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GammaRay Burst Afterglows Prospects for the NSU Rapid Response Robotic Telescope

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Title: GammaRay Burst Afterglows Prospects for the NSU Rapid Response Robotic Telescope


1
Gamma-Ray Burst AfterglowsProspects for the
NSURapid Response Robotic Telescope
  • David McDavid
  • Department of Astronomy
  • University of Virginia
  • June 22, 2004

2
Outline
  • 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

3
RRRT Collaboration
  • Norfolk State University
  • University of Virginia
  • NASA Goddard Space Flight Center

4
NSU 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

5
GCNThe GRB Coordinates Network
  • (an example based on pre-Swift configuration)

6
Decay 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

7
Small 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

8
The 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).

9
Origin 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

10
SynchrotronRadiation
  • 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.

11
Why 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.

12
Kepler'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.

13
Observational 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.

14
Polarization of the OpticalAfterglow of GRB
030329
15
Reality 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.

16
Acknowledgements
  • 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
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