Abstract
DURING the period September 1–December 31, 1963, observations of the polarization of radio-wave emission from Jupiter were made at 15.2, 16.2, 18.2, 22.2, and 24.2 Mc/s. The Southwest Research Institute two-helix polarimeter1, utilizing a twin channel receiver, was expanded so that determination of the cross-correlation of the right and left circular components, in addition to the two opposite circular components, was made separately for each Jupiter burst. This type of radio polarimeter scheme has been described by Cohen2. The calibrated polarimeter thus provided determination of the polarization fraction (m), axial ratio (r) and sense of the Jupiter bursts observed.
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References
Sherrill, W. M., and Castles, M. P., Astrophys., J., 138, 587 (1963).
Cohen, M. H., Proc. Inst. Rad. Eng., 46, 172 (1958).
Ellis, G. R. A., and McCulloch, P. M., Austral. J. Phys., 16, 380 (1963).
Dowden, R. L., Austral. J. Phys., 16, 398 (1963).
Carr, T. D., et al., Astrophys. J., 134, 105 (1961).
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SHERRILL, W. Polarization of Jovian Emission at Decametre Wave-lengths. Nature 205, 270–271 (1965). https://doi.org/10.1038/205270a0
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DOI: https://doi.org/10.1038/205270a0
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