1976•Physical Review LettersOpen access

Splitting and Structure of the Giant Quadrupole Resonances in Deformed Nuclei

Dieter Zawischa, Josef Speth

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Abstract

We have performed microscopic calculations of the low-lying and high-lying ${K}^{\ensuremath{\pi}}={0}^{+}, {1}^{+}, \mathrm{and} {2}^{+}$ states in deformed rare-earth nuclei. The centroids of the isoscalar giant quadrupole resonance in $^{160}\mathrm{Dy}$, $^{170}\mathrm{Yb}$, and $^{184}\mathrm{W}$ are at 11.58, 11.44, and 11.22 MeV, respectively. A broadening of these resonances due to the deformation is predicted which varies appreciably in the different nuclei. About 20% of the monopole strength is found in the same energy range.

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We have performed microscopic calculations of the low-lying and high-lying ${K}^{\ensuremath{\pi}}={0}^{+}, {1}^{+}, \mathrm{and} {2}^{+}$ states in deformed rare-earth nuclei. The centroids of the isoscalar giant quadrupole resonance in $^{160}\mathrm{Dy}$, $^{170}\mathrm{Yb}$, and $^{184}\mathrm{W}$ are at 11.58, 11.44, and 11.22 MeV, respectively. A broadening of these resonances due to the deformation is predicted which varies appreciably in the different nuclei. About 20% of the monopole strength is found in the same energy range.

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Available abstract

We have performed microscopic calculations of the low-lying and high-lying ${K}^{\ensuremath{\pi}}={0}^{+}, {1}^{+}, \mathrm{and} {2}^{+}$ states in deformed rare-earth nuclei. The centroids of the isoscalar giant quadrupole resonance in $^{160}\mathrm{Dy}$, $^{170}\mathrm{Yb}$, and $^{184}\mathrm{W}$ are at 11.58, 11.44, and 11.22 MeV, respectively. A broadening of these resonances due to the deformation is predicted which varies appreciably in the different nuclei. About 20% of the monopole strength is found in the same energy range.

Key concepts: Isoscalar, Physics, Quadrupole, Atomic physics, Magnetic monopole, Resonance (particle physics), Deformation (meteorology), Range (aeronautics)

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