Optical Polarization of the Supernova in NGC 5253

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Scientific paper

IF a type I supernova is the result of the explosion of a star with a degenerate nucleus (see, for example, Baglin1) it is likely that a large magnetic field will be present in the radiating region for a short period following the outburst. Depending on the emission process a sufficiently large field could produce a measurable optical circular polarization. For example, for bremsstrahlung in an optically thick but very dilute plasma in an ordered magnetic field of H gauss, the fractional circular polarization in the optical continuum is q ~ 10-9 H (see refs. 2 and 3). If the degenerate progenitor of the supernova is entirely destroyed in the explosion, conservation of magnetic flux dictates that q would reach the limit of detectability (qLIM~3 × 10-6 : HLIM~3,000 G) in only 20 s for either a white dwarf (initial radius r0~109 cm, initial field H0~106 G) or a neutron star (r0~106 cm, H0~1012 G) assuming an expansion velocity of 104 km s-1. If a sizable fragment survives, however, a measurable polarization might be seen for a much longer period. For synchrotron emission smaller fields can produce a detectable polarization. According to Legg and Westfold4 a hypothetical field H~106 G in the Crab nebula would produce q~10% in the visible: since q ~ H½ a polarization qLIM~3 × 10-6 corresponds to HLIM ~ 10-3 G. However, the precise conditions strongly influence5,6 the relations between q and H; the interpretation would therefore be uncertain even if this mechanism were shown to be dominant. The influence of radiative transfer in the dense layers near the star and of a possible fluorescence emission in the outer layers of the shell7 would make the interpretation for the synchrotron process even more difficult.

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