James C. Kemp

Circular polarimetry of fifteen interesting objects.

The results of a search are presented for circular polarization of visible light in 15 objects, including two eclipsing binaries, six magnetic Ap stars, three planetary nebulae, Hubbles Nebula, M87, Sirius, and the Orion A region. On the whole, the results were null, down to typical upper limits for q of 0.01 per cent. A complete description of the used photoelastic polarimeter is given, with special attention to the incidental linear-circular conversion.

NGC 1068, 3C 273, and Scorpius X-1 - Circular polarization disputed.

Discussion of data for the Seyfert galaxy NGC 1068, the quasar 3C 273, and the X-ray source Sco X-1, for all of which it has been claimed or strongly suggested that they have large circular polarization of the order of 1% (Severny et al., 1971). In contrast the present authors obtained unambiguously null results with upper limits about 0.05% for NGC 1068 and 3C 273. For Sco X-1 no statistically significant polarization was found on three nights, and only some marginal evidence for a fluctuation or transient polarization on one night.

Interstellar Circular Polarization of Upper Scorpius Stars

Circular polarization of interstellar or perhaps circumstellar origin has been clearly established in two reddened stars in the Upper Scorpius region, o-Sco and σ-Sco A; and detected preliminarily in a third, HD 154445. In the Corning 5–60 filter band λλ 3800–4600, measured values of 104 q were: o-Sco, -(2.9 ± 0.2); σ-Sco A, -(1.7 ± 0.2); and HD 154445, +(2.8 ± 0.8). Complete wavelength dependences q(λ) for o-Sco and σ-Sco A are under study, but so far are known to have the following similarity. Each shows a broad maximum (of negative q) centered in the range λλ 3800–4300; and the values are smaller by a factor ~ 4, but still negative, in the range λλ 5000–6000. The effect here is most likely due to a twisting grain alignment along the line of sight. In that case a simple model predicts q(λ) ∝ (n′ ι – n′ r ) • (n″ ι - n″ r ) θ0 z 0 2, where n = n′+ i n″ is a formal, complex refractive index (in van de Hulst’s forward-scattering approximation), l and r referring to longitudinal and transverse grain axes, and θ 0 is the total twist angle over the interaction length z0. An alternate mechanism would be multiple scattering (at large angles, not along the line of sight) within asymmetrical, well-localized clouds around the individual stars. The similar sign and magnitudes of q for o-Sco and σ-Sco A, which are 1.5° apart in the sky, argue for the line-of-sight mechanism — for example through a large cloud in front of the entire local region. Comparative studies of many stars in Upper Scorpius will be of obvious interest.