1995
DOI: 10.1016/0370-2693(95)00131-4
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Coulomb dissociation reaction and correlations of two halo neutrons in 11Li

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Cited by 169 publications
(202 citation statements)
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“…These numbers are consistent with the experimental data given in [47]. In columns 2 and 4 of table 4 we give the computed 11 Li resonance energies and widths for the 10 Li spectra in the left and right parts of fig.1, respectively. From the resonance energies shown in table 4 we see that only the 1/2 + excited state in column 4, and to a lower extent the 3/2 + state in the same column, gives rise to an excitation energy of around 1 MeV in agreement with the available experimental values ( E ⋆ = 1.25 ± 0.15 [12] and E ⋆ = 1.02 ± 0.07 [14]).…”
Section: Dipole Excitationssupporting
confidence: 87%
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“…These numbers are consistent with the experimental data given in [47]. In columns 2 and 4 of table 4 we give the computed 11 Li resonance energies and widths for the 10 Li spectra in the left and right parts of fig.1, respectively. From the resonance energies shown in table 4 we see that only the 1/2 + excited state in column 4, and to a lower extent the 3/2 + state in the same column, gives rise to an excitation energy of around 1 MeV in agreement with the available experimental values ( E ⋆ = 1.25 ± 0.15 [12] and E ⋆ = 1.02 ± 0.07 [14]).…”
Section: Dipole Excitationssupporting
confidence: 87%
“…We observe in the figure insets that for the 1/2 + and the 3/2 + excited states the presence of a low-lying 1 − s-state is making the lowest λ slightly deeper than when we have the 2 − level at 50 keV. For the 5/2 + state it is the opposite, the 2 − level in 10 Li favors a deeper λ-function. The reason is that 1/2 + , but not 5/2 + , can be constructed when both neutron-core states simultaneously are relative 1 − -states and vice versa, 5/2 + , but not 1/2 + , can be constructed when both neutron-core states simultaneously are relative 2 − -states.…”
Section: Complex Rotated Hyperspherical Adiabatic Potentialsmentioning
confidence: 62%
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