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Magnetic Dipole and Electric Quadrupole Moments of the First 2+ State of Sm154

Roscoe M. Wheeler, Uzi Atzmony, J. C. Walker

Open publisher page 11 citations

Abstract

The hyperfine interactions of the first excited ${2}^{+}$ state of ${\mathrm{Sm}}^{154}$ have been measured in Sm${\mathrm{Cl}}_{3}$\ifmmode\cdot\else\textperiodcentered\fi{}6${\mathrm{H}}_{2}$O and SmIG at 4.2\ifmmode^\circ\else\textdegree\fi{}K, using the M\"ossbauer effect following Coulomb excitation. The results in Sm${\mathrm{Cl}}_{3}$\ifmmode\cdot\else\textperiodcentered\fi{}6${\mathrm{H}}_{2}$O have been used to determine the magnetic dipole and electric quadrupole moments ${\ensuremath{\mu}}^{154}=(0.778\ifmmode\pm\else\textpm\fi{}0.036){\ensuremath{\mu}}_{N}$ and ${Q}^{154}(1\ensuremath{-}R)=\ensuremath{-}1.33\ifmmode\pm\else\textpm\fi{}0.46$ b, respectively. ${\ensuremath{\mu}}^{154}$ has been used to determine ${H}_{\mathrm{eff}}=3.04\ifmmode\pm\else\textpm\fi{}0.12$ MG in SmIG at 4.2\ifmmode^\circ\else\textdegree\fi{}K. This value for ${H}_{\mathrm{eff}}$ (SmIG) agrees with the value used by Atzmony et al. to measure ${{g}_{R}}^{152}$ in SmIG; thus their value for ${{g}_{R}}^{152}$ is confirmed. An improved technique for using the M\"ossbauer effect following Coulomb excitation is reported.

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What this paper is about

The hyperfine interactions of the first excited ${2}^{+}$ state of ${\mathrm{Sm}}^{154}$ have been measured in Sm${\mathrm{Cl}}_{3}$\ifmmode\cdot\else\textperiodcentered\fi{}6${\mathrm{H}}_{2}$O and SmIG at 4.2\ifmmode^\circ\else\textdegree\fi{}K, using the M\"ossbauer effect following Coulomb excitation. The results in Sm${\mathrm{Cl}}_{3}$\ifmmode\cdot\else\textperiodcentered\fi{}6${\mathrm{H}}_{2}$O have been used to determine the magnetic dipole and electric quadrupole moments ${\ensuremath{\mu}}^{154}=(0.778\ifmmode\pm\else\textpm\fi{}0.036){\ensuremath{\mu}}_{N}$ and ${Q}^{154}(1\ensuremath{-}R)=\ensuremath{-}1.33\ifmmode\pm\else\textpm\fi{}0.46$ b, respectively. ${\ensuremath{\mu}}^{154}$ has been used to determine ${H}_{\mathrm{eff}}=3.04\ifmmode\pm\else\textpm\fi{}0.12$ MG in SmIG at 4.2\ifmmode^\circ\else\textdegree\fi{}K. This value for ${H}_{\mathrm{eff}}$ (SmIG) agrees with the value used by Atzmony et al. to measure ${{g}_{R}}^{152}$ in SmIG; thus their value for ${{g}_{R}}^{152}$ is confirmed. An improved technique for using the M\"ossbauer effect following Coulomb excitation is reported.

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Available abstract

The hyperfine interactions of the first excited ${2}^{+}$ state of ${\mathrm{Sm}}^{154}$ have been measured in Sm${\mathrm{Cl}}_{3}$\ifmmode\cdot\else\textperiodcentered\fi{}6${\mathrm{H}}_{2}$O and SmIG at 4.2\ifmmode^\circ\else\textdegree\fi{}K, using the M\"ossbauer effect following Coulomb excitation. The results in Sm${\mathrm{Cl}}_{3}$\ifmmode\cdot\else\textperiodcentered\fi{}6${\mathrm{H}}_{2}$O have been used to determine the magnetic dipole and electric quadrupole moments ${\ensuremath{\mu}}^{154}=(0.778\ifmmode\pm\else\textpm\fi{}0.036){\ensuremath{\mu}}_{N}$ and ${Q}^{154}(1\ensuremath{-}R)=\ensuremath{-}1.33\ifmmode\pm\else\textpm\fi{}0.46$ b, respectively. ${\ensuremath{\mu}}^{154}$ has been used to determine ${H}_{\mathrm{eff}}=3.04\ifmmode\pm\else\textpm\fi{}0.12$ MG in SmIG at 4.2\ifmmode^\circ\else\textdegree\fi{}K. This value for ${H}_{\mathrm{eff}}$ (SmIG) agrees with the value used by Atzmony et al. to measure ${{g}_{R}}^{152}$ in SmIG; thus their value for ${{g}_{R}}^{152}$ is confirmed. An improved technique for using the M\"ossbauer effect following Coulomb excitation is reported.

Key concepts: Physics, Quadrupole, Excited state, Excitation, Atomic physics, Mössbauer effect, Magnetic moment, Hyperfine structure

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