Title: GammaRay Burst Afterglows Prospects for the NSU Rapid Response Robotic Telescope
1Gamma-Ray Burst AfterglowsProspects for the
NSURapid Response Robotic Telescope
- David McDavid
- Department of Astronomy
- University of Virginia
- June 22, 2004
2Outline
- RRRT Collaboration
- Observatory plan
- The GRB Coordinates Network
- Examples of GRB optical afterglow monitoring
- The Supernova Connection
- Theory of the origin of GRB OAs
- Synchrotron radiation
- Why study polarization of OAs?
- A lesson from Kepler's Supernova Remnant
- Observational technique imaging polarimetry
- Reality Check
- Acknowledgements
3RRRT Collaboration
- Norfolk State University
- University of Virginia
- NASA Goddard Space Flight Center
4NSU RRRT ObservatoryFan Mountain, Virginia
- 0.6-m (24-in) aperture reflecting
telescope - CCD camera for optical imaging and
polarimetry of GRB afterglows - connection to Swift for rapid response to
GRB trigger - robotic (automatic) and remote (NSU)
control modes
5GCNThe GRB Coordinates Network
- (an example based on pre-Swift configuration)
6Decay of an Optical Afterglow(HST Photometry
Example)
- GRB 990123
- power law decay of brightness f(t)
f0t -a - breaks (changes in value of a) give
info on changes of physical conditions
in radiation source
7Small Telescope Success Story!!GRB 030329 SN
Connection Burstnearby (2.3 Gly) ?
exceptionally bright
- monitoring with small telescopes
beginning 76 min after the burst - apertures 20-60cm (8-24in)
- continuous data for 11 hours
- result evidence for deviation from
power-law decay in early afterglow
8The Supernova ConnectionGRB 030329 / SN 2003dh
- One of the most luminous supernovae
on record, and the one with the highest
measured velocities, was
observed to accompany a GRB. - This was interpreted as evidence that GRBs
are associated with the deaths of massive
stars (core collapse).
9Origin of Optical Afterglows(currently accepted
working hypothesis)
- rotating black hole remnant of a collapsed
massive star (double?) produces jet of
relativistic electrons, positrons, and ?-rays - OA is synchrotron emission from shock front
between jet and surrounding medium
10SynchrotronRadiation
- Synchrotron radiation is produced by
relativistic charged particles in
strong magnetic fields. - The radiation is beamed along the velocity
vector of the charged particle. - A characteristic spectrum results from the
frequency of pulsation of the beam across
the line of sight with each spiral
revolution. - The radiation is linearly polarized
perpendicular to the magnetic field.
11Why study polarization of OAs?
- Spectra and light curves of GRB afterglows
match a synchrotron radiation
model over a wide range of frequencies. - Synchrotron radiation is highly polarized
(up to 70), as verified in many
astrophysical cases. - Optical polarization of GRB afterglows
is small, (rarely greater than 2),
so theories of the origin of OAs must
explain this.
12Kepler's Supernova Remnantpolarization dilution
by spatial averaging
- GRB afterglows appear as unresolved point
sources of light because they are so distant. - Localized patches may have strong magnetic
fields and high polarization, but the net
polarization is small unless the fields are
globally aligned.
13Observational TechniqueImaging Polarimetry
UsingDouble Refraction
- An optically corrected calcite prism
produces double polarized images
which can be analyzed by aperture
photometry to give the polarization of
each object in the field. - Errors from seeing and transparency
variations vanish since they affect
both images equally.
14Polarization of the OpticalAfterglow of GRB
030329
15Reality Check
- GRB afterglows are difficult to observe with
small telescopes since most of them are faint. - Swift pointing is an advantage.
- GRB polarimetry data are scarce, inconclusive,
and subject to error in statistical analysis. - There is much room for improvement.
- Interpretation of GRB polarimetry is complicated
because multiple physical effects may be
present - intrinsic
- interstellar (Galactic host galaxy)
- associated supernova
- Any variability must be due either to the GRB or
to the associated SN.
16Acknowledgements
- Official NASA Swift Home Page (http//swift.gsfc.n
asa.gov/) - The GRB Coordinates Network (http//gcn.gsfc.nasa.
gov/) - The Decay of an Optical Afterglow (HST
Photometry) - Andrew Fruchter, STScI
(http//www-int.stsci.edu/fruchter/GRB/990123/
index.html) - Small Telescope Success Story
- Uemura et al. 2003, Nature, 423, 843
- Rie Sato, Tokyo Institute of Technology
(http//www.hp.phys.titech.ac.jp/nkawai/030329/ind
ex_e.html) - The Supernova Connection
- Hjorth et al. 2003, Nature, 423, 847
- NASA Goddard Space Flight Center Top Story
(http//www.gsfc.nasa.gov/topstory/2003/0618rosett
aburst.html) - Origin of Optical Afterglows
- Meszaros, P. 2001, Science, 291, 79
- Penn State Swift Page (http//www.swift.psu.edu/)
- Synchrotron spectra and light curves of GRB
afterglows - Panaitescu, A. and Kumar, P. 2001, ApJ, 554, 667
- Kepler's Supernova Remnant
- DeLaney et al. 2002, ApJ, 580, 914
- XMM-Newton X-ray Observatory
- Imaging Polarimetry by Double Refraction