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Pulsar radio emission geometry

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dc.contributor.author Gangadhara, R. T
dc.date.accessioned 2009-07-03T13:56:17Z
dc.date.available 2009-07-03T13:56:17Z
dc.date.issued 2008
dc.identifier.citation Hasan, S. S., Gangadhara, R. T. and Krishan, V. eds., Turbulence, dynamos, accretion disks, pulsars and collective plasma processes, First Kodai-Trieste workshop on plasma astrophysics held at the Kodaikanal Observatory., Astrophysics and space science proceedings., Kodaikanal., India, 2007., pp. 113 - 135 en
dc.identifier.isbn 978-1-4020-8867-4
dc.identifier.uri http://hdl.handle.net/2248/4618
dc.description Restricted Access en
dc.description The original publication is available at springerlink.com
dc.description.abstract Pulsar radio emission is belived to come from relativistic plasma accelerated along the dipolar magnetic field lines in pulsar magnetosphere. The beamed emission by relativistic sources occur in the direction of tangents to the field lines in the corotating frame, but in an inertial (lab) frame it is aberrated toward the direction of rotation. To receive such a beamed emission line-of-sight must align with the source velocity within the beaming angle 1/γ, where γ is the Lorentz factor of the source. By solving the viewing geometry, in an inclined and rotating dipole magnetic field, we find the coordinates of the emission region in corotating frame. Next, give a general expression for the phase shift in the intensity profile in lab frame by taking into account of aberration, retardation and polar cap currents. en
dc.language.iso en en
dc.publisher Springer Netherlands en
dc.relation.uri http://dx.doi.org/10.1007/978-1-4020-8868-1_8 en
dc.relation.uri http://adsabs.harvard.edu/abs/2008tdad.conf..113G en
dc.rights © Springer en
dc.subject Astrophysical Turbulence en
dc.subject Pulsar en
dc.subject Dynamos en
dc.subject Solar and Space Plasmas en
dc.subject Radio Emission en
dc.subject Geometry en
dc.title Pulsar radio emission geometry en
dc.type Article en


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