Algorithm for localization of a gamma-burst source using three satellites

1981 ◽  
Vol 75 (1) ◽  
pp. 31-34
Author(s):  
G. A. Mersov
Keyword(s):  
1981 ◽  
Vol 75 (1) ◽  
pp. 219-224 ◽  
Author(s):  
G. S. Bisnovaty-Kogan ◽  
I. V. Estulin ◽  
N. G. Havenson ◽  
V. G. Kurt ◽  
G. A. Mersov ◽  
...  

1981 ◽  
Vol 30 (1-4) ◽  
pp. 467-470 ◽  
Author(s):  
G. Pizzichini ◽  
J. Danziger ◽  
P. Grosb� ◽  
M. Tarenghi ◽  
T. L. Cline ◽  
...  

1981 ◽  
pp. 467-470
Author(s):  
G. Pizzichini ◽  
J. Danziger ◽  
P. Grosbøl ◽  
M. Tarenghi ◽  
T. L. Cline ◽  
...  

1986 ◽  
Vol 89 ◽  
pp. 305-321
Author(s):  
Richard I. Epstein

AbstractThe power per logarithmic bandwidth in gamma-ray burst spectra generally increases rapidly with energy through the x-ray range and does not cut off sharply above a few MeV. This spectral form indicates that a very small fraction of the energy from a gamma-ray burst source is emitted at low energies or is reprocessed into x-rays and that the high-energy gamma rays are not destroyed by photon-photon interactions. The implications are that the emission mechanism for the gamma-ray bursts is not synchrotron radiation from electrons that lose most of their energy before being re-accelerated and that either the regions from which the gamma rays are emitted are large compared to the size of a neutron star or the emission is collimated and beamed away from the stellar surface.


2004 ◽  
Vol 11 (3) ◽  
pp. 411-420 ◽  
Author(s):  
G. Thejappa ◽  
R. J. MacDowall

Abstract. Short wavelength ion sound waves (2-4kHz) are detected in association with the Langmuir waves (~15-30kHz) in the source regions of several local type III radio bursts. They are most probably not due to any resonant wave-wave interactions such as the electrostatic decay instability because their wavelengths are much shorter than those of Langmuir waves. The Langmuir waves occur as coherent field structures with peak intensities exceeding the Langmuir collapse thresholds. Their scale sizes are of the order of the wavelength of an ion sound wave. These Langmuir wave field characteristics indicate that the observed short wavelength ion sound waves are most probably generated during the thermalization of the burnt-out cavitons left behind by the Langmuir collapse. Moreover, the peak intensities of the observed short wavelength ion sound waves are comparable to the expected intensities of those ion sound waves radiated by the burnt-out cavitons. However, the speeds of the electron beams derived from the frequency drift of type III radio bursts are too slow to satisfy the needed adiabatic ion approximation. Therefore, some non-linear process such as the induced scattering on thermal ions most probably pumps the beam excited Langmuir waves towards the lower wavenumbers, where the adiabatic ion approximation is justified.


2017 ◽  
Vol 851 (2) ◽  
pp. 151 ◽  
Author(s):  
Patrick I. McCauley ◽  
Iver H. Cairns ◽  
John Morgan ◽  
Sarah E. Gibson ◽  
James C. Harding ◽  
...  

1983 ◽  
Vol 270 ◽  
pp. 226 ◽  
Author(s):  
L. Cominsky ◽  
W. Ossmann ◽  
W. H. G. Lewin
Keyword(s):  

1994 ◽  
Vol 423 ◽  
pp. 436 ◽  
Author(s):  
A. Claret ◽  
A. Goldwurm ◽  
B. Cordier ◽  
J. Paul ◽  
J.-P. Roques ◽  
...  
Keyword(s):  

1982 ◽  
Vol 254 ◽  
pp. L1 ◽  
Author(s):  
G. Hammerschlag-Hensberge ◽  
J. van Paradijs ◽  
J. E. McClintock
Keyword(s):  

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