2018
DOI: 10.1007/s12043-017-1503-z
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Dipole and spin-dipole strength distributions in $$^{124,126,128,130}\mathrm {Te}$$124,126,128,130Te isotopes

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Cited by 9 publications
(7 citation statements)
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“…For the TGI-QPNM calculations, the strength parameter of the isovector dipole-dipole interaction has been chosen to be χ 1 =300 A −5/3 MeVfm −2 . This value of χ 1 gives reasonably good results in explaining the observed E1 transitions at the energies below 4 MeV and in the PDR region in both spherical [53] and deformed even-even nuclei [54].…”
Section: Resultssupporting
confidence: 64%
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“…For the TGI-QPNM calculations, the strength parameter of the isovector dipole-dipole interaction has been chosen to be χ 1 =300 A −5/3 MeVfm −2 . This value of χ 1 gives reasonably good results in explaining the observed E1 transitions at the energies below 4 MeV and in the PDR region in both spherical [53] and deformed even-even nuclei [54].…”
Section: Resultssupporting
confidence: 64%
“…Pyatov method is a suitable way to restore broken symmetries [48,49]. This method is used to restore Rotational, Translational, and Galilean symmetries in deformed nuclei [41][42][43][44][45][46][47][48][49][50][51][52][53][54]. In this way, the coupling constant and matrix elements of the effective interactions can be found self-consistently for the radial part of the mean-field potential and explicitly separate the zero energy branch of the excitation related to the spurious state [51].…”
Section: Restoration Of Broken Symmetriesmentioning
confidence: 99%
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“…where | ñ core is the core with its Fermi level at some magic number. The detail solutions of the GT and FF transitions for the odd−A nuclei can be seen from [20,21].…”
Section: Extension For Odd-a Nucleimentioning
confidence: 99%