Abstract

Resonances of the rotational magnetic moments were observed in molecular beams of lithium hydride and lithium deuteride. The shape of the LiH rotational magnetic resonance curve was observed to be asymmetric and width of the curve was observed to increase with increasing magnetic field. These effects were ascribed to centrifugal stretching causing the magnetic moment per unit of angular momentum to vary with angular momentum. The variation was assumed to be of the form, /sub R//J = g/sub 0/ + CJ(J + 1), where /sub R/ is the rotational magnetic moment and J is the quantuim number of the total rotational angular momentum. The values of the constants g/sub 0/ and C assigned to LiH were: g/sub 0/ = -0.654 450 deg C in a 0.007 nuclear magneton and C (1.2 450 deg C in a 0.6) x 10/sup -4/ nuclear magneton. For LiD, these constants were found to be: g/ sub 0/ = -0.272 450 deg C in a 0.005 nuclear magneton and C = (3.4 450 deg C in a 1.7) x 10/sup -5/ nuclear magneton. The electric dipole moment and its polarity were calculated from the rotational magnetic moments of LiH and LiD. The results of thismore » calculation were /sub e/ = 5.9 450 deg C in a 0.5 debyes with the polarity Li/sup +/H/sup -/. The magnitude of the rotational magnetic moment resonance signals suggest the occurrence of multiple-quantum transitions, which may make possible the observation of rotational magnetic moment resonances in other molecules, even if the rotational gyromagnetic ratios are quite small. (auth)« less

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