1974
DOI: 10.1016/0375-9474(74)90373-x
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The giant dipole resonance in the transition region of the samarium isotopes

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Cited by 120 publications
(104 citation statements)
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“…The IVD strengths of the K = 0 and |K| = 1 modes split in 154 Sm due to the ground state deformation, whereas those are identical for spherical 144 Sm. In both cases, FAM-QRPA shows a good agreement with the experimental data [53]: the typical frequency and width of the GDR can be well reproduced with our model parameters, with the smearing width of = 1.0 MeV. The plateau distribution for the deformed 154 Sm can be understood as a product of the split between K = 0 and |K| = 1 modes [13,14].…”
Section: A Benchmark Calculationsupporting
confidence: 72%
“…The IVD strengths of the K = 0 and |K| = 1 modes split in 154 Sm due to the ground state deformation, whereas those are identical for spherical 144 Sm. In both cases, FAM-QRPA shows a good agreement with the experimental data [53]: the typical frequency and width of the GDR can be well reproduced with our model parameters, with the smearing width of = 1.0 MeV. The plateau distribution for the deformed 154 Sm can be understood as a product of the split between K = 0 and |K| = 1 modes [13,14].…”
Section: A Benchmark Calculationsupporting
confidence: 72%
“…The TLO parametrization is compared with photoneutron cross sections for Sm-isotopes measured using positron-annihilation in flight [17]. see Fig.…”
Section: Triple Lorentzian Parameterisation Of the Gdrmentioning
confidence: 99%
“…For instance, the peak splitting of the giant dipole resonance (GDR), which is caused by the different frequencies of oscillation along the long and short axes, has been observed in experiments [4]. A typical example of the shape phase transition from spherical to deformed ground states and the evolution of deformation splitting in GDRs have been observed in Nd and Sm isotopes [2,3,4,5,6].…”
Section: Introductionmentioning
confidence: 99%