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Title: BLACK HOLES: FROM STARS TO GALAXIES


1
BLACK HOLES FROM STARS TO GALAXIES ACROSS THE
RANGE OF MASSES
Felix Mirabel
European Southern Observatory.
Chile (on
leave from CEA. France)
  • In last decade there have been overwhelming
    evidences
  • for the existence of BHs as stellar remnants in
    binaries,
  • as supermassive objects at the centers of
    galaxies, and
  • possibly, as intermediate-mass compact objects
    in
  • ultraluminous X-ray sources.
  • BHs are real physical entities that play an
    important role
  • in several areas of modern astrophysics

2
STELLAR BLACK HOLES
  • Compact objects in stellar binaries with mass
    functions greater than 4.
  • 20 known out of a total population that could be
    as large as 100 million.
  • Is there a real gap for MBH 2.2 - 4 M? ?
  • Why in the Milky Way has not been found a stellar
    BH with MBH gt18 M? ?
  • Is this due to poor statistics or to the metal
    content of BH progenitors ?
  • Are BHs always form in energetic supernovae as
    suggested by the chemical composition of some
    donors, or could they also be form directly ?
  • Does explosion vs. implosion depend on the mass
    of the collapsing core ?
  • The observation of GRBs of long duration should
    shed light for our understanding of the
    mechanisms of stellar-mass black hole formation.

Synergy needed
3
SUPERMASSIVE BLACK HOLES
  • Dynamics is the most direct method to determine
    the masses of compact objects, and therefore, the
    best evidence for their existence.
  • First dynamic evidence by the motion of H2O
    masers in NGC 4258.
  • Best dynamic evidence by the motion of stars
    around the dormant BH of 3-4 x 106 M? at the
    center of our Galaxy.
  • Presence of a cluster of massive stars
    distributed along randomly inclined disks of 0.04
    pc and 0.5 pc radii.
  • This cluster seems to have been formed in situ
    and its study may open new horizons for our
    understanding of the formation of massive BHs and
    its relation with massive formation of stars in
    galactic centers.
  • SMBHs are ubiquitous. Their mass is proportional
    to that of the bulge.
  • The most massive are at z gt 6 and must have
    assembled in t lt 109 yr.
  • Lower mass SMBHs formed more slowly by mergers at
    z lt 3.
  • The peak accretion rate took place at z0.7 as
    the peak IR background.
  • Due to gravitational recoil SMBHs could be off
    center and running away.
  • HOW WERE SMBHs
    FORMED ?

4
BHs OF INTERMEDIATE MASS
  • Possible existence of BHs with M gt 100 M? in ULXs
    because of X-ray spectra properties, QPOs, and
    injected energy in surrounding nebulae.
    Furthermore, stellar BHs show luminosity
    saturation.
  • The luminosity of ULXs fits the luminosity
    function of BHXRBs.
  • No dynamic evidence found so far by the motion of
    satellite objects.
  • No hyper-luminous stellar BH such as SS433 or GRS
    1915105 has been found in our Galaxy hosting an
    IMBHs. Upper limit is M 20 M?
  • Why in our Galaxy -where the determination of the
    mass functions is possible-, no IMBH is found ?
  • IMBHs may be there but are difficult to identify.

5
ANALOGOUS PHENOMENA IN BHs ACROSS THE RANGE OF
MASSES
  • Accretion-ejection coupling in microquasars and
    quasars (e.g. 3C120).
  • Analogous time lags in adiabatically expanding
    clouds in quasi-periodic flares of Sgr A and
    microquasars. Rotating blobs or jets ?
  • At low accretion rates the power is dominated by
    synchrotron, compact, flat spectrum jets, and
    universal correlations are being found.
  • In high accretion states there are
    non-relativistic outflows with masses as large as
    30 the accreting mass.
  • The joint action of massive outflows and jets
    heat and blow away the surrounding medium
    (ISM/IGM). Solve the cooling flow problem.
  • Bended disks re-direct the jets. This geometry
    could account for the unified model of AGN, and
    the large fraction of obscured AGN.
  • Inflow of mass jet collimation close to the BH
    in terms of the gravitational radius can be
    zoomed with better angular resolution in SMBH
    than in stellar-mass BHs.

6
BHs AS PROBES OF GRAVITY IN THE STRONG-FIELD
REGIME
  • Much of the radiation emerges within 6 Rg
  • BHs are determined by mass, spin and electric
    charge.
  • THE SPIN CAN BE DERIVED FROM
  • X-ray flux and temperature.
  • Skewed fluorescence iron lines.
  • QPOs of maximum fix frequency.

BH ASTROPHYSICS IS TODAY IN SIMILAR SITUATION AS
STELLAR ASTROPHYSICS IN THE FIRST DECADES OF THE
XX CENTURY. EMPIRICAL CORRELATIONS PRECEEDS THE
PHYSICAL UNDERSTANDING OF STARS AND BHs.
7
  • Thank to G. Matt, V. Karas and the local
    support !
  • have a good trip back home !
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