References quoted in the ENSDF dataset: 159PM ADOPTED LEVELS, GAMMAS
17 references found.
Clicking on a keynumber will list datasets that reference the given article.
Proc.Conf on Exotic Nuclei and Atomic Masses, Bellaire, Michigan, June 23-27, 1998, p.540 (1998); AIP Conf.Proc. 455 (1998)
S.Ichikawa, K.Tsukada, M.Asai, A.Osa, M.Sakama, Y.Kojima, M.Shibata, I.Nishinaka, Y.Nagame, Y.Oura, K.Kawade
β-Decay Half-Lives of New Neutron-Rich Lanthanide Isotopes
RADIOACTIVITY 159Pm, 161Sm, 165Gd, 166,167,168Tb(β-) [from 238U(p, F)]; measured T1/2. Mass separator, gas-jet transport. Comparison with model predictions.
Proc.2nd Intern.Conf Fission and Properties of Neutron-Rich Nuclei, St Andrews, Scotland, June 28-July 3, 1999, J.H.Hamilton, W.R.Phillips, H.K.Carter, Eds., World Scientific, Singapore, p.203 (2000)
S.Ichikawa, M.Asai, K.Tsukada, I.Nishinaka, Y.Nagame, A.Osa, Y.Kojima, M.Shibata, K.Kawade, M.Sakama, Y.Oura
Decay Studies of Neutron-Rich Isotopes Produced in Proton-Induced Fisson of Actinides
RADIOACTIVITY 159Pm, 161,162Sm, 165,166Gd, 166,167,168Tb(β-) [from 238U(p, F), E=20 MeV]; measured Eβ, Eγ, βγ-, β(x-ray)-coin, T1/2. 166,168Dy deduced levels, J, π. Comparison with RPA calculations.
Japan Atomic Energy Res.Inst.Tandem VDG Ann.Rept., 2000, p.13 (2001); JAERI-Review 2001-030 (2001)
M.Asai, K.Tsukada, S.Ichikawa, H.Haba, A.Osa, Y.Nagame, S.Goto, M.Sakama, Y.Kojima, M.Shibata, K.Akiyama, A.Toyoshima
Identification of 159Pm, 162Sm, and 166Gd
NUCLEAR REACTIONS 238U(p, X), E=15.5 MeV; measured fragment masses, delayed Eγ, βγ-coin; deduced evidence for 159Pm, 162Sm, 166Gd, 166Tb.
RADIOACTIVITY 159Pm, 162Sm, 166Gd, 166Tb(β-) [from 238U(p, X)]; measured T1/2.
Japan Atomic Energy Res.Inst.Tandem VDG Ann.Rept., 2002, p.32 (2003); JAERI-Review 2003-028 (2003)
M.Shibata, O.Suematsu, K.Kawade, M.Asai, S.Ichikawa, Y.Nagame, A.Osa, K.Tsukada, Y.Kojima, A.Taniguchi
Qβ measurements of neutron-rich rare earth nuclei produced with proton induced fission of 238U
RADIOACTIVITY 158,159Pm, 159,161Sm, 166Tb(β-) [from 238U(p, F)]; measured Eβ, Eγ, T1/2; deduced Qβ. Comparisons with previous results and model predictions. Total absorption spectrometer.
Phys.Rev. C 71, 067302 (2005)
S.Ichikawa, M.Asai, K.Tsukada, H.Haba, Y.Nagame, M.Shibata, M.Sakama, Y.Kojima
β-decay half-lives of new neutron-rich rare-earth isotopes 159Pm, 162Sm, and 166Gd
RADIOACTIVITY 159Pm, 162Sm, 166Gd, 166Tb(β-) [from 238U(p, F)]; measured Eγ, Iγ, βγ-, γγ-coin, T1/2. 166Tb deduced levels, β-feeding intensities.
doi: 10.1103/PhysRevC.71.067302
JAEA-Review 2006-029, p.33 (2006)
H.Hayashi, Y.Akita, M.Shibata, T.K.Sato, A.Osa, M.Asai, K.Tsukada, T.Ishii, S.Ichikawa, Y.Kojima, A.Taniguchi
Qβ determinations of 160-165Eu, 163Gd, 158, 159Pm, 159, 161Sm and 166Tb using a total absorption BGO detector
RADIOACTIVITY 158,159Pm, 159,161Sm, 160,161,162,163,164,165Eu, 163Gd, 166Tb(β-) [from U(p, F)]; measured Qβ; deduced two-neutron separation energies. BGO total absorption detector.
Eur.Phys.J. A 34, 363 (2007)
H.Hayashi, Y.Akita, O.Suematsu, M.Shibata, M.Asai, T.K.Sato, S.Ichikawa, I.Nishinaka, Y.Nagame, A.Osa, K.Tsukada, T.Ishii, Y.Kojima, A.Taniguchi
Qβ measurements of 158, 159Pm, 159, 161Sm, 160-165Eu, 163Gd and 166Tb using a total absorption BGO detector
RADIOACTIVITY 158,159Pm, 159,161Sm, 160,161,162,163,164,165Eu, 163Gd, 166Tb(β-) [from 238U(p, F), E=24 MeV and subsequent decay]; measured Eγ, Iγ, Eβ, Iβ; deduced Qβ, mass excess and two-neutron separation energies. Mass separator.
doi: 10.1140/epja/i2006-10522-9
Nucl.Phys. A835, 192c (2010)
K.Hashimoto
Nuclear Force from String Theory
doi: 10.1016/j.nuclphysa.2010.01.193
Phys.Rev. C 85, 045805 (2012)
J.Van Schelt, D.Lascar, G.Savard, J.A.Clark, S.Caldwell, A.Chaudhuri, J.Fallis, J.P.Greene, A.F.Levand, G.Li, K.S.Sharma, M.G.Sternberg, T.Sun, B.J.Zabransky
Mass measurements near the r-process path using the Canadian Penning Trap mass spectrometer
ATOMIC MASSES 133,134Sb, 134,135,136,137Te, 135,136,137,138,139I, 137,138,139,140,141Xe, 141,142Cs, 153,155Pr, 153,155,157Nd, 153,155,156,157,158,159Pm, 155,157,158,159,160,161Sm, 158,159,160,161Eu, 163Gd; measured cyclotron frequency ratios; deduced mass excess, atomic masses. Canadian Penning Trap mass spectrometer at ANL. Comparison with AME-2003 evaluation and theoretical mass models. Systematics of S(2n) values.
doi: 10.1103/PhysRevC.85.045805
Phys.Rev. C 95, 014304 (2017)
P.Sarriguren
β-decay properties of neutron-rich rare-earth isotopes
NUCLEAR STRUCTURE 140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180Xe, 142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182Ba, 146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184Ce, 152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186Nd, 158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188Sm, 162,164,166,168,170,172,174,176,178,180,182,184,186,188,190Gd, 168,170,172,174,176,178,180,182,184,186,188,190,192Dy; calculated quadrupole deformation β2 from SLy4, energy curves that show the energy as a function of quadrupole deformation β2 using constrained Hartree-Fock (HF) + BCS formalism.
RADIOACTIVITY 140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180Xe, 142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182Ba, 146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184Ce, 152,154,156,158,160,162,164,166,168,170,172,174,176,178,180,182,184,186Nd, 158,160,162,164,166,168,170,172,174,176,178,180,182,184,186,188Sm, 162,164,166,168,170,172,174,176,178,180,182,184,186,188,190Gd, 168,170,172,174,176,178,180,182,184,186,188,190,192Dy(β-), (β-n); calculated Gamow-Teller strength distributions, β-decay half-lives, β-delayed neutron emission probabilities. Self-consistent deformed Skyrme-Hartree-Fock calculations with pairing and QRPA correlations. Comparison with other theoretical calculations, phenomenological model, and with available experimental data.
doi: 10.1103/PhysRevC.95.014304
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 144,145,146,147,148,149,150,151Cs, 146,147,148,149,150,151,152,153,154Ba, 148,149,150,151,152,153,154,155,156La, 150,151,152,153,154,155,156,157,158Ce, 153,154,155,156,157,158,159,160Pr, 156,157,158,159,160,161,162Nd, 159,160,161,162,163Pm, 160,161,162,163,164,165,166Sm, 161,162,163,164,165,166,167,168Eu, 165,166,167,168,169,170Gd, 166,167,168,169,170,171,172Tb, 169,170,171,172,172m,173Dy, 172,173,174,175Ho, 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
Phys.Rev. C 98, 024301 (2018)
D.Bucurescu, N.V.Zamfir
Empirical signatures of shape phase transitions in nuclei with odd nucleon numbers
NUCLEAR STRUCTURE 128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152Ba, 133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154La, 130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157Ce, 130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158Pr, 132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161Nd, 133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162Pm, 134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164Sm, 135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,167Eu, 136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166Gd, 137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170Tb, 138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169Dy, 140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171Ho, 142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172Er, 146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173Tm, 149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174Yb, 72,73,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,98,100Kr, 75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,98,100Rb, 76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104Sr, 80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106Y, 80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107Zr, 84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110Nb, 84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110Mo, 87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,112Tc, 88,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,111,112,113Ru, 89,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115Rh; analyzed nuclear level density parameter a for back-shifted Fermi gas model formula (BSFG), S(2n), mean square charge radii, isotope shifts, correlation between the energy ratios and the relative energies for the favored band of the νi13/2 structures in the odd-mass nuclei for even Z=64-76. 152,154,156Tb; analyzed correlation between relative excitation energies of the favored sequence of the (πh11/2, νi13/2) structure. Discussed nuclear level density at low excitation energies as indicator of first order shape phase transition in nuclei.
doi: 10.1103/PhysRevC.98.024301
Chin.Phys.C 44, 094107 (2020)
V.Rani, P.Verma, S.Singh, M.Rajput, A.Bharti, G.H.Bhat, J.A.Sheikh
Systematic study of odd-mass 151-161Pm and 154, 156Pm isotopes using projected shell model
NUCLEAR STRUCTURE 151,153,155,157,159,161Pm, 154,156Pm; calculated yrast bands, B(E2), B(M1).
doi: 10.1088/1674-1137/44/9/094107
Thesis, Univ. of Valencia (2020)
A.Tolosa-Delgado
Study of beta-delayed neutron emitters in the region of 78Ni and its impact on r-process nucleosynthesis
NUCLEAR REACTIONS 9Be(238U, F)75Co/76Co/75Ni/76Ni/77Ni/78Ni/79Ni/76Cu/77Cu/78Cu/79Cu/80Cu/81Cu/82Cu/79Zn/80Zn/81Zn/82Zn/83Zn/84Zn/85Zn/82Ga/83Ga/84Ga/85Ga/86Ga/87Ga/85Ge/86Ge/87Ge/88Ge/89Ge/90Ge/88As/89As/90As/91As/92As/91Se/92Se/93Se/94Se/94Br/95Br, E=345 MeV/nucleon; measured fission fragments using BigRIPS and ZeroDegree spectrometers at RIBF-RIKEN facility for separation of fragments by A/Q and Z through measurements of time-of-flight (TOF), magnetic rigidity (Bρ) and energy loss (ΔE); deduced A/Q versus Z particle identification plots.
RADIOACTIVITY 75Co, 75,76,77,78Ni, 76,77,78,79,80,81Cu, 79,80,81,82,83,84Zn, 82,83,84,85,86,87Ga, 85,86,87,88,89Ge, 87,88,89,90,91,92As, 91,92,93Se, 92,94Br(β-), (β-n); 80,81Cu, 83,84Zn, 84,85,86,87Ga, 87,88,89Ge, 88,89,90,91,92As, 93Se(β-2n);[from 9Be(238U, F), E=345 MeV/nucleon]; measured implanted ions, neutrons, β, γ, β(implants)β-, (implants)β(1n)- and (implants)β(2n)-correlations, T1/2 of decays of ground states using BRIKEN neutron counter with 140 3He-filled proportional counters, AIDA array of DSSSDs for implants and β decays, two Clover HPGe detectors for γ radiation, and two thick plastic scintillators; deduced T1/2, %β-n or Pn, %β-2n or P2n from simultaneous fits of β-, β-1n and β-2n-decay curves, with uncertainties from Monte Carlo method, elemental abundances and effects on r-process nucleosynthesis. Comparison with previous experimental results, and with theoretical calculations in 2019Mo01 (At. Data Nucl. Data Tables 125, 1 (2019)) and 2016Ma12 (Phys. Rev. C 93, 025805 (2016)). Discussed systematics of T1/2 and Pn values for nuclei in the region of 78Ni.
Chin.Phys.C 45, 030003 (2021)
M.Wang, W.J.Huang, F.G.Kondev, G.Audi, S.Naimi
The AME 2020 atomic mass evaluation (II). Tables, graphs and references
ATOMIC MASSES A=1-295; compiled, evaluated atomic masses, mass excess, β-, ββ and ββββ-decay, binding, neutron and proton separation energies, decay and reaction Q-value data.
Phys.Rev. C 104, L021303 (2021)
R.Yokoyama, E.Ideguchi, G.S.Simpson, M.Tanaka, Y.Sun, C.-J.Lv, Y.-X.Liu, L.-J.Wang, S.Nishimura, P.Doornenbal, G.Lorusso, P.-A.Soderstrom, T.Sumikama, J.Wu, Z.Y.Xu, N.Aoi, H.Baba, F.L.Bello Garrote, G.Benzoni, F.Browne, R.Daido, Y.Fang, N.Fukuda, A.Gottardo, G.Gey, S.Go, S.Inabe, T.Isobe, D.Kameda, K.Kobayashi, M.Kobayashi, I.Kojouharov, T.Komatsubara, T.Kubo, N.Kurz, I.Kuti, Z.Li, M.Matsushita, S.Michimasa, C.B.Moon, H.Nishibata, I.Nishizuka, A.Odahara, Z.Patel, S.Rice, E.Sahin, H.Sakurai, H.Schaffner, L.Sinclair, H.Suzuki, H.Takeda, J.Taprogge, Zs.Vajta, H.Watanabe, A.Yagi
Three-quasiparticle isomers in odd-even 159, 161Pm: Calling for modified spin-orbit interaction for the neutron-rich region
RADIOACTIVITY 159,161Pm(IT)[from 9Be(238U, F), E=345 MeV/nucleon, followed by separation of fission fragments using the BigRIPS in-flight separator and implantation of fragments in WAS3ABi setup at RIBF-RIKEN facility]; measured Eγ, Iγ, γγ-coin, half-lives of the isomers by γ(t) using the EURICA array of 12 EUROBALL clusters. 159,161Pm; deduced high-spin levels, J, π, bands, 2-quasiparticle Nilsson configurations for the isomeric states, and 3-quasiparticle configurations from theory, existence of the deformed N=98 subshell gap in odd-mass nuclei. Comparison with projected shell model (PSM) calculations. Discussed modification of strength of spin-orbit interactions in standard Nilsson parameters for neutron-rich rare-earth nuclei around A=165.
doi: 10.1103/PhysRevC.104.L021303
Astrophys.J. 936, 107 (2022)
G.G.Kiss, A.Vitez-Sveiczer, Y.Saito, A.Tarifeno-Saldivia, M.Pallas, J.L.Tain, I.Dillmann, J.Agramunt, A.Algora, C.Domingo-Pardo, A.Estrade, C.Appleton, J.M.Allmond, P.Aguilera, H.Baba, N.T.Brewer, C.Bruno, R.Caballero-Folch, F.Calvino, P.J.Coleman-Smith, G.Cortes, T.Davinson, N.Fukuda, Z.Ge, S.Go, C.J.Griffin, R.K.Grzywacz, O.Hall, A.Horvath, J.Ha, L.J.Harkness-Brennan, T.Isobe, D.Kahl, T.T.King, A.Korgul, S.Kovacs, R.Krucken, S.Kubono, M.Labiche, J.Liu, J.Liang, M.Madurga, K.Miernik, F.Molina, A.I.Morales, M.R.Mumpower, E.Nacher, A.Navarro, N.Nepal, S.Nishimura, M.Piersa-Silkowska, V.Phong, B.C.Rasco, B.Rubio, K.P.Rykaczewski, J.Romero-Barrientos, H.Sakurai, L.Sexton, Y.Shimizu, M.Singh, T.Sprouse, T.Sumikama, R.Surman, H.Suzuki, T.N.Szegedi, H.Takeda, A.Tolosa, K.Wang, M.Wolinska-Cichocka, P.Woods, R.Yokoyama, Z.Xu
Measuring the β-decay Properties of Neutron-rich Exotic Pm, Sm, Eu, and Gd Isotopes to Constrain the Nucleosynthesis Yields in the Rare-earth Region
NUCLEAR REACTIONS 9Be(238U, X), E=345 MeV/nucleon; measured reaction products, TOF, Eβ, Iβ. 159,160,161,162,163,164,165,166Pm, 161,162,163,164,165,166,167,168Sm, 165,166,167,168,169,170Eu, 167,168,169,170,171,172Gd; deduced new isotopes T1/2 and β-delayed neutron emission probabilities, relative r-process abundance pattern for the neutron-star merger scenario. RIKEN Nishina Center, the Advanced Implantation Detector Array (AIDA) and the BRIKEN neutron detector array.