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Deformation parameters of the charge distribution and the optical potential for some nuclei in and near the rare earth region
66
Citations
19
References
1975
Year
Rare Earth MineralEngineeringNuclear PhysicsNuclear DataNuclear MaterialsMeteoriticsHigh-energy Nuclear ReactionPhysicsRare Earth RegionNuclear TheoryAtomic PhysicsNuclear EngineeringOptical-potential Deformation ParametersExperimental Nuclear PhysicsNatural SciencesParticle PhysicsApplied PhysicsInterference Data.nuclear ReactionsDeformation ParametersNeutron ScatteringExcitation FunctionsCharge Distribution
Elastic and inelastic scattering of $\ensuremath{\alpha}$ particles on $^{154}\mathrm{Sm}$, $^{166}\mathrm{Er}$, $^{168}\mathrm{Er}$, $^{182}\mathrm{W}$, $^{184}\mathrm{W}$, and $^{186}\mathrm{W}$ was performed with incident energies between 11 and 21 MeV. Excitation functions for ${0}^{+}$, ${2}^{+}$, and ${4}^{+}$ states of the ground-state rotational band were measured. Pronounced destructive nuclear-Coulomb interference effects were observed. Reduced $E2$ and $E4$ transition moments, and charge and optical-potential deformation parameters were determined from coupled-channel analysis of both the sub-Coulomb and interference data.NUCLEAR REACTIONS $^{154}\mathrm{Sm}(\ensuremath{\alpha}, {\ensuremath{\alpha}}^{\ensuremath{'}})$, $E=11\ensuremath{-}19$ MeV; $^{166}\mathrm{Er}(\ensuremath{\alpha}, {\ensuremath{\alpha}}^{\ensuremath{'}})$, $E=12.5\ensuremath{-}19.5$ MeV; $^{182}\mathrm{W}(\ensuremath{\alpha}, {\ensuremath{\alpha}}^{\ensuremath{'}})$, $E=13\ensuremath{-}21$ MeV; measured $\ensuremath{\sigma}({E}_{\ensuremath{\alpha}}, \ensuremath{\theta}=150\ifmmode^\circ\else\textdegree\fi{})$. $^{168}\mathrm{Er}(\ensuremath{\alpha}, {\ensuremath{\alpha}}^{\ensuremath{'}})$, $E=13\ensuremath{-}19$ MeV; $^{184}\mathrm{W}(\ensuremath{\alpha}, {\ensuremath{\alpha}}^{\ensuremath{'}})$, $E=12.5\ensuremath{-}19$ MeV; $^{186}\mathrm{W}(\ensuremath{\alpha}, {\ensuremath{\alpha}}^{\ensuremath{'}})$, $E=13.25\ensuremath{-}19$ MeV, measured $\ensuremath{\sigma}({E}_{\ensuremath{\alpha}}, \ensuremath{\theta}=140\ifmmode^\circ\else\textdegree\fi{}, 173.5\ifmmode^\circ\else\textdegree\fi{})$ deduced $\mathfrak{M}(E2)$, $\mathfrak{M}(E4)$, charge and optical potential deformations ${\ensuremath{\beta}}_{2}$ and ${\ensuremath{\beta}}_{4}$; coupled channel calculation.
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