2018
DOI: 10.1016/j.nuclphysa.2018.09.040
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Low-energy dipole strength in even–even 152–164Dy isotopes within the quasiparticle random phase approximation (QRPA) including symmetry restoring interactions

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Cited by 13 publications
(6 citation statements)
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“…In this study, the high-lying E1 excitations were systematically investigated within the TGI-QPNM in oddmass [153][154][155][156][157][158][159] Eu nuclei for the first time. The QPNM [49,50] model used for odd-mass nuclei is an upper version of the QRPA [51,52] model, which successfully explains dipole excitations in even-even deformed nuclei. However, this success is possible by the restoration of the symmetries, such as rotational, translational, and Galilean, broken due to nuclear mean-field approximations or by isolating the spurious states mixing to real dipole excitations.…”
Section: Introductionmentioning
confidence: 99%
“…In this study, the high-lying E1 excitations were systematically investigated within the TGI-QPNM in oddmass [153][154][155][156][157][158][159] Eu nuclei for the first time. The QPNM [49,50] model used for odd-mass nuclei is an upper version of the QRPA [51,52] model, which successfully explains dipole excitations in even-even deformed nuclei. However, this success is possible by the restoration of the symmetries, such as rotational, translational, and Galilean, broken due to nuclear mean-field approximations or by isolating the spurious states mixing to real dipole excitations.…”
Section: Introductionmentioning
confidence: 99%
“…In the calculations, the mean-field-potential was set as the axially symmetric deformed Woods-Saxon potential [59]. The isovector spin-spin interaction parameter was set as χ στ = 20/A MeV [48], while the isovector dipole-dipole interaction parameter was set to be χ 1 =300/A 5 /3 MeV•fm −2 [60]. The pairing parameters (D and l) and the mean-field deformation parameter (δ 2 ) are given in table 1.…”
Section: Resultsmentioning
confidence: 99%
“…In the employed model, by selecting suitable separable, effective isoscalar and isovector forces, the rotational invariance (RI-) was restored to describe the magnetic dipole (M1) excitations [17,[37][38][39], as well as the translational and Galilean invariance (TGI-) [9,19] for calculating the E1 excitations. This model also satisfactorily described the fragmentation of electric and magnetic dipole strength in well-deformed [40][41][42][43][44][45][46][47][48][49][50][51], transitional, and γ-soft [9,10,13,19] nuclei, as well as the giant dipole resonance and pygmy dipole resonance [40, 42-44, 46, 49, 50] in deformed nuclei [17, 37, 40-48, 52, 53].…”
Section: Introductionmentioning
confidence: 87%
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“…The importance of spin-spin forces is not only limited to the description of the spin polarization effect and ground-state magnetic properties in odd-A nuclei, it is also known that the spin-dependent part of neutron-proton interactions is responsible for the Gammow-Teller β transitions between the low energy levels of the nuclei [45,46]. More importantly, the studies performed to now show that spin-spin forces have successfully explained 1+ excitations and scissor mode in even-even nuclei [47][48][49][50][51][52][53][54][55][56]. For these reasons, it is very important to determine the spin-spin interaction parameters that are the subject of this article.…”
Section: K πmentioning
confidence: 99%