Nuclear magnetic resonance absorption peaks have been observed for seventeen nuclear species. The technique used in observing the resonances involves the use of super-regenerative oscillators and is different in many respects from the bridge method of Purcell and the nuclear induction method of Bloch. Resonance absorption has been observed for the following nuclei: ${\mathrm{H}}^{1}$, ${\mathrm{H}}^{2}$, ${\mathrm{Li}}^{7}$, ${\mathrm{Be}}^{9}$, ${\mathrm{B}}^{11}$, ${\mathrm{F}}^{19}$, ${\mathrm{Na}}^{23}$, ${\mathrm{Al}}^{27}$, ${\mathrm{P}}^{31}$, ${\mathrm{Cu}}^{63}$, ${\mathrm{Cu}}^{65}$, ${\mathrm{Br}}^{79}$, ${\mathrm{Br}}^{81}$, ${\mathrm{Rb}}^{85}$, ${\mathrm{Rb}}^{87}$, ${\mathrm{I}}^{127}$, and ${\mathrm{Cs}}^{133}$. By comparison of various resonance peaks with the proton resonance peak observed simultaneously in the same magnetic field, values for nuclear gyromagnetic ratios and nuclear magnetic moments can be determined in terms of the gyromagnetic ratio and the magnetic moment of the proton. The following frequency ratios have been obtained:
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