References quoted in the XUNDL dataset: 150CS 9BE(238U,F):T1/2:XUNDL-5

5 references found.

Clicking on a keynumber will list datasets that reference the given article.

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2017LI06

J.Phys.(London) G44, 054002 (2017)

R.Lica, G.Benzoni, A.I.Morales, M.J.G.Borge, L.M.Fraile, H.Mach, M.Madurga, C.Sotty, V.Vedia, H.De Witte, J.Benito, T.Berry, N.Blasi, A.Bracco, F.Camera, S.Ceruti, V.Charviakova, N.Cieplicka-Orynczak, C.Costache, F.C.L.Crespi, J.Creswell, G.Fernandez-Martinez, H.Fynbo, P.Greenlees, I.Homm, M.Huyse, J.Jolie, V.Karayonchev, U.Koster, J.Konki, T.Kroll, J.Kurcewicz, T.Kurtukian-Nieto, I.Lazarus, S.Leoni, M.Lund, N.Marginean, R.Marginean, C.Mihai, R.Mihai, A.Negret, A.Orduz, Z.Patyk, S.Pascu, V.Pucknell, P.Rahkila, J.M.Regis, F.Rotaru, N.Saed-Samii, V.Sanchez-Tembleque, M.Stanoiu, O.Tengblad, M.Thuerauf, A.Turturica, P.Van Duppen, N.Warr

β decay studies of n-rich Cs isotopes with the ISOLDE Decay Station

RADIOACTIVITY ^148,149,150Cs(β^-), (β^-n)[from U(p, X), E=1.4 GeV at ISOLDE-CERN]; measured reaction products, Eγ, Iγ, βγ-, γγ-coin, half-lives of ground states of ^148,149,150Cs, %P_n for the decay of ¹⁴⁹Cs, half-lives of levels in ¹⁴⁹Ba and ¹⁴⁸Ce by βγγ(t). ¹⁴⁹Ba; deduced levels, β feedings, multipolarities, half-lives. ¹⁴⁸Ce; deduced half-life of the first 2+ state. Comparison with previous experimental half-lives, and with theoretical calculations.

doi: 10.1088/1361-6471/aa6015

2017WU04

Phys.Rev.Lett. 118, 072701 (2017)

J.Wu, S.Nishimura, G.Lorusso, P.Moller, E.Ideguchi, P.-H.Regan, G.S.Simpson, P.-A.Soderstrom, P.M.Walker, H.Watanabe, Z.Y.Xu, H.Baba, F.Browne, R.Daido, P.Doornenbal, Y.F.Fang, G.Gey, T.Isobe, P.S.Lee, J.J.Liu, Z.Li, Z.Korkulu, Z.Patel, V.Phong, S.Rice, H.Sakurai, L.Sinclair, T.Sumikama, M.Tanaka, A.Yagi, Y.L.Ye, R.Yokoyama, G.X.Zhang, T.Alharbi, N.Aoi, F.L.Bello Garrote, G.Benzoni, A.M.Bruce, R.J.Carroll, K.Y.Chae, Z.Dombradi, A.Estrade, A.Gottardo, C.J.Griffin, H.Kanaoka, I.Kojouharov, F.G.Kondev, S.Kubono, N.Kurz, I.Kuti, S.Lalkovski, G.J.Lane, E.J.Lee, T.Lokotko, G.Lotay, C.-B.Moon, H.Nishibata, I.Nishizuka, C.R.Nita, A.Odahara, Zs.Podolyak, O.J.Roberts, H.Schaffner, C.Shand, J.Taprogge, S.Terashima, Z.Vajta, S.Yoshida

94 β-Decay Half-Lives of Neutron-Rich ₅₅Cs to ₆₇Ho: Experimental Feedback and Evaluation of the r-Process Rare-Earth Peak Formation

RADIOACTIVITY ^{144,145,146,147,148,149,150,151}Cs, ^{146,147,148,149,150,151,152,153,154}Ba, ^{148,149,150,151,152,153,154,155,156}La, ^{150,151,152,153,154,155,156,157,158}Ce, ^{153,154,155,156,157,158,159,160}Pr, ^{156,157,158,159,160,161,162}Nd, ^{159,160,161,162,163}Pm, ^{160,161,162,163,164,165,166}Sm, ^{161,162,163,164,165,166,167,168}Eu, ^{165,166,167,168,169,170}Gd, ^{166,167,168,169,170,171,172}Tb, ^{169,170,171,172,172m,173}Dy, ^{172,173,174,175}Ho, ^174mEr(β^-)[from Be(²³⁸U, X), E=345 MeV/nucleon]; measured and analyzed reaction products using BigRIPS separator and ZeroDegree Spectrometer (ZDS), γ rays, half-lives by (implant)β correlations using WAS3ABi and EURICA detection systems at RIBF-RIKEN facility; deduced Gamow-Teller strength functions, r-process abundance pattern in the solar system. Comparison with previous experimental half-lives, and with three theoretical calculations using FRDM+QRPA, KTUY+GT2, and RHB+pn-RQRPA models. Numerical values of half-lives listed in supplementary file.

doi: 10.1103/PhysRevLett.118.072701

2018LI06

Phys.Rev. C 97, 024305 (2018)

R.Lica, for the IDS Collaboration

Evolution of deformation in neutron-rich Ba isotopes up to A=150

RADIOACTIVITY ^148,150Cs(β^-), (β^-n)[from U(p, X), E=1.4 GeV using General Purpose Separator (GPS) at ISOLDE-CERN]; measured Eγ, Iγ, Eβ, γγ- and βγ-coin, half-lives of the decays of ^148,150Cs, half-lives of first 2+ states in ^148,150Ba by fast-timing technique using four HPGe detectors, three LaBr₃(Ce) detectors for fast-timing and three plastic scintillators for β particle detection. ^148,150Ba; deduced levels, J, π, B(E2), deformations, β feedings, logft. ¹⁴⁸Cs; deduced %β^-n for its decay. Comparison with previous experimental data, and with symmetry conserving configuration mixing (SCCM) calculations. Level systematics in neighboring nuclides.

NUCLEAR STRUCTURE ^{142,144,146,148,150}Ba; calculated potential energy surfaces in (β₂, β₃) plane; deduced evolution of quadrupoledeformed shapes with a definite octupolar character. Symmetry conserving configuration mixing (SCCM) calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.97.024305

2020LI32

Nucl.Data Sheets 168, 1 (2020)

J.Liang, B.Singh, E.A.McCutchan, I.Dillmann, M.Birch, A.A.Sonzogni, X.Huang, M.Kang, J.Wang, G.Mukherjee, K.Banerjee, D.Abriola, A.Algora, A.A.Chen, T.D.Johnson, K.Miernik

Compilation and Evaluation of Beta-Delayed Neutron Emission Probabilities and Half-Lives for Z > 28 Precursors

RADIOACTIVITY ^{73,74,75,76,77,78,79,80,81,82,83}Cu, ^{78,79,80,81,82,83,84,85}Zn, ^{79,80,81,82,83,84,85,86,87}Ga, ^{83,84,85,86,87,88,89,90}Ge, ^{84,85,86,87,88,89,90,91,92}As, ^{86,87,88,89,90,91,92,93,94,95}Se, ^{87,88,89,90,91,92,93,94,95,96,97,98}Br, ^{91,92,93,94,95,96,97,98,99,100,101}Kr, ^{91,92,93,94,95,96,97,98,99,100,101,102,103,104}Rb, ^{96,97,98,99,100,101,102,103,104,105,106,107}Sr, ^{97,98,99,100,101,102,103,104,105,106,107,108,109}Y, ^{103,104,105,106,107,108,109,110,111,112,113}Zr, ^{103,104,105,106,107,108,109,110,111,112,113,114,115,116}Nb, ^{109,110,111,112,113,114,115,116,117,118,119}Mo, ^{109,110,111,112,113,114,115,116,117,118,119,120,121,122}Tc, ^{114,115,116,117,118,119,120,121,122,123,124,125}Ru, ^{115,116,117,118,119,120,121,122,123,124,125,126,127,128}Rh, ^{119,120,121,122,123,124,125,126,127,128,129,130,131}Pd, ^{120,121,122,123,124,125,126,127,128,129,130,131,132}Ag, ^{126,127,128,129,130,131,132,133,134}Cd, ^{127,128,129,130,131,132,133,134,135,136,137}In, ^{133,134,135,136,137,138,139,140}Sn, ^{134,135,136,137,138,139,140,141,142}Sb, ^{136,137,138,139,140,141,142,143,144,145}Te, ^{137,138,139,140,141,142,143,144,145,146,147}I, ^{141,142,143,144,145,146,147,148,149,150}Xe, ^{141,142,143,144,145,146,147,148,149,150,151,152}Cs, ^{147,148,149,150,151,152,153,154}Ba, ^{147,148,149,150,151,152,153,154,155,156,157}La, ^{153,154,155,156,157,158}Ce, ^{153,154,155,156,157,158,159,160,161}Pr, ^{158,159,160,161,162,163}Nd, ^{159,160,161,162,163,164,165}Pm, ^{163,164,165,166,167}Sm, ^{165,166,167,168,169}Eu, ^169,170,171Gd, ^{169,170,171,172,173,174}Tb, ^174,175,176Dy, ^{174,175,176,177,178}Ho, ¹⁸⁰Er, ^179,180,181Tm, ¹⁸⁵Yb, ^186,187,188Lu, ^{191,192,193,194}Ta, ^198,199Re, ²⁰³Os, ^203,204,205Ir, ^206,207,208Pt, ^{206,207,208,209,210}Au, ^{209,210,211,212,213,214,215,216}Hg, ^{210,211,212,213,214,215,216,217}Tl, ^{219,220,221,222,223,224}Bi, ^{225,226,227,228,229}At, ²²³Fr(β^-); analyzed available data; deduced β-delayed neutron emission probabilities (Pn) and T_1/2 for known or potential β-delayed neutron precursors. Comparison with systematics using three different approaches.

doi: 10.1016/j.nds.2020.09.001

2020WU04

Phys.Rev. C 101, 042801 (2020)

J.Wu, S.Nishimura, P.Moller, M.R.Mumpower, R.Lozeva, C.B.Moon, A.Odahara, H.Baba, F.Browne, R.Daido, P.Doornenbal, Y.F.Fang, M.Haroon, T.Isobe, H.S.Jung, G.Lorusso, B.Moon, Z.Patel, S.Rice, H.Sakurai, Y.Shimizu, L.Sinclair, P.-A.Soderstrom, T.Sumikama, H.Watanabe, Z.Y.Xu, A.Yagi, R.Yokoyama, D.S.Ahn, F.L.Bello Garrote, J.M.Daugas, F.Didierjean, N.Fukuda, N.Inabe, T.Ishigaki, D.Kameda, I.Kojouharov, T.Komatsubara, T.Kubo, N.Kurz, K.Y.Kwon, S.Morimoto, D.Murai, H.Nishibata, H.Schaffner, T.M.Sprouse, H.Suzuki, H.Takeda, M.Tanaka, K.Tshoo, Y.Wakabayashi

β-decay half-lives of 55 neutron-rich isotopes beyond the N = 82 shell gap

RADIOACTIVITY ^{134,135,136,137,138,139}Sn, ^{134,135,136,137,138,139,140,141,142}Sb, ^{137,138,139,140,141,142,143,144}Te, ^{140,141,142,143,144,145,146}I, ^{142,143,144,145,146,147,148}Xe, ^{145,146,147,148,149,150,151}Cs, ^{148,149,150,151,152,153}Ba, ^{151,152,153,154,155}La(β^-)[from ⁹Be(²³⁸U, F), E=345 MeV/nucleon, followed by separation of fragments using BigRIPS separator at RIBF-RIKEN]; measured β and γ radiations, half-lives by (implant)β and (implant)βγ correlations using the Wide range Active Silicon-Strip Stop per Array for Beta and ion (WAS3ABi) detection system and Euroball RIKEN Cluster Array (EURICA) of 84 Ge cluster detectors. Comparison with previously available experimental half-lives, and with theoretical calculations using FRDM+QRPA, KTUY+GT2, RHB+pn-RQRPA, and DF+CQRPA models. ¹⁴¹Te(β^-); calculated half-life and Gamow-Teller strengths using FRDM+QRPA(2019) model, and compared with experimental data. Discussed and calculated effects of new half-life data on r-process abundance.

doi: 10.1103/PhysRevC.101.042801