References quoted in the ENSDF dataset: 235U ADOPTED LEVELS, GAMMAS

110 references found.

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

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1939NI03

Phys.Rev. 55, 150 (1939)

A.O.Nier

The Isotopic Constitution of Uranium and the Half-Lives of the Uranium Isotopes. I

doi: 10.1103/PhysRev.55.150

1950KN17

K-663 (1950)

G.B.Knight

Specific Alpha Activity of U-235

1951SA30

Compt.Rend. 232, 2091 (1951)

G.J.Sayag

Mesure du Rapport des Activites de U²³⁵ et U²³⁴ dans l'Uranium Naturel a l'Aide d'Une Chambre d'Ionisation a Grille

1952FL20

Phys.Rev. 88, 642 (1952)

E.H.Fleming, Jr., A.Ghiorso, B.B.Cunningham

The Specific Alpha Activity and Half-Lives of U²³⁴, U²³⁵, and U²³⁶

doi: 10.1103/PhysRev.88.642

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

1955VA07

J.Opt.Soc.Am. 45, 65 (1955)

K.L.Vander Sluis, J.R.McNally, Jr.

Nuclear Spin of Uranium-235

1956HU26

Phys.Rev. 102, 292 (1956)

C.A.Hutchison, Jr., P.M.Llewellyn, E.Wong, P.Dorain

Paramagnetic Resonance Absorption in Uranium (III) Chloride and the Nuclear Spin of Uranium-235

doi: 10.1103/PhysRev.102.292

1956KA53

Optika i Spektroskopiya 1, 809 (1956); AEC-tr-2890; Nucl.Sci.Abstr. 11, 700, Abstr. 6512 (1957)

N.I.Kaliteevskii, M.P.Chaika

The Ratios of the Magnetic Spin and Quadrupole Moments of the Nuclei U²³³ and U²³⁵

1957BL66

J.Phys.Radium 18, 318 (1957)

J.Blaise, S.Gerstenkorn, M.Louvegnies

Spin of ²³⁵U and Ratios of the Nuclear Moments of ²³⁵U and ²³³U

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

1957NE07

Nuclear Phys. 3, 345 (1957)

J.O.Newton

The Coulomb Excitation of U²³⁵, Pu²³⁹, and U²³⁸

doi: 10.1016/0029-5582(57)90030-5

1957WU39

Helv.Phys.Acta 30, 157 (1957)

E.Wurger, K.P.Meyer, P.Huber

Lebensdauer und Zerfallschema von U²³⁵

1958DA21

Physica 24, S69 (1958)

J.W.T.Dabbs, L.D.Roberts, G.W.Parker

Alpha-Particle and Fission Anisotropies from Oriented Actinide Nuclei

doi: 10.1016/S0031-8914(58)80503-0

1965DE06

Nucl.Sci.Eng. 21, 325 (1965)

A.J.Deruytter, I.G.Schroder, J.A.Moore

Measurement of the Half-Life of U²³⁵ for Alpha Emission

NUCLEAR STRUCTURE ²³⁵U; measured not abstracted; deduced nuclear properties.

1965WH05

J.Nucl.Energy A/B19, 33 (1965)

P.H.White, G.J.Wall, F.R.Pontet

A Remeasurement of the Half-Life of ²³⁵U

NUCLEAR STRUCTURE ²³⁵U; measured not abstracted; deduced nuclear properties.

1966AL23

At.Energ. 20, 315 (1966); Sov.At.Energy 20, 352 (1966)

B.M.Aleksandrov, A.S.Krivokhatskii, L.Z.Malkin, K.A.Petrzhak

Determination of the Probabilities of Spontaneous Fission in U²³³, U²³⁵, and Am²⁴³

RADIOACTIVITY, Fission ^233,235U(SF), ²⁴³Am(SF); measured T_1/2 for spontaneous fission.

1966BA58

J.Geophys.Res. 71, 4037 (1966)

P.O.Banks, L.T.Silver

Evaluation for the Decay Constant of Uranium 235 from Lead Isotope Ratios

COMPILATION ^206,207Pb, ^235,238U;compiled experimental data.

RADIOACTIVITY ²³⁵U(α); analyzed available data, ²⁰⁷Pb/²⁰⁶Pb and ²⁰⁶Pb/²³⁸U ratios; deduced decay constant and its uncertainty. Comparison with available data.

doi: 10.1029/JZ071i016p04037

1966MA20

Phys.Rev. 148, 1161 (1966)

H.Mazaki, S.Shimizu

Effect of Chemical State on the Decay Constant of U²³⁵m

NUCLEAR STRUCTURE ²³⁵U; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.148.1161

1968NE04

Phys.Letters 26B, 615 (1968)

M.Neve de Mevergnies

Effect of Environment on the Half-Life of U-235m

NUCLEAR STRUCTURE ²³⁵U; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(68)90432-2

1970HO02

Nucl.Phys. A141, 249 (1970)

M.Hojeberg, S.G.Malmskog

Transition Probabilities in the 1/2⁺ (631) Band in ²³⁵U

RADIOACTIVITY ²³⁹Pu [enriched to 94.4%]; measured αce-delay. ²³⁵U levels deduced T_1/2, quadrupole moment , gK, gR, B(E2), B(M1).

doi: 10.1016/0375-9474(70)90845-6

1970TOZZ

Thesis, Univ.Amsterdam (1970)

H.Ton

Lifetimes of Excited States in Heavy Nuclei

RADIOACTIVITY ²¹²Bi, ²²⁸Th, ²³²U, ^238,240Pu, ^242,244Cm, ²⁴³Am, ²⁵²Cf; measured αce-delay. ²²⁴Ra, ²²⁸Th, ^234,236U, ^238,240Pu, ²³⁹Np, ²⁴⁸Cm levels deduced T_1/2, B(E2), quadrupole moment. ²³³U, ²³⁹Pu; measured αce-delay. ²²⁹Th, ²³⁵U levels deduced T_1/2, gK, gR. ^198mTl; measured ceγ-delay. ^196mIr; measured ceγ-, βγ-delay. ^194mIr; measured ceγ-, βγ-, γγ-delay. ^200mAu; measured γγ-, ceγ-delay. ^194,196Pt, ^198,200Hg levels deduced T_1/2, B(EL).

1971AR48

Nucl.Data Sheets B6, 287 (1971)

A.Artna-Cohen

Nuclear Data Sheets for A = 235

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

1972NE12

Phys.Rev.Lett. 29, 1188 (1972)

M.Neve de Mevergnies

Perturbation of the ^235mU Decay Rate by Implantation in Transition Metals

RADIOACTIVITY ^235mU; measured decay constant, T_1/2 in transition metals.

doi: 10.1103/PhysRevLett.29.1188

1972RI08

Phys.Rev. C5, 2072 (1972)

F.A.Rickey, E.T.Jurney, H.C.Britt

Level Scheme of ²³⁵U and the Distribution of Single-Particle Strength in its Excited States

NUCLEAR REACTIONS ²³⁴U(n, γ), E=thermal; measured Eγ, Iγ; deduced Q. ²³⁴U(d, p), E=20 MeV; measured σ(Ep, θ). ²³³U(t, p), E=20 MeV; measured σ(Ep). ²³⁵U(d, d'), E=20 MeV; measured σ(Ed'). ²³⁶U(d, t), E=20 MeV; measured σ(Et). ²³⁵U deduced levels, J, π, L.

doi: 10.1103/PhysRevC.5.2072

1974DE19

Phys.Rev. C10, 383 (1974)

A.J.Deruytter, G.Wegener-Penning

Redetermination of the Half-Life of ²³⁵U for α Emission

RADIOACTIVITY ²³⁵U; measured Eα, Iα; deduced α-branching, T_1/2.

doi: 10.1103/PhysRevC.10.383

1974GRZA

Proc.Symp.Phys.Chem.of Fission, 3rd, Rochester, N.Y. (1973), Int.At.En.Agency, Vienna, Vol.1, p.305 (1974)

A.Grutter, H.R.von Gunten, V.Herrnberger, B.Hahn, U.Moser, H.W.Reist, G.Sletten

Spontaneous-Fission Decay of ²³⁵U

RADIOACTIVITY, Fission ²³⁵U(SF); measured decay constant. Spinner detector technique.

NUCLEAR STRUCTURE ^166,168,170Yb; calculated backbending.

1974JA17

Phys.Rev. C10, 386 (1974)

A.H.Jaffey

Redetermination of the Half-Life of ²³⁵U for α Emission: A Reply

RADIOACTIVITY ²³⁵U; measured T_1/2.

doi: 10.1103/PhysRevC.10.386

1974NE09

Phys.Lett. 49B, 428 (1974)

M.Neve de Mevergnies, P.Del Marmol

Effect of the Oxidation State on the Half-Life of ²³⁵U-m

RADIOACTIVITY ^235mU; measured chemical effects on T_1/2.

doi: 10.1016/0370-2693(74)90626-1

1979IZ02

Phys.Lett. 88B, 59 (1979)

Y.Izawa, C.Yamanaka

Production of ²³⁵U-m by Nuclear Excitation by Electron Transition in A Laser Produced Uranium Plasma

NUCLEAR REACTIONS ²³⁵U(γ, γ), E ≈ 70 eV [from laser excitation of U atom]; measured Iγ(t). ²³⁵U level deduced T_1/2.

doi: 10.1016/0370-2693(79)90113-8

1979ZH05

Pisma Zh.Eksp.Teor.Fiz. 30, 549 (1979); JETP Lett. (USSR) 30, 516 (1979)

V.I.Zhudov, A.G.Zelenkov, V.M.Kulakov, V.I.Mostovoi, B.V.Odinov

Differential Spectrum of the Conversion Electrons and the Excitation Energy of(1/2⁺)-Uranium-235 Isomer

RADIOACTIVITY ^235mU [from ²³⁹Pu α-decay]; measured E(ce), I(ce). ²³⁵U transition deduced energy. Comparison of conversion, x-ray electron spectra.

1981VO02

Phys.Rev. C23, 1110 (1981)

H.R.von Gunten, A.Grutter, H.W.Reist, M.Baggenstos

Ground-State Spontaneous-Fission Half-Lives of Uranium Isotopes

RADIOACTIVITY, Fission ^{233,234,235,236}U(SF); measured T_1/2. ^233,235U deduced hindrance factor. Enriched solutions of Uranium, spinner detectors.

doi: 10.1103/PhysRevC.23.1110

1983NI08

Phys.Rev.Lett. 51, 1749 (1983)

U.Nielsen, O.Poulsen, P.Thorsen, H.Crosswhite

Collinear Laser-rf Double-Resonance Spectroscopy: ²³⁵U II hyperfine structure

NUCLEAR MOMENTS ²³⁵U; measured hfs; deduced 7s electron spin density parameter. ²³⁵U level deduced μ. Combined laser-rf double resonance, fast beam collinear laser spectroscopy techniques.

doi: 10.1103/PhysRevLett.51.1749

1984ZU02

Phys.Rev.Lett. 53, 1888 (1984)

J.D.Zumbro, E.B.Shera, Y.Tanaka, C.E.Bemis, Jr., R.A.Naumann, M.V.Hoehn, W.Reuter, R.M.Steffen

E2 and E4 Deformations in ^{233,234,235,238}U

NUCLEAR MOMENTS ^{233,234,235,238}U; measured muonic X-rays. ^234,238U deduced intrinsic quadrupole, hexadecapole moments, charge distribution parameters, rms radii. ^233,235U deduced intrinsic quadrupole, hexadecapole moments, charge distribution parameters, B(E2).

ATOMIC PHYSICS, Mesic-Atoms ^{233,234,235,238}U; measured muonic X-rays.

doi: 10.1103/PhysRevLett.53.1888

1989KO52

Izv.Akad.Nauk SSSR, Ser.Fiz. 53, 2085 (1989); Bull.Acad.Sci.USSR, Phys.Ser. 53, No.11, 21 (1989)

V.V.Koltsov, A.A.Rimsky-Korsakov

Influence of Conducting Surroundings on the Decay of the Isomer ^235mU

RADIOACTIVITY ^235mU; measured T_1/2; deduced dependence on source surroundings. Source inside, at surface of metallic silver.

1989TR11

Z.Phys. A333, 349 (1989)

S.P.Tretyakova, Yu.S.Zamyatnin, V.N.Kovantsev, Yu.S.Korotkin, V.L.Mikheev, G.A.Timofeev

Observation of Nucleon Clusters in the Spontaneous Decay of ²³⁴U

RADIOACTIVITY ^234,236U(²⁴Ne), (²⁶Ne), (²⁸Mg), (³⁰Mg); ²³⁵U(²⁵Ne), (²⁶Ne), (²⁸Mg), (³⁰Mg); measured cluster emission probabilities relative to α-decay, T_1/2.

1990GA28

Izv.Akad.Nauk SSSR, Ser.Fiz. 54, 830 (1990); Bull.Acad.Sci.Ussr, Phys.Ser. 54, No.5, 13 (1990)

Yu.P.Gangrsky, S.G.Zemlyanoi, B.K.Kuldzhanov, K.P.Marinova, B.N.Markov

Determination of the Difference between the Charge Radii and of the Ratio of the Electromagnetic Moments of Uranium Nuclei by Resonant Laser Fluorescence

NUCLEAR MOMENTS ^{233,234,235,236,238}U; measured optical hfs, isotope shifts; deduced hyperfine constants. ^{233,234,235,236,238}U deduced rms charge radii differences, μ, quadrupole moment ratios. Resonant laser fluorescence.

1991BO20

Phys.Rev. C44, 888 (1991)

R.Bonetti, C.Chiesa, A.Guglielmetti, C.Migliorino, A.Cesana, M.Terrani, P.B.Price

Neon Radioactivity of Uranium Isotopes

RADIOACTIVITY ^234,232,235U(²⁴Ne); measured partial T_1/2; deduced branching ratio relative to α-decay.

doi: 10.1103/PhysRevC.44.888

1992AN17

Hyperfine Interactions 74, 31 (1992)

A.Anastassov, Yu.P.Gangrsky, K.P.Marinova, B.N.Markov, B.K.Kuldzhanov, S.G.Zemlyanoi

Nuclear Charge Radii Changes of Uranium and Hafnium Isotopes Determined by Laser Spectroscopy

NUCLEAR MOMENTS ^{174,176,178,180}Hf, ^{235,236,238,233,234}U; measured hfs, isotope shifts; deduced rms charge radii differences. Laser spectroscopy.

1992BO26

Phys.Rev. C46, 852 (1992)

J.A.Bounds, P.Dyer

Search for Nuclear Excitation by Laser-Driven Electron Motion

RADIOACTIVITY ^235mU(IT); measured I(ce); deduced ²³⁵U atom excitation probability upper limit. Pulsed infrared laser, high brightness UV laser beam, nuclear excitation by electron motion, channel electron multiplier detector.

doi: 10.1103/PhysRevC.46.852

1992VO05

Bull.Rus.Acad.Sci.Phys. 56, 81 (1992)

O.V.Voryhalov, E.A.Zaitsev, V.V.Koltsov, A.A.Rimsky-Korsakov

Study of Isomer Decay Inside a Conductor

RADIOACTIVITY ^235mU(IT); measured conversion electron count rate; deduced decay suppression inside dielectric. Isomer decay in conductor.

1992VS01

Yad.Fiz. 55, 304 (1992); Sov.J.Nucl.Phys. 55, 165 (1992)

M.M.Vsevolodov, V.Yu.Dobretsov, D.P.Grechukhin

Effect of Hybridization of the Electron Orbitals of Uranium Immersed in Silver on the ^235mU Conversion Rate

RADIOACTIVITY ^235mU; calculated isomer decay conversion rate; deduced hybridization effects role, immersion in Ag consequences. Cluster model, muffin-tin approximation.

1993BU10

Appl.Radiat.Isot. 44, 567 (1993)

C.C.Bueno, M.D.S.Santos

Measurement of the Absolute Activity of ²³⁵U by the Generalized Coincidence Method

RADIOACTIVITY ²³⁵U(α); measured Eγ, Iγ, Eα, Iα, αγ-coin; deduced T_1/2, absolute activity.

doi: 10.1016/0969-8043(93)90171-6

1993KO32

Bull.Rus.Acad.Sci.Phys. 57, 93 (1993)

V.V.Koltsov

On a Probablity of Conversion Transition in the ^235mU Nuclei Placed in Silver

RADIOACTIVITY ^235mU(IT); analyzed T_1/2 increase, source in Ag; deduced possible transition stimulation by electromagnetic field zeroth oscillations.

1995PA45

Bull.Rus.Acad.Sci.Phys. 59, 834 (1995)

A.D.Panov

Zeno's Quantum Paradox and Decay of the ^235mU Isomer in Matter

RADIOACTIVITY ^235mU(IT); analyzed decay constant, source implanted in metallic host; deduced evidence for phenomena akin to Zeno's quantum paradox.

1996PAZY

Program and Thesis, Proc.46th Ann.Conf.Nucl.Spectrosc.Struct.At.Nuclei, Moscow, p.340 (1996)

A.D.Panov

Statistical Modeling of the Secondary Electron Emission in Decay of Ultrasoft Isomer of ²³⁵U and New Determination of the Isomer Transition Energy

RADIOACTIVITY ^235mU(IT); measured E(ce), I(ce); deduced isomer Eγ.

1997BE64

Nucl.Phys. A626, 357c (1997)

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

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

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

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

1997ER02

Yad.Fiz. 60, No 2, 206 (1997); Phys.Atomic Nuclei 60, 149 (1997)

D.O.Eremenko, V.O.Kordyukevich, S.Yu.Platonov, A.F.Tulinov, O.V.Fotina, O.A.Yuminov

Lifetime of Excited ^234,235U Nuclei Produced in the Reaction ²³²Th(α, xnf)

NUCLEAR REACTIONS ²³²Th(α, F)²³⁴U/²³⁵U, E=20-31.2 MeV; measured residuals excited states T_1/2. ²³⁴U deduced level density, fission barrier. Blocking technique.

1997KA11

Yad.Fiz. 60, No 1, 16 (1997); Phys.Atomic Nuclei 60, 12 (1997)

S.G.Kadmensky, V.I.Furman, Yu.M.Tchuvilsky

Structure Effects in Cluster Decays of Odd Nuclei

RADIOACTIVITY ^221,223Fr, ²²³Ra, ^223,225Ac, ²²⁹Th(¹⁴C), ²²⁹Th, ²³¹Pa, ^233,235U(²⁴Ne), (²⁶Ne), (²⁸Mg), ²³⁷Np(³⁰Mg), ²⁴¹Am(³⁴Si); calculated quasifavored, semifavored, nondiagonal cluster transitions prohibition factors.

1997MIZP

Proc.Intern.on Nuclear Data for Science and Technology, Trieste, Italy, 19-24 May, 1997, G.Reffo, A.Ventura, C.Grandi, Eds., Editrice Compositori, Italy, Pt.1, p.826 (1997)

V.L.Mikheev, S.P.Tretyakova

Experimental Data on the Cluster Decay of Heavy Nuclei and the Correlations between the Probabilities of Alpha Decay, Cluster Decay and Spontaneous Fission

RADIOACTIVITY ²²¹Fr, ^{221,222,223,224,226}Ra, ²²⁵Ac(¹⁴C); ²²⁸Th(²⁰O); ²³⁰Th, ²³¹Pa, ^{232,233,234,235,236}U(²⁴Ne); ²³²Th, ^233,235,236U(²⁶Ne); ²³¹Pa(²³F); ²³⁰U(²²Ne); ^232,234,235U, ^236,238,239Pu(²⁸Mg); ²³⁵U(²⁵Ne); ²³⁶U, ²³⁷Np, ²³⁸Pu(³⁰Mg); ²³⁸Pu(³²Si); ²⁴⁰Pu, ²⁴¹Am, ²⁴²Cm(³⁴Si); ¹¹⁴Ba(¹²C); compiled, analyzed cluster decay data; deduced correlation with α-decay, SF-decay probabilities.

1997RO24

Nuovo Cim. 110A, 1061 (1997)

G.Royer

Nuclear Clusters in Exit and Entrance Channels

RADIOACTIVITY ^{222,223,224,226}Ra(¹⁴C); ²²⁸Th(²⁰O); ²³⁰Th, ²³¹Pa, ^232,233,234U(²⁴Ne); ^234,235U, ^236,238Pu(²⁸Mg); ²³⁸Pu(³²Si); calculated T_1/2, barrier, tunneling features. Generalized liquid drop model.

1997TR17

Nuovo Cim. 110A, 1043 (1997)

S.P.Tretyakova, V.L.Mikheev

Experimental Investigation of the Cluster Radioactivity of Atomic Nuclei

RADIOACTIVITY ²²¹Fr, ^{221,222,223,224}Ra, ²²⁵Ac(¹⁴C); ²²⁸Th(²⁰O); ²³⁰Th, ²³¹Pa, ^{232,233,234,235,236}U(²⁴Ne); ²³²Th, ^234,235,236U(²⁶Ne); ²³¹Pa(²³F); ²³⁰U(²²Ne); ^{232,233,234,235}U, ^236,238,239Pu(²⁸Mg); ^233,235U(²⁵Ne); ²³⁶U, ²³⁷Np, ²³⁸Pu(³⁰Mg); ²³⁸Pu(³²Si); ²⁴⁰Pu, ²⁴¹Am, ²⁴²Cm(³⁴Si); ¹¹⁴Ba(¹²C); compiled, analyzed cluster decay data.

1998EL02

Phys.Rev. C57, 583 (1998)

S.R.Elliott, P.Beiersdorfer, M.H.Chen, V.Decaux, D.A.Knapp

Measurements of the Differences in the Nuclear Charge Radii Among Uranium Isotopes

NUCLEAR MOMENTS ^233,235U; measured isotope shifts; deduced relative nuclear charge radii. X-ray spectroscopy, high-energy electron beam ion trap, highly-charged ions. Results for other uranium isotopes compared.

doi: 10.1103/PhysRevC.57.583

1998RO11

Nucl.Phys. A632, 275 (1998)

G.Royer, R.K.Gupta, V.Yu.Denisov

Cluster Radioactivity and Very Asymmetric Fission Through Compact and Creviced Shapes

RADIOACTIVITY ^{222,223,224,226}Ra(¹⁴C), ²²⁸Th(²⁰O), ²³⁰Th, ²³¹Pa, ^232,233,234U(²⁴Ne), ^234,235U, ^236,238Pu(²⁸Mg), ²³⁸Pu(³²Si); calculated cluster decay potential barriers, deformation energy, Q-values, T_1/2. Liquid drop model.

NUCLEAR STRUCTURE ^{222,223,224,226}Ra, ^228,230Th, ²³¹Pa, ^{232,233,234,235}U, ^236,238Pu; calculated cluster decay potential barriers, deformation energy, Q-values, T_1/2. Liquid drop model.

doi: 10.1016/S0375-9474(97)00801-4

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.

2000SI04

Phys.Rev. C61, 034612 (2000)

S.Sinha, R.Varma, R.K.Choudhury, B.K.Nayak, A.Saxena, R.G.Thomas, B.V.Dinesh

Measurement of Quasielastic and Transfer Excitation Functions in ¹⁶O, ¹⁹F + ²³²Th Reactions

NUCLEAR REACTIONS ²³²Th(¹⁶O, X), (¹⁶O, ¹⁴N), (¹⁶O, ¹⁵N), (¹⁶O, ¹²C), (¹⁶O, ¹³C), (¹⁶O, ¹⁴C), E=73-99 MeV; ²³²Th(¹⁹F, X), (¹⁹F, ¹⁶O), (¹⁹F, ¹⁷O), (¹⁹F, ¹⁸O), (¹⁹F, ¹⁴N), (¹⁹F, ¹⁵N), (¹⁹F, ¹⁶N), (¹⁹F, ¹²C), (¹⁹F, ¹³C), (¹⁹F, ¹⁴C), (¹⁹F, ¹⁵C), E=83-109 MeV; measured quasielastic and transfer excitation functions; deduced fusion barrier distributions, transfer probabilities. Comparison with semiclassical model.

doi: 10.1103/PhysRevC.61.034612

2004BA64

Phys.Rev. C 70, 017301 (2004)

M.Balasubramaniam, S.Kumarasamy, N.Arunachalam, R.K.Gupta

New semiempirical formula for exotic cluster decay

RADIOACTIVITY ²²¹Fr, ^{221,222,223,224,226}Ra, ²²⁵Ac(¹⁴C); ²²⁸Th(²⁰O); ²³⁰U(²²Ne); ²³¹Pa(²³F); ²³⁰Th, ²³¹Pa, ^{232,233,234,235}U(²⁴Ne); ^233,235U(²⁵Ne); ²³⁴U(²⁶Ne); ^234,236U, ^236,238Pu(²⁸Mg); ²³⁶U, ²³⁸Pu(³⁰Mg); ²³⁸Pu(³²Si); ^{177,178,179,180,181,182,183,184,185,186,187}Hg(⁸Be), (¹²C), (¹⁶O); calculated cluster decay T_1/2. Semiempirical formula, comparison with data.

doi: 10.1103/PhysRevC.70.017301

2004DU20

Nucl.Sci.Eng. 148, 30 (2004)

M.E.Dunn, L.C.Leal

Calculating Probability Tables for the Unresolved-Resonance Region Using Monte Carlo Methods

NUCLEAR REACTIONS ²³⁵U(n, X), (n, γ), (n, F), (n, n'), E=2.25-25.0 keV; calculated average σ in unresolved-resonance region. Monte-Carlo approach.

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

2005BH02

Phys.Rev. C 71, 017301 (2005)

A.Bhagwat, Y.K.Gambhir

Relativistic mean field description of cluster radioactivity

NUCLEAR STRUCTURE ²²¹Fr, ^{221,222,223,224}Ra, ²²⁵Ac, ^{226,228,230,232}Th, ²³¹Pa, ^{230,232,233,234,235,236}U, ²³⁷Np, ^236,238,240Pu, ²⁴²Am, ²⁴²Cm; calculated charge radii. ^{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}Ra; calculated isotope shifts. Comparison with data.

RADIOACTIVITY ^224,226,228Th, ²²¹Ra, ²²¹Fr, ²²³Ra, ²²⁵Ac(¹⁴C); ²³¹Pa, ^{232,233,234,235}U, ^230,232Th(²⁴Mg); ^233,234U, ^236,237Np(²⁸Mg); ²³⁶U, ^237,238Np(³⁰Mg); ²⁴⁰Np, ²⁴²Cm, ²⁴¹Am(³⁴Si); ²³⁸Pu(³²Si); ²³¹Pa(²³F); ²²⁶Th(¹⁸O); ^233,235U(²⁵Ne); ²²⁸Th(²⁰O); calculated cluster decay T_1/2, Q-values. Relativistic mean field approach, comparisons with data.

doi: 10.1103/PhysRevC.71.017301

2005HA23

Nucl.Sci.Eng. 150, 170 (2005)

Y.Han

Calculation and Analysis of n + ^{233, 235, 237}U Reactions

NUCLEAR REACTIONS ^233,235,237U(n, X), (n, n), (n, γ), (n, 2n), (n, 3n), E ≤ 20 MeV; calculated total, elastic, inelastic, capture σ. ^233,235,237U(n, n), (n, n'), E ≤ 20 MeV; calculated σ(E, θ). ^233,235,237U(n, F), E ≤ 20 MeV; calculated fission σ, prompt neutron spectra. Optical model, Hauser-Feshbach theory, exciton model, comparisons with data.

2005KO18

Nucl.Instrum.Methods Phys.Res. B235, 76 (2005)

Y.S.Kozhedub, V.M.Shabaev

Electric quadrupole moment of a hydrogen-like ion in s and p_1/2 states

ATOMIC PHYSICS ¹H, ¹³C, ¹⁷O, ⁴³Ca, ¹³¹Xe, ²⁰⁷Pb, ²⁰⁹Bi, ²³⁵U; calculated hfs, induced quadrupole moments in hydrogen-like ions.

NUCLEAR MOMENTS ¹H, ¹³C, ¹⁷O, ⁴³Ca, ¹³¹Xe, ²⁰⁷Pb, ²⁰⁹Bi, ²³⁵U; calculated hfs, induced quadrupole moments in hydrogen-like ions.

doi: 10.1016/j.nimb.2005.03.149

2005KU04

Phys.Rev. C 71, 014301 (2005)

S.N.Kuklin, G.G.Adamian, N.V.Antonenko

Spectroscopic factors and cluster decay half-lives of heavy nuclei

RADIOACTIVITY ^{112,114,116,118}Ba, ¹¹⁸Ce, ¹²²Nd, ^124,126Sm, ²²⁰Ra(¹²C), (¹⁶O); ¹²²Nd(²⁰Ne), (²⁴Mg); ¹²⁶Sm(²⁴Mg), (²⁸Si); ²²¹Fr(¹⁴C); ^221,222,223Ra(¹⁴C), (¹⁵N), (¹⁸O); ^224,226Ra(¹⁴C), (²⁰O), (²⁴Ne); ²²⁵Ac(¹⁴C), (¹⁷N), (¹⁸O), (²³F), (²⁴Ne), (²⁷Na), (²⁸Mg); ²²⁴Th(¹⁴C), (¹⁵N), (¹⁶O), (²¹F), (²⁴Ne), (²⁸Mg), (²⁹Al), (³²Si); ²²⁶Th(¹⁴C), (¹⁵N), (¹⁸O), (²¹F), (²⁴Ne), (²⁷Na), (²⁸Mg), (³²Si); ²²⁸Th(¹⁴C), (²⁰O), (²³F), (²⁴Ne), (²⁸Mg); ²²⁹Th(¹⁴C), (¹⁶N), (²¹O), (²³F), (²⁴Ne), (²⁸Mg); ²³⁰Th(²⁴Ne); ²³¹Pa(²²O), (²³F), (²⁴Ne), (²⁷Na), (²⁸Mg), (³¹Al); ²³²Pa(²⁵Ne), (²⁷Na), (²⁸Mg); ²³⁰U(¹⁴C), (²⁰O), (²⁴Ne), (²⁷Na), (²⁸Mg), (³²Si); ²³²U(²³F), (²⁴Ne), (²⁷Na), (²⁸Mg), (³²Si); ²³³U(²⁵Ne), (²⁷Na), (²⁸Mg); ²³⁴U(²⁶Ne), (²⁷Na), (²⁸Mg); ²³⁵U(²⁶Ne), (²⁹Mg); ²³⁶U(³⁰Mg); ^234,236Pu(²⁴Ne), (²⁷Na), (²⁸Mg), (²⁹Al), (³²Si); ²³⁷Pu(²⁹Mg), (³⁰Al), (³²Si); ²³⁸Pu(³⁰Mg), (³¹Al), (³²Si); ²⁴²Cm(³⁴Si); calculated cluster decay T_1/2, Q-values.

doi: 10.1103/PhysRevC.71.014301

2005KU32

Yad.Fiz. 68, 1501 (2005); Phys.Atomic Nuclei 68, 1443 (2005)

S.N.Kuklin, G.G.Adamian, N.V.Antonenko

Spectroscopic Factors and Barrier Penetrabilities in Cluster Radioactivity

RADIOACTIVITY ^{112,114,116,118}Ba, ¹¹⁸Ce, ¹²²Nd, ^124,126Sm, ²²⁰Ra(¹²C), (¹⁶O); ¹²²Nd(²⁰Ne), (²⁴Mg); ¹²⁶Sm(²⁴Mg), (²⁸Si); ²²¹Fr(¹⁴C); ^221,222,223Ra(¹⁴C), (¹⁵N), (¹⁸O); ^224,226Ra(¹⁴C), (²⁰O), (²⁴Ne); ²²⁵Ac(¹⁴C), (¹⁷N), (¹⁸O), (²³F), (²⁴Ne), (²⁷Na), (²⁸Mg); ²²⁴Th(¹⁴C), (¹⁵N), (¹⁶O), (²¹F), (²⁴Ne), (²⁸Mg), (²⁹Al), (³²Si); ²²⁶Th(¹⁴C), (¹⁵N), (¹⁸O), (²¹F), (²⁴Ne), (²⁷Na), (²⁸Mg), (³²Si); ²²⁸Th(¹⁴C), (²⁰O), (²³F), (²⁴Ne), (²⁸Mg); ²²⁹Th(¹⁴C), (¹⁶N), (²¹O), (²³F), (²⁴Ne), (²⁸Mg); ²³⁰Th(²⁴Ne); ²³¹Pa(²²O), (²³F), (²⁴Ne), (²⁷Na), (²⁸Mg), (³¹Al); ²³²Pa(²⁵Ne), (²⁷Na), (²⁸Mg); ²³⁰U(¹⁴C), (²⁰O), (²⁴Ne), (²⁷Na), (²⁸Mg), (³²Si); ²³²U(²³F), (²⁴Ne), (²⁷Na), (²⁸Mg), (³²Si); ²³³U(²⁵Ne), (²⁷Na), (²⁸Mg); ²³⁴U(²⁶Ne), (²⁷Na), (²⁸Mg); ²³⁵U(²⁶Ne), (²⁹Mg); ²³⁶U(³⁰Mg); ^234,236Pu(²⁴Ne), (²⁷Na), (²⁸Mg), (²⁹Al), (³²Si); ²³⁷Pu(²⁹Mg), (³⁰Al), (³²Si); ²³⁸Pu(³⁰Mg), (³¹Al), (³²Si); ²⁴²Cm(³⁴Si); calculated cluster decay T_1/2, Q-values, spectroscopic factors, penetrabilities. Dinuclear system approach.

doi: 10.1134/1.2053330

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

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

2006SA35

J.Phys.(London) G32, 2157 (2006)

O.S.K.S.Sastri, R.K.Jain, P.C.Sood

Intrinsically forbidden "allowed" beta transitions in actinides

NUCLEAR STRUCTURE ^228,230,231Th, ^{228,230,231,232,233}Pa, ^{230,231,232,233,235}U, ^{235,238,239,240}Np, ^238,239,240Pu, ^239,240Am, ²⁵⁰Bk, ²⁵⁰Cf, ²⁵⁴Es, ²⁵⁴Fm; analyzed β-decay data; deduced hindrance mechanism.

doi: 10.1088/0954-3899/32/11/009

2007OB02

Phys.Rev.Lett. 99, 042502 (2007)

A.Oberstedt, S.Oberstedt, M.Gawrys, N.Kornilov

Identification of a Shape Isomer in ²³⁵U

NUCLEAR REACTIONS ²³⁴U(n, γ)²³⁵U, E=0.95, 1.27 MeV; measured delayed fission fragment spectra from the decay of the shape isomer, isomeric fission T_1/2 and cross section.

doi: 10.1103/PhysRevLett.99.042502

2007RO08

J.Radioanal.Nucl.Chem. 272, 237 (2007)

G.Royer, C.Bonilla

Multiple-humped fission and fusion barriers of actinide and superheavy elements

NUCLEAR REACTIONS ¹³²Sn(⁹⁹Zr, X), (¹⁰¹Zr, X), (¹⁰⁴Mo, X), (¹⁰⁵Mo, X), (¹⁰⁶Mo, X), (¹¹¹Ru, X), (¹¹²Rh, X), ¹³⁴Te(⁹⁸Zr, X), ¹³¹Sn(¹⁰³Mo, X), (¹⁰⁴Mo, X), (¹¹⁰Ru, X), (¹¹¹Ru, X), ¹³⁰Sn(¹⁰⁹Ru, X), (¹¹⁰Ru, X), (¹¹³Pd, X), (¹¹⁵Pd, X), (¹¹⁸Pd, X), (¹²⁰Ag, X), ¹²⁵In(¹²⁵In, X), ¹²⁸Sn, ¹²⁷Sb(¹²⁸In, X), E not given; calculated potential barrier parameters.

RADIOACTIVITY ^{232,234,235,236,238}U, ^238,239,240Pu, ²⁴³Am, ^243,245,248Cm, ²⁵⁰Cf, ²⁵⁵Es, ²⁵⁶Fm, ²⁵⁶No(SF); calculated T_1/2. ^{284,285,286,287,288,289,290,291,292}Fl, ^{285,286,287,288,289,290,291,292,293}Mc, ^{287,288,289,290,291,292,293,294,295}Lv, ^{290,291,292,293,294,295,296,297,298}Ts, ^{292,293,294,295,296,297,298,299,300}Og, ^{295,296,297,298,299,300,301,302,303}120(α); calculated T_1/2, Qα.

doi: 10.1007/s10967-007-0507-4

2008HUZW

Triangle Univ.Nuclear Lab., Ann.Rept., p.84 (2007-08); TUNL-XLVII (2008)

A.Hutcheson, C.T.Angell, M.Boswell, A.S.crowell, J.H.Esterline, B.Fallin, C.R.Howell, J.H.Kelley, H.J.Karwowski, M.R.Kiser, A.P.Tonchev, W.Tornow, J.A.Becker, D.Dashdorj, R.A.Macri, R.O.Nelson

Neutron-Induced Partial γ-Ray Cross-Section Measurements on ^235-238U

NUCLEAR REACTIONS ^235,238U(n, n'γ), ^235,238U(n, 2nγ), E=5-14MeV; measured Eγ, Iγ using clover and planar HPGe; deduced excitation function.compared with Hauser-Feshbach model (codes GNASH and TALYS).

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

2008WE01

Geochim.Cosmochim.Act. 72, 345 (2008)

S.Weyer, A.D.Anbar, A.Gerdes, G.W.Gordon, T.J.Algeo, E.A.Boyle

Natural fractionation of ²³⁸U/²³⁵U

RADIOACTIVITY ^238,235U(α); measured isotopic ratios in natural samples.

doi: 10.1016/j.gca.2007.11.012

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

2009CH24

Nucl.Instrum.Methods Phys.Res. B267, 1882 (2009)

Y.-S.Cho, Y.-O.Lee, G.Kim

A new approach for cross section evaluations in the high energy region

NUCLEAR REACTIONS ²³⁵U(n, x), (n, n), (n, F), (n, γ), (n, 2n), (n, 3n), E=reactor spectrum, fast; Calculated σ. Optical model, TALYS and KALMAN codes.

doi: 10.1016/j.nimb.2009.03.109

2009DO16

Eur.Phys.J. A 41, 197 (2009)

J.M.Dong, H.F.Zhang, J.Q.Li, W.Scheid

Cluster preformation in heavy nuclei and radioactivity half-lives

RADIOACTIVITY ²²⁶Th(¹⁴C), ²²⁶Th(¹⁸O), ²³⁰U(²²Ne), (²⁴Ne), ²³²Th(²⁴Ne), (²⁶Ne), ²³⁶U(²⁶Ne), ²³²U, ²³³U, ²³⁵U(²⁸Mg), ²³⁷Np(³⁰Mg), ²⁴⁰Pu, ²⁴¹Am(³⁴Si); calculated T_1/2 for cluster decay using unified fission model; deduced cluster preformation factors. Comparison with data. A=114-124(¹²C), (¹⁶O); A=215-252(⁸Be), (¹²C), (¹⁴C), (¹⁵N), (¹⁶O), (¹⁷O), (¹⁸O), (²⁰O), (²²O), (²²Ne), (²⁴Ne), (²⁵Ne), (²⁶Ne), (²³F), (²⁸Mg), (²⁹Mg), (³⁰Mg), (³²Si), (³³Si), (³⁴Si), (³⁶S), (³⁸S), (⁴²S), (⁴⁶Ar), (⁴⁸Ca), (⁵⁰Ca); calculated T_1/2 for cluster decay using unified fission model.

doi: 10.1140/epja/i2009-10819-1

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

2009MU14

Phys.Rev. C 80, 034612 (2009); Publishers Note Phys.Rev. C 82, 029904 (2010)

D.Mulhall

Using the Δ₃ statistics to test for missed levels in mixed sequence neutron resonance data

NUCLEAR REACTIONS ^50,58Cr, ^58,60Ni, ¹⁰³Rh, ¹⁴⁷Sm, ¹⁶⁷Er, ¹⁸⁵Re, ¹⁹⁷Au, ^235,238U, ²⁴¹Pu(n, n)(n, γ), E not given; analyzed neutron resonance data using random matrix theory (RMT) and Δ₃ statistics to detect missing levels.

doi: 10.1103/PhysRevC.80.034612

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

2010NI02

Phys.Rev. C 81, 024315 (2010)

D.Ni, Z.Ren

Systematic calculation of α decay within a generalized density-dependent cluster model

RADIOACTIVITY ²²⁹Th, ^225,227Pa, ^{225,229,233,235}U, ^235,237Np, ^237,239,241Pu, ^{239,240,241,242,243}Am, ^{241,242,243,245,247}Cm, ^245,247,249Bk, ^{245,247,249,253}Cf, ^{245,247,249,251,253,255}Es, ^251,255,257Fm(α); Z=52-104, N=84-156(α); Z=52, N=54-58(α); Z=91-100, N=133-157(α); calculated half-lives and branching ratios for even-even, odd-A and odd-odd α emitters using generalized density-dependent cluster model. Comparison with experimental data.

doi: 10.1103/PhysRevC.81.024315

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

2010QU01

Int.J.Mod.Phys. E19, 611 (2010)

P.Quentin, L.Bonneau, N.Minkov, D.Samsoen

Odd nuclei, time-reversal symmetry breaking, and magnetic polarization of the even-even core

NUCLEAR STRUCTURE ^48,49Cr, ⁴⁹Mn, ^98,99Sr, ⁹⁹Y, ^102,103Mo, ¹⁰³Tc, ^174,175Yb, ¹⁷⁵Lu, ^178,179Hf, ¹⁷⁹Ta, ^234,235U, ²³⁵Np; calculated spin operators and quenching factors, core polarization of magnetic moments. Skyrme force parameterization.

doi: 10.1142/S0218301310015023

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

2011BE53

Pure Appl.Chem. 83, 397 (2011)

M.Berglund, M.E.Wieser

Isotopic compositions of the elements 2009

COMPILATION Z=1-92; compiled isotopic abundance data.

doi: 10.1351/PAC-REP-10-06-02

2011BU11

J.Korean Phys.Soc. 59, 1892s (2011)

J.T.Burke, J.J.Ressler, J.E.Escher, N.D.Scielzo, I.J.Thompson, R.Henderson, J.Gostic, L.Bernstein, D.Bluel, M.Weideking, V.Meot, O.Roig, L.W.Phair, R.Hatarik, J.Munson, C.Angell, B.Goldblum, C.W.Beausang, T.Ross, R.Hughes, M.Aiche, G.Barreau, N.Cappelan, S.Czajkowski, B.Hass, B.Jurado, L.Mathieu, I.Companis

Experimental Approaches to Studying the Fission Process Using the Surrogate Reaction Technique

NUCLEAR REACTIONS ^235,236U, ²³⁹Pu(α, α'), E=55 MeV; measured E(charged particle), I(charged particle), Eγ, Iγ(θ), γγ-coin, fission products using STARS (Silicon Telescope Array for Reaction Studies), LIBERACE, HYDRA; deduced σ ²³⁸Pu(n, F) below 20 MeV using surrogate reactions. Comparison with other data.

doi: 10.3938/jkps.59.1892

2011HU06

Phys.Rev. C 84, 024617 (2011); Erratum Phys.Rev. C 85, 029901 (2012)

P.Huber

Determination of antineutrino spectra from nuclear reactors

RADIOACTIVITY ²³⁵U, ^239,241Pu(SF); analyzed antineutrino spectra and fluxes created from the inverse of previously measured total β spectra and synthetic β spectra from the decays of fission fragments; estimated and evaluated associated theory errors due to induced currents like weak magnetism. Effect of higher-order corrections to the allowed β spectrum. Estimated errors due to the effects of incomplete and inaccurate nuclear structure data.

doi: 10.1103/PhysRevC.84.024617

2011MU06

Phys.Rev. C 83, 054321 (2011)

D.Mulhall

Maximum likelihood method to correct for missed levels based on the Δ₃(L) statistic

NUCLEAR STRUCTURE ⁵⁸Ni, ¹⁵²Sm, ¹⁵⁸Gd, ^234,235,236U; analyzed number of observed neutron resonances by a maximum likelihood method; deduced missed levels and limitation of Δ₃(L) statistics. Estimate of the incompleteness of experimental spectra.

doi: 10.1103/PhysRevC.83.054321

2011MU07

Phys.Rev. C 83, 054615 (2011)

Th.A.Mueller, D.Lhuillier, M.Fallot, A.Letourneau, S.Cormon, M.Fechner, L.Giot, T.Lasserre, J.Martino, G.Mention, A.Porta, F.Yermia

Improved predictions of reactor antineutrino spectra

RADIOACTIVITY ^235,238U, ²³⁹Pu, ²⁴¹Pu(SF); calculated reactor antineutrino spectra in 2-8 MeV range, ab initio total β spectra using all available data on fission yields and β decays of fission products. Total error budget estimates in the antineutrino spectra emitted by the fission of ²³⁵U, ²³⁹Pu and ²⁴¹Pu. relevance to the surveillance of power plants in the context of nonproliferation of nuclear weapons.

doi: 10.1103/PhysRevC.83.054615

2011SH13

J.Phys.(London) G38, 055103 (2011)

Z.-q.Sheng, D.-d.Ni, Z.-z.Ren

Systematic calculations on cluster radioactivity half-lives

RADIOACTIVITY ^{112,113,114,115,116,117}Cs, ^{114,115,116,117,118,119,120}Ba, ^{117,118,119,120,121,122}La, ¹²⁰Ce, ²¹⁹Fr, ^219,220,227Ra, ^{219,220,221,222,228}Ac, ^{220,221,221,222,223}Th, ^{221,223,231,232,233,234}Pa, ^{222,223,224,225,226}U, ^{225,226,227,228}Np, ^228,229,230Pu(¹²C), ^{114,115,116,117,118,119}Ba, ^{117,118,119,120,122}La, ^{119,120,121,122,123,124}Ce, ^{121,122,123,124,125,126}Pr, ^124,125,126Nd, ^224,225Th, ^{224,225,226,227}U, ^{225,226,227,228,229}Np, ^228,229,230Pu(¹⁶O), ¹²⁶Pm(²⁴Mg), ²²⁰Fr, ²²⁴Pa(¹³C), ²²⁷Th, ^227,228Pa, ²²⁸U(¹⁸O), ^227,228Ac(²⁰O), ^229,230Ac(²²O), ^232,233,234Pu, ^233,234,235Am(²⁶Mg), ²³⁶Am, ^233,235Pu(²⁷Mg), ²³⁷Pu(²⁹Mg), ^{128,129,130,131,132}Sm, ^{130,131,132,133,134,135}Eu, ^134,135Gd, ^136,137Tb, ¹³⁸Dy(²⁸Si), ¹³¹Sm(²⁹Si), ¹³²Eu, ¹³⁵Gd(²⁹Si), ¹³⁶Tb, ¹³⁸Dy, ^140,141Ho(³²S), ¹⁴³Er(³⁶Ar), ²³⁹Pu, ^239,241Cm(³³Si), ²²⁵Ac, ^{221,222,223,224,226}Ra, ²²⁶Th, ^{220,222,224,226,223,225}Fr, ^220,228Ra, ^{221,222,224,226,227}Ac, ^{224,225,227,223}Th, ^{225,226,227,228}Pa, ^227,228U(¹⁴C), ²²⁶Th(¹⁸O), ^228,229Th(²⁰O), ^229,231Pa(²³F), ^229,230U, ^230,231Np, ^231,232Pu(²²Ne), ²³¹U(²³Ne), ²²⁹Ac, ^{230,231,232,233}Pa, ^{229,230,231,232}Th, ^{230,231,232,233,234,235,236}U, ^231,232,233Np(²⁴Ne), ²³⁴Pa, ²³⁵U(²⁵Ne), ²³²Th, ²³⁶U(²⁶Ne), ¹²⁷Pm(²⁴Mg), ^{232,233,234,235}U, ^234,235,236Np, ^{234,235,236,237,238}Pu, ²³⁵Am(²⁸Mg), ²³⁵U, ²³⁵Np(²⁹Mg), ^236,238Pu, ²³⁷Np(³⁰Mg), ²³⁸Pu, ^236,238Am(³²Si), ²³⁸Np, ^{239,240,241,242}Am, ^{238,239,240,241,242,243}Cm, ^240,241Bk(³⁴Si); calculated T_1/2.

doi: 10.1088/0954-3899/38/5/055103

2011STZZ

INDC(NDS)-0594 (2011)

N.J.Stone

Table of nuclear magnetic dipole and electric quadrupole moments

COMPILATION Z=1-99, N=1-254; compiled experimental data on nuclear magnetic and electrical quadrupole moments.

2012BA35

J.Phys.(London) G39, 095103 (2012)

X.J.Bao, H.F.Zhang, B.S.Hu, G.Royer, J.Q.Li

Half-lives of cluster radioactivity with a generalized liquid-drop model

RADIOACTIVITY ²²¹Fr, ^{221,222,223,224,226}Ra, ²²⁵Ac, ²²⁶Th(¹⁴C), ²²⁶Th(¹⁸O), ²²⁸Th(²⁰O), ²³⁰Th(²⁴Ne), ²³²Th(²⁶Ne), ²³¹Pa(²⁴Ne), (²³F), ²³⁰U(²²Ne), (²⁴Ne), ²³²U(²⁸Mg), (²⁴Ne), ²³³U(²⁴Ne), (²⁵Ne), (²⁸Mg), ²³⁴U(²⁴Ne), (²⁶Ne), (²⁸Mg), ²³⁵U(²⁴Ne), (²⁵Ne), (²⁸Mg), ²³⁶U, ²⁴⁷Np(³⁰Mg), ²³⁶Pu(²⁸Mg), ²³⁸Pu(²⁸Mg), (³⁰Mg), (³²Si), ²²⁰Rn(¹²C), ²²¹Rn(¹⁵N), ²²²Rn(¹⁸O), ²²³Ra(¹⁸O), ²²⁶Ra(²⁰O), ²²⁵Ac(¹⁸O), ²²⁴Th(¹⁵N), ²²⁴Th(²⁴Ne), ²²⁶Th(¹⁵N), ^226,228Th(²⁴Ne), ²²⁹Th(²¹O), (²⁴Ne), ²³¹Pa(²⁷Na), ²³²Pa(²⁵Ne), (²⁸Mg), ²³⁰U(²⁰O), (²⁴Ne), (³²Si), ²³²U(²⁸Mg), ^233,234U(²⁷Na), ²²⁵Np(¹²C), (¹⁶O), ²²⁷Np(¹⁶O), (¹⁸O), ²³¹Np(²⁰O), ²³³Np(²²Ne), (²⁵Ne), ²³⁴Np(²⁸Mg), ²³⁵Np(²⁹Mg), ²³⁶Np(²⁹Mg), ²³⁷Np(³²Si), ²³⁴Pu(²⁷Na), (²⁹Al), ²³⁶Pu(²⁴Ne), (²⁹Al), ²³⁷Pu(²⁹Mg), (³²Si), ²³⁷Am(²⁸Mg), (³²Si), ²³⁸Am(²⁹Mg), (³³Si), ²³⁹Am(³²Si), (³⁴Si), ²⁴⁰Am(³⁴Si), ²⁴¹Am(³⁴Si), ²³⁸Cm(³²Si), ²⁴⁰Cm(³⁰Mg), (³⁴Si), ²⁴²Cm(³²Si), ²⁴³Cm(³⁴Si), ²⁴²Cf(³²Si), (³⁴Si), ²⁴⁴Cf(³⁴Si), ²⁴⁶Cf(³⁸S), ²⁴⁹Cf(⁴⁶Ar), (⁵⁰Ca), ^{250,252,253,254,255,256,257,258}No(⁴⁸Ca), ²⁵⁸Rf(⁴⁹Ca), (⁵¹Ti), (⁵³Ti); calculated T_1/2 for cluster radioactivity. WKB barrier-penetrating probabilities, generalized liquid drop model, comparison with available data.

doi: 10.1088/0954-3899/39/9/095103

2012BR11

Phys.Rev. C 86, 014617 (2012)

P.A.Bradley, G.P.Grim, A.C.Hayes, Gerard Jungman, R.S.Rundberg, J.B.Wilhelmy, G.M.Hale, R.C.Korzekwa

Neutron reactions in the hohlraum at the LLNL National Ignition Facility

NUCLEAR REACTIONS ¹⁹⁷Au, ²³⁸U(n, γ), ¹⁹⁷Au(n, n')^197mAu, ¹⁹⁷Au, ²³⁸U(n, 2n), (n, 3n), (n, 4n), ²³⁸U(n, F), E=0-30 MeV; analyzed techniques to measure neutron yields and neutron fluence spectra from (d, t) reaction at the LLNL National Ignition Facility for deuterium-tritium (DT) inertial confinement fusion. Neutron diagnostics and dosimetry.

doi: 10.1103/PhysRevC.86.014617

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

2012HA06

Phys.Rev. C 85, 024617 (2012)

A.C.Hayes, H.R.Trellue, M.M.Nieto, W.B.Wilson

Antineutrino monitoring of burning mixed oxide plutonium fuels

RADIOACTIVITY ^235,238U, ^239,241Pu(SF); analyzed fission fraction, effective antineutrino detection cross section, and antineutrino signal as function of burn-up of LEU and MOX reactor and weapon grade fuels using Monteburns (MCNP+CINDER90) code. Relevance to nuclear accountability.

doi: 10.1103/PhysRevC.85.024617

2012HU01

Phys.Rev. C 85, 024613 (2012)

R.O.Hughes, C.W.Beausang, T.J.Ross, J.T.Burke, N.D.Scielzo, M.S.Basunia, C.M.Campbell, R.J.Casperson, H.L.Crawford, J.E.Escher, J.Munson, L.W.Phair, J.J.Ressler

Utilizing (p, d) and (p, t) reactions to obtain (n, f) cross sections in uranium nuclei via the surrogate-ratio method

NUCLEAR REACTIONS ^236,238U(p, d), (p, t), E=28 MeV; measured E(d), I(d), E(t), I(t), fission spectra, (particle)(fission)-, (particle)γ-coin, fission fragment anisotropy ratios using STARS detector array at LBNL cyclotron facility; deduced σ[²³⁶U(n, F)]/σ[²³⁴U(n, F)], σ[²³⁵U(n, F)]/σ[²³³U(n, F)], σ[²³⁴U(n, F)]/σ[²³³U(n, F)], σ[²³⁶U(n, F)]/σ[²³⁵U(n, F)] reaction cross section ratios for E(n)=0-7 MeV. Surrogate-ratio method. Comparison with ENDF/B-VII evaluation.

doi: 10.1103/PhysRevC.85.024613

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

2012LEZZ

Proc.3rd International Workshop on Compound-Nuclear Reactions and Related Topics, Prague, Czech Republic, September 19-23, 2011, M.Krticka, F.Becvar, J.Kroll, Eds.p.03003 (2012)

L.S.Leong, L.Tassan-Got, L.Audouin, C.Paradela, J.N.Wilson, D.Tarrio, B.Berthier, I.Duran, C.Le Naour, M.O.Sornein, C.Stephan

Criticality experiments for validation of cross sections: the ²³⁷Np case

NUCLEAR REACTIONS ²³⁵U, ²³⁷Np(n, n'), (n, f), E=0-4 MeV; re-analyzed fission σ, inelastic σ ENDF/B-7.0, ENDF/B-6.8 and critical ²³⁷Np benchmark data. ²³⁷Np deduced criticity k_eff.

doi: 10.1051/epjconf/20122103003

2012PA40

Phys.Rev. C 86, 064601 (2012)

S.Panebianco, J.-L.Sida, H.Goutte, J.-F.Lemaitre, N.Dubray, S.Hilaire

Role of deformed shell effects on the mass asymmetry in nuclear fission of mercury isotopes

RADIOACTIVITY ^180,198Hg, ²³⁵U(SF); calculated minimum absolute available energy at scission for all possible fragmentations, symmetric and asymmetric fission. Microscopic scission-point model.

doi: 10.1103/PhysRevC.86.064601

2012PRZZ

Astrophysics, InTech, I.Kucuk Ed., p.21 (2012)

B.Pritychenko

Stellar Nucleosynthesis Nuclear Data Mining

NUCLEAR REACTIONS ⁹⁶Mo, ¹⁰⁰Ru, ¹⁰⁴Pd, ¹¹⁰Cd, ¹¹⁶Sn, ^122,123,124Te, ^128,130Xe, ^134,136Ba, ¹⁴²Nd, ^148,150Sm, ¹⁵⁴Gd, ¹⁶⁰Dy, ¹⁷⁶Hf, ¹⁹⁸Hg, ²⁰⁴Pb(n, γ), E=30 keV; calculated Maxwellian-averaged σ and their uncertainties. JENDL-4, ROSFOND 2010, ENDF/B-VII.1, KADONIS libraries, ENDF/B-VII.1 and Low-Fidelity covariances, s-process.

NUCLEAR REACTIONS ²³²Th, ^235,238U, ²³⁷Np, ²³⁹Pu, ²⁴¹Am, ²⁵⁰Cm, ²⁵⁰Bk, ²⁵²Cf, ²⁵⁵Es, ²⁵⁵Fm(n, F), E=400 keV; calculated Maxwellian-averaged σ. ENDF/B-VII.1 evaluated nuclear library, r-process data.

RADIOACTIVITY ²³²Th, ^235,238U, ²³⁷Np, ²³⁹Pu, ²⁴¹Am, ²⁵⁰Cm, ²⁵⁰Bk, ²⁵²Cf, ²⁵⁵Es, ²⁵⁵Fm(α), (SF), (β^-); analyzed T_1/2 decay data for r-process.

COMPILATION ^{127,128,129,130}Ag, ^130,131,132Cd, ^{131,132,133,134,135}In, ^{130,131,132,133,134,135,136,138,139,140}Sn, ^{136,137,138,139}Sb, ^137,138,139Te; compiled evaluated nuclear structure r-process data.

doi: 10.5772/2091

2012QI02

Nucl.Instrum.Methods Phys.Res. A665, 70 (2012)

Y.Qiao, J.Wu, Y.Yang, M.Zhang, S.Liu

Determination of ²³⁵U isotope abundance by measuring selected pairs of fission products

NUCLEAR REACTIONS U(n, F)⁹²Sr/¹⁰⁵Ru/¹³⁵I, E=14 MeV; measured fission fragments, Eγ, Iγ. ²³⁵U; deduced isotopic abundance.

doi: 10.1016/j.nima.2011.10.020

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

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.

2013HE11

Ann.Nucl.Energy 57, 230 (2013)

A.Hernandez-Solis, C.Demaziere, C.Ekberg

Uncertainty and sensitivity analyses applied to the DRAGONv4.05 code lattice calculations and based on JENDL-4 data

NUCLEAR REACTIONS ¹H, ¹⁶O, ⁵⁶Fe, ^235,238U(n, n), (n, γ), ^235,238U(n, n'), (n, F), E<20 MeV; calculated JENDL-4.0 covariances. Comparison with available data.

doi: 10.1016/j.anucene.2013.01.061

2013KA26

Phys.Atomic Nuclei 76, 423 (2013); Yad.Fiz. 76, 462 (2013)

S.G.Kadmensky, L.V.Titova

P-Odd, P-Even, and T-Odd Asymmetries in True Quaternary Fission of Nuclei

RADIOACTIVITY ²³⁵U(SF); calculated parameters for quaternary fission. Comparison with available data.

doi: 10.1134/S1063778813030095

2013KE02

Phys.Rev. C 87, 024609 (2013)

M.Kerveno, J.C.Thiry, A.Bacquias, C.Borcea, P.Dessagne, J.C.Drohe, S.Goriely, S.Hilaire, E.Jericha, H.Karam, A.Negret, A.Pavlik, A.J.M.Plompen, P.Romain, C.Rouki, G.Rudolf, M.Stanoiu

Measurement of ²³⁵U(n, n'γ) and ²³⁵U(n, 2nγ) reaction cross sections

NUCLEAR REACTIONS ²³⁵U(n, n'), (n, 2n), E=0-20 MeV; measured Eγ, Iγ, σ(E), TOF, prompt gamma-ray spectroscopy at GELINA facility in Geel. Activation method. Comparison with calculations using TALYS-1.2 computer code.

doi: 10.1103/PhysRevC.87.024609

2013MA15

Nucl.Data Sheets 114, 397 (2013)

A.MacDonald, B.Karamy, K.Setoodehnia, B.Singh

Compilation of directly measured nuclear spins of ground states and long-lived isomers

COMPILATION Z=0-99; compiled evaluated nuclear structure data, J, π.

doi: 10.1016/j.nds.2013.03.002

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

2013ZD01

Phys.Rev. C 87, 024308 (2013)

A.Zdeb, M.Warda, K.Pomorski

Half-lives for α and cluster radioactivity within a Gamow-like model

RADIOACTIVITY ^{188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,206,208,209,210,211,212,213,214,215,216,217,218}Po, ^{193,194,195,196,197,198,199,200,201,202,203,204,205,207,209,211,212,213,214,215,216,217,218,219,220}At, ^{195,196,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222}Rn, ^{200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221}Fr, ^{202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,226}Ra, ^{206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225}Ac, ^{209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,232}Th, ^{212,213,214,215,216,217,218,219,220,221,223,224,225,226,227,231}Pa, ^{217,218,219,223,225,226,227,228,229,230,232,233,234,235,236,238}U, ^{226,227,229,230,231,237}Np, ^{229,230,232,234,236,237,238,239,240,242,244}Pu, ^241,243Am, ^{234,238,240,242,243,244,245,246,247,248}Cm, ²⁴⁷Bk, ^{240,242,243,244,245,246,248,249,250,251,252}Cf, ^{243,245,247,252,253,254}Es, ^{243,246,247,248,250,251,252,253,254,255,256,257}Fm, ^{246,248,249,255,256,257,258}Md, ^{252,253,254,255,256,257,259}No, ^{253,255,257,258}Lr, ^{255,257,259,261}Rf, ^{257,259,260,262}Db, ^260,265Sg, ^261,262Bh, ^265,266Hs, ²⁶⁶Mt, ^{269,270,271,273,281}Ds(α); ²²¹Fr, ^{221,222,223,224,226}Ra, ^223,225Ac(¹⁴C); ²²³Ac(¹⁵N), ²²⁶Th(¹⁸O); ²²⁸Th(²⁰O); ²³⁰U(²²Ne); ²³¹Pa(²³F); ^230,232Th, ²³¹Pa, ^{232,233,234,235,236}U(²⁴Ne); ^233,235U(²⁵Ne); ²³²Th, ^234,236U(²⁶Ne); ^233,234,236U, ^236,238Pu(²⁸Mg); ²³⁶U, ²³⁷Np, ²³⁸Pu(³⁰Mg); ²³⁸Pu(³²Si); ²⁴⁰Pu, ²⁴¹Am, ²⁴²Cm(³⁴Si); calculated T_1/2 for α decay and cluster emissions. Phenomenological model based on Gamow theory with WKB approximation for the penetration of Coulomb barrier. Comparison with experimental values of half-lives.

doi: 10.1103/PhysRevC.87.024308

2013ZD02

Phys.Scr. T154, 014029 (2013)

A.Zdeb, M.Warda, K.Pomorski

Half-lives for α and cluster radioactivity in a simple model

RADIOACTIVITY ²²¹Fr, ^{221,222,223,224,226}Ra, ²²⁵Ac(¹⁴C), ²²⁶Th(¹⁸O), ²²⁸Th(²⁰O), ²³⁰Th(²⁴Ne), ²³⁰U(²²Ne), ²³¹Pa(²³F), (²⁴Ne), ²³²Th(²⁴Ne), (²⁵Ne), ²³²U(²⁴Ne), ²³³U(²⁴Ne), (²⁵Ne), (²⁸Mg), ²³⁴U(²⁴Ne), (²⁵Ne), (²⁸Mg), ²³⁵U(²⁴Ne), (²⁵Ne), ²³⁶U(²⁴Ne), (²⁵Ne), (²⁸Mg), (³⁰Mg), ²³⁶Pu(²⁸Mg), ²³⁷Np(³⁰Mg), ²³⁸Pu(²⁸Mg), (³⁰Mg), (³²Si), ²⁴⁰Pu(³⁴Si), ²⁴¹Am(³⁴Si), ²⁴²Cm(³⁴Si); calculated cluster radioactivity T_1/2. Simple phenomenological model based on the WKB theory, comparison with available data.

doi: 10.1088/0031-8949/2013/T154/014029

Note: Additional references listed in dataset: 2008KIAA,. See dataset contents for details.