Optical studies of an ultraluminous X-ray source: NGC1313 X-2

Similar documents
HLX-1: unsolved puzzles

XRBs in Star-forming Galaxies X-ray Luminosity Functions Ultra-Luminous X-ray Sources

Ultraluminous X-ray Sources forming in low metallicity natal environments

Investigating Ultraluminous X-ray Sources through multi-wavelength variability, broadband spectra, and theoretical modelling

Ultraluminous X-ray Sources: The most extreme X-ray binaries

A confirmed stellar-mass ULX with recurrent X-ray occultations from its precessing disk

Optical counterparts of ULXs. S. Fabrika

HUBBLE SPACE TELESCOPE IDENTIFICATION OF THE OPTICAL COUNTERPARTS OF ULTRALUMINOUS X-RAY SOURCES IN M51

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

High Redshift Universe

A new catalogue of ultraluminous X-ray sources (and more!)

v Characteristics v Possible Interpretations L X = erg s -1

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

Tidal disruption events from the first XMM-Newton Slew Survey

Astrophysical Quantities

Understanding the nature of ULX with SIMBOL-X

Quasars and Active Galactic Nuclei (AGN)

Modelling multiwavelength emission of ULXs

Basics, types Evolution. Novae. Spectra (days after eruption) Nova shells (months to years after eruption) Abundances

A Supermassive Black Hole in the Dwarf Starburst Galaxy Henize Amy Reines Einstein Fellow National Radio Astronomy Observatory

Accretion in Binaries

HR Diagram, Star Clusters, and Stellar Evolution

The impact of metallicity on the demographics of ULXs

Distribution of X-ray binary stars in the Galaxy (RXTE) High-Energy Astrophysics Lecture 8: Accretion and jets in binary stars

The Black Hole in the Galactic Center. Eliot Quataert (UC Berkeley)

Lecture 9. Quasars, Active Galaxies and AGN

The Milky Way Galaxy

ASTRO 310: Galactic & Extragalactic Astronomy Prof. Jeff Kenney

Stellar Populations: Resolved vs. unresolved

What tool do astronomers use to understand the evolution of stars?

Star systems like our Milky Way. Galaxies

Key issues in black hole accretion - Science by ASTRO-H - Shin Mineshige (Kyoto Univ.)

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

Chapter 17. Active Galaxies and Supermassive Black Holes

Ultra Luminous X-ray sources ~one of the most curious objects in the universe~

2 July 2018 Toshinori Hayashi. Discovery of an Extraordinary Binary System

Crossing the Eddington limit: examining disc spectra at high accretion rates. Andrew Sutton

ASTR 200 : Lecture 25. Galaxies: internal and cluster dynamics

Announcement: Quiz Friday, Oct 31

FORMATION OF SUPERMASSIVE BLACK HOLES Nestor M. Lasso Cabrera

arxiv:astro-ph/ v1 25 Sep 2003

Scientific cases for Simbol-X of interest of the Italian community

SUPER STAR CLUSTERS: High Resolution Observations. James R. Graham (UCB) Nate McCrady (UCLA) & Andrea Gilbert (LLNL) KIPT

Stellar Dynamics and Structure of Galaxies

Molecular Gas and the Host Galaxies of Infrared-Excess Quasi-Stellar Objects

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

A Shock Model for the the Outburst from the Supermassive Black Hole in M87 Bill Forman - SAO/CfA

Ultraluminous X-ray Sources in Nearby Galaxies

OPTICAL/INFRARED COUNTERPARTS OF ULXS

Astronomy. Stellar Evolution

Active Galactic Nuclei - Zoology

Hubble Science Briefing: 25 Years of Seeing Stars with the Hubble Space Telescope. March 5, 2015 Dr. Rachel Osten Dr. Alex Fullerton Dr.

Observational Evidence of Black Holes Kolkata (India), Feb 2008

Star Formation and U/HLXs in the Cartwheel Galaxy Paper & Pencil Version

ASTRON 449: Stellar (Galactic) Dynamics. Fall 2014

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

Active Galaxies and Galactic Structure Lecture 22 April 18th

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

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

GALAXIES. Edmund Hodges-Kluck Andrew Ptak

A RADIO SEARCH FOR BLACK HOLES IN THE MILKY WAY GLOBULAR CLUSTER M10

Galaxies. The majority of known galaxies fall into one of three major classes: spirals (78 %), ellipticals (18 %) and irregulars (4 %).

Searching for intermediate-mass black holes in Galactic globular clusters

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

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

Matt Brorby (U of Iowa) with Philip Kaaret (U of Iowa) Illustration: NASA/CXC/M.Weiss

The Classification of Galaxies

Other Galaxy Types. Active Galaxies. A diagram of an active galaxy, showing the primary components. Active Galaxies

Astr 5465 Feb. 13, 2018 Distribution & Classification of Galaxies Distribution of Galaxies

Galaxies. Galaxy Diversity. Galaxies, AGN and Quasars. Physics 113 Goderya

Quasars ASTR 2120 Sarazin. Quintuple Gravitational Lens Quasar

Searching for signs of IMBH astrometric microlensing in M 22

Stellar populations of quasar host galaxies

Gaia News:Counting down to launch A. Vallenari. INAF, Padova Astronomical Observatory on behalf of DPACE

Population of BHs in the Galaxy and in the MCs

Accretion Disks. 1. Accretion Efficiency. 2. Eddington Luminosity. 3. Bondi-Hoyle Accretion. 4. Temperature profile and spectrum of accretion disk

LECTURE 1: Introduction to Galaxies. The Milky Way on a clear night

Source plane reconstruction of the giant gravitational arc in Abell 2667: a condidate Wolf-Rayet galaxy at z 1

The dynamics of neutron star and black hole binaries in young star clusters

Objectives. HR Diagram

Simultaneous X-ray and Radio Observations of Seyferts, and Disk-Jet Connections

LARGE QUASAR GROUPS. Kevin Rahill Astrophysics

Active Galactic Nuclei OIII

Lecture 28: Spiral Galaxies Readings: Section 25-4, 25-5, and 26-3

Active Galactic Alexander David M Nuclei

11 days exposure time. 10,000 galaxies. 3 arcminutes size (0.1 x diameter of moon) Estimated number of galaxies in observable universe: ~200 billion

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

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

AS1001:Extra-Galactic Astronomy

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

Measuring the Spin of the Accreting Black Hole In Cygnus X-1

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

Lecture 19: Galaxies. Astronomy 111

Lecture Outlines. Chapter 24. Astronomy Today 8th Edition Chaisson/McMillan Pearson Education, Inc.

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.

In a dense region all roads lead to a black Hole (Rees 1984 ARAA) Deriving the Mass of SuperMassive Black Holes

Chapter 15 2/19/2014. Lecture Outline Hubble s Galaxy Classification. Normal and Active Galaxies Hubble s Galaxy Classification

The Hot Gaseous Halos of Spiral Galaxies. Joel Bregman, Matthew Miller, Edmund Hodges Kluck, Michael Anderson, XinyuDai

Feeding the Beast. Chris Impey (University of Arizona)

Dr G. I. Ogilvie Lent Term 2005 INTRODUCTION

Transcription:

Optical studies of an ultraluminous X-ray source: NGC1313 X-2 Jifeng Liu Harvard-Smithsonian Center for Astrophysics in collaboration with Joel Bregman, Jon Miller, Philip Kaaret

outline background: ultraluminous X-ray sources a case study: NGC1313 X2 X-ray observations optical observations astrometry photometry color-magnitude diagram spectral energy distribution discussion IMBH formation period? radial velocity

ultraluminous X-ray sources

ultraluminous X-ray sources ULXs are non-nuclear X-ray point sources with Lx > 2 X 10 39 erg/s, i.e., more luminous than the Eddington luminosity for stellar mass black holes, and could be intermediate mass black holes of 30-10 5 Ms

ultraluminous X-ray sources ULXs are non-nuclear X-ray point sources with Lx > 2 X 10 39 erg/s, i.e., more luminous than the Eddington luminosity for stellar mass black holes, and could be intermediate mass black holes of 30-10 5 Ms key questions

ultraluminous X-ray sources ULXs are non-nuclear X-ray point sources with Lx > 2 X 10 39 erg/s, i.e., more luminous than the Eddington luminosity for stellar mass black holes, and could be intermediate mass black holes of 30-10 5 Ms key questions are they stellar mass black holes or IMBHs

ultraluminous X-ray sources ULXs are non-nuclear X-ray point sources with Lx > 2 X 10 39 erg/s, i.e., more luminous than the Eddington luminosity for stellar mass black holes, and could be intermediate mass black holes of 30-10 5 Ms key questions are they stellar mass black holes or IMBHs how do they form if IMBH?

ultraluminous X-ray sources ULXs are non-nuclear X-ray point sources with Lx > 2 X 10 39 erg/s, i.e., more luminous than the Eddington luminosity for stellar mass black holes, and could be intermediate mass black holes of 30-10 5 Ms key questions are they stellar mass black holes or IMBHs how do they form if IMBH? how do they radiate if stellar mass black holes?

ULXs in NGC1313 a barred SB(s)d galaxy at 3.7Mpc low metallicity of 0.1-0.2 Zs irregular SW satellite regions - a tidally disrupted companion galaxy? a collision of huge HI clouds with the disk? ULXs: X1, X2, and SN1978K

ULXs in NGC1313 a barred SB(s)d galaxy at 3.7Mpc low metallicity of 0.1-0.2 Zs irregular SW satellite regions - a tidally disrupted companion galaxy? a collision of huge HI clouds with the disk? ULXs: X1, X2, and SN1978K X1 SN1978K X2

X-ray observations: light curves Zampieri et al. 2004

X-ray observations: light curves XMM Feng & Kaaret 2006

X-ray observations: spectroscopy light curves observed since EINSTEIN variability on time scales from days to months to years maximum Lx up to 3x10 40 erg/s X-ray spectra can be fitted with a power-law (Γ~2.3, 63%) plus a cool accretion disk (~160 ev, 37%) suggestive of a IMBH of ~10 3 Ms (Miller et al. 2003) but the cool accretion disk component is dominated by the power-law component, and the fit is not unique it can also be fitted with a power-law (Γ~2.9,64%) plus a hot disk (~2.7 kev, 36%). (Stobbart et al. 2006)

optical observations

optical observations ESO 3.6m R counterpart: C (later resolved to C1 and C2) Zampieri et al. 2004

optical observations ESO VLT true-color image Pakull et al. 2006

optical observations

optical observations: astrometry

optical observations: astrometry

optical observations: astrometry

optical observations: astrometry x3: foreground star x4: background AGN

optical observations: astrometry

optical observations: astrometry

optical observations: astrometry Counterpart: C1

optical observations: environments

optical observations: environments

optical observations: photometry IRAF/DAOPHOT was used VEGAmag and STMAG were computed

optical observations: variability

optical observations: variability only 12 out of 400 stars are variable above 3 sigma counterpart: ΔF555W = 0.153±0.047 mag

color-magnitude diagrams use HST ACS/WFC VEGAmag photometric system for data and isochrones Z=0.2Zs isochrones (Leo Girardi), E(B-V)=0.11 (a) t=1e7,5e7,2e8,5e8 years (b) t=1e7,5e7,3e8,1e9,3e9

color-magnitude diagrams two populations young: < a few 10 7 years old: 3-30x10 8 years ULX age for E(B-V)=0.11 mag 10 7 years from F435W-F555W 3x10 7 years from F555W-F814W two ages converge at 5 X10 6 years for E(B-V)= 0.33 mag [E(B-V)=0.44 mag from X-ray absorption] initial/current mass of 52/8.5 Ms, radius of 7 Rs

spectral energy distribution

spectral energy distribution

spectral energy distribution

spectral energy distribution

summary counterpart identified with C1 showed 15% variability SED consistent with O7V (Zs, 30Ms, 9Rs) for E(B-V) =0.33 mag E(B-V)=0.33 mag, Z=0.2Zs: an age of 5 million years, mass 8.5 Ms, and radius 7 Rs on the edge of a young open cluster, amid dominant old stars

IMBH formation

IMBH formation if an IMBH, cannot form from evolution of high metallicity stars...

IMBH formation if an IMBH, cannot form from evolution of high metallicity stars... three merging scenarios

IMBH formation if an IMBH, cannot form from evolution of high metallicity stars... three merging scenarios merging of black holes massive stars proto stars birthplace globular cluster super star cluster proto cluster timescale >>10 7 years <3Myr <0.5Myr IMBH location GC centers (1pc) SSC centers (3pc) around open clusters (100 pc) note low Z, external impact

IMBH formation if an IMBH, cannot form from evolution of high metallicity stars... three merging scenarios merging of black holes massive stars proto stars birthplace globular cluster super star cluster proto cluster timescale >>10 7 years <3Myr <0.5Myr IMBH location GC centers (1pc) SSC centers (3pc) around open clusters (100 pc) note low Z, external impact X2 s location close to a young open cluster, the low Z, and possible collision/ disruption may point to the merging of proto stars in proto clusters

orbital period? estimate the period assuming C1 overflows its Roche lobe Roche lobe size Rcr = a * f(q) q = Msec/Mprimary Kopal tabulation (1959) Paczynski approximation (1971) Eggleton approximation (1983) equating Rsec = Rcr... shorter P for larger q ρ=110/p 2 for q < 0.3 constraints P=56 hr? P<56 hr => M<15 Ms propose observations to detect such a period

radial velocity

radial velocity Pakull et al. 2006

radial velocity HeII line FWHM: 600 km/s line shift: 300 km/s Pakull et al. 2006

radial velocity

radial velocity if He II line from X-ray illuminated accretion disk, then a stellar mass black hole!

radial velocity if He II line from X-ray illuminated accretion disk, then a stellar mass black hole! however... emission lines from X-ray illuminated accretion disks are broad, >1200 km/s radial velocity for a stellar mass black hole lower than 300 km/s He II line from X-ray photoionized nebula/secondary line shift severely affected by noise

radial velocity if He II line from X-ray illuminated accretion disk, then a stellar mass black hole! however... emission lines from X-ray illuminated accretion disks are broad, >1200 km/s radial velocity for a stellar mass black hole lower than 300 km/s He II line from X-ray photoionized nebula/secondary line shift severely affected by noise need further observations with higher signal-to-noise ratios and higher spectral resolution to sample radial velocities at different phases

radial velocity if He II line from X-ray illuminated accretion disk, then a stellar mass black hole! however... emission lines from X-ray illuminated accretion disks are broad, >1200 km/s radial velocity for a stellar mass black hole lower than 300 km/s He II line from X-ray photoionized nebula/secondary line shift severely affected by noise need further observations with higher signal-to-noise ratios and higher spectral resolution to sample radial velocities at different phases

radial velocity if He II line from X-ray illuminated accretion disk, then a stellar mass black hole! however... emission lines from X-ray illuminated accretion disks are broad, >1200 km/s radial velocity for a stellar mass black hole lower than 300 km/s He II line from X-ray photoionized nebula/secondary line shift severely affected by noise need further observations with higher signal-to-noise ratios and higher spectral resolution to sample radial velocities at different phases