The Nuclear Spin and Magnetic Moment ofLi6
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Abstract
The spin of the ${\mathrm{Li}}^{6}$ nucleus and the h.f.s. separation of the $^{2}S_{\frac{1}{2}}$ normal state have been measured by the atomic beam method of zero moments. The evaluation of the contribution of ${\mathrm{Li}}^{7}$ to the intensity in the neighborhood of the ${\mathrm{Li}}^{6}$ zero moment peak was made by an extension of the method of analysis previously used in determining the spin of ${\mathrm{K}}^{41}$ and ${\mathrm{Rb}}^{87}$. The spin of ${\mathrm{Li}}^{6}$ was found to be 2/2 and the h.f.s. separation 0.0077\ifmmode\pm\else\textpm\fi{}0.0001 ${\mathrm{cm}}^{\ensuremath{-}1}$ on the basis of the value of Fox and Rabi for ${\mathrm{Li}}^{7}$. The ratio of the magnetic moments of the isotopes is $\frac{{\ensuremath{\mu}}_{6}}{{\ensuremath{\mu}}_{7}}=0.258\ifmmode\pm\else\textpm\fi{}0.5$ percent. From the value calculated by Breit and Doerman for ${\mathrm{Li}}^{7}$, the moment of ${\mathrm{Li}}^{6}$ is 0.85 nuclear magneton.
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