References quoted in the ENSDF dataset: 149ND ADOPTED LEVELS, GAMMAS
120 references found.
Clicking on a keynumber will list datasets that reference the given article.
Phys.Rev. 53, 437 (1938)
M.L.Pool, L.L.Quill
Radioactivity Induced in the Rare Earth Elements by Fast Neutrons
Z.Naturforsch. 1, 179 (1946)
W.Bothe
Die Aktivierung der Seltenen Erden durch thermische Neutronen II
Phys.Rev. 76, 300 (1949)
D.C.Hess, M.G.Inghram
Slow Neutron Cross Sections Of The Neodymium Isotopes
NUCLEAR REACTIONS 142Nd(n, γ), 143Nd(n, γ), 144Nd(n, γ), 145Nd(n, γ), 146Nd(n, γ), 148Nd(n, γ), 150Nd(n, γ), E=0.0253 eV; measured products, 144Nd, Eγ, Iγ; deduced σ, σ(E). Data were imported from EXFOR entry 12067.
NNES 9, paper 194 1264 (1950), Radiochemical Studies: The Fission Products, Book 2, Part V, McGraw-Hill, p.1264 (1951)
J.A.Marinsky, L.E.Glendenin
Study of Neodymium and Promethium Activities Induced by Neutron Irradiation of Neodymium
Phys.Rev. 88, 412 (1952)
H.Pomerance
Thermal Neutron Capture Cross Sections
NUCLEAR REACTIONS 24Mg(n, γ), 25Mg(n, γ), 26Mg(n, γ), 28Si(n, γ), 29Si(n, γ), 30Si(n, γ), 39K(n, γ), 40K(n, γ), 41K(n, γ), 40Ca(n, γ), 42Ca(n, γ), 46Ti(n, γ), 47Ti(n, γ), 48Ti(n, γ), 49Ti(n, γ), 50Ti(n, γ), 50Cr(n, γ), 52Cr(n, γ), 53Cr(n, γ), 54Cr(n, γ), 54Fe(n, γ), 56Fe(n, γ), 57Fe(n, γ), 58Fe(n, γ), 58Ni(n, γ), 60Ni(n, γ), 61Ni(n, γ), 62Ni(n, γ), 63Cu(n, γ), 65Cu(n, γ), 69Ga(n, γ), 71Ga(n, γ), 70Ge(n, γ), 72Ge(n, γ), 73Ge(n, γ), 74Ge(n, γ), 76Ge(n, γ), 74Se(n, γ), 76Se(n, γ), 77Se(n, γ), 78Se(n, γ), 80Se(n, γ), 82Se(n, γ), 90Zr(n, γ), 91Zr(n, γ), 92Zr(n, γ), 94Zr(n, γ), 96Zr(n, γ), 92Mo(n, γ), 95Mo(n, γ), 96Mo(n, γ), 97Mo(n, γ), 98Mo(n, γ), 100Mo(n, γ), 107Ag(n, γ), 109Ag(n, γ), 121Sb(n, γ), 123Sb(n, γ), 120Te(n, γ), 122Te(n, γ), 123Te(n, γ), 124Te(n, γ), 125Te(n, γ), 126Te(n, γ), 128Te(n, γ), 130Te(n, γ), 134Ba(n, γ), 135Ba(n, γ), 136Ba(n, γ), 137Ba(n, γ), 138Ba(n, γ), 136Ce(n, γ), 138Ce(n, γ), 140Ce(n, γ), 142Ce(n, γ), 142Nd(n, γ), 143Nd(n, γ), 144Nd(n, γ), 145Nd(n, γ), 146Nd(n, γ), 148Nd(n, γ), 150Nd(n, γ), 174Hf(n, γ), 176Hf(n, γ), 177Hf(n, γ), 178Hf(n, γ), 179Hf(n, γ), 180Hf(n, γ), 180W(n, γ), 182W(n, γ), 183W(n, γ), 184W(n, γ), 186W(n, γ), 185Re(n, γ), 187Re(n, γ), 203Tl(n, γ), 205Tl(n, γ), 204Pb(n, γ), 206Pb(n, γ), 207Pb(n, γ), 208Pb(n, γ), 232Th(n, γ), E=0.0253 eV; measured products, 25Mg, Eγ, Iγ; deduced σ, σ(E). Data were imported from EXFOR entry 11507.
Phys.Rev. 86, 775 (1952)
W.C.Rutledge, J.M.Cork, S.B.Burson
Gamma-Rays Associated with Selected Neutron-Induced Radioactivities
Phys.Rev. 91, 1423 (1953)
D.J.Hughes, R.C.Garth, J.S.Levin
Fast Neutron Cross Sections and Nuclear Level Density
NUCLEAR REACTIONS 23Na, 26Mg, 27Al, 30Si, 37Cl, 40Ar, 41K, 48Ca, 50Ti, 51V, 55Mn, 59Co, 64Ni, 63,65Cu, 68Zn, 69Ga, 74Ge, 75As, 79,81Br, 84,86Kr, 85,87Rb, 88Sr, 89Y, 93Nb, 98,100Mo, 102,104Ru, 103Rh, 108Pd, 107,109Ag, 115In, 120,122,124Sn, 121Sb, 127I, 136Xe, 138Ba, 139La, 140,142Ce, 141Pr, 146,148Nd, 175,176Lu, 181Ta, 186W, 185,187Re, 198Pt, 197Au, 204Hg, 208Pb, 209Bi(n, γ), E=fast; measured activation σ; deduced level density features.
Phys.Rev. 90, 447 (1953)
W.H.Walker, H.G.Thode
Relative Abundances And Neutron Capture Cross Sections Of The Neodymium Isotopes
NUCLEAR REACTIONS 142Nd(n, γ), 143Nd(n, γ), 144Nd(n, γ), 145Nd(n, γ), 146Nd(n, γ), 148Nd(n, γ), 150Nd(n, γ), E=0.0253 eV; measured products, 144Nd, Eγ, Iγ; deduced σ, σ(E). Data were imported from EXFOR entry 12059.
Phys.Rev. 118, 242 (1960)
R.G.Wille, R.W.Fink
Activation Cross Sections for 14.8 MeV Neutrons and Some New Radioactive Nuclides in the Rare Earth Region
NUCLEAR STRUCTURE 169Er, 168Ho, 167Ho, 167Dy, 165Dy, 165Er, 163Tb, 174Lu, 173Er, 174Tm, 176Lu, 175Yb, 176Tm, 177Yb, 152Pm, 152Eu, 153Sm, 154Pm, 150Eu, 151Nd, 149Nd, 157Sm, 159Gd, 161Gd, 133Ba, 136Cs, 140La, 140Pr, 139Ba, 139Ce, 141Ce, 135Ba, 138Cs, 137Ba, 147Nd, 145Ce, 143Sm, 148Pr, 142La, 141Nd, 142Pr, 143Ce; measured not abstracted; deduced nuclear properties.
Thesis, Univ.California (1962); UCRL-10245 (1962)
B.Budick
Investigation of Electronic and Nuclear Properties of Some Rare Earth Isotopes
NUCLEAR STRUCTURE 143Pr, 147Pm, 165Er, 149Nd, 151Pm, 161Ho; measured not abstracted; deduced nuclear properties.
Phys. Rev. 135, B1281 (1964)
B.Budick, I.Maleh, R.Marrus
Atomic-Beam Studies of Nuclear Properties of Some Rare-Earth Isotopes
NUCLEAR STRUCTURE 165Er, 171Er, 171Tm, 161Ho, 161Tb, 149Nd, 143Pr; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.135.B1281
J.Inorg.Nucl.Chem. 26, 1769 (1964)
D.C.Hoffman, W.R.Daniels
Some Short-Lived Isotopes of Cerium and Praseodymium
NUCLEAR STRUCTURE 148Ce, 148Pr, 147Pr, 147Ce, 147Nd, 146Pr, 145Pr, 149Nd, 149Pr; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(64)80001-4
Phys.Rev. 143, 923 (1966)
R.G.Helmer, L.D.McIsaac
Decay of Nd149
NUCLEAR STRUCTURE 149Nd; measured not abstracted; deduced nuclear properties.
J.Inorg.Nucl.Chem. 28, 266 (1966)
B.F.Rider, J.P.Peterson, Jr., C.P.Ruiz
The Half-Life of Nd-149
NUCLEAR STRUCTURE 149Nd; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(66)80258-0
Phys.Rev. 156, 1340 (1967)
M.P.Menon, M.Y.Cuypers
14.5-MeV Neutron Activation Cross Section for Some of the Rare-Earth Nuclides and Their Relation to the Nuclear Shell Structure
NUCLEAR REACTIONS 140Ce, 141Pr, 142,150Nd, 144Sm(n, 2n), E=14.5 MeV; measured production σ for 140Pr, 143m,143Sm, 149Nd, 141mNd, 139mCe. Activation technique, thick target. 130Te, 133Cs, 134,136,138Ba, 142,140Ce, 141Pr, 142,148,150Nd, 144,154Sm, 151,153Eu, 160Gd deduced neutron, proton binding energy ratio. Activation technique, thick target.
Yadern.Fiz. 8, 639 (1968); Soviet J.Nucl.Phys. 8, 371 (1969)
E.N.Karzhavina, N.N.Fong, A.B.Popov, A.I.Taskaev
Neutron Resonances of Nd Isotopes
NUCLEAR REACTIONS 142,143,144,145,146,148,150Nd(n, X), (n, γ), E < 10 keV; measured σ(E;Eγ), transmission. 143,144,145,146,147,149,151Nd deduced resonances, level-width, strength functions, average level spacings.
Nucl.Phys. A134, 118 (1969)
R.N.Alves, S.de Barros, P.L.Chevillon, J.Julien, J.Morgenstern, C.Samour
Determination du Spin et des Parametres des Resonances pour Cl+n, Cu+n, Ba+n et Nd+n
NUCLEAR REACTIONS Cl(n, X), E < 115 keV; Cu(n, X), E < 32 keV; Ba(n, X), E < 1300 eV; Nd(n, X), E < 740 eV; measured σ(nt)(E). 36,38Cl, 64,66Cu, 131,133,135,136,137,138Ba, 144,145,146,149,151Nd deduced resonances, resonance parameters, strength function.
doi: 10.1016/0375-9474(69)90688-5
Yadern.Fiz. 10, 929 (1969); Soviet J.Nucl.Phys. 10, 536 (1970)
Z.G.Gritchenko, T.P.Makarova, Y.T.Oganesyan, Y.E.Penionzhkevich, A.V.Stepanov
γ Radiation of Certain Rare-Earth Products of Fission of U by Heavy Ions
RADIOACTIVITY 140,141,142La, 135,137,139,141,143,144Ce, 138,139,142,143,145Pr, 139,140,147,149Nd, 144,148,149,150,151Pm, 153,156Sm, 150,155,156,157Eu, 147,149,159Gd[from 238U(HI, F), with HI = 12C, 20,22Ne, 40Ar]; measured Eγ, Iγ.
NUCLEAR REACTIONS 238U(HI, F), E=80-290 MeV with HI= 12C, 20,22Ne, 40Ar; measured Eγ, Iγ; deduced yields of several La, Ce, Pr, Nd, Pm, Sm, Eu, Gd isotopes. Ge(Li) detector.
Yadern.Fiz. 10, 460 (1969); Soviet J.Nucl.Phys. 10, 263 (1970)
O.V.Vasilev, G.N.Zalesnyi, S.F.Semenko, V.A.Semenov
Giant Resonance in the Region of Transition from Spherical Nuclei to Deformed Ones
NUCLEAR REACTIONS 148,150Nd, 150,152,154Sm(γ, n), E < 23 MeV; measured σ(E).
Phys.Letters 30B, 97 (1969)
O.V.Vasilijev, G.N.Zalesny, S.F.Semenko, V.A.Semenov
The Giant Dipole Resonance in the Transition Region from Spherical to Deformed Nuclear Shapes
NUCLEAR REACTIONS 148,150Nd, 150,152,154Sm(γ, n), (γ, X), E < 23 MeV; measured σ(E), σ(E;En); deduced giant resonance shapes, α-width.
doi: 10.1016/0370-2693(69)90407-9
Bull.Amer.Phys.Soc. 15, No.6, 769, BE9 (1970)
A.R.Pierce, R.G.Summers-Gill
Nuclear Moments of 147Nd and 149Nd
NUCLEAR MOMENTS 147,149Nd; measured a, b. Deduced μ, Q. Atomic beam magnetic resonance.
Radiokhimiya 12, 487 (1970): Sov.Radiochem. 12, 453 (191970)
N.V.Skovorodkin, A.V.Sorokina, S.S.Bugorkov, A.S.Krivokhatskii, K.A.Petrzhak
Radiochemical determination of the yields of rare-earth elements in the fission 239Pu and 241Pu by slow neutrons I: Yields of isotopes of the rare-earth elements with half-lives of more than ten days
NUCLEAR REACTIONS 239,241Pu(n, F)141La/143Ce/145Pr/149Nd/149Pm/151Pm/153Sm/156Sm/157Eu/159Gd/161Tb, E thermal; measured fission products; deduced cumulative yields relative to 144Ce.
Nucl.Phys. A172, 437 (1971)
P.Carlos, H.Beil, R.Bergere, A.Lepretre, A.Veyssiere
The Giant Dipole Resonance in the Transition Region for the Neodymium Isotopes
NUCLEAR REACTIONS 142,143,144,145,146,148,150Nd(γ, n)(γ, 2n), E=9-20 MeV; measured σ(E). 150Nd deduced thresholds, integrated σ, Lorentz line parameters, quadrupole moment. Enriched targets.
doi: 10.1016/0375-9474(71)90725-1
C.R.Acad.Sci., Ser.B 272, 695 (1971)
H.Tellier
Fonction Densite pour les Neutrons 's' et Parametre de la Densite de Niveaux des Isotopes Stables du Neodyme
NUCLEAR REACTIONS 142,143,144,145,146,148,150Nd(n, X), E < 31 keV; measured σ(nT)(E). 143,144,145,146,147,149,151Nd deduced resonances, level spacing, strength functions.
Thesis Univ.Arkansas (1972); Diss.Abst.Int. 32B, 5091 (1972)
A.Bari
14.8 Neutron Activation Cross Sections of Rubidium, Strontium, Zirconium, Niobium and Rare-Earth Nuclides
NUCLEAR REACTIONS 85Rb, 87Rb, 86Sr, 88Sr, 90Zr, 139La, 140Ce, 141Pr, 146Nd, 150Sm, 153Eu, 159Tb, 166Er, 174Yb(n, p), 90Zr, 93Nb, 139La, 142Ce, 142Nd, 150Sm, 152Sm, 154Sm, 162Dy(n, α), 85Rb, 87Rb, 84Sr, 86Sr, 88Sr, 90Zr, 93Nb, 136Ce, 138Ce, 140Ce, 142Ce, 141Pr, 142Nd, 148Nd, 150Nd, 144Sm, 154Sm, 151Eu, 153Eu, 160Gd, 156Dy, 158Dy, 162Er, 169Tm, 168Yb, 170Yb(n, 2n), E=14.8 MeV; measured activation σ.
Thesis, Univ.Arkansas (1972); Diss.Abstr.Int., 32B, 5091 (1972)
A.Bari
14.8 MeV Neutron Activation Cross Sections of Rubidium, Strontium, Zirconium, Niobium and Rare-Earth Nuclides
NUCLEAR REACTIONS 85,87Rb, 86,88Sr, 90Zr, 139La, 140Ce, 141Pr, 146Nd, 150Sm, 153Eu, 159Tb, 166Er, 174Yb(n, p), 90Zr, 93Nb, 139La, 142Ce, 142Nd, 150,152,154Sm, 162Dy(n, α), 85,87Rb, 84,86,88Sr, 90Zr, 93Nb, 136,138,140,142Ce, 141Pr, 142,148,150Nd, 144,154Sm, 151,153Eu, 160Gd, 156,158Dy, 162Er, 159Tb, 168,170Yb(n, 2n), E=14.8 MeV; measured σ(θ).
Radiochim.Acta 17, 191 (1972)
J.I.Kim, E.Gryntakis
The Thermal Neutron Cross Section and the Resonance Integral of 146Nd, 148Nd, 150Nd and 41K
NUCLEAR REACTIONS 146,148,150Nd, 41K(n, γ);E=thermal; measured Iγ, deduced σ, resonance integral.
J.Phys.(London) A5, 468 (1972)
B.V.Thirumala Rao, J.Rama Rao, E.Kondaiah
Neutron Capture Cross Sections at 25 keV
NUCLEAR REACTIONS 84Kr, 110Cd, 115In, 130Te, 146,148,150Nd, 158Gd, 160Gd(n, γ), E=25 keV; measured σ.
doi: 10.1088/0305-4470/5/3/016
Can.J.Phys. 51, 455 (1973)
D.G.Burke, J.C.Waddington, D.E.Nelson, J.Buckley
A Study of Levels in 149Nd Using the (d, t) and (3He, α) Reactions
NUCLEAR REACTIONS 150Nd(d, t), E=12 MeV; 150Nd(3He, d), E=24 MeV; measured σ(θ), Q. 149Nd deduced levels, J, π.
Can.J.Phys. 51, 1454 (1973)
M.D.Ricabarra, R.Turjanski, G.H.Ricabarra
Measurement and Evaluation of the Activation Resonance Integral of 146Nd, 148Nd, and 150Nd
NUCLEAR REACTIONS 146,148,150Nd(n, γ), E not given; measured σ. Deduced resonance integral.
Nuovo Cim. 18A, 48 (1973)
K.Siddappa, M.Sriramachandra Murty, J.Rama Rao
Neutron Activation Cross-Sections in Rare Earths and Heavier Nuclei
NUCLEAR REACTIONS 138Ba, 140,142Ce, 146,148Nd, 160Gd, 165Ho, 180Hf, 181Ta, 190Os, 197Au, 202Hg(n, γ), E=23 keV; measured σ.
Phys.Rev. C8, 1448 (1973)
P.M.Starzyk, N.Sugarman
Studies of the Recoil Properties of Products of the Interaction of 238U with 11.5-GeV Protons
RADIOACTIVITY 131,135,140La, 143Ce, 138m,145Pr, 147,149Nd, 153Sm, 147Gd, 149,151,152,153,154,156Tb, 155,157Dy, 159,160m,161,162mHo, 165Tm; measured Eγ, T1/2.
NUCLEAR REACTIONS 238U(p, X), E=11.5 GeV; measured fragment recoil ranges, charge dispersion.
Izv.Akad.Nauk SSSR, Ser.Fiz. 38, 2119 (1974); Bull.Acad.Sci.USSR, Phys.Ser. 38, No.10, 90 (1974)
L.K.Peker, V.M.Sigalov
The Alaga Model and the Structure of the Spherical States of Odd-Neutron Nuclei with A of 145-153
NUCLEAR STRUCTURE 143,145,147,149Nd, 145,147,149,151Sm levels calculated μ.
Nucl.Phys. A224, 319 (1974)
S.M.Qaim
Total (n, 2n) Cross Sections and Isomeric Cross-Section Ratios at 14.7 MeV in the Region of Rare Earths
NUCLEAR REACTIONS 136,138,140,142Ce, 142,148,150Nd, 144,154Sm, 151,153Eu, 152,154,160Gd, 159Tb, 156,158,160Dy, 165Ho, 162,164,166Er, 169Tm, 168,170,176Yb, 175Lu, 174,176Hf(n, 2n), E=14.7+-0.3 MeV; measured σ, isomeric cross-section ratios. Natural targets; Ge(Li) detector.
doi: 10.1016/0375-9474(74)90690-3
Ann.Phys.(New York) 83, 355 (1974)
K.Siddappa, M.S.Murty, J.R.Rao
Neutron Strength Functions of Nuclei in the Deformed Region
NUCLEAR REACTIONS 138Ba, 140,142Ce, 146,148Nd, 152,154Sm, 158,160Gd, 159Tb, 169Tm, 170Er, 174,176Yb, 180Hf, 181Ta, 186W, 190,192Os, 197Au, 202Hg(n, γ), E=18-28 keV; measured σ; deduced p-wave strength functions.
doi: 10.1016/0003-4916(74)90203-6
Nucl.Phys. A224, 411 (1974)
V.G.Soloviev, C.Stoyanov, A.I.Vdovin
Semi-Microscopic Calculation of the Level Density in Spherical Nuclei
NUCLEAR STRUCTURE 50,51Ti, 53,54,55Cr, 55,57,58Fe, 59,61,62,63,65Ni, 65,67,68,69Zn, 71,73,74,75,77Ge, 75,77,78,79,81,83Se, 85,87,88,89Sr, 91,92,93,95,97Zr, 96,97,98,99,101Mo, 100,102Ru, 106Pd, 112,113,114Cd, 113,115,116,117,118,119,120,121,123,125Sn, 123,124,126,129,131Te, 132,136Xe, 131,135,136,137,138,139Ba, 137,139,141,143Ce, 143,144,145,146,147,149Nd, 145,148,149Sm, 195,196,197,199Pt, 199,200,201,202,203Hg, 205,207Pb; calculated density of states.
doi: 10.1016/0375-9474(74)90696-4
Yad.Fiz. 19, 516 (1974); Sov.J.Nucl.Phys. 19, 260 (1974)
A.I.Vdovin, V.V.Voronov, L.A.Malov, V.G.Solovev, C.Stoyanov
Mass Number Dependence of the Density of 1/2+ States in the Vicinity of the Neutron Binding Energy
NUCLEAR STRUCTURE 139Ba, 141,143Ce, 143,145,147,149Nd, 145,149,153Sm, 157,159Gd, 163,165Dy, 167,169Er, 173,175,177Yb, 179Hf, 185W, 199,201,203Hg, 205Pb calculated level density.
Trans.Amer.Nucl.Soc. 22, 677 (1975)
K.F.Flynn, S.Nagy, L.E.Glendenin, J.E.Gindler, J.W.Meadows
Monoenergetic Neutron Fission of 238U
NUCLEAR REACTIONS 238U(n, F)83Br/85Kr/87Kr/88Kr/89Rb/89Sr/91Y/92Sr/93Y/94Y/95Zr/97Zr/99Mo/101Mo/103Ru/105Ru/106Ru/107Rh/109Pd/111Ag/112Pd/115Cd/121Sn/125Sn/131I/132Te/133I/135I/138Xe/139Ba/140Ba/141Ce/142La/143Ce/144Ce/146Ce/147Nd/149Nd/149Pm/151Pm/153Sm/156Eu, E=2, 8 MeV; measured reaction products, Eγ, Iγ; deduced fission product yields.
Phys.Rev. C12, 1054 (1975)
D.C.Kayser, W.H.Johnson, Jr.
New Mass Measurements of Samarium and Gadolinium and a Mass Table for the Light Rare Earths
ATOMIC MASSES 152,154Sm; measured atomic mass. 141,142,143,144Pr, 142,143,144,145,146,147,148,149,150Nd, 144,145,147,148,149,150,151,152,153,154,155Sm, 145,147,149Pm, 151,152,153,154,155Eu, 151,152,153,154,155,156,157,158,160Gd deduced mass excesses.
J.Nucl.Sci.Technol. 12, 681 (1975)
T.Sato, Y.Kanda, I.Kumabe
Activation Cross Sections for (n, p) and (n, α) Reactions on Nd, Sm, Yb And Lu at 14.6 MeV
NUCLEAR REACTIONS 150Sm, 173Yb, 175Lu(n, p), 146Nd, 152Sm, 174Yb, 176Lu(n, α), E=14.6 MeV; measured activation σ. Ge(Li) detector, pre-equilibrium model.
JYFL Ann.Rept. 1976, p.57 (1977)
E.Hammaren, E.Liukkonen, R.Katajanheimo, T.Tuurnala, T.Raunemaa
Nanosecond Lifetime Measurements for Levels in the Transitional Isotopes 147Nd and 149Nd
NUCLEAR REACTIONS 146,148Nd(d, pγ), E=10 MeV; measured γγ-coin, γγ(t), pγ(t). 147Nd, 149Nd levels deduced T1/2.
J.Nucl.Sci.Technol. 14, 319 (1977)
I.Kumabe, E.Kotake, F.Nagahama
Activation Cross Sections for (n, 2n) Reaction on Neodymium, Samarium, Gadolinium and Ytterbium at 14.6 MeV
NUCLEAR REACTIONS 142,148,150Nd, 154Sm, 160Gd, 176Yb(n, 2n), E=14.6 MeV; measured σ.
J.Nucl.Sci.Technol. 14, 460 (1977)
I.Kumabe
Analysis of (n, 2n) Cross Sections at 14.7 MeV in Region of Rare-Earths
NUCLEAR REACTIONS 136,138,140,142Ce, 142,148,150Nd, 144,154Sm, 151,153Eu, 152,154,160Gd, 159Tb, 156,158,160Dy, 165Ho, 162,164,166Er, 169Tm, 168,170,176Yb, 175Lu, 174,176Hf(n, 2n), E=14.7 MeV; calculated σ.
Yad.Fiz. 27, 10 (1978); Sov.J.Nucl.Phys. 27, 5 (1978)
V.N.Kononov, B.D.Yurlov, E.D.Poletaev, V.M.Timokhov
Fast-Neutron Capture Cross Sections for Even-Even Isotopes of Neodymium, Samarium, Gadolinium, and Erbium
NUCLEAR REACTIONS 142,144,146,148,150Nd, 144,148,150,152,154Sm, 156,158,160Gd, 166,168,170Er(n, γ), E=5-350 keV; measured σ(E).
Phys.Scr. 19, 497 (1979)
R.Katajanheimo, E.Hammaren
Particle-Rotor Model Study of the Transitional N = 89 and Some N = 91-95 Nuclei
NUCLEAR STRUCTURE 161,163Er, 155,157,161Dy, 153,155,157Gd, 151,153Sm, 149Nd; calculated energy levels, relative Iγ; deduced Nilsson assignments. Particle-rotor model.
Phys.Scr. 20, 125 (1979)
R.Katajanheimo, A.Siivola, T.Tuurnala, E.Hammaren, E.Liukkonen
The Isomeric 9/2+ and the Lowest 7/2- State in the Weakly Deformed N = 89 Nuclei
NUCLEAR REACTIONS 148Nd(d, pγ), E=10 MeV; 154Sm(3He, 4nγ), 155Gd(3He, 3nγ), E=27 MeV; measured γγ(t), pγ(t), Eγ. 149Nd, 151Sm, 153Gd, 155,157Dy, 159,161Er deduced levels, T1/2, J, π. Nilsson assignments, B(E1) particle-rotor model, nonspheroidal Woods-Saxon potential.
Acta Phys.Pol. B11, 445 (1980)
S.Cwiok, W.Nazarewicz, W.Zych
The Dependence of Coulomb Displacement Energy on Deformation of a Nucleus
NUCLEAR STRUCTURE 149,151Nd, 149,151Pm, 169Er, 169Tm, 169,171Yb, 169,171Lu; calculated Coulomb displacement energies; deduced deformation effects. Woods-Saxon deformed potential, monopole pairing interaction.
Proc.Conf.Neutron Physics, Kiev, Part 3, p.153 (1980)
A.N.Gudkov, V.M.Zhivun, V.V.Kovalenko, A.B.Koldobsky, V.M.Kolobashkin, V.N.Kosyakov, S.V.Krivasheev
Determination of Independent and Cumulative Fission Product Yields from Thermal Neutron Induced Fission of Californium-249
NUCLEAR REACTIONS 249Cf(n, F)89Rb/91Sr/92Sr/94Y/97Zr/98Nb/99Mo/101Mo/99mTc/101Tc/104Tc/105Tc/103Ru/105Ru/105Rh/112Pd/115Ag/117mCd/128Sn/122Sb/127Sb/128mSb/129Sb/130mSb/131Sb/131mTe/131Te/132Te/133mTe/133Te/134Te/131I/132I/133I/134I/134mI/135I/135mXe/135Xe/138Xe/136Cs/138Cs/139Ba/140Ba/141Ba/142Ba/140La/142La/143Ce/146Ce/148Nd/149Nd/151Nd/150Pm/151Pm/156Eu, E=thermal; measured cumulative, independent fission yields. Direct γ-spectroscopic techniques.
Phys.Scr. 22, 321 (1980)
R.Katajanheimo
Existence of the 7/2+ State in N=89 Nuclei
NUCLEAR STRUCTURE 155Dy, 153Gd, 151Sm, 149Nd; calculated levels, band structure, γ-branching; deduced existence of 7/2+ in N=89 nuclei. Particle-rotor model, nonspheriodal Woods-Saxon potential.
Nuovo Cim. 66A, 1 (1981)
V.Benzi, G.Maino, E.Menapace
Nuclear Level Densities with Blocking Effect
NUCLEAR STRUCTURE 90Y, 91,92,93,95Zr, 94Nb, 93,95,96,97,98,99,101Mo, 100Tc, 102,103,104,105Ru, 104Rh, 106,109Pd, 108,110Ag, 111,112,113,114,115,117Cd, 114,116In, 113,115,116,117,118,119,121Sn, 124,125,126,127,129Te, 128,130I, 130,132Xe, 134,135,136Cs, 131,135,136,137,138,139Ba, 139,140La, 137,141Ce, 142Pr, 143,144,145,146,147,149,151Nd, 148Pm, 150,151,152,153,155Sm, 152,153,154,155,156Eu, 153,155,156,157,158,159,161Gd, 160Tb, 157,161,162,163,164,165Dy, 166Ho, 163,165,167,168,169,171Er, 170Tm, 171,172,173,174,175,177Yb, 176,177Lu, 175,177,178,179,180,181Hf, 182Ta, 183,184,185,187W, 186,188Re, 227Ra, 230,231,233Th, 232,234Pa, 233,234,235,236,237,239U, 238Np, 239,240,241,242,243Pu, 242,243,244Am, 244,245,246,248Cm, 250Cf; calculated level spacings. Blocking effect, s-wave neutron resonance analysis.
Phys.Rev. C23, 331 (1981)
J.K.Dickens, J.W.McConnell
Yields of Fission Products Produced by Thermal-Neutron Fission of 245Cm
NUCLEAR REACTIONS, Fission 245Cm(n, F), E=thermal; measured σ(Eγ), T1/2. 87,90Kr, 91,93,94Y, 91,92,93,94Sr, 84Br, 88,89Rb, 95,97,99Nb, 99,101Mo, 105,106,103,104,102Tc, 108,109,105,103Ru, 106,111,107,109,105,110Rh, 113,111,114,112Ag, 115In, 131,136,133,137,132,134,135I, 139,137,135,138Xe, 149,147,151Nd, 97,95Zr, 152,153,151Pm, 141,146,148,143,145,136,139,138,140Cs, 139,142,141,140Ba, 132,133,134,131Te, 144,140,142La, 128,127Sn, 146Pr, 127,128,132,129,130,131,133Sb, 156Eu deduced cumulative yields.
Can.J.Phys. 59, 1183 (1981)
L.Haugen, J.R.Lien, G.Lovhoiden, O.Straume, D.G.Burke, J.C.Waddington
Levels in 149Nd Studied with the (d(pol), t) Reaction
NUCLEAR REACTIONS 150Nd(polarized d, t), E=16 MeV; measured σ(θ), σ(Et), iT11(θ). 149Nd deduced levels, L, J, π, structure factors. DWBA ananysis.
J.Radioanal.Chem. 75, 189 (1982)
A.Bari
14.8 MeV Neutron Activation Cross-Sections for (n, p) and (n, α) Reactions of some Rare Earth Nuclides
NUCLEAR REACTIONS 139La, 140Ce, 141Pr, 146Nd, 150Sm, 153Eu, 159Tb, 166Er, 174Yb(n, p), 139La, 142Ce, 142Nd, 150,152,154Sm, 162Dy(n, α), E=14.8 MeV; measured σ. Activation technique. Semi-empirical model.
J.Nucl.Radiochem. 5, 176 (1983)
W.Li, T.Sun, M.Zhen, T.Dong, X.Sun
Determination of the Yields for the Rare-Earth Nuclides from 14 MeV Neutron Fission of 238U Using Ge(Li) Detector
NUCLEAR REACTIONS 238U(n, F)93Y/141Ce/142La/143Ce/144Ce/145Pr/147Nd/149Nd/149Pm/151Pm/153Sm/156Sm/156Eu/157Eu, E=14 MeV; measured fission products, Eγ, Iγ; deduced cumulative yields.
J.Phys.(London) G10, 91 (1984)
An Jong Do, J.Dresler, U.Garuska, M.Herman, A.Marcinkowski
The Cross Sections of the (n, 2n) Reactions on 134Ba, 142Nd, 150Nd and 144Sm
NUCLEAR REACTIONS 134Ba, 142,150Nd, 144Sm(n, 2n), E=13-18 MeV; measured σ(E). Activation method. Compound nucleus, precompound theory analyses.
doi: 10.1088/0305-4616/10/1/014
Proc.Conf.Neutron Physics, Kiev, Vol.2, p.259 (1984)
A.N.Gudkov, A.N.Davletshin, V.M.Zhivun, A.V.Zvonarev, V.V.Kovalenko, A.B.Koldobsky, Yu.F.Koleganov, V.M.Kolobashkin, S.V.Krivasheev, V.G.Liforov, N.C.Piven, A.O.Tipunkov, V.A.Tolstikov
Measurement of Uranium-236 and Uramium-238 Fission Product Yields Using Monoenergetic Neutrons and the Semi-Conductor Gamma Spectrometry Method
NUCLEAR REACTIONS 236U(n, F)91Sr/92Sr/93Sr/92Y/93Y/94Y/97Zr/99Mo/101Mo/99mTc/101Tc/128Sb/129Sb/130Sb/131mTe/132Te/133mTe/134Te/133I/134I/135I/139Ba/140Ba/142La/146Pr/149Nd, E=960, 3300 eV; 238U(n, F)91Sr/97Zr/105Ru/132Te/133I/135I/135Xe/139Ba/142La/149Nd, E=1050 eV; measured absolute fission fragment yields. Semiconductor γ-spectrometry.
Radiochim.Acta 35, 5 (1984)
S.M.Qaim
Activation Cross Sections of (n, α) Reactions at 14.7 MeV in the Region of Rare Earths
NUCLEAR REACTIONS 139La, 140,142Ce, 142,144,146Nd, 150,152,154Sm, 151,153Eu, 156,158Gd, 159Tb, 162,164Dy, 165Ho, 168Er, 169Tm, 172,174Yb, 175,176Lu, 178,180Hf(n, α), E ≈ 14.7 MeV; measured σ; deduced target relative neutron excess dependence. Activation technique.
Radiochim.Acta 38, 173 (1985)
Chien Chung, L.-K.Pan
Cumulative Fission Product Yields of Fast-Neutron Fission of 232Th
NUCLEAR REACTIONS 232Th(n, F)84Se/87Kr/88Br/89Rb/91Y/91mY/93Sr/94Sr/95Sr/97Sr/99Mo/131Sb/131I/132Sb/132Te/133Te/134I/135Xe/135mXe/136I/136mI/138Cs/139Xe/139Ba/140Cs/140La/141Ba/141Ce/143Ba/144La/145Ce/146Ce/148Ce/149Nd, E=fast; measured residuals cumulative yields following fission; deduced absolute yields. Activation technique.
Chin.J.Nucl.Phys. 7, 97 (1985)
Li Ze, Zhang Chunhua, Liu Conggui, Wang Xiuzhi, Qi Linkun, Cui Anzhi, Lu Huijun, Zhang Sujing, Liu Yonghui, Ju Changxin, Liu Daming, Tang Peijia, Meng Jiangchen, Jing Kexing
Mass Distribution in 8.3 MeV Neutron-Induced Fission of 238U
NUCLEAR REACTIONS 238U(n, F)83Br/84Br/85Kr/85mKr/87Kr/88Kr/89Rb/91Sr/92Sr/93Y/94Y/95Zr/97Nb/99Mo/101Tc/103Ru/104Tc/105Ru/106Ru/107Rh/109Pd/111Ag/113Ag/112Pd/115Cd/121Sb/125Sn/127Sb/128Sn/129Sb/130Sb/131I/132Te/133I/134I/135Xe/136Cs/137Cs/138Cs/139Ba/140Ba/141Ba/141Ce/142La/143Ce/144Ce/146Pr/147Nd/149Pm/149Nd/151Pm/153Sm/156Eu/161Tb, E=8.3 MeV; measured absolute fission yields. Radiochemical methods, Ge(Li) γ-detector.
Pramana 24, 461 (1985)
R.Majumdar
Low-Lying Vibrational States of 145,147,149Nd
NUCLEAR STRUCTURE 145,147Nd; calculated levels, spectroscopic factors, B(λ), branching ratios. 145Nd; calculated μ, quadrupole moment. 147Nd; calculated μ. 149Nd; calculated levels, spectroscopic factors. Anharmonic vibrator, quasiparticles.
Nucl.Sci.Eng. 94, 413 (1986)
A.E.Richardson, H.L.Wright, J.L.Meason, J.R.Smith
Mass Distribution in the Fission of 232Th by Degraded-Fission-Spectrum Neutrons
NUCLEAR REACTIONS 232Th(n, F)83Se/84Br/85Kr/85mKr/87Kr/88Kr/91Sr/91Y/91mY/92Sr/92Y/94Y/95Nb/97Nb/97mNb/99Mo/99Tc/99mTc/129Sb/130Sb/131I/132I/133I/134I/135I/132Te/135Xe/135mXe/138Cs/139Ba/140La/142La/141Ce/143Ce/146Pr/147Nd/149Nd, E=fission spectrum; measured residual yields, fission fragment mass distribution. Degraded fission spectrum, activation technique.
J.Radioanal.Nucl.Chem. 144, 359 (1990)
A.Abzouzi, M.S.Antony, A.Hachem, V.B.Ndocko Ndongue
Precision Measurements of the Half-Lives of 60mCo, 79mSe, 104mRh, 149Nd, 176mLu, 177Lu and 198Au
RADIOACTIVITY 60mCo, 79mSe, 104mRh, 149Nd, 176m,177Lu, 198Au; measured T1/2. High precision.
Z.Phys. A345, 285 (1993)
A.Kirov, N.Nenoff, E.Georgieva, C.Necheva, I.Ephtimov
Activation Cross Sections and Isomeric Ratios in Reactions Induced by 14.5 MeV Neutrons on 152Sm, 154Sm and 178Hf
NUCLEAR REACTIONS 152,154Sm, 178Hf(n, p), 154Sm(n, d), 152Sm(n, α), E=14.5 MeV; measured σ, isomeric ratios. Activation technique. Compound, precompound models comparison.
J.Alloys and Compounds 213/214, 414 (1994)
K.Tsukada, N.Shinohara, Y.Nagame, S.Ichikawa, M.Magara, M.Hoshi, K.Sueki, M.Tanikawa, I.Nishinaka, T.Kobayashi, H.Nakahara, T.Ohtsuki
Mass yield and angular distribution of rare earth elements produced in proton-induced fission of 244Pu
NUCLEAR REACTIONS 244Pu(p, F)115mCd/131mTe/142La/149Nd/156Sm/162Tb, E=10-16 MeV; measured fission fragment production σ. 244Pu(p, F), E=15 MeV; measured fission fragments angular distributions, mass yields.
doi: 10.1016/0925-8388(94)90947-4
Phys.Rev. C51, 1540 (1995)
K.A.Toukan, K.Debus, F.Kappeler, G.Reffo
Stellar Neutron Capture Cross Sections of Nd, Pm, and Sm Isotopes
NUCLEAR REACTIONS 146,148,150Nd(n, γ), E=25, 30 keV; measured Eγ, Iγ; deduced stellar capture σ(E), s-, r-, p-process abundances from 142Nd-150Sm. 147Nd, 147,148,149Pm, 147,148,149,150,151Sm(n, γ), E=1-600 keV; 146,147,148Nd, 147,148,149Pm, 151Sm(n, γ), E=12-52 keV; calculated σ(E). 148Nd, 147,148,149,150Pm, 147,148,149,150,151,152,153Sm deduced level density parameters, Γγ.
Nucl.Phys. A621, 270c (1997)
K.Wisshak, F.Voss, F.Kappeler, L.Kazakov
Neutron Capture in Neodymium Isotopes: Implications for the s-process
NUCLEAR REACTIONS 142,143,144,145,146,148Nd(n, γ), E=10, 30 keV; measured capture σ. Other data compared, astrophysical s-process implications.
doi: 10.1016/S0375-9474(97)00253-4
Appl.Radiat.Isot. 49, 1529 (1998)
X.Kong, Y.Wang, J.Yang
Cross Sections for (n, 2n), (n, p) and (n, α) Reactions on Rare-Earth Isotopes at 14.7 MeV
NUCLEAR REACTIONS 154Sm, 162Er, 168Yb, 174,176Hf(n, 2n), 142Ce, 144,148,150Sm, 160,162,163Dy, 166,167,168Er, 174Yb(n, p), 150,152,154Sm, 159Tb, 153Eu, 162,164Dy, 168Er, 169Tm, 178,180Hf(n, α), E=14.7 MeV; measured σ. Activation technique. Comparison with previous measurements.
doi: 10.1016/S0969-8043(98)00018-9
Bull.Rus.Acad.Sci.Phys. 63, 140 (1999)
N.A.Abibullaev, U.T.Asatov, O.F.Mailova, A.K.Mukhamedov, U.S.Salikhbaev, A.N.Safarov
Yields of Photonuclear Reactions on Bremsstrahlung of Electrons with the Energy 20 MeV
NUCLEAR REACTIONS 77Se, 79Br, 87Sr, 89Y, 111Cd, 115In, 137Ba, 167Er, 179,180Hf, 183W, 190Os, 191Ir, 197Au, 204Pb(γ, γ'), 12C, 14N, 16O, 19F, 23Na, 24Mg, 27Al, 31P, 32S, 45Sc, 55Mn, 59Co, 58Ni, 63,65Cu, 64Zn, 70,76Ge, 75As, 76,78,80,82Se, 89Y, 90Zr, 93Nb, 92,94,100Mo, 103Rh, 107Ag, 112,116Cd, 115In, 118,124Sn, 121,123Sb, 124,130Te, 127I, 133Cs, 138Ba, 140,142Ce, 141Pr, 142,148,150Nd, 144,154Sm, 153Eu, 165Ho, 175Lu, 181Ta, 186W, 186,192Os, 197Au, 232Th, 238U(γ, n), 59Co, 91Zr, 93Nb, 103Rh, 107Ag, 115In, 119Sn, 141Pr, 143Nd, 165Ho, 175Lu, 192Os, 193Ir, 195Pt, 197Au, 206Pb(γ, 2n), E=20 MeV bremsstrahlung; measured beam characteristics, differential and integral yields versus θ.
Bull.Rus.Acad.Sci.Phys. 63, 149 (1999)
N.A.Abibullaev, U.T.Asatov, A.K.Mukhamedov, U.S.Salikhbaev
Differential and Integral Effective Cross Sections for Photonuclear Reactions Excited by Bremsstrahlung of 20-MeV Electrons in a Thick Tungsten Target
NUCLEAR REACTIONS 77Se, 79Br, 87Sr, 89Y, 111Cd, 115In, 137Ba, 167Er, 179,180Hf, 183W, 190Os, 191Ir, 197Au, 204Pb(γ, γ'), 12C, 14N, 16O, 19F, 23Na, 24Mg, 27Al, 31P, 32S, 45Sc, 55Mn, 59Co, 58Ni, 63,65Cu, 64Zn, 70,76Ge, 75As, 76,78,80,82Se, 89Y, 90Zr, 93Nb, 92,94,100Mo, 103Rh, 107Ag, 112,116Cd, 115In, 118,124Sn, 121,123Sb, 124,130Te, 127I, 133Cs, 138Ba, 140,142Ce, 141Pr, 142,148,150Nd, 144,154Sm, 153Eu, 165Ho, 175Lu, 181Ta, 186W, 186,192Os, 197Au, 232Th, 238U(γ, n), 59Co, 91Zr, 93Nb, 103Rh, 107Ag, 115In, 119Sn, 141Pr, 143Nd, 165Ho, 175Lu, 192Os, 193Ir, 195Pt, 197Au, 206Pb(γ, 2n), E=20 MeV bremsstrahlung; measured beam characteristics, average effective σ(θ).
Ann.Nucl.Energy 26, 553 (1999)
M.A.Ansari, R.K.Y.Singh, R.P.Gautam, S.Kailas
Fast Neutron Radiative Capture Cross-Sections in Fission Product Isotopes of Neodymium
NUCLEAR REACTIONS 148,150Nd(n, γ), E=0.46-3.44 MeV; measured σ.
doi: 10.1016/S0306-4549(98)00021-8
Radiochemistry 41, 24 (1999); Radiokhimiya 41, 25 (1999)
Y.S.Popov, N.Y.Nezgovorov, G.A.Timofeev
Radioactive Decay of Lanthanides
RADIOACTIVITY 141Ce, 147,149Nd, 147,148,149Pm, 153Sm, 154,155,156Eu, 160Tb(β-), 152Eu(EC), (β-), 151,153Gd(EC) [from 252Cf(SF)]; measured decay products, Eγ, Iγ; deduced T1/2, γ-ray energies and intensities.
Astrophys.J. 582, 1251 (2003)
R.Reifarth, C.Arlandini, M.Heil, F.Kappeler, P.V.Sedyshev, A.Mengoni, M.Herman, T.Rauscher, R.Gallino, C.Travaglio
Stellar Neutron Capture on Promethium: Implications for the s-Process Neutron Density
NUCLEAR REACTIONS 147Pm(n, γ), E=25 keV; measured reaction products, Eγ, Iγ; deduced Maxwellian-averaged σ and its uncertainties.
NUCLEAR REACTIONS 147,148,149Pm(n, γ), E=5-100 keV; calculated Maxwellian-averaged σ.
COMPILATION 146,147,148Nd, 147,148,149Pm, 147,148,149,150Sm(n, γ), E=10, 25, 30 keV; compiled Maxwellian-averaged σ and its uncertainties.
doi: 10.1086/344718
J.Radioanal.Nucl.Chem. 260, 143 (2004)
Z.Pu, J.Yang, X.Kong
Cross section measurements for (n, p) and (n, 2n) reactions of rare-earth isotopes at neutron energies from 13.5 to 14.6 MeV
NUCLEAR REACTIONS 142,148,150Nd(n, 2n), E=13.5-14.6 MeV; 146Nd, 141Pr, 139La, 158Gd(n, p), E=13.5-14.6 MeV; measured σ. Activation technique, comparison with previous results.
doi: 10.1023/B:JRNC.0000027073.70271.99
Eur.Phys.J. A 28, 147 (2006)
Ts.Venkova, M.-G.Porquet, M.Houry, R.Lucas, Ch.Theisen, J.Durell, A.Roach
A new high-spin level scheme for 149Nd from a fusion-fission reaction
NUCLEAR REACTIONS 238U(12C, X)149Nd/147Ce, E=90 MeV; measured Eγ, Iγ, γγ-coin. 149Nd, 147Ce deduced high-spin levels, J, π, configurations. Euroball III array.
doi: 10.1140/epja/i2005-10046-4
Phys.Rev. C 77, 015803 (2008)
J.Hasper, S.Muller, D.Savran, L.Schnorrenberger, K.Sonnabend, A.Zilges
Investigation of photoneutron reactions close to and above the neutron emission threshold in the rare earth region
NUCLEAR REACTIONS 148,150Nd, 154Sm, 154,160Gd(γ, n), E=7450-9800 keV [from Cu(e, γ)]; measured Eγ, Iγ, photon flux, normalization, cross section; deduced reaction rates.
doi: 10.1103/PhysRevC.77.015803
Acta Phys.Pol. B39, 695 (2008)
M.Jaskola
A Study of Levels in 149Nd Using the (d, p) and (d, t) Reactions
NUCLEAR REACTIONS 148Nd(d, p), E=12.1 MeV; 150Nd(d, t), E=12.1 MeV; measured reaction product spectra and angular distributions, cross sections. 149Nd; deduced levels, J, π. DWBA analysis.
Phys.Rev. C 80, 054606 (2009)
G.Chaudhuri, F.Gulminelli, S.Das Gupta
Symmetry energy from fragment observables in the canonical thermodynamic model
NUCLEAR STRUCTURE 135,149Nd, 202,222Th, 165,186Re; calculated isoscaling parameters as a function of temperature, and symmetry energy of fragmenting source as a function of cluster charge using McGill canonical thermodynamic model (CTM) for heavy-ion collisions.
doi: 10.1103/PhysRevC.80.054606
Eur.Phys.J. A 45, 1 (2010)
E.Ruchowska, W.A.Plociennik, H.Mach, K.Gulda, B.Fogelberg, H.Gausemel, L.M.Fraile, W.Kurcewicz, K.Mezilev, M.Sanchez-Vega
Quenching of the E1 strength in 149Nd
RADIOACTIVITY 149Pr(β-) [from 235U(n, F), E=thermal and subsequent decays]; measured Eγ, Iγ(t), γγ-coin, βγ-coin. 149Nd; deduced levels, J , π, isomeric transition, T1/2, band structure, B(E1), nuclear dipole moment; calculated deformation.
doi: 10.1140/epja/i2010-10979-9
J.Korean Phys.Soc. 59, 875s (2011)
S.T.Holloway, T.Kawano, P.Moller
Time Dependent Particle Emission From Fission Products
RADIOACTIVITY 232Th, 239Pu(SF); calculated β-delayed neutron production, β-delayed γ decay, decay heat for cooling time up to 1.E5 s. 89,90,91,93Rb, 93,93,95Sr, 94,95Y, 138,139,140,141Cs, 141,142,143,144,145Ba, 142,143,144,145La, 145,146,147,148Ce, 146,147,148,149,151Pr, 149,151,153,154,155Nd, 152,153,154,155,156,157Pm, 157,158Sm, 158Eu(β-); calculated heat C/E (data from TAGS). Calculations using FRDM plus QRPA for β-decay, Hauser-Feshbach statistical decay, CINDER code. Comparison to data.
doi: 10.3938/jkps.59.875
Phys.Rev. C 85, 014602 (2012); Erratum Phys.Rev. C 89, 049905 (2014)
O.Lebeda, V.Lozza, P.Schrock, J.Stursa, K.Zuber
Excitation functions of proton-induced reactions on natural Nd in the 10-30 MeV energy range, and production of radionuclides relevant for double-β decay
NUCLEAR REACTIONS Nd(p, X)140Pm/140mPm/141Pm/143Pm/144Pm/146Pm/148Pm/148mPm/149Pm/150Pm/140Nd/141Nd/147Nd/149Nd/138mPr/139Pr/140Pr/142Pr/147Pr/149Pr/139Ce, E=10-30 MeV; measured Eγ, Iγ, elemental and cumulative cross sections by activation method. Discussed activation of natural neodymium by cosmic rays, and SNO+ experiment. Comparison with predictions of TENDL-2010 database (TALYS code).
doi: 10.1103/PhysRevC.85.014602
Phys.Rev. C 85, 024623 (2012); Erratum Phys.Rev. C 85, 039901
H.Naik, T.N.Nathaniel, A.Goswami, G.N.Kim, M.W.Lee, S.V.Suryanarayana, S.Ganesan, E.A.Kim, M.-H.Cho, K.L.Ramakumar
Mass distribution in the 50-, 60-, and 70-MeV bremsstrahlung-induced fission of 232Th
NUCLEAR REACTIONS 232Th(γ, F)77Ge/78Ge/84Br/85mKr/87Kr/88Kr/89Rb/91Sr/92Sr/93Y/94Y/95Zr/97Zr/99Mo/101Mo/107Mo/103Ru/105Ru/104Tc/105Rh/112Ag/113Ag/115Cd/117Cd/117mCd/127Sb/129Sb/128Sn/131I/133I/134I/135I/132Te/134Te/138Cs/139Ba/140Ba/141Ce/143Ce/144Ce/142La/146Pr/147Nd/149Nd/149Pm/149Sm/153Sm, E=50, 60, 70 MeV; measured Eγ, Iγ, fission product mass and cumulative yields, and yields of fission products for A=133-134, 138-139, and 143-144 by activation method, average neutron number. 232Th(n, F), E*=7.61, 12.61, 19.41 MeV; 238U(n, F), E*=7.35, 12.45, 19.15 MeV; 232Th(γ, F), E*=7.35, 13.22, 21.25 MeV; 232Th, 238U(γ, F), E=10, 40, 70 MeV; analyzed and compared yields of fission products as function of mass, yields of symmetric and asymmetric fission products, peak to valley ratios, average neutron number, average values of light mass and heavy mass as function of excitation energy.
doi: 10.1103/PhysRevC.85.024623
Ann.Nucl.Energy 62, 274 (2013)
M.Karadag
Measurement of thermal neutron cross section and resonance integral for 148Nd(n, γ)149Nd reaction by using a 55Mn monitor
NUCLEAR REACTIONS 148Nd, 55Mn(n, γ), E thermal; measured reaction products, Eγ, Iγ; deduced σ, resonance integrals. Relative measurement, comparison with available data.
doi: 10.1016/j.anucene.2013.06.033
Nucl.Data Sheets 118, 233 (2014)
Y.Alhassid, C.Ozen, H.Nakada
Calculating Level Densities of Heavy Nuclei by the Shell Model Monte Carlo Method
NUCLEAR STRUCTURE 148,150,152,154Sm; calculated average total nuclear spin. 143,144,145,146,147,148,149,150,152Nd, 148,149,150,151,152,153,154,155Sm; calculated state density vs excitation energy, even-mass nuclei collective enhancement factor using Monte Carlo microscopic approach. Compared with available data.
doi: 10.1016/j.nds.2014.04.045
Nucl.Data Sheets 120, 52 (2014)
Y.Kojima, Y.Shima, H.Hayashi, A.Taniguchi, M.Shibata
Half-life Measurements of Excited Levels in Fission Products around Mass Number 150
RADIOACTIVITY 149Pr, 149Ce(β-) [from 235U(n, F), E thermal]; measured decay products, Eγ, Iγ.; deduced level energies, T1/2. Comparison with available data.
doi: 10.1016/j.nds.2014.07.004
Nucl.Phys. A929, 129 (2014)
O.Lebeda, V.Lozza, J.Petzoldt, J.Stursa, V.Zdychova, K.Zuber
Excitation functions of proton-induced reactions on natural Nd and production of radionuclides relevant for double beta decay: Completing measurement in 5-35 MeV energy range.
NUCLEAR REACTIONS Nd(p, x), E=5-10, 30-35.4 MeV; measured activation Eγ, Iγ(t). 139Ce, 138m,142Pr, 140,141,147,149Nd, 141,143,144,146,148,148m,149,150Pm deduced formation σ. Data supplemented by data of the same group covering the intermediate energy interval. 139Ce, 147Nd, 143,144,146,148,148mPm deduced T1/2; calculated T1/2 using TENDL2012 library in the energy range 5-36 MeV.
doi: 10.1016/j.nuclphysa.2014.06.010
J.Radioanal.Nucl.Chem. 299, 127 (2014)
H.Naik, B.S.Shivashankar, H.G.Raj Prakash, D.Raj, G.Sanjeev, N.Karunakara, H.M.Somashekarappa, S.Ganesan, G.N.Kim, A.Goswami
Measurements of fission yield in 8 MeV bremsstrahlung induced fission of 232Th and 238U
NUCLEAR REACTIONS 232Th(γ, F)77Ge/78Ge/85Kr/87Kr/88Kr/89Rb/91Sr/92Sr/93Y/94Y/95Y/95Zr/97Zr/99Mo/101Mo/103Ru/104Tc/105Ru/105Rh/107Rh/127Sb/128Sn/129Sb/131Sb/131I/132Te/133I/134Te/134I/135I/137Xe/138Xe/138Cs/139Ba/140Ba/141Ba/141Ce/142Ba/142La/143Ce/144Ce/146Ce/146Pr/147Nd/149Nd/149Pm/151Pm/153Sm, 238U(γ, F)84Br/85Kr/87Kr/88Kr/89Rb/91Sr/92Sr/93Y/94Y/95Y/95Zr/97Zr/99Mo/101Mo/103Ru/104Tc/105Ru/105Rh/107Rh/112Ag/113Ag/127Sb/128Sn/129Sb/131Sb/131I/132Te/133I/134Te/134I/135I/137Xe/138Xe/138Cs/139Ba/140Ba/141Ba/141Ce/142Ba/142La/143Ce/144Ce/146Ce/146Pr/147Nd/149Nd/149Pm/151Pm/153Sm, E=8 MeV; measured reaction products, Eγ, Iγ; deduced fission yields. Comparison with available data.
doi: 10.1007/s10967-013-2719-0
Nucl.Instrum.Methods Phys.Res. B325, 15 (2014)
F.Tarkanyi, S.Takacs, F.Ditroi, A.Hermanne, H.Yamazaki, M.Baba, A.Mohammadi, A.V.Ignatyuk
Activation cross-sections of deuteron induced nuclear reactions on neodymium up to 50 MeV
NUCLEAR REACTIONS Nd(d, X)151Pm/150Pm/149Pm/148Pm/146Pm/144Pm/143Pm/149Nd/147Nd/139Nd/142Pr/139Ce, E < 50 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with TENDL-2012, ALICE-D, EMPIRE-D calculations, available data.
doi: 10.1016/j.nimb.2014.01.024
Phys.Rev. C 91, 024617 (2015)
D.Banerjee, A.Saha, T.Bhattacharjee, R.Guin, S.K.Das, P.Das, D.Pandit, A.Mukherjee, A.Chowdhury, S.Bhattacharya, S.Das Gupta, S.Bhattacharyya, P.Mukhopadhyay, S.R.Banerjee
Role of p-induced population of medium-mass (A∼150) neutron-rich nuclei
NUCLEAR REACTIONS 150Nd(p, n), (p, 2n), (p, p'n), (p, d), E=7-15 MeV; measured Eγ, Iγ, σ(E), half-lives by activation method using K=130 AVF cyclotron at VECC facility. Comparison with previous experimental results, and with model calculations using CASCADE, ALICE, and EMPIRE3.1 computer codes.
RADIOACTIVITY 149Nd, 149,150Pm(β-); measured Eγ, Iγ, ground state half-lives of 149Nd, 149,150Pm.
doi: 10.1103/PhysRevC.91.024617
Phys.Rev. C 91, 064615 (2015)
J.S.Barrett, W.Loveland, R.Yanez, S.Zhu, A.D.Ayangeakaa, M.P.Carpenter, J.P.Greene, R.V.F.Janssens, T.Lauritsen, E.A.McCutchan, A.A.Sonzogni, C.J.Chiara, J.L.Harker, W.B.Walters
136Xe+208Pb reaction: A test of models of multinucleon transfer reactions
NUCLEAR REACTIONS 208Pb(136Xe, X), E=85 MeV; measured Eγ, Iγ, γγ-coin using Gammasphere at ATLAS-ANL facility, σ for projectile-like fragments (PLFs) and target-like fragments (TLFs) by off-line γ-ray spectroscopy for radioactive decay measurements (RD), prompt γ decays recorded during the beam burst (IB), and delayed γ decays recorded between the beam bursts (OB). 116,118Cd, 119,121In, 118,120,122,123,124,126Sn, 119,121,123,125,126,127,128,130Sb, 124,126,128,130,131,132,134Te, 127,128,129,130,131,132,133,135,136I, 128,130,132Xe, 133,134,135,136,137,138Xe, 131,132,133,134,136,137,139,141Cs, 130Ba, 132,134,136,138,139,140,141,142,143Ba, 132,135,136,137,139,140,143La, 136,138,139,140,141,142,143,144,145,146Ce, 139,141,142Pr, 140,142,143,144,145,146,147,148,149Nd, 142,143,145,147,149Pm, 145,146,147,148,149,150,151,152,154Sm, 147,149,151Eu, 152,154,156Gd, 156,158,160,162,164Dy, 160,161Er, 176Yb, 176,178,180,181,182Hf, 179,181Ta, 176,180,182,184,186,187W, 179,185,187Re, 186,188,190,191,192,194,197Os, 188,190,192Ir, 190,191,192,194,196,197,198,200,201,202Pt, 191,192,193,194,196,198,199Au, 194,196,198,200,202,203,204,205,206,208Hg, 196,197,198,199,201,202,203,204,205,206,207Tl, 198,201,202,203,204,206,207,208,209,210,211Pb, 199,201,202,203,204,205,206,207,209,211Bi, 202,204,205,206,207,208,209,210,212,213,214Po, 207,208,209,210,211,213At, 210,211,212,213,214,215,216,218Rn, 211,212,213,215,216Fr, 214Ra; deduced projectile-like fragment cumulative and independent production yields. Comparison with predictions of GRAZING model, and those of Zagrebaev and Greiner model using a quantitative metric. Discussed correlations between TLF and PLF yields.
doi: 10.1103/PhysRevC.91.064615
Int.J.Mod.Phys. E24, 1550073 (2015)
Y.El Bassem, M.Oulne
Ground state properties of even-even and odd Nd, Ce and Sm isotopes in Hartree-Fock-Bogoliubov method
NUCLEAR STRUCTURE 124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161Nd, 123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158Ce, 132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166Sm; calculated ground state energies, two-neutron separation energies. HFB method with SLy5 Skyrme and 1SGogny forces, comparison with experimental data.
doi: 10.1142/S0218301315500731
J.Radioanal.Nucl.Chem. 306, 79 (2015)
E.C.Finn, L.Metz, L.Greenwood, B.Pierson, R.Wittman, J.Friese, R.Kephart
Cumulative fission yields of short-lived isotopes under natural-abundance-boron-carbide-moderated neutron spectrum
NUCLEAR REACTIONS 233,235,238U, 239Pu, 237Np(n, F)84Br/87Kr/89Rb/90Rb/91Sr/92Sr/93Sr/93Y/94Y/94Sr/95Y/95Zr/97Zr/100Mo/101Mo/103Ru/104Tc/105Ru/129Sb/130Sn/131I/131Sb/139Ba/140Ba/141Ba/141Ce/142La/143Ce/145Ce/146Ce/147Nd/149Nd, E ∼ 700 keV; measured fission products; deduced fission yields. Comparison with ENDF/B-VII.1, JEFF-3.1.1 and JENDL-4 libraries.
doi: 10.1007/s10967-015-4085-6
Phys.Rev. C 91, 034329 (2015)
C.Ozen, Y.Alhassid, H.Nakada
Nuclear state densities of odd-mass heavy nuclei in the shell model Monte Carlo approach
NUCLEAR STRUCTURE 143,145,147,149Nd, 149,150,151,153,155Sm; calculated thermal excitation energy and partition function as function of temperature, level densities versus excitation energy. Shell model Monte Carlo (SMMC) calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.91.034329
Nucl.Instrum.Methods Phys.Res. B362, 142 (2015)
S.-C.Yang, K.Kim, T.-Y.Song, Y.-O.Lee, G.Kim
Production cross sections of products in the proton induced reactions on natNd in the energy region up to 45 MeV
NUCLEAR REACTIONS Nd(p, X)141Pm/143Pm/144Pm/146Pm/148Pm/149Pm/150Pm/139Nd/147Nd/149Nd/138Pr/142Pr/139Ce, E<45 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with TALYS 1.6 calculations.
doi: 10.1016/j.nimb.2015.09.061
Phys.Rev. C 94, 024309 (2016)
X.Guan, H.Xu, Y.Zhang, F.Pan, J.P.Draayer
Ground state phase transition in the Nilsson mean-field plus standard pairing model
NUCLEAR STRUCTURE 144,145,146,147,148,149,150,151,152,153,154,155Nd, 146,147,148,149,150,151,152,153,154,155,156,157Sm, 148,149,150,151,152,153,154,155,156,157,158,159Gd; calculated Pairing interaction strength G, odd-even mass differences, odd-even differences of S(2n) values, odd-even differences of α-, and β--decay energies. Nilsson mean-field plus standard pairing model for the ground state phase transitions. Comparison with experimental values taken from NNDC databases.
doi: 10.1103/PhysRevC.94.024309
Phys.Rev. C 96, 054328 (2017)
W.M.Seif, N.V.Antonenko, G.G.Adamian, H.Anwer
Correlation between observed α decays and changes in neutron or proton skins from parent to daughter nuclei
RADIOACTIVITY 105,106,107,108,109,110Te, 107,108,109,110,111,112,113I, 109,110,111,112,113,115Xe, 124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,143,144,145,146,147,148,149Nd, 133,134,135,136,137,138,139,143,145,146,147,148,149,150,151,152Sm, 133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155Gd, 148,149,150,151,152Yb, 147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166Ho, 153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177Yb, 186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,211,222,223,224Po, 212,213,214,215,216,217,218,219,220,211,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241Pa, 241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260Fm(α); calculated difference between the proton or neutron skin thicknesses, Q(α), partial α-decay half-lives for 140-155Gd, 232-241Pa and 258-260Fm. Comparison with available experimental half-lives. Hartree-Fock-Bogoliubov (HFB) method based on the Skyrme-like effective interactions.
doi: 10.1103/PhysRevC.96.054328
Phys.Rev. C 97, 014614 (2018)
H.Naik, G.N.Kim, K.Kim
Mass-yield distributions of fission products in bremsstrahlung-induced fission of 232Th
NUCLEAR REACTIONS 232Th(γ, F)77Ge/78Ge/84Br/85mKr/87Kr/88Kr/89Rb/91Sr/92Sr/93Y/94Y/97Zr/99Mo/101Mo/103Ru/104Tc/105Ru/105Rh/107Rh/111Ag/113Ag/115Cd/117Cd/117mCd/127Sb/128Sn/129Sb/131I/132Te/133I/134Te/134I/135I/138xe/138Cs/139Ba/140Ba/141Ba/141Ce/142La/143Ce/146Ce/146Pr/147Nd/149Nd/153Sm, E=2.5 GeV bremsstrahlung; measured Eγ, Iγ, mass yield distributions of fission products in A=77-153 mass region using the recoil catcher and an off-line γ-ray spectrometric at the Pohang Accelerator Laboratory, Korea; deduced peak-to-valley ratio, average values of light and heavy masses, average postfission number of neutrons. Comparison with literature experimental data for 238U(γ, F) reaction at various excitation energies.
doi: 10.1103/PhysRevC.97.014614
Int.J.Mod.Phys. E27, 1850059 (2018)
M.Ouhachi, M.R.Oudih, M.Fellah, N.H.Allal
Nuclear structure and decay properties of Nd isotopes
NUCLEAR STRUCTURE 120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170,171,172,173,174,175,176,177,178,179,180,181,182,183,184,185,186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206Nd; calculated binding energies per nucleon, one- and two-neutron separation energies, nuclear radii, quadrupole-deformation parameters, potential energy curves, Q-values, β-decay T1/2. Comparison with available data.
doi: 10.1142/S0218301318500593
Phys.Rev. C 100, 014608 (2019)
Krishichayan, M.Bhike, C.R.Howell, A.P.Tonchev, W.Tornow
Fission product yield measurements using monoenergetic photon beams
NUCLEAR REACTIONS 235,238U, 239Pu(polarized γ, F)84Br/85mKr/87Kr/88Kr/91Sr/92Sr/92Y/93Y/94Y/95Zr/97Zr/99Mo/103Ru/104Tc/105Ru/105Rh/115Cd/127Sb/128Sn/129Sb/130Sb/131Sb/131I/132Te/132Cs/133Te/133I/134Te/135I/136Cs/138Cs/139Ba/140Ba/141Ba/141Ce/142La/143Ce/146Pr/147Nd/149Nd/151Pm, E=13 MeV; measured fission fragments, Eγ, Iγ, fission product yields (FPY) using dual fission chamber for fission fragments and offline γ detection at TUNL-HIγS facility. Comparison with previous experimental neutron- and photon-induced fission product yields.
RADIOACTIVITY 91,92Sr, 142La(β-)[from 235,238U, 239Pu(polarized γ, F), E=13 MeV at TUNL-HIγS facility]; measured half-lives of decay of 91Sr, 92Sr, and 142La, and compared with values from ENSDF database at NNDC.
doi: 10.1103/PhysRevC.100.014608
Phys.Rev. C 100, 014606 (2019)
H.Naik, G.N.Kim, K.Kim, M.Zaman
Mass yield distributions in the 232Th (n, f) reaction with fast neutrons
NUCLEAR REACTIONS 232Th(n, F)77Ge/78Ge/84Br/85mKr/87Kr/88Kr/89Rb/91Sr/92Sr/93Y/94Y/95Zr/97Zr/99Mo/101Mo/103Ru/104Tc/105Ru/105Rh/107Rh/112Ag/113Ag/115Cd/115mCd/117Cd/117mCd/127Sb/128Sn/129Sb/131Sb/131I/132Te/133I/134Te/134I/135I/138Cs/139Ba/140Ba/141Ba/141Ce/142La/143Ce/146Pr/147Nd/149Nd/149Pm/151Pm/153Sm, E=7.46, 13.4, 18.0 MeV; measured Eγ, Iγ, cumulative and mass fission product yields, fission yield mass distribution, average light and heavy fragment mass, average neutron multiplicity, and peak to valley ratio using offline γ-ray spectroscopy at the MC-50 Cyclotron facility of Korea Institute of Radiological and Medical Sciences. Comparison with other experimental values, and with similar quantities in 238U(n, F), E=fast. Discussed effect of deformed shells closure proximity due to the octupole deformation of fragments.
doi: 10.1103/PhysRevC.100.014606
INDC(NDS)-0794 (2019)
N.J.Stone
Table of Recommended Nuclear Magnetic Dipole Moments: Part I - Long-lived States
COMPILATION Z=0-99; compiled experimental values of nuclear magnetic moments.
Phys.Rev. C 99, 024327 (2019)
D.Zinatulina, V.Brudanin, V.Egorov, C.Petitjean, M.Shirchenko, J.Suhonen, I.Yutlandov
Ordinary muon capture studies for the matrix elements in ββ decay
NUCLEAR REACTIONS Se(μ-, νxn)76As/77As/79As/81As, Kr(μ-, νxn)84Br/85Br, Cd(μ-, νxn)109Ag/110Ag/111Ag/113Ag/115Ag, Sm(μ-, νxn), 48Ti(μ-, νxn)47Sc/48Sc, 76Se(μ-, νxn)71As/72As/74As/75mAs/76As, 82Kr(μ-, νxn)81Br/82Br, 106Cd(μ-, νxn)105Ag, 150Sm(μ-, νxn)148Pm/148mPm/149Pm/149mPm/150Pm/149Nd, E at 20-30 MeV/c PSI muon beam; measured muon x rays, Eγ, Iγ of decaying ordinary (non-radiative) μ capture products, half-lives of ordinary μ capture products using HPGe detectors for γ detection; deduced μ capture rates, partial capture probabilities. 48Sc, 76As, 106Ag; deduced levels, partial ordinary muon capture (OMC) probabilities to different excited states in daughter nuclei.
doi: 10.1103/PhysRevC.99.024327
Eur.Phys.J. A 56, 227 (2020)
H.Naik, S.P.Dange, W.Jang, R.J.Singh
Post-neutron mass yield distribution in the thermal neutron induced fission of 245Cm
NUCLEAR REACTIONS 245Cm(n, F), E thermal; measured fission products, Eγ, Iγ. 83,84Se, 84Br, 85Kr, 86,87Br, 87,88,89,90Kr, 87,88,89,90,91Rb, 91,92,93,94Sr, 91,92,93,94,95Y, 91,92,93,94Sr, 95,97Zr, 100,101Mo, 103Mo, 102,103,104,105,106Tc, 103Ru, 105Ru, 107,108,109Ru, 105,107,109Rh, 111,112,113Ag, 116Ag, 115,117Cd, 119In, 123,125,127Sn, 128,129,130Sn, 128,129,130,131Sb, 131,132,133,134,135,136I, 131,132,133,134Te, 135Xe, 137,138,139Xe, 138,139,140,141Cs, 139,140,141,142Ba, 142,144La, 141,143,145,147Ce, 148Ce, 146Pr, 147,149Nd, 152Nd, 151Pm, 153,154Pm, 152,153,154,155,156,157Sm, 157,158,159Eu, 161,162Gd; deduced cumulative, independent and chain yields. Comparison with ENDF/B-VIII.0 library.
doi: 10.1140/epja/s10050-020-00228-3
Nucl.Data Sheets 163, 249 (2020)
B.D.Pierson, L.R.Greenwood, S.C.Stave, J.T.Burke, S.W.Padgett, A.M.Prinke, J.M.Goda, J.A.Bounds, D.K.Hayes, A.S.Tamashiro, R.S.Wittman, G.Slavik, M.P.Dion, J.G.Burch, T.S.Palmer
Improved Cumulative Fission Yield Measurements with Fission Spectrum Neutrons on 238U
NUCLEAR REACTIONS 238U(n, F)84Br/93Y/94Y/104Tc/128Sn/129Sb/130Sb/131Te/133I/134I/135I/138Xe/139Ba/141Ba/142Ba/142La/146Ce/149Nd, E ∼ 2 MeV; measured fission products, Eγ, Iγ; deduced fission yields. Comparison with ENDF/B-VIII.0 library evaluations.
doi: 10.1016/j.nds.2019.12.006
Eur.Phys.J. A 57, 112 (2021)
H.Naik, S.P.Dange, W.Jang, R.J.Singh
Post-neutron mass yield distribution in the epi-cadmium neutron induced fission of 240Pu
NUCLEAR REACTIONS 240Pu(n, F)83Se/84Se/84Br/85Kr/87Kr/88Kr/89Kr/89Rb/90Rb/91Rb/91Sr/91Y/92Sr/92Y/93Sr/93Y/94Sr/94Y/95Y/95Zr/97Zr/99Mo/101Mo/103Mo/102Tc/104Tc/105Tc/103Ru/105Ru/108Ru/105Rh/109Rh/111Ag/112Ag/113Ag/115Cd/117Cd/123Sn/125Sn/127Sn/128Sn/130Sn/127Sb/129Sb/130Sb/131Sb/132Sb/133Sb/131Te/132Te/133Te/134Te/131I/132I/133I/134I/135I/136I/135Xe/137Xe/138Xe/138Cs/139Cs/140Cs/141Cs/139Ba/140Ba/141Ba/142Ba/142La/144La/141Ce/143Ce/144Ce/145Ce/146Ce/147Ce/148Ce/146Pr/147Nd/149Nd/151Nd/151Pm/153Sm/155Sm/156Sm/157Eu, E thermal; measured reaction products, Eγ, Iγ; deduced cumulative and independent fission yields. Comparison with experimental data, EXFOR and ENDF/B-VIII.0 libraries.
doi: 10.1140/epja/s10050-021-00377-z
Eur.Phys.J.Plus 136, 694 (2021)
H.Naik, S.P.Dange, W.Jang, R.J.Singh
Post-neutron mass chain yield distribution in the epi-cadmium neutron-induced fission of 232Th
NUCLEAR REACTIONS 232Th(n, F)78As/80Ge/81As/83Se/84Se/84Br/85Kr/86Br/87Br/87Kr/88Kr/89Kr/89Rb/90Kr/90Rb/91Sr/91Y/92Sr/92Y/93Sr/93Y/94Sr/94Y/95Y/95Zr/97Zr/99Mo/101Mo/101Tc/102Tc/103Mo/103Tc/104Tc/105Tc/105Ru/106Tc/107Rh/108Ru/109Rh/112Ag/113Ag/116Ag/117Cd/119Cd/123Sn/125Sn/127Sn/128Sn/129Sn/129Sb/130Sn/130Sb/131Sb/131Te/131I/132Sb/132Te/132I/133Sb/133Te/133I/134Te/134I/135I/135Xe/136I/137Xe/138Xe/138Cs/139Xe/139Cs/139Ba/140Cs/140Ba/141Ba/141Ce/142Ba/142La/143Ce/144La/145Ce/146Ce/146Pr/147Ce/147Nd/148Ce/149Nd/151Nd/152Nd/153Pm, E>0.5 eV; measured reaction products, Eγ, Iγ; deduced cumulative and independent fission yields. Comparison with ENDF/B-VIII.0 evaluations, available data.
doi: 10.1140/epjp/s13360-021-01690-8
Eur.Phys.J. A 57, 176 (2021)
H.Naik, S.P.Dange, R.J.Singh, W.Jang
Mass yield distribution in the fission of 244Cm induced by a spectrum of epi-cadmium to fast neutron
NUCLEAR REACTIONS 244Cm(n, F), E>0.0253 eV; measured reaction products, Eγ, Iγ. 83,84Se, 84,86,87Br, 85,87,88,89,90Kr, 89,90,91Rb, 91,92,93,94Sr, 92,93,94,95Y, 95,97Zr, 99,101,103Mo, 102,104,105Tc, 103,105,108Ru, 105,107,109Rh, 111,112,113,116Ag, 115,117Cd, 119In, 123,125,127,128,129,130Sn, 127,129,130,131,132,133Sb, 131,132,133,134,135,136I, 131,132,133,134Te, 135,137,138Xe, 138,139,140Cs, 139,140,141,142Ba, 141,143,144,145,146,147,148Ce, 142,144La, 146Pr, 147,149,151Nd, 151,153Pm, 153,155,156Sm, 157,158Eu; deduced mass chain yields of fission products. Comparison with ENDF/B-VIII.0 library.
doi: 10.1140/epja/s10050-021-00485-w
Ann.Nucl.Energy 162, 108493 (2021)
H.Naik, S.P.Dange, R.J.Singh, W.Jang
Post-neutron mass yield distribution in the thermal neutron induced fission of 238Pu
NUCLEAR REACTIONS 238Pu(n, F)83Se/84Se/84Br/85Kr/86Br/87Br/87Kr/88Kr/88Br/88Rb/89Kr/89Rb/90Kr/90Rb/91Rb/91Sr/91Y/92Sr/92Y/93Sr/93Y/94Sr/94Y/95Y/95Zr/97Zr/99Mo/101Mo/102Tc/103Tc/103Ru/104Tc/105Tc/105Ru/107Ru/107Rh/108Ru/109Rh/112Ag/125Sn/127Sn/127Sb/128Sn/128Sb/129Sn/129Sb/130Sn/130Sb/131Sb/131Te/131I/132Sb/132Te/132I/133Sb/133Te/133I/134Te/134I/135I/135Xe/136I/137Xe/138Xe/138Cs/139Xe/139Cs/139Ba/140Cs/140Ba/141Ba/141Ce/142Ba/142La/143Ce/144La/145Ce/146Ce/146Pr/147Nd/148Ce/149Nd/151Nd/151Pm/153Sm/155Sm, E thermal; measured reaction products, Eγ, Iγ; deduced cumulative and independent fission yields, chain yields. Comparison with JEFF-3.3 evaluations, experimental data.
doi: 10.1016/j.anucene.2021.108493
Nucl.Instrum.Methods Phys.Res. B505, 34 (2021)
H.Naik, G.Kim, T.H.Nguyen, K.Kim
Mass yield distribution in the 3 GeV bremsstrahlung induced fission of 232Th
NUCLEAR REACTIONS 232Th(γ, F), E<3 GeV; measured fission products, Eγ, Iγ. 77,78Ge, 84Br, 85,87,88Kr, 89Rb, 91,92Sr, 99,101Mo, 103,105Ru, 104Tc, 105,107Rh, 112,113Ag, 115,117Cd, 127,129,131Sb, 128Sn, 131,133,134,135I, 132,134Te, 138Xe, 138Cs, 139,140,141Ba, 142La, 141,143,146Ce, 146Pr, 147,149Nd, 153Sm; deduced cumulative and mass yields, average excitation energy of compound nucleus, asymmetric or symmetric absolute yields, relative fission yields, σ. Comparison with available data.
doi: 10.1016/j.nimb.2021.08.007
Phys.Rev. C 103, 014608 (2021)
R.Prajapat, M.Maiti, D.Kumar
Fusion-fission events in the 11B + 181Ta reaction up to 5.7 MeV/nucleon energy
NUCLEAR REACTIONS 181Ta(11B, 6n)186Pt, (11B, 5n)187Pt, (11B, 4n)188Pt, (11B, 3n)189Pt, (11B, 5np)186Ir/186mIr, (11B, 4np)187Ir, (11B, 3np)188Ir, (11B, 5nα)183mOs, (11B, F)24Na/34mCl/66Ge/74mBr/83Br/77Kr/87mSr/90Mo/97mRh/103Cd/108In/109In/110mIn/115Ag/123Xe/129Sb/130Sb/131La/137Nd/139mNd/149Nd/160mHo, E=53.5, 54.9, 56.6, 58.7, 59.6, 62.4 MeV; measured activation σ(E) by off-line Eγ, Iγ measurements at 14UD BARC-TIFR Pelletron facility; deduced σ(E) of residues and fission fragments, complete and incomplete fusion evaporation σ(E), isotopic, isobaric and isomeric yields as function of beam energy, isomeric cross-section ratios, preequilibrium (PEQ) reaction strength in 181Ta(11B, 3n)189Pt, and compared with experimental data for other reaction systems. Comparison with theoretical calculations using statistical model codes EMPIRE3.2.2, and PACE4. Comparison of measured isotopic yield distributions for 181Ta, 232Th, 238U(11B, F), 181Ta(16O, F), 169Tm(19F, F), and 238U(22Ne, F). Comparison of measured reduced fusion excitation functions for 159Tb, 181Ta, 209Bi(11B, X), 159Tb, 181Ta(12C, X), and 174,176Yb(16O, X).
doi: 10.1103/PhysRevC.103.014608
Appl.Radiat.Isot. 176, 109826 (2021)
M.Sakaguchi, M.Aikawa, N.Ukon, Y.Komori, H.Haba, N.Otuka, S.Takacs
Activation cross section measurement of alpha-particle induced reactions on natural neodymium
NUCLEAR REACTIONS Nd(α, X)153Sm/145Sm/151Pm/150Pm/149Pm/148Pm/144Pm/143Pm/149Nd/147Nd, E<50 MeV; measured reaction products, Eγ, Iγ; deduced σ and uncertainties. Comparison with available data, EXFOR library, TALYS calculations.
doi: 10.1016/j.apradiso.2021.109826
INDC(NDS)-0833 (2021)
N.J.Stone
Table of Nuclear Electric Quadrupole Moments
COMPILATION Z=1-102; compiled experimental measurements of static electric quadrupole moments of ground states and excited states of atomic nuclei throughout the periodic table.
Chin.Phys.C 45, 030003 (2021)
M.Wang, W.J.Huang, F.G.Kondev, G.Audi, S.Naimi
The AME 2020 atomic mass evaluation (II). Tables, graphs and references
ATOMIC MASSES A=1-295; compiled, evaluated atomic masses, mass excess, β-, ββ and ββββ-decay, binding, neutron and proton separation energies, decay and reaction Q-value data.
Phys.Rev. C 105, 014325 (2022)
R.An, X.Jiang, L.-G.Cao, F.-S.Zhang
Odd-even staggering and shell effects of charge radii for nuclei with even Z from 36 to 38 and from 52 to 62
NUCLEAR STRUCTURE 72,73,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102Kr, 74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90,91,92,93,94,95,96,97,98,99,100,101,102,103,104Sr, 110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150Te, 110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156Xe, 116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162Ba, 126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158Ce, 126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160Nd, 130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165Sm; calculated charge radii and odd-even staggering (OES) effects by the relativistic mean field (RMF-BCS) and the modified RMF(BCS)* approaches; deduced no significant influence of neutron-proton short-range correlations (np-SRCs) for some nuclei due to the strong coupling between different levels around Fermi surface. Comparison with available experimental data.
doi: 10.1103/PhysRevC.105.014325
Nucl.Phys. A1020, 122399 (2022)
G.T.Bholane, T.S.Ganesapandy, A.B.Phatangare, F.M.D.Attar, S.S.Dahiwale, S.V.Suryanarayana, V.N.Bhoraskar, S.D.Dhole
Measurements and estimation of cross sections of neutron and bremsstrahlung induced nuclear reactions for neodymium isotopes with covariance analysis
NUCLEAR REACTIONS 142,148,150Nd(n, 2n), E=14.77 MeV; 142,148,150Nd(γ, n), E=10, 15 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with ENDF/B-VIII.0, JEFF-3.3, JENDL-4.0, CENDL-3.2 and EXFOR libraries, TALYS 1.95 calculations.
doi: 10.1016/j.nuclphysa.2022.122399
Nucl.Sci.Eng. 196, 16 (2022)
H.Naik, S.P.Dange, W.Jang, R.J.Singh
Post-Neutron Mass Yield Distribution in the Epi-Cadmium Neutron-Induced Fission of 237Np
NUCLEAR REACTIONS 237Np(n, F), E ∼ 0.5 eV; measured reaction products, Eγ, Iγ. 78,81As, 80Ge, 83,84Se, 84,86,87Br, 85,87,88,89,90Kr, 88,89,90Rb, 91,92,93,94Sr, 91,93,94,95Y, 95,97Zr, 99,101,103Mo, 102,103,104,105Tc, 103,105,107,108Ru, 105,107,109Rh, 111,112,113Ag, 115,117Cd, 123,125,127,129,130Sn, 127,129,130,131Sb, 131,132,133,134Te, 131,132,133,134,135I, 135,137,139Xe, 138,139,140Cs, 139,140,141,142Ba, 141,143,144,145,146,147Ce, 146Pr, 147,149,151,152Nd, 149,151,153Pm, 153,155,156Sm, 156,157Eu; deduced cumulative or independent fission yields, mass chain yields. Comparison with ENDF/B-VIII.0, available data.
doi: 10.1080/00295639.2021.1951078
Nucl.Sci.Eng. 196, 433 (2022)
H.Naik, R.J.Singh, W.Jang, S.P.Dange
Post-Neutron Mass Yield Distribution in the Thermal Neutron Induced Fission of 232U
NUCLEAR REACTIONS 232U(n, F), E thermal; measured reaction products, Eγ, Iγ. 72,73,74Ga, 77,78Ge, 78As, 81As, 83,84Se, 84Br, 86,87Br, 85Kr, 87,88,89,90Kr, 88,89,90,91Rb, 91,92,93,94Sr, 91,92,93,94,95Y, 99Mo, 101Mo, 101,102,103,104,105,106Tc, 95Zr, 97Zr, 103Ru, 105Rh, 107Rh, 123Sn, 125Sn, 127,128,129,130Sn, 128,129,130,131,132,133Sb, 131,132,133,134Te, 131,132,133,134,135,136I, 135Xe, 137,138,139Xe, 138,139,140Cs, 141Ce, 143Ce, 145,146Ce, 148Ce, 146Pr, 147Nd, 149Nd, 151,152Nd, 151Pm, 153Pm, 153Sm, 155,156Sm, 157,158Eu; measured reaction products, Eγ, Iγ; deduced cumulative and independent yields of various fission products, mass yield distributions. Comparison with available data, EXFOR library. Off-line gamma-ray spectrometric technique. The highly enriched uranium-fueled light water-moderated swimming pool reactor APSARA.
doi: 10.1080/00295639.2021.1993425
Nucl.Sci.Eng. 196, 694 (2022)
H.Naik, R.J.Singh, S.P.Dange, W.Jang
Post-Neutron Mass Yield Distribution in the Epi-Cadmium Neutron-Induced Fission of 243Am
NUCLEAR REACTIONS 243Am(n, F), E∼0.5 eV; measured reaction products, Eγ, Iγ. 83,82Se, 84,86,87Br, 85,87,89Kr, 89,90Rb, 91,92,93,94Sr, 91,82,93,94,95Y, 95,97Zr, 99,101Mo, 102,104,105,106Tc, 103,105,108Ru, 105,107,109Rh, 111,112,113,116Ag, 117Cd, 119In, 123,125,127,128,129,130Sn, 127,128,129,130,131,132,133Sb, 131,132,133,134Te, 131,132,133,134,135,136I, 135,137,138Xe, 138,138,140Cs, 139,140,141,142Ba, 142,144La, 141,143,145,146,148Ce, 146Pr, 147,149,151,152Nd, 151,153Pm, 155,156Sm, 157,158Eu; deduced mass yields, cumulative yields of fission products, the average number of neutrons. Two different reactor facilities in Bhabha Atomic Research Centre (BARC), India.
doi: 10.1080/00295639.2021.2014753
Nucl.Sci.Eng. 196, 824 (2022)
H.Naik, S.P.Dange, R.J.Singh, W.Jang
Post-Neutron Mass Yield Distribution in the Thermal Neutron-Induced Fission of 239Pu
NUCLEAR REACTIONS 239Pu(n, F), E thermal; measured reaction products, Eγ, Iγ. 78,81As, 79,80Ge, 83,84Se, 84,86,87Br, 85,87,88,89,90Kr, 88,89,90,91Rb, 91,92,93,94Sr, 91,92,93,94Y, 95,97Zr, 99,101Mo, 101,102,103,104,105,106Tc, 105,107,108,109Ru, 105,109Rh, 111,113,116Ag, 117Cd, 119In, 123,125,127,128,129,130Sn, 129,130,131Sb, 131,132,133,134Te, 131,132,133,134,135,136I, 135,137,138,139Xe, 139,140,141,142Ba, 142,144La, 141,143,145,146,147Ce, 146Pr, 147,149,151,152Nd, 151,153,154Pm, 153,155,156,157Sm, 158,159Eu; deduced cumulative or independent yields. Comparison with ENDF/B-VIII.0 and JEFF-3.3 libraries. The reactors CIRUS and APSARA at Bhabha Atomic Research Centre (BARC), India.
doi: 10.1080/00295639.2021.2025298
Nucl.Sci.Eng. 196, 982 (2022)
H.Naik, S.P.Dange, W.Jang, R.J.Singh
Post-Neutron Mass Yield Distribution in the Epi-Cadmium Neutron-Induced Fission of 241Am
NUCLEAR REACTIONS 241Am(n, F), E ∼ 0.5 eV; measured reaction products, Eγ, Iγ. 80Ge, 81As, 83,84Se, 84Br, 86,87Br, 85Kr, 87,88,89,90Kr, 89,90,91Rb, 91,92Sr, 91,92,93,94Y, 95Zr, 97Zr, 99,101,103Mo, 102Tc, 104,105,106Tc, 103,105Ru, 108Ru, 105,107,109Rh, 111,113Ag, 116Ag, 115,117Cd, 119In, 123,125,127,129Sn, 130Sn, 129,130,131,132,133Sb, 131,132,133,134Te, 131,132,133,134,135,136I, 135Xe, 137,138,139Xe, 138,139,140Cs, 139,140,141,142Ba, 142,144La, 140,141Ce, 143,144,145,146Ce, 148Ce, 146Pr, 147,149Nd, 151Pm, 153,154Pm, 153Sm, 155,156,157Sm, 157,158Eu, 159,161Gd; deduced cumulative, independent and chain yields. Comparison with evaluated data. Two reactor facilities of Bhabha Atomic Research Centre (BARC) in India.
doi: 10.1080/00295639.2022.2038529
Eur.Phys.J. A 58, 80 (2022)
N.S.Tawade, S.Patra, R.Tripathi, H.Kumawat, T.Patel, P.K.Pujari
Determination of (n, 2n) reaction cross-section for 154Sm, 150Nd and 82Se at 14.6 MeV neutron energy
NUCLEAR REACTIONS 154Sm, 150Nd, 82Se(n, 2n), E=14.6 MeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with ENDF library, TALYS calculations.
doi: 10.1140/epja/s10050-022-00720-y