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NSR database version of April 25, 2024.

Search: Author = N.Zeldes

Found 16 matches.

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2002LI49      Phys.Rev. C66, 024303 (2002)

S.Liran, A.Marinov, N.Zeldes

Applications of semiempirical shell model masses based on a proton magic number Z=126 to heavy and superheavy nuclei

ATOMIC MASSES Pu, Cm, Cf, Fm, No, Rf, Sg, Hs; Z=110-116; calculated Qα. Semiempirical shell model, comparisons with data. Application to analysis of fusion-evaporation results discussed.

doi: 10.1103/PhysRevC.66.024303
Citations: PlumX Metrics


2001LI01      Phys.Rev. C63, 017302 (2001)

S.Liran, A.Marinov, N.Zeldes

Semiempirical Shell Model Masses with Magic Number Z = 126 for Translead Elements with N ≤ 126

ATOMIC MASSES Z=82-118; analyzed masses for nuclei with N ≤ 126; deduced parameters. Semiempirical shell model mass equation.

doi: 10.1103/PhysRevC.63.017302
Citations: PlumX Metrics


2001LI65      Hyperfine Interactions 132, 425 (2001)

S.Liran, A.Marinov, N.Zeldes

Semiempirical Shell Model Masses with Magic Proton Number Z = 126 for Translead Elements

ATOMIC MASSES 293Og, 289Lv, 285Fl, 281Cn, 277Ds, 273Hs, 269Sg; calculated Qα. Semiempirical shell model, comparison with data and other calculations.

NUCLEAR STRUCTURE 293Og, 289Lv, 285Fl, 281Cn, 277Ds, 273Hs, 269Sg; calculated Qα. Semiempirical shell model, comparison with data and other calculations.

doi: 10.1023/A:1011962525421
Citations: PlumX Metrics


2000LI36      Phys.Rev. C62, 047301 (2000)

S.Liran, A.Marinov, N.Zeldes

Semiempirical Shell Model Masses with Magic Number Z = 126 for Superheavy Elements

ATOMIC MASSES Z=88-126; analyzed data; deduced mass formula parameters. 293Og, 289Lv, 285Fl, 281Cn, 277Ds, 273Hs, 269Sg; calculated Qα. Neutron shell effects discussed.

doi: 10.1103/PhysRevC.62.047301
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2000LI47      Acta Phys.Hung.N.S. 12, 143 (2000)

S.Liran, A.Marinov, N.Zeldes

Semiempirical Shell Model Masses with Magic Proton Number Z = 126 for Superheavy Elements

NUCLEAR STRUCTURE 293Og, 289Lv, 285Fl, 281Cn, 277Ds, 273Hs, 269Sg; calculated Qα. Semiempirical shell model equation, comparisons with data, other calculations.

ATOMIC MASSES 293Og, 289Lv, 285Fl, 281Cn, 277Ds, 273Hs, 269Sg; calculated Qα. Semiempirical shell model equation, comparisons with data, other calculations.


1999ZE01      J.Phys.(London) G25, 949 (1999)

N.Zeldes

The Wigner Term in Heavy Nuclei

NUCLEAR STRUCTURE A=72-73; A=207-208; calculated masses; deduced Wigner term contribution.

ATOMIC MASSES A=72-73; A=207-208; calculated masses; deduced Wigner term contribution.

doi: 10.1088/0954-3899/25/4/077
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1999ZE02      Phys.Lett. 455B, 7 (1999)

N.Zeldes

Numbers of Coupled Nucleon Pairs and the Competition between J = 0 and T = 0 Pairs in Odd-Odd Nuclei

NUCLEAR STRUCTURE 6Li, 10B, 14N, 18F, 22Na, 26Al, 30P, 34Cl, 38K, 42Sc, 46V, 50Mn, 54Co, 58Cu, 62Ga, 66As; analyzed data; deduced isovector, isoscalar two-body matrix element features, implications for shell model calcuations.

doi: 10.1016/S0370-2693(99)00414-1
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1998ZE03      Phys.Lett. 429B, 20 (1998)

N.Zeldes

The Physical Origin of the Wigner Term and Its Persistence in Heavy Nuclei

NUCLEAR STRUCTURE A=72, 73, 131, 132, 207, 208; analyzed masses, double beta-decay energies; deduced parameters, persistence of Wigner term.

doi: 10.1016/S0370-2693(98)00458-4
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1997ZE05      Phys.Rev. C56, R2938 (1997)

N.Zeldes

Valence Correlation Scheme for Single Nucleon Separation Energies and the Shell Model

doi: 10.1103/PhysRevC.56.R2938
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1990AS05      Nucl.Phys. A517, 27 (1990)

K.Ashktorab, S.Elitzur, J.Janecke, S.Liran, N.Zeldes

Coulomb Energies and the Shell Model

NUCLEAR STRUCTURE A ≤ 238; analyzed Coulomb displacement energies. Shell model approach.

doi: 10.1016/0375-9474(90)90259-O
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1983ZE02      Nucl.Phys. A399, 11 (1983)

N.Zeldes, T.S.Dumitrescu, H.S.Kohler

Mutual Support of Magicities and Residual Effective Interactions near 208Pb

NUCLEAR STRUCTURE 207,209Pb, 207,209,211,213Bi, 205,207,209,211Tl, 211,209Po, 207,205Hg, 213,211Rn; calculated proton, neutron separation energies, excitations; deduced nucleon magic number role. Shell model, empirical effective interactions. 204,206,208Hg, 206,208,210Pb, 208,210,212Po; calculated binding, single nucleon energies, two-nucleon separation energies. Hartree-Fock, Skyrme-type interactions, effective interaction shell model comparisons.

doi: 10.1016/0375-9474(83)90592-4
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1976LI30      At.Data Nucl.Data Tables 17, 431 (1976)

S.Liran, N.Zeldes

A Semiempirical Shell-Model Formula

NUCLEAR STRUCTURE A=17-297; calculated mass excess, 2-proton and 2-neutron separation energies, alpha Q-value, proton and neutron drip line. Comparison with data.

doi: 10.1016/0092-640X(76)90033-4
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1969LI23      Nucl.Phys. A136, 190 (1969)

S.Liran, N.Zeldes

Adjusted Nuclear Masses for 130 < A < 208

doi: 10.1016/0375-9474(69)90049-9
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1968ZE02      Arkiv Fysik 36, 361 (1968)

N.Zeldes

A Shell Model Approach to Nuclear Masses and Some Problems Connected with Extrapolation


1967ZE05      Kgl.Danske Videnskab.Selskab., Mat.-Fys.Skrifter 3, No.5 (1967)

N.Zeldes, A.Grill, A.Simievic

Shell-Model Semi-Empirical Nuclear Masses (II)


1965ZE02      Nucl.Phys. 63, 1 (1965)

N.Zeldes, M.Gronau, A.Lev

Shell-Model Semi-Empirical Nuclear Masses (I)

doi: 10.1016/0029-5582(65)90851-5
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