References quoted in the ENSDF dataset: 149SM ADOPTED LEVELS, GAMMAS

140 references found.

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

Return to ADOPTED LEVELS, GAMMAS

1952BO21

Proc.Phys.Soc.(London) 65A, 368 (1952)

G.S.Bogle, H.E.D.Scovil

Nuclear Spins of Samarium 147 and 149

1954MU15

Phys.Rev. 93, 1232 (1954)

K.Murakawa

Hyperfine Structure in the Spectra of Sb, Sm, Hg and Cl

doi: 10.1103/PhysRev.93.1232

1955PE59

Can.J.Phys. 33, 693 (1955)

J.A.Petruska, H.G.Thode, R.H.Tomlinson

The absolute fission yields of twenty-eight mass chains in the thermal neutron fission of U²³⁵

NUCLEAR REACTIONS ²³⁵U(n, F)⁸⁵Rb/⁸⁷Rb/⁸⁶Sr/⁸⁸Sr/⁹⁰Sr/¹⁴³Nd/¹⁴⁴Nd/¹⁴⁵Nd/¹⁴⁶Nd/¹⁴⁸Nd/¹⁵⁰Nd/¹⁴⁷Sm/¹⁴⁹Sm/¹⁵¹Sm/¹⁵²Sm/¹⁵⁴Sm/¹⁴⁰Ce/¹⁴²Ce/¹⁴⁴Ce/⁸³Kr/⁸⁴Kr/⁸⁵Kr/⁸⁶Kr/¹³¹Xe/¹³²Xe/¹³⁴Xe/¹³⁶Xe/¹³³Cs/¹³⁵Cs/¹³⁷Cs, E thermal; measured fission products; deduced absolute and relative fission yields.

doi: 10.1139/p55-085

1956WI48

Can.J.Chem. 34, 227 (1956)

D.M.Wiles, J.A.Petruska, R.H.Tomlinson

Some Cumulative Yields of Isotopes Formed in the Thermal Neutron Fission of Pu²³⁹

NUCLEAR REACTIONS ²³⁹Pu(n, F)¹³³Cs/¹³⁵Cs/¹³⁷Cs/¹⁴⁰Ce/¹⁴²Ce/¹⁴⁴Ce/¹⁴³Nd/¹⁴⁴Nd/¹⁴⁵Nd/¹⁴⁶Nd/¹⁴⁸Nd/¹⁵⁰Nd/¹⁴⁷Sm/¹⁴⁹Sm/¹⁵⁰Sm/¹⁵¹Sm/¹⁵²Sm/¹⁵⁴Sm/¹³¹Xe/¹³²Xe/¹³³Xe/¹³⁴Xe/¹³⁶Xe, E thermal; measured fission products; deduced relative and absolute fission yields.

doi: 10.1139/v56-034

1957IV01

At.Energ. 3, 546 (1957), Soviet J.At.Energy 3, 1436 (1957)

R.N.Ivanov, V.K.Gorshkov, M.P.Anikina, G.M.Kukavadze, B.V.Ershler

Yields of certain heavy fragments in the fission of U²³³

NUCLEAR REACTIONS ²³³U(n, F)¹³³Cs/¹³⁵Cs/¹³⁷Cs/¹⁴⁰Ce/¹⁴²Ce/¹⁴⁴Ce/¹⁴³Nd/¹⁴⁴Nd/¹⁴⁵Nd/¹⁴⁶Nd/¹⁴⁸Nd/¹⁵⁰Nd/¹⁴⁹Sm/¹⁵⁰Sm/¹⁵¹Sm/¹⁵²Sm/¹⁵⁴Sm, E thermal; measured fission products; deduced absolute fission yields.

doi: 10.1007/BF01522511

1957KR57

At.Energ. 2, 334 (1957), Soviet J.At.Energy 2, 334 (1957)

L.M.Krizhansky, Ya.Maly, A.N.Murin, B.K.Preobrazhensky

Rare-earth isotope yields in the fission of Pu²³⁹ by pile neutrons

NUCLEAR REACTIONS ²³⁹Pu(n, F)¹⁴⁰Ce/¹⁴²Ce/¹⁴⁴Ce/¹⁴²Nd/¹⁴³Nd/¹⁴⁴Nd/¹⁴⁵Nd/¹⁴⁶Nd/¹⁴⁸Nd/¹⁵⁰Nd/¹⁴⁷Sm/¹⁴⁹Sm/¹⁵¹Sm/¹⁵²Sm/¹⁵⁴Sm/¹⁴⁸Sm/¹³⁷Cs/¹³⁵Cs/¹³³Cs, E thermal; measured reaction products with a mass-spectrographic analysis; deduced fission yields.

doi: 10.1007/bf01514616

1957KR58

Atomnaya Energ. 2, 276 (1957); J.Nuclear Energy 6A, 260 (1958)

L.M.Krizhanskii, Ya.Maly, A.N.Murin, B.K.Preobrazhenskii

The yields of rare-earth isotopes from the fission of ²³⁹Pu by pile neutrons

NUCLEAR REACTIONS ²³⁹Pu(n, F)¹⁴⁰Ce/¹⁴²Ce/¹⁴⁴Ce/¹⁴²Nd/¹⁴³Nd/¹⁴⁴Nd/¹⁴⁵Nd/¹⁴⁶Nd/¹⁴⁸Nd/¹⁵⁰Nd/¹⁴⁷Sm/¹⁴⁹Sm/¹⁵¹Sm/¹⁵²Sm/¹⁵⁴Sm/¹⁴⁸Sm/¹³⁷Cs/¹³⁵Cs/¹³³Cs, E thermal; measured reaction products with a mass-spectrographic analysis; deduced fission yields.

doi: 10.1016/0891-3919(58)90051-2

1958HU17

J.Chem.Phys. 29, 754 (1958)

C.A.Hutchison, Jr., E.Wong

Paramagnetic Resonance in Rare Earth Trichlorides

1959FI34

Can.J.Phys. 37, 926 (1959); see keynumber 1959FI37

H.R.Fickel, R.H.Tomlinson

The Cumulative Fission Yields, of 21 Heavy Mass Nuclides Produced in the Thermal Fission of Pu²³⁹

NUCLEAR REACTIONS ²³⁹Pu(n, F)¹³³Cs/¹³⁶Cs/¹³⁷Cs/¹⁴³Nd/¹⁴⁴Nd/¹⁴⁵Nd/¹⁴⁶Nd/¹⁴⁸Nd/¹⁵⁰Nd/¹⁴⁰Ce/¹⁴²Ce/¹⁴⁴Ce/¹⁴⁷Sm/¹⁴⁹Sm/¹⁵⁰Sm/¹⁵¹Sm/¹⁵²Sm/¹⁵⁴Sm/¹³⁸Ba, E thermal; measured fission products; deduced fission yields.

doi: 10.1139/p59-103

1959FI37

Can.J.Phys. 37, 926 (1959); see keynumber 1959FI34

H.R.Fickel, R.H.Tomlinson

The cumulative fission yields of 21 heavy mass nuclides produced in the thermal fission of Pu²³⁹

NUCLEAR REACTIONS ²³⁹Pu(n, F)¹³³Cs/¹³⁶Cs/¹³⁷Cs/¹⁴³Nd/¹⁴⁴Nd/¹⁴⁵Nd/¹⁴⁶Nd/¹⁴⁸Nd/¹⁵⁰Nd/¹⁴⁰Ce/¹⁴²Ce/¹⁴⁴Ce/¹⁴⁷Sm/¹⁴⁹Sm/¹⁵⁰Sm/¹⁵¹Sm/¹⁵²Sm/¹⁵⁴Sm/¹³⁸Ba, E thermal; measured reaction products; deduced cumulative fission yields.

doi: 10.1139/p59-103

1960CH15

Proc.Roy.Soc.(London) 259A, 377 (1960)

C.J.S.Chapman, M.A.Grace, J.M.Gregory, C.V.Sowter

The Nuclear Alinement of Promethium Isotopes and the Decay Scheme of ¹⁴⁹Pm

NUCLEAR STRUCTURE ¹⁴⁹Pm; measured not abstracted; deduced nuclear properties.

1960KA23

Ann.Acad.Sci.Fennicae, Ser. A VI, No.65 (1960)

M.Karras

On the Natural Radioactivity of Samarium

NUCLEAR STRUCTURE ¹⁴⁷Sm, ¹⁴⁸Sm, ¹⁴⁶Sm, ¹⁴⁹Sm; measured not abstracted; deduced nuclear properties.

1960MA27

Thesis, Univ.California (1960); UCRL-8740 (1960)

T.V.Marshall

I. Beta-Spectroscopic Studies in the Promethium Region II. The Coriolis Interaction in Deformed Nuclei

NUCLEAR STRUCTURE ¹⁴²Pm, ¹⁴²Sm, ¹⁴⁹Pm; measured not abstracted; deduced nuclear properties.

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

1962AL13

Zh.Eksperim.i. Teor.Fiz. 42, 1036 (1962); Soviet Phys.JETP 15, 718 (1962)

V.P.Alfimenkov, Y.M.Ostanevich, T.Ruskov, A.V.Strelkov, F.L.Shapiro, W.K.Yen

Observation of the Mossbauer Effect in Sm₂¹⁴⁹Os₃

NUCLEAR STRUCTURE ¹⁴⁹Sm; measured not abstracted; deduced nuclear properties.

1962JH04

Phys.Letters 2, 117 (1962)

S.Jha, R.Segnan, G.Lang

On the 22 keV State of Sm¹⁴⁹

NUCLEAR STRUCTURE ¹⁴⁹Sm; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(62)90204-4

1962SP03

Proc.Phys.Soc.(London) 79, 787 (1962)

I.J.Spalding, K.F.Smith

Some Rare Earth Spins, and the Hyperfine Structure of ¹⁷⁶Lu

NUCLEAR STRUCTURE ¹⁴⁹Sm, ¹⁷⁶Lu, ¹⁶¹Dy, ¹⁶³Dy, ¹⁶⁷Er, ^147mSm, ¹⁴⁵Nd, ¹⁴³Nd; measured not abstracted; deduced nuclear properties.

doi: 10.1088/0370-1328/79/4/315

1963KI15

Phys.Rev. 132, 1733 (1963)

O.C.Kistner, A.C.Li, S.Monaro

Lifetimes of the 22-keV First Excited States in Eu¹⁵¹ and Sm¹⁴⁹

NUCLEAR STRUCTURE ¹⁵¹Gd, ¹⁴⁹Eu; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.132.1733

1964FA12

Can.J.Phys. 42, 2063 (1964)

H.Farrar, W.B.Clarke, H.G.Thode, R.H.Tomlinson

Cumulative yields of the heavy fragments in the thermal-neutron fission of ²⁴¹Pu

NUCLEAR REACTIONS ²⁴¹Pu(n, F)¹³¹Xe/¹³²Xe/¹³³Xe/¹³⁴Xe/¹³⁵Xe/¹³⁶Xe/¹³⁸Xe/¹³³Cs/¹³⁵Cs/¹³⁷Cs/¹³⁶Ba/¹³⁸Ba/¹⁴⁰Ba/¹⁴⁰Ce/¹⁴¹Ce/¹⁴²Ce/¹⁴⁴Ce/¹⁴²Nd/¹⁴³Nd/¹⁴⁴Nd/¹⁴⁵Nd/¹⁴⁶Nd/¹⁴⁸Nd/¹⁵⁰Nd/¹⁴⁷Sm/¹⁴⁸Sm/¹⁴⁹Sm/¹⁵⁰Sm/¹⁵¹Sm/¹⁵²Sm/¹⁵⁴Sm/¹³⁷Cs, E thermal; measured fission products with mass spectrometer; deduced fission yields. Comparison with available data.

doi: 10.1139/p64-191

1965CU01

Nucl.Phys. 61, 561 (1965)

W.M.Currie, P.W.Dougan

Levels and Lifetimes in Pm¹⁴⁹ and Sm¹⁴⁹

RADIOACTIVITY ¹⁴⁹Nd[from Nd(n, γ)]; measured Eγ, Iγ, γγ-coin, γγ-delay. ¹⁴⁹Pm[from ¹⁴⁹Nd(β)]; measured βγ-delay. ¹⁴⁹Pm deduced levels, T_1/2. ¹⁴⁹Sm, deduced T_1/2. Natural target.

doi: 10.1016/0029-5582(65)90607-3

1965MA68

Trans.Amer.Nucl.Soc. 8, 10 (1965)

W.J.Maeck, R.M.Abernathy, J.E.Rein

Absolute U-235 Thermal-Fission Yields of Cs-137 and Stable Kr, Xe, Nd, and Sm Isotopes

NUCLEAR REACTIONS ²³⁵U(n, F), E thermal; measured reaction products. ^83,84,85,86Kr, ^131,132,134Xe, ¹³⁷Cs, ^{143,144,145,146,148,150}Nd, ^{147,149,151,152,154}Sm; deduced absolute fission yields.

1966BE39

Izv.Akad.Nauk SSSR, Ser.Fiz. 30, 194 (1966); Bull.Acad.Sci.USSR, Phys.Ser. 30, 201 (1967)

E.E.Berlovich, V.V.Golovin, A.G.Polyakov, M.Khodzhaev, T.Khaidarov

Lifetime of the First Excited State of Sm¹⁴⁹

NUCLEAR STRUCTURE ¹⁴⁹Eu; measured not abstracted; deduced nuclear properties.

1966KA27

Yad.Fiz. 4, 686 (1966); Soviet J. of Nucl.Phys. 4, 486 (1967)

S.P.Kapchigashev, Yu.P.Popov

Determination of level densities and the parameter α from the average capture cross sections

NUCLEAR REACTIONS ⁵¹V(n, n), ⁵¹V(n, γ), Cu(n, n), Cu(n, γ), Ga(n, n), Ga(n, γ), ⁷⁵As(n, n), ⁷⁵As(n, γ), Br(n, n), Br(n, γ), Rb(n, n), Rb(n, γ), ⁸⁹Y(n, n), ⁸⁹Y(n, γ), ⁹⁰Zr(n, n), ⁹⁰Zr(n, γ), ⁹¹Zr(n, n), ⁹¹Zr(n, γ), ⁹²Zr(n, n), ⁹²Zr(n, γ), ⁹⁴Zr(n, n), ⁹⁴Zr(n, γ), ⁹³Nb(n, n), ⁹³Nb(n, γ), ⁹⁵Mo(n, n), ⁹⁵Mo(n, γ), ⁹⁶Mo(n, n), ⁹⁶Mo(n, γ), ⁹⁷Mo(n, n), ⁹⁷Mo(n, γ), ⁹⁸Mo(n, n), ⁹⁸Mo(n, γ), ¹⁰⁰Mo(n, n), ¹⁰⁰Mo(n, γ), ¹⁰³Rh(n, n), ¹⁰³Rh(n, γ), Ag(n, n), Ag(n, γ), ¹¹⁵In(n, n), ¹¹⁵In(n, γ), ¹¹²Sn(n, γ), ¹¹⁶Sn(n, n), ¹¹⁶Sn(n, γ), ¹¹⁷Sn(n, n), ¹¹⁷Sn(n, γ), ¹¹⁹Sn(n, n), ¹¹⁹Sn(n, γ), ¹²²Sn(n, n), ¹²⁴Sn(n, n), ¹²⁴Sn(n, γ), Sb(n, n), Sb(n, γ), ¹²⁷I(n, n), ¹²⁷I(n, γ), ¹³³Cs(n, n), ¹³³Cs(n, γ), ¹³⁹La(n, n), ¹³⁹La(n, γ), ¹⁴¹Pr(n, n), ¹⁴¹Pr(n, γ), ¹⁴⁷Sm(n, n), ¹⁴⁷Sm(n, γ), ¹⁴⁹Sm(n, n), ¹⁴⁹Sm(n, γ), ¹⁵¹Eu(n, n), ¹⁵¹Eu(n, γ), ¹⁵³Eu(n, n), ¹⁵³Eu(n, γ), ¹⁵⁹Tb(n, n), ¹⁵⁹Tb(n, γ), ¹⁶⁵Ho(n, n), ¹⁶⁵Ho(n, γ), ¹⁷⁵Lu(n, n), ¹⁷⁵Lu(n, γ), ¹⁸¹Ta(n, n), ¹⁸¹Ta(n, γ), ¹⁸³W(n, n), ¹⁸³W(n, γ), ¹⁸⁴W(n, n), ¹⁸⁴W(n, γ), ¹⁸⁶W(n, n), ¹⁸⁶W(n, γ), Ir(n, n), Ir(n, γ), ¹⁹⁷Au(n, n), ¹⁹⁷Au(n, γ), ²⁰³Tl(n, n), ²⁰³Tl(n, γ), ²⁰⁵Tl(n, n), ²⁰⁵Tl(n, γ), E=0.0 eV-50 keV; measured products, Eγ, Iγ; deduced resonance parameters. Data were imported from EXFOR entry 40778.

1966MA05

Z.Naturforsch. 21a, 63 (1966)

J.D.Macdougall, W.McLatchie, S.Whineray, H.E.Duckworth

Precise Atomic Mass Differences Involving Isotopes of Nd, Sm, Cd, and Pb

NUCLEAR STRUCTURE ¹⁵²Sm, ¹⁵⁰Nd, ¹⁵⁰Sm, ¹⁵⁴Sm, ¹⁴⁹Sm, ²⁰⁸Pb, ²⁰⁶Pb, ¹¹²Cd, ¹¹⁴Cd, ¹¹⁶Cd, ¹⁴²Nd, ¹⁴⁴Nd, ¹⁴⁸Nd, ¹⁴⁸Sm, ¹⁴⁶Nd, ¹⁴⁵Nd, ¹⁴³Nd, ¹⁴⁷Sm; measured not abstracted; deduced nuclear properties.

1966WO05

Proc.Roy.Soc.(London) 293A, 117 (1966)

G.K.Woodgate

Hyperfine Structure and Nuclear Moments of Samarium

NUCLEAR STRUCTURE ¹⁴⁷Sm, ¹⁴⁹Sm; measured not abstracted; deduced nuclear properties.

1967MA59

Astrophys.J. 149, 577 (1967)

R.L.Macklin, J.H.Gibbons

Quantitative test of s-process in stellar nucleosynthesis for solar system material

NUCLEAR REACTIONS ^{116,117,118,119,120}Sn, ^{144,147,148,149,150,152,154}Sm, ^86,87,88Sr, ^{90,91,92,94,96}Zr, ^{122,123,124,125,126,128,130}Te(n, γ), E=30 keV; measured reaction products, Eγ, Iγ; deduced σ, Maxwellian-averaged σ and their uncertainties.

1967OF01

Nucl.Phys. A93, 689 (1967)

S.Ofer, I.Nowik

Magnetic and Quadrupole Moments of the 22 keV State of ¹⁴⁹Sm

NUCLEAR MOMENTS ¹⁴⁹Sm levels measured a, B; deduced μ, quadrupole moment. Mossbauer absorption, enriched ¹⁴⁹Sm absorber.

doi: 10.1016/0375-9474(67)90315-6

1968AK02

Izv.Akad.Nauk SSSR, Ser.Fiz. 32, 808 (1968); Bull.Acad.Sci.USSR, Phys.Ser. 32, 744 (1969)

F.A.Akilov, E.E.Berlovich, V.V.Lukashevich, V.M.Romanov

Lifetimes of Low-Lying States of ¹³³Cs and ¹⁴⁹Sm

RADIOACTIVITY ¹³³Ba [from ¹³²Ba(n, γ)]; measured γγ-delay. ¹⁴⁹Pm [from ¹⁴⁸Nd(n, γ)¹⁴⁹Nd(β)]; measured βγ-delay. ¹³³Cs, ¹⁴⁹Sm levels deduced T_1/2.

1968DE17

Yadern.Fiz. 8, 255 (1968); Soviet J.Nucl.Phys. 8, 147 (1969)

R.A.Demirkhanov, V.V.Dorokhov, M.I.Dzkuya

Isotope Masses and Nuclear Binding Energies in the Region from Cs to Eu

ATOMIC MASSES ^{130,132,134,135,136,137,138}Ba, ¹³³Cs, ^{136,138,140,142}Ce, ¹⁴¹Pr, ^138,139La, ^{142,143,144,145,146,148,150}Nd, ^151,153Eu, ^{144,147,148,149,150,152,154}Sm; measured masses.

1968KO06

Yadern.Fiz. 8, 227 (1968); Soviet J.Nucl.Phys. 8, 131 (1969)

V.A.Korolev, G.D.Alkhazov, A.A.Vorobev, A.I.Egorov, L.M.Vasileva

Investigation of α-Radioactivity of Sm Isotopes

RADIOACTIVITY ^147,148,149Sm; measured Eα. ^149,148Sm deduced T_1/2.

1968MC23

Phys.Rev. 172, 1160 (1968)

J.A.McHugh, M.C.Michel

Fission-Fragment Mass and Charge Distribution for the Moderately Excited U²³⁶ Compound Nucleus

NUCLEAR REACTIONS ²³²Th, ²³⁵U(α, F)¹⁴²Ce/¹⁴⁴Ce/¹⁴³Nd/¹⁴⁴Nd/¹⁴⁵Nd/¹⁴⁶Nd/¹⁴⁸Nd/¹⁵⁰Nd/¹⁴⁷Sm/¹⁴⁹Sm/¹⁵¹Sm/¹⁵²Sm/¹⁵⁴Sm/⁸³Kr/⁸⁴Kr/⁸⁵Kr/⁸⁶Kr/⁸⁸Sr/⁹⁰Sr/¹³¹Xe/¹³²Xe/¹³⁴Xe/¹³⁶Xe/¹³³Cs/¹³⁵Cs/¹³⁷Cs/¹³⁶Ba/¹³⁸Ba/¹³⁵Cs/¹³⁵I/¹³⁵Xe/⁸⁰Br/⁸²Br/¹²⁶I/¹²⁸I/¹²⁹Xe/⁸¹Kr/⁸⁶Rb¹³²Cs/¹³⁴Cs/¹³⁶Cs/¹⁵⁰Pm/¹³⁰I, E=20-57 MeV; measured fission products. ²³⁶U; deduced relative cumulative yields, fractional chain yields, charge distributions, neutron yields. Comparison with available data.

doi: 10.1103/physrev.172.1160

1968RO16

Can.J.Phys. 46, 2499 (1968)

R.G.H.Robertson, J.C.Waddington, R.G.Summers-Gill

Hyperfine Interactions in the J = 5 States of ¹⁴⁷Sm and ¹⁴⁹Sm

NUCLEAR STRUCTURE ¹⁴⁷Sm, ¹⁴⁹Sm; measured not abstracted; deduced nuclear properties.

1969VA22

Yadern.Fiz. 10, 460 (1969); Soviet J.Nucl.Phys. 10, 263 (1970)

O.V.Vasilev, G.N.Zalesnyi, S.F.Semenko, V.A.Semenov

Giant Resonance in the Region of Transition from Spherical Nuclei to Deformed Ones

NUCLEAR REACTIONS ^148,150Nd, ^150,152,154Sm(γ, n), E < 23 MeV; measured σ(E).

1969VA26

Phys.Letters 30B, 97 (1969)

O.V.Vasilijev, G.N.Zalesny, S.F.Semenko, V.A.Semenov

The Giant Dipole Resonance in the Transition Region from Spherical to Deformed Nuclear Shapes

NUCLEAR REACTIONS ^148,150Nd, ^150,152,154Sm(γ, n), (γ, X), E < 23 MeV; measured σ(E), σ(E;En); deduced giant resonance shapes, α-width.

doi: 10.1016/0370-2693(69)90407-9

1970AN17

Z.Phys. 237, 285 (1970)

S.Antman, H.Pettersson, Z.Zehlev, I.Adam

High Resolution L- and M-Subshell Internal Conversion Studies of Low Energy Transitions in ¹⁴⁹Sm and ¹⁵¹Eu

RADIOACTIVITY ¹⁴⁹Eu, ¹⁵¹Gd; measured I(ce), L-, M-subshell ratios. ¹⁴⁹Sm, ¹⁵¹Eu transitions deduced γ-multipolarity, partial T_1/2, hindrance factors.

1970EIZY

Proc.Int.Conf.Hyperfine Interactions in Excited Nuclei, Rehovot and Jerusalem, Israel (1970), G.Goldring, R.Kalish, Eds., Gordon and Breach, London, Vol.2, p.720 (1971)

M.Eibschutz, R.L.Cohen, J.H.Wernick

Solid State and Nuclear Results in ¹⁴⁹Sm Mossbauer Measurements

NUCLEAR MOMENTS ¹⁴⁹Sm levels measured quadrupole, other moments.

1970GU14

J.Inorg.Nucl.Chem. 32, 3425 (1970)

M.C.Gupta, R.D.MacFarlane

The Natural Alpha Radioactivity of Samarium

RADIOACTIVITY ^147,148Sm; measured Eα, T_1/2; deduced Q. ^146,149Sm; observed no α-activity.

doi: 10.1016/0022-1902(70)80149-X

1970KO30

Acta Phys.Pol. B1, 173 (1970)

J.Kownacki, J.Ludziejewski, M.Moszynski, K.Stryczniewicz

Electromagnetic Transition Probabilities in ¹⁵¹Eu, ¹⁴⁹Sm and ¹⁴⁷Sm Isotopes

RADIOACTIVITY ¹⁵¹Gd; measured Xce-, cece-delay. ¹⁵¹Eu level deduced T_1/2. ¹⁵¹Gd; measured Xγ-delay. ¹⁵¹Eu levels deduced T_1/2. ¹⁴⁹Eu; measured Xce-delay. ¹⁴⁹Sm level deduced T_1/2. ¹⁴⁷Eu; measured ceγ-delay. ¹⁴⁷Sm level deduced T_1/2.

1970MA05

Nucl.Phys. A145, 223 (1970)

J.D.Macdougall, W.McLatchie, S.Whineray, H.E.Duckworth

Precise Atomic Mass Differences and Mass Systematics in the Region of 90 Neutrons

ATOMIC MASSES ¹⁴¹Pr, ^{142,143,144,145,146,148,150}Nd, ^{147,148,149,150,152,154}Sm, ^151,153Eu, ^{154,155,156,157,158,160}Gd; measured mass differences; deduced nucleon pairing, separation energies.

doi: 10.1016/0375-9474(70)90316-7

1971DO19

Int.J.Mass Spectrom.Ion Phys. 6, 435 (1971)

R.Dobrozemsky, F.Pichlmayer, F.P.Viehbock

Massenspektrometrische Bestimmung der Neutronen-Einfangsquerschnitte von Isotopen der Seltenen Erden

NUCLEAR REACTIONS ^147,148Sm, ^154,158Gd, ^{160,161,162,163}Dy, ¹⁶⁶Er, ^{170,171,172,173}Yb(n, γ), E=pile, thermal; measured σ; deduced effective resonance integral.

1971KAZS

JINR-P3-5655 (1971)

E.N.Karzhavina, A.B.Popov

Neutron Resonances of the Samarium Isotopes

NUCLEAR REACTIONS Sm(n, X), (n, γ), E < 500 eV; measured σ(E;Eγ), transmission. ^147,149Sm deduced resonance parameters.

1971LE12

Phys.Lett. 35B, 33 (1971)

P.L.Lee, F.Boehm

X-Ray Isotope Shifts and Nuclear Radii in Sm

NUCLEAR MOMENTS ^{147,148,149,150,152,154}Sm; measured Kα₁ shifts; deduced nuclear radius shifts.

doi: 10.1016/0370-2693(71)90432-1

1972BA08

Can.J.Phys. 50, 34 (1972)

R.C.Barber, R.L.Bishop, J.O.Meredith, F.C.G.Southon, P.Williams, H.E.Duckworth, P.Van Rookhuyzen

Precise Atomic-Mass Differences in the Region 59 < Z < 69

ATOMIC MASSES ^{142,144,146,148,150}Nd, ¹⁵⁰Sm, ^{144,148,150,152,154}Sm, ¹⁵⁴Gd, ^{152,154,156,158,160}Gd, ¹⁶⁰Dy, ^{156,158,160,162,164}Dy, ^{162,164,166,168,170}Er, ¹⁴¹Pr, ^143,145,147Nd, ^147,149Sm, ^151,153Eu, ^155,157Gd, ¹⁵⁹Tb, ^161,163Dy, ¹⁶⁵Ho, ¹⁶⁷Er, ¹⁶⁹Tm, ¹⁶⁷Er; measured mass differences.

1972CH27

Phys.Rev. B5, 3387 (1972)

I.Y.Chan, C.A.Hutchison, Jr.

Electron-Nuclear Double Resonance of Samarium 147 and Samarium 149 Tripositive Ions in Lanthanum Trichloride Single Crystals

NUCLEAR MOMENTS ^147,149Sm; measured μ, quadrupole moment ratios. ENDOR.

doi: 10.1103/PhysRevB.5.3387

1972CH55

Phys.Rev. A6, 2011 (1972)

W.J.Childs, L.S.Goodman

Reanalysis of the Hyperfine Structure of the 4f⁶6s^{2 7}F Multiplet in ^147,149Sm, Including Measurements for the ⁷F₆ State

NUCLEAR MOMENTS ^147,149Sm; measured a, b, g; deduced μ(¹⁴⁷Sm)/μ(¹⁴⁹Sm), quadrupole moment ratio. Atomic beam magnetic resonance.

doi: 10.1103/PhysRevA.6.2011

1972EI05

Phys.Rev. B6, 18 (1972)

M.Eibschutz, R.L.Cohen, E.Buehler, J.H.Wernick

Mossbauer Isomer Shifts in Sm¹⁴⁹ Compounds

NUCLEAR REACTIONS ¹⁴⁹Sm(γ, γ), E=22.5 keV; measured Mossbauer effect in compounds; deduced isomer shift. ¹⁴⁹Sm deduced rms charge radius variation with excitation energy.

doi: 10.1103/PhysRevB.6.18

1973LE16

Phys.Rev. C8, 819 (1973)

P.L.Lee, F.Boehm

X-Ray Isotope Shifts and Variations of Nuclear Charge-Radii in Isotopes of Nd, Sm, Dy, Yb and Pb

NUCLEAR REACTIONS ^{142,143,144,145,146,148,150}Nd, ^{147,148,149,150,152,154}Sm, ^{161,162,163,164}Dy, ^{170,171,172,173,174,176}Yb, ^{204,206,207,208}Pb(γ, X-ray); measured isotope shift. ^{142,143,144,145,146,148,150}Nd, ^{147,148,149,150,152,154}Sm, ^{161,162,163,164}Dy, ^{170,171,172,173,174,176}Yb, ^{204,206,207,208}Pb deduced nuclear charge radii.

doi: 10.1103/PhysRevC.8.819

1974CA12

Nucl.Phys. A225, 171 (1974)

P.Carlos, H.Beil, R.Bergere, A.Lepretre, A.De Miniac, A.Veyssiere

The Giant Dipole Resonance in the Transition Region of the Samarium Isotopes

NUCLEAR REACTIONS ^{144,148,150,152,154}Sm(γ, n), (γ, 2n), E=7-30 MeV; measured σ(E). ^{144,148,150,152,154}Sm resonances deduced thresholds, integrated σ, Lorentz line parameters, intrinsic quadrupole moments. Enriched targets.

doi: 10.1016/0375-9474(74)90373-X

1974PE18

Izv.Akad.Nauk SSSR, Ser.Fiz. 38, 2119 (1974); Bull.Acad.Sci.USSR, Phys.Ser. 38, No.10, 90 (1974)

L.K.Peker, V.M.Sigalov

The Alaga Model and the Structure of the Spherical States of Odd-Neutron Nuclei with A of 145-153

NUCLEAR STRUCTURE ^{143,145,147,149}Nd, ^{145,147,149,151}Sm levels calculated μ.

1974SO04

Nucl.Phys. A224, 411 (1974)

V.G.Soloviev, C.Stoyanov, A.I.Vdovin

Semi-Microscopic Calculation of the Level Density in Spherical Nuclei

NUCLEAR STRUCTURE ^50,51Ti, ^53,54,55Cr, ^55,57,58Fe, ^{59,61,62,63,65}Ni, ^65,67,68,69Zn, ^{71,73,74,75,77}Ge, ^{75,77,78,79,81,83}Se, ^85,87,88,89Sr, ^{91,92,93,95,97}Zr, ^{96,97,98,99,101}Mo, ^100,102Ru, ¹⁰⁶Pd, ^112,113,114Cd, ^{113,115,116,117,118,119,120,121,123,125}Sn, ^{123,124,126,129,131}Te, ^132,136Xe, ^{131,135,136,137,138,139}Ba, ^{137,139,141,143}Ce, ^{143,144,145,146,147,149}Nd, ^145,148,149Sm, ^{195,196,197,199}Pt, ^{199,200,201,202,203}Hg, ^205,207Pb; calculated density of states.

doi: 10.1016/0375-9474(74)90696-4

1974VD01

Yad.Fiz. 19, 516 (1974); Sov.J.Nucl.Phys. 19, 260 (1974)

A.I.Vdovin, V.V.Voronov, L.A.Malov, V.G.Solovev, C.Stoyanov

Mass Number Dependence of the Density of 1/2⁺ States in the Vicinity of the Neutron Binding Energy

NUCLEAR STRUCTURE ¹³⁹Ba, ^141,143Ce, ^{143,145,147,149}Nd, ^145,149,153Sm, ^157,159Gd, ^163,165Dy, ^167,169Er, ^173,175,177Yb, ¹⁷⁹Hf, ¹⁸⁵W, ^199,201,203Hg, ²⁰⁵Pb calculated level density.

1975KA25

Phys.Rev. C12, 1054 (1975)

D.C.Kayser, W.H.Johnson, Jr.

New Mass Measurements of Samarium and Gadolinium and a Mass Table for the Light Rare Earths

ATOMIC MASSES ^152,154Sm; measured atomic mass. ^{141,142,143,144}Pr, ^{142,143,144,145,146,147,148,149,150}Nd, ^{144,145,147,148,149,150,151,152,153,154,155}Sm, ^145,147,149Pm, ^{151,152,153,154,155}Eu, ^{151,152,153,154,155,156,157,158,160}Gd deduced mass excesses.

doi: 10.1103/PhysRevC.12.1054

1975ST15

Phys.Rev. B12, 4653 (1975)

R.L.Streever

Hyperfine Interactions of Sm in SmCo₅

NUCLEAR MOMENTS ^147,149Sm; measured hyperfine field in SmCo₅. NMR.

doi: 10.1103/PhysRevB.12.4653

1976CLZY

Bull.Amer.Phys.Soc. 21, No.4, 658, JF4 (1976)

D.L.Clark, M.E.Cage, G.W.Greenlees

Optical Isotope Shifts and Differences in Nuclear Charge Radii for Nd, Sm, Dy, Er, and Yb

NUCLEAR MOMENTS ^{142,143,144,145,146,148,150}Nd, ^{144,147,148,149,150,152,154}Sm, ^{156,158,160,161,162,163,164}Dy, ^{162,164,166,167,168}Er, ^{168,170,171,172,173,174,176}Yb; measured optical isotope shift, differences in nuclear charge radii. No data.

1976CO14

J.Inorg.Nucl.Chem. 38, 1139 (1976)

J.M.D.Coey

¹⁴⁹Sm³⁺ Isomer Shifts

NUCLEAR REACTIONS ¹⁴⁹Sm(γ, γ); measured Mossbauer effect. ¹⁴⁹Sm deduced isomer shift.

doi: 10.1016/0022-1902(76)80236-9

1977KL04

Nucl.Phys. A283, 189 (1977)

P.Kleinheinz, A.M.Stefanini, M.R.Maier, R.K.Sheline, R.M.Diamond, F.S.Stephens

Different Structure Collective Bands in the N = 87 Nuclei ¹⁴⁹Sm, ¹⁵¹Gd And ¹⁵³Dy

NUCLEAR REACTIONS ¹⁴⁸Nd, ¹⁵⁰Sm, ¹⁵²Gd(α, 3nγ), E=35-45 MeV; measured σ(E, Eγ, θ), γ linear polarization, γγ-coin. ¹⁴⁹Sm, ¹⁵¹Gd, ¹⁵³Dy deduced levels, J, π. Enriched targets.

doi: 10.1016/0375-9474(77)90428-6

1978KO04

Yad.Fiz. 27, 10 (1978); Sov.J.Nucl.Phys. 27, 5 (1978)

V.N.Kononov, B.D.Yurlov, E.D.Poletaev, V.M.Timokhov

Fast-Neutron Capture Cross Sections for Even-Even Isotopes of Neodymium, Samarium, Gadolinium, and Erbium

NUCLEAR REACTIONS ^{142,144,146,148,150}Nd, ^{144,148,150,152,154}Sm, ^156,158,160Gd, ^166,168,170Er(n, γ), E=5-350 keV; measured σ(E).

1979HA19

Nucl.Phys. A321, 71 (1979)

E.Hammaren, E.Liukkonen, M.Piiparinen, J.Kownacki, Z.Sujkowski, T.Lindblad, H.Ryde

Structural Connections between ¹⁴⁸Sm and ¹⁴⁹Sm Nuclei

NUCLEAR REACTIONS ¹⁴⁶Nd(α, 2n), ¹⁴⁸Nd(α, 3n), E=20-37 MeV; ¹⁴⁸Nd(³He, 3n), ¹⁵⁰Nd(³He, 4n), E=19-27 MeV; measured Eγ, Iγ(E), Iγ(θ), γγ-coin, αγ(t), Iγ(t), I(ce), I(ce)(t). ^148,149Sm deduced levels, J, π, T_1/2, ICC. Enriched targets. Ge(Li), Ge intrinsic detectors, solenoidal, double focussing electron spectrometers, Si(Li) detectors.

doi: 10.1016/0375-9474(79)90686-9

1979PO04

Nucl.Phys. A316, 295 (1979)

R.J.Powers, P.Barreau, B.Bihoreau, J.Miller, J.Morgenstern, J.Picard, L.Roussel

A Muonic X-Ray Study of the Charge Distribution of ^{144,148,150,152,154}Sm

ATOMIC PHYSICS, Mesic-Atoms ^{144,148,150,152,154}Sm(μ^-, X-ray); measured E(X-ray), I(X-ray); deduced nuclear charge distribution parameters.

NUCLEAR MOMENTS ^{144,148,150,152,154}Sm; measured muonic X-rays; deduced nuclear charge distribution parameters. ^152,154Sm levels deduced quadrupole moment, isomer shift, B(E2).

doi: 10.1016/0375-9474(79)90039-3

1980BR15

Z.Phys. A296, 281 (1980)

H.Brand, B.Seibert, A.Steudel

Laser-Atomic-Beam Spectroscopy in Sm: Isotope Shifts and Changes in Mean-Square Nuclear Charge Radii

NUCLEAR MOMENTS ^{144,147,148,149,150,152,154}Sm; measured optical isotope shift, hfs; deduced rms charge radii. Laser atomic beam spectroscopy.

1981BA28

Nucl.Phys. A364, 446 (1981)

P.Barreau, L.Roussel, R.J.Powers

A Muonic X-Ray Study of the Charge Distribution of ¹⁴⁷Sm and ¹⁴⁹Sm

ATOMIC PHYSICS, Mesic-Atoms ^147,149Sm; measured E(X-ray), I(X-ray); deduced charge parameters, rms radius. Model independent analysis.

NUCLEAR MOMENTS ^147,149Sm; measured muonic X-rays, hfs. ^147,149Sm deduced spectroscopic quadrupole moments, B(E2), isotope shifts, charge parameters, rms radius. Model independent analysis.

doi: 10.1016/0375-9474(81)90581-9

1982BA15

Izv.Akad.Nauk SSSR, Ser.Fiz. 46, 63 (1982)

I.F.Barchuk, V.I.Golyshkin, E.N.Gorban

γ-Quanta from the Reactions ^148,152,154Sm(n, γ)^149,153,155Sm using Thermal Neutrons

NUCLEAR REACTIONS ^148,152,154Sm(n, γ), E=thermal; measured Eγ, Iγ. ^149,153,155Sm deduced levels.

1982FI02

Nucl.Phys. A377, 217 (1982)

C.A.Fields, F.W.N.De Boer, R.A.Ristinen, P.A.Smith, E.Sugarbaker

A Systematic Investigation of the (α, 2nγ) Reaction on Medium-Heavy Nuclei

NUCLEAR REACTIONS ⁸⁵Rb, ⁸⁹Y, ⁹⁰Zr, ^{104,106,108,110}Pd, ¹³⁹La, ¹⁶⁵Ho, ¹⁴⁸Nd, ¹⁹⁷Au, ^{112,118,120,124}Sn, ²⁰⁸Pb(α, 2n), E=35 MeV; ¹¹⁰Pd, ¹⁴⁸Nd(α, 2n), E=28, 32 MeV; ¹¹⁰Pd, ^118,120,124Sn, ¹⁴⁸Nd, ¹⁹⁷Au(α, 3n), E=35 MeV; ¹⁰⁸Pd(α, 2n), ¹⁴⁸Nd(α, 3n), E=32 MeV; measured nγ-coin, Iγ, σ(θn), σ(En); deduced neutron decay mechanism, spectrum parameters, entry state spins. Ge(Li), hyperpure Ge and NE224 detectors.

doi: 10.1016/0375-9474(82)90330-X

1982ME10

J.Phys.(London) G8, 1413 (1982)

R.A.Meyer, J.W.T.Meadows, E.S.Macias

Opposing Properties of Particle-Hole and Intruder-Hole Bands in N = 87 Nuclei and ¹⁴⁹Sm Levels Populated by ¹⁴⁹Pm(β^-) and ¹⁴⁹Eu(EC)

RADIOACTIVITY ¹⁴⁹Eu(EC) [from Sm(p, xn), ¹⁴⁹Sm(α, 4n)¹⁴⁹Gd(EC-decay)]; ¹⁴⁹Pm(β^-) [from ¹⁴⁸Nd(n, γ)¹⁴⁹Nd(β-decay)]; measured Eγ, Iγ, γγ-coin, I(ce). ¹⁴⁹Sm deduced levels, ICC, γ-multipolarity, band structure, configuration. Compton suppression, Ge(Li), Si detectors.

doi: 10.1088/0305-4616/8/10/012

1983GA07

Nucl.Phys. A398, 19 (1983)

S.Gales, G.M.Crawley, D.Weber, B.Zwieglinski

Neutron-Hole Strength Distributions in Heavy Nuclei (II). The ^144,148,152Sm(³He, α)^143,147,151Sm and the ^{144,148,150,152,154}Sm(p, d)^{143,147,149,151,153}Sm Reactions

NUCLEAR REACTIONS ^144,148,152Sm(³He, α), E=70 MeV; measured σ(Eα, θ); ^{144,148,150,152,154}Sm(p, d), E=42 MeV; measured σ(Ed, θ). ^{143,147,149,151,153}Sm deduced levels, L, J, π, C²S. Enriched target, magnetic spectrometer. Zero-range, finite-range DWBA calculations, inner-shells analysis. Comparison with the quasiparticle phonon, Nilsson models.

doi: 10.1016/0375-9474(83)90646-2

1983MA71

Nucl.Phys. A411, 125 (1983)

K.Maki-Kuutti, E.Hammaren

A Quasiparticle-Rotor Model with Variable Moments of Inertia: Application to ^149,151,153Sm and ¹⁰⁹Pd

NUCLEAR STRUCTURE ^149,151,153Sm, ¹⁰⁹Pd; calculated levels, rotational level characteristics. Quasiparticle-rotor model, variable moments of inertia.

doi: 10.1016/0375-9474(83)90511-0

1983ST17

Hyperfine Interactions 13, 221 (1983)

J.G.Stevens

Isomer Shift Reference Scales

COMPILATION ⁵⁷Fe, ⁹⁹Ru, ¹²¹Sb, ^127,129I, ¹⁴⁹Sm, ^151,153Eu, ¹⁵⁵Gd, ¹⁶¹Dy, ¹⁷⁰Yb, ¹⁸¹Ta, ¹⁹³Ir, ¹⁹⁷Au, ²³⁷Np, ¹¹⁹Sn, ¹²⁵Te; compiled, evaluated relative isomer shift values from Mossbauer spectra.

1984AL30

Izv.Akad.Nauk SSSR, Ser.Fiz. 48, 875 (1984)

B.A.Alikov, K.Zuber, V.V.Pashkevich, E.G.Tsoi

Equilibrium Deformations of Single-Particle States of Odd Nuclei in the Rare Earth Region

NUCLEAR STRUCTURE ^{147,149,151,153,155,157,159,161}Eu, ^{153,155,157,159,161,163,165,167,169,171,173}Ho, ^{155,157,159,161,163,165,167,169,171,173}Tm, ^{149,151,153,155,157,159,161}Sm, ^{151,153,155,157,159,161,163}Gd, ^{155,157,159,161,163,165,167,169,171,173}Er, ^{157,159,161,163,165,167,169,171,173}Yb; calculated quadrupole, hexadecapole moments, ground state energies. ¹⁵¹Pm, ^{155,157,161,163,165}Dy, ^175,177Lu, ¹⁵⁷Tb; calculated quadrupole moments. ¹⁶⁵Er, ¹⁶⁵Tm; calculated hexadecapole moment level dependence.

1984AL35

Pisma Zh.Eksp.Teor.Fiz. 40, 483 (1984); JETP Lett.(USSR) 40, 1317 (1984)

G.D.Alkhazov, E.E.Berlovich, H.Wagner, K.Dorschel, V.N.Panteleev, E.W.Peau, A.G.Polyakov, V.I.Tikhonov, W.Heddrich, H.Huhnermann

Static and Dynamic Deformation of the Nuclei of Europium and Samarium Isotopes in the Transition Region

NUCLEAR MOMENTS ^151,153Eu; ^147,149Sm; measured hfs, isotope shifts. ^151,153Eu, ^147,149Sm deduced rms charge radii isotope dependence, static, dynamic deformation differences.

RADIOACTIVITY ^{145,147,149,155}Eu; ^{145,151,153,155}Sm; measured hfs, isotope shifts. ^{145,147,149,155}Eu, ^{145,151,153,155}Sm deduced rms charge radii isotope dependence, static, dynamic deformation differences.

1984EA02

J.Phys.(London) G10, L271 (1984)

D.A.Eastham, J.G.England, D.E.Evans, M.J.Fawcett, I.S.Grant, J.A.R.Griffith, G.W.A.Newton, P.M.Walker

Optical Isotope Shift and Hyperfine Structure of ¹⁵³Sm

RADIOACTIVITY ¹⁵³Sm(β^-) [from ¹⁵²Sm neutron irradiation]; measured optical isotope shift, hfs. ^{146,147,148,149,150,151,152,153,154}Sm deduced rms charge radii relative to ¹⁴⁴Sm.

doi: 10.1088/0305-4616/10/12/002

1984MA21

Yad.Fiz. 39, 341 (1984)

V.S.Masterov, N.S.Rabotnov

Influence of the Quantum Number K on Statistical Distribution of Reduced Neutron Widths

NUCLEAR STRUCTURE ^147,149Sm, ^151,153Eu, ^155,157Gd, ¹⁵⁹Tb, ^161,163Dy, ¹⁶⁵Ho, ¹⁶⁷Er, ¹⁶⁹Tm, ^171,173Yb, ^177,179Hf, ¹⁸¹Ta, ¹⁸³W, ^185,187Re, ^233,235U, ²³⁷Np, ^239,241Pu; analyzed reduced neutron width distribution data; deduced K quantum number role.

1985AL06

Izv.Akad.Nauk SSSR, Ser.Fiz. 49, 24 (1985); Bull.Acad.Sci.USSR, Phys.Ser. 49, No.1, 25 (1985)

G.D.Alkhazov, A.A.Akhmonen, E.E.Berlovich, Yu.S.Blinnikov, W.Wagner, V.P.Denisov, K.Dorschel, V.N.Panteleev, E.V.Peau, A.G.Polyakov, Yu.Ya.Sergeev, V.I.Tikhonov, M.M.Trukhin, W.Heddrich, H.Huhnermann

Laser-Spectroscopic Investigation of Nuclear Charge Radii and Electromagnetic Moments of the Transition Region Europium and Samarium Isotopes

NUCLEAR MOMENTS ^{144,146,147,148,149,150,151,152,154}Sm, ^{147,149,151,152,153,154,155,156}Eu; measured isotope shifts; deduced μ, quadrupole moments, rms charge radii. Laser spectroscopy.

1986AL33

Yad.Fiz. 44, 1134 (1986); Sov.J.Nucl.Phys 44, No.5, 734 (1986)

G.D.Alkhasov, E.E.Berlovich, H.Wagner, K.Dorschel, V.N.Panteleev, E.V.Peau, A.G.Polyakov, V.I.Tikhonov, W.Heddrich, H.Huhnermann

Shape of Nuclei of Eu and Sm Isotopes in the Transition Region with N = 84-92

RADIOACTIVITY ^{147,149,152,152m,154,155,156}Eu, ¹⁵¹Sm; measured hfs, isotope shifts; deduced charge radii, quadrupole, magnetic moments, deformation parameters. Laser spectroscopy.

NUCLEAR MOMENTS ^151,153Eu, ¹⁴⁶Sm; measured hfs, isotope shifts; deduced charge radii, quadrupole, magnetic moments, deformation parameters. Laser spectroscopy.

1986BE28

Phys.Lett. 177B, 260 (1986)

E.E.Berlovich, F.F.Karpeshin

On the Nature of the Phase Transition in Nuclei with Neutron Number N = 88-90

NUCLEAR STRUCTURE ^{147,149,151,153,155}Eu, ^{147,149,151,153,155}Sm; calculated intrinsic quadrupole moments. Mottelson-Nilsson method without pairing mode.

doi: 10.1016/0370-2693(86)90749-5

1986WI02

Astrophys.J. 300, 41 (1986)

R.R.Winters, F.Kappeler, K.Wisshak, A.Mengoni, G.Reffo

^148,150Sm: A test for s-process nucleosynthesis

NUCLEAR REACTIONS ^148,149,150Sm(n, γ), E=4-250 keV; measured σ(E); deduced Maxwellian < σ >, parameters, s-process neutron density. ^148,150Sm deduced s-process current ratio.

doi: 10.1086/163781

1987BO58

Zh.Eksp.Teor.Fiz. 93, 1545 (1987)

S.K.Borisov, Yu.P.Gangrsky, C.Hradecny, S.G.Zemlyanoi, B.B.Krynetsky, K.P.Marinova, B.N.Markov, V.A.Mishin, Yu.Ts.Oganesian, O.M.Stelmakh, Hoang Thi Kim Hue, Tran Cong Tam

Measurement of Mean-Square Nuclear Radii of Nd, Sm and Gd by Laser Excited Fluorescence

NUCLEAR MOMENTS ^{149,146,147,152,154,150,144,148}Sm, ^{142,144,146,150,148}Nd, ^{152,154,156,158,160,155,157}Gd; measured optical isotope shifts; deduced rms radii differences. Laser excited fluorescence.

1987VA22

Phys.Lett. 194B, 334 (1987)

A.M.Van den Berg, K.E.Rehm, D.G.Kovar, W.Kutschera, G.S.F.Stephans

Systematics of Quasi-Elastic Neutron Transfer Cross Sections for Heavy-Ion Induced Reactions

NUCLEAR REACTIONS ^144,149,154Sm(⁵⁸Ni, ⁵⁸Ni), (⁵⁸Ni, ⁵⁸Ni'), (⁵⁸Ni, ⁵⁷Ni), (⁵⁸Ni, ⁵⁹Ni), (⁵⁸Ni, ⁶⁰Ni), E=245 MeV; measured σ, σ(θ); deduced target mass dependence, quasielastic transfer systematics. Enriched targets. DWBA calculations.

doi: 10.1016/0370-2693(87)91060-4

1987YO05

Phys.Rev. A36, 2148 (1987)

L.Young, W.J.Childs, H.G.Berry, C.Kurtz, T.Dinneen

Hyperfine Structure of ^147,149Sm II by Collinear Laser-Ion-Beam Spectroscopy

NUCLEAR MOMENTS ^147,149Sm; measured hfs; deduced hyperfine constants. Collinear laser-ion beam spectroscopy.

doi: 10.1103/PhysRevA.36.2148

1988AL13

Phys.Rev. C37, 1667 (1988)

B.Al-Bataina, J.Janecke

Reduced Alpha Widths for Nuclei with N ≥ 84, Z ≤ 84

NUCLEAR STRUCTURE Z=60-84; analyzed α-decay width data. ¹⁴²Ce, ¹⁴⁹Sm, ¹⁵⁶Dy, ^162,164Er, ¹⁶⁸Yb, ^176,174Hf, ¹⁸⁰W, ^184,186,188Os, ¹⁹²Pt, ¹⁹⁶Hg, ²⁰⁴Pb; calculated α-decay T_1/2.

doi: 10.1103/PhysRevC.37.1667

1990EN01

J.Phys.(London) G16, 105 (1990)

J.G.England, I.S.Grant, J.A.R.Griffith, D.E.Evans, D.A.Eastham, G.W.A.Newton, P.M.Walker

Isotope Shifts and Hyperfine Splittings in ^144-154Sm I

RADIOACTIVITY ^{145,151,153,146}Sm; measured isotope shifts, hfs; deduced hfs constants, rms radii differences, μ, Q. Other data input.

NUCLEAR MOMENTS ^{144,147,148,149,150,152,154}Sm; measured isotope shifts, hfs; deduced hfs constants, rms radii differences, μ, Q. Other data input.

NUCLEAR STRUCTURE ^{145,147,149,151,153}Sm; calculated μ, quadrupole moment.

doi: 10.1088/0954-3899/16/1/014

1990LY01

At.Data Nucl.Data Tables 44, 191 (1990)

J.E.Lynn, P.A.Seeger

Resonance Effects in Neutron Scattering Lengths of Rare-Earth Nuclides

NUCLEAR REACTIONS Sm, Eu, Gd, Er, Yb, ¹⁴⁹Sm, ¹⁵¹Eu, ^155,157Gd, ¹⁶⁴Dy, ¹⁶⁷Er, ^168,174Yb, ¹⁷⁶Lu(n, n), E=0.01-0.5 eV; analyzed data; deduced coherent scattering lengths. Generalized single-level formalism.

doi: 10.1016/0092-640X(90)90013-A

1990URZR

KVI 1989 Ann.Rept., p.30 (1990)

W.Urban, J.C.Bacelar, W.Gast, G.Hebbinghaus, A.Kramer-Flecken, R.M.Lieder, T.Rzaca-Urban, M.Thoms

High-Spin Parity Doublets in the ¹⁴⁹Sm Nucleus

NUCLEAR STRUCTURE ¹⁴⁹Sm; analyzed data; deduced levels, J, π, configuration.

1990URZX

JUL-Spez-562, p.60 (1990)

W.Urban, W.Gast, G.Hebbinghaus, A.Kramer-Flecken, R.M.Lieder, T.Rzaca-Urban, M.Thoms

High-Spin Parity Doublets in ¹⁴⁹Sm

NUCLEAR STRUCTURE ¹⁴⁹Sm; analyzed data; deduced levels, J, π.

1990WA25

J.Phys.Soc.Jpn. 59, 2700 (1990)

M.Wakasugi, T.Horiguchi, W.G.Jin, H.Sakata, Y.Yoshizawa

Changes of the Nuclear Charge Distribution of Nd, Sm, Gd and Dy from Optical Isotope Shifts

NUCLEAR MOMENTS ^{142,144,146,148,150,143,145}Nd, ^{144,148,150,152,154,147,149}Sm, ^{152,154,156,158,160,155,157}Gd, ^{156,158,160,162,164,161,163}Dy; measured isotope shifts, hfs; deduced rms charge radii changes, nuclear parameter. Atomic beam laser spectroscopy.

1991NA14

Nucl.Phys. A533, 223 (1991)

P.Navratil, J.Dobes

Similarity-Transformed Dyson Mapping and SDG-Interacting Boson Hamiltonian

NUCLEAR STRUCTURE ^{144,145,146,148,149,150,151,152,153,154}Sm, ¹⁵⁰Nd, ¹⁹⁶Pt; calculated levels, B(λ). sdg-interacting boson hamiltonian.

doi: 10.1016/0375-9474(91)90488-R

1992LE09

J.Phys.(London) G18, 1177 (1992)

V.S.Letokhov, V.I.Mishin, S.K.Sekatsky, V.N.Fedoseyev, G.D.Alkhazov, A.E.Barzakh, V.P.Denisov, V.E.Starodubsky

Laser Spectroscopic Studies of Nuclei with Neutron Number N < 82 (Eu, Sm and Nd Isotopes)

RADIOACTIVITY ^{135,137,139,141}Nd, ^{139,141,141m,143,145}Sm; measured hfs; deduced parameters a, b, quadrupole moments. ^{132,134,135,136,137,138,139,140,141}Nd, ^{138,139,140,141,141m,142,143,145}Sm, ^{138,139,140,141,142,143,144,145}Eu; measured isotope shifts; deduced mean square charge radii. Resonance ionization spectroscopy.

NUCLEAR MOMENTS ¹⁴²Nd, ¹⁴⁴Sm; measured isotope shifts; deduced mean square charge radii. Resonance ionization spectroscopy.

doi: 10.1088/0954-3899/18/7/008

1993GE07

Nucl.Phys. A565, 643 (1993)

G.Georgiev, Yu.S.Zamyatnin, L.B.Pikelner, G.V.Muradian, Yu.V.Grigorev, T.Madjarski, N.Janeva

Determination of ¹⁴⁷Sm and ¹⁴⁸Sm Resonance Parameters

NUCLEAR REACTIONS ^147,148Sm(n, γ), E=15-4000 eV; measured σ(n, γ), σ(n, n'), for capture, neutron scattering. ^148,149Sm deduced resonances, Γγ, Γ(n), J. Multisectional scintillation detector, IBR-30 pulse booster.

doi: 10.1016/0375-9474(93)90050-8

1993WI12

Phys.Rev. C48, 1401 (1993)

K.Wisshak, K.Guber, F.Voss, F.Kappeler, G.Reffo

Neutron Capture in ^148,150Sm: A sensitive probe of the s-process neutron density

NUCLEAR REACTIONS ^{147,148,149,150,152}Sm(n, γ), E=3-225 keV; measured σ(E); deduced stellar cross sections at kT=10-100 keV, s-process neutron density.

doi: 10.1103/PhysRevC.48.1401

1994BA01

Phys.Rev. C49, 650 (1994)

S.Basu, J.M.Chatterjee, D.Banik, R.K.Chattopadhyay, R.P.Sharma, S.K.Pardhasaradhi

Octupole Deformation in ^149,151Sm Nuclei

NUCLEAR REACTIONS ^148,150Nd(α, 3nγ), E=35, 37 MeV; measured Eγ, Iγ, γγ-coin. ^149,151Sm deduced levels, J, π, B(E1)/B(E2) ratios, shape features, average electric dipole moment, band structure. Cranked shell model.

doi: 10.1103/PhysRevC.49.650

1994JI08

Phys.Rev. A49, 4398 (1994)

W.G.Jin, T.Horiguchi, W.Yang, I.Endo

J Dependences of the Isotope Shift and Hyperfine Structure in the Sm I 4f⁶5d6s ⁹H Term

NUCLEAR MOMENTS ^{144,148,150,152,154,147,149}Sm; measured isotope shifts, hfs; deduced hyperfine parameters for ^147,149Sm.

doi: 10.1103/PhysRevA.49.4398

1995TO01

Phys.Rev. C51, 1540 (1995)

K.A.Toukan, K.Debus, F.Kappeler, G.Reffo

Stellar Neutron Capture Cross Sections of Nd, Pm, and Sm Isotopes

NUCLEAR REACTIONS ^146,148,150Nd(n, γ), E=25, 30 keV; measured Eγ, Iγ; deduced stellar capture σ(E), s-, r-, p-process abundances from ¹⁴²Nd-¹⁵⁰Sm. ¹⁴⁷Nd, ^147,148,149Pm, ^{147,148,149,150,151}Sm(n, γ), E=1-600 keV; ^146,147,148Nd, ^147,148,149Pm, ¹⁵¹Sm(n, γ), E=12-52 keV; calculated σ(E). ¹⁴⁸Nd, ^{147,148,149,150}Pm, ^{147,148,149,150,151,152,153}Sm deduced level density parameters, Γγ.

doi: 10.1103/PhysRevC.51.1540

1997KO33

Z.Phys. D39, 209 (1997)

T.Kobayashi, I.Endo, A.Fukumi, T.Horiguchi, Y.Ishida, T.Kondo, T.Kuwamoto, N.Minamoto, T.Nakamura, T.Takahashi

Measurement of Hyperfine Structure Constants, g Values and Tensor Polarizability of Excited States of Sm I

NUCLEAR MOMENTS ^{144,147,148,149,150,152,154}Sm; measured hfs, Zeeman spectra; deduced hfs constants.

1999DU16

J.Nucl.Sci.Technol.(Tokyo) 36, 865 (1999)

B.Duamet, M.Igashira, M.Mizumachi, S.Mizuno, J.-I.Hori, K.Masuda, T.Ohsaki

Measurement of keV-Neutron Capture Cross Sections and Capture Gamma-Ray Spectra of ^{147, 148, 149, 150, 152, 154}Sm

NUCLEAR REACTIONS ^{147,148,149,150,152,154}Sm(n, γ), E=10-90, 550 keV; measured Eγ, Iγ, capture σ. Comparison with previous results.

1999KU26

J.Phys.Soc.Jpn. 68, 1877 (1999)

T.Kuwamoto, I.Endo, A.Fukumi, T.Horiguchi, M.Iinuma, Y.Ishida, T.Kondo, H.Matsuzaki, T.Takahashi

Hyperfine Constants and Tensor Polarizabilities of 4f⁶6s6p⁹G_0-6 States in Sm I

NUCLEAR MOMENTS ^147,149Sm; measured hfs, isotope shifts. Atomic-beam laser spectroscopy.

2000KI15

J.Phys.Soc.Jpn. 69, 683 (2000)

S.Kitao, T.Mitsui, M.Seto

Nuclear Resonant Scattering of Synchrotron Radiation by ¹²¹Sb and ¹⁴⁹Sm

NUCLEAR REACTIONS ¹²¹Sb(γ, γ'), E=22.5 keV; ¹⁴⁹Sm(γ, γ'), E=37.1 keV; measured X-ray spectra following internal conversion. ¹²¹Sb, ¹⁴⁹Sm levels deduced T_1/2. Nuclear resonant scattering, synchrotron radiation.

2000RO32

Pisma Zh.Eksp.Teor.Fiz. 72, 337 (2000); JETP Lett. 72, 229 (2000)

P.I.Romasheva

Retarded Decays of Low-Lying (∼ 30 keV) Mossbauer Levels as a Result of Their Combined Structure

NUCLEAR STRUCTURE ⁵⁷Fe, ⁶⁹Ga, ⁷³Ge, ⁸³Kr, ⁹³Nb, ⁹⁷Ru, ^107,109Ag, ¹¹²In, ¹¹⁹Sn, ¹²⁹I, ¹³³Ba, ¹⁴⁹Sm, ¹⁵¹Eu, ¹⁶¹Dy, ¹⁶⁹Tm, ¹⁹¹Ir, ²²⁵Fr, ²⁴³Am; calculated Mossbauer levels configurations, T_1/2, ICC.

doi: 10.1134/1.1324016

2003GU12

Phys.Rev. C 68, 034311 (2003)

M.Guttormsen, R.Chankova, M.Hjorth-Jensen, J.Rekstad, S.Siem, A.Schiller, D.J.Dean

Free energy and criticality in the nucleon pair breaking process

NUCLEAR STRUCTURE ^171,172Yb, ^166,167Er, ^161,162Dy, ^148,149Sm; analyzed level densities; deduced Helmholtz free energy, other thermodynamic quantities, continuous nucleon pair breaking.

doi: 10.1103/PhysRevC.68.034311

2003KA23

Yad.Fiz. 66, 837 (2003); Phys.Atomic Nuclei 66, 804 (2003)

M.Kaczmarczyk

The Analysis of the Densities of s-Wave Neutron Resonances Separated with Respect to Spin

NUCLEAR STRUCTURE ⁴⁵Sc, ⁵¹V, ⁵⁵Mn, ⁵⁹Co, ^63,65Cu, ⁶⁷Zn, ⁸⁹Y, ^147,149Sm, ^155,157Gd, ¹⁵⁹Tb, ¹⁶³Dy, ¹⁶⁵Ho, ¹⁶⁷Er, ^177,179Hf, ¹⁹⁷Au, ²³⁵U, ²³⁷Np, ²³⁹Pu; analyzed neutron resonance level densities vs spin. Gilbert-Cameron formula.

doi: 10.1134/1.1576453

2003PA30

J.Korean Phys.Soc. 43, 336 (2003)

H.Park, M.Lee, Y.Rhee

Hyperfine Structure of ^{147, 149}Sm Measured Using Saturated Absorption Spectroscopy in Combination with Resonance-Ionization Mass Spectroscopy

NUCLEAR MOMENTS ^147,149Sm; measured hfs; deduced hyperfine constants. Saturated absorption spectroscopy.

2003RE39

Astrophys.J. 582, 1251 (2003)

R.Reifarth, C.Arlandini, M.Heil, F.Kappeler, P.V.Sedyshev, A.Mengoni, M.Herman, T.Rauscher, R.Gallino, C.Travaglio

Stellar Neutron Capture on Promethium: Implications for the s-Process Neutron Density

NUCLEAR REACTIONS ¹⁴⁷Pm(n, γ), E=25 keV; measured reaction products, Eγ, Iγ; deduced Maxwellian-averaged σ and its uncertainties.

NUCLEAR REACTIONS ^147,148,149Pm(n, γ), E=5-100 keV; calculated Maxwellian-averaged σ.

COMPILATION ^146,147,148Nd, ^147,148,149Pm, ^{147,148,149,150}Sm(n, γ), E=10, 25, 30 keV; compiled Maxwellian-averaged σ and its uncertainties.

doi: 10.1086/344718

2004XU02

Phys.Rev. C 69, 024614 (2004)

C.Xu, Z.Ren

α decay of nuclei in extreme cases

RADIOACTIVITY ¹⁴⁵Nd, ¹⁴⁹Sm, ¹⁵⁶Dy, ¹⁶²Er, ¹⁷⁸Yb, ^176,178Hf, ^180,182W, ^161,162,162mRe, ¹⁸⁸Os, ^166,167,192Pt, ¹⁷²Au, ^174,196Hg, ^177,177m,180Tl, ¹⁸⁰Pb, ¹⁸⁵Bi, ^188,189,190Po, ^{261,263,265,266}Sg, ^264,266,267Bh, ^{264,265,266,267,269}Hs, ²⁶⁸Mt, ^{269,270,271,273,281}Ds, ²⁷²Rg, ^277,284,285Cn, ^287,288,289Fl, ^290,292Lv, ²⁹⁴Og(α); calculated α-decay T_1/2. Cluster model, comparisons with data.

doi: 10.1103/PhysRevC.69.024614

2005CA27

Phys.Rev. C 71, 064320 (2005)

R.Capote, A.Ventura, F.Cannata, J.M.Quesada

Level densities of transitional Sm nuclei

NUCLEAR STRUCTURE ^{148,149,150,152}Sm; calculated level densities, resonance spacing. Interacting boson model, comparison with data.

doi: 10.1103/PhysRevC.71.064320

2010DA13

Nucl.Instrum.Methods Phys.Res. B268, 114 (2010)

D.Dashdorj, G.E.Mitchell, T.Kawano, M.Devlin, N.Fotiades, R.O.Nelson, J.A.Becker, C.Y.Wu, P.E.Garrett, S.Kuneida

(n, 2n) and (n, 3n) cross-sections of neutron-induced reactions on ¹⁵⁰Sm for E_n=1-35 MeV

NUCLEAR REACTIONS ¹⁵⁰Sm(n, 2n), (n, 3n), (n, 2nγ), (n, 3nγ), E<35 MeV; measured TOF, Eγ, Iγ; deduced σ. Comparison with FKK GNASH calculations.

doi: 10.1016/j.nimb.2009.10.189

2011IN01

Eur.Phys.J. A 47, 64 (2011)

A.Kh.Inoyatov, D.V.Filosofov, V.M.Gorozhankin, A.Kovahik, I.Adam, L.L.Perevoshchikov, M.Rysavy

Improved characteristics of the 22.5 keV (M1 + E2) nuclear transition in ¹⁴⁹Sm

RADIOACTIVITY ^{145,146,147,148,149}Eu(EC)[from Eu+p at E=500 MeV]; measured E(CE), I(CE), Eγ, Iγ; deduced intensity ratios, transition strengths, γ-multipolarity.

doi: 10.1140/epja/i2011-11064-9

2011QI12

Phys.Rev. C 84, 064307 (2011)

Y.Qian, Z.Ren

Systematic study of new data for extreme α decays

RADIOACTIVITY ¹⁰⁹I, ^112,113Cs, ¹⁴²Ce, ^{146,147,148,149}Sm, ¹⁵¹Eu, ¹⁵²Gd, ¹⁵⁶Dy, ^162,164Er, ¹⁶⁸Yb, ^174,176Hf, ¹⁸⁰W, ¹⁵⁹Re, ^161,184,188Os, ^167,169Ir, ^172,190,192Pt, ^172,175,177Au, ^176,196Hg, ^179,181Tl, ^{179,180,181,204}Pb, ¹⁸⁷Bi, ¹⁸⁷Po, ²³⁸U, ²⁴⁴Pu, ^233,236Cm, ²³⁷Cf, ²⁴⁹Md, ²⁵³Lr, ²⁵⁷Db, ^{260,265,267,282}Sg, ^261,262,274Bh, ^263,265Hs, ²⁷⁸Mt, ²⁸¹Ds, ²⁸⁵Cn, ^285,286Nh, ^288,289Fl, ^289,290Mc, ^293,294Ts(α); calculated half-lives using Modified two-potential approach (MTPA) for deformed nuclei associated with the density-dependent cluster model. Comparison with experimental data.

doi: 10.1103/PhysRevC.84.064307

2012GU16

Phys.Rev. C 86, 024313 (2012)

X.Guan, K.D.Launey, M.-x.Xie, L.Bao, F.Pan, J.P.Draayer

Heine-Stieltjes correspondence and the polynomial approach to the standard pairing problem

NUCLEAR STRUCTURE ^{42,43,44,45,46,47,48,49}Ca, ^{58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74,75,76,77}Ni, ^{146,147,148,149,150,151,152,153}Sm; calculated pairing gaps. ¹¹⁰Sn; calculated relevant polynomials and the corresponding eigen-energies. Solution of the Bethe ansatz (Gaudin-Richardson) equations based on Heine-Stieltjes polynomials. Comparison with BCS (pairing) calculations and experimental data.

doi: 10.1103/PhysRevC.86.024313

2012HI11

Phys.Rev. C 86, 064317 (2012)

S.Hilaire, M.Girod, S.Goriely, A.J.Koning

Temperature-dependent combinatorial level densities with the D1M Gogny force

NUCLEAR STRUCTURE ⁵⁴Cr, ¹⁰⁰Ru, ¹³⁰Xe, ¹⁸⁰Hf, ²⁰⁸Pb, ²³⁸U; calculated excitation energies, quadrupole deformations, moments of inertia as function of nuclear temperature. A=20-250; deduced ratio of HFB plus combinatorial densities to experimental s-wave neutron resonance spacings as function of temperature. ⁴⁰Ca, ⁴²K, ^50,51V, ^56,57Fe, ⁵⁸Ni, ⁶⁰Co, ⁶⁸Zn, ⁹⁰Zr, ^90,94Nb, ^{93,94,95,96,97,98}Mo, ¹⁰⁷Cd, ¹²⁷Te, ¹³²Xe, ^148,149Sm, ¹⁵⁵Eu, ^160,161,162Dy, ^166,167,168Er, ^171,172Yb, ¹⁷⁸Hf, ¹⁹⁴Ir, ²⁰⁸Pb, ²¹⁰Bi, ²³⁷U, ²³⁸U, ²³⁸Np, ²³⁹Pu, ²⁴²Am; calculated combinatorial nuclear level densities (NLD) using temperature-dependent D1M Gogny interaction. Comparison with experimental data. Z=50, N=50-120; deduced ratio of Maxwellian-averaged (n, γ) rates for T₉=1 obtained with current NLDs and those in previous calculations.

doi: 10.1103/PhysRevC.86.064317

2012NA04

Phys.Rev. C 85, 024623 (2012); Erratum Phys.Rev. C 85, 039901

H.Naik, T.N.Nathaniel, A.Goswami, G.N.Kim, M.W.Lee, S.V.Suryanarayana, S.Ganesan, E.A.Kim, M.-H.Cho, K.L.Ramakumar

Mass distribution in the 50-, 60-, and 70-MeV bremsstrahlung-induced fission of ²³²Th

NUCLEAR REACTIONS ²³²Th(γ, F)⁷⁷Ge/⁷⁸Ge/⁸⁴Br/^85mKr/⁸⁷Kr/⁸⁸Kr/⁸⁹Rb/⁹¹Sr/⁹²Sr/⁹³Y/⁹⁴Y/⁹⁵Zr/⁹⁷Zr/⁹⁹Mo/¹⁰¹Mo/¹⁰⁷Mo/¹⁰³Ru/¹⁰⁵Ru/¹⁰⁴Tc/¹⁰⁵Rh/¹¹²Ag/¹¹³Ag/¹¹⁵Cd/¹¹⁷Cd/^117mCd/¹²⁷Sb/¹²⁹Sb/¹²⁸Sn/¹³¹I/¹³³I/¹³⁴I/¹³⁵I/¹³²Te/¹³⁴Te/¹³⁸Cs/¹³⁹Ba/¹⁴⁰Ba/¹⁴¹Ce/¹⁴³Ce/¹⁴⁴Ce/¹⁴²La/¹⁴⁶Pr/¹⁴⁷Nd/¹⁴⁹Nd/¹⁴⁹Pm/¹⁴⁹Sm/¹⁵³Sm, E=50, 60, 70 MeV; measured Eγ, Iγ, fission product mass and cumulative yields, and yields of fission products for A=133-134, 138-139, and 143-144 by activation method, average neutron number. ²³²Th(n, F), E*=7.61, 12.61, 19.41 MeV; ²³⁸U(n, F), E*=7.35, 12.45, 19.15 MeV; ²³²Th(γ, F), E*=7.35, 13.22, 21.25 MeV; ²³²Th, ²³⁸U(γ, F), E=10, 40, 70 MeV; analyzed and compared yields of fission products as function of mass, yields of symmetric and asymmetric fission products, peak to valley ratios, average neutron number, average values of light mass and heavy mass as function of excitation energy.

doi: 10.1103/PhysRevC.85.024623

2012PL06

Iader.Fiz.Enerh. 13, 340 (2012); Nuc.phys.atom.energ. 13, 340 (2012)

V.A.Plujko, O.M.Gorbachenko, E.P.Rovenskykh, V.O.Zheltonoshskii

E1 gamma-transitions in hot atomic nuclei

NUCLEAR STRUCTURE A=40-230; calculated energy and width of giant dipole resonance. ⁹⁰Zr, ¹⁰⁰Mo, ¹²⁴Te, ^149,150Sm, ¹⁷¹Yb; calculated gamma-decay strength distribution. Comparison to experimentak data.

NUCLEAR REACTIONS Fe(n, γ), E<20 MeV; ¹⁸³W(n, γ), E<2 MeV; calculated σ. Comparison to experimental data.

doi: 10.15407/jnpae

2012SA18

Phys.Rev. C 85, 057601 (2012)

B.Sahu

Extremely long α-decay lifetimes and predictions based on an analytical expression

RADIOACTIVITY ¹⁴⁴Nd, ^{146,147,148,149}Sm, ¹⁵¹Eu, ¹⁵²Gd, ¹⁵⁶Dy, ^162,164Er, ¹⁶⁸Yb, ^174,176Hf, ^180,183W, ^184,186,188Os, ¹⁹⁶Hg, ²⁰⁴Pb, ^{166,168,170,172,174,176,182,184,186,188,190,192}Pt(α); calculated Q(α), T_1/2. Analytical expression, exactly solvable global potential in potential scattering theory. Comparison with experimental data, and with calculations using modified two-potential approximation (MTPA) method.

doi: 10.1103/PhysRevC.85.057601

2013AN02

At.Data Nucl.Data Tables 99, 69 (2013)

I.Angeli, K.P.Marinova

Table of experimental nuclear ground state charge radii: An update

COMPILATION Z=0-96; compiled nuclear radii, rms nuclear charge radii.

doi: 10.1016/j.adt.2011.12.006

2013UH01

Nucl.Phys. A913, 127 (2013)

H.Uhrenholt, S.Aberg, A.Dobrowolski, Th.Dossing, T.Ichikawa, P.Moller

Combinatorial nuclear level-density model

NUCLEAR STRUCTURE ⁶⁰Co, ⁶⁸Zn, ^{76,78,80,82,84,86}Sr, ⁹⁴Nb, ^97,98Mo, ^{107,109,111,112,113,114,115,117}Cd, ¹²⁷Te, ¹⁴⁸Pm, ^148,149Sm, ¹⁵⁵Eu, ^161,162Dy, ^166,167Er, ^{169,170,171,172,173,174,175,177}Yb, ¹⁹⁴Ir, ²³⁷U, ²³⁹Pu; calculated level density, angular momentum distribution, parity ratio, pairing gap. ⁹⁰Zr, ⁹⁰Nb; calculated J, π level density. A=20-255; calculated level density at neutron separation energy, vibrational enhancement. Combinatorial (microcanonical) model with folded Yukawa, pairing, rotational and vibrational states. Compared with available data.

doi: 10.1016/j.nuclphysa.2013.06.002

2013ZH28

Phys.Rev. C 88, 014304 (2013)

Y.Zhang, F.Pan, Y.-X.Liu, Y.-A.Luo, J.P.Draayer

Shape phase transition and phase coexistence in odd Sm nuclei

NUCLEAR STRUCTURE ^{146,147,148,149,150,151,152,153,154,155,156,157}Sm; calculated energies of ground-state band members using several collective rotor and vibrator models; deduced shape phase transition in odd-A Sm nuclei from experimental S(2n) values and experimental energies of ground-band members in even and odd-A Sm nuclei. ^150,152Sm; analyzed ground-state and β band members. ^151,153Sm; analyzed four collective bands in each nucleus; deduced phase coexistence of rotational and vibrational excitations in ¹⁵¹Sm.

doi: 10.1103/PhysRevC.88.014304

2014AL12

Nucl.Data Sheets 118, 233 (2014)

Y.Alhassid, C.Ozen, H.Nakada

Calculating Level Densities of Heavy Nuclei by the Shell Model Monte Carlo Method

NUCLEAR STRUCTURE ^{148,150,152,154}Sm; calculated average total nuclear spin. ^{143,144,145,146,147,148,149,150,152}Nd, ^{148,149,150,151,152,153,154,155}Sm; calculated state density vs excitation energy, even-mass nuclei collective enhancement factor using Monte Carlo microscopic approach. Compared with available data.

doi: 10.1016/j.nds.2014.04.045

2014FI17

Phys.Rev. C 90, 064616 (2014)

D.M.Filipescu, I.Gheorghe, H.Utsunomiya, S.Goriely, T.Renstrom, H.-T.Nyhus, O.Tesileanu, T.Glodariu, T.Shima, K.Takahisa, S.Miyamoto, Y.-W.Lui, S.Hilaire, S.Peru, M.Martini, A.J.Koning

Photoneutron cross sections for samarium isotopes: Toward a unified understanding of (γ, n) and (n, γ) reactions in the rare earth region

NUCLEAR REACTIONS ^{144,147,148,149,150,152,154}Sm(γ, n), E=6-17 MeV; measured E(n), I(n), monochromatic and nonmonochromatic σ(E). Comparison with previous experimental results, and predictions from Skyrme HFB+QRPA using BSk7 interaction, and axially deformed Gogny HFB+QRPA models using D1M interaction. ^{147,148,149,150,151,152}Sm(n, γ), E=0.001-1 MeV; analyzed measured σ(E) with a TALYS calculation using D1M+QRPA calculation for the E1 strength function. ¹⁵³Sm(n, γ), E=0.001-1 MeV; predicted σ(E) from TALYS calculations using γ-strength function (γSF) approach. Comparison with evaluated libraries JENDL-4.0, ENDF/B-VII.1, ROSFOND-2010.

doi: 10.1103/PhysRevC.90.064616

2015BA10

Phys.Rev. C 91, 024617 (2015)

D.Banerjee, A.Saha, T.Bhattacharjee, R.Guin, S.K.Das, P.Das, D.Pandit, A.Mukherjee, A.Chowdhury, S.Bhattacharya, S.Das Gupta, S.Bhattacharyya, P.Mukhopadhyay, S.R.Banerjee

Role of p-induced population of medium-mass (A∼150) neutron-rich nuclei

NUCLEAR REACTIONS ¹⁵⁰Nd(p, n), (p, 2n), (p, p'n), (p, d), E=7-15 MeV; measured Eγ, Iγ, σ(E), half-lives by activation method using K=130 AVF cyclotron at VECC facility. Comparison with previous experimental results, and with model calculations using CASCADE, ALICE, and EMPIRE3.1 computer codes.

RADIOACTIVITY ¹⁴⁹Nd, ^149,150Pm(β^-); measured Eγ, Iγ, ground state half-lives of ¹⁴⁹Nd, ^149,150Pm.

doi: 10.1103/PhysRevC.91.024617

2015BA20

Phys.Rev. C 91, 064615 (2015)

J.S.Barrett, W.Loveland, R.Yanez, S.Zhu, A.D.Ayangeakaa, M.P.Carpenter, J.P.Greene, R.V.F.Janssens, T.Lauritsen, E.A.McCutchan, A.A.Sonzogni, C.J.Chiara, J.L.Harker, W.B.Walters

¹³⁶Xe+²⁰⁸Pb reaction: A test of models of multinucleon transfer reactions

NUCLEAR REACTIONS ²⁰⁸Pb(¹³⁶Xe, X), E=85 MeV; measured Eγ, Iγ, γγ-coin using Gammasphere at ATLAS-ANL facility, σ for projectile-like fragments (PLFs) and target-like fragments (TLFs) by off-line γ-ray spectroscopy for radioactive decay measurements (RD), prompt γ decays recorded during the beam burst (IB), and delayed γ decays recorded between the beam bursts (OB). ^116,118Cd, ^119,121In, ^{118,120,122,123,124,126}Sn, ^{119,121,123,125,126,127,128,130}Sb, ^{124,126,128,130,131,132,134}Te, ^{127,128,129,130,131,132,133,135,136}I, ^128,130,132Xe, ^{133,134,135,136,137,138}Xe, ^{131,132,133,134,136,137,139,141}Cs, ¹³⁰Ba, ^{132,134,136,138,139,140,141,142,143}Ba, ^{132,135,136,137,139,140,143}La, ^{136,138,139,140,141,142,143,144,145,146}Ce, ^139,141,142Pr, ^{140,142,143,144,145,146,147,148,149}Nd, ^{142,143,145,147,149}Pm, ^{145,146,147,148,149,150,151,152,154}Sm, ^147,149,151Eu, ^152,154,156Gd, ^{156,158,160,162,164}Dy, ^160,161Er, ¹⁷⁶Yb, ^{176,178,180,181,182}Hf, ^179,181Ta, ^{176,180,182,184,186,187}W, ^179,185,187Re, ^{186,188,190,191,192,194,197}Os, ^188,190,192Ir, ^{190,191,192,194,196,197,198,200,201,202}Pt, ^{191,192,193,194,196,198,199}Au, ^{194,196,198,200,202,203,204,205,206,208}Hg, ^{196,197,198,199,201,202,203,204,205,206,207}Tl, ^{198,201,202,203,204,206,207,208,209,210,211}Pb, ^{199,201,202,203,204,205,206,207,209,211}Bi, ^{202,204,205,206,207,208,209,210,212,213,214}Po, ^{207,208,209,210,211,213}At, ^{210,211,212,213,214,215,216,218}Rn, ^{211,212,213,215,216}Fr, ²¹⁴Ra; deduced projectile-like fragment cumulative and independent production yields. Comparison with predictions of GRAZING model, and those of Zagrebaev and Greiner model using a quantitative metric. Discussed correlations between TLF and PLF yields.

doi: 10.1103/PhysRevC.91.064615

2015DA07

Phys.Rev. C 92, 014319 (2015)

E.D.Davis, L.Hamdan

Reappraisal of the limit on the variation in α implied by the Oklo natural fission reactors

NUCLEAR REACTIONS ¹⁴⁹Sm, ^155,157Gd(n, γ), E=natural (Oklo) reactor neutrons; analyzed sensitivity of neutron resonance energies to changes in fine structure constant α; deduced α_Oklo-α_now. Comparison of change in α with results from atomic clock experiments. Relevance to astrophysical measurements of redshift dependence on parameters such as α.

NUCLEAR STRUCTURE ^149,150Sm, ^156,158Gd; calculated proton and charge density parameters for ground states of ^149,150Sm, excitation, Coulomb, and deformation corrections using deformed Fermi density distributions fitted to the output of Hartree-Fock (HF)+BCS calculations with SLy4 and SkM* Skyrme functionals.

doi: 10.1103/PhysRevC.92.014319

2015EL05

Int.J.Mod.Phys. E24, 1550073 (2015)

Y.El Bassem, M.Oulne

Ground state properties of even-even and odd Nd, Ce and Sm isotopes in Hartree-Fock-Bogoliubov method

NUCLEAR STRUCTURE ^{124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161}Nd, ^{123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158}Ce, ^{132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166}Sm; calculated ground state energies, two-neutron separation energies. HFB method with SLy5 Skyrme and 1SGogny forces, comparison with experimental data.

doi: 10.1142/S0218301315500731

2015OZ01

Phys.Rev. C 91, 034329 (2015)

C.Ozen, Y.Alhassid, H.Nakada

Nuclear state densities of odd-mass heavy nuclei in the shell model Monte Carlo approach

NUCLEAR STRUCTURE ^{143,145,147,149}Nd, ^{149,150,151,153,155}Sm; calculated thermal excitation energy and partition function as function of temperature, level densities versus excitation energy. Shell model Monte Carlo (SMMC) calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.91.034329

2015ZH37

Chin.Phys.C 39, 104103 (2015)

Y.Zhang, X.Guan, Y.Wang, Y.Zuo, L.N.Bao, F.Pan

Shape phase transition in the odd Sm nuclei: effective order parameter and odd-even effect

NUCLEAR STRUCTURE ^{145,146,147,148,149,150,151,152,153,154,155,156,157,158}Sm; calculated two-neutron separation energies, odd-even mass difference, evolution of the pairing strength, first pairing-excitation energy. BCS theory, CBCS scheme.

doi: 10.1088/1674-1137/39/10/104103

2016DU04

Phys.Rev. C 93, 024602 (2016)

S.Dutta, D.Chakraborty, G.Gangopadhyay, A.Bhattacharyya

Neutron capture reactions near the N=82 shell-closure

NUCLEAR REACTIONS ¹⁴⁰Ce(n, n), E=1.5, 2.0, 2.5, 3.0 MeV; ¹⁴¹Pr(n, n), E=0.878, 1.2 MeV; ¹⁴²Nd(n, n), E=2.5 MeV; ¹⁴⁸Sm(n, n), E=2.7; calculated σ(θ) and compared to experimental data. ¹³³Cs, ¹³⁹La, ¹⁴⁰Ce, ¹⁴¹Pr, ^{135,136,137,138}Ba, ^{142,143,144,145,146}Nd, ^{144,147,148,149}Sm(n, γ), E=0.001-1 MeV; calculated σ(E), Maxwellian-averaged cross sections (MACS) at kT=30 keV, and compared to experimental data. Semimicroscopic optical model with the DDM3Y nucleon-nucleon interaction. Relevance to astrophysical s- and p-processes for nuclei near N=82 neutron shell-closure.

NUCLEAR STRUCTURE ^{133,134,135,136,137}Cs, ^{130,132,134,135,136,137,138}Ba, ^138,139La, ^{136,138,140,141,142}Ce, ^141,142,143Pr, ^{142,143,144,145,146,147}Nd, ^147,148Pm, ^{144,147,148,149}Sm; calculated charge densities, and root-mean-square (rms) charge radii using relativistic mean-field approach. Comparison with experimental values.

doi: 10.1103/PhysRevC.93.024602

2016GU12

Phys.Rev. C 94, 024309 (2016)

X.Guan, H.Xu, Y.Zhang, F.Pan, J.P.Draayer

Ground state phase transition in the Nilsson mean-field plus standard pairing model

NUCLEAR STRUCTURE ^{144,145,146,147,148,149,150,151,152,153,154,155}Nd, ^{146,147,148,149,150,151,152,153,154,155,156,157}Sm, ^{148,149,150,151,152,153,154,155,156,157,158,159}Gd; calculated Pairing interaction strength G, odd-even mass differences, odd-even differences of S(2n) values, odd-even differences of α-, and β^--decay energies. Nilsson mean-field plus standard pairing model for the ground state phase transitions. Comparison with experimental values taken from NNDC databases.

doi: 10.1103/PhysRevC.94.024309

2016NO13

Phys.Rev. C 94, 064310 (2016)

K.Nomura, T.Niksic, D.Vretenar

Signatures of shape phase transitions in odd-mass nuclei

NUCLEAR STRUCTURE ^{148,150,152,154}Sm; calculated self-consistent RHB triaxial quadrupole binding energy contours in (β, γ) plane, equilibrium deformation parameter for Kπ=0+ bandheads, B(E2) for the two lowest 0+ states. ^{147,149,151,153,155}Sm, ^{147,149,151,153,155}Eu; calculated levels, J, π, excitation energies of low-lying positive- and negative-parity yrast states as functions of neutron number, equilibrium deformation parameter for bandheads for the lowest three positive- and negative-parity bands, B(E2) between the bandheads and the lowest five states, S(p) and S(n). Microscopic framework based on nuclear energy density functional theory and the particle-plus-boson-core coupling scheme. Comparison with experimental data taken from the NNDC-BNL databases.

doi: 10.1103/PhysRevC.94.064310

2016SA16

Phys.Rev. C 93, 044301 (2016)

B.Sahu, S.Bhoi

Viola-Seaborg relation for α-decay half-lives: Update and microscopic determination of parameters

RADIOACTIVITY ^106,108Te, ¹¹²Xe, ¹¹⁴Ba, ¹⁴⁴Nd, ^146,148Sm, ^148,150,152Gd, ^150,152,154Dy, ^152,154Er, ^154,156,158Yb, ^{156,158,160,162,174}Hf, ^{160,162,164,166,180}W, ^{162,166,168,170,172,174,186}Os, ^{168,170,174,176,178,180,188,190}Pt, ^{174,176,180,182,184,186,188}Hg, ^{178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210}Pb, ^{190,192,194,196,198,200,202,204,206,210,212,214,216,218}Po, ^{198,204,206,208,210,212,214,216,218,220,222}Rn, ^{210,212,214,216,218,220,222,224,226}Ra, ^{216,218,220,222,224,226,228,230,232}Th, ^{226,228,230,232,234,236,238}U, ^{232,234,236,238,240,242,244}Pu, ^{238,240,242,244,246,248}Cm, ^{240,246,248,250,252,254}Cf, ^{246,248,250,252,254,256}Fm, ^252,254,256No, ^260,266Sg(α); calculated ground-state to ground-state (l=0) half-lives and compared with experimental values; deduced analytic closed formula, as possible replacement of empirical Viola-Seaborg rule.

RADIOACTIVITY ^144,145Nd, ^{145,146,147,148}Pm, ^{146,147,148,149,150}Sm, ^{130,131,132,133,134,135,136,137,138,139,140,141,148,151}Eu, ^{135,136,137,138,139,140,141,142,143,148,149,150,151,152,153}Gd, ^{136,137,138,139,140,141,142,144,145,149,150,151,152,154}Tb, ^{138,139,140,141,142,143,144,145,146,147,149,150,151,152,153,154,155,156}Dy, ^{140,141,142,143,144,145,147,148,149,150,151,152,153,154,155,156,157}Ho, ^{145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,164}Er, ^{153,154,155,156,157,158,159,160,161,162,163,164,165}Tm, ^{154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,170}Yb, ^{155,156,157,158,159,160,161,162,163,164,165,167,168,169,170,171,172,173,174}Lu, ^{156,157,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178}Hf, ^{157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,179}Ta, ^{158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181}W, ^{160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,183,184,185,186}Re, ^{162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186,187,188,189}Os, ^{164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186,187,188,189,190,191}Ir, ^{166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193}Pt(α); calculated α-decay half-lives using analytical formula and parameters deduced in the present work. Comparison with available experimental results.

doi: 10.1103/PhysRevC.93.044301

2017BA01

Nucl.Phys. A957, 123 (2017)

A.Badola, S.K.Singhal, M.Bhatnagar, H.M.Agrawal

J-dependence of s-wave neutron strength function and presence of intermediate structure in medium and heavy mass nuclides

NUCLEAR STRUCTURE ³⁵Cl, ⁴³Ca, ⁴⁵Sc, ^47,49Ti, ⁵¹V, ⁵³Cr, ⁵⁵Mn, ⁵⁷Fe, ⁵⁹Co, ⁶¹Ni, ^63,65Cu, ⁶⁷Zn, ^69,71Ga, ⁷³Ge, ⁷⁵As, ⁷⁷Se, ^79,81Br, ^85,87Rb, ⁸⁹Y, ^91,93Zr, ⁹³Nb, ^95,97Mo, ⁹⁹Tc, ¹⁰¹Ru, ¹⁰³Rh, ¹⁰⁹Pd, ^107,109Ag, ¹¹¹Cd, ¹¹⁵In, ¹²¹Sb, ^123,125Te, ¹²⁷I, ^129,131Xe, ¹³³Cs, ^135,137Ba, ¹⁴¹Pr, ^143,145Nd, ¹⁴⁹Sm, ^155,157Gd, ¹⁵⁹Tb, ^161,163Dy, ¹⁶⁵Ho, ¹⁶⁷Er, ¹⁶⁹Tm, ^171,173Yb, ^177,179Hf, ¹⁸¹Ta, ¹⁸³W, ¹⁸⁵Re, ¹⁸⁹Os, ¹⁹⁵Pt, ^199,201Hg, ^203,205Tl, ²⁰⁷Pb, ²⁰⁹Bi, ^233,235U, ²³⁷Np, ^239,241Pu; calculated s-wave neutron strength function, presence of intermediate structure for different spin vs spin of target nuclei; deduced spin dependence of the strength function. Recommend to include this in the optical model.

doi: 10.1016/j.nuclphysa.2016.08.004

2017ME07

Phys.Rev. C 96, 014308 (2017)

H.Mei, K.Hagino, J.M.Yao, T.Motoba

Transition from vibrational to rotational character in low-lying states of hypernuclei

NUCLEAR STRUCTURE ^{144,146,148,150,152,154}Sm; calculated total energy in the mean-field approximation as a function of quadrupole deformation, yrast levels, E(first 4+)/E(first 2+) using multireference covariant density functional theory (MR-CDFT), and compared with experimental data. ^{145,147,149,151,153,155}Sm; calculated levels, J, π, B(E2) of hypernuclei, probability of the dominant components of configurations using microscopic particle-core coupling scheme based on the covariant density functional theory.

doi: 10.1103/PhysRevC.96.014308

2017NO07

Phys.Rev. C 96, 014314 (2017)

K.Nomura, R.Rodriguez-Guzman, L.M.Robledo

Description of odd-mass nuclei within the interacting boson-fermion model based on the Gogny energy density functional

NUCLEAR STRUCTURE ^{149,151,153,155}Eu, ^{149,151,153,155}Sm, ¹⁹⁵Pt, ¹⁹⁵Au; calculated spherical single-particle energies, occupation probabilities of the single-particle orbitals, parameters of the boson-fermion Hamiltonian, coupling constants of the boson-fermion interaction, levels, J, π, B(E2), B(M1), electric quadrupole and magnetic dipole moments, bands and wavefunction amplitudes for levels in ¹⁹⁵Pt and ¹⁹⁵Au. ^{148,150,152,154}Sm, ¹⁹⁴Pt; calculated parameters of the boson Hamiltonian, potential energy surface contours in (β, γ) plane, low-lying levels, J, π, B(E2) for ¹⁹⁴Pt. Interacting boson fermion model (IBFM) with parameters based on the Hartree-Fock-Bogoliubov (HFB) approximation, and with the Gogny-D1M energy density functional (EDF) at the mean-field level. Comparison with experimental data.

doi: 10.1103/PhysRevC.96.014314

2017SE19

Phys.Rev. C 96, 054328 (2017)

W.M.Seif, N.V.Antonenko, G.G.Adamian, H.Anwer

Correlation between observed α decays and changes in neutron or proton skins from parent to daughter nuclei

RADIOACTIVITY ^{105,106,107,108,109,110}Te, ^{107,108,109,110,111,112,113}I, ^{109,110,111,112,113,115}Xe, ^{124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,143,144,145,146,147,148,149}Nd, ^{133,134,135,136,137,138,139,143,145,146,147,148,149,150,151,152}Sm, ^{133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155}Gd, ^{148,149,150,151,152}Yb, ^{147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166}Ho, ^{153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177}Yb, ^{186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,211,222,223,224}Po, ^{212,213,214,215,216,217,218,219,220,211,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241}Pa, ^{241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260}Fm(α); calculated difference between the proton or neutron skin thicknesses, Q(α), partial α-decay half-lives for ^140-155Gd, ^232-241Pa and ^258-260Fm. Comparison with available experimental half-lives. Hartree-Fock-Bogoliubov (HFB) method based on the Skyrme-like effective interactions.

doi: 10.1103/PhysRevC.96.054328

2017WI01

Phys.Rev. C 95, 034618 (2017)

H.Wilsenach, K.Zuber, D.Degering, R.Heller, V.Neu

High precision half-life measurement of ¹⁴⁷Sm α decay from thin-film sources

RADIOACTIVITY ¹⁴⁷Sm(α); measured Eα, Iα, isotopic abundance of ¹⁴⁷Sm, half-life of ¹⁴⁷Sm decay using natural Sm samples and ultra-low-background twin Frisch-grid ionization chamber (TF-GIC). GEANT4 simulation to determine the geometrical efficiency for each sample. Comparison with previous half-life measurements.

ATOMIC MASSES ^{144,147,148,149,150,152,154}Sm; measured isotopic abundances of natural Sm samples using inductively coupled plasma mass spectrometry (ICP-MS). Comparison with literature data.

doi: 10.1103/PhysRevC.95.034618

2018GO15

Phys.Rev. C 98, 014327 (2018)

S.Goriely, S.Hilaire, S.Peru, K.Sieja

Gogny-HFB+QRPA dipole strength function and its application to radiative nucleon capture cross section

NUCLEAR STRUCTURE ^72,74,76Ge, ⁷⁵As, ^76,80,82Se, ^90,92,94Zr, ¹⁰³Rh, ^107,109Ag, ¹¹⁵In, ^{112,114,117,118,119,120,122,124}Sn, ¹²⁷I, ¹³³Cs, ^136,138Ba, ¹⁴¹Pr, ^{142,143,144,145,146,148,150}Nd, ^{144,148,149,150,152,153,154}Sm, ¹⁵³Eu, ^156,160Gd, ¹⁵⁹Tb, ¹⁶⁵Ho, ¹⁶⁸Er, ^171,174Yb, ^175,176Lu, ^178,180Hf, ^182,184,186W, ^{186,188,189,190,192}Os, ^191,193Ir, ^{194,195,196,198}Pt, ⁴⁴Sc, ⁴⁴Ti, ¹³⁴Xe, ⁵⁰V, ⁵⁶Fe, ⁸⁹Y, ^92,94,96,98Mo, ^106,108Pd, ^106,112Cd, ¹³⁹La, ^162,164Dy, ¹⁶⁷Er, ^180,182Ta, ^206,208Pb, ²³²Th, ²³²Pa, ^237,238,239U, ²³⁸Np; calculated E1 and M1 deexcitation strength functions, and compared with experimental GDR and Oslo strengths. A=40-250, Z=20-83; calculated total average radiative widths, and compared with experimental data, ratios of theoretical to experimental MACS at kT=30 keV. Z=8-94, N=10-190; calculated ratio of (n, γ) and (p, γ) MACS at T=10⁹ K obtained using D1M+QRPA+0lim⁺ and the ones obtained using the generalized Lorentzian (GLO) model for nuclei between the neutron and proton driplines. Axially symmetric deformed quasiparticle random-phase approximation with finite-range D1M Gogny force (Gogny-HFB+QRPA).

NUCLEAR REACTIONS ¹³⁵Ba(n, γ), E=1 keV-1 MeV; ¹⁰⁰Mo(n, γ), E=1 keV-20 MeV; calculated σ(E) with D1M+QRPA E1 and M1 strengths, and compared with experimental data. Cl(p, γ), E=172.5 MeV; calculated ratio of (n, γ) MACS at T=10⁹ K obtained using D1M+QRPA+0lim⁺ and the ones obtained using the generalized Lorentzian (GLO) model.

doi: 10.1103/PhysRevC.98.014327

2019FE04

J.Radioanal.Nucl.Chem. 320, 153 (2019)

E.K.Fenske, B.D.Roach, D.C.Glasgow, R.H.Ilgner, J.M.Giaquinto

Rapid measurements of ²³⁵U fission product isotope ratios using an online, high-pressure ion chromatography inductively coupled plasma mass spectrometry protocol with comparison to isotopic depletion models

NUCLEAR REACTIONS ²³⁵U(n, F), E thermal; measured reaction products. ^135,137Cs, ^89,90Sr, ^101,102Ru, ^141,144Ce, ¹⁴⁷Nd, ¹⁴⁷Pm, ^149,151Sm; deduced isotopic ratios. Comparison with ORIGEN calculations.

doi: 10.1007/s10967-019-06438-4

2019STZV

INDC(NDS)-0794 (2019)

N.J.Stone

Table of Recommended Nuclear Magnetic Dipole Moments: Part I - Long-lived States

COMPILATION Z=0-99; compiled experimental values of nuclear magnetic moments.

doi: 10.61092/iaea.yjpc-cns6

2019VI04

Phys.Rev. C 100, 034318 (2019)

A.V.Viatkina, D.Antypas, M.G.Kozlov, D.Budker, V.V.Flambaum

Dependence of atomic parity-violation effects on neutron skins and new physics

ATOMIC PHYSICS ^85,87Rb, ^{131,134,135,136,137}Cs, ^{130,132,133,134,135,136,137,138}Ba, ^{144,145,146,147,148,149,150,151,152,153,154}Sm, ^{156,158,161,162,163,164}Dy, ^{168,170,171,172,173,174,176}Yb, ^203,204,205Tl, ^{202,204,205,206,207,208}Pb, ^{207,208,209,210,211,212,213,220,221,222,223,224,225,226,227,228}Fr, ^{208,209,210,211,212,213,214,220,221,222,223,224,225,226,227,228,229,230,232}Ra; calculated mean values of the coefficients as functions of the radius parameter for different elements, assuming Fermi distribution of nuclear density; evaluated relevant coefficients from for the nuclear factor of the Parity-nonconserving (PNC) amplitude in low energy atomic experiments. Relevance to Yb experiment in Mainz and the Fr experiment at TRIUMF.

doi: 10.1103/PhysRevC.100.034318

2020STZV

INDC(NDS)-0816 (2020)

N.Stone

Table of Recommended Nuclear Magnetic Dipole Moments: Part II, Short-Lived States

COMPILATION Z=5-95; compiled experimental values of nuclear magnetic moments.

doi: 10.61092/iaea.1p48-p6c6

2021FA08

Phys.Rev. C 103, 064310 (2021)

P.Fanto, Y.Alhassid

State densities of heavy nuclei in the static-path plus random-phase approximation

NUCLEAR STRUCTURE ^{148,149,150,151,152,153,154,155}Sm; calculated ground-state energies, canonical entropies as function of inverse temperature, state densities as function of excitation energy using the static-path plus random-phase approximation (SPA+RPA) in the configuration-interaction (CI) shell-model framework against exact shell-model Monte Carlo (SMMC) state densities. Comparison with mean-field state densities calculated with the finite-temperature Hartree-Fock-Bogoliubov (HFB) approximation. Comparison with experimental data.

doi: 10.1103/PhysRevC.103.064310

2021STZZ

INDC(NDS)-0833 (2021)

N.J.Stone

Table of Nuclear Electric Quadrupole Moments

COMPILATION Z=1-102; compiled experimental measurements of static electric quadrupole moments of ground states and excited states of atomic nuclei throughout the periodic table.

doi: 10.61092/iaea.a6te-dg7q

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

2022AN05

Phys.Rev. C 105, 014325 (2022)

R.An, X.Jiang, L.-G.Cao, F.-S.Zhang

Odd-even staggering and shell effects of charge radii for nuclei with even Z from 36 to 38 and from 52 to 62

NUCLEAR STRUCTURE ^{72,73,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102}Kr, ^{74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104}Sr, ^{110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150}Te, ^{110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156}Xe, ^{116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162}Ba, ^{126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158}Ce, ^{126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160}Nd, ^{130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165}Sm; calculated charge radii and odd-even staggering (OES) effects by the relativistic mean field (RMF-BCS) and the modified RMF(BCS)^* approaches; deduced no significant influence of neutron-proton short-range correlations (np-SRCs) for some nuclei due to the strong coupling between different levels around Fermi surface. Comparison with available experimental data.

doi: 10.1103/PhysRevC.105.014325

2022FA06

Chin.Phys.C 46, 054105 (2022)

J.Fan, C.Xu

Exploring the half-lives of extremely long-lived α emitters

RADIOACTIVITY ¹⁴²Ce, ^145,146Nd, ¹⁴⁹Sm, ¹⁵⁶Dy, ^162,164Er, ¹⁶⁸Yb, ^182,183,184W, ¹⁸⁶W, ^{187,188,189,190}Os, ¹⁹²Pt, ¹⁹⁵Pt, ^204,206Pb(α); calculated T_1/2. ¹⁸⁷Os, ¹⁴⁹Sm; deduced recommendation for experiments.

doi: 10.1088/1674-1137/ac500d