Abstract
Thin films of Na, K, Rb, and Cs are quench condensed, then covered with 1/100 of a monolayer of Ti and finally covered with the original host. The magnetization of the films is measured by means of the anomalous Hall effect. An anomalous Hall resistance ${R}^{\mathrm{AHE}}$ is observed for Ti on the surface of K, Rb, and Cs and for Ti inside of Cs. Essentially the ${R}^{\mathrm{AHE}}$ varies linearly with the magnetic field and is inversely proportional to the inverse temperature. A small nonlinearity of ${R}^{\mathrm{AHE}}$ suggests a Ti moment of about $1{\ensuremath{\mu}}_{B}.$
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