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Haidinger's brush

Visible effect of polarised light

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Through Pigment

Many people are able to perceive polarization of light. Haidinger's brushes may be seen as a yellowish horizontal bar or bow-tie shape (with "fuzzy" ends, hence the name "brush") visible in the center of the visual field against the blue sky viewed while facing approximately 90° from the sun, or on any bright background. Haidinger's yellow bar is observed perpendicular to the direction of light polarization (i.e., if light polarization is vertical, then Haidinger's yellow bar is observed horizontal - like around dawn and dusk, the natural skylight maximum polarization around the north and south horizon is almost vertical as per Rayleigh sky model and so Haidinger's yellow bar is observed horizontal). The perception of this effect vanishes within a few seconds due to neural adaptation unless the observer rotates the eyes (like by moving the head sideways). It typically occupies roughly 3–5 degrees of vision, about twice or three times the width of one's thumb held at arm's length. Fainter bluish or purplish areas may be visible between the yellow brushes (see illustration). Haidinger's brush may also be seen by looking at a white area on many LCD flat panel computer screens (due to the polarization effect of the display), in which case it is often diagonal.

Physiological causes

Haidinger's brush is usually attributed to the dichroism of the xanthophyll pigment found in the macula lutea. As described by the Fresnel laws, the behavior and distribution of oblique rays in the cylindrical geometry of the foveal blue cones produce an extrinsic dichroism. The size of the brush is consistent with the size of the macula.

It is thought that the macula's dichroism arises from some of its pigment molecules being arranged circularly; (the small proportion of circularly arranged molecules accounts for the faintness of the phenomenon.) Xanthophyll pigments tend to be parallel to the retinal ganglion cell axons that (because the fovea is not flat) are almost orthogonal to the fovea in its central part but nearly parallel in its outer region. As a result, two different areas of the fovea can be sensitive to two different degrees of polarization.

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