Gravitational waves from GRBs - PowerPoint PPT Presentation

1 / 48
About This Presentation
Title:

Gravitational waves from GRBs

Description:

Maurice H.P.M. van Putten. Pisa 2003. LIGO. Edmonton 2004. Black holes, ... Black holes mass about 3e9 MSolar. Biretta et al. 2000. Machetto et al. 1997. LIGO ... – PowerPoint PPT presentation

Number of Views:34
Avg rating:3.0/5.0
Slides: 49
Provided by: maur114
Category:

less

Transcript and Presenter's Notes

Title: Gravitational waves from GRBs


1
Black holes, gamma-ray bursts and gravitational
waves
Maurice H.P.M. van Putten
Pisa 2003
Edmonton 2004
2
Active nuclei supermassive black holes
Biretta et al. 2000
Black holes mass about 3e9 MSolar
Machetto et al. 1997
3
Active nuclei stellar mass black holes
Mirabel Rodriques 1992
Black holes mass about 14 MSolar
Greiner et al. 2001
Greiner et al. 2001
4
BATSE Group, NASA http//image.gsfc.nasa.gov/docs/
science/know_l1/bursts.html
5
Vela/Konus (1963-1979)
6
BATSE (1991-2000)
BATSE on the CGRO (NASA)
7
Cosmological origin isotropic energy emissions
up to 1MSolar
8
Beppo-Sax (Italian-Dutch, 1996-2002)
9
GRBs with known redshifts
HETE-II
10
GRB-supernova in 1998?
GRB980425/SN1998bw (z0.008, D37Mpc)
Clear supernova signature GRB appeared to be
anomalously weak
11
GRBs a new class of supernovae
March 29 2003
Clear supernova signature GRB with near-typical
luminosity
12
Supernovae of massive stars
A black hole?
13
Compact objects out of which no particle or light
escapes (Michel 1794, Laplace 1798)
Black objects in Newtons theory of gravitation
14
Maxwell (1879) light described by EM waves with
c3e8m/s Einstein (1915) New spacetime
structure (a) abandon Newtons absolute
space and time, and (b) velocity of light c is
universal
Gravitation in this new spacetime has a new face
  • Gravitational redshift
  • Black holes (Schwarzschild 1916)
  • Rotating black holes (Kerr 1963)
  • Gravitational waves

15
Gravitational aging of Alice and Bluey
t
distance
16
t
distance
17
Black holes
Bluey freezes at Schwarzschild radius A
compact and featureless one-way membrane where
light may be absorbed, but from which no light
can escape
18
Rotating black holetorus
19
Frame-dragging around rotating black holes (Kerr
1963)
Frame-dragging around rotating black holes (Kerr
1963)
20
Spin-spin interactions between rotating objects
21
Shedding of like-angular momentum
repel
attract
22
Magnetic fields facilitate spin-connection to
black hole
Extracting energy through horizon Maxwell
stresses Ruffini Wilson (1975)
weak B accreted onto BH Blandford Znajek
(1977) strong B (force-free limit)
accreted onto BH Van Putten (1999), van Putten
Ostriker (2001) strong B around BH in
suspended accretion
23
(No Transcript)
24
(No Transcript)
25
Black hole-spin coupling to charged particles
B
A potential energy driving charged outflows
Van Putten 2000 Hawking 1975 Wald 1974
26
Black hole-luminosity creating a GRB
GRB

27
Frail et al. 01
True GRB-energies
Van Putten Regimbau 2003
Where does most of the black hole-spin energy go?
28
The three faces of a torus
The black hole needs a partner!
Slowing down black holes
Making supernovae
Making gravitational waves
29
Suspended accretion by spin-connection black
hole-to-torus
PSR
PSR -
BH
30
Most of black hole-luminosity is incident onto
the torus
Most of black hole-spin energy dissipated
unseen in the event horizon, slowly slowing
down the black hole
31
Radiation-driven supernova with X-ray
line-emissions
32
Frail et al. 01
Observed energies
33
LIGO Hanford site, WA
An ACIGA-LIGO Collaboration
similar LIGO Livingston, LA similar VIRGO in
Pisa, Italy
34
Gravitational radiation
Spin-2 waves
Theory agrees with observed orbital decay to
within 0.1 Nobel Prize 1993
35
Gravitational radiation from blobs
Both radiate at twice the Keplerian frequency
36
Radiation energies
Rotational energy of black hole
37
(1/year)
MGRB030329lt150MSolar (current LIGO sensitivity)
38
Simulation instantaneous S/N-ratio 0.15
D1
39
Simulation instantaneous S/N-ratio 0.15
D1
D2
40
Simulation instantaneous S/N-ratio 0.15
D1
D2
D1D2
41
Credits
Collaborators Amir Levinson (Tel Aviv) Hyun
Kyu Lee (Hanyang U) Chul H. Lee (Hanyang
U) Hongsu Kim (SNU) Tania Regimbau (MIT-LIGO)
Gregory M. Harry (MIT-LIGO) Michele Punturo
(VIRGO, INFN) Eve C. Ostriker (U Maryland) David
Coward (UWA) Ronald Burman (UWA)
Pisa 2003
Edmonton 2004
42
Conclusions
Observations GRBs originate in supernovae of
massive stars this solves the GRB-mystery! The
inner engine of GRB-SNe remains to be observed
Theory GRB-SNe from rotating black holes
produced in core-collapse of massive stars
GRBs produced by spin-orbit interactions to
charged particles along open magnetic flux-tubes
Radiatively driven supernovae produced by
black hole-spin energy through torus winds

We predict Most of black hole-luminosity
is catalyzed into gravitational radiation
(0.2MSolar_at_500Hz) Detection hereof provides
a method for establishing Kerr black holes as
physical objects
Upcoming gravitational wave-experiments (2008-)
promise to be exciting
43
first-ever detections of gravitational
radiation observing the Universe in
gravitational waves (new sources, relic waves
early universe,) probing the inner engines
of GRB-SNe observing life the process of
spin-down of Kerr black holes (within one
minute) testing fully nonlinear theory of
general relativity (serendipitous discoveries)
44
The end
45
(No Transcript)
46
Black hole-luminosity by shedding angular momentum
GRB
B
Van Putten 2000 Hawking 1975 Wald 1974
47
Questions/discussion 1. Audience Type of
SNe associated with GRBs 2. Ian MCarthur
(UWA) Origin of beaming 3. Igor Bray (IAP)
status of gravity 4. van Putten TeV-gravity
in early universe
48
Supernovae of massive stars (Mgt8MSolar)
Chandrasekhar (1931) maximal mass of a
degenerate object is 1.4MSolar Beyond
Chandrasekhar limit, further collapse into a
neutron star (Landau) Supernova explosion by
shock rebounce, or liberation of rotational
energy (Bisnovatii-Kogan 1970)
Exceeding the neutron star mass limit
a black hole the most compact object
Write a Comment
User Comments (0)
About PowerShow.com