References quoted in the XUNDL dataset: 95CD 9BE(124XE,X):T1/2,%B+P:XUNDL-2

4 references found.

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1997HE24

Nucl.Phys. A627, 35 (1997)

H.Herndl, B.A.Brown

Shell-Model Calculations for the Properties of Nuclei with A = 86-100 Near the Proton Drip Line

NUCLEAR STRUCTURE ^92,94Pd, ^90,91,92Rh, ⁸⁹Tc; calculated levels, J, π. ^86,87,88Sr, ^86,87,88,89Y, ^{86,87,88,89,90}Zr, ^{86,87,88,89,90,91}Nb, ^{86,87,88,89,90,91,92}Mo, ^{86,87,88,89,90,91,92,93}Tc, ^{86,87,88,89,90,91,92,93,94}Ru, ^{86,87,88,89,90,91,92,93,94,95}Rh, ^{86,87,88,89,90,91,92,93,94,95,96}Pd, ^{87,88,89,90,91,92,93,94,95,96,97}Ag, ^{88,89,90,91,92,93,94,95,96,97,98}Cd, ^{89,90,91,92,93,94,95,96,97,98,99}In, ^{90,91,92,93,94,95,96,97,98,99,100}Sn; calculated binding energies; deduced proton drip line. ^86,87,88Sr, ^86,87,88,89Y, ^{86,87,88,89,90}Zr, ^{86,87,88,89,90,91}Nb, ^{86,87,88,89,90,91,92}Mo, ^{86,87,88,89,90,91,92,93}Tc, ^{86,87,88,89,90,91,92,93,94}Ru, ^{90,91,92,93,94,95}Rh, ^{88,89,90,91,92,93,94,95,96}Pd, ^94,95,96,97Ag, ^{92,93,94,95,96,97,98}Cd, ^98,99In, ^98,99,100Sn; calculated ground-state spin, T_1/2. Shell model.

doi: 10.1016/S0375-9474(97)00407-7

2017DA07

Phys.Lett. B 767, 474 (2017)

P.J.Davies, H.Grawe, K.Moschner, A.Blazhev, R.Wadsworth, P.Boutachkov, F.Ameil, A.Yagi, H.Baba, T.Back, M.Dewald, P.Doornenbal, T.Faestermann, A.Gengelbach, J.Gerl, R.Gernhaeuser, S.Go, M.Gorska, E.Gregor, T.Isobe, D.G.Jenkins, H.Hotaka, J.Jolie, I.Kojouharov, N.Kurz, M.Lewitowicz, G.Lorusso, L.Maier, E.Merchan, F.Naqvi, H.Nishibata, D.Nishimura, S.Nishimura, F.Nowacki, N.Pietralla, H.Schaffner, P.-A.Soderstrom, H.S.Jung, K.Steiger, T.Sumikama, J.Taprogge, P.Thole, N.Warr, H.Watanabe, V.Werner, Z.Y.Xu, K.Yoshinaga, Y.Zhu

The role of core excitations in the structure and decay of the 16⁺ spin-gap isomer in ⁹⁶Cd

RADIOACTIVITY ⁹⁶Cd(EC), (ECp), ⁹⁵Cd(EC) [from ⁹Be(¹²⁴Xe, X)⁹⁶Cd/⁹⁵Cd, E=345 MeV/nucleon]; measured decay products, Eβ, Iβ, Eγ, Iγ, Ep, Ip; deduced first evidence for β-delayed proton emission, βp branching ratios, precise T_1/2 for the ground and isomeric states. Comparison with shell model calculations employing the Gross-Frenkel (GF) effective interaction.

doi: 10.1016/j.physletb.2017.02.013

2017WA10

Chin.Phys.C 41, 030003 (2017)

M.Wang, G.Audi, F.G.Kondev, W.J.Huang, S.Naimi, X.Xu

The AME2016 atomic mass evaluation (II). Tables, graphs and references

ATOMIC MASSES A=1-295; compiled, evaluated atomic masses data.

doi: 10.1088/1674-1137/41/3/030003

2018PA20

Phys.Rev. C 97, 051301R (2018)

J.Park, R.Krucken, D.Lubos, R.Gernhauser, M.Lewitowicz, S.Nishimura, D.S.Ahn, H.Baba, B.Blank, A.Blazhev, P.Boutachkov, F.Browne, I.Celikovic, G.de France, P.Doornenbal, T.Faestermann, Y.Fang, N.Fukuda, J.Giovinazzo, N.Goel, M.Gorska, H.Grawe, S.Ilieva, N.Inabe, T.Isobe, A.Jungclaus, D.Kameda, G.D.Kim, Y.-K.Kim, I.Kojouharov, T.Kubo, N.Kurz, G.Lorusso, K.Moschner, D.Murai, I.Nishizuka, Z.Patel, M.M.Rajabali, S.Rice, H.Sakurai, H.Schaffner, Y.Shimizu, L.Sinclair, P.-A.Soderstrom, K.Steiger, T.Sumikama, H.Suzuki, H.Takeda, Z.Wang, H.Watanabe, J.Wu, Z.Y.Xu

β decays of the heaviest N=Z-1 nuclei and proton instability of ⁹⁷In

RADIOACTIVITY ⁹¹Pd, ⁹⁵Cd, ⁹⁷In, ^97mIn, ⁹⁹Sn(β⁺p) [from ⁹Be(¹²⁴Xe, X), E=345 MeV/nucleon]; measured decay products, Iβ, Eβ, Ip, Ep, Iγ, Eγ; deduced T_1/2, Q-values, β-delayed proton emission branching ratios, log ft, isomeric ratio. Comparison shell model calculations, available experimental and mass evaluated data.

doi: 10.1103/PhysRevC.97.051301