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J is the current density, the zero magnetic field resistivity, a the H A L L coefficient, and M a second rank tensor which, when referred to the cubic axes, is diagonal and has the components B2, B22, B32. The magnetoresistance coefficients were determined experimentally at 4.2 °K from the change of resistance in transverse and longitudinal magnetic fields. Results are shown in Fig. 1 and Fig. 2. The axes of the rod shaped crystals examined were parallel to the [110] direction which is the most favourable orientation for determining b', c , and d'. The resistance ratio ^293 °kAR4 .2 °K ranged from 150 to 300. The small voltage drop across a sample was measured by means of a superconducting modulator 3.

Notizen: Low-Field Magnetoresistance of Copper and Silver Single Crystals