It is shown that previous measurements on the magnetic susceptibility of oxygen in a clathrate compound can be explained if it is assumed that the molecule, instead of being completely free as previously assumed, is subject to a potential V0(1 —cos 2θ) with V0/k = 32° K. θ is the angle between the figure axis of the molecule and the c axis of the crystal. The susceptibility measurements were extended down to 0⋅25° K and showed good agreement with the theory.
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H. Meyer (1958) studied this question.
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