References quoted in the XUNDL dataset: 130TE 130SB B- DECAY:T1/2:XUNDL-11

8 references found.

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

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2004BR19

Eur.Phys.J. A 20, 145 (2004)

R.Broda, B.Fornal, W.Krolas, T.Pawlat, J.Wrzesinski, D.Bazzacco, G.de Angelis, S.Lunardi, C.Rossi Alvarez

Hard-to-reach nuclei studied with deep-inelastic heavy-ion reactions

NUCLEAR STRUCTURE ^125,126Sn, ¹³⁰Te, ²⁰⁸Pb; compiled, analyzed γ-spectra, levels, J, π. ²⁰⁶Hg, ^206,207Tl, ^{206,207,208,209,210}Pb, ²⁰⁹Bi; analyzed yrast E3 transitions.

doi: 10.1140/epja/i2003-10206-0

2004VA03

Phys.Rev. C 69, 024316 (2004)

J.J.Valiente-Dobon, P.H.Regan, C.Wheldon, C.Y.Wu, N.Yoshinaga, K.Higashiyama, J.F.Smith, D.Cline, R.S.Chakrawarthy, R.Chapman, M.Cromaz, P.Fallon, S.J.Freeman, A.Gorgen, W.Gelletly, A.Hayes, H.Hua, S.D.Langdown, I.Y.Lee, X.Liang, A.O.Macchiavelli, C.J.Pearson, Zs.Podolyak, G.Sletten, R.Teng, D.Ward, D.D.Warner, A.D.Yamamoto

¹³⁶Ba studied via deep-inelastic collisions: Identification of the (νh_11/2)^-2₁₀₊ isomer

NUCLEAR REACTIONS ¹⁹⁸Pt(¹³⁶Xe, X), E=850 MeV; measured prompt and delayed Eγ, Iγ, γγ-, (particle)γ-coin. ¹³⁶Ba deduced levels, J, π, B(E2), isomer T_1/2. ^128,130Te, ^131,133I, ^132,136Xe, ¹³⁸Ba, ¹³⁷La, ¹⁸⁴W, ¹⁸⁵Re, ^191,192,195Os, ^192,198Pt, ¹⁹³Au; deduced isomers T_1/2. Gammasphere, Chico arrays.

doi: 10.1103/PhysRevC.69.024316

2013ST24

Phys.Rev. C 88, 051304 (2013)

A.E.Stuchbery, J.M.Allmond, A.Galindo-Uribarri, E.Padilla-Rodal, D.C.Radford, N.J.Stone, J.C.Batchelder, J.R.Beene, N.Benczer-Koller, C.R.Bingham, M.E.Howard, G.J.Kumbartzki, J.F.Liang, B.Manning, D.W.Stracener, C.-H.Yu

Electromagnetic properties of the 2⁺₁ state in ¹³⁴Te: Influence of core excitation on single-particle orbits beyond ¹³²Sn

NUCLEAR REACTIONS C(¹³⁰Te, ¹³⁰Te'), (¹³⁴Te, ¹³⁴Te'), E=390 MeV, also 343 MeV for ¹³⁰Te; measured scattered particle spectra, Eγ, Iγ, (particle)γ-coin, (particle)γ(θ) using HyBall array for particles and Clarion array of Clover Ge detectors for γ rays at HRIBF-ORNL facility. Combined analysis of B(E2) from Coulomb excitation and g factor from recoil-in vacuum (RIV) method. ^130,134Te; deduced level, B(E2) and g factors of first 2+ states. Comparison with previous experimental results, and with theoretical calculations. Systematics of g factors and B(E2) values for ^{130,132,134,136}Te, and for first 2+, 4+ and 6+ states in ¹³⁴Te.

NUCLEAR MOMENTS ¹³⁴Te; measured g factor of first 2+ state by recoil-in vacuum (RIV) method in Coulomb excitation at HRIBF-ORNL facility. Combined analysis of Coulomb excitation and recoil-in vacuum (RIV) method. Systematics of g factors of first 2+ states in ^{130,132,134,136}Te. Comparison with theoretical calculations.

doi: 10.1103/PhysRevC.88.051304

2014AS01

Eur.Phys.J. A 50, 2 (2014)

A.Astier, M.-G.Porquet, Ts.Venkova, Ch.Theisen, G.Duchene, F.Azaiez, G.Barreau, D.Curien, I.Deloncle, O.Dorvaux, B.J.P.Gall, M.Houry, R.Lucas, N.Redon, M.Rousseau, O.Stezowski

High-spin structures of ^124-131Te: Competition of proton- and neutron-pair breakings

NUCLEAR REACTIONS ²⁰⁸Pb(¹⁸O, X), E=85 MeV;²³⁸U(¹²C, X), E=90 MeV; measured thick target prompt Eγ, Iγ, γγ-coin using unsuppressed Ge detectors, delayed and off-line Eγ, Iγ, γγ-coin. ^{124,125,126,127,128,129,130,131,132,134}Te deduced levels, J, π, γ transitions. ^128,130Te deduced isomeric transitions, T_1/2. ^{126,128,130,132}Te deduced isomeric and/or some other states B(E1), B(E2). ^125,126Sn, ^{128,129,130,131}Te calculated high-spin states using shell model. Compared with data.

doi: 10.1140/epja/i2014-14002-5

2020COZY

Proc.Intern.Conf.Heavy Ion Accelerator Symposium (HIAS 2019), Canberra, Australia, Sept. 9-13, 2019, A.J. Mitchell, et al. Eds., p.04003 (2020);EPJ Web of Conf.Vol.232 (2020)

B.J.Coombes, A.E.Stuchbery, J.M.Allmond, A.Gargano, J.T.H.Dowie, G.Georgiev, M.S.M.Gerathy, T.J.Gray, T.Kibedi, G.J.Lane, B.P.McCormick, A.J.Mitchell, N.J.Spinks, B.P.E.Tee

Emerging nuclear collectivity in ^124-130Te

NUCLEAR REACTIONS ^{124,126,128,130}Te(⁶⁸Ni, ⁶⁸Ni') E=198, 200, 205 MeV; measured Eγ, Iγ, γγ-coin with four HPGe clover detectors, part of CLARION array; ¹²⁴Te, ¹²⁶Te, ¹²⁶Te, ¹²⁸Te, ¹³⁰Te deduced B(E2). Comparison to large-scale shell-model calculations performed with code Antoine. ANU 14UD Pelletron accelerator.

doi: 10.1051/epjconf/202023204003

2021WA16

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.

doi: 10.1088/1674-1137/abddaf

2022KU31

Phys.Rev. C 106, 034306 (2022)

D.Kumar, T.Bhattacharjee, S.S.Alam, S.Basak, L.Gerhard, L.Knafla, A.Esmaylzadeh, M.Ley, F.Dunkel, K.Schomaker, J.-M.Regis, J.Jolie, Y.H.Kim, U.Koster, G.S.Simpson, L.M.Fraile

Lifetimes and transition probabilities for low-lying yrast levels in ^{130, 132}Te

RADIOACTIVITY ^130,132Sb(β^-); ^130m,132mTe(IT) [from ²³³U(n, γ), E=thermal, followed by mass-separation of fission fragments by the Lohengrin separator at Institut Laue-Langevin, Grenoble]; measured Eγ, Iγ, γγ-coin, isomer and level T_1/2 by γ(t) and γγ(t) fast-timing method using four LaBr₃(Ce) detectors and two Clover HPGe detectors, and analyzed using generalized centroid difference (GCD) method, and by slope method. ^130,132Te; deduced levels, T_1/2 of levels and isomers, B(E2) for yrast members of the g.s. bands up to 10+, configurations. Comparison with large-basis shell model calculations, and with previous experimental results. Systematics of B(E2) values for g.s. band members up to 10+ for ^{126,128,130,132,134}Te.

doi: 10.1103/PhysRevC.106.034306

2022PR02

Phys.Rev. C 105, 034319 (2022)

S.Prill, A.Bohn, V.Everwyn, G.Hafner, F.Heim, M.Spieker, M.Weinert, J.Wilhelmy, A.Zilges

Lifetime analysis of ^{128, 130}Te via the Doppler-shift attenuation method

NUCLEAR REACTIONS ¹²⁸Te(p, p'γ), E=8.8 MeV; ¹³⁰Te(p, p'γ), E=10 MeV; measured Ep, Ip, Eγ, Iγ, pγ-coin. ^128,130Te; deduced levels, J, π, T_1/2 of excited states, B(E2), B(M1). p-γ-coincidence DSA technique for half-life determination. Comparison to shell-model calculations performed with NuShellX in the jj55pn model space. Combined SONIC (Si-detectors) and HORUS (HPGe-detectors) arrays.

doi: 10.1103/PhysRevC.105.034319