References quoted in the ENSDF dataset: 154ND ADOPTED LEVELS, GAMMAS

26 references found.

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

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1970JO20

Phys.Rev. C2, 1451 (1970)

W.John, F.W.Guy, J.J.Wesolowski

Four-Parameter Measurements of Isomeric Transitions in ²⁵²Cf Fission Fragments

RADIOACTIVITY ^134mTe, ^136mXe; measured T_1/2, Eγ, Iγ.

RADIOACTIVITY, Fission ²⁵²Cf(SF); measured (fragment)(fragment)(γ)-coin, (fragment)(γ)-delay.

doi: 10.1103/PhysRevC.2.1451

1970WI16

Phys.Rev.Lett. 25, 1122 (1970)

J.B.Wilhelmy, S.G.Thompson, R.C.Jared, E.Cheifetz

Ground-State Bands in Neutron-Rich Even Te, Xe, Ba, Ce, Nd, and Sm Isotopes Produced in the Fission of ²⁵²Cf

RADIOACTIVITY, Fission ²⁵²Cf(SF); measured (fragment)(fragment)(X)-, (fragment)(fragment)(X)(γ)-coin. ^132,134Te, ^138,140Xe, ^{140,142,144,146}Ba, ^{144,146,148,150}Ce, ^152,154Nd, ^156,158Sm; measured Eγ, Iγ; deduced levels, T_1/2, B(E2).

doi: 10.1103/PhysRevLett.25.1122

1974BU09

Atomkernenergie 22, 268 (1974)

K.Buchtela

Anwendungsbeispiele der Hochspannungselektrophorese zur Trennung von Radionukliden. II. Trennung kurzlebiger Uranspaltungsprodukte

RADIOACTIVITY ^142,143,144La, ¹⁴⁶Ce, ^{146,148,149,150}Pr, ¹⁵⁴Nd, ¹⁵⁴Pm; measured Iγ, Eγ, T_1/2.

1974CLZX

Proc.Symp.Phys.Chem.Fission, 3rd, Rochester, N.Y. (1973), Int.At.En.Agency, Vienna, Vol.2, p.221 (1974)

R.G.Clark, L.E.Glendenin, W.L.Talbert, Jr.

Fission Fragment Isomers from Spontaneous Fission of ²⁵²Cf

RADIOACTIVITY, Fission ²⁵²Cf(SF); measured Eγ, Iγ, γf(t), Xγ-, γγ-coin. ⁸⁷Br, ⁸⁹Kr, ⁹²Rb, ^95,96,97Sr, ^97,98Y, ^{99,100,101,102,103}Zr, ¹⁰²Nb, ^{103,104,106,107}Mo, ^105,107,108Tc, ^109,110,111Ru, ^109,111Rh, ^132,134Sb, ^134,135Te, ^134,136,137I, ^136,137Xe, ^147,148,149Ce, ^139,140,141Cs, ^{141,143,144,146}Ba, ^146,147La, ^149,150,151Pr, ¹⁵⁴Nd, ^156,158Sm deduced transitions, T_1/2, fission yields.

1974JAYY

Proc.Symp.Phys.Chem.Fission, 3rd, Rochester, N.Y. (1973); Intern.At.En.Agency, Vienna, Vol.2, p.211 (1974)

R.C.Jared, H.Nifenecker, S.G.Thompson

Measurement of Prompt Gamma-Ray Lifetimes of Fission Fragments of ²⁵²Cf

RADIOACTIVITY ^100,102Zr, ^104,106Mo, ^108,110,112Ru, ^114,116Pd, ^142,144,146Ba, ^146,148,150Ce, ¹⁵⁴Nd [from ²⁵²Cf(SF)]; measured Eγ, T_1/2; deduced B(E2), β₂, quadrupole moment.

1981CA12

Phys.Rev.Lett. 47, 1433 (1981)

R.F.Casten, D.D.Warner, D.S.Brenner, R.L.Gill

Relation between the Z = 64 Shell Closure and the Onset of Deformation at N = 88-90

NUCLEAR STRUCTURE ^142,144,146Ba, ^{144,146,148,150}Ce, ^{146,148,150,152,154}Nd, ^{148,150,152,154,156,158}Sm, ^{150,152,154,156,158,160}Gd, ^{152,154,156,160,162}Dy, ^{154,156,158,160,162,164}Er, ^{156,158,160,162,164,166}Yb; analyzed E(2), E(4) systematics; deduced shell closure effects at Z=64.

doi: 10.1103/PhysRevLett.47.1433

1983MA03

Nuovo Cim. 73A, 1 (1983)

G.Maino, A.Ventura

Collective Features in the Spectroscopy of Even Neodymium Isotopes

NUCLEAR STRUCTURE ^{136,138,140,144,146,148,150,152,154}Nd; calculated levels, B(λ), B(λ) ratios. ^{144,146,148,150,152}Nd; calculated quadrupole moments. Interacting boson model.

1984NA22

Nucl.Phys. A429, 269 (1984)

W.Nazarewicz, P.Olanders, I.Ragnarsson, J.Dudek, G.A.Leander, P.Moller, E.Ruchowska

Analysis of Octupole Instability in Medium-Mass and Heavy Nuclei

NUCLEAR STRUCTURE ¹⁴⁶Ba, ²²⁴Ra; calculated octupole deformation energy. ⁷²Se, ⁹²Kr, ¹⁴⁶Ba, ²²⁴Th; calculated octupole deformation potential energy. ^74,90Kr; calculated shell plus pairing, Strutinsky energies. ^{140,142,144,146,148}Xe, ^{142,144,146,148,150}Ba, ^{142,144,146,148,150,152}Ce, ^{146,148,150,152,154}Nd, ²¹⁸Po, ^{218,220,222,224,226}Rn, ^{218,220,222,224,226,228,230}Ra, ^{220,222,224,226,228,230}Th, ^{222,224,226,228,230}U; calculated equilibrium shapes. Strutinsky type calculations.

doi: 10.1016/0375-9474(84)90208-2

1985CA29

Nucl.Phys. A443, 1 (1985)

R.F.Casten

N(p)N(n) Systematics in Heavy Nuclei

NUCLEAR STRUCTURE ^96,94,98,100Sr, ^{98,96,100,102}Zr, ^{98,100,102,104,106}Mo, ^{100,102,104,106,108,110}Ru, ^{102,104,106,108,110,112}Pd, ^{134,132,130,128,126,124,122,120}Xe, ^{150,136,134,132,130,128,126,156,154,152,124,122}Ba, ^{138,136,134,132,130,128,126,150,148,146,144,142}Ce, ^{140,138,136,134,132,130,128,156,154,152,150,148,146,144}Nd, ^{158,156,154,152,150,148,146}Sm, ^{160,158,156,154,152,150,148}Gd, ^{162,160,158,156,154,152,150}Dy, ^{164,162,160,158,156,154,152}Er, ^{166,164,162,160,158}Yb; analyzed level, valance nucleon product systematics; deduced deformation near A=100 mechanism.

doi: 10.1016/0375-9474(85)90318-5

1985CA33

Nucl.Phys. A444, 133 (1985)

R.F.Casten, W.Frank, P.von Brentano

Multi-Nucleus IBA Calculations in the (N(π)N(ν)) Scheme

NUCLEAR STRUCTURE ^{94,96,102,104,98,100}Sr, ^{96,98,104,106,100,102}Zr, ^{98,108,100,102,104,106}Mo, ^{100,102,104,106,108,110}Ru, ^{102,104,106,108,110,112}Pd, ^{142,144,146,148}Ba, ^{144,146,148,150,152}Ce, ^{146,148,150,152,154,156}Nd, ^{148,150,152,154,156,158,160}Sm, ^{150,152,154,156,158,160,162,164}Gd, ^{152,154,156,158,160,162,164}Dy, ^{154,156,158,160,162,164,166,168}Er, ^{158,160,162,164,166,168,170}Yb, ^{164,166,168,170,172}Hf, ^170,172,174W, ^{104,106,108,110,112,114}Cd; calculated levels, B(E2) ratios. Multi-nucleus interacting boson approximation.

doi: 10.1016/0375-9474(85)90295-7

1985KA17

Z.Phys. A322, 177 (1985)

T.Karlewski, N.Hildebrand, G.Herrmann, N.Kaffrell, N.Trautmann, M.Brugger

Decay of the Heaviest Isotope of Neodymium: ¹⁵⁴Nd

RADIOACTIVITY ¹⁵⁴Nd(β^-) [from ²³⁵U fission product separation]; measured Eγ, Iγ, E X-ray, I X-ray, γ(X-ray)-, γγ-coin; deduced T_1/2. ¹⁵⁴Pm deduced levels, γ-branching.

1985RO21

Nucl.Phys. A445, 495 (1985)

P.Rozmej

The Influence of Zero-Point Vibrations on Multipole Moments of Rare-Earth Nuclei

NUCLEAR STRUCTURE ^{160,162,164,166,168,170,172,174,176,178,180,182,194,196,198}Hf; calculated static quadrupole, hexadecapole reduced matrix elements, equilibrium deformations. ^{146,148,150,152,154,156,158,160,162}Nd, ^{148,150,152,154,156,158,160,162,164}Sm, ^{150,152,154,156,158,160,162,164,166}Gd, ^{152,154,156,158,160,162,164,166}Dy, ^{154,156,158,160,162,164,166,168,170}Er, ^{174,176,178,180,182,184,186,188,190}W, ^{176,178,180,182,184,186,188,190,192}Os, ^{178,180,182,184,186,188,190,192,194}Pt; calculated electric quadrupole, hexadecapole transition reduced matrix elements. ^160,152Gd; calculated potential energy surfaces, collective probability densities. Zero-point vibration effects, macroscopic-microscopic method.

doi: 10.1016/0375-9474(85)90454-3

1985VO08

Nucl.Phys. A439, 207 (1985)

O.K.Vorov, V.G.Zelevinsky

Quartic Anharmonicity and Angular Momentum Effects in Even-Even Spherical Nuclei

NUCLEAR STRUCTURE ^{98,100,102,104,106,108,110}Pd; calculated levels, energy ratio rms deviations, B(E2) ratios. ^{95,96,97,98,99,100,102,104,106,108,112}Ru, ^{100,102,104,106,108,110,112,114,116,118,120,122}Cd, ^{134,136,138,140,142,144,146,148,150,152,154}Nd, ^{138,140,142,146,148,150,152,154,156,158}Sm, ^{146,148,150,152,154,156,158,160,162}Gd, ^{154,156,158,160,152,162}Dy; calculated energy parameter vs neutron number.

doi: 10.1016/0375-9474(85)90428-2

1986GRZZ

Bull.Am.Phys.Soc. 31, No.4, 873, JI3 (1986)

R.C.Greenwood, J.D.Cole, R.A.Anderl

Identification of New Isotopes ¹⁵⁴Nd and ¹⁵⁵Nd, Produced in ²⁵²Cf Fission

RADIOACTIVITY ²⁵²Cf(SF); measured X-ray, γ-ray spectra following fission. ^154,155Nd deduced T_1/2. ^154,155Pm deduced γ-transitions.

1987GR12

Phys.Rev. C35, 1965 (1987)

R.C.Greenwood, R.A.Anderl, J.D.Cole, H.Willmes

Identification of New Neutron-Rich Rare-Earth Isotopes Produced in ²⁵²Cf Fission

RADIOACTIVITY ²⁵²Cf(SF); measured K X-ray decay rates, Eγ, Iγ. ¹⁵³Pr, ^{153,154,155,156}Nd, ^156,157,158Pm, ^159,160Sm, ¹⁶²Eu deduced T_1/2. Isotope separation, on-line system.

doi: 10.1103/PhysRevC.35.1965

1987NE03

Nucl.Phys. A462, 252 (1987)

B.Nerlo-Pomorska, K.Pomorski, M.Brack, E.Werner

Multipole Moments of Rare-Earth Nuclei in the Generator Coordinate Method

NUCLEAR STRUCTURE ¹⁶⁶Er; calculated potential energy surface, charge monopole, electric quadrupole, hexadecapole moments, overlap width mass parameters; ^{148,150,152,154,156,158,160,162,164,166}Nd, ^{150,152,154,156,158,160,162,164,166,168}Sm, ^{152,154,156,158,160,162,164,166,168,170}Gd, ^{160,162,164,166,168,170,172,174,176,178}Hf, ^{158,160,162,164,166,168,170,172,174,176}Yb, ^{156,158,160,162,164,166,168,170,172,174}Er, ^{154,156,158,160,162,164,168,170,172}Dy; calculated charge rms radii, hexadecapole electric moments. Generator coordinate method, gaussian overlap approximation.

doi: 10.1016/0375-9474(87)90547-1

1987NE07

Z.Phys. A328, 11 (1987)

B.Nerlo-Pomorska

Deformation Energies of Rare-Earth Nuclei in Generator Coordinate Method

NUCLEAR STRUCTURE ^{144,146,148,150,152,154,156,158,160,162,164}Ce, ^{144,146,148,152,154,156,158,160,162,164,166}Nd, ^{148,150,152,154,156,158,160,162,164,166,168}Sm, ^{150,152,154,156,158,160,162,164,166,168}Gd, ^{152,154,156,158,160,162,164,166,168,170,172}Dy, ^{154,156,158,160,162,164,166,168,170,172,174,176}Er, ^{156,158,160,162,164,166,168,170,172,174,176}Yb, ^{158,160,162,164,166,168,170,172,174,176,178}Hf; calculated deformation. Mean field Nilsson hamiltonian.

1988GRZY

Proc. 5th Int.Conf.Nuclei Far from Stability, Rosseau Lake, Canada 1987, Ed., I.S.Towner, p.782 (1988), AIP Conf.Proc. 164 (1987)

R.C.Greenwood, R.A.Anderl, J.D.Cole, M.A.Lee, H.Willmes

Identification of New Neutron-Rich Rare-Earth Isotopes Produced in ²⁵²Cf Spontaneous Fission

RADIOACTIVITY ^153,152,151Pr, ^{155,156,153,154}Nd, ^{157,158,153,155,156}Pm, ^162,161Eu, ¹⁶⁴Gd, ^{157,158,159,160}Sm(β^-) [from ²⁵²Cf(SF)]; measured decay products; deduced T_1/2.

doi: 10.1063/1.36957

1990AN31

J.Radioanal.Nucl.Chem. 142, 203 (1990)

R.A.Anderl, R.C.Greenwood

Nuclear Decay Studies of Fission-Product Nuclides Using an On-Line Mass Separation Technique

RADIOACTIVITY ^151,152,153Pr, ^{153,154,155,156,157,158}Pm, ^{157,159,158,160}Sm, ^161,162Eu, ¹⁶⁴Gd; measured T_1/2, γγ-, βγ-coin. ¹⁵⁴Pm deduced levels. On-line isotope separation.

1990MO15

Nucl.Phys. A514, 1 (1990)

P.Moller, J.Randrup

New Developments in the Calculation of β-Strength Functions

RADIOACTIVITY ^151,152,153Pr, ^{153,154,155,156}Nd, ^153,155,156Pm, ^{158,159,160,157}Sm, ^161,162Eu, ¹⁶⁴Gd; calculated β-decay T_1/2. ¹²⁹Nd, ^93,95,97Rb; calculated β-decay strength functions. Quasiparticle RPA.

doi: 10.1016/0375-9474(90)90330-O

1994SM07

Phys.Rev.Lett. 73, 2540 (1994)

A.G.Smith, W.R.Phillips, J.L.Durell, W.Urban, B.J.Varley, C.J.Pearson, J.A.Shannon, I.Ahmad, C.J.Lister, L.R.Morss, K.L.Nash, C.W.Williams, M.Bentaleb, E.Lubkiewicz, N.Schulz

Lifetimes in Neutron-Rich Nd Isotopes Measured by a Doppler Profile Method

RADIOACTIVITY ²⁴⁸Cm(SF); measured γγ-coin, Doppler-broadened line shapes. ^152,154,156Nd deduced level T_1/2, transition quadrupole moments.

doi: 10.1103/PhysRevLett.73.2540

1998GA12

Eur.Phys.J. A 1, 391 (1998)

C.Gautherin, M.Houry, W.Korten, Y.Le Coz, R.Lucas, X.H.Phan, Ch.Theisen, Ch.Badimon, G.Barreau, T.P.Doan, G.Pedemey, G.Belier, M.Girod, V.Meot, S.Peru, A.Astier, L.Ducroux, M.Meyer, N.Redon

New Isomeric States in ^152,154,156Nd Produced by Spontaneous Fission of ²⁵²Cf

RADIOACTIVITY ²⁵²Cf(SF); measured Eγ, Iγ, γγ-, (fragment)γ-coin, (fragment)γ(t). ^152,154,156Nd, ^156,158Sm deduced levels, J, π, isomeric states T_1/2. Potential energy surface, shell-model calculations.

doi: 10.1007/s100500050074

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

2009SI21

Phys.Rev. C 80, 024304 (2009)

G.S.Simpson, W.Urban, J.Genevey, R.Orlandi, J.A.Pinston, A.Scherillo, A.G.Smith, J.F.Smith, I.Ahmad, J.P.Greene

Two-quasiparticle isomers and bands of ^{154, 156}Nd and ^{156, 158, 160}Sm

NUCLEAR REACTIONS ²³⁹Pu(n, X)¹⁵⁴Nd, E=thermal; measured Eγ, Iγ, γγ-coin, half-lives. ¹⁵⁴Nd; deduced levels, J, π, isomer, bands and configurations. Comparison with QPRM calculations.

RADIOACTIVITY ²⁵²Cf(SF); measured Eγ, Iγ, γγ-coin, half-lives. ¹⁵⁶Nd, ^156,158,160Sm; deduced levels, J, π, isomers, bands and configurations. Comparison with QPRM calculations.

doi: 10.1103/PhysRevC.80.024304

2013YOZZ

CNS-REP-90, Ann.Report 2011, p.34 (2013)

R.Yokoyama, D.Kameda, T.Kubo, N.Inabe, N.Fukuda, H.Takeda, H.Suzuki, K.Yoshida, K.Kusaka, K.Tanaka, Y.Yanagisawa, M.Ohtake, H.Sato, Y.Shimizu, H.Baba, M.Kurokawa, D.Nishimura, T.Ohnishi, N.Iwasa, A.Chiba, T.Yamada, E.Ideguchi, S.Go, T.Fujii, H.Nishibata, K.Ieki, D.Murai, S.Momota, Y.Sato, J.Hwang, S.Kim, O.B.Tarasov, D.J.Morrissey, B.M.Sherrill, G.Simpson

Search for short-lived isomers in neutron-rich Z∼60 nuclei produced by in-flight fission of 345 MeV/nucleon ²³⁸U

NUCLEAR REACTIONS ⁹Be(²³⁸U, X), E=345 MeV/nucleon; measured Eγ, Iγ, other thick target fragmentation products. ^136,154,156Nd deduced delayed γ energy spectra, isomeric transitions. Analysis in progress, especially for other candidates of isomeric transitions. Numbers within figures are totally unreadable because of wrong font conversion.

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