References quoted in the ENSDF dataset: 58NI ADOPTED LEVELS, GAMMAS

114 references found.

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

Return to ADOPTED LEVELS, GAMMAS

1959AL95

Izvest.Akad.Nauk SSSR, Ser.Fiz. 23, 223 (1959); Columbia Tech.Transl. 23, 215 (1960)

D.G.Alkhazov, A.P.Grinberg, K.I.Erokhina, I.Kh.Lemberg

Coulomb Excitation of Nuclear Levels in Spherical Even-Even Nuclei

1960AN07

Nuclear Phys. 19, 400 (1960)

D.S.Andreyev, A.P.Grinberg, K.I.Erokhina, I.Kh.Lemberg

Coulomb Excitation of the First Levels of Spherical Even Nuclei by Multiply Charged Ions

NUCLEAR STRUCTURE ²⁸Si, ⁶⁰Ni, ⁵⁸Ni, ⁵⁸Fe, ⁴⁸Ti, ⁴⁶Ti, ⁵⁶Fe, ⁵⁴Cr, ⁶²Ni, ⁶⁴Ni, ⁶⁴Zn, ⁶⁶Zn, ²⁰Ne, ²²Ne, ⁹⁴Zr, ⁷⁶Se, ⁶⁸Zn, ²⁴Mg, ⁹²Zr, ⁷⁸Se, ⁸⁰Se, ⁸²Se; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(60)90251-0

1960GO08

Proc. Conf. Reactions between Complex Nuclei, 2nd, Gatlinburg, A.Zucker, E.C.Halbert, F.T.Howard, Eds., John Wiley and Sons, Inc., New York, p.57 (1960)

H.E.Gove, C.Broude

Coulomb Excitation in Nuclei from A = 23 to A = 60 Using O¹⁶ Ions

NUCLEAR STRUCTURE ⁶⁰Ni, ⁵⁸Ni, ⁵¹V, ⁵⁶Fe, ⁵⁵Mn, ²⁸Si, ²⁴Mg, ²⁷Al, ²³Na; measured not abstracted; deduced nuclear properties.

1961CR01

Phys.Rev. 123, 923 (1961)

H.Crannell, R.Helm, H.Kendall, J.Oeser, M.Yearian

Electron-Scattering Study of Nuclear Levels in Cobalt, Nickel, Lead, and Bismuth

NUCLEAR STRUCTURE ²⁰⁹Bi, ²⁰⁸Pb, ⁵⁸Ni, ⁵⁹Co, ⁶⁰Ni; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.123.923

1962ST02

Nuclear Phys. 32, 652 (1962)

P.H.Stelson, F.K.McGowan

Coulomb Excitation of the First 2⁺ State of Even Nuclei with 58 < A < 82

NUCLEAR STRUCTURE ⁶⁰Ni, ⁵⁸Ni, ^64,66,68Zn, ⁶²Ni, ⁷⁶Ge, ⁷⁶Se, ⁷⁰Ge, ⁷⁰Zn, ⁷⁴Ge, ⁷²Ge, ⁶⁸Zn, ⁸²Se, ⁸⁰Se, ⁷⁸Se; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(62)90368-1

1964BO22

Nucl. Phys. 57, 403 (1964)

E.C.Booth, B.Chasan, K.A.Wright

Nuclear Resonance Fluorescence from Light and Medium Weight Nuclei

NUCLEAR REACTIONS ⁷Li, ¹¹B, ¹⁹F, ^24,25,26Mg, ²⁷Al, ^28,29,30Si, ³¹P, ³²S, ^{46,47,48,49,50}Ti, ⁵¹V, ^50,52,53,54Cr, ⁵⁵Mn, ⁵⁶Fe, ^58,60Ni, ⁵⁹Co, ^63,65Cu(γ, γ), Eγ=0.5 to 3.0 MeV; measured σ. ⁷Li, ¹¹B, ¹⁹F, ^24,25,26Mg, ²⁷Al, ^28,29,30Si, ³¹P, ³²S, ^{46,47,48,49,50}Ti, ⁵¹V, ^50,52,53,54Cr, ⁵⁵Mn, ⁵⁶Fe, ^58,60Ni, ⁵⁹Co, ^63,65Cu deduced level-width.

doi: 10.1016/0029-5582(64)90338-4

1967DU07

Phys.Rev. 163, 1259 (1967)

M.A.Duguay, C.K.Bockelman, T.H.Curtis, R.A.Eisenstein

Inelastic Electron Scattering from Ni⁵⁸, Ni⁶⁰, and Ni⁶²

NUCLEAR REACTIONS ^58,60,62Ni(e, e'), E=40-70 MeV; measured σ(E;Ee'); deduced form factors. ^58,60,62Ni levels deduced B(EL), transition radii.

doi: 10.1103/PhysRev.163.1259

1969AF01

Yadern.Fiz. 10, 33 (1969); Soviet J.Nucl.Phys. 10, 18 (1970)

V.D.Afanasev, N.G.Afanasev, I.S.Gulkarov, G.A.Savitskii, V.M.Khvastunov, N.G.Shevchenko, A.A.Khomich

Electroexcitation of Low Lying Collective States in the Isotopes Ni^58,60,64

NUCLEAR REACTIONS ^58,60,64Ni(e, e), (e, e'), E=150, 225 MeV; measured σ(Ee', θ); deduced elastic, inelastic form factors. ^58,60,64Ni deduced B(E2), B(E3), transition radii, charge distributions.

1969BE48

Phys.Rev. 183, 964 (1969)

M.C.Bertin, N.Benczer-Koller, G.G.Seaman, J.R.MacDonald

Electromagnetic Transition Rates in ⁵⁸Ni

NUCLEAR REACTIONS ^58,60,62Ni(p, p'γ), E = 7-9 MeV; measured Doppler shift attenuation. ^58,60,62Ni deduced levels, T_1/2, matrix elements. Ge(Li) detector.

doi: 10.1103/PhysRev.183.964

1970BA06

Phys.Rev. C1, 207 (1970)

B.Barman Roy, R.Raj, M.L.Rustgi

Nuclear-Structure Calculations for Cr⁵² and Even Ni Isotopes

NUCLEAR STRUCTURE ⁵²Cr, ^58,60,62,64Ni; calculated levels, B(λ).

doi: 10.1103/PhysRevC.1.207

1970JA12

Phys.Lett. 32B, 448 (1970)

A.Jaffrin

Positive Parity Deformed States in ⁵⁶Ni and ⁵⁸Ni

NUCLEAR STRUCTURE ^56,58Ni; calculated positive-parity states. Diagonalization of residual interaction in basis of projected Slater determinants.

doi: 10.1016/0370-2693(70)90379-5

1970LE17

Nucl.Phys. A151, 257 (1970)

P.M.S.Lesser, D.Cline, J.D.Purvis

Static Quadrupole Moments of the First Excited States of ^58,60,62Ni

NUCLEAR REACTIONS Ni(¹²C, ¹²C'γ), E=21-22 MeV; Ni(¹⁶O, ¹⁶O'γ), E=25-30 MeV; Ni(³²S, ³²S'γ), E=60-70 MeV; measured σ(E;Eγ). ^58,60,62Ni levels deduced B(E2), quadrupole moment. Natural targets.

doi: 10.1016/0375-9474(70)90278-2

1970ME18

Nucl.Phys. A158, 88 (1970)

F.R.Metzger

Radiative Widths of Levels in ⁵⁸Ni and ⁶⁰Ni

NUCLEAR REACTIONS ^58,60Ni(γ, γ'), E < 4.5 MeV; measured σ(E, Eγ), nuclear resonances fluorescence. ^58,60Ni deduced levels, level-width, B(M1).

doi: 10.1016/0375-9474(70)90053-9

1970RA34

Nucl.Phys. A158, 65 (1970)

S.Raman

The Decay of 3.2 sec ⁵⁸Cu and an Unusually Hindered E2 Transition in ⁵⁸Ni

RADIOACTIVITY ⁵⁸Cu[from ⁵⁸Ni(p, n)]; measured Eγ, Iγ, γγ-delay; deduced log ft, Iβ. ⁵⁸Ni levels deduced T_1/2, branching ratios. Ge(Li), NE213 detectors.

doi: 10.1016/0375-9474(70)90050-3

1970RU10

Phys.Rev. C2, 2446 (1970)

M.L.Rustgi, B.B.Roy, R.Raj

M1 and E2 Transitions from 1⁺ and 3⁺ States in Even-A Nickel Isotopes

NUCLEAR STRUCTURE ^58,60,62,64Ni; calculated B(M1), B(E2).

doi: 10.1103/PhysRevC.2.2446

1971CHZF

Bull.Amer.Phys.Soc. 16, No.4, 625, JH2 (1971); See keynumber 1971CHZT

J.Charbonneau, N.V.De Castro Faria, J.L'Ecuyer, D.Vitoux

Quadrupole Moments of the First Excited State of ^58,60,62,64Ni

NUCLEAR REACTIONS ^58,60,62,64Ni(¹⁶O, ¹⁶O'), E=30, 32, 34 MeV; measured σ(E(¹⁶O'), θ(¹⁶O')). ^58,60,62,64Ni levels deduced B(E2), quadrupole moment.

1971ST02

Nucl.Phys. A162, 49 (1971)

D.F.H.Start, R.Anderson, L.E.Carlson, A.G.Robertson, M.A.Grace

The Spins and Lifetimes of Some Low-Lying States of ⁵⁸Ni

NUCLEAR REACTIONS ⁵⁸Ni(p, p'γ), E=7.8-8.6 MeV; measured σ(E;Ep', Eγ, θ(p'γ), θ(γγ)), p'γ-delay, ICC, p'γγ-triple correlation, Doppler-shift attenuation. ⁵⁸Ni deduced levels, branching ratios, J, γ-mixing, π, T_1/2, ICC. Enriched target.

doi: 10.1016/0375-9474(71)90485-4

1972ARZD

Thesis, Univ.Boston (1972); Diss.Abst.Int. 33B, 1723 (1972)

R.G.Arnold

Nuclear Resonance Fluorescence with Bremsstrahlung

NUCLEAR REACTIONS ^63,65Cu, ^64,66,68Zn, ⁵⁹Co, ^58,60Ni, ⁸⁹Y, ⁵⁵Mn, ²⁵Mg, ²⁸Si, ⁴⁵Sc, ^71,69Ga, ¹¹B, ²⁷Al, ³²S, ³¹P, ²³Na, ¹⁹F, ³⁵Cl(γ, γ), E not given; measured nuclear resonance fluorescence. ¹⁹F, ³⁵Cl, ²³Na, ¹¹B, ²⁷Al, ³²S, ³¹P, ²⁵Mg, ²⁸Si, ⁴⁵Sc, ^69,71Ga, ⁵⁹Co, ^58,60Ni, ⁸⁹Y, ⁵⁵Mn, ^63,65Cu, ^66,68Zn deduced levels, level-width, γ-mixing.

1972BA55

Phys.Rev.Lett. 29, 230 (1972)

P.D.Barnes, R.A.Einstein, W.C.Lam, J.Miller, R.B.Sutton, M.Eckhause, J.Kane, R.E.Welsh, D.A.Jenkins, R.J.Powers, R.Kunselman, R.P.Redwine, R.E.Segel, J.P.Schiffer

Nuclear γ Rays Associated with Stopped Kaons

NUCLEAR REACTIONS Al, Si, Cu, Ni(K^-, γ), measured Eγ, Iγ. ⁵⁰Cr, ^55,56,58Fe, ⁴⁶Ti, ⁵²Cr, ^58,60,62,63Ni, ^63,65Cu, ^57,59Co deduced transitions.

doi: 10.1103/PhysRevLett.29.230

1972GL05

Nucl.Phys. A198, 609 (1972)

P.W.M.Glaudemans, M.J.A.de Voigt, E.F.M.Steffens

Shell-Model Calculations on the Nickel Isotopes

NUCLEAR STRUCTURE ^{57,58,59,60,62,61,63,64,65,66}Ni; calculated levels, B(λ), quadrupole moment, binding energies. Shell model.

doi: 10.1016/0375-9474(72)90712-9

1972OB02

Nucl.Phys. A191, 577 (1972)

G.Oberlechner, J.Richert

Shell-Model Study of ⁵⁶Ni, ⁵⁸Ni, ⁵⁴Fe and ⁵⁶Fe

NUCLEAR STRUCTURE ^56,58Ni, ^54,56Fe; calculated levels. Shell model.

doi: 10.1016/0375-9474(72)90633-1

1973BEYD

Thesis, Vrije Univ., Amsterdam (1973)

W.Beens

Lifetimes of Excited States in Nuclei with Mass Number Around A = 88 by Means of the Doppler Shift Attenuation Method

NUCLEAR REACTIONS ⁵⁸Ni(p, p'γ), E=8 MeV; ⁸⁹Y(p, p'γ), E=8, 14.4, 17 MeV; ⁹⁰Zr(p, p'γ), E=7 MeV; measured DSA, p'γ-coin; ⁸⁹Y(α, 2nγ), E=17.3-19.8 MeV; ⁸⁹Y(p, 2nγ), E=14, 15, 15.2, 17.0 MeV; measured Eγ, Iγ. ⁵⁸Ni, ⁹⁰Zr levels deduced T_1/2. ⁸⁹Y, ⁹¹Nb, ⁸⁸Zr levels deduced T_1/2, B(λ), γ-branching ratios.

1974LE13

Nucl.Phys. A223, 563 (1974)

P.M.S.Lesser, D.Cline, C.Kalbach-Cline, A.Bahnsen

Reorientation Measurements in the Even Nickel Isotopes

NUCLEAR REACTIONS ^58,60Ni(³²S, ³²S'γ), E=70 MeV; measured ³²S'γ(θ). ^58,60Ni levels deduced quadrupole moment.

doi: 10.1016/0375-9474(74)90706-4

1974PA13

Phys.Rev. C10, 2568 (1974)

J.K.Parikh

Projected Band-Mixed Spectra of Fe and Ni Isotopes

NUCLEAR STRUCTURE ^54,56,58Fe, ^58,60,62Ni calculated energy levels. Projected Hartree-Fock method, band mixing.

doi: 10.1103/PhysRevC.10.2568

1975VA08

Z.Phys. A274, 51 (1975)

G.Vanden Berghe

Interplay of Valence-Shell Clusters and the Vibrational Field in ⁵⁸Ni

NUCLEAR STRUCTURE ⁵⁸Ni; calculated levels, B(λ), quadrupole moment, δ, γ-branching, T_1/2.

1977KO02

Z.Phys. A280, 181 (1977)

J.E.Koops, P.W.M.Glaudemans

Shell-Model Calculations on Ni and Cu Isotopes

NUCLEAR STRUCTURE ^{57,58,59,60,61,62,63,64,65,66,67}Ni, ^{58,59,60,61,62,63,64,65,66,67,68}Cu; calculated levels, S, binding energies.

1978HA13

Phys.Rev. C17, 997 (1978)

M.Hass, N.Benczer-Koller, J.M.Brennan, H.T.King, P.Goode

Magnetic Moments of the 2⁺₁ States of Even Ni Isotopes

NUCLEAR REACTIONS ^58,60,62,64Ni(³²S, ³²S'), E=72 MeV; measured γγ(θ, H). ^58,60,62,64Ni levels deduced Q. Enriched targets.

doi: 10.1103/PhysRevC.17.997

1979VA19

Z.Phys. A293, 327 (1979)

A.G.M.van Hees, P.W.M.Glaudemans, B.C.Metsch

The Influence of f₇/₂ Hole Configurations on Properties of ^57-59Ni

NUCLEAR STRUCTURE ^57,58,59Ni; calculated energy levels, B(λ), S, μ, quadrupole moment. Shell model, surface delta interactions.

1981CA10

J.Phys.(London) G7, 1539 (1981)

Y.Cauchois, H.Ben Abdelaziz, R.Kherouf, C.Schloesing-Moller

Etude de Niveaux Nucleaires d'Isotopes Naturels, par Resonance ou Fluorescence, avec Rayonnement X de Freinage

NUCLEAR REACTIONS ²⁴Mg, ²⁷Al, ⁴⁸Ti, ^58,61,62Ni, ^63,65Cu, ^64,66,68Zn, ⁷⁵As, ¹⁰³Rh, ⁵⁹Co, ^113,115In, ^116,118,120Sn, ^121,123Sb(γ, γ'), E ≈ 0.5-1.65 MeV bremsstrahlung; measured γ(θ), self absorption, absolute γ-transition strength. ²⁴Mg, ²⁷Al, ⁴⁸Ti, ⁵⁹Co, ^58,61,62Ni, ^63,65Cu, ^64,66,68Zn, ⁷⁵As, ¹⁰³Rh, ^113,115In, ^116,118,120Sn, ^121,123Sb levels deduced T_1/2. Nuclear resonance fluorescence technique.

doi: 10.1088/0305-4616/7/11/013

1982BE20

Lett.Nuovo Cim. 33, 273 (1982)

E.Bellotti, E.Fiorini, C.Liguori, A.Pullia, A.Sarracino, L.Zanotti

An Experimental Investigation on Lepton Number Conservation in Double-Beta Processes.

RADIOACTIVITY Nd, Mo, Ge; measured Eγ, Iγ; deduced no evidence for neutrinoless process, right handed current fraction limits. ^148,150Nd, ^92,100Mo deduced limit on double β-decay T_1/2. ⁷⁶Ge deduced limit on neutrinoless double β-decay T_1/2.

1983KL09

Nuovo Cim. 76A, 369 (1983)

R.Klein, P.Grabmayr, Y.Kawazoe, G.J.Wagner, J.Friedrich, N.Voegler

Distribution of Electric Multipole Strengths in ⁵⁸Ni

NUCLEAR REACTIONS ⁵⁸Ni(e, e'), E=124, 180 MeV; measured σ(E(e')), σ(θ). ⁵⁸Ni levels deduced B(λ), EWSR strength. DWBA form factors, Tassie transition densities.

1984NO09

Phys.Lett. 148B, 31 (1984)

E.B.Norman, M.A.DeFaccio

Searches for Double β⁺, β⁺/EC and Double Electron-Capture Decays

RADIOACTIVITY ⁵⁸Ni, ¹⁰⁶Cd(2β⁺), (2EC), (β⁺), (EC); measured summed γ spectra; deduced T_1/2 lower limits.

doi: 10.1016/0370-2693(84)91604-6

1986HO15

Nucl.Phys. A454, 237 (1986)

K.Hosono, M.Fujiwara, H.Ikegami, M.Kondo, N.Matsuoka, T.Saito, T.Yamazaki, S.Matsuki, K.Ogino, S.Kato, T.Yanagihara

Excitation of M1 States in ⁵⁸Ni and ⁶⁰Ni by 65 MeV Polarized Proton Inelastic Scattering

NUCLEAR REACTIONS ⁵⁸Ni, ⁶⁰Ni(polarized p, p'), E=65 MeV; measured σ(θ), analyzing power A(θ). ⁵⁸Ni, ⁶⁰Ni levels deduced M1 character. Microscopic DWBA analysis.

doi: 10.1016/0375-9474(86)90267-8

1987FEZX

ORNL-6326, p.32 (1987)

M.A.G.Fernandes, F.E.Bertrand, D.J.Horen, J.L.Blankenship, B.L.Burks, R.O.Sayer, G.R.Satchler, D.Shapira, R.L.Auble, C.W.Glover

Elastic and Inelastic Scattering of ¹²C and ⁵⁸Ni at 300 MeV

NUCLEAR REACTIONS ⁵⁸Ni(¹²C, ¹²C), (¹²C, ¹²C'), E=300 MeV; measured σ(θ); deduced model parameters. ⁵⁸Ni levels deduced deformation, B(λ).

1987KA50

Yad.Fiz. 46, 1623 (1987)

D.K.Kaipov, R.N.Kasymbalinov

Description of the 2⁺, 3^-, and 5^- States in Nickel Isotopes

NUCLEAR STRUCTURE ^58,60,62,64Ni; calculated charge transition densities, B(λ). Finite Fermi systems.

1989GE09

Fiz.Elem.Chastits At.Yadra 20, 930 (1989); Sov.J.Part.Nucl. 20, 393 (1989)

M.K.Georgieva, D.V.Elenkov, D.P.Lefterov, G.H.Toumbev

Measurement of the Lifetimes of Excited Nuclear States by the Doppler Shift Attenuation Method Using the Reaction (n, n'γ) with Two Targets

NUCLEAR REACTIONS ¹¹B, ²³Na, ²⁴Mg, ²⁷Al, ²⁸Si, ³¹P, ³²S, ^35,37Cl, ³⁹K, ⁴⁰Ca, ⁴⁵Sc, ⁴⁸Ti, ⁵¹V, ⁵²Cr, ⁵⁵Mn, ⁵⁶Fe, ^58,60,64Ni(n, n'γ), E=fast; measured γ-spectra, DSA. ¹¹B, ²³Na, ²⁴Mg, ²⁷Al, ²⁸Si, ³¹P, ³²S, ^35,37Cl, ³⁹K, ⁴⁰Ca, ⁴⁵Sc, ⁴⁸Ti, ⁵¹V, ⁵²Cr, ⁵⁵Mn, ⁵⁶Fe, ^58,60,64Ni level deduced T_1/2, B(λ).

1989NA11

Phys.Rev. C40, 1237 (1989)

A.Nadasen, M.McMaster, M.Fingal, J.Tavormina, J.S.Winfield, R.M.Ronningen, P.Schwandt, F.D.Becchetti, J.W.Janecke, R.E.Warner

Inelastic Scattering of 210 MeV ⁶Li Ions from ¹²C, ²⁸Si, and ⁵⁸Ni: Test of unique ⁶Li potentials

NUCLEAR REACTIONS ¹²C, ²⁸Si, ⁵⁸Ni(⁶Li, ⁶Li'), E=210 MeV; measured σ(θ). ¹²C, ²⁸Si, ⁵⁸Ni level deduced deformation length, quadrupole moments. DWBA, coupled-channels analyses.

doi: 10.1103/PhysRevC.40.1237

1989OA01

Phys.Rev. C40, 859 (1989)

D.S.Oakley, M.R.Braunstein, J.J.Kraushaar, R.A.Loveman, R.J.Peterson, D.J.Rilett, R.L.Boudrie

Isospin Asymmetries in Pion Scattering to Isoscalar Giant Quadrupole States in Ni Isotopes

NUCLEAR REACTIONS ^58,60,62,64Ni(π⁺, π⁺'), (π^-, π^-'), E=180 MeV; measured σ(θ), σ(E(π')). ^58,60,62,64Ni deduced giant quadrupole resonance neutron, proton matrix elements, B(λ).

doi: 10.1103/PhysRevC.40.859

1989RA17

At.Data Nucl.Data Tables 42, 189 (1989)

P.Raghavan

Table of Nuclear Moments

COMPILATION Z=1-99; compiled μ, electric quadrupole moments.

doi: 10.1016/0092-640X(89)90008-9

1990GA07

Phys.Rev. C41, 1845 (1990)

U.Garg, K.B.Beard, D.Ye, A.Galonsky, T.Murakami, J.S.Winfield, Y.-W.Lui, D.H.Youngblood

Experimental Test of a Newly Proposed Empirical Relationship between the Centroid and Width of the Giant Quadrupole Resonance and the Neutron Binding Energy of the Nucleus

NUCLEAR REACTIONS ^58,64Ni(¹⁴N, ¹⁴N'), E=700 MeV; measured σ(E(¹⁴N)). ^58,64Ni deduced GDR parameters.

doi: 10.1103/PhysRevC.41.1845

1990KU08

Nucl.Phys. A514, 589 (1990)

R.Kunselman, J.D.Zumbro, E.B.Shera, M.V.Hoehn

Pionic-Atom 3d2p X-Ray Measurements in ^54,56Fe, ⁵⁹Co, and ^{58,60,61,62,64}Ni

ATOMIC PHYSICS, Mesic-Atoms ^54,56Fe, ⁵⁹Co, ^{58,60,61,62,64}Ni; measured 3d-2p pionic X-rays, isotope shifts, strong-interaction shifts, widths.

NUCLEAR MOMENTS ^54,56Fe, ⁵⁹Co, ^{58,60,61,62,64}Ni; measured 3d-2p pionic X-rays, isotope shifts, strong-interaction shifts, widths.

doi: 10.1016/0375-9474(90)90011-A

1991RA22

Phys.Rev. C44, 2484 (1991)

Md.A.Rahman, H.M.Sen Gupta, M.Rahman

Strong Absorption Model for Pion-Nucleus Scattering Around the (3, 3) Resonance

NUCLEAR REACTIONS ¹⁸O, ^24,26Mg, ^56,54Fe, ^48,50Ti, ^40,44Ca, ⁵²Cr(π⁺, π⁺), (π^-, π^-), E=180 MeV; ¹⁸O(π⁺, π⁺), (π^-, π^-), E=164, 230 MeV; ^40,48,44Ca(π⁺, π⁺), (π^-, π^-), E=116 MeV; ²⁸Si, ⁵⁸Ni, ²⁰⁸Pb(π⁺, π⁺), (π^-, π^-), E=162 MeV; ^40,42,44,48Ca, ⁵⁴Fe(π⁺, π⁺), (π^-, π^-), E=292.5 MeV; analyzed σ(θ); deduced model parameters. ^24,26Mg, ^42,44,48Ca, ⁴⁸Ti, ^54,56Fe, ¹⁸O, ^24,26Mg, ²⁸Si, ⁵⁸Ni, ⁵²Cr levels deduced β₂. Strong absorption model.

doi: 10.1103/PhysRevC.44.2484

1992DU08

Bull.Rus.Acad.Sci.Phys. 56, 453 (1992)

L.V.Dubar, D.Sh.Eleukenov, O.F.Nemets, L.I.Slyusarenko, V.V.Tokarevsky, N.P.Yurkuts

On Mean-Square Radii of Matter Distribution in Nuclei

NUCLEAR STRUCTURE ^52,54,50Cr, ^54,56,58Fe, ^58,60,64Ni, ^124,116Sn, ⁶⁴Zn, ⁵⁰Ti; analyzed data; deduced matter rms radii differences. Data on (α, X) reaction input.

1993INZZ

Cyclotron Rad.Center, Tohoku Univ., Ann.Rept., 1992, p.16 (1993)

T.Inomata, T.Tohei, T.Nakagawa, A.Terakawa, A.Narita, T.Matsumoto, H.Orihara, K.Ishii, M.Hosaka, S.Miyamoto, Z.Guan, Y.Ishimaru, K.Miura, H.Ohnuma

The ^58,60Ni(d, n)^59,61Cu Reactions at 25 MeV

NUCLEAR REACTIONS ^58,60Ni(d, n), E=25 MeV; measured En, σ(θ). ^59,61Cu levels deduced C²S. ^58,60Ni deduced occupation probabilities of proton orbits. Tof.

1993VA19

Pisma Zh.Eksp.Teor.Fiz. 57, 614 (1993); JETP Lett.(USSR) 57, 631 (1993)

S.I.Vasilev, A.A.Klimenko, S.B.Osetrov, A.A.Pomansky, A.A.Smolnikov

Experimental Search for the Decay of ⁵⁸Ni Nuclei by the e^-e⁺-Conversion Channel

RADIOACTIVITY ⁵⁸Ni; measured e^-e⁺ conversion channel T_1/2 lower limit. Two-Crystal γ-ray spectrometer.

1994ME24

Nucl.Instrum.Methods Phys.Res. A350, 491 (1994)

D.J.Mercer, D.Mikolas, J.Yurkon, S.M.Austin, D.Bazin, S.Gaff, E.Kashy, D.Kataria, J.S.Winfield, R.R.Betts, D.J.Henderson, A.L.Hallin, M.Liu, F.L.H.Wolfs

A Large Solid-Angle Array for Heavy Ions from APEX

NUCLEAR REACTIONS ⁵⁸Ni(⁵⁸Ni, ⁵⁸Ni), E=200 MeV; measured σ(θ). ¹⁸¹Ta(²³⁸U, X), E=1.45 GeV; measured fragment tof, mass spectra. Large solid-angle array of low pressure multi-wire proportional counters. Other reactions studied.

doi: 10.1016/0168-9002(94)91249-1

1994SA33

Nuovo Cim. 107A, 511 (1994)

D.R.Sarker, Md.A.Rahman, M.Rahman, H.S.Sen Gupta

The ⁶Li-Nucleus Scattering

NUCLEAR REACTIONS ¹²C(⁶Li, ⁶Li), E=28-210 MeV; ⁴⁴Ca, ^24,25,26Mg, ²⁷Al, ^58,60Ni, ²⁰⁸Pb(⁶Li, ⁶Li), ⁶⁰Ni, ^24,26Mg(⁶Li, ⁶Li'), E=88 MeV; ²⁸Si(⁶Li, ⁶Li), E=46-210 MeV; ⁴⁰Ca(⁶Li, ⁶Li), E=50.6-210 MeV; ⁹⁰Zr, ²⁰⁸Pb(⁶Li, ⁶Li), E=99, 210 MeV; ¹²C, ²⁸Si, ⁵⁸Ni(⁶Li, ⁶Li'), E=210 MeV; analyzed σ(θ). ¹²C, ^24,26Mg, ²⁸Si, ^58,60Ni deduced deformation parameter β₂. Strong absorption model.

1995DE06

Phys.Rev. C51, 1356 (1995)

P.R.Dee, C.O.Blyth, H.D.Choi, N.M.Clarke, S.J.Hall, O.Karban, I.Martel-Bravo, S.Roman, G.Tungate, R.P.Ward, N.J.Davis, D.B.Steski, K.A.Connell, K.Rusek

Coupled-Channels Analysis of the Elastic Scattering of Polarized ⁶Li by ⁵⁸Ni Using Cluster-Folding Potentials

NUCLEAR REACTIONS ⁵⁸Ni(polarized ⁷Li, ⁷Li), E=70.5 MeV; measured σ(θ), iT₁₁(θ), other analyzing powers vs θ; deduced scattering mechanism, spin-dependent potentials, ⁶Li D-state roles. Coupled-channels approach, cluster-folding method.

doi: 10.1103/PhysRevC.51.1356

1996LA04

Phys.Rev. C53, 1167 (1996)

C.M.Laymon, W.Amos, M.G.Burlein, H.T.Fortune, T.Ekenberg, A.Kotwal, J.M.O'Donnell, J.D.Silk, J.D.Zumbro, C.L.Morris, S.J.Seestrom, K.S.Dhuga, R.Garnett, M.W.Rawool-Sullivan, C.F.Moore, S.L.Morris, D.L.Watson

Pion Elastic and Inelastic 2⁺₁ Scattering on ^58,60,62,64Ni at T(π) = 180 MeV

NUCLEAR REACTIONS ^58,60,62,64Ni(π⁺, π⁺), (π⁺, π⁺'), (π^-, π^-), (π^-, π^-'), E=180 MeV; measured σ(θ); deduced nucleon radii, deformation parameters. ^58,60,62,64Ni levels deduced neutron, proton matrix elements.

doi: 10.1103/PhysRevC.53.1167

1996VA10

Z.Phys. A355, 41 (1996)

L.Vannucci, U.Abbondanno, M.Bettiolo, M.Bruno, N.Cindro, M.D'Agostino, P.M.Milazzo, R.A.Ricci, T.Ritz, W.Scheid, G.Vannini

Evidence of Non-Statistical Structures in the Elastic and Inelastic Scattering of ⁵⁸Ni + ⁵⁸Ni and ⁵⁸Ni + ⁶²Ni and Intermediate Dinuclear States

NUCLEAR REACTIONS ⁶²Ni(⁵⁸Ni, ⁵⁸Ni), (⁵⁸Ni, ⁵⁸Ni'), E=220-230 MeV; ⁵⁸Ni(⁵⁸Ni, ⁵⁸Ni), (⁵⁸Ni, ⁵⁸Ni'), E=220-240 MeV; measured spectra, σ(θ) vs E; deduced nonstatistical structures evidence.

doi: 10.1007/s002180050076

1997SI13

Phys.Rev. C55, 3155 (1997)

C.P.Silva, D.Pereira, L.C.Chamon, E.S.Rossi, Jr., G.Ramirez, A.M.Borges, C.E.Aguiar

Fusion and Peripheral Processes in the ^16,18O + ^58,60,64Ni Systems

NUCLEAR REACTIONS, ICPND ^58,60,64Ni(¹⁶O, X), (¹⁸O, X), E=38-64 MeV; measured fusion σ(E). ⁵⁸Ni(¹⁸O, ¹⁸O), E=35.1-55.1 MeV; measured fusion σ(E), σ(θ); deduced fusion barriers, standard radius deviation, reaction mechanism.

doi: 10.1103/PhysRevC.55.3155

1998PA39

Phys.Lett. 442B, 7 (1998)

F.Pan, J.P.Draayer

New Algebraic Approach for an Exact Solution of the Nuclear Mean-Field plus Orbit-Dependent Pairing Hamiltonian

NUCLEAR STRUCTURE ^{58,59,60,61,62,63,64,65,66,67}Ni; calculated levels, J, π, spectroscopic factors. Orbit-dependent pairing, exact solution. Comparison with data, other models.

doi: 10.1016/S0370-2693(98)01259-3

1998PA43

Pramana 51, 433 (1998)

H.S.Patel, B.Srinivasan, B.J.Roy, M.G.Betigeri

Investigation of Two- and Three-Nucleon Transfer Reactions in ¹²C + ⁵⁶Fe

NUCLEAR REACTIONS ⁵⁶Fe(¹²C, ¹²C), (¹²C, ¹⁰Be), (¹²C, ⁹Be), E=60 MeV; measured σ(E), σ(θ); deduced spectroscopic factors, transfer probabilities, reaction mechanism.

1999GU02

Nucl.Phys. A646, 161 (1999)

D.Gupta, C.Samanta, R.Kanungo, M.K.Sharan, S.Kailas, A.Chatterjee, K.Mahata, A.Shrivastava

Measurement of 42 MeV ⁷Li Projectile Breakup on ⁵⁸Ni Target Beyond Grazing Incidence

NUCLEAR REACTIONS ⁵⁸Ni(⁷Li, ⁷Li), E=42 MeV; measured σ(θ). ⁵⁸Ni(⁷Li, X), E=42 MeV; measured particle spectra. ⁵⁸Ni(⁷Li, tα), E=42 MeV; measured Eα, Et, σ(θ(α), θ(t), Eα); deduced sequential breakup contribution.

doi: 10.1016/S0375-9474(98)00635-6

1999HA21

J.Phys.(London) G25, 867 (1999)

M.K.Harder, P.Halse, L.Frankland

Shell-Model Calculations Near N = Z = 28

NUCLEAR STRUCTURE ^53,54,55Co, ^52,53Fe, ^55,58Ni, ⁶⁰Zn; calculated levels, J, π. ⁵⁵Ni, ⁵⁵Co deduced high-K isomers. Shell model. Comparison with data.

doi: 10.1088/0954-3899/25/4/057

2000BA63

Phys.Rev. C62, 024302 (2000)

F.Bauwens, J.Bryssinck, D.De Frenne, K.Govaert, L.Govor, M.Hagemann, J.Heyse, E.Jacobs, W.Mondelaers, V.Yu.Ponomarev

Dipole Transitions to Bound States in ⁵⁶Fe and ⁵⁸Ni

NUCLEAR REACTIONS ⁵⁶Fe, ⁵⁸Ni(γ, γ'), E=6.5, 10 MeV bremsstrahlung; ⁵⁶Fe, ⁵⁸Ni(polarized γ, γ'), E=12 MeV bremsstrahlung; measured Eγ, Iγ. ⁵⁶Fe, ⁵⁸Ni deduced levels, J, π, widths, dipole transition strength distributions. Nuclear resonance fluorescence. Quasiparticle phonon model calculations.

doi: 10.1103/PhysRevC.62.024302

2000GU17

J.Phys.(London) G26, L81 (2000)

D.Gupta, C.Samanta, A.Chatterjee, K.Rusek, Y.Hirabayashi

Channel Coupling Effects in Resonant Breakup of 42 MeV ⁷Li with ⁵⁸Ni Target

NUCLEAR REACTIONS ⁵⁸Ni(⁷Li, ⁷Li'), E=42 MeV; measured σ(θ) for elastic scattering and sequential α + t breakup of projectile. Comparison with coupled channel calculations.

doi: 10.1088/0954-3899/26/6/102

2000SC11

Eur.Phys.J. A 7, 367 (2000)

K.Schwarz, C.Samanta, M.Fujiwara, H.Rebel, R.De Leo, N.Matsuoka, H.Utsunomiya, H.Akimune, I.Daito, H.Fujimura, F.Ihara, K.Ishibashi, Y.Maeda, T.Yamanaka, H.Yoshida, A.Okihana, T.Yoshimura, P.K.J.van Aarle, W.A.T.Uijen, M.Ito, Y.Sakuragi

Reaction Mechanism of ⁶Li Scattering at 600 MeV

NUCLEAR REACTIONS ¹²C, ⁵⁸Ni, ⁹⁰Zr, ²⁰⁸Pb(⁶Li, ⁶Li), (⁶Li, dα), E= 600 MeV; measured elastic and breakup σ(θ), particle spectra. Comparison with theoretical calculations.

doi: 10.1007/PL00013619

2000SU19

Phys.Rev. C62, 044605 (2000)

E.Sh.Sukhovitsky, Y.-O.Lee, J.Chang, S.Chiba, O.Iwamoto

Nucleon Interaction with ⁵⁸Ni up to 150 MeV Studied in the Coupled-Channels Approach Based on the Soft-Rotator Nuclear Structure Model

NUCLEAR STRUCTURE ⁵⁸Ni; calculated levels, J, π. Soft-rotator model. Comparison with data.

NUCLEAR REACTIONS ⁵⁸Ni(n, n), E < 150 MeV; calculated σ. ⁵⁸Ni(n, n), (n, n'), (p, p), (p, p'), E=5-65 MeV; calculated σ(E, θ). Coupled channels method. Comparisons with data.

doi: 10.1103/PhysRevC.62.044605

2000VA28

Acta Phys.Hung.N.S. 11, 319 (2000)

L.Vannucci, U.Abbondanno, A.Bologna, M.Bruno, N.Cindro, M.D'Agostino, P.M.Milazzo, R.A.Ricci, W.Scheid, G.Vannini

Statistical Analysis Methods in the Search of Resonances in Low-Energy Heavy-Ion Reactions

NUCLEAR REACTIONS ⁵⁸Ni(⁴⁶Ti, ⁴⁶Ti'), (⁵⁸Ni, ⁵⁸Ni'), (⁶²Ni, ⁶²Ni'), E(cm)=96.9-116.5 MeV; measured elastic, inelastic σ(θ, E); deduced resonance and reaction mechanism features. Statistical analysis.

2001KE02

Phys.Rev. C63, 021302 (2001)

O.Kenn, K.-H.Speidel, R.Ernst, J.Gerber, N.Benczer-Koller, G.Kumbartzki, P.Maier-Komor, F.Nowacki

Striking Harmony between the Nuclear Shell Model and New Experimental g Factors and B(E2) Values of Even Ni Isotopes

NUCLEAR REACTIONS ¹²C(⁵⁸Ni, ⁵⁸Ni'), (⁶⁰Ni, ⁶⁰Ni'), (⁶²Ni, ⁶²Ni'), (⁶⁴Ni, ⁶⁴Ni'), E=155, 160 MeV; measured Eγ, (¹²C)γ-coin following Coulomb excitation and Ni orientation in cooled, magnetized foil. ^58,60,62,64Ni deduced first 2+ T_1/2, B(E2), g-factors. Transient magnetic field technique, comparison with Shell Model calculations.

doi: 10.1103/PhysRevC.63.021302

2001KE08

Phys.Rev. C63, 064306 (2001)

O.Kenn, K.-H.Speidel, R.Ernst, J.Gerber, P.Maier-Komor, F.Nowacki

Measurements of g Factors and Lifetimes of Low Lying States in ^58-64 Ni and Their Shell Model Implications

NUCLEAR REACTIONS Ta(⁵⁸Ni, ⁵⁸Ni'), (⁶⁰Ni, ⁶⁰Ni'), (⁶²Ni, ⁶²Ni'), (⁶⁴Ni, ⁶⁴Ni'), E=155, 160 MeV; measured Eγ, Iγ(θ, H, t), DSA following projectile Coulomb excitation. ^58,60,62,64Ni levels deduced T_1/2, g factors, B(E2). Transient field technique. Comparisons with previous results, model predictions.

doi: 10.1103/PhysRevC.63.064306

2001RA27

At.Data Nucl.Data Tables 78, 1 (2001)

S.Raman, C.W.Nestor, P.Tikkanen

Transition Probability from the Ground to the First-Excited 2⁺ State of Even-Even Nuclides

COMPILATION Z=4-100; compiled, evaluated B(E2) for transition from ground to first-excited 2⁺ states in even-even nuclides.

doi: 10.1006/adnd.2001.0858

2001RU03

Phys.Rev.Lett. 86, 1450 (2001)

D.Rudolph, C.Baktash, M.Devlin, D.R.LaFosse, L.L.Riedinger, D.G.Sarantites, C.-H.Yu

Prompt α Decay of a Well-Deformed Band in ⁵⁸Ni

NUCLEAR REACTIONS ²⁸Si(³⁶Ar, 2pα), E=143 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin. ⁵⁸Ni deduced high-spin levels, J, π, configurations, α-decay from excited band. Gammasphere, Microball arrays.

doi: 10.1103/PhysRevLett.86.1450

2002BE86

Bull.Rus.Acad.Sci.Phys. 65, 1696 (2002)

O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, B.S.Ishkhanov, E.A.Romanovsky, T.I.Spasskaya

Calculation of Single-Particle Characteristics of Proton Levels in ⁵⁸Ni Nucleus within Dispersion Optical Model

NUCLEAR STRUCTURE ⁵⁸Ni; calculated single-particle level energies. Dispersion optical model, comparison with previous results.

2002FU07

Eur.Phys.J. A 13, 411 (2002)

Y.Fujita, H.Fujita, T.Adachi, G.P.A.Berg, E.Caurier, H.Fujimura, K.Hara, K.Hatanaka, Z.Janas, J.Kamiya, T.Kawabata, K.Langanke, G.Martinez-Pinedo, T.Noro, E.Roeckl, Y.Shimbara, T.Shinada, S.Y.van der Werf, M.Yoshifuku, M.Yosoi, R.G.T.Zegers

Gamow-Teller Transitions from ⁵⁸Ni to Discrete States of ⁵⁸Cu the Study of Isospin Symmetry in Atomic Nuclei

NUCLEAR REACTIONS ⁵⁸Ni(³He, t), E=150 MeV/nucleon; measured triton spectra, σ(θ=0°). ⁵⁸Cu deduced levels, Gamow-Teller strength distribution. ⁵⁸Ni deduced excitation B(M1). Comparison with shell model.

doi: 10.1007/s10050-002-8771-8

2002GA16

Phys.Rev. C65, 044314 (2002)

L.R.Gasques, L.C.Chamon, C.P.Silva, D.Pereira, M.A.G.Alvarez, E.S.Rossi, Jr., V.P.Likhachev, B.V.Carlson, C.De Conti

Determination of the ¹²C Nuclear Density Through Heavy-Ion Elastic Scattering Experiments

NUCLEAR REACTIONS ⁵⁸Ni(¹²C, ¹²C), E=26-28.5 MeV; ²⁰⁸Pb(¹²C, ¹²C), E=54.5-57 MeV; measured σ(θ); deduced potential features. ¹²C deduced nucleon density distribution. Comparisons with other reactions and with model predictions.

doi: 10.1103/PhysRevC.65.044314

2002HO08

Phys.Rev. C65, 061301 (2002)

M.Honma, T.Otsuka, B.A.Brown, T.Mizusaki

Effective Interaction for pf-Shell Nuclei

NUCLEAR STRUCTURE Ca, Ti, Cr, Fe, Ni; calculated 2⁺ energy levels, single-particle energies. ^{56,57,58,59,61,63,65}Ni; calculated levels, J, π. Unified effective interaction, comparisons with data.

doi: 10.1103/PhysRevC.65.061301

2002KI06

At.Data Nucl.Data Tables 80, 35 (2002)

T.Kibedi, R.H.Spear

Reduced Electric-Octupole Transition Probabilities, B(E3;0₁⁺ → 3₁^-) - An Update

COMPILATION Z=4-98; compiled transitions B(E3), octupole deformation parameters.

doi: 10.1006/adnd.2001.0871

2003AU03

Nucl.Phys. A729, 337 (2003)

G.Audi, A.H.Wapstra, C.Thibault

The AME2003 atomic mass Evaluation (II). Tables, graphs, and references

COMPILATION A=1-293; compiled, evaluated atomic mass data.

doi: 10.1016/j.nuclphysa.2003.11.003

2003GA04

Phys.Rev. C 67, 024602 (2003)

L.R.Gasques, L.C.Chamon, D.Pereira, V.Guimaraes, A.Lepine-Szily, M.A.G.Alvarez, E.S.Rossi, Jr., C.P.Silva, B.V.Carlson, J.J.Kolata, L.Lamm, D.Peterson, P.Santi, S.Vincent, P.A.De Young, G.Peasley

Experimental determination of the surface density for the ⁶He exotic nucleus

NUCLEAR REACTIONS ⁵⁸Ni(α, α), (⁶He, ⁶He), E=8.1, 9.0, 9.1, 9.6 MeV; measured σ(θ). ⁵⁸Ni(α, α), E=82-288 MeV; analyzed σ(θ). ^4,6He deduced ground-state nuclear densities. Unfolding method, comparison with model predictions.

doi: 10.1103/PhysRevC.67.024602

2003GA18

Phys.Rev. C 67, 067603 (2003)

L.R.Gasques, L.C.Chamon, D.Pereira, M.A.G.Alvarez, E.S.Rossi, Jr., C.P.Silva, G.P.A.Nobre, B.V.Carlson

Systematical study of the optical potential for systems like A+⁵⁸Ni from sub-barrier data analyses

NUCLEAR REACTIONS ⁵⁸Ni(²⁸Si, ²⁸Si), E=74, 75.5, 77 MeV; measured σ(θ); deduced optical model parameters. ²⁸Si deduced density distribution.

NUCLEAR STRUCTURE ^4,6He, ¹²C, ^16,18O, ²⁸Si; analyzed scattering data; deduced radii, density distributions.

doi: 10.1103/PhysRevC.67.067603

2004AN14

At.Data Nucl.Data Tables 87, 185 (2004)

I.Angeli

A consistent set of nuclear rms charge radii: properties of the radius surface R(N, Z)

COMPILATION A=1-248; compiled, analyzed charge radii.

doi: 10.1016/j.adt.2004.04.002

2004HO08

Phys.Rev. C 69, 034335 (2004)

M.Honma, T.Otsuka, B.A.Brown, T.Mizusaki

New effective interaction for pf-shell nuclei and its implications for the stability of the N = Z = 28 closed core

NUCLEAR STRUCTURE ⁵³Mn, ⁵⁴Fe, ^54,55Co, ^56,57,58,59Ni, ⁵⁸Cu; calculated levels, J, π, B(M1), B(E2). Shell model, new effective interaction, comparison with data.

NUCLEAR MOMENTS ^47,49Ca, ⁴⁷Sc, ^47,48,49,50Ti, ^48,49,50,51V, ^{49,50,51,52,53,54}Cr, ^{51,52,53,54,55,56}Mn, ^{53,54,55,56,57,58,59}Fe, ^{55,56,57,58,59,60}Co, ^{57,58,59,60,61,62,63,64,65,67}Ni, ^{60,61,62,63,64,65,66}Cu, ^{62,63,64,65,66,67,68,70}Zn, ^{66,67,68,69,71}Ga, ^69,70,71,72Ge; calculated μ, quadrupole moments. Comparison with data.

doi: 10.1103/PhysRevC.69.034335

2004LI64

Phys.Rev. C 70, 044314 (2004)

A.F.Lisetskiy, B.A.Brown, M.Horoi, H.Grawe

New T=1 effective interactions for the f_5/2 p_3/2 p_1/2 g_9/2 model space: Implications for valence-mirror symmetry and seniority isomers

NUCLEAR STRUCTURE ^{58,60,62,64,66,68,70,72,74,76}Ni, ⁸⁰Zn, ⁸²Ge, ⁸⁴Se, ⁸⁶Kr, ⁸⁸Sr, ⁹⁰Zr, ⁹²Mo, ⁹⁴Ru, ⁹⁶Pd, ⁹⁸Cd; calculated level energies. ^70,72,74,76Ni, ⁹²Mo, ⁹⁴Ru, ⁹⁶Pd, ⁹⁸Cd; calculated transitions B(E2). New T=1 effective interactions. Comparisons with data.

doi: 10.1103/PhysRevC.70.044314

2004VA38

Braz.J.Phys. 34, 837 (2004)

J.P.Valencia, H.C.Wu

Pseudo-SU(4) Model and Beta Decay of pf-shell Nuclei

NUCLEAR STRUCTURE ^58,59,60Ni, ^58,59,60Cu, ^58,59,60Zn; calculated levels, J, π. Pseudo-SU(4) model.

RADIOACTIVITY ^58,59Cu, ^58,59Zn(EC); calculated log ft. Pseudo-SU(4) model.

2004YU10

Phys.Rev. C 70, 054319 (2004)

K.L.Yurkewicz, D.Bazin, B.A.Brown, C.M.Campbell, J.A.Church, D.C.Dinca, A.Gade, T.Glasmacher, M.Honma, T.Mizusaki, W.F.Mueller, H.Olliver, T.Otsuka, L.A.Riley, J.R.Terry

Nuclear structure in the vicinity of N=Z=28 ⁵⁶Ni

NUCLEAR REACTIONS ¹⁹⁷Au(⁵⁸Ni, ⁵⁸Ni'), E=77.8 MeV/nucleon; ¹⁹⁷Au(⁵⁶Ni, ⁵⁶Ni'), E=85.8 MeV/nucleon; ¹⁹⁷Au(⁵⁴Ni, ⁵⁴Ni'), E=70.3 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. ^54,56,58Ni levels deduced excitation B(E2). Comparison with model predictions.

doi: 10.1103/PhysRevC.70.054319

2005KI02

At.Data Nucl.Data Tables 89, 77 (2005)

T.Kibedi, R.H.Spear

Electric monopole transitions between 0⁺ states for nuclei throughout the periodic table

COMPILATION A=4-250; compiled, analyzed 0⁺ → 0⁺ transition energies, T_1/2, ICC, electric monopole transition strengths.

doi: 10.1016/j.adt.2004.11.002

2005NIZS

Thesis, Univ. Heidelberg, Germany (2005)

O.T.Niedermaier

Low-Energy Coulomb Excitation of the Neutron-Rich Mg Isotopes ³⁰Mg and ³²Mg

NUCLEAR REACTIONS Ni(²²Ne, ²²Ne'), E=2.25 MeV/nucleon; ¹⁰⁷Ag(²²Ne, ²²Ne'), E=2.86 MeV/nucleon; Ni(³⁰Mg, ³⁰Mg'), E=2.25 MeV/nucleon; ⁶⁰Ni, ¹⁰⁷Ag(³⁰Mg, ³⁰Mg'), E=2.69 MeV/nucleon; U(p, X)²²Ne/³⁰Mg/³²Mg, E=1.01-1.40 GeV; measured Eγ, Iγ(θ), (particle)γ-coinc, cross sections following projectile and target Coulomb excitation. ²²Ne, ³⁰Mg, ³²Mg, ¹⁰⁷Ag deduced levels, B(E2), half-lives, deformations. REX-ISOLDE-CERN facility. Coupled-channel and GOSIA analyses. ²⁴Mg, ²⁶Mg, ²⁸Mg, ³⁰Mg, ³²Mg, ³⁴Mg systematics of B(E2) values. Comparisons with shell-model calculations.

2005RU06

Nucl.Phys. A752, 241c (2005)

D.Rudolph, E.K.Johansson, L.-L.Andersson, J.Ekman, C.Fahlander, R.du Rietz

Exotic Decay Modes in Rotating Nuclei

NUCLEAR STRUCTURE ⁵⁸Ni; analyzed proton spectra, angular distributions following prompt decay of rotational band states.

NUCLEAR REACTIONS ²⁴Mg(⁴⁰Ca, 2np), (⁴⁰Ca, 2n), E=104 MeV; measured Eγ, Iγ, γγ-, (recoil)γ-coin. ⁶¹Ga, ⁶²Ge deduced levels, transitions.

doi: 10.1016/j.nuclphysa.2005.02.083

2005ST24

At.Data Nucl.Data Tables 90, 75 (2005)

N.J.Stone

Table of nuclear magnetic dipole and electric quadrupole moments

NUCLEAR MOMENTS Z=0-99; A=1-255; compiled μ, electric quadrupole moments.

COMPILATION Z=0-99; A=1-255; compiled μ, electric quadrupole moments.

doi: 10.1016/j.adt.2005.04.001

2006AN27

Phys.Rev. C 74, 054313 (2006)

A.Ansari, P.Ring

Lowest lying 2⁺ and 3^- vibrational states in Pb, Sn, and Ni isotopes in relativistic quasiparticle random-phase approximation

NUCLEAR STRUCTURE ^{56,58,60,62,64,66,68,70,72,74,76,78,80}Ni, ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134}Sn, ^{194,196,198,200,202,204,206,208,210,212,214}Pb; calculated vibrational states level energies, B(E2), B(E3). Relativistic quasiparticle RPA.

doi: 10.1103/PhysRevC.74.054313

2006RU02

Phys.Rev.Lett. 96, 092501 (2006)

D.Rudolph, B.G.Carlsson, I.Ragnarsson, S.Aberg, C.Andreoiu, M.A.Bentley, M.P.Carpenter, R.J.Charity, R.M.Clark, M.Cromaz, J.Ekman, C.Fahlander, P.Fallon, E.Ideguchi, A.O.Macchiavelli, M.N.Mineva, W.Reviol, D.G.Sarantites, D.Seweryniak, S.J.Williams

⁵⁸Ni: An Unpaired Band Crossing at New Heights of Angular Momentum for Rotating Nuclei

NUCLEAR REACTIONS ²⁸Si(³²S, 2p), E=130 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin. ⁵⁸Ni deduced high-spin levels, J, π, configurations, unpaired band crossing. Gammasphere, Microball arrays.

doi: 10.1103/PhysRevLett.96.092501

2006VA21

Braz.J.Phys. 36, 1275 (2006)

J.P.Valencia, H.C.Wu

Pseudo-Orbital SO(6) Symmetry for pf-Shell Nuclei

NUCLEAR STRUCTURE ⁵⁸Ni, ⁵⁸Cu, ⁵⁸Zn; calculated level energies and beta-decay transion matrix elements using the pseudo-orbital SO(6) symmetry. Compared results to available data.

2007BE25

Bull.Rus.Acad.Sci.Phys. 71, 438 (2007); Izv.Akad.Nauk RAS, Ser.Fiz. 71, 451 (2007)

O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, B.S.Ishkhanov, E.A.Romanovskii, T.I.Spasskaya, T.P.Timokhina

On Double Magicity of the ⁶⁸₂₈Ni₄₀ Nucleus

NUCLEAR STRUCTURE ^58,60,62,64Ni; analyzed single-particle energies. ⁶⁸Ni; deduced estimate for single-particle energies. Compared with dispersive optical model results.

doi: 10.3103/S1062873807030276

2007FU04

Phys.Rev. C 75, 034310 (2007)

H.Fujita, Y.Fujita, T.Adachi, A.D.Bacher, G.P.A.Berg, T.Black, E.Caurier, C.C.Foster, H.Fujimura, K.Hara, K.Harada, K.Hatanaka, J.Janecke, J.Kamiya, Y.Kanzaki, K.Katori, T.Kawabata, K.Langanke, G.Martinez-Pinedo, T.Noro, D.A.Roberts, H.Sakaguchi, Y.Shimbara, T.Shinada, E.J.Stephenson, H.Ueno, T.Yamanaka, M.Yoshifuku, M.Yosoi

Isospin structure of J^π = 1⁺ states in ⁵⁸Ni and ⁵⁸Cu studied by ⁵⁸Ni(p, p') and ⁵⁸Ni(³He, t)⁵⁸Cu measurements

NUCLEAR REACTIONS ⁵⁸Ni(p, p'), E=160 MeV; measured Ep, σ(θ=0°). ⁵⁸Ni(³He, t), E=140 MeV/nucleon; measured triton spectra, σ(θ=0°). ⁵⁸Ni, ⁵⁸Cu deduced 1⁺ level energies, B(GT), isospin symmetry features. Comparison with shell model predictions.

doi: 10.1103/PhysRevC.75.034310

2007HI06

Phys.Rev. C 76, 014617 (2007)

D.J.Hinde, R.L.Ahlefeldt, R.G.Thomas, K.Hagino, M.L.Brown, M.Dasgupta, M.Evers, L.R.Gasques, M.D.Rodriguez

Probing the tail of the nuclear potential between identical nuclei with quasi-elastic Mott scattering

NUCLEAR REACTIONS ⁵⁸Ni(⁵⁸Ni, ⁵⁸Ni), E=260=220 MeV; measured angular distributions. Deduced Mott oscillations.

doi: 10.1103/PhysRevC.76.014617

2007LE07

Phys.Lett. B 647, 82 (2007)

H.Lenske, P.Kienle

Probing matter radii of neutron-rich nuclei by antiproton scattering

NUCLEAR REACTIONS ^{48,50,52,54,56,58,60,62,64,66,68,70,72,74,76,78,80,82,84,86,88}Ni(p-bar, X), E=50, 100, 200, 300, 400 MeV; calculated absorption σ. Microscopic optical potential.

NUCLEAR STRUCTURE ^{48,50,52,54,56,58,60,62,64,66,68,70,72,74,76,78,80,82,84,86,88}Ni; calculated radii. Microscopic optical potential.

doi: 10.1016/j.physletb.2007.02.009

2007LI55

Nucl.Phys. A789, 103 (2007)

X.Li, C.Liang, C.Cai

Global triton optical model potential

NUCLEAR REACTIONS ^6,7Li, ⁹Be, ^12,13C, ¹⁶O, ¹⁹F, ^24,26Mg, ²⁷Al, ^27,28Si, ³²S, ^40,48Ca, ^46,48Ti, ⁵¹V, ⁵²Cr, ^54,56Fe, ^58,60,62,64Ni, ⁶⁸Zn, ⁸²Se, ⁸⁷Rb, ⁸⁶Sr, ⁸⁹Y, ^90,92,94,96Zr, ^{112,116,118,120,122,124}Sn, ¹⁴⁰Ce, ¹⁸⁷W, ^207,208Pb, ²³²Th(t, t'), E < 40 MeV; analyzed elastic scattering σ and angular distribution data to obtain a set of global optical model potential parameters. Compared results to other calculations.

doi: 10.1016/j.nuclphysa.2007.03.004

2007LI72

Chinese Physics 16, 3624 (2007)

J.-J.Liu, Z.-Q.Luo

Neutrino energy loss by electron capture on strongly screened iron group nuclei

RADIOACTIVITY ^{52,53,54,55,56,57,58,59,60,61}Fe, ^{55,56,57,58,59,60}Co, ^{56,57,58,59,60,61,62,63}Ni, ^{53,54,55,56,57,58,59,60}Cr, ^{55,56,57,58,59,60,61,62}Mn, ^47,48,49,50V(EC); calculated neutrino energy loss by electron capture using a new strong screening potential derived from the linear response theory; analyzed neutrino energy loss rates in the absence and presence of strong electron screening.

doi: 10.1088/1009-1963/16/12/012

2007LO10

Phys.Rev. C 76, 034314 (2007)

W.Long, H.Sagawa, N.Van Giai, J.Meng

Shell structure and ρ-tensor correlations in density dependent relativistic Hartree-Fock theory

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ^56,58,68,72Ni, ⁹⁰Zr, ^116,124,132Sn, ¹⁴⁰Ce, ¹⁴⁶Gd, ^{182,194,204,208,214}Pb, ²¹⁰Po; calculated binding energies, charge radii, and spin orbit splittings using density dependent HF theory and a new effective interaction.

doi: 10.1103/PhysRevC.76.034314

2007LU01

J.Phys.(London) G34, 513 (2007)

J.Lubian, F.M.Nunes

Searching for a polarization potential in the breakup of ⁸B

NUCLEAR REACTIONS ⁵⁸Ni(⁸B, p⁷Be), E=30 MeV; calculated σ(θ), polarization potential; deduced non-local continuum couplings.

doi: 10.1088/0954-3899/34/3/009

2007MU19

Phys.Rev. C 76, 064611 (2007)

D.Mulhall, Z.Huard, V.Zelevinsky

Ergodicity of the Δ₃ statistic and purity of neutron resonance data

NUCLEAR STRUCTURE ⁵⁰Cr, ⁵⁴Fe, ⁵⁸Ni, ¹⁵²Sm, ^152,154,158Gd, ¹⁸²W, ^234,236U, ^240,242Pu; calculated Δ₃(L), level densities, resonances, fluctuations of number of levels as a function of length of the spectral interval.

doi: 10.1103/PhysRevC.76.064611

2007OZ03

Phys.Rev. C 75, 064307 (2007)

C.Ozen, K.Langanke, G.Martinez-Pinedo, D.J.Dean

Parity-projected shell model Monte Carlo level densities for fp-shell nuclei

NUCLEAR STRUCTURE ^58,62,65,66Fe, ^58,59Ni; calculated level densities, occupation numbers and pairing strength for neutrons using shell model monte carlo method.

doi: 10.1103/PhysRevC.75.064307

2007SA53

Phys.Rev. C 76, 044322 (2007)

P.Sarriguren, M.K.Gaidarov, E.Moya de Guerra, A.N.Antonov

Nuclear skin emergence in Skyrme deformed Hartree-Fock calculations

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136}Sn, ^{48,50,52,54,56,58,60,62,64,66,68,70,72,74,76,78}Ni, ^{70,72,74,76,78,80,82,84,86,88,90,92,94,96,98,100}Kr; calculated charge density, matter density, rms radii for even isotopes. Used Skyrme-deformed Hartree-Fock+BCS calculations.

doi: 10.1103/PhysRevC.76.044322

2007SV01

Nucl.Phys. A786, 31 (2007)

K.D.Sviratcheva, J.P.Draayer, J.P.Vary

Global properties of fp-shell interactions in many-nucleon systems

NUCLEAR STRUCTURE ⁵⁸Ni, ⁵⁸Cu; calculated levels, J, π. Effective interactions compared using spectral distribution theory.

doi: 10.1016/j.nuclphysa.2007.01.087

2008AG11

Phys.Atomic Nuclei 71, 1163 (2008)

E.F.Aguilera, E.Martinez-Quiroz, T.L.Belyaeva, J.J.Kolata, R.Leyte-Gonzalez

New measurements on breakup of ⁸B + ⁵⁸Ni at energies around the Coulomb barrier

NUCLEAR REACTIONS ⁵⁸Ni(⁸B, p⁷Be), E=25.0, 26.9, 28.4 MeV; measured light fragments energy spectra, single angle excitation function, σ(θ); Comparison with CDCC calculation.

doi: 10.1134/S1063778808070065

2008BAZX

Proc.Nuclear Physics and Astrophysics: From Stable Beams to Exotic Nuclei, Cappadocia, Turkey, June 25-30, 2008, I.Boztosun, A.B.Balantekin, Eds., p.82 (2008); AIP Conf. Proc. 1072 (2008)

A.B.Balantekin, N.Guven, Y.Pehlivan

An Exactly Solvable Supersymmetric Model of Semimagic Nuclei

NUCLEAR STRUCTURE ^58,62Ni; calculated J, π, eigenstates energies.

doi: 10.1063/1.3039869

2008BI04

Nucl.Phys. A802, 67 (2008)

M.Biswas, S.Roy, M.Sinha, M.K.Pradhan, A.Mukherjee, P.Basu, H.Majumdar, K.Ramachandran, A.Shrivastava

The study of threshold behaviour of effective potential for ⁶Li + ^{58, 64}Ni systems

NUCLEAR REACTIONS ⁶⁴Ni(⁶Li, ⁶Li), E=13?26 MeV; measured σ(θ); ⁵⁸Ni(⁶Li, ⁶Li), E=12?20 MeV; analyzed σ(θ). Double folding optical model, threshold behaviour.

doi: 10.1016/j.nuclphysa.2008.01.025

2008KU01

Nucl.Phys. A798, 1 (2008); Erratum Nucl.Phys. A831, 137 (2009)

A.Kumar, H.Singh, R.Kumar, I.M.Govil, R.P.Singh, R.Kumar, B.K.Yogi, K.S.Golda, S.K.Datta, G.Viesti

Pre-compound neutron evaporation in low energy heavy ion fusion reactions

NUCLEAR REACTIONS ⁴⁶Ti(¹²C, X)⁵⁸Ni, E=80 MeV; ²⁷Al(³¹P, X)⁵⁸Ni, E=131 MeV; measured inclusive and exclusive neutron evaporation spectra, Eγ, Iγ, nγ-coin. ^53,55Fe, ⁵⁶Co deduced average excitation energy and angular momenta. Comparison with statistical model calculations.

doi: 10.1016/j.nuclphysa.2007.10.007

2008MA17

Phys.Rev. C 77, 054309 (2008)

J.Margueron, H.Sagawa, K.Hagino

Effective pairing interactions with isospin density dependence

NUCLEAR STRUCTURE ^{36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53,54,55,56,57,58,59,60,61,62}Ca, ^{52,53,54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74,75,76,77,78,79,80,81,82,83,84,85,86,87,88,89,90}Ni, ^{100,101,102,103,104,105,106,107,108,109,110,111,112,113,114,115,116,117,118,119,120,121,122,123,124,125,126,127,128,129,130,131,132,133,134,135,136,137,138,139,140,141,142,143,144,145,146,147,148,149,150,151,152,153,154,155,156,157,158,159,160,161,162,163,164,165,166,167,168,169,170}Sn, ^{182,183,184,185,186,187,188,189,190,191,192,193,194,195,196,197,198,199,200,201,202,203,204,205,206,207,208,209,210,211,212,213,214,215,216,217,218,219,220,221,222,223,224,225,226,227,228,229,230,231,232,233,234,235,236,237,238,239,240,241,242,243,244,245,246,247,248,249,250,251,252,253,254,255,256,257,258,259,260,261,262,263,264,265,266,267}Pb; calculated odd-even mass staggering, binding energies, two-neutron separation energies, pairing gaps. Comparison with experimental data. ^110,150Sn; calculated particle densities, neutron Fermi momentum. Hartree-Fock-Bogoliubov model.

doi: 10.1103/PhysRevC.77.054309

2008OR02

Phys.Rev. C 77, 064301 (2008)

J.N.Orce, B.Crider, S.Mukhopadhyay, E.Peters, E.Elhami, M.Scheck, B.Singh, M.T.McEllistrem, S.W.Yates

Determination of the 2⁺₁ → 0⁺₁ transition strengths in ⁵⁸Ni and ⁶⁰Ni

NUCLEAR REACTIONS ^58,60Ni(n, n'γ)E=1.6, 1.8 MeV; measured Eγ, Iγ, half-life of 2⁺ states. ⁵⁸Ni, ⁶⁰Ni; deduced B(E2) values. Doppler shift attenuation method. ^{56,62,64,66,68}Ni; calculated lifetimes, B(E2).

doi: 10.1103/PhysRevC.77.064301

2008TE03

Phys.Rev. C 77, 024317 (2008)

S.Terashima, H.Sakaguchi, H.Takeda, T.Ishikawa, M.Itoh, T.Kawabata, T.Murakami, M.Uchida, Y.Yasuda, M.Yosoi, J.Zenihiro, H.P.Yoshida, T.Noro, T.Ishida, S.Asaji, T.Yonemura

Proton elastic scattering from tin isotopes at 295 MeV and systematic change of neutron density distributions

NUCLEAR REACTIONS ^{116,118,120,122,124}Sn(p, p), E=295 MeV; measured σ(θ), analyzing powers, nucleon density distributions, rms radii. ⁵⁸Ni; calculated proton, neutron density distributions.

doi: 10.1103/PhysRevC.77.024317

2008US02

Phys.Rev. C 77, 034312 (2008)

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

Core nucleus polarization in Λ hypernuclei

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

doi: 10.1103/PhysRevC.77.034312

2009AG02

Phys.Rev. C 79, 021601 (2009)

E.F.Aguilera, E.Martinez-Quiroz, D.Lizcano, A.Gomez-Camacho, J.J.Kolata, L.O.Lamm, V.Guimaraes, R.Lichtenthaler, O.Camargo, F.D.Becchetti, H.Jiang, P.A.DeYoung, P.J.Mears, T.L.Belyaeva

Reaction cross sections for ⁸B, ⁷Be, and ⁶Li+⁵⁸Ni near the Coulomb barrier: Proton-halo effects

NUCLEAR REACTIONS ⁵⁸Ni(⁶Li, ⁶Li), E=9.9, 11.2, 12.1, 13.0, 14.0 MeV; ⁵⁸Ni(⁷Be, ⁷Be), E=15.1, 17.1, 18.5, 19.9, 21.4 MeV; ⁵⁸Ni(⁸B, ⁸B), E=20.7, 23.4, 25.3, 27.2, 29.3 MeV; measured σ, angular distributions; deduced total reaction and breakup cross section for (⁸B, ⁸B) reaction, and proton halo effects for ⁸B. Comparison with optical-model calculations.

doi: 10.1103/PhysRevC.79.021601

2009AUZZ

Priv.Comm. (2009)

G.Audi, W.Meng, D.Lunney, B.Pfeiffer

Atomic Mass Evaluation 2009

2009BE24

Bull.Rus.Acad.Sci.Phys. 73, 820 (2009); Izv.Akad.Nauk RAS, Ser.Fiz 73, 867 (2009)

O.V.Bespalova, I.N.Boboshin, V.V.Varlamov, T.A.Ermakova, B.S.Ishkhanov, S.Yu.Komarov, H.Koura, E.A.Romanovskii, T.I.Spasskaya

Energies of the single-particle proton 1f and 2p states in the ^{58, 60, 62, 64}Ni isotopes

NUCLEAR STRUCTURE ^58,60,62,64Ni; calculated energies of single-particle states; deduced importance of proton dispersive optical potential (dop). Comparison with experiment.

doi: 10.3103/S1062873809060264

2009CA14

Phys.Rev. C 79, 054329 (2009)

L.Capelli, G.Colo, J.Li

Dielectric theorem within the Hartree-Fock-Bogoliubov framework

NUCLEAR STRUCTURE ^{40,42,44,46,48,50,52,54,56,58,60,62,64,66,68,70,72,74,76}Ca, ^{56,58,60,62,64,66,68,70,72,74,76,78,80,82,84}Ni; calculated constrained monopole energies, monopole inverse energy-weighted sum rule (IEWSR), isoscalar 0⁺ strength functions, proton and neutron transition densities. Quasiparticle random phase approximation (QRPA) calculations based on Hartree-Fock-Bogoliubov (HFB) with SKM* and volume pairing forces.

doi: 10.1103/PhysRevC.79.054329

2009JO03

Phys.Rev. C 80, 014321 (2009)

E.K.Johansson, D.Rudolph, I.Ragnarsson, L.-L.Andersson, D.A.Torres, C.Andreoiu, C.Baktash, M.P.Carpenter, R.J.Charity, C.J.Chiara, J.Ekman, C.Fahlander, O.L.Pechenaya, W.Reviol, R.du Rietz, D.G.Sarantites, D.Seweryniak, L.G.Sobotka, C.H.Yu, S.Zhu

Thorough γ-ray and particle decay investigations of ⁵⁸Ni

NUCLEAR REACTIONS ²⁸Si(³⁶Ar, 2pα), E=136, 143, 148 MeV; measured Eγ, Iγ, Ep, Ip, Eα, (particle)γ-, nγ-, pγ-, αγ-, γγ-coin, γγ(θ), DCO. ⁵⁸Ni; deduced levels, J, π, multipolarity, mixing ratio, bands and configurations. ⁵⁷Co, ⁵⁴Fe; deduced levels, J, π from prompt proton and α emission from ⁵⁸Ni high-spin states. Comparison with large-scale shell model and cranked Nilsson-Strutinsky calculations.

doi: 10.1103/PhysRevC.80.014321

2009KU25

Phys.Rev. C 80, 054602 (2009)

Y.Kucuk, I.Boztosun, T.Topel

Global optical potential for the elastic scattering of ⁶He at low energies

NUCLEAR REACTIONS ¹²C(⁶He, ⁶He), E=8.79, 9.18, 18.0 MeV; ²⁷Al(⁶He, ⁶He), E=9.5, 11.0, 12.0, 13.4 MeV; ⁵⁸Ni(⁶He, ⁶He), E=9.0 MeV; ⁶⁴Zn(⁶He, ⁶He), E=10.0 MeV; ⁶⁵Cu(⁶He, ⁶He), E=22.6 MeV; ¹⁹⁷Au(⁶He, ⁶He), E=27.0, 29, 40.0 MeV; ²⁰⁸Pb(⁶He, ⁶He), E=14.0, 16.0, 18.0, 22.0, 27.0 MeV; ²⁰⁹Bi(⁶He, ⁶He), E=14.7, 16.3, 17.8, 19.0, 22.5 MeV; analyzed elastic scattering σ and angular distributions using optical model analysis; deduced global optical model potential parameters. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.054602

2009OG04

J.Phys.Soc.Jpn. 78, 084201 (2009)

K.Ogata, T.Matsumoto, Y.Iseri, M.Yahiro

Properties of Nuclear and Coulomb Breakup of ⁸B

NUCLEAR REACTIONS ¹²C, ¹⁶O, ⁴⁰Ca, ⁵⁸Ni, ⁹⁰Zr, ¹⁵²Sm, ²⁰⁸Pb(⁸B, p⁷Be), E=65 MeV/nucleon; calculated dependence of breakup σ on target mass; deduced nuclear-Coulomb interference. Continuum-discretized coupled-channels (CDCC) method.

doi: 10.1143/JPSJ.78.084201

2009PA07

Phys.Rev. C 79, 024615 (2009); Erratum Phys.Rev. C 81, 019902 (2010)

D.Y.Pang, P.Roussel-Chomaz, H.Savajols, R.L.Varner, R.Wolski

Global optical model potential for A = 3 projectiles

NUCLEAR REACTIONS ⁶Li, ²⁷Al, ²⁸Si, ³²S, ⁴⁶Ti, ⁴⁸Ti, ⁵⁶Fe, ⁶⁸Zn(t, t), E=17 MeV; ⁹Be, ⁶⁰Ni, ¹⁴⁰Ce(t, t), E=15, 17 MeV; ¹²C(t, t), E=15, 17, 20, 33, 36, 38 MeV; ¹³C(t, t), E=38 MeV; ¹⁴C(t, t), E=71.7 MeV; ¹⁶O(t, t), E=33, 36 MeV; ¹⁹F, ⁴⁸Ca, ⁵¹V, ⁸⁹Y(t, t), E=33 MeV; ²⁰Ne, ²²Ne(t, t), E=33.4 MeV; ²⁴Mg(t, t), E=15, 33.4 MeV; ²⁶Mg, ³⁰Si(t, t), E=17, 36 MeV; ⁴⁰Ca(t, t), E=17, 20, 33 MeV; ⁵²Cr, ⁶²Ni(t, t), E=15, 20 MeV; ⁵⁸Ni, ²³²Th(t, t), E=17, 33 MeV; ⁶⁴Ni(t, t), E=20 MeV; ⁸²Se, ⁸⁶Sr, ⁸⁷Rb(t, t), E=15 MeV; ⁹⁰Zr(t, t), E=15, 17, 20 MeV; ⁹⁴Zr, ¹¹⁶Sn(t, t), E=17, 20 MeV; ⁹⁶Zr, ¹¹⁸Sn, ¹²²Sn, ¹²⁴Sn, ¹⁸²W, ²⁰⁷Pb(t, t), E=20 MeV; ²⁰⁸Pb(t, t), E=20, 33 MeV; ⁶Li(³He, ³He), E=8-217 MeV; ⁹Be(³He, ³He), E=4-217 MeV; ¹²C(³He, ³He), E=11-217 MeV; ¹³C(³He, ³He), E=450 MeV; ²⁴Mg(³He, ³He), E=12-130 MeV; ²⁷Al(³He, ³He), E=5.5-118.5 MeV; ²⁸Si(³He, ³He), E=450 MeV; ⁴⁰Ca(³He, ³He), E=8.5-130, 31.0-217, 450 MeV; ⁵⁸Ni(³He, ³He), E=12-217, 450 MeV; ⁶⁴Ni(³He, ³He), E=21-118.5 MeV; ⁹⁰Zr(³He, ³He), E=12-217, 450 MeV; ¹¹⁶Sn(³He, ³He), E=18-109.2 MeV; ¹²⁰Sn(³He, ³He), E=130 MeV; ²⁰⁸Pb(³He, ³He), E=33.3-217, 450 MeV; analyzed σ(θ) using global optical model potential GDP08; deduced set of global optical potential parameters.

2009ZH25

Int.J.Mod.Phys. E18, 1761 (2009)

S.S.Zhang

Pairing correlations with resonant continuum effect in the RMF + ACCC + BCS approach

NUCLEAR STRUCTURE ^{58,60,62,64,66,68,70,72,74,76,78,80,82,84,86,88,90,92,94,96,98}Ni; calculated binding, two-neutron separation energies, pairing correlation energies, neutron rms radii, neutron density distributions, occupation probabilities. RMF+ACCC+BCS approach, comparison with experiment.

doi: 10.1142/S0218301309013828

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.