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Gamma-ray bursts and hypernovae

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GRB as superstrong cosmic explosions. Association with supernovae a critical view ... HETE2: GRB-X-ray rich-XRF (Lamb et al. 2003) Apparently continuous. transition ... – PowerPoint PPT presentation

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Title: Gamma-ray bursts and hypernovae


1
Gamma-ray bursts and hypernovae
  • Konstantin Postnov
  • Sternberg Astronomical Institute
  • Moscow

Erice-2004, July 6, 2004
2
Outlook
  • Introduction
  • GRB as superstrong cosmic explosions
  • Association with supernovae a critical view
  • Thermal effects in ambient plasma
  • Conclusions

3
BATSE rate 1 per day No repetions, full isotropy
4
Brief 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 (?)

5
General 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

6
GRB spectra
  • Two power laws smoothly joined together (Band et
    al 1993)

Slopes a, ß and peak energy Epeak vary with time
7
Generally, spectrum gets softer
...but not always
8
and 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)
10
Amati 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?
11
Explanation 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

12
Basic 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

14
Evolution of massive stars Mlt25 M?? neutron
star Mgt25 M?? black hole Hypernova MNigt0.1
M? Ekingt1 foe Faint supernova
Nomoto et al.2004
15
Fireball 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

16
ES
RS
IS
G1
G2gt
?
Afterglow
GRB
17
Optical 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
18
Jet 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
19
Observed 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)
20
Evidence for associated SNe
  1. GRB980425 and peculiar type Ib/c SN 1998bw in
    nearby galaxy ESO184-g8 (z0.0085)

21
1998bw model light curve
22
SN2002ap spectral evolution modeling
23
2. Bumps in the late (10-30 days) optical
afterglows
24
Yet another case GRB 021211
25
Special cases GRB 030329 nearest (z0.168),
brightest (S10-4erg/cm2)
Host a SMC-like star-forming galaxy
26
SN 2003dh signature in light curve?
Difficult to directly accommodate!
27
SN2003dh spectral apperance (Matheson et al 2003)
28
Zooming in MMT spectra
29
Also in the VLT spectra
30
Detailed light curve
31
GRB030329 but earliest optical spectra (BTA 6m
telescope, Sokolov et al. 2003)
difficult to explain by shock breakout as pre-SN
must be compact!
32
Light-curve residuals could supernova do this?
33
Optical variability and polarisation suggests
structured environment
Greiner et al. 2003
34
List of GRB/SN associations
s
(from Dar 2004)
35
W49B 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?
36
Clues 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
37
Radio observations of GRB030329 (Taylor et al
2004)
  1. Directly reveal apparent superluminal expansion
    v3-5c, in accord with relativistic blast wave
    model for GRB afterglows
  2. 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)

38
But radio luminosities of GRB and SN1b/c are
strongly different (Berger et al.2003)
39
SN/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

40
Standard 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
41
Jet-corrected energy release (Frail et al)
Beaming-correction factor for the rate/energy
30-200
42
Radio calorimetry structured jet(Berger et al.
2003)
43
Current models universal jet vs uniform jet
44
Recent discoveries Light echo on dust for GRB
031203 (loc. INTEGRAL, X-ray rich)
45
GRB031203 SN 2003lw appears
46
HETE2 GRB-X-ray rich-XRF (Lamb et al. 2003)
Apparently continuous transition GRBgtX-ray
richgtXRF
47
X-ray flashes XRF 020903 localization
48
XRF 020903 host galaxy spectrum
Z0.251 Star-forming galaxy
49
Thermal effects in ambient plasma(Kosenko,
Blinnikov, Sorokina, PK, Lundqvist 2001, 2002)
Bisnovatyj-Kogan Timokhin 1997 First
consideration of environmental effects
50
Fading 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
51
Structured 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!
52
Mini-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
53
Statistical 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)
54
Problem 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)
55
Quantile diagrams for error-weighted GRB positions
56
Error-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)
57
Central 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)

58
Conclusions (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!

59
Conclusion (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(?)
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