Abstract

We present a simple device, which allows us to determine the areal mass density of thin targets in UHV with an accuracy better than 3%. It is a modification of the principle used by Andersen et al. [Nucl. Instr. and Meth. 149 (1978) 137]. We compare the Rutherford backscattering rate from a reference target to that of the target under investigation. Both targets are alternately exposed to the beam. As a reference target we use a polished cone made of commercial aluminum alloy, which rotates at constant speed upstream of the measured target. In this way, we can obtain absolute stopping cross sections of highly reactive targets, produced in-situ by evaporation.

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