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Search: Author = A.P.Zuker

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2021ZU02      Phys.Rev. C 103, 024322 (2021)

A.P.Zuker

Quadrupole dominance in the light Sn and in the Cd isotopes

NUCLEAR STRUCTURE ^{104,106,108,110,112,114,116,118,120,122,124,126,128,130}Sn, ^{102,104,106,108,110,112,114,116,118,120,122,124,126}Cd; calculated B(E2) for the first 2+ state using shell-model with a minimally renormalized realistic interaction, supplemented by quasi- and pseudo-SU3 symmetries and Nilsson-SU3 self-consistent calculations, with general monopole Hamiltonian GEMO. Comparison with experimental and evaluated data. Discussed B(E2)(first 4+ to first 2+)/B(E2)(first 2+ to g.s.).

doi: 10.1103/PhysRevC.103.024322
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2020SI10      Phys.Lett. B 806, 135474 (2020)

M.Siciliano, J.J.Valiente-Dobon, A.Goasduff, F.Nowacki, A.P.Zuker, D.Bazzacco, A.Lopez-Martens, E.Clement, G.Benzoni, T.Braunroth, F.C.L.Crespi, N.Cieplicka-Orynczak, M.Doncel, S.Erturk, G.de France, C.Fransen, A.Gadea, G.Georgiev, A.Goldkuhle, U.Jakobsson, G.Jaworski, P.R.John, I.Kuti, A.Lemasson, T.Marchi, D.Mengoni, C.Michelagnoli, T.Mijatovic, C.Muller-Gatermann, D.R.Napoli, J.Nyberg, M.Palacz, R.M.Perez-Vidal, B.Saygi, D.Sohler, S.Szilner, D.Testov, M.Zielinska, D.Barrientos, B.Birkenbach, H.C.Boston, A.J.Boston, B.Cederwall, J.Collado, D.M.Cullen, P.Desesquelles, C.Domingo-Pardo, J.Dudouet, J.Eberth, F.J.Egea Canet, V.Gonzalez, L.J.Harkness-Brennan, H.Hess, D.S.Judson, A.Jungclaus, W.Korten, M.Labiche, A.Lefevre, S.Leoni, H.Li, A.Maj, R.Menegazzo, B.Million, A.Pullia, F.Recchia, P.Reiter, M.D.Salsac, E.Sanchis, O.Stezowski, Ch.Theisen

Pairing-quadrupole interplay in the neutron-deficient tin nuclei: First lifetime measurements of low-lying states in ^{106, 108}Sn

NUCLEAR REACTIONS ⁹²Mo(¹⁰⁶Cd, X)¹⁰⁶Sn/¹⁰⁸Sn, E=770 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, lifetimes, B(E2), B(E4). Differential plunger device.

doi: 10.1016/j.physletb.2020.135474
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2018BO17      Phys.Rev.Lett. 121, 032502 (2018)

A.Boso, S.M.Lenzi, F.Recchia, J.Bonnard, A.P.Zuker, S.Aydin, M.A.Bentley, B.Cederwall, E.Clement, G.de France, A.Di Nitto, A.Dijon, M.Doncel, F.Ghazi Moradi, A.Gadea, A.Gottardo, T.Henry, T.Huyuk, G.Jaworski, P.R.John, K.Juhasz, I.Kuti, B.Melon, D.Mengoni, C.Michelagnoli, V.Modamio, D.R.Napoli, B.M.Nyako, J.Nyberg, M.Palacz, J.Timar, J.J.Valiente-Dobon

Neutron Skin Effects in Mirror Energy Differences: The Case of ²³Mg-²³Na

NUCLEAR REACTIONS ¹²C(¹⁶O, nα), (¹⁶O, pα), E=60-70 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, mirror energy differences, high-spin states. Comparison with available data.

doi: 10.1103/PhysRevLett.121.032502
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2016BO14      Phys.Rev.Lett. 116, 212501 (2016)

J.Bonnard, S.M.Lenzi, A.P.Zuker

Neutron Skins and Halo Orbits in the sd and pf Shells

NUCLEAR STRUCTURE ⁴⁸Ca, ⁶⁸Ni, ¹²⁰Sn, ²⁰⁸Pb; calculated nuclear radii, neutron skin, halo orbits.

doi: 10.1103/PhysRevLett.116.212501
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2015ZU02      Phys.Rev. C 92, 024320 (2015)

A.P.Zuker, A.Poves, F.Nowacki, S.M.Lenzi

Nilsson-SU3 self-consistency in heavy N=Z nuclei

NUCLEAR STRUCTURE ²⁸Si, ⁶⁰Zn, ⁶⁴Ge, ⁶⁸Se, ⁷²Kr, ⁸⁰Zr, ⁸⁴Mo, ⁸⁸Ru, ⁹²Pd, ⁹⁶Cd; calculated energies, B(E2), intrinsic quadrupole moments of low-lying positive-parity states up to 8+ for N=Z nuclei using shell model. Nilsson-SU3 self-consistency, quasi and pseudo-SU3 quadrupole moments. Coexistence of prolate and oblate deformations in ⁷²Kr and ⁸⁴Mo.

doi: 10.1103/PhysRevC.92.024320
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2012GO19      Phys.Rev.Lett. 109, 162502 (2012)

A.Gottardo, J.J.Valiente-Dobon, G.Benzoni, R.Nicolini, A.Gadea, S.Lunardi, P.Boutachkov, A.M.Bruce, M.Gorska, J.Grebosz, S.Pietri, Zs.Podolyak, M.Pfutzner, P.H.Regan, H.Weick, J.Alcantara Nunez, A.Algora, N.Al-Dahan, G.de Angelis, Y.Ayyad, N.Alkhomashi, P.R.P.Allegro, D.Bazzacco, J.Benlliure, M.Bowry, A.Bracco, M.Bunce, F.Camera, E.Casarejos, M.L.Cortes, F.C.L.Crespi, A.Corsi, A.M.D.Bacelar, A.Y.Deo, C.Domingo-Pardo, M.Doncel, Zs.Dombradi, T.Engert, K.Eppinger, G.F.Farrelly, F.Farinon, E.Farnea, H.Geissel, J.Gerl, N.Goel, E.Gregor, T.Habermann, R.Hoischen, R.Janik, S.Klupp, I.Kojouharov, N.Kurz, S.M.Lenzi, S.Leoni, Mandal, R.Menegazzo, D.Mengoni, B.Million, A.I.Morales, D.R.Napoli, F.Naqvi, C.Nociforo, A.Prochazka, W.Prokopowicz, F.Recchia, R.V.Ribas, M.W.Reed, D.Rudolph, E.Sahin, H.Schaffner, A.Sharma, B.Sitar, D.Siwal, K.Steiger, P.Strmen, T.P.D.Swan, I.Szarka, C.A.Ur, P.M.Walker, O.Wieland, H-J.Wollersheim, F.Nowacki, E.Maglione, A.P.Zuker

New Isomers in the Full Seniority Scheme of Neutron-Rich Lead Isotopes: The Role of Effective Three-Body Forces

NUCLEAR REACTIONS Be(²³⁸U, X)²¹⁰Pb/²¹²Pb/²¹⁴Pb/²¹⁶Pb, E=1 GeV/nucleon; measured reaction products, Eγ, Iγ; deduced level schemes, J, π, B(E2). Comparison with shell model calculations.

doi: 10.1103/PhysRevLett.109.162502
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2010ME12      Nucl.Phys. A843, 14 (2010)

J.Mendoza-Temis, J.G.Hirsch, A.P.Zuker

The anatomy of the simplest Duflo-Zuker mass formula

ATOMIC MASSES Z=8-108; A=16-256; analyzed masses using DZ10 model. Comparison with other models and data.

doi: 10.1016/j.nuclphysa.2010.05.055
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2007DE14      Phys.Rev. C 75, 034317 (2007)

F.Della Vedova, S.M.Lenzi, M.Ionescu-Bujor, N.Marginean, M.Axiotis, D.Bazzacco, A.M.Bizzeti-Sona, P.G.Bizzeti, A.Bracco, F.Brandolini, D.Bucurescu, E.Farnea, A.Iordachescu, S.Lunardi, T.Martinez, P.Mason, R.Menegazzo, B.Million, D.R.Napoli, M.Nespolo, P.Pavan, C.Rossi Alvarez, C.A.Ur, R.Venturelli, A.P.Zuker

Isospin symmetry breaking at high spin in the mirror nuclei ³⁵Ar and ³⁵Cl

NUCLEAR REACTIONS ²⁴Mg(¹⁶O, nα), (¹⁶O, pα), E=70 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin. ³⁵Ar, ³⁵Cl deduced high-spin levels, J, π, configurations, analog states, spin-orbit interaction effects, isospin symmetry features. GASP, ISIS arrays.

doi: 10.1103/PhysRevC.75.034317
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2006GA33      Phys.Rev.Lett. 97, 152501 (2006)

A.Gadea, S.M.Lenzi, S.Lunardi, N.Marginean, A.P.Zuker, G.de Angelis, M.Axiotis, T.Martinez, D.R.Napoli, E.Farnea, R.Menegazzo, P.Pavan, C.A.Ur, D.Bazzacco, R.Venturelli, P.Kleinheinz, P.Bednarczyk, D.Curien, O.Dorvaux, J.Nyberg, H.Grawe, M.Gorska, M.Palacz, K.Lagergren, L.Milechina, J.Ekman, D.Rudolph, C.Andreoiu, M.A.Bentley, W.Gelletly, B.Rubio, A.Algora, E.Nacher, L.Caballero, M.Trotta, M.Moszynski

Observation of ⁵⁴Ni: Cross-Conjugate Symmetry in f_7/2 Mirror Energy Differences

NUCLEAR REACTIONS ²⁴Mg(³²S, 2n), E=75 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. ⁵⁴Ni deduced levels, J, π. Euroball IV, Euclides arrays. Level systematics in neighboring isobars discussed.

doi: 10.1103/PhysRevLett.97.152501
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2006HI14      Phys.Scr. T125, 158 (2006)

J.G.Hirsch, V.Velazquez, A.Frank, J.Barea, P.Van Isacker, A.P.Zuker

An upper limit of ground-state energy fluctuations in nuclear masses

doi: 10.1088/0031-8949/2006/T125/036
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2006SC29      Phys.Rev.C 74, 061302 (2006)

A.Schwenk, A.P.Zuker

Shell-model phenomenology of low-momentum interactions

NUCLEAR STRUCTURE ^39,41,47,49Ca, ⁴⁹Sc, ⁵⁷Ni; calculated single-particle level energies. Low-momentum interactions, G matrices.

doi: 10.1103/PhysRevC.74.061302
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2005CA39      Rev.Mod.Phys. 77, 427 (2005)

E.Caurier, G.Martinez-Pinedo, F.Nowacki, A.Poves, A.P.Zuker

The shell model as a unified view of nuclear structure

doi: 10.1103/RevModPhys.77.427
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2005MO19      Phys.Rev. C 71, 064317 (2005)

R.A.Molina, A.P.Zuker, A.Relano, J.Retamosa

Spectral statistics of Hamiltonian matrices in tridiagonal form

doi: 10.1103/PhysRevC.71.064317
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2004EK01      Phys.Rev.Lett. 92, 132502 (2004)

J.Ekman, D.Rudolph, C.Fahlander, A.P.Zuker, M.A.Bentley, S.M.Lenzi, C.Andreoiu, M.Axiotis, G.de Angelis, E.Farnea, A.Gadea, Th.Kroll, N.Marginean, T.Martinez, M.N.Mineva, C.Rossi-Alvarez, C.A.Ur

Unusual Isospin-Breaking and Isospin-Mixing Effects in the A = 35 Mirror Nuclei

NUCLEAR REACTIONS ¹⁶O(²⁴Mg, nα), (²⁴Mg, pα), E=60 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. ³⁵Ar deduced levels, J, π, isospin mixing. GASP, ISIS arrays.

doi: 10.1103/PhysRevLett.92.132502
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2004ZU01      Int.J.Mod.Phys. E13, 53 (2004)

A.P.Zuker

Shell formation and three-body forces

doi: 10.1142/S0218301304001722
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2003VE01      Phys.Rev. C 67, 034311 (2003)

V.Velazquez, J.G.Hirsch, A.Frank, A.P.Zuker

A study of randomness, correlations, and collectivity in the nuclear shell model

NUCLEAR STRUCTURE ²⁴Mg, ⁴⁴Ti, ⁴⁸Cr; calculated levels, J, π, B(E2), rotational bands. Comparison of random and collective behavior.

doi: 10.1103/PhysRevC.67.034311
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2003ZU01      Phys.Rev.Lett. 90, 042502 (2003)

A.P.Zuker

Three-Body Monopole Corrections to Realistic Interactions

NUCLEAR STRUCTURE ¹⁰B, ^22,23Na, ²⁴Mg, ^27,28Si, ⁴⁸Cr; calculated level energies, J, contribution from three-body monopole term.

doi: 10.1103/PhysRevLett.90.042502
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2002DU20      Phys.Rev. C 66, 051304 (2002)

J.Duflo, A.P.Zuker

Mirror displacement energies and neutron skins

NUCLEAR STRUCTURE A=6-250; analyzed radii, Coulomb displacement energies; deduced neutron skin parameters.

doi: 10.1103/PhysRevC.66.051304
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2002VE01      Phys.Rev.Lett. 88, 072502 (2002)

V.Velazquez, A.P.Zuker

Spectroscopy with Random and Displaced Random Ensembles

NUCLEAR STRUCTURE ⁴⁸Ca, ^44,46Ti, ⁴⁸Cr; calculated probability densities for level energy ratios, B(E2), collectivity features. Two-body random ensemble.

doi: 10.1103/PhysRevLett.88.072502
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2002ZU04      Phys.Rev.Lett. 89, 142502 (2002)

A.P.Zuker, S.M.Lenzi, G.Martinez-Pinedo, A.Poves

Isobaric Multiplet Yrast Energies and Isospin Nonconserving Forces

NUCLEAR STRUCTURE ⁴⁷V, ^47,49,50Cr, ^49,51Mn, ^50,51Fe; analyzed rotational bands energy differences; deduced role of isospin nonconserving forces.

doi: 10.1103/PhysRevLett.89.142502
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2001LE31      Phys.Rev.Lett. 87, 122501 (2001)

S.M.Lenzi, N.Marginean, D.R.Napoli, C.A.Ur, A.P.Zuker, G.de Angelis, A.Algora, M.Axiotis, D.Bazzacco, N.Belcari, M.A.Bentley, P.G.Bizzeti, A.Bizzeti-Sona, F.Brandolini, P.von Brentano, D.Bucurescu, J.A.Cameron, C.Chandler, M.De Poli, A.Dewald, H.Eberth, E.Farnea, A.Gadea, J.Garces-Narro, W.Gelletly, H.Grawe, R.Isocrate, D.T.Joss, C.A.Kalfas, T.Klug, T.Lampman, S.Lunardi, T.Martinez, G.Martinez-Pinedo, R.Menegazzo, J.Nyberg, Zs.Podolyak, A.Poves, R.V.Ribas, C.Rossi Alvarez, B.Rubio, J.Sanchez-Solano, P.Spolaore, T.Steinhardt, O.Thelen, D.Tonev, A.Vitturi, W.von Oertzen, M.Weiszflog

Coulomb Energy Differences in T = 1 Mirror Rotational Bands in ⁵⁰Fe and ⁵⁰Cr

NUCLEAR REACTIONS ²⁸Si(²⁸Si, 2nα), (²⁸Si, 2pα), E=110 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-, (neutron)γ-coin. ⁵⁰Fe, ⁵⁰Cr deduced high-spin levels, J, π, Coulomb energy differences. Euroball, ISIS arrays. Comparison with shell model calculations.

doi: 10.1103/PhysRevLett.87.122501
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2001ZU01      Phys.Rev. C64, 021303 (2001)

A.P.Zuker

Binomial Level Densities

NUCLEAR STRUCTURE ⁵⁵Mn, ⁵⁶Fe, ⁶⁰Ni; calculated level densities vs excitation energy. Continuous binomial function, comparison with data.

doi: 10.1103/PhysRevC.64.021303
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2001ZU02      Phys.Rev. C64, 021304 (2001)

A.P.Zuker, L.Waha Ndeuna, F.Nowacki, E.Caurier

Canonical Form of Hamiltonian Matrices

NUCLEAR STRUCTURE ⁴⁸Sc, ⁴⁸Ca; calculated matrix elements.

doi: 10.1103/PhysRevC.64.021304
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2000ZU02      Phys.Scr. T88, 157 (2000)

A.P.Zuker

Monopole, Quadrupole and Pairing: A shell model view

doi: 10.1238/Physica.Topical.088a00157
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1999CA12      Phys.Rev. C59, 2033 (1999)

E.Caurier, G.Martinez-Pinedo, F.Nowacki, A.Poves, J.Retamosa, A.P.Zuker

Full 0(h-bar)ω Shell Model Calculation of the Binding Energies of the 1f_7/2 Nuclei

NUCLEAR STRUCTURE ^{42,43,44,45,46,47,48}Ca, ^{42,43,44,45,46,47,48,49}Sc, ^{42,43,44,45,46,47,48,49,50}Ti, ^{43,44,45,46,47,48,49,50,51}V, ^{44,45,46,47,48,49,50,51,52}Cr, ^{45,46,47,48,49,50,51}Mn, ^{46,47,48,49,50,51,52,54}Fe, ^{48,49,50,51,54}Co, ^{50,51,52,54,56}Ni; calculated binding energies, M1, E2, Gamow-Teller sum rules. Shell model, quasispin formalism.

doi: 10.1103/PhysRevC.59.2033
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1999CA60      Nucl.Phys. (Supplement) A654, 747c (1999)

E.Caurier, F.Nowacki, A.P.Zuker, G.Martinez-Pinedo, A.Poves, J.Retamosa

Large Scale Diagonalizations in the pf Shell: Achievements and perspectives

NUCLEAR STRUCTURE ^48,50Cr; calculated levels, J, π. Shell model, comparison with data and with Hartree-Fock-Bogolyubov results. ^58,60Ni; calculated level densities vs excitation energy. Shell model, comparison with data.

doi: 10.1016/S0375-9474(00)88541-3
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1999DE07      Phys.Rev. C59, 2474 (1999)

D.J.Dean, M.T.Ressell, M.Hjorth-Jensen, S.E.Koonin, K.Langanke, A.P.Zuker

Shell-Model Monte Carlo Studies of Neutron-Rich Nuclei in the 1s-0d-1p-0f Shells

NUCLEAR STRUCTURE ^22,32Mg, ²⁰Ne, ^36,46Ar, ^40,42,44S, ⁴²Si, ⁴⁴Ti; calculated binding energies, levels J, π, B(E2), Gamow-Teller strength, configurations. Shell model Monte Carlo calculations.

doi: 10.1103/PhysRevC.59.2474
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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
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1997MA01      Phys.Rev. C55, 187 (1997)

G.Martinez-Pinedo, A.P.Zuker, A.Poves, E.Caurier

Full pf Shell Study of A = 47 and A = 49 Nuclei

NUCLEAR STRUCTURE ⁴⁹Ca, ⁴⁹Sc, ⁴⁹Ti, ⁴⁹V, ⁴⁹Cr; calculated levels, B(λ), μ, binding energies, quadrupole moment, β-decay T_1/2. ⁴⁷Ca, ⁴⁷Sc, ⁴⁷V, ⁴⁷Cr, ⁴⁷Mn, ⁴⁷Fe; calculated β-decay T_1/2, levels, intrinsic quadrupole moments, g-factors, B(λ) ratios in some cases. Shell model approach.

doi: 10.1103/PhysRevC.55.187
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1996DU13      Phys.Rev. C54, 1641 (1996)

M.Dufour, A.P.Zuker

Realistic Collective Nuclear Hamiltonian

NUCLEAR STRUCTURE A=18-38; analyzed level spectra predictions; deduced different realistic interactions similarity.

doi: 10.1103/PhysRevC.54.1641
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1996MA17      Phys.Rev. C53, R2602 (1996)

G.Martinez-Pinedo, A.Poves, E.Caurier, A.P.Zuker

Effective g(A) in the pf Shell

RADIOACTIVITY A=41-50; calculated β-decay associated Gamow-Teller matrix elements; deduced average quenching factor.

doi: 10.1103/PhysRevC.53.R2602
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1995CA08      Phys.Rev.Lett. 74, 1517 (1995)

E.Caurier, A.Poves, A.P.Zuker

Missing and Quenched Gamow-Teller Strength

NUCLEAR REACTIONS ⁴⁸Ca(p, n), E not given; calculated Gamow-Teller transition strength; deduced missing strength, quenching related features, correlations role.

doi: 10.1103/PhysRevLett.74.1517
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1995CA31      Phys.Rev. C52, R1736 (1995)

E.Caurier, G.Martinez-Pinedo, A.Poves, A.P.Zuker

Gamow-Teller Strength in ⁵⁴Fe and ⁵⁶Fe

NUCLEAR REACTIONS ^54,56Fe(p, n), (n, p), E not given; calculated Gamow-Teller transition strength. Large scale shell model.

doi: 10.1103/PhysRevC.52.R1736
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1995CA33      Phys.Rev.Lett. 75, 2466 (1995)

E.Caurier, J.L.Egido, G.Martinez-Pinedo, A.Poves, J.Retamosa, L.M.Robledo, A.P.Zuker

Intrinsic vs Laboratory Frame Description of the Deformed Nucleus ⁴⁸Cr

NUCLEAR STRUCTURE ⁴⁸Cr; calculated levels, g vs spin, B(E2), intrinsic quadrupole moment. Spherical shell model, HFB method.

doi: 10.1103/PhysRevLett.75.2466
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1995DU06      Phys.Rev. C52, R23 (1995)

J.Duflo, A.P.Zuker

Microscopic Mass Formulas

NUCLEAR STRUCTURE Z ≥ 8; N ≥ 8; analyzed binding energies; deduced parameters, rms errors. General scaling arguments based mass formulas.

doi: 10.1103/PhysRevC.52.R23
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1995ZU02      Phys.Rev. C52, R1741 (1995)

A.P.Zuker, J.Retamosa, A.Poves, E.Caurier

Spherical Shell Model Description of Rotational Motion

NUCLEAR STRUCTURE ^{152,154,156,158}Nd, ^{154,156,158,160}Sm, ^{156,158,160,162}Gd, ^{158,160,162,164}Dy; calculated B(E2). Spherical shell model.

doi: 10.1103/PhysRevC.52.R1741
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1994CA21      Phys.Rev. C50, 225 (1994)

E.Caurier, A.P.Zuker, A.Poves, G.Martinez-Pinedo

Full pf Shell Model Study of A = 48 Nuclei

NUCLEAR STRUCTURE ⁴⁸Ca, ⁴⁸Sc, ⁴⁸Ti, ⁴⁸V, ⁴⁸Cr, ⁴⁸Mn; calculated levels, B(λ), Gamow-Teller strength functions. ⁴⁸Fe deduced binding energy. Full pf shell model study.

doi: 10.1103/PhysRevC.50.225
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1994ZU06      Nucl.Phys. A576, 65 (1994)

A.P.Zuker

On the Microscopic Derivation of a Mass Formula

NUCLEAR STRUCTURE Z > 20; N > 20; calculated Coulomb corrected 2 proton-2 neutron separation energies. General microscopic mass formula.

doi: 10.1016/0375-9474(94)90738-2
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1991AB07      Phys.Rev.Lett. 66, 1134 (1991)

A.Abzouzi, E.Caurier, A.P.Zuker

Influence of Saturation Properties on Shell-Model Calculations

NUCLEAR STRUCTURE N=50, 82; Z=28; analyzed radii, spectroscopic data; deduced monopole field role in saturation. Shell model.

doi: 10.1103/PhysRevLett.66.1134
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1991CA07      Phys.Lett. 256B, 301 (1991)

E.Caurier, A.Poves, A.P.Zuker

Spin Quenching and Orbital Enhancement in the Ti Isotopes

NUCLEAR STRUCTURE ^{44,45,46,47,48}Ti; calculated spin, M1 transition strength functions; deduced intruder states features. Exact shell model.

doi: 10.1016/0370-2693(91)91765-N
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1990CA42      Phys.Lett. 252B, 13 (1990)

E.Caurier, A.Poves, A.P.Zuker

A Full 0(h-bar x Omega) Description of the 2νββ Decay of ⁴⁸Ca

RADIOACTIVITY ⁴⁸Ca(2β); calculated 2β-decay T_1/2, Gamow-Teller transition amplitude. ⁴⁸Ti, ⁴⁸Ca; calculated Gamow-Teller β-decay strength function. Shell model.

doi: 10.1016/0370-2693(90)91071-I
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1988DU14      At.Data Nucl.Data Tables 39, 205 (1988)

G.Dussel, E.Caurier, A.P.Zuker

Mass Predictions Based on α-Line Systematics

NUCLEAR STRUCTURE N ≤ 152; compiled 4-nucleon separation energies; deduced masses.

doi: 10.1016/0092-640X(88)90021-6
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1982CO13      Phys.Lett. 115B, 1 (1982)

A.Cortes, R.U.Haq, A.P.Zuker

Transition between Random and Collective Behaviour in Spectra Generated by Two-Body Forces

NUCLEAR STRUCTURE ²⁰Ne; calculated levels, rotational band; deduced random to collective behavior transition. Monte Carlo calculations, gaussian orthogonal ensemble.

doi: 10.1016/0370-2693(82)90502-0
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1979CO09      Phys.Lett. 84B, 25 (1979)

A.Cortes, A.P.Zuker

Self-Consistency and Many-Body Monopole Forces in Shell Model Calculations

NUCLEAR STRUCTURE ^18,19O, ^18,19F, ^20,21,22Ne, ²²Na, ²⁴Mg, ²⁸Si, ³²S, ^34,35,36Cl, ^36,37,38Ar, ³⁸K, ^39,40Ca; calculated binding energies. Many-body monopole forces, self-consistent shell model.

doi: 10.1016/0370-2693(79)90641-5
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1972SO10      Phys.Lett. 41B, 135 (1972)

M.Soyeur, A.P.Zuker

Structure of ²⁸Si, Some Answers and their Problems

NUCLEAR STRUCTURE ²⁸Si; calculated levels, B(E2). Shell model analysis of Hartree-Fock failure.

doi: 10.1016/0370-2693(72)90444-3
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1972WO26      Phys.Lett. 42B, 157 (1972)

S.K.M.Wong, J.M.G.Gomez, A.P.Zuker

A Truncation Scheme for Shell Model Spaces

NUCLEAR STRUCTURE ²⁴Mg; calculated levels, B(E2), B(M1). Wave functions. Shell model;truncation scheme.

doi: 10.1016/0370-2693(72)90049-4
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1971WO13      Phys.Lett. 36B, 437 (1971)

S.K.M.Wong, A.P.Zuker

A Simple Coupling Scheme for Exact Shell Model Calculations

NUCLEAR STRUCTURE ²⁰Ne, ²²Na, ²⁴Mg; calculated basis states. Shell model, antisymmetrized weak coupling basis.

doi: 10.1016/0370-2693(71)90523-5
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1968ZU02      Phys.Rev.Letters 21, 39 (1968)

A.P.Zuker, B.Buck, J.B.McGrory

Structure of O¹⁶

doi: 10.1103/PhysRevLett.21.39
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