Abstract
An apparatus for the measurement of the Hall effect in materials of low mobility and high resistivity is described. An ac technique is used: The sample is rotated in a static magnetic field at 20 cps, an electric field is applied at 13⅓ cps, and the Hall signal, preamplified by field‐effect transistors mounted on the rotating shaft near the sample, is synchronously detected at 33⅓ cps. Hall mobilities as small as 0.2 cm2/Vsec in samples of resistance up to 109 Ω can be measured with negligible detector loading. A discussion is also given of the fundamental limitations of Hall effect measuring equipment. Typical Hall mobilities in iodine single crystals and in iodine complexed 1:1 with poly‐n‐vinyl carbazole are reported.

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