References quoted in the ENSDF dataset: 167HO ADOPTED LEVELS, GAMMAS

19 references found.

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

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1955HA45

Phys.Rev. 98, 688 (1955)

T.H.Handley, W.S.Lyon, E.L.Olson

Holmium-167

doi: 10.1103/PhysRev.98.688

1960WI10

Phys.Rev. 118, 242 (1960)

R.G.Wille, R.W.Fink

Activation Cross Sections for 14.8 MeV Neutrons and Some New Radioactive Nuclides in the Rare Earth Region

NUCLEAR STRUCTURE ¹⁶⁹Er, ¹⁶⁸Ho, ¹⁶⁷Ho, ¹⁶⁷Dy, ¹⁶⁵Dy, ¹⁶⁵Er, ¹⁶³Tb, ¹⁷⁴Lu, ¹⁷³Er, ¹⁷⁴Tm, ¹⁷⁶Lu, ¹⁷⁵Yb, ¹⁷⁶Tm, ¹⁷⁷Yb, ¹⁵²Pm, ¹⁵²Eu, ¹⁵³Sm, ¹⁵⁴Pm, ¹⁵⁰Eu, ¹⁵¹Nd, ¹⁴⁹Nd, ¹⁵⁷Sm, ¹⁵⁹Gd, ¹⁶¹Gd, ¹³³Ba, ¹³⁶Cs, ¹⁴⁰La, ¹⁴⁰Pr, ¹³⁹Ba, ¹³⁹Ce, ¹⁴¹Ce, ¹³⁵Ba, ¹³⁸Cs, ¹³⁷Ba, ¹⁴⁷Nd, ¹⁴⁵Ce, ¹⁴³Sm, ¹⁴⁸Pr, ¹⁴²La, ¹⁴¹Nd, ¹⁴²Pr, ¹⁴³Ce; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.118.242

1970RI02

Z.Phys. 231, 10 (1970)

P.Ring, R.Beck, H.J.Mang

On the Application of the Hartree-Fock-Bogolyubov-Equations to a Microscopic Theory of Nuclear Rotations

NUCLEAR STRUCTURE ¹⁶⁷Ho, ¹⁷⁰Hf; calculated levels. Hartree-Fock-Bogolyubov theory.

1977TU01

Z.Phys. A280, 309 (1977)

T.Tuurnala, R.Katajanheimo, E.Hammaren

States of ¹⁶⁷Ho from the Decay of Neutron Rich Nuclide ¹⁶⁷Dy

RADIOACTIVITY ¹⁶⁷Dy; measured T_1/2, Eβ, γγ-, βγ-coin, Eγ, Iγ, γ(t), I(ce); deduced Q, ICC. ¹⁶⁷Ho deduced levels, K, J, π, λ, B(λ).

1979LO02

Nucl.Phys. A315, 90 (1979)

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

Levels in ^167,169Ho Populated in the (t, α) Reaction

NUCLEAR REACTIONS ^168,170Er(polarized t, α), E=17 MeV; measured σ(Eα, θ), Ay(Eα, θ). ^167,169Ho deduced levels, J, π. Nilsson assignments. Enriched targets.

doi: 10.1016/0375-9474(79)90635-3

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.

1984KR06

Nucl.Phys. A417, 419 (1984)

J.Krumlinde, P.Moller

Calculation of Gamow-Teller β-Strength Functions in the Rubidium Region in the RPA Approximation with Nilsson-Model Wave Functions

NUCLEAR STRUCTURE ²⁰⁸Pb, ¹⁴⁴Sm; calculated β^--decay Gamow-Teller strength function; deduced interaction strength for RPA. ^{159,161,165,167,169}Ho, ¹⁶¹Gd, ¹⁶³Er, ^167,175Yb, ¹⁷⁹W, ¹⁸¹Os; calculated transition matrix elements. ^{89,91,93,95,97,99}Sr; calculated potential energy surfaces. ^{89,91,93,95,97,99}Rb; calculated β^--decay Gamow-Teller strength function. RPA, Nilsson basis, BCS pairing treatment.

doi: 10.1016/0375-9474(84)90406-8

1990NA14

Nucl.Phys. A512, 61 (1990)

W.Nazarewicz, M.A.Riley, J.D.Garrett

Equilibrium Deformations and Excitation Energies of Single-Quasiproton Band Heads of Rare-Earth Nuclei

NUCLEAR STRUCTURE ^{148,150,152,154,156,158,160}Sm, ^{150,152,154,156,158,160,162,164,166}Gd, ^{152,154,156,158,160,162,164,166,168}Dy, ^{154,156,158,160,162,164,166,168,170}Er, ^{154,156,158,160,162,164,166,168,170,172,174,176,178,180}Yb, ^{158,160,162,164,166,168,170,172,174,176,178,180,182}Hf, ^{164,166,168,170,172,174,176,178,180,182,184,186,188}W, ^{170,172,174,176,178,180,182,184,186,188,190,192,194}Os, ^{151,153,155,157,159,161}Eu, ^{153,155,157,159,161,163,165}Tb, ^{153,155,157,159,161,163,165,167,169,171}Ho, ^{157,159,161,163,165,167,169,171,173}Tm, ^{161,163,165,167,169,171,173,175,177}Lu, ^{167,169,171,173,175,177,179,181,183,185}Ta, ^{173,175,177,179,181,183,185,187,189}Re; calculated equilibrium deformations. Shell correction method, average Woods-Saxon potential, monopole pairing residual interaction.

doi: 10.1016/0375-9474(90)90004-6

1991BE31

Phys.Lett. 267B, 431 (1991)

B.Belgoumene, J.Dudek, T.Werner

A New Realisation of the Realistic Average Field Approach with Density-Dependent Spin-Orbit Term

NUCLEAR STRUCTURE N=83, Z=51; ²⁰⁸Pb, ¹⁴⁶Gd; calculated single particle excitations. ^{157,159,161,163,165,167,169,171,173}Ho; calculated proton-quasiparticle levels. Realistic average field, density-dependent spin-orbit term.

doi: 10.1016/0370-2693(91)90889-X

1994ZE06

Phys.Rev. C50, 746 (1994)

J.Y.Zeng, Y.A.Lei, T.H.Jin, Z.J.Zhao

Blocking Effect and Odd-Even Differences in the Moments of Inertia of Rare-Earth Nuclei

NUCLEAR STRUCTURE ^155,157,159Eu, ^{157,159,161,163}Tb, ^{159,161,163,165,167}Ho, ^{163,165,167,169,171,173}Tm, ^{169,171,173,175}Lu; analyzed moments of inertia odd-even differences. ^160,161,162Dy, ^164,165,166Er, ¹⁷¹Lu, ¹⁷⁰Yb, ¹⁷²Hf; calculated bandhead moments of inertia; deduced blocked levels associated features. Particle-number conserving treatment.

doi: 10.1103/PhysRevC.50.746

2002KA45

J.Nucl.Sci.Technol.(Tokyo) 39, 705 (2002)

T.Katoh, S.Nakamura, K.Furutaka, H.Harada, T.Baba, T.Fujii, H.Yamana

Measurement of Thermal Neutron Capture Cross Section and Resonance Integral of the ^166mHo(n, γ)¹⁶⁷Ho Reaction using a Two-Step Irradiation Technique

NUCLEAR REACTIONS ^166mHo(n, γ), E=thermal; measured capture σ; deduced resonance integral. Two-step irradiation technique.

RADIOACTIVITY ¹⁶⁷Ho(β^-) [from ¹⁶⁶Ho(n, γ)]; measured Eγ, Iγ, T_1/2.

2010SC05

Phys.Rev. C 81, 024316 (2010)

N.Schunck, J.Dobaczewski, J.McDonnell, J.More, W.Nazarewicz, J.Sarich, M.V.Stoitsov

One-quasiparticle states in the nuclear energy density functional theory

NUCLEAR STRUCTURE ¹²¹Sn; calculated quasineutron energies, neutron chemical potential, neutron pairing energy, average neutron pairing gap, total rms radius, axial quadrupole deformation, total quadrupole moment, kinetic energy (for protons and neutrons), total spin-orbit energy, direct Coulomb energy, and total energy. ¹⁶³Tb; calculated quasiproton energies, quadrupole moments and configurations. ¹⁶⁴Dy; calculated Nilsson proton levels as a function of axial quadrupole deformation. ^{155,157,159,161,163,165,167,169,171}Ho; calculated one-quasiproton bandhead energies with SkP, SIII and SLy4 Skyrme functionals. ^{159,161,163,165,167}Ho, ^157,159,161Lu, ^161,163Ta; calculated equilibrium deformation of the 3/2[402] blocked configuration with the SLy4 interaction. All calculations performed in the framework of nuclear density functional theory in the Skyrme-Hartree-Fock-Bogoliubov variant. Comparison with experimental data.

doi: 10.1103/PhysRevC.81.024316

2017TA12

Nucl.Phys. A964, 1 (2017)

E.Tabar, A.Kuliev

Microscopic investigation of the low-lying magnetic dipole transitions in the odd-mass ^155-169Ho isotopes

NUCLEAR STRUCTURE ^{155,157,159,161,163,165,167,169}Ho; calculated low-lying magnetic dipole strength (B(M1)), quadrupole deformation parameter using RI-QPNM (Rotational Invariant Quasiparticle Phonon Nuclear Model); compared to neighbouring even-even nuclei; deduced giant M1 resonance for Ho nuclei at energies 7-15 MeV.

doi: 10.1016/j.nuclphysa.2017.04.039

2017TA13

Chin.Phys.C 41, 074101 (2017)

E.Tabar, H.Yakut, A.A.Kuliev, H.Quliyev, G.Hocsgor

Magnetic moments and g-factors in odd-A Ho isotopes

NUCLEAR STRUCTURE ^{155,157,159,161,163,165,167,169}Ho; calculated ground-state structures, moments of inertia and gyromagnetic ratios, B(M1), magnetic moments, deformations. Quasiparticle Phonon Nuclear Model (QPNM), comparison with available data.

doi: 10.1088/1674-1137/41/7/074101

2018BU13

Phys.Rev. C 98, 024301 (2018)

D.Bucurescu, N.V.Zamfir

Empirical signatures of shape phase transitions in nuclei with odd nucleon numbers

NUCLEAR STRUCTURE ^{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}Ba, ^{133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154}La, ^{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}Ce, ^{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}Pr, ^{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, ^{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}Pm, ^{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}Sm, ^{135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,167}Eu, ^{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}Gd, ^{137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170}Tb, ^{138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169}Dy, ^{140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171}Ho, ^{142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172}Er, ^{146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173}Tm, ^{149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174}Yb, ^{72,73,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,98,100}Kr, ^{75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,98,100}Rb, ^{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, ^{80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106}Y, ^{80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107}Zr, ^{84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110}Nb, ^{84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110}Mo, ^{87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,112}Tc, ^{88,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,111,112,113}Ru, ^{89,91,92,93,94,95,96,97,98,99,100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115}Rh; analyzed nuclear level density parameter a for back-shifted Fermi gas model formula (BSFG), S(2n), mean square charge radii, isotope shifts, correlation between the energy ratios and the relative energies for the favored band of the νi_13/2 structures in the odd-mass nuclei for even Z=64-76. ^152,154,156Tb; analyzed correlation between relative excitation energies of the favored sequence of the (πh_11/2, νi_13/2) structure. Discussed nuclear level density at low excitation energies as indicator of first order shape phase transition in nuclei.

doi: 10.1103/PhysRevC.98.024301

2018MUZZ

Atlas of Neutron Resonances, 6th ed. Vol.2, Resonance Properties and Thermal Cross Sections Z = 61-102, Elsevier, Amsterdam (2018)

S.Mughabghab

COMPILATION Z=61-102; compiled experimental nuclear reaction data, σ, resonance parameters.

2019NO05

Phys.Rev. C 99, 064306 (2019)

N.M.Nor, N.-A.Rezle, K.-W.Kelvin-Lee, M.-H.Koh, L.Bonneau, P.Quentin

Consistency of two different approaches to determine the strength of a pairing residual interaction in the rare-earth region

NUCLEAR STRUCTURE ^{156,157,158,159,160}Sm, ^159,161Eu, ^{160,161,162,163,164,165,166}Gd, ^{161,163,165,167}Tb, ^{162,163,164,165,166,167,168}Dy, ^167,169Ho, ^{168,169,170,171,172}Er, ^169,171,173Tm, ^{170,171,172,173,174,175,176,177,178}Yb, ^177,179Lu, ^{176,177,178,179,180,181,182}Hf, ¹⁷⁹Ta, ¹⁸⁰W; analyzed odd-even staggering of binding energies, and moments of inertia of the first 2+ states of even-even nuclei; calculated neutron and proton pairing residual interaction strengths, binding energies, and moments of inertia. Self-consistent Hartree-Fock plus BCS framework, with the implementation of a self-consistent blocking in the case of odd-mass nuclei, using Skyrme SIII parametrization. Comparison with experimental values, and with other theoretical predictions.

doi: 10.1103/PhysRevC.99.064306

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

2023PO08

Phys.Rev. C 107, 064614 (2023)

F.Pogliano, A.C.Larsen, S.Goriely, L.Siess, M.Markova, A.Gorgen, J.Heines, V.W.Ingeberg, R.G.Kjus, J.E.L.Larsson, K.C.W.Li, E.M.Martinsen, G.J.Owens-Fryar, L.G.Pedersen, S.Siem, G.S.Torvund, A.Tsantiri

Experimentally constrained ^{165, 166}Ho(n, γ) rates and implications for the s process

NUCLEAR REACTIONS ¹⁶⁴Dy(α, pγ)¹⁶⁷Ho, E=26 MeV; measured Ep, Ip, Eγ, Iγ, pγ-coin. ¹⁶⁷Ho; deduced nuclear level density (NLD) and γ-ray strength function, resonance components of the GSF (Giant Dipole Resonance, Pigmy Dipole Resonance, M1 scissors resonance), upward scissor resonance strength. ^165,166Ho(n, γ), E=0.001-10 MeV; calculated σ(E) using obtained NLD and GSF (for ¹⁶⁷Ho from present work, for ¹⁶⁶Ho - from 2023PO02), Maxwellian-averaged σ(E) MACS (kT<105 keV). Oslo method type of analysis. Comparison with other experimental data and TALYS calculations. Comparison of obtained MACS with JINA REACLIB, BRUSLIB and KADONIS data. AGB nucleosynthesis predictions with STARERVOL code using obtained MACS. Oslo SCintillator ARray (OSCAR) and the Silicon Ring (SiRi) detector arrays at MC-35 Scanditronix cyclotron.

doi: 10.1103/PhysRevC.107.064614