AGN, GAMMA RAYS, & BLACK HOLE EVAPORATION

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AGN, GAMMA RAYS, & BLACK HOLE EVAPORATION
4/6/20

 AGN, GAMMA RAYS, &
 BLACK HOLE EVAPORATION
 HOMEWORK #7 AVAILABLE ON WEBWORK – DUE WEDNESDAY, 4/15, AT
 11:59PM EDT

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 AGN, GAMMA RAYS, &
 BLACK HOLE EVAPORATION
 Accretion disks in AGN
 Gamma-ray bursts & black hole formation
 Hawking’s “area increase” theorem
 Entropy and the area of the event
 horizon: the thermodynamics of black
 holes
 Quantum-mechanical vacuum fluctuations
 and the emission of light by black hole:
 “Hawking radiation”
 Evaporation of black holes
 Exotic matter
 Virtual particles near a black hole’s horizon (S.W. Hawking)

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AGN, GAMMA RAYS, & BLACK HOLE EVAPORATION
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 TYPES OF AGN
 Radio galaxy Seyfert galaxy
 • Elliptical galaxy with active nucleus at • Spiral galaxy with active nucleus at center
 center
 • Zero, one, or two jets
 • Two jets, visible in the radio

 Quasar Blazar
 • Galaxy with active nucleus at center • Galaxy with active nucleus at center
 • One jet, visible in the radio (line of sight is • Extremely bright, no jets (line of sight is
 close to jet axis) along the jet axis)

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 A B C D

 FIND THE ACTIVE GALAXY
 Which of these is a visible-light picture of a radio galaxy?

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 A B C D

 FIND THE ACTIVE GALAXY
 Which of these is a radio image of a radio galaxy?

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 A B C D

 FIND THE ACTIVE GALAXY
 Which of these is a visible-light picture of a Seyfert galaxy?

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AGN, GAMMA RAYS, & BLACK HOLE EVAPORATION
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 MATTER FALLING INTO AGN BLACK HOLES: LARGE
 ACCRETION DISKS

 The disk-shaped collection of matter surrounding the black hole in an AGN arises rather
 naturally from the influence of the black hole on stars and other material in the galactic center.
 • Stars in a galaxy perpetually interact with each other’s gravity as well as the gravity of the
 galaxy at large.
 • These interactions – long-range collisions – usually result in transfers of energy and
 momentum between stars. Two stars, originally in similar orbits and undergoing such a
 collision, will usually find themselves pushed to different orbits: one going to a smaller-
 circumference orbit and the other going to a larger orbit.

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 MATTER FALLING INTO AGN BLACK HOLES: LARGE
 ACCRETION DISKS

 Thus, some stars are pushed to the very
 center of the galaxy after a number of these
 encounters. What happens if there is a black
 hole there?
 • The star begins to fall in, but the spin of its
 orbital motion and the tidal forces that
 tend to rip the star apart keep this from
 happening all at once.
 • Stellar material spreads out into a rotating,
 flat distribution around the black hole: the
 beginnings of an accretion disk.

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 AGN ACCRETION DISK FORMATION
 Eventually, the tidally-disrupted material from many stellar encounters settles down into a
 flattened disk. Collisions among particles in the disk cause material to lose its spin and become
 accreted by the black hole. The disk is thus gradually consumed.

 Black hole horizon
 Perspective view

 Accretion disk
 Can contain − ⊙
 and extend hundreds of ly
 from the black hole
 Rotation of disk

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 OPERATION OF AGN ACCRETION DISKS

 • Recall that for non-spinning black holes, orbits with circumference less than 3 $ are unstable,
 and no orbits exist with circumference less than 1.5 $ . Within this volume, the disk structure
 breaks down and material tends to stream in toward the horizon.
 • A large amount of power, mostly in the form of X-rays and -rays, is emitted by the infalling
 material. Pressure exerted by this light slows down the rate at which accretion takes place.
 • Much of this high-energy light is absorbed by the disk which heats up and re-radiates the
 energy as longer wavelength light.
 • Heated disk = compact central object seen in radio images of radio galaxies and quasars.

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 OPERATION OF AGN ACCRETION DISKS

 • Some of the particles absorbing the highest-energy light are accelerated to speeds
 approaching that of light. If their velocity takes them into the disk, they just collide with the
 disk material and lose their energy to heat. If their velocity takes them perpendicular to the
 disk, they may escape (Blandford & Rees 1975).
 • High-speed particles escaping perpendicular to the disk = jets seen in radio and visible images of
 radio galaxies and quasars. Their high speeds (approaching ) explain the one-sidedness and
 “faster than light” motion of quasar jets.
 • Several other possibilities exist for jet acceleration.

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 STRUCTURE OF AN AGN ACCRETION DISK
 Jet
 Innermost stable orbit

 Ingoing: matter, Outgoing: X and g rays,
 heating disk and accelerating
 being accreted
 jets

 Accretion disk (cross-section view)

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 DISK AT THE CENTER OF RADIO GALAXY NGC 4261

 Jaffe et al. (1996)

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 GAMMA-RAY BURSTS

 • The -ray bursts (below) come
 from locations spread randomly
 and uniformly all over the sky. This
 is very different from non-burst -
 ray sources (above).
 • Bright sources of -rays: neutron
 stars or black holes?
 • There is no tendency for the -ray
 bursts to cluster in the Milky Way,
 which would be the case if their
 sources were stellar remnants.

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 ANALYSIS OF THE GAMMA-RAY BURST DISTRIBUTION

 Obviously, -ray bursts are not numerously distributed throughout our galaxy as the stars are.
 What other explanations are there?
 • Very nearby objects that are evenly distributed on the sky, like the very nearest stars, or the
 cloud of comets surrounding the Solar system.
 • But how would these objects emit -rays?
 • Very distant objects. Distant galaxies and galaxy clusters are evenly distributed on the sky.
 • But if the -ray bursts are that far away, their energy outputs are (problematically) enormous.

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 -RAY BURSTS ORIGINATE IN DISTANT GALAXIES
 Green crosses indicate where the bursts were seen; all lie within distant galaxies (Andy Fruchter, STScI)

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 TWO TYPES OF -RAY BURSTS

 The -ray bursts come in two major
 varieties: long (> 2 s, typically 30 s) and
 short (typically 0.01-0.1 s).
 • The short bursts are also less luminous
 and emit a larger fraction of their -
 rays at the highest energies observed
 than the long bursts.

 Histogram of BATSE -ray bursts

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 LONG BURSTS OCCUR IN
 STAR-FORMATION REGIONS
 Their afterglows resemble supernovae.
 Images of the -ray burst of 23 January
 1999, taken with the STIS instrument on
 the HST 16, 59, and 380 days after the
 outburst (Andy Fruchter, STScI). It faded
 at the same pace supernovae do.

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 SHORT BURSTS DO NOT
 The NASA Swift satellite, launched in 2004, was built with visible-UV (UVOT) and X-ray (XRT)
 telescopes along with a -ray detector (BAT) that can sort more finely by burst duration.
 • Swift has found and localized many more GRBs than was previously possible, including
 examples at the greatest distances at which galaxies have been detected.
 • Swift also localized short bursts for the first time and showed that they do not resemble
 supernovae.

 Visible afterglow of the short -ray burst of 7/9/2005, pictured by HST 6, 10, 19, and 35 days after Swift discovered it.
 It fades too fast to be a supernova. (Derek Fox, Penn State U.)

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 EXTRAGALACTIC ORIGIN: -RAY BURSTS ARE EXTREMELY
 ENERGETIC

 The spectrum of the galaxy in which the -ray burst of January 23, 1999 lives indicates that its
 distance is 39 billion light years.
 • At that distance, the -ray burst amounted to an energy of × erg in -rays alone, if it
 emitted its energy uniformly in all directions.
 • For scale: that is equivalent to a mass of
 3×10() erg
 = = 3.3×10++ g = 1.7 ⊙
 *
 suddenly (in a span of about 40 seconds) converted completely into -rays.

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 -RAY ENERGY IS PROBABLY LESS THAN THAT…

 • The most efficient way to produce lots of -rays quickly is in shock waves within exploding
 relativistic jets.
 • Assuming, therefore, an explosion violent enough to be relativistic, and noting that relativistic
 objects tend to emit light mostly in the direction they are going…
 • As is the case with quasar / radio galaxy radio jets.
 • …the same brightness could be produced with a smaller energy: smaller by a factor of about
 ,!
 1− , where is the outward speed of the explosion.
 -!

 • That reduces the energy requirement to about erg. Still a huge amount of energy,
 considering the short time and the fact that it is all -rays.

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 WHAT ARE THE SOURCES OF -RAY BURSTS?
 10(* erg is an awful lot of energy to release in less than one minute, and -rays are an extreme form for
 the energy to assume.
 • 10 ordinary supernovae account for this much emitted light, but it would take months and would do so
 at much longer wavelengths.
 • The entire Milky Way emits this much light in about 10 years, but it also does so with much longer
 wavelength light.
 So, it is difficult to imagine how to do this with normal stellar processes. But, now you know about more
 powerful tools. How about:
 • Accretion of a very massive compact object by a black hole (compact, so the accretion does not take
 very long) and radiation of much of its mass energy?
 • Formation of a rapidly-spinning black hole, and driving a relativistic expansion with its ergosphere?
 (Requires strong magnetic fields threading the ergosphere.)

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 LEADING CONTENDERS FOR THE SOURCES OF -RAY BURSTS

 • Binary neutron stars, coalescing to form a black hole? Observationally confirmed as a source
 of short bursts.
 • Neutron star – black hole binary, with the neutron star captured by the black hole?
 • Hypernova (a.k.a. Collapsar): collapse of a very massive (50 − 120 ⊙ ) star to form a black
 hole, accompanied by a supernova-like explosion?
 • Currently-favored model for long bursts
 • Works even better with collapse that follows soon after a binary-star merger
 Maybe all three mechanisms are represented among the sources. All involve black hole
 formation or growth. All three naturally produce rapidly spinning black holes. All should be
 rare processes.

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 GW170817 – A NS-NS MERGER
 • On August 17, 2017, LIGO and VIRGO
 detected a gravitational wave signal, the
 intensity and frequency of which matched
 the theoretical values for a NS-NS merger.
 • 1.7 seconds after the GW reached us, Fermi
 and INTEGRAL detected a short GRB
 coming from the same region in the sky.
 • Follow-up observations were made with
 numerous telescopes over the following
 hours, days, and weeks across the EM
 spectrum. These observations were
 consistent with the debris ejected from a
 NS-NS merger (a fast-moving, rapidly- Artist’s impression of a NS-NS merger (Dana Berry, NASA)
 cooling cloud of neutron-rich material).

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 “Pair production”
 150 ⊙ supernova (no BH
 produced)

 FATES OF THE MOST “Quiet” BH
 120 ⊙
 MASSIVE STARS formation
 CXO/CfA/NASA
 100 ⊙
 Hypernova/
 GRB/SN II
 50 ⊙

 20 ⊙ Ordinary
 SN II
 10 ⊙

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 BLACK HOLE FORMATION?
 SN 2006gy, in NGC 1260 (238 Mly away) was
 the most luminous supernova every observed
 (100 times more luminous than the naked-
 eye-visible SN 1987a, a Type II SN). Swift
 detected no -ray burst, but a relatively weak
 X-ray emission is seen in the afterglow.
 Is SN 2006gy most likely to be
 A. An ordinary (I or II) supernova
 B. A NS-NS or NS-BH merger
 C. BH formation from stellar collapse (plus
 hypernova)
 D. An extraordinary supernova, but not
 linked to BH formation

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 BLACK HOLE FORMATION?
 On March 19, 2008, a simultaneous burst was seen by
 Swift at , X, and UV wavelengths, and by the Pi of the
 Sky camera at visible wavelengths. The brightest part
 of the burst – bright enough to have been seen with
 the naked eye – was about 30 seconds long.
 Which of the following events is this most likely to be?
 A. An ordinary (I or II) supernova
 B. A NS-NS or NS-BH merger
 C. BH formation from stellar collapse (plus
 hypernova)
 D. An extraordinary supernova, but not linked to BH
 formation

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 THE HORIZON AREA THEOREM

 In 1970, Stephen Hawking used general relativity to prove a useful rule called the horizon area
 theorem:
 The total horizon area in an enclosed system containing black holes never decreases. It can
 only increase or stay the same.

 Increases in total horizon area come from growth of black holes by collapse or accretion of
 “normal” matter, and by the coalescence of black holes.

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