References quoted in the ENSDF dataset: 238U ADOPTED LEVELS, GAMMAS

288 references found.

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

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1949KI26

Phys.Rev. 76, 1561 (1949)

C.A.Kienberger

The U²³⁴ Content of Natural Uranium and the Specific Alpha-Activities of the Isotopes

doi: 10.1103/PhysRev.76.1561

1952SE67

Phys.Rev. 86, 21 (1952)

E.Segre

Spontaneous Fission

RADIOACTIVITY ^230,232Th, ²³¹Pa, ^{232,233,234,235,238}U, ^237,239Np, ^238,239Pu(SF); analyzed available data; deduced recommended T_1/2.

doi: 10.1103/PhysRev.86.21

1955KO13

Phys.Rev. 98, 46 (1955)

A.F.Kovarik, N.I.Adams

Redetermination of the Disintegration Constant of U²³⁸

doi: 10.1103/PhysRev.98.46

1957CL16

J.S.African Chem.Inst. 10, 62 (1957)

F.L.Clark, H.J.Spencer-Palmer, R.N.Woodward

The Determination of the Half-Lives and α-Particle Energies of Some Radioactive Isotopes. Part I. The Determination of the Half-Lives of Uranium 235 and Uranium 238

1957LE21

J.Nuclear Energy 4, 38 (1957)

R.B.Leachman, H.W.Schmitt

The Cross-Section for U²³⁸ Fission by Fission Neutrons

1959GE30

Radiokhimiya 1, 223 (1959)

E.K.Gerling, Y.A.Shukolyukov, B.A.Makarochkin

Determination of the Spontaneous Fission Half-Life of ²³⁸U by Xenon Content in Uranium Minerals

1959KU81

Zhur.Eksptl.i Teoret.Fiz. 37, 406 (1959); Soviet Phys.JETP 10, 290 (1960)

B.D.Kuzminov, L.S.Kutsaeva, V.G.Nesterov, L.I.Prokhorova, G.N.Smirenkin

Some Features of the Spontaneous Fission of U²³⁸

1959ST45

Proc.Symp.Metrology Radionuclides, Vienna, Austria (1959), Intern.At.Energy Agency, Vienna, p.155 (1960)

J.Steyn, F.W.E.Strelow

The Determination of the Half-Life of U²³⁸ by Absolute Counting of α Particles in a 4 π-Liquid Scintillation Counter

1960BE25

Kgl.Danske Videnskab.Selskab, Mat.-fys.Medd. 32, No.12 (1960)

R.E.Bell, S.Bjornholm, J.C.Severiens

Half Lives of First Excited States of Even Nuclei of Fm, Ra, Th, U, and Pu

NUCLEAR STRUCTURE ²³³U, ²³²Th, ²³²U, ²³⁴Th, ²³⁶Pu, ²³⁶U, ²³⁴U, ²²⁰Rn, ²²²Th, ²¹⁸Rn, ²²²Ra, ²²⁴Ra, ²²²Rn, ²³⁰Pa, ²³⁰Th, ²³⁰U, ²²⁸Th, ²²⁸Ac, ²²⁶Ra, ²²⁸Ra, ²²⁶Th, ²⁴²Cm, ²⁴⁴Cm, ²⁴⁰Pu, ²³⁸U, ²³⁸Pu; measured not abstracted; deduced nuclear properties.

1963ME14

Thesis, Univ.Arkansas (1963); Nucl.Sci.Abstr. 18, 158, Abstr.1079 (1964)

M.P.Menon

14.7-MeV Neutron-Induced and Spontaneous Fission Yields of Uranium-238 In the Rare Earth Region

NUCLEAR STRUCTURE, Fission ²³⁸U; measured not abstracted; deduced nuclear properties.

1964FL07

Phys.Rev. 133, B63 (1964)

R.L.Fleischer, P.B.Price

Decay Constant for Spontaneous Fission of U²³⁸

RADIOACTIVITY, Fission ²³⁸U; measured T_1/2 (SF).

doi: 10.1103/PhysRev.133.B63

1965SO04

At.Energy Rev. 3, No.2, 117 (1965)

V.G.Solovev

Non-Rotational Collective States of Deformed Even-Even Nuclei

NUCLEAR STRUCTURE ¹⁵⁰Nd, ^152,154Sm, ^{154,156,158,160}Gd, ^{158,160,162,164}Dy, ^{164,166,168,170}Er, ^{168,172,174,176}Yb, ^174,176,178Hf, ^{180,182,184,186}W, ^184,186,188Os, ^{228,230,232,234}Th, ^{232,234,236,238}U, ^{236,238,240,242}Pu, ^242,244,246Cm, ^250,252Cf, ^252,254Fm; calculated levels.

1966RA25

Phys.Rev. 147, 884 (1969)

M.N.Rao, P.K.Kuroda

Decay Constant and Mass-Yield Curve for the Spontaneous Fission of Uranium-238

RADIOACTIVITY, Fission ²³⁸U; measured ¹³²Te/²³⁸U equilibrium ratio in nonirradiated U; deduced decay constant, T_1/2(SF), mass-yield curve.

doi: 10.1103/PhysRev.147.884

1967IS04

Radiochim.Acta 7, 95 (1967)

T.Ishimori, K.Ueno, K.Kimura, E.Akatsu, Y.Kobayashi, J.Akatsu, R.Ono, M.Hoshi

The Spontaneous Fission of Uranium-238

RADIOACTIVITY, Fission ²³⁸U(SF); measured T_1/2. ^90,91,93Y; measured T_1/2. ^141,143Ce; measured T_1/2.

1967SP12

Helv.Phys.Acta 40, 1063 (1967)

A.Spadavecchia, B.Hahn

Die Rotationskammer und einige Anwendungen

RADIOACTIVITY, Fission ²³²Th(SF), ²³⁸U(SF); measured T_1/2.

1968HO28

Nucl.Phys. A117, 552 (1968)

P.Holmberg, P.O.Lipas

A New Formula for Rotational Energies

NUCLEAR STRUCTURE ¹⁵⁸Dy, ¹⁶⁶Hf, ^172,180W, ¹⁵²Sm, ^154,156Gd, ¹⁷⁰Hf, ¹⁸⁴Pt, ²³⁸U, ¹²²Xe, ¹²⁶Ba; calculated ground-state rotational bands. Hydrodynamic model.

doi: 10.1016/0375-9474(68)90830-0

1968RO15

Phys.Rev. 174, 1482 (1968)

J.H.Roberts, R.Gold, R.J.Armani

Spontaneous-Fission Decay Constant of ²³⁸U

NUCLEAR STRUCTURE ²³⁸U; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.174.1482

1969BL13

Phys.Letters 30B, 458 (1969)

J.Blocki, W.Kurcewicz

Octupole Vibrations of Even Nuclei in the Transuranic Region

NUCLEAR STRUCTURE ^228,230Th, ^{232,234,236,238}U, ^238,240Pu, ²⁴⁶Cm, ²⁵²Cf; calculated first excited odd-parity vibrational levels.

doi: 10.1016/0370-2693(69)90169-5

1970GA27

Helv.Phys.Acta 43, 593 (1970)

D.Galliker, E.Hugentobler, B.Hahn

Spontane Kernspaltung von ²³⁸U and ²⁴¹Am

RADIOACTIVITY, Fission ²³⁸U, ²⁴¹Am(SF); measured T_1/2(SF).

1970NE08

Nucl.Phys. A149, 217 (1970)

K.Neergard, P.Vogel

On the Microscopic Description of Nuclear Vibrations When Phonons Occur at Relatively Low Energy (II). Octupole States of the Even Deformed Nuclei with A > 222

NUCLEAR STRUCTURE ^{222,224,226,228}Ra, ^{224,226,228,230,232,234}Th, ^{230,232,234,236,238}U, ^{236,238,240,242,244}Pu, ^{242,244,246,248}Cm, ^250,252Cf, ^252,254Fm; calculated levels, B(E3).

doi: 10.1016/0375-9474(70)90388-X

1971BE62

Yad.Fiz. 14, 685 (1971); Sov.J.Nucl.Phys. 14, 385 (1972)

A.G.Belov, Y.P.Gangrskii, B.Dalkhsuren, A.M.Kucher

Production of the Spontaneously Fissioning U²³⁶ Isomer in Thermal Neutron Radiative Capture

NUCLEAR REACTIONS, Fission ²³⁵U(n, γF), E=thermal; measured σ, (fragment)(ce)-delay. ^236mU deduced T_1/2.

1971CO35

J.Nucl.Energy 25, 331 (1971)

H.Conde, M.Holmberg

Prompt ν-Bar in Spontaneous and Neutron Induced Fission of ²³⁶U and its Half-Life for Spontaneous Fission

RADIOACTIVITY, Fission ²³⁶U (SF), ²³⁸U (SF); measured T_1/2 ratio.

NUCLEAR REACTIONS ²³⁶U(n, F), E=0.8-6.7 MeV; measured energy dependence of prompt ν-bar.

doi: 10.1016/0022-3107(71)90065-7

1971JA07

Phys.Rev. C4, 1889 (1971)

A.H.Jaffey, K.F.Flynn, L.E.Glendenin, W.C.Bentley, A.M.Essling

Precision Measurement of Half-Lives and Specific Activities of ²³⁵U and ²³⁸U

RADIOACTIVITY ^235,238U; measured T_1/2.

doi: 10.1103/PhysRevC.4.1889

1971KL14

Geochim.Cosmochim.Acta 35, 637 (1971)

J.D.Kleeman, J.F.Lovering

A Determination of the Decay Constant for Spontaneous Fission of Natural Uranium Using Fission Track Accumulation

RADIOACTIVITY, Fission ²³⁸U(SF); measured T_1/2.

1971KO31

Izv.Akad.Nauk SSSR, Ser.Fiz. 35, 1550 (1971); Bull.Acad.Sci.USSR, Phys.Ser. 35, 1413 (1972)

A.L.Komov, L.A.Malov, V.G.Solovev

One-Phonon States in Even-Even Nuclei and Nonrotational States in Some Odd Nuclei in the Actinide Region

NUCLEAR STRUCTURE ^{234,236,238,240}U, ^{236,238,240,242,244}Pu, ^{240,242,244,246,248}Cm, ^246,248,250Cf, ^248,250Fm; calculated 1-phonon states, B(E3). ²³⁹U, ^235,239Np, ^237,243Pu, ^243,245Am, ²⁴³Cm, ²⁴⁷Bk; calculated non-rotational states.

1971LE11

Nucl.Instrum.Methods 91, 577 (1971)

M.P.T.Leme, C.Renner, M.Cattani

Determination of the Decay Constant for Spontaneous Fission of ²³⁸U

RADIOACTIVITY, Fission ²³⁸U(SF); measured T_1/2.

1971SA08

J.Inorg.Nucl.Chem. 33, 1509 (1971)

D.D.Sabu

On Mass-Yield of Xenon and Krypton Isotopes in the Spontaneous Fission Of Uranium

RADIOACTIVITY, Fission ²³⁸U(SF); measured Kr, Xe fission yields; reevaluated T_1/2(SF).

doi: 10.1016/0022-1902(71)80448-7

1971TH17

Acta Phys.Austr. 33, 375 (1971)

W.M.Thury

Die Bestimmung der Spontanspaltrate von U-238 mit Hilfe der Messung von Korrelationsfunktionen dritter Ordnung

RADIOACTIVITY ²³⁸U; measured T_1/2.

1972MC19

Z.Phys. 253, 289 (1972)

W.R.McMurray, I.J.van Heerden

The Level Structures of the Nuclei ²³²Th and ²³⁸U

NUCLEAR REACTIONS ²³²Th, ²³⁸U(n, n'γ), E < 1.9 MeV; measured σ(E;Eγ), Eγ, Iγ. ²³²Th, ²³⁸U deduced levels, γ-branching. Ge(Li) detectors.

1972NI19

Ganseki Kobutsu Kosho Gakkaishi 67, 139 (1972)

S.Nishimura

On the Value of the Decay Constant for Spontaneous Fission of ²³⁸U

RADIOACTIVITY, Fission ²³⁸U(SF); measured T_1/2.

1973KH10

Radiat.Eff. 17, 133 (1973)

H.A.Khan, S.A.Durrani

Measurement of Spontaneous-Fission Decay Constant of ²³⁸U with a Mica Solid State Track Detector

RADIOACTIVITY, Fission ²³⁸U(SF); measured T_1/2.

1974DU09

Acta Phys.Pol. B5, 725 (1974)

W.Dudek

Coupling between Quadrupole and Hexadecapole Degrees of Freedom

NUCLEAR STRUCTURE ²³⁸U, ^238,240Pu; calculated energies of quadrupole, hexadecapole vibrational states.

1974IV04

At.Energ. 36, 403 (1974); Sov.At.Energy 36, 514 (1974)

K.N.Ivanov, K.A.Petrzhak

Probability of Fission by 1.33-MeV γ-Rays and Spontaneous Fission Half-Life for ²³⁸U

RADIOACTIVITY, Fission ²³⁸U(SF); measured T_1/2.

NUCLEAR REACTIONS ²³⁸U(γ, F), E(max)=1.332 MeV; measured fission rate. ²³⁸U(SF) deduced T_1/2.

1974ME18

Nucl.Phys. A224, 429 (1974)

R.D.Meeker, G.M.Kalvius, B.D.Dunlap, S.L.Ruby, D.Cohen

Hyperfine Interactions and Nuclear Moments in Even Uranium Isotopes from Mossbauer Spectroscopy

NUCLEAR REACTIONS ^234,236,238U(γ, γ'); measured hyperfine splitting, Mossbauer effect. ^234,236,238U levels deduced μ, quadrupole moment ratios.

doi: 10.1016/0375-9474(74)90547-8

1975EM03

Nucl.Instrum.Methods 128, 355 (1975)

V.Emma, S.Lo Nigro

Decay Constant for Spontaneous Fission of ²³⁸U and ²³²Th

RADIOACTIVITY, Fission ²³⁸U(SF), ²³²Th(SF); measured decay constant.

1975IVZZ

JINR-E4-9070 (1975)

S.P.Ivanova, A.L.Komov, G.Kyrchev, V.G.Soloviev, C.Stoyanov

On the Anharmonicity of Vibrational States with K = 2⁺, 0^-, 1^- and 2^- in Doubly Even Deformed Nuclei 228 ≤ A ≤ 240

NUCLEAR STRUCTURE Xe, Ba, Ce; calculated β.

1975LEZR

CEA-N-1798, p.121 (1975)

A.Le Brun, R.Perrier

Calcul d'Etats Non-Rotationnels dans les Actinides par un Modele R.P.A. Schematique

NUCLEAR STRUCTURE ^228,230Th, ^{232,234,236,238,240,242,244}U, ^{236,238,240,242,244}Pu; calculated non-rotational levels.

1975WA37

Geochim.Cosmochim.Acta 39, 1279 (1975)

G.A.Wagner, G.M.Reimer, B.S.Carpenter, H.Faul, R.Van der Linden, R.Gubels

The Spontaneous Fission Rate of U-238 and Fission Track Dating

RADIOACTIVITY, Fission ²³⁸U(SF); measured T_1/2, spontaneous fission rate.

1976AZ01

Phys.Rev. C13, 1702 (1976)

N.Azziz, J.C.Palathingal, R.Mendez-Placido

Treatment of Centrifugal Elastic Stresses in Nuclear Rotation

NUCLEAR STRUCTURE ¹⁵⁴Gd, ^160,162,164Dy, ^176,178,180Hf, ^{232,234,236,238}U; analyzed rotational levels using elastic stress analysis.

doi: 10.1103/PhysRevC.13.1702

1976RA02

Phys.Rev. C13, 229 (1976)

J.Randrup, S.E.Larsson, P.Moller, S.G.Nilsson, K.Pomorski, A.Sobiczewski

Spontaneous-Fission Half-Lives for Even Nuclei with Z ≥ 92

RADIOACTIVITY, Fission ^{232,234,236,238}U, ^{236,238,240,242,244}Pu, ^{240,242,244,246,248,250}Cm, ^{246,248,250,252,254}Cf, ^{244,246,248,250,252,254,256,258,260,262,264}Fm, ^{252,254,256,258}No; calculated (SF)T_1/2. ^{252,254,256,258}No, ^{256,258,260,262}Rf, ^{260,262,264,266}Sg, ^{260,262,264,266,268,270}Hs; calculated Qα, α-decay T_1/2.

doi: 10.1103/PhysRevC.13.229

1976RA04

Nucl.Phys. A258, 109 (1976)

A.A.Raduta, R.M.Dreizler

On the Description of the Ground-State Bands by Means of a Boson Hamiltonian

NUCLEAR STRUCTURE ¹⁰²Pd, ¹²⁶Ba, ^148,152Sm, ^154,156Dy, ^{166,168,170,172,174}Hf, ^{182,184,186,190}Pt, ²³⁸U; calculated levels.

doi: 10.1016/0375-9474(76)90532-7

1976TH12

Earth Planet.Sci.Lett. 30, 50 (1976)

K.Thiel, W.Herr

The ²³⁸U Spontaneous Fission Decay Constant Re-Determined by Fission Tracks

RADIOACTIVITY, Fission ²³⁸U(SF); measured fission tracks in glass; deduced decay constant.

1976VO01

Phys.Lett. 60B, 431 (1976)

P.Vogel

Negative Parity Yrast States in Deformed Nuclei

NUCLEAR STRUCTURE ²³⁸U, ¹⁶²Er; calculated levels.

doi: 10.1016/0370-2693(76)90699-7

1977MA23

Phys.Rev. C16, 1179 (1977)

C.W.Ma, J.O.Rasmussen

Microscopic Calculations of High-Spin Rotational States

NUCLEAR STRUCTURE ¹⁶²Er, ¹⁶⁸Yb, ¹⁷⁴Hf, ²³⁸U; calculated high-spin rotational states. Diagonalization cranking model using BCS, fully particle-number-projection wave functions.

doi: 10.1103/PhysRevC.16.1179

1977RA25

Rev.Roum.Phys. 22, 613 (1977)

A.A.Raduta, C.Sabac

Upon a Simplified Version of the Coherent-States-Model for the Yrast Bands of Even-Even Nuclei

NUCLEAR STRUCTURE ¹⁵⁴Gd, ¹⁵⁶Dy, ¹⁶⁶Yb, ¹⁵⁸Er, ^{166,168,170,172,174}Hf, ^182,184Os, ^184,186Pt, ²³⁸U; calculated levels in yrast band.

1978BA46

Phys.Scr. 18, 167 (1978)

M.Badea, A.A.Raduta, H.Stock

Upon an Extension of the Coherent State Model to the Description of the Negative Parity Bands

NUCLEAR STRUCTURE ¹⁵⁰Sm, ¹⁵²Gd, ²³⁸U; calculated ground-state band levels.

1978BEYR

JINR-P4-11982 (1978)

R.B.Begzhanov, I.N.Mikhailov, R.Kh.Safarov, B.Choriev

Anomalous Moment of Inertia and the Coriolis Interaction in the Actinides.

NUCLEAR STRUCTURE ^236,238U, ²³²Th; calculated rotational band spectra. Matrix elements of Coriolis interaction given by semi-microscopic theory.

1978DE41

Atlas of Gamma-Ray Spectra from the Inelastic Scattering of Reactor Fast Neutrons, Part I and II, Atomizdat, Moscow (1978)

A.M.Demidov, I.Govor, Yu.K.Cherepantsev, M.R.Ahmed, S.Al-Najjar, M.A.Al-Amili, N.Al-Assafi, N.Rammo

COMPILATION Z=3-92; compiled experimental values of Eγ, Iγ, decay schemes, energy levels.

1978GE10

Phys.Scr. 18, 311 (1978)

S.Gerstenkorn, J.Chauville, F.Tomkins

Deplacements Isotopiques et Moments Quadrupolaires Intrinseques des Isotopes Pairs 234, 236 et 238 de l'Uranium

NUCLEAR MOMENTS ^234,236,238U; measured isotope shift; deduced quadrupole moment. Relative optical isotope shift method.

1978KA40

Nucl.Instrum.Methods 154, 335 (1978)

M.Kase, J.Kikuchi, T.Doke

Half-Life of ²³⁸U Spontaneous Fission and Its Fragment Kinetic Energies

RADIOACTIVITY ²³⁸U(SF); measured T_1/2, fragment kinetic energy. Cylindrical gridded ionization chamber.

1978KO03

Z.Phys. A284, 233 (1978)

J.Konijn, F.W.N.de Boer, P.Koldewijn, R.Beetz, L.K.Peker

Aligned Rotation of Octupole-Vibrational States in Deformed Nuclei

NUCLEAR STRUCTURE ¹⁵⁴Gd, ¹⁵⁶Dy, ¹⁶²Er, ²³⁸U; calculated levels. VMI model.

1978RI07

Ann.Acad.Brasil.Cienc. 50, 303 (1978)

D.M.de C.Rizzo

Fissao Espontanea do ²³⁸U e Medida da sua Constante de Desintegracao

RADIOACTIVITY ²³⁸U(SF); measured decay constant.

1978TO13

Prog.Theor.Phys. 60, 1002 (1978)

M.Toyama

Level Energies and B(E2) Ratios of the Deformed Even Nuclei in the Actinide Region

NUCLEAR STRUCTURE ^228,230,232Th, ^{232,234,236,238}U, ^238,240Pu, ²⁴⁶Cm, ²⁵⁰Cf; calculated energies of ground state rotational band, B(E2). Collective Hamiltonian, anharmonic term in β-vibration plus rotation, adiabatic treatment.

1979AT01

J.Inorg.Nucl.Chem. 41, 1 (1979)

M.Attrep, Jr., W.B.Ledbetter, D.K.Riddle

The Effects of Boron and Lithium on the Ratio of Induced to Spontaneous Fission in Natural Uranium

RADIOACTIVITY, Fission ²³⁸U (SF); measured activity; deduced effect of lithium, boron on T_1/2(SF) from changes in ²³⁵U(n, F) yield. Natural uranium source.

doi: 10.1016/0022-1902(79)80383-8

1979UL01

Phys.Rev.Lett. 42, 1596 (1979)

G.Ulfert, V.Metag, D.Habs, H.J.Specht

Quadrupole Moment of the 200-ns Fission Isomer in ²³⁷U

NUCLEAR REACTIONS ²³⁸U(d, pn), E=20 MeV; measured yield of fission-isomeric recoil. ^238mU level deduced quadrupole moment.

doi: 10.1103/PhysRevLett.42.1596

1980MIZL

Proc.Intern.Conf. on Nuclear Cross Section for Technology, Knoxville, 1979, p.680 (1980); NBS-SP-594 (1980)

A.Mittler, G.P.Couchell, W.A.Schier, S.Ashar, J.H.Chang, A.T.Y.Wang

Neutron Inelastic Scattering Cross Sections of ²³⁸U via (n, n'γ)

NUCLEAR REACTIONS ²³⁸U(n, n'γ), E=0.7-1.96 MeV; measured Eγ, Iγ, γ production σ(E). ²³⁸U deduced levels, γ transitions, level production σ.

1980PO09

Nucl.Instrum.Methods 178, 163 (1980)

A.G.Popeko, G.M.Ter-Akopian

Measurement of the ²³⁸U Spontaneous-Fission Halflife by Detecting Prompt Neutrons

RADIOACTIVITY, Fission ²³⁸U(SF); measured T_1/2. ³He-filled proportional counter neutron detector.

1980SP10

Ann.Acad.Brasil.Cienc. 52, 213 (1980)

E.R.V.Spaggiari

Determinacao do Alcance Efectivo de Fragmentos de Fissao no UO₂ e da Constante de Desintegracao para a Fissao Espontanea do Uranio-238

NUCLEAR STRUCTURE ^238,235U; measured not abstracted; deduced fission characteristics.

1981BA70

Ann.Acad.Brasil.Cienc. 53, 437 (1981)

Z.N.R.Baptista, M.S.M.Mantovani, F.B.Ribeiro

Contribuicao para a Determinacao da Constante de Fissao Espontanea do Uranio

NUCLEAR STRUCTURE ²³⁸U; measured not abstracted; deduced SF-decay constant.

1981GR10

Phys.Scr. 24, 337 (1981)

E.Grosse, A.Balanda, H.Emling, F.Folkmann, P.Fuchs, R.B.Piercey, D.Schwalm, R.S.Simon, H.J.Wollersheim, D.Evers, H.Ower

Collective Rotation of ²³⁸U at High Spins

NUCLEAR REACTIONS ²³⁸U(²⁰⁸Pb, ²⁰⁸Pb'), E=5.3, 5.9 MeV/nucleon; measured Eγ, Iγ, γγ-coin, Coulomb excitation, DSA. ²³⁸U deduced ground state band B(E2), T_1/2, octupole bands, high-spin state collectivity. Rigid rotor description.

1982DE22

Nucl.Instrum.Methods 197, 417 (1982)

H.G.De Carvalho, J.B.Martins, E.L.Medeiros, O.A.P.Tavares

Decay Constant for the Spontaneous-Fission Process in ²³⁸U

RADIOACTIVITY, Fission ²³⁸U(SF); measured decay constant. Etched track technique.

1983BE66

At.Energ. 55, 97 (1983); Sov.At.Energy 55, 528 (1983)

S.N.Belenky, M.D.Skorokhvatov, A.V.Etenko

Measurement of the Characteristics of Spontaneous Fission of ²³⁸U and ²³⁶U

RADIOACTIVITY ^238,236U(SF); measured T_1/2, prompt neutron average number per fission, its variance.

1983FA15

Z.Phys. A313, 351 (1983)

H.R.Faust

On the Octupole Excitation in ²³⁶U

NUCLEAR REACTIONS ²³⁶U(n, e^-), E=thermal; measured I(ce). ²³⁶U deduced subshell ICC. Electron penetration formalism.

1984BLZS

INDC(CCP)-240/G, Vol.3, p.3 (1984)

M.V.Blinov, B.D.Stsiborsky, A.A.Filatenkov, B.M.Shiryaev

γ-Radiation Spectra Produced by the Interaction of 3 MeV Neutrons with ²³²Th, ²³⁵U and ²³⁸U

NUCLEAR REACTIONS ²³²Th, ^235,238U(n, n'γ), E=3 MeV; measured Eγ, Iγ. ²³²Th, ^235,238U deduced levels.

1984VA34

Helv.Phys.Acta 57, 292 (1984)

R.Vartanian

Spontaneous Fission Decay Constant of ²³⁸U: Measured by fission track technique

RADIOACTIVITY ²³⁸U(SF); measured SF decay constant. Fission track technique.

1984VA35

Helv.Phys.Acta 57, 416 (1984)

R.Vartanian

Spontaneous Fission Decay Constant of ²³⁸U: Measured by the fission track technique

RADIOACTIVITY ²³⁸U(SF); measured SF decay constant. Fission track technique.

1985IV01

Nucl.Instrum.Methods 234, 152 (1985)

M.P.Ivanov, G.M.Ter-Akopian, B.V.Fefilov, A.S.Voronin

Study of ²³⁸U Spontaneous Fission using a Double Ionization Chamber

RADIOACTIVITY ²³⁸U(SF); measured fission fragment total kinetic energy, mass, energy distributions, T_1/2(SF).

1987RA01

At.Data Nucl.Data Tables 36, 1 (1987)

S.Raman, C.H.Malarkey, W.T.Milner, C.W.Nestor, Jr., P.H.Stelson

Transition Probability, B(E2), from the Ground to the First-Excited 2⁺ State of Even-Even Nuclides

COMPILATION A=6-254; compiled, evaluated 2⁺ level energies, B(E2), T_1/2, β₂, β₂/β₂(sp), EWSR, intrinsic quadrupole moments.

doi: 10.1016/0092-640X(87)90016-7

1988HE02

Nucl.Phys. A476, 39 (1988)

R.D.Heil, H.H.Pitz, U.E.P.Berg, U.Kneissl, K.D.Hummel, G.Kilgus, D.Bohle, A.Richter, C.Wesselborg, P.von Brentano

Observation of Orbital Magnetic Dipole Strength in the Actinide Nuclei ²³²Th and ²³⁸U

NUCLEAR REACTIONS ²³²Th, ²³⁸U(e, e'), E=20.2-55.9 MeV; measured σ(E(e^-)), θ=165°. ²³²Th, ²³⁸U(γ, γ'), E=2.9-4.1 MeV bremsstrahlung; measured Eγ, Iγ. ²³²Th, ²³⁸U deduced levels, J, π, B(M1), transition form factors.

doi: 10.1016/0375-9474(88)90371-5

1989MA54

Nucl.Phys. A502, 363c (1989)

V.E.Makarenko, Yu.D.Molchanov, G.A.Otroshchenko, G.B.Yankov

Ternary Fission of Neutron Induced Uranium Fissioning Isomers

RADIOACTIVITY ^236m,238mU(SF) [from ^238,236U(n, n'), E=4.5 MeV]; measured T_1/2, fission fragment; deduced relative fission probabilities.

doi: 10.1016/0375-9474(89)90675-1

1994MC03

Nucl.Phys. A571, 569 (1994)

F.K.McGowan, W.T.Milner

Coulomb Excitation of States in ²³⁸U

NUCLEAR REACTIONS ²³⁸U(α, α'γ), E=18 MeV; measured Iγ, Eγ, γ(θ) following Coulomb excitation. ²³⁸U levels deduced B(λ), J, π, δ.

doi: 10.1016/0375-9474(94)90226-7

1994MC04

Phys.Rev. C49, 3346 (1994)

R.J.McLeod

Klein-Gordon Versus Relativistic Schrodinger Equations in Pion-Nucleus Scattering

NUCLEAR REACTIONS ⁴⁰Ca(π⁺, π⁺), E=180-500 MeV; calculated σ(θ); deduced models difference. Relativistic Schrodinger, Klein-Gordon equations.

doi: 10.1103/PhysRevC.49.3346

1994MI14

J.Phys.(London) G20, L67 (1994)

N.Minkov, R.P.Roussev, P.P.Raychev

Shell Correlations in the SU(q)(2) Rotor Model

NUCLEAR STRUCTURE ¹⁴⁶Gd, ^{170,172,174,176,178}Hf, ^164,166Er, ^{170,172,174,168,176}Yb, ^228,230,232Th, ^{230,232,234,236,238}U, ^{236,238,240,242,244}Pu, ²⁴⁸Cm; calculated spectra; deduced nucleon pairs number, quantum algebraic parameter τ correlation. Data comparison, SU(q)(2) rotor model.

doi: 10.1088/0954-3899/20/6/002

1994TR09

Nucl.Phys. A576, 351 (1994)

D.Troltenier, J.P.Draayer, P.O.Hess, O.Castanos

Investigations of Rotational Nuclei via the Pseudo-Symplectic Model

NUCLEAR STRUCTURE ¹⁶⁰Dy, ¹⁶⁸Er, ^234,236,238U; calculated levels, B(λ), static quadrupole moments; deduced model limiting features. Pseudo-symplectic theory, review.

doi: 10.1016/0375-9474(94)90249-6

1995ZI02

Phys.Rev. C52, R468 (1995)

A.Zilges, P.von Brentano, R.-D.Herzberg, U.Kneissl, J.Margraf, H.Maser, N.Pietralla, H.H.Pitz

Strong Dipole Excitations Around 1.8 MeV in ²³⁸U

NUCLEAR REACTIONS ²³⁸U(γ, γ'), E=1.5-2.0 MeV; measured Eγ, Iγ. ²³⁸U deduced levels, J, π, γ-multipolarity, K-quantum number, γ-branching, Γ₀, T_1/2, B(λ). High resolution strudy.

doi: 10.1103/PhysRevC.52.R468

1996EL03

Phys.Rev.Lett. 76, 1031 (1996); Erratum Phys.Rev.Lett. 77, 4278 (1996)

S.R.Elliott, P.Beiersdorfer, M.H.Chen

Trapped-Ion Technique for Measuring the Nuclear Charge Radii of Highly Charged Radioactive Isotopes

NUCLEAR MOMENTS ^233,238U; measured charge radii. Crystal spectrometer, X-ray spectra analysis.

doi: 10.1103/PhysRevLett.76.1031

1996WA11

Nucl.Phys. A600, 88 (1996)

D.Ward, H.R.Andrews, G.C.Ball, A.Galindo-Uribarri, V.P.Janzen, T.Nakatsukasa, D.C.Radford, T.E.Drake, J.DeGraaf, S.Pilotte, Y.R.Shimizu

Rotational Bands in ²³⁸U

NUCLEAR REACTIONS ²³⁸U(²⁰⁹Bi, ²⁰⁹Bi'), E=1.13, 1.33 GeV; measured Eγ, Iγ, γγ-coin following Coulomb excitation. ²³⁸U deduced levels, J, π, K, band structure. Compton suppressed hyperpure Ge detector array, 4π-BGO ball. Cranked RPA calculation.

doi: 10.1016/0375-9474(95)00490-4

1998TS13

J.Phys.Soc.Jpn. 67, 2641 (1998)

S.Tsutsui, S.Nasu, M.Nakada, N.M.Masaki, M.Saeki, K.Ikushima, H.Yasuoka, A.Nakamura

Nuclear Magnetic Moment of the First Excited State (I = 2⁺) of ²³⁸U

NUCLEAR REACTIONS ²³⁸U(γ, γ), E=44.91 keV; measured Mossbauer spectra vs temperature. ²³⁸U deduced excited state magnetic moment.

2000HO27

Pure Appl.Chem. 72, 1525 (2000); Erratum Pure Appl.Chem. 73, 1225 (2001)

N.E.Holden, D.C.Hoffman

Spontaneous Fission Half-Lives for Ground-State Nuclides (Technical Report)

COMPILATION ²⁰⁸Pb, ^230,232Th, ²³¹Pa, ^{230,232,233,234,235,236,238}U, ²³⁷Np, ^{236,238,239,240,241,242,244}Pu, ^241,242m,243Am, ^{240,242,243,244,245,246,248,250}Cm, ²⁴⁹Bk, ^{237,238,240,242,246,248,249,250,252,254,256}Cf, ^{253,254,254m,255}Es, ^{242,243,244,245,246,248,250,250m,252,254,255,256,257,258,259,260}Fm, ^{245,247,248,255,256,257,258,258m,259,260}Md, ^{250,251,252,254,254m,256,257,258,259,260,262}No, ^{252,253,254,255,256,257,258,259,261,262}Lr, ^{253,254,255,256,257,258,259,260,261,262}Rf, ^{255,256,257,258,260,261,262,262}Db, ^{258,259,260,261,263,265,266}Sg, ^261,262,262mBh, ^264,265,267Hs, ²⁶⁶Mt; compiled, evaluated spontaneous fission T_1/2.

2001AF12

Acta Phys.Hung.N.S. 13, 139 (2001)

A.V.Afanasjev, P.Ring

Properties of Superdeformed Fission Isomers in the Cranked Relativistic Hartree-Bogoliubov Theory

NUCLEAR STRUCTURE ^236,238U, ^236,239,240Pu, ²⁴²Am; calculated superdeformed fission isomers moments of inertia, quadrupole moments. Cranked relativistic Hartree-Bogoliubov theory, comparison with data.

doi: 10.1556/APH.13.2001.1-3.15

2001BE81

Geochim.Cosmochim.Act. 65, 111 (2001)

F.Begemann, K.R.Ludwig, G.W.Lugmair, K.Min, L.E.Nyquist, P.J.Patchett, P.R.Renne, C.-Y.Shih, I.M.Villa, R.J.Walker

Call for an improved set of decay constants for geochronological use

RADIOACTIVITY ⁴⁰K, ⁸⁷Rb, ¹⁴⁷Sm, ¹⁷⁶Lu, ¹⁸⁷Re, ¹⁹⁰Pt, ^235,238U; compiled, analyzed T_1/2. Application to geo- and cosmochronology discussed.

2001BU02

Phys.Rev. C63, 014312 (2001)

B.Buck, A.C.Merchant, S.M.Perez

Transition Quadrupole Moments in Superdeformed Bands

NUCLEAR STRUCTURE ^60,62Zn, ^80,82Sr, ^84,86Zr, ¹³²Ce, ¹³⁴Nd, ¹⁴²Sm, ^146,148,150Gd, ^152,154Dy, ^190,192,194Hg, ^194,196Pb, ^236,238U; calculated superdeformed bands transition quadrupole moments; deduced cluster configuration features. Binary cluster model, comparisons with data.

doi: 10.1103/PhysRevC.63.014312

2001DE45

Nucl.Phys. A695, 95 (2001)

P.Demetriou, S.Goriely

Microscopic Nuclear Level Densities for Practical Applications

NUCLEAR STRUCTURE ²⁹Si, ⁴⁵Ca, ⁵⁴Cr, ⁶⁰Co, ⁶²Ni, ⁷²Ga, ⁸¹Se, ⁸⁷Sr, ^93,96Mo, ¹⁰⁴Rh, ¹¹¹Cd, ¹¹⁸Sn, ¹²⁷Te, ¹³¹Ba, ¹⁴³Ce, ¹⁴⁸Sm, ¹⁵⁵Eu, ¹⁶²Dy, ¹⁷⁰Tm, ¹⁷⁷Lu, ¹⁸³W, ¹⁹²Ir, ^208,209Pb, ²¹⁰Bi, ²³⁸U; calculated level density distributions. Global microscopic model.

doi: 10.1016/S0375-9474(01)01095-8

2001FA07

Chin.Phys.Lett. 18, 193 (2001)

X.-Z.Fang, T.-N.Ruan

Analysis of the Yrast Bands with q-Deformed Moment of Inertia

NUCLEAR STRUCTURE ¹⁵⁶Gd, ^162,164Dy, ^164,166Er, ^{168,170,172,174,176}Yb, ^{170,172,174,176,178}Hf, ^228,230,232Th, ^236,238U, ^{236,238,240,242,244}Pu, ²⁴⁸Cm; calculated yrast rotational band parameters. Comparisons with data.

doi: 10.1088/0256-307X/18/2/313

2001GA55

Phys.Rev. C64, 047303 (2001)

Z.Gacsi, M.Csatlos, A.Krasznahorkay, D.Sohler, J.Gulyas, J.Timar, M.Hunyadi, J.L.Weil, J.van Klinken

Low-Lying, Excited K = 0 Bands in ²³⁸U

NUCLEAR REACTIONS ^234,236,238U(α, α'), E=19 MeV; measured Eγ, Iγ, E(ce), I(ce) following Coulomb excitation. ²³⁸U deduced transitions ICC, enhancement of E0 strength, K=0 bands moments of inertia.

doi: 10.1103/PhysRevC.64.047303

2001GO07

Nucl.Phys. A683, 383 (2001)

E.Gotsman, E.Levin, U.Maor, L.McLerran, K.Tuchin

Higher Twists and Maxima for DIS on Nuclei in High Density QCD Region

NUCLEAR STRUCTURE A=30; Zn, ¹¹⁹Sn, ²³⁸U; calculated structure functions, twist contributions for deep inelastic scattering.

doi: 10.1016/S0375-9474(00)00464-4

2001IC02

Prog.Theor.Phys.(Kyoto) 105, 915 (2001)

T.Ichikawa, T.Wada, M.Ohta

Fission Width of Compound Nuclei Calculated Using the Mean First Passage Time Method

NUCLEAR STRUCTURE ²³⁸U; calculated fission width vs angular momentum. Mean first passage time method.

NUCLEAR REACTIONS ¹⁰⁰Mo, ¹¹⁰Pd(¹⁰⁰Mo, X), ¹¹⁰Pd(¹¹⁰Pd, X), E(cm)=170-290 MeV; calculated fission barrier, evaporation residue σ. Mean first passage time method.

2001MA66

Yad.Fiz. 64, No 6, 1228 (2001); Phys.Atomic Nuclei 64, 1152 (2001)

L.Majling, Yu.A.Batusov

Spectroscopy of the Λ Hypernuclei: New problems and prospects

NUCLEAR STRUCTURE ^3,4H, ^4,5He, ⁹Be, ¹¹B, ¹²C, ¹⁶O, ²⁸Si, Fe, ²⁰⁹Bi, ²³⁸U; analyzed hypernucleus decay features.

doi: 10.1134/1.1383633

2001MI34

Phys.Rep. 354, 157 (2001)

G.E.Mitchell, J.D.Bowman, S.I.Penttila, E.I.Sharapov

Parity Violation in Compound Nuclei: Experimental methods and recent results

NUCLEAR STRUCTURE ⁸¹Br, ⁹³Nb, ¹⁰³Rh, ^107,109Ag, ^{104,105,106,108}Pd, ¹¹³Cd, ¹¹⁵In, ¹¹⁷Sn, ^121,123Sb, ¹²⁷I, ¹³¹Xe, ¹³³Cs, ¹³⁹La, ²³²Th, ²³⁸U; compiled, analyzed resonance parameters, parity nonconserving asymmetry data.

doi: 10.1016/S0370-1573(01)00016-3

2001MO13

Nature(London) 409, 785 (2001)

P.Moller, D.G.Madland, A.J.Sierk, A.Iwamoto

Nuclear Fission Modes and Fragment Mass Asymmetries in a Five-Dimensional Deformation Space

NUCLEAR STRUCTURE ²²⁸Ra, ²³⁴U, ^256,258Fm; calculated potential energy surfaces; deduced fission mode features. ^{220,222,224,226,228,230,232}Th, ^{228,230,232,234,236,238,240}U, ^{234,236,238,240,242,244,246}Pu, ^{240,242,244,246,248,250,252}Cm, ^{246,248,250,252,254,256,258}Cf, ^{246,248,250,252,254,256,258}Fm; calculated average fragment mass division in asymmetric fission. Five-dimensional shape-coordinate grid. Comparisons with data.

doi: 10.1038/35057204

2001MO28

Phys.Lett. 515B, 269 (2001)

J.Morgenstern, Z.-E.Meziani

Is the Coulomb Sum Rule Violated in Nuclei ?

NUCLEAR STRUCTURE ^40,48Ca, ⁵⁶Fe, ¹⁹⁷Au, ²⁰⁸Pb, ²³⁸U; analyzed electron scattering response functions; deduced quenching, no saturation of Coulomb sum.

doi: 10.1016/S0370-2693(01)00873-5

2001SA54

Yad.Fiz. 64, No 8, 1496 (2001); Phys.Atomic Nuclei 64, 1419 (2001)

A.R.Safarov, R.Kh.Safarov, A.S.Sitdikov

Parity Splitting in Nuclei Involving Octupole Correlations and the Alignment of the Angular Momentum

NUCLEAR STRUCTURE ^224,226,228Ra, ^{226,228,230,232}Th, ^{230,232,234,236,238}U; calculated rotational bands parity-splitting energy, angular momentum alignment.

doi: 10.1134/1.1398934

2001TR19

Phys.Rev.Lett. 87, 082501 (2001)

A.Trzcinska, J.Jastrzebski, P.Lubinski, F.J.Hartmann, R.Schmidt, T.von Egidy, B.Klos

Neutron Density Distributions Deduced from Antiprotonic Atoms

NUCLEAR REACTIONS ^40,48Ca, ^54,56,57Fe, ⁵⁹Co, ^58,60,64Ni, ^90,96Zr, ^{112,116,120,124}Sn, ¹¹⁶Cd, ¹²⁸Te, ²⁰⁸Pb, ²⁰⁹Bi, ²³²Th, ²³⁸U(p-bar, X), E at rest; measured x-ray spectra, residual annihilation yields. ^40,48Ca, ^54,56,57Fe, ⁵⁹Co, ^58,60,64Ni, ^90,96Zr, ^{112,116,120,124}Sn, ¹¹⁶Cd, ¹²⁸Te, ²⁰⁸Pb, ²⁰⁹Bi, ²³²Th, ²³⁸U deduced neutron radii, density distributions.

doi: 10.1103/PhysRevLett.87.082501

2001TR23

Nucl.Phys. A692, 176c (2001)

A.Trzcinska, J.Jastrzebski, T.Czosnyka, T.von Egidy, K.Gulda, F.J.Hartmann, J.Iwanicki, B.Ketzer, M.Kisielinski, B.Klos, W.Kurcewicz, P.Lubinski, P.J.Napiorkowski, L.Pienkowski, R.Schmidt, E.Widmann

Information on Antiprotonic Atoms and the Nuclear Periphery from the PS209 Experiment

NUCLEAR STRUCTURE ⁴⁸Ca, ^{112,116,120,124}Sn, ²⁰⁸Pb; analyzed antiproton annihilation data; deduced neutron-to-proton density ratios.

ATOMIC PHYSICS ¹⁶O, ^{40,42,43,44,48}Ca, ^54,56,57,58Fe, ⁵⁹Co, ^58,60,62,64Ni, ^90,96Zr, ^106,116Cd, ^{112,116,120,124}Sn, ^{122,124,126,128,130}Te, ^172,176Yb, ²⁰⁸Pb, ²⁰⁹Bi, ²³²Th, ²³⁸U; measured antiprotonic atoms strong interaction level widths, shifts.

doi: 10.1016/S0375-9474(01)01176-9

2002BA52

Czech.J.Phys. 52, 567 (2002)

A.S.Barabash

Average (Recommended) Half-Life Values for Two-Neutrino Double-Beta Decay

RADIOACTIVITY ⁴⁸Ca, ⁷⁶Ge, ⁸²Se, ⁹⁶Zr, ¹⁰⁰Mo, ¹¹⁶Cd, ^128,130Te, ¹⁵⁰Nd, ²³⁸U(2β^-); compiled, analyzed 2ν-accompanied 2β-decay T_1/2.

doi: 10.1023/A:1015369612904

2002BU13

Yad.Fiz. 65, 701 (2002); Phys.Atomic Nuclei 65, 669 (2002)

B.Buck, A.C.Merchant, S.M.Perez

Transition Quadrupole Moments in Superdeformed Bands

NUCLEAR STRUCTURE ^60,62Zn, ^80,82Sr, ^84,86Zr, ¹³²Ce, ¹³⁴Nd, ¹⁴²Sm, ^146,148,150Gd, ^152,154Dy, ^190,192,194Hg, ^194,196Pb, ^236,238U; calculated superdeformed bands transition quadrupole moments. Binary cluster approach, comparisons with data.

doi: 10.1134/1.1471271

2002GA34

Phys.Rev. C66, 034306 (2002)

Y.K.Gambhir, A.A.Bhagwat

Relativistic Mean Field for Nuclear Periphery

NUCLEAR STRUCTURE ⁴⁸Ca, ⁵⁸Ni, ⁹⁶Zr, ^96,104Ru, ¹⁰⁰Mo, ^106,116Cd, ^112,124Sn, ^128,130Te, ^144,154Sm, ¹⁴⁸Nd, ¹⁶⁰Gd, ¹⁷⁶Yb, ²³²Th, ²³⁸U; calculated binding energies, deformation parameters, radii, density distributions, peripheral factors. Relativistic mean field approach, comparisons with data.

doi: 10.1103/PhysRevC.66.034306

2002GI11

Eur.Phys.J. A 15, 209 (2002)

M.Girod, J.Libert, J.P.Delaroche, P.Romain

Microscopic structure of superdeformed states in Th, U, Pu and Cm isotopes with Gogny force

NUCLEAR STRUCTURE ^{226,228,230,232,234}Th, ^{230,232,234,236,238,240}U, ^{240,242,244,246}Pu, ^{242,244,246,248}Cm; calculated normal and superdeformed level energies, collective features. Microscopic mean-field approach, Gogny force. Comparisons with data.

doi: 10.1140/epja/i2001-10256-2

2002HI09

Czech.J.Phys. 52, 513 (2002)

J.G.Hirsch, O.Castanos, P.O.Hess, V.E.Ceron, O.Civitarese

Double-Beta Decay in Deformed Nuclei

RADIOACTIVITY ^146,148,150Nd, ¹⁶⁰Gd, ¹⁸⁶W, ¹⁹²Os, ²³⁸U(2β^-); ¹⁵⁶Dy, ¹⁶²Er, ¹⁶⁸Yb(2EC); calculated 0ν- and 2ν-accompanied 2β-decay T_1/2. Pseudo-SU(3) model, deformed nuclei.

doi: 10.1023/A:1015357210178

2002KA53

J.Nucl.Sci.Technol.(Tokyo) 39, 807 (2002)

T.Kawano, K.Shibata

Uncertainty Analyses in the Resolved Resonance Region of ²³⁵U, ²³⁸U, and ²³⁹Pu with the Reich-Moore R-Matrix Theory for JENDL-3.2

NUCLEAR STRUCTURE ^235,238U, ²³⁹Pu; analyzed data; deduced covariances for resolved resonance parameters. Reich-Moore R-matrix theory.

2002MA85

Acta Phys.Hung.N.S. 16, 419 (2002)

G.Maino

A Simple Model of Superheavy Nuclei

NUCLEAR STRUCTURE ^230,232Th, ^234,236,238U, ^238,242Pu, ^246,248Cm, ²⁵⁴No, ²⁵⁶Rf, ^260,266Sg, ²⁶²No, ²⁶²Rf, ^264,268,270Hs, ²⁷⁸Fl, ²⁹²120; calculated transitions B(E2). Algebraic model, comparisons with data.

doi: 10.1556/APH.16.2002.1-4.44

2002OB01

Eur.Phys.J. D 21, 255 (2002)

M.Oba, K.Akaoka, M.Miyabe, I.Wakaida

Isotope Shift and Hyperfine Structure of the Highly Excited Atomic Uranium

NUCLEAR MOMENTS ^{234,235,236,238}U; measured hfs, isotope shifts. Two-color Doppler-free two-photon absorption technique.

doi: 10.1140/epjd/e2002-00215-y

2002PO16

J.Nucl.Radiochem.Sci. 3, No 1, 43 (2002)

D.N.Poenaru, W.Greiner, Y.Nagame, R.A.Gherghescu

Nuclear Shapes in Complex Fission Phenomena

NUCLEAR STRUCTURE ²³⁸U, ^228,232Th; calculated fission associated deformations, saddle-point deformation energies.

2002RA25

Phys.Rev. C65, 064322 (2002)

A.A.Raduta, D.Ionescu, A.Faessler

Unified Description of Three Positive and Three Negative Parity Interacting Bands

NUCLEAR STRUCTURE ¹⁵⁸Gd, ¹⁷²Yb, ^218,226Ra, ²³²Th, ²³⁸U, ²³⁸Pu; calculated rotational bands moments of inertia, excitation energies, transition probabilities. Unified description of multiple bands, comparison with data.

doi: 10.1103/PhysRevC.65.064322

2002TR04

At.Data Nucl.Data Tables 80, 83 (2002)

V.I.Tretyak, Y.G.Zdesenko

Table of Double Beta Decay Data - An Update

COMPILATION ³⁶Ar, ^40,46,48Ca, ⁵⁰Cr, ⁵⁴Fe, ⁵⁸Ni, ^64,70Zn, ⁷⁶Ge, ^74,80,82Se, ^78,86Kr, ⁸⁴Sr, ^94,96Zr, ^92,98,100Mo, ^96,104Ru, ^102,110Pd, ^{106,108,114,116}Cd, ^102,122,124Sn, ^120,128,130Te, ^{124,126,134,136}Xe, ^130,132Ba, ^136,138,142Ce, ^146,148,150Nd, ^144,154Sm, ^152,160Gd, ^156,158Dy, ^162,164,170Er, ^168,176Yb, ¹⁷⁴Hf, ^180,186W, ^184,192Os, ^190,198Pt, ^196,204Hg, ²³²Th, ²³⁸U; compiled 2β-decay T_1/2, limits.

doi: 10.1006/adnd.2001.0873

2002TR12

Nucl.Instrum.Methods Phys.Res. B194, 229 (2002)

R.K.Tripathi, J.W.Wilson, F.A.Cucinotta

A method for calculating proton-nucleus elastic cross-sections

NUCLEAR REACTIONS ⁹Be, ¹²C, ²⁷Al, ⁵⁶Fe, ²⁰⁸Pb, ²³⁸U(p, p), E ≈ 5-10000 MeV; calculated elastic σ, medium corrections. Comparison with data.

doi: 10.1016/S0168-583X(02)00690-0

2002TS01

J.Phys.(London) G28, 2187 (2002)

A.Tsvetkov, J.Kvasil, R.G.Nazmitdinov

Octupole Deformations in Actinides at High Spins within the Cranking Skyrme-Hartree-Fock Approach

NUCLEAR STRUCTURE ^{218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233}Ra, ^{218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233}Th, ^{223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238}U; calculated dipole, quadrupole, and octupole moments vs angular frequency. Cranked Skyrme-Hartree-Fock approach.

doi: 10.1088/0954-3899/28/8/305

2003AD31

Acta Phys.Pol. B34, 2147 (2003)

G.G.Adamian, A.V.Andreev, N.V.Antonenko, S.P.Ivanova, R.V.Jolos, W.Scheid, T.M.Shneidman

Dinuclear system phenomena in nuclear structure and nuclear reactions

NUCLEAR STRUCTURE ¹⁴⁶Ba, ¹⁴⁸Nd, ²²²Ra, ²⁴²Pu; calculated level energies for alternating-parity states. ¹⁹⁴Hg, ¹⁹⁴Pb, ^234,236,238U, ^236,239,240Pu, ²⁴⁰Am, ^230,231,233Th; calculated cluster states quadrupole moments, related features. Dinuclear system approach, comparison with data.

2003AD32

Acta Phys.Pol. B34, 1729 (2003)

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

Cluster features in reactions and structure of heavy nuclei

NUCLEAR STRUCTURE ^{220,222,224,226}Ra, ^{222,224,226,228,230,232}Th, ^236,238U; calculated levels, J, π, transition moments; deduced cluster effects. Comparison with data.

2003AD34

Acta Phys.Hung.N.S. 18, 311 (2003)

G.G.Adamian, A.V.Andreev, N.V.Antonenko, S.P.Ivanova, N.Nenoff, W.Scheid, T.M.Shneidman

Cluster Interpretation of Highly Deformed Nuclear States

NUCLEAR STRUCTURE ¹⁹⁴Hg, ¹⁹⁴Pb, ^236,238U, ^236,239,240Pu, ²⁴⁰Am, ^230,231,233Th, ^234,236U; calculated superdeformed and hyperdeformed cluster configurations transition energies. Dinuclear system approach.

doi: 10.1556/APH.18.2003.2-4.32

2003BU11

Phys.Rev. C 68, 024313 (2003)

B.Buck, A.C.Merchant, S.M.Perez

Theory of band comparison in even-even nuclei

NUCLEAR STRUCTURE ^142,144,146Ba, ^146,148Ce, ^{146,148,150,152}Nd, ^150,152,154Sm, ^{218,220,222,224,226}Ra, ^{222,224,226,228,230,232,234}Th, ^{230,232,234,236,238}U, ^{236,238,240,242,244}Pu; calculated rotational bands relative μ, B(E2). ^148,150Gd, ^152,154Dy, ^190,192,194Hg, ^194,196Pb; calculated superdeformed bands relative μ, B(E2). ²¹²Pb, ²¹²Po; calculated superdeformed bands features. Cluster model.

doi: 10.1103/PhysRevC.68.024313

2003BU27

Acta Phys.Hung.N.S. 18, 303 (2003)

B.Buck, A.C.Merchant, S.M.Perez

Criteria for Comparison of Bands in Even-Even Nuclei

NUCLEAR STRUCTURE ^142,144,146Ba, ^146,148Ce, ^{146,148,150,152}Nd, ^150,152,154Sm, ^{218,222,224,226}Ra, ^{222,226,228,230,232,234}Th, ^{230,232,234,236,238}U, ^{238,240,242,244}Pu; analyzed rotational bands, fractional change in transition energies and reduced mass. Cluster model.

doi: 10.1556/APH.18.2003.2-4.31

2003CR04

Nucl.Phys. B(Proc.Supp.) S118, 287 (2003)

O.Cremonesi

Neutrinoless Double Beta Decay: Present and Future

RADIOACTIVITY ⁴⁸Ca, ⁷⁶Ge, ⁸²Se, ⁹⁶Zr, ¹⁰⁰Mo, ¹¹⁶Cd, ^128,130Te, ¹³⁶Xe, ¹⁵⁰Nd, ²³⁸U(2β^-); compiled, analyzed 2β-decay T_1/2.

doi: 10.1016/S0920-5632(03)01331-8

2003DE20

Nucl.Instrum.Methods Phys.Res. B211, 15 (2003)

A.Deppman, O.A.P.Tavares, S.B.Duarte, J.D.T.Arruda-Neto, M.Goncalves, V.P.Likhachev, J.Mesa, E.C.de Oliveira, S.R.de Pina, O.Rodriguez

A Monte Carlo method for nuclear evaporation and fission at intermediate energies

NUCLEAR STRUCTURE ²³⁷Np, ²³⁸U, ²³²Th; calculated fissility vs excitation energy, competition with evaporation channels. Monte Carlo approach.

doi: 10.1016/S0168-583X(03)01265-5

2003DE44

Rev.Mod.Phys. 75, 35 (2003)

R.D.Deslattes, E.G.Kessler, Jr., P.Indelicato, L.de Billy, E.Lindroth, J.Anton

X-ray transition energies: new approach to a comprehensive evaluation

COMPILATION Ne, Na, Mg, Al, Si, P, S, Cl, Ar, K, Ca, Sc, Ti, V, Cr, Mn, Fe, Ni, Cu, Zn, Ga, Ge, As, Se, Br, Kr, Rb, Sr, Y, Zr, Nb, Mo, Tc, Ru, Rh, Pd, Ag, Cd, In, Sn, Sb, Te, I, Xe, Cs, Ba, La, Ce, Pr, Nd, Pm, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb, Lu, Hf, Ta, W, Re, Os, Ir, Pt, Au, Hg, Tl, Pb, ²⁰⁹Bi, ²⁰⁹Po, ²¹⁰At, ²²²Rn, ²²³Fr, ²²⁶Ra, ²²⁷Ac, ²³²Th, ²³¹Pa, ^233,238U, ²³⁷Np, ^239,244Pu, ^241,243Am, ^245,248Cm, ^249,250Bk, ^249,250,251Cf, ²⁵¹Es, ²⁵⁴Fm; compiled, analyzed, evaluated E(K X-ray), E(L X-ray) and provide X-rays tabulations.

doi: 10.1103/RevModPhys.75.35

2003FI13

Nucl.Phys. A721, 171c (2003)

E.Fiorini

Searches on Double Beta Decay and Dark Matter

RADIOACTIVITY ⁴⁸Ca, ⁷⁶Ge, ⁸²Se, ⁹⁶Zr, ¹⁰⁰Mo, ¹¹⁶Cd, ^128,130Te, ^134,136Xe, ¹⁵⁰Nd, ²³⁸U(2β); compiled, analyzed 0ν-accompanied 2β-decay T_1/2 and neutrino mass data. Implications for dark matter search discussed.

doi: 10.1016/S0375-9474(03)01030-3

2003GU18

J.Radioanal.Nucl.Chem. 258, 117 (2003)

S.Guedes, J.C.Hadler, J.E.S.Sarkis, K.M.G.Oliveira, M.H.Kakazu, P.J.Iunes, M.Saiki, C.A.Tello, S.R.Paulo

Spontaneous-fission decay constant of ²³⁸U measured by nuclear track techniques without neutron irradiation

RADIOACTIVITY ²³⁸U(α), (SF); measured track densities; deduced fission decay constant.

doi: 10.1023/A:1026218411554

2003HA06

J.Radioanal.Nucl.Chem. 256, 155 (2003)

J.C.Hadler, G.Bigazzi, S.Guedes, P.J.Iunes, M.Oddone, C.A.Tello, S.R.Paulo

Spontaneous ²³⁸U fission half-life measurements based on fission-track techniques

RADIOACTIVITY ²³⁸U(SF); analyzed T_1/2 data. Comparison of fission-track and other techniques. Determination of recommended values discussed.

doi: 10.1023/A:1023328915783

2003HO07

Phys.Rev. C 67, 048501 (2003)

Y.Horikawa, A.Haga

Gauge invariant evaluation of nuclear polarization with the collective model

NUCLEAR MOMENTS ²⁰⁸Pb, ²³⁸U; calculated nuclear polarization energy shifts in hydrogenlike ions.

ATOMIC PHYSICS ²⁰⁸Pb, ²³⁸U; calculated nuclear polarization energy shifts in hydrogenlike ions.

doi: 10.1103/PhysRevC.67.048501

2003LI01

Nucl.Phys. A713, 24 (2003)

V.P.Likhachev, J.Mesa, J.D.T.Arruda-Neto, B.V.Carlson, W.R.Carvalho, Jr., L.C.Chamon, A.Deppman, H.Dias, M.S.Hussein

Quasi-free ²³⁸U(e, e'f) cross section in macroscopic-microscopic approach

NUCLEAR REACTIONS ²³⁸U(e, e'X), E=720 MeV; calculated quasifree electrofission σ(E, θ). Comparison with data.

NUCLEAR STRUCTURE ²³⁸U; calculated single-particle level energies. ^237,238U, ²³⁷Pa; calculated fissility vs excitation energy.

doi: 10.1016/S0375-9474(02)01302-7

2003LI25

Phys.Rev. C 68, 014615 (2003)

V.P.Likhachev, J.D.T.Arruda-Neto, W.R.Carvalho, Jr., A.Deppman, I.G.Evseev, F.Garcia, M.S.Hussein, L.F.R.Macedo, A.Margaryan, J.Mesa, V.O.Nesterenko, O.Rodriguez, S.A.Pashchuk, H.R.Schelin, M.S.Vaudeluci

Inclusive quasifree electrofission cross section for ²³⁸U

NUCLEAR STRUCTURE ^237,238U, ²³⁷Pa; calculated fissility vs excitation energy.

NUCLEAR REACTIONS ²³⁸U(e, e'p), (e, e'), E=300 MeV; calculated σ(E, θ). ²³⁸U(e, F), E=100-250 MeV; measured fission σ; deduced reaction mechanism features.

doi: 10.1103/PhysRevC.68.014615

2003MB02

Bull.Rus.Acad.Sci.Phys. 67, 1763 (2003)

V.M.Maslov, Yu.V.Porodzinsky, M.Baba, A.Hasegawa

Neutron scattering from U and Th nuclei with excitation of collective levels in nuclei

NUCLEAR REACTIONS ^232,238U, ²³²Th(n, n'X), E=1.2 MeV; calculated neutron spectra, role of collective level excitation. Comparison with data.

NUCLEAR STRUCTURE ^232,238U, ²³²Th; calculated levels, J, π.

2003NE06

J.Phys.(London) G29, L37 (2003)

V.O.Nesterenko, V.P.Likhachev, P.-G.Reinhard, J.Mesa, W.Kleinig, J.D.T.Arruda-Neto, A.Deppman

Deformation effects in low-momentum distributions of heavy nuclei

NUCLEAR STRUCTURE ²³⁸U; calculated momentum distributions of deep hole proton states, ground-state quadrupole moments. Comparison of Woods-Saxon and Skyrme-Hartree-Fock approaches.

doi: 10.1088/0954-3899/29/4/101

2003PO15

Europhys.Lett. 64, 164 (2003)

D.N.Poenaru, W.Greiner

Deformation energy minima at finite mass asymmetry

NUCLEAR STRUCTURE ^{226,228,230,232,234,236,238}Th, ^{230,232,234,236,238}U; calculated saddle point deformation energy vs mass asymmetry. Phenomenological shell corrections.

doi: 10.1209/epl/i2003-00612-8

2003RA17

Phys.Rev. C 67, 044312 (2003)

A.A.Raduta, D.Ionescu

New signatures for octupole deformation in some actinide nuclei

NUCLEAR STRUCTURE ²¹⁸Ra, ^228,232Th, ²³⁸Pu, ^{232,234,236,238}U; calculated rotational and vibrational bands transition energies, moments of inertia, octupole deformation effects. Extended coherent state model.

doi: 10.1103/PhysRevC.67.044312

2003SH02

Phys.Rev. C 67, 014313 (2003)

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

Cluster interpretation of properties of alternating parity bands in heavy nuclei

NUCLEAR STRUCTURE ^{222,224,226,228,230,232}Th, ^{220,222,224,226}Ra, ^240,242Pu, ^{232,234,236,238}U, ^144,146,148Ba, ^146,148Ce, ^146,148Nd; calculated alternating parity bands levels, J, π, electric multipole transition moments. Cluster model, comparison with data.

doi: 10.1103/PhysRevC.67.014313

2003ZA01

Phys.Rev. C 67, 014305 (2003)

N.V.Zamfir, D.Kusnezov

Octupole correlations in U and Pu nuclei

NUCLEAR STRUCTURE ^{230,232,234,236,238}U, ^{238,240,242,244}Pu; calculated, analyzed levels, J, π, B(E1), B(E2), B(E3); deduced octupole deformation, correlations. spdf interacting boson model.

doi: 10.1103/PhysRevC.67.014305

2004AD15

Nucl.Phys. A734, 433 (2004)

G.G.Adamian, N.V.Antonenko, R.V.Jolos, Yu.V.Palchikov, W.Scheid, T.M.Shneidman

Manifestation of cluster effects in the structure of medium mass and heavy nuclei

NUCLEAR STRUCTURE ^144,146,148Ba, ¹⁴⁶Ce; calculated alternating parity bands levels, J, π. ⁶⁰Zn; calculated superdeformed band transitions branching ratios. ^{220,222,224,226}Ra, ^{222,224,226,228,230,232}Th, ^234,236,238U; calculated dipole and quadrupole transition moments. Cluster model, comparisons with data.

doi: 10.1016/j.nuclphysa.2004.01.079

2004AD30

Yad.Fiz. 67, 1729 (2004); Phys.Atomic Nuclei 67, 1701 (2004)

G.G.Adamian, N.V.Antonenko, R.V.Jolos, Yu.V.Palchikov, W.Scheid, T.M.Shneidman

Nuclear Structure with the Dinuclear Model

NUCLEAR STRUCTURE ^{232,234,236,238}U, ²²³Ra; calculated rotational bands level energies. ²²⁶Ra; calculated B(E2). ⁶⁰Zn; calculated ground-state band and superdeformed band levels, J, π. Dinuclear system approach.

doi: 10.1134/1.1806910

2004BA16

Int.J.Mod.Phys. E13, 337 (2004)

A.Baran, P.Mierzynski

Nuclear periphery in Mean-Field models

NUCLEAR STRUCTURE ⁴⁸Ca, ⁵⁸Ni, ⁹⁶Zr, ^96,104Ru, ¹⁰⁰Mo, ^106,116Cd, ^112,124Sn, ^128,130Te, ^144,154Sm, ¹⁴⁸Nd, ¹⁶⁰Gd, ¹⁷⁶Yb, ²³²Th, ²³⁸U; calculated neutron excess factor. Comparison with data.

doi: 10.1142/S0218301304002156

2004GA03

Phys.Rev. C 69, 014305 (2004)

H.Ganev, V.P.Garistov, A.I.Georgieva

Description of the ground and octupole bands in the symplectic extension of the interacting vector boson model

NUCLEAR STRUCTURE ^224,226Ra, ^{222,224,226,228,232}Th, ^234,236,238U, ¹⁶⁸Yb, ¹⁵²Sm; analyzed ground-state and octupole rotational band energies; deduced parameters. Symplectic extension of interacting vector boson model.

doi: 10.1103/PhysRevC.69.014305

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

2004JA03

Int.J.Mod.Phys. E13, 343 (2004)

J.Jastrzebski, A.Trzcinska, P.Lubinski, B.Klos, F.J.Hartmann, T.von Egidy, S.Wycech

Neutron density distributions from antiprotonic atoms compared with hadron scattering data

NUCLEAR STRUCTURE ^40,48Ca, ^54,56,57Fe, ^58,60,64Ni, ⁵⁹Co, ^90,96Zr, ^106,116Cd, ^{112,116,120,124}Sn, ^{122,124,126,128,130}Te, ²⁰⁸Pb, ²⁰⁹Bi, ²³²Th, ²³⁸U; analyzed antiproton annihilation data; deduced neutron and proton density distributions, radii.

doi: 10.1142/S0218301304002168

2004MO06

Phys.Rev.Lett. 92, 072501 (2004)

P.Moller, A.J.Sierk, A.Iwamoto

Five-Dimensional Fission-Barrier Calculations from ⁷⁰Se to ²⁵²Cf

NUCLEAR STRUCTURE ^70,76Se, ^90,94,98Mo, ¹⁹⁸Hg, ^210,212Po, ²²⁸Ra, ^{228,230,232,234}Th, ^{232,234,236,238,240}U, ^{236,238,240,242,244,246}Pu, ^{242,244,246,248,250}Cm, ^250,252Cf; calculated fission barrier parameters. Macroscopic-microscopic model, comparison with previous results.

doi: 10.1103/PhysRevLett.92.072501

2004NE12

Phys.Rev. C 70, 057304 (2004)

V.O.Nesterenko, V.P.Likhachev, P.-G.Reinhard, V.V.Pashkevich, W.Kleinig, J.Mesa

Momentum distribution in heavy deformed nuclei: Role of effective mass

NUCLEAR STRUCTURE ²³⁸U; calculated proton states momentum distributions, role of deformation and effective mass. Self-consistent Skyrme-Hartree-Fock and Woods-Saxon models.

doi: 10.1103/PhysRevC.70.057304

2004RA13

Phys.Rev. C 69, 064321 (2004)

A.A.Raduta, A.Escuderos, A.Faessler, E.Moya de Guerra, P.Sarriguren

Two neutrino double-β decay in deformed nuclei with an angular momentum projected basis

RADIOACTIVITY ⁷⁶Ge, ⁸²Se, ^148,150Nd, ¹⁵⁴Sm, ¹⁶⁰Gd, ²³²Th, ²³⁸U(2β^-); calculated 2ν-accompanied 2β-decay Gamow-Teller amplitudes, strength distributions, T_1/2. Proton-neutron quasiparticle RPA.

doi: 10.1103/PhysRevC.69.064321

2004RO01

Ann.Nucl.Energy 31, 323 (2004)

Y.Ronen

Indications of the validity of the liquid drop model for spontaneous fission half-lives

RADIOACTIVITY ^230,232Th, ²³¹Pa, ^{232,233,234,235,236,238}U, ²³⁷Np, ^{236,238,239,240,241,242,244}Pu, ^241,243Am, ^{240,242,243,244,245,246,248,250}Cm, ^{246,248,249,250,252,254,256}Cf, ^253,254,255Es, ^{246,248,250,252,254,255,256,257,258,259}Fm, ²⁵⁹Md, ^{250,252,256,258}No, ^{253,254,255,256,257,258,259,260,262}Rf, ^{255,256,257,261,262}Db, ^259,260,263Sg, ²⁶¹Bh(SF); analyzed spontaneous fission T_1/2 relative to liquid drop model predictions.

doi: 10.1016/S0306-4549(03)00221-4

2004SA55

Phys.Rev. C 70, 044309 (2004)

M.Samyn, S.Goriely, M.Bender, J.M.Pearson

Further explorations of Skyrme-Hartree-Fock-Bogoliubov mass formulas. III. Role of particle-number projection

NUCLEAR STRUCTURE Z=8-120; calculated masses. ^230,231,233Th, ^{235,236,237,238,239}U, ^237,238Np, ^{235,237,238,239,240,241,243,244}Pu, ^{239,240,241,242,243,244}Am, ^{241,242,243,244,245}Cm, ²⁴⁴Bk; analyzed shape isomer energies. ³²S, ²⁰⁸Pb; calculated charge density distributions. Skyrme-Hartree-Fock-Bogoliubov mass formulas.

doi: 10.1103/PhysRevC.70.044309

2004SC03

Appl.Radiat.Isot. 60, 263 (2004)

R.Schon, G.Winkler, W.Kutschera

A critical review of experimental data for the half-lives of the uranium isotopes ²³⁸U and ²³⁵U

RADIOACTIVITY ^235,238U(α), (SF); compiled, analyzed T_1/2 data.

doi: 10.1016/j.apradiso.2003.11.027

2004SH47

Ukr.J.Phys. 49, 836 (2004)

Sh.Sharipov, M.S.Nadirbekov, S.K.Nuriyev

Reduced probabilities of E2 transitions and quadrupolar moments of the excited states of deformable nonaxial even-even nuclei

NUCLEAR STRUCTURE ¹⁰⁴Ru, ¹⁶⁶Er, ²³⁸U; calculated quadrupole moments, transitions B(E2). Comparison with data.

2004SU12

J.Phys.(London) G30, 905 (2004)

E.Sh.Sukhovitskii, S.Chiba, J.-Y.Lee, O.Iwamoto, T.Fukahori

Global coupled-channel optical potential for nucleon-actinide interaction from 1 keV to 200 MeV

NUCLEAR REACTIONS ²³²Th, ^233,235,238U, ^239,240,242Pu(n, X), E=0.1-200 MeV; calculated total σ, resonance parameters. ²³²Th, ²³⁸U(n, n), (n, n'), E=3.4-15 MeV; ²³²Th, ²³⁸U(p, p), (p, p'), E=20-65 MeV; calculated σ(θ). ²³²Th, ^233,235,238U, ^239,240,242Pu deduced deformation parameters. Global coupled-channel optical potential, comparison with data.

doi: 10.1088/0954-3899/30/7/007

2005AL40

J.Phys.(London) G31, S1813 (2005)

H.H.Alharbi, H.A.Alhendi, S.U.El-Kameesy

Nuclear structure study of some actinide nuclei

NUCLEAR STRUCTURE ^238,242,244Pu, ²³⁰Th, ^236,238U; calculated rotational bands moments of inertia. Exponential model with pairing attenuation, comparison with data.

doi: 10.1088/0954-3899/31/10/078

2005CH12

Phys.Rev. C 71, 024310 (2005)

R.J.Charity, L.G.Sobotka

Continuum corrections to the level density and its dependence on excitation energy, n-p asymmetry, and deformation

NUCLEAR STRUCTURE ⁴⁰Si, ⁴⁰S, ⁴⁰Ar, ⁴⁰Ca, ^40,60Ti, ⁶⁰Cr, ⁶⁰Fe, ⁶⁰Ni, ⁶⁰Zn, ⁶⁰Ge, ^{150,160,170,180,190}Yb, ¹⁷⁰Nd, ¹⁷⁰Hg, ²³⁸U; calculated level density parameters, deformation dependence, continuum corrections.

doi: 10.1103/PhysRevC.71.024310

2005DE44

Nucl.Phys. A758, 627c (2005)

P.Demetriou, M.Samyn, S.Goriely

Fission properties relevant to r-process nucleosynthesis

NUCLEAR REACTIONS ²³¹Pa, ^233,234,238U, ²³⁹Pu, ²⁴⁸Cm(n, F), E(cm)=0-5 MeV; calculated fission σ. Comparison with data.

RADIOACTIVITY ^{232,234,236,238,240}U, ^{238,240,242,244,246}Pu, ^{242,244,246,248,250}Cm, ^250,252Cf(SF); calculated fission T_1/2.

doi: 10.1016/j.nuclphysa.2005.05.113

2005DO10

Int.J.Mod.Phys. E14, 457 (2005)

A.Dobrowolski, J.Bartel, K.Pomorski

Influence of different proton and neutron deformations on nuclear energies

NUCLEAR STRUCTURE ^232,238U, ²⁴⁰Pu, ²⁷⁰Hs, ²⁷²Ds; calculated energy vs deformation. Yukawa-folded model, shell corrections.

doi: 10.1142/S0218301305003272

2005DU11

Int.J.Mod.Phys. E14, 383 (2005)

J.Dudek, K.Mazurek, B.Nerlo-Pomorska

Search for the tri-axial hexadecapole-deformation effects in trans-actinide nuclei

NUCLEAR STRUCTURE ²³⁸U, ^250,252Cf, ^256,258Fm; calculated energy vs deformation, tri-axial hexadecapole-deformation effects. Macroscopic-microscopic method, comparison with Hartree-Fock-Bogoliubov approach.

doi: 10.1142/S0218301305003168

2005EN01

Phys.Rev. C 71, 014306 (2005)

J.Enders, P.von Neumann-Cosel, C.Rangacharyulu, A.Richter

Parameter-free description of orbital magnetic dipole strength

NUCLEAR STRUCTURE ^46,48Ti, ⁵⁰Cr, ⁵⁶Fe, ⁶⁶Zn, ⁹²Zr, ⁹⁴Mo, ^108,112,114Cd, ^{122,124,126,130}Te, ^134,136Ba, ¹⁴²Ce, ^{144,146,148,150}Nd, ^{148,150,152,154}Sm, ^{154,156,158,160}Gd, ^160,162,164Dy, ^166,168,170Er, ^172,174,176Yb, ^176,178,180Hf, ^182,184,186W, ^190,192Os, ^194,196Pt, ²³²Th, ^236,238U; analyzed scissors mode excitation energies, deformation parameters, magnetic dipole strength distributions. Sum-rule approach.

doi: 10.1103/PhysRevC.71.014306

2005GO03

Phys.Rev. C 71, 024316 (2005)

H.Goutte, J.F.Berger, P.Casoli, D.Gogny

Microscopic approach of fission dynamics applied to fragment kinetic energy and mass distributions in ²³⁸U

NUCLEAR STRUCTURE ²³⁸U; calculated fission fragments kinetic energy and mass distributions, dynamical effects. Hartree-Fock-Bogoliubov and time-dependent generator coordinate methods.

doi: 10.1103/PhysRevC.71.024316

2005LA04

Phys.Rev. C 71, 024312 (2005)

G.A.Lalazissis, T.Niksic, D.Vretenar, P.Ring

New relativistic mean-field interaction with density-dependent meson-nucleon couplings

NUCLEAR STRUCTURE ^{12,14,16,18,20,22,24}O, ^40,48Ca, ⁷²Ni, ⁹⁰Zr, ^116,124,132Sn, ^{190,192,194,196,198,200,202,204,206,208,210,212,214}Pb, ²¹⁰Po, ^{224,226,228,230}Ra, ^{228,230,232,234}Th, ^{232,234,236,238,240}U, ^{238,240,242,244,246}Pu, ^{244,246,248,250}Cm, ^250,252,254Cf, ^252,254,256Fm, ^252,254,256No, ²⁵⁶Rf, ²⁶⁰Sg, ²⁶⁴Hs; calculated binding energies, radii. ^{116,118,120,124}Sn, ²⁰⁸Pb; calculated giant resonance strength distributions. ^287,288Mc, ^283,284Nh, ^279,280Rg, ^275,276Mt, ^271,272Bh; calculated Qα, deformation parameters. Relativistic mean-field effective interaction with density-dependent meson-nucleon couplings.

doi: 10.1103/PhysRevC.71.024312

2005MA41

Phys.Rev. C 71, 064328 (2005)

J.A.Maruhn, P.G.Reinhard, P.D.Stevenson, J.Rikovska Stone, M.R.Strayer

Dipole giant resonances in deformed heavy nuclei

NUCLEAR STRUCTURE ¹³²Sn, ^{142,144,146,148,150}Nd, ¹⁵²Dy, ¹⁸⁸Os, ²³⁸U; calculated dipole strength distributions, resonance features, deformation dependence. Time-dependent Skyrme-Hartree-Fock method.

doi: 10.1103/PhysRevC.71.064328

2005NA44

Phys.Rev. C 72, 064329 (2005)

H.Nakamura, T.Fukahori

Unified model of nuclear mass and level density formulas

NUCLEAR STRUCTURE ²³⁸U; calculated pairing, shell, and deformation energy corrections vs excitation energy. ⁵⁵Mn, ⁶⁰Co, ¹³⁹La, ¹⁴¹Pr, ¹⁹⁷Au, ²⁰⁹Po, ^230,232Th, ²³⁸U; calculated level densities vs excitation energy. Analytical expression of the single-particle state density.

doi: 10.1103/PhysRevC.72.064329

2005PO01

Nucl.Phys. A747, 182 (2005)

D.N.Poenaru, R.A.Gherghescu, W.Greiner

Complex fission phenomena

NUCLEAR STRUCTURE ¹⁷⁰Yb, ^{226,228,230,232,234,236,238}Th, ^{230,232,234,236,238}U, ²⁵²Cf; calculated saddle-point deformation parameters and energies for binary, ternary, and multicluster fission. Integro-differential equation.

doi: 10.1016/j.nuclphysa.2004.09.104

2005RE16

Nucl.Phys. A759, 64 (2005)

Z.Ren, C.Xu

Spontaneous fission half-lives of heavy nuclei in ground state and in isomeric state

RADIOACTIVITY ^{235,236m,238m}U, ^237mNp, ^{235m,236m,237m,238m,239,239m,240m,241m,242m,243m,244m,245m}Pu, ^{237m,238m,239m,240m,241,241m,242m,243,243m,244m,245m,246m}Am, ^{241m,242m,243,243m,244m,245,245m}Cm, ^{242m,244m,245m,249}Bk, ^244,247,249Cf, ^253,255Es, ^{251,253,255,257,259}Fm, ^245,247,260Md, ^259,261Lr, ^253,255,259Rf, ^{255,257,260,263}Db, ^{261,263,265,267}Sg, ^{263,265,267,269}Bh, ^{269,271,273,275}Ds, ^{271,273,275,277}Rg(SF); calculated T_1/2. Several formulas compared with data.

doi: 10.1016/j.nuclphysa.2005.04.019

2005SH05

Ukr.J.Phys. 50, 21 (2005)

Sh.Sharipov, M.S.Nadyrbekov

Electrical dipole and quadrupole transitions in even-even nuclei with quadrupole and octupole deformations

NUCLEAR STRUCTURE ¹⁰⁴Ru, ¹⁶⁶Er, ²²⁶Ra, ²³⁸U; calculated transitions B(E2), B(E1). Comparison with data.

2005SH57

Bull.Rus.Acad.Sci.Phys. 69, 141 (2005)

Sh.Sharipov, M.S.Nadyrbekov, S.K.Nuriev

Collective states of even-even nuclei with quadrupole and octupole deformations

NUCLEAR STRUCTURE ^222,230Th, ²³⁸U; calculated level energies, J, π, collective features. ¹⁰⁴Ru, ¹⁶⁶Er, ²²⁶Ra, ²³⁸U; calculated reduced transition probabilities.

2005SW02

Phys.Rev. C 71, 047301 (2005)

W.J.Swiatecki, A.Trzcinska, J.Jastrzebski

Difference of the root-mean-square sizes of neutron and proton distributions in nuclei: Comparison of theory with data

NUCLEAR STRUCTURE ^40,48Ca, ^54,56,57Fe, ^58,60,64Ni, ⁵⁹Co, ^90,96Zr, ^106,116Cd, ^{112,116,120,124}Sn, ^{122,124,126,128}Te, ²⁰⁸Pb, ²⁰⁹Bi, ²³²Th, ²³⁸U; calculated neutron-proton radius difference. Droplet model, comparison with data.

doi: 10.1103/PhysRevC.71.047301

2005TR01

Europhys.Lett. 69, 41 (2005)

V.I.Tretyak, F.A.Danevich, S.S.Nagorny, Yu.G.Zdesenko

On the possibility to search for 2β decay of initially unstable (α/β radioactive) nuclei

RADIOACTIVITY ²¹⁰Pb, ²²²Rn, ²²⁶Ra, ^232,234Th, ²³⁸U(2β^-); measured 2β-decay T_1/2 lower limits.

doi: 10.1209/epl/i2004-10319-x

2005XU01

Phys.Rev. C 71, 014309 (2005)

C.Xu, Z.Ren

Systematical law of spontaneous fission half-lives of heavy nuclei

RADIOACTIVITY ²³²Th, ^234,236,238U, ^{236,238,240,242,244}Pu, ^{240,242,244,246,248,250}Cm, ^{238,240,242,246,248,250,252,254,256}Cf, ^{244,246,248,250,252,254,256,258,260}Fm, ^{250,252,254,256,258,260,262}No, ^{256,258,260,262,264}Rf, ^{264,266,268,270,272}Hs, ^{260,262,264,266,268}Sg, ^{268,270,272,274,276}Ds(SF); calculated fission T_1/2. Comparisons with data.

doi: 10.1103/PhysRevC.71.014309

2005YO12

Nucl.Instrum.Methods Phys.Res. A555, 386 (2005); Erratum Nucl.Instrum.Methods Phys.Res. A557, 689 (2006)

T.Yoshioka, T.Tsuruta, H.Iwano, T.Danhara

Spontaneous fission decay constant of ²³⁸U determined by SSNTD method using CR-39 and DAP plates

RADIOACTIVITY ²³⁸U(SF); measured spontaneous fission decay constant. Solid-state nuclear track detectors.

doi: 10.1016/j.nima.2005.09.014

2005YUZZ

Proc.Intern.Conf.Nuclear Data for Science and Technology, Santa Fe, New Mexico, 26 September-1 October, 2004, R.C.Haight, M.B.Chadwick, T.Kawano, P.Talou, Eds., Vol.1, p. 153 (2005); AIP Conf.Proc. 769 (2005)

H.Yu, C.Cai, Z.Zhao

Calculations of Neutron- and Proton-Induced Reactions up to 200 MeV for Target ²³⁸U

NUCLEAR REACTIONS ²³⁸U(n, X), (n, F), (p, X), (p, F), E=0-200 MeV; calculated total and fission σ. ²³⁸U(n, n), E=0.55-14.1 MeV; ²³⁸U(p, p), E=20, 26, 65 MeV; calculated elastic σ(θ). ²³⁸U(n, F), E=14 MeV; calculated fission neutron spectra, yields. Comparison with data.

doi: 10.1063/1.1944979

2005ZA02

Int.J.Mod.Phys. E14, 147 (2005)

N.V.Zamfir, D.Kusnezov, M.Babilon

Octupole correlations in Z or N ∼ 88 nuclei

NUCLEAR STRUCTURE ^218,220,222Rn, ^{218,220,222,224,226}Ra, ^{220,222,224,226,228,230,232}Th, ^{230,232,234,236,238}U, ^{238,240,242,244}Pu, ^{148,150,152,154}Sm; calculated levels, J, π, octupole excitations. Interacting boson approximation.

doi: 10.1142/S0218301305002874

2006BA35

Czech.J.Phys. 56, 437 (2006)

A.S.Barabash

Average and recommended half-life values for two-neutrino double-beta decay: Upgrade '05

RADIOACTIVITY ⁴⁸Ca, ⁷⁶Ge, ⁸²Se, ⁹⁶Zr, ¹⁰⁰Mo, ¹¹⁶Cd, ^128,130Te, ¹⁵⁰Nd, ²³⁸U(2β^-); ¹³⁰Ba(2EC); compiled, analyzed 2νββ-decay T_1/2. Recommended values.

doi: 10.1007/s10582-006-0106-6

2006BAZZ

nucl-ex/0602009, 2/8/2006 (2006)

A.S.Barabash

Average and recommended half-life values for two neutrino double beta decay: Upgrade '05

RADIOACTIVITY ⁴⁸Ca, ⁷⁶Ge, ⁸²Se, ⁹⁶Zr, ¹⁰⁰Mo, ¹¹⁶Cd, ^128,130Te, ¹⁵⁰Nd, ²³⁸U(2β^-); ¹³⁰Ba(2EC); compiled, analyzed 2νββ-decay T_1/2.

2006DE05

Phys.Rev. C 73, 014315 (2006)

D.S.Delion, S.Peltonen, J.Suhonen

Systematics of the α-decay to rotational states

RADIOACTIVITY ^{226,228,230,232,234}Th, ^{230,232,234,236,238}U, ^{236,238,240,242,244}Pu, ^{242,244,246,248}Cm, ^248,250Cf(α); analyzed T_1/2, decay widths for α-decay to rotational states; deduced parameters. Stationary coupled channels approach.

doi: 10.1103/PhysRevC.73.014315

2006DE25

Phys.Rev. C 73, 054309 (2006)

A.S.de Castro, P.Alberto, R.Lisboa, M.Malheiro

Relating pseudospin and spin symmetries through charge conjugation and chiral transformations: The case of the relativistic harmonic oscillator

doi: 10.1103/PhysRevC.73.054309

2006FR21

Can.J.Phys. 84, 677 (2006)

J.B.French, S.Rab, J.F.Smith, R.U.Haq, V.K.B.Kota

Nuclear spectroscopy in the chaotic domain: level densities

NUCLEAR STRUCTURE ^150,153,155Sm, ^{155,156,157,158,159}Gd, ¹⁶²Dy, ^167,168,169Er, ^{170,171,172,173,174,175}Yb, ^{175,178,179,180}Hf, ¹⁸¹W, ²⁰⁷Pb, ^{233,234,235,236,237,238,239}U, ²³³Th; analyzed resonance energies, J, π, configurations, level density parameters.

doi: 10.1139/P06-047

2006GO07

Int.J.Mod.Phys. E15, 292 (2006)

H.Goutte, J.-F.Berger, D.Gogny

Fission collective dynamics in a microscopic framework

NUCLEAR STRUCTURE ²³⁸U; calculated potential energy along scission line, fission fragments kinetic energies, charge and mass distributions, deformation. Time-dependent microscopic approach.

doi: 10.1142/S0218301306004120

2006NE10

Phys.Rev.C 74, 064306 (2006)

V.O.Nesterenko, W.Kleinig, J.Kvasil, P.Vesely, P.-G.Reinhard, D.S.Dolci

Self-consistent separable random-phase approximation for Skyrme forces: Giant resonances in axial nuclei

NUCLEAR STRUCTURE ¹⁵⁴Sm, ²³⁸U, ²⁵⁴No; calculated GDR and GQR strength distributions, related features. Self-consistent separable RPA.

doi: 10.1103/PhysRevC.74.064306

2006NI17

Bull.Rus.Acad.Sci.Phys. 70, 824 (2006)

G.K.Nie

Alpha cluster model based on pn-pair interactions

NUCLEAR STRUCTURE ¹¹⁶Sn, ¹²²Sb, ¹²⁶Te, ¹³³Cs, ¹³⁶Xe, ¹³⁸Ba, ¹³⁹La, ¹⁴⁰Ce, ¹⁴¹Pr, ¹⁴²Nd, ¹⁴⁸Sm, ¹⁵³Eu, ¹⁵⁶Gd, ¹⁵⁸Dy, ¹⁶⁰Er, ¹⁶²Yb, ¹⁷⁶Hf, ¹⁹⁰Os, ¹⁹⁷Au, ²⁰⁴Hg, ²⁰⁵Tl, ²⁰⁸Pb, ²⁰⁹Bi, ²³²Th, ²³⁸U; calculated radii. Spherical lattice model.

2006RA21

Phys.Rev. C 74, 044312 (2006)

A.A.Raduta, Al.H.Raduta, C.M.Raduta

Simultaneous description of four positive parity bands and four negative parity bands

NUCLEAR STRUCTURE ¹⁵⁸Gd, ¹⁷²Yb, ^228,232Th, ²²⁶Ra, ²³⁸U, ²³⁸Pu; calculated rotational bands energies, moments of inertia, configurations. Comparison with data.

doi: 10.1103/PhysRevC.74.044312

2006SH37

Int.J. Mass Spectrom. 251, 109 (2006)

V.M.Shabaev, O.V.Andreev, A.N.Artemyev, S.S.Baturin, A.A.Elizarov, Y.S.Kozhedub, N.S.Oreshkina, I.I.Tupitsyn, V.A.Yerokhin, O.M.Zherebtsov

QED effects in heavy few-electron ions

NUCLEAR MOMENTS ^203,205Tl, ²⁰⁹Bi, ²³⁸U; calculated hydrogen-like ion hyperfine splitting (hfs), hydrogen-like, lithium-like, and helium-like ion binding energies, bound electron g-factor, and parity nonconservation (PNC) effects. Calculations include relativistic quantum electrodynamics (QED), electron-correlation, and nuclear effects.

doi: 10.1016/j.ijms.2006.01.012

2006XU08

Nucl.Phys. A778, 1 (2006)

C.Xu, Z.Ren

Branching ratios of α-decay to excited states of even-even nuclei

RADIOACTIVITY ^180,182,184Hg, ^186,188Pb, ^{190,194,196,198}Po, ²⁰²Rn, ^{226,228,230,232}Th, ^{230,232,234,236}U, ^{236,238,240,242}Pu, ^242,244Cm, ²⁴⁶Cf(α); calculated branching ratios for decays to excited states. Comparisons with data.

doi: 10.1016/j.nuclphysa.2006.08.002

2007AD24

Phys.Atomic Nuclei 70, 1350 (2007)

G.G.Adamian, N.V.Antonenko, R.V.Jolos, Yu.V.Palchikov, T.M.Shneidman, W.Scheid

Nuclear structure in the dinuclear model with rotating clusters

NUCLEAR STRUCTURE ²³⁸U; calculated level energies, J, π using the dinuclear-system model.

doi: 10.1134/S1063778807080054

2007BA18

Int.J.Mod.Phys. E16, 459 (2007)

J.Bartel, A.Dobrowolski, K.Pomorski

Saddle-point masses of even-even actinide nuclei

NUCLEAR STRUCTURE ^232,234Th, ^{234,236,238,240}U, ^{236,238,240,242,244,246}Pu, ^{242,244,246,248,250}Cm, ²⁵⁰Cf; calculated fission barrier energies, inner and outer saddle point masses. Modified funny-hills shape parameterization.

doi: 10.1142/S0218301307005892

2007BO46

Phys.Rev. C 76, 064312 (2007)

D.Bonatsos, E.A.McCutchan, N.Minkov, R.F.Casten, P.Yotov, D.Lenis, D.Petrellis, I.Yigitoglu

Exactly separable version of the Bohr Hamiltonian with the Davidson potential

NUCLEAR STRUCTURE ¹⁵⁴Sm, ^{156,158,160,162}Gd, ^{158,160,162,164,166}Dy, ^{160,162,164,166,168,170}Er, ^{164,166,168,170,172,174,176,178}Yb, ^{168,170,172,174,176,178,180}Hf, ^{176,178,180,182,184,186}W, ^{180,182,184,186,188}Os, ²²⁸Ra, ^228,230,232Th, ^{232,234,236,238}U, ^238,240,242Pu, ²⁴⁸Cm, ²⁵⁰Cf; calculated excitation energy ratios, angular momenta, B(E2) ratios, bandhead energies, deformation parameters using Bohr Hamiltonian with Davidson Potential, compared with experimental values.

doi: 10.1103/PhysRevC.76.064312

2007BU20

J.Phys.(London) G34, 1985 (2007)

B.Buck, A.C.Merchant, S.M.Perez

Negative parity bands in ²³⁸U

NUCLEAR STRUCTURE ²³⁸U; calculated level energies, K, J, π in terms of a Pb-Ne cluster model.

doi: 10.1088/0954-3899/34/9/010

2007DO03

Phys.Rev. C 75, 024613 (2007)

A.Dobrowolski, K.Pomorski, J.Bartel

Fission barriers in a macroscopic-microscopic model

NUCLEAR STRUCTURE ^232,234Th, ^236,238U, ^236,240Pu, ²⁷²Ds, ²⁹⁸Fl; calculated fission barriers. Macroscopic-microscopic model, four-dimensional shape parameterization.

doi: 10.1103/PhysRevC.75.024613

2007DO06

Int.J.Mod.Phys. E16, 431 (2007)

A.Dobrowolski, H.Goutte, J.-F.Berger

Microscopic determinations of fission barriers (mean-field and beyond)

NUCLEAR STRUCTURE ²²⁶Th, ²³⁸U; calculated potential energy vs deformation, fission barrier features.

doi: 10.1142/S0218301307005867

2007GH11

Eur.Phys.J. A 33, 65 (2007)

O.N.Ghodsi, J.Ariai

Calculation of the Coulomb potential between spherical-deformed and deformed-deformed nuclei using the Monte Carlo method

NUCLEAR STRUCTURE ¹⁶O, ²⁷Al, ⁷⁰Ge, ²³⁸U; calculated deformations parameters using HFB model.

NUCLEAR REACTIONS ²³⁸U(¹⁶O, X), E not given; ⁷⁰Ge(²⁷Al, X), E not given; calculated coulomb potentials using Monte Carlo simulations.

doi: 10.1140/epja/i2007-10412-8

2007NE04

Int.J.Mod.Phys. E16, 624 (2007)

V.O.Nesterenko, W.Kleinig, J.Kvasil, P.Vesely, P.-G.Reinhard

Giant dipole resonance in deformed nuclei: dependence on Skyrme forces

NUCLEAR STRUCTURE ¹⁵⁰Nd, ²³⁸U; calculated GDR strength distributions. Separable RPA method, four Skyrme forces compared.

doi: 10.1142/S0218301307006071

2008BH07

J.Phys.(London) G35, 065109 (2008)

A.Bhagwat, Y.K.Gambhir

The α-nucleus potential for fusion and decay

RADIOACTIVITY ²³⁸U, ²²⁵Pa, ²⁷¹Ds(α); calculated α-decay half-lives.

NUCLEAR REACTIONS ^206,208Pb, ²⁰⁹Bi(α, X), E=16-21 MeV; calculated fusion cross sections.

doi: 10.1088/0954-3899/35/6/065109

2008BU11

J.Phys.(London) G35, 085101 (2008)

B.Buck, A.C.Merchant, S.M.Perez

Negative parity bands in even-even isotopes of Ra, Th, U and Pu

NUCLEAR STRUCTURE ²²⁶Ra, ²³⁰Th, ^234,236,238U, ^238,240,242Pu; calculated level energies and B(E3) for negative parity bands using a Pb core plus exotic cluster model.

doi: 10.1088/0954-3899/35/8/085101

2008CH15

Phys.Rev. C 77, 061305 (2008)

Y.-S.Chen, Y.Sun, Z.-C.Gao

Nonaxial-octupole effect in superheavy nuclei

NUCLEAR STRUCTURE ^{220,222,224,226,228,230}Ra, ^{224,226,228,230,232}Th, ^{230,232,234,236,238}U, ^{236,238,240,242}Pu, ^246,248Cm, ^248,250,252Cf, ²⁵⁰Fm, ²⁵²No; calculated band head energies, comparison with experimental data. ²⁴⁶Cm, ²⁴⁸Cf, ²⁵⁰Fm, ²⁵²No; calculated levels, J, π, B(E3). Reflection Asymmetric Shell Model.

doi: 10.1103/PhysRevC.77.061305

2008JU06

Phys.Lett. B 670, 200 (2008)

A.R.Junghans, G.Rusev, R.Schwengner, A.Wagner, E.Grosse

Photon data shed new light upon the GDR spreading width in heavy nuclei

NUCLEAR STRUCTURE ⁸⁸Sr, ^94,98Mo, ¹⁵⁶Gd, ¹⁹⁰Os, ¹⁹⁶Pt, ²⁰⁰Hg, ²³⁸U; analyzed dipole strength functions.

doi: 10.1016/j.physletb.2008.10.055

2008KL03

Phys.Rev. C 78, 044313 (2008)

W.Kleinig, V.O.Nesterenko, J.Kvasil, P.-G.Reinhard, P.Vesely

Description of the dipole giant resonance in heavy and superheavy nuclei within Skyrme random-phase approximation

NUCLEAR STRUCTURE ^156,160Gd, ^166,168Er, ^176,178,180Hf, ^182,184,186W, ^{170,172,174,176}Yb, ^{186,188,190,192}Os, ²³²Th, ^234,236,238U, ^{242,248,254,262,270}No, ^{264,274,284,294,304}Fl, ^{280,288,294,304,312}120; calculated isovector giant dipole resonance strengths, energies and widths. Skyrme random-phase approximation. Comparison with experimental data.

doi: 10.1103/PhysRevC.78.044313

2008LI05

Nucl.Phys. A801, 43 (2008)

X.Li, C.Cai

Global dispersive optical model potential for proton as projectile in the energy region up to 200 MeV

NUCLEAR REACTIONS ^24,26Mg, ²⁷Al, ²⁸Si, ³¹P, ⁴⁰Ar, ^40,42,44,48Ca, ⁴⁵Sc, ^46,48,50Ti, ⁵¹V, ^50,52Cr, ⁵⁵Mn, ^54,56,57,58Fe, ⁵⁹Co, ^58,60,62,64Ni, ^63,65Cu, ^64,66,68,70Zn, ⁷⁰Ge, ^{74,76,78,80,82}Se, ^86,88Sr, ⁸⁹Y, ^{90,91,92,94,96}Zr, ^{92,94,96,98,100}Mo, ¹⁰²Ru, ^{104,106,108,110}Pd, ^{106,108,110,111,112,113,114,116}Cd, ^116,120,124Sn, ^134,136,138Ba, ¹⁴⁴Nd, ^{144,148,150,152,154}Sm, ¹⁶⁰Gd, ¹⁶⁴Dy, ¹⁶⁵Ho, ^166,168Er, ^172,174,176Yb, ^178,180Hf, ^182,184,186W, ^188,190,192Os, ^194,198Pt, ¹⁹⁷Au, ^206,207,208Pb, ²⁰⁹Bi, ²³²Th, ^235,238U(p, p), E≈1-200 MeV; calculated σ(θ). ^{112,114,116,118,120,122,124}Sn(p, p'), E=0-200 MeV; calculated nonelastic σ. New global proton dispersive optical model parameters. Comparison with Koning and Delaroche potential.

doi: 10.1016/j.nuclphysa.2007.12.004

2008PO06

J.Radioanal.Nucl.Chem. 277, 207 (2008)

S.Pomme, E.Garcia-Torano, G.Sibbens, S.Richter, R.Wellum, A.Stolarz, A.Alonso

²³⁴U/²³⁵U activity ratios as a probe for the ²³⁸U/²³⁵U half-life ratio

RADIOACTIVITY ^234,235U(α); measured Eα, Iα. ^235,238U; deduced half-life ratio.

doi: 10.1007/s10967-008-0731-6

2008PR05

Int.J.Mod.Phys. E17, 160 (2008)

L.Prochniak

Collective excitations of transactinide nuclei in a self-consistent mean field theory

NUCLEAR STRUCTURE ²³⁸U, ^240,242Pu, ^246,248Cm, ^250,252Cf; calculated potential energy surfaces, mass parameter, probability distributions, level energies, and B(E2) using the Adiabatic Time Dependent Hartree-Fock-Bogolyubov (ATDHFB) approach. Comparisons with experimental results.

doi: 10.1142/S0218301308009653

2008RAZX

Proc.of the 9th Internat. Spring Seminar on Nuclear Physics: Changing Facets of Nuclear Structure, Vico Equense, Italy, May 20-24 2007, A.Covello, Ed., World Scientific, Singapore, p.209 (2008)

A.A.Raduta, C.M.Raduta

Double beta decay to the first 2⁺ state

NUCLEAR STRUCTURE ⁴⁸Ca, ⁷⁶Ge, ⁸²Se, ⁹⁶Zr, ¹⁰⁰Mo, ¹⁰⁴Ru, ¹¹⁰Pd, ¹¹⁶Cd, ^128,130Te, ^134,136Xe, ^148,150Nd, ¹⁵⁴Sm, ¹⁶⁰Gd, ²³²Th, ²³⁸U; calculated Gamow-Teller transition amplitudes, ββ-decay T_1/2.

2008SA24

Nucl.Sci.Eng. 160, 190 (2008)

P.Santi, M.Miller

Reevaluation of Prompt Neutron Emission Multiplicity Distributions for Spontaneous Fission

RADIOACTIVITY ²³²Th, ^236,238U, ^{236,238,240,242,244}Pu, ^{242,244,246,248,250}Cm, ²⁴⁹Bk, ^{246,249,250,252,254}Cf, ²⁵³Es, ^{244,246,254,256,257}Fm, ²⁵²No(SF); analyzed prompt neutron emission probabilities.

2008SH06

Ukr.J.Phys. 53, 112 (2008)

Sh.Sharipov, M.S.Nadirbekov, G.A.Yuldasheva

Excited rotational-vibrational states of even-even nuclei with quadrupole and octupole deformations

NUCLEAR STRUCTURE ¹⁵⁰Sm, ^154,162Dy, ²³²Th, ^232,236,238U; calculated level energies for excited rotational-vibrational states with quadrupole and octupole deformations.

2008SK02

Int.J.Mod.Phys. E17, 151 (2008)

J.Skalski

Relative motion correction to fission barriers

NUCLEAR STRUCTURE ¹⁹⁸Hg, ²³⁸U; calculated fission barrier features. Hartree-Fock approach.

doi: 10.1142/S0218301308009641

2008SO03

Phys.Rev. C 77, 035806 (2008), Erratum Phys.Rev. C 81, 049902 (2010)

H.Sonoda, G.Watanabe, K.Sato, K.Yasuoka, T.Ebisuzaki

Phase diagram of nuclear "pasta" and its uncertainties in supernova cores

NUCLEAR STRUCTURE ⁵⁶Fe, ⁹⁰Zr, ²⁰⁸Pb, ²³⁸U; calculated binding energies, central nucleon density, surface diffusiveness parameters, surface tension, nucleon distributions, phase diagrams. Quantum-molecular dynamics (QMD) model.

doi: 10.1103/PhysRevC.77.035806

2008TE01

Ann.Nucl.Energy 35, 220 (2008)

E.Tel, H.M.Sahin, A.Kaplan, A.Aydin, T.Altinok

Investigation of the properties of the nuclei used on the new generation reactor technology systems

NUCLEAR STRUCTURE ¹⁸⁴W, ²⁰⁷Pb, ²⁰⁹Bi, ²³²Th, ²³⁸U; calculated RMS charge and mass radius, neutron and proton densities using the Hartree Fock method with Skyrme interaction.

doi: 10.1016/j.anucene.2007.06.012

2008US02

Phys.Rev. C 77, 034312 (2008)

Q.N.Usmani, A.R.Bodmer, Z.Sauli

Core nucleus polarization in Λ hypernuclei

NUCLEAR STRUCTURE ^3,4H, ^4,5He; calculated binding energies. ¹⁰B, ^11,12C, ^15,16,18O, ²⁰Ne, ²³Na, ^27,28Si, ^31,32S, ^{39,40,42,44,48}Ca, ^50,51V, ⁵⁸Ni, ^88,89Y, ⁹¹Y, ¹⁰⁰Mo, ¹²²Sn, ^138,139La, ¹⁵⁰Nd, ¹⁶⁹Tm, ¹⁷⁴Yb, ¹⁹⁸Hg, ^207,208,210Pb, ²³⁸U, ²⁴³Am; calculated single particle energies, rms radii, wave functions for hypernuclei.

doi: 10.1103/PhysRevC.77.034312

2009AR11

Phys.Rev. C 80, 034317 (2009)

S.K.Arun, R.K.Gupta, S.Kanwar, B.Singh, M.K.Sharma

Cluster radioactivity with effects of deformations and orientations of nuclei included

RADIOACTIVITY ¹¹⁴Ba(¹²C), ²²¹Fr, ^{221,222,223,224,226}Ra, ^223,225Ac, ²²⁶Th(¹⁴C), ²²³Ac(¹⁵N), ²²⁶Th(¹⁸O), ²²⁸Th(²⁰O), ²³⁰U(²²Ne), ^{230,232,233,234}U, ²³⁰Th, ²³¹Pa(²⁴Ne), ²³¹Pa(²³F), ²³⁴U(²⁵Ne), ²³⁴U(²⁶Ne), ^{232,233,234,235,236}U, ^236,238Pu(²⁸Mg), ²³⁷Np, ²³⁸Pu(³⁰Mg), ²³⁸Pu(³²Si), ²³⁸U, ²⁴¹Am, ²⁴²Cm(³⁴Si), ²⁵²Cf(⁴⁶Ar), (⁴⁸Ca), (⁵⁰Ca); calculated half-lives of cluster decays for different deformations using preformed cluster model (PCM). Comparison with experimental data.

doi: 10.1103/PhysRevC.80.034317

2009BU09

J.Phys.(London) G36, 085101 (2009)

B.Buck, A.C.Merchant, S.M.Perez, T.T.Ibrahim, S.M.Wyngaardt

Electromagnetic transition strength ratios in ²³⁸U

NUCLEAR STRUCTURE ²³⁸U; calculated B(E1), B(E2), B(E1)/B(E2). Pb-Ne cluster model, comparison with experiment.

doi: 10.1088/0954-3899/36/8/085101

2009DE32

Phys.Rev. C 80, 034603 (2009); Erratum Phys.Rev. C 82, 059902 (2010)

V.Yu.Denisov, A.A.Khudenko

α decays to ground and excited states of heavy deformed nuclei

RADIOACTIVITY ^222,224,226Ra, ^{226,228,230,232}Th, ^{228,230,232,234,235,236,238}U, ^{234,236,238,240,242,244}Pu, ^{238,240,242,244,246,248}Cm, ^{244,246,248,250,252}Cf, ^248,250,252Fm, ²⁵²No(α); calculated half-lives and branching ratios for g.s. to g.s. decays and g.s. to excited states using Unified model for α decay and α capture (UMADAC). Comparison with experimental data.

doi: 10.1103/PhysRevC.80.034603

2009GO05

Phys.Rev. C 79, 024612 (2009)

S.Goriely, S.Hilaire, A.J.Koning, M.Sin, R.Capote

Towards a prediction of fission cross sections on the basis of microscopic nuclear inputs

NUCLEAR REACTIONS ²³²Th, ^235,236,238U, ^{238,239,240,241,242}Pu, ²³⁷Np(n, F), E=0.01-30 MeV; calculated fission σ using global renormalization of barrier heights within the HFB fission path and microscopic nuclear level densities at saddle points. Comparison with experimental data. ^{234,235,236,237,238,239}U, ^{238,239,240,241,242,243}Pu; calculated fission path total energy.

doi: 10.1103/PhysRevC.79.024612

2009KU13

J.Nucl.Sci.Technol.(Tokyo) 46, 914 (2009)

S.Kunieda, S.Chiba, K.Shibata, A.Ichihara, O.Iwamoto, N.Iwamoto, T.Fukahori, E.Sh.Sukhovitskii

Extensive Study of the Soft-Rotator Model Hamiltonian Parameters for Medium and Heavy Even-Even Nuclei

NUCLEAR STRUCTURE ^56,58Fe, ^60,62,64Ni, ^64,66,68,70Zn, ^70,72,74,76Ge, ^{74,76,78,80,82}Se, ⁸⁶Sr, ^96,98,100Mo, ¹⁰²Ru, ^{104,106,108,110}Pd, ^{106,108,110,112,114,116}Cd, ^{116,118,120,122,124}Sn, ^{122,124,126,128,130}Te, ^144,150Nd, ^{148,150,152,154}Sm, ¹⁶⁰Gd, ¹⁶⁴Dy, ^166,168Er, ^174,176Yb, ^178,180Hf, ^182,184W, ¹⁹²Os, ¹⁹⁴Pt, ²³²Th, ²³⁸U; calculated excitation energy levels, J, π, quadrupole deformation parameters, B(E2), B(E3); deduced shell structure effects, agreement with mass-model results. Comparison with experimental results, SRM-CC analysis.

NUCLEAR REACTIONS ^56,58Fe, ^60,62,64Ni, ^64,66,68,70Zn, ^70,72,74,76Ge, ^{74,76,78,80,82}Se, ⁸⁶Sr, ^96,98,100Mo, ¹⁰²Ru, ^{104,106,108,110}Pd, ^{106,108,110,112,114,116}Cd, ^{116,118,120,122,124}Sn, ^{122,124,126,128,130}Te, ^144,150Nd, ^{148,150,152,154}Sm, ¹⁶⁰Gd, ¹⁶⁴Dy, ^166,168Er, ^174,176Yb, ^178,180Hf, ^182,184W, ¹⁹²Os, ¹⁹⁴Pt, ²³²Th, ²³⁸U(p, p'), E = 22.3, 65 MeV; calculated inelastic proton σ(θ). Coupled-channel optical model analysis.

doi: 10.3327/jnst.46.914

2009NI06

Nucl.Phys. A825, 145 (2009)

D.Ni, Z.Ren

Microscopic calculation of α-decay half-lives within the cluster model

RADIOACTIVITY ²¹⁰Pb, ^{212,214,216,218}Po, ^{214,216,218,220,222}Rn, ^{216,218,220,222,224,226}Ra, ^{218,220,222,224,226,228,230,232}Th, ^{222,224,226,228,230,232,234,236,238}U, ^{232,234,236,238,240,242,244}Pu, ^{240,242,244,246,248}Cm, ^{240,242,244,246,248,250,252,254}Cf, ^{246,248,250,252,254,256}Fm, ^252,254,256No, ^256,258Rf, ^260,266Sg, ^264,266,270Hs, ²⁷⁰Ds, ^278,279,280Rg, ^283,284,285Cn, ^282,283,284Nh, ^{286,287,288,289}Fl, ^287,288Mc, ^{290,291,292,293}Lv, ²⁹⁴Og(α); calculated α-decay half-lives using a cluster model. Comparison with data.

doi: 10.1016/j.nuclphysa.2009.04.010

2009PA46

Phys.Rev. C 80, 064602 (2009)

S.K.Patra, R.N.Panda, P.Arumugam, R.K.Gupta

Nuclear reaction cross sections of exotic nuclei in the Glauber model for relativistic mean field densities

NUCLEAR REACTIONS ¹²C(⁶Li, X), (⁷Li, X), (⁸Li, X), (⁹Li, X), (¹¹Li, X), E=790 MeV/nucleon; ¹²C(²⁰Mg, X), (²⁰Na, X), (²⁰Ne, X), (²⁰F, X), (²⁰O, X), (²⁰N, X), E=30-2200 MeV/nucleon; ²⁰⁸Pb(α, X), (⁶He, X), (⁸He, X), (⁶Li, X), (⁷Li, X), (⁸Li, X), (⁹Li, X), (¹¹Li, X), (¹⁰B, X), E=30-1000 MeV/nucleon; ²³⁵U(α, X), (⁶He, X), (⁸He, X), (⁶Li, X), (⁷Li, X), (⁸Li, X), (⁹Li, X), (¹¹Li, X), (²⁰C, X), E=30-1000 MeV/nucleon; ²³⁰Th(α, X), (⁶Li, X), (⁷Li, X), (⁸Li, X), (⁹Li, X), (¹¹Li, X), E=30-1000 MeV/nucleon; ^{218,228,248,260}Pb, ^250,260,270U(⁶Li, X), E=30-1000 MeV/nucleon; ^{218,228,248,260}Pb, ^250,260,270U(¹¹Li, X), 30-1000 MeV/nucleon; ^218,228,248Pb(¹⁰B, X), E=30-1000 MeV/nucleon; ^240,250,270Th(α, X), E=30-1000 MeV/nucleon; ^250,260,270U(⁸He, X), E=30-1000 MeV/nucleon; ^250,260,270U(²⁰C, X), E=30-1000 MeV/nucleon; ^208,210,260Pb(⁶Li, ⁶Li), E=30-1000 MeV/nucleon; ²⁶⁰Pb, ^292,320122(¹¹Li, X), E=30-1000 MeV/nucleon; ²⁶⁰Pb, ^292,320122(¹¹Li, ¹¹Li), E=30-1000 MeV/nucleon; ²⁰⁸Pb, ^235,238,250U(¹²C, ¹²C), E=30-1000 MeV/nucleon; ^235,238,250U(²⁰C, ²⁰C), E=30-1000 MeV/nucleon; calculated σ and σ(θ) using the relativistic mean field (RMF(NL3) and E-RMF(G2)) formalisms and the Glauber model. Comparison with experimental data.

NUCLEAR STRUCTURE ^4,5,6,7,8He, ^{6,7,8,9,10,11}Li, ^10,15,17,20B, ^{12,14,16,18,20}C, ^{208,210,218,228,238,248,258,260}Pb, ^{230,240,250,260,270}Th, ^{235,238,250,260,270,280}U, ^292,320122; calculated binding energies, rms radii and ground-state densities for lighter projectiles and heavier target nuclei using relativistic mean field (RMF(NL3) and E-RMF(G2)) formalisms. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.064602

2009RU12

Eur.Phys.J. A 41, 399 (2009)

K.Rusek

Polarization potentials due to inelastic excitations

NUCLEAR REACTIONS ²³⁸U(α, α), E=24.7 MeV; ²⁰⁸Pb(⁶He, ⁶He), E=22 MeV; ²⁰⁸Pb(⁷Li, ⁷Li), E=33 MeV; calculated σ(θ) comparing optical model and coupled-channels methods with data and the effect of using a dynamic polarization potential.

doi: 10.1140/epja/i2009-10838-x

2009SO12

Int.J.Mod.Phys. E18, 869 (2009)

A.Sobiczewski, M.Kowal

Description of experimental fission barriers of heavy nuclei

NUCLEAR STRUCTURE ^{232,234,236,238,240}U, ^{232,234,236,238,240,242,244,246}Pu, ^{242,246,248,250}Cm, ^250,252Cf, ^{260,262,264,266,268,270,272,274,276,278,280,282,284,286,288,290,292,294,296}Ds; calculated fission barriers, compared to other calculations and experiment.

doi: 10.1142/S0218301309012975

2009VE07

Phys.Rev. C 80, 031302 (2009)

P.Vesely, J.Kvasil, V.O.Nesterenko, W.Kleinig, P.-G.Reinhard, V.Yu.Ponomarev

Skyrme random-phase-approximation description of spin-flip M1 giant resonance

NUCLEAR STRUCTURE ⁴⁸Ca, ¹⁵⁸Gd, ²⁰⁸Pb, ²³⁸U; calculated spin-flip M1 giant resonance energies and strength distributions using random-phase approximation (RPA) calculations and Skyrme energy functionals with a set of eight Skyrme parametrizations. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.031302

2009WA01

Phys.Rev. C 79, 014316 (2009)

Y.Z.Wang, H.F.Zhang, J.M.Dong, G.Royer

Branching ratios of α decay to excited states of even-even nuclei

RADIOACTIVITY ^180,182,184Hg(α), ^186,188Pb(α), ^{190,194,196,198}Po(α), ²⁰²Rn(α), ^{226,228,230,232}Th(α), ^{230,232,234,236}U(α), ^{236,238,240,242}Pu(α), ^242,244Cm(α), ²⁴⁶Cf(α); calculated branching ratios for decays to ground excited states in the framework of generalized liquid-drop model. Comparison with experimental data.

doi: 10.1103/PhysRevC.79.014316

2010AB21

Nucl.Phys. A839, 1 (2010)

A.Y.Abul-Magd, S.A.Mazen, M.Abdel-Mageed, A.Al-Sayed

Identification of nuclei exhibiting the SU(3) dynamical symmetry

NUCLEAR STRUCTURE ¹⁵²Nd, ^154,156Sm, ^158,160,162Gd, ^{160,162,164,166}Dy, ^{164,166,168,170}Er, ^{168,170,172,178}Yb, ^{174,176,178,180}Hf, ^180,182,184W, ^230,232Th, ^232,234,238U, ^238,240,242Pu, ^244,246,248Cm, ²⁵⁰Cf, ²⁵⁶Fm; calculated energy levels, J, π, B(E2), related features for 2⁺ states using interactive boson model.

doi: 10.1016/j.nuclphysa.2010.03.007

2010AB23

Phys.Rev. C 82, 044303 (2010)

H.Abusara, A.V.Afanasjev, P.Ring

Fission barriers in actinides in covariant density functional theory: The role of triaxiality

NUCLEAR STRUCTURE ^{228,230,232,234}Th, ^{232,234,236,238,240}U, ^{236,238,240,242,244,246}Pu, ^{242,244,246,248,250}Cm, ^250,252Cf; calculated β₂- and γ-deformation energy curves, potential energy surfaces, proton and neutron single-particle energies as a function of β₂ and γ parameter, fission barriers as a function of proton and neutron number using relativistic mean-field theory and covariant density functional theory. Comparison with experimental data.

doi: 10.1103/PhysRevC.82.044303

2010BA07

Phys.Rev. C 81, 035501 (2010)

A.S.Barabash

Precise half-life values for two-neutrino double-β decay

RADIOACTIVITY ⁴⁸Ca, ⁷⁶Ge, ⁸²Se, ⁹⁶Zr, ¹⁰⁰Mo, ¹¹⁶Cd, ^128,130Te, ¹⁵⁰Nd, ²³⁸U(2β^-); ¹³⁰Ba(2EC); analyzed and recommended half-lives for double beta decays; deduced nuclear matrix elements. Reviewed experimental data.

doi: 10.1103/PhysRevC.81.035501

2010BO25

J.Phys.:Conf.Ser. 205, 012020 (2010)

D.Bonatsos, I.Boztosun, I.Inci

A long sought result: Closed analytical solutions of the Bohr Hamiltonian with the Morse potential

NUCLEAR STRUCTURE ^{98,100,102,104}Ru, ^{102,104,106,108,110,112,114,116}Pd, ^{106,108,110,112,114,116,118,120}Cd, ^{118,120,122,124,126,128,130,132,134}Xe, ^{130,132,134,136,142}Ba, ^134,136,138Ce, ^140,148,150Nd, ^{140,142,152,154}Sm, ^{142,144,152,154,156,158,160,162}Gd, ^{158,160,162,164,166}Dy, ^{156,160,162,164,166,168,170}Er, ^{164,166,168,170,172,174,176,178}Yb, ^{168,170,172,174,176,178,180}Hf, ^{176,178,180,182,184,186}W, ^{178,180,184,186,188}Os, ^{186,188,190,192,194,196,198,200}Pt, ²²⁸Ra, ^228,230,232Th, ^{232,234,236,238}U, ^{238,240,242,248}Cm, ²⁵⁰Cf; calculated low-lying 0⁺, 2⁺, 4⁺ states, β and γ bandheads, deformation using Bohr Hamiltonian with Morse potential; deduced Morse potential shapes. Compared with data.

doi: 10.1088/1742-6596/205/1/012020

2010BU02

Phys.Rev. C 81, 034322 (2010)

B.Buck, A.C.Merchant, S.M.Perez

Theory of recursive nuclear band spectra

NUCLEAR STRUCTURE ^102,104,106Mo, ^{102,104,106,110,112}Ru, ^{102,110,114,116}Pd, ¹⁴⁰Xe, ^144,146Ba, ^146,148Ce, ^148,150,152Nd, ^150,152,154Sm, ^{152,154,156,158,160}Gd, ^{154,156,158,160,162,164}Dy, ^{156,158,160,162,164,166,168,170}Er, ^{158,160,162,164,166,168,170,172,174,176}Yb, ^{164,166,168,170,172,174,176,178,180}Hf, ^{168,170,172,174,180,182,186}W, ^{172,174,180,182,184,186,188,192}Os, ^{176,180,184,186,188}Pt, ^222,224,226Ra, ^{222,226,228,230,232,234}Th, ^{230,232,234,236,238}U, ^{238,240,242,244}Pu, ²⁴⁸Cm; analyzed nuclear band spectra using recursion formula based on a quantum mechanical model.

doi: 10.1103/PhysRevC.81.034322

2010HA06

Phys.Rev. C 81, 024616 (2010)

Y.Han, Y.Xu, H.Liang, H.Guo, Q.Shen

Global phenomenological optical model potential for nucleon-actinide reactions at energies up to 300 MeV

NUCLEAR REACTIONS ²³²Th, ^233,235,238U, ²³⁷Np, ^239,240,242Pu, ²⁴¹Am(n, X), E=0.01-300 MeV; calculated total σ. ^235,238U(n, n), E=0.01-300 MeV; calculated σ. ²³²Th, ^235,238U, ²³⁹Pu(n, n'), E=0.1-300 MeV; calculated non-inelastic σ. ²³²Th, ^235,238U, ²³⁹Pu(n, n), (n, n'), E=0.14-15.2 MeV; ²³⁸U(n, n), E=96 MeV; calculated σ(θ) for elastic σ, inelastic σ and elastic+inelastic σ. ²³²Th, ²³⁸U(p, X), E=0-300 MeV; calculated σ. ²³²Th, ^235,238U(p, p), (p, p'), E=16-95 MeV; calculated σ(θ). global phenomenological optical model potential. Deduced of neutron and proton global optical model potential parameters. Comparison and analysis with experimental data.

doi: 10.1103/PhysRevC.81.024616

2010KO36

Phys.Rev. C 82, 054303 (2010)

M.Kowal, J.Skalski

Low-energy shape oscillations of negative parity in the main and shape-isomeric minima in actinides

NUCLEAR STRUCTURE ²⁴⁰Pu; calculated fission barrier and cranking mass contour plots as function of various deformation parameters. ^{230,232,234,236}Th, ^{230,232,234,236,238,240}U, ^{234,236,238,240,242,244,246}Pu, ^{234,236,238,240,242,244,246,250}Cm, ^{238,240,242,244,246,248,250,252,254}Cf; calculated stiffness coefficients at the first and second minima, energies of negative-parity shape oscillations in the first and second minima for K=0, 1 and 2, and transition electric dipole (E1) moments. Single-particle Hamiltonian with the deformed Woods-Saxon potential defined in terms of the nuclear surface and variety of shape deformations. Comparison with experimental data.

doi: 10.1103/PhysRevC.82.054303

2010KU17

Eur.Phys.J. A 43, 313 (2010)

A.A.Kuliev, E.Guliyev, F.Ertugral, S.Ozkan

The low-energy dipole structure of ²³²Th, ²³⁶U and ²³⁸U actinide nuclei

NUCLEAR STRUCTURE ²³²Th, ^236,238U; calculated B(M1), B(E1) strength distributions, transition widths, level energies; deduced scissors mode features. Quasiparticle RPA. Comparison with data.

doi: 10.1140/epja/i2010-10933-y

2010NI13

Phys.Rev. C 82, 024311 (2010)

D.Ni, Z.Ren

Half-lives and cluster preformation factors for various cluster emissions in trans-lead nuclei

RADIOACTIVITY ²¹⁰Pb, ²¹¹Bi, ^{211,212,213,214}Po(α); ^219,220Rn, ²²¹Fr, ^{221,222,223,224,225,226}Ra, ^223,225Ac, ²²⁶Th(¹⁴C); ²²¹Fr, ²²³Ac(¹⁵N); ²²³Ra, ^226,227Th, ²²⁷Pa(¹⁸O); ^225,226Ra, ²²⁷Ac, ^228,229Th(²⁰O); ²²⁸Th, ²²⁹Pa, ²³⁰U, ²³¹Np(²²Ne); ²²⁹Ac, ²³¹Pa(²³F); ^{229,230,231,232}Th, ²³¹Pa, ^{230,232,233,234,235,236}U, ²³³Np(²⁴Ne); ²³¹Th, ^233,235U(²⁵Ne); ²³²Th, ^234,236U(²⁶Ne); ^{232,233,234,235,236}U, ²³⁵Np, ^236,237,238Pu, ²³⁷Am(²⁸Mg); ²³⁵U, ²³⁷Pu(²⁹Mg); ^236,238U, ²³⁷Np, ^238,239Pu(³⁰Mg); ^237,238Pu, ²³⁹Am, ^240,241Cm(³²Si); ²³⁹Pu, ²⁴¹Am, ^242,243,244Cm(³⁴Si); calculated half-lives and cluster preformation factors using generalized density-dependent cluster model (GDDCM). Comparison with experimental data.

doi: 10.1103/PhysRevC.82.024311

2010PI02

Phys.Rev. C 81, 034307 (2010)

N.Pillet, N.Sandulescu, P.Schuck, J.-F.Berger

Two-particle spatial correlations in superfluid nuclei

NUCLEAR STRUCTURE ¹⁰²Sr, ¹⁵²Sm, ²³⁸U; calculated local and nonlocal parts of the pairing tensor, and coherence lengths. ⁶⁰Ni, ^120,136Sn, ²¹²Pb; calculated pairing correlation energies and average pairing fields, and coherence lengths. Effect of pairing on two-neutron spatial correlations in deformed nuclei. Hartree-Fock Bogoliubov calculations with D1S Gogny force.

doi: 10.1103/PhysRevC.81.034307

2010RA10

J.Phys.(London) G37, 085108 (2010)

A.A.Raduta, R.Budaca, A.Faessler

Closed formulas for ground band energies of nuclei with various symmetries

NUCLEAR STRUCTURE ¹⁰⁴Ru, ¹⁰²Pd, ¹⁰⁸Te, ^150,154,156Nd, ^{150,152,156,158}Sm, ^{152,154,160,162}Gd, ^{154,156,162,164}Dy, ¹⁶⁶Er, ^172,174Yb, ¹⁷⁶Hf, ^170,182,186W, ^{174,178,180,186}Os, ^176,178,180Pt, ^228,232Th, ^{232,234,236,238}U, ^{236,238,240,242}Pu, ²⁴⁸Cm; calculated level energies, J, π; deduced generalized Holmberg-Lipas formula. A time-dependent variational principal.

doi: 10.1088/0954-3899/37/8/085108

2010SA09

Nucl.Phys. A832, 220 (2010)

K.P.Santhosh, R.K.Biju, S.Sahadevan

Semi-empirical formula for spontaneous fission half life time

RADIOACTIVITY ²³²Th, ^{228,230,232,234,236,238}U, ^{232,234,236,238,240,242,244}Pu, ^{240,242,244,246,248,250}Cm, ^{240,242,244,246,248,250,252,254}Cf, ^{246,248,250,252,254,256,258,260}Fm, ^{250,252,254,256,258,260,262,264,266}No, ^{254,256,258,260,262,264,266,268}Rf, ^{258,260,262,264,266,268,270,272}Sg, ^{264,266,268,270,272,274,276}Hs, ^{260,262,264,266,268,270,272,274,276,278,280,282,284}Ds, ^{264,266,268,270,272,274,276,278,280,282,284,286,288}Cn, ^{268,270,272,274,276,278,280,282,284,286,288,290,292}Fl, ^{272,274,276,278,280,282,284,286,288,290,292,294,296}Lv, ^{276,278,280,282,284,286,288,290,292,294,296,298,300}Og, ^{274,276,278,280,282,284,286,288,290,292,294,296,298,300,302,304,306,308,310,312,314,316,318,320}120, ^{276,278,280,282,284,286,288,290,292,294,296,298,300,302,304,306,308,310,312,314,316}122(α), (SF); calculated T_1/2 using a Coulomb and Proximity Potential model and semi-empirical formula. Discussed SHE survivability. Comparison with data and systematics.

doi: 10.1016/j.nuclphysa.2009.10.160

2010SI12

Phys.Rev. C 82, 014607 (2010)

B.Singh, S.K.Patra, R.K.Gupta

Cluster radioactive decay within the preformed cluster model using relativistic mean-field theory densities

RADIOACTIVITY ²²¹Fr, ^{221,222,223,224,226}Ra, ^223,225Ac, ²²⁶Th(¹⁴C); ²²³Ac(¹⁵N); ²²⁶Th(¹⁸O); ²²⁸Th(²⁰O); ²³⁰Th, ²³¹Pa, ²³⁰U(²²Ne); ²³¹Pa(²³F); ^{230,232,233,234}U(²⁴Ne); ^{232,233,234,235,236}U, ^236,238Pu(²⁸Mg); ²³⁴U(²⁵Ne), (²⁶Ne); ²³⁸U, ²⁴¹Am, ²⁴²Cm(³⁴Si); ²³⁷Np, ²³⁸Pu(³⁰Mg); ²³⁸Pu(³²Si); calculated empirical preformation probabilities for cluster decays using preformed cluster model (PCM) and relativistic mean-field (RMF) theory densities.

doi: 10.1103/PhysRevC.82.014607

2010TO07

Phys.Atomic Nuclei 73, 1684 (2010); Yad.Fiz. 73, 1731 (2010)

S.V.Tolokonnikov, E.E.Saperstein

Description of superheavy nuclei on the basis of a modified version of the DF3 energy functional

NUCLEAR STRUCTURE ^{35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54,55,56,57}Ca, ^{176,177,178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214}Pb, ^{218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267,268,269,270,271,272,273,274,275,276,277,278,279,280,281,282}U, ²⁹⁸Fl; calculated proton and neutron single-particle spectrum, neutron separation energies, rms charge radii. DF-3, HFB-17 functionals.

doi: 10.1134/S1063778810100054

2010TR08

Phys.Atomic Nuclei 73, 1838 (2010); Yad.Fiz. 73, 1890 (2010)

V.A.Tryasuchev, A.V.Isaev

Calculation of eta-meson-nucleus quasibound states with optical potentials of the square-well and woods-saxon forms

NUCLEAR STRUCTURE ⁷Li, ¹¹B, ¹²C, ¹⁵N, ¹⁶O, ²⁴Mg, ⁴⁰Ca, ⁸⁴Kr, ¹⁵⁰Sm, ²⁰⁸Pb, ²³⁸U; calculated bound states of eta mesons and nuclei.

doi: 10.1134/S1063778810110050

2010VR01

Int.J.Mod.Phys. E19, 548 (2010)

D.Vretenar, T.Niksic, P.Ring

Relativistic nuclear energy density functionals

NUCLEAR STRUCTURE ^{226,228,230,232,234,236}Th, ^{228,230,232,234,236,238,240,242}U, ^{232,234,236,238,240,242,244,246}Pu, ^{238,240,242,244,246,248,250}Cm, ^{242,244,246,248,250,252,254,256}Cf, ^{242,244,246,248,250,252,254,256}Fm, ^{250,252,254,256,258,260,262}No; calculated ground-state axial quadrupole and hexadecapole moments.

doi: 10.1142/S0218301310014960

2010WA13

Phys.Rev. C 81, 054309 (2010)

M.Warda, X.Vinas, X.Roca-Maza, M.Centelles

Analysis of bulk and surface contributions in the neutron skin of nuclei

NUCLEAR STRUCTURE ^100,132Sn, ²⁰⁸Pb; Z=50, A=100-176; Z=82, A=168-268; calculated halo factor, neutron and proton densities, neutron skin thicknesses using Gogny, Skyrme, and covariant nuclear mean-field interactions. ^40,48Ca, ^54,56,57Fe, ^58,60,64Ni, ⁵⁹Co, ^90,96Zr, ^106,116Cd, ^{112,116,120,124}Sn, ^{122,124,126,128,130}Te, ²⁰⁸Pb, ²⁰⁹Bi, ²³²Th, ²³⁸U; analyzed experimental neutron skin thicknesses with results of the covariant NL3 and FSUGold parameter sets of the nonrelativistic Skyrme SLy4 and Gogny D1S forces.

doi: 10.1103/PhysRevC.81.054309

2010WA23

Phys.Rev. C 81, 067301 (2010)

Y.Z.Wang, J.M.Dong, B.B.Peng, H.F.Zhang

Fine structure of α decay to rotational states of heavy nuclei

RADIOACTIVITY ^172,174,186Os, ^{180,182,184,186,188,190}Pt, ^186,188Hg, ^228,230,232Th, ^{230,232,234,236,238}U, ^{232,234,236,238,240,242,244}Pu, ^{238,240,242,244,246,248,250,252,254}Cm, ^{246,248,250,252,254,256}Fm, ^252,254,256No, ²⁵⁶Rf, ²⁶⁰Sg(α); calculated Q-values, α branches to 2+ and 4+ states using generalized liquid drop model and improved Royer's formula calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.81.067301

2010WA31

Eur.Phys.J. A 44, 287 (2010)

Y.Z.Wang, J.Z.Gu, J.M.Dong, B.B.Peng

Properties of α-decay to ground and excited states of heavy nuclei

RADIOACTIVITY ^222,224,226Ra, ^{226,228,230,232}Th, ^{228,230,232,234,236,238}U, ^{234,236,238,240,242,244}Pu, ^{238,240,242,244,246,248}Cm, ^{244,246,248,250,252}Cf, ^248,250,252Fm, ²⁵²No(α); calculated branching ratios, T_1/2 using generalized liquid drop model and Royer's formula. Comparison with data and other models.

doi: 10.1140/epja/i2010-10948-4

2010ZH09

Phys.Rev. C 81, 041306 (2010)

S.Zhu, M.P.Carpenter, R.V.F.Janssens, S.Frauendorf, I.Ahmad, T.L.Khoo, F.G.Kondev, T.Lauritsen, C.J.Lister, D.Seweryniak

Possible double-octupole phonon band in ²³⁸U

NUCLEAR REACTIONS ²³⁸U(²⁰⁷Pb, ²⁰⁷Pb'), E=1400 MeV; measured Eγ, γγ-coin using Gammasphere array, unsafe Coulomb excitation. ²³⁸U; deduced levels, J, π, bands, Routhians, double-octupole phonon excitation. Comparison with band structures in ²⁴⁰Pu.

doi: 10.1103/PhysRevC.81.041306

2011AF04

J.Phys.:Conf.Ser. 312, 092004 (2011)

A.V.Afanasjev, H.Abusara, E.Litvinova, P.Ring

Spectroscopy of the heaviest nuclei (theory)

NUCLEAR STRUCTURE ²⁴⁰Pu, ²⁴¹Am, ²⁵¹Md; calculated moments of inertia of one-quasiproton configurations using CDFT (covariant density functional theory); compared with data. ^{228,230,232,234}Th, ^{232,234,236,238,240}U, ^{237,238,240,242,244,246}Pu, ^{242,244,246,248,250}Cm, ^252,254Cf; calculated deformation energy curves, fission barriers using RMF plus BCS with NL3* parameterization; compared to data.

doi: 10.1088/1742-6596/312/9/092004

2011BA28

Physics of Part.and Nuclei 42, 613 (2011)

A.S.Barabash

Double beta decay experiments

COMPILATION ⁴⁸Ca, ⁷⁶Ge, ^74,82Se, ⁹⁶Zr, ¹⁰⁰Mo, ^106,116Cd, ^128,130Te, ¹⁵⁰Nd, ²³⁸U, ^130,132Ba, ¹³⁶Xe, ⁷⁸Kr, ⁵⁸Ni, ⁹⁶Ru, ¹¹²Sn, ¹³⁶Ce, ¹⁶²Er; compiled experimental and evaluated double beta decay data.

doi: 10.1134/S1063779611040022

2011BO12

Phys.Rev. C 83, 044321 (2011)

D.Bonatsos, P.E.Georgoudis, D.Lenis, N.Minkov, C.Quesne

Bohr Hamiltonian with a deformation-dependent mass term for the Davidson potential

NUCLEAR STRUCTURE ^{98,100,102,104}Ru, ^{102,104,106,108,110,112,114,116}Pd, ^{106,108,110,112,114,116,118,120}Cd, ^{118,120,122,124,126,128,130,132,134}Xe, ^{130,132,134,136,142}Ba, ^134,136,138Ce, ^140,148,150Nd, ^{140,142,152,154}Sm, ^{142,144,152,154,156,158,160,162}Gd, ^{154,156,158,160,162,164,166}Dy, ^{156,160,162,164,166,168,170}Er, ^{162,164,166,168,170,172,174,176,178}Yb, ^{166,168,170,172,174,176,178,180}Hf, ^{176,178,180,182,184,186}W, ^{176,178,180,184,186,188,190}Os, ^{186,188,190,192,194,196,198,200}Pt, ²²⁸Ra, ^228,230,232Th, ^{232,234,236,238}U, ^238,240,242Pu, ²⁴⁸Cm, ²⁵⁰Cf; calculated levels, J, π, B(E2). Bohr collective Hamiltonian, β₂ deformation dependent mass, curved space, Davidson potential. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.044321

2011CH65

Phys.Atomic Nuclei 74, 1713 (2011)

V.P.Chechev

The evaluation of half-lives and other decay data used in nuclear astrophysics and cosmochronology

COMPILATION ²⁶Al, ⁴⁰K, ⁵³Mn, ⁶⁰Fe, ⁸⁷Rb, ⁹³Zr, ⁹⁸Tc, ¹⁰⁷Pd, ¹²⁹I, ¹³⁵Cs, ¹⁴⁶Sm, ¹⁷⁶Lu, ¹⁸²Hf, ¹⁸⁷Re, ²⁰⁵Pb, ²³²Th, ^235,238U, ²⁴⁴Pu, ²⁴⁷Cm; compiled experimental nuclear structure data, T_1/2. Cosmochronology applications.

doi: 10.1134/S106377881111007X

2011DU30

Phys.Rev. C 84, 061301 (2011)

J.Dukelsky, SH.Lerma, L.M.Robledo, R.Rodriguez-Guzman, S.M.A.Rombouts

Exactly solvable pairing Hamiltonian for heavy nuclei

NUCLEAR STRUCTURE ²³⁸U, ¹⁵⁴Sm; calculated state-dependent gaps, proton pairing tensor, pairing energies. Exactly solvable Hamiltonian from Richardson-Gaudin models. Comparison with Gogny self-consistent mean-field calculations in the Hartree-Fock basis.

doi: 10.1103/PhysRevC.84.061301

2011HE12

Radiochim.Acta 99, 441 (2011)

R.-D.Herzberg, D.M.Cox

Spectroscopy of actinide and transactinide nuclei

COMPILATION ^{183,185,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,210,212}Pb, ^{184,186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212}Bi, ^{191,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212}Po, ^{191,193,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214}Po, ^{195,197,199,200,201,202,203,204,205,206,207,208,210,211,212,213,214,217,219}Rn, ^{201,202,203,204,205,206,207,208,209,210,211,212,213,214}Po, ^{195,197,199,200,201,202,204,206,208,211,212,213,214,215,218,227}Rn, ^{203,205,207,208,210,212,213,214,215,216,217,225,229,231}Ra, ^{206,208,215,216,217,218,222,227}Ac, ^216,217Th, ^217,233,234Pa, ^{218,234,235,236,238,239}U, ^{235,236,237,239,240,242}Np, ^{235,236,237,238,239,240,241,242,243,245}Pu, ^{236,237,238,239,240,241,242,243,244,245,246}Am, ^{240,241,242,243,244,245,246,247}Cm, ^{242,243,244,245,250}Bk, ^249,251Cf, ^250,254Es, ^{247,248,250,251,256}Fm, ²⁵⁸Md, ^{250,251,252,253,254}No, ²⁵³Lr, ^253,256,257Rf, ^257,258Db, ^261,263,265Sg, ²⁶²Bh, ^265,267Hs, ^270,271Ds; compiled T_1/2, J, π, energy for the longest-lived isomers.

doi: 10.1524/ract.2011.1858

2011HI13

J.Korean Phys.Soc. 59, 803s (2011)

S.Hilaire, M.Girod, S.Goriely

Improving the Description of Collective Effects within the Combinatorial Model of Nuclear Level Densities

NUCLEAR STRUCTURE ⁴²K, ⁵⁶Fe, ⁶⁰Co, ⁹⁴Nb, ¹⁰⁷Cd, ¹²⁷Te, ¹⁴⁸Pm, ¹⁷²Yb, ¹⁹⁴Ir, ²⁰⁸Pb, ²³⁷U, ²³⁹Pu; calculated level density. ⁵⁴Cr, ¹⁰⁰Ru, ¹³⁰Xe, ¹⁸⁰Hf, ²⁰⁸Pb, ²³⁸U; calculated temperature, deformation. ²³⁸U; calculated level density, temperatures from 0 to 100 MeV. HFB plus combinatorial approach.

NUCLEAR REACTIONS ^235,236U, ²³⁷Np, ^238,240,241Pu(n, f), E=0.01-30 MeV; calculated σ using microscopic fission path and combinatorial level density.

doi: 10.3938/jkps.59.803

2011IN03

Phys.Rev. C 84, 024309 (2011)

I.Inci, D.Bonatsos, I.Boztosun

Electric quadrupole transitions of the Bohr Hamiltonian with the Morse potential

NUCLEAR STRUCTURE ^{98,100,102,104}Ru, ^{102,104,106,108}Pd, ^{108,110,112,114,116,118}Cd, ^{118,120,124,128}Xe, ^{130,132,134,142}Ba, ¹⁴⁸Nd, ¹⁵²Gd, ¹⁵⁴Dy, ^{192,194,196,198}Pt, ¹⁵⁴Sm, ¹⁵⁶Gd, ¹⁵⁸Gd, ^158,160Dy, ¹⁶²Dy, ¹⁶⁴Dy, ^{156,162,164,166,168,170}Er, ^{166,168,170,172,174,176}Yb, ^174,176,178Hf, ^182,184,186W, ^186,188Os, ^230,232Th, ^234,236,238U, ²³⁸Pu, ²⁵⁰Cf; calculated B(E2) ratios for ground-state bands and interband transitions in γ-soft and deformed nuclei. Asymptotic iteration method (AIM) for collective Bohr Hamiltonian with the Morse potential. Comparison with experimental data.

doi: 10.1103/PhysRevC.84.024309

2011KO35

Phys.Rev. C 84, 034312 (2011)

P.E.Koehler

Reduced neutron widths in the nuclear data ensemble: Experiment and theory do not agree

NUCLEAR STRUCTURE ^64,66,68Zn, ¹¹⁴Cd, ^152,154Sm, ^{154,156,158,160}Gd, ^160,162,164Dy, ^166,168,170Er, ^172,174,176Yb, ^182,184,186W, ²³²Th, ²³⁸U; analyzed reduced neutron widths for 1245 neutron resonances in the nuclear data ensemble (NDE); deduced disagreement with Porter Thomas distribution (PTD) based on Random matrix theory (RMT) predictions.

doi: 10.1103/PhysRevC.84.034312

2011LE21

Phys.Rev. C 84, 014310 (2011)

J.Le Bloas, M.Koh, P.Quentin, L.Bonneau, J.I.A.Ithnin

Exact Coulomb exchange calculations in the Skyrme-Hartree-Fock-BCS framework and tests of the Slater approximation

NUCLEAR STRUCTURE ¹⁶O, ²⁴Mg, ^40,48Ca, ⁴⁸Cr, ^48,56Ni, ⁹⁰Zr, ¹⁰⁶Mo, ^100,132Sn, ^174,176,178Hf, ^206,208,210Pb, ²³⁸U, ²⁹⁸Fl, ³¹⁰126; Z=20-34, N=28; Z=40-58, N=64; Z=52-62, N=78; Z=68-80, N=106; Z=76-88, N=126; Z=86-100, N=146; calculated Coulomb interaction and fission properties for even-even nuclei within the Skyrme-Hartree-Fock/Bardeen-Cooper-Schrieffer approach. Pairing correlations. ⁷⁰Se; calculated deformation energy curves. ²¹²Po, ²¹⁴Rn, ²¹⁶Ra, ²¹⁸Th; calculated α decay properties.

doi: 10.1103/PhysRevC.84.014310

2011LI44

Eur.Phys.J. A 47, 135 (2011)

H.L.Liu, F.R.Xu, Y.Sun, P.M.Walker, R.Wyss

On the stability of high-K stability of high-K isomers in the second well of actinide nuclei

NUCLEAR STRUCTURE ²³⁸U, ^236,238,242Pu, ^240,242,244Cm; calculated levels, K, π, β₂, β₄, configurations, energy surface for broken-pair excitations. Energies compared to data.

doi: 10.1140/epja/i2011-11135-y

2011LI53

J.Korean Phys.Soc. 59, 1900s (2011)

O.Litaize, C.De Saint Jean, G.Noguere, P.Archier

Statistical Analysis of a Set of Actinide Resolved Resonance Parameters with CONRAD Code

NUCLEAR STRUCTURE ²³⁸U; calculated, analyzed resonance parameters using CONRAD code; deduced different distributions. Compared with JEFF-3.1, ENDF-B/VII.0.

doi: 10.3938/jkps.59.1900

2011MA89

Eur.Phys.J.Plus 126, 49 (2011)

S.G.Mashnik

Validation and verification of MCNP6 against intermediate and high-energy experimental data and results by other codes

NUCLEAR REACTIONS ¹⁸O(p, γ), ¹⁹⁷Au(p, α), ²³⁸U(p, p), (p, d), (p, t), ⁵⁶Fe(p, X)Na/Al/P/Cl/K/Sc/V/Mn, ⁴⁰Ca(⁴⁰Ar, p), ⁶⁴Cu(²⁰Ne, d), ²³⁸U(²⁰Ne, t), (²⁰Ne, ³He), (²⁰Ne, α), ⁴⁰Ca(⁹Be, X)Si, ⁶⁴Cu(²⁸Si, n), ¹²C(¹²C, π^-), Cu(¹⁹⁷Au, X), (²⁰⁸Pb, X), ¹⁸¹Ta(p, K⁺), (p, t), (p, π⁺), (p, π^-), E<400 GeV; calculated σ, σ(θ, E) with MCNP6 code. Comparison with experimental data.

doi: 10.1140/epjp/i2011-11049-1

2011NA24

Ukr.J.Phys. 56, 511 (2011)

M.S.Nadirbekov, G.A.Yuldasheva

"Staggering" Effect in Even-even Nuclei with Quadrupole and Octupole Deformations

NUCLEAR STRUCTURE ^{230,234,236,238}U, ²³²Th; calculated staggering effect in energy spectra. Comparison with experimental data.

2011NI05

Eur.Phys.J. A 47, 9 (2011)

I.Nishinaka, M.Tanikawa, Y.Nagame, H.Nakahara

Nuclear-charge polarization at scission in proton-induced fission of ²³³U

NUCLEAR REACTIONS ²³³U(p, F), E=11.5 MeV; measured fission fragments, (fragment)(fragment)-coin, En, In, (fragment)n-coin; deduced yields, average kinetic energy, neutron multiplicity vs fragment mass, neutron-to-proton ratio, nuclear charge polarization vs fragment mass. Measurements compared with other data.

doi: 10.1140/epja/i2011-11009-4

2011NO04

Phys.Rev. C 83, 041302 (2011); Pub.Note Phys.Rev. C 83, 059901 (2011)

K.Nomura, T.Otsuka, N.Shimizu, L.Guo

Microscopic formulation of the interacting boson model for rotational nuclei

NUCLEAR STRUCTURE ^{146,148,150,152,154}Sm, ^{230,232,234,236,238}U; calculated overlap between the intrinsic state and its rotation angle, and moments of inertia. ^{146,148,150,152,154}Sm, ^{148,150,152,154,156,158,160}Gd, ²³⁰Th, ²³²U; calculated yrast spectra of ground state rotational bands, J, π. Interacting boson model for rotational nuclei with axially symmetric strong deformation. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.041302

2011PE01

Phys.Rev. C 83, 014314 (2011)

S.Peru, G.Gosselin, M.Martini, M.Dupuis, S.Hilaire, J.-C.Devaux

Giant resonances in ²³⁸U within the quasiparticle random-phase approximation with the Gogny force

NUCLEAR STRUCTURE ²³⁸U; calculated Kπ=0-, 0+, 1-, 1+ eigenvalues, B(E0), B(E1), B(E2) and B(E3) strengths for dipole, monopole, quadrupole, and octupole giant resonances and low-energy states. Fully consistent microscopic axially-symmetric deformed quasiparticle random-phase approximation (QRPA) approach using a finite-range Gogny force for Hartree-Fock-Bogolyubov mean field and QRPA matrix. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.014314

2011RI05

Int.J.Mod.Phys. E20, 235 (2011)

P.Ring, H.Abusara, A.V.Afanasjev, G.A.Lalazissis, T.Niksic, D.Vretenar

Modern applications of Covariant Density Functional theory

NUCLEAR STRUCTURE ^{228,230,232,234}Th, ^{232,234,236,238,240}U, ^{236,238,240,242,244,246}Pu, ^{242,244,246,248,250}Cm, ^250,252Cf, ¹⁵⁰Nd; calculated potential and deformation energy surfaces, J, π.

doi: 10.1142/S0218301311017570

2011WA30

Phys.Rev. C 84, 044608 (2011)

M.Warda, L.M.Robledo

Microscopic description of cluster radioactivity in actinide nuclei

RADIOACTIVITY ^222,224,226Ra(¹⁴C); ²²⁶Th(¹⁸O); ²²⁶Ra, ²²⁸Th, ²³⁰U(²⁰O); ^230,232Th(²²O); ^230,232Th, ²³²U(²⁴Ne); ²³²Th, ²³⁴U(²⁶Ne); ^234,238U(²⁸Mg); ²³⁸Pu(³⁰Mg), (³²Si); ²⁴⁰Pu, ²⁴²Cm(³⁴Si); calculated hyper-asymmetric fission barriers, T_1/2. Hartree-Fock-Bogoliubov model for cluster decay. Comparison with experimental data.

NUCLEAR STRUCTURE ²²⁴Ra, ²³⁸Pu; calculated potential energy surfaces, fission barriers, shape evolution with quadrupole moment, potential energies, density distributions.

doi: 10.1103/PhysRevC.84.044608

2011WU03

Phys.Rev. C 83, 034323 (2011)

X.Wu, Z.H.Zhang, J.Y.Zeng, Y.A.Lei

Nuclear pairing reduction due to rotation and blocking

NUCLEAR STRUCTURE ¹⁶⁸Yb, ¹⁶⁸Hf, ¹⁷⁷Ta, ¹⁷⁸W, ^193,194Hg, ²³⁸U, ²⁵³No; calculated moments of inertia and pairing gaps for normal deformed and superdeformed bands. Particle number-conserving (PNC) formalism for the cranked shell model. Comparison with number-projected Hartree-Fock-Bogolyubov approach, and with experimental data.

doi: 10.1103/PhysRevC.83.034323

2011ZH36

Phys.Rev. C 84, 044312 (2011)

X.Zhang, C.Xu, Z.Ren

α decay to members of favored bands in both even-even and odd-A nuclei

RADIOACTIVITY ^224,226Ra, ^227,229Pa, ^{224,226,228,230,232}Th, ^{226,228,230,232,233,234,235,236,238}U, ^{232,234,236,237,238,239,240,241,242,244}Pu, ^239,241,243Am, ^{240,241,242,243,244,245,246,247,248}Cm, ^{243,245,247,249}Bk, ^{240,242,244,246,247,248,249,250,251,252,253,254}Cf, ^{245,251,253,255}Es, ^{246,248,250,251,252,253,254,255,256,257}Fm, ^252,254,256No, ^256,258Rf(α); calculated partial α-decay T_1/2 to members of favored bands. Geiger-Nuttall law, microscopic quantum tunneling theory. Comparison with experimental data.

doi: 10.1103/PhysRevC.84.044312

2012BU08

Phys.Rev. C 85, 054302 (2012)

B.Buck, A.C.Merchant, S.M.Perez

Electromagnetic transition strengths in heavy nuclei

NUCLEAR STRUCTURE ^230,232Th, ^234,238U; calculated reduced B(E2), B(M1) for transitions within and between K=0+, 1+ and 2+ bands. Cluster Model for the structure of heavy nuclei. Discussion of beta and gamma bands. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.054302

2012FA12

Phys.Rev.Lett. 109, 202504 (2012)

M.Fallot, S.Cormon, M.Estienne, A.Algora, V.M.Bui, A.Cucoanes, M.Elnimr, L.Giot, D.Jordan, J.Martino, A.Onillon, A.Porta, G.Pronost, A.Remoto, J.L.Tain, F.Yermia, A.-A.Zakari-Issoufou

New Antineutrino Energy Spectra Predictions from the Summation of Beta Decay Branches of the Fission Products

RADIOACTIVITY ^{102,104,105,106,107}Tc, ¹⁰⁵Mo, ¹⁰¹Nb(β^-); analyzed available data. ^235,238U, ^239,241Pu; deduced impact on the calculated antineutrino energy spectrum from ^235,238U, ^239,241Pu. Comparison with available data.

doi: 10.1103/PhysRevLett.109.202504

2012FR06

Phys.Rev. C 86, 044303 (2012)

S.Fracasso, E.B.Suckling, P.D.Stevenson

Unrestricted Skyrme-tensor time-dependent Hartree-Fock model and its application to the nuclear response from spherical to triaxial nuclei

NUCLEAR STRUCTURE ¹⁶O, ²⁴Mg, ²⁸Si, ¹²⁰Sn, ¹⁷⁸Os, ¹⁹⁰W, ²³⁸U; calculated transition strength distributions of isovector giant dipole resonances using the Skyrme energy density functional (EDF) in the three dimensional time-dependent Hartree-Fock. Comparison with predictions from the (quasi)-particle random-phase approximation and experimental data.

doi: 10.1103/PhysRevC.86.044303

2012GO13

J.Phys.:Conf.Ser. 337, 012027 (2012)

S.Goriely, S.Hilaire, M.Girod

Latest development of the combinatorial model of nuclear level densities

NUCLEAR STRUCTURE ²³⁸U; calculated deformation, positive parity level density vs excitation energy, temperature using combinatorial approach. A=15-255; calculated s-wave neutron resonance spacings using HFB plus combinatorial densities. Compared with published compilation by Capote et al.

doi: 10.1088/1742-6596/337/1/012027

2012HI11

Phys.Rev. C 86, 064317 (2012)

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

Temperature-dependent combinatorial level densities with the D1M Gogny force

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

doi: 10.1103/PhysRevC.86.064317

2012IS08

Phys.Rev. C 86, 044317 (2012)

M.Ismail, A.Y.Ellithi, M.M.Botros, A.Abdurrahman

Penetration factor in deformed potentials: Application to α decay with deformed nuclei

RADIOACTIVITY ²¹⁰Pb, ^{212,214,216,218}Po, ^{214,216,218,220,222}Rn, ^{216,218,220,222,224,226}Ra, ^{218,220,222,224,226,228,230,232}Th, ^{220,222,224,226,228,230,232,234,236,238}U, ^{228,230,232,234,236,238,240,242,244}Pu, ^{238,240,242,244,246,248}Cm, ^{240,242,244,246,248,250,252,254}Cf, ^{246,248,250,252,254,256}Fm, ^{252,254,256,258}No, ^256,258,260Rf, ^260,266Sg, ^264,266,270Hs, ^270,280Ds, ²⁸⁴Cn, ^286,288Fl, ^290,292Lv, ²⁹⁴118(α); calculated half-lives using deformed density dependent cluster model. Comparison with experimental data.

doi: 10.1103/PhysRevC.86.044317

2012JA08

Phys.Rev. C 85, 034305 (2012)

P.Jachimowicz, M.Kowal, J.Skalski

Secondary fission barriers in even-even actinide nuclei

NUCLEAR STRUCTURE ^{226,228,230,232,234,236}Th, ^{230,232,234,236,238,240,242}U, ^{234,236,238,240,242,244,246,248}Pu, ^{240,242,244,246,248,250,252}Cm, ^{248,250,252,254}Cf; calculated mass excess, microscopic and macroscopic energies, deformation parameters, second fission barriers, surface contours, second minima excitation energies. macroscopic-microscopic model in six-dimensional deformation space for even-even actinides. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.034305

2012JO02

Phys.Rev. C 86, 024319 (2012)

R.V.Jolos, P.von Brentano, J.Jolie

Second order phase transitions from octupole-nondeformed to octupole-deformed shape in the alternating parity bands of nuclei around ²⁴⁰Pu based on data

NUCLEAR STRUCTURE ²³²Th, ²³⁸U, ²⁴⁰Pu; calculated potential energy of the octupole collective motion as function of β₃ parameter and angular momentum; analyzed levels, J, π, ground-state alternating parity bands. Supersymmetric quantum mechanics, two-center octupole wave functions ansatz, and Landau theory of phase transitions. Evidence for second order phase transition from reflection-symmetric to reflection-asymmetric shapes.

doi: 10.1103/PhysRevC.86.024319

2012KO06

Phys.Rev. C 85, 024304 (2012)

M.Kortelainen, J.McDonnell, W.Nazarewicz, P.-G.Reinhard, J.Sarich, N.Schunck, M.V.Stoitsov, S.M.Wild

Nuclear energy density optimization: Large deformations

NUCLEAR STRUCTURE ^236,238U, ²⁴⁰Pu, ²⁴²Cm; calculated energies of fission isomers in UNEDF1 optimization. ^192,194Hg, ^192,194,196Pb; calculated energies of bandheads in superdeformed nuclei. ²⁰⁸Pb; calculated single particle energies. ^236,238U, ^{238,240,242,244}Pu, ^{242,244,246,248}Cm; calculated inner barrier heights, outer barrier heights. N=14-156, Z=10-104; deduced rms deviations from experimental values for binding energy, S(2n), S(2p), three-point odd-even mass difference, rms proton radii for even-even nuclei. Hartree-Fock-Bogoliubov theory, POUNDerS optimization algorithm, UNEDF0 and UNEDF1 parameterizations. Neutron drops. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.024304

2012KO10

Phys.Rev. C 85, 034316 (2012)

J.Kotila, F.Iachello

Phase-space factors for double-β decay

RADIOACTIVITY ⁴⁸Ca, ⁷⁶Ge, ⁸²Se, ⁹⁶Zr, ¹⁰⁰Mo, ¹¹⁰Pd, ¹¹⁶Cd, ¹²⁴Sn, ¹²⁸Te, ¹³⁰Te, ¹³⁶Xe, ¹⁴⁸Nd, ¹⁵⁰Nd, ¹⁵⁴Sm, ¹⁶⁰Gd, ¹⁹⁸Pt, ²³²Th, ²³⁸U(2β^-); calculated phase-space factors, Single-electron spectra, summed energy spectra, half-lives, angular correlations, effective nuclear matrix elements for 2νββ and 0νββ decay modes. Exact Dirac wave functions with finite nuclear size and electron screening. Comparison with previous studies and experimental data.

doi: 10.1103/PhysRevC.85.034316

2012KU23

Eur.Phys.J. A 48, 112 (2012)

S.N.Kuklin, T.M.Shneidman, G.G.Adamian, N.V.Antonenko

Alpha-decay fine structures of U isotopes and systematics for isotopic chains of Po and Rn

RADIOACTIVITY ²²⁸Th(²⁰O), ²²²Ra(¹⁴C), ²³²U(²⁴Ne), ²³⁴U(²⁶Ne), ²³⁶U(³⁰Mg), ²³⁶Pu(²⁸Mg), ²³⁸Pu(³²Si); calculated T_1/2. ^{184,186,188,190,192,194,196,198,200,202,204,206,208}Po, ^{194,196,198,200,202,204,206,208,210}Rn, ^{224,226,228,230,232,234,236,238}U(α); calculated α spectroscopic factor for low-lying positive parity states, T_1/2. Zero-point vibrations in the charge-asymmetry coordinate; compared to data.

NUCLEAR STRUCTURE ^{184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218}Po, ^{194,196,198,200,202,204,206,208,210,212,214,216,218,220,222}Rn; calculated α cluster spectroscopic factor using zero-point vibrations in the charge-asymmetry coordinate. Compared to data.

doi: 10.1140/epja/i2012-12112-8

2012KU29

Phys.Rev. C 86, 044612 (2012)

R.Kumar

Cluster radioactivity using various versions of nuclear proximity potentials

RADIOACTIVITY ¹¹⁴Ba(¹²C); ²²¹Fr, ²²¹Ra, ^{222,223,224,226}Ra, ^223,225Ac, ²²⁶Th(¹⁴C); ²²¹Fr, ²²³Ac(¹⁵N); ²²³Ra, ^{226,227,228,230}Th, ²²⁸U, ²²⁷Pa(¹⁸O); ^225,226Ra, ²²⁷Ac, ^228,230Th, ²²⁹Pu(²⁰O); ^230,232U, ²³²Pu, ²²⁸Th, ²²⁹Pa, ²³¹Np(²²Ne); ²²⁹Ac, ²³¹Pa(²³F); ^{228,229,230,231,232}Th, ²³¹Pa, ^{230,232,233,234,235,236}U, ²³³Np, ²³⁴Pu(²⁴Ne); ^233,234,235U, ²³¹Th(²⁵Ne); ²³⁵U(²⁵Mg); ²³²U, ^232,234Pu(²⁶Mg); ^234,236U, ²³²Th(²⁶Ne); ^{232,233,234,235,236}U, ^234,236,238Pu, ²³⁸Cm, ²³⁵Np, ²³⁷Pu, ²³⁷Am(²⁸Mg); ²³⁵U, ²³⁷Pu(²⁹Mg); ^236,238U, ²³⁷Np, ^238,239Pu(³⁰Mg); ²³⁸Cm(³⁰Si); ^236,237,238Pu, ²³⁹Am, ^240,241Cm(³²Si); ²³⁸U, ^238,240Pu, ²⁴¹Am, ^{240,242,243,244}Cm(³⁴Si); ²³⁹Pu(³⁴Mg); ²⁵²Cf(⁴⁶Ar), (⁴⁸Ca), ⁵⁰Ca; calculated half-lives for cluster decay for different nuclear proximity potentials and for spherical and deformed structures, preformation probability. The preformed cluster-decay model. Comparison with experimental data, and with universal decay law (UDL) and generalized density-dependent cluster model (GDDCM) calculations.

doi: 10.1103/PhysRevC.86.044612

2012LU02

Phys.Rev. C 85, 011301 (2012)

B.-N.Lu, E.-G.Zhao, S.-G.Zhou

Potential energy surfaces of actinide nuclei from a multidimensional constrained covariant density functional theory: Barrier heights and saddle point shapes

NUCLEAR STRUCTURE ²⁴⁰Pu, ²⁴⁸Cm; calculated potential energy surfaces. ^230,232Th, ^{232,234,236,238}U, ^{238,240,242,244}Pu, ^{242,244,246,248}Cm; calculated inner and outer fission barrier heights. Importance of triaxial and octupole shapes in fission path. Multidimensional constrained covariant density functional theory. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.011301

2012NA10

Int.J.Mod.Phys. E21, 1250044 (2012)

M.S.Nadirbekov, G.A.Yuldasheva, N.Minkov, W.Scheid

Collective excited states in even-even nuclei with quadrupole and octupole deformations

NUCLEAR STRUCTURE ¹⁵⁰Nd, ^152,154Sm, ^154,156,158Gd, ¹⁵⁶Dy, ^162,164Er, ²²⁴Ra, ²²⁸Th, ^{232,234,236,238}U, ²⁴⁰Pu; calculated energy levels, J, π, staggering effects, yrast bands. Comparison with available data.

doi: 10.1142/S0218301312500449

2012NE04

Int.J.Mod.Phys. E21, 1250050 (2012)

B.Nerlo-Pomorska, K.Pomorski, J.Bartel

Dynamical coupling of rotation with the pairing field in heavy nuclei

NUCLEAR STRUCTURE ^{230,232,234,236,238,240}U, ^242,246,248Cm, ^{248,250,252,254}No; calculated level energies, J, π, rotational bands. Macroscopic-macroscopic model with the Lublin-Strasbourg Drop, the Yukawa-folded single-particle potential, comparison with available data.

doi: 10.1142/S0218301312500504

2012PR09

Phys.Rev. C 86, 024317 (2012)

V.Prassa, T.Niksic, G.A.Lalazissis, D.Vretenar

Relativistic energy density functional description of shape transitions in superheavy nuclei

NUCLEAR STRUCTURE ^{226,228,230,232,234,236}Th, ^{228,230,232,234,236,238,240,242}U, ^{232,234,236,238,240,242,244,246}Pu, ^{238,240,242,244,246,248,250}Cm, ^{242,244,246,248,250,252,254,256}Cf, ^{242,244,246,248,250,252,254,256}Fm, ^{250,252,254,256,258,260,262}No; calculated binding energies, ground-state axial quadrupole moments. ^236,238U, ²⁴⁰Pu, ²⁴²Cm; calculated constrained energy curves as a function of quadrupole deformation parameter. ^298,300120, ^294,296Og, ^290,292Lv, ^286,288Fl, ^282,284Cn, ^278,280Ds; calculated RHB axially symmetric energy curves, triaxial energy contours in β-γ plane. ²⁸⁴Cn, ²⁹²Lv, ³⁰⁰120; calculated proton and neutron density distributions. Microscopic, relativistic energy density functional (REDF)-based, quadrupole collective Hamiltonian model.

RADIOACTIVITY ^{234,236,238,240,242,244}Pu, ^{238,240,242,244,246,248,250,252}Cm, ^{242,244,246,248,250,252,254}Cf, ^{246,248,250,252,254,256}Fm, ^252,254,256No, ^256,258Rf, ^260,262Sg, ^271,272Bh, ^275,276Mt, ^278,280Ds, ^279,280Rg, ^282,284Cn, ^283,284Nh, ^286,288Fl, ^287,288Mc, ^290,292Lv, ^293,294Ts, ^294,296Og, ^298,300120(α); calculated Q(α), half-lives. Microscopic, relativistic energy density functional (REDF)-based, quadrupole collective Hamiltonian model. Comparison with experimental data.

doi: 10.1103/PhysRevC.86.024317

2012RE06

Phys.Rev. C 85, 044608 (2012)

Y.Ren, Z.-Z.Ren

New Geiger-Nuttall law for α decay of heavy nuclei

RADIOACTIVITY ^{190,191,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,212,213,214,215,216,217,218}Po, ^{204,206,208,210,212,213,214,216,218,220,222}Rn, ^{202,204,206,214,215,216,218,220,222,224,226}Ra, ^{212,214,216,217,218,220,222,224,226,228,230,232}Th, ^{218,219,222,224,226,228,230,232,234,236,238}U, ^{158,160,162,164,166,168}W, ^{156,158,160,162}Hf, ^154,156,158Yb, ^152,154,156Er, ^150,152,154Dy, ^148,150,152Gd, ^146,148Sm, ¹⁴⁴Nd(α); calculated T_1/2 by new Geiger-Nuttall law. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.044608

2012RO29

J.Phys.(London) G39, 105103 (2012)

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

Octupole deformation properties of actinide isotopes within a mean-field approach

NUCLEAR STRUCTURE ^{220,222,224,226,228,230,232,234,236,238,240}U, ^{222,224,226,228,230,232,234,236,238,240,242}Pu, ^{222,224,226,228,230,232,234,236,238,240,242}Cm, ^{222,224,226,228,230,232,234,236,238,240,242}Cf; calculated octupole deformation, B(E1), B(E3). Systematic mean-field calculations, comparison with experimental data.

doi: 10.1088/0954-3899/39/10/105103

2012RO34

Phys.Rev. C 86, 044326 (2012)

G.Royer, M.Jaffre, D.Moreau

Fission barriers and half-lives of actinides in the quasimolecular shape valley

RADIOACTIVITY ^230,231,233Th, ^{232,234,235,236,237,238,239}U, ²³⁸Np, ^{238,239,240,241,243}Pu, ^242,243,244Am, ^243,245,248Cm, ²⁵⁰Bk, ²⁵⁰Cf, ^255,256Es, ^255,256Fm, ²⁵⁶No(SF); calculated half-lives, fission barriers using the generalized liquid-drop model. Quasi-molecular shapes. Comparison with experimental data.

doi: 10.1103/PhysRevC.86.044326

2012SA31

Nucl.Phys. A889, 29 (2012)

K.P.Santhosh, B.Priyanka, M.S.Unnikrishnan

Cluster decay half-lives of trans-lead nuclei within the Coulomb and proximity potential model

RADIOACTIVITY ^{199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226}Fr(¹⁴C), ^{202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230}Ra(¹⁴C), (²⁰O), ^{206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232}Ac(¹⁴C), (¹⁵N), ^{209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237}Th(¹⁶C), (¹⁸O), (²⁰O), (²²O), (²⁴Ne), (²⁶Ne), ^{212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238}Pa(²³F), (²⁴Ne), ^{217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241}U(²⁰O), (²²Ne), (²⁴Ne), (²⁵Ne), (²⁶Ne), (²⁸Mg), (²⁹Mg), (³⁰Mg), ^{225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242}Np(³⁰Mg), ^{225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244}Pu(²⁸Mg), (³⁰Mg), (³²Si), (³⁴Si), ^{231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246}Am(³⁴Si), ^{233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249}Cm(³⁴Si); calculated Q-value, T_1/2 using CPPM (Coulomb and proximity potential model), Universal formula for cluster decay, Universal decay law and Scaling Law.

doi: 10.1016/j.nuclphysa.2012.07.002

2012TA10

Phys.Scr. 86, 015201 (2012)

O.A P.Tavares, E.L.Medeiros

A simple description of cluster radioactivity

RADIOACTIVITY ²³⁸U, ^239,240Pu, ^241,243Am, ^240,242,243Cm(³⁴Si), ^236,237Np, ²³⁸Pu, ²⁴¹Am, ^240,242Cm(³²Si), ²⁵²Cf, ²⁵⁴Es(⁴⁶Ar), ²⁵²Es(⁴⁸Ca), ²⁵⁴Es, ²⁵⁸Md, ²⁵⁹No(⁵⁰Ca), ²⁵⁹No(⁴⁹Ca), ²²⁸Th(²⁰O), ²⁴⁰Pu(³⁴Si), ²⁵⁹No(⁵⁰Ca), ²⁸²Rg(⁷³Ni), ²⁹¹Mc(⁸⁵Br); calculated T_1/2, Q-values, branching ratios. Comparison with available data.

doi: 10.1088/0031-8949/86/01/015201

2012WA38

Chin.Phys.C 36, 1603 (2012)

M.Wang, G.Audi, A.H.Wapstra, F.G.Kondev, M.MacCormick, X.Xu, B.Pfeiffer

The AME2012 atomic mass evaluation (II). Tables, graphs and references

COMPILATION A=1-295; compiled, evaluated atomic mass data.

2012ZU07

J.Phys.(London) G39, 124009 (2012)

K.Zuber

Double beta decay experiments

RADIOACTIVITY ⁴⁸Ca, ⁷⁶Ge, ⁸²Se, ⁹⁶Zr, ¹⁰⁰Mo, ¹¹⁰Pd, ¹¹⁶Cd, ¹²⁴Sn, ¹³⁰Te, ¹³⁶Xe, ¹⁵⁰Nd, ²³⁸U(2β^-), ¹⁵²Gd, ¹⁶⁴Er, ¹⁸⁰W, ¹⁵⁶Dy, ¹⁰⁶Cd, ⁴⁰Ca, ¹³⁸Ce, ¹⁹⁶Hg, ³⁶Ar, ¹³²Ba, ¹²⁴Xe, ⁵⁴Fe(2EC); analyzed available experimental data; deduced sensitivity.

doi: 10.1088/0954-3899/39/12/124009

2013AF01

Phys.Rev. C 88, 014320 (2013)

A.V.Afanasjev, O.Abdurazakov

Pairing and rotational properties of actinides and superheavy nuclei in covariant density functional theory

NUCLEAR STRUCTURE ^{228,230,232,234,236,238,240}Th, ^{230,232,234,236,238,240}U, ^{234,236,238,240,242,244,246}Pu, ^{240,242,244,246,248,250}Cm, ^{244,246,248,250,252,254}Cf, ^{246,248,250,252,254,256}Fm, ^{248,250,252,254,256,258}No, ^{254,256,258,260,262}Rf, ^{258,260,262,266}Sg; calculated scaling factors, moments of inertia, β₂, neutron and proton three-point indicators, moment of inertia versus rotational frequency. ^242,244Pu, ²⁴⁸Cm; calculated kinematic moment of inertia for ground state bands. ²⁴⁴Cm; calculated neutron and proton single-particle energies. ²³⁷U, ^239,243Pu, ^235,237Np, ²⁴¹Am, ^247,249Cm, ²⁴⁹Cf, ²⁵¹Md, ²⁵³No, ^234,236U, ^238,240,242Pu, ^246,248Cm, ²⁴⁸Cf, ²⁵⁰Fm, ²⁵²No; calculated kinematic moment of inertia for one-quasiparticle bands in odd-A nuclei and ground-state bands in even-A nuclei. ^236,238U, ^236,239,240Pu, ²⁴²Am; calculated kinematic moment of inertia, and quadrupole moments of superdeformed (SD) rotational bands and SD fission isomers. N=144-176, Z=102, 104, 106, 108, 110; calculated moments of inertia and β₂ parameter for superheavy nuclides. Cranked relativistic Hartree-Bogoliubov theory and Lipkin-Nogami method (CRHB+LN) with NL1 and NL3* interaction parameters of covariant density functional theory (CFDT). Comparison with experimental data.

doi: 10.1103/PhysRevC.88.014320

2013AG06

Phys.Rev. C 87, 051306 (2013)

B.K.Agrawal, J.N.De, S.K.Samaddar, G.Colo, A.Sulaksono

Constraining the density dependence of the symmetry energy from nuclear masses

NUCLEAR STRUCTURE ²⁰⁸Pb, ²³⁸U; calculated symmetry slope parameter L, neutron skin thickness for spherical and deformed nuclei, symmetry energy using a microscopic framework with different energy density functionals.

doi: 10.1103/PhysRevC.87.051306

2013BO24

Phys.Rev. C 88, 034316 (2013)

D.Bonatsos, P.E.Georgoudis, N.Minkov, D.Petrellis, C.Quesne

Bohr Hamiltonian with a deformation-dependent mass term for the Kratzer potential

NUCLEAR STRUCTURE ^{98,100,102,104}Ru, ^{102,104,106,108,110,112,114,116}Pd, ^{106,108,110,112,114,116,118,120}Cd, ^{118,120,122,124,126,128,130,132,134}Xe, ^{130,132,134,136,142}Ba, ^134,136,138Ce, ^140,148,150Nd, ^{140,142,152,154}Sm, ^{142,144,152,154,156,158,160,162}Gd, ^{154,156,158,160,162,164,166}Dy, ^{156,160,162,164,166,168,170}Er, ^{162,164,166,168,170,172,174,176,178}Yb, ^{166,168,170,172,174,176,178,180}Hf, ^{176,178,180,182,184,186}W, ^{176,178,180,184,186,188,190}Os, ^{186,188,190,192,194,196,198,200}Pt, ²²⁸Ra, ^228,230,232Th, ^{232,234,236,238}U, ^238,240,242Pu, ²⁴⁸Cm, ²⁵⁰Cf; calculated levels, J, π, ground, β and γ bands, B(E2), ratios of level energies of yrast bands and low-lying positive-parity levels. Deformation-dependent mass (DDM) Bohr Hamiltonian with Kratzer potential obtained for γ-unstable, axially symmetric prolate deformed, and triaxial nuclei. Techniques of supersymmetric quantum mechanics (SUSYQM).

doi: 10.1103/PhysRevC.88.034316

2013FR03

At.Data Nucl.Data Tables 99, 345 (2013)

C.Fry, M.Thoennessen

Discovery of actinium, thorium, protactinium, and uranium isotopes

COMPILATION ^{206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236}Ac, ^{208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238}Th, ^{212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239}Pa, ^{217,218,219,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,242}U; compiled first identification (or discovery) of isotopes.

doi: 10.1016/j.adt.2012.03.002

2013GI06

Phys.Rev. C 88, 054325 (2013)

S.A.Giuliani, L.M.Robledo

Fission properties of the Barcelona-Catania-Paris-Madrid energy density functional

RADIOACTIVITY ^{226,228,230,232,234,236,238,240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272,274,276,278,280,282}U, ^{238,240,242,244}Pu, ^{240,242,244,246,248}Cm, ^250,252Cf, ^{250,252,254,256}Fm, ^252,254,256No, ^256,258,260Rf, ^258,260,262Sg, ²⁶⁴Hs, ²⁸⁶Fl(SF); calculated SF half-lives, fission barrier height parameters and excitation energies of fission isomers, Z, N and A of emitted fragments, HFB energies as a function of the quadrupole moment Q₂₀. Barcelona-Catania-Paris-Madrid (BCPM) energy density functional with mean-field techniques. Comparison with experimental data.

doi: 10.1103/PhysRevC.88.054325

2013JO05

Phys.Rev. C 88, 034306 (2013)

R.V.Jolos, P.von Brentano, R.F.Casten

Anharmonicity of the excited octupole band in actinides using supersymmetric quantum mechanics

NUCLEAR STRUCTURE ²³²Th, ²³⁸U, ²⁴⁰Pu; calculated levels, J, π of ground-state, octupole and alternating parity bands. E1 and E2 transition matrix elements. Supersymmetric quantum mechanical techniques. Comparison with experimental data.

doi: 10.1103/PhysRevC.88.034306

2013LI30

Phys.Rev. C 87, 067304 (2013)

H.L.Liu, F.R.Xu

Enhanced octupole correlation due to unpaired nucleons in actinide K-isomeric states

NUCLEAR STRUCTURE ^{230,232,234,236,238,240,242}Th, ^{232,234,236,238,240,242,244}U, ^{234,236,238,240,242,244,246}Pu, ^{236,238,240,242,244,246,248}Cm; calculated 2-qp high-K levels, J, π, deformation parameters β₂, β₃, β₄. ²³²Th, ²³⁴U, ^236,238,240Pu; calculated potential-energy-surface in (β₂, β₃) plane. Configuration-constrained calculations with reflection asymmetry. Enhanced octupole correlations. K-isomers in actinides. Comparison with experimental data.

doi: 10.1103/PhysRevC.87.067304

2013NI02

Phys.Rev. C 87, 024310 (2013)

D.Ni, Z.Ren, T.Dong, Y.Qian

Nuclear charge radii of heavy and superheavy nuclei from the experimental α-decay energies and half-lives

NUCLEAR STRUCTURE ¹⁴⁰Ce, ^142,144Nd, ^144,146,148Sm, ¹⁴⁶Gd, ^148,150,152Dy, ^150,152,154Er, ^{152,154,156,158}Yb, ¹⁸²W, ^184,186Os, ^{178,180,182,184}Pt, ^{182,184,186,188,190,206}Hg, ^{190,192,194,196,198,200,202,204,206,208,210,212,214}Pb, ^{200,202,204,206,208,210}Po, ^{202,204,206,208,210,212,218,220,222}Rn, ^{208,210,212,214,220,222,224,226,228}Ra, ^228,230,232Th, ^234,236,238U, ^{238,240,242,244}Pu, ^{242,244,246,248}Cm, ^{242,244,246,248,250,252}Cf, ^248,250,252Fm, ^252,254No, ²⁵⁶Rf, ^{260,262,264,266}Sg, ²⁶⁶Hs, ^282,284Cn, ^286,288Fl, ²⁹⁰Lv; calculated rms charge radii, charge distribution using the generalized density dependent cluster model (GDDCM). A formula derived from Wentzel-Kramers-Brillouin (WKB) barrier penetration probability is proposed to calculate nuclear charge radii from the experimental α-decay energies and half-lives. Comparison with experimental data.

doi: 10.1103/PhysRevC.87.024310

2013RA05

J.Phys.(London) G40, 035104 (2013)

N.S.Rajeswari, M.Balasubramaniam

Nuclear surface energy coefficients in α-decay

RADIOACTIVITY ^{178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210}Pb, ^{188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218}Po, ^{198,200,202,204,206,208,210,212,214,216,218,220,222}Rn, ^{202,204,206,208,210,212,214,216,218,220,222,224,226}Ra, ^{210,212,214,216,218,220,222,224,226,228,230,232}Th, ^{220,222,224,226,228,230,232,234,236,238}U, ^{228,230,232,234,236,238,240,242,244}Pu, ^{240,242,244,246,248,250}Cm, ^{240,242,244,246,248,250,252,254}Cf, ^{246,248,250,252,254,256}Fm, ^{250,252,254,256}No(α); calculated T_1/2. Modified unified fission model approach, comparison with experimental data.

doi: 10.1088/0954-3899/40/3/035104

2013SE17

J.Phys.(London) G40, 105102 (2013)

W.M.Seif

The α decay spectroscopic factor of heavy and superheavy nuclei

RADIOACTIVITY ¹⁴⁴Nd, ^146,148Sm, ^148,150,152Gd, ^150,152,154Dy, ^152,154,156Er, ^154,156,158Yb, ^{156,158,160,162}Hf, ^{158,160,162,164,166,168}W, ^{162,164,166,168,170,172,174}Os, ¹⁸⁶Os, ^{166,168,170,172,174,176,178,180,182,184,186,188,190}Pt, ^{172,174,176,178,180,182,184,186,188}Hg, ^{178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210}Pb, ^{188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218}Po, ^{196,198,200,202,204,206,208,210,212,214,216,218,220,222}Rn, ^{202,204,206,208,210,212,214,216,218,220,222,224,226}Ra, ^{210,212,214,216,218,220,222,224,226,228,230,232}Th, ^{218,220,222,224,226,228,230,232,234,236,238}U, ^{238,240,242,244}Pu, ^{238,240,242,244,246,248,250}Cm, ^{240,242,244,246,248,250,252,254}Cf, ^{246,248,250,252,254,256}Fm, ^{252,254,256,258}No, ^256,258,260Rf, ²⁶⁰Sg, ²⁶⁶Sg, ^{264,266,268,270}Hs, ²⁷⁰Ds, ^286,288Fl, ^290,292Lv, ²⁹⁴Og(α); calculated T_1/2, spectroscopic factor. Comparison with experimental data.

doi: 10.1088/0954-3899/40/10/105102

2013ST19

Phys.Rev. C 88, 037303 (2013)

S.Stoica, M.Mirea

New calculations for phase space factors involved in double-β decay

RADIOACTIVITY ⁴⁸Ca, ⁷⁶Ge, ⁸²Se, ⁹⁶Zr, ¹⁰⁰Mo, ¹¹⁰Pd, ¹¹⁶Cd, ^128,130Te, ¹³⁶Xe, ¹⁵⁰Nd, ²³⁸U(2β^-); calculated phase space factors (PSF) for ββ transitions to ground states and excited 0+ states. Numerical solution of Dirac equation including the finite nuclear size and electron screening effects. Comparison with other theoretical calculations using different approximations, and discussed possible causes of differences.

doi: 10.1103/PhysRevC.88.037303

2013TA07

Eur.Phys.J. A 49, 6 (2013)

O.A.P.Tavares, E.L.Medeiros

A calculation method to estimate partial half-lives for exotic radioactivities

RADIOACTIVITY ^222,223Fr, ²²⁵Ra, ²²⁷Ac, ²²⁴Th(¹⁴C);²²⁴Ac, ²²⁵Pa(¹⁵N);^226,227Th(¹⁸O);²²⁹Th(²⁰O);²³²Th(²⁶Ne);^233,235U, ^235,236Np(²⁸Mg);²³⁵U(²⁹Mg);²³⁸U, ^239,240Pu, ^241,243Am, ²⁴⁰Cm(³⁴Si);²³⁷Np(³⁰Mg);²³⁷Np, ²⁴¹Am, ²⁴⁰Cm(³²Si); calculated T_1/2 using semi-empirical model; deduced model parameters. Compared with other calculations.

doi: 10.1140/epja/i2013-13006-y

2013TO12

Phys.Atomic Nuclei 76, 708 (2013); Yad.Fiz. 76, 758 (2013)

S.V.Tolokonnikov, Yu.S.Lutostansky, E.E.Saperstein

Self-consistent calculations of alpha-decay energies

NUCLEAR STRUCTURE ^{200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236}Th, ^{208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244}U, ^{222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248}Pu, ²⁹⁴Og, ^293,294Ts, ²⁹¹Lv; calculated α-decay energies, mass excess. Self-consistent theory of finite Fermi systems, comparison with available data.

doi: 10.1134/S1063778813060136

2013ZO02

J.Phys.(London) G40, 075101 (2013)

M.Zouioueche, A.Bouldjedri

A proton-neutron nuclear vibron model

NUCLEAR STRUCTURE ^234,236,238U; calculated energy levels, J, π. The SU(3) limit of the nuclear vibron model of Daley and Iachello.

doi: 10.1088/0954-3899/40/7/075101

2014LU01

Phys.Rev. C 89, 014323 (2014)

B.-N.Lu, J.Zhao, E.-G.Zhao, S.-G.Zhou

Multidimensionally-constrained relativistic mean-field models and potential-energy surfaces of actinide nuclei

NUCLEAR STRUCTURE ²⁴⁰Pu; calculated potential energy curves as function of deformation and truncations, three-dimensional potential energy surface contours as function of deformation around the ground state, the inner barrier, and fission isomer. ^230,232Th, ^{232,234,236,238,240}U, ^{238,240,242,244,246}Pu, ^{242,244,246,248,250}Cm, ^250,252Cf; calculated potential energy curves around the ground states and the first and second fission barriers, heights of the first second fission barriers. Multidimensionally-constrained relativistic mean-field (MDC-RMF) models, with the solution of Dirac equation in an axially deformed harmonic oscillator (ADHO) basis. Importance of nonaxial and spatial reflection asymmetric shapes in the study of potential energy surfaces and fission barriers of actinides and Superheavy nuclei. Comparison with available experimental data.

doi: 10.1103/PhysRevC.89.014323

2014NE03

Phys.Scr. 89, 054004 (2014)

B.Nerlo-Pomorska, K.Pomorski, P.Quentin, J.Bartel

Rotational bands in well deformed heavy nuclei

NUCLEAR STRUCTURE ^230,232Th, ^234,236,238U, ^240,242Pu, ²⁴⁶Cm, ²⁵²No; calculated energy levels, J, π, rotational bands. Comparison with experimental data.

doi: 10.1088/0031-8949/89/5/054004

2014VI01

Eur.Phys.J. A 50, 27 (2014)

X.Vinas, M.Centelles, X.Roca-Maza, M.Warda

Density dependence of the symmetry energy from neutron skin thickness in finite nuclei

COMPILATION ⁴⁰Ca, ^54,56,57Fe, ⁵⁹Co, ^58,60,64Ni, ^90,96Zr, ^106,116Cd, ^116,120,124Sn, ^{124,126,128,130}Te, ²⁰⁸Pb, ²⁰⁹Bi, ²³²Th, ²³⁸U; compiled, calculated neutron skin thickness vs symmetry energy slope parameter. ²⁰⁸Pb; compiled calculations of mean-field model of parity-violating asymmetry vs skin thickness vs symmetry energy ope parameter and vs central radius, surface difuseness vs central radii.

doi: 10.1140/epja/i2014-14027-8