Title: Gamma-ray bursts and hypernovae
1Gamma-ray bursts and hypernovae
- Konstantin Postnov
- Sternberg Astronomical Institute
- Moscow
Erice-2004, July 6, 2004
2Outlook
- Introduction
- GRB as superstrong cosmic explosions
- Association with supernovae a critical view
- Thermal effects in ambient plasma
- Conclusions
3BATSE rate 1 per day No repetions, full isotropy
4Brief course of history of GRBs
- 1967- Discovery by American military Vela
satellite - 1973 Declassified for scientific community
- End of 1970s Konus experiments onboard
Russian Veneras - (E.P.Mazets et al)
- 1991-2000 BATSE (CGRO) era. Largest
homogeneous data (a few thousands) on GRBs.
Debates on galactic vs extragalactic origin - 1997- Afterglow era. Discovery of afterglows in
X-ray (BeppoSAX, 1997), optical, radio. Triumph
of cosmological model for (long) GRB origin.
Multivawelength GRB astronomy -
- 1998 possible association of GRB980425 with
nearby peculiar type Ic SN1998bw. Start of
hypernova era (?)
5General properties
- Observed
- Duration 0.1-1000 s
- Fluence S10-7-10-3 erg/cm2
- Spectrum nonthermal,
- 10keV-100 MeV
- Variability high, 1-10 ms
- Rate 1 per day
- Location z0.17-4.5, (but 980425 z0.0085),
star-forming galaxies - Associated events X-ray (100), optical (70),
radio (50) afterglows - F(t)t-a a1-2
- Environment signatures transient X-ray
em./abs. lines, metal rich material
- Derived (for long GRBs only!)
- Isotropic energy release
- E?4pdl2/(1z) 1051 -1054 erg (but 980425
1048) - Evidence for jets from afterglow breaks
?j0.01-0.1 - Points to standard energy release
?E1050-1051erg equally shared in kinetic energy
and radiation - Photon energy correlations
- vF?Eiso
- Association with SN Ib/c
6GRB spectra
- Two power laws smoothly joined together (Band et
al 1993)
Slopes a, ß and peak energy Epeak vary with time
7Generally, spectrum gets softer
...but not always
8and even gets harderGRB 941017 (Gonzalez et
al. 2003)
EGRET-TASC detection Duration 150 s A new,
very hard component appeared E2 FEE1,
Epeakgt200 MeV Signals hadronic component
(UHECR) with subsequent photomeson
interactions? (Dermer Atoyan,2004)
9(Gonzalez et al.03)
10Amati et al. (02,03) Eiso-z, Ep-Eiso
correlations
22 events with known z and spectra
Lg Epeak0.45 lg Eiso
Are older GRB more energetic?
11Explanation of GRB spectra (not fully
satisfactory)
- Standard synchrotron shock model (SSM)
- Optically thin synchrotron radiation by
energetic electrons left to radiate without
further acceleration. Electrons are accelerated
by the Fermi mechanism in relativistic shocks
created by the central engine (dN/dEE-p,
p2.2-2.3) - BUT many individual GRB do not fit this!
Additional acceleration, IC, change in electron
energy index p with time, etc., etc., etc. are
invoked
12Basic model ultrarelativistic (Ggt100) jets
associated with hyperstrong (1051 erg)
explosion (a hypernova)
13- Term hypernova introduced by B.Paczynski
(1998) according to energy release in an
explosive cosmic event - Nova (thermonuclear explosion on white dwarf
surface) ?E 10-9M?c21045erg - galactic rate 1 per a few year
- Supernova (core collapse of massive star,
SNII,Ib,Ibc or th/n explosion of a WD with
MCh(mPl/mp)3mp 1.3 M?) - ?E 10-1M?c21053erg (binding energy of
neutron star, mostly in neutrino) - kinetic energy 1050erg (binding energy
of stellar envelope) - galactic rate 1 per a few 10s years
- ? Hypernova (core collapse associated with black
hole formation? Requires the most extremal
conditions e.g.B1015G, rapid rotation, etc.) - ?E? 1051-52erg
- kinetic energy gt1051erg
- galactic rate 1 per a few 104-106 years
14Evolution of massive stars Mlt25 M?? neutron
star Mgt25 M?? black hole Hypernova MNigt0.1
M? Ekingt1 foe Faint supernova
Nomoto et al.2004
15Fireball models for GRBs
- Rees Meszaros (1992, 1994) Recent review
Piran 2004 - Thermal energy of explosion is converted to
kinetic energy of thin baryon shell with
ultrarelativistic speed (Ggt100) to avoid
compactness problem and explain non-thermal
spectra - GRB is produced by internal (most likely) shocks
within the expanding shell, or by external shock
in inhomogeneous ISM. - Internal shocks ? GRB itself, external shock in
ISM ? X-ray, optical, radio emission of the GRB
afterglow - Initial interaction of GRB ejecta ? Reverse shock
propagating inward and decelerating fireball
ejecta. Erases the memory of the initial
conditions. Expansion approaches self-similarity
(Blandford McKee solution, 1976) GBMr-3/2 - (simply from E0(4p/3)r3n0 mpc2G2 )
- Parameters E0, no (const or 1/r2), G0, p, eB, ee
16ES
RS
IS
G1
G2gt
?
Afterglow
GRB
17Optical afterglows (synchrotron emission from
relativistic blast wave in ISM)
Early reverse shock in the ejecta
990123
Late external shock in ISM
021211
Breaks in ag lc decelerated jet
18Jet beaming effect in the GRB light curves
T1/G(t)t3/8
?0
G(r)r-3/2t-3/8 tr/G2
r
Emitting area Ar2?2r2/G2G4 t2/G2t10/8,
?lt?0,tlttj
Ar2?02G4t2t1/2, ?gt?0, tgttj
T(tj)?0
? A increases slower after tgttj
19Observed emission(emitting area)x(specific
intensity) For SSM, I(B2?e2)
G(eBG2)(eeG2)GG5t-15/8 so F(tlttj) AxI
t10/8t-15/8 t-5/8 F(tgttj)
t1/2t-15/8 t-11/8
?00.16(n0/E0,iso)1/8(tj/days)3/8 E?E0,iso(?o2/2
) E0,iso4pdl(z)2S/(1z)
20Evidence for associated SNe
- GRB980425 and peculiar type Ib/c SN 1998bw in
nearby galaxy ESO184-g8 (z0.0085)
211998bw model light curve
22SN2002ap spectral evolution modeling
232. Bumps in the late (10-30 days) optical
afterglows
24Yet another case GRB 021211
25Special cases GRB 030329 nearest (z0.168),
brightest (S10-4erg/cm2)
Host a SMC-like star-forming galaxy
26SN 2003dh signature in light curve?
Difficult to directly accommodate!
27SN2003dh spectral apperance (Matheson et al 2003)
28Zooming in MMT spectra
29Also in the VLT spectra
30Detailed light curve
31GRB030329 but earliest optical spectra (BTA 6m
telescope, Sokolov et al. 2003)
difficult to explain by shock breakout as pre-SN
must be compact!
32Light-curve residuals could supernova do this?
33Optical variability and polarisation suggests
structured environment
Greiner et al. 2003
34List of GRB/SN associations
s
(from Dar 2004)
35W49B a hypernova remnant? (Keohane et al. 2004)
red molecular hydrogen 2.12µ (Palomar Hale
WIRC) green 1.64µ FeII (Palomar Hale
WIRC) blue Fe Ka (Chandra). No NS. HN
explosion in a molecular cloud a few thousand
yrs ago?
36Clues from radio observations
- Radio scintillations in ISM Fresnel radius 5
µas?direct measurement of angular size ? evidence
for relativistic motion (970508, 030329) - Vapp 4c
Frail et al. 1997
37Radio observations of GRB030329 (Taylor et al
2004)
- Directly reveal apparent superluminal expansion
v3-5c, in accord with relativistic blast wave
model for GRB afterglows - Inconsistent with cannonball model prediction for
plasmoid superluminal motion (Dado et al 2004)
(NB general problem for CB model is absence of
rapid radio diffractive scintillations in
GRB030329, though the expected anglular size of
plasmoids 0.01 µas ltlt Fresnel (5 µas ) scale)
38But radio luminosities of GRB and SN1b/c are
strongly different (Berger et al.2003)
39SN/GRB rates
- SNIbc in spiral galaxies 0.2/100yrs/1010L?(B)
- Local univesre 108L?(B) Mpc-3
- SNIbc rate 2 104Gpc-3
- GRB rate 250 Gpc-3 (factor 3-10 uncert. due
to collimation) - Only a few percent of SNIbc can be associated
with GRBs (unlike CB model). Additional
conditions (e.g. binarity etc.) must be imposed
on the progenitors
40Standard energy issue
- Postnov, Prokhorov and Lipunov 1999, 2001 (idea)
- Standard explosions ?E 5x1051 ergs
- Structured jets
Frail et al. 2001 standard energy from
jet-corrected afterglow observations. Berger et
al. 2003 structured jets from radio calorimetry
of GRB 030329, 980425
41Jet-corrected energy release (Frail et al)
Beaming-correction factor for the rate/energy
30-200
42Radio calorimetry structured jet(Berger et al.
2003)
43Current models universal jet vs uniform jet
44Recent discoveries Light echo on dust for GRB
031203 (loc. INTEGRAL, X-ray rich)
45GRB031203 SN 2003lw appears
46HETE2 GRB-X-ray rich-XRF (Lamb et al. 2003)
Apparently continuous transition GRBgtX-ray
richgtXRF
47X-ray flashes XRF 020903 localization
48XRF 020903 host galaxy spectrum
Z0.251 Star-forming galaxy
49Thermal effects in ambient plasma(Kosenko,
Blinnikov, Sorokina, PK, Lundqvist 2001, 2002)
Bisnovatyj-Kogan Timokhin 1997 First
consideration of environmental effects
50Fading X-ray emission lines in 011211
Reves et al XMM observations of fading (10 ks)
emission lines
Kosenko et al 2002 thermal cooling of
plasma clouds heated by GRB
N106 1-3AU-sized clds ne1011 cm-3 within 0.1
pc are needed
51Structured environment from X-ray and optical
variability
Jakobsson et al.2004, ?t1 hr in optical
and X-ray afterglows
0.5-10 keV
3-5 AU structures!
52Mini-SN effects (Blinnikov Postnov 1997) on
clouds
1.Optical thickness increases with plasma cooling
? appearance of effective photosphere
2. Clouds cool down producing bumps in
afterglow lc
53Statistical analysis of GRB distribution inside
host galaxies (Dasha Kosenkos talk on Wed. July
7)
Bloom et al 2000, 2001 Tsvetkov et
al 2001 Kosenko et al 2004
Basic idea to compare GRB distribution with
other astronomical objects (SNe, XRB)
54Problem GRB error boxes are (still) a few
arcsec-arcmin ? no straightforward comparison can
be made
Quantile-diagrams (surface density)
DM NFW, rs 15 kpc (right) rs 4 kpc (left)
55Quantile diagrams for error-weighted GRB positions
56Error-weighted GRB distribution vs NFW and
Burkert DM profiles
rs 15 kpc
rs4 kpc
Dark matter NFW profile (cuspy) ?(r)
1/(r/rs)(1(r/rs))2
Burkert (w/o cusp) ?(r) 1/(1r)(1r2)
57Central engine
- Requirements
- Energy 1051 erg (thermal or Poynting-dominated)
- Collimation ?01-20 degrees
- Long short GRBs (two different engines?)
- Rate 0.1-1 of SN rate
- Variability dt1 ms ? compact object GRB
duration T10-100 s ? prolong activity - Models
- Collapsar 10 M? black hole 0.1 M? accretion
disk formed in a hypernova explosion - Poynting-dominated energy release by rapidly
rotating strongly magnetized newborn neutron star
(Usov 1992) - Binary neutron star merging (for short GRBs)
58Conclusions (statements)
- GRBs are (rare) violent cosmic explosions in
remote galaxies some of them are associated with
extremely strong (Ekingt 1051 erg) peculiar SNe
(hypernovae) - GRB power (1044erg/yr/Mpc3) is comparable with
UHECR power - GRB explosions produce ultrarelativistic jets and
drive strong shocks in the ambient medium - Environmental effects are important in shaping
GRB afterglows - We understand better GRB afterglows than GRB!
59Conclusion (Issues to be solved)
- Are all GRB (including short/hard) and XRF
really universal (jets? energies? Off-axis jets?) - Do GRB really associate with core-collapse
supernovae and (rotating) black hole formation? - Which is the mechanism for gamma-ray emission
(relativistic shocks? If yes, internal vs
external shocks?) - Hot (fireball) or cold (Poynting-dominated) jets?
- Association with dark matter? (Are there
elliptical hosts?) - Close expectations SWIFT mission (sep 04) X-op
afterglows, rapid alerts, good statistics
(100/yr) - More remote future GLAST mission (06),
high-energy neutrinos(?), gravitational waves(?)