2015
DOI: 10.1103/physrevc.92.014608
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Relativistic Coulomb excitation inMg32near 200 MeV/nucleon with a thick target

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Cited by 13 publications
(13 citation statements)
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“…[39] were employed, which were demonstrated to lead to a good agreement with the known B(E2)↑ value for 32 Mg in Ref. [35]. For inelastic scattering on the carbon target, respective nuclear deformation lengths of δ N = 1.98(11) and 1.93(11) fm were determined for 30 Ne and 36 Mg, corresponding to nuclear deformation parameters of β N = 0.53(2) and 0.49 (2), assuming the radius R = , with β C = δ C /R and R = 1.2A 1/3 fm, is applied.…”
Section: Resultssupporting
confidence: 54%
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“…[39] were employed, which were demonstrated to lead to a good agreement with the known B(E2)↑ value for 32 Mg in Ref. [35]. For inelastic scattering on the carbon target, respective nuclear deformation lengths of δ N = 1.98(11) and 1.93(11) fm were determined for 30 Ne and 36 Mg, corresponding to nuclear deformation parameters of β N = 0.53(2) and 0.49 (2), assuming the radius R = , with β C = δ C /R and R = 1.2A 1/3 fm, is applied.…”
Section: Resultssupporting
confidence: 54%
“…An analysis of the feeding from levels between 2 and 5 MeV for the well-known nucleus 32 Mg yielded 14(3)% at similar beam energies [35]. In the present case, the proximity of the neutron drip-line and the low neutron separation energies of 3430(300) and 3330(490) keV for 30 Ne and 36 Mg [36] should reduce this contribution by more than 50%.…”
Section: Resultsmentioning
confidence: 46%
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“…Many other 32 Mg properties such as the excess binding [1], the reduced 2 + 1 energy [7], and the enhanced B(E2; 2 + 1 → 0 + 1 ) value [5,[20][21][22][23][24] are consistent with 2p2h configurations dominating the low-energy states. However, the 4p4h configurations appear essential to reproduce the known properties of the long-lived (τ > 10 ns) 0 + 2 state reported at 1058 keV [6].…”
mentioning
confidence: 99%