of Quasars Radio Observations of the Sky Reber (an amateur

More information

In class presentations!

In class presentations! Nov 23, 2015 High-Redshift Galaxies III - Current Redshift Frontier - Gravitational Lensing - Star Formation/Stellar Mass Histories - Galaxy Main Sequence - Star Formation Law, Gas Fractions HW#10 is due

More information

What s the fuss about AGN?

What s the fuss about AGN? What s the fuss about AGN? Mari Polletta (IASF-INAF Milan, Italy) 1 Outline What is an Active Galactic Nucleus (AGN)? AGN role and importance AGN evolutionary models and feedback Star-formation and AGN

More information

The Excited and Exciting ISM in Galaxies: PDRs, XDRs and Shocks as Probes and Triggers

The Excited and Exciting ISM in Galaxies: PDRs, XDRs and Shocks as Probes and Triggers The Excited and Exciting ISM in Galaxies: PDRs, XDRs and Shocks as Probes and Triggers Marco Spaans (Groningen) Rowin Meijerink (Groningen), Paul van der Werf (Leiden), Juan Pablo Pérez Beaupuits (Bonn),

More information

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

Lecture 11: SDSS Sources at Other Wavelengths: From X rays to radio. Astr 598: Astronomy with SDSS Astr 598: Astronomy with SDSS Spring Quarter 4, University of Washington, Željko Ivezić Lecture : SDSS Sources at Other Wavelengths: From X rays to radio Large Surveys at Many Wavelengths SDSS: UV-IR five-band

More information

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

MASSIVE BLACK HOLES AMY REINES IN NEARBY DWARF GALAXIES HUBBLE FELLOW NATIONAL OPTICAL ASTRONOMY OBSERVATROY MASSIVE BLACK HOLES IN NEARBY DWARF GALAXIES AMY REINES HUBBLE FELLOW NATIONAL OPTICAL ASTRONOMY OBSERVATROY Motivation: The origin of massive black holes (BHs) Massive BHs are fundamental components of

More information

Hubble Space Telescope ultraviolet spectroscopy of blazars: emission lines properties and black hole masses. E. Pian, R. Falomo, A.

Hubble Space Telescope ultraviolet spectroscopy of blazars: emission lines properties and black hole masses. E. Pian, R. Falomo, A. Hubble Space Telescope ultraviolet spectroscopy of blazars: emission lines properties and black hole masses E. Pian, R. Falomo, A. Treves 1 Outline Extra Background Introduction Sample Selection Data Analysis

More information

TEMA 3. Host Galaxies & Environment

TEMA 3. Host Galaxies & Environment TEMA 3. Host Galaxies & Environment AGN Dr. Juan Pablo Torres-Papaqui Departamento de Astronomía Universidad de Guanajuato DA-UG (México) papaqui@astro.ugto.mx División de Ciencias Naturales y Exactas,

More information

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

A zoo of transient sources. (c)2017 van Putten 1 A zoo of transient sources (c)2017 van Putten 1 First transient @ first light UDFj-39546284, z~10.3 Bouwens, R.J., et al., Nature, 469, 504 Cuchiara, A. et al., 2011, ApJ, 736, 7 z=9.4: GRB 090429B, z~9.4

More information

THE GAS MASS AND STAR FORMATION RATE

THE GAS MASS AND STAR FORMATION RATE THE GAS MASS AND STAR FORMATION RATE OF STAR-FORMING GALAXIES AT z ~ 1.3 Nissim Kanekar National Centre for Radio Astrophysics, Pune Apurba Bera Shiv Sethi Ben Weiner K. Dwarakanath Image: B. Premkumar

More information

Test #1! Test #2! Test #2: Results!

Test #1! Test #2! Test #2: Results! High-Redshift Galaxies II - Populations (cont d) - Current Redshift Frontier - Gravitational Lensing I will hand back Test #2 HW#10 will be due next Monday. Nov 18, 2015 Test #1 Test #2 Test #2: Results

More information

SURVEYS: THE MASS ASSEMBLY AND STAR FORMATION HISTORY

SURVEYS: THE MASS ASSEMBLY AND STAR FORMATION HISTORY Lecture #4 SURVEYS: THE MASS ASSEMBLY AND STAR FORMATION HISTORY Observational facts Olivier Le Fèvre ON Rio de Janeiro School 2014 Putting it all together Clear survey strategies Instrumentation and observing

More information