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Giant radio pulses from the Crab pulsar
Institution:1. Max Planck Institute for Radioastronomy, Auf dem Hügel 69, D-53121 Bonn, Germany;2. Nicolaus Copernicus Astronomical Center, Rabiańska 8, 87-100 Toruń, Poland;3. Institut für Astronomie und Astrophysik LMU, Scheinerstr. 1, D-81679 München, Germany;4. Max Planck Institute for Extraterrestrial Physics, Postfach 1312, D-85741 Garching, Germany;5. Physics Department, New Mexico Institute of Mining and Technology, Soccoro, NM 87801, USA;1. Harvard-Smithsonian Center for Astrophysics, 60 Garden Street MS-70, Cambridge, MA 02138, USA;2. Jansky Fellow, National Radio Astronomy Observatory, and Harvard-Smithsonian Center for Astrophysics, 60 Garden Street MS-70, Cambridge, MA 02138, USA
Abstract:Individual giant radio pulses (GRPs) from the Crab pulsar last only a few microseconds. However, during that time they rank among the brightest objects in the radio sky reaching peak flux densities of up to 1500 Jy even at high radio frequencies. Our observations show that GRPs can be found in all phases of ordinary radio emission including the two high frequency components (HFCs) visible only between 5 and 9 GHz Moffett, D.A., Hankins, T.H. Multifrequency radio observations of the Crab pulsar. Astrophys. J. 468, 779–783, 1996]. This leads us to believe that there is no difference in the emission mechanism of the main pulse (MP), inter pulse (IP) and HFCs. High resolution dynamic spectra from our recent observations of giant pulses with the Effelsberg telescope at a center frequency of 8.35 GHz show distinct spectral maxima within our observational bandwidth of 500 MHz for individual pulses. Their narrow band components appear to be brighter at higher frequencies (8.6 GHz) than at lower ones (8.1 GHz). Moreover, there is an evidence for spectral evolution within and between those structures. High frequency features occur earlier than low frequency ones. Strong plasma turbulence might be a feasible mechanism for the creation of the high energy densities of ~6.7 × 104 erg cm?3 and brightness temperatures of ~1031 K.
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