2021
DOI: 10.1103/physrevc.104.l051301
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Evolution of single-particle structure near the N=20 island of inversion

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Cited by 9 publications
(2 citation statements)
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“…Well-documented islands of inversion are known to occur [535,536] at N = 8 [537], N = 20 [533,[537][538][539][540][541][542][543], N = 28 [49,544,545], N = 40 [50,[546][547][548][549][550][551], and N = 50 [534]. Merging of the IoIs occurring at N = 20 and N = 28 has been suggested in [49,545], while merging of the IoIs occurring at N = 40 and N = 50 has been proposed in [534,551].…”
Section: Islands Of Inversionmentioning
confidence: 99%
“…Well-documented islands of inversion are known to occur [535,536] at N = 8 [537], N = 20 [533,[537][538][539][540][541][542][543], N = 28 [49,544,545], N = 40 [50,[546][547][548][549][550][551], and N = 50 [534]. Merging of the IoIs occurring at N = 20 and N = 28 has been suggested in [49,545], while merging of the IoIs occurring at N = 40 and N = 50 has been proposed in [534,551].…”
Section: Islands Of Inversionmentioning
confidence: 99%
“…The energies for these two states cross at approximately Z = 10. Recent experimental information on the ESPE near 28 Mg and their interpretation similar to those of Figure 8 with a Woods-Saxon potential is given in [75]. For the FSU Hamiltonian, the loose binding effects are implicitly built into the monopole components of the TBME from the SVD fit to data on the BE and excitations energies.…”
Section: The Region Of 28 Omentioning
confidence: 97%