Nuclear structure and β -decay schemes for Te nuclides beyond N = 82

We study for the first time the internal structure of Te140 through the β-delayed γ-ray spectroscopy of Sb140. The very neutron-rich Sb140 nuclei with Z=51 and N=89 were produced by the in-flight fission of U238 beams at the Radioactive Isotope Beam Factory, RIKEN. The half-life and spin-parity of S...

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Veröffentlicht in:Phys.Rev.C 2017-04, Vol.95 (4), Article 044322
Hauptverfasser: Moon, B., Moon, C.-B., Söderström, P.-A., Odahara, A., Lozeva, R., Hong, B., Browne, F., Jung, H. S., Lee, P., Lee, C. S., Yagi, A., Yuan, C., Nishimura, S., Doornenbal, P., Lorusso, G., Sumikama, T., Watanabe, H., Kojouharov, I., Isobe, T., Baba, H., Sakurai, H., Daido, R., Fang, Y., Nishibata, H., Patel, Z., Rice, S., Sinclair, L., Wu, J., Xu, Z. Y., Yokoyama, R., Kubo, T., Inabe, N., Suzuki, H., Fukuda, N., Kameda, D., Takeda, H., Ahn, D. S., Shimizu, Y., Murai, D., Bello Garrote, F. L., Daugas, J. M., Didierjean, F., Ideguchi, E., Ishigaki, T., Morimoto, S., Niikura, M., Nishizuka, I., Komatsubara, T., Kwon, Y. K., Tshoo, K.
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container_issue 4
container_start_page
container_title Phys.Rev.C
container_volume 95
creator Moon, B.
Moon, C.-B.
Söderström, P.-A.
Odahara, A.
Lozeva, R.
Hong, B.
Browne, F.
Jung, H. S.
Lee, P.
Lee, C. S.
Yagi, A.
Yuan, C.
Nishimura, S.
Doornenbal, P.
Lorusso, G.
Sumikama, T.
Watanabe, H.
Kojouharov, I.
Isobe, T.
Baba, H.
Sakurai, H.
Daido, R.
Fang, Y.
Nishibata, H.
Patel, Z.
Rice, S.
Sinclair, L.
Wu, J.
Xu, Z. Y.
Yokoyama, R.
Kubo, T.
Inabe, N.
Suzuki, H.
Fukuda, N.
Kameda, D.
Takeda, H.
Ahn, D. S.
Shimizu, Y.
Murai, D.
Bello Garrote, F. L.
Daugas, J. M.
Didierjean, F.
Ideguchi, E.
Ishigaki, T.
Morimoto, S.
Niikura, M.
Nishizuka, I.
Komatsubara, T.
Kwon, Y. K.
Tshoo, K.
description We study for the first time the internal structure of Te140 through the β-delayed γ-ray spectroscopy of Sb140. The very neutron-rich Sb140 nuclei with Z=51 and N=89 were produced by the in-flight fission of U238 beams at the Radioactive Isotope Beam Factory, RIKEN. The half-life and spin-parity of Sb140 are reported as 173±12 ms and 3−, respectively. In addition to the excited states of Te140 produced by the β-decay branch, the β-delayed one-neutron and two-neutron emission branches were also established. By identifying the first 2+ and 4+ excited states of Te140, we found that Te isotopes persist in their vibrator character with E(4+)/E(2+)=2. We discuss the distinctive features manifest in this region revealed in pairs of isotopes with the same neutron holes and particles with respect to N=82.
doi_str_mv 10.1103/PhysRevC.95.044322
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K.</creatorcontrib><creatorcontrib>Tshoo, K.</creatorcontrib><title>Nuclear structure and β -decay schemes for Te nuclides beyond N = 82</title><title>Phys.Rev.C</title><description>We study for the first time the internal structure of Te140 through the β-delayed γ-ray spectroscopy of Sb140. The very neutron-rich Sb140 nuclei with Z=51 and N=89 were produced by the in-flight fission of U238 beams at the Radioactive Isotope Beam Factory, RIKEN. The half-life and spin-parity of Sb140 are reported as 173±12 ms and 3−, respectively. In addition to the excited states of Te140 produced by the β-decay branch, the β-delayed one-neutron and two-neutron emission branches were also established. By identifying the first 2+ and 4+ excited states of Te140, we found that Te isotopes persist in their vibrator character with E(4+)/E(2+)=2. We discuss the distinctive features manifest in this region revealed in pairs of isotopes with the same neutron holes and particles with respect to N=82.</description><subject>Nuclear Experiment</subject><subject>Physics</subject><issn>2469-9985</issn><issn>2469-9993</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><recordid>eNo9kMtOAjEUhhujiQR5AVfduhjs6b0LF4SgmBA0BtdNp5eAAca0QDKv5YP4TAxBWZ1Lvv9ffAjdAxkCEPb4vmzLRzyMh0YMCeeM0ivUo1yayhjDri-7FrdoUMoXIQQkMQpID03me7-OLuOyy3u_2-eI3Tbg3x9chehdi4tfxk0sODUZLyLedvgqdHcd26YD5_gJa3qHbpJblzj4m330-TxZjKfV7O3ldTyaVZ5q2FWgVBKUSuA06VoKYDUH4niotQQwIlGlAteSBhWY1NFRiIl7poTyUoFmffRw7l26tf3Oq43LrW3cyk5HM3v6ERCCE0IP0LH0zPrclJJjugSA2JM3--_NGmHP3tgRTGRfgQ</recordid><startdate>20170425</startdate><enddate>20170425</enddate><creator>Moon, B.</creator><creator>Moon, C.-B.</creator><creator>Söderström, P.-A.</creator><creator>Odahara, A.</creator><creator>Lozeva, R.</creator><creator>Hong, B.</creator><creator>Browne, F.</creator><creator>Jung, H. 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S. ; Yagi, A. ; Yuan, C. ; Nishimura, S. ; Doornenbal, P. ; Lorusso, G. ; Sumikama, T. ; Watanabe, H. ; Kojouharov, I. ; Isobe, T. ; Baba, H. ; Sakurai, H. ; Daido, R. ; Fang, Y. ; Nishibata, H. ; Patel, Z. ; Rice, S. ; Sinclair, L. ; Wu, J. ; Xu, Z. Y. ; Yokoyama, R. ; Kubo, T. ; Inabe, N. ; Suzuki, H. ; Fukuda, N. ; Kameda, D. ; Takeda, H. ; Ahn, D. S. ; Shimizu, Y. ; Murai, D. ; Bello Garrote, F. L. ; Daugas, J. M. ; Didierjean, F. ; Ideguchi, E. ; Ishigaki, T. ; Morimoto, S. ; Niikura, M. ; Nishizuka, I. ; Komatsubara, T. ; Kwon, Y. 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In addition to the excited states of Te140 produced by the β-decay branch, the β-delayed one-neutron and two-neutron emission branches were also established. By identifying the first 2+ and 4+ excited states of Te140, we found that Te isotopes persist in their vibrator character with E(4+)/E(2+)=2. We discuss the distinctive features manifest in this region revealed in pairs of isotopes with the same neutron holes and particles with respect to N=82.</abstract><doi>10.1103/PhysRevC.95.044322</doi><orcidid>https://orcid.org/0000-0001-7477-2319</orcidid><orcidid>https://orcid.org/0000-0002-2409-4019</orcidid><orcidid>https://orcid.org/0000-0002-7262-5339</orcidid><orcidid>https://orcid.org/0000-0002-5940-2667</orcidid><orcidid>https://orcid.org/0000-0002-6215-4254</orcidid></addata></record>
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title Nuclear structure and β -decay schemes for Te nuclides beyond N = 82
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