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- W811945006 abstract "Using the technique of nuclear magnetic resonance on oriented nuclei, the magnetic hyperfine splitting frequencies ${ensuremath{nu}}_{M}=frac{g{ensuremath{mu}}_{N}{B}_{mathrm{HF}}}{h}$ of the 11/${2}^{ensuremath{-}}$ state in $^{195}mathrm{Au}$ (${T}_{frac{1}{2}}=31$ sec; $E=319$ keV) in Fe and Ni have been determined as ${ensuremath{nu}}_{M}(^{195}mathrm{Au}^{m}Fe)=979.8(4)$ MHz and ${ensuremath{nu}}_{M}(^{195}mathrm{Au}^{m}Ni)=226.3(2)$ MHz. Taking the known hyperfine fields of $^{197,198}mathrm{Au}$ in Fe and Ni and correcting for hyperfine anomalies a value of $|g|=1.123(17)$ is derived for the nuclear $g$ factor of $^{195}mathrm{Au}^{m}$.[RADIOACTIVITY $^{195}mathrm{Au}^{m}$ daughter of $^{195}mathrm{Hg}^{m}$ [from $^{194}mathrm{Pt}(ensuremath{alpha},3n)$]; measured ${I}_{ensuremath{gamma}}(ensuremath{theta},T,ensuremath{nu})$ of oriented states; NMR on oriented nuclei. $^{195}mathrm{Au}^{m}$ deduced $g$, $ensuremath{mu}$.]" @default.
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- W811945006 date "1981-08-01" @default.
- W811945006 modified "2023-09-25" @default.
- W811945006 title "gfactor of the 30.6 sec 11/2−isomerAum195" @default.
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- W811945006 doi "https://doi.org/10.1103/physrevc.24.631" @default.
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