2005
DOI: 10.1103/physrevc.72.064327
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β-decay of the neutron-rich nucleusN18

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Cited by 51 publications
(83 citation statements)
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“…As an illustration of three-body force effects on the symmetry energy, we quote in the following results of a study [121] using the MDI energy density functional [43]. The latter has been used extensively in both simulating heavy-ion reactions [58,122,123] and studying properties of neutron stars [124,125,126,127,128,129]. It is developed from a modified Gogny-type interaction within the Hartree-Fock approach [43].…”
Section: The Role Of the Spin-isospin Dependence Of Three-body Forcesmentioning
confidence: 99%
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“…As an illustration of three-body force effects on the symmetry energy, we quote in the following results of a study [121] using the MDI energy density functional [43]. The latter has been used extensively in both simulating heavy-ion reactions [58,122,123] and studying properties of neutron stars [124,125,126,127,128,129]. It is developed from a modified Gogny-type interaction within the Hartree-Fock approach [43].…”
Section: The Role Of the Spin-isospin Dependence Of Three-body Forcesmentioning
confidence: 99%
“…[380]. The rectangular region (solid black lines) of I ⋆ = [1.29 − 1.62] × 10 45 g cm 2 and R = [11.5 − 13.6] km represents the constraints on I and R from analyzing heavy ion collision data [122,123,124,125]. As explained in Ref.…”
Section: Symmetry Energy Effects On the Moment Of Inertia Of Slowly Rmentioning
confidence: 99%
“…Nuclear symmetry energy E sym (ρ) and the equation of state (EOS) of pure neutron matter (PNM) E PNM (ρ) have profound impact on many important physics problems in nuclear physics and astrophysics [1][2][3][4][5] as well as some issues in new physics beyond the standard model [6][7][8][9][10]. For instance, the density dependence of the symmetry energy or neutron matter EOS at subsaturation densities is intimately related to the neutron skin thickness of finite nuclei [11][12][13][14][15][16][17][18][19][20][21][22][23], the properties of neutron star crust [23][24][25][26], the cluster formations in nuclear matter at low densities [27][28][29][30][31], and the isospin diffusion in heavy ion collisions at Fermi energies [32][33][34][35].…”
Section: Introductionmentioning
confidence: 99%
“…After passing through the 25-μm kapton foil, which separated the vacuum of the beam line from the air, and a stack of aluminum degraders, the neutron-rich ions were finally transported into the target chamber filled with low-temperature nitrogen and implanted in a 1500-μm-thick double-side Si strip detector (DSSD) of 50 mm×50 mm. The experiment was performed in the continuous beam mode, which has a higher beam efficiency compared to the traditional beam-on/off mode [20,21]. By correlating the implanted nuclei with their subsequent β-particles within the same pixel or adjacent pixels of the DSSD, the β-decay properties of the implanted nuclei could be measured with much less disturbance from other unstable nuclei and the random background [22].…”
mentioning
confidence: 99%