The high-spin states in 184Au were populated by using the 159Tb( 29Si, 4ng) 184Au reaction at a bombarding energy of 140 MeV. The 29Si beam of 8 pnA was provided by the accelerator complex of the Tandem-XTU and ALPI a...The high-spin states in 184Au were populated by using the 159Tb( 29Si, 4ng) 184Au reaction at a bombarding energy of 140 MeV. The 29Si beam of 8 pnA was provided by the accelerator complex of the Tandem-XTU and ALPI at the Laroratori Nazionale di Legnero, Italy, and focussed onto a natural metallic 159Tb foil展开更多
High-spin states in 183Au have been studied experimentally by using the 159Tb(29Si, 5n)183Au reaction at a beam energy of 140 MeV. The 29Si beam of 8 pnA was provided by the accelerator complex of the Tandem-XTU and A...High-spin states in 183Au have been studied experimentally by using the 159Tb(29Si, 5n)183Au reaction at a beam energy of 140 MeV. The 29Si beam of 8 pnA was provided by the accelerator complex of the Tandem-XTU and ALPI at the Laroratori Nazionali di Legnero, Italy, and focussed onto a natural metallic 159Tb foil of展开更多
Low-spin signature inversion has been systematically observed throughout the chart of nuclides in the πg9/2(■) vg9/2, πh11/2(■)vh11/2, πh11/2(■)vh13/2, and πh9/2(■) vi13/2, configurations. Considering the high...Low-spin signature inversion has been systematically observed throughout the chart of nuclides in the πg9/2(■) vg9/2, πh11/2(■)vh11/2, πh11/2(■)vh13/2, and πh9/2(■) vi13/2, configurations. Considering the high-j nature of these configurations, we have tried to find the similar signature inversion phenomenon in the πi13/2 (■) vi13/2, bands展开更多
High-spin states in 69As were populated via the 40Ca(32S, 3p)69As reaction at 95 MeV beam energy. The 32S beam was provided by the VIVITRON accelerator of the IreS Strasbourg. A target of 1 mg/cm2 With 15 mg/cm2 gold ...High-spin states in 69As were populated via the 40Ca(32S, 3p)69As reaction at 95 MeV beam energy. The 32S beam was provided by the VIVITRON accelerator of the IreS Strasbourg. A target of 1 mg/cm2 With 15 mg/cm2 gold backing was used. Measurements of γ-γand γ-γ-γcoincidences were performed with the EUROBALL展开更多
基金Supported by NNSFC (10375077, 10025525,10221003)the Major State Basic Research Development Program of China (G2000077400)Chinese Academy of Sciences.
文摘The high-spin states in 184Au were populated by using the 159Tb( 29Si, 4ng) 184Au reaction at a bombarding energy of 140 MeV. The 29Si beam of 8 pnA was provided by the accelerator complex of the Tandem-XTU and ALPI at the Laroratori Nazionale di Legnero, Italy, and focussed onto a natural metallic 159Tb foil
文摘High-spin states in 183Au have been studied experimentally by using the 159Tb(29Si, 5n)183Au reaction at a beam energy of 140 MeV. The 29Si beam of 8 pnA was provided by the accelerator complex of the Tandem-XTU and ALPI at the Laroratori Nazionali di Legnero, Italy, and focussed onto a natural metallic 159Tb foil of
基金Supported by NNSFC (10375077, 10025525,10221003)the Major State Basic Research Development Program of China (G2000077400)the Chinese Academy of Sciences.
文摘Low-spin signature inversion has been systematically observed throughout the chart of nuclides in the πg9/2(■) vg9/2, πh11/2(■)vh11/2, πh11/2(■)vh13/2, and πh9/2(■) vi13/2, configurations. Considering the high-j nature of these configurations, we have tried to find the similar signature inversion phenomenon in the πi13/2 (■) vi13/2, bands
文摘High-spin states in 69As were populated via the 40Ca(32S, 3p)69As reaction at 95 MeV beam energy. The 32S beam was provided by the VIVITRON accelerator of the IreS Strasbourg. A target of 1 mg/cm2 With 15 mg/cm2 gold backing was used. Measurements of γ-γand γ-γ-γcoincidences were performed with the EUROBALL
