“…Most of these gamma rays have been seen in previous experiments [11,20,21]. The branching ratios and the energies of the gamma rays extracted from the current experiment agree well with these formerly established values.…”
Section: B Gamma-ray Transitionssupporting
confidence: 90%
“…6) that is evidence of a long lifetime and which is consistent with the previously measured half-life of 133(8) ps [20]. This corresponds to a traversal distance of 1.76(11) cm in the setup which results in a additional systematic uncertainty for the efficiency of about 10% which is not quoted in Table II…”
Section: B Gamma-ray Transitionssupporting
confidence: 88%
“…For the other excited states observed in the reaction, the AMD+GCM calculations [13] provides a useful insight into their nature together with previous experiments [11,20,21,29,30]. In particular, the neutron knockout experiment [11] populated the 3/2 − , 7/2 − states at 221 keV and 481 keV respectively labeled as 1p2h in the AMD+GCM calculation which agrees well with the removal of a fp-shell neutron from the 2p2h ground state of 32 Mg.…”
Section: B Structure Of Observed Excited Statesmentioning
confidence: 95%
“…For the 171 keV decays to the 50 keV state, the ratio of counts of the forward to backward ring of SeGA differs from that of the 221 keV decay to the ground state by more than 4σ . Previous lifetime measurements [20] and Weisskopf estimates conclude these are dipole transitions, limiting the spin assignment of the 221 keV state to 1/2 or 3/2 given the known ground state spin of 1/2 + [10]. As these gamma rays originate from the same state, the distribution of magnetic substates of the initial level must be the same, and so the B λ are identical.…”
Section: Spin Alignment In Residuesmentioning
confidence: 97%
“…b Established values since measured values are subject to effects due to the previously measured lifetime of the state [20]. c Tentatively placed in the decay scheme based on energy balance.…”
Section: A Cross Sections and Momentum Distributionmentioning
The "island of the inversion" isotope 31 Mg was investigated using an intermediate energy proton knockout reaction from 32 Al at 90 MeV/nucleon at the National Superconducting Cyclotron Laboratory. A negligible cross section to the ground state supports an intruder-dominant configuration in 31 Mg. The partial cross sections to excited final states preferentially populate configurations in the 31 Mg residues which have no neutron excitations across the N = 20 shell closure. There is strong evidence that the reaction populates the 3/2 + and 5/2 + states which correspond with the neutron-hole states predicted by the shell model with the model space truncated above the sd-shell.
“…Most of these gamma rays have been seen in previous experiments [11,20,21]. The branching ratios and the energies of the gamma rays extracted from the current experiment agree well with these formerly established values.…”
Section: B Gamma-ray Transitionssupporting
confidence: 90%
“…6) that is evidence of a long lifetime and which is consistent with the previously measured half-life of 133(8) ps [20]. This corresponds to a traversal distance of 1.76(11) cm in the setup which results in a additional systematic uncertainty for the efficiency of about 10% which is not quoted in Table II…”
Section: B Gamma-ray Transitionssupporting
confidence: 88%
“…For the other excited states observed in the reaction, the AMD+GCM calculations [13] provides a useful insight into their nature together with previous experiments [11,20,21,29,30]. In particular, the neutron knockout experiment [11] populated the 3/2 − , 7/2 − states at 221 keV and 481 keV respectively labeled as 1p2h in the AMD+GCM calculation which agrees well with the removal of a fp-shell neutron from the 2p2h ground state of 32 Mg.…”
Section: B Structure Of Observed Excited Statesmentioning
confidence: 95%
“…For the 171 keV decays to the 50 keV state, the ratio of counts of the forward to backward ring of SeGA differs from that of the 221 keV decay to the ground state by more than 4σ . Previous lifetime measurements [20] and Weisskopf estimates conclude these are dipole transitions, limiting the spin assignment of the 221 keV state to 1/2 or 3/2 given the known ground state spin of 1/2 + [10]. As these gamma rays originate from the same state, the distribution of magnetic substates of the initial level must be the same, and so the B λ are identical.…”
Section: Spin Alignment In Residuesmentioning
confidence: 97%
“…b Established values since measured values are subject to effects due to the previously measured lifetime of the state [20]. c Tentatively placed in the decay scheme based on energy balance.…”
Section: A Cross Sections and Momentum Distributionmentioning
The "island of the inversion" isotope 31 Mg was investigated using an intermediate energy proton knockout reaction from 32 Al at 90 MeV/nucleon at the National Superconducting Cyclotron Laboratory. A negligible cross section to the ground state supports an intruder-dominant configuration in 31 Mg. The partial cross sections to excited final states preferentially populate configurations in the 31 Mg residues which have no neutron excitations across the N = 20 shell closure. There is strong evidence that the reaction populates the 3/2 + and 5/2 + states which correspond with the neutron-hole states predicted by the shell model with the model space truncated above the sd-shell.
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