References quoted in the ENSDF dataset: 165HO ADOPTED LEVELS, GAMMAS

158 references found.

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

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1935SC02

Naturwissenschaften 23, 69 (1935)

H.Schuler, T.Schmidt

1949GO21

Phys.Rev. 75, 1969 (1949)

M.Goeppert-Mayer

On Closed Shells in Nuclei.II

NUCLEAR STRUCTURE ¹H, ⁷Li, ¹¹B, ¹⁵N, ¹⁹F, ²³Na, ²⁷Al, ³¹P, ³⁵Cl, ³⁹K, ⁴⁵Sc, ⁵¹V, ⁵⁵Mn, ⁵⁹Co, ⁶³Cu, ⁶⁹Ga, ⁷⁵As, ⁷⁹Rb, ⁸⁹Y, ⁹³Nb, Tc, Rh, ¹⁰⁷Ag, ¹¹³In, ¹²¹Sb, ¹²⁷I, ¹³³Cs, ¹³⁹La, ¹⁴¹Pr, Pm, ¹⁵¹Eu, ¹⁵⁹Tb, ¹⁶⁵Ho, Tm, ¹⁷⁵Lu, ¹⁸¹Ta, ¹⁸⁵Re, ¹⁹¹Ir, ¹⁹⁷Au, ²⁰³Tl, ²⁰⁹Bi; analyzed shell structure; deduced systematics, shell model.

doi: 10.1103/PhysRev.75.1969

1955BA04

Proc.Phys.Soc.(London) 68A, 1090 (1955)

J.M.Baker, B.Bleaney

The Nuclear Magnetic Moment of Holmium 165

doi: 10.1088/0370-1298/68/11/123

1956PO16

Z.Naturforsch. 11a, 143 (1956)

W.Porschen, W.Riezler

Sehr langlebige naturliche α-Strahler

1957BE39

Optika i Spektroskopiya 3, 322 (1957); Nucl.Sci.Abstr. 12, 1317, Abstr. 11158 (1958)

V.B.Belyanin

Hyperfine Structure of Spectral Lines of Holmium

1958BA35

Proc.Roy.Soc.(London) 245A, 156 (1958); See Also 55Ba04 (Ho), 55Ba08 (Pr)

J.M.Baker, B.Bleaney

Paramagnetic Resonance in Some Lanthanon Ethyl Sulphates

1958BE85

Optika i Spektroskopia 5, 340 (1958); Chem.Abstr. 53, 12842g (1959)

V.B.Belyanin

Magnetic Moment of Holmium

1958HU17

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

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

Paramagnetic Resonance in Rare Earth Trichlorides

1958KA10

Bull.Am.Phys.Soc. 3, No.3, 209, S8 (1958)

J.V.Kane, R.Sher, E.V.Weinstock

States in Ho¹⁶⁵ Formed in the β^- Decay by Dy¹⁶⁵

1959CR80

Thesis, Stanford University (1959); Dissertation Abstr. 19, 2990 (1959)

F.P.Cranston

Low-Lying Energy States of Holmium-165 and Thulium-171

1962FR14

Phys.Rev. 127, 2058 (1962)

A.J.Freeman, R.E.Watson

Theoretical Investigation of Some Magnetic and Spectroscopic Properties of Rare-Earth Ions

NUCLEAR STRUCTURE ¹⁴³Nd, ¹⁴⁷Sm, ¹⁴¹Pr, ¹⁷³Yb, ¹⁶⁷Er, ¹⁶⁵Ho; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.127.2058

1962GO20

Naturwissenschaften 49, 101 (1962)

L.S.Goodman, H.Kopfermann, K.Schlupmann

NUCLEAR STRUCTURE ¹⁶⁵Ho; measured not abstracted; deduced nuclear properties.

1962LI06

Nuclear Phys. 32, 151 (1962); Recalculation of Earlier Data

I.Lindgren

Nuclear Magnetic Moments in the Rare Earth Region

doi: 10.1016/0029-5582(62)90326-7

1962WY04

J.Chem.Phys. 37, 1807 (1962); Recalculation of Data of 53Le22(Pr¹⁴¹) and 62Go20(Ho¹⁶⁵)

B.G.Wybourne

NUCLEAR STRUCTURE ¹⁴¹Pr, ¹⁶⁵Ho; measured not abstracted; deduced nuclear properties.

1963BL25

Proc.Intern.Congr. Quantum Electronics, 3rd, Paris, France, (1963); P.Grivet, N.Bloembergen, Ed., Columbia University Press, New York, Vol.I, p.595 (1964)

B.Bleaney

Nuclear Moments of the Lanthanons

NUCLEAR STRUCTURE ¹⁵⁹Tb, ¹⁵⁵Gd, ¹⁵⁷Gd, ¹⁶¹Dy, ¹⁷⁰Tm, ¹⁶⁵Ho, ¹⁶⁶Tm, ¹⁶³Dy, ¹⁴²Pr, ¹⁴⁷Pm, ¹⁴¹Ce, ¹⁴¹Pr; measured not abstracted; deduced nuclear properties.

1964GO09

Z.Physik 178, 235 (1964)

L.S.Goodman, K.Schlupmann

Bestimmung der Kernmomente des Ho¹⁶⁵ Aus der Hyperfeinstruktur des Grundzustandes im Ho I-Spektrum

NUCLEAR STRUCTURE ¹⁶⁵Ho; measured not abstracted; deduced nuclear properties.

1964VA27

Physica 30, 229 (1964)

H.Van Kempen, A.R.Miedema, W.J.Huiskamp

Heat Capacities of the Metals Terbium and Holmium below 1°K

doi: 10.1016/0031-8914(64)90217-4

1967BA27

Arkiv Fysik 34, 495 (1967)

A.Backlin, S.G.Malmskog, H.Solhed

Transitions, Lifetimes and Levels in ¹⁴⁹Pm

NUCLEAR STRUCTURE ¹⁴⁷Nd, ¹⁴⁷Pm, ¹⁴¹Pr, ¹⁴¹Ce, ¹⁹⁹Hg, ¹⁹⁹Au, ¹⁹⁷Au, ¹⁹⁷Hg, ²⁰³Hg, ²⁰³Tl, ¹⁷⁰Tm, ¹⁶⁵Ho, ¹⁶⁵Dy, ¹⁶¹Tb, ¹⁶¹Dy, ¹⁵²Sm, ¹⁵²Eu, ¹⁴⁹Nd, ¹⁷⁰Yb; measured not abstracted; deduced nuclear properties.

1968SU04

J. Opt. Soc. Am. 58, 1519 (1968)

J.Sugar

Nuclear Magnetic Dipole Moment of ¹⁶⁵Ho

NUCLEAR STRUCTURE ¹⁶⁵Ho; measured not abstracted; deduced nuclear properties.

1969KR19

Phys.Rev. 177, 910 (1969)

M.Krusius, A.C.Anderson, B.Holmstrom

Calorimetric Investigation of Hyperfine Interactions in Metallic Ho and Tb

doi: 10.1103/PhysRev.177.910

1970AR02

Nucl.Phys. A143, 315 (1970)

R.Armbruster, Y.Dar, J.Gerber, A.Macher, J.P.Vivien

The Mean Lives of the First Excited States in ¹⁸¹Ta and ¹⁶⁵Ho

NUCLEAR REACTIONS ¹⁸¹Ta, ¹⁶⁵Ho(α, α'γ), Eα = 3.8 MeV; microwave-pulsed beam; measured αce delay. ¹⁸¹Ta, ¹⁶⁵Ho level deduced T_1/2, B(M1), gK, gR.

doi: 10.1016/0375-9474(70)90566-X

1970BLZT

BMBW-FBK-70-09, p.22 (1970)

H.Blunck, J.Braunsfurth, E.Gerdau, W.Hautsch, W.Muller, W.Rath, D.Repsilber, D.Ruter, F.Sabathil, B.Scharnberg, H.Winkler, G.Wittkemper, H.J.Wolf

Experimente der Kernmomentengruppe

RADIOACTIVITY ^105mPd, ^184mW, ^169mTm, ^100mRh, ^134mCs; measured T_1/2.

NUCLEAR MOMENTS ¹⁸⁴W levels measured g.

1972DAYT

Priv.Comm. (1972)

W.Dankwort, J.Ferch, S.Penselin

16-Pole-Interaction in Ho¹⁶⁵ and Dy^161,163

NUCLEAR MOMENTS ^161,163Dy, ¹⁶⁵Ho; measured a, b, c, d. Atomic beam magnetic resonance method.

1972GE21

Z.Phys. 257, 29 (1972)

E.Gerdau, W.Rath, H.Winkler

Determination of Hyperfine Interactions from Partly Resolved Mossbauer Spectra

NUCLEAR REACTIONS ¹⁶⁵Ho(γ, γ), E=94.7 keV; measured Mossbauer effect. ¹⁶⁵Ho level deduced T_1/2. ¹⁷⁸Hf(γ, γ), E=93 keV; measured Mossbauer effect in Fe; deduced hyperfine field.

NUCLEAR MOMENTS ¹³³Cs, ¹⁶⁵Ho levels measured g ratios.

1972HA45

Z.Phys. 252, 421 (1972)

R.A.Haberstroh, T.I.Moran, S.Penselin

Direct Measurement of the Nuclear Magnetic Dipole Moment of Ho¹⁶⁵ with The Atomic Beam Magnetic Resonance Method

NUCLEAR MOMENTS ¹⁶⁵Ho; measured g(J), μ. Atomic-beam magnetic resonance.

1972ME16

Z.Phys. 252, 412 (1972)

G.Merzyn, S.Penselin, G.Wolber

The Hyperfine Structure of the Ground State of Ho¹⁶⁵

NUCLEAR MOMENTS ¹⁶⁵Ho; measured a, b, c, d. Atomic-beam magnetic resonance.

1974DA10

Z.Phys. 267, 229 (1974)

W.Dankwort, J.Ferch, H.Gebauer

Hexadecapole Interaction in the Atomic Ground State of ¹⁶⁵Ho

NUCLEAR MOMENTS ¹⁶⁵Ho; measured quadrupole moment, ±, π. Atomic beam.

1974DA11

Z.Phys. 267, 239 (1974)

W.Dankwort, J.Ferch

Reevaluation of the Atomic g(J)-Factor and the Nuclear g(I)-Factor Of ¹⁶⁵Ho

NUCLEAR MOMENTS ¹⁶⁵Ho; analyzed g.

1974EB03

Phys.Lett. 53B, 48 (1974)

P.Ebersold, B.Aas, W.Dey, R.Eichler, J.Hartmann, H.J.Leisi, W.W.Sapp

Spectroscopic Quadrupole Moment of Holmium from Pionic X-Ray Measurement

NUCLEAR MOMENTS, Mesic-Atoms ¹⁶⁵Ho; measured E(X-ray) in pionic Ho; deduced quadrupole moment.

doi: 10.1016/0370-2693(74)90340-2

1975PO03

Phys.Rev.Lett. 34, 492 (1975)

R.J.Powers, F.Boehm, P.Vogel, A.Zehnder, T.King, A.R.Kunselman, P.Roberson, P.Martin, G.H.Miller, R.E.Welsh, D.A.Jenkins

Precise Determination of E2 and E4 Moments in ¹⁶⁵Ho from Muonic X Rays

NUCLEAR MOMENTS ¹⁶⁵Ho; analyzed hfs data; deduced quadrupole moment.

doi: 10.1103/PhysRevLett.34.492

1976PO05

Nucl.Phys. A262, 493 (1976)

R.J.Powers, F.Boehm, P.Vogel, A.Zehnder, T.King, A.R.Kunselman, P.Roberson, P.Martin, G.H.Miller, R.E.Welsh, D.A.Jenkins

Muonic X-Ray Study of the Charge Distribution of ¹⁶⁵Ho

ATOMIC PHYSICS ¹⁶⁵Ho(μ^-, X-ray); measured E(X-ray), I(X-ray). ¹⁶⁵Ho deduced quadrupole moment, hexadecapole moment, nuclear charge distribution.

NUCLEAR MOMENTS ¹⁶⁵Ho; measured muonic X-rays, quadrupole moment, hexadecapole moment, nuclear charge distribution.

doi: 10.1016/0375-9474(76)90511-X

1977GA08

Phys.Rev. C15, 2219 (1977)

A.Gaigalas, D.McLoughlin, S.Raboy, C.C.Trail, E.Deci, R.Sutton, R.A.Carrigan

¹⁶⁵Ho by Muonic X Rays

ATOMIC PHYSICS, Mesic-Atoms ¹⁶⁵Ho; measured K X-ray, L X-ray in muonic atoms.

doi: 10.1103/PhysRevC.15.2219

1978CH37

Hyperfine Interactions 4, 145 (1978)

S.C.Cheng, A.Shor, B.Olaniyi, G.Dugan, W.Patton, C.S.Wu, M.Y.Chen

The Study of Quadrupole Hyperfine Interactions in Pionic Atoms of ¹⁸¹Ta and ¹⁶⁵Ho

ATOMIC PHYSICS, Mesic-Atoms ¹⁸¹Ta, ¹⁶⁵Ho; measured pionic hfs; deduced effective, spectroscopic quadrupole moments.

NUCLEAR MOMENTS ¹⁸¹Ta, ¹⁶⁵Ho; measured pionic hfs; deduced effective, spectroscopic quadrupole moments.

1978EB01

Nucl.Phys. A296, 493 (1978)

P.Ebersold, B.Aas, W.Dey, R.Eichler, H.J.Leisi, W.W.Sapp, F.Scheck

Monopole and Quadrupole Strong Interaction Effects in Pionic Atoms of ¹⁷⁵Lu and ¹⁶⁵Ho

NUCLEAR MOMENTS ¹⁶⁵Ho; measured quadrupole moment. Generalized moments of neutron distribution.

ATOMIC PHYSICS, Mesic-Atoms ¹⁷⁵Lu, ¹⁶⁵Ho(π^-, X-ray); measured pionic X-rays; deduced monopole, quadrupole interactions, strong-interaction contribution.

doi: 10.1016/0375-9474(78)90087-8

1980BO26

Nucl.Instrum.Methods 178, 209 (1980)

G.L.Borchert, P.G.Hansen, B.Jonson, H.L.Ravn, O.W.B.Schult, P.Tidemand-Petersson, and the ISOLDE Collaboration

A Curved Crystal Spectrometer for Measurements of Small K X-Ray Energy Shifts

ATOMIC PHYSICS ¹⁰³Rh, ¹⁰³Pd, ^131,132Cs, ¹⁵⁹Tb, ¹⁵⁹Dy, ¹⁶⁵Ho, ¹⁶⁵Er, ¹⁹⁷Au, ¹⁹⁷Hg; measured E(K X-ray) differences. Rh, Xe, Tb, Ho, Au deduced hyperfine shift, unresolved satellite, electron configuration effects. DuMond curved crystal spectrometer.

1980BU16

Phys.Rev.Lett. 45, 1667 (1980)

M.Buenerd, D.Lebrun, Ph.Martin, P.de Saintignon, C.Perrin

Evidence for Deformation Effect on the Giant Monopole Resonance

NUCLEAR REACTIONS ¹⁴⁰Ce, ^144,150,152Sm, ¹⁵⁹Tb, ¹⁶⁵Ho, ¹⁶⁹Tm, ¹⁸¹Ta, ¹⁹⁷Au, ²⁰⁸Pb, ²³²Th(³He, ³He'), E=108.5 MeV; measured σ(E(³He), θ). ¹⁴⁰Ce, ^144,150,152Sm, ¹⁵⁹Tb, ¹⁶⁵Ho, ¹⁶⁹Tm, ¹⁸¹Ta, ¹⁹⁷Au, ²⁰⁸Pb, ²³²Th deduced giant monopole resonance, Γ, EWSR strengths, coupling to giant quadrupole vibrations.

doi: 10.1103/PhysRevLett.45.1667

1980DA08

Phys.Rev. C21, 2253 (1980)

W.W.Daehnick, J.D.Childs, Z.Vrcelj

Global Optical Model Potential for Elastic Deuteron Scattering from 12 to 90 MeV

NUCLEAR REACTIONS ²⁷Al, ²⁸Si, ³¹P, ³²S, ⁴⁰Ar, ⁴⁰Ca, ^52,53Cr, ⁵⁶Fe, ⁸⁸Sr, ⁹³Nb, ¹⁰³Rh, ¹¹⁵In, ¹³⁸Ba, ¹⁴⁰Ce, ¹⁶⁵Ho, ¹⁸¹Ta, ¹⁹⁷Au, ^206,208Pb, ²³²Th(d, d), E=11.8 MeV; ²⁷Al, ⁴⁸Ca, ⁵¹V, ⁵²Cr, ^54,56Fe, ⁵⁹Co, ^58,62,64Ni, ⁶⁸Zn, ⁹³Nb, ¹⁰⁰Mo, ¹⁰⁵Pd, ¹¹²Cd, ¹¹⁵In, ^112,120,124Sn, ²⁰⁸Pb, ²⁰⁹Bi, ²³²Th(d, d), E=17 MeV; ⁴⁰Ca, ^48,49,50Ti, ⁵¹V, ⁵²Cr, ⁵⁴Fe, ⁶⁰Ni, ⁶³Cu, ^{90,91,92,94,96}Zr, ⁹³Nb(d, d), E=34 MeV; ²⁷Al, ²⁸Si, ³²S, ⁴⁰Ar, ^48,50Ti, ⁵⁴Fe, ^58,64Ni, ⁸⁹Y, ⁹³Nb, ¹⁰³Rh, ¹⁴⁰Ce, ¹⁸¹Ta, ¹⁹⁷Au, ²⁰⁸Pb, ²⁰⁹Bi, ²³⁸U(d, d), E=52 MeV; analyzed σ(θ). ⁵²Cr, ⁵⁶Fe, ⁶⁰Ni, ⁹⁰Zr, ¹²²Sn, ¹⁹⁷Au(d, d), E=15 MeV; ⁴⁰Ca, ⁵⁶Fe, ⁹⁰Zr, ¹²⁰Sn, ²⁰⁸Pb(d, d), E=30 MeV; ⁵⁸Ni, ²⁰⁸Pb(d, d), E=79.5 MeV; analyzed P(θ); deduced global optical model, real, imaginary volume integrals, rms radii.

doi: 10.1103/PhysRevC.21.2253

1980GU18

Phys.Rev. C22, 1308 (1980)

E.M.de Guerra, S.Kowalski

Current Densities in the Projected Hartree-Fock Approach. II. Transverse Form Factors

NUCLEAR STRUCTURE ¹⁵⁹Tb, ¹⁶⁵Ho, ¹⁶⁶Er, ¹⁸¹Ta; calculated elastic, inelastic form factors, B(λ). Effective Hamiltonian, density matrix, projected Hartree-Fock method.

doi: 10.1103/PhysRevC.22.1308

1980KO11

Nucl.Phys. A340, 221 (1980)

J.Koch, F.Scheck

Quadrupole Interactions in Pionic and Kaonic Atoms

NUCLEAR MOMENTS ¹⁶⁵Ho, ^175,176Lu, ¹⁸¹Ta, Re; calculated pionic, kaonic hfs; deduced strong interaction shifts, widths. Optical potential, nonspherical density distributions.

doi: 10.1016/0375-9474(80)90272-9

1980OLZZ

Diss.Abst.Int. 41B, 246 (1980)

B.H.Olaniyi

Electric Quadrupole Moments and Strong Interaction Effects in Pionic Atoms of ¹⁶⁵Ho, ¹⁷⁵Lu, ¹⁷⁶Lu, ¹⁷⁹Hf and ¹⁸¹Ta

NUCLEAR MOMENTS ¹⁶⁵Ho, ^175,176Lu, ¹⁷⁹Hf, ¹⁸¹Ta; measured pionic X-rays; deduced strong interaction shifts, widths. ¹⁶⁵Ho, ^175,176Lu, ¹⁷⁹Hf, ¹⁸¹Ta deduced quadrupole moments.

1981BA07

Nucl.Phys. A355, 383 (1981)

C.J.Batty, S.F.Biagi, R.A.J.Riddle, B.L.Roberts, G.J.Pyle, G.T.A.Squier, D.M.Asbury, A.S.Clough

Nuclear Quadrupole Deformation Effects on Pionic and Kaonic X-Rays

NUCLEAR MOMENTS In, Ho, ¹⁶⁸Er, Yb, Ta, Bi; measured pionic X-rays, hfs; Ho, Yb, Ta measured kaonic X-rays, hfs; deduced strong interaction shifts, widths. In, Ho, Ta deduced quadrupole moments. Deformed optical model calculations.

doi: 10.1016/0375-9474(81)90534-0

1981DO09

Phys.Rev. A24, 693 (1981)

M.Dost, S.Hoppenau, J.Kising, S.Rohl, P.Schorn

K-Shell Ionization Probability in Close Collisions of 7-12 MeV Protons with Targets of Z = 24-83

NUCLEAR REACTIONS Cr, Fe, Ni, Cu, Zn, Se, Sr, Zr, Mo, Ru, Ag, ¹⁰⁶Cd, ¹¹²Sn, ¹³⁰Te, Ba, Ce, Sm, ¹⁶⁵Ho, ¹⁶⁹Tm, Ta, Pt, ¹⁹⁷Au, Pb, ²⁰⁹Bi(p, p), (p, X), E=7 MeV; measured pp-, p(X-ray)-coin; deduced K-shell ionization probability.

doi: 10.1103/PhysRevA.24.693

1981GU02

Nucl.Phys. A351, 257 (1981)

G.M.Gurevich, L.E.Lazareva, V.M.Mazur, S.Yu.Merkulov, G.V.Solodukhov, V.A.Tyutin

Total Nuclear Photoabsorption Cross Sections in the Region 150 < A < 190

NUCLEAR REACTIONS ¹⁵⁴Sm, ¹⁵⁶Gd, ¹⁶⁵Ho, ¹⁶⁸Er, ¹⁷⁴Yb, ^178,180Hf, ¹⁸¹Ta, ^182,184,186W, ¹⁹⁷Au(γ, X), E=7-20 MeV; measured total σ(E); deduced integrated σ, Lorentz line parameters. ¹⁵⁴Sm, ¹⁵⁶Gd, ¹⁶⁵Ho, ¹⁶⁸Er, ¹⁷⁴Yb, ^178,180Hf, ¹⁸¹Ta, ^182,184,186W, ¹⁹⁷Au deduced deformation β, quadrupole moment, Γ, giant resonance evolution, enriched, natural targets.

doi: 10.1016/0375-9474(81)90443-7

1981SP01

Nucl.Phys. A352, 19 (1981)

D.W.L.Sprung, S.G.Lie, M.Vallieres

Collective Gyromagnetic Ratio from Density Dependent Hartree-Fock Calculations (II). Odd nuclei

NUCLEAR STRUCTURE ¹⁵⁷Gd, ^161,163Dy, ¹⁶⁷Er, ^171,173Yb, ^177,179Hf, ¹⁸³W, ¹⁵⁸Eu, ¹⁵⁹Tb, ¹⁶⁵Ho, ¹⁷⁵Lu, ¹⁸¹Ta, ^185,187Re; calculated collective g(R), moment of inertia. Cranking approximation, Skyrme forces.

doi: 10.1016/0375-9474(81)90556-X

1982BH07

Indian J.Phys. 56A, 283 (1982)

S.Bhuloka Reddy, P.R.L.Sarma, V.Lakshminarayana, K.Subba Rao

Systematics of Penetration Effects of l-Forbidden M1 Transitions

NUCLEAR STRUCTURE ¹⁴³Pr, ¹⁵⁵Gd, ¹⁶¹Dy, ¹⁶⁵Ho, ¹⁶⁹Tm, ¹⁷⁵Lu, ¹⁹¹Os, ¹⁸⁷Ir, ¹⁹⁵Pt, ^193,195Au, ¹⁹³Hg; calculated l-forbidden M1 transition penetration parameters; deduced penetration parameter, hindrance factor empirical relationship. Conversion electron intensity input.

1982BU13

Z.Phys. A307, 193 (1982)

B.Burghardt, S.Buttgenbach, N.Glaeser, R.Harzer, G.Meisel, B.Roski, F.Traber

Hyperfine Structure Measurements in Metastable States of ¹⁶⁵Ho

NUCLEAR MOMENTS ¹⁶⁵Ho; measured hfs; deduced nuclear electric quadrupole moment. ABMR, dye laser.

1982TO17

Pisma Zh.Eksp.Teor.Fiz. 35, 403 (1982); JETP Lett.(USSR) 35, 499 (1982)

S.V.Tolokonnikov, S.A.Fayans

Sum Rules for Dipole Transitions in Finite Systems and the Giant Dipole Resonance in Nuclei

NUCLEAR STRUCTURE ¹⁵⁰Nd, ^152,154Sm, ¹⁵³Eu, ¹⁵⁹Tb, ¹⁶⁰Gd, ¹⁶⁵Ho, ¹⁷⁵Lu, ¹⁸¹Ta, ¹⁸⁶W, ²³²Th, ^235,238U, ²³⁷Np; calculated quadrupole moment vs GDR splitting. A ≤ 250; calculated GDR energy vs mass. Self-consistent theory, finite Fermi systems.

1983BA71

Nucl.Phys. A411, 399 (1983)

C.J.Batty

Hadron-Nucleus Scattering Lengths Derived from Exotic Atom Data

NUCLEAR REACTIONS Li, ⁹Be, ^10,11B, C, O, Mg, ²⁷Al, Si, ³¹P, S, Cl, ⁵⁹Co, Ni, Cu, Ag, Cd, In, Sn, ¹⁶⁵Ho, Yb, Pb, U(K^-, K^-), E not given; ^6,7Li, C, N, ^16,18O, Si, ³¹P, S, Fe, ⁸⁹Y, Zr, Pb(p-bar, p-bar), E not given; analyzed data; deduced hadron-nucleus S-wave scattering lengths.

doi: 10.1016/0375-9474(83)90538-9

1983JE01

Phys.Rev. C27, 697 (1983)

R.H.Jeppesen, M.J.Jakobson, M.D.Cooper, D.C.Hagerman, M.B.Johnson, R.P.Redwine, G.R.Burleson, K.F.Johnson, R.E.Marrs, H.O.Meyer, I.Halpern, L.D.Knutson

Pion-Nucleus Forward Scattering Amplitudes from Total Cross Section Measurements

NUCLEAR REACTIONS ²⁷Al, ⁴⁰Ca, ^63,65Cu, Sn, ¹⁶⁵Ho, Pb(π⁺, π⁺), (π⁺, X), (π^-, π^-), (π^-, X), E=114-215 MeV; measured total σ, attenuation σ; deduced Coulomb distorted forward scattering amplitude real, imaginary parts. Strong absorption model.

doi: 10.1103/PhysRevC.27.697

1983OL03

Nucl.Phys. A403, 572 (1983)

B.Olaniyi, A.Shor, S.C.Cheng, G.Dugan, C.S.Wu

Electric Quadrupole Moments and Strong Interaction Effects in Pionic Atoms of ¹⁶⁵Ho, ¹⁷⁵Lu, ¹⁷⁶Lu, ¹⁷⁹Hf and ¹⁸¹Ta

NUCLEAR MOMENTS ¹⁶⁵Ho, ^175,176Lu, ¹⁷⁹Hf, ¹⁸¹Ta; measured pionic X-ray hfs; deduced monopole strong interaction shifts, widths, quadrupole moments.

doi: 10.1016/0375-9474(83)90623-1

1983PO12

Izv.Akad.Nauk SSSR, Ser.Fiz. 47, 2187 (1983)

Yu.A.Pozdnyakov, K.O.Terenetsky

Modified Boundary Conditions and the Optical Model for Scattering

NUCLEAR REACTIONS Fe, Ni, Ag, ²⁰⁹Bi, ⁵⁹Co, Te, U, ¹⁶⁵Ho(d, d), E=13.6 MeV; calculated phase shifts for different L. Modified boundary conditions, optical model.

1983PR06

J.Phys.(London) C16, L903 (1983)

O.Prakash, M.A.H.McCausland

Free Precession of ¹⁶⁵Ho Nuclei in a Single Crystal of Holmium Iron Garnet

NUCLEAR MOMENTS ¹⁶⁵Ho; measured NMR; deduced Ho moment at inequivalent crystallographic sites. Single HoIG crystal, free precession.

1983RA02

Nucl.Instrum.Methods 205, 259 (1983)

J.Raisanen, R.Hanninen

Heavy Element (Z > 30) Thick-Target Gamma-Ray Yields Induced by 1.7 and 2.4 MeV Protons

NUCLEAR REACTIONS ⁸⁹Y, ^87,86,88Sr, ⁸⁵Rb, ⁷⁹Br, ^74,72,70Ge, ⁶⁹Ga, ⁸⁰Se, ^92,90,94Zr, ⁹³Nb(p, γ), ^69,71Ga, ^74,76Ge, ⁷⁵As, ^77,76,80Se, ^79,81Br, ⁸⁵Rb, ⁹⁴Zr, ^{95,97,96,100,98}Mo, ^{99,101,100,102,104}Ru, ¹⁰³Rh, ^{102,105,108,110,104}Pd, ^109,107Ag, ^{110,111,112,113,114}Cd, ¹¹⁵In, ^123,121Sb, ¹²⁶Te, ¹²⁷I, ¹³³Cs, ^134,135,137Ba, ¹⁴¹Pr, ^{144,146,148,150}Nd, ^{147,148,150,152,154}Sm, ^151,153Eu, ^{154,156,157,152,155,158}Gd, ^162,163,164Dy, ¹⁶⁵Ho, ¹⁶⁹Tm, ^172,173Yb, ^176,175Lu, ^{177,178,179,180}Hf, ¹⁸¹Ta, ^{182,183,184,186}W, ^{194,195,196,198}Pt, ¹⁹⁷Au, ^198,199,200Hg, ^203,205Tl(p, p'γ), ^85,87Rb, ⁸¹Br, ⁷⁵As, ⁷³Ge, ⁷¹Ga(p, nγ), E=1.7, 2.4 MeV; measured thick target γ-yields, Eγ, Iγ. Elemental targets.

1983SH21

J.Phys.(London) F13, 1735 (1983)

K.I.Shaw, I.S.Mackenzie, M.A.H.McCausland

Experimental Determination of the Sign of the Nuclear Quadrupole Interaction of ¹⁶⁵Ho in Ferromagnetic Gadolinium

NUCLEAR MOMENTS ¹⁶⁵Ho; measured NMR vs temperature; deduced nuclear quadrupole interaction sign in ferromagnetic Gd. Spin-echo method.

1983SO01

Z.Phys. A309, 353 (1983)

V.G.Soloviev, V.O.Nesterenko, S.I.Bastrukov

On Vibrational States in Deformed Odd-A Nuclei

NUCLEAR STRUCTURE ¹⁵⁵Sm, ¹⁶¹Tb, ^159,165Ho, ¹⁶⁷Er, ¹⁶⁹Yb, ¹⁷⁹Hf, ²³³Th, ^{233,235,237,239}U, ²³⁷Np, ²³⁹Pu; calculated levels, Pauli effect significance. ^155,159,161Gd, ¹⁶⁹Er, ¹⁷⁹Hf, ^233,237,239U, ²³⁹Pu; calculated Pauli principle violation in levels. Quasiparticle-phonon model.

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.

1984IL01

Izv.Akad.Nauk SSSR, Ser.Fiz. 48, 359 (1984)

A.P.Ilin, K.O.Terenetsky

Description of Deuteron Elastic Scattering on Heavy Nuclei by the Adiabatic Approximation

NUCLEAR REACTIONS ²⁰⁸Pb(d, d), E=8-15 MeV; ¹⁹⁷Au, Ta, Pd, Ag, Cd, ¹⁶⁵Ho, ¹⁰³Rh(d, d), E=11.8 MeV; ⁶⁰Ni(d, d), E=4.86-8.86 MeV; ¹¹⁴Cd(d, d), E=7.96-12 MeV; Ti, V, Cr, ⁵⁹Co, Ni, Cu(d, d), E=3.32, 4.07 MeV; analyzed σ(θ). Adiabatic approximation.

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

1984LO06

J.Phys.(London) G10, 1071 (1984)

M.Lozano, A.Mandly, G.Madurga

Fusion Barriers for Heavy Systems with 1000 < Z₁Z₂ < 3000

NUCLEAR REACTIONS ⁶⁵Cu(⁸⁶Kr, X), E(cm)=157.4-308.2 MeV; ¹⁶⁵Ho(⁴⁰Ar, X), E(cm)=181, 240.9 MeV; ⁵⁶Fe(¹³⁶Xe, X), E(cm)=225 MeV; ¹³⁹La(⁸⁶Kr, X), E(cm)=312, 376.8, 438.6 MeV; ¹⁶⁵Ho(⁸⁴Kr, X), E=298.2, 326 MeV; ²⁰⁹Bi(⁸⁴Kr, X), E(cm)=356.7, 374.5; calculated fusion σ. ¹⁴¹Pr(³⁵Cl, X), E(cm)=120-135 MeV; ^144,148,154Sm(⁴⁰Ar, X), E(cm)=125-145 MeV; calculated fusion σ(E), barriers. Shell model nuclear density, effective interaction generated folding optical potential.

NUCLEAR STRUCTURE ³⁵Cl, ⁴⁰Ar, ⁵⁶Fe, ⁶⁵Cu, ^84,86Kr, ⁹⁰Zr, ¹⁰⁹Ag, ¹³²Xe, ¹³⁹La, ¹⁴¹Pr, ^144,148,154Sm, ¹⁶⁵Ho, ²⁰⁹Bi, ²³⁸U; calculated nuclear density distribution rms radii.

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

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.

1984STZV

Diss.Abst.Int. 45B, 913 (1984)

J.H.Stanley

Elastic Proton Scattering from ¹⁴¹Pr and ¹⁶⁵Ho Nuclei with Polarized Beams and Thin Polarized Targets

NUCLEAR REACTIONS ¹⁴¹Pr, ¹⁶⁵Ho(polarized p, p), E not given; measured σ(θ), analyzing power; deduced spin-spin contribution upper limit to σ. ¹⁴²Nd deduced IAR properties. Thin polarized targets.

1985BH08

Indian J.Phys. 59A, 528 (1985)

S.Bhuloka Reddy, B.Mallikarjuna Rao, D.K.S.Reddy, D.D.Reddy

Nuclear Structure Effects through Penetration Parameter in the Deformed Region (A = 150-190)

NUCLEAR STRUCTURE ¹⁵³Gd, ¹⁶¹Dy, ¹⁶⁵Ho, ¹⁷³Yb, ¹⁷⁵Lu, ¹⁸³W, ¹⁸⁷Re; calculated M1 transition penetration parameters.

1985BU21

J.Phys.(London) C18, L1151 (1985)

D.St P.Bunbury, C.Carboni, M.A.H.McCausland

NMR of ¹⁶⁵Ho in the Ising Ferromagnet Ho(OH)₃

NUCLEAR MOMENTS ¹⁶⁵Ho; measured NMR in Ising ferromagnet; deduced hyperfine parameters.

1985CH13

Phys.Rev. A31, 2775 (1985)

K.T.Cheng, W.J.Childs

Ab Initio Calculation of 4f(N)6S² Hyperfine Structure in Neutral Rare-Earth Atoms

ATOMIC PHYSICS ¹⁵¹Eu, ¹⁵⁹Tb, ¹⁶¹Dy, ¹⁶⁵Ho, ¹⁶⁷Er, ¹⁶⁹Tm; calculated level energies, Lande' g factors, hfs constants. Multi-configurational Dirac-Fock method.

doi: 10.1103/PhysRevA.31.2775

1985CH15

Phys.Rev. C31, 2140 (1985)

H.-C.Chiang, M.B.Johnson

Pion Scattering on Aligned ¹⁶⁵Ho

NUCLEAR REACTIONS ¹⁶⁵Ho(π⁺, π⁰), E=180, 200 MeV; ¹⁶⁵Ho(π⁺, π^-), E=180 MeV, calculated σ(θ), orientation asymmetry variable vs θ. ¹⁶⁵Ho(π⁺, π^-), (π⁺, π⁰), (π⁺, π⁺), E=100-240 MeV; calculated orientation asymmetry variable vs θ; deduced neutron, proton deformation role. Oriented, deformed target, approximate Klein-Gordon equations.

doi: 10.1103/PhysRevC.31.2140

1985DO01

Nucl.Phys. A433, 280 (1985)

T.Dossing, J.Randrup

Dynamical Evolution of Angular Momentum in Damped Nuclear Reactions. (II). Observation of Angular Momentum through Sequential Decay

NUCLEAR REACTIONS ¹⁵⁴Sm(⁸⁶Kr, X), E=490, 610 MeV; calculated fragment average spin, variances vs total kinetic energy. ²⁰⁸Pb(²³⁸U, F), E=8.5 MeV/nucleon; calculated fission fragment σ(θ), absolute fission probability. ¹⁸²W(¹⁶O, F), ¹⁹⁷Au(¹⁴N, F), E not given; calculated compound nuclear angular distribution coeffcient vs excitation energy. Damped nuclear reaction product decay, dynamical evolution.

NUCLEAR STRUCTURE ¹⁶⁵Ho; calculated γ angular distribution coefficients vs angular momentum. ¹⁹⁸Pb; calculated fission parameters. ²⁰⁸Po; calculated γ angular distribution coefficients, fission parameters, decay probability vs angular momentum. Damped nuclear reaction product sequential decay, dynamical evolution.

doi: 10.1016/0375-9474(85)90179-4

1985KH06

Phys.Rev. C32, 1551 (1985)

H.A.Khan, I.E.Qureshi, W.Westmeier, R.Brandt, P.A.Gottschalk

Elastic and Inelastic Scattering of Uranium Ions by Holmium, Gold, and Bismuth Targets

NUCLEAR REACTIONS ¹⁶⁵Ho, ¹⁹⁷Au, ²⁰⁹Bi(²³⁸U, ²³⁸U), E=10 MeV/nucleon; measured σ(θ); deduced reaction parameters, σ. Optical, sharp cutoff model analysis. Solid state track detectors, 2π geometry.

doi: 10.1103/PhysRevC.32.1551

1985SU19

Acta Phys.Pol. B16, 1079 (1985)

A.Superson, K.Pomorski

Rotational Properties of One-Quasiparticle Excited States of Odd-A Rare-Earth Nuclei

NUCLEAR STRUCTURE ^153,155Eu, ^{155,157,159,161}Tb, ^161,163,165Ho, ^167,169,171Tm, ^{171,173,175,177}Lu, ^{177,179,181,183}Ta, ^{181,183,185,187}Re; calculated moment of inertia, Coriolis decoupling parameters. Cranking model, adiabatic approximation, deformed Nilsson potential, BCS approximation, pairing forces.

1986KU17

Izv.Akad.Nauk SSSR, Ser.Fiz. 50, 1914 (1986); Bull.Acad.Sci.USSR, Phys.Ser. 50, No.10, 41 (1986)

N.K.Kuzmenko, V.M.Mikhailov, V.O.Nesterenko

Coupling of Many Quasiparticle States

NUCLEAR STRUCTURE ¹⁶⁴Dy, ¹⁶⁵Ho, ¹⁶⁸Er, ^172,174,176Yb, ^175,177Lu, ^{176,177,178,179}Hf, ¹⁷⁷Ta; calculated levels, energy correlation, Nilsson configurations. Many quasiparticle state coupling model.

1987ARZT

Contrib.Proc. 5th Int.Conf.Nuclei Far from Stability, Rosseau Lake, Canada, C3 (1987)

E.Arnold, C.Ekstrom, W.Neu, R.Neugart, G.Ulm, K.Wendt

Spins, Moments and Radii of Holmium Isotopes in the Transitional Region Around N = 90

NUCLEAR MOMENTS ¹⁶⁵Ho; measured hfs, isotope shifts; deduced spectroscopic quadrupole moment, rms charge radii difference. Other data input. Laser spectroscopy.

RADIOACTIVITY ^{151,152,153,154,155,156,157,158,159,160,161,162,163,164}Ho; measured hfs, isotope shifts; deduced spectroscopic quadrupole moment, rms charge radii difference. Other data input. Laser spectroscopy.

1987HI05

Phys.Rev. C36, 208 (1987)

D.Hilscher, H.Rossner, A.Gamp, U.Jahnke, B.Cheynis, B.Chambon, D.Drain, C.Pastor, A.Giorni, C.Morand, A.Dauchy, P.Stassi, G.Petitt

Energy and Linear-Momentum Dissipation in the Fusion Reaction of ¹⁶⁵Ho + ²⁰Ne at 30 MeV/Nucleon

NUCLEAR REACTIONS ¹⁶⁵Ho(²⁰Ne, ²⁰Ne), (²⁰Ne, X), (²⁰Ne, F), E=600 MeV; measured fission fragment, evaporation residue, elastic σ(θ), σ(En, θn, fragment θ, E); deduced neutron multiplicities, preequilibrium emission hot moving source parameters, A ≈ 180 level density parameters.

doi: 10.1103/PhysRevC.36.208

1987LI34

Chin.J.Nucl.Phys. 9, 329 (1987)

Ling Youguang, Qiu Zhihong

Probability of Forming Six-Quark Clusters and the Increase of Nucleon Radius in Nuclei

NUCLEAR STRUCTURE ²H, ^3,4He, ^6,7Li, ⁹Be, ¹²C, ¹⁴N, ¹⁶O, ¹⁹F, ²⁰Ne, ²³Na, ²⁴Mg, ²⁷Al, ²⁸Si, ³¹P, ³²S, ⁴⁰Ar, ³⁹K, ⁴⁰Ca, ⁵¹V, ⁵⁶Fe, ⁵⁹Co, ⁵⁸Ni, ⁶³Cu, ⁶⁴Zn, ⁸⁸Sr, ⁸⁹Y, ⁹⁰Zr, ⁹³Nb, ⁹⁸Mo, ¹¹⁴Cd, ¹²⁰Sn, ¹³⁸Ba, ¹⁴²Nd, ¹⁵⁴Sm, ¹⁶⁵Ho, ¹⁸¹Ta, ¹⁸⁴W, ¹⁹⁷Au, ²⁰⁸Pb, ²⁰⁸Bi, ²³²Th, ²³⁸U; calculated six quark cluster probabilities, nuclear radii. Fermi gas model.

1987PF01

Z.Phys. D4, 351 (1987)

V.Pfeufer

On the Hyperfine Structure in the Configurations 4f(n)6s², 4f(n)5d6s, 4f(n)6s6p, and 4f(n-1)5d6s² of the Lanthanides

NUCLEAR MOMENTS ¹⁴¹Pr, ¹⁴³Nd, ¹⁴⁷Sm, ¹⁵¹Eu, ¹⁵⁵Gd, ¹⁵⁹Tb, ¹⁶¹Dy, ¹⁶⁵Ho, ¹⁶⁷Er, ¹⁶⁹Tm, ¹⁷³Yb; analyzed spin, magnetic dipole, spectroscopic electric quadrupole moments, hfs parameters; calculated core-polarization contributions; deduced electric quadrupole correction factors. Optimized Hartree-Fock-Slater calculations.

1988DO05

Phys.Rev. C37, 1633 (1988)

M.Dobeli, M.Doser, L.van Elmbt, M.W.Schaad, P.Truol, A.Bay, J.P.Perroud, J.Imazato, T.Ishikawa

Radiative Muon Capture in Nuclei

NUCLEAR REACTIONS ¹²C, ¹⁶O, ²⁷Al, ⁴⁰Ca, Fe, ¹⁶⁵Ho, ²⁰⁹Bi(μ^-, γ), E at rest; measured Eγ, Iγ; deduced (g(p)/g(A)). ¹²C, ¹⁶O, ²⁷Al, ⁴⁰Ca, Fe, ¹⁶⁵Ho, ²⁰⁹Bi deduced branching ratio.

doi: 10.1103/PhysRevC.37.1633

1988FE10

Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 2123 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.11, 41 (1988)

A.P.Feresin, M.A.Listengarten

Anapole Moments of Odd Deformed Nuclei

NUCLEAR STRUCTURE ^179,181Ta, ^175,177Lu, ¹⁸⁵Re, ¹⁶⁵Ho, ²⁴³Am, ²³⁷Np, ¹⁵³Eu, ¹⁵⁹Tb, ¹⁷⁷Hf, ¹⁶¹Dy, ¹⁷⁵Hf, ²⁴⁵Cm, ²³³U, ²³¹Th, ¹⁶⁵Er, ¹⁵⁵Gd; calculated anapole moments. Nilsson model.

1988LI03

Nucl.Phys. A476, 684 (1988)

M.Lifshitz, P.Singer

Meson-Exchange Currents and Energetic Particle Emission from μ^- Capture

NUCLEAR STRUCTURE ²⁴Mg, ²⁷Al, ³²S, ⁴⁰Ca, ⁶³Cu, ⁷⁹Br, ¹⁰⁷Ag, ¹⁶⁵Ho, ¹⁸¹Os, ¹⁸⁶Ir, ¹⁹⁴Tl, ²⁰⁷Pb, ²⁰⁹Bi; calculated μ-capture probability, average excitation energy. Meson exchange currents, Fermi gas model.

NUCLEAR REACTIONS ²⁷Al, Si, Mg, Cu, Ag, Br, Pb(μ^-, xp), E at rest; calculated proton spectra. Meson exchange currents, Fermi gas model.

doi: 10.1016/0375-9474(88)90330-2

1989AL27

Nucl.Phys. A504, 549 (1989)

G.D.Alkhazov, A.E.Barzakh, I.Ya.Chubukov, V.P.Denisov, V.S.Ivanov, N.B.Buyanov, V.N.Fedoseyev, V.S.Letokhov, V.I.Mishin, S.K.Sekatsky

Nuclear Deformation of Holmium Isotopes

RADIOACTIVITY ^{152,152m,153,153m,154,154m,155,156,157,158,158m,159,160,160m,161,162m,163}Ho; measured isotope shifts, hfs; deduced mean square charge radius, J, magnetic dipole moment, electric quadrupole moment. Resonance ionization spectroscopy.

NUCLEAR MOMENTS ¹⁶⁵Ho; measured isotope shifts, hfs; deduced mean square charge radius, J, magnetic dipole moment, electric quadrupole moment. Resonance ionization spectroscopy.

doi: 10.1016/0375-9474(89)90557-5

1989BA43

Yad.Fiz. 49, 1588 (1989)

A.E.Barzakh, V.E.Starodubsky

Description of Deformed Nuclei in the Quasiparticle Lagrange Method

NUCLEAR STRUCTURE ^{158,160,162,164,166,170,172,174,176}Yb, ^{155,157,161,165}Ho; calculated quadrupole moments, rms charge radii. Quasiparticle Lagrange method.

1989BA75

Ann.Phys.(New York) 196, 89 (1989)

J.Bartel, M.B.Johnson, M.K.Singham

Pion Single-Charge-Exchange Scattering and Nuclear Structure in Deformed Nuclei

NUCLEAR REACTIONS ¹⁶⁵Ho(π⁺, π⁺), (π⁺, π⁺'), (π^-, π^-), (π^-, π^-'), (π^-, π⁰), E=165 MeV; calculated σ(θ). Coupled-channel optical model.

doi: 10.1016/0003-4916(89)90046-8

1989BU04

J.Phys.Condens.Matter 1, 1309 (1989)

D.St.P.Bunbury, C.Carboni, M.A.H.McCausland

Field Dependence of the Hyperfine Splitting of Holmium in Holmium Hydroxide

NUCLEAR MOMENTS ¹⁶⁵Ho; measured hfs; deduced field dependence. Spin-echo NMR technique.

doi: 10.1088/0953-8984/1/7/014

1989CU04

Nucl.Instrum.Methods Phys.Res. B40/41, 25 (1989)

N.Cue

Nuclear Excitation by Target Electron Capture

NUCLEAR STRUCTURE ¹⁶⁵Ho, ¹⁷³Yb, ^185,187Re, ¹⁹⁵Pt, ¹⁸³W, ²³⁶U, ²³⁹Pu; calculated nuclear excitation by electron capture σ.

doi: 10.1016/0168-583X(89)90914-2

1989KO47

Fiz.Tverd.Tela 31, 263 (1989); Sov.Phys.Solid State 31, 698 (1989)

Yu.Yu.Kostetsky

Nuclear Magnetic Resonance Spectra of the Jahn-Teller System Rb₂NaHoF₆ Under Quadrupole Ordering Conditions

NUCLEAR MOMENTS ¹⁶⁵Ho; analyzed NMR spectra; deduced quadrupole ordering role in anisotropy.

1989LI18

Nucl.Instrum.Methods Phys.Res. B43, 162 (1989)

Z.Liu, X.Cai, S.Ma, J.Liu, J.Feng, S.Liu, Z.Zheng

L-Subshell Ionization of Dy and Ho by 0.4-3.0 MeV Protons

NUCLEAR REACTIONS Dy, ¹⁶⁵Ho(p, X), E=0.4-3 MeV; measured L X-ray production σ; deduced subshell ionization σ.

ATOMIC PHYSICS Dy, ¹⁶⁵Ho(p, X), , E=0.4-3 MeV; measured L X-ray production σ; deduced subshell ionization σ.

doi: 10.1016/0168-583X(89)90031-1

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

1989SA09

Z.Phys. A332, 383 (1989)

M.Saha, S.Bhattacharya, A.Goswami, S.Sen

Coriolis Attenuation in the Rare Earth Region

NUCLEAR STRUCTURE ¹⁶³Er, ¹⁵⁷Dy, ¹⁶⁵Ho, ¹⁶⁵Tm; calculated levels. ^157,159,161Dy, ^161,163,165Er; calculated Nilsson orbital occupation probability. ^161,163Dy, ¹⁶⁵Ho; calculated B(E2). ¹⁶⁵Tm, ^{165,163,159,157}Ho; calculated stripping spectroscopic factors; deduced pairing gap parameter role.

1990GE04

Nuovo Cim. 103A, 9 (1990)

P.M.Gensini

A Current Algebra Description of Kaon-Nucleus Scattering Lengths

NUCLEAR REACTIONS ¹H, ¹n, ⁴He, Li, ⁹Be, ^10,11B, C, O, Mg, ²⁷Al, Si, ³¹P, S, ^35,37Cl, ⁵⁹Co, Ni, ^63,65Cu, Ag, Cd, In, Sn, ¹⁶⁵Ho, Yb, ¹⁸¹Ta, Pb, U(K^-, K^-), E=low; calculated threshold amplitudes. Current algebra description.

1990LE21

Phys.Rev.Lett. 65, 2853 (1990)

A.Leviatan, J.N.Ginocchio, M.W.Kirson

Proton-Neutron Deformations and F-Spin Symmetry in Nuclei

NUCLEAR STRUCTURE ¹⁶⁵Ho; calculated ground state band F-spin mixing; deduced proton, neutron deformations role.

doi: 10.1103/PhysRevLett.65.2853

1990MA71

Nucl.Phys. A519, 548 (1990)

M.Matsuzaki

Signature-Dependent Effects of Gamma Vibration on E2 Transitions in Rotating Odd-A Nuclei (II). Triaxial Nuclei

NUCLEAR STRUCTURE ¹³³Cs, ¹³⁹La, ¹⁴¹Pr, ¹⁴⁷Pm, ^151,153Eu, ¹⁵⁹Tb, ¹⁶⁵Ho, ¹⁶⁹Tm, ¹⁷⁵Lu, ^{159,161,163,165,167,169}Yb; calculated B(λ) ratios. Quasiparticle-vibration coupling.

doi: 10.1016/0375-9474(90)90446-S

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

1990WO08

Phys.Scr. 42, 569 (1990)

T.Worm, P.Shi, O.Poulsen

Lifetimes and Hyperfine Structure in Ho II

NUCLEAR MOMENTS ¹⁶⁵Ho; measured hfs; deduced hyperfine constants.

1990ZA08

Phys.Rev. C42, 1461 (1990)

D.Zawischa, M.Macfarlane, J.Speth

Magnetic Dipole Strength Functions in Heavy Deformed Nuclei

NUCLEAR STRUCTURE ¹⁵⁶Gd, ¹⁶⁴Dy, ²³⁸U, ¹⁶⁵Ho; calculated T=1 spin flip M1 strength function, Gamow-Teller, IAS resonances. ⁹⁰Zr, ²⁰⁸Pb, ¹⁵⁶Gd, ²³⁸U; calculated B(M1). Quasiparticle RPA.

doi: 10.1103/PhysRevC.42.1461

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

1991BR31

J.Phys.(London) B24, 1669 (1991)

E.Braziewicz, J.Braziewicz, T.Czyzewski, L.Glowacka, M.Jaskola, T.Kauer, A.P.Kobzev, M.Pajek, D.Trautmann

L-Subshell Ionization of Rare Earth Elements by Light Ion Bombardment

NUCLEAR REACTIONS ¹³⁹La, Pr, Nd, Eu, Tb, ¹⁶⁵Ho, Er(p, X), E=0.1-0.9 MeV; ¹³⁹La, Pr, Nd, Eu, Tb, ¹⁶⁵Ho, Er(d, X), E=0.2-2.1 MeV; ¹³⁹La, Pr, Nd, Eu, Tb, ¹⁶⁵Ho, Er(³He, X), E=0.3-0.9 MeV; ¹³⁹La, Pr, Nd, Eu, Tb, ¹⁶⁵Ho, Er(α, X), E=0.4-0.9 MeV; measured L-subshell ionization σ(E). Model comparison.

ATOMIC PHYSICS ¹³⁹La, Pr, Nd, Eu, Tb, ¹⁶⁵Ho, Er(p, X), E=0.1-0.9 MeV; ¹³⁹La, Pr, Nd, Eu, Tb, ¹⁶⁵Ho, Er(d, X), E=0.2-2.1 MeV; ¹³⁹La, Pr, Nd, Eu, Tb, ¹⁶⁵Ho, Er(³He, X), E=0.3-0.9 MeV; ¹³⁹La, Pr, Nd, Eu, Tb, ¹⁶⁵Ho, Er(α, X), E=0.4-0.9 MeV; measured L-subshell ionization σ(E). Model comparison.

doi: 10.1088/0953-4075/24/7/020

1991FR07

Nucl.Phys. A531, 125 (1991)

A.Frank, J.M.Arias, P.Van Isacker

Search for Scissors States in Odd-Mass Nuclei

NUCLEAR STRUCTURE ¹⁶⁶Er; calculated levels. ¹⁶⁵Ho; calculated levels, μ, quadrupole moment, δ(E2/M1), B(λ). Interacting boson-fermion model.

doi: 10.1016/0375-9474(91)90573-O

1991JA01

Nucl.Phys. A524, 321 (1991)

H.R.Jaqaman, D.H.E.Gross

Signals of the Liquid-Gas Phase Transition in the Fragmentation of Hot Nuclei: Finite-size scaling

NUCLEAR STRUCTURE ¹³¹Xe, ¹⁶⁵Ho, ¹⁹⁷Au, ²⁰⁹Bi, ²³²Th, ²⁵²Es; calculated fragment size vs second moment; deduced phase transition features. Hot nuclei fragmentation, finite size scaling.

doi: 10.1016/0375-9474(91)90029-6

1991KN01

Phys.Rev.Lett. 66, 1026 (1991)

J.N.Knudson, J.D.Bowman, S.I.Penttila, J.R.Comfort, B.G.Ritchie, J.Gorgen, D.Mathis, J.Tinsley, S.S.Hanna, B.King, D.Pocanic, R.A.Loveman, L.S.Fritz, N.S.Dixon

Neutron Deformation in ¹⁶⁵Ho

NUCLEAR REACTIONS ¹⁶⁵Ho(π⁺, π⁰), E=165 MeV; measured σ(E(π⁰)), orientation asymmetries. ¹⁶⁵Ho deduced neutral, charge quadrupole deformation ratio. Aligned, unaligned targets.

doi: 10.1103/PhysRevLett.66.1026

1991MA54

Pramana 37, 293 (1991)

K.S.Mann, K.S.Kahlon, H.S.Aulakh, N.Singh, R.Mittal, K.L.Allawadhi, B.S.Sood

Determination of L-Shell X-Ray Production Cross-Sections in Holmium by 10-40 keV Photons

NUCLEAR REACTIONS ¹⁶⁵Ho(γ, X), E=10-40 keV; measured L X-ray production σ.

ATOMIC PHYSICS ¹⁶⁵Ho(γ, X), E=10-40 KeV; measured L X-ray production σ.

1991PI05

Phys.Rev. C43, 2224 (1991)

J.-L.Pin, J.-Q.Chen, C.-L.Wu, D.H.Feng

Nuclear Stretching

NUCLEAR STRUCTURE ¹⁵²Sm, ¹⁵⁸Gd, ¹⁶⁰Dy, ¹⁶⁶Er, ¹⁶⁶Yb, ¹⁷⁰Hf, ¹⁸⁸W; calculated B(λ). ^{162,164,166,168,170,172}Er, ^{168,170,172,174,176,178,180}Yb, ^{230,232,234,236,238,240}U, ^{238,240,242,244,246}Cm; calculated levels. Fermion dynamical symmetry model, stretching.

doi: 10.1103/PhysRevC.43.2224

1992BO45

Bull.Rus.Acad.Sci.Phys. 56, 1694 (1992)

N.A.Bonch-Osmolovskaya, V.O.Nesterenko

Microscopic Description of Irrotational States in Deformed Odd Ho Nuclei with A = 157-165

NUCLEAR STRUCTURE ^{157,159,161,163}Ho; calculated levels. ¹⁶⁵Ho; calculated levels, B(λ). Quasiparticle-phonon model.

1992LA12

Nucl.Phys. A543, 469 (1992)

R.Larsson, S.Pittel, R.Bijker

Mean-Field Approximations for Deformed Odd-Mass Nuclei

NUCLEAR STRUCTURE ¹⁶⁶Er, ¹⁶⁵Ho; calculated levels. Hartree-Bose-Fermi, Tamm-Dancoff, RPA approximations, neutron-proton interacting boson fermion approximation.

doi: 10.1016/0375-9474(92)90276-P

1993BO32

Phys.Rev. B47, 14696 (1993)

T.Boonyarith, J.P.D.Martin, N.B.Manson

Hyperfine Structure of ⁵I₈ → ⁵F₅ Optical Transitions within the Trigonal Center of CaFa₂:Ho³⁺

NUCLEAR MOMENTS ¹⁶⁵Ho; measured optical hfs; deduced quadrupole, off-diagonal hyperfine interactions. Optically detected nuclear magnetic resonance, two-laser hole burning.

doi: 10.1103/PhysRevB.47.14696

1993ME16

Nucl.Instrum.Methods Phys.Res. B79, 175 (1993)

R.Mehta, J.L.Duggan, F.D.McDaniel, M.R.McNeir, Y.C.Yu, D.K.Marble, G.Lapicki

L-Shell X-Ray Production Cross Sections for ₂₉Cu, ₃₁Ga, ₃₂Ge, ₃₅Br, ₃₉Y, ₆₀Nd, ₆₄Gd, ₆₇Ho, ₇₀Yb, ₇₉Au, and ₈₂Pb for 2-25 MeV Carbon Ions

NUCLEAR REACTIONS Cu, Ga, Ge, Br, ⁸⁹Y, Nd, Gd, ¹⁶⁵Ho, Yb, ¹⁹⁷Au, Pb(C, X), E=2-25 MeV; measured L X-ray production σ; deduced Si(Li) detector efficiency. Multiple normalization techniques.

ATOMIC PHYSICS Cu, Ga, Ge, Br, ⁸⁹Y, Nd, Gd, ¹⁶⁵Ho, Yb, ¹⁹⁷Au, Pb(C, X), E=2-25 MeV; measured L X-ray production σ; deduced Si(Li) detector efficiency. Multiple normalization techniques.

doi: 10.1016/0168-583X(93)95318-Y

1993MU27

J.Phys.Condens.Matter 5, 3937 (1993)

M.Mujaji, T.Boonyarith, J.P.D.Martin, N.B.Manson, G.D.Jones

High-Resolution Spectroscopy and Optically Detected Nuclear Magnetic Resonance Studies of Ho³⁺ Ions in SrF₂ Crystals Containing Ba²⁺ and Ca²⁺ Impurities

NUCLEAR MOMENTS ¹⁶⁵Ho; measured NMR for Ho³⁺ ions in SrF₂ crystals, Ba²⁺, Ca²⁺ impurities.

doi: 10.1088/0953-8984/5/23/019

1993PA04

Phys.Rev. C47, 1514 (1993)

S.K.Patra, P.K.Panda

Systematic Study of Neutron-Deficient Ho Isotopes in a Relativistic Mean Field Theory

NUCLEAR STRUCTURE ^{148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165}Ho; calculated binding energies, rms radii, quadrupole, hexadecupole moments. Relativistic mean field theory.

doi: 10.1103/PhysRevC.47.1514

1993SU29

Nucl.Instrum.Methods Phys.Res. B79, 186 (1993)

H.L.Sun, J.F.Kirchhoff, A.R.Azordegan, J.L.Duggan, F.D.McDaniel, R.M.Wheeler, R.P.Chaturvedi, G.Lapicki

M-Shell X-Ray Production Cross Sections of Rare-Earth Elements by ⁴He²⁺ Impact in the Energy Range 0.7-7.0 MeV

NUCLEAR REACTIONS ¹³⁹La, Nd, Sm, Eu, Gd, Dy, ¹⁶⁵Ho, Er, Yb, Lu, Hf(α, X), E=0.7-7 MeV; measured M-shell X-ray production σ; deduced detector efficiency. Windowless Si(Li) detector.

ATOMIC PHYSICS ¹³⁹La, Nd, Sm, Eu, Gd, Dy, ¹⁶⁵Ho, Er, Yb, Lu, Hf(α, X), E=0.7-7 MeV; measured M-shell X-ray production σ; deduced detector efficiency. Windowless Si(Li) detector.

doi: 10.1016/0168-583X(93)95321-U

1993SU30

Nucl.Instrum.Methods Phys.Res. B79, 194 (1993)

H.L.Sun, J.F.Kirchhoff, A.R.Azordegan, J.L.Duggan, D.McDaniel, R.M.Wheeler, R.P.Chaturvedi, G.Lapicki

M-Shell Ionization of Rare Earth Elements by Proton Impact in the Energy Range 0.6-4.6 MeV

NUCLEAR REACTIONS La, Nd, Sm, Eu, Gd, Dy, ¹⁶⁵Ho, Er, Yb, Lu, Hf(p, X), E=0.6-4.6 MeV; measured M-shell X-ray production σ; deduced detector efficiency. Windowless Si(Li) detector.

ATOMIC PHYSICS La, Nd, Sm, Eu, Gd, Dy, ¹⁶⁵Ho, Er, Yb, Lu, Hf(p, X), E=0.6-4.6 MeV; measured M-shell X-ray production σ; deduced detector efficiency. Windowless Si(Li) detector.

doi: 10.1016/0168-583X(93)95323-W

1993YU02

Phys.Rev. C47, 323 (1993)

Z.-S.Yuan, J.C.Kimball

First-Principles Calculation of the Cross Sections for Nuclear Excitation by Electron Capture of Channeled Nuclei

NUCLEAR STRUCTURE ¹⁶⁵Ho, ¹⁷³Yb, ^187,185Re, ¹⁸⁵Pt; calculated σ for excitation by electron capture. Highly stripped nuclei, channelling along Si <110> crystal axis.

doi: 10.1103/PhysRevC.47.323

1994KN01

Phys.Rev. C50, 909 (1994)

J.N.Knudson, J.D.Bowman, S.I.Penttila, J.R.Comfort, J.Tinsley, B.G.Ritchie, J.Gorgen, D.Mathis, S.S.Hanna, B.King, D.Pocanic, R.A.Loveman, L.S.Fritz, N.S.Dixon

Neutron Deformation in ¹⁶⁵Ho

NUCLEAR REACTIONS ¹⁶⁵Ho(π⁺, π⁰), E=165 MeV; measured σ(E, θ), oriented, unoriented nuclei; deduced asymmetry vs θ. ¹⁶⁵Ho deduced neutron distribution deformation features.

doi: 10.1103/PhysRevC.50.909

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

1996BO26

Phys.Lett. 384B, 30 (1996)

K.Boretzky, J.Stroth, E.Wajda, T.Aumann, Th.Blaich, J.Cub, Th.W.Elze, H.Emling, W.Henning, R.Holzmann, H.Klingler, R.Kulessa, J.V.Kratz, D.Lambrecht, Y.Leifels, E.Lubkiewicz, K.Stelzer, W.Walus, M.Zinser, E.Zude, and the LAND Collaboration

Two-Phonon Giant Dipole Resonance in ²⁰⁸Pb

NUCLEAR REACTIONS C, Sn, ¹⁶⁵Ho, Pb, U(²⁰⁸Pb, ²⁰⁸Pb'), E=640 MeV/nucleon; measured integrated projectile excitation; deduced excitation mechanism, σ. ²⁰⁸Pb deduced two-phonon isovector GDR excitation, Γ.

doi: 10.1016/0370-2693(96)00797-6

1996DU06

Phys.Rev. C54, 189 (1996)

J.C.Durand, R.Piepenbring

Anharmonicities of γ Vibrations in Odd-Mass Deformed Nuclei

NUCLEAR STRUCTURE ¹⁶⁵Ho, ^163,167Er, ¹⁶³Tb; calculated levels, E2 matrix elements. Multi-phonon method.

doi: 10.1103/PhysRevC.54.189

1996RA32

Can.J.Phys. 74, 230 (1996)

D.V.Rao, R.Cesareo, G.E.Gigante

L X-Ray Fluorescence Cross Sections in the Atomic Region 59 ≤ Z ≤ 82 Excited by 16.58 KeV photons

NUCLEAR REACTIONS Pt, Sm, Gd, Dy, ¹⁶⁵Ho, Er, Yb, Pt, ¹⁹⁷Au, Pb(γ, X), E=16.58 keV; measured L X-ray fluorescence σ. Relativistic Dirac-Hartree-Slater theory.

ATOMIC PHYSICS Pt, Sm, Gd, Dy, ¹⁶⁵Ho, Er, Yb, Pt, ¹⁹⁷Au, Pb(γ, X), E=16.58 keV; measured L X-ray fluorescence σ. Relativistic Dirac-Hartree-Slater theory.

1996SU14

Phys.Rev. C54, 2967 (1996)

Y.Sun, J.-Y.Zhang, M.Guidry

Properties of ΔI = 4 Bifurcation from the Projected Shell Model

NUCLEAR STRUCTURE ^162,166Tm, ¹⁶⁷Er, ¹⁶⁵Ho, ¹⁷⁰Yb; analyzed levels data. ¹³⁶Pm; analyzed superdeformed bands; deduced ΔI=4 bifurcation sensitivity to quasiparticle distribution near Fermi surface. Projected shell model.

doi: 10.1103/PhysRevC.54.2967

1997BE64

Nucl.Phys. A626, 357c (1997)

P.Beiersdorfer, S.R.Elliott, J.C.Lopez-Urrutia, K.Widmann

Measurements of Nuclear Parameters of High-Z Isotopes Performed on a High-Energy Electron Beam Ion Trap

NUCLEAR MOMENTS ¹⁶⁵Ho; measured hfs; deduced magnetic moment. ^233,235U; measured charge radii. Highly charged ions, electron beam ion trap.

doi: 10.1016/S0375-9474(97)00558-7

1997KR06

Phys.Scr. 55, 579 (1997)

S.Kroger, J.-F.Wyart, P.Luc

Theoretical Interpretation of Hyperfine Structures in Doubly-Excited Configurations 4f¹⁰5d6s6p and 4f¹⁰5d²6s and New Energy Levels in Neutral Holmium (Ho I)

NUCLEAR MOMENTS ¹⁶⁵Ho; calculated hfs; deduced hyperfine parameters. Comparison with data.

1997MA36

Nucl.Phys. A620, 296 (1997)

M.Matsuo, T.Dossing, E.Vigezzi, S.Aberg

Level Statistics of Near-Yrast States in Rapidly Rotating Nuclei

NUCLEAR STRUCTURE ^{160,161,162,163,164,165}Dy, ^{162,163,164,165,166,167}Er, ^{166,167,168,169,170,171,172,173}Yb, ^{161,162,163,164,165,166}Ho, ^{163,164,165,166,167,168}Tm, ^{167,168,169,170,171,172,173,174}Lu; analyzed high-spin level data; deduced nearest neighbor level spacing distribution related features. Cranked shell model.

doi: 10.1016/S0375-9474(97)00170-X

1997SH42

Phys.Rev. A56, 252 (1997)

V.M.Shabaev, M.Tomaselli, T.Kuhl, A.N.Artemyev, V.A.Yerokhin

Ground-State Hyperfine Splitting of High-Z Hydrogenlike Ions

NUCLEAR MOMENTS ¹¹³In, ^121,123Sb, ¹²⁷I, ¹³³Cs, ¹³⁹La, ¹⁴¹Pr, ¹⁵¹Eu, ¹⁵⁹Tb, ¹⁶⁵Ho, ¹⁷⁵Lu, ¹⁸¹Ta, ¹⁸⁵Re, ^203,205Tl, ²⁰⁷Pb, ²⁰⁹Bi; calculated hydrogen-like ions hfs. Relativistic, nuclear, QED corrections.

doi: 10.1103/PhysRevA.56.252

1998GU22

Phys.Rev. A58, 3611 (1998)

M.G.H.Gustavsson, A.-M.Martensson-Pendrill

Need for Remeasurements of Nuclear Magnetic Dipole Moments

NUCLEAR MOMENTS ²³Na, ¹⁶⁵Ho, ^185,187Re, ¹⁹⁹Hg, ^203,205Tl, ²⁰⁷Pb, ²⁰⁹Bi; compiled, analyzed μ; deduced need for remeasurement. Limitations on accuracy of hyperfine structures measurement discussed.

doi: 10.1103/PhysRevA.58.3611

1998OK04

Phys.Rev. C58, 2180 (1998)

H.Okamura, S.Ishida, N.Sakamoto, H.Otsu, T.Uesaka, T.Wakasa, H.Sakai, T.Niizeki, H.Toyokawa, Y.Tajima, H.Ohnuma, M.Yosoi, K.Hatanaka, T.Ichihara

Mechanism of the Forward-Angle (d, pn) Reaction at Intermediate Energies

NUCLEAR REACTIONS ¹²C, ²⁸Si, ⁴⁰Ca, ⁹⁰Zr, ¹¹⁸Sn, ¹⁶⁵Ho, ²⁰⁸Pb(d, np), E=140, 270 MeV; measured elastic breakup σ(Ep, En, θ=0°); deduced Coulomb breakup contribution. Post-form DWBA analysis.

doi: 10.1103/PhysRevC.58.2180

1998SH21

Appl.Radiat.Isot. 49, 1481 (1998)

M.Shibata, Y.Satoh, S.Itoh, H.Yamamoto, K.Kawade, Y.Kasugai, Y.Ikeda

Beta-Decay Half-Lives and Level Ordering of ^{102m, g}Rh

RADIOACTIVITY ¹⁰²Rh(β^-), (EC); ^102mRh(EC), (IT) [from ¹⁰³Rh(n, 2n)]; measured Eγ, Iγ(t), (X-ray)γ-coin; deduced T_1/2.

doi: 10.1016/S0969-8043(98)00057-8

1998TO08

Phys.Lett. 424B, 219 (1998)

J.A.Tostevin, S.Rugmai, R.C.Johnson, H.Okamura, S.Ishida, N.Sakamoto, H.Otsu, T.Uesaka, T.Wakasa, H.Sakai, T.Niizeki, H.Toyokawa, Y.Tajima, H.Ohnuma, M.Yosoi, K.Hatanaka, T.Ichihara

Coulomb Breakup of Light Composite Nuclei

NUCLEAR REACTIONS ¹²C, ²⁸Si, ⁴⁰Ca, ⁹⁰Zr, ¹¹⁸Sn, ¹⁶⁵Ho, ²⁰⁸Pb(d, np), E=140 MeV; measured σ(Ep, θ(p), θ(n)); deduced Coulomb dissociation mechanism. Core-valence model.

doi: 10.1016/S0370-2693(98)00228-7

1998TO10

Phys.Rev. C57, 3225 (1998)

J.A.Tostevin, S.Rugmai, R.C.Johnson

Coulomb Dissociation of Light Nuclei

NUCLEAR REACTIONS ¹²C, ²⁸Si, ⁴⁰Ca, ⁹⁰Zr, ¹¹⁸Sn, ¹⁶⁵Ho, ²⁰⁸Pb(d, np), E=56, 140, 270 MeV; calculated σ(Ep, θ(n), θ(p)); deduced Coulomb breakup mechanism importance. Comparison with data.

doi: 10.1103/PhysRevC.57.3225

1998TO20

Phys.Rev. C58, 1524 (1998)

M.Tomaselli, T.Kuhl, P.Seelig, C.Holbrow, E.Kankeleit

Hyperfine Splittings of Hydrogenlike Ions and the Dynamic-Correlation Model for One-Hole Nuclei

NUCLEAR MOMENTS ¹⁶⁵Ho, ^185,187Re, ²⁰⁷Pb; calculated hfs, magnetic moments in hydrogen-like ions. Dynamic-correlation model.

doi: 10.1103/PhysRevC.58.1524

1999PA08

Phys.Rev. C59, 1199 (1999)

K.Patel, M.S.Desai, V.Potbhare

Spectral Averaging Methods and Nilsson Model

NUCLEAR STRUCTURE ^152,153Sm, ¹⁵¹Eu, ¹⁵⁶Gd, ¹⁶⁹Er, ^159,160Tb, ¹⁶⁵Ho, ^172,174Yb, ^178,179,180Hf, ¹⁸⁴W; calculated level densities, related quantities. Nilsson model, spectral averaging method.

doi: 10.1103/PhysRevC.59.1199

2000BA45

Nucl.Phys. A673, 335 (2000)

A.Baca, C.Garcia-Recio, J.Nieves

Deeply Bound Levels in Kaonic Atoms

ATOMIC PHYSICS, Mesic-atoms ⁷Li, ⁹Be, ^10,11B, ¹²C, ¹⁶O, ²⁴Mg, ²⁷Al, ²⁸Si, ³¹P, ³²S, ³⁵Cl, ⁵⁹Co, ⁵⁸Ni, ⁶³Cu, ¹⁰⁸Ag, ¹¹²Cd, ¹¹⁵In, ¹¹⁸Sn, ¹⁶⁵Ho, Ta, ²⁰⁸Pb, ²³⁸U; calculated kaonic atoms level energy shifts, widths.

NUCLEAR STRUCTURE ¹²C, ⁴⁰Ca, ²⁰⁸Pb; calculated deeply bound kaonic states binding energies, widths. Optical potential, chiral model.

doi: 10.1016/S0375-9474(00)00152-4

2000JO21

Prog.Theor.Phys.(Kyoto), Suppl. 140, 33 (2000)

R.Johnson

Scattering and Reactions of Halo Nuclei - A Theorist's Perspective -

NUCLEAR REACTIONS ¹²C(¹¹Be, ¹¹Be), E=49.3 MeV/nucleon; ¹²C(¹⁹C, ¹⁹C), E=30 MeV/nucleon; calculated form factors, σ(θ). ¹²C, ²⁸Si, ⁴⁰Ca, ⁹⁰Zr, ¹¹⁸Sn, ¹⁶⁵Ho, ²⁰⁸Pb(d, np), E=140 MeV; calculated σ(E, θ). Adiabatic model, comparisons with data.

2000SH26

Phys.Scr. T86, 7 (2000)

V.M.Shabaev, A.N.Artemyev, V.A.Yerokhin

QED and Nuclear Effects in High-Z Few-Electron Atoms

NUCLEAR MOMENTS ¹⁶⁵Ho, ^185,187Re, ²⁰⁷Pb, ²⁰⁹Bi; calculated ground state hfs, nuclear contributions. Hydrogenlike ions.

doi: 10.1238/Physica.Topical.086a00007

2000SH50

Hyperfine Interactions 127, 279 (2000)

V.M.Shabaev, A.N.Artemyev, O.M.Zherebtsov, V.A.Yerokhin, G.Plunien, G.Soff

Calculation of the hyperfine structure of heavy H- and Li-like ions

NUCLEAR MOMENTS ¹⁶⁵Ho, ^185,187Re, ²⁰⁷Pb, ²⁰⁹Bi; calculated hfs in hydrogen-like and lithium-like ions. Comparison with data.

doi: 10.1023/A:1012616322709

2000ZH44

Can.J.Phys. 78, 701 (2000)

O.M.Zherebtsov, V.M.Shabaev

Higher Order Interelectronic-Interaction Corrections to the Ground-State Hyperfine Splitting in Lithiumlike Ions

NUCLEAR MOMENTS ¹¹³In, ^121,123Sb, ¹²⁷I, ¹³³Cs, ¹³⁹La, ¹⁴¹Pr, ¹⁵¹Eu, ¹⁵⁹Tb, ¹⁶⁵Ho, ¹⁷⁵Lu, ¹⁸¹Ta, ^185,187Re, ^203,205Tl, ²⁰⁷Pb, ²⁰⁹Bi; calculated corrections to hfs for lithium-like ions.

doi: 10.1139/cjp-78-7-701

2001AR10

Phys.Rev. A63, 062504 (2001)

A.N.Artemyev, V.M.Shabaev, G.Plunien, G.Soff, V.A.Yerokhin

Vacuum-Polarization Corrections to the Hyperfine Splitting in Heavy Ions and to the Nuclear Magnetic Moments

NUCLEAR MOMENTS ¹¹³Sn, ^121,123Sb, ¹²⁷I, ¹³³Cs, ¹³⁹La, ¹⁴¹Pr, ¹⁵¹Eu, ¹⁵⁹Tb, ¹⁶⁵Ho, ¹⁷⁵Lu, ¹⁸¹Ta, ¹⁸⁵Re, ^203,205Tl, ²⁰⁷Pb, ²⁰⁹Bi; calculated vacuum polarization corrections to μ, hyperfine splitting.

doi: 10.1103/PhysRevA.63.062504

2002TO01

Phys.Rev. A65, 022502 (2002)

M.Tomaselli, T.Kuhl, W.Nortershauser, S.Borneis, A.Dax, D.Marx, H.Wang, S.Fritzsche

Hyperfine Splitting of Hydrogenlike Thallium

NUCLEAR STRUCTURE ¹⁶⁵Ho, ^185,187Re, ^203,205,207Tl, ²⁰⁷Pb, ²⁰⁹Bi; calculated wave functions, radii, μ, hyperfine splitting for hydrogenlike ions. Dynamic correlation model, comparisons with data.

NUCLEAR MOMENTS ¹⁶⁵Ho, ^185,187Re, ^203,205,207Tl, ²⁰⁷Pb, ²⁰⁹Bi; calculated wave functions, radii, μ, hyperfine splitting for hydrogenlike ions. Dynamic correlation model, comparisons with data.

doi: 10.1103/PhysRevA.65.022502

2002TO21

Can.J.Phys. 80, 1347 (2002)

M.Tomaselli, Th.Kuhl, W.Nortershauser, G.Ewald, R.Sanchez, S.Fritzsche, S.G.Karshenboim

Systematic model calculations of the hyperfine structure in light and heavy ions

NUCLEAR MOMENTS ¹⁶⁵Ho, ^185,187Re, ^203,205Tl, ²⁰⁷Pb, ²⁰⁹Bi; calculated hfs for hydrogen-like ions. ^6,7,9,11Li; calculated radii, μ.

doi: 10.1139/p02-092

2003BE28

Nucl.Instrum.Methods Phys.Res. B205, 62 (2003)

P.Beiersdorfer, J.R.C.Lopez-Urrutia, S.B.Utter, E.Trabert, M.G.H.Gustavsson, C.Forssen, A.-M.Martensson-Pendrill

Hyperfine structure of heavy hydrogen-like ions

NUCLEAR MOMENTS ^203,205Tl; measured hfs of hydrogen-like ions; deduced radii, μ. ¹⁶⁵Ho, ^185,187Re, ^203,205Tl, ²⁰⁷Pb, ²⁰⁹Bi; calculated hfs of hydrogen-like ions.

doi: 10.1016/S0168-583X(03)00534-2

2003NE02

Phys.Lett. 552B, 35 (2003)

A.V.Nefiodov, G.Plunien, G.Soff

Nuclear-polarization effect to the hyperfine structure in heavy multicharged ions

NUCLEAR MOMENTS ¹⁵⁹Tb, ¹⁶⁵Ho, ¹⁷⁵Lu, ¹⁸⁷Re, ²⁰³Tl, ²⁰⁹Bi, ²³⁵U; analyzed hfs, core polarization effects for hydrogenlike ions.

doi: 10.1016/S0370-2693(02)03093-9

2003TO22

Hyperfine Interactions 146-147, 145 (2003)

M.Tomaselli, T.Kuhl, W.Nortershauser, G.Ewald, R.Sanchez, A.Gluzicka, S.Fritzsche, L.C.Liu

Nuclear and Electron Polarization Contributions to the HFS of Hydrogen- and Lithium-like Ions

NUCLEAR MOMENTS ¹⁶⁵Ho, ^185,187Re, ^203,205Tl, ²⁰⁷Pb, ²⁰⁹Bi; calculated hfs, contributions from nuclear core polarization. Dynamic correlation model.

doi: 10.1023/B:HYPE.0000004241.59336.43

2004HU05

Nucl.Phys. A731, 163 (2004)

M.S.Hussein, B.V.Carlson, L.F.Canto

Multiple giant resonances in nuclei: their excitation and decay

NUCLEAR STRUCTURE ⁴⁰Ca, ¹²⁰Sn, ¹³²Xe, ¹⁶⁵Ho, ²⁰⁸Pb, ²³⁸U; calculated double and triple GDR excitation and decay features.

doi: 10.1016/j.nuclphysa.2003.11.029

2004IS05

Yad.Fiz. 67, 614 (2004); Phys.Atomic Nuclei 67, 595 (2004)

B.S.Ishkhanov, V.N.Orlin

Generalized Model of Giant-Dipole-Resonance Splitting

NUCLEAR STRUCTURE ¹²C, ¹⁶O, ²³Na, ²⁴Mg, ²⁷Al, ²⁸Si, ³⁴S, ⁴⁰Ca, ⁴⁸Ti, ⁵⁴Fe, ⁶³Cu, ⁷²Ge, ⁸²Se, ^116,120Sn, ^142,150Nd, ¹⁵⁴Sm, ¹⁵⁶Gd, ¹⁶⁵Ho, ¹⁶⁸Er, ¹⁷⁸Hf, ¹⁸¹Ta, ^182,184W, ¹⁹⁷Au, ²⁰⁸Pb, ²⁰⁹Bi, ²³²Th, ^235,238U, ²³⁹Pu; calculated GDR energies, widths, splitting, photoabsorption σ. Semimicroscopic model, comparison with data.

doi: 10.1134/1.1690070

2005IS09

Yad.Fiz. 68, 1407 (2005); Phys.Atomic Nuclei 68, 1352 (2005)

B.S.Ishkhanov, V.N.Orlin

Employing Spheroidal Global Potential to Estimate the Quadrupole Deformation of Nuclei

NUCLEAR STRUCTURE A=11-241; Z=5-95; analyzed quadrupole moments, deformation. ²⁵Na, ²⁵Mg, ⁷⁷Kr, ^153,165Ho, ²²⁹Ra; calculated single-particle level energies vs deformation. Spheroidal global potential.

doi: 10.1134/1.2011495

2005KO15

Phys.Scr. 71, 464 (2005)

E.Y.Korzinin, N.S.Oreshkina, V.M.Shabaev

Hyperfine Splitting of Low-Lying Levels in Heavy Li-Like Ions

NUCLEAR MOMENTS ¹¹³In, ^121,123Sb, ¹²⁷I, ¹³³Cs, ¹³⁹La, ¹⁴¹Pr, ¹⁵¹Eu, ¹⁵⁹Tb, ¹⁶⁵Ho, ¹⁷⁵Lu, ¹⁸¹Ta, ¹⁸⁵Re, ^203,205Tl, ²⁰⁷Pb, ²⁰⁹Bi; calculated hfs for lithium-like ions.

2005SI30

J.Phys.(London) G31, S1959 (2005)

S.K.Singhal, M.Bhatnagar, Prajapati, R.Kumar, G.C.Joshi, H.M.Agrawal

Re-investigation of the spin dependence of the S-wave neutron strength function

NUCLEAR STRUCTURE ^35,37Cl, ⁴⁵Sc, ⁴⁷Ti, ⁵³Cr, ⁵⁹Co, ⁶⁵Cu, ⁶⁷Zn, ⁸⁹Y, ⁹³Nb, ⁹⁹Tc, ¹⁰³Rh, ¹⁰⁵Pd, ¹⁰⁹Ag, ^147,149Sm, ^155,157Gd, ¹⁵⁹Tb, ¹⁶³Dy, ¹⁶⁵Ho, ¹⁶⁷Er, ¹⁶⁹Tm, ^171,173Yb, ¹⁷⁵Lu, ¹⁷⁷Hf, ¹⁸³W, ¹⁹⁵Pt, ¹⁹⁷Au, ^239,241Pu; analyzed data; deduced neutron strength functions vs spin.

doi: 10.1088/0954-3899/31/10/110

2006SH08

Int.J.Mod.Phys. E15, 719 (2006)

Sh.Sharipov, M.J.Ermamatov, J.K.Bayimbetova

Excited states of deformable triaxial odd ¹⁶⁵Ho and ¹⁶⁷Er Nuclei

NUCLEAR STRUCTURE ¹⁶⁵Ho, ¹⁶⁷Er; calculated levels, J, π, reduced transition probabilities, quadrupole moments.

doi: 10.1142/S0218301306004557

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

2012KI23

Ukr.J.Phys. 57, 1097 (2012)

V.I.Kirishchuk, A.P.Lashko, T.N.Lashko

Anomalies in Internal Conversion Coefficients for Hindered γ-Transitions

NUCLEAR STRUCTURE ¹⁶¹Dy, ^163,165Er, ¹⁶⁵Ho, ¹⁷⁵Lu, ¹⁷⁷Hf, ¹⁸¹Ta, ^191,193Ir; calculated B(M1), ICC, level schemes. Nilsson model, comparison with available data.

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

2016BO28

Phys.Rev. C 94, 054615 (2016)

A.S.Botvina, N.Buyukcizmeci, A.Ergun, R.Ogul, M.Bleicher, J.Pochodzalla

Formation of hypernuclei in evaporation and fission processes

NUCLEAR STRUCTURE ^112,124Sn, ¹⁶⁵Ho, ²⁰⁹Bi, ²³⁸U; calculated fragment mass distributions, probabilities of nuclear and hypernuclear fission, and evaporation of light hypernuclei, average mass numbers, charges, yields, excitation energies and the fission barriers of the fissioning hypernuclei. Generalization of nuclear evaporation and fission models applied to excited hot hypernuclei.

doi: 10.1103/PhysRevC.94.054615

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

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

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

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

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

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

2020VL02

Bull.Rus.Acad.Sci.Phys. 84, 1191 (2020)

A.K.Vlasnikov, A.I.Zippa, V.M.Mikhajlov

Polynomial Description of the Masses of Odd Deformed Nuclei

NUCLEAR STRUCTURE ¹⁵⁷Gd, ¹⁶⁵Ho, ¹⁷¹Yb, ¹⁷⁵Lu, ¹⁷⁹Hf; calculated parameter values. Comparison with available data.

doi: 10.3103/S1062873820100275

2020VL03

Bull.Rus.Acad.Sci.Phys. 84, 1309 (2020)

A.K.Vlasnikov, A.I.Zippa, V.M.Mikhajlov

Masses and Pairing Energies of Deformed Nuclei

NUCLEAR STRUCTURE ^154,157Gd, ¹⁶⁵Ho, ¹⁶⁰Dy, ^170,171Yb, ¹⁷⁵Lu, ¹⁷⁹Hf, ¹⁸⁰W, ¹⁸⁸Os; analyzed available data; deduced parameters ofthe expansion of energy surfaces for even-even nuclei, pairing energies.

doi: 10.3103/S1062873820100287

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

2021XU04

Phys.Rev. C 104, 044301 (2021)

Y.Xu, S.Goriely, E.Khan

Systematical studies of the E1 photon strength functions combining the Skyrme-Hartree-Fock-Bogoliubov plus quasiparticle random-phase approximation model and experimental giant dipole resonance properties

NUCLEAR STRUCTURE ^70,72,74Ge, ^80,82Se, ⁸⁹Y, ^90,91,92,94Zr, ⁹³Nb, ^96,100Mo, ¹⁰³Rh, ¹⁰⁷Ag, ¹¹⁵In, ^119,120,124Sn, ^124,126,128Te, ¹²⁷I, ^128,134Xe, ¹³³Ce, ¹³⁸Ba, ¹⁴⁰Ce, ¹⁴¹Pr, ^143,145,146Nd, ^144,150Sm, ¹⁶⁵Ho, ¹⁸¹Ta, ¹⁸⁸Os, ¹⁹⁷Au, ^206,208Pb, ²⁰⁹Bi, ²³⁹Pu; calculated E1 photon strength function using BSk27+QRPA, and compared with extracted strength from experimental photoabsorption cross sections. A=70-190; calculated parameters of giant-dipole resonances (GDR) using BSk27+QRPA, and compared with compiled in the RIPL-3 database. A=25-250; calculated E1 strength functions and compared with compiled data in RIPL3 for 60 nuclei from ²⁵Mg to ²³⁹U, and comparison between ARC E1 strength function for 25 nuclei from ⁹⁶Mo to ²⁴⁰Pu. ^{115,120,125,130,135,140,145,150,155}Sn; calculated E1 photon strength functions from empirical Lorentzian model SMLO, D1M+QRPA, BSk7+QRPA, and the present BSk27+QRPA. ^{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}Sn; calculated neutron capture reaction rates at the temperature of T₉=1 using present BSk27+QRPA model and compared with those from BSk7+QRPA, D1M+QRPA, SMLO. Z=1-110, N=0-255; calculated neutron capture reaction rates at T₉=1 present BSk27+QRPA model and compared with those from previous D1M+QRPA model. ^43,44Sc, ^44,45Ti; calculated temperature-dependent E1 strength functions using present BSk27+QRPA, and compared with shell-model calculationsSystematic investigation of E1 photon strength functions for about 10, 000 nuclei with Z=8-124 lying between the proton and neutron drip lines by combining simultaneously microscopic Hartree-Fock-Bogoliubov plus quasiparticle random-phase approximation (HFB+QRPA) model and the constraints from available experimental results for photon strength functions from giant dipole resonance (GDR) data, and other types of experiments. Relevance to future measurement of the photonuclear excitation using the Extreme Light Infrastructure (ELI-NP) facilities, and to improve study of r and p nucleosynthesis processes.

doi: 10.1103/PhysRevC.104.044301