References quoted in the ENSDF dataset: 142CE ADOPTED LEVELS, GAMMAS

34 references found.

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1957RI43

Z.Naturforsch. 12a, 665 (1957)

W.Riezler, G.Kauw

Naturliche Radioaktivitat von Cer 142

1959SE49

Nature 184, 630 (1959)

F.E.Senftle, T.W.Stern, V.P.Alekna

α-Radioactivity of Cerium-142

1961MA05

Phys.Rev. 121, 1758 (1961)

R.D.Macfarlane, T.P.Kohman

Natural Alpha Radioactivity in Medium-Heavy Elements

NUCLEAR STRUCTURE ¹⁵²Gd, ¹⁴⁹Sm, ¹⁸⁰W, ¹⁷⁴Hf, ¹⁴⁴Nd, ¹⁴²Ce, ¹⁴⁸Sm, ¹⁴⁶Sm, ¹⁴⁷Sm, ¹⁹⁰Pt; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.121.1758

1970EN01

Phys.Rev. C1, 734 (1970)

G.Engler

Determination of the Static Quadrupole Moment of the First 2⁺ Excited State in ¹⁴²Ce

NUCLEAR REACTIONS ¹⁴²Ce(¹⁶O, ¹⁶O'), E=42 MeV; measured σ(E(¹⁶O'), θ). ¹⁴²Ce level deduced B(E2), quadrupole moment.

doi: 10.1103/PhysRevC.1.734

1975BA15

Phys.Rev. C11, 1755 (1975)

G.J.Basinger, W.C.Schick, Jr., W.L.Talbert, Jr.

γ-γ Angular Correlations of Transitions in ¹⁴²Ce

RADIOACTIVITY ¹⁴²La; measured γγ(θ). ¹⁴²Ce levels deduced L, J, π, γ-mixing.

doi: 10.1103/PhysRevC.11.1755

1977COZO

Diss.Abst.Int. 38B, 2173 (1977)

E.L.Cooper

Directional Correlation Studies of Even-Even Nuclei ⁷⁶Se, ⁸²Kr, ¹¹²Cd, ¹⁴²Ce

RADIOACTIVITY ⁷⁶As; measured γ(θ), γγ-coin. ⁷⁶Se levels deduced δ. ⁸²Br, ¹¹²Ag, ¹⁴²La; measured γγ(θ), oriented nuclei. ⁸²Kr, ¹¹²Cd, ¹⁴²Ce levels deduced δ. Ge(Li), NaI(Tl) spectrometer. Single-particle, collective-vibration, asymmetric rotor models.

1979BO26

Nucl.Instrum.Methods 164, 579 (1979)

H.G.Borner, W.F.Davidson, J.Almeida, J.Blachot, J.A.Pinston, P.H.M.Van Assche

High Precision Gamma-Ray Energy Measurements of Fission Products

NUCLEAR REACTIONS ²³⁵U, ²³⁹Pu(n, F), E=reactor spectrum; measured Eγ. ⁷⁹Ge, ^{85,87,88,89,90,91,92,93,94}Kr, ^92,93,95,98Rb, ^92,93,96,98Sr, ^{92,94,96,97,98,99,100}Y, ^{97,99,100,101}Zr, ^{99,100,101,102,103,104}Nb, ^{99,101,103,104,105,108}Mo, ^{99,101,102,103,104,105,106}Tc, ^105,109Ru, ^105,107,109Rh, ¹⁰⁹Pd, ¹²¹Cd, ^{125,128,130,131,132}Sn, ^{128,130,132,133,134}Sb, ^{131,132,133,134,135,136}Te, ^{131,132,133,134,135,136,138,140}I, ^{133,138,139,140,141,142}Xe, ^{138,140,141,143,144,145,146}Cs, ^{139,140,141,142,143,144,145,146}Ba, ^{141,143,144,146,147,148}Ce, ^{140,142,144,146,147,148}La, ^146,147,148Pr deduced transitions. ^234,235U targets.

1982MI01

J.Phys.(London) G8, 111 (1982)

E.Michelakakis, W.D.Hamilton, P.Hungerford, G.Jung, P.Pfeiffer, S.M.Scott

Levels and Transitions in ^142,144Ce Populated following the β Decay of ^142,144La

RADIOACTIVITY ^142,144La [from fission product Cs decay]; measured Eγ, Iγ, γγ(θ), oriented nuclei, γγ-coin; deduced Qβ. ^142,144Ce deduced levels, J, π, δ. Ge(Li) detectors.

doi: 10.1088/0305-4616/8/1/013

1983WO09

Phys.Rev. C28, 352 (1983)

A.Wolf, C.Chung, W.B.Walters, R.L.Gill, M.Shmid, R.E.Chrien, G.Peaslee

Gamma-Gamma Angular Correlation Studies for ¹⁴²Ce

RADIOACTIVITY ¹⁴²La(β^-) [from ²³⁵U(n, F), E=thermal]; measured γγ(θ). ¹⁴²Ce levels deduced J, π, δ. Mass separation, Ge detectors.

doi: 10.1103/PhysRevC.28.352

1988VE08

Phys.Rev. C38, 2982 (1988)

W.J.Vermeer, C.S.Lim, R.H.Spear

Mixed Symmetry in the Vibrational Nucleus ¹⁴²Ce

NUCLEAR REACTIONS ¹⁴²Ce(α, α'), E=10-12 MeV; ¹⁴²Ce(¹²C, ¹²C'), E=31-38 MeV; ¹⁴²Ce(¹⁶O, ¹⁶O'), E=44-50 MeV; measured particle spectra following Coulomb excitation. ¹⁴²Ce levels deduced B(λ), quadrupole moment.

doi: 10.1103/PhysRevC.38.2982

1990LA04

Phys.Rev. C41, 2312 (1990)

A.L.Lapolli, C.B.Zamboni, R.N.Saxena

Directional Correlations of γ Transitions in ¹⁴²Ce

RADIOACTIVITY ¹⁴²La(β^-) [from fission of U]; measured γγ(θ). ¹⁴²Ce levels deduced J, π, δ(E2/M1). Hyperpure Ge, Ge(Li) detectors.

doi: 10.1103/PhysRevC.41.2312

1991BA38

Nucl.Phys. A533, 541 (1991)

D.Bazzacco, F.Brandolini, K.Loewenich, P.Pavan, C.Rossi-Alvarez, E.Maglione, M.De Poli, A.M.I.Haque

Transient-Field g-Factor Measurement of the First 2⁺ States in the N = 82 Nuclei ¹⁴⁰Ce, ¹⁴²Nd and ¹⁴⁴Sm

NUCLEAR REACTIONS ¹⁴⁰Ce, ¹⁴²Nd, ¹⁴⁴Sm(³²S, ³²S'), E=110-116 MeV; measured γ(θ, H, t) in polarized Fe, (particle)γ-coin, Coulomb excitation. ¹⁴⁰Ce, ¹⁴²Nd, ¹⁴⁴Sm deduced 2⁺ level, g. Enriched targets, thin foil technique.

NUCLEAR STRUCTURE ¹⁴⁰Ce, ¹⁴²Nd, ¹⁴⁴Sm; calculated levels, g. Shell model, quasiparticle random phase approximation.

doi: 10.1016/0375-9474(91)90532-B

1992AL11

Yad.Fiz. 55, 890 (1992); Sov.J.Nucl.Phys. 55, 496 (1992)

M.M.Alhamidi, A.M.Demidov, M.M.Dyufani, M.S.Elahrash, V.A.Kurkin, I.V.Mikhailov, J.M.Rateb, S.M.Sergiwa, A.M.Shermit, S.M.Zlitni

Study of ¹⁴²Ce in the (n, n'γ) Reaction

NUCLEAR REACTIONS ¹⁴²Ce(n, n'γ), E=fast; measured Eγ, Iγ, γ(θ), linear polarization. ¹⁴²Ce deduced levels, J, π, δ.

1992CO21

Phys.Rev. C46, 1301 (1992)

J.Copnell, S.J.Robinson, J.Jolie, K.Heyde

Structure of the N = 84 Isotones ¹³⁸Xe-¹⁴⁶Sm

NUCLEAR STRUCTURE ¹³⁸Xe, ¹⁴⁰Ba, ¹⁴²Ce, ^143,144Nd, ¹⁴⁸Sm; calculated levels, B(λ). Interacting boson model, particle-core model.

doi: 10.1103/PhysRevC.46.1301

1992CO25

J.Phys.(London) G18, 1943 (1992)

J.Copnell, K.Kumar, S.J.Robinson, C.Tenreiro

An Application of the Dynamic Deformation Model to the N = 84 Isotones ¹³⁸Xe-¹⁴⁶Sm

NUCLEAR STRUCTURE ¹³⁸Xe, ¹⁴⁶Sm, ¹⁴⁰Ba, ¹⁴²Ce, ¹⁴⁴Nd; calculated levels, B(λ), δ. Dynamic deformation model.

doi: 10.1088/0954-3899/18/12/010

1992DI01

J.Phys.(London) G18, 329 (1992)

T.K.Dinh, M.Grinberg, C.Stoyanov

Interplay of Collective and Non-Collective Modes in Low-Lying Quadrupole States of ¹⁴⁰Ba, ¹⁴²Ce, ¹⁴⁴Nd and ¹⁴⁶Sm

NUCLEAR STRUCTURE ¹⁴⁰Ba, ¹⁴²Ce, ¹⁴⁴Nd, ¹⁴⁶Sm; calculated levels, B(λ), μ, quadrupole moment, δ. Quasiparticle-phonon model.

doi: 10.1088/0954-3899/18/2/014

1992EG01

Nucl.Phys. A545, 589 (1992)

J.L.Egido, L.M.Robledo

A Systematic Study of the Octupole Correlations in the Lanthanides with Realistic Forces

NUCLEAR STRUCTURE ^{148,146,144,142,140}Ba, ^{142,144,146,148,150}Ce, ^{144,146,148,150,152}Nd, ^{146,148,150,152,154}Sm; calculated collective potential energies, level splittings, B(λ), dipole moments, ground state deformations. Adiabatic time dependent Hartree-Fock plus zero point energy, cranking approximation.

doi: 10.1016/0375-9474(92)90294-T

1992NA07

Phys.Rev. C45, 2226 (1992)

W.Nazarewicz, S.L.Tabor

Octupole Shapes and Shape Changes at High Spins in the Z ≈ 58, N ≈ 88 Nuclei

NUCLEAR STRUCTURE ^224,226Th, ^144,146Ba, ¹⁴⁶Ce, ¹⁴⁰Xe, ¹⁵⁰Sm; calculated total Routhian surfaces. ^{138,140,142,144,146,148}Xe, ^{140,142,144,146,148,150}Ba, ^{144,146,148,150,152,156}Nd, ^{142,144,146,148,150,152}Ce, ^{146,148,150,152,154,156}Sm, ^{148,150,152,154,156,158}Gd; calculated equilibrium deformation vs rotational frequency; deduced shape change features. Cranking model, Woods-Saxon average potential, pairing.

doi: 10.1103/PhysRevC.45.2226

1992WO11

Phys.Rev. C46, 1323 (1992)

A.Wolf, R.F.Casten

Effective Charges and Their Relation to Collectivity and Shell Structure

NUCLEAR STRUCTURE ^{126,128,130,132,134}Xe, ^{154,156,158,160}Gd, ^{164,166,168,170,172,176}Yb, ^138,142,144Ba, ^140,142,146Ce, ^142,144,146Nd, ^144,148,150Sm; analyzed B(E2) data; deduced effective charges relation to collectivity, shell structure.

doi: 10.1103/PhysRevC.46.1323

1995VA25

Phys.Rev. C52, 2387 (1995)

J.R.Vanhoy, J.M.Anthony, B.M.Haas, B.H.Benedict, B.T.Meehan, S.F.Hicks, C.M.Davoren, C.L.Lundstedt

Structural Characteristics of ¹⁴²Ce Through Inelastic Neutron Scattering

NUCLEAR REACTIONS ¹⁴²Ce(n, n'γ), E=2-2.53 MeV; measured Eγ, Iγ, Doppler shifts, Iγ(θ). ¹⁴²Ce deduced levels, J, π, δ, B(λ), T_1/2. Phonon, interacting boson, particle core coupling models.

doi: 10.1103/PhysRevC.52.2387

1995ZH26

Phys.Rev. C52, 1453 (1995)

Y.M.Zhao, Y.Chen

Regional Regularities for the Even-Even Nuclei: Medium to heavy systems

NUCLEAR STRUCTURE ^{144,146,148,150,152}Nd; calculated energy spectra rms deviations. ^{142,144,146,148,150}Ce, ^{144,146,150,152}Nd, ^{146,148,150,152,154}Sm, ^{148,150,152,154,156}Gd, ^{150,152,154,156,158}Dy, ^{152,154,156,158,160}Er, ^{154,156,158,160,162}Yb, ^{74,76,78,80,82,84,88,90,92}Kr, ^{80,82,84,86,90}Sr, ⁷²Se, ^{92,94,96,98,100}Sr, ^{82,84,86,88,92,94,96,98,100,102}Zr, ^{88,90,94,96,98,100}Mo, ^164,166Yb, ^166,168Hf, ^168,170W; calculated effective boson numbers. Z=50-82; N=82-126; analyzed levels, B(E2) systematics.

doi: 10.1103/PhysRevC.52.1453

1998TS05

Yad.Fiz. 61, No 5, 816 (1998); Phys.Atomic Nuclei 61, 734 (1998)

N.Tsoneva, A.I.Vdovin, Ch.Stoyanov, M.Grinberg

Magnetic Polarization and Two-Phonon States

NUCLEAR STRUCTURE ¹⁴²Ce, ¹⁴⁴Sm; calculated two-phonon states wave functions, B(M2); deduced magnetic core polarization effect.

1999GAZX

Program and Thesis, Proc.49th Ann.Conf.Nucl.Spectrosc.Struct.At.Nuclei, Dubna, p.98 (1999)

Yu.P.Gangrsky, S.G.Zemlyanoy, B.N.Markov, K.P.Marinova

Charge Radii of Nuclei Near the Neutron Closed Shells

NUCLEAR MOMENTS ^{39,40,41,42,46,47,48}Ca, ^48,49,50Ti, ^{84,85,86,87,88}Kr, ^{86,87,88,89,90}Sr, ^90,91,92Zr, ^{136,137,138,139,140}Ba, ^138,140,142Ce, ^{140,141,142,143,144}Nd, ^{142,143,144,145,146}Sm, ^204,205,206Hg, ^{206,207,208,209,210}Pb; measured mean square radii difference. Laser resonance fluorescence method.

1999IS02

Phys.Rev. C59, 1794 (1999)

Y.Ishida, H.Iimura, S.Ichikawa, T.Horiguchi

Mean-Square Nuclear Charge Radius of Radioactive ¹⁴⁴Ce by Laser Spectroscopy

NUCLEAR MOMENTS ^{136,138,140,142,144}Ce; measured isotope shifts; deduced mean square charge radii, quadrupole deformation. Collinear laser-ion-beam spectroscopy.

doi: 10.1103/PhysRevC.59.1794

1999ZA09

Eur.Phys.J. A 5, 53 (1999)

D.A.Zaikin, I.V.Surkova, M.V.Mordovsky

Low-Energy Neutron Interaction with Even-Even Nuclei and Coupled Channel Optical Model

NUCLEAR REACTIONS ^58,60,62,64Ni, ^64,66,68,70Zn, ^70,72,74,76Ge, ^{74,76,78,80,82}Se, ^84,86,88Sr, ^90,92,94,96Zr, ^{92,94,96,98,100}Mo, ^{106,108,110,112,114,116}Cd, ^{112,114,116,118,120,122,124}Sn, ^{122,124,126,128,130}Te, ^134,136,138Ba, ^140,142Ce, ¹⁴⁴Nd, ^144,148Sm, ¹⁹²Os, ¹⁹⁸Pt, ²⁰²Hg, ^204,206Pb(n, X), (n, n), E=low; calculated total, elastic, inelastic scattering strength functions, scattering lengths. Coupled channel optical model.

doi: 10.1007/s100500050256

2003AU03

Nucl.Phys. A729, 337 (2003)

G.Audi, A.H.Wapstra, C.Thibault

The AME2003 atomic mass Evaluation (II). Tables, graphs, and references

COMPILATION A=1-293; compiled, evaluated atomic mass data.

doi: 10.1016/j.nuclphysa.2003.11.003

2006YU04

Int.J.Mod.Phys. E15, 939 (2006)

M.Yu, P.-F.Zhang, T.-N.Ruan, J.-Y.Guo

Shape evolution for Ce isotopes in relativistic mean-field theory

NUCLEAR STRUCTURE ^{120,122,124,126,128,130,132,134,136,138,140,142}Ce; calculated binding energies, potential energy surfaces, single-particle energies, deformation. Relativistic mean-field approach.

doi: 10.1142/S0218301306004661

2007JI05

Phys.Rev. C 75, 034307 (2007)

L.Y.Jia, H.Zhang, Y.M.Zhao

Systematic calculations of low-lying states of even-even nuclei within the nucleon pair approximation

NUCLEAR STRUCTURE ^{124,126,128,130,134,136,138,140}Sn, ^{126,128,130,132,134,136,138,140,142}Te, ^{128,130,132,134,136,138,140,142,144}Xe, ^{130,132,134,136,138,140,142,144,146}Ba, ^{132,134,136,138,140,142,144,146,148}Ce; calculated levels, J, π, B(E2), g factors. Shell model, pair approximation.

doi: 10.1103/PhysRevC.75.034307

2007VE14

Eur.Phys.J. A 34, 349 (2007)

Ts.Venkova, M.-G.Porquet, I.Deloncle, P.Petkov, A.Astier, A.Prevost, F.Azaiez, A.Bogachev, A.Buta, D.Curien, O.Dorvaux, G.Duchene, J.Durell, B.J.P.Gall, M.Houry, F.Khalfallah, R.Lucas, M.Meyer, I.Piqueras, N.Redon, A.Roach, M.Rousseau, O.Stezowski, Ch.Theisen

New high-spin states of ¹⁴²₅₈Ce and ¹⁴⁰₅₆Ba from fusion-fission reactions: Proton excitations in the N = 84 isotones

NUCLEAR REACTIONS ²³⁸U(¹²C, X)¹⁴⁰Ba/¹⁴²Ce, E=90 MeV; ²⁰⁸Pb(¹⁸O, X)¹⁴⁰Ba/¹⁴²Ce, E=85 MeV; measured Eγ, Iγ, γγ-coin. ¹⁴⁰Ba, ¹⁴²Ce deduced high-spin levels, J, π, configurations. Euroball III and IV arrays.

doi: 10.1140/epja/i2007-10526-y

2008KI07

Nucl.Instrum.Methods Phys.Res. A589, 202 (2008)

T.Kibedi, T.W.Burrows, M.B.Trzhaskovskaya, P.M.Davidson, C.W.Nestor, Jr.

Evaluation of theoretical conversion coefficients using BrIcc

COMPILATION Z=5-110; compiled and evaluated ICC data. BrICC database.

doi: 10.1016/j.nima.2008.02.051

2009LO02

Phys.Rev. C 80, 024311 (2009)

N.Lo Iudice, Ch.Stoyanov, N.Pietralla

Splitting of the 2⁺ mixed symmetry mode in the proximity of the N = 82 shell closure

NUCLEAR STRUCTURE ^138,142Ce, ¹⁴⁴Nd; calculated 2+ mixed symmetry states, B(E2), B(M1), configurations using quasiparticle phonon model calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.024311

2010PRZZ

arXiv:1004.3280v1 [nucl-th] (2010)

B.Pritychenko

On Double-Beta Decay Half-Life Time Systematics

COMPILATION ⁴⁸Ca, ⁷⁶Ge, ⁸²Se, ⁹⁶Zr, ¹⁰⁰Mo, ¹¹⁶Cd, ^128,130Te, ¹³⁰Ba, ¹⁵⁰Nd, ²³⁸U; compiled evaluated 2β-decay data.

NUCLEAR STRUCTURE ^46,48Ca, ⁷⁰Zn, ⁷⁶Ge, ^80,82Se, ⁸⁶Kr, ^94,96Zr, ^98,100Mo, ¹⁰⁴Ru, ¹¹⁰Pd, ^114,116Cd, ^122,124Sn, ^128,130Te, ^134,136Xe, ¹⁴²Ce, ^146,148,150Nd, ¹⁵⁴Sm, ¹⁶⁰Gd, ¹⁷⁰Er, ¹⁷⁶Yb, ¹⁸⁶W, ¹⁹²Os, ¹⁹⁸Pt, ²⁰⁴Hg, ²³²Th, ²³⁸U; calculated 2β^--decay T_1/2; deduced T_1/2 energy trend. Comparison with experimental data.

2011AUZZ

Priv.Comm. (2011)

G.Audi, W.Meng

Atomic Mass Evaluation 2011

2012WA38

Chin.Phys.C 36, 1603 (2012)

M.Wang, G.Audi, A.H.Wapstra, F.G.Kondev, M.MacCormick, X.Xu, B.Pfeiffer

The AME2012 atomic mass evaluation (II). Tables, graphs and references

COMPILATION A=1-295; compiled, evaluated atomic mass data.