2021
DOI: 10.1103/physrevc.103.064307
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Nuclear charge-exchange excitations based on a relativistic density-dependent point-coupling model

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Cited by 19 publications
(24 citation statements)
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“…For all three nuclei shown in Fig. 1, the non-perturbed IV-spin-M1 strength is equal to the higher-energy GT(−) strength: R M1 ∼ = R GT(−) (E x ) with E x = 13, 6.6, and 8.5 MeV in 16 O, 42 Ca, and 48 Ca, respectively. By analyzing the transition components, this equivalence can be explained from the identical set of quasi-particle transitions.…”
Section: A Non-perturbed Responsementioning
confidence: 91%
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“…For all three nuclei shown in Fig. 1, the non-perturbed IV-spin-M1 strength is equal to the higher-energy GT(−) strength: R M1 ∼ = R GT(−) (E x ) with E x = 13, 6.6, and 8.5 MeV in 16 O, 42 Ca, and 48 Ca, respectively. By analyzing the transition components, this equivalence can be explained from the identical set of quasi-particle transitions.…”
Section: A Non-perturbed Responsementioning
confidence: 91%
“…That is, ν(1d 5/2 ) −→ ν(1d 3/2 ) in IV M1, and ν(1d 5/2 ) −→ π(1d 3/2 ) in GT(−), for 18 O, where the symbol π (ν) indicates the proton (neutron) state. Similarly for 42,48 Ca,…”
Section: A Non-perturbed Responsementioning
confidence: 95%
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