References quoted in the ENSDF dataset: 100SN ADOPTED LEVELS

228 references found.

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

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1990AL07

Z.Phys. A335, 265 (1990)

D.Alber, H.H.Bertschat, H.Grawe, H.Haas, B.Spellmeyer, X.Sun

First In-Beam Observation of ⁹⁷Ag - The Three-Proton-Hole Spectrum in ¹⁰⁰Sn

NUCLEAR REACTIONS ⁴⁶Ti(⁵⁸Ni, 2npα), (⁵⁸Ni, n2pα), (⁵⁸Ni, 2n3pα), E=230 MeV; ⁶⁴Zn(³⁶Ar, 2np), E=130 MeV; measured γ(particle), γγ(particle)-coin, γ(t). ⁹⁷Ag deduced levels, J, π, T_1/2. ⁹⁷Pd deduced isomer J, π, T_1/2. ⁹⁵Rh deduced levels, J, π. Shell model comparison.

NUCLEAR STRUCTURE ⁹⁷Ag, ⁹⁵Rh, ¹⁰⁰Sn; calculated levels. Shell model.

1990BO48

Yad.Fiz. 52, 985 (1990); Sov.J.Nucl.Phys. 52, 627 (1990)

I.N.Borzov, E.L.Trykov, S.A.Fayans

Strength Functions of Gamow-Teller Excitations of Stable and Neutron-Deficient Nuclei

NUCLEAR STRUCTURE ⁵⁴Fe, ⁶⁰Ni, ⁹⁴Ru, ⁹⁶Pd, ^{110,108,106,104,102,100}Sn, ¹⁴⁸Dy, ¹⁵⁰Er; calculated Gamow-Teller transition strength functions.

1992CI03

Z.Phys. A341, 261 (1992)

O.Civitarese, A.Faessler, M.C.Licciardo

Pair Density Fluctuations in a Number Projected BCS Approximation

NUCLEAR STRUCTURE ^100,124Sn; calculated microscopic, macroscopic one-body density, pair density fluctuations; deduced number projection role. BCS treatment.

1993BO43

Bull.Rus.Acad.Sci.Phys. 57, 1783 (1993)

I.N.Borzov, S.A.Fayans, K.Rykaczewski

Gamow-Teller β-Decay of Nuclei in the Vicinity of ¹⁰⁰Sn

RADIOACTIVITY ^{100,101,102,103,104,105,106,107,108,109}Sn(β⁺); calculated β⁺-decay energy, Q(EC), Gamow-Teller transition strength; deduced renormalization features. Finite Fermi systems theory.

1993HA23

Phys.Rev. C48, R960 (1993)

I.Hamamoto, H.Sagawa

Gamow-Teller Beta Decay and Isospin Impurity in Nuclei Near the Proton Drip Line

NUCLEAR STRUCTURE ⁵⁶Ni, ⁶⁴Ge, ⁷⁶Sr, ⁷⁸Zr, ^100,106Sn; calculated Gamow-Teller transition strength nonenergy weighted sum rule percentage. ¹²C, ¹⁶O, ⁴⁰Ca, ⁵⁶Ni, ⁶⁴Ge, ⁷⁶Sr, ⁸⁰Zr, ¹⁰⁰Sn; calculated isospin mixing probabilities. Hartree-Fock plus TDA approximation.

doi: 10.1103/PhysRevC.48.R960

1993KA25

Z.Phys. A346, 253 (1993)

S.Kamerdzhiev, J.Speth, G.Tertychnyi, J.Wambach

M1 Resonances in Unstable Magic Nuclei

NUCLEAR STRUCTURE ⁴⁸Ca, ²⁰⁸Pb, ^56,78Ni, ^100,132Sn; calculated M1 transition strength distributions, B(M1). Microscopic approach, RPA configurations, single particle continuum.

1994BR28

Phys.Rev. C50, R2270 (1994)

B.A.Brown, K.Rykaczewski

Gamow-Teller Strength in the Region of ¹⁰⁰Sn

NUCLEAR STRUCTURE ¹⁰⁰Sn, ⁹⁸Cd, ⁹⁶Pd, ⁹⁴Ru; calculated β⁺ decay associated Gamow-Teller transition strength distribution. Shell model approach.

doi: 10.1103/PhysRevC.50.R2270

1994BR29

Nucl.Phys. A577, 13c (1994)

B.A.Brown

Gamow-Teller Strength in Nuclei with N = Z from ¹²C to ¹⁰⁰Sn

NUCLEAR STRUCTURE ⁴He, ¹²C, ¹⁶O, ²⁸Si, ²⁰Ne, ²⁴Mg, ³²S, ⁴⁰Ca, ⁵⁶Ni, ¹⁰⁰Sn; calculated Gamow-Teller strength. Shell model.

doi: 10.1016/0375-9474(94)90827-3

1994DO02

Phys.Rev.Lett. 72, 981 (1994)

J.Dobaczewski, I.Hamamoto, W.Nazarewicz, J.A.Sheikh

Nuclear Shell Structure at Particle Drip Lines

NUCLEAR STRUCTURE ¹⁰⁰Sn, ¹⁰⁰Zn; calculated nucleon densities, central potentials radial dependences. A=120; calculated single particles levels for isobars. Self-consistent mean-field theory.

doi: 10.1103/PhysRevLett.72.981

1994DO19

Acta Phys.Pol. B25, 541 (1994)

J.Dobaczewski, I.Hamamoto, W.Nazarewicz, J.A.Sheikh

Nuclear Structure at Particle Drip Lines

NUCLEAR STRUCTURE ^{100,118,132,150}Sn; calculated single particle nucleonic densities. A=100, 120, 150; calculated single particle levels. A=94-110; calculated Q(EC) for Ru, PD, Cd, Sn isotopes. ^76,78,80,82Sr; calculated levels. Mean field approach.

1994HJ02

Phys.Rev. C50, 501 (1994)

M.Hjorth-Jensen, H.Muther, A.Polls

Width of the Δ Resonance in Nuclei

NUCLEAR STRUCTURE ⁴⁰Ca, ¹⁶O, ¹⁰⁰Sn; calculated two-body absorption component of Δ self-energy vs distance from center of nucleus, imaginary part vs deposited energy.

doi: 10.1103/PhysRevC.50.501

1994KA10

Nucl.Phys. A569, 313c (1994)

S.Kamerdzhiev, G.Tertychnyi, J.Speth

Theoretical Description of Giant Resonances in Stable and Unstable Magic Nuclei

NUCLEAR REACTIONS ²⁰⁸Pb(γ, X), E ≤ 35 MeV; calculated photoabsorption σ(E). Microscopic approach, Green function method, RPA with complex configuration.

NUCLEAR STRUCTURE ⁴⁰Ca, ^56,78Ni, ^100,132Sn, ²⁰⁸Pb; calculated diverse giant resonance excitation functions, B(λ). Microscopic approach, Green function method, RPA with complex configuration.

doi: 10.1016/0375-9474(94)90122-8

1994LE27

Phys.Lett. 332B, 20 (1994)

M.Lewitowicz, R.Anne, G.Auger, D.Bazin, C.Borcea, V.Borrel, J.M.Corre, T.Dorfler, A.Fomichov, R.Grzywacz, D.Guillemaud-Mueller, R.Hue, M.Huyse, Z.Janas, H.Keller, S.Lukyanov, A.C.Mueller, Yu.Penionzhkevich, M.Pfutzner, F.Pougheon, K.Rykaczewski, M.G.Saint-Laurent, K.Schmidt, W.D.Schmidt-Ott, O.Sorlin, J.Szerypo, O.Tarasov, J.Wauters, J.Zylicz

Identification of the Doubly-Magic Nucleus ¹⁰⁰Sn in the Reaction ¹¹²Sn + (nat)Ni at 63 MeV/Nucleon

NUCLEAR REACTIONS Ni(¹¹²Sn, X)¹⁰⁰Sn, E=63 MeV/nucleon; measured fragment Z vs mass to charge ratio; deduced evidence for ¹⁰⁰Sn. Production σ lower limit given.

doi: 10.1016/0370-2693(94)90852-4

1994SC22

Z.Phys. A348, 241 (1994)

R.Schneider, J.Friese, J.Reinhold, K.Zeitelhack, T.Faestermann, R.Gernhauser, H.Gilg, F.Heine, J.Homolka, P.Kienle, H.J.Korner, H.Geissel, G.Munzenberg, K.Summerer

Production and Identification of ¹⁰⁰Sn

NUCLEAR REACTIONS ⁹Be(¹²⁴Xe, X)¹⁰⁰Sn, E=1095 MeV/nucleon; measured residual production σ following projectile fragmentation. Fragment identification by event by event magnetic rigidity, tof, energy deposition.

1994SC34

Z.Phys. A350, 91 (1994)

J.Schaffner, J.A.Maruhn, H.Stocker, W.Greiner

Proton Halos in ¹⁰⁰Sn using a Relativistic Shell Model

NUCLEAR STRUCTURE ¹⁰⁰Sn; calculated binding energy, proton, neutron separation energies.

1995CH57

Phys.Scr. T56, 231 (1995)

E.Chabanat, P.Bonche, P.Haensel, J.Meyer, R.Schaeffer

New Skyrme Effective Forces for Supernovae and Neutron Rich Nuclei

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140}Sn; calculated two neutron separation energies. Z=32-78; calculated two proton separation energies. Hartree-Fock plus BCS formalism, new Skyrme-like effective interactions.

1995CO16

Phys.Rev. C52, R1175 (1995)

G.Colo, M.A.Nagarajan, P.Van Isacker, A.Vitturi

Isospin Mixing in Proton-Rich N ≈ Z Nuclei

NUCLEAR STRUCTURE ⁹⁰Zr, ^99,100Sn, ⁹⁹In, ⁴⁰Ca, ⁸⁸Sr, ²⁰⁸Pb; calculated isospin admixtures. ¹⁰⁰Sn; calculated isovector giant monopole resonance strength distribution. Hartree-Fock approach, Skyrme forces.

doi: 10.1103/PhysRevC.52.R1175

1995DO05

Phys.Rev. C51, R1070 (1995)

J.Dobaczewski, W.Nazarewicz

Limits of Proton Stability Near ¹⁰⁰Sn

NUCLEAR STRUCTURE ^94,96,98,100Cd, ^{96,98,100,102}Sn, ^{98,100,102,104}Te; calculated total energy. ^106,108,110Te, ^{94,96,98,100,102}Sn; calculated two proton separation energies; deduced proton stability features. ^{92,94,96,98,100,102}Sn; calculated single particle proton energies. Skyrme HFB theory.

doi: 10.1103/PhysRevC.51.R1070

1995DO08

Phys.Lett. 345B, 181 (1995)

J.Dobaczewski, I.Hamamoto

Isospin Impurities in Ground States of N = Z Nuclei Near the Proton-Drip Line

NUCLEAR STRUCTURE ⁵⁶Ni, ⁶⁴Ge, ⁷⁶Sr, ⁸⁰Zr, ¹⁰⁰Sn; calculated isospin mixing probabilities. Deformed Hartree-Fock solutions, Skyrme interaction.

doi: 10.1016/0370-2693(94)01634-O

1995GR10

Acta Phys.Pol. B26, 341 (1995)

H.Grawe, R.Schubart, M.Gorska, K.H.Maier, J.B.Fitzgerald, J.Heese, M.Rejmund, K.Spohr, and the OSIRIS and NORDBALL Collaborations

The Experimental and Shell Model Approach to ¹⁰⁰Sn

NUCLEAR REACTIONS ^46,48Ti(⁵⁸Ni, 2n2p), E=230 MeV; measured nγγ-, pγγ-coin. ^100,102Cd deduced levels, J, π. Model comparison.

NUCLEAR STRUCTURE ⁹⁸Ag, ^100,104,106Sn; analyzed levels, B(λ) data in some cases. ¹⁰⁵Sb; calculated proton-, γ-decay schemes.

1995GR16

Phys.Scr. T56, 71 (1995)

H.Grawe, R.Schubart, K.H.Maier, D.Seweryniak, and the OSIRIS/NORDBALL Collaborations

The Shell Model at ¹⁰⁰Sn-An Experimental Status Report

NUCLEAR STRUCTURE ⁹¹Zr, ⁹³Mo, ⁹⁵Ru, ^95,97Pd, ⁹⁹Cd, ^{104,105,106,107,101}Sn; calculated levels. ¹⁶O, ⁴⁰Ca, ⁵⁶Ni; analyzed Coulomb energy shifts. ¹⁰⁰Sn; deduced single particle energies, Coulomb energy shifts between protons, neutrons. Shell model.

1995JO14

Phys.Rev. C51, 2817 (1995)

I.P.Johnstone, L.D.Skouras

Binding Energies of Proton-Rich Nuclei in the Vicinity of ¹⁰⁰Sn

NUCLEAR STRUCTURE ^90,91,92Zr, ^91,92,93Nb, ^92,93,94Mo, ^93,94,95Tc, ^94,95,96Ru, ^95,96,97Rh, ^96,97,98Pd, ^97,98,99Ag, ^98,99,100Cd, ^99,100,101In, ^100,101,102Sn; calculated binding energies; deduced relevance to β-decay, β-delayed proton emission.

doi: 10.1103/PhysRevC.51.2817

1995JO15

J.Phys.(London) G21, L63 (1995)

I.P.Johnstone, L.D.Skouras

The Spectrum and Decay of ¹⁰⁰Sn

NUCLEAR STRUCTURE ¹⁰⁰Sn, ¹⁰⁰In; calculated levels; deduced β⁺-decay characteristics.

doi: 10.1088/0954-3899/21/8/001

1995LE14

Nucl.Phys. A588, 197c (1995)

M.Lewitowicz, R.Anne, G.Auger, D.Bazin, C.Borcea, V.Borrel, J.M.Corre, T.Dorfler, A.Fomichov, R.Grzywacz, D.Guillemaud-Mueller, R.Hue, M.Huyse, Z.Janas, H.Keller, S.Lukyanov, A.C.Mueller, Yu.Penionzhkevich, M.Pfutzner, F.Pougheon, K.Rykaczewski, M.G.Saint-Laurent, K.Schmidt, W.D.Schmidt-Ott, O.Sorlin, J.Szerypo, O.Tarasov, J.Wauters, J.Zylicz

Identification of ¹⁰⁰Sn and Other Proton Drip-Line Nuclei in the Reaction ¹¹²Sn(63 MeV/nucl.)+(Nat)Ni

NUCLEAR REACTIONS Ni(¹¹²Sn, X), E=63 MeV/nucleon; measured (fragment)γ(t), fragment mass distribution; deduced evidence for ^103,104Sb, ⁹⁸In, ⁹¹Pd, ⁸⁹Rh, ⁸⁷Ru, ^66mAs.

doi: 10.1016/0375-9474(95)00139-R

1995RE10

J.Phys.(London) G21, 691 (1995)

Z.Ren, G.-O.Xu, B.Chen, Z.Ma

Ground-State Properties of the Nucleus ¹⁰⁰Sn in Relativistic and Non-Relativistic Mean-Field Approaches

NUCLEAR STRUCTURE ^100,114,132Sn; calculated binding energy per nucleon, n-, p- radii, differences. Mean field approach, Skyrme interactions.

doi: 10.1088/0954-3899/21/5/013

1995RY03

Phys.Rev. C52, R2310 (1995)

K.Rykaczewski, R.Anne, G.Auger, D.Bazin, C.Borcea, V.Borrel, J.M.Corre, T.Dorfler, A.Fomichov, R.Grzywacz, D.Guillemaud-Mueller, R.Hue, M.Huyse, Z.Janas, H.Keller, M.Lewitowicz, S.Lukyanov, A.C.Mueller, Yu.Penionzhkevich, M.Pfutzner, F.Pougheon, M.G.Saint-Laurent, K.Schmidt, W.D.Schmidt-Ott, O.Sorlin, J.Szerypo, O.Tarasov, J.Wauters, J.Zylicz

Identification of New Nuclei at and Beyond the Proton Drip Line Near the Doubly Magic Nucleus ¹⁰⁰Sn

NUCLEAR REACTIONS Ni(¹¹²Sn, X), E=58, 62 MeV/nucleon; measured heavy fragments energy loss, total kinetic energy, Eγ, Iγ; deduced evidence for ^103,104Sb, ⁹⁸In, ⁹¹Pd, ⁸⁹Rh, ⁸⁷Ru. Other fragments atomic, mass numbers, charge state deduced. Tof.

doi: 10.1103/PhysRevC.52.R2310

1995SA10

Nucl.Phys. A583, 755c (1995)

H.Sagawa

Perspectives on Study of Unstable Nuclei Near Drip Lines

NUCLEAR STRUCTURE ¹¹Be; calculated dipole transition strength. ⁵⁶Ni, ⁶⁴Ge, ⁷⁸Zr, ¹⁰⁰Sn; calculated Gamow-Teller giant resonance energy. ⁶He; calculated monopole, dipole, quadrupole RPA responses. Microscopic Hartree-Fock + RPA.

doi: 10.1016/0375-9474(94)00754-B

1995SA34

Nucl.Phys. A588, 209c (1995)

H.Sagawa

Structure of Unstable Nuclei Near Proton Drip Line

NUCLEAR STRUCTURE ⁵⁶Co, ⁶⁴Ga, ⁷⁸Zn, ¹⁰⁰In; calculated Gamow-Teller giant resonance energy relative to mother nucleus ground state. ¹²C, ¹⁶O, ⁴⁰Ca, ⁵⁶Ni, ⁶⁴Ge, ⁷⁸Sr, ⁸⁰Zr, ¹⁰⁰Sn; calculated isospin mixing probabilities. ⁷⁶Sr, ⁶⁴Ge, ⁵⁶Ni, ^100,106Sn; calculated potential energy vs deformation. Hartree-Fock+TDA (or RPA), finite-range droplet model.

doi: 10.1016/0375-9474(95)00141-M

1995SA49

Phys.Scr. T56, 84 (1995)

N.Sandulescu, J.Blomqvist, R.J.Liotta

Microscopic Description of Light Sn Isotopes

NUCLEAR STRUCTURE A=100-114; compiled, reviewed level calculation, Sn isotopes. Shell model.

1995SC28

Nucl.Phys. A588, 191c (1995)

R.Schneider, T.Faestermann, J.Friese, R.Gernhauser, H.Geissel, H.Gilg, F.Heine, J.Homolka, P.Kienle, H.-J.Korner, G.Munzenberg, J.Reinhold, K.Summerer, K.Zeitelhack

Production, Identification, and Halflife Measurement of ¹⁰⁰Sn

NUCLEAR REACTIONS ⁹Be(¹²⁴Xe, X), E=1.095 GeV/nucleon; measured fragment energy deposition vs mass to charge ratio for ^100,101Sn, ^100,98,99In.

RADIOACTIVITY ^102,100Sn(β⁺); ¹⁰⁴Sb(β⁺p); ¹⁰⁵Sb(β⁺); ¹⁰⁸Te(β⁺), (α) [from ⁹Be(¹²⁴Xe, X), E=1.095 GeV/nucleon]; measured T_1/2.

doi: 10.1016/0375-9474(95)00138-Q

1995SC33

Phys.Scr. T56, 67 (1995)

R.Schneider, T.Faestermann, J.Friese, R.Gernhauser, H.Gilg, F.Heine, J.Homolka, P.Kienle, H.J.Korner, J.Reinhold, K.Zeitelhack, H.Geissel, G.Munzenberg, K.Summerer

Identification and Halflife Measurement of ¹⁰⁰Sn and Neighbouring Nuclei

NUCLEAR REACTIONS ⁹Be(¹²⁴Xe, X), E=1095 MeV/nucleon; measured energy deposition vs (M/Q), fragment decay event energy spectra; deduced evidence for ¹⁰⁰Sn.

RADIOACTIVITY ^105,104,100Sn(β⁺) [from ⁹Be(¹²⁴Xe, X), E=1095 MeV/nucleon]; measured T_1/2.

1995SC50

Z.Phys. A352, 373 (1995)

R.Schubart, H.Grawe, J.Heese, H.Kluge, K.H.Maier, M.Schramm

Shell Model Structure at ¹⁰⁰Sn - The Nuclides ⁹⁸Ag, ¹⁰³In, and ^104,105Sn

NUCLEAR REACTIONS, ICPND ⁵⁰Cr(⁵⁸Ni, xnypzα), E=250 MeV; measured γγ-, nγγ-, pγγ-, αγγ-coin, Eγ, Iγ; deduced production σ for ^102-105Sn, ^102-105In, ^98-104Cd, ^98-103Ag, ^95-100Pd, ^94-97Rh. ^106,104,105Sn, ⁹⁸Ag, ¹⁰³In deduced levels, J, π, B(λ), Iγ. Shell model comparison.

1995SCZZ

GSI-94-1, p.26 (1995)

R.Schneider, T.Faestermann, J.Friese, R.Gernhauser, H.Geissel, H.Gilg, F.Heine, J.Homolka, P.Kienle, H.-J.Korner, G.Munzenberg, J.Reinhold, K.Summerer, K.Zeitelhack

Production and Decay Measurements of ¹⁰⁰Sn

NUCLEAR REACTIONS ⁹Be(¹²⁴Xe, X), E=1.095 GeV/nucleon; measured fragment mass to charge ratio, α-decay characteristics of ¹⁰⁸Te, ^105,104Sb, ^100,102Sn.

RADIOACTIVITY ^102,100Sn(β⁺), ¹⁰⁴Sb(β⁺); ¹⁰⁸Te(β⁺), (α) [from ⁹Be(¹²⁴Xe, X), E=1.095 GeV/nucleon]; measured decay characteristics.

1996BO11

Z.Phys. A355, 117 (1996)

I.N.Borzov, S.A.Fayans, E.Kromer, D.Zawischa

Ground State Properties and β-Decay Half-Lives Near ¹³²Sn in a Self-Consistent Theory

NUCLEAR STRUCTURE ^100,132Sn; calculated nucleon, matter density distributions. ⁴⁰Ca, ²⁰⁸Pb; calculated density distributions. ^{127,129,128,130}Cd, ^133,134Sn, ¹³⁸Te, ^{123,125,127,129}Ag, ^131,133,135In, ¹³⁵Sb; calculated levels, J, π, Qβ, T_1/2, Gamow-Teller strength distributions. ^{124,125,126,131,132,133}Cd; calculated T_1/2.

doi: 10.1007/s002180050088

1996CH32

Phys.Rev.Lett. 77, 2400 (1996)

M.Chartier, G.Auger, W.Mittig, A.Lepine-Szily, L.K.Fifield, J.M.Casandjian, M.Chabert, J.Ferme, A.Gillibert, M.Lewitowicz, M.Mac Cormick, M.H.Moscatello, O.H.Odland, N.A.Orr, G.Politi, C.Spitaels, A.C.C.Villari

Mass Measurement of ¹⁰⁰Sn

ATOMIC MASSES ¹⁰⁰Cd, ¹⁰⁰In, ¹⁰⁰Sn; measured masses with respect to ¹⁰⁰Ag. Secondary mass=100 ions from ⁵⁸Ni(⁵⁰Cr, X) reactions.

doi: 10.1103/PhysRevLett.77.2400

1996DE63

Phys.Lett. 367B, 17 (1996)

D.J.Dean, S.E.Koonin, T.T.S.Kuo, K.Langanke, P.B.Radha

Complete 0(h-bar x Omega) Shell Model Carlo Calculations of ⁹⁴Ru, ⁹⁶Pd, ^96,98Cd and ¹⁰⁰Sn

NUCLEAR STRUCTURE ⁹⁴Ru, ⁹⁶Pd, ^96,98Cd, ¹⁰⁰Sn; calculated Gamow-Teller transition, masses, strengths. Shell model Monte Carlo technique.

doi: 10.1016/0370-2693(95)01446-2

1996DO06

Phys.Rev. C53, 2809 (1996)

J.Dobaczewski, W.Nazarewicz, T.R.Werner, J.F.Berger, C.R.Chinn, J.Decharge

Mean-Field Description of Ground-State Properties of Drip-Line Nuclei: Pairing and continuum effects

NUCLEAR STRUCTURE ^{132,120,150,172,100}Sn; calculated neutron, pairing densities, other aspects. Mean-field approach.

doi: 10.1103/PhysRevC.53.2809

1996HA02

Phys.Rev. C53, 765 (1996)

I.Hamamoto, H.Sagawa, X.Z.Zhang

Single-Particle and Collective Properties of Drip-Line Nuclei

NUCLEAR STRUCTURE ¹¹⁰Ni, ^100,120Sn, ¹²⁰Sr; calculated Hartree-Fock density, Hartree-Fock potential vs r. ¹¹⁰Ni, ¹⁰⁰Sn; calculated isoscalar, isovector monopole, isovector dipole, isoscalar quadrupole modes strength functions. Hartree-Fock with Skyrme interactions, RPA.

doi: 10.1103/PhysRevC.53.765

1996HJ02

J.Phys.(London) G22, 321 (1996)

M.Hjorth-Jensen, H.Muther, E.Osnes, A.Polls

Comparison of the Effective Interaction to Various Orders in Different Mass Regions

NUCLEAR STRUCTURE ⁴He, ¹⁶O, ⁴⁰Ca, ¹⁰⁰Sn, ²⁰⁸Pb; calculated diagonal, nondiagonal matrix elements, mean value ratios; deduced higher-order terms contributions stability mass dependence. Effective interaction to various orders, shell model.

doi: 10.1088/0954-3899/22/3/006

1996KA09

Nucl.Phys. A599, 373c (1996)

S.Kamerdzhiev, J.Speth

Distribution of Giant Resonance Strength in Stable and Unstable Nuclei

NUCLEAR REACTIONS ²⁰⁸Pb(γ, X), E ≤ 40 MeV; compiled, reviewed calculations of giant resonance photoabsorption σ(E). ²⁰⁸Pb(γ, n), E ≤ 22 MeV; calculated σ(E). Microscopic theory.

NUCLEAR STRUCTURE ^48,40Ca, ^56,78Ni, ^100,132Sn, ²⁰⁸Pb; compiled, reviewed calculations of B(M1).

doi: 10.1016/0375-9474(96)00080-2

1996KI23

Hyperfine Interactions 103, 49 (1996)

P.Kienle

On the Limit of Nuclear Stability - The Region of Double Magic ¹⁰⁰Sn and Bound-State β-Decay of ¹⁸⁷Re⁷⁵

RADIOACTIVITY ¹⁰⁰Sn(β⁺) [from ⁹Be(¹²⁴Xe, X), E=1.1 GeV/nucleon]; measured β⁺ endpoint energy, T_1/2. ¹⁸⁷Re(β^-); measured bound state β-decay associated T_1/2.

NUCLEAR REACTIONS ²⁷Al(¹²⁹Xe, X)¹⁰⁴Sn/¹⁰⁵Sn/¹⁰⁶Sn/¹⁰⁷Sn, E=790 MeV/nucleon; ⁹Be(¹²⁹Xe, X)¹⁰⁰Sn/¹⁰¹Sn/¹⁰²Sn/¹⁰³Sn/¹⁰⁴Sn/¹⁰⁵Sn/¹⁰⁶Sn, E=1.1 GeV/nucleon; measured residuals production σ.

1996SH18

Z.Phys. A355, 247 (1996)

Y.-S.Shen, Z.Ren

Skyrme-Hartree-Fock Approach to Cd, Sn and Te Isotopes

NUCLEAR STRUCTURE ^{98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130}Cd, ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134}Sn, ^{108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138}Te; calculated binding energies, nucleon, charge radii. Skyrme Hartree-Fock approach.

doi: 10.1007/s002180050106

1996SH20

Z.Phys. A356, 133 (1996)

Y.-S.Shen, Z.Ren

Skyrme-Hartree-Fock Approach to Spherical Nuclei with Density-Dependent Pairing Correlations

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ⁹⁰Zr, ^{178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214}Pb, ^{50,52,54,56,58,60,62,64,66,68,70,72,74,76,78}Ni, ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132}Sn; calculated binding energy, nucleon, charge, matter radii, isotope shifts. ²⁸O, ³⁰Ne, ³²Mg, ³⁴Si, ³⁶S, ³⁸Ar, ⁴²Ti, ⁴⁴Cr, ⁴⁶Fe, ^{32,34,36,38,42,44,50,52}Ca; calculated binding energy, nucleon, matter radii. Skyrme-Hartree-Fock model plus density-dependent correlation.

doi: 10.1007/s002180050159

1997CH49

Nucl.Phys. A627, 710 (1997)

E.Chabanat, P.Bonche, P.Haensel, J.Meyer, R.Schaeffer

A Skyrme Parametrization from Subnuclear to Neutron Star Densities

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ^56,78Ni, ^100,132Sn, ²⁰⁸Pb; calculated binding energies, radii; deduced parameters. Skyrme parametrization.

doi: 10.1016/S0375-9474(97)00596-4

1997DU06

Phys.Rev. C56, 804 (1997); Comment Phys.Rev. C59, 2952 (1999)

G.G.Dussel, H.M.Sofia, A.Tonina

Pairing Interaction and Galilei Invariance

NUCLEAR STRUCTURE ⁶⁰Ni, ^70,72Ge, ⁸⁸Sr, ^90,96Zr, ^{100,114,116,120,132}Sn, ¹³⁸Ba, ¹⁵⁴Gd, ¹⁵⁶Dy, ¹⁷⁰Yb, ^206,208Pb; calculated effective nucleon mass, energy-weighted sum rule; deduced mass dipole operator effect.

doi: 10.1103/PhysRevC.56.804

1997GR12

Z.Phys. A358, 185 (1997)

H.Grawe, M.Gorska, M.Lipoglavsek, R.Schubart, A.Atac, A.Axelsson, J.Blomqvist, J.Cederkall, G.de Angelis, M.de Poli, C.Fahlander, A.Johnson, K.H.Maier, L.-O.Norlin, J.Nyberg, D.Foltescu, M.Palacz, J.Persson, M.Rejmund, H.A.Roth, T.Shizuma, O.Skeppstedt, G.Sletten, M.Weiszflog, and the OSIRIS/NORDBALL-PEX/EUROBALL Collaboration

Present Status and Future Aspects of Nuclear Structure Close to ¹⁰⁰Sn

NUCLEAR STRUCTURE ⁹⁴Pd, ^98,96Cd, ⁹²Ru; compiled, reviewed level data, analyses. ^99,101,100Cd, ^104,106Sn, ⁹⁰Zr, ⁴⁸Ca, ^56,68Ni; compiled, reviewed B(λ) data. ¹⁶O, ⁴⁰Ca, ⁵⁶Ni, ¹⁰⁰Sn; compiled, reviewed Coulomb shift corrected single particle energies.

doi: 10.1007/s002180050302

1997HA17

Phys.Lett. 394B, 1 (1997)

I.Hamamoto, H.Sagawa

Electric Quadrupole Polarization Charges in Proton Drip Line Nuclei

NUCLEAR STRUCTURE ⁴⁸Ni, ¹⁰⁰Sn; calculated isoscalar, isovector quadrupole strength function, nucleon polarization charges, B(E2). Hartree-Fock with Skyrme interactions, RPA solved in coordinate space with the Green's function method.

doi: 10.1016/S0370-2693(96)01657-7

1997HE24

Nucl.Phys. A627, 35 (1997)

H.Herndl, B.A.Brown

Shell-Model Calculations for the Properties of Nuclei with A = 86-100 Near the Proton Drip Line

NUCLEAR STRUCTURE ^92,94Pd, ^90,91,92Rh, ⁸⁹Tc; calculated levels, J, π. ^86,87,88Sr, ^86,87,88,89Y, ^{86,87,88,89,90}Zr, ^{86,87,88,89,90,91}Nb, ^{86,87,88,89,90,91,92}Mo, ^{86,87,88,89,90,91,92,93}Tc, ^{86,87,88,89,90,91,92,93,94}Ru, ^{86,87,88,89,90,91,92,93,94,95}Rh, ^{86,87,88,89,90,91,92,93,94,95,96}Pd, ^{87,88,89,90,91,92,93,94,95,96,97}Ag, ^{88,89,90,91,92,93,94,95,96,97,98}Cd, ^{89,90,91,92,93,94,95,96,97,98,99}In, ^{90,91,92,93,94,95,96,97,98,99,100}Sn; calculated binding energies; deduced proton drip line. ^86,87,88Sr, ^86,87,88,89Y, ^{86,87,88,89,90}Zr, ^{86,87,88,89,90,91}Nb, ^{86,87,88,89,90,91,92}Mo, ^{86,87,88,89,90,91,92,93}Tc, ^{86,87,88,89,90,91,92,93,94}Ru, ^{90,91,92,93,94,95}Rh, ^{88,89,90,91,92,93,94,95,96}Pd, ^94,95,96,97Ag, ^{92,93,94,95,96,97,98}Cd, ^98,99In, ^98,99,100Sn; calculated ground-state spin, T_1/2. Shell model.

doi: 10.1016/S0375-9474(97)00407-7

1997KA50

Bull.Rus.Acad.Sci.Phys. 61, 122 (1997)

S.P.Kamerdzhiev

Microscopic Theory of Giant Resonances (A Review)

NUCLEAR STRUCTURE ^40,48Ca, ²⁰⁸Pb, ^100,132Sn, ^56,78Ni, ¹⁶O; compiled, reviewed giant multipole resonance calculations; deduced models improvement related features.

1997LE36

Acta Phys.Hung.N.S. 6, 157 (1997)

A.Lepine-Szily, M.Chartier, G.Auger, W.Mittig, J.M.Casandjian, M.Chabert, L.K.Fifield, J.Ferme, A.Gillibert, M.Lewitowicz, M.MacCormick, MM.H.Moscatello, O.H.Odland, N.A.Orr, G.Politi, C.Spitaels, A.C.C.Villari

Mass Measurements Far from Stability Around the N = Z Line (¹⁰⁰Sn, ¹⁰⁰In, ¹⁰⁰Cd)

ATOMIC MASSES ¹⁰⁰Sn, ¹⁰⁰In, ¹⁰⁰Cd; measured masses with respect to ¹⁰⁰Ag. Secondary A=100 ions from ⁵⁸Ni(⁵⁰Cr, X) reaction.

NUCLEAR REACTIONS, ICPND ⁵⁸Ni(⁵⁰Cr, X)¹⁰⁰Ag/¹⁰⁰Cd/¹⁰⁰In/¹⁰⁰Sn, E=5.3 MeV/nucleon; measured production σ. Comparison with statistical models.

1997MI07

Nucl.Phys. A616, 329c (1997)

W.Mittig, M.Chartier, J.C.Angelique, G.Audi, J.M.Casandjian, A.Cunsolo, C.Donzaud, M.Chabert, J.Ferme, L.K.Fifield, A.Foti, A.Gillibert, A.Lepine-Szily, M.Lewitowicz, S.Lukyanov, M.Mac Cormick, D.J.Morrissey, M.H.Moscatello, O.H.Odland, N.A.Orr, A.Ostrowski, G.Politi, C.Spitaels, B.M.Sherrill, C.Stephan, T.Suomijarvi, L.Tassan-Got, D.J.Vieira, A.C.C.Villari, J.M.Wouters

Mass Measurements Near N = Z

NUCLEAR REACTIONS Ni(⁷⁸Kr, X), E=73 MeV/nucleon; measured fragment tof; deduced secondary beams (with mass ≈ 60-80) production related features. ⁵⁸Ni(⁵⁰Cr, X), E=5.1 MeV/nucleon; measured fragment tof; deduced ¹⁰⁰Sn production σ. ¹⁰⁰Cd, ¹⁰⁰Sn, ¹⁰⁰In deduced masses relative to ¹⁰⁰Ag. Pure secondary beams from ions stripping technique, α-, SPEG spectrometers.

doi: 10.1016/S0375-9474(97)00104-8

1997SU06

Nucl.Phys. A616, 341c (1997)

K.Summerer, R.Schneider, T.Faestermann, J.Friese, H.Geissel, R.Gernhauser, H.Gilg, F.Heine, J.Homolka, P.Kienle, H.J.Korner, G.Munzenberg, J.Reinhold, K.Zeitelhack

Identification and Decay Spectroscopy of ¹⁰⁰Sn at the GSI Projectile Fragment Separator FRS

RADIOACTIVITY ¹⁰⁰Sn(β⁺) [from ¹²⁴Xe projectile fragmentation]; measured β-decay energy, T_1/2, β-delayed proton emission associated probability; deduced Qβ, Gamow-Teller strength, hindrance factor. Decay times for ¹⁰⁰In, ¹⁰⁰Cd also reported.

doi: 10.1016/S0375-9474(97)00106-1

1998AV03

Bull.Rus.Acad.Sci.Phys. 62, 23 (1998)

A.V.Avdeenkov

M1 Resonances in ¹⁰⁰Sn and ¹³²Sn Nuclei

NUCLEAR STRUCTURE ^100,132Sn; calculated isovector M1 resonances energy, B(M1); deduced resonance splitting contributions. Microscopic model.

1998BR12

Phys.Rev. C58, 220 (1998)

B.A.Brown

New Skyrme Interaction for Normal and Exotic Nuclei

NUCLEAR STRUCTURE ^16,24O, ³⁴Si, ^40,48Ca, ^48,68Ni, ⁸⁸Sr, ^100,132Sn, ²⁰⁸Pb; analyzed binding energies, radii, single-particle energies; deduced Skyrme parameters.

doi: 10.1103/PhysRevC.58.220

1998HA39

J.Phys.(London) G24, 1417 (1998)

I.Hamamoto, H.Sagawa, X.Z.Zhang

Collective Modes of Nuclei Far from β-Stability Line

NUCLEAR STRUCTURE ²⁸O, ³⁴Ca, ¹⁰⁰Sn, ²⁰⁸Pb; calculated isoscalar, isovector dipole strength distributions.

doi: 10.1088/0954-3899/24/8/016

1998KA29

Phys.Rev. C58, 172 (1998)

S.Kamerdzhiev, R.J.Liotta, E.Litvinova, V.Tselyaev

Continuum Quasiparticle Random-Phase Approximation Description of Isovector E1 Giant Resonances

NUCLEAR STRUCTURE ^{100,104,120,132}Sn; calculated E1 photoabsorption σ; deduced continuum effect on giant resonances. Continuum RPA, forced consistency procedure.

doi: 10.1103/PhysRevC.58.172

1998RU03

Nucl.Phys. A634, 67 (1998)

K.Rutz, M.Bender, P.-G.Reinhard, J.A.Maruhn, W.Greiner

Odd Nuclei and Single-Particle Spectra in the Relativistic Mean-Field Model

NUCLEAR STRUCTURE ^16,17O, ¹⁷F, ^40,41,48,49Ca, ^41,49Sc, ^56,57Ni, ⁵⁷Cu, ^{100,101,132,133}Sn, ^101,133Sb, ^208,209Pb, ²⁰⁹Bi, ^218,219U, ²¹⁹Np; calculated levels, J, π, neutron, proton separation energies; deduced core polarization effects. Relativistic mean-field approach.

doi: 10.1016/S0375-9474(98)00153-5

1998VE02

Phys.Rev. C57, 3089 (1998)

T.Vertse, A.T.Kruppa, R.J.Liotta, W.Nazarewicz, N.Sandulescu, T.R.Werner

Shell Corrections for Finite Depth Potentials: Particle continuum effects

NUCLEAR STRUCTURE ⁷⁸Ni, ^{90,96,104,106,108,110,122}Zr, ¹²⁴Zr, ¹³²Sn, ¹⁴⁶Gd, ²⁰⁸Pb, ²⁹⁸Fl; calculated neutron shell correction energies. ⁴⁸Ni, ⁹⁰Zr, ^100,132Sn, ¹⁴⁶Gd, ^180,208Pb; calculated proton shell correction energies. ¹⁴⁶Gd, ²⁰⁸Pb calculated smoothed level densities. Smoothing procedure with particle continuum contribution.

doi: 10.1103/PhysRevC.57.3089

1998YO10

Phys.Rev. C58, 2796 (1998)

S.Yoshida, H.Sagawa, N.Takigawa

Incompressibility and Density Distributions in Asymmetric Nuclear Systems

NUCLEAR STRUCTURE ^{100,104,108,112,116,120,124,128,132,136,140,150,160}Sn; calculated neutron, charge, matter radii, density distributions; deduced correlation between surface diffuseness, incompressibility.

doi: 10.1103/PhysRevC.58.2796

1999DU05

Phys.Rev. C59, R2347 (1999)

J.Duflo, A.P.Zuker

The Nuclear Monopole Hamiltonian

NUCLEAR STRUCTURE ^39,41,47,49Ca, ⁴⁷K, ⁴⁹Sc, ^15,17,21,23O, ²¹N, ²³F, ^{27,29,33,35,41,43}Si, ^33,41Al, ^35,43P, ^{55,57,67,69,77,79}Ni, ^67,77Co, ^69,79Cu, ^79,81,89,91Zr, ⁸⁹Y, ⁹¹Nb, ^{99,101,131,133}Sn, ¹³¹In, ¹³³Sb, ²⁰⁷Tl, ^207,209Pb, ²⁰⁹Bi; calculated single-particle orbits. ^12,14C, ^16,22,28O, ^18,34,42Si, ^40,48Ca, ^56,68,78Ni, ^80,90Zr, ^100,132Sn, ²⁰⁸Pb; calculated shell gaps. Monopole Hamiltonian.

doi: 10.1103/PhysRevC.59.R2347

1999RE09

Nucl.Phys. A649, 305c (1999)

P.-G.Reinhard

Skyrme Forces and Giant Resonances in Exotic Nuclei

NUCLEAR STRUCTURE ^14,16,24O, ³⁴Si, ³⁶S, ^36,40,48,60Ca, ^56,66Ni, ⁹⁰Zr, ^100,132Sn, ¹⁴⁶Gd, ²⁰⁸Pb; calculated dipole strength distributions. ¹⁶O, ²⁰⁸Pb calculated average resonance frequencies. ¹³²Sn calculated neutron skin thickness. Skyrme-Hartree-Fock model, several Skyrme forces compared.

doi: 10.1016/S0375-9474(99)00076-7

1999SA22

Nucl.Phys. A649, 319c (1999)

H.Sagawa, I.Hamamoto, X.Z.Zhang

A Microscopic Study of Giant Resonances in Nuclei Near Drip Lines

NUCLEAR STRUCTURE ²⁰⁸Pb, ^34,40,48,60Ca; calculated giant monopole resonance strength distributions. ¹⁰⁰Sn; calculated core polarization charges, B(E2). ⁹⁰Zr, ¹⁰⁰Sn; calculated neutron, proton effective charges. Self-consistent Hartree-Fock plus RPA model.

doi: 10.1016/S0375-9474(99)00094-9

2000BO07

Acta Phys.Pol. B31, 953 (2000)

A.Bobyk, W.Kaminski, I.N.Borzov

Gamow-Teller Beta-Decay Strengths of Neutron-Deficient Tin Isotopes: Comparison of FFST and pnBCS + QRPS Results

RADIOACTIVITY ^{100,102,104,106,108}Sn(β⁺); calculated Gamow-Teller strength distributions. Comparisons with data. Self-consistent finite Fermi-system theory and BCS plus quasiparticle RPA compared.

NUCLEAR STRUCTURE ^{100,102,104,106,108}Sn; calculated Gamow-Teller β-decay strength distributions. Comparisons with data. Self-consistent finite Fermi-system theory and BCS plus quasiparticle RPA compared.

2000SA56

Int.J.Mod.Phys. E9, 507 (2000)

S.V.S.Sastry, A.K.Jain, Y.K.Gambhir

Two-Oscillator Basis Expansion for the Solution of Relativistic Mean Field Equations

NUCLEAR STRUCTURE ¹⁶O, ⁵⁶Ni, ¹⁰⁰Sn, ²⁰⁸Pb; calculated binding energies, radii, density distributions. Relativistic mean field, two-oscillator basis.

doi: 10.1142/S0218301300000374

2000TS06

Bull.Rus.Acad.Sci.Phys. 64, 434 (2000)

V.I.Tselyaev

Integral Characteristics of Giant Resonances and Lorentz Distribution Parameters

NUCLEAR STRUCTURE ⁴⁰Ca, ¹⁰⁰Sn, ²⁰⁸Pb; calculated GDR widths, energies, strength distributions. Lorentz distribution.

2001DE01

Phys.Rev. C63, 024314 (2001)

M.Del Estal, M.Centelles, X.Vinas, S.K.Patra

Effects of New Nonlinear Couplings in Relativistic Effective Field Theory

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ^56,58,78Ni, ⁹⁰Zr, ^{100,116,124,132}Sn, ^196,208,214Pb; calculated ground-state energies, radii, surface thickness. Z=30-82; calculated isotopic shifts, two-neutron separation energies. ²⁰⁸Pb; calculated single-particle energies. Extended relativistic mean field.

doi: 10.1103/PhysRevC.63.024314

2001HA44

Phys.Rev. C64, 024306 (2001)

M.A.Hasan, J.P.Vary, T.-S.H.Lee

Medium-Mass Nuclei with Δ Excitations under Compression

NUCLEAR STRUCTURE ⁹⁰Zr, ^100,132Sn; calculated constrained spherical Hartree-Fock energy vs radius, sensitivity to size of nucleon and Δ isobar model spaces.

doi: 10.1103/PhysRevC.64.024306

2001HO28

Phys.Rev. C64, 034314 (2001)

F.Hofmann, C.M.Keil, H.Lenske

Density Dependence Hadron Field Theory for Asymmetric Nuclear Matter and Exotic Nuclei

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ^48,56,68Ni, ⁹⁰Zr, ^100,132Sn, ²⁰⁸Pb; calculated charge radii, binding energies. Ni, Sn; calculated binding energies, two-neutron separation energies. Density-dependent hadron field theory.

doi: 10.1103/PhysRevC.64.034314

2001RA11

Phys.Rev. C63, 044303 (2001); Comment Phys.Rev. C67, 019801 (2003)

M.Rashdan

Structure of Exotic Nuclei and Superheavy Elements in a Relativistic Shell Model

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ⁵⁶Ni, ^100,132Sn, ²⁰⁸Pb; calculated binding energies, charge radii. ¹⁶O, ⁴⁰Ca, ²⁹⁸Fl; calculated single-particle energies. Sn, Pb, Cf, Fm, No, ²⁵⁶Rf, ²⁵⁸Db, ²⁶⁰Sg, ²⁶²Bh, ²⁶⁴Hs, ²⁶⁶Mt, ²⁶⁹Ds, ²⁷¹Rg; calculated binding energies. Relativistic mean field theory, new relativistic force.

doi: 10.1103/PhysRevC.63.044303

2001SA77

Prog.Theor.Phys.(Kyoto), Suppl. 142, 1 (2001)

H.Sagawa

Giant Multipole States in Stable and Unstable Nuclei

NUCLEAR STRUCTURE ²⁰⁸Pb, ^34,40,48,60Ca, ²⁸O, ¹⁰⁰Sn; calculated giant resonance strength distributions, transition densities, related features. Self-consistent RPA response functions.

2001SI21

Phys.Rev. C63, 055501 (2001)

T.Siiskonen, M.Hjorth-Jensen, J.Suhonen

Renormalization of the Weak Hadronic Current in the Nuclear Medium

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca, ⁵⁶Ni, ¹⁰⁰Sn; calculated weak charge-changing hadronic current renormalization.

doi: 10.1103/PhysRevC.63.055501

2001SK02

Phys.Rev. C63, 024312 (2001)

J.Skalski

Self-Consistent Calculations of the Exact Coulomb Exchange Effects in Spherical Nuclei

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca, ⁴⁸Ni, ⁹⁰Zr, ^100,132Sn, ²⁰⁸Pb, ²⁹⁸Fl, ³¹⁰126; calculated single-proton level shifts due to Coulomb exchange, related features; deduced force independence. Comparison of exact results, Slater approximation.

doi: 10.1103/PhysRevC.63.024312

2001ST12

Phys.Rev. C63, 054309 (2001)

P.Stevenson, M.R.Strayer, J.Rikovska-Stone

Many-Body Perturbation Calculation of Spherical Nuclei with a Separable Monopole Interaction

NUCLEAR STRUCTURE ¹⁶O, ³⁴Si, ^40,48Ca, ^48,56,68,78Ni, ⁹⁰Zr, ^100,114,132Sn, ¹⁴⁶Gd, ²⁰⁸Pb; calculated binding energies, charge radii. ⁴⁰Ca, ²⁰⁸Pb; calculated charge form factors, single-particle energies. Many-body perturbation, separable monopole interaction, comparisons with data.

doi: 10.1103/PhysRevC.63.054309

2001VR02

Nucl.Phys. A692, 496 (2001)

D.Vretenar, N.Paar, P.Ring, G.A.Lalazissis

Collectivity of the Low-Lying Dipole Strength in Relativistic Random Phase Approximation

NUCLEAR STRUCTURE ^16,22,24,28O, ^40,48,54,60Ca, ^48,56,68,78Ni, ^{100,114,120,132}Sn, ¹²²Zr, ²⁰⁸Pb; calculated isovector dipole strength distributions, transition densities. Relativistic RPA.

doi: 10.1016/S0375-9474(01)00653-4

2002BU07

Phys.Rev. C65, 044308 (2002)

T.Burvenich, D.G.Madland, J.A.Maruhn, P.-G.Reinhard

Nuclear Ground State Observables and QCD Scaling in a Refined Relativistic Point Coupling Model

NUCLEAR STRUCTURE Ca, Ni, Sn, Pb, Cf, Fm, No, Rf, Sg, Hs; calculated binding energies. ²⁴⁰Pu; calculated fission barrier. Sn, Pb; calculated radii, surface thickness. ⁴⁸Ca, ¹⁰⁰Sn; calculated total baryon densities. ⁴⁸Ca; calculated charge form factor. Relativistic point-coupling model, comparison with other models.

doi: 10.1103/PhysRevC.65.044308

2002BU35

Prog.Theor.Phys.(Kyoto), Suppl. 146, 130 (2002)

T.Burvenich, D.G.Madland, A.Sulaksono, J.Maruhn, P.-G.Reinhard

A Relativistic Point Coupling Model for Nuclear Structure Calculations

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ^56,58Ni, ⁸⁸Sr, ⁹⁰Zr, ^{100,112,120,124,132}Sn, ¹³⁶Xe, ¹⁴⁴Sm, ^202,204,208Pb; calculated binding energies, radii. Relativistic point coupling model.

2002CO06

Phys.Rev.Lett. 88, 122701 (2002)

M.Colonna, Ph.Chomaz, S.Ayik

Mechanical and Chemical Spinodal Instabilities in Finite Quantum Systems

NUCLEAR STRUCTURE ^36,40,48Ca, ^100,120,132Sn; calculated instability regions in phase diagram.

doi: 10.1103/PhysRevLett.88.122701

2002DE27

Yad.Fiz. 65, 847 (2002); Phys.Atomic Nuclei 65, 814 (2002)

V.Yu.Denisov, V.A.Nesterov

Binding Energies of Nuclei and Their Density Distributions in a Nonlocal Extended Thomas-Fermi Approximation

NUCLEAR STRUCTURE ^32,40,48,56Ca, ^{48,50,58,60,62,64,78}Ni, ⁹⁰Zr, ^{100,114,124,132}Sn, ¹⁴⁰Ce, ²⁰⁸Pb, ²⁹⁶Fl, ³⁰⁰Og, ³⁰²120, ³⁰⁸126; calculated binding energies, radii, chemical potentials, particle density distributions. Nonlocal extended Thomas-Fermi approximation, Skyrme forces.

doi: 10.1134/1.1481472

2002FA13

Eur.Phys.J. A 15, 185 (2002)

T.Faestermann, R.Schneider, A.Stolz, K.Summerer, E.Wefers, J.Friese, H.Geissel, M.Hellstrom, P.Kienle, J.J.Korner, M.Mineva, M.Munch, G.Munzenberg, C.Schlegel, K.Schmidt, P.Thirolf, H.Weick, K.Zeitelhack

Decay studies of N ≈ Z nuclei from ⁷⁵Sr to ¹⁰²Sn

NUCLEAR REACTIONS Be(¹¹²Sn, X), E=1 GeV/nucleon; measured fragments isotopic yields; deduced evidence for ⁷⁶Y, ⁷⁸Zr, ¹⁰⁰Sn. Mass separator.

RADIOACTIVITY ⁷⁵Sr, ^77,78Y, ⁸⁰Zr, ⁸²Nb, ⁸⁴Mo, ⁸⁶Tc, ^88,89Ru, ⁹⁰Rh, ^92,93Pd, ⁹⁴Ag, ⁹⁸In, ¹⁰²Sn(β⁺), (EC) [from ¹¹²Sn fragmentation]; measured Eβ, Eγ, T_1/2. ⁷⁸Y, ⁸²Nb, ⁸⁶Tc, ⁹⁰Rh, ⁹⁴Ag, ⁹⁸In deduced Q(EC). Comparisons with model predictions.

doi: 10.1140/epja/i2001-10251-7

2002HU12

Phys.Rev. C66, 024318 (2002); Erratum Phys.Rev. C67, 019901 (2003)

M.A.Huertas

Effective Lagrangian approach to structure of selected nuclei far from stability

NUCLEAR STRUCTURE ⁷⁷Co, ^48,77,78,79Ni, ⁷⁹Cu, ^99,131In, ^{99,100,101,131,132,133}Sn, ¹³³Sb; calculated binding energies, single-particle level energies. ^100,132Sn; calculated nucleon density distributions. Effective Lagrangian approach.

doi: 10.1103/PhysRevC.66.024318

2002IS04

Eur.Phys.J. A 14, 29 (2002)

V.I.Isakov, K.I.Erokhina, H.Mach, M.Sanchez-Vega, B.Fogelberg

On the Difference between Proton and Neutron Spin-Orbit Splittings in Nuclei

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca, ^100,132Sn, ²⁰⁸Pb; calculated single-particle level energies, isotopic dependence of spin-orbit splitting. Several models compared.

doi: 10.1007/s10050-002-8786-1

2002IS08

Yad.Fiz. 65, 1466 (2002); Phys.Atomic Nuclei 65, 1431 (2002)

V.I.Isakov, K.I.Erokhina

Nuclear Masses and Properties of Nuclei in the Vicinity of the Remote Magic Nucleus ¹⁰⁰Sn

NUCLEAR STRUCTURE ^{96,97,98,99,100}Cd, ^{97,98,99,100,101}In, ^{98,99,100,101,102}Sn, ^{99,100,101,102,103}Sb, ^{100,101,102,103,104}Te; calculated mass differences. ^100,132Sn; calculated nucleon density distributions. ⁹²Mo, ⁹⁴Ru, ⁹⁶Pd, ⁹⁸Cd, ¹⁰⁰Sn; calculated levels, J, π, B(E2).

doi: 10.1134/1.1501655

2002MA54

Phys.Rev. C66, 024321 (2002)

Z.Y.Ma, L.Liu

Effective Dirac Brueckner-Hartree-Fock method for asymmetric nuclear matter and finite nuclei

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ^48,56,68Ni, ⁹⁰Zr, ^100,132Sn, ²⁰⁸Pb; calculated binding energies, radii. ¹⁶O, ^40,48Ca, ⁴⁸Ni; calculated spin-orbit splitting. Dirac-Brueckner-Hartree-Fock approach.

doi: 10.1103/PhysRevC.66.024321

2002NO08

Nucl.Phys. A704, 223c (2002)

F.Nowacki

Shell Model Description of Correlations in ⁵⁶Ni and ¹⁰⁰Sn

NUCLEAR STRUCTURE ^56,58,60Ni, ^100,102,104Sn; calculated level energies, B(E2), core polarization effects.

doi: 10.1016/S0375-9474(02)00782-0

2002RI17

Prog.Theor.Phys.(Kyoto), Suppl. 146, 120 (2002)

P.Ring

Relativistic Random Phase Approximation and Applications for Nuclei with Large Neutron Excess

NUCLEAR STRUCTURE ¹¹⁶Sn; calculated giant monopole resonance strength distribution. ^{100,114,120,132}Sn; calculated dipole strength distributions. Relativistic RPA.

2002SU31

Prog.Theor.Phys.(Kyoto), Suppl. 146, 437 (2002)

S.Sugimoto, K.Ikeda, H.Toki

Relativistic Mean Field Theory with Pion Field for Finite Nuclei

NUCLEAR STRUCTURE ¹²C, ¹⁶O, ⁴⁰Ca, ⁵⁶Ni, ⁸⁰Zr, ¹⁰⁰Sn, ¹⁶⁴Pb; calculated pion energies. Relativistic mean field theory.

2002TO22

Prog.Theor.Phys.(Kyoto) 108, 903 (2002)

H.Toki, S.Sugimoto, K.Ikeda

Relativistic mean-field theory with the pion in finite nuclei

NUCLEAR STRUCTURE ¹²C, ¹⁶O, ⁴⁰Ca, ⁵⁶Ni, ⁸⁰Zr, ¹⁰⁰Sn, ¹⁶⁴Pb; calculated binding energy, effect of pion mean field.

2003GI09

Nucl.Phys. A726, 3 (2003)

G.Giambrone, S.Scheit, F.Barranco, P.F.Bortignon, G.Colo, D.Sarchi, E.Vigezzi

Collective excitations in superfluid nuclei with finite-range interactions

NUCLEAR STRUCTURE ^{16,17,18,19,20,21,22,23,24,26}O, ^{56,58,60,62,64,66,68}Ni, ^{100,102,112,116,120,124,130,132}Sn; calculated binding energies, radii, density, pairing energy, transitions B(E2). ^{56,58,60,62,64,66,68}Ni, ^{112,116,120,124}Sn; calculated GQR energy, strength distributions. Quasiparticle RPA, Gogny force, comparison with data.

doi: 10.1016/S0375-9474(03)01602-6

2003ID01

Phys.Rev. C 67, 014322 (2003)

R.Id Betan, R.J.Liotta, N.Sandulescu, T.Vertse

Shell model in the complex energy plane and two-particle resonances

NUCLEAR STRUCTURE ⁷⁸Ni, ¹⁰⁰Sn; calculated single-particle states, two-particle resonance features. Shell model in the complex energy plane.

doi: 10.1103/PhysRevC.67.014322

2003SU22

Nucl.Phys. A721, 669c (2003)

S.Sugimoto, H.Toki, K.Ikeda

Surface pion condensation in finite nuclei

NUCLEAR STRUCTURE ¹²C, ¹⁶O, ⁴⁰Ca, ⁵⁶Ni, ⁸⁰Zr, ¹⁰⁰Sn, ¹⁶⁴Pb; calculated pion mean field, pion energy per nucleon. Relativistic mean field approach.

doi: 10.1016/S0375-9474(03)01149-7

2003SU27

Nucl.Phys. A722, 360c (2003)

S.Sugimoto, H.Toki, K.Ikeda, N.Minkov

Relativistic mean field theory with the pion of finite nuclei

NUCLEAR STRUCTURE ¹²C, ¹⁶O, ⁴⁰Ca, ⁵⁶Ni, ⁸⁰Zr, ¹⁰⁰Sn, ¹⁶⁴Pb; calculated pion mean field, pion energy per nucleon. Relativistic mean field approach.

doi: 10.1016/S0375-9474(03)01390-3

2003TO16

J.Korean Phys.Soc. 43, S6 (2003)

H.Toki, K.Ikeda, S.Sugimoto

Surface Pion Condensation of Finite Nuclei in Relativistic Mean Field Theory

NUCLEAR STRUCTURE ¹²C, ¹⁶O, ⁴⁰Ca, ⁵⁶Ni, ⁸⁰Zr, ¹⁰⁰Sn, ¹⁶⁴Pb; calculated pion mean-field potential energy. Relativistic mean field theory.

2003TO24

Eur.Phys.J. A 18, 363 (2003)

H.Toki, K.Ikeda, S.Sugimoto

Surface pion condensation in finite nuclei

NUCLEAR STRUCTURE ¹²C, ¹⁶O, ⁴⁰Ca, ⁵⁶Ni, ⁸⁰Zr, ¹⁰⁰Sn, ¹⁶⁴Pb; calculated pion mean-field potential energy. Relativistic mean field theory.

doi: 10.1140/epja/i2002-10238-x

2004AG04

Phys.Rev. C 70, 014308 (2004)

B.K.Agrawal, S.Shlomo

Consequences of self-consistency violations in Hartree-Fock random-phase approximation calculations of the nuclear breathing mode energy

NUCLEAR STRUCTURE ^40,60Ca, ⁵⁶Ni, ^80,90,110Zr, ¹⁰⁰Sn, ²⁰⁸Pb; calculated giant monopole resonance energies, effect of self-consistency violations. Hartree-Fock RPA.

doi: 10.1103/PhysRevC.70.014308

2004AM11

Phys.Rev. C 70, 024607 (2004)

K.Amos, S.Karataglidis, J.Dobaczewski

Probing the densities of Sn isotopes

NUCLEAR STRUCTURE ^{100,110,120,130,140,150,160,170}Sn; calculated particle density distributions, radii, wave functions. HFB model, Skyrme interaction.

NUCLEAR REACTIONS ^{100,102,104,106,108,110,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176}Sn(p, p), E=200 MeV; calculated σ, σ(θ). ^{116,118,120,122,124}Sn(p, p), E=39.8, 65 MeV; calculated σ(θ), polarization observables. HFB model, Skyrme interaction.

doi: 10.1103/PhysRevC.70.024607

2004BA45

J.Phys.(London) G30, 759 (2004)

T.Babacan, D.Salamov, A.Kucukbursa, H.Babacan, I.Maras, H.A.Aygor, A.Unal

The effect of the pairing interaction on the energies of isobar analogue resonances in ^112-124Sb and isospin admixture in ^100-124Sn isotopes

NUCLEAR STRUCTURE ^{112,114,116,118,120,122,124}Sb; calculated IAR energies, pairing interaction effect. ^{100,102,104,106,108,110,112,114,116,118,120,122,124}Sn; calculated ground state isospin admixtures, pairing interaction effect. Comparisons with data.

NUCLEAR REACTIONS ^{112,114,116,118,120,122,124}Sn(³He, t), E=200 MeV; calculated σ(θ), volume integral. Comparison with data.

doi: 10.1088/0954-3899/30/6/006

2004CO10

Nucl.Phys. A738, 108 (2004)

M.Colonna, S.Ayik, V.Baran, Ph.Chomaz, M.Di Toro

Dynamics of cluster formation in liquid-gas phase transitions

NUCLEAR STRUCTURE ^36,40,48Ca, ^100,120,132Sn; calculated cluster formation arising from unstable collective modes.

doi: 10.1016/j.nuclphysa.2004.04.018

2004CO13

Phys.Rev. C 70, 024307 (2004)

G.Colo, N.Van Giai, J.Meyer, K.Bennaceur, P.Bonche

Microscopic determination of the nuclear incompressibility within the nonrelativistic framework

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ^56,78Ni, ^100,132Sn, ²⁰⁸Pb; analyzed binding energies, radii; deduced parameters. ²⁰⁸Pb; calculated giant monopole resonance energy; deduced nuclear incompressibility.

doi: 10.1103/PhysRevC.70.024307

2004IK02

Nucl.Phys. A738, 73 (2004)

K.Ikeda, S.Sugimoto, H.Toki

New mean field theory with the parity and charge mixing for the pion in nuclei

NUCLEAR STRUCTURE ¹²C, ¹⁶O, ⁴⁰Ca, ⁵⁶Ni, ⁸⁰Zr, ¹⁰⁰Sn, ¹⁶⁴Pb; calculated pion energy per nucleon as a function of pion-nucleon coupling constant.

doi: 10.1016/j.nuclphysa.2004.04.014

2004ME13

Pramana 62, 841 (2004)

M.S.Mehta, T.K.Jha, S.K.Patra, R.K.Gupta

Potential energy surfaces for N = Z, ²⁰Ne-¹¹²Ba nuclei

NUCLEAR STRUCTURE ²⁰Ne, ²⁴Mg, ²⁸Si, ³²S, ³⁶Ar, ⁴⁰Ca, ⁴⁴Ti, ⁴⁸Cr, ⁵²Fe, ⁵⁶Ni, ⁶⁰Zn, ⁶⁴Ge, ⁶⁸Se, ⁷²Kr, ⁷⁶Sr, ⁸⁰Zr, ⁸⁴Mo, ⁸⁸Ru, ⁹²Pd, ⁹⁶Cd, ¹⁰⁰Sn, ¹⁰⁴Te, ¹⁰⁸Xe, ¹¹²Ba; calculated energy vs deformation. Deformed relativistic mean field approach.

2004PE03

Int.J.Mod.Phys. E13, 175 (2004)

S.Peru, J.F.Berger

Giant resonances in exotic spherical nuclei within the HF + RPA approach

NUCLEAR STRUCTURE ⁷⁸Ni, ^100,132Sn; calculated giant resonance strength distributions, related features.

doi: 10.1142/S0218301304001916

2004YO01

Phys.Rev. C 69, 024318 (2004)

S.Yoshida, H.Sagawa

Neutron skin thickness and equation of state in asymmetric nuclear matter

NUCLEAR STRUCTURE ^100,132Sn, ^182,208Pb; calculated relative binding energies, neutron skin thicknesses, dependence on equation of state. Skyrme Hartree-Fock and relativistic mean-field models.

doi: 10.1103/PhysRevC.69.024318

2005AG10

Phys.Rev. C 72, 014310 (2005)

B.K.Agrawal, S.Shlomo, V.K.Au

Determination of the parameters of a Skyrme type effective interaction using the simulated annealing approach

NUCLEAR STRUCTURE ^16,24O, ³⁴Si, ^40,48Ca, ^48,56,68,78Ni, ⁸⁸Sr, ⁹⁰Zr, ^100,132Sn, ²⁰⁸Pb; analyzed binding energies, radii, breathing-mode energies, related data; deduced Skyrme parameters. ⁴⁰Ca, ²⁰⁸Pb; calculated single-particle energies. Simulated annealing approach.

doi: 10.1103/PhysRevC.72.014310

2005AL41

J.Phys.(London) G31, S1819 (2005)

D.Almehed, P.D.Stevenson

Isovector giant monopole resonances in spherical nuclei

NUCLEAR STRUCTURE ⁹⁰Zr, ^100,120,132Sn, ¹⁴⁰Ce, ²⁰⁸Pb; calculated isovector giant monopole resonance energies, energy-dependent mixing with isoscalar resonance. Time-dependent Hartree-Fock method, Skyrme forces.

doi: 10.1088/0954-3899/31/10/079

2005AN21

Phys.Lett. B 623, 37 (2005)

A.Ansari

Study of the lowest 2⁺ excitations and B(E2) transition strengths in relativistic QRPA for Sn-, and Pb-isotopes

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136}Sn, ^{204,206,208,210}Pb; ; calculated levels energies, B(E2), B(E3). Relativistic quasiparticle RPA, comparison with data.

doi: 10.1016/j.physletb.2005.07.031

2005DU13

Int.J.Mod.Phys. E14, 493 (2005)

N.Dubray, J.Dudek, N.Schunck

The problem of universality of nuclear mean-field parametrizations

NUCLEAR STRUCTURE ^40,48Ca, ⁵⁶Ni, ⁹⁰Zr, ^100,132Sn, ¹⁴⁶Gd, ²⁰⁸Pb; analyzed neutron and proton single-particle level energies; deduced mean-field parameters.

doi: 10.1142/S0218301305003326

2005KA47

Eur.Phys.J. A 25, Supplement 1, 135 (2005)

M.Karny, L.Batist, A.Banu, F.Becker, A.Blazhev, K.Burkard, W.Bruchle, J.Doring, T.Faestermann, M.Gorska, H.Grawe, Z.Janas, A.Jungclaus, M.Kavatsyuk, O.Kavatsyuk, R.Kirchner, M.La Commara, S.Mandal, C.Mazzocchi, K.Miernik, I.Mukha, S.Muralithar, C.Plettner, A.Plochocki, E.Roeckl, M.Romoli, K.Rykaczewski, M.Schadel, K.Schmidt, R.Schwengner, J.Zylicz

Beta-decay studies near ¹⁰⁰Sn

RADIOACTIVITY ¹⁰²Sn(β⁺) [from ⁵⁸Ni(⁵⁰Cr, X)]; measured Eγ, Iγ, γγ-coin, Eβ, B(GT). ¹⁰²In levels deduced β-feeding intensities, log ft, hindrance factor. ¹⁰⁰Sn(β⁺); analyzed data; deduced B(GT), hindrance factor.

NUCLEAR REACTIONS ⁵⁸Ni(⁵⁰Cr, X)¹⁰¹Sn/¹⁰²Sn/¹⁰³Sn/¹⁰⁴Sn/¹⁰⁵Sn, E ≈ 5 MeV/nucleon; measured production σ. ⁵⁸Ni(⁵⁰Cr, X)¹⁰⁰Sn, E=5.8 MeV/nucleon; deduced approximate production σ.

doi: 10.1140/epjad/i2005-06-037-9

2005PA12

J.Phys.(London) G31, 185 (2005)

P.Papakonstantinou, E.Mavrommatis, J.Wambach, V.Yu.Ponomarev

A microscopic investigation of the transition form factor in the region of collective multipole excitations of stable and unstable nuclei

NUCLEAR STRUCTURE ^56,78,110Ni, ^100,120,132Sn; calculated isoscalar and isovector response functions, transition form factor. Self-consistent Skyrme-Hartree-Fock plus continuum RPA model.

doi: 10.1088/0954-3899/31/3/003

2005PE21

Eur.Phys.J. A 26, 25 (2005)

S.Peru, J.F.Berger, P.F.Bortignon

Giant resonances in exotic spherical nuclei within the RPA approach with the Gogny force

NUCLEAR STRUCTURE ⁷⁸Ni, ^100,132Sn, ²⁰⁸Pb; calculated giant resonance energies, strength distributions, related features. Gogny force, RPA approach.

doi: 10.1140/epja/i2005-10149-4

2005TE01

Phys.Rev. C 71, 034310 (2005)

J.Terasaki, J.Engel, M.Bender, J.Dobaczewski, W.Nazarewicz, M.Stoitsov

Self-consistent description of multipole strength in exotic nuclei: Method

NUCLEAR STRUCTURE ^{100,120,174,176}Sn; calculated isoscalar and isovector monopole, dipole, and quadrupole strength functions. Self-consistent quasiparticle RPA.

doi: 10.1103/PhysRevC.71.034310

2005TY01

Phys.Rev. C 71, 064301 (2005)

S.Typel

Relativistic model for nuclear matter and atomic nuclei with momentum-dependent self-energies

NUCLEAR STRUCTURE ^16,24O, ^40,48Ca, ⁵⁶Ni, ^100,132Sn, ²⁰⁸Pb; calculated binding energies, surface thickness, diffraction and charge radii. ¹⁶O, ⁴⁸Ca, ⁵⁶Ni, ¹³²Sn, ²⁰⁸Pb; calculated spin-orbit splitting. ^100,132Sn, ²⁰⁸Pb; calculated single particle energies. Relativistic mean field calculations, density-dependent meson-nucleon coupling, isoscalar meson field and nucleon field derivatives coupling, comparison with data.

doi: 10.1103/PhysRevC.71.064301

2006AG07

Phys.Rev. C 73, 034319 (2006)

B.K.Agrawal, S.K.Dhiman, R.Kumar

Exploring the extended density-dependent Skyrme effective forces for normal and isospin-rich nuclei to neutron stars

NUCLEAR STRUCTURE ^16,24O, ^40,48Ca, ^48,56,68,78Ni, ⁸⁸Sr, ⁹⁰Zr, ^100,132Sn, ²⁰⁸Pb; binding energies, analyzed radii, single-particle energies; deduced parameters. Generalized Skyrme effective force.

doi: 10.1103/PhysRevC.73.034319

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

2006CA04

Phys.Rev. C 73, 014313 (2006)

L.G.Cao, U.Lombardo, C.W.Shen, N.Van Giai

From Brueckner approach to Skyrme-type energy density functional

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ^56,78Ni, ⁹⁰Zr, ^100,132Sn, ²⁰⁸Pb; calculated radii, binding energies, spin-orbit potentials, particle densities. Skyrme-type energy density functional.

doi: 10.1103/PhysRevC.73.014313

2006KR11

Phys.Rev.C 74, 064310 (2006)

S.Krewald, V.B.Soubbotin, V.I.Tselyaev, X.Vinas

Density matrix functional theory that includes pairing correlations

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132}Sn; calculated ground-state energies, two-neutron separation energies, related features. Quasilocal density matrix functional theory with pairing correlations.

doi: 10.1103/PhysRevC.74.064310

2006LI13

Chin.Phys.Lett. 23, 804 (2006)

M.Liu, N.Wang, Z.-X.Li, X.-Z.Wu

Neutron Skin Thickness of Nuclei and Effective Nucleon-Nucleon Interactions

NUCLEAR STRUCTURE ¹⁸O, ⁴⁸Ca, ^{114,116,118,120,122,124,132}Sn, ²⁰⁸Pb; calculated radii, neutron skin thickness. ^38,40,48,56Ca, ^82,90,96,116Zr, ^{92,100,112,130}Sn, ^{180,208,220,240}Pb; calculated neutron and proton density distributions. Skyrme energy density functional, comparisons with data.

doi: 10.1088/0256-307X/23/4/012

2006PA30

Phys.Atomic Nuclei 69, 1345 (2006)

N.Paar, P.Papakonstantinou, H.Hergert, R.Roth

Collective Excitations in the Unitary Correlation Operator Method and Relativistic QRPA Studies of Exotic Nuclei

NUCLEAR STRUCTURE ⁴⁰Ca; calculated single-particle level energies. ⁴He, ^16,24O, ³⁴Si, ^40,48Ca, ^48,56,68,78Ni, ⁸⁸Sr, ⁹⁰Zr, ^100,114,132Sn, ¹⁴⁶Gd, ²⁰⁸Pb; calculated binding energies. ¹⁶O, ^40,48Ca, ⁴²Ti, ⁴⁴Cr, ⁴⁶Fe, ⁹⁰Zr, ¹³²Sn, ²⁰⁸Pb; calculated transition strength distributions. Self-consistent RPA approach, unitary correlation operator method.

doi: 10.1134/S1063778806080114

2006PI06

Phys.Rev. C 73, 044325 (2006)

J.Piekarewicz

Pygmy dipole resonance as a constraint on the neutron skin of heavy nuclei

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132}Sn; calculated binding energies, radii, isovector dipole strength distributions, pygmy and giant dipole resonance features. Relativistic RPA approach.

doi: 10.1103/PhysRevC.73.044325

2006RO15

Phys.Rev. C 73, 044312 (2006)

R.Roth, P.Papakonstantinou, N.Paar, H.Hergert, T.Neff, H.Feldmeier

Hartree-Fock and many body perturbation theory with correlated realistic NN interactions

NUCLEAR STRUCTURE ⁴He, ^16,24O, ³⁴Si, ^40,48Ca, ^48,56,78Ni, ⁸⁸Sr, ⁹⁰Zr, ^100,114,132Sn, ¹⁴⁶Gd, ²⁰⁸Pb; calculated ground-state energies, radii. ¹⁶O, ⁴⁰Ca, ^100,132Sn, ²⁰⁸Pb; calculated single-particle energies. O, Ca, Ni, Sn; calculated ground-state energies for even-A isotopes. Correlated realistic nucleon-nucleon interactions.

doi: 10.1103/PhysRevC.73.044312

2006SH17

Phys.Atomic Nuclei 69, 1132 (2006)

S.Shlomo, T.Sil, V.K.Au, O.G.Pochivalov

Current Status of Equation of State of Nuclear Matter

NUCLEAR STRUCTURE ⁸⁰Zr, ^100,116Sn; calculated isoscalar strength distributions. ⁹⁰Zr, ¹¹⁶Sn, ¹⁴⁴Sm, ²⁰⁸Pb; calculated isoscalar giant monopole resonance energies. Fully self-consistent approach.

doi: 10.1134/S1063778806070064

2006SI10

Phys.Rev. C 73, 034316 (2006)

T.Sil, S.Shlomo, B.K.Agrawal, P.-G.Reinhard

Effects of self-consistency violation in Hartree-Fock RPA calculations for nuclear giant resonances revisited

NUCLEAR STRUCTURE ¹⁶O, ^40,60Ca, ⁵⁶Ni, ^80,90,110Zr, ^100,116Sn, ¹⁴⁴Sm, ²⁰⁸Pb; calculated isoscalar and isovector giant resonance energies, consequences of self-consistency violation. ²⁰⁸Pb; calculated giant resonance strength functions.

doi: 10.1103/PhysRevC.73.034316

2006TE06

Phys.Rev. C 74, 044301 (2006)

J.Terasaki, J.Engel

Self-consistent description of multipole strength: Systematic calculations

NUCLEAR STRUCTURE ^{36,38,40,42,44,46,48,50,52,54,56,58,60,62,64,66,68,70,72,74,76}Ca, ^{50,52,54,56,58,60,62,64,66,68,70,72,74,76,78,80,82,84,86,88,90,92,94,96,98}Ni, ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176}Sn; calculated isoscalar and isovector 0⁺, 1^-, 2⁺ strength functions, transition densities, partial energy-weighted sums. Quasiparticle RPA, Skyrme density functionals.

doi: 10.1103/PhysRevC.74.044301

2006VO08

Eur.Phys.J. A 29, 133 (2006)

W.von Oertzen

Dynamics of α-clusters in N = Z nuclei

NUCLEAR STRUCTURE ⁴He, ¹²C, ¹⁶O, ²⁰Ne, ²⁴Mg, ²⁸Si, ³²S, ³⁶Ar, ⁴⁰Ca, ⁵²Fe, ⁵⁶Ni, ⁷²Kr, ⁸⁰Zr, ¹⁰⁰Sn, ¹⁶⁴Pb; calculated binding energies, α-cluster features.

doi: 10.1140/epja/i2006-10076-x

2007AN16

Phys.Lett. B 649, 128 (2007)

A.Ansari, P.Ring

Magnetic dipole moment of the first excited 2⁺ state of Z = 50 isotopes and N = 82 isotones in relativistic QRPA

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134}Sn; calculated magnetic dipole moments. ¹³²Sn, ¹³⁴Te, ¹³⁶Xe, ¹³⁸Ba, ¹⁴⁰Ce, ¹⁴²Nd, ¹⁴⁴Sm, ¹⁴⁶Gd, ¹⁴⁸Dy, ¹⁵⁰Er, ¹⁵²Yb; calculated excited state level energies, magnetic dipole moments, proton pairing energy, binding energy. Relativistic quasiparticle RPA and relativistic Hartree-Bogoliubov models, comparison with data.

doi: 10.1016/j.physletb.2007.04.009

2007BE24

Bull.Rus.Acad.Sci.Phys. 71, 434 (2007); Izv.Akad.Nauk RAS, Ser.Fiz. 71, 448 (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

Analysis of Single-Particle Energies of Doubly Magic ^{100, 132}Sn Nuclei within the Dispersive Optical Model

NUCLEAR STRUCTURE ^{112,116,118,120,124}Sn; analyzed single-particle energies. ^100,132Sn; deduced estimate for single-particle energies of doubly-magic isotopes. Compared with dispersive optical model results.

doi: 10.3103/S1062873807030264

2007MO03

Eur.Phys.J. A 31, 23 (2007)

P.Mohr

Super-allowed α decay above doubly-magic ¹⁰⁰Sn and properties of ¹⁰⁴Te = ¹⁰⁰Sn (X) α

RADIOACTIVITY ^104,105,106Te, ^108,109,110Xe, ^212,213,214Po, ^216,217,218Rn(α); calculated α-decay T_1/2, Qα, preformation factors. Double-folding potentials.

doi: 10.1140/epja/i2006-10168-7

2007PA08

Phys.Rev. C 75, 014310 (2007)

P.Papakonstantinou, R.Roth, N.Paar

Nuclear collective excitations using correlated realistic interactions: The role of explicit random-phase approximation correlations

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca, ⁹⁰Zr, ¹⁰⁰Sn, ²⁰⁸Pb; calculated giant resonance energies, strength distributions.

doi: 10.1103/PhysRevC.75.014310

2007RE23

Eur.Phys.J. A 32, 19 (2007)

P.-G.Reinhard, L.Guo, J.A.Maruhn

Nuclear giant resonances and linear response

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca, ^100,120,132Sn, ²⁰⁸Pb; calculated isovector dipole and isoscalar quadrupole GR strength distributions using time dependent HF dynamics using Skyrme forces.

doi: 10.1140/epja/i2007-10366-9

2007RO22

Nucl.Phys. A788, 12c (2007)

R.Roth, H.Hergert, N.Paar, P.Papakonstantinou

Nuclear Structure in the UCOM Framework: From Realistic Interactions to Collective Excitations

NUCLEAR STRUCTURE ⁴He, ^16,24O, ³⁴Si, ^40,48Ca, ^48,56,78Ni, ⁸⁸Sr, ⁹⁰Zr, ^100,114,132Sn, ¹⁴⁶Gd, ²⁰⁸Pb; calculated ground-state energies. ⁴⁰Ca, ⁹⁰Zr, ²⁰⁸Pb; calculated giant resonance strength distributions. Unitary correlation operator method, no-core shell model, Hartree-Fock, RPA, many-body perturbation theory. Comparison with data.

doi: 10.1016/j.nuclphysa.2007.01.008

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

2007VI01

Int.J.Mod.Phys. E16, 249 (2007)

X.Vinas, V.I.Tselyaev, V.B.Soubbotin, S.Krewald

Quasilocal density functional theory for nuclei including pairing correlations

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ⁹⁰Zr, ¹³²Sn, ²⁰⁸Pb; calculated binding energies, radii. ^{198,200,202,204,206,210,212}Pb; calculated binding energies. ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132}Sn; calculated pair gap energies. Density functional theory.

doi: 10.1142/S0218301307005697

2008BA53

Phys.Rev.Lett. 101, 252501 (2008)

D.Bazin, F.Montes, A.Becerril, G.Lorusso, A.Amthor, T.Baumann, H.Crawford, A.Estrade, A.Gade, T.Ginter, C.J.Guess, M.Hausmann, G.W.Hitt, P.Mantica, M.Matos, R.Meharchand, K.Minamisono, G.Perdikakis, J.Pereira, J.Pinter, M.Portillo, H.Schatz, K.Smith, J.Stoker, A.Stolz, R.G.T.Zegers

Production and β Decay of rp-Process Nuclei ⁹⁶Cd, ⁹⁸In, and ¹⁰⁰Sn

NUCLEAR REACTIONS ⁹Be(¹¹²Sn, X)⁹⁶Cd/⁹⁸In/¹⁰⁰Sn, E=120 MeV/nucleon; measured cross sections.

RADIOACTIVITY ⁹⁶Cd, ⁹⁸In, ¹⁰⁰Sn; measured decay spectra, half-lives.

doi: 10.1103/PhysRevLett.101.252501

2008ER05

Eur.Phys.J. A 37, 81 (2008)

J.Erler, P.Klupfel, P.-G.Reinhard

A stabilized pairing functional

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142}Sn; calculated average neutron-, proton-pairing gaps, binding energy, charge radius and low-lying 2⁺ state energy. Comparison with data.

doi: 10.1140/epja/i2008-10615-5

2008HA13

Nucl.Phys. A803, 159 (2008)

M.M.Haidari, M.M.Sharma

Sigma-omega meson coupling and properties of nuclei and nuclear matter

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ⁷⁶Ni, ⁹⁰Zr, ^{100,116,124,132}Sn, ^202,208,214Pb; calculated binding energies and charge radii of spherical nuclei. ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134}Sn; calculated binding energies. ^202,208,214Pb; calculated charge radii and isotopic shifts. ^36,38,40,42Si, ^80,86,88Sr, ^108,110Mo, ¹²⁰Xe, ¹⁷⁴Yb; calculated binding energies and quadrupole deformation. ⁹⁰Zr, ¹²⁰Sn, ²⁰⁸Pb; calculated GMR energies. Lagrangian model using relativistic mean field theory meson coupling.

doi: 10.1016/j.nuclphysa.2008.02.296

2008KO09

Phys.Rev. C 77, 064307 (2008)

M.Kortelainen, J.Dobaczewski, K.Mizuyama, J.Toivanen

Dependence of single-particle energies on coupling constants of the nuclear energy density functional

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ^48,56Ni, ^100,132Sn, ²⁰⁸Pb; calculated single particle levels, regression coefficients, neutron densities, coupling constants. Energy density functional methods, Skyrme functionals.

doi: 10.1103/PhysRevC.77.064307

2008LI30

Phys.Rev. C 78, 014312 (2008); Erratum Phys.Rev. C 78, 049902 (2008)

E.Litvinova, P.Ring, V.Tselyaev

Relativistic quasiparticle time blocking approximation: Dipole response of open-shell nuclei

NUCLEAR STRUCTURE ⁸⁸Sr, ⁹⁰Zr, ⁹²Mo, ^{100,106,114,116,120,130}Sn; calculated dipole spectra, photoproduction σ, B(E1). Relativistic quasiparticle random phase approximation.

doi: 10.1103/PhysRevC.78.014312

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

2008NA25

Phys.Rev. C 78, 054301 (2008)

H.Nakada

Mean-field approach to nuclear structure with semi-realistic nucleon-nucleon interactions

NUCLEAR STRUCTURE ^16,24O, ^40,48Ca, ⁹⁰Zr, ¹³²Sn, ²⁰⁸Pb; calculated binding energies, rms matter radii. ^{14,16,18,20,22,24,26,28}O, ⁴⁰Ca, ²⁰⁸Pb; calculated single-particle energies. ^{18,20,22,24,26}O; calculated two-neutron separation energy. Comparison with experimental data. Mean-field Hartree-Fock, Hartree-Fock-Bogoliubov calculations.

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140}Sn; calculated mass differences. Comparison with experimental data.

doi: 10.1103/PhysRevC.78.054301

2008PI04

Phys.Rev. C 78, 024305 (2008)

N.Pillet, J.-F.Berger, E.Caurier

Variational multiparticle-multihole configuration mixing method applied to pairing correlations in nuclei

NUCLEAR STRUCTURE ^100,106,116Sn; calculated correlation energies, wave functions, levels, configurations. ^{100,106,112,114,116,118,120,122,124,132}Sn; calculated charge radii, energies of first excited 0⁺ state. Variational multiparticle-multihole configuration mixing method. Comparison with experimental data. DIS parameterization of Gogny force.

doi: 10.1103/PhysRevC.78.024305

2008TS01

Phys.Rev. C 77, 024321 (2008)

N.Tsoneva, H.Lenske

Pygmy dipole resonances in the tin region

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132}Sn; calculated nucleon densities, B(E1), energy of first 1^- state, configurations, pygmy-dipole resonance strengths, dipole transition densities, dipole energies, cross sections.

doi: 10.1103/PhysRevC.77.024321

2008TS02

J.Phys.(London) G35, 014047 (2008)

N.Tsoneva, H.Lenske

Low-energy dipole excitations in nuclei at the N = 50, 82 and Z = 50 shell closures as signatures for a neutron skin

NUCLEAR STRUCTURE ⁸⁸Sr, ⁹⁰Zr, ^{100,102,106,108,110,112,122,132}Sn, ¹³⁶Xe, ¹³⁸Ba, ¹⁴⁰Ce, ¹⁴²Nd, ¹⁴⁴Sm; Z=50; N=50, 82; calculated one-phonon dipole transition densities, total PDR strength. Hartree-Fock-Bogoljubov (HFB) and quasiparticle-phonon model (QPM).

doi: 10.1088/0954-3899/35/1/014047

2008ZA02

Phys.Rev. C 77, 024316 (2008)

M.Zalewski, J.Dobaczewski, W.Satula, T.R.Werner

Spin-orbit and tensor mean-field effects on spin-orbit splitting including self-consistent core polarizations

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ⁵⁶Ni, ⁹⁰Zr, ¹³²Sn, ²⁰⁸Pb; calculated single particle energies, spin-orbit splittings, grounds state energies. ¹⁶O, ^40,48Ca, ⁵⁶Ni, ⁹⁰Zr, ^100,132Sn, ²⁰⁸Pb; analyzed single particle levels.

doi: 10.1103/PhysRevC.77.024316

2009BE45

Phys.Rev. C 80, 064302 (2009)

M.Bender, K.Bennaceur, T.Duguet, P.-H.Heenen, T.Lesinski, J.Meyer

Tensor part of the Skyrme energy density functional. II. Deformation properties of magic and semi-magic nuclei

NUCLEAR STRUCTURE ^40,48Ca, ^56,68,78Ni, ^{80,90,96,100,110}Zr, ^100,120,132Sn, ^186,208Pb; calculated proton and neutron Nilsson diagrams, single-particle energy spectra, deformation energy curves, isoscalar tensor energies using nuclear energy density functionals (EDF) and T22, T26, T44, T62, SLy5, SLy5+T, SLy4, SLy4T, SLy4T(min), SLy4T(self) and TZA parametrizations. Investigated impact of tensor terms in the Skyrme energy density functional on deformation properties of magic and semi-magic nuclei.

doi: 10.1103/PhysRevC.80.064302

2009BO22

Int.J.Mod.Phys. E18, 951 (2009)

L.Bonneau, J.Le Bloas, P.Quentin, J.Bartel, D.Strottman

Isospin mixing in the higher Tamm-Dancoff approximation

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca, ⁵⁶Ni, ¹⁰⁰Sn; calculated mass excess; ¹⁰⁰Sn; calculated isospin mixing.

doi: 10.1142/S0218301309013099

2009GA39

Phys.Rev. C 80, 054305 (2009)

M.K.Gaidarov, G.Z.Krumova, P.Sarriguren, A.N.Antonov, M.V.Ivanov, E.Moya de Guerra

Momentum distributions in medium and heavy exotic nuclei

NUCLEAR STRUCTURE ^50,64,78Ni, ^84,86,98Kr, ^100,120,136Sn; calculated proton, neutron, and total momentum distributions using self-consistent mean-field Skyrme Hartree-Fock + BCS method.

doi: 10.1103/PhysRevC.80.054305

2009HE09

Phys.Rev. C 79, 057602 (2009)

M.Hemalatha, Y.K.Gambhir, W.Haider, S.Kailas

Predicted weakening of the spin-orbit interaction with the addition of neutrons

NUCLEAR REACTIONS ^{76,78,80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110}Zr(polarized p, p), E=39.6, 50 MeV; ^{96,98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136}Sn(polarized p, p), E=22.5, 50 MeV; calculated volume integral per nucleon, σ, analyzing powers using microscopic proton-nucleus optical potential in the framework of first-order Brueckner theory with Urbana V14 soft core interaction. Comparison with experimental data.

doi: 10.1103/PhysRevC.79.057602

2009HE14

Phys.Rev. C 80, 024312 (2009)

H.Hergert, R.Roth

Pairing in the framework of the unitary correlation operator method (UCOM): Hartree-Fock-Bogoliubov calculations

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132}Sn; calculated ground state energies, charge radii, canonical single-particle spectra, canonical and average gaps using self-consistent Hartree-Fock-Bogoliubov framework and effective interactions from the unitary correlation operator method (UCOM). Comparison with experimental data.

doi: 10.1103/PhysRevC.80.024312

2009LA11

Phys.Rev. C 79, 054615 (2009)

E.G.Lanza, F.Catara, D.Gambacurta, M.V.Andres, Ph.Chomaz

Multiphonon excitations and pygmy resonances in tin isotopes

NUCLEAR REACTIONS ^100,120,132Sn(γ, γ'), E not given; calculated proton and neutron densities, isoscalar strength distributions for monopole, quadrupole and octupole states, isovector strength distributions for dipole states, transition probabilities, transition densities for low-lying dipole state for pygmy dipole resonance and giant dipole resonance. Microscopic RPA and boson expansion calculations. ^120,132Sn(²⁰⁸Pb, X), E=500 MeV/nucleon; calculated relativistic Coulomb inelastic cross sections using coupled-channel method.

doi: 10.1103/PhysRevC.79.054615

2009LA22

Phys.Rev. C 80, 041301 (2009)

G.A.Lalazissis, S.Karatzikos, M.Serra, T.Otsuka, P.Ring

Covariant density functional theory: The role of the pion

NUCLEAR STRUCTURE ^40,48Ca, ^48,56Ni, ^100,132Sn, ²⁰⁸Pb, Sn A=116-152; calculated binding energies, single particle energies and spin orbit splitting of the doublets using relativistic mean field (RMF) theory and relativistic Hartree-Fock approximation. Discussed the role of the pion in covariant density functional theory. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.041301

2009NA43

Eur.Phys.J. A 42, 565 (2009)

H.Nakada

Mean-field and RPA approaches to stable and unstable nuclei with semi-realistic interactions

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ²⁰⁸Pb; calculated binding energies, rms radii. ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144}Sn; calculated proton single-particle levels. ^16,24O; calculated levels, J, π. ²⁰⁸Pb; calculated B(M1). Comparison with data.

doi: 10.1140/epja/i2008-10750-y

2009RO06

Phys.Rev. C 79, 054308 (2009)

V.Rotival, T.Duguet

New analysis method of the halo phenomenon in finite many-fermion systems: First applications to medium-mass atomic nuclei

NUCLEAR STRUCTURE ^{54,56,58,60,62,64,66,68,70,72,74,76,78,80}Cr, ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170}Sn; calculated neutron densities, neutron canonical and two-neutron separation energies, charge and Helm rms radii for protons and neutrons, halo parameters using Hartree-Fock-Bogoliubov calculations with Skyrme plus pairing functionals.

doi: 10.1103/PhysRevC.79.054308

2009SA24

Phys.Rev.Lett. 103, 012502 (2009)

W.Satula, J.Dobaczewski, W.Nazarewicz, M.Rafalski

Isospin Mixing in Nuclei within the Nuclear Density Functional Theory

NUCLEAR STRUCTURE ^{40,42,44,46,48,50,52,54,56,58,60}Ca, ¹⁰⁰Sn; calculated isospin-mixing parameters. Extended mean-field approach.

doi: 10.1103/PhysRevLett.103.012502

2009TI04

Phys.Rev. C 79, 064301 (2009)

Y.Tian, Z.-y.Ma, P.Ring

Separable pairing force for relativistic quasiparticle random-phase approximation

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136}Sn, ¹²²Zr, ¹²⁴Mo, ¹²⁶Ru, ¹²⁸Pd, ¹³⁰Cd, ¹³²Sn, ¹³⁴Te, ¹³⁶Xe, ¹³⁸Ba, ¹⁴⁰Ce, ¹⁴²Nd, ¹⁴⁴Sm, ¹⁴⁶Gd, ¹⁴⁸Dy, ¹⁵⁰Er, ¹⁵²Yb; calculated energies of first 2+, first and second 3-, B(E2), proton average gap, and isoscalar giant monopole resonance (ISGMR) using Relativistic Hartree-Bogoliubov (RHB) and relativistic quasiparticle random phase approximation (RQRPA). Comparison with experimental data.

doi: 10.1103/PhysRevC.79.064301

2009ZA08

Phys.Rev. C 80, 064307 (2009)

M.Zalewski, P.Olbratowski, M.Rafalski, W.Satula, T.R.Werner, R.A.Wyss

Global nuclear structure effects of the tensor interaction

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ⁵⁶Ni, ^80,90Zr, ^100,132Sn, ²⁰⁸Pb; calculated binding energies, mechanism for superdeformed structures, and potential energy curves using energy-density-functional (EDF) methods with spherical and deformed HFB approaches and SLy4T interaction. Z=1-84, N=1-130; calculated tensor contribution to nuclear binding energy. Comparison with experimental data.

doi: 10.1103/PhysRevC.80.064307

2010AF02

Phys.Rev. C 82, 034329 (2010)

A.V.Afanasjev, H.Abusara

Time-odd mean fields in covariant density functional theory: Rotating systems

NUCLEAR STRUCTURE ⁴⁷V, ⁶⁰Zn, ⁹²Mo, ¹⁰⁰Sn, ¹⁰⁸Cd, ¹¹⁸Te, ¹¹⁸Ba, ¹³⁶Nd, ¹⁴²Sm, ¹⁴⁶Gd, ¹⁵²Dy, ^158,160Eu, ¹⁹⁴Pb; calculated proton-single particle energies, kinematic and dynamic moments of inertia, transition quadrupole moments and hexadecapole moments, and neutron current distributions for normal-deformed (ND), superdeformed (SD), hyperdeformed (HD) structures and terminating states in a rotating frame. Z=50-74, N=50-110; Z=42-58, N=44-78; calculated contribution of nuclear magnetism (NM) to kinematic moments of inertia for ND, SD and HD structures. Z=63, N=131-209; calculated contribution of nuclear magnetism to binding energies of odd-odd Eu nuclei. Time-odd mean field (nuclear magnetism) calculations in the framework of covariant density functional theory (CDFT).

doi: 10.1103/PhysRevC.82.034329

2010AY04

Phys.Atomic Nuclei 73, 922 (2010)

H.Aytekin, R.Baldik, E.Tel

Calculation of the ground state properties of even-even Sn isotopes

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148,150,152,154,156}Sn; calculated binding energies, neutron and proton density radii, rms nuclear charge radii. Skyrme-Hartree-Fock-Bogolyubov (SHFB) methods.

doi: 10.1134/S1063778810060025

2010BA51

Eur.Phys.J. A 46, 45 (2010)

L.Batist, M.Gorska, H.Grawe, Z.Janas, M.Kavatsyuk, M.Karny, R.Kirchner, M.La Commara, I.Mukha, A.Plochocki, E.Roeckl

Systematics of Gamow-Teller beta decay "Southeast" of ¹⁰⁰Sn

RADIOACTIVITY Z=44-50(β⁺), (EC); A=94-108(β⁺), (EC); analyzed BT transitions strengths, energy, centroid. ^100,101Sn(β⁺), (EC); deduced T_1/2, decay properties, β-quenching factor, Q-value. ¹⁰⁰Cd(β⁺), (EC); calculated ¹⁰⁰Ag T_1/2, isomer transition T_1/2.

doi: 10.1140/epja/i2010-11025-x

2010BH05

Phys.Rev. C 81, 044321 (2010)

A.Bhagwat, X.Vinas, M.Centelles, P.Schuck, R.Wyss

Microscopic-macroscopic approach for binding energies with the Wigner-Kirkwood method

NUCLEAR STRUCTURE ⁴⁰Ca, ¹³²Sn, ²⁰⁸Pb; calculated coulomb potential, Wigner-Kirkwood energies and ground state energies as function of quadrupole deformation. ^{136,138,140,142,144,146,148,150,152,154,156}Gd, ^{138,140,142,144,146,148,150,152,154,156,158}Dy, ^{178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214}Pb; calculated Strutinsky shell corrections. ^{38,40,42,44,46,48,50,52}Ca, ^{40,42,44,46,48,50,52}Sc, ^{40,42,44,46,48,50,52,54}Ti, ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134}Sn, ^{178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214}Pb; calculated binding energies, one-neutron and two-neutron separation energies. A=40-152, A=18-220; calculated binding energies for a set of 367 spherical nuclei. Classical Wigner-Kirkwood expansion method for spherical and deformed nuclei. Comparison with experimental data.

doi: 10.1103/PhysRevC.81.044321

2010CA23

Phys.Rev.Lett. 105, 122501 (2010)

B.G.Carlsson, J.Dobaczewski

Convergence of Density-Matrix Expansions for Nuclear Interactions

NUCLEAR STRUCTURE ⁴He, ¹⁶O, ^40,48Ca, ^56,78Ni, ^100,132Sn, ²⁰⁸Pb; calculated direct and exchange energies, rms deviations between the exact and approximate exchange energies, density matrix expansion.

doi: 10.1103/PhysRevLett.105.122501

2010CH34

Phys.Rev. C 82, 024321 (2010)

L.-W.Chen, Che Ming Ko, B.-A.Li, J.Xu

Density slope of the nuclear symmetry energy from the neutron skin thickness of heavy nuclei

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ^56,78Ni, ⁹⁰Zr, ^100,120,132Sn, ²⁰⁸Pb; calculated binding energies, charge rms radii, and neutron skin thickness using Skyrme-Hartree-Fock approach. Comparison with experimental data.

doi: 10.1103/PhysRevC.82.024321

2010GA08

Phys.Rev. C 81, 054316 (2010)

T.Gaitanos, A.B.Larionov, H.Lenske, U.Mosel

Breathing mode in an improved transport approach

NUCLEAR STRUCTURE ¹²C, ¹⁰⁰Sn; calculated rms radii, binding energies, neutron and proton density profiles, proton mean-field potentials. ¹²C, ⁵⁶Ni, ⁹⁶Ru, ^124,136Sn, ²⁰⁸Pb; calculated rms radii. A=10-210; calculated excitation energies and widths of giant-monopole resonances (GMR).Improved relativistic Boltzmann-Uehling-Uhlenbeck (BUU) transport approach.

doi: 10.1103/PhysRevC.81.054316

2010GU13

Phys.Rev. C 82, 024319 (2010)

A.Gunther, R.Roth, H.Hergert, S.Reinhardt

Systematics of binding energies and radii based on realistic two-nucleon plus phenomenological three-nucleon interactions

NUCLEAR STRUCTURE ⁴He, ^16,24O, ³⁴Si, ^40,48Ca, ^48,56,60,78Ni, ⁸⁸Sr, ⁹⁰Zr, ^100,114,132Sn, ¹⁴⁶Gd, ²⁰⁸Pb; calculated ground-state energies and binding energies per nucleon and charge radii of closed-shell nuclei. ⁴⁰Ca, ⁹⁰Zr; calculated single-particle spectra. Hartree-Fock calculations using MBPT, S-UCOM(SRG) and S-SRG interactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.82.024319

2010MA41

Phys.Rev. C 82, 024318 (2010)

M.Matsuo, Y.Serizawa

Surface-enhanced pair transfer amplitude in quadrupole states of neutron-rich Sn isotopes

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142}Sn; calculated average neutron gap, energies, B(E2) and transition densities, transition strength functions, pairing residual interactions associated with the first 2+ states. Investigated neutron pair transfer modes using QRPA based on the Skyrme-Hartree-Fock-Bogoliubov mean-fields. Comparisons with experimental data.

doi: 10.1103/PhysRevC.82.024318

2010MO13

Phys.Rev. C 81, 065803 (2010)

Ch.C.Moustakidis, T.Niksic, G.A.Lalazissis, D.Vretenar, P.Ring

Constraints on the inner edge of neutron star crusts from relativistic nuclear energy density functionals

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134}Sn, ^{196,198,200,202,204,206,208,210,212,214}Pb; calculated rms radii using Hartree-Bogoliubov (RHB) model. Comparison with experimental data.

doi: 10.1103/PhysRevC.81.065803

2010NI15

Nucl.Phys. A834, 370c (2010)

D.Ni, Z.Ren

α-decay calculations of light mass nuclei above doubly magic ¹⁰⁰Sn

RADIOACTIVITY ^{104,105,106,107,108,109,110}Te, ^{106,107,108,109,110,111,112,113}I, ^{108,109,110,111,112,113}Xe, ^{111,112,113,114}Cs, ^112,113,114Ba(α); analyzed Q-value; calculated T_1/2 using a generalized density-dependent cluster model. Comparison with data.

doi: 10.1016/j.nuclphysa.2010.01.042

2010OT01

Phys.Rev.Lett. 104, 012501 (2010)

T.Otsuka, T.Suzuki, M.Honma, Y.Utsuno, N.Tsunoda, K.Tsukiyama, M.Hjorth-Jensen

Novel Features of Nuclear Forces and Shell Evolution in Exotic Nuclei

NUCLEAR STRUCTURE Z=8-20, 28, 40, N=20, 40-50; ⁴⁰Ca, ⁶⁸Ni, ⁷⁸Ni, ⁹⁰Zr, ¹⁰⁰Sn; calculated monopole matrix elements, single-particle energies for pf and sd-shells; deduced monopole-based universal interaction, shell evolution. Comparison with USD, KB3, GXPF1A interactions.

doi: 10.1103/PhysRevLett.104.012501

2010SA13

Phys.Rev. C 81, 064322 (2010)

P.Salamon, A.T.Kruppa, T.Vertse

New method for calculating shell correction

NUCLEAR STRUCTURE ^{16,18,20,22,24}O, ²⁰Ne, ^40,48Ca, ^68,78Ni, ^90,122,124Zr, ^100,132Sn, ¹⁴⁶Gd, ^180,208Pb; calculated neutron shell corrections using the smoothed finite-range weight function and the generalized Strutinski procedure. Comparison with the semiclassical shell correction.

doi: 10.1103/PhysRevC.81.064322

2010SH32

Eur.Phys.J. A 46, 241 (2010)

Z.-q.Sheng, Z.-z.Ren

Deformed relativistic mean-field calculations on nuclei near Z = 50 with FSUGold

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136}Sn, ^{108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138}Te, ^{110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,138,140,142}Xe, ^{112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148}Ba; calculated binding energies, quadrupole deformation parameters, hexadecupole moments, charge radii, two-neutron separation energies. Deformed relativistic mean-field theory, comparison with experimental data.

doi: 10.1140/epja/i2010-11038-5

2010WA13

Phys.Rev. C 81, 054309 (2010)

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

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

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

doi: 10.1103/PhysRevC.81.054309

2010ZA03

Phys.Rev. C 81, 044314 (2010)

M.Zalewski, P.Olbratowski, W.Satula

Surface-peaked effective mass in the nuclear energy density functional and its influence on single-particle spectra

NUCLEAR STRUCTURE ⁴⁰Ca, ⁵⁶Ni, ¹⁰⁰Sn; calculated spin-orbit splittings, isoscalar particle densities, saturation density, binding energy, incompressibility modulus, effective mass for infinite nuclear matter with realistic nucleon-nucleon interactions using SkXc Skyrme functionals.

doi: 10.1103/PhysRevC.81.044314

2010ZA06

Int.J.Mod.Phys. E19, 794 (2010)

M.Zalewski, P.Olbratowski, W.Satula

The nuclear energy density functionals with modified radial dependence of the isoscalar effective mass

NUCLEAR STRUCTURE ⁴⁰Ca, ⁵⁶Ni, ¹⁰⁰Sn; calculated spin-orbit splitting, radial dependence. Standard Skyrme energy-density functionals (EDF).

doi: 10.1142/S0218301310015242

2010ZH45

Phys.Rev. C 82, 054319 (2010)

P.W.Zhao, Z.P.Li, J.M.Yao, J.Meng

New parametrization for the nuclear covariant energy density functional with a point-coupling interaction

NUCLEAR STRUCTURE ^16,18,20,22O, ¹⁸Ne, ²⁰Mg, ³⁴Si, ³⁶S, ³⁸Ar, ^{36,38,40,42,44,46,48,50}Ca, ^42,50Ti, ^56,58,72Ni, ⁸⁴Se, ⁸⁶Kr, ⁸⁸Sr, ⁹⁰Zr, ⁹²Mo, ⁹⁴Ru, ⁹⁸Cd, ^{100,106,108,112,116,120,122,124,126,128,130,132,134}Sn, ¹³⁴Te, ¹³⁶Xe, ¹³⁸Ba, ¹⁴⁰Ce, ¹⁴²Nd, ¹⁴⁴Sm, ¹⁴⁶Gd, ¹⁴⁸Dy, ¹⁵⁰Er, ²⁰⁶Hg, ^{200,202,204,206,208,210,212,214}Pb, ²¹⁰Po, ²¹²Rn, ²¹⁴Ra, ²¹⁶Th, ²¹⁸U; calculated binding energies and charge radii for spherical nuclei by PC-PK1 parametrization of energy density functional. Z=20, N=16-32; Z=28, N=26-44; Z=50, N=52-84; Z=82, N=100-132; Z=12-22, N=20; Z=30-46, N=50; Z=50-66, N=82; Z=80-92, N=126; Z=70, N=88-108; Z=92, N=138-148; deduced deviations of calculated binding energies from those in AME-2003. Z=8, N=6-22; Z=20, N=18-40; Z=28, N=28-50; Z=50, N=52-90; calculated S(2n) values. ¹⁶O, ⁴⁰Ca, ¹³²Sn, ²⁰⁸Pb; calculated single-particle energies. Z=50, N=56-82; Z=82, N=114-132; calculated charge radii and neutron skin thickness. ²⁴⁰Pu; calculated potential energy curve. ¹⁵⁰Nd; calculated yrast states and B(E2) values. ^{144,146,148,150,152,154}Nd; calculated E(4+)/E(2+) and B(E2) for first 2+ states. Comparison with experimental data and AME-2003.

doi: 10.1103/PhysRevC.82.054319

2011AB12

J.Phys.Soc.Jpn. 80, 104201 (2011)

M.H.E.Abu-Seileek

Doubly-Magic ¹⁰⁰Sn Nucleus with Delta Excitation under Compression

NUCLEAR STRUCTURE ¹⁰⁰Sn; calculated proton-, neutron-density distributions, single-particle energies of the lowest states, Δ orbitals. Hartree-Fock method.

doi: 10.1143/JPSJ.80.104201

2011AN17

Phys.Rev. C 83, 064306 (2011)

M.Anguiano, G.Co, V.De Donno, A.M.Lallena

Tensor effective interaction in self-consistent random-phase approximation calculations

NUCLEAR STRUCTURE ¹²C, ^{14,16,22,24,28}O, ^40,48,52,60Ca, ^48,56,68,78Ni, ⁹⁰Zr, ^{100,114,116,132}Sn, ²⁰⁸Pb; calculated energies of lowest 0- states, binding energies, neutron and proton rms radii, neutron and proton single-particle energies, neutron and proton energy gaps, single particle levels near the Fermi surface, level energies, J, π for N=Z nuclei with isoscalar and isovector characters. Hartree-Fock and random-phase approximation calculations with finite-range Gogny forces, with and without a tensor-isospin term.

NUCLEAR REACTIONS ¹²C, ⁴⁰Ca, ²⁰⁸Pb(e, e'), E not given; calculated transverse response as a function of the effective momentum transfer using RPA wave functions obtained in fully self-consistent approach. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.064306

2011AV04

Phys.Rev. C 83, 064316 (2011)

A.Avdeenkov, S.Goriely, S.Kamerdzhiev, S.Krewald

Self-consistent calculations of the strength function and radiative neutron capture cross section for stable and unstable tin isotopes

NUCLEAR STRUCTURE ^{100,110,112,114,120,124,132,136,142,150,156,166,176}Sn; calculated E1 strength functions, integral characteristics of GDR versus A, giant-dipole and pygmy-dipole resonances (GDR, PDR), neutron and proton transitional densities using self-consistent microscopic theory as well as standard quasiparticle random phase approximation (QRPA, QTBA). Comparison with experimental data. Discussed properties of GDR and PDR.

NUCLEAR REACTIONS ^123,131,149Sn(n, γ), E=0.001-10 MeV; calculated neutron capture cross sections obtained with E1 strength functions calculated within the QRPA, QTBA, and Kopecky-Uhl approaches.

doi: 10.1103/PhysRevC.83.064316

2011BE21

Bull.Rus.Acad.Sci.Phys. 75, 585 (2011); Izv.Akad.Nauk RAS, Ser.Fiz 75, 621 (2011)

O.V.Bespalova, T.A.Ermakova, A.A.Klimochkina, H.Koura, E.A.Romanovskii, T.I.Spasskaya

Evaluation and analysis of neutron single-particle energies in ⁷⁸Ni nucleus

NUCLEAR STRUCTURE ⁷⁸Ni, ⁹⁰Zr, ¹⁰⁰Sn; analyzed experimental data; calculated single-particle energies. Koura-Yamada potential.

doi: 10.3103/S1062873811040071

2011BE22

Phys.Rev. C 83, 064319 (2011)

M.Bender, P.-H.Heenen

What can be learned from binding energy differences about nuclear structure: The example of δV_pn

NUCLEAR STRUCTURE Z=15-100, N=15-150; ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132}Sn, ^{180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212}Pb, ^{120,122,124,126,128,130,132,134,136,138,140,142,144,146,148}Ba, ^{130,132,134,136,138,140,142,144,146,148,150,152,154}Nd, ^{140,142,144,146,148,150,152,154,156,158,160}Gd; A=130-210, N-Z=32; A=132, 168, N-Z=12-34; calculated maps of binding energy difference δV_pn, deformation of mean-field ground state. ^204,206Hg, ^206,208Pb; calculated decomposition of δV_pn into contributions from the different terms of the energy density functionals. Angular momentum and particle-number projected generator coordinate method and the Skyrme interaction SLy4Skyrme interaction SLy4. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.064319

2011BH06

Int.J.Mod.Phys. E20, 1663 (2011)

A.Bhagwat, Y.K.Gambhir

Evolution of shell structure in nuclei

NUCLEAR STRUCTURE ^{14,16,18,20,22,24,26,28,30,32}O, ^{54,56,58,60,62,64,66,68,70,72,74,76,78,80,82,84,86,88,90,92,94,96,98,100,102}Ni, ^{80,82,84,86,88,90,92,94,96,98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148,150,152,154}Zr, ^{98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174,176,178,180}Sn, ^{180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214,216,218,220,222,224,226,228,230,232,234,236,238,240,242,244,246,248,250,252,254,256,258,260,262,264,266,268,270,272}Pb, ^{130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166,168,170,172,174}Gd; calculated pairing energy, two-neutron separation energy. RMF calculations, comparison with experimental data.

doi: 10.1142/S0218301311019581

2011DO23

J.Phys.:Conf.Ser. 312, 092002 (2011)

J.Dobaczewski

Current Developments in Nuclear Density Functional Methods

NUCLEAR STRUCTURE ^40,48Ca, ^56,78Ni, ^100,132Sn, ²⁰⁸Pb; calculated proton radius, binding energy, mass excess using Gogny D1S and second-order Skyrme-like EDF (energy density formalism).

doi: 10.1088/1742-6596/312/9/092002

2011GA37

Phys.Rev. C 84, 024301 (2011)

D.Gambacurta, L.Li, G.Colo, U.Lombardo, N.Van Giai, W.Zuo

Determination of local energy density functionals from Brueckner-Hartree-Fock calculations

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca, ⁴⁸Ca, ⁵⁶Ni, ⁷⁸Ni, ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132}Sn, ²⁰⁸Pb; calculated binding energies, charge radii. ²⁰⁸Pb; calculated energies of giant monopole (ISGMR), dipole (IVGDR), quadrupole (ISGQR) and Gamow-Teller resonances. Brueckner-Hartree-Fock approximation, Skyrme parameterization and local energy density functionals. Comparison with experimental data.

doi: 10.1103/PhysRevC.84.024301

2011HE11

Phys.Rev. C 83, 064317 (2011)

H.Hergert, P.Papakonstantinou, R.Roth

Quasiparticle random-phase approximation with interactions from the Similarity Renormalization Group

NUCLEAR STRUCTURE ⁵⁶Ca; calculated number operator response for nonspurious monopole states, isoscalar and isovector dipole strengths. ⁴He, ^16,24O, ³⁴Si, ^40,48Ca, ^56,68,78Ni, ⁸⁸Sr, ⁹⁰Zr, ^100,114,132Sn, ¹⁴⁶Gd, ²⁰⁸Pb; calculated ground-state energy per nucleon and charge radii. ¹⁶O, ^40,48Ca, ^100,132Sn; calculated proton and neutron spin-orbit splittings. ^{36,38,40,42,44,46,48,50,52,54,56,58,60}Ca; calculated ground-state energies per nucleon, charge radii, odd-even mass differences, and pairing energies, isoscalar and isovector monopole, dipole and quadrupole responses, isoscalar monopole centroids and energies of the first excited 0+ states, centroids of isovector dipole response, isoscalar quadrupole centroids and energies of the first 2+ states. ^40,48Ca; calculated single particle energies. ¹²⁰Sn; calculated canonical single-neutron energies, isoscalar monopole response, running energy-weighted sums, centroid energies of the isoscalar monopole strength distribution. ⁵⁰Ca; calculated proton and neutron transition densities for monopole peaks. ^36,44Ca; calculated proton and neutron dipole transition densities. ⁵⁴Ca; calculated proton and neutron quadrupole transition densities for a pygmy and a GQR mode. Quasiparticle random phase approximation built on the HFB ground states. Comparison with experimental data.

doi: 10.1103/PhysRevC.83.064317

2011KV01

Int.J.Mod.Phys. E20, 281 (2011)

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

Skyrme-Hartree-Fock description of the dipole strength in neutron-rich tin isotopes

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148,150,152,154,156,158,160,162,164,166}Sn; analyzed low-energy E1 strengths, neutron and proton quadrupole deformations.

doi: 10.1142/S0218301311017636

2011LA22

Phys.Rev. C 84, 064602 (2011)

E.G.Lanza, A.Vitturi, M.V.Andres, F.Catara, D.Gambacurta

Excitations of pygmy dipole resonances in exotic and stable nuclei via Coulomb and nuclear fields

NUCLEAR REACTIONS ¹³²Sn(α, α'), (⁴⁰Ca, ⁴⁰Ca'), (⁴⁸Ca, ⁴⁸Ca'), E=30, 60, 100 MeV; ²⁰⁸Pb(¹⁷O, ¹⁷O'), E=20, 50 MeV; calculated form factors for PDR states and GDR, partial wave cross sections, differential cross sections. ¹⁰⁰Sn, ¹²⁰Sn, ¹³²Sn, ²⁰⁸Pb; calculated isovector strength distributions B(E1), RPA transition strengths for low-lying states. Hartree-Fock plus RPA random phase approximation (RPA), with Skyrme interaction.

doi: 10.1103/PhysRevC.84.064602

2011LE06

Prog.Part.Nucl.Phys. 66, 368 (2011)

H.Lenske, S.E.A.Orrigo, N.Tsoneva

Density functional theory for reactions of astrophysical interest

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132}Sn; calculated electric dipole strength distributions, B(E1), nuclear skin thickness. QRPA results.

NUCLEAR REACTIONS ¹³⁸Ba(γ, X), E<9 mEV; calculated photo-absorption σ. QRPA results.

doi: 10.1016/j.ppnp.2011.01.036

2011LE21

Phys.Rev. C 84, 014310 (2011)

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

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

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

doi: 10.1103/PhysRevC.84.014310

2011LI30

Phys.Rev. C 84, 014305 (2011)

E.V.Litvinova, A.V.Afanasjev

Dynamics of nuclear single-particle structure in covariant theory of particle-vibration coupling: From light to superheavy nuclei

NUCLEAR STRUCTURE ⁵⁶Ni, ^100,132Sn, ²⁰⁸Pb; calculated single particle spectra and strength distributions, proton and neutron shell gaps, spin-orbit and pseudospin doublet splitting energies. ⁵⁵Co, ^55,57Ni, ⁵⁷Cu, ^99,131In, ^{99,101,131,133}Sn, ^101,133Sb, ²⁰⁷Tl, ^207,209Pb, ²⁰⁹Bi; calculated spectroscopic factors in single-particle transfer reactions. ²⁹²120; calculated single-particle spectrum. Relativistic particle-vibration model in combination with the cranked relativistic mean-field (CRMF) approach. Comparison with experimental data.

doi: 10.1103/PhysRevC.84.014305

2011NI06

Phys.Rev. C 83, 034305 (2011)

N.Nikolov, N.Schunck, W.Nazarewicz, M.Bender, J.Pei

Surface symmetry energy of nuclear energy density functionals

NUCLEAR STRUCTURE ^192,194Hg, ^192,194,196Pb, ^236,238U, ²⁴⁰Pu, ²⁴²Cm; calculated deformation energies versus deformation parameter, 0+ superdeformed bandhead energies in Hg and Pb nuclei, and fission isomers in actinides. ^{236,248,260,270,298}U; calculated contributions of the Coulomb, surface symmetry, curvature, and surface terms of fission isomers. ¹⁰⁰Sn, ¹⁰⁰Zr; calculated contribution to the total deformation energy per nucleon. Nuclear energy density functional (EDF) theory applied to examine the role of the surface symmetry energy in nuclei using various Skyrme energy density functionals (EDFs). Comparison with experimental data.

doi: 10.1103/PhysRevC.83.034305

2011PA12

Eur.Phys.J. A 47, 14 (2011)

P.Papakonstantinou, V.Yu.Ponomarev, R.Roth, J.Wambach

Isoscalar dipole coherence at low energies and forbidden E1 strength

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca, ⁵⁶Ni, ¹⁰⁰Sn; calculated ISD, E1 response, GDR peak energy, B(E1), γ transition strengths, transition densities using RPA with finite-range forces.

doi: 10.1140/epja/i2011-11014-7

2011RO50

Phys.Rev. C 84, 054309 (2011); Erratum Phys.Rev. C 93, 069905 (2016)

X.Roca-Maza, X.Vinas, M.Centelles, P.Ring, P.Schuck

Relativistic mean-field interaction with density-dependent meson-nucleon vertices based on microscopical calculations

NUCLEAR STRUCTURE ^{16,18,26,28,30}Ne, ^20,32Mg, ^34,36Si, ³⁶S, ^38,40Ar, ^{36,38,40,42,44,46,48,50,52}Ca, ^{40,42,44,48,50,52,54}Ti, ^46,52Cr, ^54,64,66,68Fe, ^{54,56,58,66,68,70,72}Ni, ^58,70,72Zn, ⁸²Ge, ^84,86Se, ^86,88Kr, ^86,88,90Sr, ^86,88,90,92Zr, ^{86,88,90,92,94}Mo, ^94,96Ru, ^96,98Pd, ^98,100Cd, ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134}Sn, ^{126,128,130,132,134,136}Te, ^134,136,138Xe, ^136,138,140Ba, ^{138,140,142,144}Ce, ^140,142,144Nd, ^142,144,146Sm, ¹⁴⁶Gd, ¹⁴⁸Dy, ¹⁵⁰Er, ¹⁵²Yb, ^170,172Pt, ^{172,174,176,204,206}Hg, ^{178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214}Pb, ^{204,206,208,210,212,214,216}Po, ^{208,210,212,214,216}Rn, ^{210,212,214,216,218}Ra, ^{212,214,216,218,220}Th, ²²⁴U; analyzed binding energies, and charge radii. ^100,132,176Sn; calculated isoscalar, isovector parts of the spin-orbit potential, spin orbit splitting. Relativistic Brueckner theory, high-precision density functional DD-MEδ with density-dependent meson-nucleon couplings. Comparison with experimental data.

doi: 10.1103/PhysRevC.84.054309

2011SA06

Phys.Rev. C 83, 025801 (2011)

P.Sarriguren

Stellar weak decay rates in neutron-deficient medium-mass nuclei

RADIOACTIVITY ^50,52,54Ni, ^56,58,60Zn, ^62,64,66Ge, ^66,68,70Se, ^70,72,74Kr, ^74,76,78Sr, ^80,82,84Zr, ^84,86,88Mo, ^88,90,92Ru, ^92,94,96Pd, ^96,98,100Cd, ^100,102,104Sn(β⁺), (EC); calculated G-T strength distributions, and decay rates of waiting point and neighboring nuclides under stellar density and temperature conditions in rp process using self-consistent deformed Skyrme-Hartree Fock + BCS + quasiparticle random-phase-approximation (QRPA) approach.

doi: 10.1103/PhysRevC.83.025801

2011SA07

Acta Phys.Pol. B42, 415 (2011)

W.Satula, J.Dobaczewski, W.Nazarewicz, M.Rafalski

Isospin Mixing in Nuclei around N∼Z and the Superallowed β -decay

NUCLEAR STRUCTURE ⁴⁰Ca, ⁴²Sc, ⁸⁰Zr, ¹⁰⁰Sn; calculated isospin impurities, isospin-breaking correction.

2011SA14

Int.J.Mod.Phys. E20, 244 (2011)

W.Satula, J.Dobaczewski, W.Nazarewicz, M.Borucki, M.Rafalski

Isospin mixing in the vicinity of the N = Z line

NUCLEAR STRUCTURE ¹⁴N, ⁴⁰Ca, ¹⁰⁰Sn; calculated kernels, isospin impurities, symmetry energies.

doi: 10.1142/S0218301311017582

2011SH32

Phys.Rev. C 84, 044317 (2011)

H.Shimoyama, M.Matsuo

Anomalous pairing vibration in neutron-rich Sn isotopes beyond the N=82 magic number

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148,150}Sn; calculated monopole neutron pair transfer strengths, neutron pair transition strength functions, neutron transition densities. Dependence of anomalous pair vibration on the effective pairing interaction. Skyrme-Hartree-Fock-Bogoliubov mean-field model, continuum quasiparticle random phase approximation.

doi: 10.1103/PhysRevC.84.044317

2011TI11

Phys.Rev. C 84, 054313 (2011)

N.K.Timofeyuk

Properties of one-nucleon overlap functions for A ≥ 16 double-closed-shell nuclei in the source-term approach

NUCLEAR STRUCTURE ^16,17,24O, ²⁵F, ^{40,41,48,49,60}Ca, ^41,49Sc, ^56,57,78Ni, ^100,132,133Sn, ^208,209Pb, ²⁰⁹Bi; calculated spectroscopic factors, rms radii, asymptotic normalization coefficients for one-nucleon removal and addition reactions. Source term approach, and independent-particle model. Comparison with experimental data for one nucleon knockout reactions.

doi: 10.1103/PhysRevC.84.054313

2012BH10

Phys.Rev. C 86, 044316 (2012)

A.Bhagwat, X.Vinas, M.Centelles, P.Schuck, R.Wyss

Microscopic-macroscopic approach for binding energies with the Wigner-Kirkwood method. II. Deformed nuclei

NUCLEAR STRUCTURE ⁶³Ge, ⁶⁵As, ⁶⁷Se, ^{71,80,82,84,86,88,90,92,94,96,98,100,102,104}Kr, ^{76,78,80,82,84,86,88,90,92,94,96,98,100,102}Sr, ^{84,86,88,90,92,94,96,98,100,102,104,106,108}Zr, ^{86,88,90,92,94,96,98,100,102,104,106,108,110}Mo, ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134}Sn, ^{140,142,144,146,148,150,152,154,156,158,160,162}Gd, ^{186,188,190,192,194,196,198,200,202,204,206,208,210,212,214}Po; calculated S_2n, β₂, S_p, binding energy using Microscopic-macroscopic model with Wigner-Kirkwood expansion. Comparison with experimental data. Z, N>7; deduced difference between the calculated and the corresponding experimental binding energies for 561 nuclides.

RADIOACTIVITY ^279,280Rg, ^282,283Nh, ^287,288,289Fl, ^287,288Mc, ^291,292,293Lv, ²⁹⁴Og(α); calculated Q values and half-lives. Comparison with experimental data.

doi: 10.1103/PhysRevC.86.044316

2012CA27

Phys.Rev. C 86, 014307 (2012)

B.G.Carlsson, J.Toivanen, A.Pastore

Collective vibrational states within the fast iterative quasiparticle random-phase approximation method

NUCLEAR STRUCTURE ¹⁸O; calculated levels, J, π, B(E0), B(E1), B(E2). ^{38,40,42,44,46,48,50,52,54}Ca, ^{52,54,56,58,60,62,64,66,68,70,72,74,76,78,80}Ni, ^{182,184,186,188,190,192,194,196,198,200,202,204,206,208,210,212,214}Pb, ^{98,100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138}Sn; calculated levels, J, π, B(E2), B(E3), two-quasi particle components for first 2+ and 3- states. Quasiparticle random-phase approximation (QRPA) calculations using iterative non-Hermitian Arnoldi diagonalization procedures. Comparison with experimental data.

doi: 10.1103/PhysRevC.86.014307

2012CH05

J.Phys.(London) G39, 035104 (2012)

L.-W.Chen, J.-Z.Gu

Correlations between the nuclear breathing mode energy and properties of asymmetric nuclear matter

NUCLEAR STRUCTURE ²⁰⁸Pb, ^100,132Sn; calculated nuclear isoscalar giant monopole resonance (ISGMR) energies, response functions; deduced correlations between ISGMR and symmetry energies. Microscopic HF calculations.

doi: 10.1088/0954-3899/39/3/035104

2012CO04

Phys.Rev. C 85, 024322 (2012)

G.Co, V.De Donno, P.Finelli, M.Grasso, M.Anguiano, A.M.Lallena, C.Giusti, A.Meucci, F.D.Pacati

Mean-field calculations of the ground states of exotic nuclei

NUCLEAR STRUCTURE ^16,22,24,28O, ^40,48,52,60Ca, ^48,56,68,78Ni, ^{100,114,116,132}Sn; calculated binding energies, single particle energies, rms charge radii, neutron skin thickness. Mean-field approach, nonrelativistic Hartree-Fock, relativistic Hartree calculations. Comparison with experimental data.

NUCLEAR REACTIONS ^40,48,52,60Ca(e, e'p), (e, e), E=483.2 MeV; calculated reduced cross sections, elastic scattering cross sections, neutron, proton and matter distributions, Mean-field approach, nonrelativistic Hartree-Fock, relativistic Hartree calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.024322

2012GR07

Phys.Rev. C 85, 034317 (2012)

M.Grasso, D.Lacroix, A.Vitturi

Pair-transfer probability in open- and closed-shell Sn isotopes

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144}Sn; calculated two nucleon transfer (removal or addition) strength from ground-state to ground-state, neutron Fermi energy, entropy, pairing gap for mixed pairing case and pure surface case. Canonical basis formulation, and Hartree-Fock-Bogoliubov (HFB) theory. Discussed role of particle number restoration.

doi: 10.1103/PhysRevC.85.034317

2012HI07

Nature(London) 486, 341 (2012)

C.B.Hinke, M.Bohmer, P.Boutachkov, T.Faestermann, H.Geissel, J.Gerl, R.Gernhauser, M.Gorska, A.Gottardo, H.Grawe, J.L.Grebosz, R.Krucken, N.Kurz, Z.Liu, L.Maier, F.Nowacki, S.Pietri, Zs.Podolyak, K.Sieja, K.Steiger, K.Straub, H.Weick, H.-J.Wollersheim, P.J.Woods, N.Al-Dahan, N.Alkhomashi, A.Atac, A.Blazhev, N.F.Braun, I.T.Celikovic, T.Davinson, I.Dillmann, C.Domingo-Pardo, P.C.Doornenbal, G.de France, G.F.Farrelly, F.Farinon, N.Goel, T.C.Habermann, R.Hoischen, R.Janik, M.Karny, A.Kaskas, I.M.Kojouharov, Th.Kroll, Y.Litvinov, S.Myalski, F.Nebel, S.Nishimura, C.Nociforo, J.Nyberg, A.R.Parikh, A.Prochazka, P.H.Regan, C.Rigollet, H.Schaffner, C.Scheidenberger, S.Schwertel, P.-A.Soderstrom, S.J.Steer, A.Stolz, P.Strmen

Superallowed Gamow-Teller decay of the doubly magic nucleus ¹⁰⁰Sn

RADIOACTIVITY ¹⁰⁰Sn(β⁺), (EC) [from Be(¹²⁴Xe, X)¹⁰⁰Sn, E = 1 GeV/nucleon]; measured decay products, Eγ, Iγ, Eβ, Iβ. ¹⁰⁰In; deduced T_1/2, log ft, Gamow-Teller strength, energy levels, J, π, distribution of positron energies. Comparison with available data, large scale shell model calculations.

doi: 10.1038/nature11116

2012LO08

Phys.Rev. C 86, 014313 (2012)

G.Lorusso, A.Becerril, A.Amthor, T.Baumann, D.Bazin, J.S.Berryman, B.A.Brown, R.H.Cyburt, H.L.Crawford, A.Estrade, A.Gade, T.Ginter, C.J.Guess, M.Hausmann, G.W.Hitt, P.F.Mantica, M.Matos, R.Meharchand, K.Minamisono, F.Montes, G.Perdikakis, J.Pereira, M.Portillo, H.Schatz, K.Smith, J.Stoker, A.Stolz, R.G.T.Zegers

β-delayed proton emission in the ¹⁰⁰Sn region

RADIOACTIVITY ⁸⁹Ru, ^91,92Rh, ⁹³Pd, ^95,96,96mAg, ^96,97,97mCd, ^{98,98m,99,100}In, ^100,101Sn[from ⁹Be(¹¹²Sn, X), E=140 MeV/nucleon](β⁺), (EC), (β⁺p); measured Eγ, Iγ, β spectra, E(p), I(p), βγ-coin, βp-coin, γβp-coin, fragment yields, half-lives, β-delayed proton emission branching ratios using NSCL Beta Counting System and SeGA array. Discussed rp-process implications. Comparison with previous studies and theoretical calculations. X-ray bursts calculations.

doi: 10.1103/PhysRevC.86.014313

2012LO13

Prog.Theor.Phys.(Kyoto), Suppl. 196, 39 (2012)

U.Lombardo

NN Effective Interaction from the Brueckner Theory and Applications to Nuclear Systems

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ^56,78Ni, ^100,132Sn, ²⁰⁸Pb; calculated binding energies, charge radii, isospin splitting.

doi: 10.1143/PTPS.196.39

2012MA16

Phys.Rev. C 85, 054313 (2012)

T.Marketin, G.Martinez-Pinedo, N.Paar, D.Vretenar

Role of momentum transfer in the quenching of Gamow-Teller strength

NUCLEAR REACTIONS ⁹⁰Zr(p, n), (n, p), E=300 MeV; analyzed differential cross section data; deduced pn-RQRPA strengths in β^- and β⁺ channels obtained with the Gamow-Teller (GT) operator, GT+IVSM operator, and full L=0 operator, momentum transfer. Relativistic Hartree-Bogoliubov model. Comparison with Ikeda sum rule.

NUCLEAR STRUCTURE ⁴⁸Ca, ⁹⁰Zr, ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136,138,140,142,144,146,148,150}Sn, ²⁰⁸Pb; analyzed L=0 β^- strength functions, GT and IVSM centroids using Relativistic Hartree-Bogoliubov (RHB) plus proton-neutron relativistic quasiparticle random-phase approximation (pn-RQRPA) with GT operator, the GT plus isovector spin monopole (IVSM) mode term, and the operator that contains the full momentum-transfer dependence.

doi: 10.1103/PhysRevC.85.054313

2012NA22

Prog.Theor.Phys.(Kyoto), Suppl. 196, 371 (2012)

H.Nakada

Mean-Field and RPA Approaches to Stable and Unstable Nuclei with Semi-Realistic NN Interaction

NUCLEAR STRUCTURE ²⁰⁸Pb, ⁹⁰Zr, ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130}Sn; calculated B(E2), energy levels, J, π. M3Y-type semi-realistic NN interactions in the mean-field and RPA framework.

doi: 10.1143/PTPS.196.371

2012RO26

Phys.Rev. C 86, 031306 (2012)

X.Roca-Maza, G.Colo, H.Sagawa

New Skyrme interaction with improved spin-isospin properties

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ^56,68Ni, ⁹⁰Zr, ^100,132Sn, ²⁰⁸Pb; calculated binding energies, charge radii, proton spin-orbit splittings using the Skyrme-Aizu-Milano (SAMi) functional. ⁴⁸Ca, ⁹⁰Zr, ²⁰⁸Pb; calculated Gamow-Teller (GT) strength distributions and spin dipole resonance (SDR) strength functions using several Skyrme interactions. New Skyrme energy density functional proposed. Comparison with experimental data.

doi: 10.1103/PhysRevC.86.031306

2012SM05

Phys.Rev. C 86, 034314 (2012)

N.A.Smirnova, K.Heyde, B.Bally, F.Nowacki, K.Sieja

Nuclear shell evolution and in-medium NN interaction

NUCLEAR STRUCTURE ^{16,18,20,22,28,36}O, ²⁴Ne, ²⁶Mg, ^34,42Si, ^36,44S, ^{40,42,44,46,48}Ca, ⁵⁰Ti, ⁵²Cr, ⁵⁴Fe, ⁵⁶Ni, ^{80,82,84,86,88,90}Zr, ⁹²Mo, ⁹⁴Ru, ⁹⁶Pd, ⁹⁸Cd, ¹⁰⁰Sn; calculated neutron and proton effective single-particle energies (ESPEs) based on an effective two-body shell-model interaction in sdpf shell-model space. Role of central and tensor terms in understanding evolution of the shell gaps at N=20 and N=28.

doi: 10.1103/PhysRevC.86.034314

2012UR03

Phys.Rev. C 85, 034322 (2012)

M.Urban

Pygmy resonance and torus mode within Vlasov dynamics

NUCLEAR STRUCTURE ^16,18,20,22O, ^100,116,132Sn; calculated electric dipole moment, E1 strength, transition densities and velocity fields for GDR and pygmy dipole resonances. Semiclassical Thomas-Fermi (TF) plus Vlasov approach.

doi: 10.1103/PhysRevC.85.034322

2012VO03

Phys.Rev. C 85, 054319 (2012)

D.Voitenkov, S.Kamerdzhiev, S.Krewald, E.E.Saperstein, S.V.Tolokonnikov

Self-consistent calculations of quadrupole moments of the first 2⁺ states in Sn and Pb isotopes

NUCLEAR MOMENTS ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134}Sn, ^{190,192,194,196,198,200,202,204,206,208}Pb; calculated static quadrupole moments of first 2+ states. Ground state correlations. Dependence of quadrupole moment on neutron access. Self-consistent calculations based on quasiparticle random-phase approximation (QRPA) and energy density functionals. Comparison with experimental data.

doi: 10.1103/PhysRevC.85.054319

2012WA32

Phys.Rev. C 86, 054309 (2012)

K.Washiyama, K.Bennaceur, B.Avez, M.Bender, P.-H.Heenen, V.Hellemans

New parametrization of Skyrme's interaction for regularized multireference energy density functional calculations

NUCLEAR STRUCTURE ^40,48Ca, ⁵⁶Ni, ^100,132Sn, ²⁰⁸Pb; calculated binding energy, charge radii. ²⁴Mg, ⁷⁴Kr, ^80,100Zr, ¹⁸⁶Pb; calculated potential energy curves versus β₂. ²⁴⁰Pu; calculated fission barrier versus β₂. ¹⁹⁴Hg; calculated dynamical moment of inertia of superdeformed band. ²⁴⁹Bk, ²⁵¹Cf; calculated one-quasiparticle levels. Z=20, A=36-52; Z=28, A=54-72; Z=50, A=100-134; Z=82, A=180-214; N=20, Z=10-22; N=50, Z=30-50; N=82, Z=48-70; N=126, Z=80-92; calculated binding energies, charge radii for even-even nuclei. Energy density functional calculations for spherical and deformed nuclei with new Skyrme parametrization with integer powers of the density. Comparison with experimental data.

doi: 10.1103/PhysRevC.86.054309

2012YU01

Nucl.Phys. A877, 35 (2012)

E.Yuksel, E.Khan, K.Bozkurt

Analysis of the neutron and proton contributions to the pygmy dipole mode in doubly magic nuclei

NUCLEAR STRUCTURE ^16,24O, ^40,48,70Ca, ^56,68,78Ni, ^100,132Sn, ²⁰⁸Pb; calculated GDR, Pygmy dipole strength distribution using self-consistent HF+RPA with Skyrme interactions. Comparison with data.

doi: 10.1016/j.nuclphysa.2012.01.006

2013AV03

Eur.Phys.J. A 49, 76 (2013)

B.Avez, C.Simenel

Structure and direct decay of Giant Monopole Resonances

NUCLEAR STRUCTURE ¹⁶O; calculated, analyzed giant monopole resonance, monopole moment time evolution, strength function. Compared with available data. ^100,132Sn; calculated, analyzed GMR (giant monopole resonance) strength function. RPA with time-dependent energy density functional method in linear response regime.

doi: 10.1140/epja/i2013-13076-9

2013BH06

Nucl.Phys. A913, 1 (2013)

R.Bhattacharya

Tensor interaction and its influence on evolution of nuclear shells

NUCLEAR STRUCTURE ^40,48Ca, ⁵⁶Ni, ⁹⁰Zr, ^100,132Sn, ²⁰⁸Pb; calculated levels, J, π, shell gaps for Z=8, 20, 28 and N=8, 20, 28 chains, spin-orbit splitting of shell model states near ¹³²Sn and ²⁰⁸Pb using Hartree-Fock theory with Skyrme density dependent, tensor interaction and spin-orbit; deduced parameters. Compared with available data.

doi: 10.1016/j.nuclphysa.2013.05.006

2013BR17

Phys.Rev.Lett. 111, 232502 (2013)

B.A.Brown

Constraints on the Skyrme Equations of State from Properties of Doubly Magic Nuclei

NUCLEAR STRUCTURE ^16,24O, ³⁴Si, ^40,48Ca, ^48,68Ni, ⁸⁸Sr, ^100,132Sn, ²⁰⁸Pb; analyzed properties of doubly magic nuclei; deduced the value of the neutron equation of state and Skyrme equations of state on the neutron skin. Comparison with available data.

doi: 10.1103/PhysRevLett.111.232502

2013CA08

Phys.Rev. C 87, 054303 (2013)

B.G.Carlsson, J.Toivanen, U.von Barth

Fluctuating parts of nuclear ground-state correlation energies

NUCLEAR STRUCTURE ^{14,16,18,20,22}O, ^{36,38,40,42,44,46,48,50}Ca, ^{52,54,56,58,60,62,64,66,68,70,72,74,76,78}Ni, ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132,134,136}Sn; calculated correlations and fluctuating parts in ground-state binding energies, octupole shape vibrations using QRPA and MBPT2. Comparison with experimental data.

doi: 10.1103/PhysRevC.87.054303

2013CO05

Phys.Rev. C 87, 034305 (2013)

G.Co, V.De Donno, M.Anguiano, A.M.Lallena

Pygmy and giant electric dipole responses of medium-heavy nuclei in a self-consistent random-phase approximation approach with a finite-range interaction

NUCLEAR STRUCTURE ^16,22,24,28O, ^40,48,52,60Ca, ^48,56,68,78Ni, ⁹⁰Zr, ^{100,114,116,132}Sn, ²⁰⁸Pb; calculated photoabsorption σ(E), proton and neutron transition densities, centroids of pygmy dipole and giant dipole resonances (PDR, GDR). Gogny interaction in a self-consistent Hartree-Fock plus random phase approximation method. Comparison with experimental data, and for details of PDR and GDR structures.

doi: 10.1103/PhysRevC.87.034305

2013DU07

Phys.Scr. T154, 014002 (2013)

J.Dudek, B.Szpak, B.Fornal, A.Dromard

Predictive power and theoretical uncertainties of mathematical modelling for nuclear physics

NUCLEAR STRUCTURE ¹⁶O, ^40,48Ca, ⁵⁶Ni, ⁹⁰Zr, ^100,132Sn, ²⁰⁸Pb; calculated level energies, J, π, proton radius and their uncertainties. Comparison with available data.

doi: 10.1088/0031-8949/2013/T154/014002

2013FA01

Prog.Part.Nucl.Phys. 69, 85 (2013)

T.Faestermann, M.Gorska, H.Grawe

The structure of ¹⁰⁰Sn and neighbouring nuclei

NUCLEAR STRUCTURE ^{100,108,110,112,114}Sn; compiled experimental data, B(E2), shell model results.

doi: 10.1016/j.ppnp.2012.10.002

2013IS09

Phys.Atomic Nuclei 76, 828 (2013)

V.I.Isakov

Global properties of nuclei from ¹⁰⁰Sn to ¹³²Sn

NUCLEAR STRUCTURE ^{100,102,104,106,108,110,112,114,116,118,120,122,124,126,128,130,132}Sn; calculated binding energies, two-neutron separation energy, proton separation energy, rms radii for protons and neutrons, occupancies, B(E2), energy levels, J, π. HF+BCS procedure.

doi: 10.1134/S1063778813070077

2013KV01

Phys.Scr. T154, 014019 (2013)

J.Kvasil, A.Repko, V.O.Nesterenko, W.Kleinig, P.-G.Reinhard, N.Lo Iudice

Toroidal, compression and vortical dipole strengths in ¹²⁴Sn

NUCLEAR STRUCTURE ^100,124,132Sn; calculated toroidal, vortical and compression dipole strength functions. Self-consistent separable Skyrme-RPA approach.

doi: 10.1088/0031-8949/2013/T154/014019

2013NA03

Phys.Rev. C 87, 014336 (2013)

H.Nakada

Semi-realistic nucleon-nucleon interactions with improved neutron-matter properties

NUCLEAR STRUCTURE ^16,24O, ^40,48Ca, ⁹⁰Zr, ^100,132Sn, ²⁰⁸Pb; calculated binding energies, rms matter radii, single-particle energies, proton and neutron rms radii. Z=8, N=7-18; Z=20, N=17-50; Z=28, N=24-62; Z=50, N=53-92; Z=82, N=97-134; calculated S(n). N=20, Z=14-28; N=28, Z=16-30; N=50, Z=28-50; N=82, Z=47-72; N=126, Z=70-94; calculated S(p). Z=82, N=116-134; calculated isotope shifts. Discussed tensor-force effects on shell structure. HFB calculations with new parameter sets of semi-realistic effective interactions. Comparison with experimental data.

doi: 10.1103/PhysRevC.87.014336

2013NI09

Phys.Rev. C 87, 051303 (2013)

Z.M.Niu, Y.F.Niu, Q.Liu, H.Z.Liang, J.Y.Guo

Nuclear β⁺/EC decays in covariant density functional theory and the impact of isoscalar proton-neutron pairing

RADIOACTIVITY ^32,34Ar, ^36,38Ca, ^40,42Ti, ^46,48,50Fe, ^50,52,54Ni, ^56,58Zn, ^96,98,100Cd, ^100,102,104Sn(β⁺), (EC); calculated half-lives, B(GT). Self-consistent proton-neutron QRPA with relativistic Hartree-Bogoliubov (QRPA+RHB) calculations. Comparison with experimental data.

doi: 10.1103/PhysRevC.87.051303

2013RO02

Phys.Rev. C 87, 014304 (2013)

X.Roca-Maza, M.Centelles, F.Salvat, X.Vinas

Electron scattering in isotonic chains as a probe of the proton shell structure of unstable nuclei

NUCLEAR STRUCTURE ²²O, ²⁴Ne, ²⁶Mg, ²⁸Si, ³⁰S, ³²Ar, ³⁴Ca, ⁷⁰Ca, ⁸⁴Se, ⁹⁰Zr, ¹⁰⁰Sn, ¹²²Zr, ¹⁴⁰Ce, ¹⁴⁶Gd, ¹⁵⁴Hf; calculated proton and neutron single-particle levels, and charge densities. Relativistic nuclear mean-field interaction G2.

NUCLEAR REACTIONS ¹²²Zr, ¹⁴⁰Ce, ¹⁵⁴Hf(e, e), E=250, 500 MeV; calculated DWBA and Mott differential σ(θ, E). ²²O, ²⁴Ne, ²⁶Mg, ²⁸Si, ³⁰S, ³²Ar, ³⁴Ca, ⁷⁰Ca, ⁷⁴Cr, ⁷⁸Ni, ⁸⁰Zn, ⁸²Ge, ⁸⁴Se, ⁸⁶Kr, ⁸⁸Sr, ⁹⁰Zr, ⁹²Mo, ⁹⁴Ru, ⁹⁶Pd, ⁹⁸Cd, ¹⁰⁰Sn, ¹²⁰Sr, ¹²²Zr, ¹²⁸Pd, ¹³²Sn, ¹³⁶Xe, ¹⁴⁰Ce, ¹⁴²Nd, ¹⁴⁴Sm, ¹⁴⁶Gd, ¹⁴⁸Dy, ¹⁵⁰Er, ¹⁵²Yb, ¹⁵⁴Hf(e, e), E=500 MeV; calculated Helm model parameters, mass-number dependence of Helm parameters, square charge form factors as function of Helm parameters in DWBA. Dirac partial-wave approach, and covariant mean-field model G2.

doi: 10.1103/PhysRevC.87.014304

2013WA09

Phys.Rev. C 87, 034327 (2013)

N.Wang, L.Ou, M.Liu

Nuclear symmetry energy from the Fermi-energy difference in nuclei

NUCLEAR STRUCTURE ^16,22O, ^22,42Si, ^40,48,60Ca, ⁴²Ti, ^56,68,78Ni, ¹³⁰Cd, ^100,132,134Sn, ¹³⁴Te, ¹⁴⁴Sm, ^182,208Pb; calculated neutron-proton Fermi-energy difference, nuclear symmetry energy, neutron-skin thickness. Skyrme energy density functionals and nuclear masses, with 54 Skyrme parameter sets. Comparison with experimental data.

doi: 10.1103/PhysRevC.87.034327

2013YA23

Chin.Phys.C 37, 124102 (2013)

D.Yang, L.-G.Cao, Z.-Y.Ma

Collective multipole excitations of exotic nuclei in relativistic continuum random phase approximation

NUCLEAR STRUCTURE ^34,40,48,60Ca, ^16,28O, ^100,132Sn; calculated isoscalar and isovector collective multipole excitations, strength functions. Comparison with available data.

doi: 10.1088/1674-1137/37/12/124102

2013YU05

Eur.Phys.J. A 49, 124 (2013)

E.Yuksel, E.Khan, K.Bozkurt

The soft Giant Monopole Resonance as a probe of the spin-orbit splitting

NUCLEAR STRUCTURE ^100,132Sn, ²⁰⁸Pb; calculated isoscalar monopole strength distribution using Skyrme HF plus RPA model.

doi: 10.1140/epja/i2013-13124-6

2017WA10

Chin.Phys.C 41, 030003 (2017)

M.Wang, G.Audi, F.G.Kondev, W.J.Huang, S.Naimi, X.Xu

The AME2016 atomic mass evaluation (II). Tables, graphs and references

ATOMIC MASSES A=1-295; compiled, evaluated atomic masses data.

doi: 10.1088/1674-1137/41/3/030003

2019LU08

Phys.Rev.Lett. 122, 222502 (2019)

D.Lubos, J.Park, T.Faestermann, R.Gernhauser, R.Krucken, M.Lewitowicz, S.Nishimura, H.Sakurai, D.S.Ahn, H.Baba, B.Blank, A.Blazhev, P.Boutachkov, F.Browne, I.Celikovic, G.de France, P.Doornenbal, Y.Fang, N.Fukuda, J.Giovinazzo, N.Goel, M.Gorska, S.Ilieva, N.Inabe, T.Isobe, A.Jungclaus, D.Kameda, Y.K.Kim, I.Kojouharov, T.Kubo, N.Kurz, Y.K.Kwon, G.Lorusso, K.Moschner, D.Murai, I.Nishizuka, Z.Patel, M.M.Rajabali, S.Rice, H.Schaffner, Y.Shimizu, L.Sinclair, P.-A.Soderstrom, K.Steiger, T.Sumikama, H.Suzuki, H.Takeda, Z.Wang, N.Warr, H.Watanabe, J.Wu, Z.Xu

Improved Value for the Gamow-Teller Strength of the ¹⁰⁰Sn Beta Decay

RADIOACTIVITY ¹⁰⁰Sn(β⁺) [from ⁹Be(¹²⁴Xe, X), E=345 MeV/nucleon]; measured decay products, Eγ, Iγ, Eβ, Iβ; deduced Gamow-Teller Strength, Q-value, T_1/2. Comparison with available data.

doi: 10.1103/PhysRevLett.122.222502

2019MO01

At.Data Nucl.Data Tables 125, 1 (2019)

P.Moller, M.R.Mumpower, T.Kawano, W.D.Myers

Nuclear properties for astrophysical and radioactive-ion-beam applications (II)

NUCLEAR STRUCTURE Z=8-136; calculated the ground-state odd-proton and odd-neutron spins and parities, proton and neutron pairing gaps, one- and two-neutron separation energies, quantities related to β-delayed one- and two-neutron emission probabilities, average energy and average number of emitted neutrons, β-decay energy release and T_1/2 with respect to Gamow-Teller decay with a phenomenological treatment of first-forbidden decays, one- and two-proton separation energies, and α-decay energy release and half-life.

doi: 10.1016/j.adt.2018.03.003