References from selected dataset

NUCLEAR STRUCTURE ¹⁵¹Pm, ¹⁴⁹Pm, ¹⁵³Gd, ¹⁵³Sm, ¹⁶⁶Dy, ¹⁶⁶Ho, ¹⁵⁹Dy, ¹⁶⁰Tb, ¹⁶¹Tb, ⁹¹Y, ¹⁴⁴Pr, ¹⁴³Pr, ¹⁴⁷Nd; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0022-1902(63)80144-X

1972BEWU

Program and Theses, Proc.22nd Ann.Conf.Nucl.Spectrosc.Struct.At.Nuclei, Kiev, p.62 (1972)

R.B.Begzhanov, A.I.Muminov, N.A.Ilkhamdzhanov, K.T.Salikhbaev, U.Y.Yuldashev

Determination of g-Factor of Excited States in ⁷⁴Ge, ⁷⁷As and ¹⁵¹Pm

RADIOACTIVITY ⁷⁴As, ⁷⁷Ge, ¹⁵¹Nd; measured γγ(θ, H, t). ⁷⁴Ge, ⁷⁷As, ¹⁵¹Pm levels deduced T_1/2, g.

1972BU22

Nucl.Phys. A193, 271 (1972)

D.G.Burke, J.C.Waddington

The Level Structure of ¹⁵¹Pm

NUCLEAR REACTIONS ¹⁵⁰Nd(³He, d), E=24 MeV; measured σ(Ed); ¹⁵⁰Nd(α, t), E=25 MeV; measured σ(Et); ¹⁵²Sm(t, α), E=15 MeV; measured σ(Eγ). ¹⁵¹Pm deduced levels, J, π, L. Enriched targets.

doi: 10.1016/0375-9474(72)90252-7

1973SE12

J.Phys.Soc.Jap. 34, 1443 (1973)

T.Seo, T.Hayashi, T.Mitamura

Decay of ¹⁵¹Nd

RADIOACTIVITY ¹⁵¹Nd; measured Eγ, Iγ, γγ(θ), βγ-coin, Eβ. Deduced log ft, Q. ¹⁵¹Pm deduced levels, J, π, γ-multipolarities, K.

1974MI04

Nucl.Phys. A218, 274 (1974)

L.Milazzo-Colli, G.M.Braga-Marcazzan, M.Milazzo, C.Signorini

Preformation Probability of α-Clusters in Rare Earth Nuclei Measured by Means of the (p, α) Reaction

NUCLEAR REACTIONS ¹⁴⁷Sm, ¹⁵⁰Nd, ^152,154Sm(p, α), E=18 MeV; measured σ(Eα, θ). Deduced preformation probability of α-clusters.

doi: 10.1016/0375-9474(74)90004-9

1977SE06

Nucl.Phys. A282, 302 (1977)

T.Seo

The Nuclear Structure of ¹⁵¹Pm in the Low Excitation Region < 1 MeV

RADIOACTIVITY ¹⁵¹Nd [from ¹⁵⁰Nd(n, γ)]; measured Eγ, Iγ, γγ-coin, γγ(θ), γγ(θ, H). ¹⁵¹Pm deduced levels, J, π, multipolarities, mixing ratios, g. Enriched target, Ge(Li) detectors.

doi: 10.1016/0375-9474(77)90217-2

1978SH17

Nucl.Phys. A307, 239 (1978)

M.A.M.Shahabuddin, J.C.Waddington, D.G.Burke, O.Straume, G.Lovhoiden

A Comparison of the (p, α) and (t, α) Reactions in the Shape Transitional Region Near N = 90

NUCLEAR REACTIONS ^150,152,154Sm(p, α), ^156,158Gd(p, α), E=17.0 MeV; measured σ(Eα, θ). Results compared with sequential-, direct-transfer calculations. Enriched targets.

doi: 10.1016/0375-9474(78)90615-2

1979ST06

Nucl.Phys. A322, 13 (1979)

O.Straume, G.Lovhoiden, D.G.Burke, E.R.Flynn, J.W.Sunier

Single-Proton States in ¹⁵¹Pm

NUCLEAR REACTIONS ¹⁵²Sm(polarized t, α), E=17 MeV; measured σ(θ, Eα), Ay(θ, Eα). ¹⁵⁰Nd(³He, d), E=24 MeV; measured σ(θ, Ed). ¹⁵¹Pm deduced levels, J, π, L, Nilsson assignments. Enriched targets.

doi: 10.1016/0375-9474(79)90330-0

1980CW03

Acta Phys.Pol. B11, 445 (1980)

S.Cwiok, W.Nazarewicz, W.Zych

The Dependence of Coulomb Displacement Energy on Deformation of a Nucleus

NUCLEAR STRUCTURE ^149,151Nd, ^149,151Pm, ¹⁶⁹Er, ¹⁶⁹Tm, ^169,171Yb, ^169,171Lu; calculated Coulomb displacement energies; deduced deformation effects. Woods-Saxon deformed potential, monopole pairing interaction.

1980SE09

Ann.Rep.Res.Reactor Inst., Kyoto Univ. 13, 167 (1980)

T.Seo, S.Yamada, T.Hayashi

Vibrational Excitations in ¹⁵¹Pm

NUCLEAR STRUCTURE ¹⁵¹Pm; calculated levels, J, B(λ), vibrational state configurations. Rotation-vibration coupling model.

1981DI01

Phys.Rev. C23, 331 (1981)

J.K.Dickens, J.W.McConnell

Yields of Fission Products Produced by Thermal-Neutron Fission of ²⁴⁵Cm

NUCLEAR REACTIONS, Fission ²⁴⁵Cm(n, F), E=thermal; measured σ(Eγ), T_1/2. ^87,90Kr, ^91,93,94Y, ^91,92,93,94Sr, ⁸⁴Br, ^88,89Rb, ^95,97,99Nb, ^99,101Mo, ^{105,106,103,104,102}Tc, ^{108,109,105,103}Ru, ^{106,111,107,109,105,110}Rh, ^{113,111,114,112}Ag, ¹¹⁵In, ^{131,136,133,137,132,134,135}I, ^{139,137,135,138}Xe, ^149,147,151Nd, ^97,95Zr, ^152,153,151Pm, ^{141,146,148,143,145,136,139,138,140}Cs, ^{139,142,141,140}Ba, ^{132,133,134,131}Te, ^144,140,142La, ^128,127Sn, ¹⁴⁶Pr, ^{127,128,132,129,130,131,133}Sb, ¹⁵⁶Eu deduced cumulative yields.

doi: 10.1103/PhysRevC.23.331

1982KU07

Phys.Rev. C25, 3011 (1982)

H.Kudo, H.Muramatsu, H.Nakahara, K.Miyano, I.Kohno

Fission Fragment Yields in the Fission of ²³²Th by Protons of Energies 8 to 22 MeV

NUCLEAR REACTIONS, ICPND ²³²Th(p, F)⁸⁷Kr/⁸⁸Kr/⁹¹Sr/⁹²Sr/⁹⁵Zr/⁹⁷Zr/⁹⁷Nb/⁹⁹Mo/⁹⁹Tc/¹⁰³Ru/¹⁰⁵Rh/¹¹²Pd/¹¹²Ag/¹¹⁵Cd/¹¹⁵In/¹²⁷Sb/¹²⁸Sb/¹²⁹Sb/¹³²Te/¹³⁵I/¹³⁶Cs/¹⁴¹Ce/¹⁴³Ce/¹⁴⁷Nd/¹⁴⁹Pm/¹⁵¹Pm, (p, n), (p, 2n), (p, 3n), E=8-22 MeV; measured fission σ, total σ, evaporation σ vs E, production σ vs E for residuals. ^233,232,231Pa deduced asymmetric fission barrier heights. Statistical model.

doi: 10.1103/PhysRevC.25.3011

1983SC20

Phys.Lett. 125B, 106 (1983)

O.Scholten, T.Ozzello

An Interacting Boson-Fermion Model Calculation for the Odd-Mass Promethium Isotopes

NUCLEAR STRUCTURE ^{147,149,151,153}Pm; calculated levels, stripping, pickup spectroscopic factors. Interacting boson-fermion model.

doi: 10.1016/0370-2693(83)91245-5

1986DI09

Phys.Rev. C34, 722 (1986)

J.K.Dickens, J.W.McConnell

Yields of Fission Products Produced by Thermal-Neutron Fission of ²⁴³Cm

NUCLEAR REACTIONS ²⁴³Cm(n, F)⁸⁹Rb/⁹¹Sr/⁹¹Y/^91mY/⁹²Sr/⁹³Sr/⁹⁴Sr/⁹⁴Y/⁹⁵Zr/⁹⁵Nb/⁹⁷Zr/⁹⁷Nb/⁹⁸Nb/^98mNb/⁹⁹Tc/^99mTc/⁹⁹Mo/¹⁰¹Mo/¹⁰¹Tc/¹⁰²Tc/^102mTc/¹⁰³Tc/¹⁰³Ru/¹⁰⁴Tc/¹⁰⁵Tc/¹⁰⁵Ru/¹⁰⁵Rh/¹⁰⁶Tc/¹⁰⁷Ru/¹⁰⁷Rh/¹⁰⁸Rh/¹⁰⁹Rh/¹¹²Ag/¹¹⁵In/^115mIn/¹²⁷Sb/¹²⁸Sn/¹²⁸Sb/^128mSb/¹²⁹Sb/¹³⁰Sn/^130mSn/¹³⁰Sb/^130mSb/¹³¹Sb/¹³¹Te/^131mTe/¹³¹I/¹³²Sb/^132mSb/¹³²Te/¹³²I/¹³³I/¹³⁴I/^134mI/¹³⁵I/¹³⁵Xe/^135mXe/¹³⁶I/^136mI/¹³⁶Cs/¹³⁸Xe/¹³⁹Xe/¹³⁹Cs/¹³⁹Ba/¹⁴⁰Cs/¹⁴⁰Ba/¹⁴⁰La/¹⁴¹Ba/¹⁴²Ba/¹⁴³Ce/¹⁴⁴La/¹⁴⁵Ce/¹⁴⁶Ce/¹⁴⁷Nd/¹⁵¹Pm, E=thermal; measured Eγ, Iγ following fission; deduced residual cumulative yields.

doi: 10.1103/PhysRevC.34.722

1987PF03

Z.Phys. A327, 163 (1987)

B.Pfeiffer, K.-L.Kratz

On the Correspondence between Rotational Bands in the Mass Regions A ≈ 100 and A ≈ 150

NUCLEAR STRUCTURE ^{98,99,100,102}Sr, ^{100,101,102,103,104}Zr, ^{102,103,104,105,106}Mo, ^150,152Nd, ^152,154Sm, ^154,156Gd, ^151,153Pm, ^153,155Eu; analyzed rotational bands; deduced subshell closure effects, level systematics. Projection method.

1987RA09

Nucl.Instrum.Methods Phys.Res. B24/25, 501 (1987)

S.Ram, N.L.Singh, S.K.Bose, J.Rama Rao

Absolute Yields of Some Fission Products in the Fast Neutron Induced Fission of ²³⁸U

NUCLEAR REACTIONS ²³⁸U(n, F)⁹⁹Mo/¹¹⁵Cd/¹¹⁷Cd/^117mCd/¹²⁶Sb/¹²⁸Sb/¹³¹Te/^131mTe/¹⁴⁰Ba/¹⁴¹Ce/¹⁵¹Pm/¹⁵⁷Eu, E=thermal; measured fission product yields. Plastic track detector.

doi: 10.1016/0168-583X(87)90694-X

1989II01

J.Phys.Soc.Jpn. 58, 3143 (1989)

H.Iimura, T.Seo, S.Yamada

Angular Correlations on γ-γ Cascades in the Decay of ¹⁵¹Nd

RADIOACTIVITY ¹⁵¹Nd(β^-) [from ¹⁵⁰Nd(n, γ)]; measured γγ(θ). ¹⁵¹Pm deduced levels, J, π, δ(E2/M1). Enriched target, Ge(Li) detectors.

1989MA10

Nucl.Phys. A491, 433 (1989)

M.Matsuzaki

Signature-Dependent Effects of Gamma Vibration on E2 Transitions in Rotating Odd-A Nuclei

NUCLEAR STRUCTURE ¹⁴⁵Cs, ¹⁴⁷La, ¹⁴⁹Pr, ¹⁵¹Pm, ¹⁵³Eu, ¹⁵⁵Tb, ¹⁵⁷Ho, ¹⁵⁹Tm, ¹⁶¹Lu; calculated B(E2) ratios. Quasiparticle-vibration coupling.

doi: 10.1016/0375-9474(89)90577-0

1989RA17

At.Data Nucl.Data Tables 42, 189 (1989)

P.Raghavan

Table of Nuclear Moments

COMPILATION Z=1-99; compiled μ, electric quadrupole moments.

doi: 10.1016/0092-640X(89)90008-9

1989SO08

Phys.Rev. C40, 1530 (1989)

P.C.Sood, R.K.Sheline

Evidence for Reflection Asymmetric Shape in the Nucleus ₆₁¹⁵¹Pm₉₀

NUCLEAR STRUCTURE ¹⁵¹Pm; analyzed levels, B(λ), other level properties. ¹⁵⁵Er; analyzed levels; deduced evidence for octupole shape.

doi: 10.1103/PhysRevC.40.1530

1990UR01

Phys.Lett. 247B, 238 (1990)

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

High Spin Parity Doublets in the Nucleus ¹⁵¹Pm

NUCLEAR REACTIONS ¹⁵⁰Nd(α, 2np), E=68 MeV; measured γγ-coin. ¹⁵¹Pm deduced levels, J, π, B(λ), band structure, deformation features.

doi: 10.1016/0370-2693(90)90889-E

1990VE14

Phys.Rev. C42, R1183 (1990)

W.J.Vermeer, M.K.Khan, A.S.Mowbray, J.B.Fitzgerald, J.A.Cizewski, B.J.Varley, J.L.Durell, W.R.Phillips

Octupole Correlation Effects in ¹⁵¹Pm

NUCLEAR REACTIONS ¹⁵⁰Nd(α, 2np), E=35 MeV; measured Eγ, Iγ, γγ-coin. ¹⁵¹Pm deduced levels, J, π, ICC, γ-multipolarity.

doi: 10.1103/PhysRevC.42.R1183

1993AF01

J.Phys.(London) G19, L143 (1993); Erratum J.Phys.(London) G20, 511 (1994)

A.V.Afanasiev

Evidence for the Existence of Reflection Asymmetric Shape at High Spin in the Odd-Proton ¹⁵¹Pm, ¹⁵³Eu Nuclei

NUCLEAR STRUCTURE ¹⁵¹Pm, ¹⁵³Eu, ²²³Th; analyzed high spin level data. ¹⁵¹Pm, ¹⁵³Eu deduced reflection asymmetric shape evidence.

doi: 10.1088/0954-3899/19/9/003

1993NO01

Z.Phys. A344, 277 (1993)

D.Nosek, R.K.Sheline, P.C.Sood, J.Kvasil

Microscopic Structures of Parity Doublets in the ¹⁵¹Pm, ¹⁵³Eu and ¹⁵⁵Eu Nuclei

NUCLEAR STRUCTURE ¹⁵¹Pm, ^153,155Eu; calculated levels; deduced octupole correlations role. Quasiparticle-phonon model Hamiltonian.

1993RA03

Phys.Rev. C47, 1990 (1993)

A.K.Rath, C.R.Praharaj, S.B.Khadkikar

Signature Effects in Some N = 90 Odd-Z Rare-Earth Nuclei

NUCLEAR STRUCTURE ¹⁴⁷La, ¹⁴⁹Pr, ¹⁵¹Pm; calculated levels, Eγ, B(λ), band structure deduced signature inversion features. Axially symmetric deformed configuration mixing, angular momentum projection.

doi: 10.1103/PhysRevC.47.1990

1995AF01

Phys.Rev. C51, 1259 (1995)

A.V.Afanasjev, I.Ragnarsson

Existence of Intrinsic Reflection Asymmetry at Low Spin in Odd and Odd-Odd Mass Nuclei in the Pm/Eu Region

NUCLEAR STRUCTURE ¹⁵³Eu, ¹⁵³Sm; calculated single nucleon orbitals. ¹⁵¹Pm, ^153,155Eu, ¹⁵³Sm, ¹⁵⁵Gd; calculated octupole-driving orbitals, polarization energies. ¹⁵¹Pm, ^153,155Eu; calculated decoupling parameters. Static intrinsic reflection asymmetry.

doi: 10.1103/PhysRevC.51.1259

1995DE13

Nucl.Phys. A589, 17 (1995)

V.Yu.Denisov, A.Ya.Dzyublik

Collective States of Even-Even and Odd Nuclei with β₂, β₃, ..., β(N) Deformations

NUCLEAR STRUCTURE ^144,146Ba, ¹⁴⁶Ce, ^146,148,150Nd, ¹⁵¹Pm, ¹⁵⁰Sm, ^220,222Rn, ^217,219,221Fr, ^{218,219,220,221,222,223,224,225,226,227,228}Ra, ^{219,223,225,227}Ac, ^{220,221,222,223,224,225,226,228,229}Th; calculated levels, B(λ) ratios. Extended generalization of the Davydov-Chaban model.

doi: 10.1016/0375-9474(95)00075-C

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

2003SH38

Int.J.Mod.Phys. E12, 683 (2003)

Sh.Sharipov, M.J.Ermamatov

About Excited States of Deformable Non-Axial Odd Nuclei

NUCLEAR STRUCTURE ¹⁵¹Pm, ^161,163Dy, ¹⁶⁷Er; calculated high-spin levels, B(E2), collective features. Comparison with data.

doi: 10.1142/S0218301303001545

2004AD41

Phys.Rev. C 70, 064318 (2004)

G.G.Adamian, N.V.Antonenko, R.V.Jolos, T.M.Shneidman

Cluster interpretation of parity doublet rotational bands in odd-mass nuclei

NUCLEAR STRUCTURE ^151,153Pm, ^153,155Eu, ^{221,223,225,227}Ra, ^223,225,227Ac, ^223,229,231Th, ²³¹Pa, ²³³U; calculated rotational bands level energies; ^{221,223,225,227}Ra, ^223,225,227Ac, ^223,225Th, ²²⁹Pa; calculated dipole and quadrupole moments; deduced cluster features. Cluster model, comparisons with data.

doi: 10.1103/PhysRevC.70.064318

2005ST24

At.Data Nucl.Data Tables 90, 75 (2005)

N.J.Stone

Table of nuclear magnetic dipole and electric quadrupole moments

NUCLEAR MOMENTS Z=0-99; A=1-255; compiled μ, electric quadrupole moments.

COMPILATION Z=0-99; A=1-255; compiled μ, electric quadrupole moments.

doi: 10.1016/j.adt.2005.04.001

2017WA10

Chin.Phys.C 41, 030003 (2017)

M.Wang, G.Audi, F.G.Kondev, W.J.Huang, S.Naimi, X.Xu

The AME2016 atomic mass evaluation (II). Tables, graphs and references

ATOMIC MASSES A=1-295; compiled, evaluated atomic masses data.

doi: 10.1088/1674-1137/41/3/030003