black&holes&and&quasars& - astronomy group...

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Black Holes and Quasars Black Holes Normal and Supermassive The Schwartzchild Radius (event horizon) Normal and Super Massive Black Holes (SMBHs) The GalacAc Centre (GC) The Black Hole in Andromeda AcAve GalacAc Nuclei (AGN) Discovery of Seyferts and Quasars Basic properAes Blazars, QSOs, BL Lacs, OVVs, LINERs etc. AGN UnificaAon SMBH correlaAons with host galaxy AGN AcAvity with Cosmic Time ImplicaAons for galaxy formaAon

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Page 1: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Black  Holes  and  Quasars  Black  Holes  

Normal  and  Super-­‐massive  The  Schwartzchild  Radius  (event  horizon)  Normal  and  Super  Massive  Black  Holes  (SMBHs)  The  GalacAc  Centre  (GC)  The  Black  Hole  in  Andromeda  

AcAve  GalacAc  Nuclei  (AGN)  Discovery  of  Seyferts  and  Quasars  Basic  properAes  Blazars,  QSOs,  BL  Lacs,  OVVs,  LINERs  etc.  AGN  UnificaAon  SMBH  correlaAons  with  host  galaxy  AGN  AcAvity  with  Cosmic  Time  

ImplicaAons  for  galaxy  formaAon      

 

Page 2: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Black Holes   Gravity is the curvature of space-time by matter. If sufficient mass exists

in a small enough volume space-time is distorted such that even light cannot escape

Page 3: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

The Schwarzschild Radius •  The  radius  at  which  even  light  cannot  escape  is  known  as  the  event  

horizon  or  Schwarzschild  radius.  •  For  a  non-­‐rotaAng  black  hole  this  is  simply  when  the  KineAc  Energy  =  

GravitaAonal  Energy  for  a  photon  

2

2

2

22121

cGMr

rGMmmc

rGMmmv

S

S

=

=

=

r s

Page 4: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Types of Black Hole •  Normal    

–  Formed  from  massive  stars  going  supernovae  

•  Super-­‐massive  –  Formed  in  galaxy  cores  during  iniAal  collapse?      

•  Most  galaxies  are  believed  to  harbour  a  super-­‐massive  black-­‐hole  in  their  cores  –  Existence  of  Intermediate  Mass  Black  Holes  uncertain  

!MM 10~BH

!" MM 97

BH 10~

Page 5: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Evidence for SMBHs •  We  find  that  stars  have  velociAes  of  >110km/s  within  2.5pc  of  

the  core  of  M31  

Page 6: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Super-massive BH in M31 •  IF they are in circular orbits we can use the Virial theorem to

calculate the mass inside r

•  In our Milky Way galaxy –  Velocities > 1000 km/s inside 0.01 pc!

•  => 2 x 106 Msun SMBH

!

"

#=#=

#

####==

MM

M

637CORE

11

16232

CORE

108.6104.11067.6

1035.2)10110(

kgGrv

Page 7: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Our Galactic Centre

Page 8: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Infrared Studies •  Infrared  (2  µm)  penetrates  through  the  dust    •  Can  use  to  probe  stellar  populaAons  and  dynamics  in  GC  •  Find  central  cluster  of  young  massive  stars  

–  Teff  ~  20,000  K  –  Burst  of  star  formaAon  107  years  ago?  

•  Or  masses  modified  by  star-­‐star  collisions?  –  Plus  repeated  bursts  in  the  past  (AGB  stars  present)  –  Stellar  density  ~>  106  stars  pc–3  –  Compare  solar  neighbourhood:  stellar  density  ~  0.1  stars  pc–3  

–  Use  stars  to  study  kinemaAcs  –  And  mass  of  central  object  

GRvM

RGMv

22 =!=

Page 9: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Time lapse movie of Galactic Centre over past 12 years

Page 10: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Orbital Motions

Page 11: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Proper Motions in Galactic Centre •  Measured    by  speckle  and  (now)  adapAve  opAcs  

–  In  IR  (2.2  mm)  to  see  through  dust  

•  Speckle:  many  short  exposures    –  Freeze  out  effects  of  turbulence  in  atmosphere  –  Add  coherently  to  see  image!  

•  Measures  velociAes  of  many  stars  near  GN  •  From  velociAes:  mass  

–  At  0.01  pc:  v  ~  1000  km/s  –  At  0.04  pc:  v  ~  500  km/s  

•  ImplicaAon:    

( ) constant 5.0constant 2 !<"! pcrMRv

Obs.Tech.

i.e.,  Keplerian  

Page 12: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Central Black Hole •  Mass  of  central  object  

•  Mass  within  0.01  pc  is  ~3  x  106  Msun  •  Keplerian  velociAes  inside  of  0.5  pc  

•  Mass  within  10  pc  is  ~3  x  107  Msun  •  mass  density  is  ~4  x  106  Msun  pc-­‐3  

•  So,  does  this  necessarily  mean  a  black  hole?  •  If  not,  mass  density  is  ~4  x  1012  Msun  pc-­‐3          

–  Cluster  of  neutron  stars?  

GRvM2

=

Page 13: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Mass distribution

106

mass

107

105

Radius (pc)

0.01 0.1 1.0 10.0

Msun

4 x 106 Msun pc-3 4 x 1012 Msun pc-3

3 x 106 Msun

Page 14: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Sgr A* •  Radio  source  in  centre  of  nucleus  •  Molecular  gas  disc  rotates  around  it  •  Stellar  cluster  centred  on  it  •  What  is  it?  

–  Variable  non-­‐thermal  radio  source  –  Luminosity  <  105  Lsun  

•  Size:  0.3  mas                      ~  2.4  AU!!!  •  Could  be  a  neutron  star    •  But  it  doesn’t  move!!!  Should  be  in  equilibrium  with  stellar  

cluster!        v  <  200  km/s  –  Most  probably  a  black  hole  –  Schwarschild  radius  ~                                                                ~  few  Rsun  

R = GMc2

Page 15: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Flare from black hole •   x-­‐ray  flare  from  central  locaAon  

•   Due  to  mass  falling  into  the  GC  super-­‐massive  black  hole  

•   Heats  up  and  emits  in  X-­‐rays    before  crossing  ‘event-­‐horizon’  

Page 16: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Galaxies  –  AS  3011   16  

Quasars  &  Seyferts  

•  1943  Carl  Seyfert  publishes  a  list  of  odd  galaxies:  –  Mostly  spirals  with  point-­‐like  nuclei  –  Broad  emission  lines  –  Also  high  ionisaAon  states  (O[VI])  –  Doppler  interpretaAon  implied  >1000  km/s    

•  Later  two  classes  of  Seyferts  proposed:  –  Seyfert  Is:  Broad  hydrogen  lines,  narrow  forbidden  lines  (e.g.,  O[III])  –  Seyfert  IIs:  Only  narrow  lines  present  

•  Assumed  lines  originate  from  disAnct  regions:  –  Broad  lines  from  Broad  Line  Region  –  Narrow  lines  from  Narrow  Line  Region  

Page 17: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Galaxies  –  AS  3011   17  

NGC5548  (Seyfert  I)                                          NGC3277  (Normal  Spiral)  

Page 18: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

18  

Seyfert  1  showing  both  Broad    and  Narrow  line  features  

Seyfert  2  showing  narrow  lines  only  

Images  of  both  show  a  spiral    galaxy  with  a  very  bright  central    

nucleus  

Page 19: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Galaxies  –  AS  3011   19  

Discovery  of  Quasars  -­‐   Strong  radio  sources  known  to  correlate  with  point-­‐like  objects  -­‐   Maarten  Schmidt  collected  the  first  spectrum  for  radius  source  3C273  -­‐ Contained  unexplained  broad  lines,  idenAfied  as  redshited  hydrogen  -­‐ Eventually  deduced  a  redshit  of    0.16  (Schmidt,  Nature,  1963)  -­‐ Soon  other  Quasars  were  discovered  with  redhists  upto  2  -­‐ Current  record  holder  around  z=6.0  

Page 20: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Galaxies  –  AS  3011   20  

OpAcal  jet  

3C273  

Page 21: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Typical  Quasar  or  QSO  spectrum  

Steep  conAnuum  Broad  lines  No  discernable  host  galaxy  

 point-­‐like.  

Page 22: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Galaxies  –  AS  3011   22  

ObservaAons  -­‐>  ProperAes  Point-­‐like                  =  compact  Distant                                =  luminous  Broad  lines      =  high  velociAes  High  excitaAon  lines  =  energeAc  Variable                    =  small  (<1  lyr)  

 

Page 23: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Galaxies  –  AS  3011   23  

at  1  Gpc  

Oten  have  associated  jets  visible  in  raAo  due  to  relaAvisAc  charged  material  zipping  out  along  open  field  lines:    Synchrotron  radiaAon    Jets  oten  extend  10-­‐500kpc!  

Page 24: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

24  

Emit  over  all  wavelengths:,  e.g.,Mk421  

Page 25: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

25  

Other  AGN  types  Quasars,  radio-­‐loud  QSO  (Quasi-­‐stellar  objects),  radio  quiet  Seyfert  I(Broad  lines)  Seyfert  II(Narrow  lines)  Blazers  (Highly  variable  systems),  superluminous  

-  BL  Lacs  (BL  Lacertae)=no  features  -  OVV  (OpAcally  violently  variable)  

LINERS  -  Weak  Seyferts  (no  broad  lines)  

Page 26: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Galaxies  –  AS  3011   26  

Page 27: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

Theories    Two  compeAng  theories:  

-   Nuclear  starbursts  -   Super-­‐massive  black  holes  

Page 28: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

28  

Evidence  for  black  holes  •  Gas  moving  at  ~10,000  km/s,  inconsistent  with  stellar  orbits  •  Emission  lines  change  in  brightness  over  days  to  weeks  

–  light  travel  Ame  implies  emission  from  region  only  ~  light-­‐weeks  across  (~0.01  pc)  

•  Hence  must  have  very  high  density,  because    –  fast  orbits  within  very  small  region:  vorbit  ~  (G  M  /  r)1/2  

•  Only  a  black  hole  can  pack  this  much  maver  in  so  densely  –  the  power  is  generated  at  a  few  Schwartzschild  radii    RS  =  2  G  Mbh  /  c2    (≈  3  km  x  Mbh  /  Msolar)  

•  However  SMBHs  as  central  mechanism  only  adopted  following  discovery  of  the  GC  SMBH  and  that  in  M31  and  M84  which  also  exhibits  a  jet  

Page 29: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

29  

unified  model  

•  The  several  types  may  be  the  same  kind  of  object  seen  from  different  angles  (Unified  Model)  –  see  narrower  lines  if  a  spectrum  comes  from  gas  orbiAng  further  out  –  fastest  stuff  is  in  an  accreAon  disk  around  the  black  hole  

(not  to  scale!)  

see  Seyfert  1  

see  Seyfert  2  

narrow  line  region  clouds  at  ~0.1-­‐1  kpc  

broad  line  region  

accreAon  torus  

can  also  see  polarized  light  from    near  the  nucleus  if  scavered    

Page 30: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

30  

AGN Unification

Seyfert 2 galaxy

Seyfert 1 galaxy

Quasar Blazar

Jet !!!

Torus

Antonucci, 1993

Page 31: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

31  

CorrelaAon  between  SMBH  mass  and  bulge  velocity  dispersion  

Page 32: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

CorrelaAon  between  SMBH  mass  and  Bulge  Absolute  magnitude  

Page 33: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

AGN  acAvity  much  more  common  in  the  past.  Consistent  with  bulge  formaAon  preceeding  disc  formaAon  

AGN  ac+vity  

Page 34: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

The  Cosmic  Star-­‐formaAon  History  

Constructed  from  measurements  of  Hα  or  UV  fluxes  at  various  redshits  

Page 35: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

CSFH  v  AGN  AcAvity  

AGN  acAvity  does  not  seem  to  trace  SFH  at  high-­‐z    1.  Data  uncertain  2.  Redshit  axis  misleading  

…..lets  switch  to  Ame  à  

Page 36: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

CSFH  v  AGN  acAvity  v  Time  

.  

.  

.  

Page 37: Black&Holes&and&Quasars& - ASTRONOMY GROUP …star-spd3/Teaching/PHYS2220/phys2220_lecture11… · Black Holes Gravity is the curvature of space-time by matter. If sufficient mass

37  

Puxng  it  together  ?  Dark  Maver                                                        Baryonic  Maver  0yrs      5Gyrs  

   

   13Gyrs  

Rapid  merging  

Slow  merging  

SMBHs  AGN  

BULG

ES  

DISKS  

P-­‐BU

LGES  

??  

COLLAPSE/MERGERS  

INFALL  

SECULAR  

ACCE

LERA

TING                      DEC

ELER

ATING  

U  

AGN  acAvity  

AGN  no  longer  acAve