Z = 50 shell gap near 100Sn from intermediate-energy Coulomb excitations in even-mass 106-112Sn isotopes.
Z = 50 shell gap near 100Sn from intermediate-energy Coulomb excitations in even-mass 106-112Sn isotopes.
复制标题
DOI:
10.1103/physrevlett.99.162501
复制
发表时间:
2006-12
影响因子:
8.6
通讯作者:
C. Vaman;C. Andreoiu;D. Bazin;A. Becerril;B. A. Brown;C. Campbell;A. Chester;J. Cook;D. Dinca;A. Gade;D. Galaviz;T. Glasmacher;M. Hjorth-Jensen;M. Horoi;D. Miller;V. Moeller;W. Mueller;A. Schiller;K. Starosta;A. Stolz;J. R. Terry;A. Volya;V. Zelevinsky;H. Zwahlen
中科院分区:
文献类型:
--
作者:
C. Vaman;C. Andreoiu;D. Bazin;A. Becerril;B. A. Brown;C. Campbell;A. Chester;J. Cook;D. Dinca;A. Gade;D. Galaviz;T. Glasmacher;M. Hjorth-Jensen;M. Horoi;D. Miller;V. Moeller;W. Mueller;A. Schiller;K. Starosta;A. Stolz;J. R. Terry;A. Volya;V. Zelevinsky;H. Zwahlen
Rare isotope beams of neutron-deficient 106,108,110Sn from the fragmentation of 124Xe were employed in an intermediate-energy Coulomb excitation experiment. The measured B(E2,0(1)(+)-->2(1)(+)) values for 108Sn and 110Sn and the results obtained for the 106Sn show that the transition strengths for these nuclei are larger than predicted by current state-of-the-art shell-model calculations. This discrepancy might be explained by contributions of the protons from within the Z = 50 shell to the structure of low-energy excited states in this region.