By use of a radio‐frequency carrier and capacitive coupling it has been possible to measure the resistance and lifetime of silicon rods without making direct ohmic contact to the samples. Even with contacts, the use of an RF carrier to observe lifetime by photoconduction decay eliminates the need for insuring solid ohmic contacts as is required with a d‐c carrier. With low loss insulation between coupling capacitors and sample, an RF bridge will measure separately both the sample resistance between the coupling capacitors and the value of this coupling capacitance.

Hall measurements at room temperature have been used to determine the average net carrier density in polycrystalline silicon. The method does not require cutting of samples and destruction of the rods. Current contacts are made to the ends of a rod with strips of metal foil; Hall contacts are made with two titanium blades which close on the rod. Hall measurements made this way on single-crystal zone-refined rods agree with measurements on samples cut from the rods in the conventional manner. The average carrier densities measured in the polycrystalline rods have been correlated with the resistivities of these same rods after one, two, three floating zone passes. Measurement of Whole IngotsThe conventional bridge-shaped samples used for Hall measurements require that an ingot be sawed up and thus partially destroyed. It would obviously be advantageous to make Hall measurements on an ingot of semiconductor material without cutting it up (1). This was done with the apparatus ~ shown in Fig. 1. The holder was made of Lucite and was clamped between the poles of a Varian 4-in. electromagnet. The sample (which was a round ingot) was placed in the V-shaped blocks of Lucite and rested on a knife-edge titanium blade which formed one Hall contact. A pivoted Lucite arm carrying the other titanium blade Hall contact was placed on top of the sample and was held down with a nonmagnetic (lead) weight. The pivoted arm could be moved laterally by an adjusting screw to align the top blade accurately above the lower blade; this adjustment eliminated the IR voltage between the Hall contacts, so that the measured Hall voltage was zero when the magnetic field was zero. Current contacts to the sample were made on the ends of the ingot either by ultrasonic soldering with indium, by

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