The α decay of 222Th populating the low-lying J π = 3− state, and also a proposed 1− state, in 218Ra has been observed. The observations suggest an excitation energy of 853 keV for the 1− state, which is 60 keV above the 3− state. The hindrance factors of these α decays give a possible boundary to the region of ground-state octupole deformation in the light-actinide nuclei. The relative positions of the J π = 1− and 3− states suggest they are produced by an octupole-vibrational mechanism, as opposed to α clustering or rotations of a reflection-asymmetric octupole-deformed shape.peerReviewe
There is sparse direct experimental evidence that atomic nuclei can exhibit stable “pear” shapes ari...
We have observed the cu decay of Th-217 populating the low-lying two We have observed the cu decay ...
International audienceThere is sparse direct experimental evidence that atomic nuclei can exhibit st...
Fine structure in the +¦ decay of Th90221, populating excited states in Ra88217, was studied using +...
Fine structure in the α decay of 22190Th, populating excited states in 21788Ra, was studied using αγ...
Neutron-deficient uranium isotopes were studied via α spectroscopic methods. A low-lying α-decaying ...
The nucleus 207Tl, a single proton hole away from the doubly magic 208Pb nucleus, was studied in two...
There is sparse direct experimental evidence that atomic nuclei can exhibit stable pear shapes arisi...
The nucleus 207Tl, a single proton hole away from the doubly magic 208Pb nucleus, was studied in two...
Abstract High-spin states in the N = 128 nucleus 218Th have been investigated followi...
There is sparse direct experimental evidence that atomic nuclei can exhibit stable “pear” shapes ari...
High-spin states in 227Th have been populated using the reaction 226Ra(α,3n)227Th at a bombarding en...
Low spin states of Th223 have been populated via alpha-decay. The parent nucleus (U227, t 1/2 appro...
Fine structure in the +¦ decay of Th90221, populating excited states in Ra88217, was studied using +...
Short-lived α-decaying nuclei "northeast" of 208Pb in the chart of nuclides were studied using the r...
There is sparse direct experimental evidence that atomic nuclei can exhibit stable “pear” shapes ari...
We have observed the cu decay of Th-217 populating the low-lying two We have observed the cu decay ...
International audienceThere is sparse direct experimental evidence that atomic nuclei can exhibit st...
Fine structure in the +¦ decay of Th90221, populating excited states in Ra88217, was studied using +...
Fine structure in the α decay of 22190Th, populating excited states in 21788Ra, was studied using αγ...
Neutron-deficient uranium isotopes were studied via α spectroscopic methods. A low-lying α-decaying ...
The nucleus 207Tl, a single proton hole away from the doubly magic 208Pb nucleus, was studied in two...
There is sparse direct experimental evidence that atomic nuclei can exhibit stable pear shapes arisi...
The nucleus 207Tl, a single proton hole away from the doubly magic 208Pb nucleus, was studied in two...
Abstract High-spin states in the N = 128 nucleus 218Th have been investigated followi...
There is sparse direct experimental evidence that atomic nuclei can exhibit stable “pear” shapes ari...
High-spin states in 227Th have been populated using the reaction 226Ra(α,3n)227Th at a bombarding en...
Low spin states of Th223 have been populated via alpha-decay. The parent nucleus (U227, t 1/2 appro...
Fine structure in the +¦ decay of Th90221, populating excited states in Ra88217, was studied using +...
Short-lived α-decaying nuclei "northeast" of 208Pb in the chart of nuclides were studied using the r...
There is sparse direct experimental evidence that atomic nuclei can exhibit stable “pear” shapes ari...
We have observed the cu decay of Th-217 populating the low-lying two We have observed the cu decay ...
International audienceThere is sparse direct experimental evidence that atomic nuclei can exhibit st...